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710.0653 | Study of the critical point in lattice QCD at high temperature and
density | We propose a method to probe the nature of phase transitions in lattice QCD
at finite temperature and density, which is based on the investigation of an
effective potential as a function of the average plaquette. We analyze data
obtained in a simulation of two-flavor QCD using p4-improved staggered quarks
with bare q... | hep-lat | we propose a method to probe the nature of phase transitions in lattice qcd at finite temperature and density which is based on the investigation of an effective potential as a function of the average plaquette we analyze data obtained in a simulation of twoflavor qcd using p4improved staggered quarks with bare quark m... | [['we', 'propose', 'a', 'method', 'to', 'probe', 'the', 'nature', 'of', 'phase', 'transitions', 'in', 'lattice', 'qcd', 'at', 'finite', 'temperature', 'and', 'density', 'which', 'is', 'based', 'on', 'the', 'investigation', 'of', 'an', 'effective', 'potential', 'as', 'a', 'function', 'of', 'the', 'average', 'plaquette',... | [-0.11325320688373378, 0.19329837909892125, -0.10864348302932521, 0.04851168246161, 0.009709069493290937, -0.03477487297214825, 0.12203142331142364, 0.34769606004180065, -0.17302591322343155, -0.2978888877249997, 0.0584524641714685, -0.27827006006003197, -0.10481495297802933, 0.07371270837230158, 0.0850123844976569, 0.... |
710.0654 | Steady-state analysis of a multi-server queue in the Halfin-Whitt regime | We consider a multi-server queue in the Halfin-Whitt regime: as the number of
servers $n$ grows without a bound, the utilization approaches 1 from below at
the rate $\Theta(1/\sqrt{n})$. Assuming that the service time distribution is
lattice-valued with a finite support, we characterize the limiting stationary
queue ... | math.PR | we consider a multiserver queue in the halfinwhitt regime as the number of servers n grows without a bound the utilization approaches 1 from below at the rate theta1sqrtn assuming that the service time distribution is latticevalued with a finite support we characterize the limiting stationary queue length distribution ... | [['we', 'consider', 'a', 'multiserver', 'queue', 'in', 'the', 'halfinwhitt', 'regime', 'as', 'the', 'number', 'of', 'servers', 'n', 'grows', 'without', 'a', 'bound', 'the', 'utilization', 'approaches', '1', 'from', 'below', 'at', 'the', 'rate', 'theta1sqrtn', 'assuming', 'that', 'the', 'service', 'time', 'distribution'... | [-0.20384238716665534, 0.1333348944114527, -0.08119488711423811, 0.06782969658923967, 0.019391854418039832, -0.1349176335291216, 0.13302344654455797, 0.3285672151513638, -0.2704988590651943, -0.23046610605031734, 0.10954933558898647, -0.2894757069429503, -0.0595542622031644, 0.18266399357197505, -0.06305475562300172, 0... |
710.0655 | Unique Games with Entangled Provers are Easy | We consider one-round games between a classical verifier and two provers who
share entanglement. We show that when the constraints enforced by the verifier
are `unique' constraints (i.e., permutations), the value of the game can be
well approximated by a semidefinite program. Essentially the only algorithm
known prev... | quant-ph | we consider oneround games between a classical verifier and two provers who share entanglement we show that when the constraints enforced by the verifier are unique constraints ie permutations the value of the game can be well approximated by a semidefinite program essentially the only algorithm known previously was fo... | [['we', 'consider', 'oneround', 'games', 'between', 'a', 'classical', 'verifier', 'and', 'two', 'provers', 'who', 'share', 'entanglement', 'we', 'show', 'that', 'when', 'the', 'constraints', 'enforced', 'by', 'the', 'verifier', 'are', 'unique', 'constraints', 'ie', 'permutations', 'the', 'value', 'of', 'the', 'game', '... | [-0.10774258950863172, 0.03501317447010445, -0.16498056951289375, 0.09930227277627973, -0.07786110133726012, -0.25883316783648397, 0.11693920808223386, 0.3295693694648367, -0.30108084078119307, -0.3213878856488952, 0.10372939948294381, -0.26087682732656875, -0.1355542181128705, 0.20597668508136713, -0.12630179844434478... |
710.0656 | Measurement of b-Baryons with the CDF II detector | We report the observation of new bottom baryon states. The most recent result
is the observation of the baryon \Xi_b^- through the decay \Xi_b^- to J/\psi
\Xi^-. The significance of the signal corresponds to 7.7 sigma and the \Xi_b^-
mass is measured to be 5792.9 \pm 2.5(stat.) \pm 1.7(syst.) MeV/c^2. In
addition we ... | hep-ex | we report the observation of new bottom baryon states the most recent result is the observation of the baryon xi_b through the decay xi_b to jpsi xi the significance of the signal corresponds to 77 sigma and the xi_b mass is measured to be 57929 pm 25stat pm 17syst mevc2 in addition we observe four resonances in the la... | [['we', 'report', 'the', 'observation', 'of', 'new', 'bottom', 'baryon', 'states', 'the', 'most', 'recent', 'result', 'is', 'the', 'observation', 'of', 'the', 'baryon', 'xi_b', 'through', 'the', 'decay', 'xi_b', 'to', 'jpsi', 'xi', 'the', 'significance', 'of', 'the', 'signal', 'corresponds', 'to', '77', 'sigma', 'and',... | [-0.10782700180503968, 0.2304619057544482, -0.08561637611254244, 0.0670817649224773, -0.02869694763354051, -0.08159836445230285, 0.07713573714529441, 0.2902904869736852, -0.13505029764083037, -0.29774269834160805, -0.047638364716722455, -0.43980088331610767, 0.07014056079945452, 0.11156967792634827, 0.05396094935870654... |
710.0657 | A Multiresolution Census Algorithm for Calculating Vortex Statistics in
Turbulent Flows | The fundamental equations that model turbulent flow do not provide much
insight into the size and shape of observed turbulent structures. We
investigate the efficient and accurate representation of structures in
two-dimensional turbulence by applying statistical models directly to the
simulated vorticity field. Rathe... | stat.AP physics.ao-ph | the fundamental equations that model turbulent flow do not provide much insight into the size and shape of observed turbulent structures we investigate the efficient and accurate representation of structures in twodimensional turbulence by applying statistical models directly to the simulated vorticity field rather tha... | [['the', 'fundamental', 'equations', 'that', 'model', 'turbulent', 'flow', 'do', 'not', 'provide', 'much', 'insight', 'into', 'the', 'size', 'and', 'shape', 'of', 'observed', 'turbulent', 'structures', 'we', 'investigate', 'the', 'efficient', 'and', 'accurate', 'representation', 'of', 'structures', 'in', 'twodimensiona... | [-0.0728000377288513, 0.08582126226847003, -0.13436985599783888, 0.0878976024151167, -0.08755605176434313, -0.08552852392262011, -0.021143788718945233, 0.375296532727876, -0.31862531861764165, -0.30521084743617266, 0.09829520247110754, -0.2122714465582057, -0.1011123573284031, 0.19912794597289657, -0.014658865049121934... |
710.0658 | Detailed Network Measurements Using Sparse Graph Counters: The Theory | Measuring network flow sizes is important for tasks like accounting/billing,
network forensics and security. Per-flow accounting is considered hard because
it requires that many counters be updated at a very high speed; however, the
large fast memories needed for storing the counters are prohibitively
expensive. Ther... | cs.NI cs.IT math.IT | measuring network flow sizes is important for tasks like accountingbilling network forensics and security perflow accounting is considered hard because it requires that many counters be updated at a very high speed however the large fast memories needed for storing the counters are prohibitively expensive therefore cur... | [['measuring', 'network', 'flow', 'sizes', 'is', 'important', 'for', 'tasks', 'like', 'accountingbilling', 'network', 'forensics', 'and', 'security', 'perflow', 'accounting', 'is', 'considered', 'hard', 'because', 'it', 'requires', 'that', 'many', 'counters', 'be', 'updated', 'at', 'a', 'very', 'high', 'speed', 'howeve... | [-0.120017237540448, 0.08853900221929199, -0.08650995988009424, 0.09349195457143857, -0.08178215967964823, -0.21885559647370362, 0.05249760067419249, 0.41176468531185456, -0.2523895943021707, -0.3393192070741522, 0.14932796376820465, -0.24213506048808328, -0.12714991736157383, 0.20143037469594577, -0.11942603353852943,... |
710.0659 | The TrICE Prototype MAMPT Imaging Camera | The Track Imaging Cerenov Experiment (TrICE) is an air Cerenkov prototype
telescope designed to use multi-anode photomultiplier to acheive a high angular
resolution for measuring cosmic-ray composition at TeV-PeV energies. The TrICE
camera, composed of 16 Hamamatsu R8900 16-channel multi-anode photomultiplier
tubes, ... | astro-ph | the track imaging cerenov experiment trice is an air cerenkov prototype telescope designed to use multianode photomultiplier to acheive a high angular resolution for measuring cosmicray composition at tevpev energies the trice camera composed of 16 hamamatsu r8900 16channel multianode photomultiplier tubes achieves 008... | [['the', 'track', 'imaging', 'cerenov', 'experiment', 'trice', 'is', 'an', 'air', 'cerenkov', 'prototype', 'telescope', 'designed', 'to', 'use', 'multianode', 'photomultiplier', 'to', 'acheive', 'a', 'high', 'angular', 'resolution', 'for', 'measuring', 'cosmicray', 'composition', 'at', 'tevpev', 'energies', 'the', 'tri... | [-0.08615935645701195, 0.17163302080734866, -0.018887030800352946, -0.027975022318335534, -0.055518681070569786, -0.1478173938354082, -0.07183583604637533, 0.4567883209974477, -0.12934377604643954, -0.4771391543644396, 0.042830734718308755, -0.3283809495976929, 0.03530013734637054, 0.22904736605105977, -0.0909062885312... |
710.066 | Effective Dynamics of Solitons in the Presence of Rough Nonlinear
Perturbations | The effective long-time dynamics of solitary wave solutions of the nonlinear
Schr\"odinger equation in the presence of rough nonlinear perturbations is
rigorously studied. It is shown that, if the initial state is close to a slowly
travelling soliton of the unperturbed NLS equation (in $H^1$ norm), then, over
a long ... | math-ph math.MP | the effective longtime dynamics of solitary wave solutions of the nonlinear schrodinger equation in the presence of rough nonlinear perturbations is rigorously studied it is shown that if the initial state is close to a slowly travelling soliton of the unperturbed nls equation in h1 norm then over a long time scale the... | [['the', 'effective', 'longtime', 'dynamics', 'of', 'solitary', 'wave', 'solutions', 'of', 'the', 'nonlinear', 'schrodinger', 'equation', 'in', 'the', 'presence', 'of', 'rough', 'nonlinear', 'perturbations', 'is', 'rigorously', 'studied', 'it', 'is', 'shown', 'that', 'if', 'the', 'initial', 'state', 'is', 'close', 'to'... | [-0.16191248037624634, 0.10717278877212436, -0.12198388078384316, 0.08978611183004802, -0.06712992096340263, -0.09676961781671987, -0.05987897709109258, 0.31482245191767977, -0.31779778359846755, -0.21617253639499892, 0.1440955579797686, -0.27844200141543707, -0.12593750649510504, 0.14627651842618053, 0.016716236954780... |
710.0661 | Self-consistent theory of phonon renormalization and electron-phonon
coupling near a 2D Kohn singularity | We show that the usual expression for evaluating electron-phonon coupling and
the phonon linewidth in 2D metals with a cylindrical Fermi surface cannot be
applied near the wave vector corresponding to the Kohn singularity. Instead,
the Dyson equation for phonons has to be solved self-consistently. If a
self-consisten... | cond-mat.supr-con cond-mat.str-el | we show that the usual expression for evaluating electronphonon coupling and the phonon linewidth in 2d metals with a cylindrical fermi surface cannot be applied near the wave vector corresponding to the kohn singularity instead the dyson equation for phonons has to be solved selfconsistently if a selfconsistent proced... | [['we', 'show', 'that', 'the', 'usual', 'expression', 'for', 'evaluating', 'electronphonon', 'coupling', 'and', 'the', 'phonon', 'linewidth', 'in', '2d', 'metals', 'with', 'a', 'cylindrical', 'fermi', 'surface', 'can', 'not', 'be', 'applied', 'near', 'the', 'wave', 'vector', 'corresponding', 'to', 'the', 'kohn', 'singu... | [-0.11732819521581972, 0.13844510286822673, -0.06458148160683257, 0.06473508119196086, -0.09950329075482758, -0.1384030049848189, 0.042261075446164455, 0.389691020712837, -0.2658466743970556, -0.18903509660490922, 0.010841340626372242, -0.31770799686382345, -0.13348683196289296, 0.1909742717443687, 0.05435521443761498,... |
710.0662 | Modeling the line variations from the wind-wind shock emissions of WR
30a | The study of Wolf-Rayet stars plays an important role in evolutionary
theories of massive stars. Among these objects, ~ 20% are known to be in binary
systems and can therefore be used for the mass determination of these stars.
Most of these systems are not spatially resolved and spectral lines can be used
to constrai... | astro-ph | the study of wolfrayet stars plays an important role in evolutionary theories of massive stars among these objects 20 are known to be in binary systems and can therefore be used for the mass determination of these stars most of these systems are not spatially resolved and spectral lines can be used to constrain the orb... | [['the', 'study', 'of', 'wolfrayet', 'stars', 'plays', 'an', 'important', 'role', 'in', 'evolutionary', 'theories', 'of', 'massive', 'stars', 'among', 'these', 'objects', '20', 'are', 'known', 'to', 'be', 'in', 'binary', 'systems', 'and', 'can', 'therefore', 'be', 'used', 'for', 'the', 'mass', 'determination', 'of', 't... | [-0.09929752960228003, 0.10584513156574804, -0.06535161166236951, 0.08285452419271072, -0.09801342214624852, -0.10302187361491796, 0.04126313464441456, 0.41620997016628586, -0.22028419045934405, -0.3525986816829596, 0.07535471678233872, -0.23528405215877754, -0.03962667705013584, 0.19022409836552703, -0.042470594918212... |
710.0663 | SAURON's Challenge for the Major Merger Scenario of Elliptical Galaxy
Formation | The intrinsic anisotropy delta and flattening epsilon of simulated merger
remnants is compared with elliptical galaxies that have been observed by the
SAURON collaboration, and that were analysed using axisymmetric Schwarzschild
models. Collisionless binary mergers of stellar disks and disk mergers with an
additional... | astro-ph | the intrinsic anisotropy delta and flattening epsilon of simulated merger remnants is compared with elliptical galaxies that have been observed by the sauron collaboration and that were analysed using axisymmetric schwarzschild models collisionless binary mergers of stellar disks and disk mergers with an additional iso... | [['the', 'intrinsic', 'anisotropy', 'delta', 'and', 'flattening', 'epsilon', 'of', 'simulated', 'merger', 'remnants', 'is', 'compared', 'with', 'elliptical', 'galaxies', 'that', 'have', 'been', 'observed', 'by', 'the', 'sauron', 'collaboration', 'and', 'that', 'were', 'analysed', 'using', 'axisymmetric', 'schwarzschild... | [-0.10545490137554463, 0.12658099686921798, -0.07305620152341283, 0.12696732545433484, -0.10788395221183157, -0.05280736443060248, -0.02691613286278089, 0.4240357621208481, -0.12259112937963042, -0.37220294588731356, 0.005956550453708548, -0.29695532251473356, -0.05453689360232523, 0.19566051792657083, -0.0013842293182... |
710.0664 | Synthesis and Optimization of Reversible Circuits for Homogeneous
Boolean Functions | Homogenous Boolean function is an essential part of any cryptographic system.
The ability to construct an optimized reversible circuits for homogeneous
Boolean functions might arise the possibility of building cryptographic system
on novel computing paradigms such as quantum computers. This paper shows a
factorizatio... | quant-ph | homogenous boolean function is an essential part of any cryptographic system the ability to construct an optimized reversible circuits for homogeneous boolean functions might arise the possibility of building cryptographic system on novel computing paradigms such as quantum computers this paper shows a factorization al... | [['homogenous', 'boolean', 'function', 'is', 'an', 'essential', 'part', 'of', 'any', 'cryptographic', 'system', 'the', 'ability', 'to', 'construct', 'an', 'optimized', 'reversible', 'circuits', 'for', 'homogeneous', 'boolean', 'functions', 'might', 'arise', 'the', 'possibility', 'of', 'building', 'cryptographic', 'syst... | [-0.18022775957931061, 0.01862265632965374, -0.0682527987400488, 0.04471316553500234, -0.057293561534309874, -0.20359504890951272, 0.006697061649827781, 0.373614418719496, -0.36779709798949106, -0.2467126270414007, 0.05657044838049582, -0.19537661585728733, -0.24106320392872607, 0.27273585202590545, -0.0745984083231614... |
710.0665 | Infrared exponents of gluon and ghost propagators from Lattice QCD | The compatibility of the pure power law infrared solution of QCD
Dyson-Schwinger equations (DSE) and lattice data for the gluon and ghost
propagators in Landau gauge is discussed. For the gluon propagator, the lattice
data is compatible with the DSE infrared solution with an exponent
$\kappa\sim0.53$, measured using ... | hep-lat | the compatibility of the pure power law infrared solution of qcd dysonschwinger equations dse and lattice data for the gluon and ghost propagators in landau gauge is discussed for the gluon propagator the lattice data is compatible with the dse infrared solution with an exponent kappasim053 measured using a technique t... | [['the', 'compatibility', 'of', 'the', 'pure', 'power', 'law', 'infrared', 'solution', 'of', 'qcd', 'dysonschwinger', 'equations', 'dse', 'and', 'lattice', 'data', 'for', 'the', 'gluon', 'and', 'ghost', 'propagators', 'in', 'landau', 'gauge', 'is', 'discussed', 'for', 'the', 'gluon', 'propagator', 'the', 'lattice', 'da... | [-0.07960856122123759, 0.16038424639395443, -0.20466703973801398, 0.07152569614543874, -0.1402415504782722, -0.09883050478018093, 0.06177888245026513, 0.3481478037585209, -0.2166602120098726, -0.20244820147366605, 0.0816200814513694, -0.32368285648781014, -0.06020439585398247, 0.0968859494300332, -0.005061121646133138,... |
710.0666 | Thiol density dependent classical potential for methyl-thiol on a
Au(111) surface | A new classical potential for methyl-thiol on a Au(111) surface has been
developed using density functional theory electronic structure calculations.
Energy surfaces between methyl-thiol and a gold surface were investigated in
terms of symmetry sites and thiol density. Geometrical optimization was
employed over all t... | cond-mat.mtrl-sci cond-mat.soft | a new classical potential for methylthiol on a au111 surface has been developed using density functional theory electronic structure calculations energy surfaces between methylthiol and a gold surface were investigated in terms of symmetry sites and thiol density geometrical optimization was employed over all the confi... | [['a', 'new', 'classical', 'potential', 'for', 'methylthiol', 'on', 'a', 'au111', 'surface', 'has', 'been', 'developed', 'using', 'density', 'functional', 'theory', 'electronic', 'structure', 'calculations', 'energy', 'surfaces', 'between', 'methylthiol', 'and', 'a', 'gold', 'surface', 'were', 'investigated', 'in', 'te... | [-0.09503737407774754, 0.10142789023277694, -0.11117713318895293, 0.0651967487718961, -0.003885989337330301, -0.12390422783409284, 0.02309510879671482, 0.4374514161768586, -0.2169326957289691, -0.347167635770285, 0.000339055331806614, -0.2854972377878754, -0.16842006800109394, 0.17700887903609402, 0.023696095641217614,... |
710.0667 | Chaotic Period Doubling | The period doubling renormalization operator was introduced by M. Feigenbaum
and by P. Coullet and C. Tresser in the nineteen-seventieth to study the
asymptotic small scale geometry of the attractor of one-dimensional systems
which are at the transition from simple to chaotic dynamics. This geometry
turns out to not ... | math.DS | the period doubling renormalization operator was introduced by m feigenbaum and by p coullet and c tresser in the nineteenseventieth to study the asymptotic small scale geometry of the attractor of onedimensional systems which are at the transition from simple to chaotic dynamics this geometry turns out to not depend o... | [['the', 'period', 'doubling', 'renormalization', 'operator', 'was', 'introduced', 'by', 'm', 'feigenbaum', 'and', 'by', 'p', 'coullet', 'and', 'c', 'tresser', 'in', 'the', 'nineteenseventieth', 'to', 'study', 'the', 'asymptotic', 'small', 'scale', 'geometry', 'of', 'the', 'attractor', 'of', 'onedimensional', 'systems'... | [-0.13176148094180634, 0.1323276561797338, -0.12136436173224914, 0.10136951423009341, -0.05945493361006133, -0.15089569533927216, 0.05247579067024781, 0.326946544866414, -0.27384040576225227, -0.2125437999066291, 0.14776911141643895, -0.2590130957112623, -0.16332620539447512, 0.18201230407494187, -0.08552235257971195, ... |
710.0668 | Visible and invisible molecular gas in collisional debris of galaxies | Molecular gas has been searched for and found in unexpectedly large
quantities in some collisional debris of interacting galaxies: HI-rich tidal
tails, bridges and collisional rings. It was so far observed through millimeter
observations of the CO line and detected towards or near regions of
star-formation associated... | astro-ph | molecular gas has been searched for and found in unexpectedly large quantities in some collisional debris of interacting galaxies hirich tidal tails bridges and collisional rings it was so far observed through millimeter observations of the co line and detected towards or near regions of starformation associated to den... | [['molecular', 'gas', 'has', 'been', 'searched', 'for', 'and', 'found', 'in', 'unexpectedly', 'large', 'quantities', 'in', 'some', 'collisional', 'debris', 'of', 'interacting', 'galaxies', 'hirich', 'tidal', 'tails', 'bridges', 'and', 'collisional', 'rings', 'it', 'was', 'so', 'far', 'observed', 'through', 'millimeter'... | [-0.1264558666458115, 0.13546655943515007, -0.06170650269188804, 0.10441805508552778, -0.056373214394581025, -0.06997071919258593, 0.013948410018290416, 0.3830800733710753, -0.18479874253943107, -0.2983697172277039, 0.046558625277745104, -0.2985686552313315, -0.016054140812740092, 0.13748783004759788, 0.033054998036998... |
710.0669 | Gauge fixing methods and Gribov copies effects in lattice QCD | We compare two Landau gauge fixing methods, aiming to find the global maximum
of the gauge fixing functional. Moreover, a systematic effect of Gribov copies
in the gluon and ghost propagators computed in Landau gauge is presented and
discussed.
| hep-lat | we compare two landau gauge fixing methods aiming to find the global maximum of the gauge fixing functional moreover a systematic effect of gribov copies in the gluon and ghost propagators computed in landau gauge is presented and discussed | [['we', 'compare', 'two', 'landau', 'gauge', 'fixing', 'methods', 'aiming', 'to', 'find', 'the', 'global', 'maximum', 'of', 'the', 'gauge', 'fixing', 'functional', 'moreover', 'a', 'systematic', 'effect', 'of', 'gribov', 'copies', 'in', 'the', 'gluon', 'and', 'ghost', 'propagators', 'computed', 'in', 'landau', 'gauge',... | [-0.15381253806826395, 0.22196362301325187, -0.13144695171369955, 0.14517016429752588, -0.07819716895046906, -0.07363233413212956, 0.07358363621796553, 0.35474160724343395, -0.1466920221081147, -0.27427317842076987, -0.001253486533338825, -0.22056985309777352, -0.12360505196146476, 0.006396923596278215, -0.039960958326... |
710.067 | Evolution of Schrodinger Uncertainty Relation in Quantum Mechanics | In the present article, we discuss one of the basic relations of Quantum
Mechanics - the Uncertainty Relation (UR). In 1930, few years after Heisenberg,
Erwin Schrodinger generalized the famous Uncertainty Relation in Quantum
Mechanics, making it more precise than the original. The present study
discusses recent gene... | quant-ph | in the present article we discuss one of the basic relations of quantum mechanics the uncertainty relation ur in 1930 few years after heisenberg erwin schrodinger generalized the famous uncertainty relation in quantum mechanics making it more precise than the original the present study discusses recent generalizations ... | [['in', 'the', 'present', 'article', 'we', 'discuss', 'one', 'of', 'the', 'basic', 'relations', 'of', 'quantum', 'mechanics', 'the', 'uncertainty', 'relation', 'ur', 'in', '1930', 'few', 'years', 'after', 'heisenberg', 'erwin', 'schrodinger', 'generalized', 'the', 'famous', 'uncertainty', 'relation', 'in', 'quantum', '... | [-0.08342452280245902, 0.09732379713997004, -0.08679462039858223, 0.13615664302168654, -0.1043663864594794, -0.13451854142570688, 0.014289516296553156, 0.2918670069005701, -0.26757288251012085, -0.28836077028104373, 0.0785591525603987, -0.29983587124414984, -0.20919129567881745, 0.2033550193563344, -0.16784643625179607... |
710.0671 | The Cosmos in Your Pocket: How Cosmological Science Became Earth
Technology. I | Astronomy provides a laboratory for extreme physics, a window into
environments at extremes of distance, temperature and density that often can't
be reproduced in Earth laboratories, or at least not right away. A surprising
amount of the science we understand today started out as solutions to problems
in astronomy. S... | physics.pop-ph astro-ph | astronomy provides a laboratory for extreme physics a window into environments at extremes of distance temperature and density that often cant be reproduced in earth laboratories or at least not right away a surprising amount of the science we understand today started out as solutions to problems in astronomy some of t... | [['astronomy', 'provides', 'a', 'laboratory', 'for', 'extreme', 'physics', 'a', 'window', 'into', 'environments', 'at', 'extremes', 'of', 'distance', 'temperature', 'and', 'density', 'that', 'often', 'cant', 'be', 'reproduced', 'in', 'earth', 'laboratories', 'or', 'at', 'least', 'not', 'right', 'away', 'a', 'surprising... | [-0.07502245504550542, 0.13096035638222872, -0.12625090957654617, 0.07979932487198105, -0.08031400422789628, -0.09790906717387747, 0.028535504779731265, 0.37230707120291795, -0.2759524611402539, -0.36726690056627687, 0.15497412749630976, -0.28978314432256586, -0.12903863714147312, 0.24542406995049854, -0.06252943086614... |
710.0672 | Optimization of supply diversity for the self-assembly of simple objects
in two and three dimensions | The field of algorithmic self-assembly is concerned with the design and
analysis of self-assembly systems from a computational perspective, that is,
from the perspective of mathematical problems whose study may give insight into
the natural processes through which elementary objects self-assemble into more
complex on... | cs.NE | the field of algorithmic selfassembly is concerned with the design and analysis of selfassembly systems from a computational perspective that is from the perspective of mathematical problems whose study may give insight into the natural processes through which elementary objects selfassemble into more complex ones one ... | [['the', 'field', 'of', 'algorithmic', 'selfassembly', 'is', 'concerned', 'with', 'the', 'design', 'and', 'analysis', 'of', 'selfassembly', 'systems', 'from', 'a', 'computational', 'perspective', 'that', 'is', 'from', 'the', 'perspective', 'of', 'mathematical', 'problems', 'whose', 'study', 'may', 'give', 'insight', 'i... | [-0.06678465065406872, 0.06417004738447994, -0.12197846963027785, 0.03751420787437401, -0.12730494802959527, -0.1286255836292988, 0.0635022034101557, 0.3484061263243994, -0.28967088633949684, -0.3408400510688345, 0.08628670194689751, -0.236363960968964, -0.16636888499473348, 0.1838224497298724, -0.0800005205749442, 0.0... |
710.0673 | Phase diagram of the one-dimensional half-filled extended Hubbard model | We study the ground state of the one-dimensional half-filled Hubbard model
with on-site (nearest-neighbor) repulsive interaction $U$ ($V$) and
nearest-neighbor hopping $t$. In order to obtain an accurate phase diagram, we
consider various physical quantities such as the charge gap, spin gap,
Luttinger-liquid exponent... | cond-mat.str-el | we study the ground state of the onedimensional halffilled hubbard model with onsite nearestneighbor repulsive interaction u v and nearestneighbor hopping t in order to obtain an accurate phase diagram we consider various physical quantities such as the charge gap spin gap luttingerliquid exponents and bondorderwave bo... | [['we', 'study', 'the', 'ground', 'state', 'of', 'the', 'onedimensional', 'halffilled', 'hubbard', 'model', 'with', 'onsite', 'nearestneighbor', 'repulsive', 'interaction', 'u', 'v', 'and', 'nearestneighbor', 'hopping', 't', 'in', 'order', 'to', 'obtain', 'an', 'accurate', 'phase', 'diagram', 'we', 'consider', 'various... | [-0.17046628482330028, 0.1954820143809979, -0.043995402619918016, 0.039134311139153326, -0.0341296130280713, -0.14977949750419076, 0.14647778081680424, 0.3827981970127269, -0.26359705755497975, -0.24669742095964955, 0.009212606272671089, -0.3412685761928908, -0.10202392807900253, 0.12412662729443928, 0.0921892579384515... |
710.0674 | New phases of finite temperature gauge theory from an extended action | We study the behavior of the order parameter, the phase diagram, and the
thermodynamics of exotic phases of finite temperature gauge theory. Lattice
simulations were performed in SU(3) and SU(4) with an adjoint Polyakov loop
term added to the standard Wilson action. In SU(3), the pattern of Z(3)
symmetry breaking in ... | hep-lat | we study the behavior of the order parameter the phase diagram and the thermodynamics of exotic phases of finite temperature gauge theory lattice simulations were performed in su3 and su4 with an adjoint polyakov loop term added to the standard wilson action in su3 the pattern of z3 symmetry breaking in the new phase i... | [['we', 'study', 'the', 'behavior', 'of', 'the', 'order', 'parameter', 'the', 'phase', 'diagram', 'and', 'the', 'thermodynamics', 'of', 'exotic', 'phases', 'of', 'finite', 'temperature', 'gauge', 'theory', 'lattice', 'simulations', 'were', 'performed', 'in', 'su3', 'and', 'su4', 'with', 'an', 'adjoint', 'polyakov', 'lo... | [-0.17963550360685196, 0.2611181240805455, -0.14008018909247988, 0.05999118721728787, -0.046382828201684684, -0.08878915478014435, 0.08426731362741327, 0.36026659250409915, -0.18267270293312543, -0.24377765643382163, 0.0883711112164563, -0.2893165782696069, -0.09997420928751428, 0.020972069435179083, 0.0447485266780160... |
710.0675 | Finding pulsars with LOFAR | We investigate the number and type of pulsars that will be discovered with
the low-frequency radio telescope LOFAR. We consider different search
strategies for the Galaxy, for globular clusters and for galaxies other than
our own. We show an all-sky Galactic survey can be optimally carried out by
incoherently combini... | astro-ph | we investigate the number and type of pulsars that will be discovered with the lowfrequency radio telescope lofar we consider different search strategies for the galaxy for globular clusters and for galaxies other than our own we show an allsky galactic survey can be optimally carried out by incoherently combining the ... | [['we', 'investigate', 'the', 'number', 'and', 'type', 'of', 'pulsars', 'that', 'will', 'be', 'discovered', 'with', 'the', 'lowfrequency', 'radio', 'telescope', 'lofar', 'we', 'consider', 'different', 'search', 'strategies', 'for', 'the', 'galaxy', 'for', 'globular', 'clusters', 'and', 'for', 'galaxies', 'other', 'than... | [-0.09616294882555561, 0.13579206824348458, -0.05991715874534282, 0.1447179634386685, -0.1860621518586058, -0.02266729841712953, 0.10154624391778759, 0.42436399994554314, -0.17006658495789984, -0.3563130368683033, 0.03804208725767506, -0.3195526133654866, -0.0069444177504742475, 0.2896087450492082, -0.00278112142085574... |
710.0676 | Remarks on the symmetric powers of cusp forms on GL(2) | In this paper we prove the following conditional result: Let F be a number
field, and pi a cusp form on GL(2)/F which is not solvable polyhedral. Assume
that all the symmetric powers sym^m(pi) are modular, i.e., define automorphic
forms on GL(m+1)/F. If sym^6(pi) is cuspidal, then all the symmetric powers are
cuspida... | math.NT math.RT | in this paper we prove the following conditional result let f be a number field and pi a cusp form on gl2f which is not solvable polyhedral assume that all the symmetric powers symmpi are modular ie define automorphic forms on glm1f if sym6pi is cuspidal then all the symmetric powers are cuspidal for all m moreover sym... | [['in', 'this', 'paper', 'we', 'prove', 'the', 'following', 'conditional', 'result', 'let', 'f', 'be', 'a', 'number', 'field', 'and', 'pi', 'a', 'cusp', 'form', 'on', 'gl2f', 'which', 'is', 'not', 'solvable', 'polyhedral', 'assume', 'that', 'all', 'the', 'symmetric', 'powers', 'symmpi', 'are', 'modular', 'ie', 'define'... | [-0.22342460745244058, 0.1472630386874639, -0.1281508741682613, -0.00011856954502449794, -0.13451435942468898, -0.12467826932499354, -0.0747412212008562, 0.3250828783039923, -0.301564979475814, -0.14251219748531457, 0.06907366236593188, -0.2611421174067375, -0.1853282761264157, 0.19403790038490257, -0.05730903461970867... |
710.0677 | The divided cell algorithm and the inhomogeneous Lagrange and Markoff
spectra | The divided cell algorithm was introduced by Delone in 1947 to calculate the
inhomogeneous minima of binary quadratic forms and developed further by E. S.
Barnes and H. P. F. Swinnerton-Dyer in the 1950s. We show how advances of the
past fifty years in both symbolic computation and our understanding of
homogeneous sp... | math.NT | the divided cell algorithm was introduced by delone in 1947 to calculate the inhomogeneous minima of binary quadratic forms and developed further by e s barnes and h p f swinnertondyer in the 1950s we show how advances of the past fifty years in both symbolic computation and our understanding of homogeneous spectra can... | [['the', 'divided', 'cell', 'algorithm', 'was', 'introduced', 'by', 'delone', 'in', '1947', 'to', 'calculate', 'the', 'inhomogeneous', 'minima', 'of', 'binary', 'quadratic', 'forms', 'and', 'developed', 'further', 'by', 'e', 's', 'barnes', 'and', 'h', 'p', 'f', 'swinnertondyer', 'in', 'the', '1950s', 'we', 'show', 'how... | [-0.09474821763848193, 0.08722012828312013, -0.08587858772043847, 0.06518898501007026, -0.04574011051103719, -0.11837818481659224, 0.0976334230489413, 0.31614233298642824, -0.2736113822464793, -0.2959997544049724, 0.07880782537462483, -0.24209159142195827, -0.15632558056761411, 0.23637404029203718, -0.08619750701713622... |
710.0678 | Calculated Momentum Dependence of Zhang-Rice States in Transition Metal
Oxides | Using a combination of local density functional theory and cluster exact
diagonalization based dynamical mean field theory, we calculate many body
electronic structures of several Mott insulating oxides including undoped high
T_{c} materials. The dispersions of the lowest occupied electronic states are
associated wit... | cond-mat.str-el | using a combination of local density functional theory and cluster exact diagonalization based dynamical mean field theory we calculate many body electronic structures of several mott insulating oxides including undoped high t_c materials the dispersions of the lowest occupied electronic states are associated with the ... | [['using', 'a', 'combination', 'of', 'local', 'density', 'functional', 'theory', 'and', 'cluster', 'exact', 'diagonalization', 'based', 'dynamical', 'mean', 'field', 'theory', 'we', 'calculate', 'many', 'body', 'electronic', 'structures', 'of', 'several', 'mott', 'insulating', 'oxides', 'including', 'undoped', 'high', ... | [-0.11688496842798048, 0.1734100288083126, -0.025216069636327856, 0.0885294267391584, -0.003697223557406161, -0.16956662372209086, 0.09425844317111004, 0.3944980550994984, -0.20872300034613314, -0.30876686820109567, -0.0009819594554109387, -0.3779451483299574, -0.1362237269171031, 0.11089109816007788, 0.071178694322974... |
710.0679 | Antisymmetric tensor matter fields in a curved space-time | An analysis about the antisymmetric tensor matter fields Avdeev-Chizhov
theory in a curved space-time is performed. We show, in a curved spacetime,
that the Avdeev-Chizhov theory can be seen as a kind of a $\lambda\phi^{4}$
theory for a "complex self-dual" field. This relationship between
Avdeev-Chizhov theory and $\... | hep-th | an analysis about the antisymmetric tensor matter fields avdeevchizhov theory in a curved spacetime is performed we show in a curved spacetime that the avdeevchizhov theory can be seen as a kind of a lambdaphi4 theory for a complex selfdual field this relationship between avdeevchizhov theory and lambdaphi4 theory simp... | [['an', 'analysis', 'about', 'the', 'antisymmetric', 'tensor', 'matter', 'fields', 'avdeevchizhov', 'theory', 'in', 'a', 'curved', 'spacetime', 'is', 'performed', 'we', 'show', 'in', 'a', 'curved', 'spacetime', 'that', 'the', 'avdeevchizhov', 'theory', 'can', 'be', 'seen', 'as', 'a', 'kind', 'of', 'a', 'lambdaphi4', 't... | [-0.17523707600776106, 0.18849434074111152, -0.15409261990776835, 0.12881256134064376, -0.10381955954739276, -0.09371650488773252, -0.13814807946362315, 0.32145729269284534, -0.19807519002214952, -0.25125833929461594, 0.029982687318218213, -0.2053105293718331, -0.2454536447630209, 0.10968106791979688, -0.01104382252978... |
710.068 | Dynamical Threshold Enhancement and Resummation in Drell-Yan Production | Partonic cross sections for the production of massive objects in hadronic
collisions receive large corrections when the invariant mass of the
initial-state partons is just above the production threshold. Since typically
the center-of-mass energy of the hadronic collision is much higher than the
mass of the heavy obje... | hep-ph | partonic cross sections for the production of massive objects in hadronic collisions receive large corrections when the invariant mass of the initialstate partons is just above the production threshold since typically the centerofmass energy of the hadronic collision is much higher than the mass of the heavy objects it... | [['partonic', 'cross', 'sections', 'for', 'the', 'production', 'of', 'massive', 'objects', 'in', 'hadronic', 'collisions', 'receive', 'large', 'corrections', 'when', 'the', 'invariant', 'mass', 'of', 'the', 'initialstate', 'partons', 'is', 'just', 'above', 'the', 'production', 'threshold', 'since', 'typically', 'the', ... | [-0.07007262223202776, 0.17498241707186896, -0.16277514493128326, 0.17346828675209983, -0.01958242800522029, -0.01839345471418473, -0.024119235581842393, 0.3511845244843837, -0.17182634816297493, -0.26511537100431387, -0.028157480982253732, -0.34481164620197174, 0.030076813300737464, 0.11921369688175416, 0.051041318608... |
710.0681 | Yang-Mills theory over surfaces and the Atiyah-Segal theorem | In this paper we explain how Morse theory for the Yang-Mills functional can
be used to prove an analogue, for surface groups, of the Atiyah-Segal theorem.
Classically, the Atiyah-Segal theorem relates the representation ring R(\Gamma)
of a compact Lie group $\Gamma$ to the complex K-theory of the classifying
space $B... | math.AT math.DG math.KT | in this paper we explain how morse theory for the yangmills functional can be used to prove an analogue for surface groups of the atiyahsegal theorem classically the atiyahsegal theorem relates the representation ring rgamma of a compact lie group gamma to the complex ktheory of the classifying space bgamma for infinit... | [['in', 'this', 'paper', 'we', 'explain', 'how', 'morse', 'theory', 'for', 'the', 'yangmills', 'functional', 'can', 'be', 'used', 'to', 'prove', 'an', 'analogue', 'for', 'surface', 'groups', 'of', 'the', 'atiyahsegal', 'theorem', 'classically', 'the', 'atiyahsegal', 'theorem', 'relates', 'the', 'representation', 'ring'... | [-0.1418283579441777, 0.07846295155673033, -0.16798248936174787, 0.11593321581858618, -0.09378078324516537, -0.11574473769360338, -0.007140135330701014, 0.36354208424745593, -0.31934994882249157, -0.21750654919287626, 0.0672826233521846, -0.19941202524114487, -0.17621959732059622, 0.20313765783066629, -0.16646893085999... |
710.0682 | Demonstration of a New Transport Regime of Photon in Two-dimensional
Photonic Crystal | A new transport regime of photon in two-dimensional photonic crystal near the
Dirac point has been demonstrated by exact numerical simulation. In this
regime, the conductance of photon is inversely proportional to the thickness of
sample, which can be described by Dirac equation very well. Both of bulk and
surface di... | cond-mat.mtrl-sci cond-mat.dis-nn | a new transport regime of photon in twodimensional photonic crystal near the dirac point has been demonstrated by exact numerical simulation in this regime the conductance of photon is inversely proportional to the thickness of sample which can be described by dirac equation very well both of bulk and surface disorders... | [['a', 'new', 'transport', 'regime', 'of', 'photon', 'in', 'twodimensional', 'photonic', 'crystal', 'near', 'the', 'dirac', 'point', 'has', 'been', 'demonstrated', 'by', 'exact', 'numerical', 'simulation', 'in', 'this', 'regime', 'the', 'conductance', 'of', 'photon', 'is', 'inversely', 'proportional', 'to', 'the', 'thi... | [-0.125023168276722, 0.1695355329013199, -0.071718339695074, 0.0081239655430198, -0.015407185693946453, -0.1690054168249694, 0.04690556917681333, 0.36073442381046233, -0.24920334696872246, -0.33140036012601415, 0.014874404172387418, -0.32695279936861554, -0.14598847835307616, 0.21753542076522878, -0.025608778298926462,... |
710.0683 | The One-Dimensional Wigner Crystal in Carbon Nanotubes | Electron-electron interactions strongly affect the behavior of
low-dimensional systems. In one dimension (1D), arbitrarily weak interactions
qualitatively alter the ground state producing a Luttinger liquid (LL) which
has now been observed in a number of experimental systems. Interactions are
even more important at l... | cond-mat.str-el cond-mat.mes-hall | electronelectron interactions strongly affect the behavior of lowdimensional systems in one dimension 1d arbitrarily weak interactions qualitatively alter the ground state producing a luttinger liquid ll which has now been observed in a number of experimental systems interactions are even more important at low carrier ... | [['electronelectron', 'interactions', 'strongly', 'affect', 'the', 'behavior', 'of', 'lowdimensional', 'systems', 'in', 'one', 'dimension', '1d', 'arbitrarily', 'weak', 'interactions', 'qualitatively', 'alter', 'the', 'ground', 'state', 'producing', 'a', 'luttinger', 'liquid', 'll', 'which', 'has', 'now', 'been', 'obse... | [-0.15243796683142946, 0.22272515597942402, -0.08438628892925205, 0.023371850400386997, -0.005568478116118866, -0.16811524477088824, 0.0220402783054548, 0.3872239805602779, -0.25143216371846694, -0.2851004267266641, 0.039805637484338754, -0.29682477636314514, -0.10985598756621281, 0.18278035763909833, 0.028646701674895... |
710.0684 | Quantum Control Landscapes | Numerous lines of experimental, numerical and analytical evidence indicate
that it is surprisingly easy to locate optimal controls steering quantum
dynamical systems to desired objectives. This has enabled the control of
complex quantum systems despite the expense of solving the Schrodinger equation
in simulations an... | quant-ph | numerous lines of experimental numerical and analytical evidence indicate that it is surprisingly easy to locate optimal controls steering quantum dynamical systems to desired objectives this has enabled the control of complex quantum systems despite the expense of solving the schrodinger equation in simulations and th... | [['numerous', 'lines', 'of', 'experimental', 'numerical', 'and', 'analytical', 'evidence', 'indicate', 'that', 'it', 'is', 'surprisingly', 'easy', 'to', 'locate', 'optimal', 'controls', 'steering', 'quantum', 'dynamical', 'systems', 'to', 'desired', 'objectives', 'this', 'has', 'enabled', 'the', 'control', 'of', 'compl... | [-0.1348104924616343, 0.07395684121341975, -0.10026966742561938, 0.04123476547489343, -0.07402616791496767, -0.14963168239277552, 0.06310671731333518, 0.3815198917655605, -0.2827836179487825, -0.2921078768210642, 0.09457655369617463, -0.25024174712598324, -0.2082385976513778, 0.25829025754861745, -0.05965355339364332, ... |
710.0685 | Uniformly Balanced Repeated Measurements Designs in the Presence of
Subject Dropout | Low, Lewis and Prescott (1999) showed that a crossover design based on a
Williams Latin square of order 4 can suffer substantial loss of efficiency if
some observations in the final period are unavailable. Indeed, if all
observations are missing, the design becomes disconnected. We derive the
information matrix for t... | math.ST stat.TH | low lewis and prescott 1999 showed that a crossover design based on a williams latin square of order 4 can suffer substantial loss of efficiency if some observations in the final period are unavailable indeed if all observations are missing the design becomes disconnected we derive the information matrix for the direct... | [['low', 'lewis', 'and', 'prescott', '1999', 'showed', 'that', 'a', 'crossover', 'design', 'based', 'on', 'a', 'williams', 'latin', 'square', 'of', 'order', '4', 'can', 'suffer', 'substantial', 'loss', 'of', 'efficiency', 'if', 'some', 'observations', 'in', 'the', 'final', 'period', 'are', 'unavailable', 'indeed', 'if'... | [-0.15080289213801734, 0.1659179896543113, -0.05593169752197961, 0.06587057279442282, -0.053722528728152, -0.11559185388808449, 0.07235614378781369, 0.3845297683961689, -0.2324198804621119, -0.2951477844733745, 0.18257941639458294, -0.28725545412986925, -0.146880237624282, 0.1725967466753597, -0.10967812247108669, -0.0... |
710.0686 | Habitability of Planets in Binaries | A survey of currently known extrasolar planets indicates that close to 20% of
their hosting stars are members of binary systems. While the majority of these
binaries are wide (i.e., with separations between 250 and 6500 AU), the
detection of Jovian-type planets in the three binaries of Gamma Cephei
(separation of 18.... | astro-ph | a survey of currently known extrasolar planets indicates that close to 20 of their hosting stars are members of binary systems while the majority of these binaries are wide ie with separations between 250 and 6500 au the detection of joviantype planets in the three binaries of gamma cephei separation of 185 au gl 86 se... | [['a', 'survey', 'of', 'currently', 'known', 'extrasolar', 'planets', 'indicates', 'that', 'close', 'to', '20', 'of', 'their', 'hosting', 'stars', 'are', 'members', 'of', 'binary', 'systems', 'while', 'the', 'majority', 'of', 'these', 'binaries', 'are', 'wide', 'ie', 'with', 'separations', 'between', '250', 'and', '650... | [-0.18958523101612645, 0.13124973441506355, -0.02893239345237519, 0.030364874495762993, -0.0718828408111988, -0.03430103159175729, 0.10306793598402526, 0.2828094108738942, -0.1544567126613813, -0.3686792552236866, 0.09383836516351937, -0.31196693726961716, -0.10453190769320764, 0.2045913713342809, -0.05313043573024864,... |
710.0687 | Entanglement of a Laguerre-Gaussian cavity mode with a rotating mirror | It has previously been shown theoretically that the exchange of linear
momentum between the light field in an optical cavity and a vibrating end
mirror can entangle the electromagnetic field with the vibrational motion of
that mirror. In this paper we consider the rotational analog of this situation
and show that rad... | quant-ph | it has previously been shown theoretically that the exchange of linear momentum between the light field in an optical cavity and a vibrating end mirror can entangle the electromagnetic field with the vibrational motion of that mirror in this paper we consider the rotational analog of this situation and show that radiat... | [['it', 'has', 'previously', 'been', 'shown', 'theoretically', 'that', 'the', 'exchange', 'of', 'linear', 'momentum', 'between', 'the', 'light', 'field', 'in', 'an', 'optical', 'cavity', 'and', 'a', 'vibrating', 'end', 'mirror', 'can', 'entangle', 'the', 'electromagnetic', 'field', 'with', 'the', 'vibrational', 'motion... | [-0.18541420250462004, 0.22148510989958511, -0.12621487332400919, -0.004301888303531484, -0.050852319011571764, -0.14119996406651777, 0.01212890107377336, 0.42414161738211653, -0.24626023836176972, -0.2831796754751055, 0.016943443306967957, -0.23050071902830024, -0.10148739027416055, 0.19648838242323236, -0.03961413908... |
710.0688 | The type N Karlhede bound is sharp | We present a family of four-dimensional Lorentzian manifolds whose invariant
classification requires the seventh covariant derivative of the curvature
tensor. The spacetimes in questions are null radiation, type N solutions on an
anti-de Sitter background. The large order of the bound is due to the fact that
these sp... | gr-qc math.DG | we present a family of fourdimensional lorentzian manifolds whose invariant classification requires the seventh covariant derivative of the curvature tensor the spacetimes in questions are null radiation type n solutions on an antide sitter background the large order of the bound is due to the fact that these spacetime... | [['we', 'present', 'a', 'family', 'of', 'fourdimensional', 'lorentzian', 'manifolds', 'whose', 'invariant', 'classification', 'requires', 'the', 'seventh', 'covariant', 'derivative', 'of', 'the', 'curvature', 'tensor', 'the', 'spacetimes', 'in', 'questions', 'are', 'null', 'radiation', 'type', 'n', 'solutions', 'on', '... | [-0.18560757166849373, 0.11286965155224281, -0.05945931496828405, 0.06766671948517158, -0.11426574628410945, -0.1309375700144681, -0.0998309886112545, 0.32577262209978564, -0.17358902314027994, -0.2759907536848045, 0.10888204375827518, -0.2850000599343608, -0.14080453963095405, 0.1350102677260206, -0.07136205652704351,... |
710.0689 | Convexity and Cone-Vexing | The idea of convexity feeds generation, separation, calculus, and
approximation. Generation appears as duality; separation, as optimality;
calculus, as representation; and approximation, as stability. This is an
overview of the origin, evolution, and trends of convexity. Study of convexity
in the Sobolev Institute wa... | math.FA math.HO | the idea of convexity feeds generation separation calculus and approximation generation appears as duality separation as optimality calculus as representation and approximation as stability this is an overview of the origin evolution and trends of convexity study of convexity in the sobolev institute was initiated by l... | [['the', 'idea', 'of', 'convexity', 'feeds', 'generation', 'separation', 'calculus', 'and', 'approximation', 'generation', 'appears', 'as', 'duality', 'separation', 'as', 'optimality', 'calculus', 'as', 'representation', 'and', 'approximation', 'as', 'stability', 'this', 'is', 'an', 'overview', 'of', 'the', 'origin', '... | [-0.12927593420243869, 0.048418680847458685, -0.14493401234937928, 0.1394433480513803, -0.11141232478479712, -0.06654675482472373, 0.0026905278722613546, 0.3095790901994806, -0.31301684022518034, -0.30242525641727497, 0.19944774905038146, -0.25346272874434117, -0.13733794691704088, 0.07866147875596406, -0.1220078347250... |
710.069 | Deblurring of Motionally Averaged Images with Applications to
Single-Particle Cryo-Electron Microscopy | This paper addresses the deconvolution of an image that has been obtained by
superimposing many copies of an underlying unknown image of interest. The
superposition is assumed to not be exact due to noise, and is described using
an error distribution in position, orientation, or both. We assume that a good
estimate o... | math.NA | this paper addresses the deconvolution of an image that has been obtained by superimposing many copies of an underlying unknown image of interest the superposition is assumed to not be exact due to noise and is described using an error distribution in position orientation or both we assume that a good estimate of the e... | [['this', 'paper', 'addresses', 'the', 'deconvolution', 'of', 'an', 'image', 'that', 'has', 'been', 'obtained', 'by', 'superimposing', 'many', 'copies', 'of', 'an', 'underlying', 'unknown', 'image', 'of', 'interest', 'the', 'superposition', 'is', 'assumed', 'to', 'not', 'be', 'exact', 'due', 'to', 'noise', 'and', 'is',... | [-0.06789583644205506, 0.03960156415748915, -0.12299256705421399, 0.06779617190291669, -0.05447998072734063, -0.09488626743884797, -0.031910434851368415, 0.3963616386927823, -0.3158920073610522, -0.24565546423880422, 0.14584843674612707, -0.231342469371776, -0.15889957032700197, 0.2112506974322543, -0.11299128659772983... |
710.0691 | Pion mass difference from vacuum polarization | We calculate the electromagnetic contribution to the pion mass difference,
$\Delta m^2_\pi=m^2_{\pi^+}-m^2_{\pi^0}$, in the chiral limit through the
$VV-AA$ type vacuum polarization using Das-Guralnik-Mathur-Low-Young (DGMLY)
sum rule. The calculation is made with two-flavors of dynamical overlap
fermions on a $16^3\... | hep-lat hep-ph | we calculate the electromagnetic contribution to the pion mass difference delta m2_pim2_pim2_pi0 in the chiral limit through the vvaa type vacuum polarization using dasguralnikmathurlowyoung dgmly sum rule the calculation is made with twoflavors of dynamical overlap fermions on a 163times 32 lattice at asim012 fm the e... | [['we', 'calculate', 'the', 'electromagnetic', 'contribution', 'to', 'the', 'pion', 'mass', 'difference', 'delta', 'm2_pim2_pim2_pi0', 'in', 'the', 'chiral', 'limit', 'through', 'the', 'vvaa', 'type', 'vacuum', 'polarization', 'using', 'dasguralnikmathurlowyoung', 'dgmly', 'sum', 'rule', 'the', 'calculation', 'is', 'ma... | [-0.1527807347241554, 0.21611927788671073, -0.06356335125091644, 0.08030291127150056, -0.029475931548052007, -0.03998012490977475, 0.10387675978897794, 0.3425985663323789, -0.19193370321446712, -0.2510959754828028, 0.032662710588140124, -0.31259501313052335, -0.00816329815718639, 0.08474801316320359, 0.0940693175262322... |
710.0692 | Entanglement renormalization in fermionic systems | We demonstrate, in the context of quadratic fermion lattice models in one and
two spatial dimensions, the potential of entanglement renormalization (ER) to
define a proper real-space renormalization group transformation. Our results
show, for the first time, the validity of the multi-scale entanglement
renormalizatio... | quant-ph | we demonstrate in the context of quadratic fermion lattice models in one and two spatial dimensions the potential of entanglement renormalization er to define a proper realspace renormalization group transformation our results show for the first time the validity of the multiscale entanglement renormalization ansatz me... | [['we', 'demonstrate', 'in', 'the', 'context', 'of', 'quadratic', 'fermion', 'lattice', 'models', 'in', 'one', 'and', 'two', 'spatial', 'dimensions', 'the', 'potential', 'of', 'entanglement', 'renormalization', 'er', 'to', 'define', 'a', 'proper', 'realspace', 'renormalization', 'group', 'transformation', 'our', 'resul... | [-0.1548655178571329, 0.13407453842822234, -0.11679556956799815, 0.0813544574348085, 0.008641732854255455, -0.15428635723204637, 0.04831726550586683, 0.3274917014380347, -0.25081121820804414, -0.24155951913788307, 0.025855445088010888, -0.3070022916535334, -0.16024847243133247, 0.13319221755717786, 0.02140741214650322,... |
710.0693 | Scaling analysis of normal state properties of high-temperature
superconductors | We propose a model-independent scaling method to study the physical
properties of high-temperature superconductors in the normal state. We have
analyze the experimental data of the c-axis resistivity, the in-plane
resistivity, the Hall coefficient, the magnetic susceptibility, the
spin-lattice relaxation rate, and th... | cond-mat.supr-con cond-mat.str-el | we propose a modelindependent scaling method to study the physical properties of hightemperature superconductors in the normal state we have analyze the experimental data of the caxis resistivity the inplane resistivity the hall coefficient the magnetic susceptibility the spinlattice relaxation rate and the thermoelect... | [['we', 'propose', 'a', 'modelindependent', 'scaling', 'method', 'to', 'study', 'the', 'physical', 'properties', 'of', 'hightemperature', 'superconductors', 'in', 'the', 'normal', 'state', 'we', 'have', 'analyze', 'the', 'experimental', 'data', 'of', 'the', 'caxis', 'resistivity', 'the', 'inplane', 'resistivity', 'the'... | [-0.15570358578093943, 0.1613488727614771, -0.11516836383510555, 0.022454035088689737, -0.07365450736083021, -0.12437609125964483, 0.11136672770273741, 0.3607390358800364, -0.2920969900126769, -0.2572437921347462, -0.004063501146787377, -0.3499573881337506, -0.14106360556357583, 0.25417874142457947, 0.04928692745340762... |
710.0694 | Gain Stabilization of a Submillimeter SIS Heterodyne Receiver | We have designed a system to stabilize the gain of a submillimeter heterodyne
receiver against thermal fluctuations of the mixing element. In the most
sensitive heterodyne receivers, the mixer is usually cooled to 4 K using a
closed-cycle cryocooler, which can introduce ~1% fluctuations in the physical
temperature of... | astro-ph | we have designed a system to stabilize the gain of a submillimeter heterodyne receiver against thermal fluctuations of the mixing element in the most sensitive heterodyne receivers the mixer is usually cooled to 4 k using a closedcycle cryocooler which can introduce 1 fluctuations in the physical temperature of the rec... | [['we', 'have', 'designed', 'a', 'system', 'to', 'stabilize', 'the', 'gain', 'of', 'a', 'submillimeter', 'heterodyne', 'receiver', 'against', 'thermal', 'fluctuations', 'of', 'the', 'mixing', 'element', 'in', 'the', 'most', 'sensitive', 'heterodyne', 'receivers', 'the', 'mixer', 'is', 'usually', 'cooled', 'to', '4', 'k... | [-0.14354451209836608, 0.13634977201556844, -0.08222147035305442, -0.03678575077498246, -0.027724659327289153, -0.1841304576661352, 0.034023065402322375, 0.38303583518912393, -0.2141727707248406, -0.29258354201019027, 0.16924870721915544, -0.27751985270042917, -0.06862888123904323, 0.19299701973260647, -0.0454591975129... |
710.0695 | Exciton spectroscopy of hexagonal boron nitride using non-resonant x-ray
Raman scattering | We report non-resonant x-ray Raman scattering (XRS) measurements from
hexagonal boron nitride for transferred momentum from 2 to 9
$\mathrm{\AA}^{-1}$ along directions both in and out of the basal plane. A
symmetry-based argument, together with real-space full multiple scattering
calculations of the projected density... | cond-mat.mtrl-sci | we report nonresonant xray raman scattering xrs measurements from hexagonal boron nitride for transferred momentum from 2 to 9 mathrmaa1 along directions both in and out of the basal plane a symmetrybased argument together with realspace full multiple scattering calculations of the projected density of states in the sp... | [['we', 'report', 'nonresonant', 'xray', 'raman', 'scattering', 'xrs', 'measurements', 'from', 'hexagonal', 'boron', 'nitride', 'for', 'transferred', 'momentum', 'from', '2', 'to', '9', 'mathrmaa1', 'along', 'directions', 'both', 'in', 'and', 'out', 'of', 'the', 'basal', 'plane', 'a', 'symmetrybased', 'argument', 'toge... | [-0.13517840127072608, 0.14408759565103327, -0.0920981887042865, -0.0069639693621824355, -0.033941341668431615, -0.08747483258959891, 0.08857600586809988, 0.4056269693584449, -0.2142231273197237, -0.2154483607831015, -0.02970595488421105, -0.3653720819616112, -0.09777228228865598, 0.1749913850424533, 0.1127206322505545... |
710.0696 | The lowest modes around Gaussian solutions of tensor models and the
general relativity | In the previous paper, the number distribution of the low-lying spectra
around Gaussian solutions representing various dimensional fuzzy tori of a
tensor model was numerically shown to be in accordance with the general
relativity on tori. In this paper, I perform more detailed numerical analysis
of the properties of ... | hep-th gr-qc | in the previous paper the number distribution of the lowlying spectra around gaussian solutions representing various dimensional fuzzy tori of a tensor model was numerically shown to be in accordance with the general relativity on tori in this paper i perform more detailed numerical analysis of the properties of the mo... | [['in', 'the', 'previous', 'paper', 'the', 'number', 'distribution', 'of', 'the', 'lowlying', 'spectra', 'around', 'gaussian', 'solutions', 'representing', 'various', 'dimensional', 'fuzzy', 'tori', 'of', 'a', 'tensor', 'model', 'was', 'numerically', 'shown', 'to', 'be', 'in', 'accordance', 'with', 'the', 'general', 'r... | [-0.11347353918629452, 0.12352201772660439, -0.1112674173046747, 0.08762828873158521, -0.04037709709450181, -0.09898760269466296, -0.029344395728878467, 0.32767380622022274, -0.1945280080028581, -0.25433216226410194, 0.03870581089297116, -0.2874969780304522, -0.17840951174181305, 0.1487119734113737, -0.0038791383080676... |
710.0697 | Toroidalization of generating sequences in dimension two function fields
of positive characteristic | We give a characteristic free proof of the main result of our previous paper
(math.AC/0509697) concerning toroidalization of generating sequences of
valuations in dimension two function fields. We show that when an extension of
two dimensional algebraic regular local rings $R\subset S$ satisfies the
conclusions of th... | math.AC math.AG | we give a characteristic free proof of the main result of our previous paper mathac0509697 concerning toroidalization of generating sequences of valuations in dimension two function fields we show that when an extension of two dimensional algebraic regular local rings rsubset s satisfies the conclusions of the strong m... | [['we', 'give', 'a', 'characteristic', 'free', 'proof', 'of', 'the', 'main', 'result', 'of', 'our', 'previous', 'paper', 'mathac0509697', 'concerning', 'toroidalization', 'of', 'generating', 'sequences', 'of', 'valuations', 'in', 'dimension', 'two', 'function', 'fields', 'we', 'show', 'that', 'when', 'an', 'extension',... | [-0.20310626516231534, 0.04264920071992409, -0.12154988555773867, 0.05802385504780845, -0.020032889230854133, -0.09844252405067284, -0.0077186224357733, 0.3112230584074771, -0.28803531515101594, -0.21654545913704418, 0.05265707971711615, -0.22679996462256619, -0.15037546250404735, 0.2274211812729129, -0.091295138308355... |
710.0698 | Theoretical progress on V_us on lattice | Recent lattice studies on (semi-)leptonic kaon decays towards a precise
determination of V_us are reviewed. Attention is given to recent unquenched
calculations and consistency of their results with chiral perturbation theory.
| hep-ph | recent lattice studies on semileptonic kaon decays towards a precise determination of v_us are reviewed attention is given to recent unquenched calculations and consistency of their results with chiral perturbation theory | [['recent', 'lattice', 'studies', 'on', 'semileptonic', 'kaon', 'decays', 'towards', 'a', 'precise', 'determination', 'of', 'v_us', 'are', 'reviewed', 'attention', 'is', 'given', 'to', 'recent', 'unquenched', 'calculations', 'and', 'consistency', 'of', 'their', 'results', 'with', 'chiral', 'perturbation', 'theory']] | [-0.06927071167756954, 0.24146517381192215, -0.019752419463569117, 0.018702360970388736, -0.13355024471398322, -0.1069780746925502, 0.0975028726182157, 0.3649823111632178, -0.09845766543801274, -0.16821703639241956, 0.02522410482408539, -0.4179111396473262, -0.05235240902871855, 0.1221775839991507, 0.03411256618282125,... |
710.0699 | Inevitability of Plate Tectonics on Super-Earths | The recent discovery of super-Earths (masses less or equal to 10
earth-masses) has initiated a discussion about conditions for habitable worlds.
Among these is the mode of convection, which influences a planet's thermal
evolution and surface conditions. On Earth, plate tectonics has been proposed
as a necessary condi... | astro-ph | the recent discovery of superearths masses less or equal to 10 earthmasses has initiated a discussion about conditions for habitable worlds among these is the mode of convection which influences a planets thermal evolution and surface conditions on earth plate tectonics has been proposed as a necessary condition for li... | [['the', 'recent', 'discovery', 'of', 'superearths', 'masses', 'less', 'or', 'equal', 'to', '10', 'earthmasses', 'has', 'initiated', 'a', 'discussion', 'about', 'conditions', 'for', 'habitable', 'worlds', 'among', 'these', 'is', 'the', 'mode', 'of', 'convection', 'which', 'influences', 'a', 'planets', 'thermal', 'evolu... | [-0.12825484023114123, 0.22421427504775962, -0.03960234909428386, 0.0314628637265634, -0.1334072046722542, -0.0948443513722929, 0.04425549151845218, 0.3328828103693686, -0.20058409520608234, -0.31514628092193697, 0.17735940988146237, -0.2876637648849741, -0.1185211421074859, 0.22214367084285816, -0.128196565518669, 0.0... |
710.07 | Directional-dependent thermally activated motion of vortex bundles and
theory of anomalous Hall effect in type-II conventional and high-Tc
superconductors | The anomalous Hall effect for type-II conventional and high-Tc
superconductors is studied based upon the theory of thermally activated motion
of vortex bundles jumping over the directional-dependent energy barrier. It is
shown that the Hall anomaly is universal for type-II conventional and high-Tc
superconductors as ... | cond-mat.supr-con | the anomalous hall effect for typeii conventional and hightc superconductors is studied based upon the theory of thermally activated motion of vortex bundles jumping over the directionaldependent energy barrier it is shown that the hall anomaly is universal for typeii conventional and hightc superconductors as well as ... | [['the', 'anomalous', 'hall', 'effect', 'for', 'typeii', 'conventional', 'and', 'hightc', 'superconductors', 'is', 'studied', 'based', 'upon', 'the', 'theory', 'of', 'thermally', 'activated', 'motion', 'of', 'vortex', 'bundles', 'jumping', 'over', 'the', 'directionaldependent', 'energy', 'barrier', 'it', 'is', 'shown',... | [-0.19997380579030616, 0.2352756228430401, -0.028974395708005155, 0.036406890822370176, -0.07375916410047485, -0.14716816875057256, 0.04235315121821964, 0.3569857605390859, -0.26899415751615047, -0.2547221836462921, 0.057655890462136046, -0.27627217659384623, -0.15580391428880014, 0.23782278685973082, 0.030284702543695... |
710.0701 | The First Lunar Ranging Constraints on Gravity Sector SME Parameters | We present the first constraints on pure-gravity sector Standard-Model
Extension (SME) parameters using Lunar Laser Ranging (LLR). LLR measures the
round trip travel time of light between the Earth and the Moon. With 34+ years
of LLR data, we have constrained six independent linear combinations of SME
parameters at t... | gr-qc astro-ph | we present the first constraints on puregravity sector standardmodel extension sme parameters using lunar laser ranging llr llr measures the round trip travel time of light between the earth and the moon with 34 years of llr data we have constrained six independent linear combinations of sme parameters at the level of ... | [['we', 'present', 'the', 'first', 'constraints', 'on', 'puregravity', 'sector', 'standardmodel', 'extension', 'sme', 'parameters', 'using', 'lunar', 'laser', 'ranging', 'llr', 'llr', 'measures', 'the', 'round', 'trip', 'travel', 'time', 'of', 'light', 'between', 'the', 'earth', 'and', 'the', 'moon', 'with', '34', 'yea... | [-0.11293049744034017, 0.15112339099869132, -0.06669910038313405, 0.02459289243084971, -0.0620991854617993, -0.11060024416920813, 0.11069300529109596, 0.3268905656313467, -0.19642130423788773, -0.4005029773283185, 0.10791925038034661, -0.33352867056700314, -0.06965410634945852, 0.24984470019681435, -0.03541121761328682... |
710.0702 | Testing for Lorentz Violation: Constraints on Standard-Model Extension
Parameters via Lunar Laser Ranging | We present constraints on violations of Lorentz Invariance based on Lunar
Laser Ranging (LLR) data. LLR measures the Earth-Moon separation by timing the
round-trip travel of light between the two bodies, and is currently accurate to
a few centimeters (parts in $10^{11}$ of the total distance). By analyzing
archival L... | gr-qc astro-ph | we present constraints on violations of lorentz invariance based on lunar laser ranging llr data llr measures the earthmoon separation by timing the roundtrip travel of light between the two bodies and is currently accurate to a few centimeters parts in 1011 of the total distance by analyzing archival llr data under th... | [['we', 'present', 'constraints', 'on', 'violations', 'of', 'lorentz', 'invariance', 'based', 'on', 'lunar', 'laser', 'ranging', 'llr', 'data', 'llr', 'measures', 'the', 'earthmoon', 'separation', 'by', 'timing', 'the', 'roundtrip', 'travel', 'of', 'light', 'between', 'the', 'two', 'bodies', 'and', 'is', 'currently', '... | [-0.1520480472800257, 0.14211729407137216, -0.0583803815669705, 0.07751924096373841, -0.06297831996452323, -0.0812593135430456, 0.0954869702379869, 0.3367433923805609, -0.18947574795158798, -0.40181861878481023, 0.091869285473665, -0.30513135148862075, -0.05661023373520652, 0.26188347823268104, -0.034941233464430066, 0... |
710.0703 | pQCD vs. AdS/CFT Tested by Heavy Quark Energy Loss | We predict the charm and bottom quark nuclear modification factors using
weakly coupled pQCD and strongly coupled AdS/CFT drag methods. The
log(pT/M_Q)/pT dependence of pQCD loss and the momentum independence of drag
loss lead to different momentum dependencies for the R_{AA} predictions. This
difference is enhanced ... | nucl-th | we predict the charm and bottom quark nuclear modification factors using weakly coupled pqcd and strongly coupled adscft drag methods the logptm_qpt dependence of pqcd loss and the momentum independence of drag loss lead to different momentum dependencies for the r_aa predictions this difference is enhanced by examinin... | [['we', 'predict', 'the', 'charm', 'and', 'bottom', 'quark', 'nuclear', 'modification', 'factors', 'using', 'weakly', 'coupled', 'pqcd', 'and', 'strongly', 'coupled', 'adscft', 'drag', 'methods', 'the', 'logptm_qpt', 'dependence', 'of', 'pqcd', 'loss', 'and', 'the', 'momentum', 'independence', 'of', 'drag', 'loss', 'le... | [-0.04619026916440238, 0.25536144749600104, -0.13208052206107163, 0.12930240919496017, -0.061225775028155606, -0.17019701118750327, 0.009081317876486784, 0.3093902633271434, -0.2527783309194175, -0.2962397267872637, -0.047670487852089785, -0.3565474650399251, -0.0003343216482211243, 0.14121163303709844, 0.0076662832024... |
710.0704 | Triage of the Sign Problem | We discuss the sign problem in QCD at nonzero chemical potential and its
relation with chiral symmetry breaking and the spectrum of the Dirac operator
using the framework of chiral random matrix theory. We show that the
Banks-Casher formula is not valid for theories with a sign problem and has to
be replaced by an al... | hep-th | we discuss the sign problem in qcd at nonzero chemical potential and its relation with chiral symmetry breaking and the spectrum of the dirac operator using the framework of chiral random matrix theory we show that the bankscasher formula is not valid for theories with a sign problem and has to be replaced by an altern... | [['we', 'discuss', 'the', 'sign', 'problem', 'in', 'qcd', 'at', 'nonzero', 'chemical', 'potential', 'and', 'its', 'relation', 'with', 'chiral', 'symmetry', 'breaking', 'and', 'the', 'spectrum', 'of', 'the', 'dirac', 'operator', 'using', 'the', 'framework', 'of', 'chiral', 'random', 'matrix', 'theory', 'we', 'show', 'th... | [-0.11557043756410065, 0.1610303096452602, -0.09896353061776608, 0.040261597259409934, -0.0685507758300648, -0.14534562377310875, 0.041981727138692, 0.3703407264159371, -0.24894880819030935, -0.22504975432012644, 0.06640553819953413, -0.2847958382658867, -0.17750153470680946, 0.10011271811607811, 0.033023042694872454, ... |
710.0705 | Hopf Algebras and Congruence Subgroups | We prove that the kernel of the natural action of the modular group on the
center of the Drinfel'd double of a semisimple Hopf algebra is a congruence
subgroup. To do this, we introduce a class of generalized Frobenius-Schur
indicators and endow it with an action of the modular group that is compatible
with the origi... | math.RA hep-th math-ph math.MP math.QA math.RT | we prove that the kernel of the natural action of the modular group on the center of the drinfeld double of a semisimple hopf algebra is a congruence subgroup to do this we introduce a class of generalized frobeniusschur indicators and endow it with an action of the modular group that is compatible with the original on... | [['we', 'prove', 'that', 'the', 'kernel', 'of', 'the', 'natural', 'action', 'of', 'the', 'modular', 'group', 'on', 'the', 'center', 'of', 'the', 'drinfeld', 'double', 'of', 'a', 'semisimple', 'hopf', 'algebra', 'is', 'a', 'congruence', 'subgroup', 'to', 'do', 'this', 'we', 'introduce', 'a', 'class', 'of', 'generalized'... | [-0.18753506762808875, 0.04677647072234673, -0.13174478918836827, 0.046593173564280985, -0.1686046372347495, -0.11256726658821367, -0.0027941449733222263, 0.34656032946026116, -0.36541165293831573, -0.18045341210407123, 0.106176373463026, -0.2307733112227237, -0.18715381047181917, 0.21143153757714717, -0.15163498915927... |
710.0706 | Area-Preserving Surface Dynamics and S. Saito's Fixed Point Formula | We show that S. Saito's fixed point formula serves as a powerful tool for
counting the number of isolated periodic points of an area-preserving surface
map admitting periodic curves. His notion of periodic curves of types I and II
plays a central role in our discussion. We establish a Shub-Sullivan type
result on the... | math.DS math.AG | we show that s saitos fixed point formula serves as a powerful tool for counting the number of isolated periodic points of an areapreserving surface map admitting periodic curves his notion of periodic curves of types i and ii plays a central role in our discussion we establish a shubsullivan type result on the stabili... | [['we', 'show', 'that', 's', 'saitos', 'fixed', 'point', 'formula', 'serves', 'as', 'a', 'powerful', 'tool', 'for', 'counting', 'the', 'number', 'of', 'isolated', 'periodic', 'points', 'of', 'an', 'areapreserving', 'surface', 'map', 'admitting', 'periodic', 'curves', 'his', 'notion', 'of', 'periodic', 'curves', 'of', '... | [-0.22181942612635638, 0.06302474359753828, -0.10239520056155633, 0.06456119493462743, -0.035118708125631906, -0.1465928482577064, 0.08682068941767661, 0.2727696846002045, -0.2562803778762244, -0.2600886893265371, 0.11277100227373424, -0.2720684578756468, -0.16032345414618557, 0.24653235794526068, -0.11416911954973948,... |
710.0707 | New branch of Kaluza-Klein compactification | We found a new branch of solutions in Freund-Rubin type flux
compactifications. The geometry of these solutions is described as the external
space which has a de Sitter symmetry and the internal space which is
topologically spherical. However, it is not a simple form of dS_p x S^q but a
warped product of de Sitter sp... | hep-th gr-qc | we found a new branch of solutions in freundrubin type flux compactifications the geometry of these solutions is described as the external space which has a de sitter symmetry and the internal space which is topologically spherical however it is not a simple form of ds_p x sq but a warped product of de sitter space and... | [['we', 'found', 'a', 'new', 'branch', 'of', 'solutions', 'in', 'freundrubin', 'type', 'flux', 'compactifications', 'the', 'geometry', 'of', 'these', 'solutions', 'is', 'described', 'as', 'the', 'external', 'space', 'which', 'has', 'a', 'de', 'sitter', 'symmetry', 'and', 'the', 'internal', 'space', 'which', 'is', 'topo... | [-0.17191783672835875, 0.0820623852214531, -0.11576954763578741, 0.08138832598802094, -0.10693698011730847, -0.11495248218508143, 0.006938540425739791, 0.30604883338275707, -0.18729496045393476, -0.22345747947447786, 0.16224085483945122, -0.26370593412338117, -0.15776558657617945, 0.17099482788655318, -0.07312561552542... |
710.0708 | A characterization of all equilateral triangles in \Bbb Z^3 | This paper is a continuation of previous work of the authors. We extend one
of the theorems that gave a way to construct equilateral triangles whose
vertices have integer coordinates to the general situation. An approximate
extrapolation formula for the sequence ET(n) of all equilateral triangles with
vertices in $\{... | math.NT | this paper is a continuation of previous work of the authors we extend one of the theorems that gave a way to construct equilateral triangles whose vertices have integer coordinates to the general situation an approximate extrapolation formula for the sequence etn of all equilateral triangles with vertices in 012n3 a 1... | [['this', 'paper', 'is', 'a', 'continuation', 'of', 'previous', 'work', 'of', 'the', 'authors', 'we', 'extend', 'one', 'of', 'the', 'theorems', 'that', 'gave', 'a', 'way', 'to', 'construct', 'equilateral', 'triangles', 'whose', 'vertices', 'have', 'integer', 'coordinates', 'to', 'the', 'general', 'situation', 'an', 'ap... | [-0.17002761580782835, 0.032447062595222585, -0.1304234308114306, 0.028492733815181085, -0.08611804330110794, -0.0901003203537987, 0.04191077613561857, 0.3341685542073406, -0.20814291518334238, -0.28962951064964787, 0.09429325500587155, -0.32684596395883403, -0.14661332136058233, 0.1118844420511703, -0.0864626494251558... |
710.0709 | Superstring vertex operators in type IIB matrix model | We clarify the relation between the vertex operators in type IIB matrix model
and superstring. Green-Schwarz light-cone closed superstring theory is obtained
from IIB matrix model on two dimensional noncommutative backgrounds.
Superstring vertex operators should be reproduced from those of IIB matrix
model through th... | hep-th | we clarify the relation between the vertex operators in type iib matrix model and superstring greenschwarz lightcone closed superstring theory is obtained from iib matrix model on two dimensional noncommutative backgrounds superstring vertex operators should be reproduced from those of iib matrix model through this con... | [['we', 'clarify', 'the', 'relation', 'between', 'the', 'vertex', 'operators', 'in', 'type', 'iib', 'matrix', 'model', 'and', 'superstring', 'greenschwarz', 'lightcone', 'closed', 'superstring', 'theory', 'is', 'obtained', 'from', 'iib', 'matrix', 'model', 'on', 'two', 'dimensional', 'noncommutative', 'backgrounds', 's... | [-0.06950374913475152, 0.12165425272721907, -0.019839780106931257, 0.19639313864924557, -0.08664342425397356, -0.188264573207439, 0.016196466948355685, 0.3450040252868798, -0.16383895740498988, -0.17768141773811888, 0.05977524758389827, -0.32007352600732214, -0.27394207476959054, 0.08714848093092023, -0.116555144256922... |
710.071 | Non-perturbative renormalization of four-quark operators and B_K with
Schroedinger functional scheme in quenched domain-wall QCD | We present non-perturbative renormalization factors for $\Delta S=2$
four-quark operators in quenched domain-wall QCD using the Schroedinger
functional method. Non-perturbative renormalization factor for $B_K$ is
evaluated at hadronic scale. Combined with the non-perturbative RG running
obtained by the Alpha collabor... | hep-lat | we present nonperturbative renormalization factors for delta s2 fourquark operators in quenched domainwall qcd using the schroedinger functional method nonperturbative renormalization factor for b_k is evaluated at hadronic scale combined with the nonperturbative rg running obtained by the alpha collaboration our resul... | [['we', 'present', 'nonperturbative', 'renormalization', 'factors', 'for', 'delta', 's2', 'fourquark', 'operators', 'in', 'quenched', 'domainwall', 'qcd', 'using', 'the', 'schroedinger', 'functional', 'method', 'nonperturbative', 'renormalization', 'factor', 'for', 'b_k', 'is', 'evaluated', 'at', 'hadronic', 'scale', '... | [-0.13906858115525986, 0.2617131959802161, -0.13360951417039527, 0.05033516308348798, -0.03985345456102449, -0.10512905547403972, 0.07482846080610114, 0.4077573251324119, -0.17854672744525252, -0.23629411515624574, -0.00340384285233018, -0.2818602272223129, -0.08750020412305647, 0.08939263672369567, 0.08339217220674511... |
710.0711 | Canes Venatici I cloud of galaxies seen in the H-alpha line | We present results of H-alpha imaging for 42 galaxies in the nearby
low-density cloud Canes Venatici I populated mainly by late-type objects.
Estimates of the H-alpha flux and integrated star formation rate (SFR) are now
available for all 78 known members of this scattered system, spanning a large
range in luminosity... | astro-ph | we present results of halpha imaging for 42 galaxies in the nearby lowdensity cloud canes venatici i populated mainly by latetype objects estimates of the halpha flux and integrated star formation rate sfr are now available for all 78 known members of this scattered system spanning a large range in luminosity surface b... | [['we', 'present', 'results', 'of', 'halpha', 'imaging', 'for', '42', 'galaxies', 'in', 'the', 'nearby', 'lowdensity', 'cloud', 'canes', 'venatici', 'i', 'populated', 'mainly', 'by', 'latetype', 'objects', 'estimates', 'of', 'the', 'halpha', 'flux', 'and', 'integrated', 'star', 'formation', 'rate', 'sfr', 'are', 'now',... | [-0.07062164273035403, 0.08499293633346967, -0.02847657732150339, 0.13214176086748533, -0.052772313775824954, -0.023349697437427992, 0.0701461177441483, 0.48925436096569747, -0.09708264379362504, -0.3771059167313766, 0.038070584804229174, -0.28379488762151056, 0.011648080812053794, 0.17450740005068005, -0.0370625179980... |
710.0712 | Molecular Evolution and Star Formation: From Prestellar Cores to
Protostellar Cores | We investigate molecular evolution in a star-forming core that is initially a
hydrostatic starless core and collapses to form a low-mass protostar. The
results of a one-dimensional radiation-hydrodynamics calculation are adopted as
a physical model of the core. We first derive radii at which CO and large
organic spec... | astro-ph | we investigate molecular evolution in a starforming core that is initially a hydrostatic starless core and collapses to form a lowmass protostar the results of a onedimensional radiationhydrodynamics calculation are adopted as a physical model of the core we first derive radii at which co and large organic species subl... | [['we', 'investigate', 'molecular', 'evolution', 'in', 'a', 'starforming', 'core', 'that', 'is', 'initially', 'a', 'hydrostatic', 'starless', 'core', 'and', 'collapses', 'to', 'form', 'a', 'lowmass', 'protostar', 'the', 'results', 'of', 'a', 'onedimensional', 'radiationhydrodynamics', 'calculation', 'are', 'adopted', '... | [-0.060494622109598904, 0.20225862354187235, -0.003853634509926515, 0.0471267216665964, 0.026841423240455478, -0.06953331834735171, 0.07063507555821655, 0.38493654445679354, -0.20165607804749877, -0.31639209841242777, 0.05248860463150294, -0.2677916557416011, 0.021115842366135097, 0.08879712988096927, 0.059839605440721... |
710.0713 | Corrections to the running of gauge couplings due to quantum gravity | Concerning the gravitational corrections to the running of gauge couplings
two different results were reported. Some authors claim that gravitational
correction at the one-loop level indicates an interesting effect of universal
gravitational decreasing of gauge couplings, that is, gravitational correction
works unive... | hep-th gr-qc hep-ph | concerning the gravitational corrections to the running of gauge couplings two different results were reported some authors claim that gravitational correction at the oneloop level indicates an interesting effect of universal gravitational decreasing of gauge couplings that is gravitational correction works universally... | [['concerning', 'the', 'gravitational', 'corrections', 'to', 'the', 'running', 'of', 'gauge', 'couplings', 'two', 'different', 'results', 'were', 'reported', 'some', 'authors', 'claim', 'that', 'gravitational', 'correction', 'at', 'the', 'oneloop', 'level', 'indicates', 'an', 'interesting', 'effect', 'of', 'universal',... | [-0.17101958786496466, 0.17141337404521995, -0.10433756535261286, 0.10235868427966979, -0.11544260046029665, -0.14620280055138452, 0.011505774440417761, 0.2907703855069332, -0.17572898523186345, -0.32033586962126104, 0.011561428097845336, -0.29283809435206004, -0.1446564292537991, 0.1546520166820005, -0.011181857335908... |
710.0714 | Light-front quark model analysis of heavy meson radiative decays | We present the magnetic dipole($M1$) transitions $V\to P\gamma$ of various
heavy-flavored mesons such as $(D,D^*,D_s,D^{*}_s,\eta_c, J/\psi)$ and
$(B,B^*,B_s,B^*_s,\eta_b,\Upsilon)$ using the light-front quark model
constrained by the variational principle for the QCD-motivated effective
Hamiltonian. The weak decay c... | hep-ph | we present the magnetic dipolem1 transitions vto pgamma of various heavyflavored mesons such as ddd_sd_seta_c jpsi and bbb_sb_seta_bupsilon using the lightfront quark model constrained by the variational principle for the qcdmotivated effective hamiltonian the weak decay constants of heavy mesons and the decay widths f... | [['we', 'present', 'the', 'magnetic', 'dipolem1', 'transitions', 'vto', 'pgamma', 'of', 'various', 'heavyflavored', 'mesons', 'such', 'as', 'ddd_sd_seta_c', 'jpsi', 'and', 'bbb_sb_seta_bupsilon', 'using', 'the', 'lightfront', 'quark', 'model', 'constrained', 'by', 'the', 'variational', 'principle', 'for', 'the', 'qcdmo... | [-0.020172081682609304, 0.21066604652774654, -0.04750728466370631, 0.1780892951585537, -0.040741250051983764, -0.14375848795420357, 0.04831454268978199, 0.37039690446995555, -0.22635979214239688, -0.2622983919365132, -0.023780825136262656, -0.3153788917587094, 0.005861560315159815, 0.17758340968672806, 0.12348290515642... |
710.0715 | Effect of Ti4+ substitution on structural, transport and magnetic
properties of La0.67Sr0.33Mn1-xTixO3 | La$_{0.67}$Sr$_{0.33}$Mn$_{1-x}$Ti$_x$O$_{3}$ ($0 \le x \le 0.20$)
polycrystalline materials are prepared by employing lower annealing temperature
compared to the temperatures reported for the materials of the same
composition. The transport and magnetic properties of these materials are
significantly different from ... | cond-mat.str-el cond-mat.mtrl-sci | la_067sr_033mn_1xti_xo_3 0 le x le 020 polycrystalline materials are prepared by employing lower annealing temperature compared to the temperatures reported for the materials of the same composition the transport and magnetic properties of these materials are significantly different from those compounds prepared at hig... | [['la_067sr_033mn_1xti_xo_3', '0', 'le', 'x', 'le', '020', 'polycrystalline', 'materials', 'are', 'prepared', 'by', 'employing', 'lower', 'annealing', 'temperature', 'compared', 'to', 'the', 'temperatures', 'reported', 'for', 'the', 'materials', 'of', 'the', 'same', 'composition', 'the', 'transport', 'and', 'magnetic',... | [-0.10732848200262454, 0.287613761041369, -0.0047607823438358616, -0.021968223455139615, 0.056311074705141136, -0.1833486494420569, 0.12622517036315775, 0.46715655945130247, -0.2588674328776438, -0.3175296812220963, 0.013228258591513636, -0.3773057613549615, -0.019149075828687245, 0.1309598877603786, 0.0321141242661249... |
710.0716 | The Boltzmann-Grad limit of the periodic Lorentz gas in two space
dimensions | The periodic Lorentz gas is the dynamical system corresponding to the free
motion of a point particle in a periodic system of fixed spherical obstacles of
radius $r$ centered at the integer points, assuming all collisions of the
particle with the obstacles to be elastic. In this Note, we study this motion
on time int... | math.DS math-ph math.MP | the periodic lorentz gas is the dynamical system corresponding to the free motion of a point particle in a periodic system of fixed spherical obstacles of radius r centered at the integer points assuming all collisions of the particle with the obstacles to be elastic in this note we study this motion on time intervals ... | [['the', 'periodic', 'lorentz', 'gas', 'is', 'the', 'dynamical', 'system', 'corresponding', 'to', 'the', 'free', 'motion', 'of', 'a', 'point', 'particle', 'in', 'a', 'periodic', 'system', 'of', 'fixed', 'spherical', 'obstacles', 'of', 'radius', 'r', 'centered', 'at', 'the', 'integer', 'points', 'assuming', 'all', 'coll... | [-0.18290576287755458, 0.13431686561832773, -0.08425665878328598, -0.0017761437096244965, 0.023324066213616688, -0.0736641880438482, 0.010905169228660978, 0.3444084720686078, -0.2811808791787674, -0.23498780079858583, 0.11492829554481432, -0.29854650535465527, -0.07289091859840685, 0.13060922857645588, -0.0306442528453... |
710.0717 | Ultrafast coelectrophoretic fluorescent staining of proteins with
carbocyanines | Protein detection on SDS gels or on 2-D gels must combine several features,
such as sensitivity, homogeneity from one protein to another, speed, low cost,
and user-friendliness. For some applications, it is also interesting to have a
nonfixing stain, so that proteins can be mobilized from the gel for further use
(ele... | q-bio.GN | protein detection on sds gels or on 2d gels must combine several features such as sensitivity homogeneity from one protein to another speed low cost and userfriendliness for some applications it is also interesting to have a nonfixing stain so that proteins can be mobilized from the gel for further use electroelution b... | [['protein', 'detection', 'on', 'sds', 'gels', 'or', 'on', '2d', 'gels', 'must', 'combine', 'several', 'features', 'such', 'as', 'sensitivity', 'homogeneity', 'from', 'one', 'protein', 'to', 'another', 'speed', 'low', 'cost', 'and', 'userfriendliness', 'for', 'some', 'applications', 'it', 'is', 'also', 'interesting', '... | [-0.04078384851415952, 0.13601802227795512, -0.057027214144666986, -0.003602680555716991, -0.012905467026866973, -0.1838862893388917, 0.051435170028513916, 0.4696168274184068, -0.2518816335126758, -0.2958642239496112, 0.10939440311786408, -0.29858350530266764, -0.1358453592301036, 0.17711279881031564, -0.05341123334908... |
710.0718 | Exchange-energy functionals for finite two-dimensional systems | Implicit and explicit density functionals for the exchange energy in finite
two-dimensional systems are developed following the approach of Becke and
Roussel [Phys. Rev. A 39, 3761 (1989)]. Excellent agreement for the
exchange-hole potentials and exchange energies is found when compared with the
exact-exchange refere... | cond-mat.str-el | implicit and explicit density functionals for the exchange energy in finite twodimensional systems are developed following the approach of becke and roussel phys rev a 39 3761 1989 excellent agreement for the exchangehole potentials and exchange energies is found when compared with the exactexchange reference data for ... | [['implicit', 'and', 'explicit', 'density', 'functionals', 'for', 'the', 'exchange', 'energy', 'in', 'finite', 'twodimensional', 'systems', 'are', 'developed', 'following', 'the', 'approach', 'of', 'becke', 'and', 'roussel', 'phys', 'rev', 'a', '39', '3761', '1989', 'excellent', 'agreement', 'for', 'the', 'exchangehole... | [-0.08026313564311373, 0.09780102011906665, -0.01965934130726609, 0.03538696669473699, 0.056872676798176564, -0.15297764450561527, 0.0304208615902675, 0.3622763075733773, -0.15106438121917407, -0.33135563528403733, -0.04323178548337438, -0.3316958600984568, -0.07542365078428169, 0.24090934719140755, -0.0120764623464244... |
710.0719 | Nuclear Structure Relevant to Neutrinoless Double Beta Decay: 76Ge and
76Se | The possibility of observing neutrinoless double beta decay offers the
opportunity of determining the neutrino mass IF the nuclear matrix element were
known. Theoretical calculations are uncertain and measurements of the
occupations of valence orbits by nucleons active in the decay can be important.
The occupation of... | nucl-ex | the possibility of observing neutrinoless double beta decay offers the opportunity of determining the neutrino mass if the nuclear matrix element were known theoretical calculations are uncertain and measurements of the occupations of valence orbits by nucleons active in the decay can be important the occupation of val... | [['the', 'possibility', 'of', 'observing', 'neutrinoless', 'double', 'beta', 'decay', 'offers', 'the', 'opportunity', 'of', 'determining', 'the', 'neutrino', 'mass', 'if', 'the', 'nuclear', 'matrix', 'element', 'were', 'known', 'theoretical', 'calculations', 'are', 'uncertain', 'and', 'measurements', 'of', 'the', 'occu... | [-0.07804455490409525, 0.25787654419927375, -0.06912147194339797, 0.12646017298764742, 0.028173529286066007, -0.10038807736870287, 0.09221385063248252, 0.36461381280216676, -0.2058783691729708, -0.3278538676717415, 0.002805848732381931, -0.3614258736307765, -0.044924567090267126, 0.19210772692619277, 0.0689617938378119... |
710.072 | The tensor of interaction of a two-level system with an arbitrary strain
field | The interaction between two-level systems (TLS) and strain fields in a solid
is contained in the diagonal matrix element of the interaction hamiltonian,
$\delta$, which, in general, has the expression $\delta=2[\gamma]:[S]$, with
the tensor $[\gamma]$ describing the TLS ``deformability'' and $[S]$ being the
symmetric... | cond-mat.dis-nn cond-mat.mtrl-sci | the interaction between twolevel systems tls and strain fields in a solid is contained in the diagonal matrix element of the interaction hamiltonian delta which in general has the expression delta2gammas with the tensor gamma describing the tls deformability and s being the symmetric strain tensor we construct gamma on... | [['the', 'interaction', 'between', 'twolevel', 'systems', 'tls', 'and', 'strain', 'fields', 'in', 'a', 'solid', 'is', 'contained', 'in', 'the', 'diagonal', 'matrix', 'element', 'of', 'the', 'interaction', 'hamiltonian', 'delta', 'which', 'in', 'general', 'has', 'the', 'expression', 'delta2gammas', 'with', 'the', 'tenso... | [-0.1664515125275486, 0.18300818234475122, -0.04015327922172016, -0.0055771799261371295, -0.04356503783414761, -0.13364913874823187, -0.01273303185744832, 0.386365426066849, -0.27770053789847426, -0.21353586219380505, 0.056626094567279024, -0.29957310829932493, -0.12018044031846027, 0.1682468817383051, 0.05191882856190... |
710.0721 | Noncommutative families of instantons | We construct $\theta$-deformations of the classical groups SL(2,H) and Sp(2).
Coacting on the basic instanton on a noncommutative four-sphere $S^4_\theta$,
we construct a noncommutative family of instantons of charge 1. The family is
parametrized by the quantum quotient of $SL_\theta(2,H)$ by $Sp_\theta(2)$.
| math.QA hep-th math-ph math.MP | we construct thetadeformations of the classical groups sl2h and sp2 coacting on the basic instanton on a noncommutative foursphere s4_theta we construct a noncommutative family of instantons of charge 1 the family is parametrized by the quantum quotient of sl_theta2h by sp_theta2 | [['we', 'construct', 'thetadeformations', 'of', 'the', 'classical', 'groups', 'sl2h', 'and', 'sp2', 'coacting', 'on', 'the', 'basic', 'instanton', 'on', 'a', 'noncommutative', 'foursphere', 's4_theta', 'we', 'construct', 'a', 'noncommutative', 'family', 'of', 'instantons', 'of', 'charge', '1', 'the', 'family', 'is', 'p... | [-0.16106693530455232, 0.14458080460317432, -0.07008335755672306, 0.08929144240973982, -0.028939601499587297, -0.10463383954484015, -0.004063017148291692, 0.2823563765734434, -0.24299310557544232, -0.1915840925183147, 0.07112870278360788, -0.24848090764135122, -0.20103272802662103, 0.16026934487745165, -0.1422637250507... |
710.0722 | Boost symmetry in the Quantum Gravity sector | We perform a canonical quantization of gravity in a second-order formulation,
taking as configuration variables those describing a 4-bein, not adapted to the
space-time splitting. We outline how, neither if we fix the Lorentz frame
before quantizing, nor if we perform no gauge fixing at all, is invariance
under boost... | gr-qc | we perform a canonical quantization of gravity in a secondorder formulation taking as configuration variables those describing a 4bein not adapted to the spacetime splitting we outline how neither if we fix the lorentz frame before quantizing nor if we perform no gauge fixing at all is invariance under boost transforma... | [['we', 'perform', 'a', 'canonical', 'quantization', 'of', 'gravity', 'in', 'a', 'secondorder', 'formulation', 'taking', 'as', 'configuration', 'variables', 'those', 'describing', 'a', '4bein', 'not', 'adapted', 'to', 'the', 'spacetime', 'splitting', 'we', 'outline', 'how', 'neither', 'if', 'we', 'fix', 'the', 'lorentz... | [-0.1465609581802379, 0.15511297713965178, -0.12391067974756217, 0.09725838379130106, -0.12445526623421095, -0.17406206958165224, 0.04072873797691004, 0.4009258748794144, -0.21630810704928907, -0.26036440655589105, 0.06459958238146184, -0.17350969013165343, -0.16205841000615195, 0.08736580495129932, -0.0929248975928534... |
710.0723 | Uncertainty Relation for the Discrete Fourier Transform | We derive an uncertainty relation for two unitary operators which obey a
commutation relation of the form UV=exp[i phi] VU. Its most important
application is to constrain how much a quantum state can be localised
simultaneously in two mutually unbiased bases related by a Discrete Fourier
Transform. It provides an unc... | quant-ph | we derive an uncertainty relation for two unitary operators which obey a commutation relation of the form uvexpi phi vu its most important application is to constrain how much a quantum state can be localised simultaneously in two mutually unbiased bases related by a discrete fourier transform it provides an uncertaint... | [['we', 'derive', 'an', 'uncertainty', 'relation', 'for', 'two', 'unitary', 'operators', 'which', 'obey', 'a', 'commutation', 'relation', 'of', 'the', 'form', 'uvexpi', 'phi', 'vu', 'its', 'most', 'important', 'application', 'is', 'to', 'constrain', 'how', 'much', 'a', 'quantum', 'state', 'can', 'be', 'localised', 'sim... | [-0.1351456884554518, 0.1680590091613535, -0.10913344715098458, 0.1114385540266175, -0.07651510891265982, -0.12793162017137058, 0.03193236754491371, 0.32373174924541975, -0.29765056498052384, -0.2600013992079526, 0.08447747707582456, -0.2882545045769412, -0.13127453793571445, 0.20527369909042353, -0.05736783308107868, ... |
710.0724 | The thermodynamic limit for fractional exclusion statistics | I discuss Haldane's concept of generalised exclusion statistics (Phys. Rev.
Lett. {\bf 67}, 937, 1991) and I show that it leads to inconsistencies in the
calculation of the particle distribution that maximizes the partition function.
These inconsistencies appear when mutual exclusion statistics is manifested
between ... | cond-mat.stat-mech cond-mat.mes-hall | i discuss haldanes concept of generalised exclusion statistics phys rev lett bf 67 937 1991 and i show that it leads to inconsistencies in the calculation of the particle distribution that maximizes the partition function these inconsistencies appear when mutual exclusion statistics is manifested between different subs... | [['i', 'discuss', 'haldanes', 'concept', 'of', 'generalised', 'exclusion', 'statistics', 'phys', 'rev', 'lett', 'bf', '67', '937', '1991', 'and', 'i', 'show', 'that', 'it', 'leads', 'to', 'inconsistencies', 'in', 'the', 'calculation', 'of', 'the', 'particle', 'distribution', 'that', 'maximizes', 'the', 'partition', 'fu... | [-0.09208657442442407, 0.157179331325876, -0.07307575983993177, 0.06628490744229307, -0.05824834408122115, -0.14077358984754287, 0.057495785646356774, 0.30535384256758596, -0.23351851188843803, -0.32732168649921994, -0.009281928502397412, -0.2805381546246021, -0.15910199293700447, 0.1313434883424114, -0.128392701486258... |
710.0725 | Near-Constant Mean Curvature Solutions of the Einstein Constraint
Equations with Non-Negative Yamabe Metrics | We show that sets of conformal data on closed manifolds with the metric in
the positive or zero Yamabe class, and with the gradient of the mean curvature
function sufficiently small, are mapped to solutions of the Einstein constraint
equations. This result extends previous work which required the conformal
metric to ... | gr-qc | we show that sets of conformal data on closed manifolds with the metric in the positive or zero yamabe class and with the gradient of the mean curvature function sufficiently small are mapped to solutions of the einstein constraint equations this result extends previous work which required the conformal metric to be in... | [['we', 'show', 'that', 'sets', 'of', 'conformal', 'data', 'on', 'closed', 'manifolds', 'with', 'the', 'metric', 'in', 'the', 'positive', 'or', 'zero', 'yamabe', 'class', 'and', 'with', 'the', 'gradient', 'of', 'the', 'mean', 'curvature', 'function', 'sufficiently', 'small', 'are', 'mapped', 'to', 'solutions', 'of', 't... | [-0.15276330631847182, 0.09165911106251631, -0.06437399150860129, 0.04863938531718415, -0.12539283914322202, -0.15007217025214975, -0.06005474381064149, 0.3177900852240396, -0.2695877318849053, -0.28261238811396516, 0.11256624143711771, -0.30620730180067546, -0.15196913944656085, 0.13050511397181475, -0.076850904688013... |
710.0726 | Distinguishing SUSY scenarios using \tau polarisation and \tilde\chi^0_1
Dark Matter | We discuss first a method of measuring $\tau$ polarisation at the ILC using
the 1--prong hadronic decays of the $\tau$. We then show in this contribution
how a study of the $\tilde \tau$ sector and particularly use of decay $\tau$
polarisation can offer a very good handle for distinguishing between mSUGRA and
a SUSY-... | hep-ph | we discuss first a method of measuring tau polarisation at the ilc using the 1prong hadronic decays of the tau we then show in this contribution how a study of the tilde tau sector and particularly use of decay tau polarisation can offer a very good handle for distinguishing between msugra and a susygut scenario both o... | [['we', 'discuss', 'first', 'a', 'method', 'of', 'measuring', 'tau', 'polarisation', 'at', 'the', 'ilc', 'using', 'the', '1prong', 'hadronic', 'decays', 'of', 'the', 'tau', 'we', 'then', 'show', 'in', 'this', 'contribution', 'how', 'a', 'study', 'of', 'the', 'tilde', 'tau', 'sector', 'and', 'particularly', 'use', 'of',... | [-0.08419896482776563, 0.1646070125584419, -0.13912184442608402, 0.14940699577295724, -0.06661305367373503, -0.17696262904657767, 0.028208890953101216, 0.32635184205495393, -0.26860303001908153, -0.28846045275433707, 0.04700140799933041, -0.23218474596595534, -0.06252979287304557, 0.1833045578848284, 0.0586158364438093... |
710.0727 | The afterglow onset for GRB060418 and GRB060607A | Gamma-ray burst are thought to be produced by highly relativistic outflows.
Although upper and lower limits for the outflow initial Lorentz factor
$\Gamma_0$ are available, observational efforts to derive a direct
determination of $\Gamma_0$ have so far failed or provided ambiguous results.
As a matter of fact, the s... | astro-ph | gammaray burst are thought to be produced by highly relativistic outflows although upper and lower limits for the outflow initial lorentz factor gamma_0 are available observational efforts to derive a direct determination of gamma_0 have so far failed or provided ambiguous results as a matter of fact the shape of the e... | [['gammaray', 'burst', 'are', 'thought', 'to', 'be', 'produced', 'by', 'highly', 'relativistic', 'outflows', 'although', 'upper', 'and', 'lower', 'limits', 'for', 'the', 'outflow', 'initial', 'lorentz', 'factor', 'gamma_0', 'are', 'available', 'observational', 'efforts', 'to', 'derive', 'a', 'direct', 'determination', ... | [-0.062002992359694184, 0.16093308419818286, -0.08784490915742225, 0.14739105885761328, -0.1853311712190138, -0.13989486066033927, 0.060860061054534426, 0.4758839433164737, -0.16573951558240244, -0.31036439040918057, 0.05832458602082802, -0.27042138053301146, 0.0428748299780385, 0.2763287236959469, 0.02722465310612981,... |
710.0728 | Fractional exclusion statistics in general systems with interaction | I show that fractional exclusion statistics (FES) is manifested in general
interacting systems and I calculate the exclusion statistics parameters. Most
importantly, I show that the mutual exclusion statistics parameters--when the
presence of particles in one Hilbert space influences the dimension of another
Hilbert ... | cond-mat.stat-mech cond-mat.mes-hall | i show that fractional exclusion statistics fes is manifested in general interacting systems and i calculate the exclusion statistics parameters most importantly i show that the mutual exclusion statistics parameterswhen the presence of particles in one hilbert space influences the dimension of another hilbert spaceare... | [['i', 'show', 'that', 'fractional', 'exclusion', 'statistics', 'fes', 'is', 'manifested', 'in', 'general', 'interacting', 'systems', 'and', 'i', 'calculate', 'the', 'exclusion', 'statistics', 'parameters', 'most', 'importantly', 'i', 'show', 'that', 'the', 'mutual', 'exclusion', 'statistics', 'parameterswhen', 'the', ... | [-0.07714232601954238, 0.15556983637582997, -0.060478270560017096, 0.04625187779184552, -0.032667180543522474, -0.12002841861154277, 0.07287092296325642, 0.2448450415800123, -0.22294388968705037, -0.2846007470405944, 0.029703014249326257, -0.27144492443387763, -0.15148878827913786, 0.17544665294901832, -0.0937853183283... |
710.0729 | Semileptonic decays of heavy-light pseudoscalar mesons | I discuss the results of a recent quenched lattice calculation of the two
independent form factors parametrizing the semileptonic decays between
heavy-light pseudoscalar mesons. The differential decay rate of the process B
--> D l nu has been calculated at non vanishing momentum transfer both in the
case of the light... | hep-lat | i discuss the results of a recent quenched lattice calculation of the two independent form factors parametrizing the semileptonic decays between heavylight pseudoscalar mesons the differential decay rate of the process b d l nu has been calculated at non vanishing momentum transfer both in the case of the light leptons... | [['i', 'discuss', 'the', 'results', 'of', 'a', 'recent', 'quenched', 'lattice', 'calculation', 'of', 'the', 'two', 'independent', 'form', 'factors', 'parametrizing', 'the', 'semileptonic', 'decays', 'between', 'heavylight', 'pseudoscalar', 'mesons', 'the', 'differential', 'decay', 'rate', 'of', 'the', 'process', 'b', '... | [-0.1516189309805336, 0.25314135952956146, -0.022198603141106783, 0.08918520552213031, 0.005830084912419793, -0.15860454571093358, 0.054170275737147125, 0.256561831822471, -0.20563185380564797, -0.15375684727988545, -0.03477402282730928, -0.3402948864839143, 0.022212948295332137, 0.10846081724952138, 0.1122615611446755... |
710.073 | Fractional Charge and Quantized Current in the Quantum Spin Hall State | A profound manifestation of topologically non-trivial states of matter is the
occurrence of fractionally charged elementary excitations. The quantum spin
Hall insulator state is a fundamentally novel quantum state of matter that
exists at zero external magnetic field. In this work, we show that a magnetic
domain wall... | cond-mat.mes-hall | a profound manifestation of topologically nontrivial states of matter is the occurrence of fractionally charged elementary excitations the quantum spin hall insulator state is a fundamentally novel quantum state of matter that exists at zero external magnetic field in this work we show that a magnetic domain wall at th... | [['a', 'profound', 'manifestation', 'of', 'topologically', 'nontrivial', 'states', 'of', 'matter', 'is', 'the', 'occurrence', 'of', 'fractionally', 'charged', 'elementary', 'excitations', 'the', 'quantum', 'spin', 'hall', 'insulator', 'state', 'is', 'a', 'fundamentally', 'novel', 'quantum', 'state', 'of', 'matter', 'th... | [-0.2125813915796614, 0.2737227947177372, -0.07840024313247464, 0.0274816100458497, -0.07049204909143228, -0.13040164748242902, 0.0567883442097244, 0.34119941001233545, -0.2708203177718283, -0.274203720059499, 0.007478707866716081, -0.2749164630884974, -0.14265042670055303, 0.15988825035317647, -0.00881178496468776, -0... |
710.0731 | Symplectic resolutions, Lefschetz property and formality | We introduce a method to resolve a symplectic orbifold into a smooth
symplectic manifold. Then we study how the formality and the Lefschetz property
of the symplectic resolution are compared with that of the symplectic orbifold.
We also study the formality of the symplectic blow-up of a symplectic orbifold
along symp... | math.SG math.AT math.DG | we introduce a method to resolve a symplectic orbifold into a smooth symplectic manifold then we study how the formality and the lefschetz property of the symplectic resolution are compared with that of the symplectic orbifold we also study the formality of the symplectic blowup of a symplectic orbifold along symplecti... | [['we', 'introduce', 'a', 'method', 'to', 'resolve', 'a', 'symplectic', 'orbifold', 'into', 'a', 'smooth', 'symplectic', 'manifold', 'then', 'we', 'study', 'how', 'the', 'formality', 'and', 'the', 'lefschetz', 'property', 'of', 'the', 'symplectic', 'resolution', 'are', 'compared', 'with', 'that', 'of', 'the', 'symplect... | [-0.2009459136813683, -0.015441461329005266, -0.17432270450027365, 0.11978898522885222, -0.15372955731949525, -0.19134967462894947, -0.007183002229583891, 0.3332104109105115, -0.28007033867271325, -0.19872709076459472, 0.0839859563710266, -0.20516137861122843, -0.17074530210934188, 0.13451950122651302, -0.2104055940810... |
710.0732 | Comment on ``Coherent Control of a V-Type Three-Level System in a Single
Quantum Dot'' | This is a Comment on Phys. Rev. Lett., {\bf 95}, 187404 (2005)
| cond-mat.mtrl-sci | this is a comment on phys rev lett bf 95 187404 2005 | [['this', 'is', 'a', 'comment', 'on', 'phys', 'rev', 'lett', 'bf', '95', '187404', '2005']] | [-0.11168505501171405, 0.050578167365694586, 0.09786337618292733, -0.42437254993075674, -0.20593649843199688, 0.03240089012648572, 0.30327611552043393, 0.2382248927077109, 0.28821268339048733, -0.3390009447254918, -0.23995896090160718, -0.24303085255351933, -0.3319421783089638, 0.21379565752365373, -0.41116136066954245... |
710.0733 | Total control over ultracold interactions via electric and magnetic
fields | The scattering length is commonly used to characterize the strength of
ultracold atomic interactions, since it is the leading parameter in the
low-energy expansion of the scattering phase shift. Its value can be modified
via a magnetic field, by using a Feshbach resonance. However, the effective
range term, which is ... | physics.atom-ph cond-mat.other | the scattering length is commonly used to characterize the strength of ultracold atomic interactions since it is the leading parameter in the lowenergy expansion of the scattering phase shift its value can be modified via a magnetic field by using a feshbach resonance however the effective range term which is the secon... | [['the', 'scattering', 'length', 'is', 'commonly', 'used', 'to', 'characterize', 'the', 'strength', 'of', 'ultracold', 'atomic', 'interactions', 'since', 'it', 'is', 'the', 'leading', 'parameter', 'in', 'the', 'lowenergy', 'expansion', 'of', 'the', 'scattering', 'phase', 'shift', 'its', 'value', 'can', 'be', 'modified'... | [-0.1483964305978212, 0.21642968541910423, -0.07377555838420763, 0.02046585307508739, -0.08014104089796029, -0.0865978623764461, 0.03416991461538067, 0.3549765451763082, -0.30159338324427093, -0.299362413360384, 0.05659426595204799, -0.20970995079099747, -0.09539777451949515, 0.22119699522917127, 0.04135961785655597, 0... |
710.0734 | Obstruction theory on 8-manifolds | This note gives a uniform, self-contained, and fairly direct approach to a
variety of obstruction-theoretic problems on 8-manifolds. We give necessary and
sufficient cohomological critera for the existence of almost complex and almost
quaternionic structures on the tangent bundle and for the reduction of the
structur... | math.AT math.GT | this note gives a uniform selfcontained and fairly direct approach to a variety of obstructiontheoretic problems on 8manifolds we give necessary and sufficient cohomological critera for the existence of almost complex and almost quaternionic structures on the tangent bundle and for the reduction of the structure group ... | [['this', 'note', 'gives', 'a', 'uniform', 'selfcontained', 'and', 'fairly', 'direct', 'approach', 'to', 'a', 'variety', 'of', 'obstructiontheoretic', 'problems', 'on', '8manifolds', 'we', 'give', 'necessary', 'and', 'sufficient', 'cohomological', 'critera', 'for', 'the', 'existence', 'of', 'almost', 'complex', 'and', ... | [-0.1653170289746562, 0.035448620363031744, -0.09619045022447578, 0.07799736600269976, -0.14028535542063048, -0.09807048812813934, 0.04013077260880563, 0.3616273581798448, -0.2794336023450386, -0.2307392557907361, 0.1253949303378458, -0.17431093654671653, -0.15443519721968008, 0.17025011461838835, -0.1033841892771545, ... |
710.0735 | Critical points of quadratic renormalizations of random variables and
phase transitions of disordered polymer models on diamond lattices | We study the wetting transition and the directed polymer delocalization
transition on diamond hierarchical lattices.These two phase transitions with
frozen disorder correspond to the critical points of quadratic renormalizations
of the partition function.(These exact renormalizations on diamond lattices can
also be c... | cond-mat.dis-nn | we study the wetting transition and the directed polymer delocalization transition on diamond hierarchical latticesthese two phase transitions with frozen disorder correspond to the critical points of quadratic renormalizations of the partition functionthese exact renormalizations on diamond lattices can also be consid... | [['we', 'study', 'the', 'wetting', 'transition', 'and', 'the', 'directed', 'polymer', 'delocalization', 'transition', 'on', 'diamond', 'hierarchical', 'latticesthese', 'two', 'phase', 'transitions', 'with', 'frozen', 'disorder', 'correspond', 'to', 'the', 'critical', 'points', 'of', 'quadratic', 'renormalizations', 'of... | [-0.13854172358463984, 0.22659858675906436, -0.04836490745190531, 0.05534471193619538, -0.0022892971118562856, -0.16377350802766158, 0.0693974587858247, 0.35873877838253976, -0.26734727738890796, -0.18942828939441825, 0.059657870231894776, -0.3654245027154684, -0.10537111825309693, 0.0828286122204736, 0.049546285942196... |
710.0736 | Colour image segmentation by the vector-valued Allen-Cahn phase-field
model: a multigrid solution | We propose a new method for the numerical solution of a PDE-driven model for
colour image segmentation and give numerical examples of the results. The
method combines the vector-valued Allen-Cahn phase field equation with initial
data fitting terms. This method is known to be closely related to the
Mumford-Shah probl... | cs.CV cs.NA | we propose a new method for the numerical solution of a pdedriven model for colour image segmentation and give numerical examples of the results the method combines the vectorvalued allencahn phase field equation with initial data fitting terms this method is known to be closely related to the mumfordshah problem and t... | [['we', 'propose', 'a', 'new', 'method', 'for', 'the', 'numerical', 'solution', 'of', 'a', 'pdedriven', 'model', 'for', 'colour', 'image', 'segmentation', 'and', 'give', 'numerical', 'examples', 'of', 'the', 'results', 'the', 'method', 'combines', 'the', 'vectorvalued', 'allencahn', 'phase', 'field', 'equation', 'with'... | [-0.04907460244482054, -0.02084211811050088, -0.10672360515232225, 0.044439467224840296, -0.06738430857658387, -0.12024752437410986, 0.01747699069845326, 0.36742791761370264, -0.27145457754240315, -0.3313150522244327, 0.13100474039640497, -0.2575202235294616, -0.1506198968519183, 0.2350685681353378, -0.0896334758466657... |
710.0737 | Dynamical Simulations with Highly Improved Staggered Quarks | It is well established that lattice artifacts can be suppressed substantially
by the use of SU(3)-projected smeared links in the fermion action. An example
is the Highly Improved Staggered Quark action where the ASQ-like effective
links are constructed from reunitarized Fat7 links. A general procedure is
presented fo... | hep-lat | it is well established that lattice artifacts can be suppressed substantially by the use of su3projected smeared links in the fermion action an example is the highly improved staggered quark action where the asqlike effective links are constructed from reunitarized fat7 links a general procedure is presented for comput... | [['it', 'is', 'well', 'established', 'that', 'lattice', 'artifacts', 'can', 'be', 'suppressed', 'substantially', 'by', 'the', 'use', 'of', 'su3projected', 'smeared', 'links', 'in', 'the', 'fermion', 'action', 'an', 'example', 'is', 'the', 'highly', 'improved', 'staggered', 'quark', 'action', 'where', 'the', 'asqlike', ... | [-0.14628242960195864, 0.2177497824637868, -0.10588089414691353, 0.07403698873567618, -0.05773186592446748, -0.13041151288323383, 0.04580498400937058, 0.38675006826923897, -0.20615417593012542, -0.28580640674970875, 0.0834028347845628, -0.2617967100929438, -0.15240773125667095, 0.1792609624733979, -0.013617685641939482... |
710.0738 | Superconductivity in novel Ge-based skutterudites: {Sr,Ba}Pt_4Ge_{12} | Combining experiments and ab initio models we report on $\rm SrPt_4Ge_{12}$
and $\rm BaPt_4Ge_{12}$ as members of a novel class of superconducting
skutterudites, where Sr or Ba atoms stabilize a framework entirely formed by
Ge-atoms. Below $T_c=5.35$ K, and 5.10 K for $\rm BaPt_4Ge_{12}$ and $\rm
SrPt_4Ge_{12}$, resp... | cond-mat.supr-con cond-mat.mtrl-sci | combining experiments and ab initio models we report on rm srpt_4ge_12 and rm bapt_4ge_12 as members of a novel class of superconducting skutterudites where sr or ba atoms stabilize a framework entirely formed by geatoms below t_c535 k and 510 k for rm bapt_4ge_12 and rm srpt_4ge_12 respectively electronphonon coupled ... | [['combining', 'experiments', 'and', 'ab', 'initio', 'models', 'we', 'report', 'on', 'rm', 'srpt_4ge_12', 'and', 'rm', 'bapt_4ge_12', 'as', 'members', 'of', 'a', 'novel', 'class', 'of', 'superconducting', 'skutterudites', 'where', 'sr', 'or', 'ba', 'atoms', 'stabilize', 'a', 'framework', 'entirely', 'formed', 'by', 'ge... | [-0.13633849430256165, 0.18649992477506971, 0.0130004552551187, 0.023208307324407193, 0.021165610405688103, -0.15755489255086733, 0.1140393184354672, 0.36824191672584183, -0.2728097132478769, -0.30156366138790663, -0.032587780355690765, -0.36085201589963756, -0.08286694681916673, 0.12910694932350172, 0.1197815690906002... |
710.0739 | Transport and spectral functions in high-temperature QCD | The current status of transport coefficients in relativistic field theories
at high temperature is reviewed. I contrast weak coupling results obtained
using kinetic theory/diagrammatic techniques with strong coupling results
obtained using gauge/gravity duality, and describe the recent developments in
extracting tran... | hep-lat hep-ph nucl-th | the current status of transport coefficients in relativistic field theories at high temperature is reviewed i contrast weak coupling results obtained using kinetic theorydiagrammatic techniques with strong coupling results obtained using gaugegravity duality and describe the recent developments in extracting transport ... | [['the', 'current', 'status', 'of', 'transport', 'coefficients', 'in', 'relativistic', 'field', 'theories', 'at', 'high', 'temperature', 'is', 'reviewed', 'i', 'contrast', 'weak', 'coupling', 'results', 'obtained', 'using', 'kinetic', 'theorydiagrammatic', 'techniques', 'with', 'strong', 'coupling', 'results', 'obtaine... | [-0.09234850435302808, 0.18049957435578107, -0.049845187896146226, 0.05458998753545949, -0.021830148865970282, -0.12220732500919929, -0.0037549176468298986, 0.35777625891451653, -0.2664705797886619, -0.23002772430101268, 0.08881225138902664, -0.29078078439029365, -0.08227295995904849, 0.18290458301512094, 0.04946726540... |
710.074 | On 3-dimensional Asymptotically Harmonic Manifolds | Let (M,g) be a complete, simply connected Riemannian manifold of dimension 3
without conjugate points. We show that M is a hyperbolic manifold of constant
sectional curvature, provided M is asymptotically harmonic of constant h > 0.
| math.DG | let mg be a complete simply connected riemannian manifold of dimension 3 without conjugate points we show that m is a hyperbolic manifold of constant sectional curvature provided m is asymptotically harmonic of constant h 0 | [['let', 'mg', 'be', 'a', 'complete', 'simply', 'connected', 'riemannian', 'manifold', 'of', 'dimension', '3', 'without', 'conjugate', 'points', 'we', 'show', 'that', 'm', 'is', 'a', 'hyperbolic', 'manifold', 'of', 'constant', 'sectional', 'curvature', 'provided', 'm', 'is', 'asymptotically', 'harmonic', 'of', 'constan... | [-0.2648845108018981, 0.16814878269926542, -0.009263875894248486, -0.001718768054464211, -0.16599211017859894, -0.28327378674617243, -0.028061041401492223, 0.40602721367031336, -0.19357645681237853, -0.21337874699383974, 0.07488123869471666, -0.29309058874948984, -0.12720375334740514, 0.13394189763089848, -0.1207813372... |
710.0741 | B Semileptonic Decays at High Recoil Momentum | We explore the possibility of studying $B\to\pi l\nu$ semileptonic decays at
large recoil momentum. Our methods include the use of a random-wall source for
the pion to reduce statistical errors, and different smearing functions are
used for the B meson to improve the overlap with the ground state. We observe,
in gene... | hep-lat | we explore the possibility of studying btopi lnu semileptonic decays at large recoil momentum our methods include the use of a randomwall source for the pion to reduce statistical errors and different smearing functions are used for the b meson to improve the overlap with the ground state we observe in general a factor... | [['we', 'explore', 'the', 'possibility', 'of', 'studying', 'btopi', 'lnu', 'semileptonic', 'decays', 'at', 'large', 'recoil', 'momentum', 'our', 'methods', 'include', 'the', 'use', 'of', 'a', 'randomwall', 'source', 'for', 'the', 'pion', 'to', 'reduce', 'statistical', 'errors', 'and', 'different', 'smearing', 'function... | [-0.051982307973415104, 0.1494997269682475, -0.06040856591773344, 0.15473194456478553, -0.026760294588644113, -0.08367404728474569, 0.10229059952179165, 0.3473642354469691, -0.21064458809681794, -0.26023696771642163, -0.005622990622268573, -0.32056015771605184, -0.0180760915425898, 0.15553140332018817, 0.04210353281293... |
710.0742 | Principle of Minimum Distance in Space of States as New Principle in
Quantum Physics | The mathematician Leonhard Euler (1707-1783) appears to have been a
philosophical optimist having written: "Since the fabric of universe is the
most perfect and is the work of the most wise Creator, nothing whatsoever take
place in this universe in which some relation of maximum or minimum does not
appear. Wherefore,... | physics.gen-ph | the mathematician leonhard euler 17071783 appears to have been a philosophical optimist having written since the fabric of universe is the most perfect and is the work of the most wise creator nothing whatsoever take place in this universe in which some relation of maximum or minimum does not appear wherefore there is ... | [['the', 'mathematician', 'leonhard', 'euler', '17071783', 'appears', 'to', 'have', 'been', 'a', 'philosophical', 'optimist', 'having', 'written', 'since', 'the', 'fabric', 'of', 'universe', 'is', 'the', 'most', 'perfect', 'and', 'is', 'the', 'work', 'of', 'the', 'most', 'wise', 'creator', 'nothing', 'whatsoever', 'tak... | [-0.1140871664460249, 0.14176510161453643, -0.13388469559815375, 0.09532254918662332, -0.07240727021311666, -0.09380271664712632, 0.08218592046878125, 0.31678113927794754, -0.2508452316228152, -0.3068562861822168, 0.07123257154608323, -0.2697875319199343, -0.1387854080440129, 0.1731560492117896, -0.05688257983959941, 0... |
710.0743 | Generalized Super-Cerenkov Radiations in Nuclear and Hadronic Media | Generalized Super-Cerenkov Radiations (SCR), as well as their SCR-signatures
are investigated and classified. Two general SCR- coherence conditions are
found as two natural extremes of the same spontaneous particles decay in
(dielectric, nuclear or hadronic) media The main results on the quantum theory
of the SCR-phe... | hep-ph | generalized supercerenkov radiations scr as well as their scrsignatures are investigated and classified two general scr coherence conditions are found as two natural extremes of the same spontaneous particles decay in dielectric nuclear or hadronic media the main results on the quantum theory of the scrphenomena as wel... | [['generalized', 'supercerenkov', 'radiations', 'scr', 'as', 'well', 'as', 'their', 'scrsignatures', 'are', 'investigated', 'and', 'classified', 'two', 'general', 'scr', 'coherence', 'conditions', 'are', 'found', 'as', 'two', 'natural', 'extremes', 'of', 'the', 'same', 'spontaneous', 'particles', 'decay', 'in', 'dielec... | [-0.0428487273479382, 0.19035554277406147, -0.07008018074198984, 0.10354876738766997, -0.021021783333988145, -0.07761012612340543, -0.043323328824883975, 0.3276498360881725, -0.2167812280374794, -0.312496033797148, 0.10393510071690588, -0.27105039321423435, -0.12887928550089084, 0.22817329595272895, 0.00052761181723326... |
710.0744 | New Nuclear And Subnuclear Exotic Decays | In this paper new nuclear and subnuclear exotic decays are investigated. Some
theoretical problems of the pionic radioactivity, such as fission-like models,
applicable to all kind of exotic nuclear and subnuclear decays are presented.
The induced nuclear and subnuclear decays are discussed. Moreover, using the
recent... | nucl-th | in this paper new nuclear and subnuclear exotic decays are investigated some theoretical problems of the pionic radioactivity such as fissionlike models applicable to all kind of exotic nuclear and subnuclear decays are presented the induced nuclear and subnuclear decays are discussed moreover using the recent results ... | [['in', 'this', 'paper', 'new', 'nuclear', 'and', 'subnuclear', 'exotic', 'decays', 'are', 'investigated', 'some', 'theoretical', 'problems', 'of', 'the', 'pionic', 'radioactivity', 'such', 'as', 'fissionlike', 'models', 'applicable', 'to', 'all', 'kind', 'of', 'exotic', 'nuclear', 'and', 'subnuclear', 'decays', 'are',... | [0.00407170521951205, 0.2745651331214184, -0.04624740467280955, 0.17145044933469664, -0.0025524760004938456, -0.08576697732850506, 0.010308443411328905, 0.32600194256047943, -0.19682809382651908, -0.23259691230801716, 0.028345236539010058, -0.34339494387795394, -0.01052425945857288, 0.20468715332901558, 0.0418829701088... |
710.0745 | Mixing Kohonen Algorithm, Markov Switching Model and Detection of
Multiple Change-Points: An Application to Monetary History | The present paper aims at locating the breakings of the integration process
of an international system observed during about 50 years in the 19th century.
A historical study could link them to special events, which operated as
exogenous shocks on this process. The indicator of integration used is the
spread between t... | q-fin.GN stat.AP | the present paper aims at locating the breakings of the integration process of an international system observed during about 50 years in the 19th century a historical study could link them to special events which operated as exogenous shocks on this process the indicator of integration used is the spread between the hi... | [['the', 'present', 'paper', 'aims', 'at', 'locating', 'the', 'breakings', 'of', 'the', 'integration', 'process', 'of', 'an', 'international', 'system', 'observed', 'during', 'about', '50', 'years', 'in', 'the', '19th', 'century', 'a', 'historical', 'study', 'could', 'link', 'them', 'to', 'special', 'events', 'which', ... | [-0.13711699332977548, 0.0664220983429899, -0.0785074573657589, 0.08005901872445058, -0.062392646689119376, -0.07069799121529834, 0.0688007803135968, 0.36122306763398937, -0.2553907435470662, -0.33526420243447874, 0.14038226889101865, -0.26856361347538366, -0.11681358805456298, 0.21305316017478765, -0.055104202166866, ... |
710.0746 | Universality and Scaling at the chiral transition in two-flavor QCD at
finite temperature | The order of the phase transition in finite-temperature QCD with two
degenerate light quarks is still an open problem and corresponds to the last
question mark in the zero-density phase diagram of QCD. We argue that
establishing the nature of the transition in this case is also a crucial test
for numerical simulation... | hep-lat | the order of the phase transition in finitetemperature qcd with two degenerate light quarks is still an open problem and corresponds to the last question mark in the zerodensity phase diagram of qcd we argue that establishing the nature of the transition in this case is also a crucial test for numerical simulations of ... | [['the', 'order', 'of', 'the', 'phase', 'transition', 'in', 'finitetemperature', 'qcd', 'with', 'two', 'degenerate', 'light', 'quarks', 'is', 'still', 'an', 'open', 'problem', 'and', 'corresponds', 'to', 'the', 'last', 'question', 'mark', 'in', 'the', 'zerodensity', 'phase', 'diagram', 'of', 'qcd', 'we', 'argue', 'that... | [-0.10969792308261324, 0.16755690732469175, -0.09845115805632974, 0.06922896768389221, -0.042912770712159966, -0.09698333051423297, 0.12247859504637554, 0.3573692593429434, -0.2249832963999851, -0.258006163750236, 0.10055528366233614, -0.26284409108522694, -0.1094968932601133, 0.13989580020394274, -0.012213791957612173... |
710.0747 | Calibration of the mirror system in the HERA-B RICH | The mirror system of the HERA-B RICH consists of two spherical and two planar
mirrors, composed of altogether 116 mirror segments. Analysis of displacements
of the \v{C}erenkov ring center relative to the charged particle track, for
given spherical-planar segment pairs, leads to accurate information regarding
the ori... | physics.ins-det | the mirror system of the herab rich consists of two spherical and two planar mirrors composed of altogether 116 mirror segments analysis of displacements of the vcerenkov ring center relative to the charged particle track for given sphericalplanar segment pairs leads to accurate information regarding the orientation of... | [['the', 'mirror', 'system', 'of', 'the', 'herab', 'rich', 'consists', 'of', 'two', 'spherical', 'and', 'two', 'planar', 'mirrors', 'composed', 'of', 'altogether', '116', 'mirror', 'segments', 'analysis', 'of', 'displacements', 'of', 'the', 'vcerenkov', 'ring', 'center', 'relative', 'to', 'the', 'charged', 'particle', ... | [-0.13118770926208426, 0.10610488848122832, -0.06225007522391946, 0.038412056866497415, -0.029339472916334458, -0.12789983971503704, -0.024401727813449115, 0.35541818627755933, -0.22875890962473333, -0.3544779954707786, 0.058586116604290084, -0.3267604624852538, -0.04581882403716955, 0.18449760680820487, -0.05596495305... |
710.0748 | A Fast Heuristic Algorithm Based on Verification and Elimination Methods
for Maximum Clique Problem | A clique in an undirected graph G= (V, E) is a subset V' V of vertices, each
pair of which is connected by an edge in E. The clique problem is an
optimization problem of finding a clique of maximum size in graph. The clique
problem is NP-Complete. We have succeeded in developing a fast algorithm for
maximum clique pr... | cs.DM cs.CC | a clique in an undirected graph g v e is a subset v v of vertices each pair of which is connected by an edge in e the clique problem is an optimization problem of finding a clique of maximum size in graph the clique problem is npcomplete we have succeeded in developing a fast algorithm for maximum clique problem by emp... | [['a', 'clique', 'in', 'an', 'undirected', 'graph', 'g', 'v', 'e', 'is', 'a', 'subset', 'v', 'v', 'of', 'vertices', 'each', 'pair', 'of', 'which', 'is', 'connected', 'by', 'an', 'edge', 'in', 'e', 'the', 'clique', 'problem', 'is', 'an', 'optimization', 'problem', 'of', 'finding', 'a', 'clique', 'of', 'maximum', 'size',... | [-0.170916928531791, 0.08200641698488692, -0.04123212898021861, 0.0030357722037782273, -0.12826285318073316, -0.17571704588034123, 0.07691417145205365, 0.39901525135813415, -0.3091996224745568, -0.35309169025403325, 0.12476011362530803, -0.25860985597777786, -0.11388677433706766, 0.1464209223429308, -0.0820045248197013... |
710.0749 | Observations of V838 Mon in the CO rotational lines | We investigate the structure of a field around the position of V838 Mon as
seen in the lowest CO rotational transitions. We also measure and analyse
emission in the same lines at the position of V838 Mon.Observations have
primarily been done in the CO J = 2-1 and J = 3-2 lines using the KOSMA
telescope. A field of 3.... | astro-ph | we investigate the structure of a field around the position of v838 mon as seen in the lowest co rotational transitions we also measure and analyse emission in the same lines at the position of v838 monobservations have primarily been done in the co j 21 and j 32 lines using the kosma telescope a field of 34 squared de... | [['we', 'investigate', 'the', 'structure', 'of', 'a', 'field', 'around', 'the', 'position', 'of', 'v838', 'mon', 'as', 'seen', 'in', 'the', 'lowest', 'co', 'rotational', 'transitions', 'we', 'also', 'measure', 'and', 'analyse', 'emission', 'in', 'the', 'same', 'lines', 'at', 'the', 'position', 'of', 'v838', 'monobserva... | [-0.09981254392232586, 0.06457847603638811, -0.054805060934086214, -0.004286166243673506, -0.044013937598720076, -0.10556238258322992, 0.033911272796331104, 0.44219495642755646, -0.18810205531372048, -0.33351650545955636, 0.06948315393083249, -0.2703886255167163, -0.021900366758927703, 0.12609280117794697, -0.012081969... |
710.075 | Nuclear Tuning and Detuning of the Electron Spin Resonance in a Quantum
Dot | We study nuclear spin dynamics in a quantum dot close to the conditions of
electron spin resonance. We show that at small frequency mismatch the nuclear
field detunes the resonance. Remarkably, at larger frequency mismatch its
effect is opposite: The nuclear system is bistable, and in one of the stable
states the fie... | cond-mat.mes-hall | we study nuclear spin dynamics in a quantum dot close to the conditions of electron spin resonance we show that at small frequency mismatch the nuclear field detunes the resonance remarkably at larger frequency mismatch its effect is opposite the nuclear system is bistable and in one of the stable states the field accu... | [['we', 'study', 'nuclear', 'spin', 'dynamics', 'in', 'a', 'quantum', 'dot', 'close', 'to', 'the', 'conditions', 'of', 'electron', 'spin', 'resonance', 'we', 'show', 'that', 'at', 'small', 'frequency', 'mismatch', 'the', 'nuclear', 'field', 'detunes', 'the', 'resonance', 'remarkably', 'at', 'larger', 'frequency', 'mism... | [-0.15728090358777091, 0.27593443721423966, -0.050408377916878695, 0.10120661142765992, -0.006286042945024061, -0.11699262279533333, -0.03573186412248035, 0.36976193056091083, -0.29114376372573053, -0.24707720876223854, 0.035319658409042116, -0.2667052243449181, -0.04276927657328643, 0.17610629436305977, 0.054937109435... |
710.0751 | Leptonic secondary emission in a hadronic microquasar model | Context: It has been proposed that the origin of the very high-energy photons
emitted from high-mass X-ray binaries with jet-like features, so-called
microquasars (MQs), is related to hadronic interactions between relativistic
protons in the jet and cold protons of the stellar wind. Leptonic secondary
emission should... | astro-ph | context it has been proposed that the origin of the very highenergy photons emitted from highmass xray binaries with jetlike features socalled microquasars mqs is related to hadronic interactions between relativistic protons in the jet and cold protons of the stellar wind leptonic secondary emission should be calculate... | [['context', 'it', 'has', 'been', 'proposed', 'that', 'the', 'origin', 'of', 'the', 'very', 'highenergy', 'photons', 'emitted', 'from', 'highmass', 'xray', 'binaries', 'with', 'jetlike', 'features', 'socalled', 'microquasars', 'mqs', 'is', 'related', 'to', 'hadronic', 'interactions', 'between', 'relativistic', 'protons... | [-0.05098925443966076, 0.2552219787339873, -0.07721076633803219, 0.18180376575850182, -0.03167445742305439, -0.07543608073883497, -0.01735286813739033, 0.4035346202619441, -0.23024895363529255, -0.325252392342451, -0.054937928632375795, -0.32680610920143155, 0.04767144670676406, 0.17871734849649254, 0.07755348456369059... |
710.0752 | The Einstein-Yang-Mills equations from Bianchi identities | We suggest a novel extension to the Kaluza-Klein scheme that allows us to
obtain consistently all SU(n) Einstein-Yang-Mills theories. This construction
is based on allowing the five-dimensional spacetime to carry some non-vanishing
torsion; however, the four-dimensional spacetime remains intrinsically
torsion-free.
| gr-qc hep-th | we suggest a novel extension to the kaluzaklein scheme that allows us to obtain consistently all sun einsteinyangmills theories this construction is based on allowing the fivedimensional spacetime to carry some nonvanishing torsion however the fourdimensional spacetime remains intrinsically torsionfree | [['we', 'suggest', 'a', 'novel', 'extension', 'to', 'the', 'kaluzaklein', 'scheme', 'that', 'allows', 'us', 'to', 'obtain', 'consistently', 'all', 'sun', 'einsteinyangmills', 'theories', 'this', 'construction', 'is', 'based', 'on', 'allowing', 'the', 'fivedimensional', 'spacetime', 'to', 'carry', 'some', 'nonvanishing'... | [-0.17867783622350544, 0.13326443985570222, -0.1339041447488853, 0.11071948995813727, -0.23304950239835306, -0.17162075195228682, -0.026744034979492425, 0.30430511478334665, -0.12723842579871417, -0.248271724418737, 0.06432144019054249, -0.18931281916484294, -0.16593429357744754, 0.14685471602715552, -0.133651220420142... |
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