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 |
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710.1053 | Extensions for supersingular representations of $GL_2(Q_p)$ | Let $p>2$ be a prime number. Let $G:=GL_2(Q_p)$ and $\pi$, $\tau$ smooth
irreducible representations of $G$ on $\bar{F}_p$-vector spaces with a central
character. We show if $\pi$ is supersingular then $Ext^1_G(\tau,\pi)\neq 0$
implies $\tau\cong \pi$. This answers affirmatively for $p>2$ a question of
Colmez. We als... | math.RT math.NT | let p2 be a prime number let ggl_2q_p and pi tau smooth irreducible representations of g on barf_pvector spaces with a central character we show if pi is supersingular then ext1_gtaupineq 0 implies taucong pi this answers affirmatively for p2 a question of colmez we also determine ext1_gtaupi when pi is the steinberg r... | [['let', 'p2', 'be', 'a', 'prime', 'number', 'let', 'ggl_2q_p', 'and', 'pi', 'tau', 'smooth', 'irreducible', 'representations', 'of', 'g', 'on', 'barf_pvector', 'spaces', 'with', 'a', 'central', 'character', 'we', 'show', 'if', 'pi', 'is', 'supersingular', 'then', 'ext1_gtaupineq', '0', 'implies', 'taucong', 'pi', 'thi... | [-0.16833636909723282, 0.10662271520788116, -0.14549193674964564, 0.03005999966823895, -0.11479198931982475, -0.17990394384999361, 0.001711145815040384, 0.32260716389864685, -0.3186448692743267, -0.19848395558074117, 0.029143234946033252, -0.2850690195070846, -0.12424645093934876, 0.22813760388110366, -0.12164992016873... |
710.1054 | Lower dimensional Yang-Mills theory as a laboratory to study the
infrared regime | Lattice studies of the infrared regime of gauge theories are complicated by
the required extensive limits, the performed gauge fixing and the demand for
high statistics. Using a general power counting scheme for the infrared limit
of Landau gauge SU(N) Yang-Mills theory in arbitrary dimensions we show that
the infrar... | hep-ph hep-lat | lattice studies of the infrared regime of gauge theories are complicated by the required extensive limits the performed gauge fixing and the demand for high statistics using a general power counting scheme for the infrared limit of landau gauge sun yangmills theory in arbitrary dimensions we show that the infrared beha... | [['lattice', 'studies', 'of', 'the', 'infrared', 'regime', 'of', 'gauge', 'theories', 'are', 'complicated', 'by', 'the', 'required', 'extensive', 'limits', 'the', 'performed', 'gauge', 'fixing', 'and', 'the', 'demand', 'for', 'high', 'statistics', 'using', 'a', 'general', 'power', 'counting', 'scheme', 'for', 'the', 'i... | [-0.08957919254598598, 0.15858669728491334, -0.10899787076691951, 0.12886703432091984, -0.019264434374147845, -0.1091605016701324, 0.03214103545648076, 0.3662174739624544, -0.13904356093256062, -0.29419845425754143, 0.08823822743274391, -0.2412640442170443, -0.16078266500925986, 0.19240080805805823, 0.01482435419494586... |
710.1055 | Optimal Controlled Teleportation | We give the analytic expressions of maximal probabilities of successfully
controlled teleportating an unknown qubit via every kind of tripartite states.
Besides, another kind of localizable entanglement is also determined.
Furthermore, we give the sufficient and necessary condition that a three-qubit
state can be col... | quant-ph | we give the analytic expressions of maximal probabilities of successfully controlled teleportating an unknown qubit via every kind of tripartite states besides another kind of localizable entanglement is also determined furthermore we give the sufficient and necessary condition that a threequbit state can be collapsed ... | [['we', 'give', 'the', 'analytic', 'expressions', 'of', 'maximal', 'probabilities', 'of', 'successfully', 'controlled', 'teleportating', 'an', 'unknown', 'qubit', 'via', 'every', 'kind', 'of', 'tripartite', 'states', 'besides', 'another', 'kind', 'of', 'localizable', 'entanglement', 'is', 'also', 'determined', 'further... | [-0.142675222306535, 0.21253341591736677, -0.044071150977709674, 0.04374981454215807, 0.0024159988530389055, -0.26997985700486093, 0.10512268777209811, 0.37525884957030053, -0.22713316762365582, -0.23783272240174616, 0.09082989879633958, -0.21255995521730767, -0.0958113761380224, 0.21177432184084888, -0.061114539210571... |
710.1056 | Entanglement of multiparty stabilizer, symmetric, and antisymmetric
states | We study various distance-like entanglement measures of multipartite states
under certain symmetries. Using group averaging techniques we provide
conditions under which the relative entropy of entanglement, the geometric
measure of entanglement and the logarithmic robustness are equivalent. We
consider important clas... | quant-ph | we study various distancelike entanglement measures of multipartite states under certain symmetries using group averaging techniques we provide conditions under which the relative entropy of entanglement the geometric measure of entanglement and the logarithmic robustness are equivalent we consider important classes of... | [['we', 'study', 'various', 'distancelike', 'entanglement', 'measures', 'of', 'multipartite', 'states', 'under', 'certain', 'symmetries', 'using', 'group', 'averaging', 'techniques', 'we', 'provide', 'conditions', 'under', 'which', 'the', 'relative', 'entropy', 'of', 'entanglement', 'the', 'geometric', 'measure', 'of',... | [-0.13967617565137802, 0.18742603835831054, -0.11816282755689032, 0.1101806252880722, 0.018382498105337857, -0.19309820201022912, 0.04320821005967446, 0.38215564743884456, -0.24166907190076456, -0.21824845070981938, 0.09732742089662551, -0.22914357788108006, -0.14126920913214852, 0.16561748868091994, -0.064184105648790... |
710.1057 | Elastic properties of cubic crystals: Every's versus Blackman's diagram | Blackman's diagram of two dimensionless ratios of elastic constants is
frequently used to correlate elastic properties of cubic crystals with
interatomic bondings. Every's diagram of a different set of two dimensionless
variables was used by us for classification of various properties of such
crystals. We compare the... | cond-mat.mtrl-sci cond-mat.other | blackmans diagram of two dimensionless ratios of elastic constants is frequently used to correlate elastic properties of cubic crystals with interatomic bondings everys diagram of a different set of two dimensionless variables was used by us for classification of various properties of such crystals we compare these two... | [['blackmans', 'diagram', 'of', 'two', 'dimensionless', 'ratios', 'of', 'elastic', 'constants', 'is', 'frequently', 'used', 'to', 'correlate', 'elastic', 'properties', 'of', 'cubic', 'crystals', 'with', 'interatomic', 'bondings', 'everys', 'diagram', 'of', 'a', 'different', 'set', 'of', 'two', 'dimensionless', 'variabl... | [-0.18032434079917817, 0.17176338655844078, -0.02765698603725706, 0.03377400285616103, -0.05498207726339304, -0.13574692185395976, 0.05582921660666543, 0.3841193495744389, -0.24871714330077463, -0.2903190694956316, 0.016361399009683798, -0.3244883783033812, -0.12236113488990692, 0.19546654951923034, 0.06275486055528745... |
710.1058 | Quantum-mechanical Landau-Lifshitz equation | Quantum-mechanical analogue of Landau-Lifshitz equation has been derived. It
has been established that Landau-Lifshitz equation is fundamental physical
equation underlying the dynamics of spectroscopic transitions and transitional
phenomena. New phenomenon is predicted: electrical spin wave resonance (ESWR)
being to ... | quant-ph | quantummechanical analogue of landaulifshitz equation has been derived it has been established that landaulifshitz equation is fundamental physical equation underlying the dynamics of spectroscopic transitions and transitional phenomena new phenomenon is predicted electrical spin wave resonance eswr being to be electri... | [['quantummechanical', 'analogue', 'of', 'landaulifshitz', 'equation', 'has', 'been', 'derived', 'it', 'has', 'been', 'established', 'that', 'landaulifshitz', 'equation', 'is', 'fundamental', 'physical', 'equation', 'underlying', 'the', 'dynamics', 'of', 'spectroscopic', 'transitions', 'and', 'transitional', 'phenomena... | [-0.18845228573469364, 0.15489145497912946, -0.12110243189027128, 0.08914704477596704, -0.22549127576791722, -0.13113343035397323, -0.0847125253032731, 0.3066539399568801, -0.2618489483492854, -0.2578731537189173, 0.03618663633444711, -0.2855846539301717, -0.18156643575766002, 0.2100560365563623, 0.10852321263645655, 0... |
710.1059 | The arrow of time and the Weyl group: all supergravity billiards are
integrable | In this paper we show that all supergravity billiards corresponding to
sigma-models on any U/H non compact-symmetric space and obtained by
compactifying supergravity to D=3 are fully integrable. The key point in
establishing the integration algorithm is provided by an upper triangular
embedding of the solvable Lie al... | hep-th astro-ph nlin.SI | in this paper we show that all supergravity billiards corresponding to sigmamodels on any uh non compactsymmetric space and obtained by compactifying supergravity to d3 are fully integrable the key point in establishing the integration algorithm is provided by an upper triangular embedding of the solvable lie algebra a... | [['in', 'this', 'paper', 'we', 'show', 'that', 'all', 'supergravity', 'billiards', 'corresponding', 'to', 'sigmamodels', 'on', 'any', 'uh', 'non', 'compactsymmetric', 'space', 'and', 'obtained', 'by', 'compactifying', 'supergravity', 'to', 'd3', 'are', 'fully', 'integrable', 'the', 'key', 'point', 'in', 'establishing',... | [-0.18687698268642028, 0.11994445527845528, -0.07811054828033472, 0.010774185959404955, -0.0891234446503222, -0.10724446161960562, 0.012833806540972242, 0.3422297608355681, -0.2790648698868851, -0.24149269242344112, 0.10503085433738306, -0.2567000007070601, -0.16501666741911322, 0.17309912819725773, -0.0736054033160932... |
710.106 | Comments on gluon scattering amplitudes via AdS/CFT | In this article we consider n gluon color ordered, planar amplitudes in N=4
super Yang Mills at strong 't Hooft coupling. These amplitudes are approximated
by classical surfaces in AdS_5 space. We compute the value of the amplitude for
a particular kinematic configuration for a large number of gluons and find that
th... | hep-th | in this article we consider n gluon color ordered planar amplitudes in n4 super yang mills at strong t hooft coupling these amplitudes are approximated by classical surfaces in ads_5 space we compute the value of the amplitude for a particular kinematic configuration for a large number of gluons and find that the resul... | [['in', 'this', 'article', 'we', 'consider', 'n', 'gluon', 'color', 'ordered', 'planar', 'amplitudes', 'in', 'n4', 'super', 'yang', 'mills', 'at', 'strong', 't', 'hooft', 'coupling', 'these', 'amplitudes', 'are', 'approximated', 'by', 'classical', 'surfaces', 'in', 'ads_5', 'space', 'we', 'compute', 'the', 'value', 'of... | [-0.1482616651587055, 0.21706349914560893, -0.07841530029961308, 0.10872072489250319, -0.0306733779908557, -0.11509992092781302, 0.07216462157250914, 0.3510557289501386, -0.15541555339004845, -0.27167679034173486, 0.04417009222670458, -0.26559832136678907, -0.14432004452184108, 0.15130385000458255, -0.01118933374195226... |
710.1061 | Massive Gravity in Minkowski Space via Gravitational Higgs Mechanism | In gravitational Higgs mechanism graviton components acquire mass in the
process of spontaneous breaking of diffeomorphisms (via scalar vacuum
expectation values). Recently, gravitational Higgs mechanism was discussed in
the context of obtaining massive gravity directly in four dimensions. We
discuss a setup, with al... | hep-th gr-qc | in gravitational higgs mechanism graviton components acquire mass in the process of spontaneous breaking of diffeomorphisms via scalar vacuum expectation values recently gravitational higgs mechanism was discussed in the context of obtaining massive gravity directly in four dimensions we discuss a setup with all diffeo... | [['in', 'gravitational', 'higgs', 'mechanism', 'graviton', 'components', 'acquire', 'mass', 'in', 'the', 'process', 'of', 'spontaneous', 'breaking', 'of', 'diffeomorphisms', 'via', 'scalar', 'vacuum', 'expectation', 'values', 'recently', 'gravitational', 'higgs', 'mechanism', 'was', 'discussed', 'in', 'the', 'context',... | [-0.19860219516392266, 0.26941851913382797, -0.02907423981678973, 0.10132209206561751, -0.11838141058158494, -0.15393213942801034, -0.03212391423355592, 0.3005833178758621, -0.16073499161739574, -0.2581601250930724, 0.06501022267550986, -0.22022569615786014, -0.12817039751776851, 0.11571555896277043, -0.002602919179918... |
710.1062 | New Insights on Interstellar Gas-Phase Iron | In this paper, we report on the gas-phase abundance of singly-ionized iron
(Fe II) for 51 lines of sight, using data from the Far Ultraviolet
Spectroscopic Explorer (FUSE). Fe II column densities are derived by measuring
the equivalent widths of several ultraviolet absorption lines and subsequently
fitting those to a... | astro-ph | in this paper we report on the gasphase abundance of singlyionized iron fe ii for 51 lines of sight using data from the far ultraviolet spectroscopic explorer fuse fe ii column densities are derived by measuring the equivalent widths of several ultraviolet absorption lines and subsequently fitting those to a curve of g... | [['in', 'this', 'paper', 'we', 'report', 'on', 'the', 'gasphase', 'abundance', 'of', 'singlyionized', 'iron', 'fe', 'ii', 'for', '51', 'lines', 'of', 'sight', 'using', 'data', 'from', 'the', 'far', 'ultraviolet', 'spectroscopic', 'explorer', 'fuse', 'fe', 'ii', 'column', 'densities', 'are', 'derived', 'by', 'measuring'... | [-0.045723072277676115, 0.04775248863127484, 0.0285601905143635, 0.030990606639062918, -0.03462957476806801, -0.13478822353944514, 0.09066936584106583, 0.5034366084756668, -0.12977013220776792, -0.33237718601111577, 0.02804100848658968, -0.3581064182676767, -0.021591436939864508, 0.15032936000738384, 0.0035094614008720... |
710.1063 | Zero modes' fusion ring and braid group representations for the extended
chiral su(2) WZNW model | The zero modes' Fock space for the extended chiral $su(2)$ WZNW model gives
room to a realization of the Grothendieck fusion ring of representations of the
restricted $U_q sl(2)$ quantum universal enveloping algebra (QUEA) at an even
($2h$-th) root of unity, and of its extension by the Lusztig operators. It is
shown ... | hep-th math-ph math.MP math.QA | the zero modes fock space for the extended chiral su2 wznw model gives room to a realization of the grothendieck fusion ring of representations of the restricted u_q sl2 quantum universal enveloping algebra quea at an even 2hth root of unity and of its extension by the lusztig operators it is shown that expressing the ... | [['the', 'zero', 'modes', 'fock', 'space', 'for', 'the', 'extended', 'chiral', 'su2', 'wznw', 'model', 'gives', 'room', 'to', 'a', 'realization', 'of', 'the', 'grothendieck', 'fusion', 'ring', 'of', 'representations', 'of', 'the', 'restricted', 'u_q', 'sl2', 'quantum', 'universal', 'enveloping', 'algebra', 'quea', 'at'... | [-0.1889850731418964, 0.11913677431115385, -0.10916357721397353, 0.042503747481649985, -0.09042560746480201, -0.1200497065137531, -0.04506370740953923, 0.26425555171895654, -0.34088551313165694, -0.16102970800092142, 0.053895453056846294, -0.22072560868341937, -0.11683064399497403, 0.17280878322649626, -0.0613158878141... |
710.1064 | The Variation of Magnesium Depletion with Line of Sight Conditions | In this paper we report on the gas-phase abundance of singly-ionized
magnesium (Mg II) in 44 lines of sight, using data from the Hubble Space
Telescope (HST). We measure Mg II column densities by analyzing medium- and
high-resolution archival STIS spectra of the 1240 A doublet of Mg II. We find
that Mg II depletion i... | astro-ph | in this paper we report on the gasphase abundance of singlyionized magnesium mg ii in 44 lines of sight using data from the hubble space telescope hst we measure mg ii column densities by analyzing medium and highresolution archival stis spectra of the 1240 a doublet of mg ii we find that mg ii depletion is correlated ... | [['in', 'this', 'paper', 'we', 'report', 'on', 'the', 'gasphase', 'abundance', 'of', 'singlyionized', 'magnesium', 'mg', 'ii', 'in', '44', 'lines', 'of', 'sight', 'using', 'data', 'from', 'the', 'hubble', 'space', 'telescope', 'hst', 'we', 'measure', 'mg', 'ii', 'column', 'densities', 'by', 'analyzing', 'medium', 'and'... | [-0.03353067625883139, 0.10266507122907098, 0.025485466421225372, 0.06183552272606319, -0.01217576524567572, -0.15845090610745513, 0.06330694902880853, 0.4982231877238294, -0.1593270540398396, -0.3776103959844252, 0.02357223371466346, -0.3334622857057386, -0.032211514976002095, 0.12066393592509866, -0.02660014115871838... |
710.1065 | Planet formation around stars of various masses: The snow line and the
frequency of giant planets | We use a semi-analytic circumstellar disk model that considers movement of
the snow line through evolution of accretion and the central star to
investigate how gas giant frequency changes with stellar mass. The snow line
distance changes weakly with stellar mass; thus giant planets form over a wide
range of spectral ... | astro-ph | we use a semianalytic circumstellar disk model that considers movement of the snow line through evolution of accretion and the central star to investigate how gas giant frequency changes with stellar mass the snow line distance changes weakly with stellar mass thus giant planets form over a wide range of spectral types... | [['we', 'use', 'a', 'semianalytic', 'circumstellar', 'disk', 'model', 'that', 'considers', 'movement', 'of', 'the', 'snow', 'line', 'through', 'evolution', 'of', 'accretion', 'and', 'the', 'central', 'star', 'to', 'investigate', 'how', 'gas', 'giant', 'frequency', 'changes', 'with', 'stellar', 'mass', 'the', 'snow', 'l... | [-0.052767535199610784, 0.1730209914648107, 0.016790744361600704, 0.05047654790870313, -0.12988093405695897, -0.022687625414026635, 0.09260757221973367, 0.3737782629472869, -0.11925846899726561, -0.38095498288050295, 0.04940195593716843, -0.26774542428553105, -0.00743141917777913, 0.17217596941494515, -0.06848025462057... |
710.1066 | Detailed Examination of Transport Coefficients in Cubic-Plus-Quartic
Oscillator Chains | We examine the thermal conductivity and bulk viscosity of a one-dimensional
(1D) chain of particles with cubic-plus-quartic interparticle potentials and no
on-site potentials. This system is equivalent to the FPU-alpha beta system in a
subset of its parameter space. We identify three distinct frequency regimes
which ... | cond-mat.stat-mech | we examine the thermal conductivity and bulk viscosity of a onedimensional 1d chain of particles with cubicplusquartic interparticle potentials and no onsite potentials this system is equivalent to the fpualpha beta system in a subset of its parameter space we identify three distinct frequency regimes which we call the... | [['we', 'examine', 'the', 'thermal', 'conductivity', 'and', 'bulk', 'viscosity', 'of', 'a', 'onedimensional', '1d', 'chain', 'of', 'particles', 'with', 'cubicplusquartic', 'interparticle', 'potentials', 'and', 'no', 'onsite', 'potentials', 'this', 'system', 'is', 'equivalent', 'to', 'the', 'fpualpha', 'beta', 'system',... | [-0.1722987305473013, 0.23082087737939144, -0.0641919353665122, 0.017045635431774023, -0.058599800367893515, -0.12018045481902447, 0.051428023859721894, 0.3209359849656909, -0.27968569353900175, -0.2358736753375231, 0.05724919055038216, -0.27712343158662195, -0.06977733078582044, 0.21639770755548154, 0.0294409733600452... |
710.1067 | Magnetic-field fluctuations around the radio galaxy 3C 31 | We present an analysis of the magnetic-field fluctuations in the magnetoionic
medium in front of the radio galaxy 3C 31 derived from rotation-measure (RM)
fits to high-resolution polarization images. We first show that the Faraday
rotation must be due primarily to a foreground medium. We determine the RM
structure fu... | astro-ph | we present an analysis of the magneticfield fluctuations in the magnetoionic medium in front of the radio galaxy 3c 31 derived from rotationmeasure rm fits to highresolution polarization images we first show that the faraday rotation must be due primarily to a foreground medium we determine the rm structure functions f... | [['we', 'present', 'an', 'analysis', 'of', 'the', 'magneticfield', 'fluctuations', 'in', 'the', 'magnetoionic', 'medium', 'in', 'front', 'of', 'the', 'radio', 'galaxy', '3c', '31', 'derived', 'from', 'rotationmeasure', 'rm', 'fits', 'to', 'highresolution', 'polarization', 'images', 'we', 'first', 'show', 'that', 'the',... | [-0.11572372724310073, 0.10288021514208641, -0.0906196160831003, 0.05486671341599053, -0.06648746433739479, -0.02308830343441576, -0.04678243938505124, 0.4229289268453916, -0.23259700649282616, -0.2967123630273546, 0.0681778558362753, -0.25133169028494096, -0.04021067565513982, 0.1991454008887084, 0.021856176752983153,... |
710.1068 | Information and Entropy | What is information? Is it physical? We argue that in a Bayesian theory the
notion of information must be defined in terms of its effects on the beliefs of
rational agents. Information is whatever constrains rational beliefs and
therefore it is the force that induces us to change our minds. This problem of
updating f... | physics.data-an cond-mat.stat-mech gr-qc math.ST physics.gen-ph stat.TH | what is information is it physical we argue that in a bayesian theory the notion of information must be defined in terms of its effects on the beliefs of rational agents information is whatever constrains rational beliefs and therefore it is the force that induces us to change our minds this problem of updating from a ... | [['what', 'is', 'information', 'is', 'it', 'physical', 'we', 'argue', 'that', 'in', 'a', 'bayesian', 'theory', 'the', 'notion', 'of', 'information', 'must', 'be', 'defined', 'in', 'terms', 'of', 'its', 'effects', 'on', 'the', 'beliefs', 'of', 'rational', 'agents', 'information', 'is', 'whatever', 'constrains', 'rationa... | [-0.053043080801090096, 0.0656855816305324, -0.14744745024349973, 0.08585302380621469, -0.15387052243986968, -0.15790580309450972, 0.09158299621590549, 0.3425777685005478, -0.2972925529560767, -0.3053591086063534, 0.07986067991120319, -0.23943359485370863, -0.13684445424655148, 0.1678093947378139, -0.08186961276738276,... |
710.1069 | Separating baryons and dark matter in cluster cores: a full 2-D lensing
and dynamic analysis of Abell 383 and MS2137-23 | (abridged) We utilize existing imaging and spectroscopic data for the galaxy
clusters MS2137-23 and Abell 383 to present improved measures of the
distribution of dark and baryonic material in the clusters' central regions.
Our method, based on the combination of gravitational lensing and dynamical
data, is uniquely c... | astro-ph | abridged we utilize existing imaging and spectroscopic data for the galaxy clusters ms213723 and abell 383 to present improved measures of the distribution of dark and baryonic material in the clusters central regions our method based on the combination of gravitational lensing and dynamical data is uniquely capable of... | [['abridged', 'we', 'utilize', 'existing', 'imaging', 'and', 'spectroscopic', 'data', 'for', 'the', 'galaxy', 'clusters', 'ms213723', 'and', 'abell', '383', 'to', 'present', 'improved', 'measures', 'of', 'the', 'distribution', 'of', 'dark', 'and', 'baryonic', 'material', 'in', 'the', 'clusters', 'central', 'regions', '... | [-0.06316168384616543, 0.060411916500327074, -0.12815076934449113, 0.11894948396773769, -0.11807359461237746, -0.06568724157402821, -0.017407695130455935, 0.3865553052218971, -0.18878611245333918, -0.3934239049800871, 0.03188989273451834, -0.2944345349239381, -0.03364548407194245, 0.20068108144303212, 0.030643087150420... |
710.107 | Decays of mesons with charm quarks on the lattice | We investigate mesons containing charm quarks on fine lattices with a^{-1}
\sim 5 GeV. The quenched approximation is employed using the Wilson gauge
action at \beta = 6.6 and nonperturbatively O(a) improved Wilson quarks. We
present results for decay constants using various interpolating fields and give
preliminary r... | hep-lat | we investigate mesons containing charm quarks on fine lattices with a1 sim 5 gev the quenched approximation is employed using the wilson gauge action at beta 66 and nonperturbatively oa improved wilson quarks we present results for decay constants using various interpolating fields and give preliminary results for form... | [['we', 'investigate', 'mesons', 'containing', 'charm', 'quarks', 'on', 'fine', 'lattices', 'with', 'a1', 'sim', '5', 'gev', 'the', 'quenched', 'approximation', 'is', 'employed', 'using', 'the', 'wilson', 'gauge', 'action', 'at', 'beta', '66', 'and', 'nonperturbatively', 'oa', 'improved', 'wilson', 'quarks', 'we', 'pre... | [-0.04323963439868142, 0.358784989399525, -0.05080268003512174, 0.15549789683621687, -0.010859154467470943, -0.1544844696763903, 0.12261860295160053, 0.42010011076927184, -0.09598116766040524, -0.17834180480955789, -0.055432890349038644, -0.3495163641559581, 0.041507571710584064, 0.08054993759530286, 0.1219271751741568... |
710.1071 | From Information Geometry to Newtonian Dynamics | Newtonian dynamics is derived from prior information codified into an
appropriate statistical model. The basic assumption is that there is an
irreducible uncertainty in the location of particles so that the state of a
particle is defined by a probability distribution. The corresponding
configuration space is a statis... | physics.class-ph gr-qc nlin.CD physics.data-an | newtonian dynamics is derived from prior information codified into an appropriate statistical model the basic assumption is that there is an irreducible uncertainty in the location of particles so that the state of a particle is defined by a probability distribution the corresponding configuration space is a statistica... | [['newtonian', 'dynamics', 'is', 'derived', 'from', 'prior', 'information', 'codified', 'into', 'an', 'appropriate', 'statistical', 'model', 'the', 'basic', 'assumption', 'is', 'that', 'there', 'is', 'an', 'irreducible', 'uncertainty', 'in', 'the', 'location', 'of', 'particles', 'so', 'that', 'the', 'state', 'of', 'a',... | [-0.130549542269566, 0.15878881269398132, -0.15427135391130126, 0.08820564992007955, -0.06623288816060974, -0.08336046846751641, 0.01451671903648983, 0.31195201984761906, -0.3008692695261238, -0.332747900140627, 0.07460573499863837, -0.24966382990694708, -0.12265606541930335, 0.14555498155095847, -0.05371402739708881, ... |
710.1072 | Quadratic algebras related to elliptic curves | We construct quadratic finite-dimensional Poisson algebras and their quantum
versions related to rank N and degree one vector bundles over elliptic curves
with n marked points. The algebras are parameterized by the moduli of curves.
For N=2 and n=1 they coincide with the Sklyanin algebras. We prove that the
Poisson s... | nlin.SI | we construct quadratic finitedimensional poisson algebras and their quantum versions related to rank n and degree one vector bundles over elliptic curves with n marked points the algebras are parameterized by the moduli of curves for n2 and n1 they coincide with the sklyanin algebras we prove that the poisson structure... | [['we', 'construct', 'quadratic', 'finitedimensional', 'poisson', 'algebras', 'and', 'their', 'quantum', 'versions', 'related', 'to', 'rank', 'n', 'and', 'degree', 'one', 'vector', 'bundles', 'over', 'elliptic', 'curves', 'with', 'n', 'marked', 'points', 'the', 'algebras', 'are', 'parameterized', 'by', 'the', 'moduli',... | [-0.19551594890257779, 0.08626002050871823, -0.04089573427707829, 0.025092972768222952, -0.11025526051092496, -0.1302953071872446, -0.0219287103564637, 0.3568690630627122, -0.35687045951155905, -0.1962226976719784, 0.07541723236283089, -0.27013430553191203, -0.1720705494183076, 0.18631412534716915, -0.1200764382436396,... |
710.1073 | The Ratio of Helium- to Hydrogen-Atmosphere White Dwarfs: Direct
Evidence for Convective Mixing | We determine the ratio of helium- to hydrogen-atmosphere white dwarf stars as
a function of effective temperature from a model atmosphere analysis of the
infrared photometric data from the Two Micron All Sky Survey combined with
available visual magnitudes. Our study surpasses any previous analysis of this
kind both ... | astro-ph | we determine the ratio of helium to hydrogenatmosphere white dwarf stars as a function of effective temperature from a model atmosphere analysis of the infrared photometric data from the two micron all sky survey combined with available visual magnitudes our study surpasses any previous analysis of this kind both in te... | [['we', 'determine', 'the', 'ratio', 'of', 'helium', 'to', 'hydrogenatmosphere', 'white', 'dwarf', 'stars', 'as', 'a', 'function', 'of', 'effective', 'temperature', 'from', 'a', 'model', 'atmosphere', 'analysis', 'of', 'the', 'infrared', 'photometric', 'data', 'from', 'the', 'two', 'micron', 'all', 'sky', 'survey', 'co... | [-0.052293151525273016, 0.18369664066594657, -0.011165561452606526, 0.04016293727251876, -0.054748993424211564, -0.05122586902447794, 0.15481567233135657, 0.33092809979996035, -0.19751844997640955, -0.40087189253853267, 0.05791630914740304, -0.32834201880173863, -0.028426562362010518, 0.1851349124776091, -0.04135760934... |
710.1074 | Sums of hermitian squares and the BMV conjecture | Recently Lieb and Seiringer showed that the Bessis-Moussa-Villani conjecture
from quantum physics can be restated in the following purely algebraic way: The
sum of all words in two positive semidefinite matrices where the number of each
of the two letters is fixed is always a matrix with nonnegative trace. We show
th... | math.OA math.OC | recently lieb and seiringer showed that the bessismoussavillani conjecture from quantum physics can be restated in the following purely algebraic way the sum of all words in two positive semidefinite matrices where the number of each of the two letters is fixed is always a matrix with nonnegative trace we show that thi... | [['recently', 'lieb', 'and', 'seiringer', 'showed', 'that', 'the', 'bessismoussavillani', 'conjecture', 'from', 'quantum', 'physics', 'can', 'be', 'restated', 'in', 'the', 'following', 'purely', 'algebraic', 'way', 'the', 'sum', 'of', 'all', 'words', 'in', 'two', 'positive', 'semidefinite', 'matrices', 'where', 'the', ... | [-0.13910380390095917, 0.12082246114877106, -0.06688874971676077, 0.03674965523510375, -0.07716645443819121, -0.15683240958539243, -0.004261214652219574, 0.32793635346763234, -0.311029008053819, -0.24805313327086678, 0.13025417093823854, -0.3007778412580689, -0.16500804678515624, 0.16072694998223847, -0.070015645671266... |
710.1075 | Fine tuning of quantum operations performed via Raman transitions | A scheme for fine tuning of quantum operations to improve their performance
is proposed. A quantum system in $\Lambda$ configuration with two-photon Raman
transitions is considered without adiabatic elimination of the excited
(intermediate) state. Conditional dynamics of the system is studied with focus
on improving ... | quant-ph | a scheme for fine tuning of quantum operations to improve their performance is proposed a quantum system in lambda configuration with twophoton raman transitions is considered without adiabatic elimination of the excited intermediate state conditional dynamics of the system is studied with focus on improving fidelity o... | [['a', 'scheme', 'for', 'fine', 'tuning', 'of', 'quantum', 'operations', 'to', 'improve', 'their', 'performance', 'is', 'proposed', 'a', 'quantum', 'system', 'in', 'lambda', 'configuration', 'with', 'twophoton', 'raman', 'transitions', 'is', 'considered', 'without', 'adiabatic', 'elimination', 'of', 'the', 'excited', '... | [-0.17165043538610575, 0.21093137060472134, -0.056377057124974955, 0.029031259275302944, 0.0164087264640638, -0.1768318653182938, 0.06532821991162277, 0.39609243057406784, -0.23721600725037748, -0.26043607068979263, 0.05199934697093181, -0.24291474707506336, -0.07185337506234646, 0.23822209607586484, 0.0088461416539305... |
710.1076 | Electrically-Driven Reverse Overhauser Pumping of Nuclear Spins in
Quantum Dots | We propose a new mechanism for polarizing nuclear spins in quantum dots,
based on periodic modulation of the hyperfine coupling by electric driving at
the electron spin resonance frequency. Dynamical nuclear polarization results
from resonant excitation rather than hyperfine relaxation mediated by a thermal
bath, and... | cond-mat.mes-hall | we propose a new mechanism for polarizing nuclear spins in quantum dots based on periodic modulation of the hyperfine coupling by electric driving at the electron spin resonance frequency dynamical nuclear polarization results from resonant excitation rather than hyperfine relaxation mediated by a thermal bath and thus... | [['we', 'propose', 'a', 'new', 'mechanism', 'for', 'polarizing', 'nuclear', 'spins', 'in', 'quantum', 'dots', 'based', 'on', 'periodic', 'modulation', 'of', 'the', 'hyperfine', 'coupling', 'by', 'electric', 'driving', 'at', 'the', 'electron', 'spin', 'resonance', 'frequency', 'dynamical', 'nuclear', 'polarization', 're... | [-0.1581177516815673, 0.258255566787634, -0.03941486589198487, 0.05243588774774092, -0.04433366879707499, -0.16933184595411824, 0.039090862656341846, 0.4138415247465657, -0.2729268442114106, -0.29557575653018675, -0.02905617794434054, -0.2425627947716193, -0.04304325942823713, 0.22332634895512488, 0.05356265628397201, ... |
710.1077 | The conservation of energy-momentum and the mass for the graviton | In this work we give special attention to the bimetric theory of gravitation
with massive gravitons proposed by Visser in 1998. In his theory, a prior
background metric is necessary to take in account the massive term. Although in
the great part of the astrophysical studies the Minkowski metric is the best
choice to ... | gr-qc astro-ph | in this work we give special attention to the bimetric theory of gravitation with massive gravitons proposed by visser in 1998 in his theory a prior background metric is necessary to take in account the massive term although in the great part of the astrophysical studies the minkowski metric is the best choice to the b... | [['in', 'this', 'work', 'we', 'give', 'special', 'attention', 'to', 'the', 'bimetric', 'theory', 'of', 'gravitation', 'with', 'massive', 'gravitons', 'proposed', 'by', 'visser', 'in', '1998', 'in', 'his', 'theory', 'a', 'prior', 'background', 'metric', 'is', 'necessary', 'to', 'take', 'in', 'account', 'the', 'massive',... | [-0.12323183088560258, 0.06775147459745538, -0.09619295455502884, 0.10955473737972445, -0.1103734697509032, -0.06192775968549736, -0.008456739374348932, 0.3000843749434731, -0.18522316830282742, -0.2904120759425947, 0.05365820263587438, -0.2532008912542447, -0.16938361350209422, 0.12992999339616865, -0.1220982691348099... |
710.1078 | Polya's conjecture in the presence of a constant magnetic field | We consider the Dirichlet Laplacian with a constant magnetic field in a
two-dimensional domain of finite measure. We determine the sharp constants in
semi-classical eigenvalue estimates and show, in particular, that Polya's
conjecture is not true in the presence of a magnetic field.
| math-ph math.MP | we consider the dirichlet laplacian with a constant magnetic field in a twodimensional domain of finite measure we determine the sharp constants in semiclassical eigenvalue estimates and show in particular that polyas conjecture is not true in the presence of a magnetic field | [['we', 'consider', 'the', 'dirichlet', 'laplacian', 'with', 'a', 'constant', 'magnetic', 'field', 'in', 'a', 'twodimensional', 'domain', 'of', 'finite', 'measure', 'we', 'determine', 'the', 'sharp', 'constants', 'in', 'semiclassical', 'eigenvalue', 'estimates', 'and', 'show', 'in', 'particular', 'that', 'polyas', 'con... | [-0.16477411076274895, 0.11647153076130984, -0.04748785112399694, 0.06741439439843647, -0.0867089894708506, -0.09471273501295337, -0.0041062723585339475, 0.35757590193561345, -0.25862990904512795, -0.22725028128818023, 0.09973704954609275, -0.2323877553206457, -0.1474058463476425, 0.1514693700253617, -0.068699648235599... |
710.1079 | Disorder parameter for confinement and vacuum field strength correlators | The possibility is explored to relate confinement to properties of gauge
invariant field strength correlators.
| hep-lat | the possibility is explored to relate confinement to properties of gauge invariant field strength correlators | [['the', 'possibility', 'is', 'explored', 'to', 'relate', 'confinement', 'to', 'properties', 'of', 'gauge', 'invariant', 'field', 'strength', 'correlators']] | [-0.21523021658261618, 0.27359052635729314, -0.11801989749073982, 0.1453825488453731, -0.12803054489195348, -0.10503289625048637, -0.05929275328914325, 0.4201558407396078, -0.24587466617425283, -0.249921648701032, -0.03001816850155592, -0.15905156234900156, -0.11386768296360969, 0.07529623955488204, 0.01347082915405432... |
710.108 | A Dense Gas Trigger for OH Megamasers | HCN and CO line diagnostics provide new insight into the OH megamaser (OHM)
phenomenon, suggesting a dense gas trigger for OHMs. We identify three physical
properties that differentiate OHM hosts from other starburst galaxies: (1) OHMs
have the highest mean molecular gas densities among starburst galaxies; nearly
all... | astro-ph | hcn and co line diagnostics provide new insight into the oh megamaser ohm phenomenon suggesting a dense gas trigger for ohms we identify three physical properties that differentiate ohm hosts from other starburst galaxies 1 ohms have the highest mean molecular gas densities among starburst galaxies nearly all ohm hosts... | [['hcn', 'and', 'co', 'line', 'diagnostics', 'provide', 'new', 'insight', 'into', 'the', 'oh', 'megamaser', 'ohm', 'phenomenon', 'suggesting', 'a', 'dense', 'gas', 'trigger', 'for', 'ohms', 'we', 'identify', 'three', 'physical', 'properties', 'that', 'differentiate', 'ohm', 'hosts', 'from', 'other', 'starburst', 'galax... | [-0.11887122402608162, 0.1355416011962905, -0.0007803127719893543, 0.06874438028513308, -0.06599550990501875, -0.06818772141960072, 0.045404718068604126, 0.416466339644658, -0.12859724541465906, -0.3294172239822736, 0.018951458333763313, -0.29149865574132366, -0.010853091838309565, 0.15670237976152554, 0.01091045296300... |
710.1081 | Confinement effects in a guided-wave interferometer with
millimeter-scale arm separation | Guided-wave atom interferometers measure interference effects using atoms
held in a confining potential. In one common implementation, the confinement is
primarily two-dimensional, and the atoms move along the nearly free dimension
under the influence of an off-resonant standing wave laser beam. In this
configuration... | physics.atom-ph | guidedwave atom interferometers measure interference effects using atoms held in a confining potential in one common implementation the confinement is primarily twodimensional and the atoms move along the nearly free dimension under the influence of an offresonant standing wave laser beam in this configuration residual... | [['guidedwave', 'atom', 'interferometers', 'measure', 'interference', 'effects', 'using', 'atoms', 'held', 'in', 'a', 'confining', 'potential', 'in', 'one', 'common', 'implementation', 'the', 'confinement', 'is', 'primarily', 'twodimensional', 'and', 'the', 'atoms', 'move', 'along', 'the', 'nearly', 'free', 'dimension'... | [-0.14132499165057916, 0.22968513915168987, -0.051525869658929115, -0.02620242430834639, 0.02333586763186184, -0.151208356747367, 0.07129074667088724, 0.4654967396912214, -0.26941239990686117, -0.3093981830109107, 0.056963710688777563, -0.24995909552212411, -0.06561492921135045, 0.16019985360387518, -0.0099128894170893... |
710.1082 | Spectroscopic Determination of the Faint End of the Luminosity Function
in the Nearby Galaxy Clusters A2199 and Virgo | We report a new determination of the faint end of the galaxy luminosity
function in the nearby clusters Virgo and Abell 2199 using data from SDSS and
the Hectospec multifiber spectrograph on the MMT. The luminosity function of
A2199 is consistent with a single Schechter function to M_r=-15.6 + 5 log h_70
with a faint... | astro-ph | we report a new determination of the faint end of the galaxy luminosity function in the nearby clusters virgo and abell 2199 using data from sdss and the hectospec multifiber spectrograph on the mmt the luminosity function of a2199 is consistent with a single schechter function to m_r156 5 log h_70 with a faintend slop... | [['we', 'report', 'a', 'new', 'determination', 'of', 'the', 'faint', 'end', 'of', 'the', 'galaxy', 'luminosity', 'function', 'in', 'the', 'nearby', 'clusters', 'virgo', 'and', 'abell', '2199', 'using', 'data', 'from', 'sdss', 'and', 'the', 'hectospec', 'multifiber', 'spectrograph', 'on', 'the', 'mmt', 'the', 'luminosit... | [-0.02728461421554117, 0.05785894848100127, -0.13830819253524826, 0.11284014154874111, -0.13019443479245402, -0.03591259070523253, 0.06252854000553744, 0.4931137530498853, -0.051658043080779245, -0.36763034023973906, 0.008761213635749367, -0.33483237951470873, -0.04207482706376917, 0.22296120816592943, -0.0977326736925... |
710.1083 | Quantum fields, non-locality and quantum group symmetries | We study the action of space-time symmetries on quantum fields in the
presence of small departures from locality determined by dynamical gravity. It
is shown that, under such relaxation of locality, the symmetries of the theory
cannot be described within the usual framework of Lie algebras but rather in
terms of non-... | hep-th | we study the action of spacetime symmetries on quantum fields in the presence of small departures from locality determined by dynamical gravity it is shown that under such relaxation of locality the symmetries of the theory cannot be described within the usual framework of lie algebras but rather in terms of noncocommu... | [['we', 'study', 'the', 'action', 'of', 'spacetime', 'symmetries', 'on', 'quantum', 'fields', 'in', 'the', 'presence', 'of', 'small', 'departures', 'from', 'locality', 'determined', 'by', 'dynamical', 'gravity', 'it', 'is', 'shown', 'that', 'under', 'such', 'relaxation', 'of', 'locality', 'the', 'symmetries', 'of', 'th... | [-0.16228292875894113, 0.16694066589233053, -0.13508257346984465, 0.10877881590464053, -0.07575774964477335, -0.13791921832619533, -0.046532370055501815, 0.310595391667448, -0.28226596203499604, -0.27327730157204705, 0.05759361608319783, -0.20726688577061786, -0.16411837003085697, 0.1680587508744793, -0.110473397364590... |
710.1084 | Axial anomaly and magnetism of nuclear and quark matter | We consider the response of the QCD ground state at finite baryon density to
a strong magnetic field B. We point out the dominant role played by the
coupling of neutral Goldstone bosons, such as pi^0, to the magnetic field via
the axial triangle anomaly. We show that, in vacuum, above a value of B ~
m_pi^2/e, a metas... | hep-ph astro-ph nucl-th | we consider the response of the qcd ground state at finite baryon density to a strong magnetic field b we point out the dominant role played by the coupling of neutral goldstone bosons such as pi0 to the magnetic field via the axial triangle anomaly we show that in vacuum above a value of b m_pi2e a metastable object a... | [['we', 'consider', 'the', 'response', 'of', 'the', 'qcd', 'ground', 'state', 'at', 'finite', 'baryon', 'density', 'to', 'a', 'strong', 'magnetic', 'field', 'b', 'we', 'point', 'out', 'the', 'dominant', 'role', 'played', 'by', 'the', 'coupling', 'of', 'neutral', 'goldstone', 'bosons', 'such', 'as', 'pi0', 'to', 'the', ... | [-0.18278981174624181, 0.2463812083643126, -0.06610453616686802, 0.06067806233308817, -0.08153738988391859, -0.06226667472357421, 0.0668555204511473, 0.3323357739338749, -0.21645796540481235, -0.26538819323636986, 0.0471314855146614, -0.25261731494806317, -0.02861010489133677, 0.08718072248157113, 0.06370556664800173, ... |
710.1085 | One Dimensional Locally Connected S-spaces | We construct, assuming Jensen's principle diamond, a one-dimensional locally
connected hereditarily separable continuum without convergent sequences. The
construction is an inverse limit in omega_1 steps, and is patterned after the
original Fedorchuk construction of a compact S-space. To make it
one-dimensional, each... | math.GN | we construct assuming jensens principle diamond a onedimensional locally connected hereditarily separable continuum without convergent sequences the construction is an inverse limit in omega_1 steps and is patterned after the original fedorchuk construction of a compact sspace to make it onedimensional each space in th... | [['we', 'construct', 'assuming', 'jensens', 'principle', 'diamond', 'a', 'onedimensional', 'locally', 'connected', 'hereditarily', 'separable', 'continuum', 'without', 'convergent', 'sequences', 'the', 'construction', 'is', 'an', 'inverse', 'limit', 'in', 'omega_1', 'steps', 'and', 'is', 'patterned', 'after', 'the', 'o... | [-0.1003399316255969, 0.15548838894729097, -0.09132587232764948, 0.08832896138429297, -0.0883898437368097, -0.1370104303824957, 0.048462556693940076, 0.4234509054157469, -0.305963354944079, -0.12288881943526643, 0.15776602417247854, -0.2688987078835015, -0.09521551235121917, 0.17830737868401533, -0.12364788695790425, 0... |
710.1086 | Comment on "Nonexponential Decay Via Tunneling in Tight-Binding Lattices
and the Optical Zeno Effect" | S. Longhi [1] studied the survival probability P(t) of an unstable state
coupled to a tight-binding lattice finding an exact analytical solution that
describes the nonexponential decay. When the first coupling is smaller than the
others, he shows that P(t) has a natural decomposition into two terms; one is
the expone... | quant-ph | s longhi 1 studied the survival probability pt of an unstable state coupled to a tightbinding lattice finding an exact analytical solution that describes the nonexponential decay when the first coupling is smaller than the others he shows that pt has a natural decomposition into two terms one is the exponential decay c... | [['s', 'longhi', '1', 'studied', 'the', 'survival', 'probability', 'pt', 'of', 'an', 'unstable', 'state', 'coupled', 'to', 'a', 'tightbinding', 'lattice', 'finding', 'an', 'exact', 'analytical', 'solution', 'that', 'describes', 'the', 'nonexponential', 'decay', 'when', 'the', 'first', 'coupling', 'is', 'smaller', 'than... | [-0.16101612224347062, 0.12902071150640645, -0.08594119475947486, 0.0665736911818385, -0.055770776640209886, -0.14239898523315786, 0.06525483278764618, 0.3155548657476902, -0.24969780871023733, -0.2576587374177244, 0.07073826321555922, -0.271709662684136, -0.1158121014924513, 0.16312847540817327, -0.0025425051194098262... |
710.1087 | $Z^{'0}Z^{'0}$, $K^{+}K^{-}$ and $K^{0}\bar{K}^{0}$ boson production
with definite helicity amplitudes through $e^{+}e^{-}$ collisions in the
3-3-1 models without exotic electric charges | A detailed analysis of $Z^{'0}Z^{'0}$, $K^{+}K^{-}$ and $K^{0}\bar{K}^{0}$
pair production in $e^{+}e^{-}$ collisions is presented by using helicity
amplitudes. The trilinear bosons couplings in the $SU(3)_{C}\otimes
SU(3)_{L}\otimes U(1)_{X}$ models without exotic electric charges are also
calculated. We carry out t... | hep-ph | a detailed analysis of z0z0 kk and k0bark0 pair production in ee collisions is presented by using helicity amplitudes the trilinear bosons couplings in the su3_cotimes su3_lotimes u1_x models without exotic electric charges are also calculated we carry out the mentioned analysis for two models one of them is a one fami... | [['a', 'detailed', 'analysis', 'of', 'z0z0', 'kk', 'and', 'k0bark0', 'pair', 'production', 'in', 'ee', 'collisions', 'is', 'presented', 'by', 'using', 'helicity', 'amplitudes', 'the', 'trilinear', 'bosons', 'couplings', 'in', 'the', 'su3_cotimes', 'su3_lotimes', 'u1_x', 'models', 'without', 'exotic', 'electric', 'charg... | [-0.13132201954572192, 0.20119064673165285, -0.07713710889220238, 0.14246645090996377, -0.057028206040887465, -0.18445668588467543, 0.019742939837141742, 0.36107921798623377, -0.210107950726524, -0.25512059737417486, 0.013256297581979343, -0.3521557479097898, -0.03286721321543859, 0.15399828292673542, 0.066593216559399... |
710.1088 | Effect of Landau Level Mixing on Braiding Statistics | We examine the effect of Landau level mixing on the braiding statistics of
quasiparticles of abelian and nonabelian quantum Hall states. While path
dependent geometric phases can perturb the abelian part of the statistics, we
find that the nonabelian properties remain unchanged to an accuracy that is
exponentially sm... | cond-mat.mes-hall cond-mat.str-el | we examine the effect of landau level mixing on the braiding statistics of quasiparticles of abelian and nonabelian quantum hall states while path dependent geometric phases can perturb the abelian part of the statistics we find that the nonabelian properties remain unchanged to an accuracy that is exponentially small ... | [['we', 'examine', 'the', 'effect', 'of', 'landau', 'level', 'mixing', 'on', 'the', 'braiding', 'statistics', 'of', 'quasiparticles', 'of', 'abelian', 'and', 'nonabelian', 'quantum', 'hall', 'states', 'while', 'path', 'dependent', 'geometric', 'phases', 'can', 'perturb', 'the', 'abelian', 'part', 'of', 'the', 'statisti... | [-0.2006792583571816, 0.3407183903793878, -0.10666659802060437, 0.09712933641384114, -0.05393505794927478, -0.08722676271227775, 0.08260890511640658, 0.3359381512359337, -0.28055232928858864, -0.2783509262458042, 0.00280970267528944, -0.26090353796327553, -0.12355570067410115, 0.14477501573317028, -0.0718373172675018, ... |
710.1089 | Eigenvalue estimates for the Aharonov-Bohm operator in a domain | We prove semi-classical estimates on moments of eigenvalues of the
Aharonov-Bohm operator in bounded two-dimensional domains. Moreover, we present
a counterexample to the generalized diamagnetic inequality which was proposed
by Erdos, Loss and Vougalter. Numerical studies complement these results.
| math-ph math.MP | we prove semiclassical estimates on moments of eigenvalues of the aharonovbohm operator in bounded twodimensional domains moreover we present a counterexample to the generalized diamagnetic inequality which was proposed by erdos loss and vougalter numerical studies complement these results | [['we', 'prove', 'semiclassical', 'estimates', 'on', 'moments', 'of', 'eigenvalues', 'of', 'the', 'aharonovbohm', 'operator', 'in', 'bounded', 'twodimensional', 'domains', 'moreover', 'we', 'present', 'a', 'counterexample', 'to', 'the', 'generalized', 'diamagnetic', 'inequality', 'which', 'was', 'proposed', 'by', 'erdo... | [-0.12155968867438405, 0.05366244722206734, -0.06233265255822947, 0.08041301011843116, -0.07528622968024329, -0.10612912379254244, 0.030448706544886687, 0.3284169481577058, -0.23355269887925764, -0.22169975882494136, 0.07194874777250286, -0.35430577311566785, -0.2140699738244477, 0.20791796928173617, -0.126353851053863... |
710.109 | Vortex lattices of bosons in deep rotating optical lattices | We study vortex-lattice phases for a Bose gas trapped in a rotating
optical-lattice near the superfluid--Mott-insulator transition. We find a
series of abrupt structural phase transitions where vortices are pinned with
their cores only on plaquettes or only on sites. We discuss connections between
these vortex struct... | cond-mat.other | we study vortexlattice phases for a bose gas trapped in a rotating opticallattice near the superfluidmottinsulator transition we find a series of abrupt structural phase transitions where vortices are pinned with their cores only on plaquettes or only on sites we discuss connections between these vortex structures and ... | [['we', 'study', 'vortexlattice', 'phases', 'for', 'a', 'bose', 'gas', 'trapped', 'in', 'a', 'rotating', 'opticallattice', 'near', 'the', 'superfluidmottinsulator', 'transition', 'we', 'find', 'a', 'series', 'of', 'abrupt', 'structural', 'phase', 'transitions', 'where', 'vortices', 'are', 'pinned', 'with', 'their', 'co... | [-0.2190876095646045, 0.2655834704155809, -0.016347969263984727, 0.025429592371500772, 0.011053360757771236, -0.13112236214159378, 0.12324131093919277, 0.4329007358515057, -0.18948241780865296, -0.21546486195514042, 0.07784351601128883, -0.33610686671053025, -0.11163461878333755, 0.10396410325333348, 0.0772908134365871... |
710.1091 | Spin Glass Theory: numerical and experimental results in
three-dimensional systems | Here I will review the theoretical results that have been obtained for spin
glasses. I will concentrate my attention on the predictions of the mean field
approach in three dimensional systems and on its numerical and experimental
verifications.
| cond-mat.dis-nn cond-mat.soft | here i will review the theoretical results that have been obtained for spin glasses i will concentrate my attention on the predictions of the mean field approach in three dimensional systems and on its numerical and experimental verifications | [['here', 'i', 'will', 'review', 'the', 'theoretical', 'results', 'that', 'have', 'been', 'obtained', 'for', 'spin', 'glasses', 'i', 'will', 'concentrate', 'my', 'attention', 'on', 'the', 'predictions', 'of', 'the', 'mean', 'field', 'approach', 'in', 'three', 'dimensional', 'systems', 'and', 'on', 'its', 'numerical', '... | [-0.07182361713708624, 0.1026257571249612, -0.09834954912137044, 0.0015924716196758183, -0.055669301924736875, -0.12031884475513116, -0.004676560577201216, 0.44244065214144557, -0.1343743837389507, -0.2301041222128429, 0.15578715577660324, -0.32691351525289447, -0.1682807623874396, 0.24607550436140677, -0.0469379662168... |
710.1092 | Testing LCDM with the Growth Function \delta(a): Current Constraints | We have compiled a dataset consisting of 22 datapoints at a redshift range
(0.15,3.8) which can be used to constrain the linear perturbation growth rate
f=\frac{d\ln\delta}{d\ln a}. Five of these data-points constrain directly the
growth rate f through either redshift distortions or change of the power
spectrum with ... | astro-ph gr-qc hep-ph | we have compiled a dataset consisting of 22 datapoints at a redshift range 01538 which can be used to constrain the linear perturbation growth rate ffracdlndeltadln a five of these datapoints constrain directly the growth rate f through either redshift distortions or change of the power spectrum with redshift the rest ... | [['we', 'have', 'compiled', 'a', 'dataset', 'consisting', 'of', '22', 'datapoints', 'at', 'a', 'redshift', 'range', '01538', 'which', 'can', 'be', 'used', 'to', 'constrain', 'the', 'linear', 'perturbation', 'growth', 'rate', 'ffracdlndeltadln', 'a', 'five', 'of', 'these', 'datapoints', 'constrain', 'directly', 'the', '... | [-0.05247575081747902, 0.06460255690352128, -0.10124983445686453, 0.05989660905016696, -0.10851776139701114, -0.07846594129634255, 0.0483710808754789, 0.31566016636788846, -0.22396611455718385, -0.33777201257043465, 0.07809664679704892, -0.2747663097072612, -0.03224643113447682, 0.2168675334274988, -0.01785794257268528... |
710.1093 | On the Design and Optimization of a Quantum Polynomial-Time Attack on
Elliptic Curve Cryptography | We consider a quantum polynomial-time algorithm which solves the discrete
logarithm problem for points on elliptic curves over $GF(2^m)$. We improve over
earlier algorithms by constructing an efficient circuit for multiplying
elements of binary finite fields and by representing elliptic curve points
using a technique... | quant-ph | we consider a quantum polynomialtime algorithm which solves the discrete logarithm problem for points on elliptic curves over gf2m we improve over earlier algorithms by constructing an efficient circuit for multiplying elements of binary finite fields and by representing elliptic curve points using a technique based on... | [['we', 'consider', 'a', 'quantum', 'polynomialtime', 'algorithm', 'which', 'solves', 'the', 'discrete', 'logarithm', 'problem', 'for', 'points', 'on', 'elliptic', 'curves', 'over', 'gf2m', 'we', 'improve', 'over', 'earlier', 'algorithms', 'by', 'constructing', 'an', 'efficient', 'circuit', 'for', 'multiplying', 'eleme... | [-0.1722807558835484, -0.007424575709956116, -0.06899922044249251, 0.00345347159600351, -0.07625499030109495, -0.17765667036001104, 0.07567856268433389, 0.38656117068603635, -0.2634843664243817, -0.29303632661467416, 0.07523606986942469, -0.22539399553788825, -0.13673890532227234, 0.29195952534209935, -0.08316207553725... |
710.1094 | The supernova rate in local galaxy clusters | We report a measurement of the supernova (SN) rates (Ia and core-collapse) in
galaxy clusters based on the 136 SNe of the sample described in Cappellaro et
al. (1999) and Mannucci et al. (2005).
Early-type cluster galaxies show a type Ia SN rate (0.066 SNuM) similar to
that obtained by Sharon et al. (2007) and more... | astro-ph | we report a measurement of the supernova sn rates ia and corecollapse in galaxy clusters based on the 136 sne of the sample described in cappellaro et al 1999 and mannucci et al 2005 earlytype cluster galaxies show a type ia sn rate 0066 snum similar to that obtained by sharon et al 2007 and more than 3 times larger th... | [['we', 'report', 'a', 'measurement', 'of', 'the', 'supernova', 'sn', 'rates', 'ia', 'and', 'corecollapse', 'in', 'galaxy', 'clusters', 'based', 'on', 'the', '136', 'sne', 'of', 'the', 'sample', 'described', 'in', 'cappellaro', 'et', 'al', '1999', 'and', 'mannucci', 'et', 'al', '2005', 'earlytype', 'cluster', 'galaxies... | [-0.07233848575582137, 0.06983679338676355, -0.053947397989573, 0.10062474845567855, -0.0979847919513903, -0.03615668624094347, 0.10038694065041477, 0.3940327204400446, -0.14870249511356035, -0.33025411736310983, 0.027064691709422665, -0.2789008654154292, -0.06771979664179792, 0.22358033868325192, -0.06383084753619098,... |
710.1095 | Real Zeuthen numbers for two lines | Given three natural numbers $k,l,d$ such that $k+l=d(d+3)/2$, the Zeuthen
number $N_{d}(l)$ is the number of nonsingular complex algebraic curves of
degree $d$ passing through $k$ points and tangent to $l$ lines in $\PP^2$. It
does not depend on the generic configuration $C$ of points and lines chosen. If
the points ... | math.AG | given three natural numbers kld such that kldd32 the zeuthen number n_dl is the number of nonsingular complex algebraic curves of degree d passing through k points and tangent to l lines in pp2 it does not depend on the generic configuration c of points and lines chosen if the points and lines are real the correspondin... | [['given', 'three', 'natural', 'numbers', 'kld', 'such', 'that', 'kldd32', 'the', 'zeuthen', 'number', 'n_dl', 'is', 'the', 'number', 'of', 'nonsingular', 'complex', 'algebraic', 'curves', 'of', 'degree', 'd', 'passing', 'through', 'k', 'points', 'and', 'tangent', 'to', 'l', 'lines', 'in', 'pp2', 'it', 'does', 'not', '... | [-0.21837075049220359, 0.10112088334913935, -0.043103017446413205, 0.038029410729401754, -0.08384408621406815, -0.15705730350127498, 0.06638669728717396, 0.3438053474426993, -0.2642607254301677, -0.2500109843982076, 0.06526996254880271, -0.28535861608762186, -0.14246480222972271, 0.23084223327041575, -0.075241092334499... |
710.1096 | Multifrequency Observations of the Blazar 3C 279 in January 2006 | We report first results of a multifrequency campaign from radio to hard X-ray
energies of the prominent gamma-ray blazar 3C 279, which was organised around
an INTEGRAL ToO observation in January 2006, and triggered on its optical
state. The variable blazar was observed at an intermediate optical state, and a
well-cov... | astro-ph | we report first results of a multifrequency campaign from radio to hard xray energies of the prominent gammaray blazar 3c 279 which was organised around an integral too observation in january 2006 and triggered on its optical state the variable blazar was observed at an intermediate optical state and a wellcovered mult... | [['we', 'report', 'first', 'results', 'of', 'a', 'multifrequency', 'campaign', 'from', 'radio', 'to', 'hard', 'xray', 'energies', 'of', 'the', 'prominent', 'gammaray', 'blazar', '3c', '279', 'which', 'was', 'organised', 'around', 'an', 'integral', 'too', 'observation', 'in', 'january', '2006', 'and', 'triggered', 'on',... | [-0.05063461900780392, 0.09474834035315981, -0.09884961056788427, 0.11846022313723698, -0.09628226460860029, -0.0907603232238268, 0.0416057820774499, 0.500553101030965, -0.21252929922760286, -0.34086506806043765, 0.05505111134837869, -0.28168280324729766, -0.005735312364126889, 0.22403269510901982, -0.00604373700627236... |
710.1097 | Curious Variables Experiment (CURVE). CCD Photometry of V419 Lyr in its
2006 July Superoutburst | We report extensive photometry of the dwarf nova V419 Lyr throughout its 2006
July superoutburst till quiescence. The superoutburst with amplitude of ~3.5
magnitude lasted at least 15 days and was characterized by the presence of
clear superhumps with a mean period of Psh=0.089985(58) days (129.58+-0.08
min). Accordi... | astro-ph | we report extensive photometry of the dwarf nova v419 lyr throughout its 2006 july superoutburst till quiescence the superoutburst with amplitude of 35 magnitude lasted at least 15 days and was characterized by the presence of clear superhumps with a mean period of psh008998558 days 12958008 min according to the stolzs... | [['we', 'report', 'extensive', 'photometry', 'of', 'the', 'dwarf', 'nova', 'v419', 'lyr', 'throughout', 'its', '2006', 'july', 'superoutburst', 'till', 'quiescence', 'the', 'superoutburst', 'with', 'amplitude', 'of', '35', 'magnitude', 'lasted', 'at', 'least', '15', 'days', 'and', 'was', 'characterized', 'by', 'the', '... | [-0.13429945655632763, 0.1925569502520375, -0.13497785439404347, 0.007295054880281289, -0.06856895585233967, -0.1303901971100519, 0.11545861506989846, 0.3700149471809467, -0.2107125048529512, -0.35689366473505896, 0.12730621494663258, -0.3104958379858484, -0.095528725568826, 0.18890295236681898, -0.12654296570224688, -... |
710.1098 | Precise Photometry and Spectroscopy of Transits | A planetary transit produces both a photometric signal and a spectroscopic
signal. Precise observations of the transit light curve reveal the planetary
radius and allow a search for timing anomalies caused by satellites or
additional planets. Precise measurements of the stellar Doppler shift
throughout a transit (the... | astro-ph | a planetary transit produces both a photometric signal and a spectroscopic signal precise observations of the transit light curve reveal the planetary radius and allow a search for timing anomalies caused by satellites or additional planets precise measurements of the stellar doppler shift throughout a transit the ross... | [['a', 'planetary', 'transit', 'produces', 'both', 'a', 'photometric', 'signal', 'and', 'a', 'spectroscopic', 'signal', 'precise', 'observations', 'of', 'the', 'transit', 'light', 'curve', 'reveal', 'the', 'planetary', 'radius', 'and', 'allow', 'a', 'search', 'for', 'timing', 'anomalies', 'caused', 'by', 'satellites', ... | [-0.17367042726286316, 0.14756291681620223, -0.13823429035443452, 0.06215220743224465, -0.18393373611553382, -0.08726049683767781, 0.13556413540756831, 0.3096793607598351, -0.1740177297283725, -0.3749408505216081, 0.12275999522097009, -0.29117725704426084, -0.12845358730516626, 0.26062572609773405, -0.10421426604271576... |
710.1099 | Multi-Line Quiet Sun Spectro-Polarimetry at 5250 and 6302 \AA | The reliability of quiet Sun magnetic field diagnostics based on the
\ion{Fe}{1} lines at 6302 \AA has been questioned by recent work. We present
here the results of a thorough study of high-resolution multi-line observations
taken with the new spectro-polarimeter SPINOR, comprising the 5250 and 6302 \AA
spectral dom... | astro-ph | the reliability of quiet sun magnetic field diagnostics based on the ionfe1 lines at 6302 aa has been questioned by recent work we present here the results of a thorough study of highresolution multiline observations taken with the new spectropolarimeter spinor comprising the 5250 and 6302 aa spectral domains the obser... | [['the', 'reliability', 'of', 'quiet', 'sun', 'magnetic', 'field', 'diagnostics', 'based', 'on', 'the', 'ionfe1', 'lines', 'at', '6302', 'aa', 'has', 'been', 'questioned', 'by', 'recent', 'work', 'we', 'present', 'here', 'the', 'results', 'of', 'a', 'thorough', 'study', 'of', 'highresolution', 'multiline', 'observation... | [-0.0648908696561821, 0.052203099755364246, -0.04181905733011931, 0.06567570311480936, -0.06557220388286278, -0.15249950247734323, 0.020518403901075698, 0.4665094838205692, -0.15636258719456012, -0.3305820607563761, 0.0714897941339522, -0.23349821561766146, -0.038842785282398415, 0.176209828116317, -0.00617971509036900... |
710.11 | $R$-Parity in Supersymmetric Left-Right Models | On this article we show explicity that Supersymmetric Left-Right Models
already satisfy the R-parity. They also respect $L$-parity and $B$-parity.
| hep-ph | on this article we show explicity that supersymmetric leftright models already satisfy the rparity they also respect lparity and bparity | [['on', 'this', 'article', 'we', 'show', 'explicity', 'that', 'supersymmetric', 'leftright', 'models', 'already', 'satisfy', 'the', 'rparity', 'they', 'also', 'respect', 'lparity', 'and', 'bparity']] | [-0.04726408468559384, 0.13702962826937437, -0.0300244902803873, 0.2309882723299476, -0.0991747769423657, -0.17638564409895074, -0.04932971900133351, 0.41371608815259403, -0.1922704523636235, -0.23200713655872582, 0.1327815739205107, -0.26527811648945016, -0.1934395618736744, 0.127129503318833, -0.12261085419191255, 0.... |
710.1101 | Deuteron spin structure functions in the resonance and DIS regions | We derive relations between spin-dependent nuclear and nucleon g_1 and g_2
structure functions within the nuclear impulse approximation, which are valid
at all Q^2, and in both the resonance and deep inelastic regions. We apply the
formalism to the specific case of the deuteron, which is often used as a source
of neu... | nucl-th hep-ph nucl-ex | we derive relations between spindependent nuclear and nucleon g_1 and g_2 structure functions within the nuclear impulse approximation which are valid at all q2 and in both the resonance and deep inelastic regions we apply the formalism to the specific case of the deuteron which is often used as a source of neutron str... | [['we', 'derive', 'relations', 'between', 'spindependent', 'nuclear', 'and', 'nucleon', 'g_1', 'and', 'g_2', 'structure', 'functions', 'within', 'the', 'nuclear', 'impulse', 'approximation', 'which', 'are', 'valid', 'at', 'all', 'q2', 'and', 'in', 'both', 'the', 'resonance', 'and', 'deep', 'inelastic', 'regions', 'we',... | [-0.020020603529504827, 0.10105198639369495, -0.08796519700538467, 0.19169572518817526, -0.03887932689080166, -0.055694898760348964, 0.03313722536974662, 0.39107317527806434, -0.2163837061081132, -0.2636332218472317, 0.03451632858549773, -0.27869219251128063, -0.0543275055903438, 0.17571799408933902, 0.1018615543961877... |
710.1102 | Multiplicative Conservation of Baryon Number and Baryogenesis | In the canonical seesaw mechanism of neutrino mass, lepton number is only
multiplicatively conserved, which enables the important phenomenon of
leptogenesis to occur, as an attractive explanation of the present baryon
asymmetry of the Universe. A parallel possibility, hitherto unrecognized, also
holds for baryon numb... | hep-ph | in the canonical seesaw mechanism of neutrino mass lepton number is only multiplicatively conserved which enables the important phenomenon of leptogenesis to occur as an attractive explanation of the present baryon asymmetry of the universe a parallel possibility hitherto unrecognized also holds for baryon number and b... | [['in', 'the', 'canonical', 'seesaw', 'mechanism', 'of', 'neutrino', 'mass', 'lepton', 'number', 'is', 'only', 'multiplicatively', 'conserved', 'which', 'enables', 'the', 'important', 'phenomenon', 'of', 'leptogenesis', 'to', 'occur', 'as', 'an', 'attractive', 'explanation', 'of', 'the', 'present', 'baryon', 'asymmetry... | [-0.11373958073440008, 0.2388129770688829, -0.0416378540545702, 0.18739310074597598, -0.1368567699752748, -0.16805368838366122, 0.028882097601890564, 0.2899983011116274, -0.20318910935893655, -0.3226345597149339, 0.010491120838560164, -0.20026662619318814, -0.08868041966110468, 0.13622327451012098, -0.00754707307554781... |
710.1103 | The Newton polygon of a rational plane curve | The Newton polygon of the implicit equation of a rational plane curve is
explicitly determined by the multiplicities of any of its parametrizations. We
give an intersection-theoretical proof of this fact based on a refinement of
the Kushnirenko-Bernstein theorem. We apply this result to the determination of
the Newto... | math.AG math.CO | the newton polygon of the implicit equation of a rational plane curve is explicitly determined by the multiplicities of any of its parametrizations we give an intersectiontheoretical proof of this fact based on a refinement of the kushnirenkobernstein theorem we apply this result to the determination of the newton poly... | [['the', 'newton', 'polygon', 'of', 'the', 'implicit', 'equation', 'of', 'a', 'rational', 'plane', 'curve', 'is', 'explicitly', 'determined', 'by', 'the', 'multiplicities', 'of', 'any', 'of', 'its', 'parametrizations', 'we', 'give', 'an', 'intersectiontheoretical', 'proof', 'of', 'this', 'fact', 'based', 'on', 'a', 're... | [-0.1798013375253878, 0.001012762908515886, -0.17506851596218126, 0.019438515548925048, -0.13780997652847704, -0.15313613870851348, 0.06537021324038506, 0.29928987865797546, -0.3157131953391238, -0.20090346059666198, 0.09983592784624094, -0.22305373815932772, -0.20038335896793438, 0.23294095586545802, -0.14175823221209... |
710.1104 | Smooth Volume Rigidity for Manifolds with Negatively Curved Targets | We establish conditions for a continuous map of nonzero degree between a
smooth closed manifold and a negatively curved manifold of dimension greater
than four to be homotopic to a smooth cover, and in particular a diffeomorphism
when the degree is one. The conditions hold when the volumes or entropy-volumes
of the t... | math.DG math.GT | we establish conditions for a continuous map of nonzero degree between a smooth closed manifold and a negatively curved manifold of dimension greater than four to be homotopic to a smooth cover and in particular a diffeomorphism when the degree is one the conditions hold when the volumes or entropyvolumes of the two ma... | [['we', 'establish', 'conditions', 'for', 'a', 'continuous', 'map', 'of', 'nonzero', 'degree', 'between', 'a', 'smooth', 'closed', 'manifold', 'and', 'a', 'negatively', 'curved', 'manifold', 'of', 'dimension', 'greater', 'than', 'four', 'to', 'be', 'homotopic', 'to', 'a', 'smooth', 'cover', 'and', 'in', 'particular', '... | [-0.1461776501829411, 0.1281289928499677, -0.07296623038886071, 0.09430742429076629, -0.05130274236462144, -0.16349143106598668, -0.010398370706541248, 0.37656039402408653, -0.23157521343768336, -0.2520730316904265, 0.11880506661471499, -0.244545774545174, -0.1357913296534355, 0.226037718476132, -0.11547458920151342, -... |
710.1105 | Fractal and Multifractal Scaling of Electrical Conduction in Random
Resistor Networks | This article is a mini-review about electrical current flows in networks from
the perspective of statistical physics. We briefly discuss analytical methods
to solve the conductance of an arbitrary resistor network. We then turn to
basic results related to percolation: namely, the conduction properties of a
large rand... | cond-mat.stat-mech cond-mat.dis-nn physics.class-ph | this article is a minireview about electrical current flows in networks from the perspective of statistical physics we briefly discuss analytical methods to solve the conductance of an arbitrary resistor network we then turn to basic results related to percolation namely the conduction properties of a large random resi... | [['this', 'article', 'is', 'a', 'minireview', 'about', 'electrical', 'current', 'flows', 'in', 'networks', 'from', 'the', 'perspective', 'of', 'statistical', 'physics', 'we', 'briefly', 'discuss', 'analytical', 'methods', 'to', 'solve', 'the', 'conductance', 'of', 'an', 'arbitrary', 'resistor', 'network', 'we', 'then',... | [-0.13931384648354392, 0.13546420510456733, -0.060227711797259484, 0.05522614820663529, -0.03809448550704734, -0.1279992167727046, 0.08257078214470918, 0.3745434953986357, -0.3015308961372024, -0.22676375058758172, 0.09228856764994339, -0.303313683958203, -0.23031637124395707, 0.18465139506761694, -0.04581328429048881,... |
710.1106 | The phase structure of a chirally invariant lattice Higgs-Yukawa model | We consider a chirally invariant lattice Higgs-Yukawa model based on the
Neuberger overlap operator. As a first step towards the eventual determination
of Higgs mass bounds we present the phase structure of the model analytically
in the large Nf-limit in the physically interesting region of the Yukawa
coupling consta... | hep-lat | we consider a chirally invariant lattice higgsyukawa model based on the neuberger overlap operator as a first step towards the eventual determination of higgs mass bounds we present the phase structure of the model analytically in the large nflimit in the physically interesting region of the yukawa coupling constant we... | [['we', 'consider', 'a', 'chirally', 'invariant', 'lattice', 'higgsyukawa', 'model', 'based', 'on', 'the', 'neuberger', 'overlap', 'operator', 'as', 'a', 'first', 'step', 'towards', 'the', 'eventual', 'determination', 'of', 'higgs', 'mass', 'bounds', 'we', 'present', 'the', 'phase', 'structure', 'of', 'the', 'model', '... | [-0.14885168193972537, 0.13729297049091352, -0.08593954693614728, 0.08488949739507266, -0.02811130504789097, -0.1250111918674693, 0.11198643620591611, 0.34447359335387034, -0.16195707071483845, -0.3044519386830784, 0.06996509052835227, -0.2540207634790845, -0.12721333289075465, 0.14250201452079983, 0.031826335842041385... |
710.1107 | On the Long Time Behavior of Second Order Differential Equations with
Asymptotically Small Dissipation | We investigate the time-asymptotic properties of solutions of the
differential equation x''(t) + a(t)x'(t) + g(x(t)) = 0 in a Hilbert space,
where a(.) is non-increasing and g is the gradient of a potential G. If the
coefficient a(.) is constant and positive, we recover the so-called ``Heavy
Ball with Friction'' syst... | math.CA math.DS | we investigate the timeasymptotic properties of solutions of the differential equation xt atxt gxt 0 in a hilbert space where a is nonincreasing and g is the gradient of a potential g if the coefficient a is constant and positive we recover the socalled heavy ball with friction system on the other hand when at1t1 we ob... | [['we', 'investigate', 'the', 'timeasymptotic', 'properties', 'of', 'solutions', 'of', 'the', 'differential', 'equation', 'xt', 'atxt', 'gxt', '0', 'in', 'a', 'hilbert', 'space', 'where', 'a', 'is', 'nonincreasing', 'and', 'g', 'is', 'the', 'gradient', 'of', 'a', 'potential', 'g', 'if', 'the', 'coefficient', 'a', 'is',... | [-0.1625976966384024, 0.0652806133491896, -0.11966283166646419, 0.05642678076962391, -0.05562173663386065, -0.12423418573642442, 0.02782356629080801, 0.318644399627067, -0.28832606472501376, -0.220915300636945, 0.13713136461355824, -0.3044094247350761, -0.12567305289551123, 0.17498779196449252, -0.05012227048401732, 0.... |
710.1108 | Precision of diffuse 21-cm lensing | We study the limits of accuracy for weak lensing maps of dark matter using
diffuse 21-cm radiation from the pre-reionization epoch using simulations. We
improve on previous "optimal" quadratic lensing estimators by using shear and
convergence instead of deflection angles. We find that non-Gaussianity provides
a limit... | astro-ph | we study the limits of accuracy for weak lensing maps of dark matter using diffuse 21cm radiation from the prereionization epoch using simulations we improve on previous optimal quadratic lensing estimators by using shear and convergence instead of deflection angles we find that nongaussianity provides a limit to the a... | [['we', 'study', 'the', 'limits', 'of', 'accuracy', 'for', 'weak', 'lensing', 'maps', 'of', 'dark', 'matter', 'using', 'diffuse', '21cm', 'radiation', 'from', 'the', 'prereionization', 'epoch', 'using', 'simulations', 'we', 'improve', 'on', 'previous', 'optimal', 'quadratic', 'lensing', 'estimators', 'by', 'using', 'sh... | [-0.07173804443883748, 0.017065558251578454, -0.08324181473975585, 0.11056586426744346, -0.08737852607568926, -0.12859423438949155, 0.04015290562048062, 0.3620147748796408, -0.22456934954201388, -0.30910381575861623, 0.06099671710278716, -0.2973511470425229, -0.057551605542275036, 0.23297506974325016, -0.00328631842632... |
710.1109 | Rough Isometries of Lipschitz Function Spaces | We show that rough isometries between metric spaces X, Y can be lifted to the
spaces of real valued 1-Lipschitz functions over X and Y with supremum metric
and apply this to their scaling limits. For the inverse, we show how rough
isometries between X and Y can be reconstructed from structurally enriched
rough isomet... | math.MG | we show that rough isometries between metric spaces x y can be lifted to the spaces of real valued 1lipschitz functions over x and y with supremum metric and apply this to their scaling limits for the inverse we show how rough isometries between x and y can be reconstructed from structurally enriched rough isometries b... | [['we', 'show', 'that', 'rough', 'isometries', 'between', 'metric', 'spaces', 'x', 'y', 'can', 'be', 'lifted', 'to', 'the', 'spaces', 'of', 'real', 'valued', '1lipschitz', 'functions', 'over', 'x', 'and', 'y', 'with', 'supremum', 'metric', 'and', 'apply', 'this', 'to', 'their', 'scaling', 'limits', 'for', 'the', 'inver... | [-0.0751917550029854, 0.1476868279511109, -0.11122069085637729, 0.1269815084815491, -0.08530775814627607, -0.0672344444009165, 0.04692255702490608, 0.5158265346040328, -0.43274352069323263, -0.21625680380966514, 0.0464084857609123, -0.31938047758303584, -0.14033765690401195, 0.18647092316144456, -0.1576643031400939, 0.... |
710.111 | Analysis of cosmic microwave background radiation in the presence of
Lorentz violation | We examine the effects Lorentz violation on observations of cosmic microwave
background radiation. In particular, we focus on changes in polarization caused
by vacuum birefringence. We place stringent constraints on previously untested
violations.
| astro-ph | we examine the effects lorentz violation on observations of cosmic microwave background radiation in particular we focus on changes in polarization caused by vacuum birefringence we place stringent constraints on previously untested violations | [['we', 'examine', 'the', 'effects', 'lorentz', 'violation', 'on', 'observations', 'of', 'cosmic', 'microwave', 'background', 'radiation', 'in', 'particular', 'we', 'focus', 'on', 'changes', 'in', 'polarization', 'caused', 'by', 'vacuum', 'birefringence', 'we', 'place', 'stringent', 'constraints', 'on', 'previously', '... | [-0.19307400351108023, 0.18351065728700522, 0.006783068151862332, 0.11475801355007922, -0.15259699523448944, -0.04285502896615953, 0.08494942525937928, 0.3409589226498748, -0.12457703051129074, -0.3370110283351757, 0.06404285386176498, -0.27630487185987557, -0.06991998732767322, 0.21756093395930348, -0.0444287632196915... |
710.1111 | B -> D* l nu with 2+1 flavors | We present a calculation of the form factor for B -> D* l nu using a 2+1
improved staggered action for the light quarks (on the MILC configurations),
and the Fermilab action for the heavy quarks. The form factor is computed at
zero recoil using a new double ratio method which yields the form factor more
directly than... | hep-lat | we present a calculation of the form factor for b d l nu using a 21 improved staggered action for the light quarks on the milc configurations and the fermilab action for the heavy quarks the form factor is computed at zero recoil using a new double ratio method which yields the form factor more directly than previous a... | [['we', 'present', 'a', 'calculation', 'of', 'the', 'form', 'factor', 'for', 'b', 'd', 'l', 'nu', 'using', 'a', '21', 'improved', 'staggered', 'action', 'for', 'the', 'light', 'quarks', 'on', 'the', 'milc', 'configurations', 'and', 'the', 'fermilab', 'action', 'for', 'the', 'heavy', 'quarks', 'the', 'form', 'factor', '... | [-0.07352727995514553, 0.20200700662493454, -0.09591556465553151, 0.03247235608247693, -0.012226404353849968, -0.13433621366018966, 0.10982454064207435, 0.3352805581575228, -0.15917560760468497, -0.27003747256377997, 0.001208616404841512, -0.29122700958938924, -0.026664247160177616, 0.1759356292817047, 0.08486810366039... |
710.1112 | Four-level systems and a universal quantum gate | We discuss a possibility of implementing a universal quantum XOR gate, by
using two coupled quantum dots subjected to external magnetic fields that are
parallel and slightly different. We consider this system in two different field
configurations. In the first case, parallel external fields with the intensity
differe... | quant-ph cond-mat.other | we discuss a possibility of implementing a universal quantum xor gate by using two coupled quantum dots subjected to external magnetic fields that are parallel and slightly different we consider this system in two different field configurations in the first case parallel external fields with the intensity difference at... | [['we', 'discuss', 'a', 'possibility', 'of', 'implementing', 'a', 'universal', 'quantum', 'xor', 'gate', 'by', 'using', 'two', 'coupled', 'quantum', 'dots', 'subjected', 'to', 'external', 'magnetic', 'fields', 'that', 'are', 'parallel', 'and', 'slightly', 'different', 'we', 'consider', 'this', 'system', 'in', 'two', 'd... | [-0.18240542124250744, 0.17985752637017202, -0.002673826757148882, 0.047671219056283486, -0.017806786727472178, -0.1653698374992054, 0.03512702691460065, 0.44346632401221525, -0.2569003216511406, -0.3251359985922189, 0.03540461344470946, -0.23548729602837923, -0.08123418542684294, 0.1979059554237775, 0.0358129301735388... |
710.1113 | Alfv\'en QPOs in Magnetars | We investigate torsional Alfv\'en oscillations of relativistic stars with a
global dipole magnetic field, via two-dimensional numerical simulations. We
find that a) there exist two families of quasi-periodic oscillations (QPOs)
with harmonics at integer multiples of the fundamental frequency, b) the
lower-frequency Q... | astro-ph | we investigate torsional alfven oscillations of relativistic stars with a global dipole magnetic field via twodimensional numerical simulations we find that a there exist two families of quasiperiodic oscillations qpos with harmonics at integer multiples of the fundamental frequency b the lowerfrequency qpo is related ... | [['we', 'investigate', 'torsional', 'alfven', 'oscillations', 'of', 'relativistic', 'stars', 'with', 'a', 'global', 'dipole', 'magnetic', 'field', 'via', 'twodimensional', 'numerical', 'simulations', 'we', 'find', 'that', 'a', 'there', 'exist', 'two', 'families', 'of', 'quasiperiodic', 'oscillations', 'qpos', 'with', '... | [-0.1727723864999285, 0.20356644466722454, -0.004519537092930228, 0.09311536329642621, -0.09620174344816654, -0.07446719810664788, 0.07474322586358867, 0.3552521817124844, -0.18902818074369496, -0.31560940380214897, 0.08301181713430707, -0.24275884372282694, -0.043100523018686894, 0.2680570630008261, 0.0222435046652986... |
710.1114 | XMM-Newton, Chandra, and CGPS observations of the Supernova Remnants
G85.4+0.7 and G85.9-0.6 | We present an XMM-Newton detection of two low radio surface brightness SNRs,
G85.4+0.7 and G85.9-0.6, discovered with the Canadian Galactic Plane Survey
(CGPS). High-resolution XMM-Newton images revealing the morphology of the
diffuse emission, as well as discrete point sources, are presented and
correlated with radi... | astro-ph | we present an xmmnewton detection of two low radio surface brightness snrs g85407 and g85906 discovered with the canadian galactic plane survey cgps highresolution xmmnewton images revealing the morphology of the diffuse emission as well as discrete point sources are presented and correlated with radio and chandra imag... | [['we', 'present', 'an', 'xmmnewton', 'detection', 'of', 'two', 'low', 'radio', 'surface', 'brightness', 'snrs', 'g85407', 'and', 'g85906', 'discovered', 'with', 'the', 'canadian', 'galactic', 'plane', 'survey', 'cgps', 'highresolution', 'xmmnewton', 'images', 'revealing', 'the', 'morphology', 'of', 'the', 'diffuse', '... | [-0.07751338812850521, 0.0949337718427753, -0.03438562430887365, 0.05248835228630582, -0.05164710619976578, -0.08498791867797154, 0.08283272480041208, 0.44491056930011424, -0.15713174681467804, -0.36438527447062197, 0.0880589925524442, -0.35059653367724775, 0.050748352573511187, 0.19985138455038548, 0.01223707170457417... |
710.1115 | Adapted Linear-Nonlinear Decomposition And Global Well-posedness For
Solutions To The Defocusing Cubic Wave Equation On $\mathbb{R}^{3}$ | We prove global well-posedness for the defocusing cubic wave equation with
data in $H^{s} \times H^{s-1}$, $1>s>{13/18}$. The main task is to estimate the
variation of an almost conserved quantity on an arbitrary long time interval.
We divide it into subintervals. On each of these subintervals we write the
solution a... | math.AP | we prove global wellposedness for the defocusing cubic wave equation with data in hs times hs1 1s1318 the main task is to estimate the variation of an almost conserved quantity on an arbitrary long time interval we divide it into subintervals on each of these subintervals we write the solution as the sum of its linear ... | [['we', 'prove', 'global', 'wellposedness', 'for', 'the', 'defocusing', 'cubic', 'wave', 'equation', 'with', 'data', 'in', 'hs', 'times', 'hs1', '1s1318', 'the', 'main', 'task', 'is', 'to', 'estimate', 'the', 'variation', 'of', 'an', 'almost', 'conserved', 'quantity', 'on', 'an', 'arbitrary', 'long', 'time', 'interval'... | [-0.13619752266410604, 0.037326772951490124, -0.07243476596559925, 0.04901161098695663, -0.05838045238304031, -0.045028404826410566, -0.0002422525985054223, 0.3446554743379063, -0.3304245129048106, -0.2472532256113657, 0.19008359235447708, -0.27545342731278344, -0.07810285553148195, 0.1495278104985447, -0.0373182540467... |
710.1116 | Radiative Penguin Decays | We discuss recent experimental studies of radiative penguin decays of B
mesons by the Belle and BaBar collaborations.
| hep-ex | we discuss recent experimental studies of radiative penguin decays of b mesons by the belle and babar collaborations | [['we', 'discuss', 'recent', 'experimental', 'studies', 'of', 'radiative', 'penguin', 'decays', 'of', 'b', 'mesons', 'by', 'the', 'belle', 'and', 'babar', 'collaborations']] | [-0.04578024104961918, 0.3168203483542634, 0.008408233626849122, 0.10796196106821299, -0.1661779246189528, -0.11835483394356237, 0.15188445909492052, 0.2820838112384081, -0.04848126735952166, -0.1334814764559269, -0.11052536799494798, -0.5200853746694823, -0.006402608058932755, 0.10749491552511851, 0.11671125557687548,... |
710.1117 | Topological spectrum of classical configurations | For any classical field configuration or mechanical system with a finite
number of degrees of freedom we introduce the concept of topological spectrum.
It is based upon the assumption that for any classical configuration there
exists a principle fiber bundle that contains all the physical and geometric
information of... | math-ph gr-qc math.MP | for any classical field configuration or mechanical system with a finite number of degrees of freedom we introduce the concept of topological spectrum it is based upon the assumption that for any classical configuration there exists a principle fiber bundle that contains all the physical and geometric information of th... | [['for', 'any', 'classical', 'field', 'configuration', 'or', 'mechanical', 'system', 'with', 'a', 'finite', 'number', 'of', 'degrees', 'of', 'freedom', 'we', 'introduce', 'the', 'concept', 'of', 'topological', 'spectrum', 'it', 'is', 'based', 'upon', 'the', 'assumption', 'that', 'for', 'any', 'classical', 'configuratio... | [-0.180559566244483, 0.13099122429380455, -0.12068877357776965, 0.030727765397624233, -0.07163249999892128, -0.11477379415325982, 0.052512030782805676, 0.3031979515014783, -0.2659643225969099, -0.29807730282292416, 0.09488568714004941, -0.2450464844258259, -0.18990464023891432, 0.18828023123585255, -0.03903395360659646... |
710.1118 | Status of the MILC light pseudoscalar meson project | We discuss the current status of our calculation of the physics of pi and K
mesons using three dynamical flavors of improved staggered quarks. This year,
we have a new ensemble with a lattice spacing of 0.06 fm and a light sea mass
of 0.2 m_s, as well as significant increases in statistics at several coarser
lattice ... | hep-lat | we discuss the current status of our calculation of the physics of pi and k mesons using three dynamical flavors of improved staggered quarks this year we have a new ensemble with a lattice spacing of 006 fm and a light sea mass of 02 m_s as well as significant increases in statistics at several coarser lattice spacing... | [['we', 'discuss', 'the', 'current', 'status', 'of', 'our', 'calculation', 'of', 'the', 'physics', 'of', 'pi', 'and', 'k', 'mesons', 'using', 'three', 'dynamical', 'flavors', 'of', 'improved', 'staggered', 'quarks', 'this', 'year', 'we', 'have', 'a', 'new', 'ensemble', 'with', 'a', 'lattice', 'spacing', 'of', '006', 'f... | [-0.09483776379401158, 0.37254885336580246, -0.048959735682920405, 0.10474325501893059, 0.02459142737911622, -0.08822949953824527, 0.14510330609291008, 0.36181279859125715, -0.15975361159929125, -0.3133563028409538, 0.06161838121203657, -0.3343399634560276, 0.03591337709344531, 0.13572193693222576, 0.04420530545451727,... |
710.1119 | Proper Mass Variation under Gravitational and Coulomb Force Action in
Relativistic Mechanics of Point Particle | The problem studied is formulated in the title: proper mass variation under
gravitational and Coulomb force action in Relativistic Mechanics of point
particle. The novelty is that equations of motion are obtained in the
relativistic Lagrangean framework for conservative force fields under
assumption of field dependen... | physics.gen-ph | the problem studied is formulated in the title proper mass variation under gravitational and coulomb force action in relativistic mechanics of point particle the novelty is that equations of motion are obtained in the relativistic lagrangean framework for conservative force fields under assumption of field dependent pr... | [['the', 'problem', 'studied', 'is', 'formulated', 'in', 'the', 'title', 'proper', 'mass', 'variation', 'under', 'gravitational', 'and', 'coulomb', 'force', 'action', 'in', 'relativistic', 'mechanics', 'of', 'point', 'particle', 'the', 'novelty', 'is', 'that', 'equations', 'of', 'motion', 'are', 'obtained', 'in', 'the'... | [-0.12366833441314827, 0.1551555203096376, -0.12102894770248374, 0.093863873523306, -0.09009125432250095, -0.10217734163202215, -0.028584272470679243, 0.3278774632255367, -0.23365656348293898, -0.30729762933418503, -0.007614761117807649, -0.23005955760252841, -0.10709462072482409, 0.22471136939664213, -0.07746013887880... |
710.112 | Iterated distributive laws | We give a framework for combining $n$ monads on the same category via
distributive laws satisfying Yang-Baxter equations, extending the classical
result of Barr and Wells which combines two monads via one distributive law. We
show that this corresponds to iterating $n$-times the process of taking the
2-category of mo... | math.CT | we give a framework for combining n monads on the same category via distributive laws satisfying yangbaxter equations extending the classical result of barr and wells which combines two monads via one distributive law we show that this corresponds to iterating ntimes the process of taking the 2category of monads in a 2... | [['we', 'give', 'a', 'framework', 'for', 'combining', 'n', 'monads', 'on', 'the', 'same', 'category', 'via', 'distributive', 'laws', 'satisfying', 'yangbaxter', 'equations', 'extending', 'the', 'classical', 'result', 'of', 'barr', 'and', 'wells', 'which', 'combines', 'two', 'monads', 'via', 'one', 'distributive', 'law'... | [-0.10375692760239222, 0.06552502732249975, -0.07675188772139206, 0.10596433735146807, -0.1183260619873181, -0.16891564457494365, 0.050496138713372475, 0.3370210473575363, -0.4069691206968855, -0.19063194423298618, 0.021598446744194786, -0.20503257607508982, -0.11121964130558938, 0.16628746104626252, -0.169782603517108... |
710.1121 | The kaon B-parameter from unquenched mixed action lattice QCD | We present a preliminary calculation of B_K using domain-wall valence quarks
and 2+1 flavors of improved staggered sea quarks. Both the size of the residual
quark mass, which measures the amount of chiral symmetry breaking, and of the
mixed meson splitting Delta_mix, a measure of taste-symmetry breaking, show
that di... | hep-lat | we present a preliminary calculation of b_k using domainwall valence quarks and 21 flavors of improved staggered sea quarks both the size of the residual quark mass which measures the amount of chiral symmetry breaking and of the mixed meson splitting delta_mix a measure of tastesymmetry breaking show that discretizati... | [['we', 'present', 'a', 'preliminary', 'calculation', 'of', 'b_k', 'using', 'domainwall', 'valence', 'quarks', 'and', '21', 'flavors', 'of', 'improved', 'staggered', 'sea', 'quarks', 'both', 'the', 'size', 'of', 'the', 'residual', 'quark', 'mass', 'which', 'measures', 'the', 'amount', 'of', 'chiral', 'symmetry', 'break... | [-0.1143865254473954, 0.3074361260507271, -0.09988440614003334, 0.0689748971192778, -0.03970877835391103, -0.06493889653280269, 0.12174968927398487, 0.397318171310055, -0.1547484123419943, -0.23524377591581674, 0.06887635292594124, -0.28770500289303436, -0.027212789193829044, 0.07846839819443378, 0.03473297892695796, 0... |
710.1122 | Sleuthing Hidden Order | Physicists have long debated whether the hidden order in URu2Si2 is itinerant
or localized, and it remains inaccessible to direct external probes. Recent
observation of an overdamped collective mode in this material (C. Weibe et al,
Nature Physics 3, 96-100 (2007)), appears to resolve this outstanding issue.
| cond-mat.str-el cond-mat.supr-con | physicists have long debated whether the hidden order in uru2si2 is itinerant or localized and it remains inaccessible to direct external probes recent observation of an overdamped collective mode in this material c weibe et al nature physics 3 96100 2007 appears to resolve this outstanding issue | [['physicists', 'have', 'long', 'debated', 'whether', 'the', 'hidden', 'order', 'in', 'uru2si2', 'is', 'itinerant', 'or', 'localized', 'and', 'it', 'remains', 'inaccessible', 'to', 'direct', 'external', 'probes', 'recent', 'observation', 'of', 'an', 'overdamped', 'collective', 'mode', 'in', 'this', 'material', 'c', 'we... | [-0.1502681343241575, 0.21112268881041288, -0.043217650079663765, 0.06594157728931292, -0.16103713947566264, -0.17725433306174077, 0.06068886618347878, 0.3497450183680717, -0.28908472109903044, -0.3846430564101072, 0.06223536734072928, -0.28837348679278757, -0.11815377820699298, 0.07655097105778119, -0.0498936009652754... |
710.1123 | Clouds, Gravity and Metallicity in Blue L dwarfs: The Case of 2MASS
J11263991-5003550 | Optical and near-infrared spectroscopy of the newly discovered peculiar L
dwarf 2MASS J11263991-5003550 are presented. Folkes et al. identified this
source as a high proper motion L9+/-1 dwarf based on its strong H2O absorption
at 1.4 micron. We find that the optical spectrum of 2MASS J1126-5003 is in fact
consistent... | astro-ph | optical and nearinfrared spectroscopy of the newly discovered peculiar l dwarf 2mass j112639915003550 are presented folkes et al identified this source as a high proper motion l91 dwarf based on its strong h2o absorption at 14 micron we find that the optical spectrum of 2mass j11265003 is in fact consistent with that o... | [['optical', 'and', 'nearinfrared', 'spectroscopy', 'of', 'the', 'newly', 'discovered', 'peculiar', 'l', 'dwarf', '2mass', 'j112639915003550', 'are', 'presented', 'folkes', 'et', 'al', 'identified', 'this', 'source', 'as', 'a', 'high', 'proper', 'motion', 'l91', 'dwarf', 'based', 'on', 'its', 'strong', 'h2o', 'absorpti... | [-0.02817757782759145, 0.10665387734169614, -0.09081617782663431, 0.07047321082027934, -0.12091359442775519, -0.11053007080021207, 0.07326112122591738, 0.4452588500561895, -0.16417706218074823, -0.3326682671255692, 0.02323339553048918, -0.29414259269070187, -0.09650366026498439, 0.1671366029577406, -0.0885019932327731,... |
710.1124 | Apostol-Bernoulli functions, derivative polynomials and Eulerian
polynomials | This is a short survey of a class of functions introduces by Tom Apostol. The
survey is focused on their relation to Eulerian polynomials, derivative
polynomials, and also on some integral representations.
| math.CA math.NT | this is a short survey of a class of functions introduces by tom apostol the survey is focused on their relation to eulerian polynomials derivative polynomials and also on some integral representations | [['this', 'is', 'a', 'short', 'survey', 'of', 'a', 'class', 'of', 'functions', 'introduces', 'by', 'tom', 'apostol', 'the', 'survey', 'is', 'focused', 'on', 'their', 'relation', 'to', 'eulerian', 'polynomials', 'derivative', 'polynomials', 'and', 'also', 'on', 'some', 'integral', 'representations']] | [-0.2052480853162706, 0.0565179327968508, -0.13103453161238576, 0.09347162164704059, -0.23139545670710504, -0.039897447131806985, 0.010183389764279127, 0.35106367320986465, -0.27276266273111105, -0.23628263652790338, 0.13285833744885167, -0.2714279268402606, -0.19086786115076393, 0.2182479296461679, -0.0990592328016646... |
710.1125 | Frontier at your fingertips | Between the nano- and micrometre scales, the collective behaviour of matter
can give rise to startling emergent properties that hint at the nexus between
biology and physics.
| cond-mat.str-el cond-mat.soft cond-mat.stat-mech | between the nano and micrometre scales the collective behaviour of matter can give rise to startling emergent properties that hint at the nexus between biology and physics | [['between', 'the', 'nano', 'and', 'micrometre', 'scales', 'the', 'collective', 'behaviour', 'of', 'matter', 'can', 'give', 'rise', 'to', 'startling', 'emergent', 'properties', 'that', 'hint', 'at', 'the', 'nexus', 'between', 'biology', 'and', 'physics']] | [-0.09382981089530168, 0.24120343255775947, -0.18392311314258863, 0.08538633740196626, -0.09405296371766815, -0.14437881265594452, -0.026241855609610124, 0.2606435782379574, -0.29438676215984205, -0.46327203346623314, -0.043037745670449955, -0.30659231819488386, -0.20597551052493077, 0.18818431902952767, 0.066995304974... |
710.1126 | Heavy electrons and the symplectic symmetry of spin | The recent discovery of two heavy fermion materials PuCoGa_{5} and
NpPd_{5}Al_{2} which transform directly from Curie paramagnets into
superconductors, reveals a new class of superconductor where local moments
quench directly into a superconducting condensate. A powerful tool in the
description of heavy fermion metal... | cond-mat.str-el cond-mat.supr-con | the recent discovery of two heavy fermion materials pucoga_5 and nppd_5al_2 which transform directly from curie paramagnets into superconductors reveals a new class of superconductor where local moments quench directly into a superconducting condensate a powerful tool in the description of heavy fermion metals is the l... | [['the', 'recent', 'discovery', 'of', 'two', 'heavy', 'fermion', 'materials', 'pucoga_5', 'and', 'nppd_5al_2', 'which', 'transform', 'directly', 'from', 'curie', 'paramagnets', 'into', 'superconductors', 'reveals', 'a', 'new', 'class', 'of', 'superconductor', 'where', 'local', 'moments', 'quench', 'directly', 'into', '... | [-0.17043651296332415, 0.24712711030079848, -0.05170279665495499, 0.04820995970929205, -0.06644852568539615, -0.19116395856468124, 0.08416084984266764, 0.33561003036703524, -0.25856227735369214, -0.28376895926744683, -0.028371962077894237, -0.31287310083657816, -0.07656236831391051, 0.11742938211125373, 0.0655544377545... |
710.1127 | The values of an Euler sum at negative integers and relation to a
convolution of Bernoulli numbers | We study a special Dirichlet series studied before by Apostol and Matsuoka
and specify its values at negative integers. These values are related to a
certain convolution of Bernoulli numbers
| math.CA math.NT | we study a special dirichlet series studied before by apostol and matsuoka and specify its values at negative integers these values are related to a certain convolution of bernoulli numbers | [['we', 'study', 'a', 'special', 'dirichlet', 'series', 'studied', 'before', 'by', 'apostol', 'and', 'matsuoka', 'and', 'specify', 'its', 'values', 'at', 'negative', 'integers', 'these', 'values', 'are', 'related', 'to', 'a', 'certain', 'convolution', 'of', 'bernoulli', 'numbers']] | [-0.14810398183763027, 0.1469149627101918, -0.014205065726613005, 0.10566612677648664, -0.10278345923870802, -0.1733104656605671, 0.05221065375953913, 0.33954688782493275, -0.2941831579354281, -0.2415947190175454, 0.14102532191512485, -0.2409679719634975, -0.13701436162615815, 0.19884357762833435, -0.05558664724230766,... |
710.1128 | Supplementary material to Heavy electrons and the symplectic symmetry of
spin | This online material provides the technical detail for ``Heavy electrons and
the symplectic symmetry of spin",(arXiv 0710.1122). Three parts. Part I -
symplectic spins, their properties and gauge symmetries. Part II - derivation
of two-chanel model for tetragonal heavy electron systems with the view to
application to... | cond-mat.str-el cond-mat.supr-con | this online material provides the technical detail for heavy electrons and the symplectic symmetry of spinarxiv 07101122 three parts part i symplectic spins their properties and gauge symmetries part ii derivation of twochanel model for tetragonal heavy electron systems with the view to application to pucoga5 and nppd_... | [['this', 'online', 'material', 'provides', 'the', 'technical', 'detail', 'for', 'heavy', 'electrons', 'and', 'the', 'symplectic', 'symmetry', 'of', 'spinarxiv', '07101122', 'three', 'parts', 'part', 'i', 'symplectic', 'spins', 'their', 'properties', 'and', 'gauge', 'symmetries', 'part', 'ii', 'derivation', 'of', 'twoc... | [-0.1175055179203785, 0.1082082967701796, -0.02793485332733473, 0.0613871354505898, -0.09523599698032076, -0.14546472186575066, 0.037433189915719665, 0.35135971880643757, -0.2663189122245672, -0.2903826676208425, 0.06854428575418235, -0.29213163583866647, -0.10319070031589551, 0.1329197447079964, 0.008849364082797783, ... |
710.1129 | The Census Taker's Hat | If the observable universe really is a hologram, then of what sort? Is it
rich enough to keep track of an eternally inflating multiverse? What physical
and mathematical principles underlie it? Is the hologram a lower dimensional
quantum field theory, and if so, how many dimensions are explicit, and how many
"emerge?"... | hep-th | if the observable universe really is a hologram then of what sort is it rich enough to keep track of an eternally inflating multiverse what physical and mathematical principles underlie it is the hologram a lower dimensional quantum field theory and if so how many dimensions are explicit and how many emerge does the ho... | [['if', 'the', 'observable', 'universe', 'really', 'is', 'a', 'hologram', 'then', 'of', 'what', 'sort', 'is', 'it', 'rich', 'enough', 'to', 'keep', 'track', 'of', 'an', 'eternally', 'inflating', 'multiverse', 'what', 'physical', 'and', 'mathematical', 'principles', 'underlie', 'it', 'is', 'the', 'hologram', 'a', 'lower... | [-0.08351714990070858, 0.1671146761232345, -0.18528493911883645, 0.138101926486265, -0.12933419877883948, -0.13213325077579555, 0.0030222918189426453, 0.2736206110743408, -0.21843230202838212, -0.2982669326772481, 0.11160722446144598, -0.23454450422421239, -0.1794879613885594, 0.14450499251423077, -0.11882297571978015,... |
710.113 | Topological susceptibility in two-flavor lattice QCD with exact chiral
symmetry | We determine the topological susceptibility $\chi_t$ in two-flavor QCD using
the lattice simulations at a fixed topological sector. The topological charge
density is unambiguously defined on the lattice using the overlap-Dirac
operator which possesses exact chiral symmetry. Simulations are performed on a
$16^3 \times... | hep-lat hep-ph hep-th | we determine the topological susceptibility chi_t in twoflavor qcd using the lattice simulations at a fixed topological sector the topological charge density is unambiguously defined on the lattice using the overlapdirac operator which possesses exact chiral symmetry simulations are performed on a 163 times 32 lattice ... | [['we', 'determine', 'the', 'topological', 'susceptibility', 'chi_t', 'in', 'twoflavor', 'qcd', 'using', 'the', 'lattice', 'simulations', 'at', 'a', 'fixed', 'topological', 'sector', 'the', 'topological', 'charge', 'density', 'is', 'unambiguously', 'defined', 'on', 'the', 'lattice', 'using', 'the', 'overlapdirac', 'ope... | [-0.12510456517017607, 0.28076501816575383, -0.1030257479062882, 0.07079662377062929, 0.0003066571878975835, -0.05763387954312152, 0.10784674051041104, 0.30595422778760306, -0.16083239722868492, -0.247568120599066, 0.03432197527285537, -0.3437733723685659, -0.042394564043858954, 0.09571680391592713, 0.06934799182646234... |
710.1131 | On the Use of Integrals to Evaluate Series of Rational Terms | This article is written with the hope to draw attention to a method that uses
integral transforms to find exact values for a large class of convergent series
(and, in particular, series of rational terms). We apply the method to some
series that generalize a problem published in `The College Mathematics
Journal'. Som... | math.CA | this article is written with the hope to draw attention to a method that uses integral transforms to find exact values for a large class of convergent series and in particular series of rational terms we apply the method to some series that generalize a problem published in the college mathematics journal some of the r... | [['this', 'article', 'is', 'written', 'with', 'the', 'hope', 'to', 'draw', 'attention', 'to', 'a', 'method', 'that', 'uses', 'integral', 'transforms', 'to', 'find', 'exact', 'values', 'for', 'a', 'large', 'class', 'of', 'convergent', 'series', 'and', 'in', 'particular', 'series', 'of', 'rational', 'terms', 'we', 'apply... | [-0.024434091422993402, -0.011029632934010946, -0.12348700878210365, 0.05243559560666864, -0.1706410132921659, -0.07698589873571808, 0.03938404658513788, 0.34920891953202393, -0.24498532440943213, -0.29063668758966604, 0.10263994372485635, -0.25110562757517285, -0.18753132603775996, 0.27044734708391704, -0.112420080043... |
710.1132 | Some bijections on set partitions | This paper has been withdrawn by the author due to an error in Lemma 3,
making the (bijective) proof of Theorem 4 and Corollary 5 invalid (symmetry of
k-nonnesting and k-noncrossing set partitions).
| math.CO | this paper has been withdrawn by the author due to an error in lemma 3 making the bijective proof of theorem 4 and corollary 5 invalid symmetry of knonnesting and knoncrossing set partitions | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'an', 'error', 'in', 'lemma', '3', 'making', 'the', 'bijective', 'proof', 'of', 'theorem', '4', 'and', 'corollary', '5', 'invalid', 'symmetry', 'of', 'knonnesting', 'and', 'knoncrossing', 'set', 'partitions']] | [-0.14841381127409864, 0.030620488158698816, -0.09275626718546405, 0.06660739409694956, -0.08289125714112412, -0.10980751421866995, 0.09256432535987573, 0.2810610252587746, -0.2863099737883066, -0.3671004053656802, 0.11401797525909249, -0.2603625435255129, -0.14534738537799002, 0.12416585109365935, -0.2300416547240633,... |
710.1133 | Craig's XY-distribution and the statistics of Lagrangian power in
two-dimensional turbulence | We examine the probability distribution function (pdf) of energy injection
rate (power) in numerical simulations of stationary two--dimensional (2D)
turbulence in the Lagrangian frame. The simulation is designed to mimic an
electromagnetically driven fluid layer, a well-documented system for generating
two--dimension... | cond-mat.stat-mech | we examine the probability distribution function pdf of energy injection rate power in numerical simulations of stationary twodimensional 2d turbulence in the lagrangian frame the simulation is designed to mimic an electromagnetically driven fluid layer a welldocumented system for generating twodimensional turbulence i... | [['we', 'examine', 'the', 'probability', 'distribution', 'function', 'pdf', 'of', 'energy', 'injection', 'rate', 'power', 'in', 'numerical', 'simulations', 'of', 'stationary', 'twodimensional', '2d', 'turbulence', 'in', 'the', 'lagrangian', 'frame', 'the', 'simulation', 'is', 'designed', 'to', 'mimic', 'an', 'electroma... | [-0.14165619735238272, 0.15151891040798793, -0.11913423154097286, 0.09861420411029047, -0.009944307308852951, -0.11395183500233237, -0.019798215049853175, 0.33260901166108725, -0.27459228381995443, -0.2656812894192881, 0.0563552663405861, -0.3237161765649706, -0.06920973268102541, 0.17720197794945894, 0.005497721502574... |
710.1134 | The History of the Particle Data Group at KEK in the 1970s | This submission has been withdrawn by arXiv admins because there was an
erroneous author included in the original version.
| physics.hist-ph | this submission has been withdrawn by arxiv admins because there was an erroneous author included in the original version | [['this', 'submission', 'has', 'been', 'withdrawn', 'by', 'arxiv', 'admins', 'because', 'there', 'was', 'an', 'erroneous', 'author', 'included', 'in', 'the', 'original', 'version']] | [-0.10470423994487837, -0.06298470650845527, -0.11449996960398398, -0.0035740458957948967, -0.1342146120181209, -0.11705157028413132, -0.02499381295944515, 0.3138268613501599, -0.1720718586278197, -0.3650157709458941, 0.12213748361988876, -0.32141780676810366, -0.09279532975664265, 0.021225144596476304, -0.360121408575... |
710.1135 | The Plasma Structure of the Cygnus Loop from the Northeastern Rim to the
Southwestern Rim | The Cygnus Loop was observed from the northeast to the southwest with
XMM-Newton. We divided the observed region into two parts, the north path and
the south path, and studied the X-ray spectra along two paths. The spectra can
be well fitted either by a one-component non-equilibrium ionization (NEI) model
or by a t... | astro-ph | the cygnus loop was observed from the northeast to the southwest with xmmnewton we divided the observed region into two parts the north path and the south path and studied the xray spectra along two paths the spectra can be well fitted either by a onecomponent nonequilibrium ionization nei model or by a twocomponent ne... | [['the', 'cygnus', 'loop', 'was', 'observed', 'from', 'the', 'northeast', 'to', 'the', 'southwest', 'with', 'xmmnewton', 'we', 'divided', 'the', 'observed', 'region', 'into', 'two', 'parts', 'the', 'north', 'path', 'and', 'the', 'south', 'path', 'and', 'studied', 'the', 'xray', 'spectra', 'along', 'two', 'paths', 'the'... | [-0.06314962384383371, 0.14218777330995958, -0.046131773912140475, 0.06496135969288074, -0.042731062251073405, -0.10519092546979546, 0.03419458506787233, 0.4280922167523489, -0.2136400562454428, -0.3353942165807312, 0.046921639742804805, -0.3139704571478823, 0.0046585492840647575, 0.15732052943081057, -0.01799312214459... |
710.1136 | Inverse problems for Einstein manifolds | We show that the Dirichlet-to-Neumann operator of the Laplacian on an open
subset of the boundary of a connected compact Einstein manifold with boundary
determines the manifold up to isometries. Similarly, for connected conformally
compact Einstein manifolds of even dimension $n+1$, we prove that the
scattering matri... | math.DG | we show that the dirichlettoneumann operator of the laplacian on an open subset of the boundary of a connected compact einstein manifold with boundary determines the manifold up to isometries similarly for connected conformally compact einstein manifolds of even dimension n1 we prove that the scattering matrix at energ... | [['we', 'show', 'that', 'the', 'dirichlettoneumann', 'operator', 'of', 'the', 'laplacian', 'on', 'an', 'open', 'subset', 'of', 'the', 'boundary', 'of', 'a', 'connected', 'compact', 'einstein', 'manifold', 'with', 'boundary', 'determines', 'the', 'manifold', 'up', 'to', 'isometries', 'similarly', 'for', 'connected', 'co... | [-0.19788287819496223, 0.09522085691966663, -0.01789617905068019, 0.013179193620407393, -0.11544589469918892, -0.1241521839022873, -0.03897103025681443, 0.36686046037172515, -0.26324495750050697, -0.19593735388110553, 0.15146795490254011, -0.3245875749086577, -0.112992907863199, 0.1525239743114937, -0.10277831372583196... |
710.1137 | Finite-size scaling of synchronized oscillation on complex networks | The onset of synchronization in a system of random frequency oscillators
coupled through a random network is investigated. Using a mean-field
approximation, we characterize sample-to-sample fluctuations for networks of
finite size, and derive the corresponding scaling properties in the critical
region. For scale-free... | cond-mat.stat-mech | the onset of synchronization in a system of random frequency oscillators coupled through a random network is investigated using a meanfield approximation we characterize sampletosample fluctuations for networks of finite size and derive the corresponding scaling properties in the critical region for scalefree networks ... | [['the', 'onset', 'of', 'synchronization', 'in', 'a', 'system', 'of', 'random', 'frequency', 'oscillators', 'coupled', 'through', 'a', 'random', 'network', 'is', 'investigated', 'using', 'a', 'meanfield', 'approximation', 'we', 'characterize', 'sampletosample', 'fluctuations', 'for', 'networks', 'of', 'finite', 'size',... | [-0.14812091750342407, 0.16250948853676317, -0.05676223045230796, 0.048935639487492646, 0.02355315387781741, -0.1503501144766618, 0.060125838555750766, 0.34094977563235246, -0.22364186486268764, -0.24113730412229137, 0.05639936217359441, -0.3073944259845352, -0.16535690531402952, 0.19911772041123801, 0.0563508287302545... |
710.1138 | The running of the bare coupling in SU(N) gauge theories | For N>4 there is a first order bulk transition that cleanly separates the
strong and weak coupling regimes of SU(N) lattice gauge theories with the
plaquette action. We find that in this case the calculated string tension can
be readily fitted throughout the weak coupling region by a standard 3-loop
perturbative expr... | hep-lat | for n4 there is a first order bulk transition that cleanly separates the strong and weak coupling regimes of sun lattice gauge theories with the plaquette action we find that in this case the calculated string tension can be readily fitted throughout the weak coupling region by a standard 3loop perturbative expression ... | [['for', 'n4', 'there', 'is', 'a', 'first', 'order', 'bulk', 'transition', 'that', 'cleanly', 'separates', 'the', 'strong', 'and', 'weak', 'coupling', 'regimes', 'of', 'sun', 'lattice', 'gauge', 'theories', 'with', 'the', 'plaquette', 'action', 'we', 'find', 'that', 'in', 'this', 'case', 'the', 'calculated', 'string', ... | [-0.09969825209735877, 0.12185220485450236, -0.08584807940878718, 0.10262552142601193, -0.03850240978728774, -0.13027369290286706, 0.06354409955054115, 0.3495029177753389, -0.2140470685975019, -0.30004746479224104, 0.07044199016829567, -0.26133686526889466, -0.10524888353156008, 0.1578770674693074, 0.009048671056278492... |
710.1139 | Kinetic Economies | We study a minimalist kinetic model for economies. A system of agents with
local trading rules display emergent demand behaviour. We examine the resulting
wealth distribution to look for non-thermal behaviour. We compare and contrast
this model with other similar models.
| q-fin.GN physics.soc-ph | we study a minimalist kinetic model for economies a system of agents with local trading rules display emergent demand behaviour we examine the resulting wealth distribution to look for nonthermal behaviour we compare and contrast this model with other similar models | [['we', 'study', 'a', 'minimalist', 'kinetic', 'model', 'for', 'economies', 'a', 'system', 'of', 'agents', 'with', 'local', 'trading', 'rules', 'display', 'emergent', 'demand', 'behaviour', 'we', 'examine', 'the', 'resulting', 'wealth', 'distribution', 'to', 'look', 'for', 'nonthermal', 'behaviour', 'we', 'compare', 'a... | [-0.09298441967949635, 0.0721432906461925, -0.16119892063845948, 0.15844913257183735, -0.07966136691592089, -0.18070115017273078, 0.06129007461685233, 0.42022788197529026, -0.2615088139243265, -0.31527207031414456, 0.03512617474330998, -0.30475896142604875, -0.15423430411553965, 0.10908260349774869, -0.0352536392793564... |
710.114 | Star Formation Density and Halpha Luminosity Function of an Emission
Line Selected Galaxy Sample at z ~ 0.24 | We use narrowband imaging (FWHM = 70 A) to select a sample of emission line
galaxies between 0.20 <~ z <~ 1.22 in two fields covering 0.5 sq. deg. We use
spectroscopic follow-up to select a sub-sample of Halpha emitting galaxies at z
~ 0.24 and determine the Halpha luminosity function and star formation density
at z ... | astro-ph | we use narrowband imaging fwhm 70 a to select a sample of emission line galaxies between 020 z 122 in two fields covering 05 sq deg we use spectroscopic followup to select a subsample of halpha emitting galaxies at z 024 and determine the halpha luminosity function and star formation density at z 024 for both of our fi... | [['we', 'use', 'narrowband', 'imaging', 'fwhm', '70', 'a', 'to', 'select', 'a', 'sample', 'of', 'emission', 'line', 'galaxies', 'between', '020', 'z', '122', 'in', 'two', 'fields', 'covering', '05', 'sq', 'deg', 'we', 'use', 'spectroscopic', 'followup', 'to', 'select', 'a', 'subsample', 'of', 'halpha', 'emitting', 'gal... | [-0.05108176875627762, 0.07053922720210017, -0.037640570122103686, 0.10789070246159646, -0.06850623049305428, -0.06608884359443201, 0.08452995234942982, 0.4780759280022811, -0.13169751363749585, -0.3613700215377355, 0.0328727432558348, -0.34058430354972263, 0.009229162839097036, 0.18663127783537262, -0.0068824117775884... |
710.1141 | Supersymmetric Tuned Inflation | We address an issue what kind of tuning realizes a flat potential for
inflaton in supergravity. We restrict ourselves to the case that inflationary
dynamics is not affected by separate supersymmetry-breaking effects, and
consider examples of a single chiral superfield as an inflaton with its vacuum
of the vanishing c... | hep-ph | we address an issue what kind of tuning realizes a flat potential for inflaton in supergravity we restrict ourselves to the case that inflationary dynamics is not affected by separate supersymmetrybreaking effects and consider examples of a single chiral superfield as an inflaton with its vacuum of the vanishing cosmol... | [['we', 'address', 'an', 'issue', 'what', 'kind', 'of', 'tuning', 'realizes', 'a', 'flat', 'potential', 'for', 'inflaton', 'in', 'supergravity', 'we', 'restrict', 'ourselves', 'to', 'the', 'case', 'that', 'inflationary', 'dynamics', 'is', 'not', 'affected', 'by', 'separate', 'supersymmetrybreaking', 'effects', 'and', '... | [-0.1661589074823441, 0.22524228806243185, 0.019259444875360437, 0.12366079407299614, -0.14183212950769247, -0.23190338224539478, -0.03484935453867145, 0.31552000906120875, -0.220683768850215, -0.2625932939029581, 0.07704596892951733, -0.21684869584825003, -0.13267302080974774, 0.14257405103522947, -0.08769702592469526... |
710.1142 | Millimeter observations of Planetary Nebulae: a contribution to the
Planck pre-launch catalogue | We present new millimetre 43 GHz observations of a sample of radio-bright
Planetary Nebulae. Such observations were carried out to have a good
determination of the high-frequency radio spectra of the sample in order to
evaluate, together with far-IR measurements (IRAS), the fluxes emitted by the
selected source in th... | astro-ph | we present new millimetre 43 ghz observations of a sample of radiobright planetary nebulae such observations were carried out to have a good determination of the highfrequency radio spectra of the sample in order to evaluate together with farir measurements iras the fluxes emitted by the selected source in the millimet... | [['we', 'present', 'new', 'millimetre', '43', 'ghz', 'observations', 'of', 'a', 'sample', 'of', 'radiobright', 'planetary', 'nebulae', 'such', 'observations', 'were', 'carried', 'out', 'to', 'have', 'a', 'good', 'determination', 'of', 'the', 'highfrequency', 'radio', 'spectra', 'of', 'the', 'sample', 'in', 'order', 'to... | [-0.05564593381653072, 0.09966234454689914, -0.012945453788857402, 0.056922515668051205, -0.07319963943440971, -0.06688025407289769, 0.0676791896071594, 0.44918494017623917, -0.1793043015730124, -0.3414878750781175, 0.10859350200923461, -0.29796712979771944, 0.007631813144203536, 0.20114831456520055, -0.006655576328267... |
710.1143 | High coherence photon pair source for quantum communication | This paper reports a novel single mode source of narrow-band entangled photon
pairs at telecom wavelengths under continuous wave excitation, based on
parametric down conversion. For only 7 mW of pump power it has a created
spectral radiance of 0.08 pairs per coherence length and a bandwidth of 10 pm
(1.2 GHz). The ef... | quant-ph | this paper reports a novel single mode source of narrowband entangled photon pairs at telecom wavelengths under continuous wave excitation based on parametric down conversion for only 7 mw of pump power it has a created spectral radiance of 008 pairs per coherence length and a bandwidth of 10 pm 12 ghz the effectively ... | [['this', 'paper', 'reports', 'a', 'novel', 'single', 'mode', 'source', 'of', 'narrowband', 'entangled', 'photon', 'pairs', 'at', 'telecom', 'wavelengths', 'under', 'continuous', 'wave', 'excitation', 'based', 'on', 'parametric', 'down', 'conversion', 'for', 'only', '7', 'mw', 'of', 'pump', 'power', 'it', 'has', 'a', '... | [-0.166416107991799, 0.18783731578538815, -0.024196916579135825, -0.01926397382132044, 0.004048888320990262, -0.20386410009648118, 0.09939316428776476, 0.45404436013528277, -0.19779884865773575, -0.3340686019909169, 0.04445656636907231, -0.30210211662841696, 0.03581489501742735, 0.25991266733700674, -0.0278159834134082... |
710.1144 | A uniform L^{\infty} estimate for complex Monge-Ampere equations | We prove uniform sup-norm estimates for the Monge-Ampere equation with
respect to a family of Kahler metrics which degenerate towards a pull-back of a
metric from a lower dimensional manifold. This is then used to show the
existence of generalized Kahler-Einstein metrics as the limits of the
Kahler-Ricci flow for som... | math.DG math.CV | we prove uniform supnorm estimates for the mongeampere equation with respect to a family of kahler metrics which degenerate towards a pullback of a metric from a lower dimensional manifold this is then used to show the existence of generalized kahlereinstein metrics as the limits of the kahlerricci flow for some holomo... | [['we', 'prove', 'uniform', 'supnorm', 'estimates', 'for', 'the', 'mongeampere', 'equation', 'with', 'respect', 'to', 'a', 'family', 'of', 'kahler', 'metrics', 'which', 'degenerate', 'towards', 'a', 'pullback', 'of', 'a', 'metric', 'from', 'a', 'lower', 'dimensional', 'manifold', 'this', 'is', 'then', 'used', 'to', 'sh... | [-0.18815388893573612, -0.027234696064387328, -0.11508061925786128, 0.08991495942345996, -0.11312373664797, -0.15710627539690747, -0.023526646466790768, 0.28266312400607957, -0.2663910933702752, -0.1520467831532174, 0.12263690545122423, -0.3045972300477434, -0.15458683488026692, 0.22551474509679753, -0.1849253443128016... |
710.1145 | ATCA observations of the very young Planetary Nebula SAO 244567 | The radio emission from the youngest known Planetary nebula, SAO244567, has
been mapped at 1384, 2368, 4800, 8640, 16832 and 18752 MHz by using the
Australian Telescope Compact Array (ATCA). These observations constitute the
first detailed radio study of this very interesting object, as they allow us to
obtain the ov... | astro-ph | the radio emission from the youngest known planetary nebula sao244567 has been mapped at 1384 2368 4800 8640 16832 and 18752 mhz by using the australian telescope compact array atca these observations constitute the first detailed radio study of this very interesting object as they allow us to obtain the overall radio ... | [['the', 'radio', 'emission', 'from', 'the', 'youngest', 'known', 'planetary', 'nebula', 'sao244567', 'has', 'been', 'mapped', 'at', '1384', '2368', '4800', '8640', '16832', 'and', '18752', 'mhz', 'by', 'using', 'the', 'australian', 'telescope', 'compact', 'array', 'atca', 'these', 'observations', 'constitute', 'the', ... | [-0.03747055684921868, 0.05827158955631383, -0.048404823148369115, 0.057045905037331535, -0.13401013773612, -0.08070157184406664, 0.03248993859372356, 0.45031298218351423, -0.163758509643517, -0.3399440640188528, 0.1347758049476948, -0.24724760879056923, -0.034880531455079716, 0.21813998542669596, -0.016005173101350946... |
710.1146 | Generalized Swanson models and their solutions | We analyze a class of non-Hermitian quadratic Hamiltonians, which are of the
form $ H = {\cal{A}}^{\dagger} {\cal{A}} + \alpha {\cal{A}} ^2 + \beta
{\cal{A}}^{\dagger 2} $, where $ \alpha, \beta $ are real constants, with $
\alpha \neq \beta $, and ${\cal{A}}^{\dagger}$ and ${\cal{A}}$ are generalized
creation and an... | quant-ph | we analyze a class of nonhermitian quadratic hamiltonians which are of the form h caladagger cala alpha cala 2 beta caladagger 2 where alpha beta are real constants with alpha neq beta and caladagger and cala are generalized creation and annihilation operators thus these hamiltonians may be classified as generalized sw... | [['we', 'analyze', 'a', 'class', 'of', 'nonhermitian', 'quadratic', 'hamiltonians', 'which', 'are', 'of', 'the', 'form', 'h', 'caladagger', 'cala', 'alpha', 'cala', '2', 'beta', 'caladagger', '2', 'where', 'alpha', 'beta', 'are', 'real', 'constants', 'with', 'alpha', 'neq', 'beta', 'and', 'caladagger', 'and', 'cala', '... | [-0.12605193821727334, 0.17835862119014714, 0.00454677525151493, 0.07331443546493922, -0.052519775485914, -0.26229429774728596, -0.04648268117072215, 0.3838345541485718, -0.2469800615270055, -0.2241254101710436, 0.05839079198133396, -0.3096074970137972, -0.18086186531910153, 0.18960877603858262, 0.04107573579408621, 0.... |
710.1147 | Newton's method and Baker domains | We show that there exists an entire function f without zeros for which the
associated Newton function N(z)=z-f(z)/f'(z) is a transcendental meromorphic
functions without Baker domains. We also show that there exists an entire
function f with exactly one zero for which the complement of the immediate
attracting basin ... | math.CV math.DS | we show that there exists an entire function f without zeros for which the associated newton function nzzfzfz is a transcendental meromorphic functions without baker domains we also show that there exists an entire function f with exactly one zero for which the complement of the immediate attracting basin has at least ... | [['we', 'show', 'that', 'there', 'exists', 'an', 'entire', 'function', 'f', 'without', 'zeros', 'for', 'which', 'the', 'associated', 'newton', 'function', 'nzzfzfz', 'is', 'a', 'transcendental', 'meromorphic', 'functions', 'without', 'baker', 'domains', 'we', 'also', 'show', 'that', 'there', 'exists', 'an', 'entire', '... | [-0.1900226981054212, 0.03017454054497648, -0.08223538789464983, 0.04357835047927057, -0.05992374544270163, -0.13846984779635488, 0.06354779512946342, 0.3096093957117477, -0.26423122759821804, -0.21670676074748815, 0.06677679604915686, -0.31617115849499094, -0.16665980977082062, 0.22428029080376374, -0.0270152897032540... |
710.1148 | A Micro Molecular Bipolar Outflow From HL Tau | We present detailed geometry and kinematics of the inner outflow toward HL
Tau observed using Near Infrared Integral Field Spectograph (NIFS) at the
Gemini-North 8-m Observatory. We analyzed H2 2.122 um emission and [Fe II]
1.644 um line emission as well as the adjacent continuum observed at a <0".2
resolution. The H... | astro-ph | we present detailed geometry and kinematics of the inner outflow toward hl tau observed using near infrared integral field spectograph nifs at the gemininorth 8m observatory we analyzed h2 2122 um emission and fe ii 1644 um line emission as well as the adjacent continuum observed at a 02 resolution the h2 emission show... | [['we', 'present', 'detailed', 'geometry', 'and', 'kinematics', 'of', 'the', 'inner', 'outflow', 'toward', 'hl', 'tau', 'observed', 'using', 'near', 'infrared', 'integral', 'field', 'spectograph', 'nifs', 'at', 'the', 'gemininorth', '8m', 'observatory', 'we', 'analyzed', 'h2', '2122', 'um', 'emission', 'and', 'fe', 'ii... | [-0.048288793314127394, 0.06175215644574663, -0.026730590346521994, 0.0580444503241659, -0.0560639774148865, -0.09965026538454487, -0.043399866231782144, 0.4932733123125725, -0.19935664107893095, -0.28995987924191263, 0.07285995444753514, -0.2779166904122879, -0.01816706908884812, 0.14912930968381796, 0.017516034175172... |
710.1149 | Z2Z4-linear codes: generator matrices and duality | A code ${\cal C}$ is $\Z_2\Z_4$-additive if the set of coordinates can be
partitioned into two subsets $X$ and $Y$ such that the punctured code of ${\cal
C}$ by deleting the coordinates outside $X$ (respectively, $Y$) is a binary
linear code (respectively, a quaternary linear code). In this paper
$\Z_2\Z_4$-additive ... | cs.IT cs.DM math.CO math.IT | a code cal c is z_2z_4additive if the set of coordinates can be partitioned into two subsets x and y such that the punctured code of cal c by deleting the coordinates outside x respectively y is a binary linear code respectively a quaternary linear code in this paper z_2z_4additive codes are studied their corresponding... | [['a', 'code', 'cal', 'c', 'is', 'z_2z_4additive', 'if', 'the', 'set', 'of', 'coordinates', 'can', 'be', 'partitioned', 'into', 'two', 'subsets', 'x', 'and', 'y', 'such', 'that', 'the', 'punctured', 'code', 'of', 'cal', 'c', 'by', 'deleting', 'the', 'coordinates', 'outside', 'x', 'respectively', 'y', 'is', 'a', 'binary... | [-0.172142655528385, 0.11272832485528918, -0.02544150637167928, 0.09056068997220437, -0.005926833369119241, -0.22876474751735762, -0.0070151187966932815, 0.3770414756463586, -0.34229196054633143, -0.2381477470848066, 0.1577722678662834, -0.25186077130141016, -0.11430038591485014, 0.2183851581736863, -0.0699967104697050... |
710.115 | The pion-pion scattering amplitude. III: Improving the analysis with
forward dispersion relations and Roy equations | We complete and improve the fits to experimental $\pi\pi$ scattering
amplitudes, both at low and high energies, that we performed in the previous
papers of this series. We then verify that the corresponding amplitudes satisfy
analyticity requirements, in the form of partial wave analyticity at low
energies, forward d... | hep-ph | we complete and improve the fits to experimental pipi scattering amplitudes both at low and high energies that we performed in the previous papers of this series we then verify that the corresponding amplitudes satisfy analyticity requirements in the form of partial wave analyticity at low energies forward dispersion r... | [['we', 'complete', 'and', 'improve', 'the', 'fits', 'to', 'experimental', 'pipi', 'scattering', 'amplitudes', 'both', 'at', 'low', 'and', 'high', 'energies', 'that', 'we', 'performed', 'in', 'the', 'previous', 'papers', 'of', 'this', 'series', 'we', 'then', 'verify', 'that', 'the', 'corresponding', 'amplitudes', 'sati... | [-0.10085777619973602, 0.12616111031887722, -0.08489737998511344, 0.1135385265992383, -0.07817354150105016, -0.12745621461604087, 0.10122252968114949, 0.3304770911123855, -0.21986858089785863, -0.30902176306931517, 0.09588497413245195, -0.283694122340873, -0.10314866162242334, 0.18988967628041112, 0.025634260391073724,... |
710.1151 | Optimal properties of some Bayesian inferences | Relative surprise regions are shown to minimize, among Bayesian credible
regions, the prior probability of covering a false value from the prior. Such
regions are also shown to be unbiased in the sense that the prior probability
of covering a false value is bounded above by the prior probability of covering
the true ... | math.ST stat.TH | relative surprise regions are shown to minimize among bayesian credible regions the prior probability of covering a false value from the prior such regions are also shown to be unbiased in the sense that the prior probability of covering a false value is bounded above by the prior probability of covering the true value... | [['relative', 'surprise', 'regions', 'are', 'shown', 'to', 'minimize', 'among', 'bayesian', 'credible', 'regions', 'the', 'prior', 'probability', 'of', 'covering', 'a', 'false', 'value', 'from', 'the', 'prior', 'such', 'regions', 'are', 'also', 'shown', 'to', 'be', 'unbiased', 'in', 'the', 'sense', 'that', 'the', 'prio... | [-0.04915926254090244, 0.0742292215089457, -0.02703385553860034, 0.11496885054265686, -0.036318480178194404, -0.05134171248377802, 0.1387093975029599, 0.4009931154052118, -0.25144362372632784, -0.33747183731219804, 0.06836914624615859, -0.26034224305140713, -0.09438908263557376, 0.1370330561946433, -0.12166822454338007... |
710.1152 | Convexity properties of gradient maps | We consider the action of a real reductive group G on a Kaehler manifold Z
which is the restriction of a holomorphic action of the complexified group G^C.
We assume that the induced action of a compatible maximal compact subgroup U of
G^C on Z is Hamiltonian. We have an associated gradient map obtained from a
Cartan ... | math.CV | we consider the action of a real reductive group g on a kaehler manifold z which is the restriction of a holomorphic action of the complexified group gc we assume that the induced action of a compatible maximal compact subgroup u of gc on z is hamiltonian we have an associated gradient map obtained from a cartan decomp... | [['we', 'consider', 'the', 'action', 'of', 'a', 'real', 'reductive', 'group', 'g', 'on', 'a', 'kaehler', 'manifold', 'z', 'which', 'is', 'the', 'restriction', 'of', 'a', 'holomorphic', 'action', 'of', 'the', 'complexified', 'group', 'gc', 'we', 'assume', 'that', 'the', 'induced', 'action', 'of', 'a', 'compatible', 'max... | [-0.20873899071536087, 0.0453445238255537, -0.11916637658938631, 0.0035619879307158225, -0.11346785831139297, -0.09325230930856354, 0.05146662432381564, 0.38543637210989856, -0.3113146845234541, -0.1564709877695989, 0.06795667066566043, -0.2535573605045274, -0.10413805238046758, 0.1809298461135309, -0.114939086164373, ... |
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