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 |
|---|---|---|---|---|---|---|
706.2714 | A Proof of Solomon's Rule | We put forward a proof of Solomon's rule, in terms of matrices, for
multiplication in the descent algebra of the symmetric group. Our proof
exploits the graphs that we can obtain from all the subsets of the set of
transpositions, $\{(i,i+1)\}_{i=1}^{n-1}$.
| math.CO | we put forward a proof of solomons rule in terms of matrices for multiplication in the descent algebra of the symmetric group our proof exploits the graphs that we can obtain from all the subsets of the set of transpositions ii1_i1n1 | [['we', 'put', 'forward', 'a', 'proof', 'of', 'solomons', 'rule', 'in', 'terms', 'of', 'matrices', 'for', 'multiplication', 'in', 'the', 'descent', 'algebra', 'of', 'the', 'symmetric', 'group', 'our', 'proof', 'exploits', 'the', 'graphs', 'that', 'we', 'can', 'obtain', 'from', 'all', 'the', 'subsets', 'of', 'the', 'set... | [-0.15518271522596477, 0.028442603070288897, -0.12138132303953171, 0.03526992227416485, -0.09144748406251893, -0.06369304669788108, 0.1007935632544104, 0.3265006814152002, -0.31654117931611836, -0.22854979863623157, 0.11899084391188808, -0.23831766545154096, -0.1403665140271187, 0.19929859878029674, -0.1040634858189150... |
706.2715 | Holographic trace anomaly at finite temperature | We find an exact coordinate transformation rule from the $AdS_5$
Schwarzschild black hole in the Poincare and the global patch to the
Fefferman-Graham coordinate system. Using these results, we evaluate the
corresponding holographic stress tensor and trace anomaly of the boundary
theory as a function of the radial co... | hep-th astro-ph hep-ph | we find an exact coordinate transformation rule from the ads_5 schwarzschild black hole in the poincare and the global patch to the feffermangraham coordinate system using these results we evaluate the corresponding holographic stress tensor and trace anomaly of the boundary theory as a function of the radial coordinat... | [['we', 'find', 'an', 'exact', 'coordinate', 'transformation', 'rule', 'from', 'the', 'ads_5', 'schwarzschild', 'black', 'hole', 'in', 'the', 'poincare', 'and', 'the', 'global', 'patch', 'to', 'the', 'feffermangraham', 'coordinate', 'system', 'using', 'these', 'results', 'we', 'evaluate', 'the', 'corresponding', 'holog... | [-0.1459356399559199, 0.030656723312161262, -0.18084207373473488, 0.061030642882193606, -0.0969170439312209, -0.08718053873449769, -0.0381001512462605, 0.30000123749040575, -0.27011762485418417, -0.20301362882329993, 0.10016505588452038, -0.2746018108286678, -0.15314231894604147, 0.07642752577691045, -0.022258261269698... |
706.2716 | Fusion algebra of critical percolation | We present an explicit conjecture for the chiral fusion algebra of critical
percolation considering Virasoro representations with no enlarged or extended
symmetry algebra. The representations we take to generate fusion are countably
infinite in number. The ensuing fusion rules are quasi-rational in the sense
that the... | hep-th cond-mat.stat-mech math-ph math.MP | we present an explicit conjecture for the chiral fusion algebra of critical percolation considering virasoro representations with no enlarged or extended symmetry algebra the representations we take to generate fusion are countably infinite in number the ensuing fusion rules are quasirational in the sense that the fusi... | [['we', 'present', 'an', 'explicit', 'conjecture', 'for', 'the', 'chiral', 'fusion', 'algebra', 'of', 'critical', 'percolation', 'considering', 'virasoro', 'representations', 'with', 'no', 'enlarged', 'or', 'extended', 'symmetry', 'algebra', 'the', 'representations', 'we', 'take', 'to', 'generate', 'fusion', 'are', 'co... | [-0.11484102428325318, 0.1454430158298367, -0.08779058906642268, 0.025407952082570687, -0.10533239339323093, -0.11969849844622547, 0.000983631209237501, 0.41216699772935717, -0.3016970557759383, -0.1777860603206569, 0.11980355432855763, -0.2604092138935812, -0.1663018002911399, 0.13987378646353527, -0.05490462391615091... |
706.2717 | Newton's 2nd Law and the Physics of Dance | In teaching the physical sciences, a significant challenge lies in the
student's tendency to consider the scientific world and the "real" world as
separate. For example, Newton's 1st Law of Motion states that an object in
motion remains in motion in a straight line unless acted on by an external
force. However, our e... | physics.ed-ph | in teaching the physical sciences a significant challenge lies in the students tendency to consider the scientific world and the real world as separate for example newtons 1st law of motion states that an object in motion remains in motion in a straight line unless acted on by an external force however our experience t... | [['in', 'teaching', 'the', 'physical', 'sciences', 'a', 'significant', 'challenge', 'lies', 'in', 'the', 'students', 'tendency', 'to', 'consider', 'the', 'scientific', 'world', 'and', 'the', 'real', 'world', 'as', 'separate', 'for', 'example', 'newtons', '1st', 'law', 'of', 'motion', 'states', 'that', 'an', 'object', '... | [-0.05179748786157807, 0.09277039411299144, -0.13878975889171177, 0.05038344255874153, -0.17129808987103265, -0.12774966301697288, 0.04219533673177404, 0.34524869009482195, -0.27589550139801866, -0.37785349324163375, 0.048994285135489445, -0.2713870597245484, -0.15594632643193979, 0.19587640669514997, -0.13242825892354... |
706.2718 | Universally defined representations of Lie conformal superalgebras | We distinguish a class of irreducible finite representations of conformal Lie
(super)algebras. These representations (called universally defined) are the
simplest ones from the computational point of view: a universally defined
representation of a conformal Lie (super)algebra $L$ is completely determined
by commutati... | math.QA math.RA | we distinguish a class of irreducible finite representations of conformal lie superalgebras these representations called universally defined are the simplest ones from the computational point of view a universally defined representation of a conformal lie superalgebra l is completely determined by commutation relations... | [['we', 'distinguish', 'a', 'class', 'of', 'irreducible', 'finite', 'representations', 'of', 'conformal', 'lie', 'superalgebras', 'these', 'representations', 'called', 'universally', 'defined', 'are', 'the', 'simplest', 'ones', 'from', 'the', 'computational', 'point', 'of', 'view', 'a', 'universally', 'defined', 'repre... | [-0.17272077963384158, 0.13189160371831524, -0.02283556260373614, 0.05801227430753205, -0.12658996965496913, -0.17352019004745906, -0.06258756399513521, 0.34984788134557393, -0.327849424760276, -0.21455359422877313, 0.07828574280421155, -0.2575236554684784, -0.18073639523135412, 0.16283756473588698, -0.0837355624807468... |
706.2719 | Do All Integrable Evolution Equations Have the Painlev\'e Property? | We examine whether the Painleve property is necessary for the integrability
of partial differential equations (PDEs). We show that in analogy to what
happens in the case of ordinary differential equations (ODEs) there exists a
class of PDEs, integrable through linearisation, which do not possess the
Painleve property... | nlin.SI math-ph math.AP math.MP | we examine whether the painleve property is necessary for the integrability of partial differential equations pdes we show that in analogy to what happens in the case of ordinary differential equations odes there exists a class of pdes integrable through linearisation which do not possess the painleve property the same... | [['we', 'examine', 'whether', 'the', 'painleve', 'property', 'is', 'necessary', 'for', 'the', 'integrability', 'of', 'partial', 'differential', 'equations', 'pdes', 'we', 'show', 'that', 'in', 'analogy', 'to', 'what', 'happens', 'in', 'the', 'case', 'of', 'ordinary', 'differential', 'equations', 'odes', 'there', 'exist... | [-0.17524244886949475, 0.054609319298631616, -0.08204191876575351, 0.1114794737458183, -0.1367660050947265, -0.20506418614797753, -0.05288764534598607, 0.339551920692126, -0.32509912824097237, -0.18159459332395114, 0.10205357439275602, -0.2884282964615174, -0.21109835536759577, 0.13352444174952438, -0.0770156107911909,... |
706.272 | Small Deviation Probability via Chaining | We obtain several extensions of Talagrand's lower bound for the small
deviation probability using metric entropy. For Gaussian processes, our
investigations are focused on processes with sub-polynomial and, respectively,
exponential behaviour of covering numbers. The corresponding results are also
proved for non-Gaus... | math.PR | we obtain several extensions of talagrands lower bound for the small deviation probability using metric entropy for gaussian processes our investigations are focused on processes with subpolynomial and respectively exponential behaviour of covering numbers the corresponding results are also proved for nongaussian symme... | [['we', 'obtain', 'several', 'extensions', 'of', 'talagrands', 'lower', 'bound', 'for', 'the', 'small', 'deviation', 'probability', 'using', 'metric', 'entropy', 'for', 'gaussian', 'processes', 'our', 'investigations', 'are', 'focused', 'on', 'processes', 'with', 'subpolynomial', 'and', 'respectively', 'exponential', '... | [-0.08228272955434826, 0.13898493668500286, -0.09313969388984752, 0.1442925340230338, -0.0017119475926917333, -0.11602219995350027, 0.07263348257551208, 0.3380333326327113, -0.24258597933639509, -0.26436585671483326, 0.14342187293238032, -0.2650580361772042, -0.11633600497122806, 0.2831376702644122, -0.0359249912703839... |
706.2721 | Associative algebras related to conformal algebras | In this note, we introduce a class of algebras that are in some sense related
to conformal algebras. This class (called TC-algebras) includes Weyl algebras
and some of their (associative and Lie) subalgebras. By a conformal algebra we
generally mean what is known as $H$-pseudo-algebra over the polynomial Hopf
algebra... | math.QA math.RA | in this note we introduce a class of algebras that are in some sense related to conformal algebras this class called tcalgebras includes weyl algebras and some of their associative and lie subalgebras by a conformal algebra we generally mean what is known as hpseudoalgebra over the polynomial hopf algebra hbbbkt_1 t_n ... | [['in', 'this', 'note', 'we', 'introduce', 'a', 'class', 'of', 'algebras', 'that', 'are', 'in', 'some', 'sense', 'related', 'to', 'conformal', 'algebras', 'this', 'class', 'called', 'tcalgebras', 'includes', 'weyl', 'algebras', 'and', 'some', 'of', 'their', 'associative', 'and', 'lie', 'subalgebras', 'by', 'a', 'confor... | [-0.15202282567216613, 0.1003907184227745, -0.04980248446339992, 0.06955680111944397, -0.18041965585035175, -0.13554138610306293, -0.08171712489861216, 0.3877387193323516, -0.35612322296252225, -0.1829763442875623, 0.1484066790835098, -0.23342617195266396, -0.23212593265656215, 0.17837003626818979, -0.1636893341818185,... |
706.2722 | Three-jet event-shapes: first NLO+NLL+1/Q results | Three-jet event-shape distributions can be exploited to investigate the
dependence of hadronisation effects on the colour and the geometry of the
underlying hard event. We present here the first comparison of data in e+e-
annihilation and state-of-the-art theoretical predictions, including
resummation of large logari... | hep-ph | threejet eventshape distributions can be exploited to investigate the dependence of hadronisation effects on the colour and the geometry of the underlying hard event we present here the first comparison of data in ee annihilation and stateoftheart theoretical predictions including resummation of large logarithms at nex... | [['threejet', 'eventshape', 'distributions', 'can', 'be', 'exploited', 'to', 'investigate', 'the', 'dependence', 'of', 'hadronisation', 'effects', 'on', 'the', 'colour', 'and', 'the', 'geometry', 'of', 'the', 'underlying', 'hard', 'event', 'we', 'present', 'here', 'the', 'first', 'comparison', 'of', 'data', 'in', 'ee',... | [-0.04305593438591037, 0.039180761708974325, -0.16980821600761906, 0.1862270019241962, -0.08252348946728583, -0.018482322598895828, -0.014124092695620392, 0.37800259486740007, -0.18423197815066267, -0.3176572282381099, 0.015568661702202698, -0.35950185522308636, 0.004079970458907814, 0.11294945037185118, 0.027772114186... |
706.2723 | Mass segregation in very young open clusters -- A case study of NGC 2244
and NGC 6530 | We derive the proper motions, membership probabilities, and velocity
dispersions of stars in the regions of the young (about 2-4 Myr-old) open
clusters NGC 2244 (the central cluster in the Monoceros R2 association) and NGC
6530 (the dominant cluster in the Sgr OB1 association) from photographic plate
material obtaine... | astro-ph | we derive the proper motions membership probabilities and velocity dispersions of stars in the regions of the young about 24 myrold open clusters ngc 2244 the central cluster in the monoceros r2 association and ngc 6530 the dominant cluster in the sgr ob1 association from photographic plate material obtained at shangha... | [['we', 'derive', 'the', 'proper', 'motions', 'membership', 'probabilities', 'and', 'velocity', 'dispersions', 'of', 'stars', 'in', 'the', 'regions', 'of', 'the', 'young', 'about', '24', 'myrold', 'open', 'clusters', 'ngc', '2244', 'the', 'central', 'cluster', 'in', 'the', 'monoceros', 'r2', 'association', 'and', 'ngc'... | [-0.10144946935775113, 0.08776078479630607, -0.10487977005763068, 0.09155841033512149, -0.08778961794340007, -0.057234780556921445, 0.0721564918623439, 0.4310380694500747, -0.1712019717762901, -0.3391862581794461, 0.049114681839654666, -0.24587268622680788, -0.02280728427715422, 0.1826463347838615, -0.03753097562335564... |
706.2724 | A search for ultra-compact dwarf galaxies in the Centaurus galaxy
cluster | Aim: To extend the investigations of ultra-compact dwarf galaxies (UCDs)
beyond the well studied Fornax and Virgo clusters. Methods: We measured
spectroscopic redshifts of about 400 compact object candidates with 19.2 < V <
22.4 mag in the central region of the Centaurus galaxy cluster (d=43Mpc), using
VIMOS@VLT. The... | astro-ph | aim to extend the investigations of ultracompact dwarf galaxies ucds beyond the well studied fornax and virgo clusters methods we measured spectroscopic redshifts of about 400 compact object candidates with 192 v 224 mag in the central region of the centaurus galaxy cluster d43mpc using vimosvlt the luminosity range of... | [['aim', 'to', 'extend', 'the', 'investigations', 'of', 'ultracompact', 'dwarf', 'galaxies', 'ucds', 'beyond', 'the', 'well', 'studied', 'fornax', 'and', 'virgo', 'clusters', 'methods', 'we', 'measured', 'spectroscopic', 'redshifts', 'of', 'about', '400', 'compact', 'object', 'candidates', 'with', '192', 'v', '224', 'm... | [-0.030133875557682016, 0.055004981114930344, -0.07230794208035582, 0.112972917065925, -0.134982132398943, -0.01725645325975595, 0.07300725719045452, 0.4672952358143561, -0.0632828039495827, -0.42169880116360103, 0.002515717610825986, -0.31111100848061424, 0.019914471233884495, 0.2175734770597699, -0.09548752869988089,... |
706.2725 | The Complexity of Determining Existence a Hamiltonian Cycle is $O(n^3)$ | The Hamiltonian cycle problem in digraph is mapped into a matching cover
bipartite graph. Based on this mapping, it is proved that determining existence
a Hamiltonian cycle in graph is $O(n^3)$.
| cs.DS cs.CC cs.DM | the hamiltonian cycle problem in digraph is mapped into a matching cover bipartite graph based on this mapping it is proved that determining existence a hamiltonian cycle in graph is on3 | [['the', 'hamiltonian', 'cycle', 'problem', 'in', 'digraph', 'is', 'mapped', 'into', 'a', 'matching', 'cover', 'bipartite', 'graph', 'based', 'on', 'this', 'mapping', 'it', 'is', 'proved', 'that', 'determining', 'existence', 'a', 'hamiltonian', 'cycle', 'in', 'graph', 'is', 'on3']] | [-0.2267883173941124, 0.07743855552267163, -0.07343437120078071, 0.05271859272503324, -0.08538569287667351, -0.1632693614435172, 0.049063076715796225, 0.39227576607898357, -0.26415879351477467, -0.2969172620364735, 0.14906628130214108, -0.2613343144616773, -0.20089527631118412, 0.09564692034356055, -0.10426760353748837... |
706.2726 | Probing the Role of the Barrier Layer in Magnetic Tunnel Junction
Transport | Magnetic tunnel junctions with a ferrimagnetic barrier layer have been
studied to understand the role of the barrier layer in the tunneling process -
a factor that has been largely overlooked until recently. Epitaxial oxide
junctions of highly spin polarized La0.7Sr0.3MnO3 and Fe3O4 electrodes with
magnetic NiMn2O4 (... | cond-mat.str-el cond-mat.mtrl-sci | magnetic tunnel junctions with a ferrimagnetic barrier layer have been studied to understand the role of the barrier layer in the tunneling process a factor that has been largely overlooked until recently epitaxial oxide junctions of highly spin polarized la07sr03mno3 and fe3o4 electrodes with magnetic nimn2o4 nmo insu... | [['magnetic', 'tunnel', 'junctions', 'with', 'a', 'ferrimagnetic', 'barrier', 'layer', 'have', 'been', 'studied', 'to', 'understand', 'the', 'role', 'of', 'the', 'barrier', 'layer', 'in', 'the', 'tunneling', 'process', 'a', 'factor', 'that', 'has', 'been', 'largely', 'overlooked', 'until', 'recently', 'epitaxial', 'oxi... | [-0.19474796772512615, 0.21522415093440786, -0.018553599619712584, 0.002661584838247847, -0.020898959973556362, -0.18247704934647196, 0.06744253409142868, 0.4194031696543734, -0.2997860541312486, -0.32896438447965515, -0.019917585940745015, -0.3129764648679739, -0.05945021030692081, 0.19323005758098558, 0.0959181086116... |
706.2727 | Truly naked spherically-symmetric and distorted black holes | We demonstrate the existence of spherically-symmetric truly naked black holes
(TNBH) for which the Kretschmann scalar is finite on the horizon but some
curvature components including those responsible for tidal forces as well as
the energy density $\bar{\rho}$ measured by a free-falling observer are
infinite. We choo... | gr-qc hep-th math.DG | we demonstrate the existence of sphericallysymmetric truly naked black holes tnbh for which the kretschmann scalar is finite on the horizon but some curvature components including those responsible for tidal forces as well as the energy density barrho measured by a freefalling observer are infinite we choose a rather g... | [['we', 'demonstrate', 'the', 'existence', 'of', 'sphericallysymmetric', 'truly', 'naked', 'black', 'holes', 'tnbh', 'for', 'which', 'the', 'kretschmann', 'scalar', 'is', 'finite', 'on', 'the', 'horizon', 'but', 'some', 'curvature', 'components', 'including', 'those', 'responsible', 'for', 'tidal', 'forces', 'as', 'wel... | [-0.16892093380057183, 0.1359549824120995, -0.10874539635324516, 0.1307919168497592, -0.09446448782146666, -0.1417636338653678, -0.05512038478358632, 0.31177880799645463, -0.19700882748856796, -0.2486131711932965, 0.12381997092888082, -0.2847903217740809, -0.1402210525352766, 0.20568792006092393, -0.052038570680262554,... |
706.2728 | Jet Areas, and What They are Good For | We introduce the concept of the area of a jet, and show how it can be used to
perform the subtraction of even a large amount of diffuse noise from hard jets.
| hep-ph | we introduce the concept of the area of a jet and show how it can be used to perform the subtraction of even a large amount of diffuse noise from hard jets | [['we', 'introduce', 'the', 'concept', 'of', 'the', 'area', 'of', 'a', 'jet', 'and', 'show', 'how', 'it', 'can', 'be', 'used', 'to', 'perform', 'the', 'subtraction', 'of', 'even', 'a', 'large', 'amount', 'of', 'diffuse', 'noise', 'from', 'hard', 'jets']] | [-0.058301739394664764, 0.10286234089289792, -0.14326923136832193, 0.13825355959124863, -0.052903714939020574, -0.053456115623703226, 0.036723429744597524, 0.41703186952508986, -0.29188970720861107, -0.34526959527283907, 0.11098570159811061, -0.23629348818212748, -0.10654513433109969, 0.19339045940432698, -0.0878928142... |
706.2729 | Polarization dependence of emission spectra of multiexcitons in
self-assembled quantum dots | We have investigated the polarization dependence of the emission spectra of
p-shell multiexcitons of a quantum dot when the single particle level spacing
is larger than the characteristic energy of the Coulomb interactions. We find
that there are many degenerate multiexciton states. The emission intensities
depend on... | cond-mat.mes-hall | we have investigated the polarization dependence of the emission spectra of pshell multiexcitons of a quantum dot when the single particle level spacing is larger than the characteristic energy of the coulomb interactions we find that there are many degenerate multiexciton states the emission intensities depend on the ... | [['we', 'have', 'investigated', 'the', 'polarization', 'dependence', 'of', 'the', 'emission', 'spectra', 'of', 'pshell', 'multiexcitons', 'of', 'a', 'quantum', 'dot', 'when', 'the', 'single', 'particle', 'level', 'spacing', 'is', 'larger', 'than', 'the', 'characteristic', 'energy', 'of', 'the', 'coulomb', 'interactions... | [-0.15828462832552545, 0.2381441427011262, -0.030501694654744557, 0.09137682973078506, 0.043764552211060244, -0.11763359354808926, 0.006208783870919005, 0.3723315620247056, -0.20997069010730177, -0.2980022392509615, -0.013629100599107059, -0.31920461339109085, -0.0413551574025084, 0.14809136538191095, 0.091765637147952... |
706.273 | Charge Exchange Spin-Dipole Excitations of 90Zr and 208Pb and Neutron
Matter Equation of State | Charge exchange spin-dipole (SD) excitations of $^{90}$Zr and $^{208}$Pb are
studied by using a Skyrme
Hartree-Fock(HF) + Random Phase approximation (RPA). The calculated
spin-dipole strength distributions are compared with experimental data obtained
by $^{90}$Zr (p,n) $^{90}$Nb and $^{90}$Zr (n,p) $^{90}$ Nb react... | nucl-th | charge exchange spindipole sd excitations of 90zr and 208pb are studied by using a skyrme hartreefockhf random phase approximation rpa the calculated spindipole strength distributions are compared with experimental data obtained by 90zr pn 90nb and 90zr np 90 nb reactions the modelindependent sd sum rule values of vari... | [['charge', 'exchange', 'spindipole', 'sd', 'excitations', 'of', '90zr', 'and', '208pb', 'are', 'studied', 'by', 'using', 'a', 'skyrme', 'hartreefockhf', 'random', 'phase', 'approximation', 'rpa', 'the', 'calculated', 'spindipole', 'strength', 'distributions', 'are', 'compared', 'with', 'experimental', 'data', 'obtaine... | [-0.0788697036303053, 0.1983628616088559, -0.046316501762685036, 0.16728294743319053, 0.011241121386939829, -0.0856631214147189, 0.06161345151074306, 0.34173787539504996, -0.14623070694035803, -0.3144100507288569, -0.0918909389551522, -0.3603684114141747, 0.024629524711406593, 0.1229553207416426, 0.12799405516360443, 0... |
706.2731 | On the behavior of Castelnuovo-Mumford regularity with respect to some
functors | We investigate the behavior of Castelnuovo-Mumford regularity with respect to
some classical functors : Tor, the Frobenius functor in positive
characteristic, taking a power or a product (on ideals). These generalizes and
refines previous results on these issues by several authors. As an application
we provide result... | math.AC math.AG | we investigate the behavior of castelnuovomumford regularity with respect to some classical functors tor the frobenius functor in positive characteristic taking a power or a product on ideals these generalizes and refines previous results on these issues by several authors as an application we provide results on the re... | [['we', 'investigate', 'the', 'behavior', 'of', 'castelnuovomumford', 'regularity', 'with', 'respect', 'to', 'some', 'classical', 'functors', 'tor', 'the', 'frobenius', 'functor', 'in', 'positive', 'characteristic', 'taking', 'a', 'power', 'or', 'a', 'product', 'on', 'ideals', 'these', 'generalizes', 'and', 'refines', ... | [-0.1885595000629504, -0.012707051924494353, -0.07710220385342836, 0.043612252988190534, -0.06392576742962182, -0.10205818678488035, 0.010631573835320502, 0.34215747232896737, -0.3209701573801597, -0.21011887562351794, 0.14985944193799094, -0.22947106016196692, -0.13665253966654012, 0.27048195147583914, -0.194444061066... |
706.2732 | A Design Methodology for Space-Time Adapter | This paper presents a solution to efficiently explore the design space of
communication adapters. In most digital signal processing (DSP) applications,
the overall architecture of the system is significantly affected by
communication architecture, so the designers need specifically optimized
adapters. By explicitly m... | cs.AR | this paper presents a solution to efficiently explore the design space of communication adapters in most digital signal processing dsp applications the overall architecture of the system is significantly affected by communication architecture so the designers need specifically optimized adapters by explicitly modeling ... | [['this', 'paper', 'presents', 'a', 'solution', 'to', 'efficiently', 'explore', 'the', 'design', 'space', 'of', 'communication', 'adapters', 'in', 'most', 'digital', 'signal', 'processing', 'dsp', 'applications', 'the', 'overall', 'architecture', 'of', 'the', 'system', 'is', 'significantly', 'affected', 'by', 'communic... | [-0.19632874479199328, -0.013485428139286274, -0.06479284800286216, 0.012839766662204412, -0.14844963891333257, -0.21056295368759856, 0.059479666193303596, 0.4227107432254446, -0.2953611311883234, -0.38575267820520615, 0.0856060742502805, -0.20017360514257013, -0.2190185861730176, 0.16659374500064528, -0.12307966904283... |
706.2733 | Ultrasoft contribution to quarkonium production and annihilation | We compute the third-order correction to electromagnetic
S-wave quarkonium production and annihilation rates due to the emission and
absorption of an ultrasoft gluon. Our result completes the analysis of the
non-relativistic quarkonium bound-state dynamics in the
next-to-next-to-next-to-leading order. The impact of... | hep-ph | we compute the thirdorder correction to electromagnetic swave quarkonium production and annihilation rates due to the emission and absorption of an ultrasoft gluon our result completes the analysis of the nonrelativistic quarkonium boundstate dynamics in the nexttonexttonexttoleading order the impact of the ultrasoft c... | [['we', 'compute', 'the', 'thirdorder', 'correction', 'to', 'electromagnetic', 'swave', 'quarkonium', 'production', 'and', 'annihilation', 'rates', 'due', 'to', 'the', 'emission', 'and', 'absorption', 'of', 'an', 'ultrasoft', 'gluon', 'our', 'result', 'completes', 'the', 'analysis', 'of', 'the', 'nonrelativistic', 'qua... | [-0.0687605118086972, 0.16095503677946507, -0.10911371066408643, 0.1718337303915424, -0.03214236088412798, -0.0428891509645066, 0.019806839071877174, 0.32212945926239933, -0.1589704575806351, -0.20109795119171425, -0.09283174037878102, -0.3841278350012282, 0.06619227677583694, 0.09019942499570928, 0.16169454334145886, ... |
706.2734 | Towards a realistic neutrino mass formula: part two | A two-parameter neutrino mass formula is described, giving a moderately
hierarchical spectrum m_1 < m_2 < m_3 consistent with the experimental
estimates of Delta m^2_{21} and Delta m^2_{32}. The formula follows from a
three-parameter empirical neutrino mass formula through imposing a parameter
constraint and leads to... | physics.gen-ph | a twoparameter neutrino mass formula is described giving a moderately hierarchical spectrum m_1 m_2 m_3 consistent with the experimental estimates of delta m2_21 and delta m2_32 the formula follows from a threeparameter empirical neutrino mass formula through imposing a parameter constraint and leads to a very simple n... | [['a', 'twoparameter', 'neutrino', 'mass', 'formula', 'is', 'described', 'giving', 'a', 'moderately', 'hierarchical', 'spectrum', 'm_1', 'm_2', 'm_3', 'consistent', 'with', 'the', 'experimental', 'estimates', 'of', 'delta', 'm2_21', 'and', 'delta', 'm2_32', 'the', 'formula', 'follows', 'from', 'a', 'threeparameter', 'e... | [-0.15621177544817327, 0.20556792129895518, -0.03387768398970366, 0.17784431322111882, -0.1262365306261927, -0.22412697757328195, 0.14591159000493853, 0.30024804116359777, -0.16083184485988958, -0.3660122753254005, 0.06705684786928552, -0.26523263012724263, -0.06263720630002874, 0.23633093695555416, -0.0253619246783533... |
706.2735 | Sums of $L$-functions over the rational function field | Friedberg, Hoffstein and Lieman have constructed two related multiple
Dirichlet series from quadratic and higher-order $L$-functions and Gauss sums.
We compute these multiple Dirichlet series explicitly in the case of the
rational function field. This is done by utilizing the functional equation of
the $L$-functions ... | math.NT | friedberg hoffstein and lieman have constructed two related multiple dirichlet series from quadratic and higherorder lfunctions and gauss sums we compute these multiple dirichlet series explicitly in the case of the rational function field this is done by utilizing the functional equation of the lfunctions and the func... | [['friedberg', 'hoffstein', 'and', 'lieman', 'have', 'constructed', 'two', 'related', 'multiple', 'dirichlet', 'series', 'from', 'quadratic', 'and', 'higherorder', 'lfunctions', 'and', 'gauss', 'sums', 'we', 'compute', 'these', 'multiple', 'dirichlet', 'series', 'explicitly', 'in', 'the', 'case', 'of', 'the', 'rational... | [-0.18419516482390463, -0.010326524854035062, -0.14944013638202758, 0.10781732163227656, -0.10447750687051345, -0.09289647717549301, 0.026622826691463534, 0.3027992818833274, -0.34699066394173045, -0.24793937805053942, 0.08312264713972314, -0.2808274380753146, -0.18094660823836045, 0.2148972087101463, 0.006520862115875... |
706.2736 | Topological gravitation on graph manifolds | A model of topological field theory is presented in which the vacuum coupling
constants are topological invariants of the four-dimensional spacetime. Thus
the coupling constants are theoretically computable, and they indicate the
topological structure of our universe.
| gr-qc | a model of topological field theory is presented in which the vacuum coupling constants are topological invariants of the fourdimensional spacetime thus the coupling constants are theoretically computable and they indicate the topological structure of our universe | [['a', 'model', 'of', 'topological', 'field', 'theory', 'is', 'presented', 'in', 'which', 'the', 'vacuum', 'coupling', 'constants', 'are', 'topological', 'invariants', 'of', 'the', 'fourdimensional', 'spacetime', 'thus', 'the', 'coupling', 'constants', 'are', 'theoretically', 'computable', 'and', 'they', 'indicate', 't... | [-0.22896527452394366, 0.23887231351958738, -0.11145850230713149, 0.08977357044224502, -0.06860368442092393, -0.12415519848818311, -0.004613301329742614, 0.33852906197913596, -0.2721287992254302, -0.253883696488432, 0.048700761751624175, -0.2402757580920651, -0.18273452749928912, 0.1541783337393222, 0.02769417539742347... |
706.2737 | Constraints on the DGP Universe Using Observational Hubble parameter | In this work, we use observations of the Hubble parameter from the
differential ages of passively evolving galaxies and the recent detection of
the Baryon Acoustic Oscillations (BAO) at $z_1=0.35$ to constrain the
Dvali-Gabadadze-Porrati (DGP) universe. For the case with a curvature term, we
set a prior $h=0.73\pm0.0... | astro-ph | in this work we use observations of the hubble parameter from the differential ages of passively evolving galaxies and the recent detection of the baryon acoustic oscillations bao at z_1035 to constrain the dvaligabadadzeporrati dgp universe for the case with a curvature term we set a prior h073pm003 and the bestfit va... | [['in', 'this', 'work', 'we', 'use', 'observations', 'of', 'the', 'hubble', 'parameter', 'from', 'the', 'differential', 'ages', 'of', 'passively', 'evolving', 'galaxies', 'and', 'the', 'recent', 'detection', 'of', 'the', 'baryon', 'acoustic', 'oscillations', 'bao', 'at', 'z_1035', 'to', 'constrain', 'the', 'dvaligabada... | [-0.07956913695670664, 0.10257524666505763, -0.08641170922459827, 0.06902482072635191, -0.16417998388513094, -0.08039292615527908, 0.031008402506510418, 0.34046089913075167, -0.1690630529515652, -0.29189407769040876, 0.051901122905999526, -0.2972036372197585, -0.04518759130991788, 0.1915649672349294, -0.021440615819301... |
706.2738 | Two-Loop Massive Operator Matrix Elements for Polarized and Unpolarized
Deep-Inelastic Scattering | The $O(\alpha_s^2)$ massive operator matrix elements for unpolarized and
polarized heavy flavor production at asymptotic values $Q^2 >> m^2$ are
calculated in Mellin space without applying the integration-by-parts method. We
confirm previous results given in Refs. \cite{BU1,BU2}, however, obtain much
more compact rep... | hep-ph | the oalpha_s2 massive operator matrix elements for unpolarized and polarized heavy flavor production at asymptotic values q2 m2 are calculated in mellin space without applying the integrationbyparts method we confirm previous results given in refs citebu1bu2 however obtain much more compact representations | [['the', 'oalpha_s2', 'massive', 'operator', 'matrix', 'elements', 'for', 'unpolarized', 'and', 'polarized', 'heavy', 'flavor', 'production', 'at', 'asymptotic', 'values', 'q2', 'm2', 'are', 'calculated', 'in', 'mellin', 'space', 'without', 'applying', 'the', 'integrationbyparts', 'method', 'we', 'confirm', 'previous',... | [-0.05536945789155164, 0.17830579595004276, -0.06167488321434797, 0.1416723574170979, -0.052034148355809655, -0.07353750300570959, 0.046728243551603175, 0.3990414684138647, -0.10911800789578659, -0.22596205205361292, 0.02891011049448535, -0.3130039675388394, -0.04270774781953816, 0.21211864344957398, 0.0112226606323951... |
706.2739 | Measuring the Balmer Jump and Effective Gravity in FGK Stars | It is difficult to accurately measure the effective gravity (log g) in
late-type stars using broadband (eg. UBV or SDSS) or intermediate-band (uvby)
photometric systems, especially when the stars can cover a range of
metallicities and reddenings. However, simple spectroscopic observational and
data reduction techniqu... | astro-ph | it is difficult to accurately measure the effective gravity log g in latetype stars using broadband eg ubv or sdss or intermediateband uvby photometric systems especially when the stars can cover a range of metallicities and reddenings however simple spectroscopic observational and data reduction techniques can yield a... | [['it', 'is', 'difficult', 'to', 'accurately', 'measure', 'the', 'effective', 'gravity', 'log', 'g', 'in', 'latetype', 'stars', 'using', 'broadband', 'eg', 'ubv', 'or', 'sdss', 'or', 'intermediateband', 'uvby', 'photometric', 'systems', 'especially', 'when', 'the', 'stars', 'can', 'cover', 'a', 'range', 'of', 'metallic... | [-0.007702625534661552, 0.05896781755761955, -0.0818917921210146, 0.10016795933445204, -0.14146411820547655, -0.1438170034534243, 0.09427999062737559, 0.4715610435780357, -0.15958244742496924, -0.4369676864212927, 0.06771252190125832, -0.34237043015823204, -0.022078361293739256, 0.28318073223208023, -0.148506133009077,... |
706.274 | Mapping Class Groups and Interpolating Complexes: Rank | A family of interpolating graphs $\calC (S, \xi)$ of complexity $\xi$ is
constructed for a surface $S$ and $-2 \leq \xi \leq \xi (S)$. For $\xi = -2,
-1, \xi (S) -1$ these specialise to graphs quasi-isometric to the marking
graph, the pants graph and the curve graph respectively. We generalise Theorems
of Brock-Farb ... | math.GT math.GR | a family of interpolating graphs calc s xi of complexity xi is constructed for a surface s and 2 leq xi leq xi s for xi 2 1 xi s 1 these specialise to graphs quasiisometric to the marking graph the pants graph and the curve graph respectively we generalise theorems of brockfarb and behrstockminsky to show that the rank... | [['a', 'family', 'of', 'interpolating', 'graphs', 'calc', 's', 'xi', 'of', 'complexity', 'xi', 'is', 'constructed', 'for', 'a', 'surface', 's', 'and', '2', 'leq', 'xi', 'leq', 'xi', 's', 'for', 'xi', '2', '1', 'xi', 's', '1', 'these', 'specialise', 'to', 'graphs', 'quasiisometric', 'to', 'the', 'marking', 'graph', 'the... | [-0.21095331275666301, 0.15838065846926636, -0.04197683860783023, 0.07587082695799192, -0.034328280510663084, -0.20714772496410092, 0.012836448551917618, 0.35167375301020315, -0.2658579654502447, -0.2812793074608451, 0.011318288262547794, -0.34085992185605896, -0.050692777083528165, 0.13773793007501148, -0.075614586020... |
706.2741 | Study of Triple-Gauge-Boson Couplings ZZZ, ZZgam and Zgamgam at LEP | Neutral triple-gauge-boson couplings ZZZ, ZZgam and Zgamgam have been studied
with the DELPHI detector using data at energies between 183 and 208 GeV. Limits
are derived on these couplings from an analysis of the reactions e+e- -> Zgam,
using data from the final states gamma f fbar, with f = q or neutrino, from
e+e- ... | hep-ex | neutral triplegaugeboson couplings zzz zzgam and zgamgam have been studied with the delphi detector using data at energies between 183 and 208 gev limits are derived on these couplings from an analysis of the reactions ee zgam using data from the final states gamma f fbar with f q or neutrino from ee zz using data from... | [['neutral', 'triplegaugeboson', 'couplings', 'zzz', 'zzgam', 'and', 'zgamgam', 'have', 'been', 'studied', 'with', 'the', 'delphi', 'detector', 'using', 'data', 'at', 'energies', 'between', '183', 'and', '208', 'gev', 'limits', 'are', 'derived', 'on', 'these', 'couplings', 'from', 'an', 'analysis', 'of', 'the', 'reacti... | [-0.0706052017219078, 0.2421014865333116, -0.051550479150878695, 0.06723713063312552, 0.01973467718523282, -0.1943742690106424, 0.12736843474066029, 0.28040379772965723, -0.19012683177581774, -0.24326848533864204, -0.13361400289353556, -0.42009844206846675, 0.06913941669671868, 0.13857939768260202, 0.13552078562788666,... |
706.2742 | Closed String Tachyons on AdS Orbifolds and Dual Yang-Mills Instantons | We study the condensation of localized closed string tachyons on AdS
orbifolds both from the bulk and boundary theory viewpoints. We first extend
the known results for AdS_5/Z_k to AdS_3/Z_k case, and we proposed that the
AdS_3/Z_k decays into AdS_3/Z_k' with k' < k. From the bulk viewpoint, we
obtain a time-dependen... | hep-th | we study the condensation of localized closed string tachyons on ads orbifolds both from the bulk and boundary theory viewpoints we first extend the known results for ads_5z_k to ads_3z_k case and we proposed that the ads_3z_k decays into ads_3z_k with k k from the bulk viewpoint we obtain a timedependent gravity solut... | [['we', 'study', 'the', 'condensation', 'of', 'localized', 'closed', 'string', 'tachyons', 'on', 'ads', 'orbifolds', 'both', 'from', 'the', 'bulk', 'and', 'boundary', 'theory', 'viewpoints', 'we', 'first', 'extend', 'the', 'known', 'results', 'for', 'ads_5z_k', 'to', 'ads_3z_k', 'case', 'and', 'we', 'proposed', 'that',... | [-0.15102108525952287, 0.18700659643018655, -0.07996729481965303, 0.11856331742746037, -0.044412482855537165, -0.15083142015413423, 0.022565987862774407, 0.32795559729333795, -0.1920899152481819, -0.22297800029171447, 0.06433333393438945, -0.293439521241227, -0.13835915610242902, 0.11503357329448453, -0.029040283651328... |
706.2743 | Obtaining New Dividing Formulas n|Q(n) From the Known Ones | In this note, we present a few methods (Theorems 1, 2, and 3) from discrete
dynamical systems theory of obtaining new functions Q(n) from the known ones so
that the dividing formulas n|Q(n) hold.
| math.NT math.DS | in this note we present a few methods theorems 1 2 and 3 from discrete dynamical systems theory of obtaining new functions qn from the known ones so that the dividing formulas nqn hold | [['in', 'this', 'note', 'we', 'present', 'a', 'few', 'methods', 'theorems', '1', '2', 'and', '3', 'from', 'discrete', 'dynamical', 'systems', 'theory', 'of', 'obtaining', 'new', 'functions', 'qn', 'from', 'the', 'known', 'ones', 'so', 'that', 'the', 'dividing', 'formulas', 'nqn', 'hold']] | [-0.07095944863094976, 0.07689168628756747, -0.12633502991362053, 0.12185653167508656, 0.008029391706892939, -0.15593556978274137, 0.06035099763098652, 0.309935366283312, -0.271415447195371, -0.28248511325342185, 0.12760796445548872, -0.27544574143195694, -0.19955305630962053, 0.2445184914395213, -0.0625122751821023, 0... |
706.2744 | Dynamical instabilities of Bose-Einstein condensates at the band-edge in
one-dimensional optical lattices | We report on experiments that demonstrate dynamical instability in a
Bose-Einstein condensate at the band-edge of a one-dimensional optical lattice.
The instability manifests as rapid depletion of the condensate and conversion
to a thermal cloud. We consider the collisional processes that can occur in
such a system, ... | cond-mat.other quant-ph | we report on experiments that demonstrate dynamical instability in a boseeinstein condensate at the bandedge of a onedimensional optical lattice the instability manifests as rapid depletion of the condensate and conversion to a thermal cloud we consider the collisional processes that can occur in such a system and perf... | [['we', 'report', 'on', 'experiments', 'that', 'demonstrate', 'dynamical', 'instability', 'in', 'a', 'boseeinstein', 'condensate', 'at', 'the', 'bandedge', 'of', 'a', 'onedimensional', 'optical', 'lattice', 'the', 'instability', 'manifests', 'as', 'rapid', 'depletion', 'of', 'the', 'condensate', 'and', 'conversion', 't... | [-0.07405416325597865, 0.09916859407099039, -0.13656024848739426, 0.07965456214600916, -0.017341386605379726, -0.08467766987178778, 0.06500067227951638, 0.3713453546643439, -0.22373372934213498, -0.26486085482486865, 0.05679784955294061, -0.2895787229130425, -0.15579879391044985, 0.21898477835338412, 0.0367307456066392... |
706.2745 | Hubble Space Telescope Imaging of the Expanding Nebular Remnant of the
Recurrent Nova RS Ophiuchi (2006) | We report Hubble Space Telescope imaging obtained 155 days after the 2006
outburst of RS Ophiuchi. We detect extended emission in both [O III] and [Ne V]
lines. In both lines, the remnant has a double ring structure. The E-W
orientation and total extent of these structures (580+-50 AU at d=1.6kpc) is
consistent with ... | astro-ph | we report hubble space telescope imaging obtained 155 days after the 2006 outburst of rs ophiuchi we detect extended emission in both o iii and ne v lines in both lines the remnant has a double ring structure the ew orientation and total extent of these structures 58050 au at d16kpc is consistent with that expected due... | [['we', 'report', 'hubble', 'space', 'telescope', 'imaging', 'obtained', '155', 'days', 'after', 'the', '2006', 'outburst', 'of', 'rs', 'ophiuchi', 'we', 'detect', 'extended', 'emission', 'in', 'both', 'o', 'iii', 'and', 'ne', 'v', 'lines', 'in', 'both', 'lines', 'the', 'remnant', 'has', 'a', 'double', 'ring', 'structu... | [-0.1014651740091316, 0.09552739305067653, -0.055536573348674644, 0.026651904956737825, -0.08685548845216755, -0.08353591674346138, 0.03302958702128804, 0.4393062108650434, -0.19639173048704262, -0.2817456324696387, 0.0836181097709579, -0.2686019335615579, -0.07014869007643712, 0.17296816640310297, -0.00317419943506641... |
706.2746 | Abstract Storage Devices | A quantum storage device differs radically from a conventional physical
storage device. Its state can be set to any value in a certain (infinite) state
space, but in general every possible read operation yields only partial
information about the stored state.
The purpose of this paper is to initiate the study of a ... | cs.DM cs.CC cs.IT math.IT | a quantum storage device differs radically from a conventional physical storage device its state can be set to any value in a certain infinite state space but in general every possible read operation yields only partial information about the stored state the purpose of this paper is to initiate the study of a combinato... | [['a', 'quantum', 'storage', 'device', 'differs', 'radically', 'from', 'a', 'conventional', 'physical', 'storage', 'device', 'its', 'state', 'can', 'be', 'set', 'to', 'any', 'value', 'in', 'a', 'certain', 'infinite', 'state', 'space', 'but', 'in', 'general', 'every', 'possible', 'read', 'operation', 'yields', 'only', '... | [-0.16360079321373058, 0.11695203191767704, -0.10335352072541258, 0.03653640905824049, -0.09435964450730305, -0.19761811980095348, 0.07065580633199332, 0.34032590347342195, -0.3483002056318678, -0.2842471640973695, 0.14111784552806056, -0.2737530018276486, -0.13198531400374028, 0.1912242543442469, -0.09783042801151934,... |
706.2747 | Cosmic strings and Natural Inflation | In the present work we discuss cosmic strings in natural inflation. Our
analysis is based entirely on the CMB quadrupole temperature anisotropy and on
the existing upper bound on the cosmic string tension. Our results show that
the allowed range for both parameters of the inflationary model is very
different from the... | hep-ph | in the present work we discuss cosmic strings in natural inflation our analysis is based entirely on the cmb quadrupole temperature anisotropy and on the existing upper bound on the cosmic string tension our results show that the allowed range for both parameters of the inflationary model is very different from the ran... | [['in', 'the', 'present', 'work', 'we', 'discuss', 'cosmic', 'strings', 'in', 'natural', 'inflation', 'our', 'analysis', 'is', 'based', 'entirely', 'on', 'the', 'cmb', 'quadrupole', 'temperature', 'anisotropy', 'and', 'on', 'the', 'existing', 'upper', 'bound', 'on', 'the', 'cosmic', 'string', 'tension', 'our', 'results... | [-0.11410924021070928, 0.1996225745396249, -0.0851110868009456, 0.09432872846523781, -0.04364439945542411, -0.07618043089306421, -0.024779367849251693, 0.3373795948357562, -0.2224045922780891, -0.33583710480774387, 0.0743602272358545, -0.264388251013719, -0.08706861123275221, 0.23711353826095885, 0.018697655058643792, ... |
706.2748 | A Survey of Unix Init Schemes | In most modern operating systems, init (as in "initialization") is the
program launched by the kernel at boot time. It runs as a daemon and typically
has PID 1. Init is responsible for spawning all other processes and scavenging
zombies. It is also responsible for reboot and shutdown operations. This
document describ... | cs.OS | in most modern operating systems init as in initialization is the program launched by the kernel at boot time it runs as a daemon and typically has pid 1 init is responsible for spawning all other processes and scavenging zombies it is also responsible for reboot and shutdown operations this document describes existing... | [['in', 'most', 'modern', 'operating', 'systems', 'init', 'as', 'in', 'initialization', 'is', 'the', 'program', 'launched', 'by', 'the', 'kernel', 'at', 'boot', 'time', 'it', 'runs', 'as', 'a', 'daemon', 'and', 'typically', 'has', 'pid', '1', 'init', 'is', 'responsible', 'for', 'spawning', 'all', 'other', 'processes', ... | [-0.09784628198482097, 0.04757357200607657, -0.07057596056445618, 0.04848657814445687, -0.05759301962563768, -0.19481388258282095, 0.03035021131625399, 0.369397231945768, -0.24555526313954032, -0.3190199687005952, 0.19383573309634813, -0.30128773871809245, -0.09727112577995285, 0.26003304874524474, -0.05406269747763872... |
706.2749 | Black holes thermodynamics to all orders in the Planck length in extra
dimensions | We investigate the effects to all orders in the Planck length, from a
generalized uncertainty principle, on the thermodynamic parameters of radiating
Schwarzschild black holes in a scenario with large extra dimesions. We show
that black holes in this framework are hotter, decay faster and are less
classical objects. ... | gr-qc | we investigate the effects to all orders in the planck length from a generalized uncertainty principle on the thermodynamic parameters of radiating schwarzschild black holes in a scenario with large extra dimesions we show that black holes in this framework are hotter decay faster and are less classical objects particu... | [['we', 'investigate', 'the', 'effects', 'to', 'all', 'orders', 'in', 'the', 'planck', 'length', 'from', 'a', 'generalized', 'uncertainty', 'principle', 'on', 'the', 'thermodynamic', 'parameters', 'of', 'radiating', 'schwarzschild', 'black', 'holes', 'in', 'a', 'scenario', 'with', 'large', 'extra', 'dimesions', 'we', '... | [-0.10582685293447153, 0.17123611991101986, -0.075225435772582, 0.12967609473816635, -0.058729925827470185, -0.10314503883230774, 0.04752837452927933, 0.3081774058039574, -0.21511153330770777, -0.27160699320409226, 0.08478597446810454, -0.3466249117673393, -0.05670315650173043, 0.22102729838304952, -0.04677588356814036... |
706.275 | Absorption Lengths in the Holographic Plasma | We consider the effect of a periodic perturbation with frequency $\omega$ on
the holographic N=4 plasma represented by the planar AdS black hole. The
response of the system is given by exponentially decaying waves. The
corresponding complex wave numbers can be found by solving wave equations in
the AdS black hole bac... | hep-th | we consider the effect of a periodic perturbation with frequency omega on the holographic n4 plasma represented by the planar ads black hole the response of the system is given by exponentially decaying waves the corresponding complex wave numbers can be found by solving wave equations in the ads black hole background ... | [['we', 'consider', 'the', 'effect', 'of', 'a', 'periodic', 'perturbation', 'with', 'frequency', 'omega', 'on', 'the', 'holographic', 'n4', 'plasma', 'represented', 'by', 'the', 'planar', 'ads', 'black', 'hole', 'the', 'response', 'of', 'the', 'system', 'is', 'given', 'by', 'exponentially', 'decaying', 'waves', 'the', ... | [-0.16774489975068718, 0.17251195954648554, -0.08544264696664303, 0.07418616962496417, -0.08516355790669804, -0.08194519866673225, -0.02595859860003976, 0.31149920290084304, -0.20485634386627558, -0.21531512612804166, 0.08565160351610905, -0.30785308510216103, -0.12572018864463913, 0.1685653556495389, 0.026944732479121... |
706.2751 | From Feynman Proof of Maxwell Equations to Noncommutative Quantum
Mechanics | In 1990, Dyson published a proof due to Feynman of the Maxwell equations
assuming only the commutation relations between position and velocity. With
this minimal assumption, Feynman never supposed the existence of Hamiltonian or
Lagrangian formalism. In the present communication, we review the study of a
relativistic... | hep-th | in 1990 dyson published a proof due to feynman of the maxwell equations assuming only the commutation relations between position and velocity with this minimal assumption feynman never supposed the existence of hamiltonian or lagrangian formalism in the present communication we review the study of a relativistic partic... | [['in', '1990', 'dyson', 'published', 'a', 'proof', 'due', 'to', 'feynman', 'of', 'the', 'maxwell', 'equations', 'assuming', 'only', 'the', 'commutation', 'relations', 'between', 'position', 'and', 'velocity', 'with', 'this', 'minimal', 'assumption', 'feynman', 'never', 'supposed', 'the', 'existence', 'of', 'hamiltonia... | [-0.18050784776860382, 0.1889655561136351, -0.1168238773709163, 0.08472111006703927, -0.14126887619495393, -0.07135903615271673, 0.012032052964786998, 0.3245796595379943, -0.27241566314478405, -0.28796973162097855, 0.004050462626037188, -0.23161123719182797, -0.21194099280546652, 0.17009649746469221, -0.053255365078803... |
706.2752 | Film transitions of receding contact lines | When a solid plate is withdrawn from a liquid bath, a receding contact line
is formed where solid, liquid, and gas meet. Above a critical speed $U_{cr}$, a
stationary contact line can no longer exist and the solid will eventually be
covered completely by a liquid film. Here we show that the bifurcation diagram
of thi... | physics.flu-dyn | when a solid plate is withdrawn from a liquid bath a receding contact line is formed where solid liquid and gas meet above a critical speed u_cr a stationary contact line can no longer exist and the solid will eventually be covered completely by a liquid film here we show that the bifurcation diagram of this coating tr... | [['when', 'a', 'solid', 'plate', 'is', 'withdrawn', 'from', 'a', 'liquid', 'bath', 'a', 'receding', 'contact', 'line', 'is', 'formed', 'where', 'solid', 'liquid', 'and', 'gas', 'meet', 'above', 'a', 'critical', 'speed', 'u_cr', 'a', 'stationary', 'contact', 'line', 'can', 'no', 'longer', 'exist', 'and', 'the', 'solid',... | [-0.15668784593272364, 0.26776011425963775, -0.09943595799921574, -0.03309003750993205, -0.06186973513341604, -0.17532049349689743, 0.07701239568818057, 0.3562927671461081, -0.2891282487318528, -0.24000827691693583, 0.12773292782545395, -0.2866800875992191, -0.12415612327429104, 0.15918192103010964, -0.0506623666971085... |
706.2753 | Implications of right-handed neutrinos with electroweak-scale masses | The possibility of constructing a model in which right-handed neutrinos have
electroweak-scale masses as well as being {\em non-sterile} was espoused in
Ref. 1. In this talk, I will review the ideas and results of Ref. 1 and discuss
its implications for colliders such as the Tevatron, LHC and ILC.
| hep-ph | the possibility of constructing a model in which righthanded neutrinos have electroweakscale masses as well as being em nonsterile was espoused in ref 1 in this talk i will review the ideas and results of ref 1 and discuss its implications for colliders such as the tevatron lhc and ilc | [['the', 'possibility', 'of', 'constructing', 'a', 'model', 'in', 'which', 'righthanded', 'neutrinos', 'have', 'electroweakscale', 'masses', 'as', 'well', 'as', 'being', 'em', 'nonsterile', 'was', 'espoused', 'in', 'ref', '1', 'in', 'this', 'talk', 'i', 'will', 'review', 'the', 'ideas', 'and', 'results', 'of', 'ref', '... | [-0.013911714889109134, 0.23121869548223914, -0.02397238447330892, 0.13960336978314444, -0.07854318778961897, -0.16339889902621507, -0.030093192495405673, 0.3284370893239975, -0.16781152628362178, -0.308326100371778, 0.11203377586090937, -0.31520400566980245, -0.07499316822737455, 0.1565355734108016, 0.0194236067216843... |
706.2754 | Detecting mode entanglement: The role of coherent states, superselection
rules and particle statistics | We discuss the possibility of observing quantum nonlocality using the
so-called mode entanglement, analyzing the differences between different types
of particles in this context. We first discuss the role of coherent states in
such experiments, and we comment on the existence of coherent states in nature.
The discuss... | quant-ph | we discuss the possibility of observing quantum nonlocality using the socalled mode entanglement analyzing the differences between different types of particles in this context we first discuss the role of coherent states in such experiments and we comment on the existence of coherent states in nature the discussion of ... | [['we', 'discuss', 'the', 'possibility', 'of', 'observing', 'quantum', 'nonlocality', 'using', 'the', 'socalled', 'mode', 'entanglement', 'analyzing', 'the', 'differences', 'between', 'different', 'types', 'of', 'particles', 'in', 'this', 'context', 'we', 'first', 'discuss', 'the', 'role', 'of', 'coherent', 'states', '... | [-0.15355719849954244, 0.22658267482092567, -0.07147366851811705, 0.10777390310525578, -0.03722065333977001, -0.09301009282372356, 0.08952293481245588, 0.28609163266929244, -0.2613041298684597, -0.288695017594138, 0.05178750631645979, -0.249035395636205, -0.11403866169755073, 0.17807086577389414, -0.037134019420573525,... |
706.2755 | On certain bounds for first-crossing-time probabilities of a
jump-diffusion process | We consider the first-crossing-time problem through a constant boundary for a
Wiener process perturbed by random jumps driven by a counting process. On the
base of a sample-path analysis of the jump-diffusion process we obtain explicit
lower bounds for the first-crossing-time density and for the
first-crossing-time d... | math.PR | we consider the firstcrossingtime problem through a constant boundary for a wiener process perturbed by random jumps driven by a counting process on the base of a samplepath analysis of the jumpdiffusion process we obtain explicit lower bounds for the firstcrossingtime density and for the firstcrossingtime distribution... | [['we', 'consider', 'the', 'firstcrossingtime', 'problem', 'through', 'a', 'constant', 'boundary', 'for', 'a', 'wiener', 'process', 'perturbed', 'by', 'random', 'jumps', 'driven', 'by', 'a', 'counting', 'process', 'on', 'the', 'base', 'of', 'a', 'samplepath', 'analysis', 'of', 'the', 'jumpdiffusion', 'process', 'we', '... | [-0.09878030167670832, 0.10299477617012426, -0.06647742774137962, 0.08980109342528089, -0.045044094878470615, -0.08247586208329137, 0.11497869147431283, 0.31595166506511824, -0.27112994333063917, -0.24124023877084255, 0.14900143673349658, -0.2431886827412416, -0.14959503645964323, 0.19979950446369393, -0.03208123261685... |
706.2756 | Electronic properties of graphene with a topological defect | Various types of topological defects in graphene are considered in the
framework of the continuum model for long-wavelength electronic excitations,
which is based on the Dirac--Weyl equation. The condition for the electronic
wave function is specified, and we show that a topological defect can be
presented as a pseud... | cond-mat.str-el cond-mat.mtrl-sci hep-th math-ph math.MP | various types of topological defects in graphene are considered in the framework of the continuum model for longwavelength electronic excitations which is based on the diracweyl equation the condition for the electronic wave function is specified and we show that a topological defect can be presented as a pseudomagneti... | [['various', 'types', 'of', 'topological', 'defects', 'in', 'graphene', 'are', 'considered', 'in', 'the', 'framework', 'of', 'the', 'continuum', 'model', 'for', 'longwavelength', 'electronic', 'excitations', 'which', 'is', 'based', 'on', 'the', 'diracweyl', 'equation', 'the', 'condition', 'for', 'the', 'electronic', 'w... | [-0.16643138021767676, 0.1620945892137316, -0.02548526868912148, 0.049268176128378825, 0.010590714289227853, -0.08956239049046023, 0.027531080845709856, 0.3671270735427603, -0.24672092156283357, -0.2958238642192907, 0.08017880712249861, -0.3075270876288414, -0.13719023866495034, 0.16326769922759282, 0.02190017508057592... |
706.2757 | Controlled dynamics of qubits in the presence of decoherence | An exactly solvable model for the decoherence of one and two-qubit states
interacting with a spin-bath, in the presence of a time-dependent magnetic
field is studied. The magnetic field is static along $\hat{z}$ direction and
oscillatory in the transverse plane. The transition probability and Rabi
oscillations betwee... | quant-ph cond-mat.mes-hall | an exactly solvable model for the decoherence of one and twoqubit states interacting with a spinbath in the presence of a timedependent magnetic field is studied the magnetic field is static along hatz direction and oscillatory in the transverse plane the transition probability and rabi oscillations between the spinsta... | [['an', 'exactly', 'solvable', 'model', 'for', 'the', 'decoherence', 'of', 'one', 'and', 'twoqubit', 'states', 'interacting', 'with', 'a', 'spinbath', 'in', 'the', 'presence', 'of', 'a', 'timedependent', 'magnetic', 'field', 'is', 'studied', 'the', 'magnetic', 'field', 'is', 'static', 'along', 'hatz', 'direction', 'and... | [-0.17984732284925745, 0.28065978920141266, -0.02144877788211618, 0.04138213246977622, 0.04303602653256219, -0.1849513975271423, -0.0027146513972963605, 0.38946892957070045, -0.22813601449930243, -0.25097817070782186, 0.030079910184888703, -0.2675125205490206, -0.013864962520476963, 0.21140160356881096, 0.0464848263222... |
706.2758 | Scaled entropy of filtrations of $\sigma$-fields | We study the notion of the scaled entropy of a filtration of $\sigma$-fields
(= decreasing sequence of $\sigma$-fields) introduced by the first author
({V4}). We suggest a method for computing this entropy for the sequence of
$\sigma$-fields of pasts of a Markov process determined by a random walk over
the trajectori... | math.PR math.DS | we study the notion of the scaled entropy of a filtration of sigmafields decreasing sequence of sigmafields introduced by the first author v4 we suggest a method for computing this entropy for the sequence of sigmafields of pasts of a markov process determined by a random walk over the trajectories of a bernoulli actio... | [['we', 'study', 'the', 'notion', 'of', 'the', 'scaled', 'entropy', 'of', 'a', 'filtration', 'of', 'sigmafields', 'decreasing', 'sequence', 'of', 'sigmafields', 'introduced', 'by', 'the', 'first', 'author', 'v4', 'we', 'suggest', 'a', 'method', 'for', 'computing', 'this', 'entropy', 'for', 'the', 'sequence', 'of', 'sig... | [-0.16127680889796467, 0.17209750082654257, -0.13354431415597598, 0.04559741414041734, 0.006443580420066913, -0.11500956592770914, 0.06333728175998354, 0.3281021691237887, -0.3168412111513317, -0.18656558771928153, 0.09163210664487755, -0.2593811847517888, -0.12891379250058282, 0.163531983186258, -0.12902582057441275, ... |
706.2759 | Molecular gas in nearby low-luminosity QSO host galaxies | This paper addresses the global molecular gas properties of a representative
sample of galaxies hosting low-luminosity quasistellar objects. An abundant
supply of gas is necessary to fuel both the active galactic nucleus and any
circum-nuclear starburst activity of QSOs.
We selected a sample of nearby low-luminosit... | astro-ph | this paper addresses the global molecular gas properties of a representative sample of galaxies hosting lowluminosity quasistellar objects an abundant supply of gas is necessary to fuel both the active galactic nucleus and any circumnuclear starburst activity of qsos we selected a sample of nearby lowluminosity qso hos... | [['this', 'paper', 'addresses', 'the', 'global', 'molecular', 'gas', 'properties', 'of', 'a', 'representative', 'sample', 'of', 'galaxies', 'hosting', 'lowluminosity', 'quasistellar', 'objects', 'an', 'abundant', 'supply', 'of', 'gas', 'is', 'necessary', 'to', 'fuel', 'both', 'the', 'active', 'galactic', 'nucleus', 'an... | [-0.05182819229005518, 0.07757051790655117, -0.036287259830378865, 0.10121903262051088, -0.08178975333620506, -0.058367374057630934, 0.04555836037066896, 0.46490681186915905, -0.09197329935135252, -0.3360572153305912, 0.028384706558076192, -0.3440614659301787, 0.027981182728635978, 0.15843396880753638, -0.0168888338339... |
706.276 | Dynamics and thermalization of the nuclear spin bath in the
single-molecule magnet Mn12-ac: test for the theory of spin tunneling | The description of the tunneling of a macroscopic variable in the presence of
a bath of localized spins is a subject of great fundamental and practical
interest, and is relevant for many solid-state qubit designs. Instead of
focusing on the the "central spin" (as is most often done), here we present a
detailed study ... | cond-mat.mes-hall cond-mat.mtrl-sci | the description of the tunneling of a macroscopic variable in the presence of a bath of localized spins is a subject of great fundamental and practical interest and is relevant for many solidstate qubit designs instead of focusing on the the central spin as is most often done here we present a detailed study of the dyn... | [['the', 'description', 'of', 'the', 'tunneling', 'of', 'a', 'macroscopic', 'variable', 'in', 'the', 'presence', 'of', 'a', 'bath', 'of', 'localized', 'spins', 'is', 'a', 'subject', 'of', 'great', 'fundamental', 'and', 'practical', 'interest', 'and', 'is', 'relevant', 'for', 'many', 'solidstate', 'qubit', 'designs', 'i... | [-0.12374250512253844, 0.2559833544868765, -0.050567486325173445, 0.03967239201323674, 0.02680390494313302, -0.12440078218449961, 0.04492378262890819, 0.3727404368233006, -0.2447604036125583, -0.2681158627107748, 0.03204679847079909, -0.2921050396589738, -0.05225899724535785, 0.19478878227396393, 0.04595896642883572, -... |
706.2761 | Spin current and rectification in Luttinger liquids | We demonstrate that spin current can be generated by an ac voltage in a
one-channel quantum wire with strong repulsive electron interactions in the
presence of a non-magnetic impurity and uniform static magnetic field. In a
certain range of voltages, the spin current can exhibit a power dependence on
the ac voltage b... | cond-mat.mes-hall cond-mat.str-el | we demonstrate that spin current can be generated by an ac voltage in a onechannel quantum wire with strong repulsive electron interactions in the presence of a nonmagnetic impurity and uniform static magnetic field in a certain range of voltages the spin current can exhibit a power dependence on the ac voltage bias wi... | [['we', 'demonstrate', 'that', 'spin', 'current', 'can', 'be', 'generated', 'by', 'an', 'ac', 'voltage', 'in', 'a', 'onechannel', 'quantum', 'wire', 'with', 'strong', 'repulsive', 'electron', 'interactions', 'in', 'the', 'presence', 'of', 'a', 'nonmagnetic', 'impurity', 'and', 'uniform', 'static', 'magnetic', 'field', ... | [-0.21958434408103736, 0.24239530688540376, 0.05811077426854657, 0.03170370444422588, -0.026476738201381522, -0.16021519980373947, 0.03989702611337028, 0.3543506016721949, -0.2538751946024907, -0.31728721127001336, -0.005481048629008001, -0.2861277076008264, -0.019942705643188674, 0.24396333921686164, 0.022477974348779... |
706.2762 | Contact mechanics: relation between interfacial separation and load | I study the contact between a rigid solid with a randomly rough surface and
an elastic block with a flat surface. I derive a relation between the (average)
interfacial separation $u$ and the applied normal squeezing pressure $p$. I
show that for non-adhesive inte raction and small applied pressure, p is
proportional ... | cond-mat.soft | i study the contact between a rigid solid with a randomly rough surface and an elastic block with a flat surface i derive a relation between the average interfacial separation u and the applied normal squeezing pressure p i show that for nonadhesive inte raction and small applied pressure p is proportional to exp uu_0 ... | [['i', 'study', 'the', 'contact', 'between', 'a', 'rigid', 'solid', 'with', 'a', 'randomly', 'rough', 'surface', 'and', 'an', 'elastic', 'block', 'with', 'a', 'flat', 'surface', 'i', 'derive', 'a', 'relation', 'between', 'the', 'average', 'interfacial', 'separation', 'u', 'and', 'the', 'applied', 'normal', 'squeezing',... | [-0.1467062412505789, 0.15570332181490695, -0.09311478394797192, -0.013293151163511098, -0.011983412126409672, -0.19553995489953988, 0.04666837342759414, 0.3770852104550408, -0.2931040612522573, -0.26983444664379463, -0.0094745502255166, -0.30056390695033536, -0.13107051724387753, 0.15617395007997872, -0.05507761035715... |
706.2763 | Electronic instabilities of a Hubbard model approached as a large array
of coupled chains: competition between d-wave superconductivity and pseudogap
phase | We study the electronic instabilities in a 2D Hubbard model where one of the
dimensions has a finite width, so that it can be considered as a large array of
coupled chains. The finite transverse size of the system gives rise to a
discrete string of Fermi points, with respective electron fields that, due to
their mutu... | cond-mat.str-el | we study the electronic instabilities in a 2d hubbard model where one of the dimensions has a finite width so that it can be considered as a large array of coupled chains the finite transverse size of the system gives rise to a discrete string of fermi points with respective electron fields that due to their mutual int... | [['we', 'study', 'the', 'electronic', 'instabilities', 'in', 'a', '2d', 'hubbard', 'model', 'where', 'one', 'of', 'the', 'dimensions', 'has', 'a', 'finite', 'width', 'so', 'that', 'it', 'can', 'be', 'considered', 'as', 'a', 'large', 'array', 'of', 'coupled', 'chains', 'the', 'finite', 'transverse', 'size', 'of', 'the',... | [-0.1717259003440279, 0.18915731823090243, -0.10183948885006168, 0.07169545098509743, -0.019044383091248365, -0.14754028264856475, 0.08592555246485228, 0.29452441417586367, -0.2637692357085851, -0.2426970297978683, 0.034225857695619845, -0.3520710138362932, -0.11242133252260095, 0.16355906257391153, 0.04734419766017792... |
706.2764 | Self-consistent calculations within the Extended Theory of Finite Fermi
Systems | The Extended Theory of Finite Fermi Systems(ETFFS) describes nuclear
excitations considering phonons and pairing degrees of freedom, using
experimental single particle energies and the effective Landau-Migdal
interaction. Here we use the Skyrme interactions in order to extend the range
of applicability of the ETFFS t... | nucl-th | the extended theory of finite fermi systemsetffs describes nuclear excitations considering phonons and pairing degrees of freedom using experimental single particle energies and the effective landaumigdal interaction here we use the skyrme interactions in order to extend the range of applicability of the etffs to exper... | [['the', 'extended', 'theory', 'of', 'finite', 'fermi', 'systemsetffs', 'describes', 'nuclear', 'excitations', 'considering', 'phonons', 'and', 'pairing', 'degrees', 'of', 'freedom', 'using', 'experimental', 'single', 'particle', 'energies', 'and', 'the', 'effective', 'landaumigdal', 'interaction', 'here', 'we', 'use',... | [-0.09444212006132628, 0.2033128559167655, -0.09229982447017529, 0.14956652221186437, -0.02667015838384066, -0.08756465137549588, 0.042198871948782635, 0.3484719982019292, -0.21286948490009275, -0.2987162105229525, -0.048909488748012216, -0.31133605551220617, -0.05561106518891976, 0.10427513689281559, 0.072394802634832... |
706.2765 | Detecting entanglement of random states with an entanglement witness | The entanglement content of high-dimensional random pure states is almost
maximal, nevertheless, we show that, due to the complexity of such states, the
detection of their entanglement using witness operators is rather difficult. We
discuss the case of unknown random states, and the case of known random states
for wh... | quant-ph nlin.CD | the entanglement content of highdimensional random pure states is almost maximal nevertheless we show that due to the complexity of such states the detection of their entanglement using witness operators is rather difficult we discuss the case of unknown random states and the case of known random states for which we ca... | [['the', 'entanglement', 'content', 'of', 'highdimensional', 'random', 'pure', 'states', 'is', 'almost', 'maximal', 'nevertheless', 'we', 'show', 'that', 'due', 'to', 'the', 'complexity', 'of', 'such', 'states', 'the', 'detection', 'of', 'their', 'entanglement', 'using', 'witness', 'operators', 'is', 'rather', 'difficu... | [-0.11937728790821982, 0.2353201987194445, -0.10499418004388537, 0.09062958266996943, 0.03664982561524227, -0.15502317723197243, 0.060434530629529894, 0.33737040051788675, -0.261493376410548, -0.2554504482449927, 0.07100275478453613, -0.23970460120186793, -0.15588910181951873, 0.13391313998156465, -0.0710941890720278, ... |
706.2766 | Notes on a SQCD-like plasma dual and holographic renormalization | We study the thermodynamics and the jet quenching parameter of a black hole
solution dual to a SQCD-like plasma which includes the backreaction of
fundamental flavors. The free energy is calculated in several ways, including
some recently proposed holographic renormalization prescriptions. The validity
of the latter ... | hep-th | we study the thermodynamics and the jet quenching parameter of a black hole solution dual to a sqcdlike plasma which includes the backreaction of fundamental flavors the free energy is calculated in several ways including some recently proposed holographic renormalization prescriptions the validity of the latter is con... | [['we', 'study', 'the', 'thermodynamics', 'and', 'the', 'jet', 'quenching', 'parameter', 'of', 'a', 'black', 'hole', 'solution', 'dual', 'to', 'a', 'sqcdlike', 'plasma', 'which', 'includes', 'the', 'backreaction', 'of', 'fundamental', 'flavors', 'the', 'free', 'energy', 'is', 'calculated', 'in', 'several', 'ways', 'inc... | [-0.11433945486941463, 0.14895522094648528, -0.12189366455181097, 0.10433192778695023, -0.051115246140398085, -0.09409989104694072, 0.01952639253225775, 0.3220849559677519, -0.17827277150848564, -0.28413089716209555, 0.07643233873015973, -0.30002680651070374, -0.06087240156770315, 0.17480793412344284, -0.01764848028125... |
706.2767 | Unruh's detector in the presence of Lorentz symmetry breaking | We investigate the quantum field theory of a Lorentz non-invariant model with
a massive nonlinear dispersion relation in Minkowski space. The model involves
some non-causal signals in the form of wave packets propagating with
super-luminal group velocities. To avoid the problems with causality we
characterize the cau... | hep-th | we investigate the quantum field theory of a lorentz noninvariant model with a massive nonlinear dispersion relation in minkowski space the model involves some noncausal signals in the form of wave packets propagating with superluminal group velocities to avoid the problems with causality we characterize the causal sec... | [['we', 'investigate', 'the', 'quantum', 'field', 'theory', 'of', 'a', 'lorentz', 'noninvariant', 'model', 'with', 'a', 'massive', 'nonlinear', 'dispersion', 'relation', 'in', 'minkowski', 'space', 'the', 'model', 'involves', 'some', 'noncausal', 'signals', 'in', 'the', 'form', 'of', 'wave', 'packets', 'propagating', '... | [-0.20038174703823525, 0.1991950389049674, -0.10300674796985139, 0.07894495950161438, -0.153001977968961, -0.1454836046728103, 0.023380214632261018, 0.3168632526031655, -0.2178688255381649, -0.26275015050879397, 0.03293474935926497, -0.2619932699219688, -0.10981641772162655, 0.12035486325621605, -0.040202439944867205, ... |
706.2768 | Towards a Holistic View of the Heating and Cooling of the Intracluster
Medium | (Abridged) X-ray clusters are conventionally divided into two classes: "cool
core" (CC) clusters and "non-cool core" (NCC) clusters. Yet relatively little
attention has been given to the origins of this dichotomy and, in particular,
to the energetics and thermal histories of the two classes. We develop a model
for th... | astro-ph | abridged xray clusters are conventionally divided into two classes cool core cc clusters and noncool core ncc clusters yet relatively little attention has been given to the origins of this dichotomy and in particular to the energetics and thermal histories of the two classes we develop a model for the entropy profiles ... | [['abridged', 'xray', 'clusters', 'are', 'conventionally', 'divided', 'into', 'two', 'classes', 'cool', 'core', 'cc', 'clusters', 'and', 'noncool', 'core', 'ncc', 'clusters', 'yet', 'relatively', 'little', 'attention', 'has', 'been', 'given', 'to', 'the', 'origins', 'of', 'this', 'dichotomy', 'and', 'in', 'particular',... | [-0.0688039232130594, 0.15704271382879612, -0.06403259385937476, 0.11190640253072508, -0.06900155895609196, -0.0945258776778431, 0.05823992236188, 0.4085794278132782, -0.24619006572293148, -0.35822301737470097, 0.07645628902383482, -0.2672785229231345, -0.020206860626282973, 0.19524578787518923, -0.012311871693568016, ... |
706.2769 | Spin gap and string order parameter in the ferromagnetic Spiral
Staircase Heisenberg Ladder: a quantum Monte Carlo study | We consider a spin-1/2 ladder with a ferromagnetic rung coupling J_\perp and
inequivalent chains. This model is obtained by a twist (\theta) deformation of
the ladder and interpolates between the isotropic ladder (\theta=0) and the
SU(2) ferromagnetic Kondo necklace model (\theta=\pi). We show that the ground
state i... | cond-mat.str-el | we consider a spin12 ladder with a ferromagnetic rung coupling j_perp and inequivalent chains this model is obtained by a twist theta deformation of the ladder and interpolates between the isotropic ladder theta0 and the su2 ferromagnetic kondo necklace model thetapi we show that the ground state in the thetaj_perp pla... | [['we', 'consider', 'a', 'spin12', 'ladder', 'with', 'a', 'ferromagnetic', 'rung', 'coupling', 'j_perp', 'and', 'inequivalent', 'chains', 'this', 'model', 'is', 'obtained', 'by', 'a', 'twist', 'theta', 'deformation', 'of', 'the', 'ladder', 'and', 'interpolates', 'between', 'the', 'isotropic', 'ladder', 'theta0', 'and',... | [-0.23493144015523315, 0.2580005216594206, -0.03273284317095991, 0.07539401974278588, -0.03803148294384239, -0.16178952947556346, 0.04492721561060733, 0.36501977581162975, -0.27069432833114593, -0.24511251271264078, 0.013251764808405786, -0.30489611545843737, -0.09374238406660176, 0.14261714277687257, 0.106607704049298... |
706.277 | Inter-individual variability in sensory weighting of a plantar
pressure-based, tongue-placed tactile biofeedback for controlling posture | The purpose of the present experiment was to investigate whether the sensory
weighting of a plantar pressure-based, tongue-placed tactile biofeedback for
controlling posture could be subject to inter-individual variability. To
achieve this goal, 60 young healthy adults were asked to stand as immobile as
possible with... | physics.med-ph q-bio.NC | the purpose of the present experiment was to investigate whether the sensory weighting of a plantar pressurebased tongueplaced tactile biofeedback for controlling posture could be subject to interindividual variability to achieve this goal 60 young healthy adults were asked to stand as immobile as possible with their e... | [['the', 'purpose', 'of', 'the', 'present', 'experiment', 'was', 'to', 'investigate', 'whether', 'the', 'sensory', 'weighting', 'of', 'a', 'plantar', 'pressurebased', 'tongueplaced', 'tactile', 'biofeedback', 'for', 'controlling', 'posture', 'could', 'be', 'subject', 'to', 'interindividual', 'variability', 'to', 'achie... | [-0.11429136370547936, 0.14706427250348497, -0.0715171395845865, 0.008120845748568722, -0.08833798181175878, -0.1578466636278248, 0.03681068755088186, 0.3786732873734121, -0.25229219524745206, -0.3504531835141771, 0.056796857271740775, -0.2592020983051577, -0.1656825541328519, 0.17908614166876635, -0.17727130527582463,... |
706.2771 | Status of art of reaction models for projectiles far from stability | This talk will review the status of art of nuclear and Coulomb breakup
theories and their relation to optical models of elastic scattering of exotic
projectiles. The effect of the final state interactions between the breakup
particle and the core and target nuclei will be clarified and some typical
numerical calculat... | nucl-th | this talk will review the status of art of nuclear and coulomb breakup theories and their relation to optical models of elastic scattering of exotic projectiles the effect of the final state interactions between the breakup particle and the core and target nuclei will be clarified and some typical numerical calculation... | [['this', 'talk', 'will', 'review', 'the', 'status', 'of', 'art', 'of', 'nuclear', 'and', 'coulomb', 'breakup', 'theories', 'and', 'their', 'relation', 'to', 'optical', 'models', 'of', 'elastic', 'scattering', 'of', 'exotic', 'projectiles', 'the', 'effect', 'of', 'the', 'final', 'state', 'interactions', 'between', 'the... | [-0.04429377258136149, 0.19055254332488403, -0.12229120221573711, 0.10637380798024507, -0.03651544315190139, -0.09805657387054949, 0.03352727469014512, 0.3388871217612177, -0.2393073536434465, -0.29575324803590775, 0.05655621009116823, -0.3286337703043087, -0.07002643758261745, 0.19180993290633938, 0.009500208816131239... |
706.2772 | Embedding Theorems and Boundary-value Problems for cusp domains | We study the Robin boundary-value problem for bounded domains with isolated
singularities. Because for such domains trace spaces of space $H^1(D)$ on its
boundaries are weighted Sobolev spaces $L^{2, \xi}(\partial D)$ existence and
uniqueness of corresponding Robin boundary-value problems depends on properties
of emb... | math.AP math.FA | we study the robin boundaryvalue problem for bounded domains with isolated singularities because for such domains trace spaces of space h1d on its boundaries are weighted sobolev spaces l2 xipartial d existence and uniqueness of corresponding robin boundaryvalue problems depends on properties of embedding operators i_1... | [['we', 'study', 'the', 'robin', 'boundaryvalue', 'problem', 'for', 'bounded', 'domains', 'with', 'isolated', 'singularities', 'because', 'for', 'such', 'domains', 'trace', 'spaces', 'of', 'space', 'h1d', 'on', 'its', 'boundaries', 'are', 'weighted', 'sobolev', 'spaces', 'l2', 'xipartial', 'd', 'existence', 'and', 'uni... | [-0.17036989339809308, 0.0037956420245550937, -0.04977601181565859, 0.09720575865545449, -0.13394022586851798, -0.14326035323948866, -0.02503051378646459, 0.33548938271043627, -0.2971942218866242, -0.20171647336890644, 0.18564196674945369, -0.3242316209985781, -0.0873239125210749, 0.19776540143608018, -0.11749972805953... |
706.2773 | Near-homeomorphisms of Nobeling manifolds | We characterize maps between $n$-dimensional N\"obeling manifolds that can be
approximated by homeomorphisms.
| math.GT math.GN | we characterize maps between ndimensional nobeling manifolds that can be approximated by homeomorphisms | [['we', 'characterize', 'maps', 'between', 'ndimensional', 'nobeling', 'manifolds', 'that', 'can', 'be', 'approximated', 'by', 'homeomorphisms']] | [-0.1563000872086447, 0.13750390944859156, -0.07251472384310685, 0.14414426311850548, 0.010267619043588638, -0.1750579040784102, -0.05757172892873104, 0.4703877820418431, -0.3445918015562571, -0.20492525584995747, 0.14259810799446243, -0.31036237720400095, -0.25555412456966364, 0.24882735598545808, -0.23674905242828223... |
706.2774 | Tunneling into low-dimensional and strongly correlated conductors | A general nonperturbative theory of the low-energy electron propagator is
developed and used to calculate the single-particle density of states in a
variety of systems. This method involves the decoupling of the
electron-electron interaction through a Hubbard-Stratonovich transformation,
followed by a saddle-point ap... | cond-mat.str-el cond-mat.mes-hall | a general nonperturbative theory of the lowenergy electron propagator is developed and used to calculate the singleparticle density of states in a variety of systems this method involves the decoupling of the electronelectron interaction through a hubbardstratonovich transformation followed by a saddlepoint approximati... | [['a', 'general', 'nonperturbative', 'theory', 'of', 'the', 'lowenergy', 'electron', 'propagator', 'is', 'developed', 'and', 'used', 'to', 'calculate', 'the', 'singleparticle', 'density', 'of', 'states', 'in', 'a', 'variety', 'of', 'systems', 'this', 'method', 'involves', 'the', 'decoupling', 'of', 'the', 'electronelec... | [-0.13050681229706118, 0.15801734452662106, -0.13897845002531142, 0.08214323394488365, 0.0025566742235959387, -0.1166973670146295, 0.05893266448500838, 0.3081560006070578, -0.2703678892089092, -0.28253345199714913, 0.029761571583629517, -0.2804988716494571, -0.1508017011037489, 0.1363002038434097, 0.00733372173905626, ... |
706.2775 | Spin alignment of dark matter haloes in the shells of the largest voids | Using the high resolution cosmological N-body simulation MareNostrum Universe
we study the orientation of shape and angular momentum of galaxy-size dark
matter haloes around large voids. We find that haloes located on the shells of
the largest cosmic voids have angular momenta that tend to be preferentially
perpendic... | astro-ph | using the high resolution cosmological nbody simulation marenostrum universe we study the orientation of shape and angular momentum of galaxysize dark matter haloes around large voids we find that haloes located on the shells of the largest cosmic voids have angular momenta that tend to be preferentially perpendicular ... | [['using', 'the', 'high', 'resolution', 'cosmological', 'nbody', 'simulation', 'marenostrum', 'universe', 'we', 'study', 'the', 'orientation', 'of', 'shape', 'and', 'angular', 'momentum', 'of', 'galaxysize', 'dark', 'matter', 'haloes', 'around', 'large', 'voids', 'we', 'find', 'that', 'haloes', 'located', 'on', 'the', ... | [-0.12286182848187402, 0.08716944011095433, -0.13409655899979556, 0.09716220930642568, -0.0938052402343601, 0.053473081615848995, -0.03704393992367654, 0.41138891694255364, -0.18032677849539772, -0.3682642152819496, -0.009661854708937403, -0.2744607816193587, -0.013120371619991671, 0.13599273808993018, 0.05210881926811... |
706.2776 | Tunneling spectroscopy of persistent currents in superconducting
microrings | It is shown that in a structure consisting of a superconducting ring-shaped
electrode overlapped by a normal metal contact through a thin oxide barrier,
measurements of the tunnel current in magnetic field can probe persistent
currents in the ring. The effect manifests itself as periodic oscillations of
the tunnel cu... | cond-mat.supr-con cond-mat.mes-hall | it is shown that in a structure consisting of a superconducting ringshaped electrode overlapped by a normal metal contact through a thin oxide barrier measurements of the tunnel current in magnetic field can probe persistent currents in the ring the effect manifests itself as periodic oscillations of the tunnel current... | [['it', 'is', 'shown', 'that', 'in', 'a', 'structure', 'consisting', 'of', 'a', 'superconducting', 'ringshaped', 'electrode', 'overlapped', 'by', 'a', 'normal', 'metal', 'contact', 'through', 'a', 'thin', 'oxide', 'barrier', 'measurements', 'of', 'the', 'tunnel', 'current', 'in', 'magnetic', 'field', 'can', 'probe', 'p... | [-0.22084664624505618, 0.21735185104469426, 0.0034952019400234465, 0.024692461173834068, -0.01034522533587687, -0.14366297871522793, 0.08900065116637351, 0.3438129544882929, -0.2569705160700162, -0.34071259900833234, 0.02167210202071745, -0.2773068492135764, -0.05771874459578267, 0.21929433615583502, 0.0124736968427896... |
706.2777 | The Ricci iteration and its applications | In this Note we introduce and study dynamical systems related to the Ricci
operator on the space of Kahler metrics as discretizations of certain geometric
flows. We pose a conjecture on their convergence towards canonical Kahler
metrics and study the case where the first Chern class is negative, zero or
positive. Thi... | math.DG | in this note we introduce and study dynamical systems related to the ricci operator on the space of kahler metrics as discretizations of certain geometric flows we pose a conjecture on their convergence towards canonical kahler metrics and study the case where the first chern class is negative zero or positive this con... | [['in', 'this', 'note', 'we', 'introduce', 'and', 'study', 'dynamical', 'systems', 'related', 'to', 'the', 'ricci', 'operator', 'on', 'the', 'space', 'of', 'kahler', 'metrics', 'as', 'discretizations', 'of', 'certain', 'geometric', 'flows', 'we', 'pose', 'a', 'conjecture', 'on', 'their', 'convergence', 'towards', 'cano... | [-0.18368281915783882, 0.03258659659128171, -0.06883510254323483, 0.08677758710303654, -0.10353750680262844, -0.15926814067022255, -0.02222800758977731, 0.3427642553548018, -0.2733628985037406, -0.22524663679301737, 0.1297722122631967, -0.255466592842713, -0.2135848036315292, 0.1864685258238266, -0.1678684342395718, 0.... |
706.2778 | Chains in the noncrossing partition lattice | We establish recursions counting various classes of chains in the noncrossing
partition lattice of a finite Coxeter group. The recursions specialize a
general relation which is proven uniformly (i.e. without appealing to the
classification of finite Coxeter groups) using basic facts about noncrossing
partitions. We s... | math.CO | we establish recursions counting various classes of chains in the noncrossing partition lattice of a finite coxeter group the recursions specialize a general relation which is proven uniformly ie without appealing to the classification of finite coxeter groups using basic facts about noncrossing partitions we solve the... | [['we', 'establish', 'recursions', 'counting', 'various', 'classes', 'of', 'chains', 'in', 'the', 'noncrossing', 'partition', 'lattice', 'of', 'a', 'finite', 'coxeter', 'group', 'the', 'recursions', 'specialize', 'a', 'general', 'relation', 'which', 'is', 'proven', 'uniformly', 'ie', 'without', 'appealing', 'to', 'the'... | [-0.1701697738551833, 0.13579636972026846, -0.07887388462906034, 0.0927265923508687, -0.14738141706900545, -0.1332790602712883, 0.11450186771458214, 0.3265329486536748, -0.2903876547674531, -0.24383789301370679, 0.03815954064303846, -0.25910099589455765, -0.0924740968525265, 0.17568064634733407, -0.08797849069950758, 0... |
706.2779 | Resistive state of quasi-one-dimensional superconductors: fluctuations
vs. sample inhomogeneity | The shape of experimentally observed R(T) transition of thin superconducting
wires is analyzed. Broadening of the transition in quasi-1-dimensional
superconducting channels is typically associated with phase slip mechanism
provided by thermal or quantum fluctuations. It is shown that consideration of
inevitable geome... | cond-mat.supr-con | the shape of experimentally observed rt transition of thin superconducting wires is analyzed broadening of the transition in quasi1dimensional superconducting channels is typically associated with phase slip mechanism provided by thermal or quantum fluctuations it is shown that consideration of inevitable geometrical i... | [['the', 'shape', 'of', 'experimentally', 'observed', 'rt', 'transition', 'of', 'thin', 'superconducting', 'wires', 'is', 'analyzed', 'broadening', 'of', 'the', 'transition', 'in', 'quasi1dimensional', 'superconducting', 'channels', 'is', 'typically', 'associated', 'with', 'phase', 'slip', 'mechanism', 'provided', 'by'... | [-0.17951495588148156, 0.19747604587841983, -0.05750824484441962, 0.008671769516665366, -0.017651953043641297, -0.15119614325218148, 0.012681667495948764, 0.3810997756382266, -0.21489771326573995, -0.26063006796495436, 0.045913193689577365, -0.2957500190148514, -0.12862462339063102, 0.23052024181707056, 0.0179385627302... |
706.278 | The chemical abundance of the very metal rich old Open Clusters NGC 6253
and NGC 6791 | In the framework of a project aiming at deriving in a homogeneous way the
properties (age, distance, reddening and detailed chemical abundances) of a
large sample of old open clusters, we present here the metal abundance and the
abundance ratios of light (C, N, O, Na, Mg, Al, Si, Ca, Ti) and heavier (Cr,
Mn, Ni, Ba, ... | astro-ph | in the framework of a project aiming at deriving in a homogeneous way the properties age distance reddening and detailed chemical abundances of a large sample of old open clusters we present here the metal abundance and the abundance ratios of light c n o na mg al si ca ti and heavier cr mn ni ba eu elements in the gal... | [['in', 'the', 'framework', 'of', 'a', 'project', 'aiming', 'at', 'deriving', 'in', 'a', 'homogeneous', 'way', 'the', 'properties', 'age', 'distance', 'reddening', 'and', 'detailed', 'chemical', 'abundances', 'of', 'a', 'large', 'sample', 'of', 'old', 'open', 'clusters', 'we', 'present', 'here', 'the', 'metal', 'abunda... | [-0.014940585577278398, 0.07129720579299222, -0.02148897195845873, 0.0535559395725108, -0.016633726832676783, -0.09302829733900984, 0.08666598497843046, 0.49662300741248244, -0.11680705908813455, -0.4012797131785596, -0.07025508598194898, -0.3224029506470995, 0.030658024949944875, 0.1667315322334212, -0.114474166989869... |
706.2781 | Degenerate Bose-Bose mixture in a three-dimensional optical lattice | We produce a heteronuclear quantum degenerate mixture of two bosonic species,
$^{87}$Rb and $^{41}$K, in a three-dimensional optical lattice. On raising the
lattice barriers, we observe the disapperance of the inference pattern of the
heavier $^{87}$Rb, shifting toward shallower lattice depths in the presence of
a mi... | cond-mat.other | we produce a heteronuclear quantum degenerate mixture of two bosonic species 87rb and 41k in a threedimensional optical lattice on raising the lattice barriers we observe the disapperance of the inference pattern of the heavier 87rb shifting toward shallower lattice depths in the presence of a minor fraction of 41k thi... | [['we', 'produce', 'a', 'heteronuclear', 'quantum', 'degenerate', 'mixture', 'of', 'two', 'bosonic', 'species', '87rb', 'and', '41k', 'in', 'a', 'threedimensional', 'optical', 'lattice', 'on', 'raising', 'the', 'lattice', 'barriers', 'we', 'observe', 'the', 'disapperance', 'of', 'the', 'inference', 'pattern', 'of', 'th... | [-0.11167856283260114, 0.22255863189565564, -0.017560995600746022, 0.03760112271728841, 0.006179083609069237, -0.14188177631509424, 0.11513842052469651, 0.38702116680867743, -0.19320363118642508, -0.2782820930346997, 0.007751041515306993, -0.2931403061375022, -0.09501785411725217, 0.14957248445863675, 0.019810910910518... |
706.2782 | Extremal subsets of {1,...,n} avoiding solutions to linear equations in
three variables | We refine previous results to provide examples, and in some cases precise
classifications, of extremal subsets of {1,...,n} containing no solutions to a
wide class of non-invariant, homogeneous linear equations in three variables,
i.e.: equations of the form ax+by=cz with a+b \neq c.
| math.NT math.CO | we refine previous results to provide examples and in some cases precise classifications of extremal subsets of 1n containing no solutions to a wide class of noninvariant homogeneous linear equations in three variables ie equations of the form axbycz with ab neq c | [['we', 'refine', 'previous', 'results', 'to', 'provide', 'examples', 'and', 'in', 'some', 'cases', 'precise', 'classifications', 'of', 'extremal', 'subsets', 'of', '1n', 'containing', 'no', 'solutions', 'to', 'a', 'wide', 'class', 'of', 'noninvariant', 'homogeneous', 'linear', 'equations', 'in', 'three', 'variables', ... | [-0.15630538174665945, 0.04460462487876675, -0.0028235634658918822, 0.01243482803016208, -0.09120340024792524, -0.1495313617010969, 0.03124283795613189, 0.33111735545965126, -0.21432615448395873, -0.24911881402827973, 0.08393195776138888, -0.3380845213785421, -0.10284823446188035, 0.20429288145414617, -0.04086991737131... |
706.2783 | Intracluster Short Gamma-Ray Bursts by Compact Binary Mergers | One of the possible origins of short gamma-ray bursts (SGRBs) is merging of
compact binaries, and the effect of large kick velocity is a signature that can
be used as an observational test for this hypothesis. Intracluster SGRBs that
escaped from a host galaxy in a galaxy cluster are interesting in this context,
sinc... | astro-ph | one of the possible origins of short gammaray bursts sgrbs is merging of compact binaries and the effect of large kick velocity is a signature that can be used as an observational test for this hypothesis intracluster sgrbs that escaped from a host galaxy in a galaxy cluster are interesting in this context since they w... | [['one', 'of', 'the', 'possible', 'origins', 'of', 'short', 'gammaray', 'bursts', 'sgrbs', 'is', 'merging', 'of', 'compact', 'binaries', 'and', 'the', 'effect', 'of', 'large', 'kick', 'velocity', 'is', 'a', 'signature', 'that', 'can', 'be', 'used', 'as', 'an', 'observational', 'test', 'for', 'this', 'hypothesis', 'intr... | [-0.08251483243536638, 0.16282131666829688, -0.1110783247518416, 0.2058160032665627, -0.1676692636237224, -0.03770565556198204, 0.025278720411187318, 0.3989437005912084, -0.14545723282396697, -0.336956218454427, 0.021431996758515738, -0.29739070797117106, -0.022745413656245165, 0.26039402461924394, -0.00218977268852795... |
706.2784 | BeppoSAX observation of 4U 1705-44: detection of hard X-ray emission in
the soft state | 4U 1705-44 is one of the best studied type I X-ray burster and atoll sources.
Since it covers a wide range in luminosity (from a few to 50 x 10^{36} erg
s^{-1}) and shows clear spectral state transitions, it represents a good
laboratory to test the accretion models proposed for atoll sources. We analysed
the energy s... | astro-ph | 4u 170544 is one of the best studied type i xray burster and atoll sources since it covers a wide range in luminosity from a few to 50 x 1036 erg s1 and shows clear spectral state transitions it represents a good laboratory to test the accretion models proposed for atoll sources we analysed the energy spectrum accumula... | [['4u', '170544', 'is', 'one', 'of', 'the', 'best', 'studied', 'type', 'i', 'xray', 'burster', 'and', 'atoll', 'sources', 'since', 'it', 'covers', 'a', 'wide', 'range', 'in', 'luminosity', 'from', 'a', 'few', 'to', '50', 'x', '1036', 'erg', 's1', 'and', 'shows', 'clear', 'spectral', 'state', 'transitions', 'it', 'repre... | [-0.05959670179825578, 0.13266051542894863, -0.05197753711427386, 0.10846741597319173, -0.04346345452642118, -0.12467506518335761, 0.062166516550791424, 0.4565484741652334, -0.1797399179014138, -0.38746015467756506, 0.07836942575255258, -0.34058235981375784, 0.06871893921917355, 0.19842416246396463, -0.0053433641578964... |
706.2785 | Metastable supergravity vacua with F and D supersymmetry breaking | We study the conditions under which a generic supergravity model involving
chiral and vector multiplets can admit viable metastable vacua with
spontaneously broken supersymmetry and realistic cosmological constant. To do
so, we impose that on the vacuum the scalar potential and all its first
derivatives vanish, and d... | hep-th | we study the conditions under which a generic supergravity model involving chiral and vector multiplets can admit viable metastable vacua with spontaneously broken supersymmetry and realistic cosmological constant to do so we impose that on the vacuum the scalar potential and all its first derivatives vanish and derive... | [['we', 'study', 'the', 'conditions', 'under', 'which', 'a', 'generic', 'supergravity', 'model', 'involving', 'chiral', 'and', 'vector', 'multiplets', 'can', 'admit', 'viable', 'metastable', 'vacua', 'with', 'spontaneously', 'broken', 'supersymmetry', 'and', 'realistic', 'cosmological', 'constant', 'to', 'do', 'so', 'w... | [-0.14861332393610613, 0.19248673698508784, -0.02240585514904754, 0.10310175932830039, -0.14017559541600053, -0.13274803846164257, 0.004140795181121896, 0.3314809440550862, -0.21843436256586257, -0.2815575564440289, 0.12975211732923916, -0.2154802726033856, -0.09802437781111856, 0.12627014533323722, -0.0130359460852568... |
706.2786 | Measurements of the CKM angle phi_3/gamma | We present a review on the measurements of the CKM angle gamma (phi_3) as
performed by the BABAR and Belle experiments at the asymmetric-energy e+e- B
factories colliders PEP-II and KEKB.
| hep-ex | we present a review on the measurements of the ckm angle gamma phi_3 as performed by the babar and belle experiments at the asymmetricenergy ee b factories colliders pepii and kekb | [['we', 'present', 'a', 'review', 'on', 'the', 'measurements', 'of', 'the', 'ckm', 'angle', 'gamma', 'phi_3', 'as', 'performed', 'by', 'the', 'babar', 'and', 'belle', 'experiments', 'at', 'the', 'asymmetricenergy', 'ee', 'b', 'factories', 'colliders', 'pepii', 'and', 'kekb']] | [-0.13250372099179414, 0.18226656350757806, -0.0743217968321856, -0.0004732675940519379, -0.12151073712495065, -0.20539489026451785, 0.1172327997929026, 0.29471029641647495, -0.109970394582037, -0.14498074448877765, -0.023899889956679073, -0.5602735765278339, 0.03672921609493994, 0.21819065793627693, 0.1742236906241986... |
706.2787 | Higher Dimensional Multiparameter Unitary and Nonunitary Braid Matrices:
Even Dimensions | A class of $(2n)^2\times(2n)^2$ multiparameter braid matrices are presented
for all $n$ $(n\geq 1)$. Apart from the spectral parameter $\theta$, they
depend on $2n^2$ free parameters $m_{ij}^{(\pm)}$, $i,j=1,...,n$. For real
parameters the matrices $R(\theta)$ are nonunitary. For purely imaginary
parameters they beca... | math.QA cond-mat.stat-mech hep-th | a class of 2n2times2n2 multiparameter braid matrices are presented for all n ngeq 1 apart from the spectral parameter theta they depend on 2n2 free parameters m_ijpm ij1n for real parameters the matrices rtheta are nonunitary for purely imaginary parameters they became unitary thus a unification is achieved with odd di... | [['a', 'class', 'of', '2n2times2n2', 'multiparameter', 'braid', 'matrices', 'are', 'presented', 'for', 'all', 'n', 'ngeq', '1', 'apart', 'from', 'the', 'spectral', 'parameter', 'theta', 'they', 'depend', 'on', '2n2', 'free', 'parameters', 'm_ijpm', 'ij1n', 'for', 'real', 'parameters', 'the', 'matrices', 'rtheta', 'are'... | [-0.1626326441413389, 0.23586354538236023, 0.0014849634893800852, 0.06304211485999162, -0.08288814049249268, -0.24869975755166895, -0.034341829802559794, 0.37515329337626135, -0.2375720594570322, -0.22973939129766427, 0.13864857740788106, -0.23041430632320214, -0.12839680199098405, 0.2560305406673337, -0.02776928065028... |
706.2788 | A Cosmic Watershed: the WVF Void Detection Technique | On megaparsec scales the Universe is permeated by an intricate filigree of
clusters, filaments, sheets and voids, the Cosmic Web. For the understanding of
its dynamical and hierarchical history it is crucial to identify objectively
its complex morphological components. One of the most characteristic aspects is
that o... | astro-ph | on megaparsec scales the universe is permeated by an intricate filigree of clusters filaments sheets and voids the cosmic web for the understanding of its dynamical and hierarchical history it is crucial to identify objectively its complex morphological components one of the most characteristic aspects is that of the d... | [['on', 'megaparsec', 'scales', 'the', 'universe', 'is', 'permeated', 'by', 'an', 'intricate', 'filigree', 'of', 'clusters', 'filaments', 'sheets', 'and', 'voids', 'the', 'cosmic', 'web', 'for', 'the', 'understanding', 'of', 'its', 'dynamical', 'and', 'hierarchical', 'history', 'it', 'is', 'crucial', 'to', 'identify', ... | [-0.06516508125544836, 0.05491692260716624, -0.13454019456976168, 0.11436709649481036, -0.08580521724855764, -0.012329732254979067, 0.021616733556295495, 0.37658895132601233, -0.25842421465241056, -0.3525709023196546, 0.0534915600289842, -0.233144642671548, -0.15850582981421746, 0.14675068217403595, -0.0223595660978129... |
706.2789 | Singular lagrangian systems and variational constrained mechanics on Lie
algebroids | The purpose of this paper is describe Lagrangian Mechanics for constrained
systems on Lie algebroids, a natural framework which covers a wide range of
situations (systems on Lie groups, quotients by the action of a Lie group,
standard tangent bundles...). In particular, we are interested in two cases:
singular Lagran... | math.DG math-ph math.MP | the purpose of this paper is describe lagrangian mechanics for constrained systems on lie algebroids a natural framework which covers a wide range of situations systems on lie groups quotients by the action of a lie group standard tangent bundles in particular we are interested in two cases singular lagrangian systems ... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'describe', 'lagrangian', 'mechanics', 'for', 'constrained', 'systems', 'on', 'lie', 'algebroids', 'a', 'natural', 'framework', 'which', 'covers', 'a', 'wide', 'range', 'of', 'situations', 'systems', 'on', 'lie', 'groups', 'quotients', 'by', 'the', 'action', 'of', 'a', '... | [-0.1796291147860197, 0.03630557744674241, -0.04731858116216384, 0.10427887886046217, -0.10760213345862352, -0.11949091564434079, -0.037085841594335554, 0.3515882582905201, -0.30654479105455373, -0.2534195688481514, 0.1297010187095461, -0.2131003179659064, -0.2281349203047844, 0.2404069839618527, -0.17375925408246426, ... |
706.279 | Filling inequalities do not depend on topology | Gromov's universal filling inequalities relate the filling radius and the
filling volume of a Riemannian manifold to its volume. The main result of the
present article is that in dimensions at least three the optimal constants in
the filling inequalities depend only on dimension and orientability, not on the
manifold... | math.GT math.DG | gromovs universal filling inequalities relate the filling radius and the filling volume of a riemannian manifold to its volume the main result of the present article is that in dimensions at least three the optimal constants in the filling inequalities depend only on dimension and orientability not on the manifold itse... | [['gromovs', 'universal', 'filling', 'inequalities', 'relate', 'the', 'filling', 'radius', 'and', 'the', 'filling', 'volume', 'of', 'a', 'riemannian', 'manifold', 'to', 'its', 'volume', 'the', 'main', 'result', 'of', 'the', 'present', 'article', 'is', 'that', 'in', 'dimensions', 'at', 'least', 'three', 'the', 'optimal'... | [-0.15730002656688585, 0.1041932196205701, -0.0711515920531169, 0.07888751372914105, -0.07077212541994146, -0.16614828898352296, 0.0651278085561524, 0.2902072756551206, -0.20907639668268316, -0.24828168525196173, 0.18215200425166747, -0.24622154895983198, -0.15667841084958875, 0.19960895775789944, -0.15087854029501185,... |
706.2791 | Composition of quantum states and dynamical subadditivity | We introduce a composition of quantum states of a bipartite system which is
based on the reshuffling of density matrices. This non-Abelian product is
associative and stems from the composition of quantum maps acting on a simple
quantum system. It induces a semi-group in the subset of states with maximally
mixed parti... | quant-ph | we introduce a composition of quantum states of a bipartite system which is based on the reshuffling of density matrices this nonabelian product is associative and stems from the composition of quantum maps acting on a simple quantum system it induces a semigroup in the subset of states with maximally mixed partial tra... | [['we', 'introduce', 'a', 'composition', 'of', 'quantum', 'states', 'of', 'a', 'bipartite', 'system', 'which', 'is', 'based', 'on', 'the', 'reshuffling', 'of', 'density', 'matrices', 'this', 'nonabelian', 'product', 'is', 'associative', 'and', 'stems', 'from', 'the', 'composition', 'of', 'quantum', 'maps', 'acting', 'o... | [-0.12992779557437947, 0.14764167498004907, -0.10090363256879048, 0.04440868772346423, 0.018549134948342625, -0.12626402406426174, 0.02820485561743327, 0.2832158857604049, -0.3271423793436649, -0.1895235040582419, 0.1300057219559676, -0.30352178746316993, -0.10964240054858641, 0.19084078200264937, -0.09972390230460507,... |
706.2792 | Practical quantum key distribution over 60 hours at an optical fiber
distance of 20km using weak and vacuum decoy pulses for enhanced security | Experimental one-way decoy pulse quantum key distribution running
continuously for 60 hours is demonstrated over a fiber distance of 20km. We
employ a decoy protocol which involves one weak decoy pulse and a vacuum pulse.
The obtained secret key rate is on average over 10kbps. This is the highest
rate reported using ... | quant-ph | experimental oneway decoy pulse quantum key distribution running continuously for 60 hours is demonstrated over a fiber distance of 20km we employ a decoy protocol which involves one weak decoy pulse and a vacuum pulse the obtained secret key rate is on average over 10kbps this is the highest rate reported using this d... | [['experimental', 'oneway', 'decoy', 'pulse', 'quantum', 'key', 'distribution', 'running', 'continuously', 'for', '60', 'hours', 'is', 'demonstrated', 'over', 'a', 'fiber', 'distance', 'of', '20km', 'we', 'employ', 'a', 'decoy', 'protocol', 'which', 'involves', 'one', 'weak', 'decoy', 'pulse', 'and', 'a', 'vacuum', 'pu... | [-0.22304750878944016, 0.13955781378279455, -0.10025943778302582, 0.017227916001174293, 0.07140173402721764, -0.2637886608431696, 0.12450582008488233, 0.4730796186772526, -0.22681937872081018, -0.25999474832330083, 0.045023522942830796, -0.18087405132389336, 0.0004124000103625118, 0.33183586597442627, -0.11200265215373... |
706.2793 | Local Approximations for Effective Scalar Field Equations of Motion | Fluctuation and dissipation dynamics is examined at all temperature ranges
for the general case of a background time evolving scalar field coupled to
heavy intermediate quantum fields which in turn are coupled to light quantum
fields. The evolution of the background field induces particle production from
the light fi... | hep-ph hep-th | fluctuation and dissipation dynamics is examined at all temperature ranges for the general case of a background time evolving scalar field coupled to heavy intermediate quantum fields which in turn are coupled to light quantum fields the evolution of the background field induces particle production from the light field... | [['fluctuation', 'and', 'dissipation', 'dynamics', 'is', 'examined', 'at', 'all', 'temperature', 'ranges', 'for', 'the', 'general', 'case', 'of', 'a', 'background', 'time', 'evolving', 'scalar', 'field', 'coupled', 'to', 'heavy', 'intermediate', 'quantum', 'fields', 'which', 'in', 'turn', 'are', 'coupled', 'to', 'light... | [-0.14285821237488452, 0.21464877776011373, -0.11194008735897527, 0.09338295026188434, -0.03728225881262033, -0.10758524615543358, -0.03379740789391552, 0.310628528373711, -0.2559396037528517, -0.3019663198540608, 0.0843465234900853, -0.23897650000554593, -0.10696400458726919, 0.16987046973187137, 0.0347362351349809, 0... |
706.2794 | Synthesis and magnetic properties of NiFe_{2-x}Al_{x}O_{4} nanoparticles | Nanocrystalline Al-doped nickel ferrite powders have been synthesized by
sol-gel auto-ignition method and the effect of non-magnetic aluminum content on
the structural and magnetic properties has been studied. The X-ray diffraction
(XRD) revealed that the powders obtained are single phase with inverse spinel
structur... | cond-mat.mtrl-sci | nanocrystalline aldoped nickel ferrite powders have been synthesized by solgel autoignition method and the effect of nonmagnetic aluminum content on the structural and magnetic properties has been studied the xray diffraction xrd revealed that the powders obtained are single phase with inverse spinel structure the calc... | [['nanocrystalline', 'aldoped', 'nickel', 'ferrite', 'powders', 'have', 'been', 'synthesized', 'by', 'solgel', 'autoignition', 'method', 'and', 'the', 'effect', 'of', 'nonmagnetic', 'aluminum', 'content', 'on', 'the', 'structural', 'and', 'magnetic', 'properties', 'has', 'been', 'studied', 'the', 'xray', 'diffraction',... | [-0.060756844073087755, 0.2336178474361077, -0.020305401255124405, -0.023768356874522095, -0.01963951331951345, -0.11410289248548604, 0.049721158662957045, 0.4440117744379677, -0.254572183524336, -0.3791441561382574, 0.03556620067259549, -0.3579299825311561, -0.05954179267549383, 0.18770668714356967, 0.0075058934817207... |
706.2795 | Dirty-paper Coding without Channel Information at the Transmitter and
Imperfect Estimation at the Receiver | In this paper, we examine the effects of imperfect channel estimation at the
receiver and no channel knowledge at the transmitter on the capacity of the
fading Costa's channel with channel state information non-causally known at the
transmitter. We derive the optimal Dirty-paper coding (DPC) scheme and its
correspond... | cs.IT math.IT | in this paper we examine the effects of imperfect channel estimation at the receiver and no channel knowledge at the transmitter on the capacity of the fading costas channel with channel state information noncausally known at the transmitter we derive the optimal dirtypaper coding dpc scheme and its corresponding achie... | [['in', 'this', 'paper', 'we', 'examine', 'the', 'effects', 'of', 'imperfect', 'channel', 'estimation', 'at', 'the', 'receiver', 'and', 'no', 'channel', 'knowledge', 'at', 'the', 'transmitter', 'on', 'the', 'capacity', 'of', 'the', 'fading', 'costas', 'channel', 'with', 'channel', 'state', 'information', 'noncausally',... | [-0.22802651251112324, -0.003288184508610535, -0.056005448405783066, 0.06025946691441907, -0.05161095196929048, -0.30293585653142896, 0.15255304833256267, 0.4247494592191347, -0.2713840823191419, -0.24496178708824456, 0.16586087271723338, -0.21655867426706404, -0.18007975706360393, 0.15124716950897005, -0.1423581017278... |
706.2796 | Single Target-Spin Asymmetry in Semi-Inclusive Deep Inelastic Scattering
on Transversely Polarized Nucleon Target | We use a new set of Collins functions to update a previous prediction on the
azimuthal asymmetries of pion productions in semi-inclusive deep inelastic
scattering (SIDIS) process on a transversely polarized nucleon target. We find
that the calculated results can give a good explanation to the HERMES
experiment with t... | hep-ph | we use a new set of collins functions to update a previous prediction on the azimuthal asymmetries of pion productions in semiinclusive deep inelastic scattering sidis process on a transversely polarized nucleon target we find that the calculated results can give a good explanation to the hermes experiment with the new... | [['we', 'use', 'a', 'new', 'set', 'of', 'collins', 'functions', 'to', 'update', 'a', 'previous', 'prediction', 'on', 'the', 'azimuthal', 'asymmetries', 'of', 'pion', 'productions', 'in', 'semiinclusive', 'deep', 'inelastic', 'scattering', 'sidis', 'process', 'on', 'a', 'transversely', 'polarized', 'nucleon', 'target', ... | [-0.03606754052067262, 0.18426699889823794, -0.16525611507441132, 0.1466508648052647, -0.05249005336536477, -0.0372515146694584, 0.018988198906010546, 0.38779681343708605, -0.1898273727455676, -0.19328893543473932, -0.04693225981430182, -0.3332148847225683, -0.03506997621167969, 0.16945212166247556, 0.08094372437316277... |
706.2797 | Extraction d'entit\'es dans des collections \'evolutives | The goal of our work is to use a set of reports and extract named entities,
in our case the names of Industrial or Academic partners. Starting with an
initial list of entities, we use a first set of documents to identify syntactic
patterns that are then validated in a supervised learning phase on a set of
annotated d... | cs.IR | the goal of our work is to use a set of reports and extract named entities in our case the names of industrial or academic partners starting with an initial list of entities we use a first set of documents to identify syntactic patterns that are then validated in a supervised learning phase on a set of annotated docume... | [['the', 'goal', 'of', 'our', 'work', 'is', 'to', 'use', 'a', 'set', 'of', 'reports', 'and', 'extract', 'named', 'entities', 'in', 'our', 'case', 'the', 'names', 'of', 'industrial', 'or', 'academic', 'partners', 'starting', 'with', 'an', 'initial', 'list', 'of', 'entities', 'we', 'use', 'a', 'first', 'set', 'of', 'docu... | [-0.05383142327579359, 0.04647273921594509, -0.05683196044750124, 0.04962340700246083, -0.16603526017473388, -0.07719967412995174, 0.11312996992722522, 0.38442075008836885, -0.2511815701417314, -0.34052507622788347, 0.06769341228549214, -0.3376023876441953, -0.07850567773566582, 0.19589523181687885, -0.1134895323387657... |
706.2798 | Rate effects on layering of a confined linear alkane | We perform drainage experiments of a linear alkane fluid (n-hexadecane) down
to molecular thicknesses, and focus on the role played by the confinement rate.
We show that molecular layering is strongly influenced by the velocity at which
the confining walls are approached: under high enough shear rates, the confined
m... | cond-mat.soft | we perform drainage experiments of a linear alkane fluid nhexadecane down to molecular thicknesses and focus on the role played by the confinement rate we show that molecular layering is strongly influenced by the velocity at which the confining walls are approached under high enough shear rates the confined medium beh... | [['we', 'perform', 'drainage', 'experiments', 'of', 'a', 'linear', 'alkane', 'fluid', 'nhexadecane', 'down', 'to', 'molecular', 'thicknesses', 'and', 'focus', 'on', 'the', 'role', 'played', 'by', 'the', 'confinement', 'rate', 'we', 'show', 'that', 'molecular', 'layering', 'is', 'strongly', 'influenced', 'by', 'the', 'v... | [-0.09562068590561726, 0.2555843041502937, -0.0482472846924793, -0.06518431078023111, 0.0005781193862536124, -0.12494799242787329, 0.06309632525309487, 0.38694233456460225, -0.23260209021723963, -0.2800248912618762, 0.03787354033452824, -0.2477196566012156, -0.10500878377933986, 0.18317380130091415, -0.0276458480220753... |
706.2799 | Gaussian localizable entanglement | We investigate localization of entanglement of multimode Gaussian states into
a pair of modes by local Gaussian measurements on the remaining modes and
classical communication. We find that for pure states and for mixed symmetric
states maximum entanglement between two modes can be localized by local
homodyne detecti... | quant-ph | we investigate localization of entanglement of multimode gaussian states into a pair of modes by local gaussian measurements on the remaining modes and classical communication we find that for pure states and for mixed symmetric states maximum entanglement between two modes can be localized by local homodyne detections... | [['we', 'investigate', 'localization', 'of', 'entanglement', 'of', 'multimode', 'gaussian', 'states', 'into', 'a', 'pair', 'of', 'modes', 'by', 'local', 'gaussian', 'measurements', 'on', 'the', 'remaining', 'modes', 'and', 'classical', 'communication', 'we', 'find', 'that', 'for', 'pure', 'states', 'and', 'for', 'mixed... | [-0.12458269046242897, 0.2728509016143268, -0.10494409482378293, 0.05780384024632547, 0.05089995320817894, -0.2264768545419964, 0.04755298154401209, 0.3779719578211798, -0.21864515249891317, -0.20173619501292706, 0.04972337893217199, -0.31676010861445, -0.09542537340209545, 0.18472985104274223, 0.007029352410052738, 0.... |
706.28 | Anisotropic small-scale constraints on energy in rotating stratified
turbulence | Rapidly rotating, stably stratified three-dimensional inviscid flows conserve
both energy and potential enstrophy. We show that in such flows, the forward
cascade of potential enstrophy imposes anisotropic constraints on the
wavenumber distribution of kinetic and potential energy. The horizontal kinetic
energy is sup... | nlin.CD | rapidly rotating stably stratified threedimensional inviscid flows conserve both energy and potential enstrophy we show that in such flows the forward cascade of potential enstrophy imposes anisotropic constraints on the wavenumber distribution of kinetic and potential energy the horizontal kinetic energy is suppressed... | [['rapidly', 'rotating', 'stably', 'stratified', 'threedimensional', 'inviscid', 'flows', 'conserve', 'both', 'energy', 'and', 'potential', 'enstrophy', 'we', 'show', 'that', 'in', 'such', 'flows', 'the', 'forward', 'cascade', 'of', 'potential', 'enstrophy', 'imposes', 'anisotropic', 'constraints', 'on', 'the', 'wavenu... | [-0.15781733920601637, 0.18875389165967996, -0.037629856376473696, 0.09433357122409354, -0.040696404898833284, -0.09239464990433159, -0.009703187734550355, 0.29321671273608346, -0.25412711819731876, -0.31858988731217225, 0.05186862311261633, -0.27569320962739813, -0.041773766095406915, 0.2081271974897582, 0.03461617072... |
706.2801 | Evidence for Growth of Eccentricity and Mass Clearing in a Disc Interior
to a Planet | We present computational results showing eccentricity growth in the inner
portions of a protoplanetary disc. We attribute this to the evolving surface
density of the disc. The planet creates a gap, which adjusts the balance
between the 3:1 (eccentricity exciting) and 2:1 (eccentricity damping)
resonances. The eccentr... | astro-ph | we present computational results showing eccentricity growth in the inner portions of a protoplanetary disc we attribute this to the evolving surface density of the disc the planet creates a gap which adjusts the balance between the 31 eccentricity exciting and 21 eccentricity damping resonances the eccentricity of the... | [['we', 'present', 'computational', 'results', 'showing', 'eccentricity', 'growth', 'in', 'the', 'inner', 'portions', 'of', 'a', 'protoplanetary', 'disc', 'we', 'attribute', 'this', 'to', 'the', 'evolving', 'surface', 'density', 'of', 'the', 'disc', 'the', 'planet', 'creates', 'a', 'gap', 'which', 'adjusts', 'the', 'ba... | [-0.1429771203905917, 0.13384427663701928, -0.10844680064026481, 0.0624369431816676, -0.11260491922743372, -0.05490871372499636, 0.010978753123289118, 0.3392547403134733, -0.250804965855083, -0.3543681458334674, 0.04470456569202265, -0.21088397521320934, -0.07831772957201842, 0.16481962673120445, -0.08767286282810537, ... |
706.2802 | Simple pairs potential-density for flat rings | Pairs potential-density in terms of elementary functions that represents flat
rings structures are presented. We study structures representing one or several
concentric flat rings. Also disks surrounded by concentric flat rings are
exhibited. The stability of concentrically circular orbits of particles moving
on a fl... | astro-ph gr-qc physics.class-ph | pairs potentialdensity in terms of elementary functions that represents flat rings structures are presented we study structures representing one or several concentric flat rings also disks surrounded by concentric flat rings are exhibited the stability of concentrically circular orbits of particles moving on a flat rin... | [['pairs', 'potentialdensity', 'in', 'terms', 'of', 'elementary', 'functions', 'that', 'represents', 'flat', 'rings', 'structures', 'are', 'presented', 'we', 'study', 'structures', 'representing', 'one', 'or', 'several', 'concentric', 'flat', 'rings', 'also', 'disks', 'surrounded', 'by', 'concentric', 'flat', 'rings', ... | [-0.2790378727950156, 0.08551255289393549, -0.07653837910710046, 0.0663895519705525, -0.0065456865032991534, -0.12875524250109896, -0.15378033641844432, 0.4478719076858117, -0.2225586180216991, -0.1929532459919126, 0.07059679216875409, -0.2751880585789107, -0.07762049613721991, 0.17934418275791147, -0.02215326640110176... |
706.2803 | Bound states in N = 4 SYM on T^3: Spin(2n) and the exceptional groups | The low energy spectrum of (3+1)-dimensional N=4 supersymmetric Yang-Mills
theory on a spatial three-torus contains a certain number of bound states,
characterized by their discrete abelian magnetic and electric 't Hooft fluxes.
At weak coupling, the wave-functions of these states are supported near points
in the mod... | hep-th | the low energy spectrum of 31dimensional n4 supersymmetric yangmills theory on a spatial threetorus contains a certain number of bound states characterized by their discrete abelian magnetic and electric t hooft fluxes at weak coupling the wavefunctions of these states are supported near points in the moduli space of f... | [['the', 'low', 'energy', 'spectrum', 'of', '31dimensional', 'n4', 'supersymmetric', 'yangmills', 'theory', 'on', 'a', 'spatial', 'threetorus', 'contains', 'a', 'certain', 'number', 'of', 'bound', 'states', 'characterized', 'by', 'their', 'discrete', 'abelian', 'magnetic', 'and', 'electric', 't', 'hooft', 'fluxes', 'at... | [-0.20210524438559238, 0.19574484758777544, -0.07592830206428108, 0.04045884901866445, -0.05560755373042976, -0.1230029548422016, 0.041994140061132355, 0.313430984308622, -0.17977622925657136, -0.3022424137372331, 0.06926110713694501, -0.27394186580104046, -0.12492602209335771, 0.1343438330716614, -0.05987190679679143,... |
706.2804 | Hot Topics from CLEO-c | I briefly review some of the results obtained using the CLEO-c detector
| hep-ex | i briefly review some of the results obtained using the cleoc detector | [['i', 'briefly', 'review', 'some', 'of', 'the', 'results', 'obtained', 'using', 'the', 'cleoc', 'detector']] | [-0.02696267111847798, 0.07069953053724021, -0.06327842098350327, 0.04025940534969171, -0.02320016532515486, -0.1324860385308663, -0.007452101136247317, 0.3169981464743614, -0.1624652991692225, -0.24315080853799978, 0.16054522742827734, -0.4627453691015641, -0.13487140399714312, 0.24862205014020825, 0.02167537692002952... |
706.2805 | Semileptonic bc to cc Baryon Decay and Heavy Quark Spin Symmetry | We study the semileptonic decays of the lowest-lying bc baryons to the
lowest-lying cc baryons (Xi_{bc}^{(\prime*)}--> Xi_{cc}^{(*)} and
Omega_{bc}^{(\prime*)}--> Omega_{cc}^{(*)}), in the limit m_b, m_c >>
Lambda_{QCD} and close to the zero recoil point. The separate heavy quark spin
symmetries make it possible to d... | hep-ph | we study the semileptonic decays of the lowestlying bc baryons to the lowestlying cc baryons xi_bcprime xi_cc and omega_bcprime omega_cc in the limit m_b m_c lambda_qcd and close to the zero recoil point the separate heavy quark spin symmetries make it possible to describe all these decays using a single form factor we... | [['we', 'study', 'the', 'semileptonic', 'decays', 'of', 'the', 'lowestlying', 'bc', 'baryons', 'to', 'the', 'lowestlying', 'cc', 'baryons', 'xi_bcprime', 'xi_cc', 'and', 'omega_bcprime', 'omega_cc', 'in', 'the', 'limit', 'm_b', 'm_c', 'lambda_qcd', 'and', 'close', 'to', 'the', 'zero', 'recoil', 'point', 'the', 'separat... | [-0.06163627667984022, 0.19733418920077384, -0.0980912496328749, 0.14555728174904783, -0.07724784242490193, -0.1464846138736572, 0.11948610094876846, 0.28547582977140945, -0.21094724449159746, -0.18600862850188138, -0.05941830592222907, -0.3638196240080464, 0.0018686367565709534, 0.10128597357790127, 0.0626591980831246... |
706.2806 | A Characterization of the Morse Minimal Set up to Topological Conjugacy | We establish necessary and sufficient conditions for a dynamical system to be
topologically conjugate to the Morse minimal set, the shift orbit closure of
the Morse sequence, and conditions for topological conjugacy to the closely
related Teoplitz minimal set.
| math.DS | we establish necessary and sufficient conditions for a dynamical system to be topologically conjugate to the morse minimal set the shift orbit closure of the morse sequence and conditions for topological conjugacy to the closely related teoplitz minimal set | [['we', 'establish', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'a', 'dynamical', 'system', 'to', 'be', 'topologically', 'conjugate', 'to', 'the', 'morse', 'minimal', 'set', 'the', 'shift', 'orbit', 'closure', 'of', 'the', 'morse', 'sequence', 'and', 'conditions', 'for', 'topological', 'conjugacy', 'to', 't... | [-0.1889370009303093, 0.1320603121406375, -0.07066753447221484, 0.1256135204442753, -0.11401355475521623, -0.14437539897297916, 0.07599468773696572, 0.32004514940751666, -0.3343508036281818, -0.2500926253314202, 0.12840013985689253, -0.19219046334425607, -0.1547646263662057, 0.19946685237571216, -0.15790583826123905, 0... |
706.2807 | On the constant in the Mertens product for arithmetic progressions. I.
Identities | The aim of the paper is the proof of new identities for the constant in the
Mertens product for arithmetic progressions. We deal with the problem of the
numerical computation of these constants in another paper.
| math.NT | the aim of the paper is the proof of new identities for the constant in the mertens product for arithmetic progressions we deal with the problem of the numerical computation of these constants in another paper | [['the', 'aim', 'of', 'the', 'paper', 'is', 'the', 'proof', 'of', 'new', 'identities', 'for', 'the', 'constant', 'in', 'the', 'mertens', 'product', 'for', 'arithmetic', 'progressions', 'we', 'deal', 'with', 'the', 'problem', 'of', 'the', 'numerical', 'computation', 'of', 'these', 'constants', 'in', 'another', 'paper']] | [-0.18139095231890678, 0.04979807466992901, -0.0795222646298094, 0.04891923102614884, -0.05311194328694708, -0.06783321429975331, 0.05278791518907787, 0.2843492412680967, -0.31941657616860336, -0.27081508171330726, 0.13616709577359465, -0.25180546925144476, -0.17081195167783234, 0.21814040097201037, -0.1333570394579308... |
706.2808 | Asymptotics of the allele frequency spectrum associated with the
Bolthausen-Sznitman coalescent | We work in the context of the infinitely many alleles model. The allelic
partition associated with a coalescent process started from n individuals is
obtained by placing mutations along the skeleton of the coalescent tree; for
each individual, we trace back to the most recent mutation affecting it and
group together ... | math.PR math.CO q-bio.PE | we work in the context of the infinitely many alleles model the allelic partition associated with a coalescent process started from n individuals is obtained by placing mutations along the skeleton of the coalescent tree for each individual we trace back to the most recent mutation affecting it and group together indiv... | [['we', 'work', 'in', 'the', 'context', 'of', 'the', 'infinitely', 'many', 'alleles', 'model', 'the', 'allelic', 'partition', 'associated', 'with', 'a', 'coalescent', 'process', 'started', 'from', 'n', 'individuals', 'is', 'obtained', 'by', 'placing', 'mutations', 'along', 'the', 'skeleton', 'of', 'the', 'coalescent', ... | [-0.08088359752112906, 0.14059507756941964, -0.05090354415116525, 0.10889435281483259, -0.059731867600562455, -0.14548210998631636, 0.1005845596126717, 0.3556065869199324, -0.260299975283833, -0.2181441358547021, 0.07482792580606346, -0.27575275453125847, -0.13948779212623316, 0.14761501894762763, -0.10304841290145547,... |
706.2809 | On the Outage Capacity of a Practical Decoder Using Channel Estimation
Accuracy | The optimal decoder achieving the outage capacity under imperfect channel
estimation is investigated. First, by searching into the family of nearest
neighbor decoders, which can be easily implemented on most practical coded
modulation systems, we derive a decoding metric that minimizes the average of
the transmission... | cs.IT math.IT | the optimal decoder achieving the outage capacity under imperfect channel estimation is investigated first by searching into the family of nearest neighbor decoders which can be easily implemented on most practical coded modulation systems we derive a decoding metric that minimizes the average of the transmission error... | [['the', 'optimal', 'decoder', 'achieving', 'the', 'outage', 'capacity', 'under', 'imperfect', 'channel', 'estimation', 'is', 'investigated', 'first', 'by', 'searching', 'into', 'the', 'family', 'of', 'nearest', 'neighbor', 'decoders', 'which', 'can', 'be', 'easily', 'implemented', 'on', 'most', 'practical', 'coded', '... | [-0.25787538753180805, -0.0009189572179863273, -0.019303641502669645, 0.0733718142538808, -0.01758994127428809, -0.2787124005195057, 0.1789821881589718, 0.39409329339342064, -0.26327381148151946, -0.23681593659810377, 0.10654074012174618, -0.21605449635806212, -0.17394930177008147, 0.18444544573579807, -0.1873912925576... |
706.281 | Quarkonium production in coherent pp/AA collisions and small-x physics | In this contribution we study the photoproduction of quarkonium in coherent
proton-proton and nucleus-nucleus interactions at the LHC. The integrated cross
sections and rapidity distributions are estimated using the Color Glass
Condensate (CGC) formalism, which takes into account the parton saturation
effects at high... | hep-ph | in this contribution we study the photoproduction of quarkonium in coherent protonproton and nucleusnucleus interactions at the lhc the integrated cross sections and rapidity distributions are estimated using the color glass condensate cgc formalism which takes into account the parton saturation effects at high energie... | [['in', 'this', 'contribution', 'we', 'study', 'the', 'photoproduction', 'of', 'quarkonium', 'in', 'coherent', 'protonproton', 'and', 'nucleusnucleus', 'interactions', 'at', 'the', 'lhc', 'the', 'integrated', 'cross', 'sections', 'and', 'rapidity', 'distributions', 'are', 'estimated', 'using', 'the', 'color', 'glass', ... | [0.016158430806343566, 0.27714810300758985, -0.26596009967308315, 0.2355629197862175, 0.046814807883973394, -0.020768958653481502, -0.10392906073972864, 0.4127268963405546, -0.16763560227030572, -0.19298278178387093, -0.11704121092070807, -0.3532362401766597, 0.11436991823204565, 0.03905217869664138, 0.1037800421516569... |
706.2811 | Lindemann Criterion and the Anomalous Melting Curve of Sodium | Recent reports of the melting curve of sodium at high pressure have shown
that it has a very steep descent after a maximum of around 1000K at 31 GPa.
This is not due to a phase transition. According to the Lindemann criterion,
this behaviour should be apparent in the evolution of the Debye temperature
with pressure. ... | cond-mat.other | recent reports of the melting curve of sodium at high pressure have shown that it has a very steep descent after a maximum of around 1000k at 31 gpa this is not due to a phase transition according to the lindemann criterion this behaviour should be apparent in the evolution of the debye temperature with pressure in thi... | [['recent', 'reports', 'of', 'the', 'melting', 'curve', 'of', 'sodium', 'at', 'high', 'pressure', 'have', 'shown', 'that', 'it', 'has', 'a', 'very', 'steep', 'descent', 'after', 'a', 'maximum', 'of', 'around', '1000k', 'at', '31', 'gpa', 'this', 'is', 'not', 'due', 'to', 'a', 'phase', 'transition', 'according', 'to', '... | [-0.09452490152842882, 0.17733601228268747, -0.18246056054333093, -0.01024622734250369, -0.021642976995519918, -0.09887010129544922, 0.11464223182863659, 0.3810566191119377, -0.2381275056580886, -0.31690501578791874, 0.06859527783458959, -0.30017081032874005, -0.09709773707495194, 0.15101667203836971, -0.01793530798808... |
706.2812 | Ultra High Energy Cosmic ray and gamma-ray signatures of inductive
acceleration in AGN jets | The highest energy cosmic rays could be produced by drifts in magnetized,
cylindrically collimated, sheared jets of powerful active galaxies (i.e. FR II
radiogalaxies; radio loud quasars and high power BL Lacs). We show that in such
scenarios proton synchrotron radiation can give rise to detectable photon
fluxes at e... | astro-ph | the highest energy cosmic rays could be produced by drifts in magnetized cylindrically collimated sheared jets of powerful active galaxies ie fr ii radiogalaxies radio loud quasars and high power bl lacs we show that in such scenarios proton synchrotron radiation can give rise to detectable photon fluxes at energies ra... | [['the', 'highest', 'energy', 'cosmic', 'rays', 'could', 'be', 'produced', 'by', 'drifts', 'in', 'magnetized', 'cylindrically', 'collimated', 'sheared', 'jets', 'of', 'powerful', 'active', 'galaxies', 'ie', 'fr', 'ii', 'radiogalaxies', 'radio', 'loud', 'quasars', 'and', 'high', 'power', 'bl', 'lacs', 'we', 'show', 'tha... | [-0.028136546723544598, 0.29240338927355863, 0.05171074098670634, 0.22993926988062213, -0.13292973173507963, -0.14444842076982703, -0.05162324655359074, 0.5018977353080981, -0.16369898284990655, -0.4060196436120797, -0.06670847225350217, -0.31662235251170096, 0.1468092840543743, 0.2510999987943698, 0.018197961571878928... |
706.2813 | Measurement of the Total Hadronic Cross Section in e+e- Annihilations
below 10.56 GeV | Using the CLEO III detector, we measure absolute cross sections for e+e- -->
hadrons at seven center-of-mass energies between 6.964 and 10.538 GeV. The
values of R, the ratio of hadronic and muon pair production cross sections, are
determined within 2% total r.m.s. uncertainty.
| hep-ex | using the cleo iii detector we measure absolute cross sections for ee hadrons at seven centerofmass energies between 6964 and 10538 gev the values of r the ratio of hadronic and muon pair production cross sections are determined within 2 total rms uncertainty | [['using', 'the', 'cleo', 'iii', 'detector', 'we', 'measure', 'absolute', 'cross', 'sections', 'for', 'ee', 'hadrons', 'at', 'seven', 'centerofmass', 'energies', 'between', '6964', 'and', '10538', 'gev', 'the', 'values', 'of', 'r', 'the', 'ratio', 'of', 'hadronic', 'and', 'muon', 'pair', 'production', 'cross', 'section... | [-0.04431446373657605, 0.19857693387758593, -0.025899651449520226, 0.15997819624148135, 0.08089754190620814, -0.08638160658437152, 0.009095147620280122, 0.36973633383249127, -0.14015006654094472, -0.36555263140173844, -0.11739340269678207, -0.44196966164853685, 0.20207235661097045, 0.1759799319741771, 0.142530243795061... |
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