id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.2453 | Quasi-Hermitian supersymmetric extensions of a non-Hermitian oscillator
Hamiltonian and of its generalizations | A harmonic oscillator Hamiltonian augmented by a non-Hermitian \pt-symmetric
part and its su(1,1) generalizations, for which a family of positive-definite
metric operators was recently constructed, are re-examined in a supersymmetric
context. Quasi-Hermitian supersymmetric extensions of such Hamiltonians are
proposed by enlarging su(1,1) to a ${\rm su}(1,1/1) \sim {\rm osp}(2/2, \R)$
superalgebra. This allows the construction of new non-Hermitian Hamiltonians
related by similarity to Hermitian ones. Some examples of them are reviewed.
| math-ph hep-th math.MP quant-ph | a harmonic oscillator hamiltonian augmented by a nonhermitian ptsymmetric part and its su11 generalizations for which a family of positivedefinite metric operators was recently constructed are reexamined in a supersymmetric context quasihermitian supersymmetric extensions of such hamiltonians are proposed by enlarging su11 to a rm su111 sim rm osp22 r superalgebra this allows the construction of new nonhermitian hamiltonians related by similarity to hermitian ones some examples of them are reviewed | [['a', 'harmonic', 'oscillator', 'hamiltonian', 'augmented', 'by', 'a', 'nonhermitian', 'ptsymmetric', 'part', 'and', 'its', 'su11', 'generalizations', 'for', 'which', 'a', 'family', 'of', 'positivedefinite', 'metric', 'operators', 'was', 'recently', 'constructed', 'are', 'reexamined', 'in', 'a', 'supersymmetric', 'context', 'quasihermitian', 'supersymmetric', 'extensions', 'of', 'such', 'hamiltonians', 'are', 'proposed', 'by', 'enlarging', 'su11', 'to', 'a', 'rm', 'su111', 'sim', 'rm', 'osp22', 'r', 'superalgebra', 'this', 'allows', 'the', 'construction', 'of', 'new', 'nonhermitian', 'hamiltonians', 'related', 'by', 'similarity', 'to', 'hermitian', 'ones', 'some', 'examples', 'of', 'them', 'are', 'reviewed']] | [-0.13132139518332314, 0.1570048270268287, 0.016051187938321908, 0.09988700147737867, -0.10012474247175727, -0.21969566864132042, -0.09435346674069132, 0.35879625572698376, -0.18749189228606475, -0.2115400187985998, 0.09387730273031171, -0.29498252687458454, -0.21974947786247226, 0.1771668818923579, -0.08997381652351207, 0.12089361343450818, 0.04017394257735618, 0.05893564175709452, -0.18956547955208472, -0.1978196300776072, 0.3288217267598694, 0.016038619841016094, 0.13634193971635064, -0.039471417055530866, 0.06977379609319107, -0.009745809479131244, 0.04276795094360558, -0.06615702583598838, -0.10374464875113376, 0.15413480404515187, 0.27180307414907384, 0.07346709786822468, 0.19497506152576125, -0.33832655729017624, -0.20846908006605588, 0.13847010578750304, 0.13804372623693986, 0.08181241762981763, -0.02255107329922243, -0.41198012437409076, 0.0003666615795711396, -0.2599547035126409, -0.19690911754519796, -0.13412555859384823, 0.0719012309236347, -0.06292871572077274, -0.2289374045778433, 0.022856965162594552, 0.06014659455124761, 0.05134131008772258, -0.020343746188995232, -0.1095799040311659, -0.06785214739576192, -0.057437363461079735, -0.03814310908422504, -0.007621080030910146, 0.09842412518075025, -0.03168630055283052, -0.17457160536645794, 0.4042440598960113, -0.02946906947714447, -0.26952794199468383, 0.10484690864531088, -0.049481597656882564, -0.16503985014311234, 0.06472571398800528, 0.08096062234589751, 0.10968194962282415, -0.1758511476612217, 0.26017660658042485, -0.07692764321683158, 0.041511207950157177, 0.05302463138056263, 0.06774230755235948, 0.15365418660598743, 0.05053266173910717, 0.04663996893623975, 0.15809838675802024, 0.08568744364966849, -0.16644297324409577, -0.3548658657556688, -0.1333366141389747, -0.21097112192549336, 0.10062572406932817, -0.09259170419712794, -0.1179928077552074, 0.47972958241130265, 0.07127419069514308, 0.1723725648308304, 0.0574003395863848, 0.13677169293375083, 0.14754935839331487, 0.14454039269533586, 0.0240047272609573, 0.21658862226283584, 0.2569004135881879, 0.03008377176879997, -0.1845732557425, -0.1714019879016658, 0.19917601238096683] |
710.2454 | Two positivity conjectures for Kerov polynomials | Kerov polynomials express the normalized characters of irreducible
representations of the symmetric group, evaluated on a cycle, as polynomials in
the free cumulants of the associated Young diagram. We present two positivity
conjectures for their coefficients. The latter are stronger than the positivity
conjecture of Kerov-Biane, recently proved by Feray.
| math.CO math.RT | kerov polynomials express the normalized characters of irreducible representations of the symmetric group evaluated on a cycle as polynomials in the free cumulants of the associated young diagram we present two positivity conjectures for their coefficients the latter are stronger than the positivity conjecture of kerovbiane recently proved by feray | [['kerov', 'polynomials', 'express', 'the', 'normalized', 'characters', 'of', 'irreducible', 'representations', 'of', 'the', 'symmetric', 'group', 'evaluated', 'on', 'a', 'cycle', 'as', 'polynomials', 'in', 'the', 'free', 'cumulants', 'of', 'the', 'associated', 'young', 'diagram', 'we', 'present', 'two', 'positivity', 'conjectures', 'for', 'their', 'coefficients', 'the', 'latter', 'are', 'stronger', 'than', 'the', 'positivity', 'conjecture', 'of', 'kerovbiane', 'recently', 'proved', 'by', 'feray']] | [-0.20714255319718194, 0.1219136520364317, -0.10698763924479789, 0.0926328628152913, -0.05857063001211809, -0.08642557174993717, -0.012233870241752997, 0.30164700024286095, -0.24807513322757216, -0.2166087269326862, 0.1049307985302555, -0.24324446230917712, -0.14710895622111098, 0.19107360449828664, -0.07794815161246427, 0.01155796632816901, 0.03228062598452884, 0.0868355171488864, -0.11617088823446206, -0.3274358689632951, 0.34878916631699824, -0.00477870874349218, 0.21886561847082814, 0.06022937687075868, 0.09630074069778226, 0.019382628640730162, -0.10389176931004135, -0.08621142927215111, -0.13617235345157738, 0.16635303127066214, 0.2414717307095701, 0.08733377033578497, 0.17985127942769655, -0.3491410835817152, -0.10656089763803293, 0.15893207612086316, 0.1382916701665951, -0.02648656701250952, 0.006627397010654059, -0.28412083870902355, 0.09434307148033867, -0.19913047190983685, -0.19425350086459395, -0.07396192928510052, 0.051949513087771376, 0.06530523360991965, -0.20962483097552037, 0.10316530062950083, 0.09247355953771241, 0.15796012769700313, -0.0513649377496723, -0.20855673405398822, -0.05024807751939005, 0.10231659514829516, 0.016804382490108207, -0.01886172554626757, 0.029663192279332756, -0.17841310542532984, -0.14691988686669846, 0.3509407430098449, -0.012802689408999868, -0.1988172354746838, 0.11566908923642975, -0.20245918858682319, -0.20646568713709712, 0.10652417125066324, 0.07692084689529574, 0.16541757084885422, -0.06072470177516189, 0.10291579041668043, -0.17254253406533782, 0.027090323285902947, 0.18294709349735355, -0.009459897001483003, 0.13353196837540185, -0.07003380303100055, 0.012330640430505179, 0.22431673375623568, 0.06679399283389009, -0.08481504969602945, -0.2881688442157239, -0.19418084632833393, -0.18643370155264072, 0.042634760880158565, -0.1522574084240715, -0.1711883534848386, 0.408151528512945, 0.08216750963914152, 0.14898796358124392, 0.1545435951224395, 0.17944844017679595, 0.1697257277817104, 0.07949438130207435, 0.02133817543104595, 0.13529853220572885, 0.31351097117710325, 0.01843002234224458, -0.18531704415586225, 0.09955261533661765, 0.25833769583580446] |
710.2455 | Superfluid turbulence and pulsar glitch statistics | Experimental evidence is reviewed for the existence of superfluid turbulence
in a differentially rotating, spherical shell at high Reynolds numbers
($\Rey\gsim 10^3$), such as the outer core of a neutron star. It is shown that
torque variability increases with $\Rey$, suggesting that glitch activity in
radio pulsars may be a function of $\Rey$ as well. The $\Rey$ distribution of
the 67 glitching radio pulsars with characteristic ages $\tau_c \leq 10^6$ {\rm
yr} is constructed from radio timing data and cooling curves and compared with
the $\Rey$ distribution of all 348 known pulsars with $\tau_c \leq 10^6$ {\rm
yr}. The two distributions are different, with a Kolmogorov-Smirnov probability
$\geq 1 - 3.9 \times 10^{-3}$. The conclusion holds for (modified) Urca and
nonstandard cooling, and for Newtonian and superfluid viscosities.
| astro-ph | experimental evidence is reviewed for the existence of superfluid turbulence in a differentially rotating spherical shell at high reynolds numbers reygsim 103 such as the outer core of a neutron star it is shown that torque variability increases with rey suggesting that glitch activity in radio pulsars may be a function of rey as well the rey distribution of the 67 glitching radio pulsars with characteristic ages tau_c leq 106 rm yr is constructed from radio timing data and cooling curves and compared with the rey distribution of all 348 known pulsars with tau_c leq 106 rm yr the two distributions are different with a kolmogorovsmirnov probability geq 1 39 times 103 the conclusion holds for modified urca and nonstandard cooling and for newtonian and superfluid viscosities | [['experimental', 'evidence', 'is', 'reviewed', 'for', 'the', 'existence', 'of', 'superfluid', 'turbulence', 'in', 'a', 'differentially', 'rotating', 'spherical', 'shell', 'at', 'high', 'reynolds', 'numbers', 'reygsim', '103', 'such', 'as', 'the', 'outer', 'core', 'of', 'a', 'neutron', 'star', 'it', 'is', 'shown', 'that', 'torque', 'variability', 'increases', 'with', 'rey', 'suggesting', 'that', 'glitch', 'activity', 'in', 'radio', 'pulsars', 'may', 'be', 'a', 'function', 'of', 'rey', 'as', 'well', 'the', 'rey', 'distribution', 'of', 'the', '67', 'glitching', 'radio', 'pulsars', 'with', 'characteristic', 'ages', 'tau_c', 'leq', '106', 'rm', 'yr', 'is', 'constructed', 'from', 'radio', 'timing', 'data', 'and', 'cooling', 'curves', 'and', 'compared', 'with', 'the', 'rey', 'distribution', 'of', 'all', '348', 'known', 'pulsars', 'with', 'tau_c', 'leq', '106', 'rm', 'yr', 'the', 'two', 'distributions', 'are', 'different', 'with', 'a', 'kolmogorovsmirnov', 'probability', 'geq', '1', '39', 'times', '103', 'the', 'conclusion', 'holds', 'for', 'modified', 'urca', 'and', 'nonstandard', 'cooling', 'and', 'for', 'newtonian', 'and', 'superfluid', 'viscosities']] | [-0.12343745624012728, 0.23934662689100064, -0.03382366707748068, 0.127920947336067, -0.05640495711538408, -0.09246399689702288, 0.04306868825935655, 0.33178338379227734, -0.1594622858489553, -0.34647298049152137, 0.05814522217094366, -0.311351257065932, 0.01099622996139621, 0.2641408922620088, -0.00481055453022395, -0.006803652929467341, 0.025343017340342087, -0.028462935173477505, -0.07134208497443488, -0.1827157139713462, 0.2203604504664702, 0.03814764175977972, 0.21459564433381376, -0.026556935091133393, 0.04737743581663669, -0.12784393577437317, 0.013244358989010965, -0.04982982091753492, -0.17166744929145641, -0.04540808388957798, 0.24485624778927081, 0.1335517047712254, 0.1547372576314956, -0.38501444419047665, -0.2030495345469616, 0.07079505842522762, 0.16472788443414693, -0.009049789433086675, -0.030522083368388905, -0.24145108840191767, 0.11074546518336449, -0.2767557632473726, -0.15426049561661093, 0.02070964748106365, 0.15586184147128185, 0.11532492512866618, -0.2657870583251, 0.18791478836820238, 0.06167052460498073, 0.09400808194556111, -0.13088718116919082, -0.181128171887914, 0.00016639099478544224, -0.008082117504691557, 0.08032174219399513, 0.10910054873896852, 0.13998820890472935, -0.09664381704189712, -0.04962312902456948, 0.36637656786848627, -0.08596721220584143, -0.05384315390672002, 0.18898285529206668, -0.2604682388242393, -0.15856568512459662, 0.15630914185876174, 0.09612230182669702, 0.1178464474718249, -0.08673748376202725, -0.010544534102322475, -0.033722483505871856, 0.2012457471000888, 0.0869326559782383, 0.010737351433832257, 0.2495063443017739, 0.16091763622142255, -0.012233951299022588, 0.05917065011130439, -0.24613126781251696, -0.007926768198284128, -0.2514420161947667, -0.0939906124498636, -0.14649612020187464, 0.1344727524630134, -0.16180063608517808, -0.08222386098373496, 0.2973455487258939, 0.06875350465166516, 0.17410741580118025, 0.10710876544250086, 0.24595397934021931, 0.08968815176991657, 0.0306279077933776, 0.17423679187361682, 0.2743172838337838, 0.22261987805610434, 0.0870578518979961, -0.21663391184004482, 0.07531718479927689, -0.030434251367484056] |
710.2456 | Localization of elastic deformation in strongly anisotropic, porous,
linear materials with periodic microstructures: exact solutions and dilute
expansions | Exact solutions are derived for the problem of a two-dimensional, infinitely
anisotropic, linear-elastic medium containing a periodic lattice of voids. The
matrix material possesses either one infinitely soft, or one infinitely hard
loading direction, which induces localized (singular) field configurations. The
effective elastic moduli are computed as functions of the porosity in each
case. Their dilute expansions feature half-integer powers of the porosity,
which can be correlated to the localized field patterns. Statistical
characterizations of the fields, such as their first moments and their
histograms are provided, with particular emphasis on the singularities of the
latter. The behavior of the system near the void close packing fraction is also
investigated. The results of this work shed light on corresponding results for
strongly nonlinear porous media, which have been obtained recently by means of
the ``second-order'' homogenization method, and where the dilute estimates also
exhibit fractional powers of the porosity.
| cond-mat.mtrl-sci | exact solutions are derived for the problem of a twodimensional infinitely anisotropic linearelastic medium containing a periodic lattice of voids the matrix material possesses either one infinitely soft or one infinitely hard loading direction which induces localized singular field configurations the effective elastic moduli are computed as functions of the porosity in each case their dilute expansions feature halfinteger powers of the porosity which can be correlated to the localized field patterns statistical characterizations of the fields such as their first moments and their histograms are provided with particular emphasis on the singularities of the latter the behavior of the system near the void close packing fraction is also investigated the results of this work shed light on corresponding results for strongly nonlinear porous media which have been obtained recently by means of the secondorder homogenization method and where the dilute estimates also exhibit fractional powers of the porosity | [['exact', 'solutions', 'are', 'derived', 'for', 'the', 'problem', 'of', 'a', 'twodimensional', 'infinitely', 'anisotropic', 'linearelastic', 'medium', 'containing', 'a', 'periodic', 'lattice', 'of', 'voids', 'the', 'matrix', 'material', 'possesses', 'either', 'one', 'infinitely', 'soft', 'or', 'one', 'infinitely', 'hard', 'loading', 'direction', 'which', 'induces', 'localized', 'singular', 'field', 'configurations', 'the', 'effective', 'elastic', 'moduli', 'are', 'computed', 'as', 'functions', 'of', 'the', 'porosity', 'in', 'each', 'case', 'their', 'dilute', 'expansions', 'feature', 'halfinteger', 'powers', 'of', 'the', 'porosity', 'which', 'can', 'be', 'correlated', 'to', 'the', 'localized', 'field', 'patterns', 'statistical', 'characterizations', 'of', 'the', 'fields', 'such', 'as', 'their', 'first', 'moments', 'and', 'their', 'histograms', 'are', 'provided', 'with', 'particular', 'emphasis', 'on', 'the', 'singularities', 'of', 'the', 'latter', 'the', 'behavior', 'of', 'the', 'system', 'near', 'the', 'void', 'close', 'packing', 'fraction', 'is', 'also', 'investigated', 'the', 'results', 'of', 'this', 'work', 'shed', 'light', 'on', 'corresponding', 'results', 'for', 'strongly', 'nonlinear', 'porous', 'media', 'which', 'have', 'been', 'obtained', 'recently', 'by', 'means', 'of', 'the', 'secondorder', 'homogenization', 'method', 'and', 'where', 'the', 'dilute', 'estimates', 'also', 'exhibit', 'fractional', 'powers', 'of', 'the', 'porosity']] | [-0.1222090051041044, 0.16444670739849318, -0.08226638375906486, 0.03160895708629599, -0.04190928204728903, -0.09806828757110458, -0.017514775660289014, 0.3761919727611462, -0.2770329216813931, -0.2498133149507437, 0.12811901611541618, -0.30218497564978647, -0.1449491359721619, 0.17731664616039536, 0.028427967973578498, 0.0772468733895045, 0.011843352083229279, 0.03773821854433389, -0.06901269731105573, -0.24799621478348172, 0.3319430807167852, -0.005174949480808221, 0.26829368488288063, 0.042781985652376744, 0.07210430894484555, -0.005457224688436461, -0.00187949088383341, 0.07753885905227105, -0.14616008493080485, 0.13552121907838263, 0.21811912672894213, -0.026569841099877985, 0.217671255774846, -0.4339397935784303, -0.22652009396420028, 0.08526606217101716, 0.1466151955537498, 0.07862061385343463, -0.05325587278063215, -0.25784158038956756, 0.07116555786010303, -0.11653787998213815, -0.1991452020249211, -0.07267744525573247, 0.025732243505475306, 0.10644949131470248, -0.2491931745457469, 0.10946636154779683, 0.0828635824630162, 0.034033072247457434, -0.0900172958253639, -0.12571661354545755, -0.028504318381103393, 0.08865093354967067, 0.07539312597582955, -0.025734170402506452, 0.13793405551063334, -0.17015757098920556, -0.04786514383021917, 0.3984868731802867, -0.03272362398186811, -0.21832046802811975, 0.1793892676551395, -0.14784933945426604, -0.07837534309739884, 0.1951779297321735, 0.18038304985169595, 0.14860483589613396, -0.1284737886396868, 0.08961393981125056, -0.08109541690905248, 0.13134560331345954, 0.10567224051040791, 0.053844407660224095, 0.20889467269732248, 0.11723672992537336, 0.03758119831905519, 0.16308000840437317, -0.061191506096280664, -0.08734033149260803, -0.26763613203277925, -0.12752683268431825, -0.2020128446431118, 0.042162359673404856, -0.15336388600079948, -0.24768365679336898, 0.363551334515464, 0.06790580468927354, 0.2063112161434787, 0.010444353699477877, 0.22024330185826294, 0.14265161595266662, 0.02840269514322031, 0.04314020314197612, 0.25858494535794846, 0.154470774063828, 0.09495912665335599, -0.1975526320873041, 0.052561589922980975, 0.09132803237728225] |
710.2457 | Multiple point principle as a mechanism for the suppression of FCNC and
CP--violation phenomena in the 2HDM | We argue that multiple point principle (MPP) can be used to ensure CP
conservation and the absence of flavour changing neutral currents within the
two Higgs doublet model (2HDM). We also discuss Higgs phenomenology in the MPP
inspired 2HDM.
| hep-ph | we argue that multiple point principle mpp can be used to ensure cp conservation and the absence of flavour changing neutral currents within the two higgs doublet model 2hdm we also discuss higgs phenomenology in the mpp inspired 2hdm | [['we', 'argue', 'that', 'multiple', 'point', 'principle', 'mpp', 'can', 'be', 'used', 'to', 'ensure', 'cp', 'conservation', 'and', 'the', 'absence', 'of', 'flavour', 'changing', 'neutral', 'currents', 'within', 'the', 'two', 'higgs', 'doublet', 'model', '2hdm', 'we', 'also', 'discuss', 'higgs', 'phenomenology', 'in', 'the', 'mpp', 'inspired', '2hdm']] | [-0.13616017107732403, 0.21866020182959545, 0.01331741482210465, 0.2267586339312868, -0.12209527466732722, -0.2894680740263982, 0.0619601268046655, 0.3224928887226643, -0.24885757176730877, -0.2855607252090405, 0.010824907699432701, -0.17257449688771978, -0.06560612078278492, 0.02196066534648148, -0.007060510303395299, 0.0585311079541078, 0.017114556919878874, -0.09160533115172233, -0.04690042880172722, -0.24584336618845087, 0.3188080348026676, -0.07370725531990711, 0.25128578934340906, 0.10711787559856208, 0.05892532287786404, -0.001841076351224612, 0.019501741020343244, -0.026592257181898907, -0.0716752220157501, 0.10165995032263872, 0.16608504487726933, 0.1313803722986426, 0.06197787861888989, -0.3803974914913758, -0.1646232028515675, 0.25367760825424623, 0.14164770528292045, 0.13746614518981332, -0.06348851094774616, -0.35571733967233926, 0.10606577190069053, -0.21478501806417719, -0.141348807929227, -0.09570592178557163, -0.15731801484257746, -0.13017204203284705, -0.35213507611591083, 0.02954719459432034, -0.07747154611234482, 0.05341800158688178, 0.014495222805402217, -0.13351317337499216, -0.12553619206524813, -0.040023113696429975, 0.25072674363409764, -0.06860016767556469, 0.17235862413564554, -0.17942952651243943, -0.230613848576561, 0.44088117389056164, -0.1516310116276145, -0.2135360038910921, 0.13070161191698831, -0.1526776151970411, -0.22985872389891973, 0.06391525440491162, 0.13714747209675038, 0.02397098576124662, -0.2149258947525269, 0.24015670250474402, -0.06202938101994686, 0.11193476252344389, 0.015788798799547248, 0.01569400891327323, 0.32343577335660273, 0.18896538028732324, 0.07998111866748868, 0.04466678643634973, -0.08035232527897908, -0.15383894007223156, -0.49569956680240396, -0.15330596134448662, -0.0243561849809992, 0.013045141521172646, -0.061415279367326714, -0.04105131535862501, 0.42843224194187385, 0.2230982101188065, 0.22347002524213913, -0.04607077461118118, 0.2553944807404127, 0.11430278666412984, 0.0720737353447662, 0.02074296232790519, 0.35715516635145134, 0.09868064489311133, 0.19217320255791911, -0.2757158551651698, -0.008527294505769625, 0.1433508844855122] |
710.2458 | Indirect Searches for Dark Matter with AMS-02 | AMS-02 is a multi-purpose spectrometer with superconducting magnet, and is
designed for 3 years of data taking aboard the International Space Station. Its
high performance regarding particle identification and energy measurement will
allow performing indirect searches for dark matter (DM) in different channels
simultaneously: gamma rays, positrons and antiprotons. AMS-02 sensitivity to
those signals are presented and --provided the positron excess is due to DM
signal-- it is shown that it allows to probe new physics models in detail. Its
high sensitivity could even be a unique opportunity to reach the Majorana
nature of the DM particle through final state polarization effects.
| astro-ph | ams02 is a multipurpose spectrometer with superconducting magnet and is designed for 3 years of data taking aboard the international space station its high performance regarding particle identification and energy measurement will allow performing indirect searches for dark matter dm in different channels simultaneously gamma rays positrons and antiprotons ams02 sensitivity to those signals are presented and provided the positron excess is due to dm signal it is shown that it allows to probe new physics models in detail its high sensitivity could even be a unique opportunity to reach the majorana nature of the dm particle through final state polarization effects | [['ams02', 'is', 'a', 'multipurpose', 'spectrometer', 'with', 'superconducting', 'magnet', 'and', 'is', 'designed', 'for', '3', 'years', 'of', 'data', 'taking', 'aboard', 'the', 'international', 'space', 'station', 'its', 'high', 'performance', 'regarding', 'particle', 'identification', 'and', 'energy', 'measurement', 'will', 'allow', 'performing', 'indirect', 'searches', 'for', 'dark', 'matter', 'dm', 'in', 'different', 'channels', 'simultaneously', 'gamma', 'rays', 'positrons', 'and', 'antiprotons', 'ams02', 'sensitivity', 'to', 'those', 'signals', 'are', 'presented', 'and', 'provided', 'the', 'positron', 'excess', 'is', 'due', 'to', 'dm', 'signal', 'it', 'is', 'shown', 'that', 'it', 'allows', 'to', 'probe', 'new', 'physics', 'models', 'in', 'detail', 'its', 'high', 'sensitivity', 'could', 'even', 'be', 'a', 'unique', 'opportunity', 'to', 'reach', 'the', 'majorana', 'nature', 'of', 'the', 'dm', 'particle', 'through', 'final', 'state', 'polarization', 'effects']] | [-0.0985953259868456, 0.2194657097570598, -0.10446162237420532, 0.12783707930779487, -0.13042237689974262, -0.16798436123987331, 0.013461518010088042, 0.36330852989910867, -0.2417847505387138, -0.4128639211914703, 0.01934311088053601, -0.3301388441572735, 0.026650303865180296, 0.22839915064190897, 0.029663879935647928, 0.08064555333283566, 0.10827422464225332, -0.02275191307040479, -0.006098275990499293, -0.23098660005694804, 0.19265910458531887, 0.23343104177026772, 0.2553101218095524, 0.08301994252685166, 0.11455215038571909, 0.003302277218751317, -0.050034152563003934, -0.05581960442285373, -0.09558606362599462, 0.0534168478950639, 0.28174949902516827, 0.13435914395513998, 0.12369611394801634, -0.4159593052486433, -0.19300616968094425, 0.21022541742023154, 0.1310840827862586, 0.021000880035845673, -0.10434346366673708, -0.35686867707865494, 0.06659977372699216, -0.21368608649308776, -0.11887984411727053, -0.07102353125468225, -0.0219862149507903, -0.01656693968848855, -0.26740503109370667, 0.014507753044074657, -0.03613066651137071, -0.03489015691950187, -0.07238563339456495, -0.11485112757951606, 0.02101775592959979, 0.05611467628292374, 0.07320783323238549, 8.821878217014612e-05, 0.1870279132488969, -0.14257117802523733, -0.11756334198164005, 0.3813579272263108, -0.05502213085955922, -0.1318915186486408, 0.21005766277712787, -0.20841789037427483, -0.11597370818786908, 0.19324628187014775, 0.17460270234333425, -0.018619288393643265, -0.1794806502704673, 0.13424872166668886, 0.021652128999395406, 0.1751239642195002, 0.008360220050877509, 0.07417679467357184, 0.304564814176867, 0.2365604679045432, 0.10968993597848833, 0.044951813730329054, -0.20915001435159689, 0.013755484529789173, -0.2844944665106881, -0.1839069609630707, -0.14577021972075396, 0.0021919980622353216, 0.014974024859553786, -0.02305742775577385, 0.3851661768641469, 0.12054593176307048, 0.15412566157094404, -0.06253099373048719, 0.3485054334011568, 0.037424341099811534, 0.025244375311897372, 0.010391044174777526, 0.3335579451100499, 0.15586013582936836, 0.15220318395443552, -0.1913128023163653, 0.039950304752553574, -0.064061177908169] |
710.2459 | The average kinetic energy density of Cooper pairs above $T_c$ in ${\rm
YBa_2Cu_3O_{7-x}}$, ${\rm Bi_2Sr_2CaCu_2O_{8+\delta}}$, and ${\rm Nb}$ | We have obtained isofield curves for the square root of the average kinetic
energy density of the superconducting state for three single crystals of
underdoped $YBa_2Cu_3O_{7-x}$, an optimally doped single crystal of
$Bi_2Sr_2CaCu_2O_{8+\delta}$, and Nb. These curves, determined from isofield
magnetization versus temperature measurements and the virial theorem of
superconductivity, probe the order parameter amplitude near the upper critical
field. The striking differences between the Nb and the high-$T_c$ curves
clearly indicate for the latter cases the presence of a unique superconducting
condensate below and above $T_c$.
| cond-mat.supr-con cond-mat.str-el | we have obtained isofield curves for the square root of the average kinetic energy density of the superconducting state for three single crystals of underdoped yba_2cu_3o_7x an optimally doped single crystal of bi_2sr_2cacu_2o_8delta and nb these curves determined from isofield magnetization versus temperature measurements and the virial theorem of superconductivity probe the order parameter amplitude near the upper critical field the striking differences between the nb and the hight_c curves clearly indicate for the latter cases the presence of a unique superconducting condensate below and above t_c | [['we', 'have', 'obtained', 'isofield', 'curves', 'for', 'the', 'square', 'root', 'of', 'the', 'average', 'kinetic', 'energy', 'density', 'of', 'the', 'superconducting', 'state', 'for', 'three', 'single', 'crystals', 'of', 'underdoped', 'yba_2cu_3o_7x', 'an', 'optimally', 'doped', 'single', 'crystal', 'of', 'bi_2sr_2cacu_2o_8delta', 'and', 'nb', 'these', 'curves', 'determined', 'from', 'isofield', 'magnetization', 'versus', 'temperature', 'measurements', 'and', 'the', 'virial', 'theorem', 'of', 'superconductivity', 'probe', 'the', 'order', 'parameter', 'amplitude', 'near', 'the', 'upper', 'critical', 'field', 'the', 'striking', 'differences', 'between', 'the', 'nb', 'and', 'the', 'hight_c', 'curves', 'clearly', 'indicate', 'for', 'the', 'latter', 'cases', 'the', 'presence', 'of', 'a', 'unique', 'superconducting', 'condensate', 'below', 'and', 'above', 't_c']] | [-0.1597247640495242, 0.20331009855141313, -0.04501435101760187, 0.022886279317411197, 0.0004133242343006463, -0.126546337499401, 0.1595830731950272, 0.33100569289948406, -0.22670875814604177, -0.2950323735856874, 0.008339935511580786, -0.390828769247251, -0.021632090039636898, 0.2584734872497361, 0.06070495668755865, 0.04834733176548248, -0.08805847247184694, 0.016540321205667723, -0.16744216071206264, -0.25057858965177643, 0.31524927860618324, -0.008213106184212983, 0.37329953172426117, 0.06833336890097065, 0.05563867589774617, -0.003698810429215945, 0.1408100416080962, 0.040828321186768594, -0.22395702848617716, 0.01957505744421619, 0.26095267976152486, -0.10230011440781427, 0.1324359243949768, -0.3782016412708266, -0.21986238649864306, 0.0809107612411695, 0.12772612833557115, 0.08059925734515078, -0.02744221473219751, -0.23878630060145908, 0.03699537130051303, -0.0441120550793799, -0.16633015851779231, -0.059270837515506936, -0.05080224400594959, 0.03471913288251079, -0.2123282217773898, 0.15539160088218493, 0.052308967650129365, 0.13222537138037674, -0.10486123309438598, -0.17195314958680893, -0.0858731821618289, -0.0007427349049683617, 0.030324998739892722, 0.0815242017758475, 0.15625723875489023, -0.14356458784969545, -0.05060831488152945, 0.2699002257880123, -0.05281545408739141, 0.003209585900988494, 0.06334994711923873, -0.2018520462958292, -0.055707964473457515, 0.17628187530984482, 0.08974992347835702, 0.05306693306192756, -0.10909157188545013, 0.040013114362419853, -0.042558048269711435, 0.2289157399329646, 0.074494034137534, 0.06733019719028781, 0.26064316651130887, 0.1847449225833875, 0.004860448245569293, 0.11941081199168774, -0.192053024461707, -0.034779913782345497, -0.2935045994764686, -0.18709570240636153, -0.1876211013061519, 0.029630711647392862, -0.16134076927796584, -0.19260784081750731, 0.3800892563986367, 0.1137176259506451, 0.20377700836879425, -0.06504111755746363, 0.20397302387389302, 0.12462697149088456, 0.04505880718151557, 0.059326009000598014, 0.28590833865662757, 0.20495666961196338, 0.13247068561399464, -0.3388649893512457, 0.04955556617257582, -0.008845969762963554] |
710.246 | On the uniqueness for the spatially homogeneous Boltzmann equation with
a strong angular singularity | We prove an inequality on the Wasserstein distance with quadratic cost
between two solutions of the spatially homogeneous Boltzmann equation without
angular cutoff, from which we deduce some uniqueness results. In particular, we
obtain a local (in time) well-posedness result in the case of (possibly very)
soft potentials. A global well-posedeness result is shown for all regularized
hard and soft potentials without angular cutoff. Our uniqueness result seems to
be the first one applying to a strong angular singularity, except in the
special case of Maxwell molecules.
Our proof relies on the ideas of Tanaka: we give a probabilistic
interpretation of the Boltzmann equation in terms of a stochastic process. Then
we show how to couple two such processes started with two different initial
conditions, in such a way that they almost surely remain close to each other.
| math.AP | we prove an inequality on the wasserstein distance with quadratic cost between two solutions of the spatially homogeneous boltzmann equation without angular cutoff from which we deduce some uniqueness results in particular we obtain a local in time wellposedness result in the case of possibly very soft potentials a global wellposedeness result is shown for all regularized hard and soft potentials without angular cutoff our uniqueness result seems to be the first one applying to a strong angular singularity except in the special case of maxwell molecules our proof relies on the ideas of tanaka we give a probabilistic interpretation of the boltzmann equation in terms of a stochastic process then we show how to couple two such processes started with two different initial conditions in such a way that they almost surely remain close to each other | [['we', 'prove', 'an', 'inequality', 'on', 'the', 'wasserstein', 'distance', 'with', 'quadratic', 'cost', 'between', 'two', 'solutions', 'of', 'the', 'spatially', 'homogeneous', 'boltzmann', 'equation', 'without', 'angular', 'cutoff', 'from', 'which', 'we', 'deduce', 'some', 'uniqueness', 'results', 'in', 'particular', 'we', 'obtain', 'a', 'local', 'in', 'time', 'wellposedness', 'result', 'in', 'the', 'case', 'of', 'possibly', 'very', 'soft', 'potentials', 'a', 'global', 'wellposedeness', 'result', 'is', 'shown', 'for', 'all', 'regularized', 'hard', 'and', 'soft', 'potentials', 'without', 'angular', 'cutoff', 'our', 'uniqueness', 'result', 'seems', 'to', 'be', 'the', 'first', 'one', 'applying', 'to', 'a', 'strong', 'angular', 'singularity', 'except', 'in', 'the', 'special', 'case', 'of', 'maxwell', 'molecules', 'our', 'proof', 'relies', 'on', 'the', 'ideas', 'of', 'tanaka', 'we', 'give', 'a', 'probabilistic', 'interpretation', 'of', 'the', 'boltzmann', 'equation', 'in', 'terms', 'of', 'a', 'stochastic', 'process', 'then', 'we', 'show', 'how', 'to', 'couple', 'two', 'such', 'processes', 'started', 'with', 'two', 'different', 'initial', 'conditions', 'in', 'such', 'a', 'way', 'that', 'they', 'almost', 'surely', 'remain', 'close', 'to', 'each', 'other']] | [-0.11563075117790478, 0.06447461667983959, -0.13033514971966328, 0.08178295000451054, -0.07902886221300055, -0.13225616763710327, 0.009735492567626246, 0.3578650109145952, -0.30715961022761423, -0.26033532635673234, 0.0903398816699864, -0.2542328447849233, -0.12467114083414925, 0.19620591934527393, -0.05913574664273124, 0.054864735615885125, 0.06928628481978523, 0.0311639831347418, -0.0646232970668833, -0.243671030806634, 0.3566338875224692, 0.004625015804355127, 0.21119929770466642, 0.07754483986038553, 0.11482373205944896, 0.015621220875207497, -0.008658311157689794, 0.0020686450846277285, -0.14235756810328737, 0.0807251769448698, 0.21143498131330463, 0.06247146440285217, 0.2879762463035413, -0.43772766319022555, -0.18970318201699873, 0.13684191236582896, 0.0983005805323626, 0.13230262379806515, -0.043862414545678206, -0.24089142905237773, 0.05651803240281246, -0.11671060436081303, -0.2082045461267125, -0.08042284223230799, -0.011765488382914791, 0.050139424090773085, -0.27873162745052704, 0.1025366376667027, 0.12515700088840895, -0.006634007558982441, -0.1419960001544298, -0.08873686264943925, 0.0035844459029697423, 0.06968899088425805, 0.08144518070532838, 0.022115938645531085, 0.04265183641615769, -0.1144879933335292, -0.10720708885270616, 0.3376333092987213, -0.09643562109398561, -0.24500017173325075, 0.2306418175795588, -0.14705600725837809, -0.16216770684063112, 0.085753326612167, 0.129338732674259, 0.15228803053606246, -0.16989746590590346, 0.10051298138737827, -0.05055065067869652, 0.13264342114595912, 0.10815389985488592, 0.03676359115870319, 0.1262010413363738, 0.10847381667227254, 0.12018412241604233, 0.14692104593099878, -0.03582853573902537, -0.12277071569722307, -0.3376872747414408, -0.13879049906804078, -0.19091788594243184, 0.12096785663279529, -0.12975660025846952, -0.16834902239729738, 0.34189818566665053, 0.12467057205925601, 0.24391355928694963, 0.0977716146617372, 0.24518853845412208, 0.1255417188808349, 0.011582418840945415, 0.10405411766976982, 0.2531415006283762, 0.1336859133620949, 0.12489237705839501, -0.1594334283347606, 0.016573658219768084, 0.1159280222111746] |
710.2461 | The Luminosity Function of X-ray Selected Active Galactic Nuclei:
Evolution of Supermassive Black Holes at High Redshift | We present a measure of the hard (2-8 keV) X-ray luminosity function (XLF) of
Active Galactic Nuclei up to z~5. At high redshifts, the wide area coverage of
the Chandra Multiwavength Project is crucial to detect rare and luminous (Lx >
10^44 erg s^-1) AGN. The inclusion of samples from deeper published surveys,
such as the Chandra Deep Fields, allows us to span the lower Lx range of the
XLF. Our sample is selected from both the hard (z < 3; f(2-8 keV) > 6.3x10^-16
erg cm^-2 s^-1) and soft (z > 3; f(0.5-2.0 keV) > 1.0x10^-16 erg cm^-2 s^-1)
energy band detections. Within our optical magnitude limits (r',i' < 24), we
achieve an adequate level of completeness (>50%) regarding X-ray source
identification (i.e., redshift). We find that the luminosity function is
similar to that found in previous X-ray surveys up to z~3 with an evolution
dependent upon both luminosity and redshift. At z > 3, there is a significant
decline in the numbers of AGN with an evolution rate similar to that found by
studies of optically-selected QSOs. Based on our XLF, we assess the resolved
fraction of the Cosmic X-ray Background, the cumulative mass density of
Supermassive Black Holes (SMBHs), and the comparison of the mean accretion rate
onto SMBHs and the star formation history of galaxies as a function of
redshift. A coevolution scenario up to z~2 is plausible though at higher
redshifts the accretion rate onto SMBHs drops more rapidly. Finally, we
highlight the need for better statistics of high redshift AGN at z > 3, which
is achievable with the upcoming Chandra surveys.
| astro-ph | we present a measure of the hard 28 kev xray luminosity function xlf of active galactic nuclei up to z5 at high redshifts the wide area coverage of the chandra multiwavength project is crucial to detect rare and luminous lx 1044 erg s1 agn the inclusion of samples from deeper published surveys such as the chandra deep fields allows us to span the lower lx range of the xlf our sample is selected from both the hard z 3 f28 kev 63x1016 erg cm2 s1 and soft z 3 f0520 kev 10x1016 erg cm2 s1 energy band detections within our optical magnitude limits ri 24 we achieve an adequate level of completeness 50 regarding xray source identification ie redshift we find that the luminosity function is similar to that found in previous xray surveys up to z3 with an evolution dependent upon both luminosity and redshift at z 3 there is a significant decline in the numbers of agn with an evolution rate similar to that found by studies of opticallyselected qsos based on our xlf we assess the resolved fraction of the cosmic xray background the cumulative mass density of supermassive black holes smbhs and the comparison of the mean accretion rate onto smbhs and the star formation history of galaxies as a function of redshift a coevolution scenario up to z2 is plausible though at higher redshifts the accretion rate onto smbhs drops more rapidly finally we highlight the need for better statistics of high redshift agn at z 3 which is achievable with the upcoming chandra surveys | [['we', 'present', 'a', 'measure', 'of', 'the', 'hard', '28', 'kev', 'xray', 'luminosity', 'function', 'xlf', 'of', 'active', 'galactic', 'nuclei', 'up', 'to', 'z5', 'at', 'high', 'redshifts', 'the', 'wide', 'area', 'coverage', 'of', 'the', 'chandra', 'multiwavength', 'project', 'is', 'crucial', 'to', 'detect', 'rare', 'and', 'luminous', 'lx', '1044', 'erg', 's1', 'agn', 'the', 'inclusion', 'of', 'samples', 'from', 'deeper', 'published', 'surveys', 'such', 'as', 'the', 'chandra', 'deep', 'fields', 'allows', 'us', 'to', 'span', 'the', 'lower', 'lx', 'range', 'of', 'the', 'xlf', 'our', 'sample', 'is', 'selected', 'from', 'both', 'the', 'hard', 'z', '3', 'f28', 'kev', '63x1016', 'erg', 'cm2', 's1', 'and', 'soft', 'z', '3', 'f0520', 'kev', '10x1016', 'erg', 'cm2', 's1', 'energy', 'band', 'detections', 'within', 'our', 'optical', 'magnitude', 'limits', 'ri', '24', 'we', 'achieve', 'an', 'adequate', 'level', 'of', 'completeness', '50', 'regarding', 'xray', 'source', 'identification', 'ie', 'redshift', 'we', 'find', 'that', 'the', 'luminosity', 'function', 'is', 'similar', 'to', 'that', 'found', 'in', 'previous', 'xray', 'surveys', 'up', 'to', 'z3', 'with', 'an', 'evolution', 'dependent', 'upon', 'both', 'luminosity', 'and', 'redshift', 'at', 'z', '3', 'there', 'is', 'a', 'significant', 'decline', 'in', 'the', 'numbers', 'of', 'agn', 'with', 'an', 'evolution', 'rate', 'similar', 'to', 'that', 'found', 'by', 'studies', 'of', 'opticallyselected', 'qsos', 'based', 'on', 'our', 'xlf', 'we', 'assess', 'the', 'resolved', 'fraction', 'of', 'the', 'cosmic', 'xray', 'background', 'the', 'cumulative', 'mass', 'density', 'of', 'supermassive', 'black', 'holes', 'smbhs', 'and', 'the', 'comparison', 'of', 'the', 'mean', 'accretion', 'rate', 'onto', 'smbhs', 'and', 'the', 'star', 'formation', 'history', 'of', 'galaxies', 'as', 'a', 'function', 'of', 'redshift', 'a', 'coevolution', 'scenario', 'up', 'to', 'z2', 'is', 'plausible', 'though', 'at', 'higher', 'redshifts', 'the', 'accretion', 'rate', 'onto', 'smbhs', 'drops', 'more', 'rapidly', 'finally', 'we', 'highlight', 'the', 'need', 'for', 'better', 'statistics', 'of', 'high', 'redshift', 'agn', 'at', 'z', '3', 'which', 'is', 'achievable', 'with', 'the', 'upcoming', 'chandra', 'surveys']] | [-0.027055881961700834, 0.09090121136222251, -0.028310440236964496, 0.15290355342494877, -0.07510132209063158, -0.04174226310351514, 0.09407202605052589, 0.4826777181951911, -0.10406827170299948, -0.3732978923126211, 0.04784936012492835, -0.3637451990279601, 0.04937653811225573, 0.224367349952999, 0.005412630503769833, -0.005998332810577267, -0.0214814523478708, -0.10631092913172324, -0.08769580529337873, -0.33719049149294733, 0.25922225326576154, 0.13277493921020778, 0.20094503681684728, -0.015240825194723584, 0.12259200322478137, -0.05354645779857492, -0.06641878774462384, -0.05589843082589141, -0.17365387508422714, 0.03226281130537245, 0.29785915297907195, 0.149967116272137, 0.256360673585732, -0.29466832309648794, -0.19103346791325748, 0.07545925642443763, 0.19591735249196063, -0.024153280459813686, -0.04679717185155141, -0.2185236150653509, 0.06972238755088256, -0.23841517070059126, -0.15292510811559623, 0.08232396866424097, 0.0371425915400323, 0.036967637469842884, -0.17410970557997985, 0.18829214551919904, -0.007006667246514553, 0.03163996193870844, -0.13716551055517812, -0.06088825869028369, -0.0627655134858287, 0.03893854013381315, 0.05279153447736462, 0.15007746127457722, 0.20048637787476764, -0.18410533346650482, -0.04680552137324412, 0.3467222948129347, -0.029368160393232756, 0.05054016221583879, 0.22173031612192062, -0.25046598285371147, -0.199232437498722, 0.21916008772677742, 0.18246007001653197, 0.10152088534414361, -0.13568254427445936, 0.01739521084914486, 0.00127298842971868, 0.3186848476907471, -0.002228095129794383, 0.06387475509291107, 0.3282330929014279, 0.13234562722755072, 0.06488269753253917, 0.08261541945648787, -0.21606005897865543, 0.06438603541573684, -0.25560861823942105, -0.06392085937523007, -0.11126395858627802, 0.18957996084645856, -0.17612914028876503, -0.08164669284269621, 0.31911656259035226, 0.11197312451622565, 0.2445299412474924, 0.11630752317842052, 0.27681098338946697, 0.11943322657680255, 0.08628921829631508, 0.09887635929771932, 0.3277747352312872, 0.1443240351663917, 0.07125719214354831, -0.202345540915303, 0.007930589685656741, 0.0002568028121459065] |
710.2462 | Two-fluid model of the truncated Euler Equations | A phenomenological two-fluid model of the (time-reversible)
spectrally-truncated 3D Euler equation is proposed. The thermalized small
scales are first shown to be quasi-normal. The effective viscosity and thermal
diffusion are then determined, using EDQNM closure and Monte-Carlo numerical
computations. Finally, the model is validated by comparing its dynamics with
that of the original truncated Euler equation.
| physics.flu-dyn | a phenomenological twofluid model of the timereversible spectrallytruncated 3d euler equation is proposed the thermalized small scales are first shown to be quasinormal the effective viscosity and thermal diffusion are then determined using edqnm closure and montecarlo numerical computations finally the model is validated by comparing its dynamics with that of the original truncated euler equation | [['a', 'phenomenological', 'twofluid', 'model', 'of', 'the', 'timereversible', 'spectrallytruncated', '3d', 'euler', 'equation', 'is', 'proposed', 'the', 'thermalized', 'small', 'scales', 'are', 'first', 'shown', 'to', 'be', 'quasinormal', 'the', 'effective', 'viscosity', 'and', 'thermal', 'diffusion', 'are', 'then', 'determined', 'using', 'edqnm', 'closure', 'and', 'montecarlo', 'numerical', 'computations', 'finally', 'the', 'model', 'is', 'validated', 'by', 'comparing', 'its', 'dynamics', 'with', 'that', 'of', 'the', 'original', 'truncated', 'euler', 'equation']] | [-0.10237369987174004, 0.12778078313567676, -0.14704635682262182, 0.06925041744086359, -0.07974664024576279, -0.1423275503579394, -0.0901680467775025, 0.27431350119877607, -0.3034139185744737, -0.2406875482660585, 0.08882365015701257, -0.2619604554659288, -0.1167713773736198, 0.18343837535108573, 0.05091248874668963, 0.11330415964455044, 0.08052270994604831, -0.025575162651616017, -0.0626891518685235, -0.21490564543221677, 0.29745088565271416, 0.08540020234483693, 0.22037848469751356, 0.006714709805757073, 0.1478427909148325, -0.12551994135303954, -0.04646082225787852, 0.08086772761972887, -0.17846206695022765, 0.02539783132462097, 0.17372288838045538, 0.023395037561255907, 0.19664794707205147, -0.4632747095477368, -0.2557463377514588, 0.005881086099959377, 0.1654863474832382, 0.11810583155602217, -0.008581840165009322, -0.28521168760822285, 0.10740269218305391, -0.20309365487524442, -0.16048739538694332, -0.13565875862592033, 0.019877352502330074, 0.054345642172847874, -0.26702456269413233, 0.1264073204589035, 0.002255259218925078, 0.01799953343080623, -0.11649916442651634, -0.10165571520753604, -0.09080528532753565, 0.05941706046827936, 0.060159161345836765, -0.027157906126896187, 0.10192165931221098, -0.11953165297329958, -0.0754193991264661, 0.4099951274817743, -0.08294765438248371, -0.2970288629154051, 0.16547857796207868, -0.12732570216758177, -0.03042876334594829, 0.17986289724441512, 0.08706294773479126, 0.16686603037773498, -0.14935853535176388, 0.10118331077683251, -0.08698991685897843, 0.1255640711128113, 0.005777997621667704, -0.12407209693420944, 0.12725780807003112, 0.21667830119154782, -0.09614096319169871, 0.12422877572368764, -0.06916378251376695, -0.18556911909087961, -0.2957329614686647, -0.12966505920797186, -0.24345840338251687, 0.050867746342971386, -0.1159103224797166, -0.15530812784553355, 0.3649844294081309, 0.18759680424617337, 0.12593732619591588, 0.13167982357221522, 0.35872226289107595, 0.2157655670328365, -0.03783706278461198, 0.11045624284140233, 0.23755413722288463, 0.1791898749444434, 0.06282651108423513, -0.3020861216770884, 0.035698974796105176, 0.17367555793108685] |
710.2463 | Random close packing of granular matter | We propose an interpretation of the random close packing of granular
materials as a phase transition, and discuss the possibility of experimental
verification.
| cond-mat.soft cond-mat.stat-mech | we propose an interpretation of the random close packing of granular materials as a phase transition and discuss the possibility of experimental verification | [['we', 'propose', 'an', 'interpretation', 'of', 'the', 'random', 'close', 'packing', 'of', 'granular', 'materials', 'as', 'a', 'phase', 'transition', 'and', 'discuss', 'the', 'possibility', 'of', 'experimental', 'verification']] | [-0.16415874528415178, 0.2058958864989741, -0.090971691371954, -0.01626000974489295, -0.03915440274969391, -0.09564631681322404, 0.1403300088384877, 0.3580846546784691, -0.25925015884896985, -0.2934369484529547, 0.10638078425646476, -0.2620449959826858, -0.20854140947694363, 0.11375811048175978, -0.044526983173969, 0.15954002770392792, -0.009205270882533945, -0.002848044199788052, -0.11657091226610962, -0.11950084656153036, 0.2929737207520267, 0.04321230255553256, 0.2971299649418696, 0.09537059034261366, 0.07788702877967255, 0.02032555757171434, 0.03908948499061491, 0.03275113034507503, -0.1966637017853234, 0.07335702767190726, 0.23138024641767793, 0.07743270031136015, 0.2421498363432677, -0.4051874850107276, -0.20719811482274014, 0.07759810331702718, 0.08021922795223477, 0.12780600211218648, -0.13196625973543394, -0.3010709836431172, 0.023438710435901, -0.17442745851028874, -0.12545685000393703, -0.1304285886656979, 0.007346652731623339, 0.016550004077346428, -0.20031664544797462, 0.035444866217996765, 0.08094237428968368, 0.05125565628480652, -0.10628485444771207, -0.10469140541618285, 0.07221876878453337, 0.07226959128013771, -0.003043826077254894, -0.00370442523094623, 0.14623595824789093, -0.16058642579161603, -0.17693009956375413, 0.48785420928312384, 0.011813378568900667, -0.06982952947525875, 0.2298428299634353, -0.10449264490086099, -0.12732052823285694, 0.11870023349057073, 0.2141304798424244, 0.06364083120032497, -0.08293456458689077, -0.00800911523654814, -0.08993030112722646, 0.1708758010164551, -0.007209537024407283, 0.016580397992030434, 0.28743963559036667, 0.26520758713393106, 0.031195826970202768, 0.2946546654338422, -0.10769340979016345, -0.0616752404274176, -0.31992685535679694, -0.24208283039700726, -0.20722084314278935, -0.008113682513003763, -0.14084915537323864, -0.25559162089358206, 0.34679372066065023, 0.21466481637047685, 0.287033886851176, 0.0508868430700639, 0.2572131275361323, 0.07683638260072179, -0.05820695246043413, -0.024921171691106712, 0.25736665498951206, 0.14914866779809413, 0.11316725004302419, -0.18707933633223825, 0.10864630375948289, 0.04446168567823327] |
710.2464 | The 26 year-long X-ray light curve and the X-ray spectrum of the BL Lac
Object 1E 1207.9+3945 in its brightest state | We studied the temporal and spectral evolution of the synchrotron emission
from the high energy peaked BL Lac object 1E 1207.9+3945. Two recent
observations have been performed by the XMM-Newton and Swift satellites; we
carried out X-ray spectral analysis for both of them, and photometry in
optical-ultraviolet filters for the Swift one. Combining the results thus
obtained with archival data we built the long-term X-ray light curve, spanning
a time interval of 26 years, and the Spectral Energy Distribution (SED) of this
source. The light curve shows a large flux increasing, about a factor of six,
in a time interval of a few years. After reaching its maximum in coincidence
with the XMM-Newton pointing in December 2000 the flux decreased in later
years, as revealed by Swift. The very good statistics available in the 0.5-10
keV XMM-Newton X-ray spectrum points out a highly significant deviation from a
single power law. A log-parabolic model with a best fit curvature parameter of
0.25 and a peak energy at ~1 keV describes well the spectral shape of the
synchrotron emission. The simultaneous fit of Swift UVOT and XRT data provides
a milder curvature (b~0.1) and a peak at higher energies (~15 keV), suggesting
a different state of source activity. In both cases UVOT data support the
scenario of a single synchrotron emission component extending from the
optical/UV to the X-ray band. New X-ray observations are important to monitor
the temporal and spectral evolution of the source; new generation gamma-ray
telescopes like AGILE and GLAST could for the first time detect its inverse
Compton emission.
| astro-ph | we studied the temporal and spectral evolution of the synchrotron emission from the high energy peaked bl lac object 1e 120793945 two recent observations have been performed by the xmmnewton and swift satellites we carried out xray spectral analysis for both of them and photometry in opticalultraviolet filters for the swift one combining the results thus obtained with archival data we built the longterm xray light curve spanning a time interval of 26 years and the spectral energy distribution sed of this source the light curve shows a large flux increasing about a factor of six in a time interval of a few years after reaching its maximum in coincidence with the xmmnewton pointing in december 2000 the flux decreased in later years as revealed by swift the very good statistics available in the 0510 kev xmmnewton xray spectrum points out a highly significant deviation from a single power law a logparabolic model with a best fit curvature parameter of 025 and a peak energy at 1 kev describes well the spectral shape of the synchrotron emission the simultaneous fit of swift uvot and xrt data provides a milder curvature b01 and a peak at higher energies 15 kev suggesting a different state of source activity in both cases uvot data support the scenario of a single synchrotron emission component extending from the opticaluv to the xray band new xray observations are important to monitor the temporal and spectral evolution of the source new generation gammaray telescopes like agile and glast could for the first time detect its inverse compton emission | [['we', 'studied', 'the', 'temporal', 'and', 'spectral', 'evolution', 'of', 'the', 'synchrotron', 'emission', 'from', 'the', 'high', 'energy', 'peaked', 'bl', 'lac', 'object', '1e', '120793945', 'two', 'recent', 'observations', 'have', 'been', 'performed', 'by', 'the', 'xmmnewton', 'and', 'swift', 'satellites', 'we', 'carried', 'out', 'xray', 'spectral', 'analysis', 'for', 'both', 'of', 'them', 'and', 'photometry', 'in', 'opticalultraviolet', 'filters', 'for', 'the', 'swift', 'one', 'combining', 'the', 'results', 'thus', 'obtained', 'with', 'archival', 'data', 'we', 'built', 'the', 'longterm', 'xray', 'light', 'curve', 'spanning', 'a', 'time', 'interval', 'of', '26', 'years', 'and', 'the', 'spectral', 'energy', 'distribution', 'sed', 'of', 'this', 'source', 'the', 'light', 'curve', 'shows', 'a', 'large', 'flux', 'increasing', 'about', 'a', 'factor', 'of', 'six', 'in', 'a', 'time', 'interval', 'of', 'a', 'few', 'years', 'after', 'reaching', 'its', 'maximum', 'in', 'coincidence', 'with', 'the', 'xmmnewton', 'pointing', 'in', 'december', '2000', 'the', 'flux', 'decreased', 'in', 'later', 'years', 'as', 'revealed', 'by', 'swift', 'the', 'very', 'good', 'statistics', 'available', 'in', 'the', '0510', 'kev', 'xmmnewton', 'xray', 'spectrum', 'points', 'out', 'a', 'highly', 'significant', 'deviation', 'from', 'a', 'single', 'power', 'law', 'a', 'logparabolic', 'model', 'with', 'a', 'best', 'fit', 'curvature', 'parameter', 'of', '025', 'and', 'a', 'peak', 'energy', 'at', '1', 'kev', 'describes', 'well', 'the', 'spectral', 'shape', 'of', 'the', 'synchrotron', 'emission', 'the', 'simultaneous', 'fit', 'of', 'swift', 'uvot', 'and', 'xrt', 'data', 'provides', 'a', 'milder', 'curvature', 'b01', 'and', 'a', 'peak', 'at', 'higher', 'energies', '15', 'kev', 'suggesting', 'a', 'different', 'state', 'of', 'source', 'activity', 'in', 'both', 'cases', 'uvot', 'data', 'support', 'the', 'scenario', 'of', 'a', 'single', 'synchrotron', 'emission', 'component', 'extending', 'from', 'the', 'opticaluv', 'to', 'the', 'xray', 'band', 'new', 'xray', 'observations', 'are', 'important', 'to', 'monitor', 'the', 'temporal', 'and', 'spectral', 'evolution', 'of', 'the', 'source', 'new', 'generation', 'gammaray', 'telescopes', 'like', 'agile', 'and', 'glast', 'could', 'for', 'the', 'first', 'time', 'detect', 'its', 'inverse', 'compton', 'emission']] | [-0.04625573997540274, 0.08850023804205613, -0.10449323875005716, 0.12671460345065078, -0.09488547431448331, -0.11709090522400892, 0.07925420926812177, 0.47956122418579, -0.20260525689675257, -0.3882865813990625, 0.09849114227287759, -0.35297760224113095, 0.02893204786277448, 0.24655575218270176, -0.018086888637536994, 0.03800593684203565, 0.09458136010529974, -0.07589316724333912, -0.05479450998402451, -0.20791687993153643, 0.23435620506956745, 0.15100089267093258, 0.23086198890635456, 0.013675588313848352, 0.09440835400153166, 0.0003286509192548692, -0.09192495616287208, -0.035778345282212215, -0.057679815685304885, 0.07815858901549991, 0.2225272480559607, 0.10898385326346705, 0.20449480509313828, -0.3402287892782344, -0.27186886884290007, 0.06570128641436056, 0.11485787155957392, -0.05992652363179681, -0.006379413221013517, -0.2642832765552717, 0.0013185817363242118, -0.20262835341362426, -0.16545124311591142, 0.04551798448620292, 0.035428626582814524, 0.022678182046645536, -0.17768333357660315, 0.09729584320000588, -0.01505052709040823, 0.08252390383724839, -0.1694402755489976, -0.05826705259163506, -0.023796320823916736, 0.06303625064902008, 0.07004851474955033, 0.046787996237309504, 0.08850951874785376, -0.11710111729961892, -0.1054868331232753, 0.34309010373321003, -0.07937582773671378, 0.07974050345454509, 0.1338780367299198, -0.2031365581143361, -0.20910842172228372, 0.23372881297881787, 0.10644677685967718, 0.10164362386536735, -0.152446452413614, 0.03448941580785546, 0.0014756817415428275, 0.2720322568399402, 0.06004199274958899, 0.04516322556256245, 0.26789707857667683, 0.14724354579050739, 0.015524150526527171, 0.14387285037127395, -0.29126424992987615, 0.01698846002198899, -0.269118429089968, -0.06058465861894477, -0.16374393937160045, 0.11037239927055242, -0.11503671590510818, -0.10418825711732586, 0.4593895364785567, 0.05495885714637832, 0.22500435326320048, 0.04714387611199457, 0.3066899007795235, 0.11146344945882447, 0.05724186854114613, 0.10455962024503745, 0.3247717793027942, 0.08437736715064742, 0.1849488688328375, -0.19415001357242895, 0.002926144778029993, -0.04233478015611092] |
710.2465 | A geometric construction for fractal sets and related linear operators | A way to add an extra dimension is briefly discussed.
| math.CA | a way to add an extra dimension is briefly discussed | [['a', 'way', 'to', 'add', 'an', 'extra', 'dimension', 'is', 'briefly', 'discussed']] | [-0.1454069759696722, 0.18376894627144794, -0.03725124299526215, 0.15386928381631151, -0.1628725770395249, -0.24740571598522365, -0.008947497606277466, 0.36320770867168906, -0.2699346859008074, -0.20162151623517274, 0.12465763185173273, -0.2695213398896158, -0.19880231767892836, 0.12175249420106411, -0.15157001866027714, -0.08274988700868562, -0.0745784037746489, 0.1111177921295166, -0.01994461417198181, -0.36626021526753905, 0.36189118325710296, 0.1694482436403632, 0.15264635980129243, 0.07268087121192365, 0.13184719532728195, -0.046425425074994565, -0.11963512934744358, 0.020496363379061223, -0.16050592688843607, 0.1716244095005095, 0.15279147773981094, 0.10825608291197568, 0.2066984847187996, -0.38540261443704366, -0.2399424746632576, 0.0420989491045475, 0.2204892948269844, 0.19281559213995933, -0.11904099211096764, -0.19510443210601808, 0.04873433783650398, -0.21875494420528413, -0.3849085198715329, -0.14399431152269243, 0.08999285325407982, -0.18328414689749478, -0.2239346497692168, -0.08820610456168651, 0.08549037724733352, 0.012669951282441616, -0.002844345883931965, -0.15201160162687302, 0.0313033452257514, 0.01354163441574201, 0.0925979221938178, 0.07430473044514656, 0.0837680222466588, -0.06829936665017158, -0.18584868176840247, 0.3729876726400107, -0.022856610547751188, -0.3130119353532791, 0.21343034142628312, -0.006641731504350901, -0.14162113033235074, -0.004818156361579895, 0.10469720996916294, -0.032526354491710666, -0.23729831129312515, 0.14269382506608963, 0.021126219350844622, 0.2504238910973072, 0.04007875695824623, 0.10277209170162678, 0.13439882192760705, 0.23677846919745207, 0.12912908419966698, 0.2440143359825015, -0.058285655826330184, -0.02829269953072071, -0.47141540944576266, -0.21884972155094146, -0.07662663832306862, 0.05896032238379121, -0.052259805239737035, -0.07133163213729858, 0.3027765844017267, 0.19623477347195148, 0.3038213811814785, -0.070637246966362, 0.3586083002388477, 0.13576783649623395, 0.06245885565876961, 0.06240801210515201, 0.1737432535737753, 0.13033019984140992, 0.06891779489815235, -0.09902837504632771, -0.0533493640832603, 0.08698604868259281] |
710.2466 | On the dynamics of (left) orderable groups | We study left orderable groups by using dynamical methods. We apply these
techniques to study the space of orderings of these groups. We show for
instance that for the case of (non-Abelian) free groups, this space is
homeomorphic to the Cantor set. We also study the case of braid groups (for
which the space of orderings has isolated points but contains homeomorphic
copies of the Cantor set). To do this we introduce the notion of the Conradian
soul of an order as the maximal subgroup which is convex and restricted to
which the original ordering satisfies the so called conradian property, and we
elaborate on this notion.
| math.GR math.DS | we study left orderable groups by using dynamical methods we apply these techniques to study the space of orderings of these groups we show for instance that for the case of nonabelian free groups this space is homeomorphic to the cantor set we also study the case of braid groups for which the space of orderings has isolated points but contains homeomorphic copies of the cantor set to do this we introduce the notion of the conradian soul of an order as the maximal subgroup which is convex and restricted to which the original ordering satisfies the so called conradian property and we elaborate on this notion | [['we', 'study', 'left', 'orderable', 'groups', 'by', 'using', 'dynamical', 'methods', 'we', 'apply', 'these', 'techniques', 'to', 'study', 'the', 'space', 'of', 'orderings', 'of', 'these', 'groups', 'we', 'show', 'for', 'instance', 'that', 'for', 'the', 'case', 'of', 'nonabelian', 'free', 'groups', 'this', 'space', 'is', 'homeomorphic', 'to', 'the', 'cantor', 'set', 'we', 'also', 'study', 'the', 'case', 'of', 'braid', 'groups', 'for', 'which', 'the', 'space', 'of', 'orderings', 'has', 'isolated', 'points', 'but', 'contains', 'homeomorphic', 'copies', 'of', 'the', 'cantor', 'set', 'to', 'do', 'this', 'we', 'introduce', 'the', 'notion', 'of', 'the', 'conradian', 'soul', 'of', 'an', 'order', 'as', 'the', 'maximal', 'subgroup', 'which', 'is', 'convex', 'and', 'restricted', 'to', 'which', 'the', 'original', 'ordering', 'satisfies', 'the', 'so', 'called', 'conradian', 'property', 'and', 'we', 'elaborate', 'on', 'this', 'notion']] | [-0.14783127398761076, 0.11375720332287988, -0.09017510209493687, 0.07156550471135632, -0.09118252640120059, -0.05317731189136785, 0.07201488466637436, 0.37474725606729425, -0.3067002040899803, -0.226151998498625, 0.11341616579235714, -0.28784075449438434, -0.14610549755324828, 0.16421560962384166, -0.1288469936002359, -0.020016847578721627, 0.018505468303076575, 0.11601562920531311, -0.08563037990662052, -0.28418481104711296, 0.43023990213905816, -0.06376582769694451, 0.22582406630722163, 0.014228205640460843, 0.11906255225468183, 0.017423298388336585, -0.016450183013471488, 0.04161783247543107, -0.19186014644443938, 0.1327418495039238, 0.22250644476414075, 0.12830936546202434, 0.23996985815117292, -0.35004465351594943, -0.15629753820754796, 0.22041681888469747, 0.1275420333215288, 0.029652878928224546, -0.022385376006164633, -0.27654125379119937, 0.13688053987989915, -0.15371850726551542, -0.12713209304427642, -0.11545718450830361, 0.025092393434040735, -0.021318796084253726, -0.2058085202213342, -0.003385015293601117, 0.12875209756007322, 0.0688199678905935, -0.0640073018561979, -0.05914469785709804, -0.031934955366234356, 0.12841310188887972, 0.03651896665290555, 0.016880992946876474, 0.056653703271333025, -0.04210508094690348, -0.1489248133566944, 0.4200482206227623, -0.016158579953154114, -0.23157336709968676, 0.19564020550357195, -0.17153255137447354, -0.2036182588471152, 0.09007924510096417, 0.11776165005307053, 0.14817840505008387, -0.06981856902086428, 0.1553917513870869, -0.15984697370990136, 0.1103018904235388, 0.06278510011285005, 0.027045087397063725, 0.10849749979565233, 0.12995990161364027, 0.14248342371859074, 0.19392408227339109, -0.009700130312224832, -0.025033618175537786, -0.33063550289093613, -0.19367598777062425, -0.11916947581535467, 0.0699458944341429, -0.027684872776050137, -0.23553810006651643, 0.40667523256128774, 0.1339516485127333, 0.14497456647386062, 0.08223401136134934, 0.21607397312176563, 0.045100627994985175, 0.07726145333068654, 0.06999227392517691, 0.11947614207502594, 0.13845470429955173, -0.056142153544786653, -0.16260209572001003, -0.00809300745724239, 0.18438989367927902] |
710.2467 | Track-Based Particle Flow | One of the most important aspects of detector development for the ILC is a
good jet energy resolution sigma_E/E. To achieve the goal of high precision
measurements sigma_E/E = 0.30/sqrt(E(GeV)} is proposed. The particle flow
approach together with highly granular calorimeters is able to reach this goal.
This paper presents a new particle flow algorithm, called Track-Based particle
flow, and shows first performance results for 45 GeV jets based on full
detector simulation of the Tesla TDR detector model.
| physics.ins-det physics.data-an | one of the most important aspects of detector development for the ilc is a good jet energy resolution sigma_ee to achieve the goal of high precision measurements sigma_ee 030sqrtegev is proposed the particle flow approach together with highly granular calorimeters is able to reach this goal this paper presents a new particle flow algorithm called trackbased particle flow and shows first performance results for 45 gev jets based on full detector simulation of the tesla tdr detector model | [['one', 'of', 'the', 'most', 'important', 'aspects', 'of', 'detector', 'development', 'for', 'the', 'ilc', 'is', 'a', 'good', 'jet', 'energy', 'resolution', 'sigma_ee', 'to', 'achieve', 'the', 'goal', 'of', 'high', 'precision', 'measurements', 'sigma_ee', '030sqrtegev', 'is', 'proposed', 'the', 'particle', 'flow', 'approach', 'together', 'with', 'highly', 'granular', 'calorimeters', 'is', 'able', 'to', 'reach', 'this', 'goal', 'this', 'paper', 'presents', 'a', 'new', 'particle', 'flow', 'algorithm', 'called', 'trackbased', 'particle', 'flow', 'and', 'shows', 'first', 'performance', 'results', 'for', '45', 'gev', 'jets', 'based', 'on', 'full', 'detector', 'simulation', 'of', 'the', 'tesla', 'tdr', 'detector', 'model']] | [-0.05869744987795492, 0.10169438776475462, -0.11802326732423979, 0.01947345295709304, -0.07402082887030655, -0.14723524084774317, -0.0628467287925713, 0.3729220853223429, -0.17758990913272726, -0.3733355012032893, 0.04898587696544536, -0.294003113862369, -0.025048211507208935, 0.2248218790869918, -0.05325792065833683, 0.16262445128492575, 0.17127202963305324, 0.0052498245805308414, -0.02327354959448098, -0.19273143187286212, 0.22296096692950307, 0.21422723967388466, 0.31689576069255926, 0.09431020853218514, 0.22436312070817915, -0.02646216347075805, -0.03270338655921159, 0.013698082163252613, -0.14524362105634306, 0.10015011511670498, 0.2613157730779381, 0.09690458915353596, 0.2245721638861472, -0.3624816589396108, -0.14098244229960558, 0.047561228650247124, 0.10587018204236089, 0.02966108415638665, -0.07958146153084401, -0.22769065924569384, 0.1534675797235898, -0.203758841017624, -0.11839453153941151, -0.043206105516715484, -0.09197655241549402, -0.00912933542647145, -0.26439604361529473, 0.033601499855058725, 0.022290338647201077, 0.04859670684612417, -0.0005196175785952961, -0.11209256316281178, 0.07670647221581116, 0.05318276708123165, 0.026363655209674368, 0.09106043559898223, 0.18451647802147192, -0.1714110522676114, -0.1519270313075175, 0.39492234515098784, -0.02901584245627383, -0.1743631563134274, 0.21129505914127963, -0.18163972343741494, -0.12422672240668303, 0.19739262958045128, 0.2543758679205528, 0.0998257448316201, -0.1742892609637037, -0.017452469326150542, -0.00454722929068587, 0.20439700315428244, -0.013780905683706332, -0.004819323091054118, 0.17891686111265284, 0.33303740047305436, 0.11469172375494396, 0.1186844655403311, -0.17604088158552328, -0.04694615210128295, -0.3485987846340452, -0.1733942637099074, -0.13718215660675875, -0.013563274756654517, -0.05342009208182496, -0.06250656875116485, 0.4412350276267374, 0.19183083345460428, 0.19044481793587859, 0.005590507494551795, 0.3615935665370848, 0.022991076146566924, 0.04237415798177773, 0.0961268741347186, 0.2959588229196606, 0.1344062585577175, 0.19160424846575244, -0.19805914308125902, 0.02069308650347271, 0.05218429196408236] |
710.2468 | Statistics in the Landscape of Intersecting Brane Models | An approach towards a statistical survey of four dimensional supersymmetric
vacua in the string theory landscape is described and illustrated with three
examples of ensembles of intersecting D-brane models. The question whether it
is conceivable to make predictions based on statistical distributions is
discussed. Especially interesting in this context are possible correlations
between low energy observables. As an example we look at correlations between
properties of the gauge sector of intersecting D-brane models and Gepner model
constructions.
| hep-th | an approach towards a statistical survey of four dimensional supersymmetric vacua in the string theory landscape is described and illustrated with three examples of ensembles of intersecting dbrane models the question whether it is conceivable to make predictions based on statistical distributions is discussed especially interesting in this context are possible correlations between low energy observables as an example we look at correlations between properties of the gauge sector of intersecting dbrane models and gepner model constructions | [['an', 'approach', 'towards', 'a', 'statistical', 'survey', 'of', 'four', 'dimensional', 'supersymmetric', 'vacua', 'in', 'the', 'string', 'theory', 'landscape', 'is', 'described', 'and', 'illustrated', 'with', 'three', 'examples', 'of', 'ensembles', 'of', 'intersecting', 'dbrane', 'models', 'the', 'question', 'whether', 'it', 'is', 'conceivable', 'to', 'make', 'predictions', 'based', 'on', 'statistical', 'distributions', 'is', 'discussed', 'especially', 'interesting', 'in', 'this', 'context', 'are', 'possible', 'correlations', 'between', 'low', 'energy', 'observables', 'as', 'an', 'example', 'we', 'look', 'at', 'correlations', 'between', 'properties', 'of', 'the', 'gauge', 'sector', 'of', 'intersecting', 'dbrane', 'models', 'and', 'gepner', 'model', 'constructions']] | [-0.09807365520119474, 0.1480323047979656, -0.09564827205976109, 0.18858126911044412, -0.01363170697571492, -0.19985338713514147, -0.00614435509204042, 0.3550581161247252, -0.19510368954438667, -0.3106533442502962, 0.06650759695194565, -0.3074298317985633, -0.1376956484474048, 0.15965855774445484, -0.04569904504914321, 0.03571535998882799, 0.016686523804900707, 0.007591832477551002, -0.05736908019148418, -0.26741162160193765, 0.3489905733603065, 0.07013512007867942, 0.2968009313108859, 0.049444163326996485, 0.08123846852837445, -0.03965860289633395, -0.03189974234669239, 0.012586602844394647, -0.14698317776397837, 0.13525379025800663, 0.24658239194822829, 0.13736353204404186, 0.13479350415336622, -0.4093459698238543, -0.23012289306898784, 0.13558510103105725, 0.13926755092046283, 0.16355607449379447, -0.01242011643540985, -0.26065921495583927, 0.011201732743579846, -0.1535222420057693, -0.16267985120822384, -0.08835683234471392, 0.019698629500465345, -0.042692072375060675, -0.21568597047650195, 0.05519052610019004, 0.00862859029855047, 0.09703482416543094, -0.02231758769432252, -0.10911118994200868, -0.05688352249683691, 0.06511397958527525, 0.1257799213597938, -0.007195045863120974, 0.09784505412877574, -0.20166475270610595, -0.17839672861548214, 0.38636873118192344, -0.010627257190160937, -0.20803102831561843, 0.19359254436990755, -0.0810390053099239, -0.20173837696262575, 0.029880180454498473, 0.13392482987036566, 0.13446149788796902, -0.1496209100300035, 0.15772796398251357, -0.03186246498741887, 0.12955435555331507, 0.05215258282524618, 0.0581982581960884, 0.31506019178777933, 0.20654189181453608, 0.00972555974474201, 0.14965111389756203, -0.030431491682644595, -0.1920294251735927, -0.4140116868709976, -0.06392292591271462, -0.11729451314872735, 0.06734665142759294, -0.08647999096043445, -0.16376933159137314, 0.4030670902703877, 0.16061071132222046, 0.22219293945856006, 0.01024508856043413, 0.20982607606459747, 0.029440447819636915, -0.004832539326426658, 0.009637943154515384, 0.22093792732006737, 0.1422742430087445, 0.017586748883757112, -0.149771867809793, -0.07206045595517793, 0.10162450554296858] |
710.2469 | CP violation and final state interactions in B --> K pi pi decays | Effects of CP violation and of final state interactions between pairs of
pseudoscalar mesons are studied in three-body B+, B-, B0 and antiB0 decays into
K pi pi. An alternative approach to the isobar model for three-body B decays is
proposed. It is based on the QCD factorization approximation and the knowledge
of the meson-meson form factors. Some phenomenological charming penguin
amplitudes are needed to describe the branching fractions, direct CP
asymmetries of the quasi-two-body B --> K*(892) pi and B --> K0*(1430) pi
decays as well as the K pi effective mass and the helicity angle distributions.
The experimental branching fractions for the B --> K0*(1430) pi decay, obtained
by the Belle and BaBar collaborations using the isobar model, are larger than
our predictions by about 52 per cent.
| hep-ph | effects of cp violation and of final state interactions between pairs of pseudoscalar mesons are studied in threebody b b b0 and antib0 decays into k pi pi an alternative approach to the isobar model for threebody b decays is proposed it is based on the qcd factorization approximation and the knowledge of the mesonmeson form factors some phenomenological charming penguin amplitudes are needed to describe the branching fractions direct cp asymmetries of the quasitwobody b k892 pi and b k01430 pi decays as well as the k pi effective mass and the helicity angle distributions the experimental branching fractions for the b k01430 pi decay obtained by the belle and babar collaborations using the isobar model are larger than our predictions by about 52 per cent | [['effects', 'of', 'cp', 'violation', 'and', 'of', 'final', 'state', 'interactions', 'between', 'pairs', 'of', 'pseudoscalar', 'mesons', 'are', 'studied', 'in', 'threebody', 'b', 'b', 'b0', 'and', 'antib0', 'decays', 'into', 'k', 'pi', 'pi', 'an', 'alternative', 'approach', 'to', 'the', 'isobar', 'model', 'for', 'threebody', 'b', 'decays', 'is', 'proposed', 'it', 'is', 'based', 'on', 'the', 'qcd', 'factorization', 'approximation', 'and', 'the', 'knowledge', 'of', 'the', 'mesonmeson', 'form', 'factors', 'some', 'phenomenological', 'charming', 'penguin', 'amplitudes', 'are', 'needed', 'to', 'describe', 'the', 'branching', 'fractions', 'direct', 'cp', 'asymmetries', 'of', 'the', 'quasitwobody', 'b', 'k892', 'pi', 'and', 'b', 'k01430', 'pi', 'decays', 'as', 'well', 'as', 'the', 'k', 'pi', 'effective', 'mass', 'and', 'the', 'helicity', 'angle', 'distributions', 'the', 'experimental', 'branching', 'fractions', 'for', 'the', 'b', 'k01430', 'pi', 'decay', 'obtained', 'by', 'the', 'belle', 'and', 'babar', 'collaborations', 'using', 'the', 'isobar', 'model', 'are', 'larger', 'than', 'our', 'predictions', 'by', 'about', '52', 'per', 'cent']] | [-0.09716327512553365, 0.2616105817789331, -0.06830924988300796, 0.10637519007556023, -0.06856924052694886, -0.14549341467832486, 0.1366104250617956, 0.2630579810677551, -0.18507114497900712, -0.2196589856753199, -0.08456614472001321, -0.35828849929201556, -0.015551956381472781, 0.09816661220791889, 0.14576313194386134, 0.1266136600701945, 0.0983730007969503, 0.01716208242349268, -0.04158613628773825, -0.168451448851155, 0.2302245502781827, -0.05271964587681875, 0.15251765530703104, 0.0901150498649208, -0.08073447018084447, 0.02690147056691642, -0.07265273665305315, -0.09544517450386614, -0.15867054175244513, 0.03214450860689357, 0.1864178917466069, 0.14958405964968885, 0.07688392216787035, -0.31817492524411267, -0.017511454618015274, 0.13860292714015823, 0.18605116853952466, 0.04664748607640609, 0.029675958620377002, -0.41355871225846563, 0.12537843878490953, -0.1905781262293898, -0.03172414020202526, -0.14107393985980843, 0.12056018970906734, -0.10387689795521066, -0.3853319742988179, 0.10727100079676584, -0.05632436436905313, 0.045925369948207395, -0.003369746601399709, -0.35937898793426437, 0.005001477963166443, 0.03891785903357145, 0.11659614034327055, 0.11672766735835925, 0.1831272527223497, -0.13546284701396513, -0.17189856317979613, 0.4159880036865838, -0.05377421621657178, -0.21315710835422821, 0.10965902663540007, -0.19336410488302666, -0.09782436249161681, 0.17679533875716014, 0.18709573063882082, 0.03771544873391784, -0.17966939955968117, 0.12839166665776067, -0.05480863925025571, 0.14708113643949425, 0.09154074446400848, 0.0554176116285215, 0.1390490923956858, 0.15596705543126646, -0.0654018996283412, 0.042420567973978876, -0.07353708286967686, -0.08588206776102462, -0.4060773227976151, -0.10889128479725263, -0.05330166334513663, 0.084356277117755, -0.03933115647079086, -0.033330280278758034, 0.32164384016041153, -0.003038873285509822, 0.31874628433972363, 0.03256791153937343, 0.3409379232733503, 0.08326522165113752, 0.051236152092515544, 0.05159594998034964, 0.2979258177850091, 0.26287260583022565, 0.10061351900304279, -0.32317039493918714, 0.06005449034640287, 0.0335417789128411] |
710.247 | Lattice Approach to Light Scalars | I report on lattice QCD calculations that study the properties of the a0 and
f0 mesons.
| hep-lat | i report on lattice qcd calculations that study the properties of the a0 and f0 mesons | [['i', 'report', 'on', 'lattice', 'qcd', 'calculations', 'that', 'study', 'the', 'properties', 'of', 'the', 'a0', 'and', 'f0', 'mesons']] | [-0.12391679873690009, 0.18541280075442046, -0.10501901112729684, 0.019549561955500394, -0.01617572200484574, -0.0934236696921289, 0.12159591284580529, 0.41261759772896767, -0.13173213065601885, -0.07665301393717527, 0.02832755062263459, -0.36163593316450715, -0.06614479434210807, 0.06157560150313657, 0.16205938148777932, 0.0545761336106807, 0.1455523887416348, 0.04389125376474112, -0.11116299375134986, -0.17806478147394955, 0.34654330171179026, -0.061288625962333754, 0.16473559010773897, 0.1819113076198846, -0.02509290730813518, -0.010503298544790596, -0.0016878489404916763, -0.0929799978621304, -0.27630502010515556, 0.0581819370854646, 0.08332961436826736, 0.03190899998298846, 0.14447821490466595, -0.35282338527031243, -0.1526896920404397, 0.041251864517107606, 0.0977348810993135, 0.06461655022576451, -0.05455317043379182, -0.2691106974380091, 0.15635147970169783, -0.05632513004820794, -0.12077587394742295, -0.17603875463828444, 0.017682203091681004, 0.007139835841371678, -0.2562508787959814, 0.05060014908667654, -0.003547235857695341, 0.10986260756499178, -0.0916405055031646, -0.3117893612361513, 0.012008168967440724, -0.00509061332559213, 0.10639229707885534, 0.1379336889804108, 0.13898549822624773, -0.24354120739735663, -0.18899706017691642, 0.5097022093905252, -0.08927004097495228, -0.12369873601710424, 0.101592309307307, -0.21019463089760393, -0.1865117505658418, 0.020402512018335983, 0.20940599963068962, 0.13601926155388355, -0.1233133509522304, 0.13686521956333308, -0.06813703570514917, 0.21311609307304025, 0.011443811643403023, 0.09278467696276493, 0.15274596912786365, 0.12233038956765085, -0.15600732434540987, 0.06782499828841537, -0.05734600992582273, -0.06995115161407739, -0.4446002384647727, -0.14594910177402198, -0.1810320614331431, 0.09989858907647431, -0.055967744584449974, -0.1351090888492763, 0.4125085175037384, 0.11148249884718098, 0.24804069148376584, 0.012314166873693466, 0.24300831113941967, 0.04193496238440275, -0.04982906801160425, 0.05738918852148345, 0.3066056817770004, 0.18938658758997917, 0.130229252303252, -0.4097295943647623, -0.07863807116518728, 0.1046709914226085] |
710.2471 | On the effective charge of hydrophobic polyelectrolytes | In this paper we analyze the behavior of hydrophobic polyelectrolytes. It has
been proposed that this system adopts a pearl-necklace structure reminiscent of
the Rayleigh instability of a charged droplet. Using a Poisson-Boltzmann
approach, we calculate the counterion distribution around a given pearl
assuming the latter to be penetrable for the counterions. This allows us to
calculate the effective electric charge of the pearl as a function of the
chemical charge. Our predictions are in very good agreement with the recent
experimental measurements of the effective charge by Essafi et al. (Europhys.
Lett. 71, 938 (2005)). Our results allow to understand the large deviation from
the Manning law observed in these experiments.
| cond-mat.soft | in this paper we analyze the behavior of hydrophobic polyelectrolytes it has been proposed that this system adopts a pearlnecklace structure reminiscent of the rayleigh instability of a charged droplet using a poissonboltzmann approach we calculate the counterion distribution around a given pearl assuming the latter to be penetrable for the counterions this allows us to calculate the effective electric charge of the pearl as a function of the chemical charge our predictions are in very good agreement with the recent experimental measurements of the effective charge by essafi et al europhys lett 71 938 2005 our results allow to understand the large deviation from the manning law observed in these experiments | [['in', 'this', 'paper', 'we', 'analyze', 'the', 'behavior', 'of', 'hydrophobic', 'polyelectrolytes', 'it', 'has', 'been', 'proposed', 'that', 'this', 'system', 'adopts', 'a', 'pearlnecklace', 'structure', 'reminiscent', 'of', 'the', 'rayleigh', 'instability', 'of', 'a', 'charged', 'droplet', 'using', 'a', 'poissonboltzmann', 'approach', 'we', 'calculate', 'the', 'counterion', 'distribution', 'around', 'a', 'given', 'pearl', 'assuming', 'the', 'latter', 'to', 'be', 'penetrable', 'for', 'the', 'counterions', 'this', 'allows', 'us', 'to', 'calculate', 'the', 'effective', 'electric', 'charge', 'of', 'the', 'pearl', 'as', 'a', 'function', 'of', 'the', 'chemical', 'charge', 'our', 'predictions', 'are', 'in', 'very', 'good', 'agreement', 'with', 'the', 'recent', 'experimental', 'measurements', 'of', 'the', 'effective', 'charge', 'by', 'essafi', 'et', 'al', 'europhys', 'lett', '71', '938', '2005', 'our', 'results', 'allow', 'to', 'understand', 'the', 'large', 'deviation', 'from', 'the', 'manning', 'law', 'observed', 'in', 'these', 'experiments']] | [-0.08239913787608882, 0.09239979830427884, -0.1190117285628845, 0.03617383060276273, -0.030530895584741154, -0.09445360389764647, 0.0777384348408747, 0.30476774529109263, -0.18082406885842248, -0.3439758490385102, -0.01620029159590837, -0.2865647300596712, -0.1766704335926218, 0.13969863175943092, -0.07129955354675248, 0.05860070699641296, 0.010084222901511836, -0.03586154718891726, -0.026075581279541325, -0.1978561930538801, 0.23331178520042617, 0.11303582216973777, 0.2991276957883357, 0.11847441207600741, 0.06565957659905827, 0.021099729490726516, -0.00018370953631830644, 0.0609944896806065, -0.20871839302977147, 0.11966105250994095, 0.20865746001872393, 0.006647348762615709, 0.20822737624172355, -0.4092305917628445, -0.23079773442198834, 0.07017786155647791, 0.10524940614479485, 0.16941943144643898, -0.06135225452079966, -0.2922966978596607, 0.10023633029882435, -0.20782034606714775, -0.15904077412644485, -0.059880218552509405, 0.06756567885377654, 0.05856662653470496, -0.30470469079519463, 0.11736836047320803, 0.04967013028710409, 0.024459217028977635, -0.06577595859516396, -0.10865157929790281, -0.011023194675946289, 0.07756451197253826, 0.06184678945925322, 0.0554866406391165, 0.16347628810887668, -0.08723955314715502, -0.06758127400183815, 0.357423892026549, -0.06908025153019037, -0.17045621145600537, 0.1979993696404235, -0.15205601131677762, -0.08870101377770707, 0.14601231351293423, 0.12568246958324233, 0.1388722685334689, -0.16470358708741245, 0.08248455427284981, -0.12715382149090637, 0.15651688095693989, 0.08986802156888754, -0.05501440848358372, 0.2071274511331508, 0.18780145821841182, -0.026972578532221885, 0.13487133114527375, -0.11978709231852344, -0.11944694271539799, -0.25588318733246745, -0.16926000169100794, -0.1883355241923316, 0.03106348382241957, -0.06383495886499684, -0.15122325911799128, 0.3920334377032411, 0.19107870391343493, 0.2306538908364805, 0.03961607575341052, 0.22821397844886593, 0.07451630968533389, 0.04995850185016254, 0.06729692031906263, 0.28183142509235926, 0.15798682052021226, 0.15858442676757034, -0.25978339155338837, 0.07166937972012034, 0.028926761174859764] |
710.2472 | EW NLO corrections to pair production of top-squarks at the LHC | Presented are complete electroweak (EW) corrections at ${\cal
O}(\alpha\alpha_{\mathrm s}^{\mathrm 2})$ to top-squark pair production at the
Large Hadron Collider (LHC) within the framework of the Minimal Supersymmetric
Standard Model (MSSM). At this order, effects from the interference of EW and
QCD contributions have to be taken into account. Also photon-induced top-squark
production is considered as additionnal partonic channel which arises from the
non-zero photon density in the proton. Furthermore, the impact of MSSM
parameters on the EW corrections is analyzed.
| hep-ph | presented are complete electroweak ew corrections at cal oalphaalpha_mathrm smathrm 2 to topsquark pair production at the large hadron collider lhc within the framework of the minimal supersymmetric standard model mssm at this order effects from the interference of ew and qcd contributions have to be taken into account also photoninduced topsquark production is considered as additionnal partonic channel which arises from the nonzero photon density in the proton furthermore the impact of mssm parameters on the ew corrections is analyzed | [['presented', 'are', 'complete', 'electroweak', 'ew', 'corrections', 'at', 'cal', 'oalphaalpha_mathrm', 'smathrm', '2', 'to', 'topsquark', 'pair', 'production', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'within', 'the', 'framework', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'at', 'this', 'order', 'effects', 'from', 'the', 'interference', 'of', 'ew', 'and', 'qcd', 'contributions', 'have', 'to', 'be', 'taken', 'into', 'account', 'also', 'photoninduced', 'topsquark', 'production', 'is', 'considered', 'as', 'additionnal', 'partonic', 'channel', 'which', 'arises', 'from', 'the', 'nonzero', 'photon', 'density', 'in', 'the', 'proton', 'furthermore', 'the', 'impact', 'of', 'mssm', 'parameters', 'on', 'the', 'ew', 'corrections', 'is', 'analyzed']] | [-0.02637324377281379, 0.24092810244381993, -0.06361032368709581, 0.18689106203928071, -0.009875732164570614, -0.13818348127437896, -0.00985598337801197, 0.31687870221448283, -0.19969066234800634, -0.25888438534604596, -0.008306930612336514, -0.33619104159547936, 0.07834627970911656, 0.08293916123235433, 0.07783455961336723, 0.09651394946429925, 0.056915848851911255, -0.015663904562309573, -0.02478402356699675, -0.24261091195659923, 0.3068650964282076, 0.058636705650464645, 0.17479172859435219, 0.21122205303392455, 0.06098172325593761, 0.01494576556820281, -0.04806339439399587, -0.032184536769231664, -0.11284516837383043, 0.04083138044121899, 0.22839508461471222, 0.04431339689306443, 0.1014489800539575, -0.3314417934964729, -0.13549157585123484, 0.1428468483441238, 0.13864507602197648, 0.12032098991094935, -0.008050204462466078, -0.2991215736617016, 0.11657952665221653, -0.2658694391079907, -0.08003738083688047, 0.0006925108830762815, -0.042701722877218, -0.13623243893343437, -0.3658168234779865, 0.04978309317950242, -0.0908698030228762, -0.00022303945491019682, 0.07239059048787325, -0.19964670328293704, -0.13686160337109166, 0.0175078396296388, 0.13714157540168426, 0.029092320801006464, 0.18894260793723922, -0.1980427318117051, -0.18121726182584144, 0.46631247375773477, -0.059450772374314315, -0.1435264566606736, 0.08560383379462329, -0.1981601405747329, -0.16864745562330266, 0.21981716036938037, 0.27462777109887404, 0.04382774044643156, -0.164853208760224, 0.21381140001563215, 0.03410202977277008, 0.16316346774066362, 0.043276534436412065, 0.12104469784122857, 0.2282011658660596, 0.19287984562401153, -0.025266781682148576, 0.07721535810652555, -0.08776005966694955, -0.1140974982570904, -0.5309076060340563, -0.06734193214274282, -0.04771266203326515, 0.024202295816267688, -0.07449242219758438, -0.08248016637266625, 0.3577099270128374, 0.13852514021829526, 0.23384714923516103, 0.028190343595062724, 0.33968946832833413, 0.1357625550280997, 0.11826229979515465, 0.02030520434428708, 0.32969378106461106, 0.11534805114887937, 0.11709151590313716, -0.2807294555344395, 0.007142502832214666, 0.08937164728789107] |
710.2473 | How does gas cool in DM halos? | In order to study the process of cooling in dark-matter (DM) halos and assess
how well simple models can represent it, we run a set of radiative SPH
hydrodynamical simulations of isolated halos, with gas sitting initially in
hydrostatic equilibrium within Navarro-Frenk-White (NFW) potential wells. [...]
After having assessed the numerical stability of the simulations, we compare
the resulting evolution of the cooled mass with the predictions of the
classical cooling model of White & Frenk and of the cooling model proposed in
the MORGANA code of galaxy formation. We find that the classical model predicts
fractions of cooled mass which, after about two central cooling times, are
about one order of magnitude smaller than those found in simulations. Although
this difference decreases with time, after 8 central cooling times, when
simulations are stopped, the difference still amounts to a factor of 2-3. We
ascribe this difference to the lack of validity of the assumption that a mass
shell takes one cooling time, as computed on the initial conditions, to cool to
very low temperature. [...] The MORGANA model [...] better agrees with the
cooled mass fraction found in the simulations, especially at early times, when
the density profile of the cooling gas is shallow. With the addition of the
simple assumption that the increase of the radius of the cooling region is
counteracted by a shrinking at the sound speed, the MORGANA model is also able
to reproduce for all simulations the evolution of the cooled mass fraction to
within 20-50 per cent, thereby providing a substantial improvement with respect
to the classical model. Finally, we provide a very simple fitting function
which accurately reproduces the cooling flow for the first ~10 central cooling
times. [Abridged]
| astro-ph | in order to study the process of cooling in darkmatter dm halos and assess how well simple models can represent it we run a set of radiative sph hydrodynamical simulations of isolated halos with gas sitting initially in hydrostatic equilibrium within navarrofrenkwhite nfw potential wells after having assessed the numerical stability of the simulations we compare the resulting evolution of the cooled mass with the predictions of the classical cooling model of white frenk and of the cooling model proposed in the morgana code of galaxy formation we find that the classical model predicts fractions of cooled mass which after about two central cooling times are about one order of magnitude smaller than those found in simulations although this difference decreases with time after 8 central cooling times when simulations are stopped the difference still amounts to a factor of 23 we ascribe this difference to the lack of validity of the assumption that a mass shell takes one cooling time as computed on the initial conditions to cool to very low temperature the morgana model better agrees with the cooled mass fraction found in the simulations especially at early times when the density profile of the cooling gas is shallow with the addition of the simple assumption that the increase of the radius of the cooling region is counteracted by a shrinking at the sound speed the morgana model is also able to reproduce for all simulations the evolution of the cooled mass fraction to within 2050 per cent thereby providing a substantial improvement with respect to the classical model finally we provide a very simple fitting function which accurately reproduces the cooling flow for the first 10 central cooling times abridged | [['in', 'order', 'to', 'study', 'the', 'process', 'of', 'cooling', 'in', 'darkmatter', 'dm', 'halos', 'and', 'assess', 'how', 'well', 'simple', 'models', 'can', 'represent', 'it', 'we', 'run', 'a', 'set', 'of', 'radiative', 'sph', 'hydrodynamical', 'simulations', 'of', 'isolated', 'halos', 'with', 'gas', 'sitting', 'initially', 'in', 'hydrostatic', 'equilibrium', 'within', 'navarrofrenkwhite', 'nfw', 'potential', 'wells', 'after', 'having', 'assessed', 'the', 'numerical', 'stability', 'of', 'the', 'simulations', 'we', 'compare', 'the', 'resulting', 'evolution', 'of', 'the', 'cooled', 'mass', 'with', 'the', 'predictions', 'of', 'the', 'classical', 'cooling', 'model', 'of', 'white', 'frenk', 'and', 'of', 'the', 'cooling', 'model', 'proposed', 'in', 'the', 'morgana', 'code', 'of', 'galaxy', 'formation', 'we', 'find', 'that', 'the', 'classical', 'model', 'predicts', 'fractions', 'of', 'cooled', 'mass', 'which', 'after', 'about', 'two', 'central', 'cooling', 'times', 'are', 'about', 'one', 'order', 'of', 'magnitude', 'smaller', 'than', 'those', 'found', 'in', 'simulations', 'although', 'this', 'difference', 'decreases', 'with', 'time', 'after', '8', 'central', 'cooling', 'times', 'when', 'simulations', 'are', 'stopped', 'the', 'difference', 'still', 'amounts', 'to', 'a', 'factor', 'of', '23', 'we', 'ascribe', 'this', 'difference', 'to', 'the', 'lack', 'of', 'validity', 'of', 'the', 'assumption', 'that', 'a', 'mass', 'shell', 'takes', 'one', 'cooling', 'time', 'as', 'computed', 'on', 'the', 'initial', 'conditions', 'to', 'cool', 'to', 'very', 'low', 'temperature', 'the', 'morgana', 'model', 'better', 'agrees', 'with', 'the', 'cooled', 'mass', 'fraction', 'found', 'in', 'the', 'simulations', 'especially', 'at', 'early', 'times', 'when', 'the', 'density', 'profile', 'of', 'the', 'cooling', 'gas', 'is', 'shallow', 'with', 'the', 'addition', 'of', 'the', 'simple', 'assumption', 'that', 'the', 'increase', 'of', 'the', 'radius', 'of', 'the', 'cooling', 'region', 'is', 'counteracted', 'by', 'a', 'shrinking', 'at', 'the', 'sound', 'speed', 'the', 'morgana', 'model', 'is', 'also', 'able', 'to', 'reproduce', 'for', 'all', 'simulations', 'the', 'evolution', 'of', 'the', 'cooled', 'mass', 'fraction', 'to', 'within', '2050', 'per', 'cent', 'thereby', 'providing', 'a', 'substantial', 'improvement', 'with', 'respect', 'to', 'the', 'classical', 'model', 'finally', 'we', 'provide', 'a', 'very', 'simple', 'fitting', 'function', 'which', 'accurately', 'reproduces', 'the', 'cooling', 'flow', 'for', 'the', 'first', '10', 'central', 'cooling', 'times', 'abridged']] | [-0.04512265604400724, 0.12614477431984097, -0.0726602331787848, 0.07244397701296464, 0.00881000883735769, -0.07525222236455119, 0.04468054781493471, 0.36114576649473645, -0.1980153127604694, -0.36936630100581974, 0.08369060637727183, -0.261885127381754, 0.010997507991938722, 0.20556124232959516, 0.007389926805647169, 0.0030142840322159733, 0.04595088981982163, 0.01777716026492927, -0.10891983663052808, -0.2748243702030922, 0.27363302823001445, 0.11702442163101302, 0.19896830021084513, 0.019538099070444914, 0.07139350328176503, -0.08423538340499144, -0.013068188545409287, -0.0026080085938737165, -0.16269058435157252, 0.013298589470689333, 0.16009750036402062, 0.07671690595175004, 0.2531762314670762, -0.4351091885695714, -0.22824401798528082, 0.11007228419974499, 0.161802693816435, 0.10224066034867264, -0.07534899234413021, -0.19079065893516733, 0.07660754363903242, -0.2064409688454082, -0.1887069167537399, -0.00728963779502749, 0.011021714241247189, 0.017596580300812507, -0.25163799883631577, 0.1614437042709807, 0.032122339412007254, 0.001482387362936571, -0.07683421281090684, -0.08758899866267644, -0.056711647042497836, 0.07149174246733823, 0.02474826922985337, 0.040549196320167964, 0.21097624945444426, -0.1415775569284157, -0.009266557952705047, 0.42362579430618846, -0.09888581353427502, -0.08483459323178977, 0.21247467587869812, -0.18627517233362467, -0.0876032267627224, 0.1677019016030689, 0.14598415802642636, 0.07376108248635811, -0.1195851883374018, -0.006727381263322332, -0.03330237988313469, 0.20874976237919907, 0.046888972344633864, -0.04308217202057994, 0.258481636205721, 0.2066920006042182, -0.0040989989256848295, 0.11103355148379351, -0.12525397747040928, -0.13752113825019593, -0.26891394204488056, -0.11742169616822903, -0.12629229584075313, 0.04826899085361708, -0.10813753794030904, -0.11823195950029411, 0.35512916175973547, 0.17327555329473063, 0.22769756479577125, 0.09915967125777984, 0.3450939379395529, 0.11389951675135006, 0.08792755754149104, 0.1028521916263016, 0.2731823046138846, 0.16385290267887154, 0.06769546151059176, -0.2839589577395298, 0.04395852379283667, -0.0011526620560144683] |
710.2474 | Thermodynamical properties of hairy black holes in n spacetimes
dimensions | The issue concerning the existence of exact black hole solutions in presence
of non vanishing cosmological constant and scalar fields is reconsidered. With
regard to this, in investigating no-hair theorem violations, exact solutions of
gravity having as a source an interacting and conformally coupled scalar field
are revisited in arbitrary dimensional non asymptotically flat space-times. New
and known hairy black hole solutions are discussed. The thermodynamical
properties associated with these solutions are investigated and the invariance
of the black hole entropy with respect to different conformal frames is proven.
| hep-th | the issue concerning the existence of exact black hole solutions in presence of non vanishing cosmological constant and scalar fields is reconsidered with regard to this in investigating nohair theorem violations exact solutions of gravity having as a source an interacting and conformally coupled scalar field are revisited in arbitrary dimensional non asymptotically flat spacetimes new and known hairy black hole solutions are discussed the thermodynamical properties associated with these solutions are investigated and the invariance of the black hole entropy with respect to different conformal frames is proven | [['the', 'issue', 'concerning', 'the', 'existence', 'of', 'exact', 'black', 'hole', 'solutions', 'in', 'presence', 'of', 'non', 'vanishing', 'cosmological', 'constant', 'and', 'scalar', 'fields', 'is', 'reconsidered', 'with', 'regard', 'to', 'this', 'in', 'investigating', 'nohair', 'theorem', 'violations', 'exact', 'solutions', 'of', 'gravity', 'having', 'as', 'a', 'source', 'an', 'interacting', 'and', 'conformally', 'coupled', 'scalar', 'field', 'are', 'revisited', 'in', 'arbitrary', 'dimensional', 'non', 'asymptotically', 'flat', 'spacetimes', 'new', 'and', 'known', 'hairy', 'black', 'hole', 'solutions', 'are', 'discussed', 'the', 'thermodynamical', 'properties', 'associated', 'with', 'these', 'solutions', 'are', 'investigated', 'and', 'the', 'invariance', 'of', 'the', 'black', 'hole', 'entropy', 'with', 'respect', 'to', 'different', 'conformal', 'frames', 'is', 'proven']] | [-0.2106094490422794, 0.09791050878176177, -0.03465798984836327, 0.14737956251640374, -0.0819935570654114, -0.2280464779972779, -0.06772506419632039, 0.2810506153998248, -0.15091644614683777, -0.2585648366091825, 0.13640409624439487, -0.33067170795304385, -0.06430491086702501, 0.14674341668155086, -0.0532516392492009, 0.09804763707719492, -0.030695481393276977, 0.06582803740637021, -0.1033781703582473, -0.24088170486136098, 0.4153167967883389, 0.07707021003615194, 0.2606912189989947, -0.00680508084720775, 0.10048976994192835, -0.03573030773864201, -0.012200670649056857, 0.10971811761179667, -0.17551530068844892, 0.06408959497917402, 0.2266709675353146, 0.08379205230497912, 0.18974970948746364, -0.3755945893569609, -0.24071978852989967, 0.0965702571720408, 0.13192643397330736, 0.16916257772971405, -0.13680963693029677, -0.3066278963527653, 0.12080554613906345, -0.16231783490962862, -0.250051833521784, -0.09404826924476899, 0.016121877363903886, -0.014786514252152168, -0.18709017949707263, 0.14608778241038156, 0.05543857218116899, -0.05451158479149087, -0.17966714725840124, -0.0044960079013547875, -0.0338961052436256, 0.06500145858362986, 0.21623352909293236, 0.012057281303313676, 0.10055617304267676, -0.13185140589787428, -0.12960491588161316, 0.34834208906617725, -0.07552531532147962, -0.27261048897033496, 0.20744880485568154, -0.1697429855448309, -0.1333518818313821, 0.06664290875091813, 0.11074046501785181, 0.21942901892817757, -0.17484082147646485, 0.2058985204922475, 0.013697580570417844, 0.1236944077791531, 0.1620402944357961, 0.09999340236856696, 0.35682212917155093, 0.039723417023196816, 0.027912906423378528, 0.18308035155308297, 0.05476000111254476, -0.1561340591366654, -0.35764711944574723, -0.154860993849867, -0.12612378371230673, 0.14600868578581663, -0.18188372160650768, -0.23845756436394674, 0.3239793265761619, 0.06842281036141061, 0.11208667566351006, 0.03659888874122015, 0.18173993834074628, 0.1037892823439782, -0.017807872359002573, 0.1212130479797135, 0.33240105040120277, 0.22901087070375764, 0.11218191836201952, -0.20712238471703917, -0.08531647358675686, 0.1164449011995928] |
710.2475 | Fast X-ray Oscillations During Magnetar Flares | The giant flares produced by highly magnetized neutron stars, "magnetars,"
are the brightest sources of high energy radiation outside our solar system.
Serendipitous observations with NASA's Rossi X-ray Timing Explorer (RXTE) of
the two most recent flares resulted in the discovery of high frequency
oscillations in their X-ray fluxes. The frequencies of these oscillations range
from about 20 Hz to as high as 1800 Hz, and may represent the first detection
of global oscillation modes of neutron stars. Here I will present an
observational and theoretical overview of these oscillations and discuss how
they might allow us to probe neutron star interiors and dense matter physics.
| astro-ph | the giant flares produced by highly magnetized neutron stars magnetars are the brightest sources of high energy radiation outside our solar system serendipitous observations with nasas rossi xray timing explorer rxte of the two most recent flares resulted in the discovery of high frequency oscillations in their xray fluxes the frequencies of these oscillations range from about 20 hz to as high as 1800 hz and may represent the first detection of global oscillation modes of neutron stars here i will present an observational and theoretical overview of these oscillations and discuss how they might allow us to probe neutron star interiors and dense matter physics | [['the', 'giant', 'flares', 'produced', 'by', 'highly', 'magnetized', 'neutron', 'stars', 'magnetars', 'are', 'the', 'brightest', 'sources', 'of', 'high', 'energy', 'radiation', 'outside', 'our', 'solar', 'system', 'serendipitous', 'observations', 'with', 'nasas', 'rossi', 'xray', 'timing', 'explorer', 'rxte', 'of', 'the', 'two', 'most', 'recent', 'flares', 'resulted', 'in', 'the', 'discovery', 'of', 'high', 'frequency', 'oscillations', 'in', 'their', 'xray', 'fluxes', 'the', 'frequencies', 'of', 'these', 'oscillations', 'range', 'from', 'about', '20', 'hz', 'to', 'as', 'high', 'as', '1800', 'hz', 'and', 'may', 'represent', 'the', 'first', 'detection', 'of', 'global', 'oscillation', 'modes', 'of', 'neutron', 'stars', 'here', 'i', 'will', 'present', 'an', 'observational', 'and', 'theoretical', 'overview', 'of', 'these', 'oscillations', 'and', 'discuss', 'how', 'they', 'might', 'allow', 'us', 'to', 'probe', 'neutron', 'star', 'interiors', 'and', 'dense', 'matter', 'physics']] | [-0.09563710492209725, 0.24498331251256014, -0.0243693964055054, 0.10232241909494097, -0.18882301470862245, -0.0009943777124204163, 0.08141656572939301, 0.3613222728500951, -0.1835812978844053, -0.40765704573044237, 0.1083402002749488, -0.3743894463229292, -0.016193440965956676, 0.28794526866250586, -0.038297745012590347, -0.004418581674745271, 0.1268714355328999, -0.04309352798571916, -0.03275076550857674, -0.18405837156559463, 0.2456664603185963, 0.13248569960266632, 0.16113868455967056, -0.02497557973717603, 0.04299096715249965, -0.10462277999393782, -0.07427871772878857, -0.07435439845090205, -0.131578086637469, 0.03972724816357752, 0.28473652688399803, 0.17757883083453085, 0.17873224399913595, -0.4601844381716735, -0.24993515504471395, 0.055301638003790156, 0.1749719867399314, -0.012539001462875673, -0.05076449115778196, -0.27664921448548446, 0.0330897871655289, -0.21728053929301788, -0.1694229435975189, -0.040528775539846636, 0.05181788697504913, 0.09292221013544444, -0.174746804576332, 0.08438187660122255, 0.005502972978646077, 0.02916845956922702, -0.1765636736944423, -0.07488166962042977, 0.010563550743204102, 0.06817000196095696, 0.08224036774756212, 0.02408440221311911, 0.14025306028647805, -0.12284891807280902, -0.10724641845170584, 0.32459255243774576, -0.06487711775555925, 0.08577993652730617, 0.23874215757966322, -0.29839221371847363, -0.19002142089928659, 0.14349132284240904, 0.15992807735741701, 0.13690451122293212, -0.1870365471585724, -0.03326179169531349, 0.04020838612110688, 0.2138994663458467, 0.09883489413186908, 0.114844694351426, 0.410005779840263, 0.18258155910693602, -0.018363958984648564, 0.07844698337732621, -0.29725641976736644, 0.03978922734265479, -0.25721756928547657, -0.025096958301047672, -0.09916362378148819, 0.09179093117083265, -0.07492898353584164, -0.146940660526216, 0.3919099183524695, 0.12103824828474624, 0.14354143560784957, -0.055153988400597195, 0.30330405878078825, 0.056133070586135016, 0.026013213662290067, 0.08381085664490764, 0.39062884991180225, 0.19108873440550184, 0.15287971567749134, -0.2522588715040705, 0.0076529061661172165, -0.05473707364169213] |
710.2476 | Effect of charge modulation in (LaVO3)m(SrVO3)n superlattices on the
insulator-metal transition | A series of epitaxial (LaVO3)6m(SrVO3)m superlattices having the same nominal
composition as La6/7Sr1/7VO3, a Mott-Hubbard insulator, were grown with
pulsed-laser deposition on [001]-oriented SrTiO3 substrates, and their
superlattice period was varied. When m=1, the insulating resistivity of
bulk-like La6/7Sr1/7VO3 is obtained; however, an increase in the periodicity
(m>=2) results in metallic samples. Comparison of the superlattice periodicity
with the coherence length of charge carriers in perovskite oxide
heterostructures are used to understand these observations. A
filling-controlled insulator-metal transition was induced by placing a single
dopant layer of SrVO3 within LaVO3 layers of varying thickness.
| cond-mat.mtrl-sci cond-mat.str-el | a series of epitaxial lavo36msrvo3m superlattices having the same nominal composition as la67sr17vo3 a motthubbard insulator were grown with pulsedlaser deposition on 001oriented srtio3 substrates and their superlattice period was varied when m1 the insulating resistivity of bulklike la67sr17vo3 is obtained however an increase in the periodicity m2 results in metallic samples comparison of the superlattice periodicity with the coherence length of charge carriers in perovskite oxide heterostructures are used to understand these observations a fillingcontrolled insulatormetal transition was induced by placing a single dopant layer of srvo3 within lavo3 layers of varying thickness | [['a', 'series', 'of', 'epitaxial', 'lavo36msrvo3m', 'superlattices', 'having', 'the', 'same', 'nominal', 'composition', 'as', 'la67sr17vo3', 'a', 'motthubbard', 'insulator', 'were', 'grown', 'with', 'pulsedlaser', 'deposition', 'on', '001oriented', 'srtio3', 'substrates', 'and', 'their', 'superlattice', 'period', 'was', 'varied', 'when', 'm1', 'the', 'insulating', 'resistivity', 'of', 'bulklike', 'la67sr17vo3', 'is', 'obtained', 'however', 'an', 'increase', 'in', 'the', 'periodicity', 'm2', 'results', 'in', 'metallic', 'samples', 'comparison', 'of', 'the', 'superlattice', 'periodicity', 'with', 'the', 'coherence', 'length', 'of', 'charge', 'carriers', 'in', 'perovskite', 'oxide', 'heterostructures', 'are', 'used', 'to', 'understand', 'these', 'observations', 'a', 'fillingcontrolled', 'insulatormetal', 'transition', 'was', 'induced', 'by', 'placing', 'a', 'single', 'dopant', 'layer', 'of', 'srvo3', 'within', 'lavo3', 'layers', 'of', 'varying', 'thickness']] | [-0.15374670294369316, 0.24134497566210683, 0.007616972861936889, -0.05842335319919205, 0.02285449539700134, -0.183787224169534, 0.1249775294992295, 0.49543261020393164, -0.2451257546391379, -0.3273860484945004, 0.008456941012160055, -0.342811244816243, -0.10104730513438091, 0.179344513023702, -0.013861704855686524, 0.0338236351960734, -0.07630436212479413, -0.15646668925758575, -0.17318219783623795, -0.25248931903535354, 0.22348231573558444, 0.029782464374675528, 0.3292569270214209, 0.04778710588976577, -0.007449860822736889, -0.05240292762915327, 0.2194188687458486, -0.026131578086578584, -0.19917363757369938, 0.03731777905844725, 0.25492564147686236, -0.23138855945237063, 0.165943491285741, -0.5100094857983865, -0.2375544715201953, -0.1259141721645022, 0.10426988800127919, 0.07272115893211666, -0.08983455304885385, -0.2693477658667489, 0.08540287465663053, -0.08818335929414728, -0.0600306599319063, 5.471610187829196e-05, -0.021771603744927343, 0.00877173114337723, -0.2528980210331361, 0.06519395139152798, 0.06202438533060498, 0.1738199177326041, -0.16760259037223327, -0.14405990051167025, -0.16458246480816832, 0.0707376204411228, 0.0727455459079695, 0.08223113703674503, 0.2222736268381046, -0.032119790864801344, -0.0995629343030217, 0.30143544644854225, -0.02842761123307295, -0.020431196757152187, 0.13348773860239557, -0.2221847667952406, -0.0012154137142575704, 0.19205672837855234, 0.06232324099311462, 0.10327475603700585, -0.134043975322089, 0.0789103209863642, -0.01379945447954994, 0.29323167209564655, 0.16920526036839154, 0.07437778379931882, 0.23382043824684653, 0.29507591985524273, -0.011172409852516356, 0.15097648454676535, -0.14037006988783704, 0.038527475588105535, -0.12691618878506944, -0.2084946137632929, -0.2491348073741032, 0.0935029947316622, -0.10101420370907303, -0.2560908119757097, 0.3936616631613655, 0.06964236448754321, 0.15903863031417131, -0.11257818405987224, 0.16503522581431074, 0.068232197231347, 0.11814520296152645, -0.07598217598745947, 0.2292602772000604, 0.1916595671829962, 0.1461208748098995, -0.21948332948978622, 0.1613549892841787, -0.010475334189422838] |
710.2477 | Supersymmetric LHC phenomenology without a light Higgs boson | After a brief discussion of the mass of the Higgs in supersymmetry, I
introduce \lambdaSUSY, a model with an extra chiral singlet superfield in
addition to the MSSM field content. The key features of the model are: the
superpotential W=\lambda S H_d H_u with a large coupling \lambda and the
resulting lightest Higgs with mass above 200GeV. The main part of my
contribution will be about how \lambdaSUSY manifests itself at the LHC.
Discoveries of gluino, squarks and in particular of the three lightest neutral
Higgs bosons are discussed.
| hep-ph | after a brief discussion of the mass of the higgs in supersymmetry i introduce lambdasusy a model with an extra chiral singlet superfield in addition to the mssm field content the key features of the model are the superpotential wlambda s h_d h_u with a large coupling lambda and the resulting lightest higgs with mass above 200gev the main part of my contribution will be about how lambdasusy manifests itself at the lhc discoveries of gluino squarks and in particular of the three lightest neutral higgs bosons are discussed | [['after', 'a', 'brief', 'discussion', 'of', 'the', 'mass', 'of', 'the', 'higgs', 'in', 'supersymmetry', 'i', 'introduce', 'lambdasusy', 'a', 'model', 'with', 'an', 'extra', 'chiral', 'singlet', 'superfield', 'in', 'addition', 'to', 'the', 'mssm', 'field', 'content', 'the', 'key', 'features', 'of', 'the', 'model', 'are', 'the', 'superpotential', 'wlambda', 's', 'h_d', 'h_u', 'with', 'a', 'large', 'coupling', 'lambda', 'and', 'the', 'resulting', 'lightest', 'higgs', 'with', 'mass', 'above', '200gev', 'the', 'main', 'part', 'of', 'my', 'contribution', 'will', 'be', 'about', 'how', 'lambdasusy', 'manifests', 'itself', 'at', 'the', 'lhc', 'discoveries', 'of', 'gluino', 'squarks', 'and', 'in', 'particular', 'of', 'the', 'three', 'lightest', 'neutral', 'higgs', 'bosons', 'are', 'discussed']] | [-0.11058275381186872, 0.28287890699598545, -0.009297474632772166, 0.13848842394124883, -0.0974695265000121, -0.19669668072457897, -0.03168525848160969, 0.29134368867707555, -0.19247104241146465, -0.27394060957705957, 0.029339036403297124, -0.28537758286477305, -0.02795246218362551, 0.05618012653077754, -0.008771486161799912, -0.0030438628249142446, 0.04797208618916822, 0.05788106182485484, -0.03172722114302386, -0.30924127011800584, 0.34195601590647456, 0.006982239465532678, 0.12030684528872371, 0.12649071500950565, 0.04931268959274788, -0.015028594490768534, 0.0006042314965403482, -0.14733551543080406, -0.1317115534578314, 0.12293832447821944, 0.16501627792865875, 0.0773358510367656, 0.16710462760222092, -0.283721275554363, -0.0932737524631653, 0.14695071493369644, 0.17325645657988747, 0.09145311283711553, -0.05980889026201173, -0.3367381339128851, 0.06464262628336594, -0.22319952578524524, -0.12784848742846275, -0.03019992074029248, -0.04513063566795854, -0.1408797029636047, -0.29263750162483143, 0.08209654200414007, -0.02929073239394118, 0.040165680817072016, 0.01758047743710909, -0.21127556008025167, -0.1525939515781369, -0.03834701808211341, 0.21493191778230783, 0.021753976386422395, 0.17059901808231567, -0.25196676868736073, -0.13654061592592115, 0.4192247194018257, -0.14223706534948577, -0.12922622595411423, 0.12176959454788293, -0.14224619929040416, -0.18421369135965793, 0.13340344395831205, 0.16086027457305554, 0.07166351052524333, -0.15728825366312868, 0.23698101961707926, -0.05867568144621851, 0.19708827751024177, 0.017000514480253952, 0.06541186441887128, 0.30079351117104564, 0.2186755466934168, 0.02542682828249546, 0.07193887914829165, -0.045852987514285556, -0.09723398375084226, -0.5181068478340514, -0.16093834074151314, -0.06736619050583142, 0.03217445645648777, -0.08188610811478438, -0.0727996138824422, 0.4438724385972103, 0.14745222955282902, 0.28506967873218353, -0.008025947830043314, 0.26601233875399893, 0.08389388638995902, 0.11412837167448375, -0.010053079227362288, 0.3028569123969319, 0.15127053635529755, 0.1461468388881074, -0.2133840069467767, -0.08962399351379174, 0.11081744988155917] |
710.2478 | Nonmonotonic energy harvesting efficiency in biased exciton chains | We theoretically study the efficiency of energy harvesting in linear exciton
chains with an energy bias, where the initial excitation is taking place at the
high-energy end of the chain and the energy is harvested (trapped) at the other
end. The efficiency is characterized by means of the average time for the
exciton to be trapped after the initial excitation. The exciton transport is
treated as the intraband energy relaxation over the states obtained by
numerically diagonalizing the Frenkel Hamiltonian that corresponds to the
biased chain. The relevant intraband scattering rates are obtained from a
linear exciton-phonon interaction. Numerical solution of the Pauli master
equation that describes the relaxation and trapping processes, reveals a
complicated interplay of factors that determine the overall harvesting
efficiency. Specifically, if the trapping step is slower than or comparable to
the intraband relaxation, this efficiency shows a nonmonotonic dependence on
the bias: it first increases when introducing a bias, reaches a maximum at an
optimal bias value, and then decreases again because of dynamic (Bloch)
localization of the exciton states. Effects of on-site (diagonal) disorder,
leading to Anderson localization, are addressed as well.
| cond-mat.dis-nn cond-mat.mtrl-sci | we theoretically study the efficiency of energy harvesting in linear exciton chains with an energy bias where the initial excitation is taking place at the highenergy end of the chain and the energy is harvested trapped at the other end the efficiency is characterized by means of the average time for the exciton to be trapped after the initial excitation the exciton transport is treated as the intraband energy relaxation over the states obtained by numerically diagonalizing the frenkel hamiltonian that corresponds to the biased chain the relevant intraband scattering rates are obtained from a linear excitonphonon interaction numerical solution of the pauli master equation that describes the relaxation and trapping processes reveals a complicated interplay of factors that determine the overall harvesting efficiency specifically if the trapping step is slower than or comparable to the intraband relaxation this efficiency shows a nonmonotonic dependence on the bias it first increases when introducing a bias reaches a maximum at an optimal bias value and then decreases again because of dynamic bloch localization of the exciton states effects of onsite diagonal disorder leading to anderson localization are addressed as well | [['we', 'theoretically', 'study', 'the', 'efficiency', 'of', 'energy', 'harvesting', 'in', 'linear', 'exciton', 'chains', 'with', 'an', 'energy', 'bias', 'where', 'the', 'initial', 'excitation', 'is', 'taking', 'place', 'at', 'the', 'highenergy', 'end', 'of', 'the', 'chain', 'and', 'the', 'energy', 'is', 'harvested', 'trapped', 'at', 'the', 'other', 'end', 'the', 'efficiency', 'is', 'characterized', 'by', 'means', 'of', 'the', 'average', 'time', 'for', 'the', 'exciton', 'to', 'be', 'trapped', 'after', 'the', 'initial', 'excitation', 'the', 'exciton', 'transport', 'is', 'treated', 'as', 'the', 'intraband', 'energy', 'relaxation', 'over', 'the', 'states', 'obtained', 'by', 'numerically', 'diagonalizing', 'the', 'frenkel', 'hamiltonian', 'that', 'corresponds', 'to', 'the', 'biased', 'chain', 'the', 'relevant', 'intraband', 'scattering', 'rates', 'are', 'obtained', 'from', 'a', 'linear', 'excitonphonon', 'interaction', 'numerical', 'solution', 'of', 'the', 'pauli', 'master', 'equation', 'that', 'describes', 'the', 'relaxation', 'and', 'trapping', 'processes', 'reveals', 'a', 'complicated', 'interplay', 'of', 'factors', 'that', 'determine', 'the', 'overall', 'harvesting', 'efficiency', 'specifically', 'if', 'the', 'trapping', 'step', 'is', 'slower', 'than', 'or', 'comparable', 'to', 'the', 'intraband', 'relaxation', 'this', 'efficiency', 'shows', 'a', 'nonmonotonic', 'dependence', 'on', 'the', 'bias', 'it', 'first', 'increases', 'when', 'introducing', 'a', 'bias', 'reaches', 'a', 'maximum', 'at', 'an', 'optimal', 'bias', 'value', 'and', 'then', 'decreases', 'again', 'because', 'of', 'dynamic', 'bloch', 'localization', 'of', 'the', 'exciton', 'states', 'effects', 'of', 'onsite', 'diagonal', 'disorder', 'leading', 'to', 'anderson', 'localization', 'are', 'addressed', 'as', 'well']] | [-0.14112246989602584, 0.18034849176818055, -0.0408910829945408, 0.08416219910686003, -0.004133210579389112, -0.14315664270605416, 0.07460775999030336, 0.3702304160638534, -0.29124731820155964, -0.2654438697574462, 0.03519385856108126, -0.2953452697132734, -0.07249601821890696, 0.17622814336766865, 0.04524694008014581, 0.009380748857090131, 0.05193245738120551, 0.02057827285867422, -0.052097147040222676, -0.21784253603719334, 0.28345325508927727, 0.11977814965970576, 0.304533295759416, 0.11332101568064475, 0.08453459375379409, 0.054422625734351894, 0.07106315491205835, -0.009751548009746253, -0.12352062027434356, 0.06256042517649822, 0.22805464840178288, -0.010091258440181574, 0.27868718555088134, -0.4076658536561151, -0.2097150864763225, 0.06326440093107522, 0.17952013876291606, 0.1693730492880469, -0.021977832318565985, -0.2586878248294716, 0.015539005287288826, -0.1487028487286768, -0.11524232066214143, -0.024384034933779945, 0.031591582964075375, 0.026643890088691596, -0.27543240068839525, 0.14329442214666607, 0.0584214925598799, 0.01408997776006606, -0.10494336625375349, -0.10549969730361246, -0.06136447066153856, 0.09901481531538749, 0.04815710989753418, -0.021843722678393997, 0.16977640172526082, -0.1268760263263446, -0.07804417117570646, 0.3530150698151122, -0.06991358880522386, -0.14415504866244985, 0.1548692965483729, -0.11700768380777593, -0.017991883375098622, 0.19118578973931552, 0.12157218924418904, 0.10816332221525335, -0.1403221013139781, 0.07986615034856863, 0.04543579036142043, 0.16752549449720003, 0.0612909081936913, 0.06433156245893383, 0.17545675126677182, 0.19571261348306856, 0.10642009785899179, 0.16397441062609358, -0.09558634241384038, -0.12765568378876815, -0.26165847190497243, -0.11750584520756248, -0.24290186355628587, 0.1070015503606323, -0.05266819635390346, -0.1103973575976697, 0.43775395404279943, 0.12219555402748968, 0.20799939715590804, 0.043139742766606044, 0.27412924107084885, 0.2418030194871306, 0.030583338366147687, 0.048029330660938285, 0.2720110476564398, 0.11948321916366075, 0.08502520517225655, -0.3657729391719492, 0.05785896080704604, 0.034473464645920916] |
710.2479 | Collisional stability of fermionic Feshbach molecules | Using a Feshbach resonance, we create ultracold fermionic molecules starting
from a Bose-Fermi atom gas mixture. The resulting mixture of atoms and weakly
bound molecules provides a rich system for studying few-body collisions because
of the variety of atomic collision partners for molecules; either bosonic,
fermionic, or distinguishable atoms. Inelastic loss of the molecules near the
Feshbach resonance is dramatically affected by the quantum statistics of the
colliding particles and the scattering length. In particular, we observe a
molecule lifetime as long as 100 ms near the Feshbach resonance.
| cond-mat.other | using a feshbach resonance we create ultracold fermionic molecules starting from a bosefermi atom gas mixture the resulting mixture of atoms and weakly bound molecules provides a rich system for studying fewbody collisions because of the variety of atomic collision partners for molecules either bosonic fermionic or distinguishable atoms inelastic loss of the molecules near the feshbach resonance is dramatically affected by the quantum statistics of the colliding particles and the scattering length in particular we observe a molecule lifetime as long as 100 ms near the feshbach resonance | [['using', 'a', 'feshbach', 'resonance', 'we', 'create', 'ultracold', 'fermionic', 'molecules', 'starting', 'from', 'a', 'bosefermi', 'atom', 'gas', 'mixture', 'the', 'resulting', 'mixture', 'of', 'atoms', 'and', 'weakly', 'bound', 'molecules', 'provides', 'a', 'rich', 'system', 'for', 'studying', 'fewbody', 'collisions', 'because', 'of', 'the', 'variety', 'of', 'atomic', 'collision', 'partners', 'for', 'molecules', 'either', 'bosonic', 'fermionic', 'or', 'distinguishable', 'atoms', 'inelastic', 'loss', 'of', 'the', 'molecules', 'near', 'the', 'feshbach', 'resonance', 'is', 'dramatically', 'affected', 'by', 'the', 'quantum', 'statistics', 'of', 'the', 'colliding', 'particles', 'and', 'the', 'scattering', 'length', 'in', 'particular', 'we', 'observe', 'a', 'molecule', 'lifetime', 'as', 'long', 'as', '100', 'ms', 'near', 'the', 'feshbach', 'resonance']] | [-0.11829838940018286, 0.2787080120211572, -0.05061154218202227, 0.06562185193950917, 0.05037999473344744, -0.197596834909715, 0.08264829743695393, 0.3454647392369388, -0.23392597620448705, -0.2533745008489389, -0.0734414574546279, -0.30601802561301317, -0.009786826393598418, 0.12859406917921026, 0.11578408502607365, 0.05648660559332772, 0.1288801255698703, 0.04787556729488744, -0.019623692418197485, -0.20335017900202382, 0.311394923989232, 0.047586936115161675, 0.19250285934154573, 0.1316886146531932, 0.07873260012430171, 0.06782144894352539, 0.14698079530819413, -0.12288927730418783, -0.12437250811522932, 0.14935554887640312, 0.26680896603606974, -0.0052509135435848085, 0.16550194734728405, -0.45403622909124647, -0.2110297902790683, 0.09985268099254437, 0.2559562963224278, 0.21807805435951758, -0.05422810754026522, -0.35916452072142213, -0.11683788345446496, -0.17993768273193514, -0.17406761831488837, -0.10598297695514192, 0.01952145109476333, 0.04196688730604528, -0.272955876393139, 0.08157953066264771, 0.03666206972485178, 0.15208605512599932, -0.05898746865764888, -0.11313782310442937, 0.0341501585678773, -0.009050865948011869, -0.04536372421079137, -0.009006204353017586, 0.2824475794423665, -0.19926498227313244, -0.052889789234888684, 0.4190415574258633, -0.16219288329175266, -0.10535951614840312, 0.30678908877451433, -0.134268989341773, -0.04591266397031003, 0.21223300402418951, 0.15765481367000914, 0.10900338218034653, -0.15603809781749262, 0.047237977687677554, -0.0913903181116735, 0.18825715170058768, 0.15279846059765373, 0.11089351711653465, 0.2938308081788461, 0.16939103823113308, -0.0018625722444626722, 0.1808291677845998, -0.19147510372437118, -0.15498895946304114, -0.19510162380011228, -0.15855831037382753, -0.2662532604979665, 0.020133067822355903, 0.0399511955012018, -0.12269606428702226, 0.31709571240281453, 0.05177199096272417, 0.2530654056123301, -0.08099190200145324, 0.2506009567518499, 0.0970915041084328, 0.0477301777560222, -0.011724762618541718, 0.22974561514814248, 0.16964070583573343, 0.022968050259887504, -0.3337154916587045, -0.023005242477788516, -0.010859225206914243] |
710.248 | Singularities of Brill-Noether loci for vector bundles on a curve | In this paper we consider the singularities of the varieties parameterizing
stable vector bundles of fixed rank and degree with sections on a smooth curve
of genus at least two. In particular, we extend results of Y. Laszlo, and of
the second author, regarding the singularities of generalized theta divisors.
| math.AG | in this paper we consider the singularities of the varieties parameterizing stable vector bundles of fixed rank and degree with sections on a smooth curve of genus at least two in particular we extend results of y laszlo and of the second author regarding the singularities of generalized theta divisors | [['in', 'this', 'paper', 'we', 'consider', 'the', 'singularities', 'of', 'the', 'varieties', 'parameterizing', 'stable', 'vector', 'bundles', 'of', 'fixed', 'rank', 'and', 'degree', 'with', 'sections', 'on', 'a', 'smooth', 'curve', 'of', 'genus', 'at', 'least', 'two', 'in', 'particular', 'we', 'extend', 'results', 'of', 'y', 'laszlo', 'and', 'of', 'the', 'second', 'author', 'regarding', 'the', 'singularities', 'of', 'generalized', 'theta', 'divisors']] | [-0.21655527201946825, 0.042706440560286864, -0.09378489595837891, 0.03442300117341802, -0.04030991879757494, -0.14718627429567277, 0.015452468560542911, 0.30326005777344106, -0.25807285994291307, -0.17378488708287476, 0.07543770786840469, -0.2841274927742779, -0.16630498901940882, 0.17505510874092578, -0.15372897006571293, 0.020628508515655994, -0.0011690501868724824, 0.0766223576106131, -0.1295907921716571, -0.3791269853385165, 0.5226061841100454, -0.044803626427892596, 0.17313967786729337, 0.11630221238359809, 0.14713199591264128, 0.06491736812517047, -0.03442275457084179, -0.003595769256353378, -0.16966239823028445, 0.17595491976477207, 0.30197060452774166, 0.05498197286389768, 0.18867223154753446, -0.3496175032481551, -0.16353601977229118, 0.2065990356076509, 0.08022457951214164, 0.026099126189947128, 0.05069022104842588, -0.1850267856568098, 0.11198680208995938, -0.11821788667497458, -0.2443195742368698, -0.043461668891832235, 0.0051063931011594834, 0.06680597711354494, -0.18614064145833253, 0.000461719436571002, 0.10441574074327946, 0.17092607174068689, -0.027415902754291892, -0.15156960025429725, -0.0726038718316704, 0.010576200848445296, 0.07472957760794088, 0.047234987765550615, -0.009824462551623583, -0.1544860097533092, -0.11457263879477977, 0.31651497703045606, -0.07593775201588869, -0.1916664944216609, 0.10925692649558187, -0.19228289502672852, -0.16866322790272534, 0.11978115411475301, 0.1888245196826756, 0.24620945698639843, 0.02297467418015003, 0.14727016772842036, -0.07055821891874076, 0.06904080705717205, 0.1842481160350144, -0.07420027498155832, 0.12592175183817744, 0.08808958889450878, 0.04546905415132642, 0.0937490081274882, -0.06869782552588731, -0.05099121837178245, -0.3949698131065816, -0.21884296709671616, -0.08865216067060828, 0.11994387349113822, -0.11291881443874445, -0.14104838088620453, 0.4834786831587553, 0.03929809014312923, 0.2906560419872403, 0.12185032285749912, 0.2511301565170288, 0.03816038122982718, -0.0388422067835927, 0.05971679605543614, 0.17390538306441158, 0.20291350154206156, -0.022588260686025024, -0.10835283854103181, -0.0054571886081248525, 0.17877102322876454] |
710.2481 | Stellar populations in the bulges of S0s and the formation of S0
galaxies | The stellar populations in the bulges of S0s, together with the galaxies'
dynamics, masses and globular clusters, contain very interesting clues about
their formation. I present here recent evidence suggesting that S0s are the
descendants of fading spirals whose star formation ceased.
| astro-ph | the stellar populations in the bulges of s0s together with the galaxies dynamics masses and globular clusters contain very interesting clues about their formation i present here recent evidence suggesting that s0s are the descendants of fading spirals whose star formation ceased | [['the', 'stellar', 'populations', 'in', 'the', 'bulges', 'of', 's0s', 'together', 'with', 'the', 'galaxies', 'dynamics', 'masses', 'and', 'globular', 'clusters', 'contain', 'very', 'interesting', 'clues', 'about', 'their', 'formation', 'i', 'present', 'here', 'recent', 'evidence', 'suggesting', 'that', 's0s', 'are', 'the', 'descendants', 'of', 'fading', 'spirals', 'whose', 'star', 'formation', 'ceased']] | [-0.10430846456438303, 0.127463738389668, -0.1371989692783072, 0.2031050824249784, -0.11279932967764103, -0.011374900516654764, 0.021412265827945833, 0.4696008459265743, -0.056020391306706836, -0.3439309013386567, 0.04303885864127161, -0.25157516600475427, -0.13527526209751764, 0.12529764459690168, -0.04439373796672693, -0.1408251399129984, 0.1036169201113461, -0.12215555973705791, -0.01720341539476067, -0.409800339091037, 0.31636559856789453, -0.019115712870621963, 0.07315521027582388, -0.13890766130671614, -0.005455311961538557, -0.1526192829922019, -0.10655750121389117, -0.10487230707492147, -0.2341630162203122, 0.019990101175305124, 0.23228865919546002, 0.141754063167831, 0.22299985136348932, -0.4423742401635363, -0.17246964580512472, 0.05612826850708751, 0.3076692128975299, 0.061416207147496085, -0.21627774738728822, -0.2758279436134866, 0.05706979649230128, -0.15069417349461997, -0.17284095555632598, 0.10934902964869425, 0.10718580037237621, 0.08348762400315277, -0.15956883203415645, 0.23357009184768512, 0.1045353006172393, 0.0817484182882167, -0.1553172903645429, -0.12167191352429134, -0.13061014953113737, 0.105656728059763, 0.04557513739425866, 0.03141560862284331, 0.24195282892989262, -0.181655375686075, -0.050778910207251705, 0.38196376115748926, 0.06526556380447887, 0.07150450178111593, 0.320679355434896, -0.2530890426021956, -0.24020086296479262, 0.0779152473634375, 0.13397332391745986, 0.04201250953511113, -0.15210883609861844, -0.04416564893160414, -0.004122933140024543, 0.1929384944516988, 0.03515124843189759, 0.16499792807735503, 0.4745382912723081, 0.1137276556387189, -0.023502977465146353, 0.03655146982609516, -0.10315360329557388, -0.09421820115364556, -0.16548011407610916, -0.07905411163699769, -0.0663184918867912, 0.12341356257508908, -0.16676335805061085, -0.11331712228379079, 0.3178823170518236, 0.02534715225920081, 0.2581996592260631, 0.11490818308222861, 0.2379521865929876, 0.0023923307834636596, 0.20301287838013932, 0.175235579233794, 0.252307877077588, 0.2618095412229498, 0.05098739227590462, -0.2908131505273992, 0.12400286990894183, -0.081131589903851] |
710.2482 | Can LHC Test the See-Saw Mechanism? | We discuss the prospects for detecting right-handed neutrinos which are
introduced in the see-saw mechanism at future colliders. This requires a very
accurate cancellation between contributions from different right-handed
neutrinos to the light neutrino mass matrix. We search for possible symmetries
behind this cancellation and find that they have to include lepton number
conservation. Light neutrino masses can be generated as a result of small
symmetry-breaking perturbations. The impact of these perturbations on LHC
physics is negligible, so that the mechanism of neutrino mass generation and
LHC physics are decoupled in general. In constrained cases, accelerator
observables and neutrino masses and mixings can be correlated.
| hep-ph | we discuss the prospects for detecting righthanded neutrinos which are introduced in the seesaw mechanism at future colliders this requires a very accurate cancellation between contributions from different righthanded neutrinos to the light neutrino mass matrix we search for possible symmetries behind this cancellation and find that they have to include lepton number conservation light neutrino masses can be generated as a result of small symmetrybreaking perturbations the impact of these perturbations on lhc physics is negligible so that the mechanism of neutrino mass generation and lhc physics are decoupled in general in constrained cases accelerator observables and neutrino masses and mixings can be correlated | [['we', 'discuss', 'the', 'prospects', 'for', 'detecting', 'righthanded', 'neutrinos', 'which', 'are', 'introduced', 'in', 'the', 'seesaw', 'mechanism', 'at', 'future', 'colliders', 'this', 'requires', 'a', 'very', 'accurate', 'cancellation', 'between', 'contributions', 'from', 'different', 'righthanded', 'neutrinos', 'to', 'the', 'light', 'neutrino', 'mass', 'matrix', 'we', 'search', 'for', 'possible', 'symmetries', 'behind', 'this', 'cancellation', 'and', 'find', 'that', 'they', 'have', 'to', 'include', 'lepton', 'number', 'conservation', 'light', 'neutrino', 'masses', 'can', 'be', 'generated', 'as', 'a', 'result', 'of', 'small', 'symmetrybreaking', 'perturbations', 'the', 'impact', 'of', 'these', 'perturbations', 'on', 'lhc', 'physics', 'is', 'negligible', 'so', 'that', 'the', 'mechanism', 'of', 'neutrino', 'mass', 'generation', 'and', 'lhc', 'physics', 'are', 'decoupled', 'in', 'general', 'in', 'constrained', 'cases', 'accelerator', 'observables', 'and', 'neutrino', 'masses', 'and', 'mixings', 'can', 'be', 'correlated']] | [-0.10779115688499241, 0.3299817806287181, -0.004357662109569425, 0.22914266287060897, -0.09464817423196066, -0.17611068306224686, 0.004298899972456552, 0.33379730756084125, -0.2471424949000634, -0.32940568578473867, 0.04908950541257149, -0.2788519987304296, -0.06147919444178808, 0.1801394900018793, 0.04128637487689654, 0.026720414119994356, 0.06059118093357289, -0.07296589964202473, -0.0853554181327733, -0.249143427486221, 0.3002501417927089, 0.10819208687614827, 0.1910929852120933, 0.10951032850758306, 0.06854428471553893, -0.0778925550879822, -0.05465216774138666, -0.1090121939566459, -0.012999403259822255, 0.027308917752954933, 0.22056107816059098, 0.1305576362381024, 0.10755355823785066, -0.4090803516762597, -0.16947536613969577, 0.18087320945979585, 0.1540751908262748, 0.1304439560233039, -0.16634328832428547, -0.2822798749520665, 0.0931111870527578, -0.21148145020096784, -0.1268628579520044, -0.07670811550203888, -0.0501320999913982, -0.06678118796220847, -0.3349167223664976, 0.07702068522395122, -0.059223223861218206, -0.05332067576902253, 0.017929014845174694, -0.1860530598920637, -0.03738409959311996, 0.05231598312744782, 0.18415520842896685, -0.07994299670681357, 0.12344252430734091, -0.17792917592894464, -0.13253479769475582, 0.44668430941445486, -0.03983637379216296, -0.1689614964006025, 0.15511151426028283, -0.16417431026874554, -0.15779155837371944, 0.09060018077670108, 0.26124563455315575, 0.0663678839628119, -0.18915224176432405, 0.112578606479136, -0.06387365853768728, 0.11582128373639924, 0.06695010037649246, 0.089977501459708, 0.3467438680607648, 0.20625050047944699, 0.09539764278812245, -0.05211093964809108, -0.10304883301391134, -0.01619849499547854, -0.42105537804641896, -0.06328165831052632, -0.10030099259068569, 0.06365749305557637, -0.02609428113182297, -0.07537187052713264, 0.448273037054709, 0.19241231844893525, 0.19418637427678775, 0.011081614971737421, 0.3036219783947759, 0.07665811625331463, 0.10518764640603746, 0.04037434463077391, 0.3617762431413645, 0.1354347896618059, 0.11978517698381828, -0.24545379367302217, 0.005305409604417426, 0.08233264607510396] |
710.2483 | On the arithmetical rank of a special class of minimal varieties | We study the arithmetical ranks and the cohomological dimensions of an
infinite class of Cohen-Macaulay varieties of minimal degree. Among these we
find, on the one hand, infinitely many set-theoretic complete intersections, on
the other hand examples where the arithmetical rank is arbitrarily greater than
the codimension.
| math.AC math.AG | we study the arithmetical ranks and the cohomological dimensions of an infinite class of cohenmacaulay varieties of minimal degree among these we find on the one hand infinitely many settheoretic complete intersections on the other hand examples where the arithmetical rank is arbitrarily greater than the codimension | [['we', 'study', 'the', 'arithmetical', 'ranks', 'and', 'the', 'cohomological', 'dimensions', 'of', 'an', 'infinite', 'class', 'of', 'cohenmacaulay', 'varieties', 'of', 'minimal', 'degree', 'among', 'these', 'we', 'find', 'on', 'the', 'one', 'hand', 'infinitely', 'many', 'settheoretic', 'complete', 'intersections', 'on', 'the', 'other', 'hand', 'examples', 'where', 'the', 'arithmetical', 'rank', 'is', 'arbitrarily', 'greater', 'than', 'the', 'codimension']] | [-0.18019135532147706, 0.058050674359385976, -0.027955114881091928, 0.11321879393530097, -0.08081817785476117, -0.19236730156030427, -0.03834739875325814, 0.28045116480875837, -0.2625693448601251, -0.2062322204694786, 0.13197108770799923, -0.32631951237612583, -0.12172325567758464, 0.21244222528122841, -0.117929742127865, -0.015786030508102254, 0.016069699970490122, 0.18459063070885678, -0.06700581912585396, -0.4056564528257289, 0.4782233623629238, -0.08761797116157856, 0.21302337204403382, 0.07234063382914409, 0.12153071054118744, -0.006574280619462754, 0.013426731915232982, 0.03808941341381758, -0.1677318108367159, 0.19756405424088874, 0.29316754258693534, 0.08823702369440109, 0.22450009622472397, -0.42489687725901604, -0.12062598009930646, 0.2605820490701243, 0.11216653205771396, 0.06070815248692289, 0.06560302162642016, -0.1962694102264148, 0.10773892284549297, -0.15390679215240796, -0.19762613683780458, -0.08737499837545638, 0.06379901447600902, 0.015378233555585463, -0.1997378172075495, -0.04690564780476245, 0.1476338010162432, 0.2140795658441617, -0.0023050192010370973, -0.15907834630776593, -0.08803862084614787, 0.027311054197080593, 0.03149273264855939, -0.07830977279871226, 0.0566075851675123, -0.14811801950774214, -0.13481175198041379, 0.3136594405278881, 0.038969237063553167, -0.2318497286673556, 0.2721718546830395, -0.18294221925687917, -0.17955701441523877, 0.10338566424523263, 0.0873794953556771, 0.19919762246253742, 0.034367363265854246, 0.15253471123287454, -0.1506413604390431, 0.14340210973503106, 0.17764907641375952, 0.07630721885869478, 0.11738271785384798, 0.1053545467773492, 0.12273986568114661, 0.12770079581706012, 0.00755751214208121, -0.045660317716921896, -0.327709430590906, -0.18749597238654153, -0.1213660430004622, 0.15659156007731848, -0.19198405214534586, -0.18359539059406899, 0.47346710318580587, 0.12630222777419903, 0.1520697220050274, 0.13905792786402904, 0.2849817482080865, 0.011352498440983448, 0.02618457842618227, 0.08357899537944097, 0.12164925214180604, 0.13036920360111176, -0.10773101524311177, -0.10665623392870134, 0.043560550191459504, 0.19281768944471123] |
710.2484 | Cosmological implications of the Higgs mass measurement | We assume the validity of the Standard Model up to an arbitrary high-energy
scale and discuss what information on the early stages of the Universe can be
extracted from a measurement of the Higgs mass. For Mh < 130 GeV, the Higgs
potential can develop an instability at large field values. From the absence of
excessive thermal Higgs field fluctuations we derive a bound on the reheat
temperature after inflation as a function of the Higgs and top masses. Then we
discuss the interplay between the quantum Higgs fluctuations generated during
the primordial stage of inflation and the cosmological perturbations, in the
context of landscape scenarios in which the inflationary parameters scan. We
show that, within the large-field models of inflation, it is highly improbable
to obtain the observed cosmological perturbations in a Universe with a light
Higgs. Moreover, independently of the inflationary model, the detection of
primordial tensor perturbations through the B-mode of CMB polarization and the
discovery of a light Higgs can simultaneously occur only with exponentially
small probability, unless there is new physics beyond the Standard Model.
| hep-ph astro-ph hep-th | we assume the validity of the standard model up to an arbitrary highenergy scale and discuss what information on the early stages of the universe can be extracted from a measurement of the higgs mass for mh 130 gev the higgs potential can develop an instability at large field values from the absence of excessive thermal higgs field fluctuations we derive a bound on the reheat temperature after inflation as a function of the higgs and top masses then we discuss the interplay between the quantum higgs fluctuations generated during the primordial stage of inflation and the cosmological perturbations in the context of landscape scenarios in which the inflationary parameters scan we show that within the largefield models of inflation it is highly improbable to obtain the observed cosmological perturbations in a universe with a light higgs moreover independently of the inflationary model the detection of primordial tensor perturbations through the bmode of cmb polarization and the discovery of a light higgs can simultaneously occur only with exponentially small probability unless there is new physics beyond the standard model | [['we', 'assume', 'the', 'validity', 'of', 'the', 'standard', 'model', 'up', 'to', 'an', 'arbitrary', 'highenergy', 'scale', 'and', 'discuss', 'what', 'information', 'on', 'the', 'early', 'stages', 'of', 'the', 'universe', 'can', 'be', 'extracted', 'from', 'a', 'measurement', 'of', 'the', 'higgs', 'mass', 'for', 'mh', '130', 'gev', 'the', 'higgs', 'potential', 'can', 'develop', 'an', 'instability', 'at', 'large', 'field', 'values', 'from', 'the', 'absence', 'of', 'excessive', 'thermal', 'higgs', 'field', 'fluctuations', 'we', 'derive', 'a', 'bound', 'on', 'the', 'reheat', 'temperature', 'after', 'inflation', 'as', 'a', 'function', 'of', 'the', 'higgs', 'and', 'top', 'masses', 'then', 'we', 'discuss', 'the', 'interplay', 'between', 'the', 'quantum', 'higgs', 'fluctuations', 'generated', 'during', 'the', 'primordial', 'stage', 'of', 'inflation', 'and', 'the', 'cosmological', 'perturbations', 'in', 'the', 'context', 'of', 'landscape', 'scenarios', 'in', 'which', 'the', 'inflationary', 'parameters', 'scan', 'we', 'show', 'that', 'within', 'the', 'largefield', 'models', 'of', 'inflation', 'it', 'is', 'highly', 'improbable', 'to', 'obtain', 'the', 'observed', 'cosmological', 'perturbations', 'in', 'a', 'universe', 'with', 'a', 'light', 'higgs', 'moreover', 'independently', 'of', 'the', 'inflationary', 'model', 'the', 'detection', 'of', 'primordial', 'tensor', 'perturbations', 'through', 'the', 'bmode', 'of', 'cmb', 'polarization', 'and', 'the', 'discovery', 'of', 'a', 'light', 'higgs', 'can', 'simultaneously', 'occur', 'only', 'with', 'exponentially', 'small', 'probability', 'unless', 'there', 'is', 'new', 'physics', 'beyond', 'the', 'standard', 'model']] | [-0.1056165943844452, 0.2317956586710799, -0.10735565999928633, 0.12524781356482406, -0.05371409909560361, -0.12948393774499814, -0.005209400083130881, 0.27869437990304313, -0.24959535803515775, -0.3141389007279493, 0.08204659479917366, -0.22224434291392398, -0.07459356421188519, 0.16789562470544983, 0.012000862900531909, 0.022667857856107955, 0.050043163386657416, 0.03617751897005728, -0.025862579686598403, -0.2792492487972509, 0.32890308159793724, 0.10206242073938646, 0.2176071679188386, 0.04290563504955622, 0.08522841451408643, -0.041076296911829846, -0.0004945236463724068, -0.04520284886830929, -0.1506353434679367, 0.0737014396724879, 0.1394028007017272, 0.14346951505106836, 0.21067946008276506, -0.3761679263754264, -0.2334704146975412, 0.1905440051832455, 0.12606482690215817, 0.17240875174470932, -0.05445169988504543, -0.29335321538545733, 0.09239405022567274, -0.1690398481278664, -0.09601146317290028, -0.048905871817634006, -0.037610555430562055, -0.07873704338539912, -0.3085600361754785, 0.09970882745829084, -0.03860084328529888, 0.00933907317601186, -0.046036732226984796, -0.06610457726244362, -0.060101339377608545, 0.021683798723089294, 0.13800050147487808, 0.014977453926229569, 0.18509109522470965, -0.2090685011847621, -0.09679420343886375, 0.3981575674361773, -0.17631587643545724, -0.0953224855358062, 0.12698467335450417, -0.1813418697286137, -0.13039985557175215, 0.09083620699216201, 0.18487013471390865, 0.07966711457204802, -0.11505722310055859, 0.16747266749653694, 0.04365163225701402, 0.17937344557595278, 0.06336147538334257, 0.026834632751308173, 0.3514499056085361, 0.1531849504089472, 0.03493870281244956, 0.10405264645827902, -0.09947380815455742, -0.07510572372722393, -0.4101209520211433, -0.10246298790229068, -0.137280863872339, 0.0584045374289925, -0.15201249126281183, -0.16778042465032145, 0.4498039339669049, 0.18319884360918787, 0.26058491649705784, 0.028192886322419362, 0.2975508616144597, 0.07895827226733591, 0.059689563126745504, 0.05487546162398834, 0.34505978418909555, 0.11519749695825385, 0.13360166304364968, -0.20692841164955048, 0.025783097236183102, 0.00904313774321582] |
710.2485 | RHIC Low-Energy Challenges and Plans | There is significant interest in RHIC heavy ion collisions at
$\sqrt{s_{NN}}=$5--50 GeV, motivated by a search for the QCD phase transition
critical point. The lowest energies for this search are well below the nominal
RHIC gold injection collision energy of $\sqrt{s_{NN}}=19.6$ GeV. There are
several operations challenges at RHIC in this regime, including longitudinal
acceptance, magnet field quality, lattice control, and luminosity monitoring.
We report on the status of work to address these challenges, including results
from beam tests of low energy RHIC operations with protons and gold, and
potential improvements from different beam cooling scenarios.
| physics.acc-ph | there is significant interest in rhic heavy ion collisions at sqrts_nn550 gev motivated by a search for the qcd phase transition critical point the lowest energies for this search are well below the nominal rhic gold injection collision energy of sqrts_nn196 gev there are several operations challenges at rhic in this regime including longitudinal acceptance magnet field quality lattice control and luminosity monitoring we report on the status of work to address these challenges including results from beam tests of low energy rhic operations with protons and gold and potential improvements from different beam cooling scenarios | [['there', 'is', 'significant', 'interest', 'in', 'rhic', 'heavy', 'ion', 'collisions', 'at', 'sqrts_nn550', 'gev', 'motivated', 'by', 'a', 'search', 'for', 'the', 'qcd', 'phase', 'transition', 'critical', 'point', 'the', 'lowest', 'energies', 'for', 'this', 'search', 'are', 'well', 'below', 'the', 'nominal', 'rhic', 'gold', 'injection', 'collision', 'energy', 'of', 'sqrts_nn196', 'gev', 'there', 'are', 'several', 'operations', 'challenges', 'at', 'rhic', 'in', 'this', 'regime', 'including', 'longitudinal', 'acceptance', 'magnet', 'field', 'quality', 'lattice', 'control', 'and', 'luminosity', 'monitoring', 'we', 'report', 'on', 'the', 'status', 'of', 'work', 'to', 'address', 'these', 'challenges', 'including', 'results', 'from', 'beam', 'tests', 'of', 'low', 'energy', 'rhic', 'operations', 'with', 'protons', 'and', 'gold', 'and', 'potential', 'improvements', 'from', 'different', 'beam', 'cooling', 'scenarios']] | [-0.07288858552561386, 0.22763377404036492, -0.0621678309637661, 0.08179933705097554, 0.02200046818654396, -0.13967656046642285, 0.04462044949790365, 0.40959183565880125, -0.21223691397003439, -0.3533487173679628, 0.04326437003175287, -0.34880893768154475, 0.08363415556714723, 0.23571844934730937, 0.02691865362423031, 0.11670545376837253, 0.1252683946568715, -0.044372601924758205, -0.08004482126500653, -0.18225950849928746, 0.2799785575437311, 0.14676023579055542, 0.28841866035210456, 0.18978680620264066, 0.0581828972226695, 0.0008653617660073857, 0.04287150636511414, -0.029641245330046667, -0.1483153664261887, 0.04542349517915251, 0.3004428453155254, 0.056604895167248814, 0.23853404731734804, -0.39151021148029125, -0.16681749217800404, 0.10131566600727016, 0.08542650230902885, 0.10190958159142419, -0.1495321372389107, -0.23273345659437933, 0.05752871763941489, -0.2110856548834004, -0.1159706477664019, -0.047060293096460794, -0.032025004564294295, 0.05684551912310876, -0.264284005291809, 0.0674621922723753, -0.04148200656115813, 0.13720003879187923, -0.051479125008183094, -0.19944809616641387, -0.006891026193472116, 0.007431059894397071, 0.09602096887844566, 0.09228444895461986, 0.1944837116538302, -0.1735757900610272, -0.1844233930846186, 0.4053270840306619, 0.03987324033116334, -0.03935319262703783, 0.20618620594277193, -0.209023595718961, -0.14779175020950405, 0.17885073194966505, 0.23919963179352252, 0.05641852659418395, -0.1858538970449253, 0.041547174546806336, 0.04531726944995554, 0.1490987850560295, 0.11916665215976537, 0.04550189858939695, 0.23763845784491613, 0.25783949149282354, 0.03753277603536844, 0.10322624778782483, -0.12038997597747335, -0.06970703312146821, -0.3700165293718639, -0.0538919473066926, -0.11466176716708823, 0.001964759483541313, -0.031047358495753113, -0.024605259446329193, 0.38578105385562306, 0.16126001275391133, 0.20584591464384605, -0.04653694878185266, 0.3306159240585801, 0.07150844901211952, 0.053183073489191504, 0.0973156817992659, 0.2877190031503376, 0.0679988624258457, 0.21656493473013766, -0.2269299107162576, 0.0004770125605558094, -0.003037747417233492] |
710.2486 | Measuring Fine Tuning In Supersymmetry | The solution to fine tuning is one of the principal motivations for
supersymmetry. However constraints on the parameter space of the Minimal
Supersymmetric Standard Model (MSSM) suggest it may also require fine tuning
(although to a much lesser extent). To compare this tuning with different
extensions of the Standard Model (including other supersymmetric models) it is
essential that we have a reliable, quantitative measure of tuning. We review
the measures of tuning used in the literature and propose an alternative
measure. We apply this measure to several toy models and the MSSM with some
intriguing results.
| hep-ph | the solution to fine tuning is one of the principal motivations for supersymmetry however constraints on the parameter space of the minimal supersymmetric standard model mssm suggest it may also require fine tuning although to a much lesser extent to compare this tuning with different extensions of the standard model including other supersymmetric models it is essential that we have a reliable quantitative measure of tuning we review the measures of tuning used in the literature and propose an alternative measure we apply this measure to several toy models and the mssm with some intriguing results | [['the', 'solution', 'to', 'fine', 'tuning', 'is', 'one', 'of', 'the', 'principal', 'motivations', 'for', 'supersymmetry', 'however', 'constraints', 'on', 'the', 'parameter', 'space', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'suggest', 'it', 'may', 'also', 'require', 'fine', 'tuning', 'although', 'to', 'a', 'much', 'lesser', 'extent', 'to', 'compare', 'this', 'tuning', 'with', 'different', 'extensions', 'of', 'the', 'standard', 'model', 'including', 'other', 'supersymmetric', 'models', 'it', 'is', 'essential', 'that', 'we', 'have', 'a', 'reliable', 'quantitative', 'measure', 'of', 'tuning', 'we', 'review', 'the', 'measures', 'of', 'tuning', 'used', 'in', 'the', 'literature', 'and', 'propose', 'an', 'alternative', 'measure', 'we', 'apply', 'this', 'measure', 'to', 'several', 'toy', 'models', 'and', 'the', 'mssm', 'with', 'some', 'intriguing', 'results']] | [-0.03391395627113525, 0.08177998024757471, -0.05656993479351513, 0.13789664816188937, -0.1273130332507814, -0.1958262846649935, 0.027066002367064357, 0.401143088999864, -0.23090830251264075, -0.34861449761956464, 0.12056009717222575, -0.23636648512911052, -0.1297774134654901, 0.18937530306963404, -0.08087680367558885, 0.07288755344537397, 0.03984676900533183, 0.006372130398328106, -0.08388083321187878, -0.2116639206663725, 0.3088169482968321, 0.0740040658468691, 0.2450100535643287, 0.07487575057893991, 0.07349766710346255, -0.0384956667063913, -0.03938129516124415, -0.013652454756387064, -0.18824373525459728, 0.17219575137035767, 0.17291222515488394, 0.12052885359056138, 0.2247003631394667, -0.37404189895217616, -0.2619731943183676, 0.1851659739816872, 0.14476210614460192, 0.12163344988706133, -0.02285341187598533, -0.23761072741278136, 0.07328083266899436, -0.16890743976303688, -0.11850378925252396, -0.13753574560784423, -0.03920528711629837, -0.05277268798211784, -0.2651105410186574, 0.01856639719062514, -0.001231320634057435, 0.04051503780647181, -0.04401001015503425, -0.12174001811945345, -0.0004490159578078116, 0.08219294511460855, 0.11173765769975337, 0.006319399195490405, 0.1353918027355879, -0.1474005481528972, -0.1493505377341838, 0.39966395212104544, -0.08590221001456182, -0.24420934692413235, 0.23616883990568263, -0.11244945250048961, -0.16873793381576738, 0.036694695513385035, 0.11556373102939688, 0.10317721472529229, -0.12384592790476745, 0.12729011698562923, -0.049511658032618776, 0.20274004004507637, -0.015545259375358, 0.05352563883934636, 0.1810290073044598, 0.22014163259154884, 0.07842734238026121, 0.11941023615084607, -0.04759242444561096, -0.121011573287736, -0.3498844318673946, -0.14474742986688702, -0.09100461371902686, -0.0024902639949383834, -0.11324915402868403, -0.16376578750593276, 0.4644723216139634, 0.2582351285248781, 0.2436029048913042, 0.013084295360992352, 0.282241406928127, 0.08236199616415736, 0.10739513473405775, -0.025468704766050603, 0.2755468361444097, 0.06393373643853313, 0.04938829462237967, -0.19661989128023075, 0.020922263836837374, 0.03025487799701902] |
710.2487 | Quantum Shared Broadcasting | A generalization of quantum broadcasting protocol is presented. Here the goal
is to copy an unknown input state into two subsystems which partially overlap.
We show that the possibility of implementing these protocols strongly depends
upon the overlap among the subsystems. Conditions for approximated shared
broadcasting are analyzed.
| quant-ph | a generalization of quantum broadcasting protocol is presented here the goal is to copy an unknown input state into two subsystems which partially overlap we show that the possibility of implementing these protocols strongly depends upon the overlap among the subsystems conditions for approximated shared broadcasting are analyzed | [['a', 'generalization', 'of', 'quantum', 'broadcasting', 'protocol', 'is', 'presented', 'here', 'the', 'goal', 'is', 'to', 'copy', 'an', 'unknown', 'input', 'state', 'into', 'two', 'subsystems', 'which', 'partially', 'overlap', 'we', 'show', 'that', 'the', 'possibility', 'of', 'implementing', 'these', 'protocols', 'strongly', 'depends', 'upon', 'the', 'overlap', 'among', 'the', 'subsystems', 'conditions', 'for', 'approximated', 'shared', 'broadcasting', 'are', 'analyzed']] | [-0.2144036117339662, 0.18906074893584446, -0.05361870214498291, 0.025903000714606605, 0.0006235378532437608, -0.20752813089832975, 0.08564227677319043, 0.3953158012203251, -0.28741826066592085, -0.2687634519922237, 0.07354768539274421, -0.2442420648682552, -0.13499987180694006, 0.16896416346814172, -0.0792109030589927, 0.04840618216015476, 0.0830678987695137, 0.03805997416687509, -0.008114141707968278, -0.27450951425513875, 0.3465008388545054, 0.007955752431977695, 0.2929800945469954, 0.01654295266295473, 0.0916806389092623, 0.047354657241764166, -0.033390081293570496, -0.009228474518749863, -0.08601730959662746, 0.07745673617561503, 0.24825724088198817, 0.19619336052952954, 0.2644988325579713, -0.38256327738054097, -0.16134004281290495, 0.1029430718626827, 0.15518623783282237, 0.1314715830643157, -0.015099234219330052, -0.30033673211801215, 0.03836226195562631, -0.16979871498188004, -0.07834524267430727, -0.054762560951833926, -0.043538727525932096, -0.01225671671757785, -0.2716708455312376, 0.010466298010821143, 0.05419791907479521, -0.020288356927570323, -0.042038025751632326, -0.07088839323841967, 0.005971777873734633, 0.19630794013210107, -0.07636462255807903, -0.019961785110353958, 0.11028042650044274, -0.1038823266911398, -0.13888884345457578, 0.332383662268209, 0.009683150933900228, -0.2383446117164567, 0.19318923089304008, -0.06609336649610971, -0.1536017698914899, 0.06089303236997997, 0.12374207107738282, 0.06876514046840991, -0.18456298966581622, 0.024892300828165997, -0.04654354623441274, 0.2350977843743749, 0.060168739689591653, 0.14376370481719883, 0.15973173526193327, 0.13956491688926084, 0.11627812307172765, 0.18560077542982376, 0.0014593973755836487, -0.18938749445563494, -0.28692844587688643, -0.14963832599460147, -0.28135712336127955, 0.0030413907564555607, -0.018359057071696345, -0.12400822804678076, 0.40865822905713384, 0.12685674657889953, 0.16379347579398504, 0.008929865369282197, 0.3249224804652234, 0.07163073174888268, 0.030653172366631527, 0.12850869776836285, 0.2134594907790112, 0.12091884699960549, 0.01814287210193773, -0.23223899258543193, 0.10244682184808578, 0.04654895603986612] |
710.2488 | Submersions and effective descent of etale morphisms | Using the flatification by blow-up result of Raynaud and Gruson, we obtain
new results for submersive and subtrusive morphisms. We show that universally
subtrusive morphisms, and in particular universally open morphisms, are
morphisms of effective descent for the fibered category of etale morphisms. Our
results extend and supplement previous treatments on submersive morphisms by
Grothendieck, Picavet and Voevodsky. Applications include the universality of
geometric quotients and the elimination of noetherian hypotheses in many
instances.
| math.AG math.AC | using the flatification by blowup result of raynaud and gruson we obtain new results for submersive and subtrusive morphisms we show that universally subtrusive morphisms and in particular universally open morphisms are morphisms of effective descent for the fibered category of etale morphisms our results extend and supplement previous treatments on submersive morphisms by grothendieck picavet and voevodsky applications include the universality of geometric quotients and the elimination of noetherian hypotheses in many instances | [['using', 'the', 'flatification', 'by', 'blowup', 'result', 'of', 'raynaud', 'and', 'gruson', 'we', 'obtain', 'new', 'results', 'for', 'submersive', 'and', 'subtrusive', 'morphisms', 'we', 'show', 'that', 'universally', 'subtrusive', 'morphisms', 'and', 'in', 'particular', 'universally', 'open', 'morphisms', 'are', 'morphisms', 'of', 'effective', 'descent', 'for', 'the', 'fibered', 'category', 'of', 'etale', 'morphisms', 'our', 'results', 'extend', 'and', 'supplement', 'previous', 'treatments', 'on', 'submersive', 'morphisms', 'by', 'grothendieck', 'picavet', 'and', 'voevodsky', 'applications', 'include', 'the', 'universality', 'of', 'geometric', 'quotients', 'and', 'the', 'elimination', 'of', 'noetherian', 'hypotheses', 'in', 'many', 'instances']] | [-0.128237549255469, 0.01587121594431145, -0.08636456322357325, 0.1272187655459025, -0.076911685988307, -0.1633098200761846, -0.0024686297135693685, 0.3465800290927291, -0.40236781553498335, -0.2027955132403544, 0.08254797127530245, -0.22056103833019733, -0.12664168813664997, 0.2588976878805884, -0.27302987591496536, -0.016554305768970934, 0.07930793075689248, -0.006763683871499129, -0.04312604322164718, -0.32325478946524006, 0.4838731320308787, -0.05786138166274343, 0.24052448246095862, 0.10317807436554825, 0.07549436121979462, 0.01490693102989878, -0.058768634564642395, -0.014712443901225924, -0.16508201986237378, 0.13067517317831517, 0.3796941810786458, 0.09831400968001357, 0.14576321275006712, -0.3691234512520688, -0.1385217631285611, 0.14891353089229337, 0.10146612515007811, 0.04946158975362778, -0.043132049352529324, -0.3307633889439915, 0.10936667078307696, -0.14828705859503577, -0.06956025610810944, -0.17761896143700662, 0.06231437117925712, 0.12334089949727059, -0.2243409024817603, -0.05654698102277637, 0.17385348941066436, 0.18607410181845938, -0.10903898419679275, -0.08860574414554451, -0.026481455787351088, 0.06747451358075653, -0.01717106285504997, 0.04685913236545665, 0.11616872274982078, -0.0935473367970969, -0.16942503838134662, 0.336420446271742, -0.08276076689362526, -0.2042818748791303, 0.17477172086281437, -0.09562642677753631, -0.19653353807516397, 0.09137708153575659, -0.011383941370461668, 0.19447058185136745, -0.015614085218736104, 0.18656587693341342, -0.13699278361164033, 0.041319879548557634, 0.14710106980720802, 0.02860557107654001, 0.08774906258497919, 0.06778887555867966, 0.03129635238936836, 0.12335482092042055, 0.06874542284889945, -0.04835247694780784, -0.381571023698364, -0.16975511176777738, -0.01501526058917599, 0.1275044877614294, -0.10671140680829662, -0.13352939513778048, 0.38372220349098957, 0.1559764176873224, 0.17159777493881329, 0.20472140970440314, 0.22539013783846581, -0.04161933956368427, 0.05803340229072741, 0.017457455449870655, 0.16867789444181003, 0.2712002261741353, -0.03632674605053451, -0.05828205841992583, -0.013207005762628147, 0.2295768767661814] |
710.2489 | Moments of nucleon distribution amplitudes from irreducible three-quark
operators | Semi-exclusive and exclusive processes are becoming more and more important
in high energy physics since they are excellently suited to study the internal
hadronic structure. To analyze such processes the knowledge of the hadron
distribution amplitudes, which are universal for different reactions, is
essential. Only rather indirect information on these nonperturbative functions
can be obtained from measurements. In this work we report on a lattice QCD
computation of moments of nucleon distribution amplitudes using suitable
three-quark operators. However, these operators have to be renormalized and the
mixing is even more complicated than in the continuum. Using the symmetry group
of the hypercubic lattice we therefore derive and implement irreducibly
transforming three-quark operators, which allow us to control the mixing
pattern and will finally lead to quantitative predictions in the MSbar scheme.
We present preliminary results for leading-twist and next-to-leading twist
nucleon distribution amplitudes based on the QCDSF/UKQCD simulations with 2
flavors of dynamical clover fermions.
| hep-lat | semiexclusive and exclusive processes are becoming more and more important in high energy physics since they are excellently suited to study the internal hadronic structure to analyze such processes the knowledge of the hadron distribution amplitudes which are universal for different reactions is essential only rather indirect information on these nonperturbative functions can be obtained from measurements in this work we report on a lattice qcd computation of moments of nucleon distribution amplitudes using suitable threequark operators however these operators have to be renormalized and the mixing is even more complicated than in the continuum using the symmetry group of the hypercubic lattice we therefore derive and implement irreducibly transforming threequark operators which allow us to control the mixing pattern and will finally lead to quantitative predictions in the msbar scheme we present preliminary results for leadingtwist and nexttoleading twist nucleon distribution amplitudes based on the qcdsfukqcd simulations with 2 flavors of dynamical clover fermions | [['semiexclusive', 'and', 'exclusive', 'processes', 'are', 'becoming', 'more', 'and', 'more', 'important', 'in', 'high', 'energy', 'physics', 'since', 'they', 'are', 'excellently', 'suited', 'to', 'study', 'the', 'internal', 'hadronic', 'structure', 'to', 'analyze', 'such', 'processes', 'the', 'knowledge', 'of', 'the', 'hadron', 'distribution', 'amplitudes', 'which', 'are', 'universal', 'for', 'different', 'reactions', 'is', 'essential', 'only', 'rather', 'indirect', 'information', 'on', 'these', 'nonperturbative', 'functions', 'can', 'be', 'obtained', 'from', 'measurements', 'in', 'this', 'work', 'we', 'report', 'on', 'a', 'lattice', 'qcd', 'computation', 'of', 'moments', 'of', 'nucleon', 'distribution', 'amplitudes', 'using', 'suitable', 'threequark', 'operators', 'however', 'these', 'operators', 'have', 'to', 'be', 'renormalized', 'and', 'the', 'mixing', 'is', 'even', 'more', 'complicated', 'than', 'in', 'the', 'continuum', 'using', 'the', 'symmetry', 'group', 'of', 'the', 'hypercubic', 'lattice', 'we', 'therefore', 'derive', 'and', 'implement', 'irreducibly', 'transforming', 'threequark', 'operators', 'which', 'allow', 'us', 'to', 'control', 'the', 'mixing', 'pattern', 'and', 'will', 'finally', 'lead', 'to', 'quantitative', 'predictions', 'in', 'the', 'msbar', 'scheme', 'we', 'present', 'preliminary', 'results', 'for', 'leadingtwist', 'and', 'nexttoleading', 'twist', 'nucleon', 'distribution', 'amplitudes', 'based', 'on', 'the', 'qcdsfukqcd', 'simulations', 'with', '2', 'flavors', 'of', 'dynamical', 'clover', 'fermions']] | [-0.0797246265052367, 0.2320519303872941, -0.13433188589049444, 0.13083737674394563, -0.08393278609240247, -0.10244749034078972, 0.04733852808844418, 0.4069694311748589, -0.17313841951019582, -0.2560012945244389, 0.058934054385510186, -0.2763386302447367, -0.09052946584058866, 0.14794588120383842, 0.04737903586684561, 0.10648258461827231, 0.07107366601666135, -0.003246496066511158, -0.09210531603049246, -0.19220561327322597, 0.36961588090465913, 0.04447916933605748, 0.23697879427383023, 0.12301726145068964, 0.01901765772772412, 0.028081824625992485, -0.09477171182271935, -0.06646463703964987, -0.09020363980183198, 0.13157392510273044, 0.23757125283441236, 0.03445161834449297, 0.11746977057398086, -0.4498752992480032, -0.1631348146223313, 0.08309763543337824, 0.17400158135212898, 0.13790021120089918, -0.0071149999207268735, -0.27207043730323355, 0.07147028795894116, -0.190168679803009, -0.13773284875337155, -0.19147806249018157, -0.023414363072163637, -0.014722708047127291, -0.3261320806607874, 0.07818908038579168, -0.028461651267641556, 0.049126803099868756, -0.007389834694444172, -0.19540840909786283, -0.020343335893666072, 0.12442957278295991, 0.0335005282544561, 0.04724686992159414, 0.12891817036490408, -0.16766372355219397, -0.13908261022260113, 0.43274136605191854, -0.023197978335496548, -0.22028748873140544, 0.1543992202834136, -0.19853326204578362, -0.1721767832314776, 0.09659965913141927, 0.2032914764398048, 0.11158698915594047, -0.19462130237408282, 0.06681261481491908, -0.017844600696116687, 0.16764819510281087, 0.05502101615551979, 0.09170658866003636, 0.15572749732002136, 0.16318496500532473, 0.01312310415800781, 0.07462707237610894, -0.03393304705800068, -0.14084869811551706, -0.33002694192072074, -0.08841465224902476, -0.12046648932680969, 0.06915579712724373, -0.08379229054459551, -0.12990134691579208, 0.37970876741725784, 0.1625766423050194, 0.20155454840766446, 0.02831352844894413, 0.28665024301698133, 0.12875389964094447, 0.11064262950883037, 0.0653217893529443, 0.23302349473139453, 0.1625482399977984, 0.08822368170254893, -0.23082240102061582, 0.006541648824819394, 0.07704267632798292] |
710.249 | Dimensional Reduction Applied to Non-Supersymmetric Theories | We consider regularisation of a Yang-Mills theory by Dimensional Reduction
(DRED). In particular, the anomalous dimensions of fermion masses and gauge
coupling are computed to four-loop order. We put special emphasis on the
treatment of evanescent couplings which appear when DRED is applied to
non-supersymmetric theories. We highlight the importance of distinguishing
between the evanescent and the real couplings. Considering the special case of
a Super-Yang-Mills theory, we find that Dimensional Reduction is sufficient to
preserve Supersymmetry in our calculations.
| hep-th | we consider regularisation of a yangmills theory by dimensional reduction dred in particular the anomalous dimensions of fermion masses and gauge coupling are computed to fourloop order we put special emphasis on the treatment of evanescent couplings which appear when dred is applied to nonsupersymmetric theories we highlight the importance of distinguishing between the evanescent and the real couplings considering the special case of a superyangmills theory we find that dimensional reduction is sufficient to preserve supersymmetry in our calculations | [['we', 'consider', 'regularisation', 'of', 'a', 'yangmills', 'theory', 'by', 'dimensional', 'reduction', 'dred', 'in', 'particular', 'the', 'anomalous', 'dimensions', 'of', 'fermion', 'masses', 'and', 'gauge', 'coupling', 'are', 'computed', 'to', 'fourloop', 'order', 'we', 'put', 'special', 'emphasis', 'on', 'the', 'treatment', 'of', 'evanescent', 'couplings', 'which', 'appear', 'when', 'dred', 'is', 'applied', 'to', 'nonsupersymmetric', 'theories', 'we', 'highlight', 'the', 'importance', 'of', 'distinguishing', 'between', 'the', 'evanescent', 'and', 'the', 'real', 'couplings', 'considering', 'the', 'special', 'case', 'of', 'a', 'superyangmills', 'theory', 'we', 'find', 'that', 'dimensional', 'reduction', 'is', 'sufficient', 'to', 'preserve', 'supersymmetry', 'in', 'our', 'calculations']] | [-0.14694004469783978, 0.1736884231446311, -0.017721586488187314, 0.11183594983012882, -0.06837130091153085, -0.15642764108488336, 0.006020646789693274, 0.33888590466231105, -0.12430043944623322, -0.2510441023623571, 0.06023986667569261, -0.2706455141014885, -0.18794602287234738, 0.11714805423689541, -0.03391564600169659, 0.022445901518221945, 0.010383682133397087, 0.029794877185486256, -0.11292620130989235, -0.31333152584556956, 0.3395025261619594, -0.029336630704347045, 0.25283716432750225, 0.1088668023236096, 0.09726801383658312, 0.025658918835688382, -0.016328818278270773, 0.015879816585220398, -0.11843722196399539, 0.13541878930991516, 0.2533199494937435, -0.01211513705784455, 0.16511261640116573, -0.42345697749406097, -0.21628957665525378, 0.08013824228546582, 0.13382307194988244, 0.16103380377608117, -0.01323935747059295, -0.2591351634677267, 0.03680719998374116, -0.15452973576029763, -0.1495708895396092, -0.14930694772629066, -0.04262050476390868, -0.12022024705947842, -0.3077063011471182, 0.05938099985651206, -0.016060519171878694, 0.057570677648527635, -0.030171526968479155, -0.09182056048884987, -0.06973166091775056, 0.07364485299804073, 0.1579163878443069, 0.00286393107380718, 0.0635804429592099, -0.20199578589763406, -0.13783834305941128, 0.4048780704208184, -0.062066718748246784, -0.23413871111115442, 0.20210965193109587, -0.17035488489200362, -0.18225907864398322, 0.07240616393100936, 0.18679121733293869, 0.1334866663441062, -0.08920505661317293, 0.22450173082615948, -0.019645729195326568, 0.11384137487330008, 0.11230337072047406, 0.03650654230150394, 0.17062581517966463, 0.1354438378068153, 0.01345918538281694, 0.1495104357425589, -0.0397745448135538, -0.12234397990978323, -0.40371683635748923, -0.13289485312998295, -0.11485498846741393, 0.08849150649330113, -0.1443785059145739, -0.155180197826121, 0.3581116913119331, 0.19464291044714627, 0.15295060960343107, 0.02456699546382879, 0.2375577285682084, 0.1825884451660386, 0.10877771314117127, -0.004715601238422096, 0.2819331219419837, 0.20840885013167282, 0.023192165268119423, -0.273273285489995, -0.1328163140286051, 0.16819113723468035] |
710.2491 | The Rapid Outbursting Star GM Cep: An EX-or in Tr 37? | We present optical, IR and millimeter observations of the solar-type star
13-277, also known as GM Cep, in the 4 Myr-old cluster Tr 37. GM Cep
experiences rapid magnitude variations of more than 2 mag at optical
wavelengths. We explore the causes of the variability, which seem to be
dominated by strong increases in the accretion, being similar to EX-or
episodes. The star shows high, variable accretion rates (up to ~10$^{-6}$
Msun/yr), signs of powerful winds, and it is a very fast rotator (Vsini~43
km/s). Its strong mid-IR excesses reveal a very flared disk and/or a remnant
envelope, most likely out of hydrostatic equilibrium. The 1.3 millimeter fluxes
suggest a relatively massive disk (Mdisk~0.1 Msun). Nevertheless, the
millimeter mass is not enough to sustain increased accretion episodes over
large timescales, unless the mass is underestimated due to significant grain
growth. We finally explore the possibility of GM Cep having a binary companion,
which could trigger disk instabilities producing the enhanced accretion
episodes.
| astro-ph | we present optical ir and millimeter observations of the solartype star 13277 also known as gm cep in the 4 myrold cluster tr 37 gm cep experiences rapid magnitude variations of more than 2 mag at optical wavelengths we explore the causes of the variability which seem to be dominated by strong increases in the accretion being similar to exor episodes the star shows high variable accretion rates up to 106 msunyr signs of powerful winds and it is a very fast rotator vsini43 kms its strong midir excesses reveal a very flared disk andor a remnant envelope most likely out of hydrostatic equilibrium the 13 millimeter fluxes suggest a relatively massive disk mdisk01 msun nevertheless the millimeter mass is not enough to sustain increased accretion episodes over large timescales unless the mass is underestimated due to significant grain growth we finally explore the possibility of gm cep having a binary companion which could trigger disk instabilities producing the enhanced accretion episodes | [['we', 'present', 'optical', 'ir', 'and', 'millimeter', 'observations', 'of', 'the', 'solartype', 'star', '13277', 'also', 'known', 'as', 'gm', 'cep', 'in', 'the', '4', 'myrold', 'cluster', 'tr', '37', 'gm', 'cep', 'experiences', 'rapid', 'magnitude', 'variations', 'of', 'more', 'than', '2', 'mag', 'at', 'optical', 'wavelengths', 'we', 'explore', 'the', 'causes', 'of', 'the', 'variability', 'which', 'seem', 'to', 'be', 'dominated', 'by', 'strong', 'increases', 'in', 'the', 'accretion', 'being', 'similar', 'to', 'exor', 'episodes', 'the', 'star', 'shows', 'high', 'variable', 'accretion', 'rates', 'up', 'to', '106', 'msunyr', 'signs', 'of', 'powerful', 'winds', 'and', 'it', 'is', 'a', 'very', 'fast', 'rotator', 'vsini43', 'kms', 'its', 'strong', 'midir', 'excesses', 'reveal', 'a', 'very', 'flared', 'disk', 'andor', 'a', 'remnant', 'envelope', 'most', 'likely', 'out', 'of', 'hydrostatic', 'equilibrium', 'the', '13', 'millimeter', 'fluxes', 'suggest', 'a', 'relatively', 'massive', 'disk', 'mdisk01', 'msun', 'nevertheless', 'the', 'millimeter', 'mass', 'is', 'not', 'enough', 'to', 'sustain', 'increased', 'accretion', 'episodes', 'over', 'large', 'timescales', 'unless', 'the', 'mass', 'is', 'underestimated', 'due', 'to', 'significant', 'grain', 'growth', 'we', 'finally', 'explore', 'the', 'possibility', 'of', 'gm', 'cep', 'having', 'a', 'binary', 'companion', 'which', 'could', 'trigger', 'disk', 'instabilities', 'producing', 'the', 'enhanced', 'accretion', 'episodes']] | [-0.12111556631551013, 0.1622589602715002, -0.043464375440171864, 0.10764651334736168, -0.1066344463260575, -0.11663968441715031, 0.09003301322864334, 0.4306569431510127, -0.1746807472213646, -0.3280075358098033, 0.12171459341064424, -0.2258899494150431, -0.03271643272688929, 0.18762042210730226, -0.08783765291683844, -0.03744915760606937, 0.09090872093487484, -0.11825674335448856, -0.06083390583341309, -0.22229467350022197, 0.24391177165360078, 0.08834329980671546, 0.10622098677976162, 0.0019799371238259024, 0.0276969493426816, -0.1674469225899369, -0.07043409854233698, -0.09464011074529972, -0.1390573028819167, -0.00910801564067977, 0.21901114831485277, 0.08159684612117005, 0.23369493010401163, -0.35657276249045516, -0.24021466397838676, 0.07628485930822906, 0.19374751382208658, 0.006460146772025048, -0.061800831913931216, -0.1816479005849387, 0.11850289386695649, -0.251851939865675, -0.18201096688321083, 0.06530773101349613, 0.10905739722726573, -0.012287177846535642, -0.27879321415551334, 0.119569654574833, 0.058989494683882863, 0.0853112907904499, -0.09878511754019807, -0.051859255800310686, -0.08372517545127643, -0.0011538382555188248, 0.0747365400549493, 0.14381249297597687, 0.21337579789061872, -0.17212031602730635, -0.01917301686539215, 0.3877088497627128, -0.09389181436654898, 0.022011924107447737, 0.31717973430465274, -0.27409804921374664, -0.1545490729426687, 0.24138938884818986, 0.14152107430320326, 0.1368464423232249, -0.11754294875247767, -0.08511884811073658, 0.028971107906527207, 0.25310681125078843, 0.06798961434115029, 0.07794230425607343, 0.38728660943994075, 0.13827426854591324, 0.010969992700683058, 0.1241546040887757, -0.23555829884402407, -0.07314085261603384, -0.1819884714541617, -0.06686496199547963, -0.08561880806015816, 0.12919348494434194, -0.16466406830011737, -0.0934071096023486, 0.3016045370268044, 0.10619021406244931, 0.2154374004622816, 0.009370731517859976, 0.2674983277471748, 0.11712416255357529, 0.16630519285458345, 0.17458450936847045, 0.3522544417342862, 0.17563590279827188, 0.14808243398522408, -0.2568341316765104, 0.09396861141266406, -0.04305500412687847] |
710.2492 | O(a^2) cutoff effects in Wilson fermion simulations | We show that the size of the O(a^2) flavour violating cutoff artifacts that
have been found to affect the value of the neutral pion mass in simulations
with maximally twisted Wilson fermions is controlled by a continuum QCD
quantity that is fairly large and is determined by the dynamical mechanism of
spontaneous chiral symmetry breaking. One can argue that the neutral pion mass
is the only physical quantity blurred by such cutoff effects. O(a^2)
corrections of this kind are also present in standard Wilson fermion
simulations, but they can either affect the determination of the pion mass or
be shifted from the latter to other observables, depending on the way the
critical mass is evaluated.
| hep-lat | we show that the size of the oa2 flavour violating cutoff artifacts that have been found to affect the value of the neutral pion mass in simulations with maximally twisted wilson fermions is controlled by a continuum qcd quantity that is fairly large and is determined by the dynamical mechanism of spontaneous chiral symmetry breaking one can argue that the neutral pion mass is the only physical quantity blurred by such cutoff effects oa2 corrections of this kind are also present in standard wilson fermion simulations but they can either affect the determination of the pion mass or be shifted from the latter to other observables depending on the way the critical mass is evaluated | [['we', 'show', 'that', 'the', 'size', 'of', 'the', 'oa2', 'flavour', 'violating', 'cutoff', 'artifacts', 'that', 'have', 'been', 'found', 'to', 'affect', 'the', 'value', 'of', 'the', 'neutral', 'pion', 'mass', 'in', 'simulations', 'with', 'maximally', 'twisted', 'wilson', 'fermions', 'is', 'controlled', 'by', 'a', 'continuum', 'qcd', 'quantity', 'that', 'is', 'fairly', 'large', 'and', 'is', 'determined', 'by', 'the', 'dynamical', 'mechanism', 'of', 'spontaneous', 'chiral', 'symmetry', 'breaking', 'one', 'can', 'argue', 'that', 'the', 'neutral', 'pion', 'mass', 'is', 'the', 'only', 'physical', 'quantity', 'blurred', 'by', 'such', 'cutoff', 'effects', 'oa2', 'corrections', 'of', 'this', 'kind', 'are', 'also', 'present', 'in', 'standard', 'wilson', 'fermion', 'simulations', 'but', 'they', 'can', 'either', 'affect', 'the', 'determination', 'of', 'the', 'pion', 'mass', 'or', 'be', 'shifted', 'from', 'the', 'latter', 'to', 'other', 'observables', 'depending', 'on', 'the', 'way', 'the', 'critical', 'mass', 'is', 'evaluated']] | [-0.11133133752635964, 0.2802188745416377, -0.08217136760282776, 0.10148476451716346, -0.045594577782827876, -0.11599852569988402, 0.051988094192727104, 0.36235870440369067, -0.1927446491935331, -0.2784487422393716, 0.07613783279717293, -0.2813945631618085, -0.060620877160893184, 0.11769779919565695, -0.014368444798595231, 0.0634050727457456, 0.02461488368394582, 0.02332579676142853, -0.10529166025656235, -0.18675746388490433, 0.378120206642653, 0.045488559454679486, 0.22058441208108612, 0.15577351382893065, 0.00789463754095461, -0.06143506728922543, -0.04835244194887903, -0.009240500126843867, -0.07568627304078647, 0.026617530790036138, 0.13062311374055952, 0.03904797627752566, 0.1319372078201369, -0.3525139461230973, -0.19989118674534637, 0.10845620463723722, 0.18522980274308634, 0.12802000172922146, -0.028788929587513532, -0.26950631270630526, 0.05837045069277772, -0.17077143643172862, -0.18075102809411675, -0.10451395855811627, -0.02818517114400216, -0.05023538240272066, -0.3086182618837642, 0.11560654826538191, -0.03463260330912738, 0.028827393854684805, 0.015936964094314887, -0.14440358854506327, -0.08229711779352764, 0.10500034065917134, 0.13972555271592801, 0.04811889218652378, 0.2082497001149813, -0.18516376651418598, -0.11591890614641749, 0.4614111486417444, -0.06078992670138731, -0.2200245567159626, 0.1252463622909525, -0.19920579679715245, -0.14435174769478973, 0.1468219134069564, 0.1274730813284607, 0.07953074870064207, -0.17251069443300365, 0.09836557686035319, -0.10843765978579936, 0.21775433056603144, 0.07409371631219983, 0.04836925237804003, 0.26313262155441486, 0.12056707209381072, 0.0033307623624315727, 0.07310789774890745, -0.02967294236118703, -0.10435378291927602, -0.3351392935475577, -0.08013300398040725, -0.1721055756242055, 0.09053095441473567, -0.10471928864299906, -0.14568768777358143, 0.3544885248269724, 0.17235908398161764, 0.228561931281634, 0.0028930526064789813, 0.2744445869192967, 0.16745083520755819, 0.16486398169527883, 0.04158096541043209, 0.30471389133726123, 0.07791359694067226, 0.08906514695643084, -0.3076604794447675, 0.013022922048264223, 0.10349586250503426] |
710.2493 | Indirect dark matter searches with H.E.S.S | The annihilations of WIMPs produce high energy gamma-rays in the final state.
These high energy gamma-rays may be detected by IACTs such as the H.E.S.S.
array of Imaging Atmospheric Cherenkov telescopes. Besides the popular targets
such as the Galactic Center or galaxy clusters such as VIRGO, dwarf spheroidal
galaxies are privileged targets for Dark Matter annihilation signal searches.
H.E.S.S. observations on the Sagittarius dwarf galaxy are presented. The
modelling of the Dark Matter halo profile of Sagittarius dwarf is discussed.
Constraints on the velocity-weighted cross section of Dark Matter particles are
derived in the framework of Supersymmetric and Kaluza-Klein models. The future
of H.E.S.S. will be briefly discussed.
| astro-ph | the annihilations of wimps produce high energy gammarays in the final state these high energy gammarays may be detected by iacts such as the hess array of imaging atmospheric cherenkov telescopes besides the popular targets such as the galactic center or galaxy clusters such as virgo dwarf spheroidal galaxies are privileged targets for dark matter annihilation signal searches hess observations on the sagittarius dwarf galaxy are presented the modelling of the dark matter halo profile of sagittarius dwarf is discussed constraints on the velocityweighted cross section of dark matter particles are derived in the framework of supersymmetric and kaluzaklein models the future of hess will be briefly discussed | [['the', 'annihilations', 'of', 'wimps', 'produce', 'high', 'energy', 'gammarays', 'in', 'the', 'final', 'state', 'these', 'high', 'energy', 'gammarays', 'may', 'be', 'detected', 'by', 'iacts', 'such', 'as', 'the', 'hess', 'array', 'of', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'besides', 'the', 'popular', 'targets', 'such', 'as', 'the', 'galactic', 'center', 'or', 'galaxy', 'clusters', 'such', 'as', 'virgo', 'dwarf', 'spheroidal', 'galaxies', 'are', 'privileged', 'targets', 'for', 'dark', 'matter', 'annihilation', 'signal', 'searches', 'hess', 'observations', 'on', 'the', 'sagittarius', 'dwarf', 'galaxy', 'are', 'presented', 'the', 'modelling', 'of', 'the', 'dark', 'matter', 'halo', 'profile', 'of', 'sagittarius', 'dwarf', 'is', 'discussed', 'constraints', 'on', 'the', 'velocityweighted', 'cross', 'section', 'of', 'dark', 'matter', 'particles', 'are', 'derived', 'in', 'the', 'framework', 'of', 'supersymmetric', 'and', 'kaluzaklein', 'models', 'the', 'future', 'of', 'hess', 'will', 'be', 'briefly', 'discussed']] | [-0.06665892750067913, 0.16479490671082642, -0.07998216301806409, 0.21528872735992385, -0.16537370427330542, -0.05769582838682389, -0.08313456760650431, 0.3807608951341266, -0.13489192176213557, -0.41815679039616416, -0.009404040538895599, -0.35419933647952145, 0.026427049730921647, 0.22249575256730034, 0.043010336063970395, 0.019332137940822308, 0.13413540158567397, -0.05459675580884019, 0.025014480620113858, -0.2893774684139148, 0.2549653982838478, 0.1567622225222833, 0.11479828334241002, -0.008997927443555521, 0.08868148640074112, -0.050093651507739666, -0.1023443775354988, -0.12744831944022467, -0.12268859845412576, -0.007090933287313588, 0.3127591871602649, 0.1705909512626628, 0.07099114786790407, -0.3997526426316687, -0.24737285970089337, 0.16316000642082482, 0.21981319810557007, -0.011183973151707539, -0.14252602188045987, -0.44852587263341304, 0.03470378013109978, -0.24840382708202083, -0.1929192504785196, 0.09216405215017774, -0.03031451963060708, 0.09021174238942978, -0.1294947769837799, 0.10272820567910525, -0.025723371717268257, -0.032853818782044714, -0.14247140096806646, -0.18702456931781922, -0.04403700731711945, -0.04301132916050308, 0.07729719562619855, -0.005013311018787876, 0.2712927426651327, -0.21740140808591, -0.05247020132783628, 0.43151460864788127, -0.07657325732159531, -0.025697437166753743, 0.2089802639589093, -0.16116346742233467, -0.22424631528944397, 0.11365833297302877, 0.1885351566252885, 0.0597545598370575, -0.19078916650161976, 0.12257352870559164, -0.0358815846266225, 0.1413120083183188, 0.06099150485048691, 0.0741718554790067, 0.4036125880234909, 0.19026353674147417, 0.13991666398080135, 0.020837523368687404, -0.31155003836223233, 0.018137261763008103, -0.31694124895579145, -0.11972982876209749, -0.1679068535687057, 0.036170753883197904, -0.0868181582556173, -0.06865077823641952, 0.33019597362726927, 0.03839262509912563, 0.1952789088504182, -0.03940582797534902, 0.3714119189211892, 0.0511854845584215, 0.05713493652486553, 0.031762631545360714, 0.3969471586557726, 0.15657213152843286, 0.08820959813979075, -0.18181600508763007, -0.006344473049803464, -0.04034393898608094] |
710.2494 | Soft diffraction at the LHC: a partonic interpretation | We present a `new generation' model for high energy proton-proton `soft'
interactions. It allows for a full set of multi-Pomeron vertices, as well as
including multichannel eikonal scattering. It describes the behaviour of the
proton-proton total, sigma(total), and elastic dsigma(el)/dt, cross sections
together with those for low and high mass proton dissociation. Although the
model contains a comprehensive set of multi-Pomeron diagrams, it has a simple
partonic interpretation. Including the more complicated multi-Pomeron vertices
reduces the absorptive effects as compared to the predictions in which only the
triple-Pomeron vertex is considered. Tuning the model to describe the available
`soft' data in the CERN ISR - Tevatron energy range, we predict the total,
elastic, single- and double-diffractive dissociation cross sections at the LHC
energy. An inescapable consequence of including multichannel eikonal and
multi-Pomeron effects is that the total cross section is expected to be lower
than before: indeed, we find sigma(total) \simeq 90 mb at the LHC energy. We
also present differential forms of the cross sections. In addition we calculate
soft diffractive central production.
| hep-ph | we present a new generation model for high energy protonproton soft interactions it allows for a full set of multipomeron vertices as well as including multichannel eikonal scattering it describes the behaviour of the protonproton total sigmatotal and elastic dsigmaeldt cross sections together with those for low and high mass proton dissociation although the model contains a comprehensive set of multipomeron diagrams it has a simple partonic interpretation including the more complicated multipomeron vertices reduces the absorptive effects as compared to the predictions in which only the triplepomeron vertex is considered tuning the model to describe the available soft data in the cern isr tevatron energy range we predict the total elastic single and doublediffractive dissociation cross sections at the lhc energy an inescapable consequence of including multichannel eikonal and multipomeron effects is that the total cross section is expected to be lower than before indeed we find sigmatotal simeq 90 mb at the lhc energy we also present differential forms of the cross sections in addition we calculate soft diffractive central production | [['we', 'present', 'a', 'new', 'generation', 'model', 'for', 'high', 'energy', 'protonproton', 'soft', 'interactions', 'it', 'allows', 'for', 'a', 'full', 'set', 'of', 'multipomeron', 'vertices', 'as', 'well', 'as', 'including', 'multichannel', 'eikonal', 'scattering', 'it', 'describes', 'the', 'behaviour', 'of', 'the', 'protonproton', 'total', 'sigmatotal', 'and', 'elastic', 'dsigmaeldt', 'cross', 'sections', 'together', 'with', 'those', 'for', 'low', 'and', 'high', 'mass', 'proton', 'dissociation', 'although', 'the', 'model', 'contains', 'a', 'comprehensive', 'set', 'of', 'multipomeron', 'diagrams', 'it', 'has', 'a', 'simple', 'partonic', 'interpretation', 'including', 'the', 'more', 'complicated', 'multipomeron', 'vertices', 'reduces', 'the', 'absorptive', 'effects', 'as', 'compared', 'to', 'the', 'predictions', 'in', 'which', 'only', 'the', 'triplepomeron', 'vertex', 'is', 'considered', 'tuning', 'the', 'model', 'to', 'describe', 'the', 'available', 'soft', 'data', 'in', 'the', 'cern', 'isr', 'tevatron', 'energy', 'range', 'we', 'predict', 'the', 'total', 'elastic', 'single', 'and', 'doublediffractive', 'dissociation', 'cross', 'sections', 'at', 'the', 'lhc', 'energy', 'an', 'inescapable', 'consequence', 'of', 'including', 'multichannel', 'eikonal', 'and', 'multipomeron', 'effects', 'is', 'that', 'the', 'total', 'cross', 'section', 'is', 'expected', 'to', 'be', 'lower', 'than', 'before', 'indeed', 'we', 'find', 'sigmatotal', 'simeq', '90', 'mb', 'at', 'the', 'lhc', 'energy', 'we', 'also', 'present', 'differential', 'forms', 'of', 'the', 'cross', 'sections', 'in', 'addition', 'we', 'calculate', 'soft', 'diffractive', 'central', 'production']] | [-0.05760559791575789, 0.146472470675037, -0.07361623198786915, 0.15892099059830583, -0.05256976938176462, -0.0774656839624239, 0.00781446641365833, 0.34444649105562886, -0.2070183131035746, -0.3186589520315037, -0.023791528166518274, -0.36595182352680505, -0.03585415176828118, 0.15427905570250006, 0.05168142005910768, 0.07515610332381638, 0.10212980195989503, 0.04147550994804239, -0.0020233320962528096, -0.18917940187418614, 0.2968612309819197, 0.1016078672837466, 0.23510878088281434, 0.19531845580512547, 0.1039753065964974, 0.14394229754038593, -0.03085902122719049, -0.028163748355034518, -0.12917214758811443, 0.0720483920427368, 0.26877782597370886, 0.04717334631063482, 0.11589244876111693, -0.40116596196723336, -0.12841626778244972, 0.10585013351622312, 0.1228047734071665, 0.10824686920968815, -0.00823342101143413, -0.19468815847957396, 0.08676548687850728, -0.2524558621294358, -0.12085763784399366, -0.06749084401903126, 0.03173215255579528, -0.023248679042958163, -0.28361641097375573, 0.06902325557226398, -0.041502704577493096, 0.0036788541864713324, -0.05800177674528266, -0.18080285543863497, -0.09304368988857331, 0.03802222275339505, 0.036490050796419385, 0.03747161179164644, 0.1510813473008217, -0.19094985563920894, -0.13168448420542786, 0.3857412503915839, -0.023782852658169918, -0.12890912124558407, 0.1726273663882988, -0.16016703150509035, -0.11944622938411639, 0.2146420995485695, 0.23491924231159775, 0.0863443878657349, -0.21291915198568911, 0.0931960801486104, 0.012757620099000633, 0.15728064132169547, 0.08221785213442191, 0.04656981904169216, 0.13491387829622803, 0.24446921364048166, -0.006501879942302099, 0.11036805328022799, -0.13335491665912902, -0.08755168771535596, -0.42375451785457485, -0.09370443609077483, -0.07102228084661286, 0.03294985286672326, -0.06930752916788847, -0.1319044680635938, 0.33567700509310644, 0.08194286712609669, 0.2962860259561293, 0.02930007550988675, 0.34168212126721353, 0.15753720080812106, 0.10334754707565641, 0.0534518008120358, 0.30866083679720757, 0.12226299757740515, 0.13731122436275817, -0.19089837062638254, 0.04633595295223024, 0.03871074998477364] |
710.2495 | A Continuity Theorem for Stinespring's Dilation | We show a continuity theorem for Stinespring's dilation: two completely
positive maps between arbitrary C*-algebras are close in cb-norm iff we can
find corresponding dilations that are close in operator norm. The proof
establishes the equivalence of the cb-norm distance and the Bures distance for
completely positive maps. We briefly discuss applications to quantum
information theory.
| quant-ph math-ph math.MP math.OA | we show a continuity theorem for stinesprings dilation two completely positive maps between arbitrary calgebras are close in cbnorm iff we can find corresponding dilations that are close in operator norm the proof establishes the equivalence of the cbnorm distance and the bures distance for completely positive maps we briefly discuss applications to quantum information theory | [['we', 'show', 'a', 'continuity', 'theorem', 'for', 'stinesprings', 'dilation', 'two', 'completely', 'positive', 'maps', 'between', 'arbitrary', 'calgebras', 'are', 'close', 'in', 'cbnorm', 'iff', 'we', 'can', 'find', 'corresponding', 'dilations', 'that', 'are', 'close', 'in', 'operator', 'norm', 'the', 'proof', 'establishes', 'the', 'equivalence', 'of', 'the', 'cbnorm', 'distance', 'and', 'the', 'bures', 'distance', 'for', 'completely', 'positive', 'maps', 'we', 'briefly', 'discuss', 'applications', 'to', 'quantum', 'information', 'theory']] | [-0.14383421609610586, 0.1432487334220371, -0.08919011595727559, 0.14230461352105653, -0.011589258310518094, -0.17832465470668726, -0.00749745148225754, 0.4025078574528119, -0.3593245953587549, -0.16778987276068488, 0.10719276620823491, -0.3321969036977472, -0.17340826545010454, 0.17702889031664068, -0.13423881954180875, 0.03608202884372856, 0.04165389068657532, 0.0890886210503855, -0.2050676172657404, -0.17819493021566554, 0.40077301434939727, -0.03337771167155422, 0.2103726797836966, 0.14897352756400192, 0.12845464339313498, -0.00769038950758321, -0.04285316485246377, -0.007552039352179106, -0.1761682711789295, 0.11213474141966019, 0.2601901265193841, 0.14620904436534538, 0.2417499238342446, -0.33436448093769805, -0.10142456467396446, 0.18894454508387884, 0.05753910624688225, 0.0671875465195626, -0.034155815856398215, -0.31770577867116245, 0.07628889393527061, -0.11412177344651095, -0.12521294512719447, -0.10163474959179959, 0.07735212423306491, 0.0020112887473909984, -0.2686176185296582, 0.07966469108526196, 0.1264372883098466, 0.06329007861495484, -0.10232396765786689, -0.05641860034250255, 0.01377295478180583, 0.14645273423853464, -0.03518861974589527, 0.03184284180211502, 0.09734118013875559, 0.007414003127321068, -0.13680204223575337, 0.28338156334523645, -0.06245175060134248, -0.23164766411563115, 0.15940473461523652, -0.17337548383511603, -0.1316327631772895, 0.0008003283790977937, 0.08529533492401242, 0.08900690926904124, -0.0861964528282572, 0.1560561409642105, -0.07092600974803125, 0.11947154865733214, 0.12339977893446173, 0.09154343998358984, 0.16689260850294627, -0.0032629160809197594, 0.17057660291071183, 0.18750867846288852, 0.03481785593300758, -0.11478273904815849, -0.3744124343086566, -0.18175612525997817, -0.1803585468192718, 0.10560844807020787, -0.14097062420972048, -0.15003312093072704, 0.2972463707285767, 0.1315459916368127, 0.1991485795920848, 0.17256446766467498, 0.22639954010290758, 0.08711620863843043, 0.014602798877084362, 0.10542474239732005, 0.24727591885519878, 0.2540508453800742, 0.004264808758827192, -0.1309224420609618, 0.006213487001202468, 0.21523094373489066] |
710.2496 | Regression estimation from an individual stable sequence | We consider univariate regression estimation from an individual (non-random)
sequence $(x_1,y_1),(x_2,y_2), ... \in \real \times \real$, which is stable in
the sense that for each interval $A \subseteq \real$, (i) the limiting relative
frequency of $A$ under $x_1, x_2, ...$ is governed by an unknown probability
distribution $\mu$, and (ii) the limiting average of those $y_i$ with $x_i \in
A$ is governed by an unknown regression function $m(\cdot)$.
A computationally simple scheme for estimating $m(\cdot)$ is exhibited, and
is shown to be $L_2$ consistent for stable sequences $\{(x_i,y_i)\}$ such that
$\{y_i\}$ is bounded and there is a known upper bound for the variation of
$m(\cdot)$ on intervals of the form $(-i,i]$, $i \geq 1$. Complementing this
positive result, it is shown that there is no consistent estimation scheme for
the family of stable sequences whose regression functions have finite
variation, even under the restriction that $x_i \in [0,1]$ and $y_i$ is
binary-valued.
| math.PR cs.IT math.IT math.ST stat.TH | we consider univariate regression estimation from an individual nonrandom sequence x_1y_1x_2y_2 in real times real which is stable in the sense that for each interval a subseteq real i the limiting relative frequency of a under x_1 x_2 is governed by an unknown probability distribution mu and ii the limiting average of those y_i with x_i in a is governed by an unknown regression function mcdot a computationally simple scheme for estimating mcdot is exhibited and is shown to be l_2 consistent for stable sequences x_iy_i such that y_i is bounded and there is a known upper bound for the variation of mcdot on intervals of the form ii i geq 1 complementing this positive result it is shown that there is no consistent estimation scheme for the family of stable sequences whose regression functions have finite variation even under the restriction that x_i in 01 and y_i is binaryvalued | [['we', 'consider', 'univariate', 'regression', 'estimation', 'from', 'an', 'individual', 'nonrandom', 'sequence', 'x_1y_1x_2y_2', 'in', 'real', 'times', 'real', 'which', 'is', 'stable', 'in', 'the', 'sense', 'that', 'for', 'each', 'interval', 'a', 'subseteq', 'real', 'i', 'the', 'limiting', 'relative', 'frequency', 'of', 'a', 'under', 'x_1', 'x_2', 'is', 'governed', 'by', 'an', 'unknown', 'probability', 'distribution', 'mu', 'and', 'ii', 'the', 'limiting', 'average', 'of', 'those', 'y_i', 'with', 'x_i', 'in', 'a', 'is', 'governed', 'by', 'an', 'unknown', 'regression', 'function', 'mcdot', 'a', 'computationally', 'simple', 'scheme', 'for', 'estimating', 'mcdot', 'is', 'exhibited', 'and', 'is', 'shown', 'to', 'be', 'l_2', 'consistent', 'for', 'stable', 'sequences', 'x_iy_i', 'such', 'that', 'y_i', 'is', 'bounded', 'and', 'there', 'is', 'a', 'known', 'upper', 'bound', 'for', 'the', 'variation', 'of', 'mcdot', 'on', 'intervals', 'of', 'the', 'form', 'ii', 'i', 'geq', '1', 'complementing', 'this', 'positive', 'result', 'it', 'is', 'shown', 'that', 'there', 'is', 'no', 'consistent', 'estimation', 'scheme', 'for', 'the', 'family', 'of', 'stable', 'sequences', 'whose', 'regression', 'functions', 'have', 'finite', 'variation', 'even', 'under', 'the', 'restriction', 'that', 'x_i', 'in', '01', 'and', 'y_i', 'is', 'binaryvalued']] | [-0.12975327960440527, 0.11771315524318246, -0.04007971300837278, 0.04757848215342543, 0.0019215146789089744, -0.19685550557524467, 0.034596822460513287, 0.41652913577229583, -0.28141499623256244, -0.18951099944119684, 0.11230767355144224, -0.28240625467776453, -0.14654491813978393, 0.19634179852827882, -0.12092478698644563, 0.051713964077581547, 0.007785969743530122, 0.09293723966451299, -0.04117103002734182, -0.2585347019801629, 0.30639771806801225, -0.042022082671810616, 0.20605095247769314, -0.05731163217745496, 0.1576540636073723, 0.018605029632356142, -0.013789179916149818, -0.010464416323042156, -0.13049011094430804, 0.07574938351113424, 0.22489416147363467, 0.1514244191004776, 0.30201925336064506, -0.30680899070607087, -0.15092823731919264, 0.20545050073430668, 0.15526622462073877, -0.012958088137315674, -0.011815424937436095, -0.23750603244321158, 0.1440364574801002, -0.11118402640138371, -0.09773691106062607, -0.02142573278647341, 0.11348046021748509, 0.04405394864062335, -0.4190169917294543, 0.09046605305633688, 0.09660982394977918, 0.0668765295985633, -0.038013906377498935, -0.17543506015079632, -0.0014391565826665236, 0.08509890842032712, 0.05143918838248832, 0.09361139659210414, 0.048916133534750786, -0.07355030935301426, -0.059387918162447144, 0.3417864476354799, -0.07766603563455927, -0.2709531133131893, 0.11338633021352275, -0.14541559567950016, -0.14547239086784472, 0.14343631883845634, 0.10055329828447312, 0.15359536934903378, -0.10971133151144764, 0.13567361853322976, -0.09787587823983807, 0.17936113795215552, 0.06327105546682674, -0.005328051049743572, 0.1584827843787861, 0.12878631094420617, 0.1297819141842325, 0.06203696595726772, -0.06607776922923857, -0.061042195645429745, -0.33946626910302263, -0.10939128031124418, -0.2527838233333306, 0.08489924841154142, -0.13583472039942762, -0.1807629264271568, 0.3172307367775579, 0.09699002471471192, 0.252520396849203, 0.12027202815445602, 0.23237001264327004, 0.1804757802247151, -0.020408744451858654, 0.1023769562832711, 0.12219516748574956, 0.10928191618225068, -0.02635849490699252, -0.1610825746734283, 0.16360248809980366, 0.022210089308846485] |
710.2497 | A Categorical Construction of Ultrafilters | Ultrafilters are useful mathematical objects having applications in
nonstandard analysis, Ramsey theory, Boolean algebra, topology, and other areas
of mathematics. In this note, we provide a categorical construction of
ultrafilters in terms of the inverse limit of an inverse family of finite
partitions; this is an elementary and intuitive presentation of a consequence
of the profiniteness of Stone spaces. We then apply this construction to answer
a question of Rosinger posed in arXiv:0709.0084v2 in the negative.
| math.CT math.GM math.GN | ultrafilters are useful mathematical objects having applications in nonstandard analysis ramsey theory boolean algebra topology and other areas of mathematics in this note we provide a categorical construction of ultrafilters in terms of the inverse limit of an inverse family of finite partitions this is an elementary and intuitive presentation of a consequence of the profiniteness of stone spaces we then apply this construction to answer a question of rosinger posed in arxiv07090084v2 in the negative | [['ultrafilters', 'are', 'useful', 'mathematical', 'objects', 'having', 'applications', 'in', 'nonstandard', 'analysis', 'ramsey', 'theory', 'boolean', 'algebra', 'topology', 'and', 'other', 'areas', 'of', 'mathematics', 'in', 'this', 'note', 'we', 'provide', 'a', 'categorical', 'construction', 'of', 'ultrafilters', 'in', 'terms', 'of', 'the', 'inverse', 'limit', 'of', 'an', 'inverse', 'family', 'of', 'finite', 'partitions', 'this', 'is', 'an', 'elementary', 'and', 'intuitive', 'presentation', 'of', 'a', 'consequence', 'of', 'the', 'profiniteness', 'of', 'stone', 'spaces', 'we', 'then', 'apply', 'this', 'construction', 'to', 'answer', 'a', 'question', 'of', 'rosinger', 'posed', 'in', 'arxiv07090084v2', 'in', 'the', 'negative']] | [-0.07995274664859313, 0.10370653967500501, -0.11087276693433523, 0.14021937802396212, -0.133729681901231, -0.06349082467951686, 0.054063421968257405, 0.3155796232230559, -0.3287751336355467, -0.2442292440116305, 0.11145836921452822, -0.23802674616072672, -0.17012796722229798, 0.19806580952796582, -0.1918164628016687, -0.01838538549664254, 0.027617111836711096, 0.040534806082645, -0.0537559596972691, -0.24672138183755246, 0.3588722570692315, 0.0015200705053536473, 0.22059676701492453, 0.07185800749229619, 0.09834389292911903, 0.02417222611178216, -0.07217791925398381, 0.0419200099375401, -0.16783133044255255, 0.19275333990682722, 0.3629931019669449, 0.1670391933923285, 0.2795918702298926, -0.3879276676908941, -0.12030770374081298, 0.12509287816371667, 0.12396997169314607, 0.09046620188431966, -0.04312418184771731, -0.2632659726046227, 0.051193317801163006, -0.1851549255472885, -0.1300029883010162, -0.07516722537174418, 0.08875192944715554, 0.00030993957173179934, -0.23314471119964444, -0.01612504873726819, 0.19196401398575463, 0.16398528699033163, -0.04451244036239144, -0.09288776376460856, 0.06926083435128266, 0.09665477611879641, 0.01626519388818869, -0.01467590349273303, 0.04834783181699144, -0.11037083607280275, -0.189686997925762, 0.3461481760707495, 0.011608310220007962, -0.21109222779302178, 0.17700031380848708, -0.13133138788209572, -0.19198812911211438, 0.05026735297429401, 0.12314166287841224, 0.1343992373880905, -0.08123100457738179, 0.19876897647014088, -0.1369166829421915, 0.10908159667097435, 0.12077273595197177, 0.06754649975462942, 0.162952338521545, 0.19186805593277756, 0.09518249687814229, 0.17741253540451588, 0.07336201167640251, -0.047588648654463876, -0.3552227704408201, -0.195275123873757, -0.14263066635592966, 0.10409558321682837, -0.07865574148859564, -0.26116787374170647, 0.3962177624422553, 0.14711345893934974, 0.15752475426809207, 0.05719420230771239, 0.2046887116204645, 0.08885649248101823, -0.004049400282973373, -0.04209814576834843, 0.11548267285389877, 0.23098896642693797, 0.0546730222130144, -0.10141534199371834, -0.014077095824570672, 0.17306687117780786] |
710.2498 | Scaling and low energy constants in lattice QCD with N_f=2 maximally
twisted Wilson quarks | We report on the scaling of basic hadronic observables in lattice QCD with
N_f=2 maximally twisted Wilson dynamical quarks. We give preliminary results
for some of the Gasser-Leutwyler low energy constants, the chiral condensate
and the average mass of u and d quarks.
| hep-lat | we report on the scaling of basic hadronic observables in lattice qcd with n_f2 maximally twisted wilson dynamical quarks we give preliminary results for some of the gasserleutwyler low energy constants the chiral condensate and the average mass of u and d quarks | [['we', 'report', 'on', 'the', 'scaling', 'of', 'basic', 'hadronic', 'observables', 'in', 'lattice', 'qcd', 'with', 'n_f2', 'maximally', 'twisted', 'wilson', 'dynamical', 'quarks', 'we', 'give', 'preliminary', 'results', 'for', 'some', 'of', 'the', 'gasserleutwyler', 'low', 'energy', 'constants', 'the', 'chiral', 'condensate', 'and', 'the', 'average', 'mass', 'of', 'u', 'and', 'd', 'quarks']] | [-0.15380200955930146, 0.3510634074485752, -0.08723726250274583, 0.060412697667299314, -0.0018196989468103925, -0.08687201150162362, 0.10812229637143224, 0.37993480698313825, -0.11388571809998951, -0.20115865754006906, 0.024049766218224758, -0.3013726741422054, -0.014708866062032621, 0.07452592446447112, 0.05264273168908995, 0.16903601277099792, 0.0865658262614594, 0.03871493717265684, -0.14749307674897272, -0.25854022378578434, 0.3610854291811932, -0.04202481239037805, 0.17950429923312608, 0.24280358374465344, 0.039540538293591075, 0.012701096949925604, -0.05514632843348176, -0.10517953104491151, -0.18101487681269646, 0.06927630322617154, 0.0950733170449344, -0.023362758748103365, 0.04738154929391174, -0.3764042897463971, -0.1114652885535602, 0.05491140185920305, 0.1169338847813738, 0.11475419500222711, -0.014764853939955492, -0.25520721343237646, 0.07317417476672766, -0.1923895987010626, -0.20633681391387484, -0.17196103308869656, -0.009245669739970635, -0.0019014505886061246, -0.3299109775486381, 0.12703458503495121, -0.07219490339657357, 0.08309911306254393, -0.04779812445604177, -0.27253900892859284, -0.052389668603969174, 0.06019839391837893, 0.10591948300946591, 0.10587448670073997, 0.11571825787338406, -0.22793431276845377, -0.15444849067649177, 0.4581353478783438, -0.08477535831666183, -0.15687282125703816, 0.13001595211735126, -0.22258929216281273, -0.19091380490964754, 0.03806513829240007, 0.1884335583985545, 0.09298958140966851, -0.12424438962236393, 0.1112609287151298, -0.12189879532643529, 0.16461742560779893, 0.056343703660680804, 0.1037188702652794, 0.21709284597877845, 0.15367664691320684, -0.03184785330018332, 0.08830841180738495, 0.0022086765086494907, -0.11311838645921198, -0.3947308346802412, -0.0807376962458325, -0.1184380609368862, 0.12604023806404235, -0.19454505540319544, -0.15615344623666863, 0.4054034084384871, 0.11033516390205816, 0.23649687774825928, 0.038521095027410704, 0.2327119633122239, 0.09105507009337808, 0.02596953971484719, 0.09530840428589388, 0.27313834646795226, 0.20990105081609514, 0.15920863172775784, -0.3502061934491923, -0.17270064844511623, 0.1976890072962919] |
710.2499 | Dynamical instability of the XY spiral state of ferromagnetic
condensates | We calculate the spectrum of collective excitations of the XY spiral state
prepared adiabatically or suddenly from a uniform ferromagnetic F=1 condensate.
For spiral wavevectors past a critical value, spin wave excitation energies
become imaginary indicating a dynamical instability. We construct phase
diagrams as functions of spiral wavevector and quadratic Zeeman energy.
| cond-mat.other | we calculate the spectrum of collective excitations of the xy spiral state prepared adiabatically or suddenly from a uniform ferromagnetic f1 condensate for spiral wavevectors past a critical value spin wave excitation energies become imaginary indicating a dynamical instability we construct phase diagrams as functions of spiral wavevector and quadratic zeeman energy | [['we', 'calculate', 'the', 'spectrum', 'of', 'collective', 'excitations', 'of', 'the', 'xy', 'spiral', 'state', 'prepared', 'adiabatically', 'or', 'suddenly', 'from', 'a', 'uniform', 'ferromagnetic', 'f1', 'condensate', 'for', 'spiral', 'wavevectors', 'past', 'a', 'critical', 'value', 'spin', 'wave', 'excitation', 'energies', 'become', 'imaginary', 'indicating', 'a', 'dynamical', 'instability', 'we', 'construct', 'phase', 'diagrams', 'as', 'functions', 'of', 'spiral', 'wavevector', 'and', 'quadratic', 'zeeman', 'energy']] | [-0.2730170988764327, 0.28326612392153877, -0.10975053581373337, 0.07820984830435079, -0.06920447883861086, -0.1072972053326129, 0.04434340366592201, 0.3795935007242056, -0.23236555465532896, -0.1959883845814217, -0.03048979782929214, -0.28873940729177916, -0.05164392719206472, 0.14046472871156696, 0.2043239968793037, 0.008026961147641907, -0.03460622247075662, -0.008569025112172732, -0.12957342174978784, -0.14908414144212237, 0.31812165319346464, -0.07069450120728177, 0.2593143722937944, -0.027976290242244992, 0.05001836065023851, 0.033525824193090484, 0.1740265279345644, -0.05073848158085289, -0.20229678821320143, -0.05980427484386242, 0.26296564933055866, -0.08896009624004364, 0.2169603305824589, -0.40773120436530846, -0.17319561888535434, 0.0949987569071639, 0.22517497439940387, 0.20412660837889865, 0.012817290459329693, -0.30693588172121405, -0.07348970495751508, -0.181839793846638, -0.24907461030838582, -0.1023306877659007, 0.02258804930450144, 0.03262406854460446, -0.2626635419169011, 0.1562868386077193, 0.061059972801348734, 0.14056154259910378, -0.13728867054809457, -0.1204418936618962, -0.13126092752925336, 0.001015959437399243, 0.044712373411479905, 0.16143681064176446, 0.19601438708531743, -0.16145550932000893, -0.10843108343676879, 0.3052292491058604, -0.07701087254771175, -0.06602613531196347, 0.11771868170203212, -0.20661673146801499, -0.018882648090276725, 0.21289717914679876, 0.1442649728638711, 0.04664764678678834, -0.052989673567935824, 0.042586907062706396, 0.04536379927510727, 0.19864339790253255, 0.09991194415264405, 0.07049536509797551, 0.33185971430458056, 0.09916235470714477, 0.044430396949442535, 0.21895972803199235, -0.08118961544599958, -0.13063957129354373, -0.20163858903106302, -0.0955925804312126, -0.2238716968926243, 0.08496588229760303, -0.031404705347575564, -0.23391631381729475, 0.4701295012178329, 0.07689494589486948, 0.20623401509622524, -0.0253312389473789, 0.26967178207213205, 0.15387510438225804, 0.032353617277784415, 0.10749551437150401, 0.2707507638977124, 0.17178588783225188, 0.0819819073479336, -0.29695675641638586, -0.039640664897608355, 0.04093247066395214] |
710.25 | Density estimation from an individual numerical sequence | This paper considers estimation of a univariate density from an individual
numerical sequence. It is assumed that (i) the limiting relative frequencies of
the numerical sequence are governed by an unknown density, and (ii) there is a
known upper bound for the variation of the density on an increasing sequence of
intervals. A simple estimation scheme is proposed, and is shown to be $L_1$
consistent when (i) and (ii) apply. In addition it is shown that there is no
consistent estimation scheme for the set of individual sequences satisfying
only condition (i).
| math.PR cs.IT math.IT math.ST stat.TH | this paper considers estimation of a univariate density from an individual numerical sequence it is assumed that i the limiting relative frequencies of the numerical sequence are governed by an unknown density and ii there is a known upper bound for the variation of the density on an increasing sequence of intervals a simple estimation scheme is proposed and is shown to be l_1 consistent when i and ii apply in addition it is shown that there is no consistent estimation scheme for the set of individual sequences satisfying only condition i | [['this', 'paper', 'considers', 'estimation', 'of', 'a', 'univariate', 'density', 'from', 'an', 'individual', 'numerical', 'sequence', 'it', 'is', 'assumed', 'that', 'i', 'the', 'limiting', 'relative', 'frequencies', 'of', 'the', 'numerical', 'sequence', 'are', 'governed', 'by', 'an', 'unknown', 'density', 'and', 'ii', 'there', 'is', 'a', 'known', 'upper', 'bound', 'for', 'the', 'variation', 'of', 'the', 'density', 'on', 'an', 'increasing', 'sequence', 'of', 'intervals', 'a', 'simple', 'estimation', 'scheme', 'is', 'proposed', 'and', 'is', 'shown', 'to', 'be', 'l_1', 'consistent', 'when', 'i', 'and', 'ii', 'apply', 'in', 'addition', 'it', 'is', 'shown', 'that', 'there', 'is', 'no', 'consistent', 'estimation', 'scheme', 'for', 'the', 'set', 'of', 'individual', 'sequences', 'satisfying', 'only', 'condition', 'i']] | [-0.11371828811799946, 0.08726233602219904, -0.06372432049829513, 0.049599876219872385, 0.00015493780981911266, -0.14235703064047772, 0.02838810800028074, 0.40582214742291556, -0.24452237047902917, -0.2666342275308283, 0.12956208684962525, -0.2464059390552828, -0.16080966198047542, 0.20483853738329819, -0.11943953217047712, 0.026553968955894285, 0.04804791438737479, 0.08903138110738086, -0.04554228412250624, -0.22940023280123412, 0.32083658887194877, 0.029368466153518177, 0.27036547402689315, -0.00028467776618250036, 0.12165317278476837, -0.023715201491975913, -0.06868627070672, 0.03472429060417673, -0.13744719709227313, 0.10981199632742969, 0.19590180422908263, 0.16457198171005788, 0.29824165254831314, -0.3425318256182515, -0.183157093529387, 0.1314891600062686, 0.1704086941494809, 0.08772199495655039, -0.05157255824356664, -0.2242184436434637, 0.12746350121502156, -0.14754807348894564, -0.074716653543241, -0.02196124975529054, 0.07009828034484678, 0.03740651014706363, -0.3726387171216471, 0.07919887504945307, 0.0747698574437179, 0.037979373715643305, -0.0689497442116313, -0.1213572312389379, -0.0038708669719357126, 0.10144549899680146, 0.06872322294435909, 0.05225174604287452, 0.047190420511786055, -0.08800086855594798, -0.03359961384178504, 0.3403924928482055, -0.052766949500200215, -0.22438703071447494, 0.1784690914361778, -0.10360268009421618, -0.1226553771968769, 0.15933063501269434, 0.08609432877805691, 0.1313503536891759, -0.13607845419297201, 0.08405990199421269, -0.07142437609676879, 0.20996750919553248, 0.02850912851990079, -0.00863334566035875, 0.17177507518183277, 0.15988668031818437, 0.14244454194862477, 0.07930665619990221, -0.09872539098242945, -0.06995874527416637, -0.35044266858502576, -0.13033773480603247, -0.2626808835800899, -0.0003027627143360998, -0.07592854668521044, -0.16139094692682746, 0.3531161545874372, 0.13985920837149024, 0.20749312732368708, 0.08386971273095063, 0.2863315752019053, 0.21489360038100605, 0.00010177212306703238, 0.09863460449623349, 0.19516719513289307, 0.13876410121472715, -0.01024549967184177, -0.20727526300596882, 0.12636869676593368, 0.026875379834445597] |
710.2501 | nuMSM and its experimental tests | $\nu$MSM is a minimal renormalizable extension of the Standard Model by right
handed neutrinos. This model explains the neutrino oscillations and provides a
candidate for the Dark Matter and a mechanism of baryon number generation in
the Early Universe. We discuss here existing constraints on the model and
possible consequences for astrophysical and laboratory experiments.
| hep-ph | numsm is a minimal renormalizable extension of the standard model by right handed neutrinos this model explains the neutrino oscillations and provides a candidate for the dark matter and a mechanism of baryon number generation in the early universe we discuss here existing constraints on the model and possible consequences for astrophysical and laboratory experiments | [['numsm', 'is', 'a', 'minimal', 'renormalizable', 'extension', 'of', 'the', 'standard', 'model', 'by', 'right', 'handed', 'neutrinos', 'this', 'model', 'explains', 'the', 'neutrino', 'oscillations', 'and', 'provides', 'a', 'candidate', 'for', 'the', 'dark', 'matter', 'and', 'a', 'mechanism', 'of', 'baryon', 'number', 'generation', 'in', 'the', 'early', 'universe', 'we', 'discuss', 'here', 'existing', 'constraints', 'on', 'the', 'model', 'and', 'possible', 'consequences', 'for', 'astrophysical', 'and', 'laboratory', 'experiments']] | [-0.10527661216699265, 0.20599984636699611, -0.03996186768636108, 0.20191158818250352, -0.13145187842574987, -0.1301664752462371, 0.06273597292602062, 0.2566543332978406, -0.21447282707826656, -0.32792731757191096, 0.055262512559155846, -0.27740634718740526, -0.07268662968311798, 0.18648534648713064, 0.04622213057750328, 0.0026941981759261, -0.008424276536838575, 0.028475110622292216, 0.016083593585062773, -0.23120782089165665, 0.27694310977716335, 0.11882753809067335, 0.22590572731569408, 0.0656388304788958, 0.15250379637899725, -0.08036352660168301, -0.07378066051116383, -0.09790736729787154, -0.11611316889677917, 0.05246989263898947, 0.1296004662967541, 0.17008689439601518, 0.15922546512447297, -0.45328422793271866, -0.2545341830361973, 0.2092285852032629, 0.12387799408964136, 0.12495875678617846, -0.16264904779170386, -0.281811382655393, 0.05894835565916517, -0.23417399486696178, -0.12911643438379872, -0.04511352494697679, -0.03560091916641051, -0.08966287204318425, -0.3161456659436226, 0.10565129352140833, -0.016150657824155958, -0.04705668419430202, -0.06809432235631076, -0.10521738060157407, 0.0304487849839709, -0.01702304326675155, 0.12135496407704936, -0.060588310328735545, 0.1150552219150334, -0.21026345322501253, -0.13881704573604195, 0.48225119642236014, -0.14209052377211098, -0.13958817715333266, 0.15101438814943488, -0.12254445579072291, -0.14555661805312742, 0.010944088400256905, 0.11154714677144181, 0.07157237157225609, -0.15490572676062583, 0.17634212926284157, -0.12117640872231938, 0.10657511008056728, 0.009092114861546593, 0.03242617462846366, 0.3589790961959145, 0.2842044527557763, 0.033777275605296544, 0.013100611198354851, -0.0845813666682013, -0.029633918464903465, -0.4176209486343644, -0.1408735986121676, -0.07954910087653182, -0.011564814403854226, -0.052627449464687906, -0.0897563215683807, 0.4932055558670651, 0.18521347780796615, 0.19003228685733947, 0.010289812934669582, 0.33786918415941974, 0.0010198848660696637, 0.024208652939308774, -0.006011464400216937, 0.28221953916786746, 0.11646871472793546, 0.10630581786178729, -0.22825446109372108, 0.015629918839443813, 0.06218055681304329] |
710.2502 | Search for rare b-meson decays at CDF | We report on the search for $B^0_s\to\mu^+\mu^-$, $B^0_d\to\mu^+\mu^-$ decays
and $b\to s \mu^+\mu^-$ transitions in exclusive decays of B mesons using the
CDF II detector at the Fermilab Tevatron Collider. Using 2 fb$^{-1}$ of Run II
data we find upper limits on the branching fractions
$\mathcal{B}(B^0_s\to\mu^+\mu^-)<5.8\times 10^{-8}$ and
$\mathcal{B}(B^0_d\to\mu^+\mu^-)<1.8\times 10^{-8}$ at 95% confidence level.
The results for the branching fractions of the $b\to s \mu^+\mu^-$ transitions
using 924 pb$^{-1}$ of Run II data are
$\mathcal{B}(B^+\to\mu^+\mu^-K^+)=(0.60\pm0.15\pm0.04)\times 10^{-6}$,
$\mathcal{B}(B^0_d\to\mu^+\mu^-K^{*0})=(0.82\pm0.31\pm0.10)\times 10^{-6}$ and
$\mathcal{B}(B^0_s\to \mu^+\mu^-\phi)/\mathcal{B}(B^0_s\to J/\psi\phi) <
2.61\times 10^{-3}$ at 95% confidence level.
| hep-ex | we report on the search for b0_stomumu b0_dtomumu decays and bto s mumu transitions in exclusive decays of b mesons using the cdf ii detector at the fermilab tevatron collider using 2 fb1 of run ii data we find upper limits on the branching fractions mathcalbb0_stomumu58times 108 and mathcalbb0_dtomumu18times 108 at 95 confidence level the results for the branching fractions of the bto s mumu transitions using 924 pb1 of run ii data are mathcalbbtomumuk060pm015pm004times 106 mathcalbb0_dtomumuk0082pm031pm010times 106 and mathcalbb0_sto mumuphimathcalbb0_sto jpsiphi 261times 103 at 95 confidence level | [['we', 'report', 'on', 'the', 'search', 'for', 'b0_stomumu', 'b0_dtomumu', 'decays', 'and', 'bto', 's', 'mumu', 'transitions', 'in', 'exclusive', 'decays', 'of', 'b', 'mesons', 'using', 'the', 'cdf', 'ii', 'detector', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'using', '2', 'fb1', 'of', 'run', 'ii', 'data', 'we', 'find', 'upper', 'limits', 'on', 'the', 'branching', 'fractions', 'mathcalbb0_stomumu58times', '108', 'and', 'mathcalbb0_dtomumu18times', '108', 'at', '95', 'confidence', 'level', 'the', 'results', 'for', 'the', 'branching', 'fractions', 'of', 'the', 'bto', 's', 'mumu', 'transitions', 'using', '924', 'pb1', 'of', 'run', 'ii', 'data', 'are', 'mathcalbbtomumuk060pm015pm004times', '106', 'mathcalbb0_dtomumuk0082pm031pm010times', '106', 'and', 'mathcalbb0_sto', 'mumuphimathcalbb0_sto', 'jpsiphi', '261times', '103', 'at', '95', 'confidence', 'level']] | [-0.04145929189312651, 0.22652922140112447, 0.01255668845763545, 0.0931884346552837, 0.006384714311103762, -0.12702801848911208, 0.22943001097056692, 0.23814634170475196, -0.06356044317147246, -0.30778688923628245, 0.013027420812171458, -0.44007383277754725, 0.1747490818163863, 0.14234929921588413, 0.15691545878157573, 0.13417088084589737, 0.1470149655389473, -0.051731501424248205, -0.05377445345813477, -0.2656267213830609, 0.10408756136894226, 0.026060344035490013, 0.231731749208713, 0.0900686269534039, 0.0023171586634154304, -0.08177020515453208, -0.062170683325808725, -0.1534232559763355, -0.19572756256057341, 0.004531410741217342, 0.26246113226358075, 0.22988907728030886, 0.07671655970913024, -0.34129108393127905, 0.11994636467554504, 0.1389434060058844, 0.14906625539915244, -0.021280443341827687, 0.0095008301899343, -0.43818524576447626, 0.17629270185429005, -0.19782259181877712, 0.030188917895250113, 0.018489506613049243, 0.10891708960457716, -0.15095690338883871, -0.39238077659665804, 0.14997113631739292, -0.13990127587300025, 0.13798284533765615, 0.017335806409885853, -0.31001189821629704, -0.04732138288126868, -0.1350077439421489, 0.010208187325869077, 0.08514949429081753, 0.2371011871361622, -0.09708430371994589, -0.24449454149070346, 0.3214523295331516, -0.12795525776613273, -0.1227622257695062, 0.1844923070827384, -0.29745552307684664, -0.2023293333771972, 0.2228240362012092, 0.3348505673010224, 0.011369350406536718, -0.2117435222859552, 0.1758679855179421, 0.03228482225609629, 0.17461619173165088, 0.10480263811409657, 0.07515374973508311, 0.17571127258333158, 0.23129659295542004, -0.04705736584915423, -0.0017022855758069106, -0.22272990949244964, 0.033679598585966926, -0.4583853546409281, -0.09627955588569612, -0.01668300750998803, 0.10311182587189072, -0.03978398990085101, 0.03047057467708249, 0.3209102737924291, 0.08845409676202654, 0.4034135268058306, 0.10701334343096357, 0.2523164442383949, 0.11664088779807459, -0.016186074569697756, 0.10301516818821885, 0.3506811198973913, 0.12376735106478502, 0.11560108366617818, -0.23281144671843468, 0.04410452745210977, -0.003283099208119107] |
710.2503 | On the mass formula and Wigner and curvature energy terms | The efficiency of different mass formulas derived from the liquid drop model
including or not the curvature energy, the Wigner term and different powers of
the relative neutron excess $I$ has been determined by a least square fitting
procedure to the experimental atomic masses assuming a constant
R$_{0,charge}$/A$^{1/3}$ ratio. The Wigner term and the curvature energy can be
used independently to improve the accuracy of the mass formula. The different
fits lead to a surface energy coefficient of around 17-18 MeV, a relative sharp
charge radius r$_0$ of 1.22-1.23 fm and a proton form-factor correction to the
Coulomb energy of around 0.9 MeV.
| nucl-ex | the efficiency of different mass formulas derived from the liquid drop model including or not the curvature energy the wigner term and different powers of the relative neutron excess i has been determined by a least square fitting procedure to the experimental atomic masses assuming a constant r_0chargea13 ratio the wigner term and the curvature energy can be used independently to improve the accuracy of the mass formula the different fits lead to a surface energy coefficient of around 1718 mev a relative sharp charge radius r_0 of 122123 fm and a proton formfactor correction to the coulomb energy of around 09 mev | [['the', 'efficiency', 'of', 'different', 'mass', 'formulas', 'derived', 'from', 'the', 'liquid', 'drop', 'model', 'including', 'or', 'not', 'the', 'curvature', 'energy', 'the', 'wigner', 'term', 'and', 'different', 'powers', 'of', 'the', 'relative', 'neutron', 'excess', 'i', 'has', 'been', 'determined', 'by', 'a', 'least', 'square', 'fitting', 'procedure', 'to', 'the', 'experimental', 'atomic', 'masses', 'assuming', 'a', 'constant', 'r_0chargea13', 'ratio', 'the', 'wigner', 'term', 'and', 'the', 'curvature', 'energy', 'can', 'be', 'used', 'independently', 'to', 'improve', 'the', 'accuracy', 'of', 'the', 'mass', 'formula', 'the', 'different', 'fits', 'lead', 'to', 'a', 'surface', 'energy', 'coefficient', 'of', 'around', '1718', 'mev', 'a', 'relative', 'sharp', 'charge', 'radius', 'r_0', 'of', '122123', 'fm', 'and', 'a', 'proton', 'formfactor', 'correction', 'to', 'the', 'coulomb', 'energy', 'of', 'around', '09', 'mev']] | [-0.07285533820758436, 0.15691660952265604, -0.07999746127533588, 0.08847031285894094, -0.011070748796285416, -0.1156312895098489, 0.07465112779178831, 0.3309361805567647, -0.22469187804525442, -0.3704080802531415, 0.03291135560260108, -0.28993793717115235, 0.011221160681106814, 0.16321791233817615, -0.008331220305846349, 0.05426999008153925, 0.016730248181167806, 0.06031224606927521, -0.13794091755136995, -0.17690440296831697, 0.29700362633471145, 0.11733953081218913, 0.25383815406314514, 0.16050876282146292, 0.10061855188635464, -0.03614865822860473, 0.007828700549826763, -0.0037244966594815842, -0.20105892671203002, 0.06942702726562425, 0.15711610033499576, 0.0012893107567572653, 0.19853499469504055, -0.35087610394832225, -0.18336133025402185, 0.1223805906380167, 0.0956159529119435, 0.06876525717054374, -0.007213015362878542, -0.23103960039149415, 0.061092578123627915, -0.22461420531836476, -0.1981507664832222, -0.020942907015064564, 0.008343157413793673, 0.0398628007050599, -0.2770921143168344, 0.164322359411341, 0.02519288823301881, -0.0023293727870551074, -0.10098496598588062, -0.21239173790154112, -0.05213511719525155, 0.09227264372143193, 0.10379315458934311, 0.06250974974977683, 0.1686780192580369, -0.10610466918880397, -0.03816230448267174, 0.35505604696008236, -0.0876194959238983, -0.14854642478743393, 0.0918821568052183, -0.14878141723739186, -0.01229734331977987, 0.2058167021426529, 0.15176664245785168, 0.08618189074504788, -0.14116092538000038, 0.05905561114829679, 0.01747717260323133, 0.2245009667009558, 0.13589843261138637, 0.004203555275603096, 0.23008459761259284, 0.09854409090326269, 0.0042540722821682395, 0.05703591524351315, -0.18243931992311435, -0.06651945174717815, -0.2865040842397599, -0.11727366495951272, -0.21019886815251948, 0.07824980357150653, -0.15634730560569632, -0.10712020574852198, 0.3987844386867058, 0.05778840706582264, 0.24134037408765663, 0.021187108701629803, 0.2857740131935271, 0.1546174854704059, 0.11510449589580518, 0.042924324686795766, 0.28927721058497996, 0.17868152577291693, 0.09439985054812514, -0.2600731202470378, 0.009066263075438466, 0.0661741531647668] |
710.2504 | Electronic band structure and exchange coupling constants in ACr2X4
spinels | We present the results of band structure calculations for ACr2X4 (A=Zn, Cd,
Hg and X=O, S, Se) spinels. Effective exchange coupling constants between Cr
spins are determined by fitting the energy of spin spirals to a classical
Heisenberg model. The calculations reproduce the change of the sign of the
dominant nearest-neighbor exchange interaction J1 from antiferromagnetic in
oxides to ferromagnetic in sulfides and selenides. It is verified that the
ferromagnetic contribution to J1 is due to indirect hopping between Cr t2g and
eg states via X p states. Antiferromagnetic coupling between 3-rd Cr neighbors
is found to be important in all the ACr2X4 spinels studied, whereas other
interactions are much weaker. The results are compared to predictions based on
the Goodenough-Kanamori rules of superexchange.
| cond-mat.other cond-mat.str-el | we present the results of band structure calculations for acr2x4 azn cd hg and xo s se spinels effective exchange coupling constants between cr spins are determined by fitting the energy of spin spirals to a classical heisenberg model the calculations reproduce the change of the sign of the dominant nearestneighbor exchange interaction j1 from antiferromagnetic in oxides to ferromagnetic in sulfides and selenides it is verified that the ferromagnetic contribution to j1 is due to indirect hopping between cr t2g and eg states via x p states antiferromagnetic coupling between 3rd cr neighbors is found to be important in all the acr2x4 spinels studied whereas other interactions are much weaker the results are compared to predictions based on the goodenoughkanamori rules of superexchange | [['we', 'present', 'the', 'results', 'of', 'band', 'structure', 'calculations', 'for', 'acr2x4', 'azn', 'cd', 'hg', 'and', 'xo', 's', 'se', 'spinels', 'effective', 'exchange', 'coupling', 'constants', 'between', 'cr', 'spins', 'are', 'determined', 'by', 'fitting', 'the', 'energy', 'of', 'spin', 'spirals', 'to', 'a', 'classical', 'heisenberg', 'model', 'the', 'calculations', 'reproduce', 'the', 'change', 'of', 'the', 'sign', 'of', 'the', 'dominant', 'nearestneighbor', 'exchange', 'interaction', 'j1', 'from', 'antiferromagnetic', 'in', 'oxides', 'to', 'ferromagnetic', 'in', 'sulfides', 'and', 'selenides', 'it', 'is', 'verified', 'that', 'the', 'ferromagnetic', 'contribution', 'to', 'j1', 'is', 'due', 'to', 'indirect', 'hopping', 'between', 'cr', 't2g', 'and', 'eg', 'states', 'via', 'x', 'p', 'states', 'antiferromagnetic', 'coupling', 'between', '3rd', 'cr', 'neighbors', 'is', 'found', 'to', 'be', 'important', 'in', 'all', 'the', 'acr2x4', 'spinels', 'studied', 'whereas', 'other', 'interactions', 'are', 'much', 'weaker', 'the', 'results', 'are', 'compared', 'to', 'predictions', 'based', 'on', 'the', 'goodenoughkanamori', 'rules', 'of', 'superexchange']] | [-0.1516980124774893, 0.16976433303245328, 0.059802830808502086, 0.10234248924324839, -0.051359989997152175, -0.18793961293155664, 0.07256198931508316, 0.4311432395680029, -0.26094520388201614, -0.27678576551881606, -0.04124748410626513, -0.37502549200883656, -0.07954803234917832, 0.13233631502523957, 0.13975693187752708, -0.10633805814031207, -0.016608786315000693, -0.0074199944597165115, -0.11665315237316135, -0.2252796158122021, 0.2610285898829671, 0.02432158456916814, 0.24255852270718725, 0.10064842562633948, -0.03643036978013935, 0.030857225710174956, 0.10951428829127403, -0.017326858547348223, -0.14358803527445205, 0.1287705693804262, 0.2590964052136262, -0.0807179338298738, 0.1381862280588811, -0.40586212567496494, -0.15453867440982189, 0.04006235400543044, 0.11426695655174, 0.11661597323073379, -0.011430356786090147, -0.28952394827788114, 0.057355967308318274, -0.1763952746911005, -0.05682455395352187, -0.09308253548520266, 0.012685869171543688, 0.03571081806936103, -0.3114801977945255, 0.12113902924966914, 0.09418502302847986, 0.08661579513494365, -0.10020884608307884, -0.19542638591078462, -0.14478417249304837, 0.08507323700201805, 0.09270164788200627, 0.06613644162101336, 0.0878259591323125, -0.054533895173827646, -0.14303401858664164, 0.408043458798259, -0.07030044400303044, -0.10092996419326318, 0.18953392635000352, -0.14624598365063307, -0.09356803162267706, 0.1430785836476344, 0.07589634403311571, 0.06226762650786426, -0.12902370275649028, 0.13277632234948228, 0.0525607942511923, 0.17605791334062815, -0.024192388707649757, 0.04053327242355244, 0.17591118930121424, 0.11847860908439214, 0.03878271838527967, 0.06606203112627196, -0.07672557798424186, -0.12410095421269109, -0.17513240388304482, -0.15316470681888159, -0.2536317931810684, 0.0564219154776303, -0.08647870233811564, -0.11578909508105306, 0.34427082224855904, 0.12174631271761323, 0.18002966224224512, -0.08329352754794184, 0.19673643009279107, 0.059924363047476156, 0.07579322956639846, 0.03929639804238057, 0.31392449926065863, 0.2268940948759068, 0.07659724034124711, -0.2799551761804576, 0.11815807503098469, 0.062379927660689734] |
710.2505 | Generic Trace Semantics via Coinduction | Trace semantics has been defined for various kinds of state-based systems,
notably with different forms of branching such as non-determinism vs.
probability. In this paper we claim to identify one underlying mathematical
structure behind these "trace semantics," namely coinduction in a Kleisli
category. This claim is based on our technical result that, under a suitably
order-enriched setting, a final coalgebra in a Kleisli category is given by an
initial algebra in the category Sets. Formerly the theory of coalgebras has
been employed mostly in Sets where coinduction yields a finer process semantics
of bisimilarity. Therefore this paper extends the application field of
coalgebras, providing a new instance of the principle "process semantics via
coinduction."
| cs.LO | trace semantics has been defined for various kinds of statebased systems notably with different forms of branching such as nondeterminism vs probability in this paper we claim to identify one underlying mathematical structure behind these trace semantics namely coinduction in a kleisli category this claim is based on our technical result that under a suitably orderenriched setting a final coalgebra in a kleisli category is given by an initial algebra in the category sets formerly the theory of coalgebras has been employed mostly in sets where coinduction yields a finer process semantics of bisimilarity therefore this paper extends the application field of coalgebras providing a new instance of the principle process semantics via coinduction | [['trace', 'semantics', 'has', 'been', 'defined', 'for', 'various', 'kinds', 'of', 'statebased', 'systems', 'notably', 'with', 'different', 'forms', 'of', 'branching', 'such', 'as', 'nondeterminism', 'vs', 'probability', 'in', 'this', 'paper', 'we', 'claim', 'to', 'identify', 'one', 'underlying', 'mathematical', 'structure', 'behind', 'these', 'trace', 'semantics', 'namely', 'coinduction', 'in', 'a', 'kleisli', 'category', 'this', 'claim', 'is', 'based', 'on', 'our', 'technical', 'result', 'that', 'under', 'a', 'suitably', 'orderenriched', 'setting', 'a', 'final', 'coalgebra', 'in', 'a', 'kleisli', 'category', 'is', 'given', 'by', 'an', 'initial', 'algebra', 'in', 'the', 'category', 'sets', 'formerly', 'the', 'theory', 'of', 'coalgebras', 'has', 'been', 'employed', 'mostly', 'in', 'sets', 'where', 'coinduction', 'yields', 'a', 'finer', 'process', 'semantics', 'of', 'bisimilarity', 'therefore', 'this', 'paper', 'extends', 'the', 'application', 'field', 'of', 'coalgebras', 'providing', 'a', 'new', 'instance', 'of', 'the', 'principle', 'process', 'semantics', 'via', 'coinduction']] | [-0.09661683246233958, 0.023046443873139203, -0.12896337432852178, 0.11520404968295975, -0.12554748396577084, -0.09444473519627201, 0.040949403766844944, 0.37124590391881374, -0.374103713886845, -0.23562516218966298, 0.07199448997689933, -0.16127894862898087, -0.12636278941410414, 0.15354404457142218, -0.18759982753953522, 0.013268530140059036, 0.07105437990813107, 0.07167106793311082, -0.02087096791518362, -0.21112787443531775, 0.43755233481224104, 0.018162506959286697, 0.26279925586851804, 0.022848046733487167, 0.09710698696800503, 0.018102779984474182, -0.013822235081246808, 0.03953888505827962, -0.11141987976123091, 0.13506702410073526, 0.33169198188146476, 0.19960531732067466, 0.29086883734245866, -0.39678672403750714, -0.1041616384969338, 0.08891347490185708, 0.08000054294774472, 0.09700299810062636, -0.02468379405980701, -0.33646579285299305, 0.08130462725826523, -0.24194806824814072, -0.0354649822938403, -0.0656001662361648, 0.06666882562945319, -0.021258665016942183, -0.2395001942064131, -0.06718383032191348, 0.14912161239618926, 0.1416508997667973, -0.07590484704307623, -0.0825604173199584, -0.025335165646474547, 0.07897140517455052, -0.017750239151370664, 0.00812131557470645, 0.1393002501909474, -0.0800037259918131, -0.22519706148784935, 0.36637416583273497, -0.05790442694795497, -0.20456261039106993, 0.20414855368557924, -0.07665830772582508, -0.2132275326937241, 0.08544749662427134, 0.06079906520123283, 0.12011757180944346, -0.1672219408685219, 0.1734171454516942, -0.10719788810156547, 0.13142009028805451, 0.1126783646218348, 0.0673166394066229, 0.17093715890465924, 0.22601989603993533, 0.021953479788192596, 0.15961037280871287, 0.03726031073867425, -0.12107823717636629, -0.33995701369355646, -0.19270866480655968, -0.0480295531696787, 0.04304301431565954, -0.050558405548432155, -0.19139626709613622, 0.3465842769170801, 0.19040675882634037, 0.167693322238496, 0.12449581717475922, 0.2769182234381636, 0.09205566012921433, 0.06549162810602993, -0.004964995411379884, 0.14754619948124806, 0.1908438278335604, 0.10013544639948298, -0.062432286190686, 0.1509934129487527, 0.16621528217046147] |
710.2506 | Stochastic Integrals and Evolution Equations with Gaussian Random Fields | The paper studies stochastic integration with respect to Gaussian processes
and fields. It is more convenient to work with a field than a process: by
definition, a field is a collection of stochastic integrals for a class of
deterministic integrands. The problem is then to extend the definition to
random integrands. An orthogonal decomposition of the chaos space of the random
field, combined with the Wick product, leads to the \Ito-Skorokhod integral,
and provides an efficient tool to study the integral, both analytically and
numerically. For a Gaussian process, a natural definition of the integral
follows from a canonical correspondence between random processes and a special
class of random fields. Some examples of the corresponding stochastic
differential equations are also considered.
| math.PR math.AP | the paper studies stochastic integration with respect to gaussian processes and fields it is more convenient to work with a field than a process by definition a field is a collection of stochastic integrals for a class of deterministic integrands the problem is then to extend the definition to random integrands an orthogonal decomposition of the chaos space of the random field combined with the wick product leads to the itoskorokhod integral and provides an efficient tool to study the integral both analytically and numerically for a gaussian process a natural definition of the integral follows from a canonical correspondence between random processes and a special class of random fields some examples of the corresponding stochastic differential equations are also considered | [['the', 'paper', 'studies', 'stochastic', 'integration', 'with', 'respect', 'to', 'gaussian', 'processes', 'and', 'fields', 'it', 'is', 'more', 'convenient', 'to', 'work', 'with', 'a', 'field', 'than', 'a', 'process', 'by', 'definition', 'a', 'field', 'is', 'a', 'collection', 'of', 'stochastic', 'integrals', 'for', 'a', 'class', 'of', 'deterministic', 'integrands', 'the', 'problem', 'is', 'then', 'to', 'extend', 'the', 'definition', 'to', 'random', 'integrands', 'an', 'orthogonal', 'decomposition', 'of', 'the', 'chaos', 'space', 'of', 'the', 'random', 'field', 'combined', 'with', 'the', 'wick', 'product', 'leads', 'to', 'the', 'itoskorokhod', 'integral', 'and', 'provides', 'an', 'efficient', 'tool', 'to', 'study', 'the', 'integral', 'both', 'analytically', 'and', 'numerically', 'for', 'a', 'gaussian', 'process', 'a', 'natural', 'definition', 'of', 'the', 'integral', 'follows', 'from', 'a', 'canonical', 'correspondence', 'between', 'random', 'processes', 'and', 'a', 'special', 'class', 'of', 'random', 'fields', 'some', 'examples', 'of', 'the', 'corresponding', 'stochastic', 'differential', 'equations', 'are', 'also', 'considered']] | [-0.11576213968883091, 0.10180170246912744, -0.1110378969864812, 0.07676214799069062, -0.1151246763111577, -0.07166546475034484, 0.02936346351153656, 0.349286170845682, -0.29454149228466814, -0.2165066918482319, 0.11512076950147132, -0.2282434607719356, -0.1954704143784263, 0.22854651128950199, -0.0684405797476734, 0.05929518599940602, 0.03968371839016245, 0.037471918808681164, -0.07923158801022209, -0.21526270883912144, 0.35920061144885446, 0.04224601201713085, 0.23595491375135305, -0.046677494690992125, 0.15145316895112887, 0.0396818852606268, -0.07567017058233831, 0.02320429873397797, -0.10493642808907966, 0.14938356800385835, 0.21001520371141513, 0.09570944669063795, 0.29265779970321526, -0.3809631967624603, -0.19715514073286913, 0.11937241935101915, 0.11047050954455563, 0.09959097191198799, -0.008231309241223657, -0.26047509773211047, 0.04972384662032108, -0.13242658767233456, -0.1611963893269566, -0.09681320150021064, 0.02193284194727913, 0.025030980606309393, -0.36314796874961575, 0.01823296473522224, 0.08384793989306455, 0.0455423963664115, -0.02761884875526298, -0.06656257480321344, 0.02600390444055569, 0.06265148749451868, 0.03236607366398699, 0.06709045831167931, 0.08837856113822161, -0.1208887287484836, -0.1557619756911227, 0.360260136048348, -0.09583988819958754, -0.27274587975183795, 0.17126142061969712, -0.11573158429689274, -0.12019342412664132, 0.15795024079251418, 0.15315261603263783, 0.15915279484484807, -0.2179045902857603, 0.12054829399316949, -0.02587678659830458, 0.06023444552051504, 0.038734599505358736, 0.009264971302776051, 0.1386721947669121, 0.11287039066549422, 0.10169148415881248, 0.18849366619290153, -0.02213504640693384, -0.18857111871119372, -0.3228502202440392, -0.20932201688632, -0.14908250475933482, 0.07307759144589736, -0.13008221072550816, -0.23432753870864054, 0.3825482957811703, 0.11808777532024571, 0.18524095541913033, 0.10350413719761717, 0.27524423025055855, 0.20227591514064014, 0.022817363546899526, 0.02658086426725442, 0.12068660606217402, 0.25037456400238345, 0.10093393452342383, -0.13802093316893255, 0.016532608700438964, 0.075939730910415] |
710.2507 | Stochastic suspensions of heavy particles | Turbulent suspensions of heavy particles in incompressible flows have gained
much attention in recent years. A large amount of work focused on the impact
that the inertia and the dissipative dynamics of the particles have on their
dynamical and statistical properties. Substantial progress followed from the
study of suspensions in model flows which, although much simpler, reproduce
most of the important mechanisms observed in real turbulence. This paper
presents recent developments made on the relative motion of a pair of particles
suspended in time-uncorrelated and spatially self-similar Gaussian flows. This
review is complemented by new results. By introducing a time-dependent Stokes
number, it is demonstrated that inertial particle relative dispersion recovers
asymptotically Richardson's diffusion associated to simple tracers. A
perturbative (homogeneization) technique is used in the small-Stokes-number
asymptotics and leads to interpreting first-order corrections to tracer
dynamics in terms of an effective drift. This expansion implies that the
correlation dimension deficit behaves linearly as a function of the Stokes
number. The validity and the accuracy of this prediction is confirmed by
numerical simulations.
| nlin.CD cond-mat.stat-mech physics.flu-dyn | turbulent suspensions of heavy particles in incompressible flows have gained much attention in recent years a large amount of work focused on the impact that the inertia and the dissipative dynamics of the particles have on their dynamical and statistical properties substantial progress followed from the study of suspensions in model flows which although much simpler reproduce most of the important mechanisms observed in real turbulence this paper presents recent developments made on the relative motion of a pair of particles suspended in timeuncorrelated and spatially selfsimilar gaussian flows this review is complemented by new results by introducing a timedependent stokes number it is demonstrated that inertial particle relative dispersion recovers asymptotically richardsons diffusion associated to simple tracers a perturbative homogeneization technique is used in the smallstokesnumber asymptotics and leads to interpreting firstorder corrections to tracer dynamics in terms of an effective drift this expansion implies that the correlation dimension deficit behaves linearly as a function of the stokes number the validity and the accuracy of this prediction is confirmed by numerical simulations | [['turbulent', 'suspensions', 'of', 'heavy', 'particles', 'in', 'incompressible', 'flows', 'have', 'gained', 'much', 'attention', 'in', 'recent', 'years', 'a', 'large', 'amount', 'of', 'work', 'focused', 'on', 'the', 'impact', 'that', 'the', 'inertia', 'and', 'the', 'dissipative', 'dynamics', 'of', 'the', 'particles', 'have', 'on', 'their', 'dynamical', 'and', 'statistical', 'properties', 'substantial', 'progress', 'followed', 'from', 'the', 'study', 'of', 'suspensions', 'in', 'model', 'flows', 'which', 'although', 'much', 'simpler', 'reproduce', 'most', 'of', 'the', 'important', 'mechanisms', 'observed', 'in', 'real', 'turbulence', 'this', 'paper', 'presents', 'recent', 'developments', 'made', 'on', 'the', 'relative', 'motion', 'of', 'a', 'pair', 'of', 'particles', 'suspended', 'in', 'timeuncorrelated', 'and', 'spatially', 'selfsimilar', 'gaussian', 'flows', 'this', 'review', 'is', 'complemented', 'by', 'new', 'results', 'by', 'introducing', 'a', 'timedependent', 'stokes', 'number', 'it', 'is', 'demonstrated', 'that', 'inertial', 'particle', 'relative', 'dispersion', 'recovers', 'asymptotically', 'richardsons', 'diffusion', 'associated', 'to', 'simple', 'tracers', 'a', 'perturbative', 'homogeneization', 'technique', 'is', 'used', 'in', 'the', 'smallstokesnumber', 'asymptotics', 'and', 'leads', 'to', 'interpreting', 'firstorder', 'corrections', 'to', 'tracer', 'dynamics', 'in', 'terms', 'of', 'an', 'effective', 'drift', 'this', 'expansion', 'implies', 'that', 'the', 'correlation', 'dimension', 'deficit', 'behaves', 'linearly', 'as', 'a', 'function', 'of', 'the', 'stokes', 'number', 'the', 'validity', 'and', 'the', 'accuracy', 'of', 'this', 'prediction', 'is', 'confirmed', 'by', 'numerical', 'simulations']] | [-0.1095409591454871, 0.15360094985745273, -0.10017102373061343, 0.0330911039889447, -0.02659419136072852, -0.06900432864707835, -0.028872194763937452, 0.3241734459876404, -0.2398126895508146, -0.2819218861173337, 0.056873160483157645, -0.26462069543198363, -0.13794357383070405, 0.20523411244881062, -0.05286388086667012, 0.08379593878311829, 0.07337425025016592, -0.012506929024705413, -0.017714933229457826, -0.21120320155955197, 0.28600487332486096, 0.09230639831277362, 0.2799682808462639, 0.05085800267614381, 0.1005590926155949, -0.028800323598729503, -0.08913855369567697, 0.08354528154156644, -0.15893051017286652, 0.11467035918371284, 0.16883853424547446, 0.0358138799446782, 0.279690291787013, -0.4241293738459983, -0.2776864451078469, 0.07045623052277063, 0.18489302478033548, 0.11227006311678159, -0.08990335425195878, -0.25570888521029933, 0.03479228148574543, -0.18675141849647664, -0.1497156567713627, -0.07974170987447995, 0.061740365462127134, 0.03248960266505199, -0.23564555220665379, 0.12438598390834063, 0.06628704322214382, 0.06922845909785894, -0.021874180271927463, -0.07961856955880223, 0.0021333400628458688, 0.09018381885171198, 0.11547955007316839, 0.016010087600239274, 0.1435821614260867, -0.17256966984847136, -0.08069677264409206, 0.4133172389964045, -0.08863115179344293, -0.22261081909834357, 0.22077734434530574, -0.15772270956975326, -0.11188986423365467, 0.16998553802449887, 0.19442480799949002, 0.1274060579997144, -0.13277737193942418, 0.06140197061610882, -0.06808883077002059, 0.1516857073800257, 0.040769922274725826, 0.00014529704274228442, 0.19565711701996844, 0.18376377227781504, 0.03221510562566463, 0.1267351137197778, -0.07527044895465883, -0.13867380001925325, -0.2759069608611583, -0.14683986632344012, -0.1801125945915517, 0.061467490624976806, -0.08129470837559505, -0.1543099031217222, 0.3695543067834792, 0.1629592130418148, 0.21598103238345936, 0.04218828203823766, 0.29414869016254247, 0.10508704892351504, 0.024229834952299096, 0.06299922948877452, 0.2821876714169456, 0.18044918833289578, 0.13262504227023725, -0.23914542413120599, 0.07442583093196371, 0.07691758416309866] |
710.2508 | Right-Chiral Sneutrino LSP in mSUGRA: Event characteristics of NLSP at
the LHC | We study a supersymmetric scenario where the lighter tau-sneutrino is the
lightest supersymmetric particle, while the lighter stau-state is the next
lightest. Such a scenario can be motivated within the framework of minimal
supergravity, with just the addition of a right-chiral neutrino superfield.
Such a spectrum leads to rather unusual signals of supersymmetry, showing
stable tracks of the stau in the muon chambers. We study the event
characteristics of the long-lived staus at the LHC and demonstrate that the
stau tracks can be distinguished from the muonic ones through proper kinematic
cuts which also enable one to remove all standard model backgrounds.
| hep-ph | we study a supersymmetric scenario where the lighter tausneutrino is the lightest supersymmetric particle while the lighter staustate is the next lightest such a scenario can be motivated within the framework of minimal supergravity with just the addition of a rightchiral neutrino superfield such a spectrum leads to rather unusual signals of supersymmetry showing stable tracks of the stau in the muon chambers we study the event characteristics of the longlived staus at the lhc and demonstrate that the stau tracks can be distinguished from the muonic ones through proper kinematic cuts which also enable one to remove all standard model backgrounds | [['we', 'study', 'a', 'supersymmetric', 'scenario', 'where', 'the', 'lighter', 'tausneutrino', 'is', 'the', 'lightest', 'supersymmetric', 'particle', 'while', 'the', 'lighter', 'staustate', 'is', 'the', 'next', 'lightest', 'such', 'a', 'scenario', 'can', 'be', 'motivated', 'within', 'the', 'framework', 'of', 'minimal', 'supergravity', 'with', 'just', 'the', 'addition', 'of', 'a', 'rightchiral', 'neutrino', 'superfield', 'such', 'a', 'spectrum', 'leads', 'to', 'rather', 'unusual', 'signals', 'of', 'supersymmetry', 'showing', 'stable', 'tracks', 'of', 'the', 'stau', 'in', 'the', 'muon', 'chambers', 'we', 'study', 'the', 'event', 'characteristics', 'of', 'the', 'longlived', 'staus', 'at', 'the', 'lhc', 'and', 'demonstrate', 'that', 'the', 'stau', 'tracks', 'can', 'be', 'distinguished', 'from', 'the', 'muonic', 'ones', 'through', 'proper', 'kinematic', 'cuts', 'which', 'also', 'enable', 'one', 'to', 'remove', 'all', 'standard', 'model', 'backgrounds']] | [-0.059019843900188954, 0.25662139878783485, -0.0563347303575956, 0.16396493815337446, -0.06908917425218786, -0.17548462925571026, -0.001060783502295392, 0.30753639049477655, -0.22108467695957953, -0.29808369040775046, 0.06580739823229943, -0.2944838776907856, -0.038991806180317806, 0.15184038854780432, -0.020869447252630156, 0.02689112393683431, 0.10422194956589749, 0.056219696408451196, -0.0706411449510678, -0.2027420272571173, 0.26510327278018586, 0.03728940608994205, 0.16051446737740005, 0.04224848203213498, 0.0719404037751368, -0.03663642947230082, 0.004635368699742721, -0.0507650294958955, -0.07360437694318318, 0.07756635980071998, 0.18385433296368706, 0.13841921293481005, 0.10010685976410266, -0.38359667290702903, -0.17399081494659185, 0.22127338766931823, 0.1866023867566249, 0.11064920528292757, -0.05830809355962394, -0.31250737493138503, 0.12983326373234538, -0.22243229915747548, -0.13279534800503734, -0.00930823580509439, -0.08129718352920644, -0.12379214763791199, -0.3003415894962036, 0.06787833135942745, -0.03420541679837031, -0.052070984201929946, -0.007458752860305923, -0.11058596719867818, -0.10512949476055432, 0.023833270788672242, 0.16955794660849405, -0.03207987993217931, 0.19039641216277411, -0.1779123119419754, -0.15983087535357415, 0.4162938060552472, -0.07873118286814061, -0.1746201800864817, 0.16896309845131074, -0.15767745928617544, -0.14029111629720814, 0.15474075473335544, 0.15633658466325834, 0.15494006336436117, -0.17748433845273293, 0.15654098775438355, -0.0682326317995344, 0.17042785729650445, 0.05585579259440967, 0.04451100158938529, 0.2969411816263553, 0.2485785738721785, 0.09364446959317671, 0.08802404733937197, -0.09781818685702759, -0.07388331849441522, -0.41633799271185484, -0.16805654934303152, -0.060854056380956555, 0.00918141954421702, -0.07330031915654839, -0.10821595020698255, 0.45639025143320017, 0.10900075603313951, 0.25109038671644607, -0.00555203901949606, 0.2923013397704552, 0.04053263123709672, 0.10055354062357161, 0.00938179148453297, 0.31281287224483817, 0.09240386936592289, 0.0906629625518834, -0.23746161623673495, -0.027988282318162448, 0.07378661045159149] |
710.2509 | Locally Compact Objects in Exact Categories | We identify two categories of locally compact objects on an exact category A.
They correspond to the well-known constructions of the Beilinson category lim A
and the Kato category k(A). We study their mutual relations and compare the two
constructions. We prove that lim A is an exact category, which gives to this
category a very convenient feature when dealing with K-theoretical invariants.
It is natural therefore to consider the Beilinson category lim A as the most
convenient candidate to the role of the category of locally compact objects
over an exact category. We also show that the categories Ind_{aleph_0}(C),
Pro_{aleph_0}(C) of countably indexed ind/pro-objects over any category C can
be described as localizations of categories of diagrams over C.
| math.CT math.KT | we identify two categories of locally compact objects on an exact category a they correspond to the wellknown constructions of the beilinson category lim a and the kato category ka we study their mutual relations and compare the two constructions we prove that lim a is an exact category which gives to this category a very convenient feature when dealing with ktheoretical invariants it is natural therefore to consider the beilinson category lim a as the most convenient candidate to the role of the category of locally compact objects over an exact category we also show that the categories ind_aleph_0c pro_aleph_0c of countably indexed indproobjects over any category c can be described as localizations of categories of diagrams over c | [['we', 'identify', 'two', 'categories', 'of', 'locally', 'compact', 'objects', 'on', 'an', 'exact', 'category', 'a', 'they', 'correspond', 'to', 'the', 'wellknown', 'constructions', 'of', 'the', 'beilinson', 'category', 'lim', 'a', 'and', 'the', 'kato', 'category', 'ka', 'we', 'study', 'their', 'mutual', 'relations', 'and', 'compare', 'the', 'two', 'constructions', 'we', 'prove', 'that', 'lim', 'a', 'is', 'an', 'exact', 'category', 'which', 'gives', 'to', 'this', 'category', 'a', 'very', 'convenient', 'feature', 'when', 'dealing', 'with', 'ktheoretical', 'invariants', 'it', 'is', 'natural', 'therefore', 'to', 'consider', 'the', 'beilinson', 'category', 'lim', 'a', 'as', 'the', 'most', 'convenient', 'candidate', 'to', 'the', 'role', 'of', 'the', 'category', 'of', 'locally', 'compact', 'objects', 'over', 'an', 'exact', 'category', 'we', 'also', 'show', 'that', 'the', 'categories', 'ind_aleph_0c', 'pro_aleph_0c', 'of', 'countably', 'indexed', 'indproobjects', 'over', 'any', 'category', 'c', 'can', 'be', 'described', 'as', 'localizations', 'of', 'categories', 'of', 'diagrams', 'over', 'c']] | [-0.13891681486692947, 0.002551597255878111, -0.0812595433428183, 0.13394815128189153, -0.08849729262451586, -0.11984752296493986, 0.008537439211534385, 0.39490248301090336, -0.370221829540335, -0.20687358545410073, 0.08557868577762802, -0.20631684588952962, -0.11957688795195685, 0.23109314329603797, -0.1951479601363341, -0.11935849922697227, 0.049343443316463224, 0.12068200559538399, -0.05053910730171821, -0.2686094510365023, 0.4311698578998574, 0.011501910261467544, 0.24845727116792884, -0.008825584653064482, 0.0859162447313404, -0.025581622193766456, -0.016275460282579448, 0.026382096676936008, -0.12681997050772498, 0.16361763581840527, 0.34396962291346145, 0.09778354643509747, 0.21071390775888044, -0.32320814828077954, -0.11419093121702854, 0.14487859681567067, 0.10807230581059797, 0.07728206207796645, 0.011994524246965272, -0.3248519930097028, 0.12677410017484084, -0.24703773506121057, -0.06278406470042901, -0.08349024708597706, 0.11933474360495551, 0.022217051291233327, -0.2651120426499436, -0.07410095710308355, 0.09207693305917275, 0.05576578327096426, -0.11746117971542999, -0.07904201161721323, -0.0632807943237643, 0.11556571026250091, -0.031429706301548094, 0.028456630326536857, 0.10542336135354434, -0.1365498367868141, -0.11846886419603585, 0.3563455091789365, -0.05572307965137128, -0.20249744749858847, 0.2347529259406858, -0.06744971648495421, -0.14501686402970654, 0.10757667613494346, 0.025483459847159367, 0.1765191620414774, -0.06718682826351888, 0.16352322948286876, -0.1486403200094803, 0.0980184918635676, 0.08956490320145574, 0.06359837976340045, 0.17881731579923987, 0.1261368214379614, 0.019949627451152883, 0.1411892198629152, -0.028595943961085543, -0.03765868079952068, -0.3453641618416907, -0.1812783556872915, -0.08161566973639986, 0.10570165633401062, -0.08083272225827448, -0.21139910486009386, 0.3786094292648073, 0.13514405731350565, 0.22628670379307528, 0.1492640431263906, 0.19685057259331912, 0.05693341482979938, 0.05781919150175447, 0.045151348082491986, 0.14850197226191178, 0.19464679926824877, -0.015262375716080204, -0.049320730523994334, -0.0007659593123433172, 0.1800127553825195] |
710.251 | Intracellular microrheology of motile Amoeba proteus | The motility of motile Amoeba proteus was examined using the technique of
passive particle tracking microrheology, with the aid of newly-developed
particle tracking software, a fast digital camera and an optical microscope. We
tracked large numbers of endogeneous particles in the amoebae, which displayed
subdiffusive motion at short time scales, corresponding to thermal motion in a
viscoelastic medium, and superdiffusive motion at long time scales due to the
convection of the cytoplasm. Subdiffusive motion was characterised by a
rheological scaling exponent of 3/4 in the cortex, indicative of the
semiflexible dynamics of the actin fibres. We observed shear-thinning in the
flowing endoplasm, where exponents increased with increasing flow rate; i.e.
the endoplasm became more fluid-like. The rheology of the cortex is found to be
isotropic, reflecting an isotropic actin gel. A clear difference was seen
between cortical and endoplasmic layers in terms of both viscoelasticity and
flow velocity, where the profile of the latter is close to a Poiseuille flow
for a Newtonian fluid.
| cond-mat.soft q-bio.CB | the motility of motile amoeba proteus was examined using the technique of passive particle tracking microrheology with the aid of newlydeveloped particle tracking software a fast digital camera and an optical microscope we tracked large numbers of endogeneous particles in the amoebae which displayed subdiffusive motion at short time scales corresponding to thermal motion in a viscoelastic medium and superdiffusive motion at long time scales due to the convection of the cytoplasm subdiffusive motion was characterised by a rheological scaling exponent of 34 in the cortex indicative of the semiflexible dynamics of the actin fibres we observed shearthinning in the flowing endoplasm where exponents increased with increasing flow rate ie the endoplasm became more fluidlike the rheology of the cortex is found to be isotropic reflecting an isotropic actin gel a clear difference was seen between cortical and endoplasmic layers in terms of both viscoelasticity and flow velocity where the profile of the latter is close to a poiseuille flow for a newtonian fluid | [['the', 'motility', 'of', 'motile', 'amoeba', 'proteus', 'was', 'examined', 'using', 'the', 'technique', 'of', 'passive', 'particle', 'tracking', 'microrheology', 'with', 'the', 'aid', 'of', 'newlydeveloped', 'particle', 'tracking', 'software', 'a', 'fast', 'digital', 'camera', 'and', 'an', 'optical', 'microscope', 'we', 'tracked', 'large', 'numbers', 'of', 'endogeneous', 'particles', 'in', 'the', 'amoebae', 'which', 'displayed', 'subdiffusive', 'motion', 'at', 'short', 'time', 'scales', 'corresponding', 'to', 'thermal', 'motion', 'in', 'a', 'viscoelastic', 'medium', 'and', 'superdiffusive', 'motion', 'at', 'long', 'time', 'scales', 'due', 'to', 'the', 'convection', 'of', 'the', 'cytoplasm', 'subdiffusive', 'motion', 'was', 'characterised', 'by', 'a', 'rheological', 'scaling', 'exponent', 'of', '34', 'in', 'the', 'cortex', 'indicative', 'of', 'the', 'semiflexible', 'dynamics', 'of', 'the', 'actin', 'fibres', 'we', 'observed', 'shearthinning', 'in', 'the', 'flowing', 'endoplasm', 'where', 'exponents', 'increased', 'with', 'increasing', 'flow', 'rate', 'ie', 'the', 'endoplasm', 'became', 'more', 'fluidlike', 'the', 'rheology', 'of', 'the', 'cortex', 'is', 'found', 'to', 'be', 'isotropic', 'reflecting', 'an', 'isotropic', 'actin', 'gel', 'a', 'clear', 'difference', 'was', 'seen', 'between', 'cortical', 'and', 'endoplasmic', 'layers', 'in', 'terms', 'of', 'both', 'viscoelasticity', 'and', 'flow', 'velocity', 'where', 'the', 'profile', 'of', 'the', 'latter', 'is', 'close', 'to', 'a', 'poiseuille', 'flow', 'for', 'a', 'newtonian', 'fluid']] | [-0.14082085476299497, 0.2101412814477155, -0.10665794992365124, -0.015123545474702174, -0.027829051196998234, -0.14678100358535787, -0.062166366117109156, 0.3608906812456198, -0.29998884970310186, -0.24660218228932423, 0.04368725372975261, -0.26126081546734475, -0.17221409212457153, 0.18016108458935534, -0.06279246721107218, 0.055000796093514596, 0.0021995594810194723, 0.00969084527516715, 0.05352404916035395, -0.13747002803805716, 0.1650435554130548, 0.05686821690306249, 0.2784967072444355, -0.0007188108571515441, 0.16384019369895503, -0.034606412933321624, -0.02222646002532778, 0.07502631697428935, -0.1781664035402284, 0.06869145709930397, 0.20936425272787057, -0.026807775917404797, 0.225994098421879, -0.4692033571191132, -0.23459093649758073, 0.06910232862275911, 0.20627788930745206, 0.07830291313741061, -0.00911371879857786, -0.28993819590385367, 0.024252708680450735, -0.13417236907010124, -0.14838208175525525, 0.00276138896701812, 0.08408342215669819, 0.0813050925938935, -0.208561116412123, 0.2027296237526859, 0.038312987882286174, 0.14234946615193267, -0.1030071805793474, 0.007721687045243637, -0.03823031955285043, 0.13634327469711624, 0.09614907480455458, 0.021422095500250777, 0.2736039277955481, -0.20972868671822475, -0.037645359628652106, 0.3849341273421376, -0.03856636697381008, -0.1761326161667523, 0.22854855402497712, -0.17735344985437512, -0.026677230769830824, 0.21780121737591376, 0.1883689593069437, 0.07414068839237344, -0.1473154713819939, -0.031320819702203864, -0.03340998051436788, 0.20548304227016093, 0.09117093774853502, -0.06313117434378578, 0.1891001635337555, 0.2610496271617438, 0.01769437595191071, 0.14384263589702798, -0.15336995097672249, -0.12129504893190886, -0.22780559366148692, -0.1798143419442878, -0.16339680216581812, 0.028638683042273197, -0.14825053922455791, -0.16431911838831517, 0.35221893902479035, 0.05838111278930361, 0.1941183328049303, 0.08677449197119397, 0.25223161096765556, 0.02314317746090748, 0.04988135165863574, 0.09035636002777099, 0.2623035316909209, 0.1432308792945838, 0.21843880177589087, -0.27606600787059016, 0.08113299516915548, 0.06761005951841248] |
710.2511 | Thermal effects in exciton harvesting in biased one-dimensional systems | The study of energy harvesting in chain-like structures is important due to
its relevance to a variety of interesting physical systems. Harvesting is
understood as the combination of exciton transport through intra-band exciton
relaxation (via scattering on phonon modes) and subsequent quenching by a trap.
Previously, we have shown that in the low temperature limit different
harvesting scenarios as a function of the applied bias strength (slope of the
energy gradient towards the trap) are possible \cite{Vlaming07}. This paper
generalizes the results for both homogeneous and disordered chains to nonzero
temperatures. We show that thermal effects are appreciable only for low bias
strengths, particularly so in disordered systems, and lead to faster
harvesting.
| cond-mat.dis-nn cond-mat.mtrl-sci | the study of energy harvesting in chainlike structures is important due to its relevance to a variety of interesting physical systems harvesting is understood as the combination of exciton transport through intraband exciton relaxation via scattering on phonon modes and subsequent quenching by a trap previously we have shown that in the low temperature limit different harvesting scenarios as a function of the applied bias strength slope of the energy gradient towards the trap are possible citevlaming07 this paper generalizes the results for both homogeneous and disordered chains to nonzero temperatures we show that thermal effects are appreciable only for low bias strengths particularly so in disordered systems and lead to faster harvesting | [['the', 'study', 'of', 'energy', 'harvesting', 'in', 'chainlike', 'structures', 'is', 'important', 'due', 'to', 'its', 'relevance', 'to', 'a', 'variety', 'of', 'interesting', 'physical', 'systems', 'harvesting', 'is', 'understood', 'as', 'the', 'combination', 'of', 'exciton', 'transport', 'through', 'intraband', 'exciton', 'relaxation', 'via', 'scattering', 'on', 'phonon', 'modes', 'and', 'subsequent', 'quenching', 'by', 'a', 'trap', 'previously', 'we', 'have', 'shown', 'that', 'in', 'the', 'low', 'temperature', 'limit', 'different', 'harvesting', 'scenarios', 'as', 'a', 'function', 'of', 'the', 'applied', 'bias', 'strength', 'slope', 'of', 'the', 'energy', 'gradient', 'towards', 'the', 'trap', 'are', 'possible', 'citevlaming07', 'this', 'paper', 'generalizes', 'the', 'results', 'for', 'both', 'homogeneous', 'and', 'disordered', 'chains', 'to', 'nonzero', 'temperatures', 'we', 'show', 'that', 'thermal', 'effects', 'are', 'appreciable', 'only', 'for', 'low', 'bias', 'strengths', 'particularly', 'so', 'in', 'disordered', 'systems', 'and', 'lead', 'to', 'faster', 'harvesting']] | [-0.14630267275112732, 0.18523503605060146, -0.05479202351333307, 0.057412824066497184, -0.026870502502008873, -0.15531914849166892, 0.05016419014282292, 0.42166798638312947, -0.27790835757124505, -0.28036256927797304, 0.04718039550789399, -0.25186780441435985, -0.13725015753464373, 0.219744990957614, 0.008484803527397031, 0.012384469287748548, 0.02887541547949825, -0.011707279563519737, -0.018224758732685586, -0.17760198414076253, 0.29665229497810025, 0.10076102683836195, 0.31732733108011807, 0.1306160074725215, 0.07313652582732695, 0.0024137139012704472, 0.07539756796489071, 0.013065068383834191, -0.13094490691959695, 0.07214894219318271, 0.2693205860393521, -0.019937769048348337, 0.2349567221244797, -0.4231482943120812, -0.28104787613431526, 0.11091163009301194, 0.187726354467616, 0.16255900886608288, -0.07793134673452837, -0.20589196003441299, 0.05257419610695381, -0.1579089299401468, -0.09242752536582495, -0.08470535295782611, 0.03323448220700292, 0.053058191454121176, -0.23088341847427987, 0.11954395609375622, 0.046824569593549574, 0.04070501611568034, -0.11004596707165806, -0.14354854023622465, -0.049224347849043885, 0.09222382209970549, 0.05754209313558282, -0.021836154950766025, 0.18397581376484595, -0.1361211652547354, -0.07337067073552005, 0.37743464444897007, -0.07097103175640639, -0.12860683782491833, 0.24735145364580344, -0.10868138963373244, -0.08376293740002438, 0.16533232910608472, 0.20097444394403802, 0.09630154818296432, -0.14917727778915182, 0.056581477725038506, 0.042499636100339036, 0.1146491087648818, 0.042194140825553665, 0.11345921831005919, 0.21937298658303916, 0.17717478617643273, 0.08155670903631419, 0.16298434173014748, -0.08078875614488165, -0.0865294254040886, -0.2285839254369161, -0.13536091677503595, -0.19996164391549037, 0.07172774873158362, -0.043622493614618306, -0.1280629116525753, 0.39167359652596395, 0.15216852361170044, 0.2229224302739437, 0.008187955943867564, 0.29611840025920955, 0.15259130019070913, 0.05530215391107569, 0.012074123664725838, 0.27738530543865636, 0.16705459129713876, 0.12593186915702453, -0.29144811767037027, 0.055349174371388345, -0.029463334021524394] |
710.2512 | Monodromy transform approach in the theory of integrable reductions of
Einstein's field equations and some applications | A brief sketch of the formulation of the monodromy transform approach and
corresponding integral equation methods as well as of various applications of
this approach for solution of integrable symmetry reductions of Einstein's
field equations is presented.
| gr-qc | a brief sketch of the formulation of the monodromy transform approach and corresponding integral equation methods as well as of various applications of this approach for solution of integrable symmetry reductions of einsteins field equations is presented | [['a', 'brief', 'sketch', 'of', 'the', 'formulation', 'of', 'the', 'monodromy', 'transform', 'approach', 'and', 'corresponding', 'integral', 'equation', 'methods', 'as', 'well', 'as', 'of', 'various', 'applications', 'of', 'this', 'approach', 'for', 'solution', 'of', 'integrable', 'symmetry', 'reductions', 'of', 'einsteins', 'field', 'equations', 'is', 'presented']] | [-0.10545558593160398, -0.026498217355913005, -0.13850900367204402, 0.0763131252716522, -0.11534703335397549, -0.12015611875953304, -0.06748987301378637, 0.2699014278682503, -0.2922159617615713, -0.31062859759942907, 0.16876721935900482, -0.24950436965839282, -0.23362841145009608, 0.22462087332560504, -0.05708099969637555, 0.1093051708932664, 0.06466466917127774, 0.05163562217274228, -0.15877861236033305, -0.24903557100962545, 0.320335407917564, -0.035719969385379066, 0.26978507839344645, 0.02415256616281899, 0.20206381735467427, 0.008182207625862714, -0.040119663887732734, 0.00220883430006939, -0.11177435369432173, 0.14075151083336487, 0.2383800844309499, 0.14981408965950077, 0.2306071926613112, -0.413361389945085, -0.19073395599686616, 0.009316390606801252, 0.14672616658405074, 0.16520241033789274, -0.051529677685450866, -0.3187767332923171, 0.014452428003219334, -0.16732098791446234, -0.218266013405613, -0.10624266899115331, 0.03942157085544455, 0.048466550211447315, -0.21268687382139065, 0.08709747155473845, 0.0717713925515528, 0.049389485672519017, -0.15704373038701108, -0.11699007146966618, 0.05037977823647796, 0.0340043000146948, 0.10950114948020594, 0.02559557947254664, 0.07142329900966, -0.16366710931037529, -0.11619900212295957, 0.45617301767138213, -0.07764994295162929, -0.22255225670901504, 0.08881389580327212, -0.023360031354870345, -0.13396550954092998, 0.12502400165524435, 0.14772296641525384, 0.18918935644968943, -0.15603208020832893, 0.17545545438298252, -0.03860424078900267, 0.05129248656433176, 0.03625295915313669, 0.03454134432045189, 0.1550032387714128, 0.16229526532461513, 0.06631478040504295, 0.11254012111473728, 0.02804096314955402, -0.13523820631608768, -0.4320922530180699, -0.214955605063084, -0.1695175568346639, 0.08496296964585781, -0.08705869452938172, -0.2033094289284703, 0.39914686766427915, 0.16440899126433037, 0.12491119884558625, 0.057828721011409887, 0.26510456566875046, 0.19538313212703812, 0.03185683554290114, -0.04187210680715538, 0.1408838201314211, 0.23613419357964113, 0.13763781506064776, -0.22816628553728396, -0.1029763659210624, 0.18433943994947383] |
710.2513 | Structural dependence of robustness and load tolerance in scale-free
networks | The structure of complex networks in previous research has been widely
described as scale-free networks generated by the preferential attachment
model. However, the preferential attachment model does not take into account
the detailed topological property observed in real networks. Here we propose
the models of scale-free networks which can reproduce the topological
assortativity of real networks. With an identical degree distribution and
network size, we study the structural robustness and fragility as well as the
dynamic change of load intensity when nodes are successively removed under
random and various intentional attack strategies. We find that disassortative
networks are structurally robust against random attacks and highly
load-tolerant, while assortative networks are most resistant to intentional
attacks yet significantly fragile against random attacks.
| cond-mat.dis-nn | the structure of complex networks in previous research has been widely described as scalefree networks generated by the preferential attachment model however the preferential attachment model does not take into account the detailed topological property observed in real networks here we propose the models of scalefree networks which can reproduce the topological assortativity of real networks with an identical degree distribution and network size we study the structural robustness and fragility as well as the dynamic change of load intensity when nodes are successively removed under random and various intentional attack strategies we find that disassortative networks are structurally robust against random attacks and highly loadtolerant while assortative networks are most resistant to intentional attacks yet significantly fragile against random attacks | [['the', 'structure', 'of', 'complex', 'networks', 'in', 'previous', 'research', 'has', 'been', 'widely', 'described', 'as', 'scalefree', 'networks', 'generated', 'by', 'the', 'preferential', 'attachment', 'model', 'however', 'the', 'preferential', 'attachment', 'model', 'does', 'not', 'take', 'into', 'account', 'the', 'detailed', 'topological', 'property', 'observed', 'in', 'real', 'networks', 'here', 'we', 'propose', 'the', 'models', 'of', 'scalefree', 'networks', 'which', 'can', 'reproduce', 'the', 'topological', 'assortativity', 'of', 'real', 'networks', 'with', 'an', 'identical', 'degree', 'distribution', 'and', 'network', 'size', 'we', 'study', 'the', 'structural', 'robustness', 'and', 'fragility', 'as', 'well', 'as', 'the', 'dynamic', 'change', 'of', 'load', 'intensity', 'when', 'nodes', 'are', 'successively', 'removed', 'under', 'random', 'and', 'various', 'intentional', 'attack', 'strategies', 'we', 'find', 'that', 'disassortative', 'networks', 'are', 'structurally', 'robust', 'against', 'random', 'attacks', 'and', 'highly', 'loadtolerant', 'while', 'assortative', 'networks', 'are', 'most', 'resistant', 'to', 'intentional', 'attacks', 'yet', 'significantly', 'fragile', 'against', 'random', 'attacks']] | [-0.14342007206287236, 0.12489722207841017, -0.025933193671517075, 0.09300010040557632, -0.03290173965506256, -0.23735415521077813, 0.035221329300353925, 0.4448058009186449, -0.25843887082786143, -0.27407069656377037, 0.03690272399884028, -0.2699839883852595, -0.305797726501684, 0.10229591122285152, -0.07817901696932192, 0.07508304270158987, -0.0037825356780861815, -0.002356536197476089, 0.05106370467886639, -0.27708326459978705, 0.33861071000768184, 0.09202626064264526, 0.39372690476399536, 0.04806273222736005, 0.004566929669817909, -0.0136430062809571, 0.0040344378290077055, 0.1044979288931548, -0.05659336538938078, 0.05116779438685626, 0.21973419694055943, 0.131885783636244, 0.2762824686884414, -0.47937755594612097, -0.32262142607942224, 0.16746018620809386, 0.1234407821611967, 0.15443787581073895, 0.004949780344031751, -0.3268774638185278, 0.1478472703155906, -0.19071974000265376, -0.08839585074456409, -0.14807458174570154, -0.0019161661931624016, 0.0772018560068318, -0.22110511019758025, 0.03381976294137227, 0.09473676542693284, 0.07829505673144013, 0.015842552667406078, -0.0982531275289754, -0.10780939485315079, 0.1415772484181313, 0.03284784958620245, -0.0476624432427343, 0.17093653332946512, -0.13866347313548127, -0.1810586543220173, 0.38241071977536195, -0.0015431874916733554, -0.18283238275907934, 0.20611720683906848, -0.041356006315133226, -0.18097054876658755, 0.1013805427084056, 0.23685182055147985, 0.07793484844344979, -0.15422906742035897, -0.03259860699175381, -0.02296302734563748, 0.1653452865468959, 0.027769318314191573, 0.0349316707191368, 0.15160963642022882, 0.19060857231379486, 0.0915593925921712, 0.14257543736991163, -0.07163907861104235, -0.1342281610161687, -0.14316575635845463, -0.02837864332056294, -0.21696344618297492, 0.05198332991579567, -0.14954322559012023, -0.20653748007801673, 0.4279586189271261, 0.1743680928174096, 0.238772081102555, 0.10699509119828386, 0.31260165668306095, 0.018083663421566597, 0.08830467822845094, 0.0905204807718595, 0.1934996110542367, 0.09858835730119608, 0.09527437034412287, -0.12164533366449178, 0.28585860467671104, -0.03638740566093475] |
710.2514 | A possible source of spin-polarized electrons: The inert
graphene/Ni(111) system | We report on an investigation of spin-polarized secondary electron emission
from the chemically inert system: graphene/Ni(111). An ordered passivated
graphene layer (monolayer of graphite, MG) was formed on Ni(111) surface via
cracking of propylene gas. The spin-polarization of the secondary electrons
obtained from this system upon photoemission is only slightly lower than the
one from the clean Ni surface, but does not change upon large oxygen exposure.
These results suggest to use such passivated Ni(111) surface as a source of
spin-polarized electrons stable against adsorption of reactive gases.
| cond-mat.mtrl-sci | we report on an investigation of spinpolarized secondary electron emission from the chemically inert system grapheneni111 an ordered passivated graphene layer monolayer of graphite mg was formed on ni111 surface via cracking of propylene gas the spinpolarization of the secondary electrons obtained from this system upon photoemission is only slightly lower than the one from the clean ni surface but does not change upon large oxygen exposure these results suggest to use such passivated ni111 surface as a source of spinpolarized electrons stable against adsorption of reactive gases | [['we', 'report', 'on', 'an', 'investigation', 'of', 'spinpolarized', 'secondary', 'electron', 'emission', 'from', 'the', 'chemically', 'inert', 'system', 'grapheneni111', 'an', 'ordered', 'passivated', 'graphene', 'layer', 'monolayer', 'of', 'graphite', 'mg', 'was', 'formed', 'on', 'ni111', 'surface', 'via', 'cracking', 'of', 'propylene', 'gas', 'the', 'spinpolarization', 'of', 'the', 'secondary', 'electrons', 'obtained', 'from', 'this', 'system', 'upon', 'photoemission', 'is', 'only', 'slightly', 'lower', 'than', 'the', 'one', 'from', 'the', 'clean', 'ni', 'surface', 'but', 'does', 'not', 'change', 'upon', 'large', 'oxygen', 'exposure', 'these', 'results', 'suggest', 'to', 'use', 'such', 'passivated', 'ni111', 'surface', 'as', 'a', 'source', 'of', 'spinpolarized', 'electrons', 'stable', 'against', 'adsorption', 'of', 'reactive', 'gases']] | [-0.08100263504853832, 0.1801342923615514, -0.02273660748985342, -0.017445741552034055, 0.03981137275695801, -0.19572374255883254, 0.12414837915408002, 0.4344448156824166, -0.25647763890976255, -0.3053596557371996, -0.06507858860475774, -0.36333370979198, -0.0613150172020224, 0.1912684604096946, -0.0010219554850746963, -0.02712074358450164, 0.04827696695098315, -0.11006962887371298, -0.07467207497790117, -0.23864509968552738, 0.2996092440496961, 0.09343072353989225, 0.3035367127211595, 0.13722176769409666, -0.014632758128837768, -0.001876025947488167, 0.11432253430955991, -0.0030259627700698647, -0.13417512766847556, 0.09890850155021656, 0.1910948637153276, -0.1116794054872695, 0.14577987091615796, -0.5620445850178261, -0.233506954444403, -0.07919706247577613, 0.12127587783404371, 0.15559250766157426, -0.12178296090198935, -0.2709907865236429, 0.039269146506161305, -0.11998225532641466, -0.08560291231101887, 0.007127842447847466, -0.06215219196482477, -0.018074188656596976, -0.18623848880154334, 0.0631288216629235, 0.0820099249077347, 0.10257329712410203, -0.1671075957896061, -0.16463150921415284, -0.201601168153998, 0.003704384180971167, 0.047606815920020876, 0.015494992734271695, 0.32190934219926765, -0.05529242594440637, -0.0003735699309882793, 0.37864339010874654, -0.1037066813635399, -0.056811153507706796, 0.25632418742911384, -0.1690048356487585, -0.07279629873598671, 0.2597902880515903, 0.10379549757238817, 0.183836478094401, -0.1350249319961718, 0.03346080890729685, -0.07761354486997747, 0.23202691455265845, 0.1063842437103052, 0.01026206301916814, 0.26851944344194967, 0.20798681462077762, 0.09761476840569892, 0.10402521488140337, -0.1595234391649931, 0.057308130484836343, -0.15849574439396913, -0.2509650146186521, -0.2196193576700435, 0.09801455064354575, -0.0059123532846570015, -0.22112334514862264, 0.3402036545078524, 0.047240438558880916, 0.14673836747269062, -0.1058266723465005, 0.2785687880082564, 0.052018133842714386, 0.02573638403026218, 0.01773779633433812, 0.23117503966204822, 0.14842662985955196, 0.0650874869368801, -0.258782835933909, 0.16232307908781382, 0.009621953718702902] |
710.2515 | Superposition of fields of two Reissner - Nordstrom sources | In this paper we present a 5-parametric family of static asymptotically flat
solutions for the superposed gravitational and electromagnetic fields of two
Reissner-Nordstr\"om sources with arbitrary parameters -- masses, charges and
separating distance. A procedure for solving of the linear singular integral
equation form of the electrovacuum Einstein - Maxwell equations for stationary
axisymmetric fields is described in detail. The 4-parametric family of
equilibrium configurations of two Reissner-Nordstr\"om sources (one of which
should be a black hole and another one -- a naked singularity) presented in our
recent paper \cite{Alekseev-Belinski:2007} arises after a restriction of the
parameters of the 5-parametric solution presented here by the equilibrium
condition which provides the absence in the solution of conical points on the
symmetry axis between the sources.
| gr-qc | in this paper we present a 5parametric family of static asymptotically flat solutions for the superposed gravitational and electromagnetic fields of two reissnernordstrom sources with arbitrary parameters masses charges and separating distance a procedure for solving of the linear singular integral equation form of the electrovacuum einstein maxwell equations for stationary axisymmetric fields is described in detail the 4parametric family of equilibrium configurations of two reissnernordstrom sources one of which should be a black hole and another one a naked singularity presented in our recent paper citealekseevbelinski2007 arises after a restriction of the parameters of the 5parametric solution presented here by the equilibrium condition which provides the absence in the solution of conical points on the symmetry axis between the sources | [['in', 'this', 'paper', 'we', 'present', 'a', '5parametric', 'family', 'of', 'static', 'asymptotically', 'flat', 'solutions', 'for', 'the', 'superposed', 'gravitational', 'and', 'electromagnetic', 'fields', 'of', 'two', 'reissnernordstrom', 'sources', 'with', 'arbitrary', 'parameters', 'masses', 'charges', 'and', 'separating', 'distance', 'a', 'procedure', 'for', 'solving', 'of', 'the', 'linear', 'singular', 'integral', 'equation', 'form', 'of', 'the', 'electrovacuum', 'einstein', 'maxwell', 'equations', 'for', 'stationary', 'axisymmetric', 'fields', 'is', 'described', 'in', 'detail', 'the', '4parametric', 'family', 'of', 'equilibrium', 'configurations', 'of', 'two', 'reissnernordstrom', 'sources', 'one', 'of', 'which', 'should', 'be', 'a', 'black', 'hole', 'and', 'another', 'one', 'a', 'naked', 'singularity', 'presented', 'in', 'our', 'recent', 'paper', 'citealekseevbelinski2007', 'arises', 'after', 'a', 'restriction', 'of', 'the', 'parameters', 'of', 'the', '5parametric', 'solution', 'presented', 'here', 'by', 'the', 'equilibrium', 'condition', 'which', 'provides', 'the', 'absence', 'in', 'the', 'solution', 'of', 'conical', 'points', 'on', 'the', 'symmetry', 'axis', 'between', 'the', 'sources']] | [-0.19856304471225789, 0.06637290341313928, -0.09478546337729009, 0.06102142288194348, -0.07426392748796691, -0.12770246864723353, -0.013786299899220467, 0.2897475225307668, -0.19387984092657765, -0.2529654981131898, 0.10412820433654511, -0.2925932701677084, -0.1051022769495224, 0.17240363292900535, -0.012815013252353917, 0.04996546498441603, 0.01798072556848638, 0.022825389580490688, -0.10364407575495231, -0.20506114237941803, 0.42391949609542884, 0.01223365902066386, 0.2344746704174516, -0.02342800535261631, 0.13869852201314642, -0.012310697118906925, 0.03097663914571361, 0.06150319431520378, -0.13907719242852182, 0.07497608822692807, 0.21987817744957283, 0.09499838423798793, 0.2172826655752336, -0.39769098865799607, -0.19300721412679803, 0.10136570337538918, 0.1318266629978704, 0.15027188084980783, -0.09198868466094913, -0.2838853558059782, 0.060658895849095035, -0.1395112675537045, -0.2552767969939547, -0.00876181696075946, 0.044328852409186464, 0.019750746001955123, -0.2566925660755563, 0.09940353586959343, 0.092422978124038, -0.009956928626828206, -0.15631952679638442, -0.06398313593041773, -0.03034064099774696, 0.06029692617109201, 0.1044576749089174, 0.02109013682541748, 0.09989260720418922, -0.11496947924412476, -0.10024483783636243, 0.36175763215190576, -0.057254704237372306, -0.26036216200639806, 0.12514129039773253, -0.14654975185791652, -0.09155049411541162, 0.13691577638383023, 0.13253396517053867, 0.2118122962769121, -0.1834920883256321, 0.13597678907929853, -0.02877121577815463, 0.11510538881799827, 0.12392650383990259, 0.0171197994844988, 0.29223005259409546, 0.08191044786944986, 0.06003442357759923, 0.17997467683065527, -0.04625556666675645, -0.1271899318865811, -0.3705892243733009, -0.1416811156901531, -0.1415109609020874, 0.10977229021955281, -0.13923698462749598, -0.22585818104998906, 0.3846934077388141, 0.0824385003807644, 0.1480215483965973, 0.002428063309829061, 0.2535312667450247, 0.09773243994568474, -0.009384009657272449, 0.1033408455143217, 0.30397931510427345, 0.12409313492826186, 0.10810841650624449, -0.19609704558194305, -0.06226442524445398, 0.10228450215266396] |
710.2516 | Are there compact heavy four-quark bound states? | We present an exact method to study four-quark systems based on the
hyperspherical harmonics formalism. We apply it to several physical systems of
interest containing two heavy and two light quarks using different quark-quark
potentials. Our conclusions mark the boundaries for the possible existence of
compact, non-molecular, four-quark bound states. While $QQ\bar n \bar n$ states
may be stable in nature, the stability of $Q\bar Qn \bar n$ states would imply
the existence of quark correlations not taken into account by simple quark
dynamical models
| hep-ph hep-ex nucl-th | we present an exact method to study fourquark systems based on the hyperspherical harmonics formalism we apply it to several physical systems of interest containing two heavy and two light quarks using different quarkquark potentials our conclusions mark the boundaries for the possible existence of compact nonmolecular fourquark bound states while qqbar n bar n states may be stable in nature the stability of qbar qn bar n states would imply the existence of quark correlations not taken into account by simple quark dynamical models | [['we', 'present', 'an', 'exact', 'method', 'to', 'study', 'fourquark', 'systems', 'based', 'on', 'the', 'hyperspherical', 'harmonics', 'formalism', 'we', 'apply', 'it', 'to', 'several', 'physical', 'systems', 'of', 'interest', 'containing', 'two', 'heavy', 'and', 'two', 'light', 'quarks', 'using', 'different', 'quarkquark', 'potentials', 'our', 'conclusions', 'mark', 'the', 'boundaries', 'for', 'the', 'possible', 'existence', 'of', 'compact', 'nonmolecular', 'fourquark', 'bound', 'states', 'while', 'qqbar', 'n', 'bar', 'n', 'states', 'may', 'be', 'stable', 'in', 'nature', 'the', 'stability', 'of', 'qbar', 'qn', 'bar', 'n', 'states', 'would', 'imply', 'the', 'existence', 'of', 'quark', 'correlations', 'not', 'taken', 'into', 'account', 'by', 'simple', 'quark', 'dynamical', 'models']] | [-0.11866264385445154, 0.21623922749302651, -0.14893630058230722, 0.11117965866099386, -0.01918822799480575, -0.14810820537044064, 0.05496926121961544, 0.32334777410416043, -0.16265952889533603, -0.21276725500493365, -0.03038019459174179, -0.27712859192534406, -0.05349164526526104, 0.12026147303335807, 0.06609185334356667, 0.07790917723494417, 0.06682136630749001, 0.007789002698572243, -0.046632699362303624, -0.24830220430431998, 0.3732013634625165, -0.11243027330321424, 0.17817129210897667, 0.1318612503736992, -0.015593814384192228, 0.01579323351273642, 0.02475197367808398, -0.08671731139149735, -0.07019859551835586, 0.0696701402125387, 0.20183005432982634, 0.10826484650263891, 0.17470188793890618, -0.44708317875423853, -0.17449004909242777, 0.12069317642051508, 0.17840596179560045, 0.13274075761574375, -0.03762643337934552, -0.3312620370320099, 0.0904541107442449, -0.19385993206490051, -0.2058209782521076, -0.15689121046487023, 0.06455016190953114, -0.04401200448970913, -0.30236651810324366, 0.05558381413712221, 0.06032924908316037, -0.02573776435764397, -0.07046562225612647, -0.2208730347564115, -0.05398470001082922, 0.08174721003126573, 0.023774512631216032, 0.01694204202195739, 0.11610367340035736, -0.11361778941662873, -0.13388913043172043, 0.38608558335724996, -0.05398451394867152, -0.2197899991317707, 0.22001311040812116, -0.12828094655209604, -0.14570370561936322, 0.11370985210489701, 0.21594035335104256, 0.13353218389127183, -0.1493146562784472, 0.08146898256655892, -0.035367753652527055, 0.16104347854852677, 0.09734510994132828, 0.1047907308291863, 0.2248396605342243, 0.12725856218706158, -0.03083549202145899, 0.09075277146253297, -0.021942569498958835, -0.12854277829105473, -0.356563182733953, -0.09774147459097816, -0.14721693860038237, 0.05516284035042832, -0.09219545014185475, -0.14699377012165155, 0.3864862157141461, 0.09763337159666288, 0.22350884730763296, -0.0171183619155165, 0.2636153060504619, 0.06907180703710765, 0.0411991706391906, 0.10508414842188359, 0.26073405775515474, 0.21048725087688688, 0.03845470097080311, -0.27371322497287215, 0.012747752874651377, 0.10699966853374944] |
710.2517 | Gluon Saturation and Black Hole Criticality | We discuss the recent proposal in hep-th/0611312 where it was shown that the
critical anomalous dimension associated to the onset of non-linear effects in
the high energy limit of QCD coincides with the critical exponent governing the
radius of the black hole formed in the spherically symmetric collapse of a
massless scalar field. We argue that a new essential ingredient in this mapping
between gauge theory and gravity is continuous self-similarity, not present in
the scalar field case but in the spherical collapse of a perfect fluid with
barotropic equation of state. We identify this property with geometric scaling,
present in DIS data at small values of Bjorken x. We also show that the
Choptuik exponent in dimension five tends to the QCD critical value in the
traceless limit of the energy momentum tensor.
| hep-th | we discuss the recent proposal in hepth0611312 where it was shown that the critical anomalous dimension associated to the onset of nonlinear effects in the high energy limit of qcd coincides with the critical exponent governing the radius of the black hole formed in the spherically symmetric collapse of a massless scalar field we argue that a new essential ingredient in this mapping between gauge theory and gravity is continuous selfsimilarity not present in the scalar field case but in the spherical collapse of a perfect fluid with barotropic equation of state we identify this property with geometric scaling present in dis data at small values of bjorken x we also show that the choptuik exponent in dimension five tends to the qcd critical value in the traceless limit of the energy momentum tensor | [['we', 'discuss', 'the', 'recent', 'proposal', 'in', 'hepth0611312', 'where', 'it', 'was', 'shown', 'that', 'the', 'critical', 'anomalous', 'dimension', 'associated', 'to', 'the', 'onset', 'of', 'nonlinear', 'effects', 'in', 'the', 'high', 'energy', 'limit', 'of', 'qcd', 'coincides', 'with', 'the', 'critical', 'exponent', 'governing', 'the', 'radius', 'of', 'the', 'black', 'hole', 'formed', 'in', 'the', 'spherically', 'symmetric', 'collapse', 'of', 'a', 'massless', 'scalar', 'field', 'we', 'argue', 'that', 'a', 'new', 'essential', 'ingredient', 'in', 'this', 'mapping', 'between', 'gauge', 'theory', 'and', 'gravity', 'is', 'continuous', 'selfsimilarity', 'not', 'present', 'in', 'the', 'scalar', 'field', 'case', 'but', 'in', 'the', 'spherical', 'collapse', 'of', 'a', 'perfect', 'fluid', 'with', 'barotropic', 'equation', 'of', 'state', 'we', 'identify', 'this', 'property', 'with', 'geometric', 'scaling', 'present', 'in', 'dis', 'data', 'at', 'small', 'values', 'of', 'bjorken', 'x', 'we', 'also', 'show', 'that', 'the', 'choptuik', 'exponent', 'in', 'dimension', 'five', 'tends', 'to', 'the', 'qcd', 'critical', 'value', 'in', 'the', 'traceless', 'limit', 'of', 'the', 'energy', 'momentum', 'tensor']] | [-0.159050118977281, 0.16870976098694077, -0.10055563285512696, 0.058421157809023405, -0.0428008145934559, -0.09272206311737348, -0.015558082082560916, 0.2839648713098657, -0.2020055980708702, -0.22863559874432876, 0.05322944231881039, -0.2613683382917504, -0.13729297847459024, 0.12669601578517517, 0.0010182582208697678, 0.0658480680427957, -0.02829334978364352, 0.08642328508667424, -0.09420883301181607, -0.20804867174133265, 0.4068906905262598, 0.038079888846977314, 0.28093254018602964, 0.06838797735614016, 0.09542788492071029, -0.010993462006904577, 0.002616266306853832, 0.04429791043197414, -0.1762066384824146, 0.03751315914542604, 0.21721642071825864, 0.0421581329608028, 0.21938798512171084, -0.373176944435091, -0.21987732431301638, 0.11396648253041103, 0.13795969338520409, 0.10998793354798879, -0.050013023321175444, -0.23091276250324472, 0.08838000664963647, -0.18704209286068335, -0.21743698335949443, -0.05190615966579968, 0.04435753301083621, -0.026441556317521667, -0.2620222087760449, 0.1499952868498508, 0.05231912115753341, -0.0028546934779313275, -0.09403923726500593, -0.07468484421925885, -0.03740904852397796, 0.05967117112683118, 0.10825313627544819, 0.06301091277019534, 0.1021404188595488, -0.2062247978992536, -0.070533548067744, 0.38232278120108787, -0.08126724404948098, -0.19312825475826412, 0.14422600231784627, -0.24609512080616996, -0.14506604887993263, 0.12270963942646083, 0.1494665494874904, 0.11816266071247428, -0.09244614739823978, 0.14077577279850884, -0.03690062111674255, 0.16616990110098168, 0.056122707448115476, 0.021708251803385138, 0.22498796531524426, 0.15109574355016975, 0.027851139429844636, 0.15388201297561926, -0.06331171933605328, -0.13888857499661303, -0.37215045805236224, -0.1619499427497499, -0.18216452737779995, 0.11863743167913683, -0.16811796250441058, -0.17515421649716845, 0.3369998135989098, 0.15944126836913533, 0.19621691491614146, 0.02775406293199867, 0.24282001449089302, 0.1253659983788778, 0.05155334641274653, 0.11459834130368847, 0.3035787830542409, 0.1617953135540947, 0.14779760924349994, -0.24716415184136845, -0.041642653387341, 0.10503141209833268] |
710.2518 | Variations of the high-level Balmer line spectrum of the helium-strong
star Sigma Orionis E | Using the high-level Balmer lines and continuum, we trace the density
structure of two magnetospheric disk segments of the prototypical Bp star sigma
Ori E (B2p) as these segments occult portions of the star during the rotational
cycle. High-resolution spectra of the Balmer lines >H9 and Balmer edge were
obtained on seven nights in January-February 2007 at an average sampling of
0.01 cycles. We measured equivalent width variations due to the star
occultations by two disk segments 0.4 cycles apart and constructed differential
spectra of the migrations of the corresponding absorptions across the Balmer
line profiles. We first estimated the rotational and magnetic obliquity angles.
We then simulated the observed Balmer jump variation using the model atmosphere
codes synspec/circus and evaluated the disk geometry and gas thermodynamics. We
find that the two occultations are caused by two disk segments. The first of
these transits quickly, indicating that the segment resides in a range of
distances, perhaps 2.5-6R_star, from the star. The second consists of a more
slowly moving segment situated closer to the surface and causing two
semi-resolved absorbing maxima. During its transit this segment brushes across
the star's "lower" limb. Judging from the line visibility up to H23-H24 during
the occultations, both disk segments have mean densities near 10^{12} cm^{-3}
and are opaque in the lines and continuum. They have semiheights less than 1/2
of a stellar radius, and their temperatures are near 10500K and 12000K,
respectively. In all, the disks of Bp stars have a much more complicated
geometry than has been anticipated, as evidenced by their (sometimes)
non-coplanarity, de-centerness, and from star to star, differences in disk
height.
| astro-ph | using the highlevel balmer lines and continuum we trace the density structure of two magnetospheric disk segments of the prototypical bp star sigma ori e b2p as these segments occult portions of the star during the rotational cycle highresolution spectra of the balmer lines h9 and balmer edge were obtained on seven nights in januaryfebruary 2007 at an average sampling of 001 cycles we measured equivalent width variations due to the star occultations by two disk segments 04 cycles apart and constructed differential spectra of the migrations of the corresponding absorptions across the balmer line profiles we first estimated the rotational and magnetic obliquity angles we then simulated the observed balmer jump variation using the model atmosphere codes synspeccircus and evaluated the disk geometry and gas thermodynamics we find that the two occultations are caused by two disk segments the first of these transits quickly indicating that the segment resides in a range of distances perhaps 256r_star from the star the second consists of a more slowly moving segment situated closer to the surface and causing two semiresolved absorbing maxima during its transit this segment brushes across the stars lower limb judging from the line visibility up to h23h24 during the occultations both disk segments have mean densities near 1012 cm3 and are opaque in the lines and continuum they have semiheights less than 12 of a stellar radius and their temperatures are near 10500k and 12000k respectively in all the disks of bp stars have a much more complicated geometry than has been anticipated as evidenced by their sometimes noncoplanarity decenterness and from star to star differences in disk height | [['using', 'the', 'highlevel', 'balmer', 'lines', 'and', 'continuum', 'we', 'trace', 'the', 'density', 'structure', 'of', 'two', 'magnetospheric', 'disk', 'segments', 'of', 'the', 'prototypical', 'bp', 'star', 'sigma', 'ori', 'e', 'b2p', 'as', 'these', 'segments', 'occult', 'portions', 'of', 'the', 'star', 'during', 'the', 'rotational', 'cycle', 'highresolution', 'spectra', 'of', 'the', 'balmer', 'lines', 'h9', 'and', 'balmer', 'edge', 'were', 'obtained', 'on', 'seven', 'nights', 'in', 'januaryfebruary', '2007', 'at', 'an', 'average', 'sampling', 'of', '001', 'cycles', 'we', 'measured', 'equivalent', 'width', 'variations', 'due', 'to', 'the', 'star', 'occultations', 'by', 'two', 'disk', 'segments', '04', 'cycles', 'apart', 'and', 'constructed', 'differential', 'spectra', 'of', 'the', 'migrations', 'of', 'the', 'corresponding', 'absorptions', 'across', 'the', 'balmer', 'line', 'profiles', 'we', 'first', 'estimated', 'the', 'rotational', 'and', 'magnetic', 'obliquity', 'angles', 'we', 'then', 'simulated', 'the', 'observed', 'balmer', 'jump', 'variation', 'using', 'the', 'model', 'atmosphere', 'codes', 'synspeccircus', 'and', 'evaluated', 'the', 'disk', 'geometry', 'and', 'gas', 'thermodynamics', 'we', 'find', 'that', 'the', 'two', 'occultations', 'are', 'caused', 'by', 'two', 'disk', 'segments', 'the', 'first', 'of', 'these', 'transits', 'quickly', 'indicating', 'that', 'the', 'segment', 'resides', 'in', 'a', 'range', 'of', 'distances', 'perhaps', '256r_star', 'from', 'the', 'star', 'the', 'second', 'consists', 'of', 'a', 'more', 'slowly', 'moving', 'segment', 'situated', 'closer', 'to', 'the', 'surface', 'and', 'causing', 'two', 'semiresolved', 'absorbing', 'maxima', 'during', 'its', 'transit', 'this', 'segment', 'brushes', 'across', 'the', 'stars', 'lower', 'limb', 'judging', 'from', 'the', 'line', 'visibility', 'up', 'to', 'h23h24', 'during', 'the', 'occultations', 'both', 'disk', 'segments', 'have', 'mean', 'densities', 'near', '1012', 'cm3', 'and', 'are', 'opaque', 'in', 'the', 'lines', 'and', 'continuum', 'they', 'have', 'semiheights', 'less', 'than', '12', 'of', 'a', 'stellar', 'radius', 'and', 'their', 'temperatures', 'are', 'near', '10500k', 'and', '12000k', 'respectively', 'in', 'all', 'the', 'disks', 'of', 'bp', 'stars', 'have', 'a', 'much', 'more', 'complicated', 'geometry', 'than', 'has', 'been', 'anticipated', 'as', 'evidenced', 'by', 'their', 'sometimes', 'noncoplanarity', 'decenterness', 'and', 'from', 'star', 'to', 'star', 'differences', 'in', 'disk', 'height']] | [-0.08098718858804532, 0.11992827854019676, -0.04256441562674604, 0.06607847859517538, -0.031013823651771685, -0.08618289147699743, 0.0594015731006866, 0.4562522705742403, -0.20634043474394576, -0.3475125890213793, 0.08257162976787685, -0.3085384668810363, -0.03837734198152207, 0.18343468049026437, -0.04648898505952377, -0.01801707985775048, 0.07029884446174242, -0.03955365999455606, -0.060307614543366674, -0.21197113413687557, 0.2611476861192544, 0.038231263669816905, 0.1352823035418637, -0.007996110556755719, 0.019392725706531114, -0.09214189574708882, -0.04643189034834364, 0.009562241134086722, -0.16148803521437208, 0.0725030085295999, 0.19165968750708534, 0.09904910141297553, 0.18850116301905645, -0.40814436193996745, -0.20777682951980628, 0.03378906555270734, 0.15528634086048188, 0.02998055925214649, 0.03120458816583846, -0.268901972921173, 0.05632055516151669, -0.11257121210464423, -0.12615762102239086, 0.07741295182145257, 0.09730490805105046, 0.01483325520530343, -0.19315547815325348, 0.07120063292611867, 0.04818769041238759, 0.15006941852520422, -0.08974791953298158, -0.11361545999359368, -0.12518295899289136, 0.11769254389744167, 0.036519403507691436, 0.03299408363129355, 0.1912553224562058, -0.1063028370245549, -0.031522407693634354, 0.3795712140906966, -0.09991167650850843, -0.022126525187080626, 0.21650312047738834, -0.217905774090222, -0.11770987146029852, 0.23724175724235916, 0.13913682552537693, 0.14740683659394727, -0.11261265000168241, -0.018847271445543413, -0.0118499583628377, 0.17708591665876539, 0.1401278788969621, -0.002384473228322944, 0.3380371045664345, 0.05026939971927427, 0.015127821473135171, 0.11892042297338612, -0.2752368178917095, -0.08254940010155586, -0.21877493970866377, -0.09721732639910695, -0.117046999665856, 0.022232002677585006, -0.11383590042259355, -0.1433564606455288, 0.38316635210487177, 0.08788663548718494, 0.2532624409681088, 0.04521755006425153, 0.28560209961930166, 0.11129685104001817, 0.09158163479331502, 0.1374937196479256, 0.28124638503291327, 0.1726324575413999, 0.098672249328163, -0.22679325367756892, 0.08972715091877582, 0.019633091209676025] |
710.2519 | Using $K^0\pi^-\to\pi^-$ transitions to compute $K\to(\pi\pi)_{I=0}$
decay amplitudes at NLO in the chiral expansion | It is proposed to compute matrix elements for the (unphysical) $K^0\pi^-\to
\pi^-$ transition to determine the next-to-leading order low energy constants
of the weak chiral Lagrangian. This allows us to evaluate $K\to(\pi\pi)_{I=0}$
decay amplitudes at this level of precision. This approach has several
significant advantages over the use of $K\to\pi\pi$ transitions, most notably
the elimination of s-channel disconnected diagrams and the use of fewer
inversions.
| hep-lat | it is proposed to compute matrix elements for the unphysical k0pito pi transition to determine the nexttoleading order low energy constants of the weak chiral lagrangian this allows us to evaluate ktopipi_i0 decay amplitudes at this level of precision this approach has several significant advantages over the use of ktopipi transitions most notably the elimination of schannel disconnected diagrams and the use of fewer inversions | [['it', 'is', 'proposed', 'to', 'compute', 'matrix', 'elements', 'for', 'the', 'unphysical', 'k0pito', 'pi', 'transition', 'to', 'determine', 'the', 'nexttoleading', 'order', 'low', 'energy', 'constants', 'of', 'the', 'weak', 'chiral', 'lagrangian', 'this', 'allows', 'us', 'to', 'evaluate', 'ktopipi_i0', 'decay', 'amplitudes', 'at', 'this', 'level', 'of', 'precision', 'this', 'approach', 'has', 'several', 'significant', 'advantages', 'over', 'the', 'use', 'of', 'ktopipi', 'transitions', 'most', 'notably', 'the', 'elimination', 'of', 'schannel', 'disconnected', 'diagrams', 'and', 'the', 'use', 'of', 'fewer', 'inversions']] | [-0.11444416129222465, 0.14751588591625767, -0.07895877748905193, 0.07350943554266696, -0.08918128770569132, -0.07169747367382996, 0.10251932771551231, 0.32521523008980446, -0.22077458034942132, -0.28326696281631786, 0.01580699632639095, -0.2872337943780521, -0.10721476628844227, 0.1032984039879271, 0.028026155890926482, 0.07073752101813813, 0.04336433063098599, 0.055991463673611484, -0.12150850000750599, -0.22311619639633193, 0.2852270547596235, 0.016026825525812687, 0.23650146090972518, 0.10546498263018235, 0.06466740533886921, 0.007525340361993701, -0.05767382875025746, -0.07755997507936424, -0.12772172624393116, 0.12878919099014075, 0.2632955985055083, 0.07062396809222206, 0.18844937224916758, -0.3812944819736812, -0.1492127935690362, 0.12171486446944375, 0.150751300082202, 0.15265805527405252, 0.046595476907751864, -0.23028649416722594, 0.13691565824583882, -0.20031436878655637, -0.15572217422803597, -0.18942833835599088, 0.008262619080524596, -0.08190315031993484, -0.28437703370027956, 0.02474425815134531, -0.011814352028840592, 0.03380457311129523, 0.048724673986841466, -0.18030865670048765, 0.0106833082446385, 0.14668365980365447, 0.08619556243028788, 0.029067777713025284, 0.0956630167802648, -0.12953993848731488, -0.11986625889345767, 0.3792283942087716, -0.06905179923318977, -0.14760217203256037, 0.17230228207532375, -0.156449926972744, -0.15877003450360563, 0.2418239626161281, 0.16482305408470213, 0.11447366989321178, -0.14090117089272963, 0.12746160287023817, 0.03982148624010502, 0.15014748304661008, 0.1173830606146819, 0.04240223426105721, 0.1227009344313826, 0.1063152061006616, 0.03712934753783639, 0.0903025438181228, -0.09657106232932872, -0.12278618747811942, -0.3508969892762483, -0.14852102177720222, -0.10539156076542679, 0.0030686823089444448, -0.11170195582639685, -0.1808849591096597, 0.42026388445602997, 0.2044545393732805, 0.20015076262689757, 0.03679330451857476, 0.35048665041990934, 0.15035735951766135, 0.11654318458888502, 0.015350686334487464, 0.25837318971013973, 0.21523742439846197, 0.05037634934867836, -0.29463779992083944, 0.02478157429510565, 0.06562803708578623] |
710.252 | The equation of state with nonzero chemical potential for 2+1 flavors | We present results for the QCD equation of state with nonzero chemical
potential using the Taylor expansion method with terms up to sixth order in the
expansion. Our calculations are performed on asqtad 2+1 quark flavor lattices
at $N_t=4$.
| hep-lat | we present results for the qcd equation of state with nonzero chemical potential using the taylor expansion method with terms up to sixth order in the expansion our calculations are performed on asqtad 21 quark flavor lattices at n_t4 | [['we', 'present', 'results', 'for', 'the', 'qcd', 'equation', 'of', 'state', 'with', 'nonzero', 'chemical', 'potential', 'using', 'the', 'taylor', 'expansion', 'method', 'with', 'terms', 'up', 'to', 'sixth', 'order', 'in', 'the', 'expansion', 'our', 'calculations', 'are', 'performed', 'on', 'asqtad', '21', 'quark', 'flavor', 'lattices', 'at', 'n_t4']] | [-0.06317904541412225, 0.16939970429461354, -0.11069182556074782, -0.041698017181494296, -0.02379456711694216, -0.011306739340607937, 0.1034040752117737, 0.3713502039034397, -0.1419854390506561, -0.2665144627292951, 0.08916747428846951, -0.3292068897340542, -0.024736212709775336, 0.09856639235901336, 0.14407473016912356, 0.10954179395085727, 0.08878715056926012, 0.030022064307465766, -0.16163380260173327, -0.3427162629385025, 0.325009574689783, -0.00015038514557557227, 0.18472637496411037, 0.14047692954922333, 0.06690781793963069, -0.09191777801905306, -0.06337071157609805, -0.05634466725855301, -0.13800936004815575, 0.08991459222176136, 0.13721002348047945, -0.06816969340285048, 0.13545748686943299, -0.3897994376050356, -0.19765848054502827, 0.05217532309679649, 0.11263320903078868, 0.168337825494699, -0.022050102638343397, -0.27371249271508974, 0.1244672130411252, -0.2192299409220234, -0.22788529119525963, -0.24135988821777013, -0.07411287295130584, -0.015609312324951857, -0.33500882792167175, 0.12480745832316387, -0.09334611105255018, 0.09314664011915925, -0.019410388759122446, -0.25158251229769146, 0.009296785819177061, 0.04821967968764978, 0.016528397034376096, 0.10732896821812177, 0.038604135756404735, -0.13643443859062898, -0.1740771083949277, 0.5034431106387041, -0.15591392061040282, -0.1781599735124753, 0.1494476902179229, -0.22705982609962425, -0.15494628848794562, 0.09989418767583676, 0.18132519776909015, 0.08988020570280078, -0.11864818131121305, 0.11388943396890774, 0.011465493016518079, 0.16885277428306067, 0.13219781937555242, -0.04079402276338675, 0.169538227459177, 0.14777902783587193, -0.039499347435477644, 0.06375503566904137, -0.015785129758744285, -0.14746557345661598, -0.35908572480846673, -0.04208881683790913, -0.18443420445785308, 0.041750438475551516, -0.18189770495519042, -0.14266260724681884, 0.40380434782650226, 0.17686537359482968, 0.13688282573070282, 0.026066982760452308, 0.25733854153599495, 0.13851633733914545, 0.05866187630006327, 0.08007527899164228, 0.20724037358871636, 0.16928681148550448, 0.18795316882479268, -0.32770324909152126, -0.1250308159714899, 0.224771831686107] |
710.2521 | A formula for the coincidence Reidemeister trace of selfmaps on bouquets
of circles | We give a formula for the coincidence Reidemeister trace of selfmaps on
bouquets of circles in terms of the Fox calculus. Our formula reduces the
problem of computing the coincidence Reidemeister trace to the problem of
distinguishing doubly twisted conjugacy classes in free groups.
| math.GN math.AT | we give a formula for the coincidence reidemeister trace of selfmaps on bouquets of circles in terms of the fox calculus our formula reduces the problem of computing the coincidence reidemeister trace to the problem of distinguishing doubly twisted conjugacy classes in free groups | [['we', 'give', 'a', 'formula', 'for', 'the', 'coincidence', 'reidemeister', 'trace', 'of', 'selfmaps', 'on', 'bouquets', 'of', 'circles', 'in', 'terms', 'of', 'the', 'fox', 'calculus', 'our', 'formula', 'reduces', 'the', 'problem', 'of', 'computing', 'the', 'coincidence', 'reidemeister', 'trace', 'to', 'the', 'problem', 'of', 'distinguishing', 'doubly', 'twisted', 'conjugacy', 'classes', 'in', 'free', 'groups']] | [-0.1991079728203741, 0.05097713209265335, -0.06344982893841172, 0.12336956832388585, -0.09300131621685895, -0.08307606956540523, 0.06200620598710058, 0.27144883725453506, -0.3163225640627471, -0.33018352489241143, 0.03845957925395024, -0.28582132641564717, -0.0764255687403916, 0.1986688363619826, -0.16109011438675225, -0.010403008983385835, 0.06093508136241739, 0.07912499668203633, -0.1185117107392712, -0.23977046917107972, 0.401621910574084, -0.03212509558282115, 0.17929907320913943, 0.10490256297436479, 0.09783574569420042, 0.01790867329956117, -0.09260650631040335, -0.037414606628854846, -0.16077752600804987, 0.18346645775653253, 0.2435930889438499, 0.13552388834465423, 0.16678292918103663, -0.3855747946284034, -0.11023221743843434, 0.2109800435560332, 0.12225746110462668, 0.011923063292422077, -0.034399689045544204, -0.29385585498742084, 0.05339473877525465, -0.1630033501000567, -0.1511404275343838, -0.006950408516621048, 0.060280591757460075, 0.021508943924511022, -0.1444350541992621, 0.03637402498332614, 0.06605213575742462, 0.0637161594349891, -0.07290501751809973, -0.06562512274831533, 0.04043344186555425, 0.15209259786008095, 0.06387835563245145, -0.015802638700485906, 0.07861524042461744, -0.1368427757935768, -0.18405657020312818, 0.3725625313818455, -0.039268629075112665, -0.2383659190328961, 0.06559820676391775, -0.15372042751617052, -0.24824242945760489, 0.17034880596805702, 0.02746325400022959, 0.2118615051308139, -0.038448471152646976, 0.17249216990206728, -0.16103452213362537, 0.031226924736984074, 0.21634050306271424, -0.04366053395311941, 0.1146726063452661, -0.020847049287774345, 0.1249193167948926, 0.2812877614474432, 0.002773442374415357, -0.04746269654821266, -0.36761120799928904, -0.297284799866082, -0.10446910028853877, 0.06974231399892067, -0.13303901711267166, -0.2562934100384485, 0.4273378377018327, 0.04537978041282093, 0.1267519493544982, 0.19929259391078216, 0.22410651467825202, 0.1297120180494279, 0.08639788818122311, 0.01098706559489735, 0.08709100705825469, 0.2528479386184534, -0.013355856602588161, -0.20935428618792107, 0.01817024747883393, 0.3112894679758359] |
710.2522 | Unconventional interaction between vortices in a polarized Fermi gas | Recently, a homogeneous superfluid state with a single gapless Fermi surface
was predicted to be the ground state of an ultracold Fermi gas with spin
population imbalance in the regime of molecular Bose-Einstein condensation. We
study vortices in this novel state using a symmetry-based effective field
theory, which captures the low-energy physics of gapless fermions and
superfluid phase fluctuations. This theory is applicable to all spin-imbalanced
ultracold Fermi gases in the superfluid regime, regardless of whether the
original fermion pairing interaction is weak or strong. We find a remarkable,
unconventional form of the interaction between vortices. The presence of
gapless fermions gives rise to a spatially oscillating potential, akin to the
RKKY indirect-exchange interaction in non-magnetic metals. We compare the
parameters of the effective theory to the experimentally measurable quantities
and further discuss the conditions for the verification of the predicted new
feature. Our study opens up an interesting question as to the nature of the
vortex lattice resulting from the competition between the usual repulsive
logarithmic (2D Coulomb) and predominantly attractive fermion-induced
interactions.
| cond-mat.supr-con cond-mat.other | recently a homogeneous superfluid state with a single gapless fermi surface was predicted to be the ground state of an ultracold fermi gas with spin population imbalance in the regime of molecular boseeinstein condensation we study vortices in this novel state using a symmetrybased effective field theory which captures the lowenergy physics of gapless fermions and superfluid phase fluctuations this theory is applicable to all spinimbalanced ultracold fermi gases in the superfluid regime regardless of whether the original fermion pairing interaction is weak or strong we find a remarkable unconventional form of the interaction between vortices the presence of gapless fermions gives rise to a spatially oscillating potential akin to the rkky indirectexchange interaction in nonmagnetic metals we compare the parameters of the effective theory to the experimentally measurable quantities and further discuss the conditions for the verification of the predicted new feature our study opens up an interesting question as to the nature of the vortex lattice resulting from the competition between the usual repulsive logarithmic 2d coulomb and predominantly attractive fermioninduced interactions | [['recently', 'a', 'homogeneous', 'superfluid', 'state', 'with', 'a', 'single', 'gapless', 'fermi', 'surface', 'was', 'predicted', 'to', 'be', 'the', 'ground', 'state', 'of', 'an', 'ultracold', 'fermi', 'gas', 'with', 'spin', 'population', 'imbalance', 'in', 'the', 'regime', 'of', 'molecular', 'boseeinstein', 'condensation', 'we', 'study', 'vortices', 'in', 'this', 'novel', 'state', 'using', 'a', 'symmetrybased', 'effective', 'field', 'theory', 'which', 'captures', 'the', 'lowenergy', 'physics', 'of', 'gapless', 'fermions', 'and', 'superfluid', 'phase', 'fluctuations', 'this', 'theory', 'is', 'applicable', 'to', 'all', 'spinimbalanced', 'ultracold', 'fermi', 'gases', 'in', 'the', 'superfluid', 'regime', 'regardless', 'of', 'whether', 'the', 'original', 'fermion', 'pairing', 'interaction', 'is', 'weak', 'or', 'strong', 'we', 'find', 'a', 'remarkable', 'unconventional', 'form', 'of', 'the', 'interaction', 'between', 'vortices', 'the', 'presence', 'of', 'gapless', 'fermions', 'gives', 'rise', 'to', 'a', 'spatially', 'oscillating', 'potential', 'akin', 'to', 'the', 'rkky', 'indirectexchange', 'interaction', 'in', 'nonmagnetic', 'metals', 'we', 'compare', 'the', 'parameters', 'of', 'the', 'effective', 'theory', 'to', 'the', 'experimentally', 'measurable', 'quantities', 'and', 'further', 'discuss', 'the', 'conditions', 'for', 'the', 'verification', 'of', 'the', 'predicted', 'new', 'feature', 'our', 'study', 'opens', 'up', 'an', 'interesting', 'question', 'as', 'to', 'the', 'nature', 'of', 'the', 'vortex', 'lattice', 'resulting', 'from', 'the', 'competition', 'between', 'the', 'usual', 'repulsive', 'logarithmic', '2d', 'coulomb', 'and', 'predominantly', 'attractive', 'fermioninduced', 'interactions']] | [-0.18275382848371713, 0.2501221879567437, -0.089665235350288, 0.09870296878191089, -0.03057983133139767, -0.16691629749297493, 0.06750653990065932, 0.2908245977229638, -0.257462583563016, -0.26169243640659345, -0.049760339132946176, -0.30330297254521205, -0.12159954459134575, 0.13092925350687795, 0.0567151147204672, 0.02420010840024993, -0.03060790473013858, -0.011913319333655642, -0.11681054068145186, -0.21606144930688245, 0.357463304499821, 0.013805590968342185, 0.3210725852724359, 0.10497796334557752, 0.02972022094629231, -0.008872615935205552, 0.10188333291931864, -0.002128107594379972, -0.14224980272772597, 0.0826542318685551, 0.22132879301516684, -0.09921914060745453, 0.1932698686220589, -0.43785224277849144, -0.22734002911198395, 0.07925595057323424, 0.16862750973894308, 0.193737584845206, -0.06263679295517181, -0.3439078263997644, -0.0546194568755525, -0.20634236616604676, -0.18816959955648793, -0.12326868167120124, 0.012496090455739786, -0.007896702284413266, -0.23492144265163667, 0.11181581115607184, 0.05328482839903347, 0.0630549574001676, -0.09770006919548863, -0.05630159696208776, -0.022824312019231865, 0.07018460833596744, 0.05244967451176439, 0.06612810939065897, 0.10177820543570153, -0.21897575657039536, -0.07711054885496164, 0.4011824344354816, -0.10992675117012436, -0.11142246789605803, 0.25474963176758647, -0.14085747092434694, -0.054282055874328224, 0.1614768650232023, 0.1225255147114563, 0.0436972464822405, -0.1264318212102345, 0.08474610849974053, -0.0906981852435846, 0.16069189922189653, -0.01325652467267254, 0.06841197864803879, 0.31770117647644414, 0.20350774068814687, 0.032508906243487415, 0.1668019780527122, -0.11626030862562875, -0.1297681876242893, -0.2657363761157185, -0.16803001210421883, -0.2157029120279799, 0.025183367633093902, -0.01918006847140506, -0.19230729793709828, 0.40268744023148684, 0.17234902026810053, 0.19286794313132047, -0.06632286035846058, 0.22220563158161422, 0.10541952478650936, 0.03745697605702219, 0.03853389506317094, 0.2841684532518676, 0.15640960510341032, 0.0627340191404599, -0.32227480544498716, -0.01583807467822136, 0.06798302412646785] |
710.2523 | An analysis of the abstracts presented at the annual meetings of the
Society for Neuroscience from 2001 to 2006 | We extracted and processed abstract data from the SFN annual meeting
abstracts during the period 2001-2006, using techniques and software from
natural language processing, database management, and data visualization and
analysis. An important first step in the process was the application of data
cleaning and disambiguation methods to construct a unified database, since the
data were too noisy to be of full utility in the raw form initially available.
The resulting co-author graph in 2006, for example, had 39,645 nodes (with an
estimated 6% error rate in our disambiguation of similar author names) and
13,979 abstracts, with an average of 1.5 abstracts per author, 4.3 authors per
abstract, and 5.96 collaborators per author (including all authors on shared
abstracts). Recent work in related areas has focused on reputational indices
such as highly cited papers or scientists and journal impact factors, and to a
lesser extent on creating visual maps of the knowledge space. In contrast,
there has been relatively less work on the demographics and community
structure, the dynamics of the field over time to examine major research trends
and the structure of the sources of research funding. In this paper we examined
each of these areas in order to gain an objective overview of contemporary
neuroscience. Some interesting findings include a high geographical
concentration of neuroscience research in north eastern United States, a
surprisingly large transient population (60% of the authors appear in only one
out of the six studied years), the central role played by the study of
neurodegenerative disorders in the neuroscience community structure, and an
apparent growth of behavioral/systems neuroscience with a corresponding
shrinkage of cellular/molecular neuroscience over the six year period.
| physics.data-an q-bio.NC | we extracted and processed abstract data from the sfn annual meeting abstracts during the period 20012006 using techniques and software from natural language processing database management and data visualization and analysis an important first step in the process was the application of data cleaning and disambiguation methods to construct a unified database since the data were too noisy to be of full utility in the raw form initially available the resulting coauthor graph in 2006 for example had 39645 nodes with an estimated 6 error rate in our disambiguation of similar author names and 13979 abstracts with an average of 15 abstracts per author 43 authors per abstract and 596 collaborators per author including all authors on shared abstracts recent work in related areas has focused on reputational indices such as highly cited papers or scientists and journal impact factors and to a lesser extent on creating visual maps of the knowledge space in contrast there has been relatively less work on the demographics and community structure the dynamics of the field over time to examine major research trends and the structure of the sources of research funding in this paper we examined each of these areas in order to gain an objective overview of contemporary neuroscience some interesting findings include a high geographical concentration of neuroscience research in north eastern united states a surprisingly large transient population 60 of the authors appear in only one out of the six studied years the central role played by the study of neurodegenerative disorders in the neuroscience community structure and an apparent growth of behavioralsystems neuroscience with a corresponding shrinkage of cellularmolecular neuroscience over the six year period | [['we', 'extracted', 'and', 'processed', 'abstract', 'data', 'from', 'the', 'sfn', 'annual', 'meeting', 'abstracts', 'during', 'the', 'period', '20012006', 'using', 'techniques', 'and', 'software', 'from', 'natural', 'language', 'processing', 'database', 'management', 'and', 'data', 'visualization', 'and', 'analysis', 'an', 'important', 'first', 'step', 'in', 'the', 'process', 'was', 'the', 'application', 'of', 'data', 'cleaning', 'and', 'disambiguation', 'methods', 'to', 'construct', 'a', 'unified', 'database', 'since', 'the', 'data', 'were', 'too', 'noisy', 'to', 'be', 'of', 'full', 'utility', 'in', 'the', 'raw', 'form', 'initially', 'available', 'the', 'resulting', 'coauthor', 'graph', 'in', '2006', 'for', 'example', 'had', '39645', 'nodes', 'with', 'an', 'estimated', '6', 'error', 'rate', 'in', 'our', 'disambiguation', 'of', 'similar', 'author', 'names', 'and', '13979', 'abstracts', 'with', 'an', 'average', 'of', '15', 'abstracts', 'per', 'author', '43', 'authors', 'per', 'abstract', 'and', '596', 'collaborators', 'per', 'author', 'including', 'all', 'authors', 'on', 'shared', 'abstracts', 'recent', 'work', 'in', 'related', 'areas', 'has', 'focused', 'on', 'reputational', 'indices', 'such', 'as', 'highly', 'cited', 'papers', 'or', 'scientists', 'and', 'journal', 'impact', 'factors', 'and', 'to', 'a', 'lesser', 'extent', 'on', 'creating', 'visual', 'maps', 'of', 'the', 'knowledge', 'space', 'in', 'contrast', 'there', 'has', 'been', 'relatively', 'less', 'work', 'on', 'the', 'demographics', 'and', 'community', 'structure', 'the', 'dynamics', 'of', 'the', 'field', 'over', 'time', 'to', 'examine', 'major', 'research', 'trends', 'and', 'the', 'structure', 'of', 'the', 'sources', 'of', 'research', 'funding', 'in', 'this', 'paper', 'we', 'examined', 'each', 'of', 'these', 'areas', 'in', 'order', 'to', 'gain', 'an', 'objective', 'overview', 'of', 'contemporary', 'neuroscience', 'some', 'interesting', 'findings', 'include', 'a', 'high', 'geographical', 'concentration', 'of', 'neuroscience', 'research', 'in', 'north', 'eastern', 'united', 'states', 'a', 'surprisingly', 'large', 'transient', 'population', '60', 'of', 'the', 'authors', 'appear', 'in', 'only', 'one', 'out', 'of', 'the', 'six', 'studied', 'years', 'the', 'central', 'role', 'played', 'by', 'the', 'study', 'of', 'neurodegenerative', 'disorders', 'in', 'the', 'neuroscience', 'community', 'structure', 'and', 'an', 'apparent', 'growth', 'of', 'behavioralsystems', 'neuroscience', 'with', 'a', 'corresponding', 'shrinkage', 'of', 'cellularmolecular', 'neuroscience', 'over', 'the', 'six', 'year', 'period']] | [-0.0687173812989118, 0.0445701758215578, -0.046631658078267184, 0.04819613648945666, -0.09098397261593216, -0.07002985100638505, 0.062108454305202676, 0.3700490293883965, -0.23100323847756954, -0.3720617709237986, 0.12312059047904125, -0.32495804230668857, -0.1500921642548158, 0.2024802049758471, -0.11677298045833595, 0.013942837354347027, 0.07431298902991008, 0.06030675688388703, -0.006535060087438016, -0.3088743951303674, 0.2657134032548022, 0.09918660132269211, 0.29926063322893565, 0.0340417021753263, 0.05762505375477143, -0.005150198621456237, -0.14205235588259016, -0.018018129887851127, -0.12355668723552406, 0.17339308811792495, 0.3310747010905556, 0.18113508865131092, 0.35457424590833186, -0.41735667437794344, -0.20128201941759685, 0.04329086601501331, 0.11534257553391987, 0.08077537661301903, -0.037033147936145885, -0.29302361341850724, 0.022115498694748728, -0.18471900055395535, -0.07080956247998127, -0.016514787652019604, 0.08901498561959563, 0.009968577345288769, -0.18153936416445718, 0.06917768093818963, 0.039961424077559704, 0.1806952959707226, -0.06868310635806718, -0.15581056049525024, -0.008644739800194442, 0.1937298568775398, 0.07218547181518635, 0.0654440667541862, 0.12270188695658683, -0.13734772481342694, -0.15248966487150242, 0.3575798727915218, -0.02025709877098587, -0.10097394195583868, 0.17719379071957733, -0.12287402691863998, -0.20913367605980432, 0.09897069963078726, 0.22052257186014151, 0.06103433505631983, -0.16132987702247406, 0.03288378683689242, -0.028639576521955486, 0.1970265685043106, 0.11879820516375783, -0.011249053526519085, 0.18173697729584734, 0.17560150395472782, 0.00906520799959681, 0.1214477051535676, -0.08500547243816339, -0.10091882327448248, -0.23156876772512025, -0.12824443126480808, -0.1587188501509766, 0.012049663332136869, -0.05176417047764784, -0.12208515491404208, 0.4364322781064616, 0.1369039686747676, 0.1593944766665278, -0.03343039858908228, 0.2467356682053137, 0.026527474772164543, 0.09809040013105379, 0.10080226786222364, 0.1705152476335891, 0.078101603229537, 0.18370294766004114, -0.11200982277403133, 0.10635081812741941, -0.0028815107879756182] |
710.2524 | Neutrino time travel | We discuss causality properties of extra-dimensional theories allowing for
effectively superluminal bulk shortcuts. Such shortcuts for sterile neutrinos
have been discussed as a solution to the puzzling LSND and MiniBooNE neutrino
oscillation results. We focus here on the sub-category of asymmetrically warped
brane spacetimes and argue that scenarios with two extra dimensions may allow
for timelike curves which can be closed via paths in the extra-dimensional
bulk. In principle sterile neutrinos propagating in the extra dimension may be
manipulated in a way to test the chronology protection conjecture
experimentally.
| hep-ph | we discuss causality properties of extradimensional theories allowing for effectively superluminal bulk shortcuts such shortcuts for sterile neutrinos have been discussed as a solution to the puzzling lsnd and miniboone neutrino oscillation results we focus here on the subcategory of asymmetrically warped brane spacetimes and argue that scenarios with two extra dimensions may allow for timelike curves which can be closed via paths in the extradimensional bulk in principle sterile neutrinos propagating in the extra dimension may be manipulated in a way to test the chronology protection conjecture experimentally | [['we', 'discuss', 'causality', 'properties', 'of', 'extradimensional', 'theories', 'allowing', 'for', 'effectively', 'superluminal', 'bulk', 'shortcuts', 'such', 'shortcuts', 'for', 'sterile', 'neutrinos', 'have', 'been', 'discussed', 'as', 'a', 'solution', 'to', 'the', 'puzzling', 'lsnd', 'and', 'miniboone', 'neutrino', 'oscillation', 'results', 'we', 'focus', 'here', 'on', 'the', 'subcategory', 'of', 'asymmetrically', 'warped', 'brane', 'spacetimes', 'and', 'argue', 'that', 'scenarios', 'with', 'two', 'extra', 'dimensions', 'may', 'allow', 'for', 'timelike', 'curves', 'which', 'can', 'be', 'closed', 'via', 'paths', 'in', 'the', 'extradimensional', 'bulk', 'in', 'principle', 'sterile', 'neutrinos', 'propagating', 'in', 'the', 'extra', 'dimension', 'may', 'be', 'manipulated', 'in', 'a', 'way', 'to', 'test', 'the', 'chronology', 'protection', 'conjecture', 'experimentally']] | [-0.14190499792712624, 0.2652110907751439, -0.06346101140122065, 0.18264994643670454, -0.13493475112854764, -0.2308291384866566, 0.027839565846897018, 0.3425559319262759, -0.1992268453278903, -0.2885307443610738, 0.050616956238760454, -0.2709596853551528, -0.09405070012749246, 0.17689434648229835, -0.08560622809454799, 0.047760351966501455, 0.02530030577621433, -0.01673986029476346, -0.045731727475970145, -0.251790187101853, 0.3217137500767503, 0.04988212310813702, 0.25785294086724686, 0.08807621789007877, 0.056886040255050646, -0.06409041796486532, 0.005467044511349516, 0.0007346989220698897, -0.10642199472334887, 0.0629528296478302, 0.23801876454917567, 0.1435345104853675, 0.11212982963561342, -0.49680567779735235, -0.28885857621992655, 0.15407509666480376, 0.23363747079647407, 0.15282637394017676, -0.056026456873665115, -0.34921147552936266, 0.03182227128928297, -0.18373619333914157, -0.1998942985272642, -0.08300317444032833, -0.015505281151429321, -0.13371370767316457, -0.2293775923591986, 0.06012675910010892, -0.00847411820706859, -0.009936354698592357, -0.06905189947633261, -0.05444781918842555, -0.013165766729062863, 0.018949314542480986, 0.18463748394187246, -0.07534991265954764, 0.09906117949540612, -0.09217705276501731, -0.20001600738196226, 0.36391945867642256, -0.07947259169762556, -0.2505856534999827, 0.14810248509342416, -0.14417634146769395, -0.11482675653997432, 0.07351869131762827, 0.1490515371826425, 0.0724302938527145, -0.16951716115719148, 0.13603929973735862, -0.10053328820765856, 0.10677911992592926, 0.14022273501234778, 0.07711431576106488, 0.31963196602451166, 0.1481779548601153, 0.08293800993581836, 0.04564692844045506, -0.08936220586163861, -0.024620226591569108, -0.4013652286670181, -0.17508001668703105, -0.06471455042489825, 0.11366603881633433, -0.13556216616841463, -0.10087314285233281, 0.36388695207058214, 0.1368211422173118, 0.16858841416038825, -0.038717560500189076, 0.251341161516945, -0.01250971843399568, 0.06482495029530164, 0.08039470560053426, 0.3355575286772814, 0.10042217936565619, 0.07079623532324528, -0.20135717450777132, -0.00857467654820406, 0.08859416712964938] |
710.2525 | Lepton Flavor Violation at the LHC | In supersymmetric scenarios, the seesaw mechanism involving heavy
right-handed neutrinos implies sizable lepton flavor violation (LFV) in the
slepton sector. We discuss the potential of detecting LFV processes at the LHC
in mSUGRA+seesaw scenarios and for general mixing in either the left- or
right-handed slepton sector. The results are compared with the sensitivity of
rare LFV mu -> e gamma decay experiments.
| hep-ph | in supersymmetric scenarios the seesaw mechanism involving heavy righthanded neutrinos implies sizable lepton flavor violation lfv in the slepton sector we discuss the potential of detecting lfv processes at the lhc in msugraseesaw scenarios and for general mixing in either the left or righthanded slepton sector the results are compared with the sensitivity of rare lfv mu e gamma decay experiments | [['in', 'supersymmetric', 'scenarios', 'the', 'seesaw', 'mechanism', 'involving', 'heavy', 'righthanded', 'neutrinos', 'implies', 'sizable', 'lepton', 'flavor', 'violation', 'lfv', 'in', 'the', 'slepton', 'sector', 'we', 'discuss', 'the', 'potential', 'of', 'detecting', 'lfv', 'processes', 'at', 'the', 'lhc', 'in', 'msugraseesaw', 'scenarios', 'and', 'for', 'general', 'mixing', 'in', 'either', 'the', 'left', 'or', 'righthanded', 'slepton', 'sector', 'the', 'results', 'are', 'compared', 'with', 'the', 'sensitivity', 'of', 'rare', 'lfv', 'mu', 'e', 'gamma', 'decay', 'experiments']] | [-0.11451705304595332, 0.38607332957132406, 0.10283476507756859, 0.27216551583260296, -0.059245598254104456, -0.26277298405766486, 0.07480966746807098, 0.27423683684319256, -0.2360881634367009, -0.22202590256929397, 0.004985211316185693, -0.3349901855768015, 0.021067855511015903, 0.10052453083141397, 0.08565696924536799, 0.04871723420607547, 0.08397618844173849, -0.052910900519539915, -0.025243143195984884, -0.19123128323505323, 0.2522125899946938, 0.0435316847016414, 0.14070280018883446, 0.14586610663294172, -0.04055473054371153, -0.08460577913404753, -0.060353550625344116, -0.21267518216433626, -0.059623337195565305, -0.006972498400136829, 0.14769708118401467, 0.12203092693040768, -0.0062523814539114635, -0.3902020367483298, -0.09922012756578624, 0.3060794147818039, 0.16297135970089585, 0.016665260788674155, -0.15721987236756832, -0.38814493889609974, 0.08113105772063137, -0.2411416236932079, -0.07812158296971271, -0.06314855719295641, -0.05268122661703577, -0.19294303405719498, -0.46131222521265347, 0.1403917928187487, -0.0969614588151065, -0.04700589089964827, 0.08351594817359001, -0.24760760148249877, -0.0286082153286164, -0.04937095095325882, 0.3457761570500831, -0.1210483726967747, 0.1803661625444268, -0.24163552801279972, -0.25376835841840756, 0.46455459414670863, -0.11119667943373011, -0.191594720511542, 0.172531255070741, -0.2553230082383379, -0.2195516667716826, 0.07538761228012542, 0.24363586991870154, 0.10182318383206924, -0.19196756284994385, 0.2966325730230892, -0.0785961470445424, 0.06735614417120814, 0.09224538763131325, 0.10097917827176085, 0.29520817905819663, 0.26551539815651876, 0.10683020242334654, -0.047573731013108043, -0.09289465562130014, -0.015588933151836197, -0.5042968719576796, -0.1010999922795842, -0.0033596429818620282, 0.06744497399777175, -0.07909833573091116, -0.01038185836126407, 0.45632790146240343, 0.0974818309613814, 0.21471484020973244, 0.0032513797787639, 0.2675126021572699, 0.05433379550619672, 0.07582844273808102, -0.003861875288809339, 0.3265324860500793, 0.12831951848541698, 0.14343114419219394, -0.32823484543090065, 0.016109877405688165, 0.06093621603989353] |
710.2526 | Angle dependent quasiparticle weights in correlated metals | The variation in the quasiparticle weight $Z$ on moving around the fermi
surface in correlated metals is studied theoretically. Our primary example is a
heavy Fermi liquid treated within the standard hybridization mean field theory.
The most dramatic variation in the quasiparticle weight happens in situations
where the hybridization vanishes along certain directions in momentum space.
Such a "hybridization node" is demonstrated for a simplified model of a
Cerium-based cubic heavy electron metal. We show that the quasiparticle weight
varies from almost unity in some directions, to values approaching zero in
others. This is accompanied by a similar variation in the quasiparticle
effective mass. Some consequences of such hybridization nodes and the
associated angle dependence are explored. Comparisons to somewhat similar
phenomena in the normal metallic state of the cuprate materials are discussed.
A phenomenological picture of the pseudogap state in the cuprates with a large
Fermi surface with a severely anisotropic spectral weight is explored.
| cond-mat.str-el | the variation in the quasiparticle weight z on moving around the fermi surface in correlated metals is studied theoretically our primary example is a heavy fermi liquid treated within the standard hybridization mean field theory the most dramatic variation in the quasiparticle weight happens in situations where the hybridization vanishes along certain directions in momentum space such a hybridization node is demonstrated for a simplified model of a ceriumbased cubic heavy electron metal we show that the quasiparticle weight varies from almost unity in some directions to values approaching zero in others this is accompanied by a similar variation in the quasiparticle effective mass some consequences of such hybridization nodes and the associated angle dependence are explored comparisons to somewhat similar phenomena in the normal metallic state of the cuprate materials are discussed a phenomenological picture of the pseudogap state in the cuprates with a large fermi surface with a severely anisotropic spectral weight is explored | [['the', 'variation', 'in', 'the', 'quasiparticle', 'weight', 'z', 'on', 'moving', 'around', 'the', 'fermi', 'surface', 'in', 'correlated', 'metals', 'is', 'studied', 'theoretically', 'our', 'primary', 'example', 'is', 'a', 'heavy', 'fermi', 'liquid', 'treated', 'within', 'the', 'standard', 'hybridization', 'mean', 'field', 'theory', 'the', 'most', 'dramatic', 'variation', 'in', 'the', 'quasiparticle', 'weight', 'happens', 'in', 'situations', 'where', 'the', 'hybridization', 'vanishes', 'along', 'certain', 'directions', 'in', 'momentum', 'space', 'such', 'a', 'hybridization', 'node', 'is', 'demonstrated', 'for', 'a', 'simplified', 'model', 'of', 'a', 'ceriumbased', 'cubic', 'heavy', 'electron', 'metal', 'we', 'show', 'that', 'the', 'quasiparticle', 'weight', 'varies', 'from', 'almost', 'unity', 'in', 'some', 'directions', 'to', 'values', 'approaching', 'zero', 'in', 'others', 'this', 'is', 'accompanied', 'by', 'a', 'similar', 'variation', 'in', 'the', 'quasiparticle', 'effective', 'mass', 'some', 'consequences', 'of', 'such', 'hybridization', 'nodes', 'and', 'the', 'associated', 'angle', 'dependence', 'are', 'explored', 'comparisons', 'to', 'somewhat', 'similar', 'phenomena', 'in', 'the', 'normal', 'metallic', 'state', 'of', 'the', 'cuprate', 'materials', 'are', 'discussed', 'a', 'phenomenological', 'picture', 'of', 'the', 'pseudogap', 'state', 'in', 'the', 'cuprates', 'with', 'a', 'large', 'fermi', 'surface', 'with', 'a', 'severely', 'anisotropic', 'spectral', 'weight', 'is', 'explored']] | [-0.17475763480895415, 0.23443845582331937, -0.05190206683264711, 0.11714410288139987, -0.028922079311600193, -0.1472311888773663, 0.09182656958280579, 0.36455102774720544, -0.27007261831805895, -0.242834471572095, -0.02879227316066718, -0.3380782374371894, -0.11995603898778939, 0.1553699974767649, -0.02990390759898732, 0.009893748376364387, 0.006546887924345449, 0.03643535693677572, -0.1511567549333006, -0.20349916739938542, 0.32673555522715336, 0.0479276326771539, 0.29228749540813553, 0.08218258594085152, 0.014744295798337612, 0.01772835866834682, 0.04506739087772962, 0.04382666464255472, -0.12799841419142374, 0.05310275060578416, 0.26500016558342254, -0.06960277608297287, 0.2347128220523397, -0.3760611020261422, -0.24730914923696753, 0.026388739871505935, 0.14588544212090662, 0.11575327138416469, -0.07601424308645968, -0.22446689274436674, 0.012390798220458703, -0.17227600848463437, -0.18482689527893223, -0.030665313438452683, -0.011428960939669289, -0.009499622019528685, -0.19385644270536992, 0.11077789064307954, 0.023767934476311963, 0.07218330542897232, -0.08260007795000163, -0.16310758830812305, -0.06331626976428267, 0.01996885397686408, 0.09330026158027184, 0.0698524911989434, 0.12590596962250764, -0.1661384125995354, -0.05218681145775824, 0.3894430198169385, -0.07368761477529262, -0.15305304929661828, 0.1755193283673949, -0.19753245504435676, -0.09388987361513174, 0.1684569279609721, 0.10643071004858193, 0.0798207119328137, -0.10435592796943055, 0.10615905717228695, -0.03789850874977091, 0.11897555474812786, 0.04587732937383967, 0.06097736761558992, 0.22664751613643977, 0.20019979761594023, 0.029762908589476958, 0.0831039949762038, -0.13094731048234584, -0.08980033689071067, -0.26184758899184185, -0.15898413293791983, -0.2336136044558281, 0.021425012508049034, -0.06540385035800565, -0.1924777775674533, 0.4348875616098014, 0.10575544904583158, 0.26269354407365125, -0.05149667233845088, 0.2181208168801207, 0.12768056723796642, 0.08195056100838627, 0.06896680754681046, 0.2382945514523621, 0.13157423400060417, 0.0682203720162551, -0.2509758968685324, 0.07496140148111571, 0.01674076211071597] |
710.2527 | Equilibrium Properties of Mixtures of Bosons and Fermions | Partial Quantum Nearest Neighbor Probability Density Functions (PQNNPDF's)
are formulated for the purpose of determining the behavior of quantum mixed
systems in equilibrium in a manner analogous to that provided for classical
multi-component systems. Developments in partial quantum m-tuplet distribution
functions, a generalization of the partial quantum radial distribution
function, along with their relationship to PQNNPDF's, are briefly elucidated.
The calculation of statistical thermodynamic properties of quantum mixtures is
presented for arbitrary material systems. Application to the limiting case of
dilute, weakly correlated quantum gas mixtures has been outlined and the second
virial coefficient is derived. The case of dilute strongly degenerate mixtures
is also addressed, providing an expression for the PQNNPDF applicable in this
thermodynamic regime.
| cond-mat.stat-mech cond-mat.mtrl-sci | partial quantum nearest neighbor probability density functions pqnnpdfs are formulated for the purpose of determining the behavior of quantum mixed systems in equilibrium in a manner analogous to that provided for classical multicomponent systems developments in partial quantum mtuplet distribution functions a generalization of the partial quantum radial distribution function along with their relationship to pqnnpdfs are briefly elucidated the calculation of statistical thermodynamic properties of quantum mixtures is presented for arbitrary material systems application to the limiting case of dilute weakly correlated quantum gas mixtures has been outlined and the second virial coefficient is derived the case of dilute strongly degenerate mixtures is also addressed providing an expression for the pqnnpdf applicable in this thermodynamic regime | [['partial', 'quantum', 'nearest', 'neighbor', 'probability', 'density', 'functions', 'pqnnpdfs', 'are', 'formulated', 'for', 'the', 'purpose', 'of', 'determining', 'the', 'behavior', 'of', 'quantum', 'mixed', 'systems', 'in', 'equilibrium', 'in', 'a', 'manner', 'analogous', 'to', 'that', 'provided', 'for', 'classical', 'multicomponent', 'systems', 'developments', 'in', 'partial', 'quantum', 'mtuplet', 'distribution', 'functions', 'a', 'generalization', 'of', 'the', 'partial', 'quantum', 'radial', 'distribution', 'function', 'along', 'with', 'their', 'relationship', 'to', 'pqnnpdfs', 'are', 'briefly', 'elucidated', 'the', 'calculation', 'of', 'statistical', 'thermodynamic', 'properties', 'of', 'quantum', 'mixtures', 'is', 'presented', 'for', 'arbitrary', 'material', 'systems', 'application', 'to', 'the', 'limiting', 'case', 'of', 'dilute', 'weakly', 'correlated', 'quantum', 'gas', 'mixtures', 'has', 'been', 'outlined', 'and', 'the', 'second', 'virial', 'coefficient', 'is', 'derived', 'the', 'case', 'of', 'dilute', 'strongly', 'degenerate', 'mixtures', 'is', 'also', 'addressed', 'providing', 'an', 'expression', 'for', 'the', 'pqnnpdf', 'applicable', 'in', 'this', 'thermodynamic', 'regime']] | [-0.12375490194798522, 0.1351775022387655, -0.05979726799821432, 0.07695944410485042, 0.010466892338168304, -0.13937910371748483, 0.012825175544939341, 0.3255723115073237, -0.2568949087959739, -0.20241831557668613, 0.06702355518463207, -0.27920017083200205, -0.13362657261880495, 0.19087834975195933, 0.004280409899301234, 0.13733529129716676, -0.004225338478264887, 0.013857160241598577, -0.09932896461692202, -0.2531374871908003, 0.3177576886028447, 0.053725433595626884, 0.2820625900892557, 0.05762511816090055, 0.0778451550100823, 0.05499203231976887, 0.001827793165709642, 0.037055215738307834, -0.15395858331071677, 0.10927260679448336, 0.27991716648592097, 0.05649574034418746, 0.2261292036721664, -0.37618542408191524, -0.25244029003928986, 0.07495845358950638, 0.14639541362535902, 0.12190620161065485, -0.055290741223194925, -0.24595437753962074, 0.04777076669795587, -0.19282409657139035, -0.20713238317964483, -0.10019987645719727, 0.03488470626525185, 0.056154429251163276, -0.2398156423154658, 0.1427617619610989, 0.08220006520571434, 0.051273154238660294, -0.06513222118744841, -0.12933248546040427, 0.051072670062344554, 0.10667631042445391, -0.03718428539351222, -0.025499144622611, 0.13585015758975055, -0.16356293921589654, -0.07299129159676027, 0.4112165862513063, -0.05783959896822946, -0.2418586119712718, 0.2208573611275977, -0.13892199202704417, -0.15454033936530484, 0.08973458490491046, 0.13412344441501903, 0.1327720642238196, -0.1900939962793702, 0.09037108839421525, -0.03573205549191617, 0.14229937651054522, 0.012138552716479891, 0.05724104669406614, 0.24144129059689565, 0.11005457513347532, 0.04158590777274386, 0.1971267861627306, -0.030813519632756973, -0.23352070903998956, -0.27179705773570895, -0.1943679931326316, -0.21490535984821288, 0.03654457724331755, -0.046686172660103324, -0.1931908090827591, 0.3132681210022584, 0.10270483522270023, 0.17617869271641284, 0.02374154202582364, 0.2408462449335452, 0.19602790021593064, -0.0497369637725199, 0.011878055300917971, 0.21449199661744378, 0.23912189847509485, 0.08205996124090346, -0.22948875803777544, 0.09227589092967389, 0.08064143944210249] |
710.2528 | Chern-Simons Modified General Relativity: Conserved charges | We construct the conserved charges (mass and angular momentum) of the
Chern-Simons modified General Relativity in asymptotically flat and Anti-de
Sitter (AdS) spacetimes. Our definition is based on background Killing
symmetries and reduces to the known expressions in the proper limits.
| gr-qc astro-ph hep-th | we construct the conserved charges mass and angular momentum of the chernsimons modified general relativity in asymptotically flat and antide sitter ads spacetimes our definition is based on background killing symmetries and reduces to the known expressions in the proper limits | [['we', 'construct', 'the', 'conserved', 'charges', 'mass', 'and', 'angular', 'momentum', 'of', 'the', 'chernsimons', 'modified', 'general', 'relativity', 'in', 'asymptotically', 'flat', 'and', 'antide', 'sitter', 'ads', 'spacetimes', 'our', 'definition', 'is', 'based', 'on', 'background', 'killing', 'symmetries', 'and', 'reduces', 'to', 'the', 'known', 'expressions', 'in', 'the', 'proper', 'limits']] | [-0.16400768153551148, 0.16290953185227586, -0.07556012511344218, 0.13528554342834778, -0.17262270917161937, -0.11228628606512779, -0.05961674651721629, 0.2995462859526458, -0.061023876014188294, -0.25370843684380284, 0.0395884300893025, -0.2704071298968501, -0.09811801377047853, 0.10965203834561313, -0.11995897825989055, 0.03621734939969894, -0.040792919990674754, 0.0744397503937163, -0.1620578796648216, -0.2233196758869581, 0.38940422963805316, 0.11361387031289136, 0.351429450711826, -0.013535678284469901, 0.2029077866478119, 0.008538924203049846, -0.07545553897393913, 0.03836835389275376, -0.2243200679786685, 0.05406820956935606, 0.1998997168933473, 0.1032188874896525, 0.05844313987508053, -0.39108403613109416, -0.1749347281420785, 0.06570386930039471, 0.17204190025151503, 0.204462294398648, -0.04099867628353489, -0.3360701314196354, 0.01820508072652468, -0.16911591687126132, -0.20619931401366867, -0.11071081674748623, 0.050785279753277214, -0.11412164464411212, -0.20240984375520452, 0.1575235718088906, 0.06891218168524707, -0.048195099662535074, -0.18854077297785296, -0.05619580178697616, -0.1568610502986192, 0.06296967218698162, 0.18576610735163274, 0.02149047525372447, 0.14540606950659576, -0.108544459203031, -0.12985076600822007, 0.3642754298861979, -0.07531006879559378, -0.39254234676680916, 0.12084498470535547, -0.21414478152717759, -0.12214472955774243, 0.07134300556669874, 0.1397434931316572, 0.2675075296812305, -0.14974915106758113, 0.2533184258088401, 0.02827127280122623, 0.07383030371331586, 0.17739894038929446, 0.06606752293258224, 0.309533219511916, 0.012719351866441528, 0.07558109595940062, 0.09982445570299538, -0.003750404098820759, -0.1664559358614497, -0.4208185496490176, -0.1863416110892303, -0.134344339552449, 0.13271621912263515, -0.21570986651186547, -0.1947931687847325, 0.3153964114807001, 0.09084456819450347, 0.10185241824152266, 0.1124220640148695, 0.2310203240230316, 0.08879011346129473, 0.06769006307486718, 0.159382534997038, 0.30365282109592157, 0.15004545229873278, 0.11313741210075777, -0.24188210183709133, -0.17404151688579741, 0.1586080156720993] |
710.2529 | Heuristic decomposition of cones in molecular conformational space | In a previous work arXiv:physics/0611108v2, it was shown that the volume
spanned by a molecular system in its conformational space can be effectively
bounded by a polyhedral cone, this cone is described by means of a simple
combinatorial formula. On the other hand it was constructed a transversal graph
structure encoding the region of conformational space accessible to the system.
From the information in this graph, it is possible to decompose the main cone
into a hierarchy of smaller ones that are more manageable, and are
progressively more tightly bound to the region in which the system evolves.
| physics.comp-ph | in a previous work arxivphysics0611108v2 it was shown that the volume spanned by a molecular system in its conformational space can be effectively bounded by a polyhedral cone this cone is described by means of a simple combinatorial formula on the other hand it was constructed a transversal graph structure encoding the region of conformational space accessible to the system from the information in this graph it is possible to decompose the main cone into a hierarchy of smaller ones that are more manageable and are progressively more tightly bound to the region in which the system evolves | [['in', 'a', 'previous', 'work', 'arxivphysics0611108v2', 'it', 'was', 'shown', 'that', 'the', 'volume', 'spanned', 'by', 'a', 'molecular', 'system', 'in', 'its', 'conformational', 'space', 'can', 'be', 'effectively', 'bounded', 'by', 'a', 'polyhedral', 'cone', 'this', 'cone', 'is', 'described', 'by', 'means', 'of', 'a', 'simple', 'combinatorial', 'formula', 'on', 'the', 'other', 'hand', 'it', 'was', 'constructed', 'a', 'transversal', 'graph', 'structure', 'encoding', 'the', 'region', 'of', 'conformational', 'space', 'accessible', 'to', 'the', 'system', 'from', 'the', 'information', 'in', 'this', 'graph', 'it', 'is', 'possible', 'to', 'decompose', 'the', 'main', 'cone', 'into', 'a', 'hierarchy', 'of', 'smaller', 'ones', 'that', 'are', 'more', 'manageable', 'and', 'are', 'progressively', 'more', 'tightly', 'bound', 'to', 'the', 'region', 'in', 'which', 'the', 'system', 'evolves']] | [-0.11398103873073795, 0.14108072126226634, -0.11542194012130044, 0.07483857166329302, -0.0940689133653014, -0.10825592867511603, 0.04481091126607558, 0.36518917866435247, -0.32594707664390354, -0.27351726434126344, 0.11349936625584192, -0.23689884527288763, -0.17047374399820553, 0.2035186700138849, -0.05622438536824889, 0.0009466000663395011, 0.0476896191482701, 0.040678104997814164, -0.05385714047520899, -0.23918784090099357, 0.3375551287929729, 0.05372936312186042, 0.22518662741820605, 0.025522739535255225, 0.08082527983165586, -0.018946522393158263, -8.727187415604124e-05, 0.08070178140889728, -0.09882175124843831, 0.1767128623215501, 0.22545440392760732, 0.15392502181270382, 0.24216542885513956, -0.37666838228241684, -0.22594425897684053, 0.08331279310196177, 0.16025059947686404, 0.11068642133073978, 0.03422017984743921, -0.28897576342749687, 0.09167570762393862, -0.14072211503444873, -0.09168400089784536, -0.06215990988355245, 0.02267815068618577, -0.05209311425263427, -0.20096380681041917, 0.002392484369620527, 0.08961117140391898, -0.010753568504293709, -0.027931683491579422, -0.08817099233652398, -0.08335901025836308, 0.0873720534577889, -0.01442149426000788, 0.1074846756690153, 0.13414609553676443, -0.08121876792079702, -0.04723556184680345, 0.3893971360605402, -0.006427885357232899, -0.24105384388996154, 0.16599567673293894, -0.17653602768292592, -0.09003263727771406, 0.19866488586880804, 0.1352367621832095, 0.15049686042841562, -0.16187626574747743, 0.09989606142807668, -0.07752811570877459, 0.16336849434109232, 0.056258772163815106, 0.002560194504936946, 0.18092328194797652, 0.18946285384524728, 0.13173666724109465, 0.19446977278212874, -0.014329009134917683, -0.1138703296946352, -0.2605558177360247, -0.161314559589769, -0.22643997857212714, 0.015971943121595483, -0.06091545652175087, -0.13580045160164184, 0.4017252353951335, 0.05250373242192508, 0.23526206082117157, 0.03542353093897751, 0.2978457435965538, 0.10614204032288999, 0.10058052846489801, 0.06503739591073437, 0.19806710122748442, 0.10193217107690103, 0.05124853103488837, -0.17838279484619973, 0.0802138515690476, 0.08574087980738] |
710.253 | Smectic ordering in athermal systems of rod-like triblock copolymers | The phase behavior of the system of parallel rigid triblock copolymers is
examined using the second-virial density functional theory. The triblock
particle consists of two identical infinitely thin hard rods of finite lengths
on the opposite ends of one central hard cylinder with nonzero length and
diameter. Stability analyses and free energy calculations show that the system
of parallel particles can form not only uniform nematic and smectic A phases,
but a smectic-C phase too. The stability and structure of the tilted structure
is controlled by only the diameter and the length of the central cylinder
segment. Interestingly, the diameter effects only the layer tilting and the
periodicity, but not the packing fraction of the nematic to smectic-C
transition. For all values of cylinder length the usual smectic-A and smectic-C
transitions compete with each other and no nematic-columnar transition is
observed. At low and high cylinder length the smectic-A phase is stabilized
first, while the smectic C is the most stable for intermediate length values.
| cond-mat.soft cond-mat.mtrl-sci | the phase behavior of the system of parallel rigid triblock copolymers is examined using the secondvirial density functional theory the triblock particle consists of two identical infinitely thin hard rods of finite lengths on the opposite ends of one central hard cylinder with nonzero length and diameter stability analyses and free energy calculations show that the system of parallel particles can form not only uniform nematic and smectic a phases but a smecticc phase too the stability and structure of the tilted structure is controlled by only the diameter and the length of the central cylinder segment interestingly the diameter effects only the layer tilting and the periodicity but not the packing fraction of the nematic to smecticc transition for all values of cylinder length the usual smectica and smecticc transitions compete with each other and no nematiccolumnar transition is observed at low and high cylinder length the smectica phase is stabilized first while the smectic c is the most stable for intermediate length values | [['the', 'phase', 'behavior', 'of', 'the', 'system', 'of', 'parallel', 'rigid', 'triblock', 'copolymers', 'is', 'examined', 'using', 'the', 'secondvirial', 'density', 'functional', 'theory', 'the', 'triblock', 'particle', 'consists', 'of', 'two', 'identical', 'infinitely', 'thin', 'hard', 'rods', 'of', 'finite', 'lengths', 'on', 'the', 'opposite', 'ends', 'of', 'one', 'central', 'hard', 'cylinder', 'with', 'nonzero', 'length', 'and', 'diameter', 'stability', 'analyses', 'and', 'free', 'energy', 'calculations', 'show', 'that', 'the', 'system', 'of', 'parallel', 'particles', 'can', 'form', 'not', 'only', 'uniform', 'nematic', 'and', 'smectic', 'a', 'phases', 'but', 'a', 'smecticc', 'phase', 'too', 'the', 'stability', 'and', 'structure', 'of', 'the', 'tilted', 'structure', 'is', 'controlled', 'by', 'only', 'the', 'diameter', 'and', 'the', 'length', 'of', 'the', 'central', 'cylinder', 'segment', 'interestingly', 'the', 'diameter', 'effects', 'only', 'the', 'layer', 'tilting', 'and', 'the', 'periodicity', 'but', 'not', 'the', 'packing', 'fraction', 'of', 'the', 'nematic', 'to', 'smecticc', 'transition', 'for', 'all', 'values', 'of', 'cylinder', 'length', 'the', 'usual', 'smectica', 'and', 'smecticc', 'transitions', 'compete', 'with', 'each', 'other', 'and', 'no', 'nematiccolumnar', 'transition', 'is', 'observed', 'at', 'low', 'and', 'high', 'cylinder', 'length', 'the', 'smectica', 'phase', 'is', 'stabilized', 'first', 'while', 'the', 'smectic', 'c', 'is', 'the', 'most', 'stable', 'for', 'intermediate', 'length', 'values']] | [-0.21031859342686154, 0.2577884791136691, -0.06208444955391866, -0.013587521873837844, -0.012887643739073114, -0.16527844902805305, -0.001793055764089028, 0.39097813402838777, -0.27701526426244527, -0.24500092541319177, 0.09634918317368085, -0.27856178082751504, -0.08145811017038244, 0.09598705062685027, 0.03361749215136198, 0.041929863954393305, -0.005307232745161111, 0.035588581383115415, -0.07691621714779599, -0.1709859784784247, 0.2469935685819523, 0.010002226321816896, 0.3107056498837968, 0.024446180849124425, 0.07720695024102249, 0.026498059520610805, 0.09770868962743517, 0.09831675937342825, -0.21187463039131024, 0.04880586885141604, 0.1902211949610236, -0.07738931957124309, 0.1744768738986529, -0.4426163686157176, -0.18265924231346808, 0.05721752218484074, 0.1273064810556896, 0.073012258267651, -0.0017286515011536805, -0.21622916595784553, 0.1056067863648588, -0.11634712871164084, -0.17025564202022822, -0.008114980432120236, 0.04913986204474261, 0.047478803457113715, -0.1909026179318034, 0.09592265866301727, 0.07748973426888837, 0.046794821166346964, -0.07833960427987305, -0.11986239919241405, -0.0767493148447212, 0.12062194231671818, 0.06455319590697234, 0.027766860304682544, 0.16358564982585835, -0.12194499590744574, -0.05271604090477481, 0.36747768959312727, -0.028323385774186163, -0.15340069375480667, 0.1964859747476029, -0.17736934690857942, -0.07936339621065241, 0.23272938144139269, 0.08494372175385555, 0.12430832521481948, -0.04672569438434121, 0.06653899197505476, -0.032682297173464166, 0.2612115681284305, 0.10240987944275592, -0.027733528198476767, 0.22761583671989766, 0.1818606344644319, 0.047818361426647187, 0.17236707320641445, -0.11657501886260103, -0.1433778271417726, -0.2831014821926753, -0.16470346445161285, -0.18138236462872362, -0.03477028926083056, -0.145452463747422, -0.2377722581566283, 0.3269733842575189, 0.04196184110672523, 0.21492404479420546, 0.03295851365705444, 0.26135272747187904, 0.022680028422848518, 0.07507123866640596, 0.057100814964735146, 0.2537834865351518, 0.15271985736238122, 0.08138455220464631, -0.2385839434905034, 0.09021893473567837, 0.07921757180610615] |
710.2531 | Lens space surgeries and L-space homology spheres | We describe necessary and sufficient conditions for a knot in an L-space to
have an L-space homology sphere surgery. We use these conditions to reformulate
a conjecture of Berge about which knots in S^3 admit lens space surgeries.
| math.GT | we describe necessary and sufficient conditions for a knot in an lspace to have an lspace homology sphere surgery we use these conditions to reformulate a conjecture of berge about which knots in s3 admit lens space surgeries | [['we', 'describe', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'a', 'knot', 'in', 'an', 'lspace', 'to', 'have', 'an', 'lspace', 'homology', 'sphere', 'surgery', 'we', 'use', 'these', 'conditions', 'to', 'reformulate', 'a', 'conjecture', 'of', 'berge', 'about', 'which', 'knots', 'in', 's3', 'admit', 'lens', 'space', 'surgeries']] | [-0.2944983093950309, 0.005881570580593114, -0.1954894511176175, 0.1474167274213151, -0.16148488099784836, -0.21825733633809968, -0.04756417801285064, 0.433693029084488, -0.20838006066256448, -0.31630202372999566, 0.14543388753908834, -0.16080198375091545, -0.2246556862159387, 0.17204514082129063, -0.24924362681217885, 0.008414627322436948, 0.11663277654320393, 0.027382561887957547, -0.06823658210372455, -0.3436107576187504, 0.3389588493584214, -0.06564740601338838, 0.06385039744016371, 0.20616063821178518, 0.134349286311159, 0.013257629072636758, 0.02432718545222949, 0.008963183413327084, -0.3686643758984773, 0.03219477798005468, 0.2871108952125436, 0.07002012642394555, 0.08828968397880856, -0.4459511613669364, -0.1383750937744289, 0.18731362174118035, 0.1585198555778908, -0.059132863268084625, 0.0026607912180847243, -0.2848092192832969, 0.05257405791627733, -0.12551596326336853, -0.17797451193052294, -0.09699611738324165, 0.045110511740571575, -0.004742222347933995, -0.16208472289144993, -0.04313257486118298, 0.07016466050653865, 0.11180890567208591, -0.052657712324473416, 0.007351713157013843, 0.026762586883514336, 0.19815157241138973, 0.003934943497082905, 0.10008071372775655, 0.05158159478665575, -0.1690855112514998, -0.14660695474594831, 0.3467000658550349, -0.031678256088573685, -0.30252898366827713, 0.14905051399316444, -0.08515394383453224, -0.30608272856395496, 0.31676951344860227, 0.035859596768492145, 0.12737007798185865, -0.03050336565234159, 0.03538919847893627, -0.18123418504470273, 0.14063173746322527, 0.14845178123735087, -0.0473787828446611, 0.1964148310944438, 0.019157389644533396, 0.1850567599819777, 0.19032331703132704, -0.038472480042592475, 0.04135424594737982, -0.32960196408002, -0.3523335113729301, -0.1120139180351735, 0.18236236769313874, -0.08356087073939546, -0.18870649908326173, 0.32918380954498916, 0.020863855257630348, 0.12068068927251979, 0.1629152634260735, 0.26040201729751733, -0.03690029009962209, 0.056002749130129814, 0.08807797465277345, 0.1297193005632021, 0.17339077910506412, -0.03673107900019539, -0.016454798886307367, -0.09863072953579065, 0.24512892754405344] |
710.2532 | Sleeping on the Job: Energy-Efficient Broadcast for Radio Networks | We address the problem of minimizing power consumption when performing
reliable broadcast on a radio network under the following popular model. Each
node in the network is located on a point in a two dimensional grid, and
whenever a node sends a message, all awake nodes within distance r receive the
message. In the broadcast problem, some node wants to successfully send a
message to all other nodes in the network even when up to a 1/2 fraction of the
nodes within every neighborhood can be deleted by an adversary. The set of
deleted nodes is carefully chosen by the adversary to foil our algorithm and
moreover, the set of deleted nodes may change periodically. This models
worst-case behavior due to mobile nodes, static nodes losing power or simply
some points in the grid being unoccupied. A trivial solution requires each node
in the network to be awake roughly 1/2 the time, and a trivial lower bound
shows that each node must be awake for at least a 1/n fraction of the time. Our
first result is an algorithm that requires each node to be awake for only a
1/sqrt(n) fraction of the time in expectation. Our algorithm achieves this
while ensuring correctness with probability 1, and keeping optimal values for
other resource costs such as latency and number of messages sent. We give a
lower-bound that shows that this reduction in power consumption is
asymptotically optimal when latency and number of messages sent must be
optimal. If we can increase the latency and messages sent by only a log*n
factor we give a Las Vegas algorithm that requires each node to be awake for
only a (log*n)/n expected fraction of the time; we give a lower-bound showing
that this second algorithm is near optimal. Finally, we show how to ensure
energy-efficient broadcast in the presence of Byzantine faults.
| cs.DS | we address the problem of minimizing power consumption when performing reliable broadcast on a radio network under the following popular model each node in the network is located on a point in a two dimensional grid and whenever a node sends a message all awake nodes within distance r receive the message in the broadcast problem some node wants to successfully send a message to all other nodes in the network even when up to a 12 fraction of the nodes within every neighborhood can be deleted by an adversary the set of deleted nodes is carefully chosen by the adversary to foil our algorithm and moreover the set of deleted nodes may change periodically this models worstcase behavior due to mobile nodes static nodes losing power or simply some points in the grid being unoccupied a trivial solution requires each node in the network to be awake roughly 12 the time and a trivial lower bound shows that each node must be awake for at least a 1n fraction of the time our first result is an algorithm that requires each node to be awake for only a 1sqrtn fraction of the time in expectation our algorithm achieves this while ensuring correctness with probability 1 and keeping optimal values for other resource costs such as latency and number of messages sent we give a lowerbound that shows that this reduction in power consumption is asymptotically optimal when latency and number of messages sent must be optimal if we can increase the latency and messages sent by only a logn factor we give a las vegas algorithm that requires each node to be awake for only a lognn expected fraction of the time we give a lowerbound showing that this second algorithm is near optimal finally we show how to ensure energyefficient broadcast in the presence of byzantine faults | [['we', 'address', 'the', 'problem', 'of', 'minimizing', 'power', 'consumption', 'when', 'performing', 'reliable', 'broadcast', 'on', 'a', 'radio', 'network', 'under', 'the', 'following', 'popular', 'model', 'each', 'node', 'in', 'the', 'network', 'is', 'located', 'on', 'a', 'point', 'in', 'a', 'two', 'dimensional', 'grid', 'and', 'whenever', 'a', 'node', 'sends', 'a', 'message', 'all', 'awake', 'nodes', 'within', 'distance', 'r', 'receive', 'the', 'message', 'in', 'the', 'broadcast', 'problem', 'some', 'node', 'wants', 'to', 'successfully', 'send', 'a', 'message', 'to', 'all', 'other', 'nodes', 'in', 'the', 'network', 'even', 'when', 'up', 'to', 'a', '12', 'fraction', 'of', 'the', 'nodes', 'within', 'every', 'neighborhood', 'can', 'be', 'deleted', 'by', 'an', 'adversary', 'the', 'set', 'of', 'deleted', 'nodes', 'is', 'carefully', 'chosen', 'by', 'the', 'adversary', 'to', 'foil', 'our', 'algorithm', 'and', 'moreover', 'the', 'set', 'of', 'deleted', 'nodes', 'may', 'change', 'periodically', 'this', 'models', 'worstcase', 'behavior', 'due', 'to', 'mobile', 'nodes', 'static', 'nodes', 'losing', 'power', 'or', 'simply', 'some', 'points', 'in', 'the', 'grid', 'being', 'unoccupied', 'a', 'trivial', 'solution', 'requires', 'each', 'node', 'in', 'the', 'network', 'to', 'be', 'awake', 'roughly', '12', 'the', 'time', 'and', 'a', 'trivial', 'lower', 'bound', 'shows', 'that', 'each', 'node', 'must', 'be', 'awake', 'for', 'at', 'least', 'a', '1n', 'fraction', 'of', 'the', 'time', 'our', 'first', 'result', 'is', 'an', 'algorithm', 'that', 'requires', 'each', 'node', 'to', 'be', 'awake', 'for', 'only', 'a', '1sqrtn', 'fraction', 'of', 'the', 'time', 'in', 'expectation', 'our', 'algorithm', 'achieves', 'this', 'while', 'ensuring', 'correctness', 'with', 'probability', '1', 'and', 'keeping', 'optimal', 'values', 'for', 'other', 'resource', 'costs', 'such', 'as', 'latency', 'and', 'number', 'of', 'messages', 'sent', 'we', 'give', 'a', 'lowerbound', 'that', 'shows', 'that', 'this', 'reduction', 'in', 'power', 'consumption', 'is', 'asymptotically', 'optimal', 'when', 'latency', 'and', 'number', 'of', 'messages', 'sent', 'must', 'be', 'optimal', 'if', 'we', 'can', 'increase', 'the', 'latency', 'and', 'messages', 'sent', 'by', 'only', 'a', 'logn', 'factor', 'we', 'give', 'a', 'las', 'vegas', 'algorithm', 'that', 'requires', 'each', 'node', 'to', 'be', 'awake', 'for', 'only', 'a', 'lognn', 'expected', 'fraction', 'of', 'the', 'time', 'we', 'give', 'a', 'lowerbound', 'showing', 'that', 'this', 'second', 'algorithm', 'is', 'near', 'optimal', 'finally', 'we', 'show', 'how', 'to', 'ensure', 'energyefficient', 'broadcast', 'in', 'the', 'presence', 'of', 'byzantine', 'faults']] | [-0.20702362418608758, 0.07437693580623768, -0.037167842097544264, -0.0028865310068854092, -0.056122654497406436, -0.24351832347026872, 0.18736562813092686, 0.3705651853143156, -0.2867788559094849, -0.3085732375901542, 0.09021263127252882, -0.3120593251750886, -0.11164530817476556, 0.11756465533442349, -0.11497613751859943, 0.025075920873924767, 0.07236182360557997, 0.14592643289504315, 0.023386945983430867, -0.3386772338912783, 0.24313273521752057, 0.08896802277168603, 0.2307431459137537, 0.025679798583344866, 0.09679355010055729, -0.004005782342362173, 0.04481334130571323, 0.02190870477163917, -0.05550207439609419, 0.04218835112922086, 0.3013306772251242, 0.179113177189296, 0.3289147969742206, -0.45509019147250185, -0.1612307655197059, 0.1580472258627897, 0.15477750002041846, 0.1138975734846564, -0.008298594536618435, -0.2446804396992001, 0.17445246680582419, -0.17323346049102886, -0.06493158472180487, 0.015599284546553764, 0.0022620851788850665, 0.031710521610940484, -0.3028356744519745, -0.00036260688339863394, -0.006348363053005394, -0.011784061620729255, -0.0003749884218188503, -0.06386553921923645, -0.015871805769563156, 0.18469232404338948, 0.012220205302488867, 0.08395433906314316, 0.11756523736375067, -0.0849117667456491, -0.12869535717950428, 0.35928320657449825, 0.01107600408521086, -0.1883158436268086, 0.10521006577743916, -0.09620728035695537, -0.14822338687589023, 0.15360800742659972, 0.2049663623314182, 0.07425533185417622, -0.1289638160579762, 0.03144017641427309, -0.04284393332723806, 0.22527862980015784, 0.08695130692011283, 0.04471107756773245, 0.13329160924018346, 0.15818048173239196, 0.17365711669454165, 0.14262647926129257, -0.07034618727422792, -0.05358290901968201, -0.2845191877006785, -0.15819313607504892, -0.2460884837588916, 0.0362459482590466, -0.144439049449067, -0.10257994804929182, 0.40921010393769897, 0.14065868416624022, 0.228124410961943, 0.13362860750907302, 0.3520110663340026, 0.09206199184224736, 0.03987317711746314, 0.2348652389006008, 0.16415554048620845, 0.006101821430560961, 0.08012098088972783, -0.1568654711701279, 0.12832774099981273, 0.05168342873044191] |
710.2533 | Modularity-Maximizing Network Communities via Mathematical Programming | In many networks, it is of great interest to identify "communities",
unusually densely knit groups of individuals. Such communities often shed light
on the function of the networks or underlying properties of the individuals.
Recently, Newman suggested "modularity" as a natural measure of the quality of
a network partitioning into communities. Since then, various algorithms have
been proposed for (approximately) maximizing the modularity of the partitioning
determined.
In this paper, we introduce the technique of rounding mathematical programs
to the problem of modularity maximization, presenting two novel algorithms.
More specifically, the algorithms round solutions to linear and vector
programs. Importantly, the linear programing algorithm comes with an a
posteriori approximation guarantee: by comparing the solution quality to the
fractional solution of the linear program, a bound on the available "room for
improvement" can be obtained. The vector programming algorithm provides a
similar bound for the best partition into two communities. We evaluate both
algorithms using experiments on several standard test cases for network
partitioning algorithms, and find that they perform comparably or better than
past algorithms.
| physics.data-an | in many networks it is of great interest to identify communities unusually densely knit groups of individuals such communities often shed light on the function of the networks or underlying properties of the individuals recently newman suggested modularity as a natural measure of the quality of a network partitioning into communities since then various algorithms have been proposed for approximately maximizing the modularity of the partitioning determined in this paper we introduce the technique of rounding mathematical programs to the problem of modularity maximization presenting two novel algorithms more specifically the algorithms round solutions to linear and vector programs importantly the linear programing algorithm comes with an a posteriori approximation guarantee by comparing the solution quality to the fractional solution of the linear program a bound on the available room for improvement can be obtained the vector programming algorithm provides a similar bound for the best partition into two communities we evaluate both algorithms using experiments on several standard test cases for network partitioning algorithms and find that they perform comparably or better than past algorithms | [['in', 'many', 'networks', 'it', 'is', 'of', 'great', 'interest', 'to', 'identify', 'communities', 'unusually', 'densely', 'knit', 'groups', 'of', 'individuals', 'such', 'communities', 'often', 'shed', 'light', 'on', 'the', 'function', 'of', 'the', 'networks', 'or', 'underlying', 'properties', 'of', 'the', 'individuals', 'recently', 'newman', 'suggested', 'modularity', 'as', 'a', 'natural', 'measure', 'of', 'the', 'quality', 'of', 'a', 'network', 'partitioning', 'into', 'communities', 'since', 'then', 'various', 'algorithms', 'have', 'been', 'proposed', 'for', 'approximately', 'maximizing', 'the', 'modularity', 'of', 'the', 'partitioning', 'determined', 'in', 'this', 'paper', 'we', 'introduce', 'the', 'technique', 'of', 'rounding', 'mathematical', 'programs', 'to', 'the', 'problem', 'of', 'modularity', 'maximization', 'presenting', 'two', 'novel', 'algorithms', 'more', 'specifically', 'the', 'algorithms', 'round', 'solutions', 'to', 'linear', 'and', 'vector', 'programs', 'importantly', 'the', 'linear', 'programing', 'algorithm', 'comes', 'with', 'an', 'a', 'posteriori', 'approximation', 'guarantee', 'by', 'comparing', 'the', 'solution', 'quality', 'to', 'the', 'fractional', 'solution', 'of', 'the', 'linear', 'program', 'a', 'bound', 'on', 'the', 'available', 'room', 'for', 'improvement', 'can', 'be', 'obtained', 'the', 'vector', 'programming', 'algorithm', 'provides', 'a', 'similar', 'bound', 'for', 'the', 'best', 'partition', 'into', 'two', 'communities', 'we', 'evaluate', 'both', 'algorithms', 'using', 'experiments', 'on', 'several', 'standard', 'test', 'cases', 'for', 'network', 'partitioning', 'algorithms', 'and', 'find', 'that', 'they', 'perform', 'comparably', 'or', 'better', 'than', 'past', 'algorithms']] | [-0.0944854687586485, -0.013929937934997062, -0.11012357791928067, 0.09804134527009657, -0.09709301577690481, -0.1584812545767239, 0.0753869691999915, 0.3927091473544186, -0.2700912809443914, -0.3522118425726975, 0.10693718857642538, -0.25525827405032364, -0.20937227431700609, 0.19734409350150434, -0.04625387528159825, 0.11021280316741798, 0.08321154849942435, 0.034942270671969956, -0.03837519739714811, -0.31874551542965823, 0.2842762137231396, 0.05662947461876849, 0.3011795516940765, 0.03578564156090248, 0.09868502709750002, -0.009703674787570808, -0.024144577732923524, 0.08027364206223163, -0.10128931747770119, 0.16478970280083807, 0.2829865773184627, 0.24359136847488116, 0.3515384003932757, -0.4218215460370464, -0.18613040311240844, 0.1269877174742181, 0.1418305539303798, 0.09658685937888963, -0.012980740433787023, -0.2839659774802964, 0.09704188102345639, -0.12092141426877458, -0.03632814643391281, -0.10619476469582878, -0.033391440910318954, 0.017567873763751282, -0.2633481550834734, 0.007486196077397009, 0.03984057854342444, 0.021414583966940303, -0.041866163853476544, -0.16726491225629367, 0.03321354893308704, 0.11354567938145589, 0.04609372646584895, 0.024949050845779395, 0.1056025071500864, -0.13695102264347786, -0.17913330084742152, 0.3731283511521972, -0.03531692149516113, -0.1975063417625775, 0.18848066601706456, -0.05465555179663087, -0.1689346931485819, 0.11384956266688691, 0.24005108733597974, 0.126956794236321, -0.1638520760514604, 0.04766319647486936, -0.07352219151454681, 0.16059762696254024, 0.06894087408231413, 0.012156075414333662, 0.14329604821713557, 0.2106515511816476, 0.13745100845732272, 0.1479279527550468, -0.014874333498565566, -0.08507255376422439, -0.17589759464185176, -0.1513202558860278, -0.19966794407016344, -0.031402229172685606, -0.12475119881971543, -0.17902383409355851, 0.4387150954889049, 0.12318023196844892, 0.17905225657424043, 0.11690404017413543, 0.3126754344259759, 0.08710953868616013, 0.08027871936726362, 0.10645079010282643, 0.20786223671695386, 0.09921175648130222, 0.07904838468212719, -0.18183707025177268, 0.10562485600927506, 0.05900597924615299] |
710.2534 | On Torsion Fields in Higher Derivative Quantum Gravity | We consider axial torsion fields which appear in higher derivative quantum
gravity. It is shown, in general, that the torsion field possesses states with
two spins, one and zero, with different masses. The first-order formulation of
torsion fields is performed. Projection operators extracting pure spin and mass
states are given. We obtain the Lagrangian in the framework of the first order
formalism and energy-momentum tensor. The effective interaction of torsion
fields with electromagnetic fields is discussed. The Hamiltonian form of the
first order torsion field equation is given.
| gr-qc hep-th | we consider axial torsion fields which appear in higher derivative quantum gravity it is shown in general that the torsion field possesses states with two spins one and zero with different masses the firstorder formulation of torsion fields is performed projection operators extracting pure spin and mass states are given we obtain the lagrangian in the framework of the first order formalism and energymomentum tensor the effective interaction of torsion fields with electromagnetic fields is discussed the hamiltonian form of the first order torsion field equation is given | [['we', 'consider', 'axial', 'torsion', 'fields', 'which', 'appear', 'in', 'higher', 'derivative', 'quantum', 'gravity', 'it', 'is', 'shown', 'in', 'general', 'that', 'the', 'torsion', 'field', 'possesses', 'states', 'with', 'two', 'spins', 'one', 'and', 'zero', 'with', 'different', 'masses', 'the', 'firstorder', 'formulation', 'of', 'torsion', 'fields', 'is', 'performed', 'projection', 'operators', 'extracting', 'pure', 'spin', 'and', 'mass', 'states', 'are', 'given', 'we', 'obtain', 'the', 'lagrangian', 'in', 'the', 'framework', 'of', 'the', 'first', 'order', 'formalism', 'and', 'energymomentum', 'tensor', 'the', 'effective', 'interaction', 'of', 'torsion', 'fields', 'with', 'electromagnetic', 'fields', 'is', 'discussed', 'the', 'hamiltonian', 'form', 'of', 'the', 'first', 'order', 'torsion', 'field', 'equation', 'is', 'given']] | [-0.23384885265444277, 0.20755656514401463, -0.06352774399221578, 0.060606353678105566, -0.10041105779237114, -0.11324178272942928, -0.12712801024793985, 0.3225342556834221, -0.2156044677302072, -0.2858798233368857, 0.023420995817022314, -0.24435935710260476, -0.12743920951404356, 0.10557070153299719, 0.0356744542633268, 0.007348009168212725, -0.023221820494985546, 0.14015847300602632, -0.09264846407247453, -0.24004029865450735, 0.40387460169503436, -0.02480392274049915, 0.24328673228790815, 0.0489173922740685, 0.14352632682262498, -0.004660452885383909, 0.01856910140486434, 0.03548863726742142, -0.10866558515053013, 0.0856737591926834, 0.21693687165878311, 0.034304089603458786, 0.16189775520681657, -0.4323602949946441, -0.1898246633037078, 0.08749552457381717, 0.04839483064874499, 0.16226669602408286, -0.046276229857043785, -0.28516315680462867, 0.03900506123318337, -0.17940611064180054, -0.15660426776263525, -0.12022141888949343, -0.00351618695739572, -0.0459461181466891, -0.257300955507989, 0.09959747857746235, 0.04249053693439981, 0.03513069140767171, -0.1225062460553917, -0.11538753019174858, -0.04295241815800017, 0.08652442412196913, 0.1165215629510137, 0.07762704381126571, 0.10207436306783083, -0.15573646932501684, -0.10836495099779726, 0.39911660574249586, -0.11921944250670177, -0.2504619356477633, 0.12356120713626627, -0.1700607396196574, -0.10513047862861474, 0.09605981112796061, 0.1165367470080541, 0.17813348463757642, -0.1448373172395143, 0.1684836206662691, 0.015448890954510054, 0.09520098409319128, 0.06785205165876752, 0.0247769253255683, 0.2120473824748346, 0.061270379927009344, 0.05007910099811852, 0.1217086949353953, -0.03109935283216394, -0.13009748645973476, -0.3599914986301552, -0.19998690358397653, -0.16364767505332234, 0.06773443859261037, -0.09866761658089342, -0.15177091934013084, 0.4133484978308182, 0.13910802646370773, 0.11337113676828184, 0.02863226619427389, 0.2772188834338026, 0.1913863442393697, 0.1019759688298853, 0.07568979415703904, 0.28677368500608613, 0.2859201810576699, 0.03834950810414739, -0.21732444982361895, -0.08300594073278428, 0.10434649389141916] |
710.2535 | O'Raifeartaigh models with spontaneous R-symmetry breaking | O'Raifeartaigh models with general R-charge assignments can have vacua where
both supersymmetry and R-symmetry are spontaneously broken. Most of these vacua
are metastable because the potential shows a runaway behaviour. We explain the
relation between runaway directions and R-symmetry.
| hep-th | oraifeartaigh models with general rcharge assignments can have vacua where both supersymmetry and rsymmetry are spontaneously broken most of these vacua are metastable because the potential shows a runaway behaviour we explain the relation between runaway directions and rsymmetry | [['oraifeartaigh', 'models', 'with', 'general', 'rcharge', 'assignments', 'can', 'have', 'vacua', 'where', 'both', 'supersymmetry', 'and', 'rsymmetry', 'are', 'spontaneously', 'broken', 'most', 'of', 'these', 'vacua', 'are', 'metastable', 'because', 'the', 'potential', 'shows', 'a', 'runaway', 'behaviour', 'we', 'explain', 'the', 'relation', 'between', 'runaway', 'directions', 'and', 'rsymmetry']] | [-0.16193494546967438, 0.2654458273154421, -0.05814226550790362, 0.16199554617588335, -0.09705617515226969, -0.24786783756019595, 0.02611169732438448, 0.3995962219360547, -0.13421964740010503, -0.3198131747925893, 0.09896486877010037, -0.2635658265163119, -0.12225257103832868, 0.002055289271550301, -0.06195386119473439, 0.002563686101124264, -0.039387026944985755, -0.04533992994290132, -0.04357403481247811, -0.2471051531819961, 0.30220132688872325, -0.06524337618014751, 0.3185127148261437, 0.031491452971330054, 0.03624291100407927, -0.15950389543118385, 0.088062459602952, -0.06274941766586824, -0.06450034732906482, 0.06703493414589992, 0.21263325888223614, 0.08352031773672654, 0.10125094542327599, -0.49220644376980954, -0.2236070841168746, 0.21152921383961654, 0.25002092321236163, 0.18064678268125042, -0.10449298466436374, -0.26278920949269563, 0.04997332199500539, -0.15044690229189703, -0.11764289266788043, -0.15006088639776677, 0.002077042889327575, -0.06262045126790419, -0.27043187188414425, 0.12146916302541892, -0.08294813134349309, 0.04468540682529028, -0.11387010746731017, -0.06215982544773187, -0.19962800892356497, 0.011436721704040583, 0.29360096433605903, -0.023829764161163416, 0.13094329902042562, -0.23898254960584334, -0.16051047789649323, 0.4118981113991676, 0.022329801789078958, -0.1659281810697837, 0.19467191418441823, -0.1386781028853968, -0.2444553193755639, 0.10731179888049762, 0.06276692487359142, 0.136546051225219, -0.08723971460205622, 0.21274157877092081, 0.03997776681222977, 0.0850942039814515, 0.10222673650162342, 0.032051773474683076, 0.3815595499980144, 0.07499388896693022, 0.03668243300098066, 0.07941034643982466, 0.011851609230805665, -0.17356044495812592, -0.4351669714236871, -0.11091831519913214, -0.04919039532661629, 0.08803492149290366, -0.09384157924050203, -0.09679196107511719, 0.36941290341126615, 0.11812013369770004, 0.21961801764197075, 0.055125333106097504, 0.10044442476609196, 0.1247985830817085, 0.09799464703656924, 0.06855015186234735, 0.25952828565660196, 0.08345297929078627, 0.05030328268185258, -0.2860657961991353, -0.08754281515780932, 0.081566361638789] |
710.2536 | Isoperimetric regions in spherical cones and Yamabe constants of
$M\times S^1$ | Given closed Riemannian manifold $(M^n, g)$ of positive Ricci curvature
$Ricci(g) \geq (n-1)g$ we study isoperimetric regions on the spherical cone
over $M$. When $g$ is Einstein we use this to compute the Yamabe constant of
$(M \times {\bf R}, g + dt^2)$ and so to obtain lower bounds for the Yamabe
invariant of $M\times S^1$.
| math.DG | given closed riemannian manifold mn g of positive ricci curvature riccig geq n1g we study isoperimetric regions on the spherical cone over m when g is einstein we use this to compute the yamabe constant of m times bf r g dt2 and so to obtain lower bounds for the yamabe invariant of mtimes s1 | [['given', 'closed', 'riemannian', 'manifold', 'mn', 'g', 'of', 'positive', 'ricci', 'curvature', 'riccig', 'geq', 'n1g', 'we', 'study', 'isoperimetric', 'regions', 'on', 'the', 'spherical', 'cone', 'over', 'm', 'when', 'g', 'is', 'einstein', 'we', 'use', 'this', 'to', 'compute', 'the', 'yamabe', 'constant', 'of', 'm', 'times', 'bf', 'r', 'g', 'dt2', 'and', 'so', 'to', 'obtain', 'lower', 'bounds', 'for', 'the', 'yamabe', 'invariant', 'of', 'mtimes', 's1']] | [-0.2713724050916872, 0.06948851815969595, -0.015139778302806729, 0.024920011536692672, -0.12710176257170597, -0.21501180656113714, -0.06884006983688418, 0.38050220892676767, -0.19403178592757234, -0.282012495932714, 0.10557729214921875, -0.28900188225198464, -0.08865424845683968, 0.11426161647826996, -0.09796438740570766, -0.025714089812816313, 0.016773694221211492, 0.1578764900486073, -0.17009550842614668, -0.2852050922459589, 0.3947398469713077, -0.06122417609154616, 0.14150229407439255, 0.11748980679373555, 0.11132763995665987, -0.09646922183873237, 0.026463404166037745, 0.04105710600204063, -0.3537779518596406, 0.10801562471842428, 0.21184427560886965, 0.09912709419984582, 0.1815493052456317, -0.3469678621985159, -0.17663424616714693, 0.22143257992728702, 0.12159479999001015, -0.08168408510117035, 0.03430748336184067, -0.3190628102506107, 0.1566852394333285, -0.02706493029616914, -0.13499832434364473, -0.03287039396686936, 0.17586828476556068, -0.08036314023500483, -0.24539428246471118, 0.0654773597412233, 0.1047438614703012, 0.01886669377673347, -0.07436085005624676, -0.17591853656823625, -0.05544384758708612, 0.03516145919302461, 0.060204649427554234, 0.13520997707547514, 0.10429603902113466, 0.003989676097056495, -0.0021825430317307416, 0.3347718297802615, -0.220410064486611, -0.24489800147009347, -0.0028256150885080955, -0.20572843341121697, -0.10345974145457149, 0.12169105176515174, 0.21688072088192095, 0.28766448172863646, 0.0019546566728199394, 0.2542315650333756, -0.11611911440092437, 0.06518580989455278, 0.13851255512321894, -0.05291397103442336, 0.094263717971461, 0.015242078657841907, 0.26287146011051143, 0.08524698294910057, -0.019652695663027325, 0.05023903669437991, -0.363977955724552, -0.21677862142898002, -0.22720054130263204, 0.30750375203261116, -0.19358393149247244, -0.14413073368783477, 0.30936421608587483, -0.03842812407550947, 0.1968116315854889, 0.1890507312052233, 0.19944235218583412, 0.022086762190567998, -0.020226600514021965, 0.25770226009365804, 0.11535509763601816, 0.285167483472318, 0.010745839617777406, -0.19203094443095461, -0.13305340866329815, 0.188677643619056] |
710.2537 | Spookytechnology and Society | New technologies based on the exploitation of so-called "second order"
quantum phenomena - such as quantum entanglement - deserve a public-friendly,
rational, and sexy name. Spookytechnology is that unifying term. From
historical and motivational perspectives, this name has greater value than the
many variations of quantum this and quantum that presently used. As many
already believe, the pursuit of spookytechnology has profound implications for
the development of the physical and information sciences and ultimately for
society at large. Spookytechnology will find its place in the increasingly
dense line of major technological revolutions of our time: quantum, info, bio,
nano, spooky.
| physics.pop-ph cond-mat.mtrl-sci physics.soc-ph quant-ph | new technologies based on the exploitation of socalled second order quantum phenomena such as quantum entanglement deserve a publicfriendly rational and sexy name spookytechnology is that unifying term from historical and motivational perspectives this name has greater value than the many variations of quantum this and quantum that presently used as many already believe the pursuit of spookytechnology has profound implications for the development of the physical and information sciences and ultimately for society at large spookytechnology will find its place in the increasingly dense line of major technological revolutions of our time quantum info bio nano spooky | [['new', 'technologies', 'based', 'on', 'the', 'exploitation', 'of', 'socalled', 'second', 'order', 'quantum', 'phenomena', 'such', 'as', 'quantum', 'entanglement', 'deserve', 'a', 'publicfriendly', 'rational', 'and', 'sexy', 'name', 'spookytechnology', 'is', 'that', 'unifying', 'term', 'from', 'historical', 'and', 'motivational', 'perspectives', 'this', 'name', 'has', 'greater', 'value', 'than', 'the', 'many', 'variations', 'of', 'quantum', 'this', 'and', 'quantum', 'that', 'presently', 'used', 'as', 'many', 'already', 'believe', 'the', 'pursuit', 'of', 'spookytechnology', 'has', 'profound', 'implications', 'for', 'the', 'development', 'of', 'the', 'physical', 'and', 'information', 'sciences', 'and', 'ultimately', 'for', 'society', 'at', 'large', 'spookytechnology', 'will', 'find', 'its', 'place', 'in', 'the', 'increasingly', 'dense', 'line', 'of', 'major', 'technological', 'revolutions', 'of', 'our', 'time', 'quantum', 'info', 'bio', 'nano', 'spooky']] | [-0.08560312234718974, 0.1307401271769777, -0.09612992249215797, 0.04854516353104069, -0.10048652095914197, -0.13988162983544802, 0.038752208412915934, 0.2817789209948387, -0.24844556073852195, -0.2898318042862229, 0.13785191522401874, -0.25667661246067536, -0.20491946182058504, 0.24967881853687382, -0.06992909010053457, 0.05572395050633835, 0.03860252863766315, 0.054277721287993096, -0.031898562786712624, -0.2272103225501875, 0.2724947755147393, 0.07705618088827275, 0.2986204588160035, 0.1203560993890278, 0.10908717040729243, -0.002061450334925515, -0.0167238076828653, -0.01566982813528739, -0.10728296552724714, 0.14185599770280533, 0.30272031582232256, 0.1780859245417711, 0.3802603791506651, -0.44307675975142047, -0.24333111660477394, 0.07521477212139871, 0.11345071114434783, 0.11604932199891967, -0.06744931074232834, -0.2963023011106998, 0.032307907352029964, -0.16765259320042483, -0.10866636222150798, -0.06280588430915184, 0.07711191226553638, -0.025653880492124397, -0.14432357758050784, 0.01712157241126988, 0.06537462519675803, 0.10831329168286175, 0.02407817441538403, -0.1486796124566657, 0.027483758072776254, 0.17782912919695568, 0.016341979828818392, 0.03017332610943413, 0.1299883035074648, -0.1583215124992421, -0.18808718299260363, 0.45058047767573345, 0.013140121732400681, -0.0725888968105816, 0.2137948066641305, -0.1205168203280967, -0.18856074976793025, 0.03839036606465621, 0.16552234060024298, 0.04371174249172327, -0.14225805773943043, 0.072304740292869, 0.001802632197116812, 0.14547805348168671, 0.07350994303124025, 0.1297385684301844, 0.2697174385151205, 0.16101247705713226, 0.07776550287477828, 0.0613513991702348, -0.04975033279576261, -0.18310675847654542, -0.2529072757315589, -0.21109999652253464, -0.1755756273632869, 0.089896603031472, -0.07895549609308243, -0.16276280004725172, 0.3663970428945807, 0.1765784410138925, 0.1217646318594537, -0.038465464844193775, 0.2589548844262026, 0.046699008521803385, 0.10830338988550163, 0.026829001940010738, 0.25068921666631167, 0.0810434462861546, 0.17737897966677943, -0.15859048710293186, 0.10171636476782926, -0.004043235050630756] |
710.2538 | Detectability of CMB tensor B modes via delensing with weak lensing
galaxy surveys | We analyze the possibility of delensing CMB polarization maps using
foreground weak lensing (WL) information. We build an estimator of the CMB
lensing potential out of optimally combined projected potential estimators to
different source redshift bins. Our estimator is most sensitive to the redshift
depth of the WL survey, less so to the shape noise level. Estimators built
using galaxy surveys like LSST and SNAP yield a 30-50% reduction in the lensing
B-mode power. We illustrate the potential advantages of a 21-cm survey by
considering a fiducial WL survey for which we take the redshift depth zmax and
the effective angular concentration of sources n as free parameters. For a
noise level of 1 muK arcmin in the polarization map itself, as projected for a
CMBPol experiment, and a beam with FWHM=10 arcmin, we find that going to
zmax=20 at n=100 gal/sqarcmin yields a delensing performance similar to that of
a quadratic lensing potential estimator applied to small-scale CMB maps: the
lensing B-mode contamination is reduced by almost an order of magnitude. In
this case, there is also a reduction by a factor of ~4 in the detectability
threshold of the tensor B-mode power. At this CMB noise level, there is little
gain from sources with zmax>20. The delensing gains are lost if the CMB beam
exceeds ~20 arcmin. The delensing efficiency and useful zmax depend acutely on
the CMB map noise level, but beam sizes below 10 arcmin do not help. Delensing
via foreground sources does not require arcminute-resolution CMB observations,
a substantial practical advantage over the use of CMB observables for
delensing.
| astro-ph | we analyze the possibility of delensing cmb polarization maps using foreground weak lensing wl information we build an estimator of the cmb lensing potential out of optimally combined projected potential estimators to different source redshift bins our estimator is most sensitive to the redshift depth of the wl survey less so to the shape noise level estimators built using galaxy surveys like lsst and snap yield a 3050 reduction in the lensing bmode power we illustrate the potential advantages of a 21cm survey by considering a fiducial wl survey for which we take the redshift depth zmax and the effective angular concentration of sources n as free parameters for a noise level of 1 muk arcmin in the polarization map itself as projected for a cmbpol experiment and a beam with fwhm10 arcmin we find that going to zmax20 at n100 galsqarcmin yields a delensing performance similar to that of a quadratic lensing potential estimator applied to smallscale cmb maps the lensing bmode contamination is reduced by almost an order of magnitude in this case there is also a reduction by a factor of 4 in the detectability threshold of the tensor bmode power at this cmb noise level there is little gain from sources with zmax20 the delensing gains are lost if the cmb beam exceeds 20 arcmin the delensing efficiency and useful zmax depend acutely on the cmb map noise level but beam sizes below 10 arcmin do not help delensing via foreground sources does not require arcminuteresolution cmb observations a substantial practical advantage over the use of cmb observables for delensing | [['we', 'analyze', 'the', 'possibility', 'of', 'delensing', 'cmb', 'polarization', 'maps', 'using', 'foreground', 'weak', 'lensing', 'wl', 'information', 'we', 'build', 'an', 'estimator', 'of', 'the', 'cmb', 'lensing', 'potential', 'out', 'of', 'optimally', 'combined', 'projected', 'potential', 'estimators', 'to', 'different', 'source', 'redshift', 'bins', 'our', 'estimator', 'is', 'most', 'sensitive', 'to', 'the', 'redshift', 'depth', 'of', 'the', 'wl', 'survey', 'less', 'so', 'to', 'the', 'shape', 'noise', 'level', 'estimators', 'built', 'using', 'galaxy', 'surveys', 'like', 'lsst', 'and', 'snap', 'yield', 'a', '3050', 'reduction', 'in', 'the', 'lensing', 'bmode', 'power', 'we', 'illustrate', 'the', 'potential', 'advantages', 'of', 'a', '21cm', 'survey', 'by', 'considering', 'a', 'fiducial', 'wl', 'survey', 'for', 'which', 'we', 'take', 'the', 'redshift', 'depth', 'zmax', 'and', 'the', 'effective', 'angular', 'concentration', 'of', 'sources', 'n', 'as', 'free', 'parameters', 'for', 'a', 'noise', 'level', 'of', '1', 'muk', 'arcmin', 'in', 'the', 'polarization', 'map', 'itself', 'as', 'projected', 'for', 'a', 'cmbpol', 'experiment', 'and', 'a', 'beam', 'with', 'fwhm10', 'arcmin', 'we', 'find', 'that', 'going', 'to', 'zmax20', 'at', 'n100', 'galsqarcmin', 'yields', 'a', 'delensing', 'performance', 'similar', 'to', 'that', 'of', 'a', 'quadratic', 'lensing', 'potential', 'estimator', 'applied', 'to', 'smallscale', 'cmb', 'maps', 'the', 'lensing', 'bmode', 'contamination', 'is', 'reduced', 'by', 'almost', 'an', 'order', 'of', 'magnitude', 'in', 'this', 'case', 'there', 'is', 'also', 'a', 'reduction', 'by', 'a', 'factor', 'of', '4', 'in', 'the', 'detectability', 'threshold', 'of', 'the', 'tensor', 'bmode', 'power', 'at', 'this', 'cmb', 'noise', 'level', 'there', 'is', 'little', 'gain', 'from', 'sources', 'with', 'zmax20', 'the', 'delensing', 'gains', 'are', 'lost', 'if', 'the', 'cmb', 'beam', 'exceeds', '20', 'arcmin', 'the', 'delensing', 'efficiency', 'and', 'useful', 'zmax', 'depend', 'acutely', 'on', 'the', 'cmb', 'map', 'noise', 'level', 'but', 'beam', 'sizes', 'below', '10', 'arcmin', 'do', 'not', 'help', 'delensing', 'via', 'foreground', 'sources', 'does', 'not', 'require', 'arcminuteresolution', 'cmb', 'observations', 'a', 'substantial', 'practical', 'advantage', 'over', 'the', 'use', 'of', 'cmb', 'observables', 'for', 'delensing']] | [-0.06826609499716702, 0.05211639991847243, -0.06937385682697193, 0.09972448693498825, -0.07965876170648978, -0.09100512630650953, 0.016029375239024656, 0.38808494705993396, -0.23748298395971337, -0.3021327107285078, 0.059144862644517654, -0.347031131600782, -0.05922149687987537, 0.2288210754690226, -0.012554642006468315, 0.026959949603322177, 0.06082550798489068, -0.08394945827939619, -0.06570702338207271, -0.32883662223332344, 0.2684016906351854, 0.22849017585842654, 0.25796797151202694, -0.00833338376782754, 0.14661490600735236, -0.051125212429234616, -0.10332245415327354, 0.0595491110929288, -0.1251235420048313, 0.03817066794547897, 0.24915393727759902, 0.18455748345452147, 0.20784212291742174, -0.29313179097102526, -0.212182777439459, 0.1613833339490856, 0.13438431716573318, 0.12568194172300326, -0.020885323258922794, -0.28644584125498884, 0.08187313337783472, -0.15525567373260857, -0.0852222824236378, -0.04822918039549572, -0.03701522425533487, -0.002128053169984084, -0.2670031626995366, 0.14991111908345303, 0.04353070666883678, 0.0916743312174311, -0.01312113244068594, -0.15903638429008424, -0.00848506198828825, 0.05754256854012895, -0.011172177846758412, 0.09097239476843522, 0.19239121562053557, -0.17281143677850755, -0.0027305998261838863, 0.3684590162995916, -0.11558126587501297, -0.1241399144109052, 0.06636969134426461, -0.20849030613003727, -0.16458606821341584, 0.11947546958108432, 0.17467398754177757, 0.006949173402077017, -0.12846854113875172, 0.076870157090553, 0.07428126524632367, 0.28136548998837285, 0.12069603096460924, 0.037430431827278184, 0.2981558593643758, 0.08322151334813008, 0.2033679926485862, 0.1174286252944372, -0.26032286549363143, 0.06288487915433227, -0.28853840810390047, -0.02277200605827742, -0.16883228237991435, 0.10834416068806044, -0.17449048170372128, -0.12645726532321602, 0.3927461602438528, 0.20385521062148304, 0.19321384218167692, 0.08752919979474078, 0.3861927619347206, 0.07399367353153559, 0.08723284677924732, 0.015165297628174392, 0.3266769519075751, 0.13393070199347745, 0.06447768092442017, -0.17869504884113738, -0.009364162697098576, -0.07030619431663161] |
710.2539 | Low energy effective theory on a regularized brane in 6D gauged chiral
supergravity | We derive the low energy effective theory on a brane in six-dimensional
chiral supergravity. The conical 3-brane singularities are resolved by
introducing cylindrical codimension one 4-branes whose interiors are capped by
a regular spacetime. The effective theory is described by the Brans-Dicke (BD)
theory with the BD parameter given by $\omega_{\rm BD}=1/2$. The BD field is
originated from a modulus which is associated with the scaling symmetry of the
system. If the dilaton potentials on the branes preserve the scaling symmetry,
the scalar field has an exponential potential in the Einstein frame. We show
that the time dependent solutions driven by the modulus in the four-dimensional
effective theory can be lifted up to the six-dimensional exact solutions found
in the literature. Based on the effective theory, we discuss a possible way to
stabilize the modulus to recover standard cosmology and also study the
implication for the cosmological constant problem.
| hep-th astro-ph gr-qc | we derive the low energy effective theory on a brane in sixdimensional chiral supergravity the conical 3brane singularities are resolved by introducing cylindrical codimension one 4branes whose interiors are capped by a regular spacetime the effective theory is described by the bransdicke bd theory with the bd parameter given by omega_rm bd12 the bd field is originated from a modulus which is associated with the scaling symmetry of the system if the dilaton potentials on the branes preserve the scaling symmetry the scalar field has an exponential potential in the einstein frame we show that the time dependent solutions driven by the modulus in the fourdimensional effective theory can be lifted up to the sixdimensional exact solutions found in the literature based on the effective theory we discuss a possible way to stabilize the modulus to recover standard cosmology and also study the implication for the cosmological constant problem | [['we', 'derive', 'the', 'low', 'energy', 'effective', 'theory', 'on', 'a', 'brane', 'in', 'sixdimensional', 'chiral', 'supergravity', 'the', 'conical', '3brane', 'singularities', 'are', 'resolved', 'by', 'introducing', 'cylindrical', 'codimension', 'one', '4branes', 'whose', 'interiors', 'are', 'capped', 'by', 'a', 'regular', 'spacetime', 'the', 'effective', 'theory', 'is', 'described', 'by', 'the', 'bransdicke', 'bd', 'theory', 'with', 'the', 'bd', 'parameter', 'given', 'by', 'omega_rm', 'bd12', 'the', 'bd', 'field', 'is', 'originated', 'from', 'a', 'modulus', 'which', 'is', 'associated', 'with', 'the', 'scaling', 'symmetry', 'of', 'the', 'system', 'if', 'the', 'dilaton', 'potentials', 'on', 'the', 'branes', 'preserve', 'the', 'scaling', 'symmetry', 'the', 'scalar', 'field', 'has', 'an', 'exponential', 'potential', 'in', 'the', 'einstein', 'frame', 'we', 'show', 'that', 'the', 'time', 'dependent', 'solutions', 'driven', 'by', 'the', 'modulus', 'in', 'the', 'fourdimensional', 'effective', 'theory', 'can', 'be', 'lifted', 'up', 'to', 'the', 'sixdimensional', 'exact', 'solutions', 'found', 'in', 'the', 'literature', 'based', 'on', 'the', 'effective', 'theory', 'we', 'discuss', 'a', 'possible', 'way', 'to', 'stabilize', 'the', 'modulus', 'to', 'recover', 'standard', 'cosmology', 'and', 'also', 'study', 'the', 'implication', 'for', 'the', 'cosmological', 'constant', 'problem']] | [-0.14085570529946503, 0.1343665585226444, -0.09126798483359036, 0.07485225950163235, -0.09263287620096644, -0.1415792927460594, -0.01631778631850171, 0.28841016153062415, -0.23245635609664778, -0.26008768548962435, 0.09266080251797354, -0.2347307074972353, -0.16077995502289283, 0.11129756293902991, -0.05922195067427851, 0.01594699752466703, -0.03834182519868419, 0.07899203710729961, -0.09554254255340926, -0.24323862594728535, 0.3722794495170584, 0.05439032216531199, 0.24513554379243302, 0.012369956789739631, 0.09770704857333298, -0.03986727936835204, 0.014156233412339478, 0.0696574345394667, -0.2006144735373095, 0.10263943518873782, 0.18177486206813892, 0.04832722121107115, 0.1639046188651559, -0.4256660137703088, -0.25534689342728945, 0.08251252784897145, 0.1445786208323379, 0.1489397925946144, -0.048104402646139216, -0.2868159395592237, 0.09676306043449487, -0.13047007378190756, -0.20807988225243282, -0.05712402787144497, 0.007345291416198519, -0.05851889800632725, -0.23475420951207698, 0.11313878629742838, -0.013646083427718966, 0.0036804181920062446, -0.1174426730250235, -0.06922885237774509, -0.040813994817309886, 0.031938536303051795, 0.12175464180984057, 0.08533878124639946, 0.12548478348086262, -0.14508731071554073, -0.0901937039602057, 0.382822337126158, -0.12212658988003544, -0.2467519940770659, 0.1260955801274552, -0.12154237774351763, -0.07830895623664146, 0.09811170840308674, 0.1009694074368658, 0.14910361122944066, -0.13874219390374884, 0.2508118048299366, 0.0012370742593161962, 0.15115385108573892, 0.10183933334475434, 0.006235587857411923, 0.2686128417923543, 0.11240608954638545, 0.049539376156816785, 0.11327769542726487, -0.021752689696448804, -0.1307413624918145, -0.3736970874833295, -0.11255223141917078, -0.15370640669307495, 0.10146988015244338, -0.17838332663607592, -0.16291366407106556, 0.3556704936781898, 0.07209105754107539, 0.17955686571076512, 0.03806736742577364, 0.23468912158136232, 0.13686733320984687, 0.08103138913645887, 0.06198296014067514, 0.3149587422345035, 0.15186533802723814, 0.07938100612797849, -0.2570593511808437, -0.08957248104018839, 0.11888735702047376] |
710.254 | Modulated Perturbations from Instant Preheating after new Ekpyrosis | We present a mechanism to transfer the spectrum of perturbations in a scalar
isocurvature field $\xi$ onto the matter content in the radiation era via
modulated, instant preheating after ekpyrosis. In this setup, $\xi$ determines
the coupling constant relevant for the decay of a preheat matter field into
Fermions. The resulting power spectrum is scale invariant if $\xi$ remains
close to a scaling solution in new ekpyrotic models of the universe; by
construction the spectrum is independent of the detailed physics near the
bounce. The process differs from the curvaton mechanism, which has been used
recently to revive the ekpyrotic scenario, in that no peculiar behavior of
$\xi$ shortly before or during the bounce is needed. In addition, a concrete
and efficient realization of reheating after ekpyrosis is provided; this
mechanism is not tied to ekpyrotic models, but could equally well be used in
other setups, for instance inflationary ones. We estimate non-Gaussianities and
find no additional contributions in the most simple realizations, in contrast
to models using the curvaton mechanism.
| hep-th astro-ph | we present a mechanism to transfer the spectrum of perturbations in a scalar isocurvature field xi onto the matter content in the radiation era via modulated instant preheating after ekpyrosis in this setup xi determines the coupling constant relevant for the decay of a preheat matter field into fermions the resulting power spectrum is scale invariant if xi remains close to a scaling solution in new ekpyrotic models of the universe by construction the spectrum is independent of the detailed physics near the bounce the process differs from the curvaton mechanism which has been used recently to revive the ekpyrotic scenario in that no peculiar behavior of xi shortly before or during the bounce is needed in addition a concrete and efficient realization of reheating after ekpyrosis is provided this mechanism is not tied to ekpyrotic models but could equally well be used in other setups for instance inflationary ones we estimate nongaussianities and find no additional contributions in the most simple realizations in contrast to models using the curvaton mechanism | [['we', 'present', 'a', 'mechanism', 'to', 'transfer', 'the', 'spectrum', 'of', 'perturbations', 'in', 'a', 'scalar', 'isocurvature', 'field', 'xi', 'onto', 'the', 'matter', 'content', 'in', 'the', 'radiation', 'era', 'via', 'modulated', 'instant', 'preheating', 'after', 'ekpyrosis', 'in', 'this', 'setup', 'xi', 'determines', 'the', 'coupling', 'constant', 'relevant', 'for', 'the', 'decay', 'of', 'a', 'preheat', 'matter', 'field', 'into', 'fermions', 'the', 'resulting', 'power', 'spectrum', 'is', 'scale', 'invariant', 'if', 'xi', 'remains', 'close', 'to', 'a', 'scaling', 'solution', 'in', 'new', 'ekpyrotic', 'models', 'of', 'the', 'universe', 'by', 'construction', 'the', 'spectrum', 'is', 'independent', 'of', 'the', 'detailed', 'physics', 'near', 'the', 'bounce', 'the', 'process', 'differs', 'from', 'the', 'curvaton', 'mechanism', 'which', 'has', 'been', 'used', 'recently', 'to', 'revive', 'the', 'ekpyrotic', 'scenario', 'in', 'that', 'no', 'peculiar', 'behavior', 'of', 'xi', 'shortly', 'before', 'or', 'during', 'the', 'bounce', 'is', 'needed', 'in', 'addition', 'a', 'concrete', 'and', 'efficient', 'realization', 'of', 'reheating', 'after', 'ekpyrosis', 'is', 'provided', 'this', 'mechanism', 'is', 'not', 'tied', 'to', 'ekpyrotic', 'models', 'but', 'could', 'equally', 'well', 'be', 'used', 'in', 'other', 'setups', 'for', 'instance', 'inflationary', 'ones', 'we', 'estimate', 'nongaussianities', 'and', 'find', 'no', 'additional', 'contributions', 'in', 'the', 'most', 'simple', 'realizations', 'in', 'contrast', 'to', 'models', 'using', 'the', 'curvaton', 'mechanism']] | [-0.13658315454043274, 0.21236751740798354, -0.1379009001528877, 0.11996805192792269, -0.0968815072259882, -0.16992798928383804, -0.01284756317696594, 0.33157555254622856, -0.24708533143877917, -0.2657087041794905, 0.08507545158738129, -0.22851854800185384, -0.11646562345749399, 0.1846931916307549, -0.008534118334343385, -0.0030879410057279622, 0.014346501487034934, 0.04986842460821421, -0.010333836251564803, -0.24701239053998686, 0.3282999961272056, 0.12503578728173823, 0.22955584516258618, 0.02008382157743936, 0.041772972287920616, -0.06616021570210394, -0.009080969156664714, -0.06357517016626764, -0.15320022680344128, 0.017583376997591632, 0.16116992414394807, 0.12589129364441867, 0.22221024120934527, -0.4228439435079607, -0.2727597070058293, 0.1870196461922636, 0.16662428078203523, 0.1621999249389199, -0.08462409688464818, -0.23549080087819643, 0.06004737580619883, -0.17253420777531744, -0.09747290916261617, -0.05969515754922963, 0.026017569992636814, -0.09924614249881117, -0.292398834746734, 0.11135785589648182, 0.01765356737948758, -0.04893272192005003, -0.046823718089457844, -0.03415175492681933, -0.012237495294777535, 0.03952042054390393, 0.11578805315323931, 0.019435843044336428, 0.15484977479512144, -0.17293744425327456, -0.06692434423426112, 0.40005645838876563, -0.15982302174799973, -0.11617643223552589, 0.11719422492236771, -0.12153385074983476, -0.15482085162762835, 0.1249723451318252, 0.11464504912844178, 0.09613905009171621, -0.12040968784008567, 0.13664286975185141, 0.06585132086932746, 0.16844637693200065, 0.06472125060159212, 0.01948205754024723, 0.30394229203549744, 0.1579095455450251, 0.014918420130212665, 0.12513545096207004, -0.014508273315000517, -0.11712328194809413, -0.3644959551461956, -0.09451676204910213, -0.16674873767943496, 0.049038980303319275, -0.0871088575333158, -0.1494103671556709, 0.41793877035597266, 0.15536046366762826, 0.22580842990210356, -0.019095907728827684, 0.29532897951658704, 0.09080599685477321, 0.06430765503489178, 0.07479051883503991, 0.2907189834292444, 0.11800819141953661, 0.15254730461655477, -0.1935626822482925, 0.05129895952587392, 0.02553209472334963] |
710.2541 | Toward Empirical Constraints on the Global Redshifted 21 cm Brightness
Temperature During the Epoch of Reionization | Preliminary results are presented from a simple, single-antenna experiment
designed to measure the all-sky radio spectrum between 100 and 200 MHz. The
system used an internal comparison-switching scheme to reduce non-smooth
instrumental contaminants in the measured spectrum to 75 mK. From the
observations, we place an initial upper limit of 450 mK on the relative
brightness temperature of the redshifted 21 cm contribution to the spectrum due
to neutral hydrogen in the intergalactic medium (IGM) during the epoch of
reionization, assuming a rapid transition to a fully ionized IGM at a redshift
of 8. With refinement, this technique should be able to distinguish between
slow and fast reionization scenarios. To constrain the duration of reionization
to dz > 2, the systematic residuals in the measured spectrum must be reduced to
3 mK.
| astro-ph | preliminary results are presented from a simple singleantenna experiment designed to measure the allsky radio spectrum between 100 and 200 mhz the system used an internal comparisonswitching scheme to reduce nonsmooth instrumental contaminants in the measured spectrum to 75 mk from the observations we place an initial upper limit of 450 mk on the relative brightness temperature of the redshifted 21 cm contribution to the spectrum due to neutral hydrogen in the intergalactic medium igm during the epoch of reionization assuming a rapid transition to a fully ionized igm at a redshift of 8 with refinement this technique should be able to distinguish between slow and fast reionization scenarios to constrain the duration of reionization to dz 2 the systematic residuals in the measured spectrum must be reduced to 3 mk | [['preliminary', 'results', 'are', 'presented', 'from', 'a', 'simple', 'singleantenna', 'experiment', 'designed', 'to', 'measure', 'the', 'allsky', 'radio', 'spectrum', 'between', '100', 'and', '200', 'mhz', 'the', 'system', 'used', 'an', 'internal', 'comparisonswitching', 'scheme', 'to', 'reduce', 'nonsmooth', 'instrumental', 'contaminants', 'in', 'the', 'measured', 'spectrum', 'to', '75', 'mk', 'from', 'the', 'observations', 'we', 'place', 'an', 'initial', 'upper', 'limit', 'of', '450', 'mk', 'on', 'the', 'relative', 'brightness', 'temperature', 'of', 'the', 'redshifted', '21', 'cm', 'contribution', 'to', 'the', 'spectrum', 'due', 'to', 'neutral', 'hydrogen', 'in', 'the', 'intergalactic', 'medium', 'igm', 'during', 'the', 'epoch', 'of', 'reionization', 'assuming', 'a', 'rapid', 'transition', 'to', 'a', 'fully', 'ionized', 'igm', 'at', 'a', 'redshift', 'of', '8', 'with', 'refinement', 'this', 'technique', 'should', 'be', 'able', 'to', 'distinguish', 'between', 'slow', 'and', 'fast', 'reionization', 'scenarios', 'to', 'constrain', 'the', 'duration', 'of', 'reionization', 'to', 'dz', '2', 'the', 'systematic', 'residuals', 'in', 'the', 'measured', 'spectrum', 'must', 'be', 'reduced', 'to', '3', 'mk']] | [-0.03509984574316499, 0.15054418752887824, -0.04150638142600656, 0.06287409477204514, -0.0629575395096953, -0.09483655964096005, 0.0743861505152801, 0.41424629784977207, -0.22570370639889287, -0.3491119856587969, 0.06880132743390277, -0.29102219831771575, 0.020664881388298594, 0.18726927952912564, 0.0013850319145533902, -0.015991967042478232, 0.012590476559797446, -0.07580420839994285, -0.04306082164123207, -0.2584497309307783, 0.23241859946686488, 0.17451199472237092, 0.2152821285578494, 0.039961497152510746, 0.08026809301943733, -0.10558345302706584, -0.101717881915661, -0.040539705796310534, -0.14950086178186422, 0.017924065069438746, 0.27241035806588254, 0.126740786465458, 0.19285347215258158, -0.36599948208134336, -0.20832411366729783, 0.11661133351198469, 0.12873983363477656, 0.08010359264981862, 0.01971278826867302, -0.291568664726443, 0.09852467006175385, -0.1739392211015981, -0.15097391142223318, 0.05722835432881346, 0.004889839061965736, -0.0381088929483667, -0.2593292348086834, 0.08881091490531197, 0.003383425016307648, 0.054033179280948106, -0.07043597845432277, -0.0567434884634657, -0.002526447674832665, 0.09295749674336268, -0.02493557033773798, 0.07012390144462607, 0.19038014218139535, -0.09316965628307886, -0.005373878519122417, 0.3787537568535369, -0.15731284068718265, -0.011268986539485363, 0.1968139337017559, -0.2254573770189801, -0.141506888731741, 0.23954055795016196, 0.19984870265023066, 0.03434462070178527, -0.16220559131425732, -0.015709853632590517, 0.07342953050079254, 0.266375958851467, 0.05960477674021744, 0.020701793380654775, 0.24853867342552313, 0.09912738548770833, 0.07339271481659335, 0.10555590100434178, -0.19384078606784058, 0.03017858560017955, -0.27269382201462017, -0.08888080512048104, -0.13277504777607435, 0.11882650509763222, -0.10552892853268601, -0.09326451138521616, 0.36523266603659205, 0.16916871754309307, 0.23850626069873285, 0.03681809399276972, 0.3439999936041064, 0.09593051260722299, 0.040736722320210764, 0.07253510412545158, 0.2801551960480328, 0.22023392187861296, 0.14448826089859582, -0.22002647614034895, 0.0033662828939178815, -0.01953887866783099] |
710.2542 | Probing clumpy stellar winds with a neutron star | INTEGRAL, the European Space Agency's gamma-ray observatory, tripled the
number of super-giant high-mass X-ray binaries (sgHMXB) known in the Galaxy by
revealing absorbed and fast transient (SFXT) systems. In these sources,
quantitative constraints on the wind clumping of the massive stars could be
obtained from the study of the hard X-ray variability of the compact accreting
object. Hard X-ray flares and quiescent emission of SFXT systems have been
characterized and used to derive wind clump parameters. A large fraction of the
hard X-ray emission is emitted in the form of flares with a typical duration of
3 ks, frequency of 7 days and luminosity of 1E36 erg/s. Such flares are most
probably emitted by the interaction of a compact object orbiting at ~10 R* with
wind clumps (1E(22-23) g) representing a large fraction of the stellar
mass-loss rate. The density ratio between the clumps and the inter-clump medium
is 1E(2-4) in SFXT systems. The parameters of the clumps and of the inter-clump
medium, derived from the SFXT flaring behavior, are in good agreement with
macro-clumping scenario and line driven instability simulations. SFXT have
probably a larger orbital radius than classical sgHMXB.
| astro-ph | integral the european space agencys gammaray observatory tripled the number of supergiant highmass xray binaries sghmxb known in the galaxy by revealing absorbed and fast transient sfxt systems in these sources quantitative constraints on the wind clumping of the massive stars could be obtained from the study of the hard xray variability of the compact accreting object hard xray flares and quiescent emission of sfxt systems have been characterized and used to derive wind clump parameters a large fraction of the hard xray emission is emitted in the form of flares with a typical duration of 3 ks frequency of 7 days and luminosity of 1e36 ergs such flares are most probably emitted by the interaction of a compact object orbiting at 10 r with wind clumps 1e2223 g representing a large fraction of the stellar massloss rate the density ratio between the clumps and the interclump medium is 1e24 in sfxt systems the parameters of the clumps and of the interclump medium derived from the sfxt flaring behavior are in good agreement with macroclumping scenario and line driven instability simulations sfxt have probably a larger orbital radius than classical sghmxb | [['integral', 'the', 'european', 'space', 'agencys', 'gammaray', 'observatory', 'tripled', 'the', 'number', 'of', 'supergiant', 'highmass', 'xray', 'binaries', 'sghmxb', 'known', 'in', 'the', 'galaxy', 'by', 'revealing', 'absorbed', 'and', 'fast', 'transient', 'sfxt', 'systems', 'in', 'these', 'sources', 'quantitative', 'constraints', 'on', 'the', 'wind', 'clumping', 'of', 'the', 'massive', 'stars', 'could', 'be', 'obtained', 'from', 'the', 'study', 'of', 'the', 'hard', 'xray', 'variability', 'of', 'the', 'compact', 'accreting', 'object', 'hard', 'xray', 'flares', 'and', 'quiescent', 'emission', 'of', 'sfxt', 'systems', 'have', 'been', 'characterized', 'and', 'used', 'to', 'derive', 'wind', 'clump', 'parameters', 'a', 'large', 'fraction', 'of', 'the', 'hard', 'xray', 'emission', 'is', 'emitted', 'in', 'the', 'form', 'of', 'flares', 'with', 'a', 'typical', 'duration', 'of', '3', 'ks', 'frequency', 'of', '7', 'days', 'and', 'luminosity', 'of', '1e36', 'ergs', 'such', 'flares', 'are', 'most', 'probably', 'emitted', 'by', 'the', 'interaction', 'of', 'a', 'compact', 'object', 'orbiting', 'at', '10', 'r', 'with', 'wind', 'clumps', '1e2223', 'g', 'representing', 'a', 'large', 'fraction', 'of', 'the', 'stellar', 'massloss', 'rate', 'the', 'density', 'ratio', 'between', 'the', 'clumps', 'and', 'the', 'interclump', 'medium', 'is', '1e24', 'in', 'sfxt', 'systems', 'the', 'parameters', 'of', 'the', 'clumps', 'and', 'of', 'the', 'interclump', 'medium', 'derived', 'from', 'the', 'sfxt', 'flaring', 'behavior', 'are', 'in', 'good', 'agreement', 'with', 'macroclumping', 'scenario', 'and', 'line', 'driven', 'instability', 'simulations', 'sfxt', 'have', 'probably', 'a', 'larger', 'orbital', 'radius', 'than', 'classical', 'sghmxb']] | [-0.12745354450307786, 0.16419997951506, -0.04769886032874255, 0.15303021050395296, -0.10344054006824369, -0.062953837255114, 0.04649915786729635, 0.44153854129345793, -0.13303804953619347, -0.37540662568675254, 0.08645892396544744, -0.3167405095588612, 0.006258587266539077, 0.24563705751084183, -0.018819152769681654, 0.014551656524724278, 0.1096686577926831, -0.08816698753814164, -0.011893999324131169, -0.20903825297289969, 0.2819457019262604, 0.08340663255106559, 0.09814538230727378, -0.060290290278039484, 0.07997216256580462, -0.1120434692840239, -0.029980174295212093, -0.04794785894321792, -0.10932684708876829, 0.05460733734071255, 0.23093306473119332, 0.11930827385574383, 0.19370173164428897, -0.3696276983785394, -0.25044399792524547, 0.046161837707347185, 0.17738766233455144, -0.08489914740386763, -0.009593954920695213, -0.26157159536929897, 0.020774126057758142, -0.24434121360659208, -0.18304629295476174, 0.10468105327730116, 0.10786069699465052, 0.09572758288857969, -0.20997413365709547, 0.13164237138851986, -0.006256683625427908, 0.059161896770820024, -0.15299107253575991, -0.02913026122841984, -0.0427481656550969, 0.03503948145754341, 0.08533292591914926, 0.08384926970190319, 0.18551115334205526, -0.1574331676072784, -0.03157573257278847, 0.4047911863970129, -0.033238449934517696, 0.06156106439517125, 0.22997575692317793, -0.24869881533208843, -0.18531423144679712, 0.25242531053525835, 0.14797685843598293, 0.13734503566826645, -0.1520280244714262, -0.03397912732907571, -0.028677627856009885, 0.25842334568672076, 0.04478307347468983, 0.09098682712957318, 0.3405309173523595, 0.14141822419202837, -0.020504028065816353, 0.176537909100788, -0.2351184807362427, -0.008571035744573333, -0.21621603268737855, -0.055435957124848896, -0.15593300584250278, 0.1340282438286139, -0.1452959421060912, -0.1461224239512567, 0.3140652223600467, 0.050964811690286486, 0.18672227241515524, -0.001303314793805935, 0.2900996430262335, 0.14856123743505267, 0.051165304323168175, 0.1887205013037218, 0.33563899329226266, 0.1712682312231903, 0.12431401006607828, -0.24828677599342833, 0.09086428730209407, 0.026635657651594986] |
710.2543 | Dynamics of Magnetized Spherical Accretion Flows | Transonic accretion flow with self-consistent treatment of random magnetic
field is presented.
| astro-ph | transonic accretion flow with selfconsistent treatment of random magnetic field is presented | [['transonic', 'accretion', 'flow', 'with', 'selfconsistent', 'treatment', 'of', 'random', 'magnetic', 'field', 'is', 'presented']] | [-0.21721458186705908, 0.17755107674747705, -0.0576305917929858, -0.03331159613056419, -0.12847344189261398, -0.1293270861109098, -0.10761309104661147, 0.41588179022073746, -0.17068744031712413, -0.280667538754642, 0.01649176678620279, -0.17079969712843499, 0.0340449915577968, 0.18431358660260835, -0.010637401137501001, 0.09376699368779857, 0.020443401920298736, -0.0683556863417228, -0.01788490917533636, -0.18048618737763414, 0.3220225759238626, 0.014718348781267801, 0.20245721253256002, -0.03682458524902662, 0.08014075349395473, -0.012966377971072992, -0.03631080399888257, 0.14271924458444118, -0.21754278677205244, -0.08001291713056465, 0.2007768382706369, 0.02179521508514881, 0.28321978356689215, -0.4936456154100597, -0.3761371709406376, -0.08053479390218854, 0.16287499254879853, 0.12670569059749445, -0.15952382205675045, -0.190416431442524, 0.06014484508583943, -0.2053991106028358, -0.1471355416191121, -0.0722875080537051, -0.02667746757894444, 0.08409401890821755, -0.36391056816016015, 0.1913636475801468, 0.07185498035202424, 0.14114696128914753, -0.1777608843985945, 0.01917812880128622, -0.10029052741204698, 0.013423420333613953, 0.21174316944476837, 0.15712985303252935, 0.3202628834793965, -0.19410714088007808, -0.029764280499269564, 0.3866907609626651, -0.03176274709403515, -0.1469493629410863, 0.1800110526382923, -0.2647382889408618, -0.023815134928251307, 0.2891866338128845, 0.19017940697570643, 0.17420278722420335, -0.17771388652424017, -0.002123139798641205, -0.11665355771159132, 0.031915257374445595, -0.05098887928761542, -0.13360668687770763, 0.31289841576168936, 0.16975746117532253, 0.03554815333336592, 0.09920668803776304, -0.1275458186864853, -0.17365023431678614, -0.315906529314816, -0.04130992409773171, -0.10925825871527195, 0.1573003720647345, -0.18467713170684874, -0.31735943102588254, 0.299128361667196, 0.16494735974508026, 0.06565585422019164, -0.0625989087857306, 0.37308877147734165, 0.18134953658348726, -0.09265185582141082, 0.25843991707855213, 0.27016764755050343, 0.389930184930563, 0.1367423559228579, -0.29164238495286554, 0.022716043090137344, 0.15488184119264284] |
710.2544 | Chern class identities from tadpole matching in type IIB and F-theory | In light of Sen's weak coupling limit of F-theory as a type IIB orientifold,
the compatibility of the tadpole conditions leads to a non-trivial identity
relating the Euler characteristics of an elliptically fibered Calabi-Yau
fourfold and of certain related surfaces. We present the physical argument
leading to the identity, and a mathematical derivation of a Chern class
identity which confirms it, after taking into account singularities of the
relevant loci. This identity of Chern classes holds in arbitrary dimension, and
for varieties that are not necessarily Calabi-Yau. Singularities are essential
in both the physics and the mathematics arguments: the tadpole relation may be
interpreted as an identity involving stringy invariants of a singular
hypersurface, and corrections for the presence of pinch-points. The
mathematical discussion is streamlined by the use of Chern-Schwartz-MacPherson
classes of singular varieties. We also show how the main identity may be
obtained by applying `Verdier specialization' to suitable constructible
functions.
| hep-th math.AG | in light of sens weak coupling limit of ftheory as a type iib orientifold the compatibility of the tadpole conditions leads to a nontrivial identity relating the euler characteristics of an elliptically fibered calabiyau fourfold and of certain related surfaces we present the physical argument leading to the identity and a mathematical derivation of a chern class identity which confirms it after taking into account singularities of the relevant loci this identity of chern classes holds in arbitrary dimension and for varieties that are not necessarily calabiyau singularities are essential in both the physics and the mathematics arguments the tadpole relation may be interpreted as an identity involving stringy invariants of a singular hypersurface and corrections for the presence of pinchpoints the mathematical discussion is streamlined by the use of chernschwartzmacpherson classes of singular varieties we also show how the main identity may be obtained by applying verdier specialization to suitable constructible functions | [['in', 'light', 'of', 'sens', 'weak', 'coupling', 'limit', 'of', 'ftheory', 'as', 'a', 'type', 'iib', 'orientifold', 'the', 'compatibility', 'of', 'the', 'tadpole', 'conditions', 'leads', 'to', 'a', 'nontrivial', 'identity', 'relating', 'the', 'euler', 'characteristics', 'of', 'an', 'elliptically', 'fibered', 'calabiyau', 'fourfold', 'and', 'of', 'certain', 'related', 'surfaces', 'we', 'present', 'the', 'physical', 'argument', 'leading', 'to', 'the', 'identity', 'and', 'a', 'mathematical', 'derivation', 'of', 'a', 'chern', 'class', 'identity', 'which', 'confirms', 'it', 'after', 'taking', 'into', 'account', 'singularities', 'of', 'the', 'relevant', 'loci', 'this', 'identity', 'of', 'chern', 'classes', 'holds', 'in', 'arbitrary', 'dimension', 'and', 'for', 'varieties', 'that', 'are', 'not', 'necessarily', 'calabiyau', 'singularities', 'are', 'essential', 'in', 'both', 'the', 'physics', 'and', 'the', 'mathematics', 'arguments', 'the', 'tadpole', 'relation', 'may', 'be', 'interpreted', 'as', 'an', 'identity', 'involving', 'stringy', 'invariants', 'of', 'a', 'singular', 'hypersurface', 'and', 'corrections', 'for', 'the', 'presence', 'of', 'pinchpoints', 'the', 'mathematical', 'discussion', 'is', 'streamlined', 'by', 'the', 'use', 'of', 'chernschwartzmacpherson', 'classes', 'of', 'singular', 'varieties', 'we', 'also', 'show', 'how', 'the', 'main', 'identity', 'may', 'be', 'obtained', 'by', 'applying', 'verdier', 'specialization', 'to', 'suitable', 'constructible', 'functions']] | [-0.19778672037524433, 0.04569756368261129, -0.12338457490299262, 0.14228621738798478, -0.11120540491195724, -0.17698136428858038, 0.0005322704422652867, 0.25435732261222954, -0.25100920351185635, -0.2392652262111797, 0.11719801755746814, -0.21436820867520093, -0.18674792289380837, 0.189308030664726, -0.1579356446734392, -0.02346800500622135, 0.021805910004022853, 0.0025119473830510688, -0.0988684007717263, -0.2835979221169563, 0.44637783065596537, -0.033233359431714016, 0.2482720249776844, 0.12497191962000787, 0.0954707207012118, -0.008846397377745388, -0.021465230065099653, 0.010224510897316184, -0.10324074598972753, 0.14100690913771652, 0.2685063607759433, 0.08286346517825877, 0.14336069639212165, -0.4231186208796073, -0.13728919760491456, 0.13224531859585564, 0.1292841199943735, 0.10373944821052278, -0.003837221964822437, -0.2862047851024792, 0.06506552652522825, -0.15126875078220384, -0.23156261916448867, -0.09445724760796996, 0.011342186538587793, 0.02640444611266158, -0.22044681381735512, 0.035514620185816005, 0.09883083814596819, 0.09395454968234487, -0.03605249243312107, -0.0753603032219461, -0.09062814853744569, 0.11028196185970301, 0.0848204395718556, 0.005613197361003437, 0.0835655196128547, -0.1626945114740189, -0.11134389764477128, 0.37996881241526675, -0.024849514957833913, -0.21433157364235206, 0.125349209020736, -0.1053288188630569, -0.16960649640646344, 0.14978118394912385, 0.06051955430531034, 0.1485372609424624, -0.09148160649731366, 0.14953261823659714, -0.054879488325312586, 0.05775786643190419, 0.09919229595392358, 0.03616927517578006, 0.21372701018878254, 0.057904736574106164, 0.026400465153011622, 0.12761459616773757, -0.020573584543954995, -0.06906678042910214, -0.43164537249291257, -0.18652191248363237, -0.10643252793599066, 0.17424273429587986, -0.13960998918314454, -0.18823512336178347, 0.4040686160727751, 0.06371135113827787, 0.19304168421327703, 0.07678765538255106, 0.22365788970556524, 0.09700893342428006, 0.07609391067895332, -0.021471056839134667, 0.18396271626142408, 0.18531570094485394, 0.0449610556220161, -0.16638024949645197, 0.006443150393250916, 0.19726524018420796] |
710.2545 | A Freiman-type theorem for locally compact abelian groups | We prove a Freiman-type theorem for locally compact abelian groups. If A is a
subset of a locally compact abelian group with Haar measure m and m(nA) <
n^dm(A) for all n>d log d then we describe A in a way which is tight up to
logarithmic factors in d.
| math.CA math.NT | we prove a freimantype theorem for locally compact abelian groups if a is a subset of a locally compact abelian group with haar measure m and mna ndma for all nd log d then we describe a in a way which is tight up to logarithmic factors in d | [['we', 'prove', 'a', 'freimantype', 'theorem', 'for', 'locally', 'compact', 'abelian', 'groups', 'if', 'a', 'is', 'a', 'subset', 'of', 'a', 'locally', 'compact', 'abelian', 'group', 'with', 'haar', 'measure', 'm', 'and', 'mna', 'ndma', 'for', 'all', 'nd', 'log', 'd', 'then', 'we', 'describe', 'a', 'in', 'a', 'way', 'which', 'is', 'tight', 'up', 'to', 'logarithmic', 'factors', 'in', 'd']] | [-0.16235293308272958, 0.137309534358792, -0.12707411928568035, 0.07025785432294167, -0.05748832724445189, -0.16092606915238625, 0.10498466703878269, 0.39654809213243425, -0.2548502629894453, -0.1958821136310386, 0.07289177685258134, -0.27555048015589517, -0.09991188442412142, 0.1993583548416306, -0.0985621192958206, -0.048022448036742084, -0.014037878456292674, 0.15177703939843923, -0.07732870525796898, -0.29103975114412606, 0.3517388144585614, -0.08140945865792067, 0.2036208570401262, 0.022995488174880546, 0.09941069606187132, -0.035111382438723616, -0.03225570289456906, 0.05208759510423988, -0.10981284014026944, 0.1354780153099758, 0.29753054067259654, 0.05947113100652738, 0.2420090417532871, -0.28591315747083473, -0.14519676482162444, 0.19998447003308684, 0.05814450489803372, 0.026800494619237725, -0.047476268455890626, -0.24878037649129206, 0.20894573931582272, -0.16452337964437902, -0.18196552106625555, -0.08999221116149177, 0.16936971404356882, -0.007087752902104209, -0.33304304914781824, -0.01080248662037775, 0.09496144310105592, 0.017572232745199774, -0.026830997795817286, -0.03475366715186586, 0.0128061508682246, 0.0719337956882858, -0.0752901172284813, 0.13735320682947835, 0.07265613289200701, -0.021425338825793006, -0.07311421726869109, 0.38412994130825, -0.1514045688090846, -0.2384000823367387, 0.14179490824850896, -0.19647849430718148, -0.19565311673795804, 0.09511679981854589, 0.1593582071751977, 0.1940660763066262, -0.0996328872279264, 0.19936379006321658, -0.16011571375808367, 0.1672232326430579, 0.0643756063800538, 0.041687890518611916, 0.0839844949465866, 0.14048482231252515, 0.14680382058334848, 0.09970100194914266, 0.0027833583299070597, 0.07404515875775057, -0.33173682452373515, -0.22152044179771715, -0.11782002799009206, 0.15431648634451753, -0.10850594899936065, -0.16316350189057025, 0.30913210155752796, -0.02805600601520079, 0.21473972664292282, 0.131894798350307, 0.21193962107645348, 0.020069767129219446, 0.057820087393338326, 0.2047102459667561, 0.06355078411676611, 0.17196302806648114, -0.14210690567657971, -0.12248190551569375, -0.04477629357522043, 0.15591652489577731] |
710.2546 | Micromagnetic Simulations of Ferromagnetic Rings | Thin nanomagnetic rings have generated interest for fundamental studies of
magnetization reversal and also for their potential in various applications,
particularly as magnetic memories. They are a rare example of a geometry in
which an analytical solution for the rate of thermally induced magnetic
reversal has been determined, in an approximation whose errors can be estimated
and bounded. In this work, numerical simulations of soft ferromagnetic rings
are used to explore aspects of the analytical solution. The evolution of the
energy near the transition states confirms that, consistent with analytical
predictions, thermally induced magnetization reversal can have one of two
intermediate states: either constant or soliton-like saddle configurations,
depending on ring size and externally applied magnetic field. The results
confirm analytical predictions of a transition in thermally activated reversal
behavior as magnetic field is varied at constant ring size. Simulations also
show that the analytic one dimensional model continues to hold even for wide
rings.
| cond-mat.mes-hall cond-mat.other | thin nanomagnetic rings have generated interest for fundamental studies of magnetization reversal and also for their potential in various applications particularly as magnetic memories they are a rare example of a geometry in which an analytical solution for the rate of thermally induced magnetic reversal has been determined in an approximation whose errors can be estimated and bounded in this work numerical simulations of soft ferromagnetic rings are used to explore aspects of the analytical solution the evolution of the energy near the transition states confirms that consistent with analytical predictions thermally induced magnetization reversal can have one of two intermediate states either constant or solitonlike saddle configurations depending on ring size and externally applied magnetic field the results confirm analytical predictions of a transition in thermally activated reversal behavior as magnetic field is varied at constant ring size simulations also show that the analytic one dimensional model continues to hold even for wide rings | [['thin', 'nanomagnetic', 'rings', 'have', 'generated', 'interest', 'for', 'fundamental', 'studies', 'of', 'magnetization', 'reversal', 'and', 'also', 'for', 'their', 'potential', 'in', 'various', 'applications', 'particularly', 'as', 'magnetic', 'memories', 'they', 'are', 'a', 'rare', 'example', 'of', 'a', 'geometry', 'in', 'which', 'an', 'analytical', 'solution', 'for', 'the', 'rate', 'of', 'thermally', 'induced', 'magnetic', 'reversal', 'has', 'been', 'determined', 'in', 'an', 'approximation', 'whose', 'errors', 'can', 'be', 'estimated', 'and', 'bounded', 'in', 'this', 'work', 'numerical', 'simulations', 'of', 'soft', 'ferromagnetic', 'rings', 'are', 'used', 'to', 'explore', 'aspects', 'of', 'the', 'analytical', 'solution', 'the', 'evolution', 'of', 'the', 'energy', 'near', 'the', 'transition', 'states', 'confirms', 'that', 'consistent', 'with', 'analytical', 'predictions', 'thermally', 'induced', 'magnetization', 'reversal', 'can', 'have', 'one', 'of', 'two', 'intermediate', 'states', 'either', 'constant', 'or', 'solitonlike', 'saddle', 'configurations', 'depending', 'on', 'ring', 'size', 'and', 'externally', 'applied', 'magnetic', 'field', 'the', 'results', 'confirm', 'analytical', 'predictions', 'of', 'a', 'transition', 'in', 'thermally', 'activated', 'reversal', 'behavior', 'as', 'magnetic', 'field', 'is', 'varied', 'at', 'constant', 'ring', 'size', 'simulations', 'also', 'show', 'that', 'the', 'analytic', 'one', 'dimensional', 'model', 'continues', 'to', 'hold', 'even', 'for', 'wide', 'rings']] | [-0.17411312962611836, 0.16501061362834016, -0.057111669690798846, 0.04586623451642452, -0.032853414815279744, -0.12846231728251423, 0.006578205229203787, 0.3992473941116083, -0.2651540987884566, -0.29801809496336407, 0.11138864129165849, -0.2355961960049406, -0.10306256075630024, 0.23694591344664653, 0.03109509628266096, 0.017694974102590594, -0.007172718019254746, 0.042283598432737976, -0.058377404757324725, -0.1919384496586938, 0.2646314271545458, 0.024613508263662938, 0.2736815829250601, 0.052684628714116354, 0.020658797257009053, -0.039391414275873574, 0.05030776069409424, 0.07466212490032757, -0.1685340072213289, 0.037822159051504586, 0.23037719034379528, -0.01725001467782403, 0.20565861482173203, -0.4974110011732386, -0.20952561832363567, 0.0779149447297377, 0.18024535768124605, 0.14253848558216686, -0.11596029160559297, -0.252359112060719, 0.10595176869462575, -0.1476906627566824, -0.17640217687153528, -0.11713087044415936, 0.05829604244190118, 0.04952299647003172, -0.2862629878053051, 0.0585338001015536, 0.07636360616212891, 0.08303055973993914, -0.11067799773487834, -0.07147431893334273, -0.04982299945963126, 0.09309394610444865, 0.07446944848559196, 0.01967965749227592, 0.1782016411694067, -0.1388782056099679, -0.15312814924325194, 0.3127688816538261, -0.06954399332509285, -0.14882193977790584, 0.18130538496827225, -0.16830062143684876, -0.09494894567516542, 0.17783770035922286, 0.1454248668355567, 0.1505712584141762, -0.11911245875300899, 0.09187045660237932, -0.02599793750972998, 0.139410717385791, 0.06568361657761758, 0.024708479057787166, 0.2598204185525256, 0.16173070262396527, 0.012076013325338041, 0.14453650151244216, -0.07295155307848848, -0.12422038950326462, -0.27347065667441534, -0.12643570923847297, -0.19685145092587317, 0.07038839642829713, -0.08557495676673904, -0.1712774092752126, 0.37517684965484566, 0.1367723253747118, 0.18170640477610212, -0.019111117167067863, 0.27240057536551066, 0.11866351466235374, 0.05221381033470313, 0.06112674282443139, 0.2595956314813286, 0.1759787313249563, 0.08124236518736823, -0.2521274632654123, 0.08473546077166834, -0.00726962664827419] |
710.2547 | Topological defects and equation of state of gluon plasma | We show that the degrees of freedom associated with magnetic monopole- and
vortexlike gluonic configurations make a strong contribution to the anomaly of
the energy-momentum tensor of Yang-Mills theory in the deconfinement phase
immediately above the critical temperature. As is well known in
zero-temperature Yang-Mills theory, the monopoles and vortices are constituents
of a generic gluonic object in which the two neighbor monopoles are connected
together by a segment of vortex string. Our results provide evidence that the
monopole-vortex chains in SU(2) gauge theory and their SU(3) counterparts, the
monopole-vortex nets, are thermodynamically relevant degrees of freedom in the
gluonic plasma.
| hep-lat hep-ph hep-th | we show that the degrees of freedom associated with magnetic monopole and vortexlike gluonic configurations make a strong contribution to the anomaly of the energymomentum tensor of yangmills theory in the deconfinement phase immediately above the critical temperature as is well known in zerotemperature yangmills theory the monopoles and vortices are constituents of a generic gluonic object in which the two neighbor monopoles are connected together by a segment of vortex string our results provide evidence that the monopolevortex chains in su2 gauge theory and their su3 counterparts the monopolevortex nets are thermodynamically relevant degrees of freedom in the gluonic plasma | [['we', 'show', 'that', 'the', 'degrees', 'of', 'freedom', 'associated', 'with', 'magnetic', 'monopole', 'and', 'vortexlike', 'gluonic', 'configurations', 'make', 'a', 'strong', 'contribution', 'to', 'the', 'anomaly', 'of', 'the', 'energymomentum', 'tensor', 'of', 'yangmills', 'theory', 'in', 'the', 'deconfinement', 'phase', 'immediately', 'above', 'the', 'critical', 'temperature', 'as', 'is', 'well', 'known', 'in', 'zerotemperature', 'yangmills', 'theory', 'the', 'monopoles', 'and', 'vortices', 'are', 'constituents', 'of', 'a', 'generic', 'gluonic', 'object', 'in', 'which', 'the', 'two', 'neighbor', 'monopoles', 'are', 'connected', 'together', 'by', 'a', 'segment', 'of', 'vortex', 'string', 'our', 'results', 'provide', 'evidence', 'that', 'the', 'monopolevortex', 'chains', 'in', 'su2', 'gauge', 'theory', 'and', 'their', 'su3', 'counterparts', 'the', 'monopolevortex', 'nets', 'are', 'thermodynamically', 'relevant', 'degrees', 'of', 'freedom', 'in', 'the', 'gluonic', 'plasma']] | [-0.18915064543218232, 0.29059813322388744, -0.07269688392931706, 0.09478082324581055, -0.06301402665748454, -0.06284204133242222, 0.001898609808332628, 0.35605362119466655, -0.15326445005686568, -0.23950398409978882, 0.05731996944944125, -0.3024362866388689, -0.1466532466693385, 0.04443434378740811, 0.039853334205575505, 0.015552370366409864, -0.02165703603647428, 0.10723154001326374, -0.07237324937901432, -0.22108824107805175, 0.3159313175947138, -0.020921674395662428, 0.2560644833057529, 0.1252915539714222, 0.06599268692056878, -0.02196128381010477, 0.024057174341218308, 0.0338858451629703, -0.09530322859409533, 0.07496878438361801, 0.23551802626709537, 0.0074804261912324345, 0.08871144193713323, -0.4435941519971826, -0.22108249833788907, 0.05383333804588396, 0.1419514225920349, 0.17052310386483585, 0.01889291790597565, -0.3006485938325082, 0.07511941676424576, -0.17052058037370443, -0.19831410431335358, -0.13300118338095374, -0.013913441975001651, -0.009635862281158715, -0.22344354603734642, 0.08477017518575533, 0.06605030295074835, 0.06179480312511989, -0.05903660091064354, -0.1348044845264919, -0.09080257347443758, 0.07161848662919042, 0.11241949937251018, 0.10940079119443746, 0.14493622467622602, -0.25244281107172517, -0.15589934924045706, 0.36891454264134316, -0.034055892728490404, -0.1793975747273405, 0.17372631493006085, -0.1283172008876532, -0.1527915001330473, 0.15467558839556642, 0.08302939757889155, 0.1486091553233564, -0.127890042508814, 0.11249880984455513, -0.05750426369267377, 0.12910642274793718, 0.047917333864929655, 0.0780101233244975, 0.32753170895768274, 0.10827283595347463, 0.04758369072921353, 0.17821778758373666, -0.02294273829458761, -0.16835007413594735, -0.3955516999052598, -0.13060184487713372, -0.1663725562808611, 0.026978521912109733, -0.13584419222284075, -0.19420550270052167, 0.35773927385983345, 0.13998804767708303, 0.15999165127580608, -0.0054182169191299544, 0.22766712208343023, 0.04494861291092129, 0.08236450392356383, 0.07297296986666203, 0.2707260053582941, 0.2497172103203501, 0.11433288711814744, -0.2677092863763175, -0.12385870458207804, 0.16705932757254727] |
710.2548 | Measurement of the inclusive B_s^0 -> X^+ l^- \nu semileptonic decay
branching fraction | Inclusive semileptonic B_s^0 -> X^+ l^- \nu decays are studied for the first
time using a 23.6 fb^{-1} data sample collected on the Y(5S) resonance with the
Belle detector at the KEKB asymmetric energy e^+ e^- collider. These decays are
identified by the means of a lepton accompanied by a same-sign D_s^+ meson
originating from the other B_s^0 in the event. The semileptonic branching
fractions are measured in the electron and muon channels to be Bf(B_s^0 -> X^+
e^- \nu) = (10.9 \pm 1.0 \pm 0.9)% and Bf(B_s^0 -> X^+ \mu^- \nu) = (9.2 \pm
1.0 \pm 0.8)%, respectively. Assuming an equal electron and muon production
rate in B_s^0 decays, a combined fit yields an average leptonic branching
fraction Bf(B_s^0 -> X^+ l^- \nu) = (10.2 \pm 0.8 \pm 0.9)%.
| hep-ex | inclusive semileptonic b_s0 x l nu decays are studied for the first time using a 236 fb1 data sample collected on the y5s resonance with the belle detector at the kekb asymmetric energy e e collider these decays are identified by the means of a lepton accompanied by a samesign d_s meson originating from the other b_s0 in the event the semileptonic branching fractions are measured in the electron and muon channels to be bfb_s0 x e nu 109 pm 10 pm 09 and bfb_s0 x mu nu 92 pm 10 pm 08 respectively assuming an equal electron and muon production rate in b_s0 decays a combined fit yields an average leptonic branching fraction bfb_s0 x l nu 102 pm 08 pm 09 | [['inclusive', 'semileptonic', 'b_s0', 'x', 'l', 'nu', 'decays', 'are', 'studied', 'for', 'the', 'first', 'time', 'using', 'a', '236', 'fb1', 'data', 'sample', 'collected', 'on', 'the', 'y5s', 'resonance', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetric', 'energy', 'e', 'e', 'collider', 'these', 'decays', 'are', 'identified', 'by', 'the', 'means', 'of', 'a', 'lepton', 'accompanied', 'by', 'a', 'samesign', 'd_s', 'meson', 'originating', 'from', 'the', 'other', 'b_s0', 'in', 'the', 'event', 'the', 'semileptonic', 'branching', 'fractions', 'are', 'measured', 'in', 'the', 'electron', 'and', 'muon', 'channels', 'to', 'be', 'bfb_s0', 'x', 'e', 'nu', '109', 'pm', '10', 'pm', '09', 'and', 'bfb_s0', 'x', 'mu', 'nu', '92', 'pm', '10', 'pm', '08', 'respectively', 'assuming', 'an', 'equal', 'electron', 'and', 'muon', 'production', 'rate', 'in', 'b_s0', 'decays', 'a', 'combined', 'fit', 'yields', 'an', 'average', 'leptonic', 'branching', 'fraction', 'bfb_s0', 'x', 'l', 'nu', '102', 'pm', '08', 'pm', '09']] | [-0.09812889179442934, 0.27751112603076084, -0.002349946110289756, 0.08865455433166003, 0.02127831121073748, -0.1738893550449634, 0.12049690128126128, 0.26107333156817814, -0.1593844375868396, -0.2925933132902151, -0.06919328360231518, -0.47334560820817706, 0.17138689461853204, 0.1586521216573542, 0.1037966469567784, 0.11786649148244925, 0.09826557319308442, -0.03318383356526009, -0.07203469959246676, -0.17090840342386468, 0.1041202218824528, 0.024287674174742487, 0.21104001752441612, 0.0449465767563722, 0.009871549805913999, -0.03301575325611161, -0.07792999657255227, -0.1357656262693851, -0.23766527366938023, -0.04104816884832169, 0.20281190994930098, 0.0684511867934853, 0.08622430232391368, -0.24022109270808278, 0.08260744701450069, 0.1904927882767184, 0.18453766513479555, -0.10842986078672603, -0.0068139387521801925, -0.40371121125432047, 0.19630017371969374, -0.22476644236670157, -0.03679831764221615, 0.03973235770287674, 0.11323709798810201, -0.13614899134528408, -0.4051478083010733, 0.1814688277218824, -0.11256077912128795, 0.09860921346362893, -0.011241550256339152, -0.34143441424864096, -0.03165364358574152, -0.09302889362235016, 0.08869432118850026, 0.20192672793443003, 0.23165960924991413, -0.022743787374196012, -0.21721795064442587, 0.35249819147695854, -0.09091609561632717, -0.15839509362339732, 0.09331151227868063, -0.2879593926974065, -0.09338322029273002, 0.2910555290982006, 0.26174324634295654, 0.03714631588436754, -0.21004538512902288, 0.13541345679763386, -0.009864583275729517, 0.20643306387081076, 0.07763026393495681, 0.05813129335581287, 0.186042438230924, 0.17805968143700857, -0.023712337940810173, -0.03141176311547179, -0.21356256747413882, 0.07642476213717364, -0.40392399402392076, -0.11382746527244042, -0.06452424503953719, 0.24908922239380882, -0.053903723546948355, 0.052599038372225154, 0.3159396781215096, -0.046236389473731807, 0.38461672408672853, 0.007532022728743713, 0.2471861304124681, 0.08902447300346007, -0.022092462571033058, 0.09427220289767209, 0.2793581131542843, 0.22580876783278536, 0.16540574772582517, -0.2874254709832764, 0.0037596175878694873, -0.01416443862641851] |
710.2549 | Congruences among modular forms on U(2,2) and the Bloch-Kato conjecture | Let k be a positive integer divisible by 4, l>k a prime, and f an elliptic
cuspidal eigenform of weight k-1, level 4, and non-trivial character. Let
\rho_f be the l-adic Galois representation attached to f. In this paper we
provide evidence for the Bloch-Kato conjecture for a twist of the adjoint motif
of \rho_f in the following way. Let L(f,s) denote the symmetric square
L-function of f. We prove that (under certain conditions) the l-adic valuation
of the algebraic part of L(f, k) is no greater than the l-adic valuation of the
order of S, where S is (the Pontryagin dual of) the Selmer group attached to
the Galois module \ad^0\rho_f|_{G_K} (-1), and K= Q(i). Our method uses an idea
of Ribet in that we introduce an intermediate step and produce congruences
between CAP and non-CAP modular forms on the unitary group U(2,2).
| math.NT math.RT | let k be a positive integer divisible by 4 lk a prime and f an elliptic cuspidal eigenform of weight k1 level 4 and nontrivial character let rho_f be the ladic galois representation attached to f in this paper we provide evidence for the blochkato conjecture for a twist of the adjoint motif of rho_f in the following way let lfs denote the symmetric square lfunction of f we prove that under certain conditions the ladic valuation of the algebraic part of lf k is no greater than the ladic valuation of the order of s where s is the pontryagin dual of the selmer group attached to the galois module ad0rho_f_g_k 1 and k qi our method uses an idea of ribet in that we introduce an intermediate step and produce congruences between cap and noncap modular forms on the unitary group u22 | [['let', 'k', 'be', 'a', 'positive', 'integer', 'divisible', 'by', '4', 'lk', 'a', 'prime', 'and', 'f', 'an', 'elliptic', 'cuspidal', 'eigenform', 'of', 'weight', 'k1', 'level', '4', 'and', 'nontrivial', 'character', 'let', 'rho_f', 'be', 'the', 'ladic', 'galois', 'representation', 'attached', 'to', 'f', 'in', 'this', 'paper', 'we', 'provide', 'evidence', 'for', 'the', 'blochkato', 'conjecture', 'for', 'a', 'twist', 'of', 'the', 'adjoint', 'motif', 'of', 'rho_f', 'in', 'the', 'following', 'way', 'let', 'lfs', 'denote', 'the', 'symmetric', 'square', 'lfunction', 'of', 'f', 'we', 'prove', 'that', 'under', 'certain', 'conditions', 'the', 'ladic', 'valuation', 'of', 'the', 'algebraic', 'part', 'of', 'lf', 'k', 'is', 'no', 'greater', 'than', 'the', 'ladic', 'valuation', 'of', 'the', 'order', 'of', 's', 'where', 's', 'is', 'the', 'pontryagin', 'dual', 'of', 'the', 'selmer', 'group', 'attached', 'to', 'the', 'galois', 'module', 'ad0rho_f_g_k', '1', 'and', 'k', 'qi', 'our', 'method', 'uses', 'an', 'idea', 'of', 'ribet', 'in', 'that', 'we', 'introduce', 'an', 'intermediate', 'step', 'and', 'produce', 'congruences', 'between', 'cap', 'and', 'noncap', 'modular', 'forms', 'on', 'the', 'unitary', 'group', 'u22']] | [-0.23777837847018432, 0.07326324365516176, -0.17175246276695963, 0.0004065625351512621, -0.11718747798438696, -0.15604138382526875, -0.02217173876657321, 0.2820178269290588, -0.33685754348432095, -0.2264847159467664, 0.023459228900962994, -0.24362617512528692, -0.12162534613326244, 0.18438358756739803, -0.09868348453595208, -0.04880627789567422, -0.03193364273527191, 0.1767747780936524, -0.053462375876900385, -0.3245665275501612, 0.3726048530636906, -0.05107384778290305, 0.16874806303366965, 0.028715555575384404, 0.0831761571552447, 0.025801587245745983, 0.04286782865078044, -0.10968348413089317, -0.14483961346610466, 0.16439537505920923, 0.36052694691436915, 0.048315030393111975, 0.25940028700688983, -0.39227427872763554, -0.07762890011006572, 0.2518033464045697, 0.10428359534945601, -0.08941539657190704, 0.019633412489857734, -0.24180285613959274, 0.1735997303392292, -0.16454878568150838, -0.1602797524062392, -0.04727818040196902, 0.10126289353430482, -0.010283593843858296, -0.3239966627803933, 0.011221398645356087, 0.10896170950612762, 0.2188667072980127, -0.07700536160034613, -0.18465066021947768, -0.03860735671076609, 0.03985644708072741, -0.01605780095740838, 0.10281502850321744, 0.07244935946893209, -0.12905761958952522, -0.10398156031913741, 0.3453648392681662, -0.0878667287282772, -0.15222815257615188, 0.06617957546087114, -0.19308949843980372, -0.13853838035671723, 0.12759610761324286, 0.07668786971587163, 0.13772044361004948, 0.03806782549519328, 0.1918533958316761, -0.1645654197782278, 0.12220527259485377, 0.08659457419933357, -0.06749044968435068, 0.1355844955451944, 0.015237735905750116, 0.09935942429944243, 0.14908341797639313, -0.026457369184895406, 0.04855519079629489, -0.3919031688759864, -0.22332584207654524, -0.1324270654528756, 0.15584111460287806, -0.09406966896033699, -0.13354233347705868, 0.41772814704970995, 0.08610906987778948, 0.16182544393609213, 0.162541542156324, 0.1713678556573118, 0.10893957055268914, 0.07345145795835366, 0.0684882932536068, 0.03597053978090014, 0.23529676920045692, -0.09166131639840003, -0.20307853550020552, -0.0031206891435431316, 0.1867506788046637] |
710.255 | The lightest neutralino in the MNSSM | We examine the allowed mass range of the lightest neutralino within the
Minimal Non--minimal Supersymmetric Standard Model. Being absolutely stable if
R-parity is conserved this lightest neutralino is a candidate for the dark
matter of the universe. We establish the theoretical upper bound on the
lightest neutralino mass and obtain an approximate solution for this mass.
| hep-ph | we examine the allowed mass range of the lightest neutralino within the minimal nonminimal supersymmetric standard model being absolutely stable if rparity is conserved this lightest neutralino is a candidate for the dark matter of the universe we establish the theoretical upper bound on the lightest neutralino mass and obtain an approximate solution for this mass | [['we', 'examine', 'the', 'allowed', 'mass', 'range', 'of', 'the', 'lightest', 'neutralino', 'within', 'the', 'minimal', 'nonminimal', 'supersymmetric', 'standard', 'model', 'being', 'absolutely', 'stable', 'if', 'rparity', 'is', 'conserved', 'this', 'lightest', 'neutralino', 'is', 'a', 'candidate', 'for', 'the', 'dark', 'matter', 'of', 'the', 'universe', 'we', 'establish', 'the', 'theoretical', 'upper', 'bound', 'on', 'the', 'lightest', 'neutralino', 'mass', 'and', 'obtain', 'an', 'approximate', 'solution', 'for', 'this', 'mass']] | [-0.11109100937444184, 0.24731758532314935, -0.03454980067908764, 0.24918934815962399, -0.09314799360332213, -0.1483626327992949, 0.04051723314179461, 0.2734883695915674, -0.17507235346628086, -0.33912377644862446, 0.025240881721921533, -0.245269767690583, 0.08251115894277714, 0.10180691813625994, 0.012785277591319755, 0.07663483525227223, 0.04837851191405207, 0.10217984792377267, -0.048878069451477914, -0.25474500900600106, 0.274815962566728, -0.008671917437043573, 0.12521250228331024, 0.10871780440876526, 0.03898027510980943, -0.06854560849023983, 0.014642400142162972, -0.20367568989916304, -0.25032025820109993, 0.09453949530974828, 0.1384946340528716, 0.12393968982256151, 0.12022258883890961, -0.3001820855071336, -0.13971998956653156, 0.3258213669593845, 0.1822312900912948, 0.04991269379388541, -0.1241703480419736, -0.31830218580684494, 0.10969837520471108, -0.2634852955650006, -0.14056812971830368, -0.05568657979061494, -0.011039975656396044, -0.1880389135497223, -0.316627912090293, 0.1728208906216813, -0.0849206857882174, -0.12210522582557003, -0.0906533083845196, -0.15230200336165062, -0.14822011073452554, -0.06202486592311678, 0.20166242710339638, -0.07302561032286446, 0.19865294983277895, -0.1742725877972719, -0.06321469933858939, 0.43071651219257284, -0.14838891396565096, -0.19834413765264408, 0.1301280454499647, -0.10600612202792295, -0.17201724786510958, 0.11528125397411973, 0.13668553270066955, 0.17923121496070443, -0.18036988914744662, 0.27290929008969605, -0.16081411477976612, 0.23182049105318064, 0.06400927101744205, 0.04878654921360846, 0.38369278569838833, 0.2970192269089499, 0.17041677517616854, 0.03144475403574428, -0.03661237953513462, -0.11350167813777391, -0.44790379154229804, -0.1964070880588094, -0.12146021572490488, -0.004592248487045124, -0.10823318908530512, -0.13813731734574372, 0.3936121905488627, 0.11531850941745299, 0.20630048396664538, 0.11326694240727063, 0.33219085247921093, 0.08724980270822666, 0.0007220888676654015, 0.04839217152246939, 0.3800308861620059, 0.1810295667590773, 0.039200978769388585, -0.22269499456576472, -0.07370329362622995, 0.09846153196745686] |
710.2551 | On general flux backgrounds with localized sources | We derive new consistency conditions for string compactifications with
generic fluxes (RR, NSNS, geometrical) and localized sources (D-branes,
NS-branes, KK-monopoles). The constraints are all related by string dualities
and share a common origin in M-theory. We also find new sources of
instabilities. We discuss the importance of these conditions for the
consistency of the effective action and for the study of interpolating
solutions between vacua.
| hep-th | we derive new consistency conditions for string compactifications with generic fluxes rr nsns geometrical and localized sources dbranes nsbranes kkmonopoles the constraints are all related by string dualities and share a common origin in mtheory we also find new sources of instabilities we discuss the importance of these conditions for the consistency of the effective action and for the study of interpolating solutions between vacua | [['we', 'derive', 'new', 'consistency', 'conditions', 'for', 'string', 'compactifications', 'with', 'generic', 'fluxes', 'rr', 'nsns', 'geometrical', 'and', 'localized', 'sources', 'dbranes', 'nsbranes', 'kkmonopoles', 'the', 'constraints', 'are', 'all', 'related', 'by', 'string', 'dualities', 'and', 'share', 'a', 'common', 'origin', 'in', 'mtheory', 'we', 'also', 'find', 'new', 'sources', 'of', 'instabilities', 'we', 'discuss', 'the', 'importance', 'of', 'these', 'conditions', 'for', 'the', 'consistency', 'of', 'the', 'effective', 'action', 'and', 'for', 'the', 'study', 'of', 'interpolating', 'solutions', 'between', 'vacua']] | [-0.17018235622403713, 0.13030446498439863, -0.04894995207969959, 0.21372807311037412, -0.08779972698181294, -0.13564268698056156, 0.06029565236889399, 0.317258673089628, -0.1533699129600651, -0.2715390207819067, 0.11934778976003424, -0.24965293675374525, -0.13872938356720485, 0.1509309224390353, -0.09659955981545723, -0.008866998596260181, 0.02230826745597789, -0.028784200764046267, -0.11954008711931798, -0.24598507061600686, 0.39734765382913445, -0.0017500792200175615, 0.29945601368179686, 0.02385033254440014, 0.09488587317844996, -0.06618975671008229, -0.0468632948369934, -0.012295258962191068, -0.1822930809110403, 0.14592118134292273, 0.21112791918791257, 0.14390900433063508, 0.070035014860332, -0.48132289544894147, -0.21285003897948906, 0.08739417399494694, 0.1479834422110938, 0.13172094505280257, -0.027491344755085616, -0.26305175356996746, 0.07558294898615434, -0.10373255354352295, -0.15627155856301006, -0.09621921191708399, 0.04081598071094889, 0.051110382603767976, -0.2509052530934031, 0.0644061944886254, -0.018586929239189396, 0.036145842347580656, -0.125844358248063, -0.05855172236378376, -0.042808237507079655, 0.11814124543363085, 0.15082412568422465, 0.011266633742847122, 0.06529462242212433, -0.2199041749852208, -0.15625724371236105, 0.3360781896859407, -0.041712231762134115, -0.21299584932052174, 0.197588870416467, -0.06779217917042282, -0.22862916744242495, 0.05353058845951007, 0.09030945425709853, 0.17140482942072244, -0.17470847876438012, 0.15110023640400658, 0.017473711202350948, 0.059598510325528105, 0.11199138483677346, 0.14135067839748583, 0.3247906143848713, 0.08377908777732115, 0.043900242182784356, 0.1579931480022004, -0.08341405138086815, -0.0868830150190311, -0.4636900657071517, -0.08706066142767668, -0.02439892312977463, 0.08858835986600472, -0.17403091905714693, -0.1674121985480619, 0.3790460714067404, 0.14017074793004072, 0.153764287274904, 0.03114802151058729, 0.14746097813432033, 0.06428393555375246, 0.025302637995292362, 0.07900296374080847, 0.24402438518233024, 0.13302603476286795, 0.03658291290585811, -0.24316280517154015, -0.09782924034561102, 0.14272816788691742] |
710.2552 | Simultaneous Estimation of Time Delays and Quasar Structure | We expand our Bayesian Monte Carlo method for analyzing the light curves of
gravitationally lensed quasars to simultaneously estimate time delays and
quasar structure including their mutual uncertainties. We apply the method to
HE1104-1805 and QJ0158-4325, two doubly-imaged quasars with microlensing and
intrinsic variability on comparable time scales. For HE1104-1805 the resulting
time delay of (Delta t_AB) = t_A - t_B = 162.2 -5.9/+6.3 days and accretion
disk size estimate of log(r_s/cm) = 15.7 -0.5/+0.4 at 0.2 micron in the rest
frame are consistent with earlier estimates but suggest that existing methods
for estimating time delays in the presence of microlensing underestimate the
uncertainties. We are unable to measure a time delay for QJ0158-4325, but the
accretion disk size is log(r_s/cm) = 14.9 +/- 0.3 at 0.3 micron in the rest
frame.
| astro-ph | we expand our bayesian monte carlo method for analyzing the light curves of gravitationally lensed quasars to simultaneously estimate time delays and quasar structure including their mutual uncertainties we apply the method to he11041805 and qj01584325 two doublyimaged quasars with microlensing and intrinsic variability on comparable time scales for he11041805 the resulting time delay of delta t_ab t_a t_b 1622 5963 days and accretion disk size estimate of logr_scm 157 0504 at 02 micron in the rest frame are consistent with earlier estimates but suggest that existing methods for estimating time delays in the presence of microlensing underestimate the uncertainties we are unable to measure a time delay for qj01584325 but the accretion disk size is logr_scm 149 03 at 03 micron in the rest frame | [['we', 'expand', 'our', 'bayesian', 'monte', 'carlo', 'method', 'for', 'analyzing', 'the', 'light', 'curves', 'of', 'gravitationally', 'lensed', 'quasars', 'to', 'simultaneously', 'estimate', 'time', 'delays', 'and', 'quasar', 'structure', 'including', 'their', 'mutual', 'uncertainties', 'we', 'apply', 'the', 'method', 'to', 'he11041805', 'and', 'qj01584325', 'two', 'doublyimaged', 'quasars', 'with', 'microlensing', 'and', 'intrinsic', 'variability', 'on', 'comparable', 'time', 'scales', 'for', 'he11041805', 'the', 'resulting', 'time', 'delay', 'of', 'delta', 't_ab', 't_a', 't_b', '1622', '5963', 'days', 'and', 'accretion', 'disk', 'size', 'estimate', 'of', 'logr_scm', '157', '0504', 'at', '02', 'micron', 'in', 'the', 'rest', 'frame', 'are', 'consistent', 'with', 'earlier', 'estimates', 'but', 'suggest', 'that', 'existing', 'methods', 'for', 'estimating', 'time', 'delays', 'in', 'the', 'presence', 'of', 'microlensing', 'underestimate', 'the', 'uncertainties', 'we', 'are', 'unable', 'to', 'measure', 'a', 'time', 'delay', 'for', 'qj01584325', 'but', 'the', 'accretion', 'disk', 'size', 'is', 'logr_scm', '149', '03', 'at', '03', 'micron', 'in', 'the', 'rest', 'frame']] | [-0.06435513256808682, 0.09537988375391691, -0.05117137460770356, 0.09993969844823193, -0.062419802611393314, -0.10597430567647662, 0.049758250453329135, 0.45536330985205786, -0.1848974943221096, -0.3589441009774624, 0.09203141679209957, -0.3100318735119917, 0.03337750247690917, 0.2056861060386103, -0.06183732689298209, 0.03459407380151172, 0.04977835392327829, -0.10535162016223636, -0.06438992144690166, -0.26146457390765837, 0.23520092146786592, 0.08881851148250844, 0.15460878552027768, -0.028050342018926335, 0.09753045182479846, -0.047826177376743044, -0.12688064823798353, -0.0027655536616821926, -0.16946306772889888, 0.038117743063447694, 0.2253187100267819, 0.09670453642555062, 0.21674651495038322, -0.3126857541708065, -0.19953038294108644, 0.10104059703618047, 0.16567154735657236, 0.06565141108547969, 0.026047231744967342, -0.27014630674309426, 0.05851028509759119, -0.13068156579749718, -0.11170820451732125, 0.06742632391321804, 0.10387613236783974, 0.02341138063028695, -0.2184781801962902, 0.19462895690793952, -0.010647497500383084, 0.05633582983676705, -0.11636070250683735, -0.09312395648580164, -0.0226959110755894, 0.06385394007778697, 0.04104580829058954, 0.08311109610358178, 0.16194597630566288, -0.04978305525747278, -0.046863536677143026, 0.37487656743295733, -0.1047367715246735, -0.04004059909212013, 0.1628931221672364, -0.19869931365904067, -0.1511754076101727, 0.1996711553374846, 0.20761541525209923, 0.1308010476613192, -0.11601989899974151, -0.004934020139532344, 0.03646462389470769, 0.27542523142220754, 0.04467787014530791, 0.06698364693476187, 0.23902807734726417, 0.11551356272238697, 0.03356221571729909, 0.04498888224629956, -0.23160185957995935, -0.051545546010827586, -0.26663546244456104, -0.08166733464872043, -0.12352803600351175, 0.06950082189042962, -0.18182128850669194, -0.09307418807199405, 0.332482971535536, 0.18311427754252368, 0.23384886430276017, 0.17472831753172702, 0.3019502531331513, 0.1005587499042327, 0.06791494604136285, 0.13587129521258776, 0.31187211023643613, 0.10960394792979763, 0.10523365949648583, -0.2571105036862014, 0.09220096064100583, 0.020534028868085794] |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.