id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
709.3835 | Correlated entanglement distillation and the structure of the set of
undistillable states | We consider entanglement distillation under the assumption that the input
states are allowed to be correlated among each other. We hence replace the
usually considered independent and identically-distributed hypothesis by the
weaker assumption of merely having identical reductions. We find that whether a
state is the... | quant-ph | we consider entanglement distillation under the assumption that the input states are allowed to be correlated among each other we hence replace the usually considered independent and identicallydistributed hypothesis by the weaker assumption of merely having identical reductions we find that whether a state is then dis... | [['we', 'consider', 'entanglement', 'distillation', 'under', 'the', 'assumption', 'that', 'the', 'input', 'states', 'are', 'allowed', 'to', 'be', 'correlated', 'among', 'each', 'other', 'we', 'hence', 'replace', 'the', 'usually', 'considered', 'independent', 'and', 'identicallydistributed', 'hypothesis', 'by', 'the', '... | [-0.13282024159347747, 0.15740010384941908, -0.10627442518591709, 0.05232176514698364, -0.008602373799758738, -0.17535849216651042, 0.06602731211935224, 0.33646772768691013, -0.27326157198544465, -0.24928077424330444, 0.10687699554763713, -0.2781451283940703, -0.1362934822080143, 0.16199193842074802, -0.037524506368074... |
709.3836 | Flares from spiral waves by lensing and time-delay amplification? | Episodically accreting black holes are thought to produce flares when a chunk
of particles is accelerated to high velocity near the black hole horizon. This
also seems to be the case of Sagittarius A* in the Galactic Center, where the
broad-band radiation is produced, likely via the synchrotron self-Compton
mechanism... | astro-ph | episodically accreting black holes are thought to produce flares when a chunk of particles is accelerated to high velocity near the black hole horizon this also seems to be the case of sagittarius a in the galactic center where the broadband radiation is produced likely via the synchrotron selfcompton mechanism it has ... | [['episodically', 'accreting', 'black', 'holes', 'are', 'thought', 'to', 'produce', 'flares', 'when', 'a', 'chunk', 'of', 'particles', 'is', 'accelerated', 'to', 'high', 'velocity', 'near', 'the', 'black', 'hole', 'horizon', 'this', 'also', 'seems', 'to', 'be', 'the', 'case', 'of', 'sagittarius', 'a', 'in', 'the', 'gal... | [-0.09083449755947759, 0.1228266931475025, -0.0935841687520787, 0.1425441483417244, -0.13534582620200758, -0.11685513319394608, 0.018981573723125672, 0.405150925608027, -0.2116171301216603, -0.3166812523841954, 0.06449868027957693, -0.27239638206953337, -0.0906766839797718, 0.2010248606905235, -0.04718504166257488, -0.... |
709.3837 | The Atiyah--Hitchin bracket for the cubic Nonlinear Schrodinger
equation. IV. the scattering potentials | This is the last in a series of four papers on Poisson formalism for the
cubic nonlinear Schrodinger equation with repulsive nonlinearity. In this paper
we consider scattering potentials.
| math-ph math.AG math.MP | this is the last in a series of four papers on poisson formalism for the cubic nonlinear schrodinger equation with repulsive nonlinearity in this paper we consider scattering potentials | [['this', 'is', 'the', 'last', 'in', 'a', 'series', 'of', 'four', 'papers', 'on', 'poisson', 'formalism', 'for', 'the', 'cubic', 'nonlinear', 'schrodinger', 'equation', 'with', 'repulsive', 'nonlinearity', 'in', 'this', 'paper', 'we', 'consider', 'scattering', 'potentials']] | [-0.14196616523610106, 0.03613964625602138, -0.06027671919557555, -0.0005649864344440144, -0.0714051066416091, -0.12532950846221427, -0.07255355733976668, 0.34200891467003985, -0.2543289228503046, -0.18408797475798377, 0.01613613996044572, -0.3581318437153923, -0.2485274836934846, 0.15996410164596706, 0.006233515378473... |
709.3838 | Transverse stability of relativistic two-component jets | Context: Astrophysical jets from various sources seem to be stratified, with
a fast inner jet and a slower outer jet. As it is likely that the launching
mechanism for each component is different, their interface will develop
differential rotation, while the outer jet radius represents a second interface
where disrupt... | astro-ph | context astrophysical jets from various sources seem to be stratified with a fast inner jet and a slower outer jet as it is likely that the launching mechanism for each component is different their interface will develop differential rotation while the outer jet radius represents a second interface where disruptions ma... | [['context', 'astrophysical', 'jets', 'from', 'various', 'sources', 'seem', 'to', 'be', 'stratified', 'with', 'a', 'fast', 'inner', 'jet', 'and', 'a', 'slower', 'outer', 'jet', 'as', 'it', 'is', 'likely', 'that', 'the', 'launching', 'mechanism', 'for', 'each', 'component', 'is', 'different', 'their', 'interface', 'will... | [-0.1827258441359953, 0.181753926694956, -0.10563287490749952, 0.07062783167733006, -0.10548956913703864, -0.09427264008090942, -0.07572291191308207, 0.3918109706157061, -0.2728060078156039, -0.273584712963646, 0.07102919990094221, -0.22141273868852543, -0.013592942818107431, 0.15802914971067428, 0.04953085801710169, 0... |
709.3839 | Estimating the final spin of a binary black hole coalescence | We present a straightforward approach for estimating the final black hole
spin of a binary black hole coalescence with arbitrary initial masses and
spins. Making some simple assumptions, we estimate the final angular momentum
to be the sum of the individual spins plus the orbital angular momentum of a
test particle o... | astro-ph gr-qc | we present a straightforward approach for estimating the final black hole spin of a binary black hole coalescence with arbitrary initial masses and spins making some simple assumptions we estimate the final angular momentum to be the sum of the individual spins plus the orbital angular momentum of a test particle orbit... | [['we', 'present', 'a', 'straightforward', 'approach', 'for', 'estimating', 'the', 'final', 'black', 'hole', 'spin', 'of', 'a', 'binary', 'black', 'hole', 'coalescence', 'with', 'arbitrary', 'initial', 'masses', 'and', 'spins', 'making', 'some', 'simple', 'assumptions', 'we', 'estimate', 'the', 'final', 'angular', 'mom... | [-0.1307935861557988, 0.12558897387635495, -0.09356282151304185, 0.11487006462711309, -0.0743982932450516, -0.12445879458050643, 0.046664080493418233, 0.3407109970599413, -0.1804407266500805, -0.3447531741751092, 0.0660272167050945, -0.2524724388282214, -0.04563248472442086, 0.21220998134264457, -0.021770992683512826, ... |
709.384 | Entanglement Entropy in the Two-Dimensional Random Transverse Field
Ising Model | The scaling behavior of the entanglement entropy in the two-dimensional
random transverse field Ising model is studied numerically through the strong
disordered renormalization group method. We find that the leading term of the
entanglement entropy always scales linearly with the block size. However,
besides this \em... | cond-mat.dis-nn cond-mat.stat-mech quant-ph | the scaling behavior of the entanglement entropy in the twodimensional random transverse field ising model is studied numerically through the strong disordered renormalization group method we find that the leading term of the entanglement entropy always scales linearly with the block size however besides this empharea ... | [['the', 'scaling', 'behavior', 'of', 'the', 'entanglement', 'entropy', 'in', 'the', 'twodimensional', 'random', 'transverse', 'field', 'ising', 'model', 'is', 'studied', 'numerically', 'through', 'the', 'strong', 'disordered', 'renormalization', 'group', 'method', 'we', 'find', 'that', 'the', 'leading', 'term', 'of', ... | [-0.13730518595548347, 0.20308386554988828, -0.11755668637924828, 0.056420858553610745, 0.02933924378885422, -0.16543462176341564, 0.04263049932087597, 0.30937278147321196, -0.28830579220084473, -0.2025764120509848, 0.0552185868829838, -0.34951791091589257, -0.13851631260477007, 0.12633403958461714, 0.03823110504308715... |
709.3841 | Inverse-Compton emission from halos around stars | Inverse Compton scattering by relativistic electrons produces a major
component of the diffuse emission from the Galaxy. The photon fields involved
are the cosmic microwave background and the interstellar radiation field from
stars and dust. Calculations of the inverse Compton distribution have usually
assumed a smoo... | astro-ph | inverse compton scattering by relativistic electrons produces a major component of the diffuse emission from the galaxy the photon fields involved are the cosmic microwave background and the interstellar radiation field from stars and dust calculations of the inverse compton distribution have usually assumed a smooth i... | [['inverse', 'compton', 'scattering', 'by', 'relativistic', 'electrons', 'produces', 'a', 'major', 'component', 'of', 'the', 'diffuse', 'emission', 'from', 'the', 'galaxy', 'the', 'photon', 'fields', 'involved', 'are', 'the', 'cosmic', 'microwave', 'background', 'and', 'the', 'interstellar', 'radiation', 'field', 'from... | [-0.015284424222436203, 0.15959229164341684, -0.06615158537602868, 0.1336318063694014, -0.1261637788881694, -0.004574617928986953, -0.0131174709238035, 0.4342432141242441, -0.1966227313084143, -0.29668059744987607, 0.015288190548654552, -0.3299451023802038, -0.03421636103182908, 0.228435406226062, -0.012095077910021809... |
709.3842 | A nonlinear Ramsey interferometer operating beyond the Heisenberg limit | We show that a dynamically evolving two-mode Bose-Einstein condensate (TBEC)
with an adiabatic, time-varying Raman coupling maps exactly onto a nonlinear
Ramsey interferometer that includes a nonlinear medium. Assuming a realistic
quantum state for the TBEC, namely the SU(2) coherent spin state, we find that
the meas... | cond-mat.other quant-ph | we show that a dynamically evolving twomode boseeinstein condensate tbec with an adiabatic timevarying raman coupling maps exactly onto a nonlinear ramsey interferometer that includes a nonlinear medium assuming a realistic quantum state for the tbec namely the su2 coherent spin state we find that the measurement uncer... | [['we', 'show', 'that', 'a', 'dynamically', 'evolving', 'twomode', 'boseeinstein', 'condensate', 'tbec', 'with', 'an', 'adiabatic', 'timevarying', 'raman', 'coupling', 'maps', 'exactly', 'onto', 'a', 'nonlinear', 'ramsey', 'interferometer', 'that', 'includes', 'a', 'nonlinear', 'medium', 'assuming', 'a', 'realistic', '... | [-0.1651880365183077, 0.278603618131367, -0.06026843609004395, 0.03644435353599852, 0.009225232350617283, -0.14260144194406343, 0.031486616736823105, 0.3371211045944109, -0.25924244861504653, -0.20112557675144294, 0.010862603968168358, -0.2786880914667031, -0.08086691848740618, 0.17339620792318317, 0.07238422066722883,... |
709.3843 | Dense Molecular Gas In A Young Cluster Around MWC 1080 -- Rule Of The
Massive Star | We present CS $J = 2 \to 1$, $^{13}$CO $J = 1 \to 0$, and C$^{18}$O $J = 1
\to 0$, observations with the 10-element Berkeley Illinois Maryland Association
(BIMA) Array toward the young cluster around the Be star MWC 1080. These
observations reveal a biconical outflow cavity with size $\sim$ 0.3 and 0.05 pc
for the se... | astro-ph | we present cs j 2 to 1 13co j 1 to 0 and c18o j 1 to 0 observations with the 10element berkeley illinois maryland association bima array toward the young cluster around the be star mwc 1080 these observations reveal a biconical outflow cavity with size sim 03 and 005 pc for the semimajor and semiminor axis and sim 45ar... | [['we', 'present', 'cs', 'j', '2', 'to', '1', '13co', 'j', '1', 'to', '0', 'and', 'c18o', 'j', '1', 'to', '0', 'observations', 'with', 'the', '10element', 'berkeley', 'illinois', 'maryland', 'association', 'bima', 'array', 'toward', 'the', 'young', 'cluster', 'around', 'the', 'be', 'star', 'mwc', '1080', 'these', 'obse... | [-0.08685977686660527, 0.13732842905327922, -0.03479941484831056, 0.05481740009731335, -0.07211883232357783, -0.054796240165027495, 0.0413816246738569, 0.4318102548199699, -0.14888398501219868, -0.32109896608553556, 0.05604833193815035, -0.2767639570133625, 0.03130558477867612, 0.11709328134838207, 0.01427328204362225,... |
709.3844 | An embedding theorem for automorphism groups of Cartan geometries | We prove a theorem relating the automorphism group of a Cartan geometry to
the group on which the geometry is modeled: a component of the adjoint
representation of the first embeds in the adjoint representation of the second.
Consequences of the theorem include general bounds on the rank and nilpotence
degree of an a... | math.DG math.DS | we prove a theorem relating the automorphism group of a cartan geometry to the group on which the geometry is modeled a component of the adjoint representation of the first embeds in the adjoint representation of the second consequences of the theorem include general bounds on the rank and nilpotence degree of an autom... | [['we', 'prove', 'a', 'theorem', 'relating', 'the', 'automorphism', 'group', 'of', 'a', 'cartan', 'geometry', 'to', 'the', 'group', 'on', 'which', 'the', 'geometry', 'is', 'modeled', 'a', 'component', 'of', 'the', 'adjoint', 'representation', 'of', 'the', 'first', 'embeds', 'in', 'the', 'adjoint', 'representation', 'of... | [-0.16615713156109754, 0.028712221658462937, -0.1490954499902381, 0.0442913059724517, -0.11723737249572184, -0.07173566389939792, 0.021550535717064383, 0.2957156261850503, -0.31954876914443003, -0.22162169934294762, 0.1453787961439784, -0.2248256791693469, -0.1273277381593029, 0.16471833105952965, -0.14495389801006586,... |
709.3845 | Multi-boson correlations using wave-packets II | We investigate the analytically solvable pion-laser model, and its
generalization to arbitrary multiplicity distributions. Although this kind of
extension of the model is possible, the pion laser model in its original form
is unique: it is the only model in its class that has an analytic solution.
| nucl-th | we investigate the analytically solvable pionlaser model and its generalization to arbitrary multiplicity distributions although this kind of extension of the model is possible the pion laser model in its original form is unique it is the only model in its class that has an analytic solution | [['we', 'investigate', 'the', 'analytically', 'solvable', 'pionlaser', 'model', 'and', 'its', 'generalization', 'to', 'arbitrary', 'multiplicity', 'distributions', 'although', 'this', 'kind', 'of', 'extension', 'of', 'the', 'model', 'is', 'possible', 'the', 'pion', 'laser', 'model', 'in', 'its', 'original', 'form', 'is... | [-0.08772459820560786, 0.03887045346282716, -0.12429211770548769, 0.10174434140587793, -0.06946114515480788, -0.1368333204831604, -0.001849861775079499, 0.38563914224505424, -0.2866507042604296, -0.24421159722639815, 0.07393093184319972, -0.2735823226925593, -0.16440149881553068, 0.15563494268723804, -0.019684665082225... |
709.3846 | Effect of external stress on the thermal melting of DNA | We discuss the effects of external stress on the thermal denaturation of
homogeneous DNA. Pulling double-stranded DNA at each end exerts a profound
effect on the thermal denaturation, or melting, of a long segment of this
molecule. We discuss the effects on this transition of a stretching force
applied to opposite en... | cond-mat.soft | we discuss the effects of external stress on the thermal denaturation of homogeneous dna pulling doublestranded dna at each end exerts a profound effect on the thermal denaturation or melting of a long segment of this molecule we discuss the effects on this transition of a stretching force applied to opposite ends of o... | [['we', 'discuss', 'the', 'effects', 'of', 'external', 'stress', 'on', 'the', 'thermal', 'denaturation', 'of', 'homogeneous', 'dna', 'pulling', 'doublestranded', 'dna', 'at', 'each', 'end', 'exerts', 'a', 'profound', 'effect', 'on', 'the', 'thermal', 'denaturation', 'or', 'melting', 'of', 'a', 'long', 'segment', 'of', ... | [-0.17339696582422545, 0.19512695083071543, -0.09008119014383814, 0.02054941958365015, -0.039913525836447535, -0.1194626198828978, 0.07835475977912734, 0.3376357328201944, -0.2919214746393895, -0.21288371270806608, 0.05613692860430801, -0.251348375095897, -0.11376303357222134, 0.15336398713851063, -0.002582451490926067... |
709.3847 | External Control of a Metal-Insulator Transition in GaMnAs Wires | Quantum transport in disordered ferromagnetic (III,Mn)V semiconductors is
studied theoretically. Mesoscopic wires exhibit an Anderson disorder-induced
metal-insulator transition that can be controlled by a weak external magnetic
field. This metal-insulator transition should also occur in other materials
with large an... | cond-mat.mes-hall cond-mat.mtrl-sci | quantum transport in disordered ferromagnetic iiimnv semiconductors is studied theoretically mesoscopic wires exhibit an anderson disorderinduced metalinsulator transition that can be controlled by a weak external magnetic field this metalinsulator transition should also occur in other materials with large anisotropic ... | [['quantum', 'transport', 'in', 'disordered', 'ferromagnetic', 'iiimnv', 'semiconductors', 'is', 'studied', 'theoretically', 'mesoscopic', 'wires', 'exhibit', 'an', 'anderson', 'disorderinduced', 'metalinsulator', 'transition', 'that', 'can', 'be', 'controlled', 'by', 'a', 'weak', 'external', 'magnetic', 'field', 'this... | [-0.2057784143059204, 0.35070586523725067, -0.022285118217890462, 0.04168672352097928, -0.047109470174958305, -0.24076826526628187, 0.053921365598216656, 0.4167091241106391, -0.2638786628221472, -0.24043574539634088, -0.014303477539215237, -0.30866955577706295, -0.2091092200173686, 0.18302576402202247, 0.05761928313101... |
709.3848 | KdV6: An Integrable System | $K^2 S^2 T [5]$ recently derived a new 6$^{th}$-order wave equation $KdV6$:
$(\partial^2_x + 8u_x \partial_x + 4u_{xx})(u_t + u_{xxx} + 6u_x^2) = 0$,
found a linear problem and an auto-B${\ddot{\rm{a}}}$ckclund transformation for
it, and conjectured its integrability in the usual sense. We prove this
conjecture by ... | nlin.SI | k2 s2 t 5 recently derived a new 6thorder wave equation kdv6 partial2_x 8u_x partial_x 4u_xxu_t u_xxx 6u_x2 0 found a linear problem and an autobddotrmackclund transformation for it and conjectured its integrability in the usual sense we prove this conjecture by constructing an infinite commuting hierarchy kdv_n6 with ... | [['k2', 's2', 't', '5', 'recently', 'derived', 'a', 'new', '6thorder', 'wave', 'equation', 'kdv6', 'partial2_x', '8u_x', 'partial_x', '4u_xxu_t', 'u_xxx', '6u_x2', '0', 'found', 'a', 'linear', 'problem', 'and', 'an', 'autobddotrmackclund', 'transformation', 'for', 'it', 'and', 'conjectured', 'its', 'integrability', 'in... | [-0.16576332796504287, 0.0957791359301452, -0.05493531611130059, 0.10388834514354886, -0.09228752767144938, -0.18160533917650024, -0.0506182467808651, 0.25508389491849, -0.31471714087996944, -0.2068890063179152, 0.11510593969283503, -0.25455205728491404, -0.16094526966215572, 0.1496401027053873, -0.04225817841921593, 0... |
709.3849 | Eliashberg theory of superconductivity and inelastic rare-earth impurity
scattering in filled skutterudite La$_{1-x}$Pr$_{x}$Os$_{4}$Sb$_{12}$ | We study the influence of inelastic rare-earth impurity scattering on
electron-phonon mediated superconductivity and mass renormalization in
(La$_{1-x}$Pr$_{x}$)Os$_{4}$Sb$_{12}$ compounds. Solving the strong coupling
Eliashberg equations we find that the dominant quadrupolar component of the
inelastic scattering on ... | cond-mat.supr-con cond-mat.str-el | we study the influence of inelastic rareearth impurity scattering on electronphonon mediated superconductivity and mass renormalization in la_1xpr_xos_4sb_12 compounds solving the strong coupling eliashberg equations we find that the dominant quadrupolar component of the inelastic scattering on pr impurities yields an ... | [['we', 'study', 'the', 'influence', 'of', 'inelastic', 'rareearth', 'impurity', 'scattering', 'on', 'electronphonon', 'mediated', 'superconductivity', 'and', 'mass', 'renormalization', 'in', 'la_1xpr_xos_4sb_12', 'compounds', 'solving', 'the', 'strong', 'coupling', 'eliashberg', 'equations', 'we', 'find', 'that', 'the... | [-0.19350569098427586, 0.23572179796402842, -0.01570299322887951, 0.09187002230093491, -0.0076702039650812445, -0.12792762733368698, 0.08968435953922417, 0.34157131352861014, -0.22099755811314953, -0.2441818250618799, -0.12400159808184609, -0.42803289007623585, -0.09920254438089168, 0.14874741739631459, 0.1267218260018... |
709.385 | Effect of Salt Concentration on the Electrophoretic Speed of a
Polyelectrolyte through a Nanopore | In a previous paper [S. Ghosal, Phys. Rev. E 74, 041901 (2006)] a
hydrodynamic model for determining the electrophoretic speed of a
polyelectrolyte through an axially symmetric slowly varying nanopore was
presented in the limit of a vanishingly small Debye length. Here the case of a
finite Debye layer thickness is co... | physics.chem-ph cond-mat.soft physics.bio-ph | in a previous paper s ghosal phys rev e 74 041901 2006 a hydrodynamic model for determining the electrophoretic speed of a polyelectrolyte through an axially symmetric slowly varying nanopore was presented in the limit of a vanishingly small debye length here the case of a finite debye layer thickness is considered whi... | [['in', 'a', 'previous', 'paper', 's', 'ghosal', 'phys', 'rev', 'e', '74', '041901', '2006', 'a', 'hydrodynamic', 'model', 'for', 'determining', 'the', 'electrophoretic', 'speed', 'of', 'a', 'polyelectrolyte', 'through', 'an', 'axially', 'symmetric', 'slowly', 'varying', 'nanopore', 'was', 'presented', 'in', 'the', 'li... | [-0.12588979301915404, 0.18750600832940004, -0.03257461619174596, -0.04887361401913561, -0.010438941482418371, -0.13742454065624804, 0.04359592515093645, 0.3488517543029727, -0.19880781601775366, -0.2525042431017619, 0.024038117391382823, -0.2714441222572717, -0.07035339956207978, 0.19211897051676166, -0.05749498682946... |
709.3851 | Asymptotic Safety | Asymptotic safety is a set of conditions, based on the existence of a
nontrivial fixed point for the renormalization group flow, which would make a
quantum field theory consistent up to arbitrarily high energies. After
introducing the basic ideas of this approach, I review the present evidence in
favor of an asymptot... | hep-th | asymptotic safety is a set of conditions based on the existence of a nontrivial fixed point for the renormalization group flow which would make a quantum field theory consistent up to arbitrarily high energies after introducing the basic ideas of this approach i review the present evidence in favor of an asymptotically... | [['asymptotic', 'safety', 'is', 'a', 'set', 'of', 'conditions', 'based', 'on', 'the', 'existence', 'of', 'a', 'nontrivial', 'fixed', 'point', 'for', 'the', 'renormalization', 'group', 'flow', 'which', 'would', 'make', 'a', 'quantum', 'field', 'theory', 'consistent', 'up', 'to', 'arbitrarily', 'high', 'energies', 'after... | [-0.1678122009214913, 0.15541134558137354, -0.18292735414258365, 0.04196243931475128, -0.05043464353115394, -0.14773331096813339, 0.09377669221882162, 0.2952593998855044, -0.1924829553282852, -0.26822196419254457, 0.1067570717824655, -0.22495612675516768, -0.13097245747159267, 0.16128140498466534, -0.06938223684595994,... |
709.3852 | Coherent Communication with Linear Optics | We show how to implement several continuous-variable coherent protocols with
linear optics. Noise can accumulate when implementing each coherent protocol
with realistic optical devices. Our analysis bounds the level of noise
accumulation. We highlight the connection between a coherent channel and a
nonlocal quantum n... | quant-ph | we show how to implement several continuousvariable coherent protocols with linear optics noise can accumulate when implementing each coherent protocol with realistic optical devices our analysis bounds the level of noise accumulation we highlight the connection between a coherent channel and a nonlocal quantum nondemo... | [['we', 'show', 'how', 'to', 'implement', 'several', 'continuousvariable', 'coherent', 'protocols', 'with', 'linear', 'optics', 'noise', 'can', 'accumulate', 'when', 'implementing', 'each', 'coherent', 'protocol', 'with', 'realistic', 'optical', 'devices', 'our', 'analysis', 'bounds', 'the', 'level', 'of', 'noise', 'ac... | [-0.19435841583062785, 0.14669514476258497, -0.14374743369102114, 0.060558713213895776, -0.028837338317840723, -0.31648957828785906, 0.08913150332647107, 0.423585157841444, -0.28624567360285735, -0.2537025074712277, 0.03317099287948114, -0.20772210101328664, -0.17612456433254026, 0.2620142216210143, -0.0685485229981368... |
709.3853 | Thermodynamics of Quasi-Particles | We present in this work a generalization of the solution of Gorenstein and
Yang for a consistent thermodynamics for systems with a temperature dependent
Hamiltonian. We show that there is a large class of solutions, work out three
particular ones, and discuss their physical relevance. We apply the particular
solution... | nucl-th hep-ph | we present in this work a generalization of the solution of gorenstein and yang for a consistent thermodynamics for systems with a temperature dependent hamiltonian we show that there is a large class of solutions work out three particular ones and discuss their physical relevance we apply the particular solutions for ... | [['we', 'present', 'in', 'this', 'work', 'a', 'generalization', 'of', 'the', 'solution', 'of', 'gorenstein', 'and', 'yang', 'for', 'a', 'consistent', 'thermodynamics', 'for', 'systems', 'with', 'a', 'temperature', 'dependent', 'hamiltonian', 'we', 'show', 'that', 'there', 'is', 'a', 'large', 'class', 'of', 'solutions',... | [-0.10507798652873714, 0.05446930139552216, -0.07362118436757362, 0.05087959517329706, -0.029047542590309273, -0.10129549021296429, 0.050394892674927236, 0.3413778602173834, -0.18849265613508495, -0.209981995401904, 0.11336072871750785, -0.308395677330819, -0.1536479578494574, 0.18264639569502888, -0.035474144529099715... |
709.3854 | Arecibo HI Absorption Measurements of Pulsars and the Electron Density
at Intermediate Longitudes in the First Galactic Quadrant | We have used the Arecibo telescope to measure the HI absorption spectra of
eight pulsars. We show how kinematic distance measurements depend upon the
values of the galactic constants R_o and Theta_o, and we select our preferred
current values from the literature. We then derive kinematic distances for the
low-latitud... | astro-ph | we have used the arecibo telescope to measure the hi absorption spectra of eight pulsars we show how kinematic distance measurements depend upon the values of the galactic constants r_o and theta_o and we select our preferred current values from the literature we then derive kinematic distances for the lowlatitude puls... | [['we', 'have', 'used', 'the', 'arecibo', 'telescope', 'to', 'measure', 'the', 'hi', 'absorption', 'spectra', 'of', 'eight', 'pulsars', 'we', 'show', 'how', 'kinematic', 'distance', 'measurements', 'depend', 'upon', 'the', 'values', 'of', 'the', 'galactic', 'constants', 'r_o', 'and', 'theta_o', 'and', 'we', 'select', '... | [-0.09390603455191013, 0.10671445496380329, -0.01699653474432125, 0.05923011681996286, -0.07815299041685649, -0.03911328945425339, 0.08334847345424351, 0.40451766942511314, -0.18210131477564573, -0.3518796602403745, 0.022437341847107745, -0.3363848545355722, 0.0010595052220742217, 0.20701848496450112, 0.037241239448630... |
709.3855 | Non-birational twisted derived equivalences in abelian GLSMs | In this paper we discuss some examples of abelian gauged linear sigma models
realizing twisted derived equivalences between non-birational spaces, and
realizing geometries in novel fashions. Examples of gauged linear sigma models
with non-birational Kahler phases are a relatively new phenomenon. Most of our
examples ... | hep-th | in this paper we discuss some examples of abelian gauged linear sigma models realizing twisted derived equivalences between nonbirational spaces and realizing geometries in novel fashions examples of gauged linear sigma models with nonbirational kahler phases are a relatively new phenomenon most of our examples involve... | [['in', 'this', 'paper', 'we', 'discuss', 'some', 'examples', 'of', 'abelian', 'gauged', 'linear', 'sigma', 'models', 'realizing', 'twisted', 'derived', 'equivalences', 'between', 'nonbirational', 'spaces', 'and', 'realizing', 'geometries', 'in', 'novel', 'fashions', 'examples', 'of', 'gauged', 'linear', 'sigma', 'mode... | [-0.15115827851990662, 0.10421077270337817, -0.02882707728179101, 0.14570310250546523, -0.10640213090949986, -0.2210905940560742, -0.037809937740705575, 0.37694325971953524, -0.23239396289771988, -0.2460744563973497, 0.0860803583894762, -0.2244730889473016, -0.250757621629591, 0.21518925908670017, -0.14473441756577998,... |
709.3856 | On the Lifetime of Quasi-Stationary States in Non-Relativistic QED | We consider resonances in the Pauli-Fierz model of non-relativistic QED. We
use and slightly modify the analysis developed by Bach, Froehlich, and Sigal to
obtain an upper and lower bound on the lifetime of quasi-stationary states.
| math-ph math.MP | we consider resonances in the paulifierz model of nonrelativistic qed we use and slightly modify the analysis developed by bach froehlich and sigal to obtain an upper and lower bound on the lifetime of quasistationary states | [['we', 'consider', 'resonances', 'in', 'the', 'paulifierz', 'model', 'of', 'nonrelativistic', 'qed', 'we', 'use', 'and', 'slightly', 'modify', 'the', 'analysis', 'developed', 'by', 'bach', 'froehlich', 'and', 'sigal', 'to', 'obtain', 'an', 'upper', 'and', 'lower', 'bound', 'on', 'the', 'lifetime', 'of', 'quasistationa... | [-0.0902571188699868, 0.1482600879555523, -0.07399627782352683, 0.10550977382808924, -3.800396290090349e-05, -0.13898795610293746, 0.06990748047569974, 0.2627698647427476, -0.11077870542390479, -0.3211579947383143, 0.02993713948914471, -0.26287052154334056, -0.08291957661923435, 0.15835007609307972, -0.0177741277342041... |
709.3857 | Confining solutions of $(n+1)$-dimensional Yang-Mills equations for flat
and curved space-time with $n \le 3$ | We obtain exact static solutions of the $(n+1)$-dimensional SU(3) Yang-Mills
equations for both flat and curved space-time cases with $n \le 3$. We find
that the solutions obtained are confining functions for $n = 1, 2, 3$. We apply
the $(3+1)$ curved space-time solution to the anti-de Sitter and Schwarzschild
metric... | hep-th | we obtain exact static solutions of the n1dimensional su3 yangmills equations for both flat and curved spacetime cases with n le 3 we find that the solutions obtained are confining functions for n 1 2 3 we apply the 31 curved spacetime solution to the antide sitter and schwarzschild metrics | [['we', 'obtain', 'exact', 'static', 'solutions', 'of', 'the', 'n1dimensional', 'su3', 'yangmills', 'equations', 'for', 'both', 'flat', 'and', 'curved', 'spacetime', 'cases', 'with', 'n', 'le', '3', 'we', 'find', 'that', 'the', 'solutions', 'obtained', 'are', 'confining', 'functions', 'for', 'n', '1', '2', '3', 'we', '... | [-0.14152730584144593, 0.12203880006447435, -0.04493573161307722, 0.12871973419561983, -0.03746605347841978, -0.20515847589820624, -0.08704957131296397, 0.3565333754569292, -0.06977001662366092, -0.25539334943285213, 0.11676109435968102, -0.329453800059855, -0.1430189135670662, 0.08314909664914012, -0.01783335020765662... |
709.3858 | Noise limits in the assembly of diffraction data | We obtain an information theoretic criterion for the feasibility of
assembling diffraction signals from noisy tomographs when the positions of the
tomographs within the signal are unknown. For shot-noise limited data, the
minimum number of detected photons per tomograph for successful assembly is
much smaller than pr... | physics.comp-ph | we obtain an information theoretic criterion for the feasibility of assembling diffraction signals from noisy tomographs when the positions of the tomographs within the signal are unknown for shotnoise limited data the minimum number of detected photons per tomograph for successful assembly is much smaller than previou... | [['we', 'obtain', 'an', 'information', 'theoretic', 'criterion', 'for', 'the', 'feasibility', 'of', 'assembling', 'diffraction', 'signals', 'from', 'noisy', 'tomographs', 'when', 'the', 'positions', 'of', 'the', 'tomographs', 'within', 'the', 'signal', 'are', 'unknown', 'for', 'shotnoise', 'limited', 'data', 'the', 'mi... | [-0.083362448776729, 0.12257977458667531, -0.042705801793521174, 0.07250688288446613, -0.07436070125550032, -0.1232353200535535, 0.05643322998596551, 0.3633865422418335, -0.2643712529312133, -0.39989144971447166, 0.11248053227992434, -0.29053913323992964, -0.08495687450417072, 0.22019901207501166, -0.05644210904383248,... |
709.3859 | Remarks on the waterbag model of dispersionless Toda Hierarchy | We construct the free energy associated with the waterbag model of dToda.
Also, the relations of conserved densities are investigated
| nlin.SI | we construct the free energy associated with the waterbag model of dtoda also the relations of conserved densities are investigated | [['we', 'construct', 'the', 'free', 'energy', 'associated', 'with', 'the', 'waterbag', 'model', 'of', 'dtoda', 'also', 'the', 'relations', 'of', 'conserved', 'densities', 'are', 'investigated']] | [-0.15258324090391398, 0.20596469365991651, -0.038099144399166104, 0.1466975338757038, 0.028896075440570712, -0.08483816720545292, -0.05859743824694306, 0.35146385356783866, -0.2401312982663512, -0.28964524720795454, 0.04332741864491254, -0.2821838902309537, -0.07963673789054156, 0.13982409703312443, 0.0407753698062151... |
709.386 | Estimating copula measure using ranks and subsampling: a simulation
study | We describe here a new method to estimate copula measure. From N observations
of two variables X and Y, we draw a huge number m of subsamples (size n<N), and
we compute the joint ranks in these subsamples. Then, for each bivariate rank
(p,q) (0<p,q<n+1), we count the number of subsamples such that there exist an
obse... | stat.ME | we describe here a new method to estimate copula measure from n observations of two variables x and y we draw a huge number m of subsamples size nn and we compute the joint ranks in these subsamples then for each bivariate rank pq 0pqn1 we count the number of subsamples such that there exist an observation of the subsa... | [['we', 'describe', 'here', 'a', 'new', 'method', 'to', 'estimate', 'copula', 'measure', 'from', 'n', 'observations', 'of', 'two', 'variables', 'x', 'and', 'y', 'we', 'draw', 'a', 'huge', 'number', 'm', 'of', 'subsamples', 'size', 'nn', 'and', 'we', 'compute', 'the', 'joint', 'ranks', 'in', 'these', 'subsamples', 'then... | [-0.07411933641718782, 0.04134332201215, -0.12261764795613894, 0.08528586820382085, -0.0883290013163418, -0.10915760175945859, 0.08339383842194102, 0.41959047862800997, -0.23677317776710496, -0.3081578167249867, 0.048578785473406584, -0.2678007090707188, -0.11046559685770341, 0.15455703388653236, -0.0873638877267207, 0... |
709.3861 | Amplification of High Harmonics Using Weak Perturbative High Frequency
Radiation | The mechanism underlying the substantial amplification of the high-order
harmonics q \pm 2K (K integer) upon the addition of a weak seed XUV field of
harmonic frequency q\omega to a strong IR field of frequency \omega is analyzed
in the framework of the quantum-mechanical Floquet formalism and the
semiclassical re-co... | physics.atom-ph | the mechanism underlying the substantial amplification of the highorder harmonics q pm 2k k integer upon the addition of a weak seed xuv field of harmonic frequency qomega to a strong ir field of frequency omega is analyzed in the framework of the quantummechanical floquet formalism and the semiclassical recollision mo... | [['the', 'mechanism', 'underlying', 'the', 'substantial', 'amplification', 'of', 'the', 'highorder', 'harmonics', 'q', 'pm', '2k', 'k', 'integer', 'upon', 'the', 'addition', 'of', 'a', 'weak', 'seed', 'xuv', 'field', 'of', 'harmonic', 'frequency', 'qomega', 'to', 'a', 'strong', 'ir', 'field', 'of', 'frequency', 'omega'... | [-0.20470348235662325, 0.18778425941732482, -0.07769600206864485, 0.048436773324265416, -0.02990105517651185, -0.06834144828297051, 0.07446361015583065, 0.34920352439184, -0.24773579912426152, -0.2600607917653305, -0.03841165992740247, -0.2439902239101063, -0.12476266945924351, 0.1704729355878593, 0.037951322345035426,... |
709.3862 | Current-Induced Torques in Magnetic Metals: Beyond Spin Transfer | Current-induced torques on ferromagnetic nanoparticles and on domain walls in
ferromagnetic nanowires are normally understood in terms of transfer of
conserved spin angular momentum between spin-polarized currents and the
magnetic condensate. In a series of recent articles we have discussed a
microscopic picture of c... | cond-mat.mes-hall | currentinduced torques on ferromagnetic nanoparticles and on domain walls in ferromagnetic nanowires are normally understood in terms of transfer of conserved spin angular momentum between spinpolarized currents and the magnetic condensate in a series of recent articles we have discussed a microscopic picture of curren... | [['currentinduced', 'torques', 'on', 'ferromagnetic', 'nanoparticles', 'and', 'on', 'domain', 'walls', 'in', 'ferromagnetic', 'nanowires', 'are', 'normally', 'understood', 'in', 'terms', 'of', 'transfer', 'of', 'conserved', 'spin', 'angular', 'momentum', 'between', 'spinpolarized', 'currents', 'and', 'the', 'magnetic',... | [-0.18155806479278827, 0.1906819369813554, -0.04106482488812128, 0.06421036243442196, -0.10358045233496979, -0.07414988600718442, 0.029946810713579963, 0.42519656179556203, -0.25231623466612263, -0.2866029914107118, 0.02374890872186967, -0.28069344714784356, -0.1281530326232314, 0.20836049702961984, -0.0282644028080377... |
709.3863 | Exact and Perturbed Friedmann-Lemaitre Cosmologies | In this thesis we first apply the 1+3 covariant description of general
relativity to analyze n-fluid Friedmann-Lemaitre (FL) cosmologies; that is,
homogeneous and isotropic cosmologies whose matter-energy content consists of n
non-interacting fluids. We are motivated to study FL models of this type as
observations su... | gr-qc | in this thesis we first apply the 13 covariant description of general relativity to analyze nfluid friedmannlemaitre fl cosmologies that is homogeneous and isotropic cosmologies whose matterenergy content consists of n noninteracting fluids we are motivated to study fl models of this type as observations suggest the ph... | [['in', 'this', 'thesis', 'we', 'first', 'apply', 'the', '13', 'covariant', 'description', 'of', 'general', 'relativity', 'to', 'analyze', 'nfluid', 'friedmannlemaitre', 'fl', 'cosmologies', 'that', 'is', 'homogeneous', 'and', 'isotropic', 'cosmologies', 'whose', 'matterenergy', 'content', 'consists', 'of', 'n', 'nonin... | [-0.1558553274558938, 0.12941476692971976, -0.10531466637381211, 0.06972698376554509, -0.1062043239099338, -0.13661799449068696, -0.05425403533078244, 0.2961421711410841, -0.1836008272457706, -0.2835831684951225, 0.05212170872533613, -0.26866625418643586, -0.10998075315121399, 0.10333344820562912, -0.009077999173947002... |
709.3864 | A lower bound on the subriemannian distance for H\"older distributions | Whereas subriemannian geometry usually deals with smooth horizontal
distributions, partially hyperbolic dynamical systems provide many examples of
subriemannian geometries defined by non-smooth (namely, H\"older continuous)
distributions. These distributions are of great significance for the behavior
of the parent dy... | math.MG math.DG | whereas subriemannian geometry usually deals with smooth horizontal distributions partially hyperbolic dynamical systems provide many examples of subriemannian geometries defined by nonsmooth namely holder continuous distributions these distributions are of great significance for the behavior of the parent dynamical sy... | [['whereas', 'subriemannian', 'geometry', 'usually', 'deals', 'with', 'smooth', 'horizontal', 'distributions', 'partially', 'hyperbolic', 'dynamical', 'systems', 'provide', 'many', 'examples', 'of', 'subriemannian', 'geometries', 'defined', 'by', 'nonsmooth', 'namely', 'holder', 'continuous', 'distributions', 'these', ... | [-0.14799976759035177, 0.07097081602974371, -0.09368873880517603, 0.13051736967713393, -0.10074165125725547, -0.1790733530369559, -0.046236122538561394, 0.36440547834141085, -0.31390186914271023, -0.20243647673421286, 0.09651360802371244, -0.2644230830247956, -0.14547203528939398, 0.2421952181241729, -0.136960777106008... |
709.3865 | Symmetry-Induced Tunnelling in One-Dimensional Disordered Potentials | A new mechanism of tunnelling at macroscopic distances is proposed for a wave
packet localized in one-dimensional disordered potential with mirror symmetry,
V(-x)=V(x). Unlike quantum tunnelling through a regular potential barrier,
which occurs only at the energies lower then the barrier height, the proposed
mechanis... | cond-mat.dis-nn | a new mechanism of tunnelling at macroscopic distances is proposed for a wave packet localized in onedimensional disordered potential with mirror symmetry vxvx unlike quantum tunnelling through a regular potential barrier which occurs only at the energies lower then the barrier height the proposed mechanism of tunnelli... | [['a', 'new', 'mechanism', 'of', 'tunnelling', 'at', 'macroscopic', 'distances', 'is', 'proposed', 'for', 'a', 'wave', 'packet', 'localized', 'in', 'onedimensional', 'disordered', 'potential', 'with', 'mirror', 'symmetry', 'vxvx', 'unlike', 'quantum', 'tunnelling', 'through', 'a', 'regular', 'potential', 'barrier', 'wh... | [-0.19077511947188114, 0.16392336997927892, -0.07363028444039325, 0.07922493820208021, -0.040863532345328066, -0.26314843214220474, 0.09987534229488422, 0.3667398349278503, -0.2918148400210258, -0.23477645236998795, 0.022710872034076603, -0.2465555084714045, -0.1667333509773016, 0.21058816419293483, 0.00459585995930764... |
709.3866 | Search for a Solution of the Pioneer Anomaly | In 1972 and 1973 the Pioneer 10 and 11 missions were launched. They were the
first to explore the outer solar system and achieved stunning breakthroughs in
deep-space exploration. But beginning in about 1980 an unmodeled force of \sim
8 \times 10^{-8} cm/s^2, directed approximately towards the Sun, appeared in
the tr... | gr-qc | in 1972 and 1973 the pioneer 10 and 11 missions were launched they were the first to explore the outer solar system and achieved stunning breakthroughs in deepspace exploration but beginning in about 1980 an unmodeled force of sim 8 times 108 cms2 directed approximately towards the sun appeared in the tracking data it ... | [['in', '1972', 'and', '1973', 'the', 'pioneer', '10', 'and', '11', 'missions', 'were', 'launched', 'they', 'were', 'the', 'first', 'to', 'explore', 'the', 'outer', 'solar', 'system', 'and', 'achieved', 'stunning', 'breakthroughs', 'in', 'deepspace', 'exploration', 'but', 'beginning', 'in', 'about', '1980', 'an', 'unmo... | [-0.10621269553666934, 0.13691696032221323, -0.05672284557658713, 0.07236994586549873, -0.07738391449239766, -0.09051732113584876, 0.04251289994360131, 0.36563459538558724, -0.22483432038347714, -0.41177584941142076, 0.18076074795218655, -0.28381765659498137, -0.12332064657533001, 0.2073221052518097, -0.118843425317098... |
709.3867 | Rapid-purification protocols for optical homodyning | We present a number of rapid-purification feedback protocols for optical
homodyne detection of a single optical qubit. We derive first a protocol that
speeds up the rate of increase of the average purity of the system, and find
that like the equivalent protocol for a non-disspative measurement, this
generates a deter... | quant-ph | we present a number of rapidpurification feedback protocols for optical homodyne detection of a single optical qubit we derive first a protocol that speeds up the rate of increase of the average purity of the system and find that like the equivalent protocol for a nondisspative measurement this generates a deterministi... | [['we', 'present', 'a', 'number', 'of', 'rapidpurification', 'feedback', 'protocols', 'for', 'optical', 'homodyne', 'detection', 'of', 'a', 'single', 'optical', 'qubit', 'we', 'derive', 'first', 'a', 'protocol', 'that', 'speeds', 'up', 'the', 'rate', 'of', 'increase', 'of', 'the', 'average', 'purity', 'of', 'the', 'sys... | [-0.16209199748878778, 0.09273312180127366, -0.0683284044551017, 0.01690455528420841, 0.05099713901133352, -0.159819735180553, 0.12780427430999708, 0.39252098243650013, -0.23756306045185271, -0.3015168742360631, 0.096950664669527, -0.22073922921071742, -0.10256002910502322, 0.25039501545472526, -0.05414074972515238, 0.... |
709.3868 | Observations of the Crab Nebula and Pulsar with VERITAS | Observations of the Crab Nebula have proven to be the best tool to calibrate
and to characterize the performance of a Cherenkov telescope. Scientifically,
it is interesting to measure the energy spectrum of the Crab Nebula close to
the inverse-Compton peak where a deviation is expected from the power law seen
at ener... | astro-ph | observations of the crab nebula have proven to be the best tool to calibrate and to characterize the performance of a cherenkov telescope scientifically it is interesting to measure the energy spectrum of the crab nebula close to the inversecompton peak where a deviation is expected from the power law seen at energies ... | [['observations', 'of', 'the', 'crab', 'nebula', 'have', 'proven', 'to', 'be', 'the', 'best', 'tool', 'to', 'calibrate', 'and', 'to', 'characterize', 'the', 'performance', 'of', 'a', 'cherenkov', 'telescope', 'scientifically', 'it', 'is', 'interesting', 'to', 'measure', 'the', 'energy', 'spectrum', 'of', 'the', 'crab',... | [-0.014003449466806896, 0.12595133047825421, -0.06580929901070628, 0.14978496283196333, -0.07376393150901918, -0.09020392558146158, 0.064527163276526, 0.4275689035786327, -0.23127939490072386, -0.41479727100118025, 0.06485604284022599, -0.31260034609200243, 0.022650710422788146, 0.28813334784646844, 0.00842159973270089... |
709.3869 | Results from the Blazar Monitoring Campaign at the Whipple 10m Gamma-ray
Telescope | In September 2005, the observing program of the Whipple 10 m gamma-ray
telescope was redefined to be dedicated almost exclusively to AGN monitoring.
Since then the five Northern Hemisphere blazars that had already been detected
at Whipple are monitored routinely each night that they are visible. Thanks to
the efforts... | astro-ph | in september 2005 the observing program of the whipple 10 m gammaray telescope was redefined to be dedicated almost exclusively to agn monitoring since then the five northern hemisphere blazars that had already been detected at whipple are monitored routinely each night that they are visible thanks to the efforts of a ... | [['in', 'september', '2005', 'the', 'observing', 'program', 'of', 'the', 'whipple', '10', 'm', 'gammaray', 'telescope', 'was', 'redefined', 'to', 'be', 'dedicated', 'almost', 'exclusively', 'to', 'agn', 'monitoring', 'since', 'then', 'the', 'five', 'northern', 'hemisphere', 'blazars', 'that', 'had', 'already', 'been', ... | [-0.051205342983492934, 0.12583066589887376, -0.09522373607361932, 0.07079832902071877, -0.14601823361590505, -0.09178475219169227, 0.04415047214285511, 0.46692787774879, -0.13045109245728742, -0.44217439986886864, 0.18428312683903167, -0.3201469029552992, -0.05280482989695409, 0.23678872300787707, -0.0545887278403034,... |
709.387 | Two-mode variational Monte Carlo study of Quasiparticle excitations in
cuprates | Recent measurements of quasiparticles in hole-doped cuprates reveal highly
unusual features: 1) the doping-independent Fermi velocity, 2) two energy
scales in the quasiparticle spectral function, and 3) a suppression of the low
energy spectral weight near the zone center. The underlying mechanism is under
hot debate.... | cond-mat.supr-con cond-mat.str-el | recent measurements of quasiparticles in holedoped cuprates reveal highly unusual features 1 the dopingindependent fermi velocity 2 two energy scales in the quasiparticle spectral function and 3 a suppression of the low energy spectral weight near the zone center the underlying mechanism is under hot debate we addresse... | [['recent', 'measurements', 'of', 'quasiparticles', 'in', 'holedoped', 'cuprates', 'reveal', 'highly', 'unusual', 'features', '1', 'the', 'dopingindependent', 'fermi', 'velocity', '2', 'two', 'energy', 'scales', 'in', 'the', 'quasiparticle', 'spectral', 'function', 'and', '3', 'a', 'suppression', 'of', 'the', 'low', 'e... | [-0.13853019945022157, 0.16203118538867464, -0.07361445673650094, 0.14208185532719225, -0.03430755979920208, -0.1366192712813762, 0.10573423431054049, 0.395882395360911, -0.24810470960230804, -0.2899679451925205, 0.016042154250374318, -0.31513556859949055, -0.10482385473362371, 0.15869314068821075, 0.004232888055198333... |
709.3871 | Signatures of the Baryon Acoustic Oscillations on 21cm Emission
Background | The baryon acoustic oscillations (BAO) prior to recombination should be
imprinted onto the 21cm emission background from the epoch of reionization
through the underlying density perturbations. Using an analytical approach for
both matter power spectrum (CDM+baryons) and reionization process, we
demonstrate the BAO in... | astro-ph | the baryon acoustic oscillations bao prior to recombination should be imprinted onto the 21cm emission background from the epoch of reionization through the underlying density perturbations using an analytical approach for both matter power spectrum cdmbaryons and reionization process we demonstrate the bao induced sig... | [['the', 'baryon', 'acoustic', 'oscillations', 'bao', 'prior', 'to', 'recombination', 'should', 'be', 'imprinted', 'onto', 'the', '21cm', 'emission', 'background', 'from', 'the', 'epoch', 'of', 'reionization', 'through', 'the', 'underlying', 'density', 'perturbations', 'using', 'an', 'analytical', 'approach', 'for', 'b... | [-0.07267425654376779, 0.11601428653357136, -0.06550430277158983, 0.08560881092848793, -0.15172204902755612, -0.06710702652784706, -0.018560601605744173, 0.3750238384143645, -0.23243124276681357, -0.287948658607681, 0.07334074072007622, -0.3249560771118693, -0.020486540716736258, 0.21797476665062063, 0.1045208849764170... |
709.3872 | The Sydney University Stellar Interferometer: A Major Upgrade to
Spectral Coverage and Performance | A new beam-combination and detection system has been installed in the Sydney
University Stellar Interferometer working at the red end of the visual spectrum
(wavelength range 500-950 nm) to complement the existing blue-sensitive system
(wavelength range 430-520 nm) and to provide an increase in sensitivity.
Dichroic ... | astro-ph | a new beamcombination and detection system has been installed in the sydney university stellar interferometer working at the red end of the visual spectrum wavelength range 500950 nm to complement the existing bluesensitive system wavelength range 430520 nm and to provide an increase in sensitivity dichroic beamsplitte... | [['a', 'new', 'beamcombination', 'and', 'detection', 'system', 'has', 'been', 'installed', 'in', 'the', 'sydney', 'university', 'stellar', 'interferometer', 'working', 'at', 'the', 'red', 'end', 'of', 'the', 'visual', 'spectrum', 'wavelength', 'range', '500950', 'nm', 'to', 'complement', 'the', 'existing', 'bluesensiti... | [-0.09960860011666278, 0.07104863151174176, -0.06564535455069911, -0.07611155196037275, -0.07509627079092701, -0.15831518534269237, -0.002128020092897432, 0.4482827163006271, -0.15432552035412633, -0.3864330661246999, 0.12454308490809972, -0.25695711262622506, -0.010424304779776385, 0.23850053963316997, -0.077914341497... |
709.3873 | The Emergent Flux and Effective Temperature of Delta Canis Majoris | New angular diameter determinations for the bright southern F8 supergiant
Delta CMa enable the bolometric emergent flux and effective temperature of the
star to be determined with improved accuracy. The spectral flux distribution
and bolometric flux have been determined from published photometry and
spectrophotometry... | astro-ph | new angular diameter determinations for the bright southern f8 supergiant delta cma enable the bolometric emergent flux and effective temperature of the star to be determined with improved accuracy the spectral flux distribution and bolometric flux have been determined from published photometry and spectrophotometry an... | [['new', 'angular', 'diameter', 'determinations', 'for', 'the', 'bright', 'southern', 'f8', 'supergiant', 'delta', 'cma', 'enable', 'the', 'bolometric', 'emergent', 'flux', 'and', 'effective', 'temperature', 'of', 'the', 'star', 'to', 'be', 'determined', 'with', 'improved', 'accuracy', 'the', 'spectral', 'flux', 'distr... | [-0.03607030877876177, 0.15083756496754, -0.04246769208673453, 0.052565638707101084, -0.0830056885943601, -0.0848457809831751, 0.08397601172327995, 0.4098042808595653, -0.11797509969440861, -0.45398435685293453, 0.06500396078346264, -0.3156823395146874, 0.06162766559997149, 0.21698328196642952, -0.08233758205090437, 0.... |
709.3874 | Open-closed moduli spaces and related algebraic structures | We set up a Batalin-Vilkovisky Quantum Master Equation for open-closed string
theory and show that the corresponding moduli spaces give rise to a solution, a
generating function for their fundamental chains. The equation encodes the
topological structure of the compactification of the moduli space of bordered
Riemann... | math.QA math.AG | we set up a batalinvilkovisky quantum master equation for openclosed string theory and show that the corresponding moduli spaces give rise to a solution a generating function for their fundamental chains the equation encodes the topological structure of the compactification of the moduli space of bordered riemann surfa... | [['we', 'set', 'up', 'a', 'batalinvilkovisky', 'quantum', 'master', 'equation', 'for', 'openclosed', 'string', 'theory', 'and', 'show', 'that', 'the', 'corresponding', 'moduli', 'spaces', 'give', 'rise', 'to', 'a', 'solution', 'a', 'generating', 'function', 'for', 'their', 'fundamental', 'chains', 'the', 'equation', 'e... | [-0.17045835274479632, 0.10784289950066364, -0.13361921881605843, 0.1447775098212624, -0.12020324643936406, -0.08656530660459573, 0.01560730389115916, 0.29248465483700764, -0.3564863631736885, -0.2193671275649075, 0.06456460315028875, -0.24282701593796605, -0.22058958994723105, 0.17193244120956047, -0.10967996908189023... |
709.3875 | Error correction optimisation in the presence of X/Z asymmetry | By taking into account the physical nature of quantum errors it is possible
to improve the efficiency of quantum error correction. Here we consider an
optimisation to conventional quantum error correction which involves exploiting
asymmetries in the rates of X and Z errors by reducing the rate of X
correction. As an ... | quant-ph | by taking into account the physical nature of quantum errors it is possible to improve the efficiency of quantum error correction here we consider an optimisation to conventional quantum error correction which involves exploiting asymmetries in the rates of x and z errors by reducing the rate of x correction as an exam... | [['by', 'taking', 'into', 'account', 'the', 'physical', 'nature', 'of', 'quantum', 'errors', 'it', 'is', 'possible', 'to', 'improve', 'the', 'efficiency', 'of', 'quantum', 'error', 'correction', 'here', 'we', 'consider', 'an', 'optimisation', 'to', 'conventional', 'quantum', 'error', 'correction', 'which', 'involves', ... | [-0.11850504755531832, 0.04347815365610463, -0.04389309218169143, 0.0740217272097529, 0.016781803220510483, -0.16925426800656368, 0.115307082832491, 0.3447035373488473, -0.25712119966007424, -0.34929273779882847, 0.11718466231536309, -0.24279461123870086, -0.10370142386152835, 0.22046121188155296, -0.11255355084204446,... |
709.3876 | Features of the Acoustic Mechanism of Core-Collapse Supernova Explosions
: Revisited using the Kinetic Approach | The discrete kinetic model is used to study the propagation of sound waves in
system of hard-disk-like rotating stars (or vortex gases). The anomalous
(negative) attenuation or amplification which is possibly due to the binary
collision of a dilute-enough rotating disk (or vortex-gas) system (each with
opposite-sign ... | astro-ph | the discrete kinetic model is used to study the propagation of sound waves in system of harddisklike rotating stars or vortex gases the anomalous negative attenuation or amplification which is possibly due to the binary collision of a diluteenough rotating disk or vortexgas system each with oppositesign rotating direct... | [['the', 'discrete', 'kinetic', 'model', 'is', 'used', 'to', 'study', 'the', 'propagation', 'of', 'sound', 'waves', 'in', 'system', 'of', 'harddisklike', 'rotating', 'stars', 'or', 'vortex', 'gases', 'the', 'anomalous', 'negative', 'attenuation', 'or', 'amplification', 'which', 'is', 'possibly', 'due', 'to', 'the', 'bi... | [-0.1918974614885743, 0.20027908655510357, -0.06570405305291598, 0.09655824145346951, -0.1243926134864943, -0.09432053093601447, -0.014921737216914503, 0.3208334794214282, -0.30150045271819603, -0.3144623213626731, 0.03739632279141985, -0.2701448846581535, -0.008731058481386684, 0.17375268920575485, 0.02566606307832094... |
709.3877 | The Cosmic MeV Gamma-ray Background and Hard X-ray Spectra of Active
Galactic Nuclei: Implications for the Origin of Hot AGN Coronae | The origin of the extragalactic gamma-ray background radiation at 1-10 MeV is
still unknown. Although the cosmic X-ray background (CXB) up to a few hundreds
keV can be accounted for by the sum of Active Galactic Nuclei (AGNs), current
models of AGN spectra cannot explain the background spectrum beyond ~1 MeV,
because... | astro-ph | the origin of the extragalactic gammaray background radiation at 110 mev is still unknown although the cosmic xray background cxb up to a few hundreds kev can be accounted for by the sum of active galactic nuclei agns current models of agn spectra cannot explain the background spectrum beyond 1 mev because of the therm... | [['the', 'origin', 'of', 'the', 'extragalactic', 'gammaray', 'background', 'radiation', 'at', '110', 'mev', 'is', 'still', 'unknown', 'although', 'the', 'cosmic', 'xray', 'background', 'cxb', 'up', 'to', 'a', 'few', 'hundreds', 'kev', 'can', 'be', 'accounted', 'for', 'by', 'the', 'sum', 'of', 'active', 'galactic', 'nuc... | [-0.044114453492816105, 0.24050018000585666, -0.03476722233300639, 0.1610602045927598, -0.057521010791411795, -0.08314151762399909, 0.030279771966296574, 0.4262598870798599, -0.21164217426246681, -0.3775270468815295, 0.024687228072434664, -0.3273178882463727, 0.024027658327547618, 0.22075610145125105, 0.017535072138403... |
709.3878 | The Keck Aperture Masking Experiment: Multi-Wavelength Observations of 6
Mira Variables | The angular diameters of six oxygen rich Mira-type long-period variables have
been measured at various near-infrared (NIR) wavelengths using the aperture
masking technique in an extensive observing program from 1997 Jan to 2004 Sep.
These data sets span many pulsation cycles of the observed objects and
represent the ... | astro-ph | the angular diameters of six oxygen rich miratype longperiod variables have been measured at various nearinfrared nir wavelengths using the aperture masking technique in an extensive observing program from 1997 jan to 2004 sep these data sets span many pulsation cycles of the observed objects and represent the largest ... | [['the', 'angular', 'diameters', 'of', 'six', 'oxygen', 'rich', 'miratype', 'longperiod', 'variables', 'have', 'been', 'measured', 'at', 'various', 'nearinfrared', 'nir', 'wavelengths', 'using', 'the', 'aperture', 'masking', 'technique', 'in', 'an', 'extensive', 'observing', 'program', 'from', '1997', 'jan', 'to', '200... | [-0.06396777419494425, 0.10999966221857695, -0.07566274545824213, 0.03700276625051372, -0.05586716554246613, -0.10621168279798808, 0.0449542995698192, 0.44946943871709744, -0.22789481292285912, -0.370422328511532, 0.06233291178972497, -0.2941202487680386, -0.05668602140398803, 0.1836664911517504, -0.06562031587864793, ... |
709.3879 | S-integral preperiodic points for dynamical systems over number fields | Given a rational map $\phi: {\mathbb P}^1\to {\mathbb P}^1$ defined over a
number field $K$, we prove a finiteness result for $\phi$-preperiodic points
which are $S$-integral with respect to a non-preperiodic point $P$, provided
$P$ satisfies a certain local condition at each place. This verifies a special
case of a ... | math.NT math.DS | given a rational map phi mathbb p1to mathbb p1 defined over a number field k we prove a finiteness result for phipreperiodic points which are sintegral with respect to a nonpreperiodic point p provided p satisfies a certain local condition at each place this verifies a special case of a conjecture of s ih | [['given', 'a', 'rational', 'map', 'phi', 'mathbb', 'p1to', 'mathbb', 'p1', 'defined', 'over', 'a', 'number', 'field', 'k', 'we', 'prove', 'a', 'finiteness', 'result', 'for', 'phipreperiodic', 'points', 'which', 'are', 'sintegral', 'with', 'respect', 'to', 'a', 'nonpreperiodic', 'point', 'p', 'provided', 'p', 'satisfie... | [-0.27712223640168615, 0.042311551576515415, -0.10025542391956134, -0.0023022788633891155, -0.021373997249130933, -0.20890448025410185, 0.06476578376484367, 0.25418249044549773, -0.30335683628635585, -0.1753626513560654, 0.044315841040169855, -0.27388151959990553, -0.07647121782010456, 0.1880557644532396, -0.0877152937... |
709.388 | A New Perspective on Multi-user Power Control Games in Interference
Channels | This paper considers the problem of how to allocate power among competing
users sharing a frequency-selective interference channel. We model the
interaction between selfish users as a non-cooperative game. As opposed to the
existing iterative water-filling algorithm that studies the myopic users, this
paper studies h... | cs.GT | this paper considers the problem of how to allocate power among competing users sharing a frequencyselective interference channel we model the interaction between selfish users as a noncooperative game as opposed to the existing iterative waterfilling algorithm that studies the myopic users this paper studies how a for... | [['this', 'paper', 'considers', 'the', 'problem', 'of', 'how', 'to', 'allocate', 'power', 'among', 'competing', 'users', 'sharing', 'a', 'frequencyselective', 'interference', 'channel', 'we', 'model', 'the', 'interaction', 'between', 'selfish', 'users', 'as', 'a', 'noncooperative', 'game', 'as', 'opposed', 'to', 'the',... | [-0.15605680068556374, -0.03370459834545774, -0.11461188978534768, 0.09791347182766275, -0.14827603440894985, -0.26233545228954136, 0.13519403316289397, 0.4078795967825218, -0.2977745838405699, -0.29018493571388293, 0.07172748197071716, -0.26803280455463857, -0.23070138436502097, 0.07294433704966237, -0.124876588357362... |
709.3881 | Logarithmic vector fields and hyperbolicity | In this article we prove that the complement of a very generic curve of
degree at least equal to 14 in the complex projective plane is hyperbolic in
the sense of Kobayashi. Thus, using a new method, we improve the former known
bound obtained by El Goul. We also improve the case of a very generic curve
with two compon... | math.AG math.CV | in this article we prove that the complement of a very generic curve of degree at least equal to 14 in the complex projective plane is hyperbolic in the sense of kobayashi thus using a new method we improve the former known bound obtained by el goul we also improve the case of a very generic curve with two components | [['in', 'this', 'article', 'we', 'prove', 'that', 'the', 'complement', 'of', 'a', 'very', 'generic', 'curve', 'of', 'degree', 'at', 'least', 'equal', 'to', '14', 'in', 'the', 'complex', 'projective', 'plane', 'is', 'hyperbolic', 'in', 'the', 'sense', 'of', 'kobayashi', 'thus', 'using', 'a', 'new', 'method', 'we', 'impr... | [-0.14014261133842548, 0.04468135982436144, -0.11382809536673634, 0.04404579643633658, -0.0670726353428879, -0.14394262536444655, 0.05223415776203245, 0.30355330048349954, -0.24099162656624437, -0.2624929500270193, 0.095490838868654, -0.2387437197395553, -0.20149952013803235, 0.26555151871200333, -0.11404539112759343, ... |
709.3882 | Hyperbolicit\'e des vari\'et\'es complexes | These notes were written for the Cours Peccot given at the Coll\`ege de
France in 2007.
| math.AG math.CV | these notes were written for the cours peccot given at the college de france in 2007 | [['these', 'notes', 'were', 'written', 'for', 'the', 'cours', 'peccot', 'given', 'at', 'the', 'college', 'de', 'france', 'in', '2007']] | [-0.013608715807398161, 0.07345604511598745, -0.13224138484025996, 0.07272821801404158, -0.08239277526736259, -0.07695871175577243, -0.08231404436131319, 0.23377800310651461, -0.08375463883082072, -0.42430815398693084, 0.18923754669570675, -0.34646858473618825, -0.09351666520039241, 0.19842924525340397, -0.174933609614... |
709.3883 | Non-linear rheology of layered systems - a phase model approach | We study non-linear rheology of a simple theoretical model developed to mimic
layered systems such as lamellar structures under shear. In the present work we
study a 2-dimensional version of the model which exhibits a Kosterlitz-Thouless
transition in equilibrium at a critical temperature Tc. While the system
behaves... | cond-mat.stat-mech cond-mat.soft | we study nonlinear rheology of a simple theoretical model developed to mimic layered systems such as lamellar structures under shear in the present work we study a 2dimensional version of the model which exhibits a kosterlitzthouless transition in equilibrium at a critical temperature tc while the system behaves as new... | [['we', 'study', 'nonlinear', 'rheology', 'of', 'a', 'simple', 'theoretical', 'model', 'developed', 'to', 'mimic', 'layered', 'systems', 'such', 'as', 'lamellar', 'structures', 'under', 'shear', 'in', 'the', 'present', 'work', 'we', 'study', 'a', '2dimensional', 'version', 'of', 'the', 'model', 'which', 'exhibits', 'a'... | [-0.16279968826869584, 0.20422497738922096, -0.11008103578047745, -0.014101445488884801, -0.024954481063025963, -0.17416847770547736, 0.05564806133043021, 0.3407551536700972, -0.28498288658153365, -0.24665524994349614, 0.035456239726677864, -0.2849061996878489, -0.17468558714482124, 0.1411841950428662, -0.0063058426477... |
709.3884 | Flexible least squares for temporal data mining and statistical
arbitrage | A number of recent emerging applications call for studying data streams,
potentially infinite flows of information updated in real-time. When multiple
co-evolving data streams are observed, an important task is to determine how
these streams depend on each other, accounting for dynamic dependence patterns
without imp... | q-fin.ST stat.AP stat.ME | a number of recent emerging applications call for studying data streams potentially infinite flows of information updated in realtime when multiple coevolving data streams are observed an important task is to determine how these streams depend on each other accounting for dynamic dependence patterns without imposing an... | [['a', 'number', 'of', 'recent', 'emerging', 'applications', 'call', 'for', 'studying', 'data', 'streams', 'potentially', 'infinite', 'flows', 'of', 'information', 'updated', 'in', 'realtime', 'when', 'multiple', 'coevolving', 'data', 'streams', 'are', 'observed', 'an', 'important', 'task', 'is', 'to', 'determine', 'ho... | [-0.1143175581151357, 0.04707633696934802, -0.1303246823708283, 0.12236485942524714, -0.14385644930271094, -0.17618702429240482, 0.029994846478685888, 0.396458896908334, -0.2945117661760707, -0.31034791346126855, 0.1397593987968144, -0.2690649690253398, -0.1686520155850523, 0.21085324054333887, -0.10335980522627598, 0.... |
709.3885 | The study of leading twist light cone wave functions of 2S state
charmonium mesons | In this paper leading twist light cone wave functions of 2S state charmonium
mesons are studied and models of these functions are built.
| hep-ph | in this paper leading twist light cone wave functions of 2s state charmonium mesons are studied and models of these functions are built | [['in', 'this', 'paper', 'leading', 'twist', 'light', 'cone', 'wave', 'functions', 'of', '2s', 'state', 'charmonium', 'mesons', 'are', 'studied', 'and', 'models', 'of', 'these', 'functions', 'are', 'built']] | [-0.12183636347965701, 0.25859344062273915, -0.08164075049369232, 0.14840056955227224, 0.00512555816575237, -0.12282213410767524, -0.018652229078883385, 0.43330112788016384, -0.18474711931270102, -0.1476007304761721, 0.01800005819709243, -0.3264637992757818, -0.08909945692057195, 0.09688099643782429, 0.0850316959809076... |
709.3886 | Loops for ILC | This contribution summarizes the on-going activities connected to the
evaluation of higher order radiative corrections in the context of a future
international linear collider (ILC).
| hep-ph | this contribution summarizes the ongoing activities connected to the evaluation of higher order radiative corrections in the context of a future international linear collider ilc | [['this', 'contribution', 'summarizes', 'the', 'ongoing', 'activities', 'connected', 'to', 'the', 'evaluation', 'of', 'higher', 'order', 'radiative', 'corrections', 'in', 'the', 'context', 'of', 'a', 'future', 'international', 'linear', 'collider', 'ilc']] | [-0.1448341093212366, 0.08743552193045616, -0.005385446101427078, 0.07920881835278124, -0.14513034038245679, -0.025572316739708185, -0.013608269914984704, 0.3052558277547359, -0.2244949934259057, -0.2547406801022589, 0.11726525203790515, -0.37069489553570745, -0.0741276852786541, 0.1852512862160802, 0.06831226509064436... |
709.3887 | Reduce Problems From Braid Groups To Braid Monoids | This paper proposes for every $n$, linear time reductions of the word and
conjugacy problems on the braid groups $B_n$ to the corresponding problems on
the braid monoids $B_n^+$ and moreover only using positive words
representations.
| math.GR math.GT | this paper proposes for every n linear time reductions of the word and conjugacy problems on the braid groups b_n to the corresponding problems on the braid monoids b_n and moreover only using positive words representations | [['this', 'paper', 'proposes', 'for', 'every', 'n', 'linear', 'time', 'reductions', 'of', 'the', 'word', 'and', 'conjugacy', 'problems', 'on', 'the', 'braid', 'groups', 'b_n', 'to', 'the', 'corresponding', 'problems', 'on', 'the', 'braid', 'monoids', 'b_n', 'and', 'moreover', 'only', 'using', 'positive', 'words', 'repr... | [-0.11266226812990175, 0.11763119256162706, -0.024729029482437506, 0.05752717075908246, -0.12196054701538135, -0.139436252525128, 0.08007182013049412, 0.34078835592501694, -0.4247817700314853, -0.22637545631732792, 0.09870448574009869, -0.3311499037469427, -0.1333771901942479, 0.2108648889714257, -0.13430917115571597, ... |
709.3888 | Fluctuation Theorems | Fluctuation theorems, which have been developed over the past 15 years, have
resulted in fundamental breakthroughs in our understanding of how
irreversibility emerges from reversible dynamics, and have provided new
statistical mechanical relationships for free energy changes. They describe the
statistical fluctuation... | cond-mat.stat-mech | fluctuation theorems which have been developed over the past 15 years have resulted in fundamental breakthroughs in our understanding of how irreversibility emerges from reversible dynamics and have provided new statistical mechanical relationships for free energy changes they describe the statistical fluctuations in t... | [['fluctuation', 'theorems', 'which', 'have', 'been', 'developed', 'over', 'the', 'past', '15', 'years', 'have', 'resulted', 'in', 'fundamental', 'breakthroughs', 'in', 'our', 'understanding', 'of', 'how', 'irreversibility', 'emerges', 'from', 'reversible', 'dynamics', 'and', 'have', 'provided', 'new', 'statistical', '... | [-0.0957401847075401, 0.1609728576462974, -0.14291629599461306, 0.1185022383899617, 0.0013161964032906985, -0.11855346623106279, 0.023665158778253564, 0.34752950423221657, -0.2537321909668221, -0.30246454801585904, 0.09997858985941317, -0.26667160328340117, -0.15369116195369567, 0.2834628124272559, -0.05808262582665876... |
709.3889 | A Neutrino Factory for both Large and Small theta_13 | An analysis of the neutrino oscillation physics capability of a low energy
Neutrino Factory is presented, including a first simulation of the detector
efficiency and event energy threshold. The sensitivity of the physics reach to
the presence of backgrounds is also studied. We consider a representative
baseline of 14... | hep-ph | an analysis of the neutrino oscillation physics capability of a low energy neutrino factory is presented including a first simulation of the detector efficiency and event energy threshold the sensitivity of the physics reach to the presence of backgrounds is also studied we consider a representative baseline of 1480 km... | [['an', 'analysis', 'of', 'the', 'neutrino', 'oscillation', 'physics', 'capability', 'of', 'a', 'low', 'energy', 'neutrino', 'factory', 'is', 'presented', 'including', 'a', 'first', 'simulation', 'of', 'the', 'detector', 'efficiency', 'and', 'event', 'energy', 'threshold', 'the', 'sensitivity', 'of', 'the', 'physics', ... | [-0.09343353135360254, 0.17107436284113484, -0.026327535405184503, 0.13538832690352826, -0.05304901470715465, -0.10941028668805286, 0.06236917877502672, 0.29442517476173136, -0.21496540594946695, -0.38957505097595957, 0.09098160275686029, -0.28442104373479615, -0.012179730508816303, 0.20467043848842517, 0.0186800683705... |
709.389 | Mass transport and variants of the logarithmic Sobolev inequality | We develop the optimal transportation approach to modified log-Sobolev
inequalities and to isoperimetric inequalities. Various sufficient conditions
for such inequalities are given. Some of them are new even in the classical
log-Sobolev case. The idea behind many of these conditions is that measures
with a non-convex... | math.PR math.FA | we develop the optimal transportation approach to modified logsobolev inequalities and to isoperimetric inequalities various sufficient conditions for such inequalities are given some of them are new even in the classical logsobolev case the idea behind many of these conditions is that measures with a nonconvex potenti... | [['we', 'develop', 'the', 'optimal', 'transportation', 'approach', 'to', 'modified', 'logsobolev', 'inequalities', 'and', 'to', 'isoperimetric', 'inequalities', 'various', 'sufficient', 'conditions', 'for', 'such', 'inequalities', 'are', 'given', 'some', 'of', 'them', 'are', 'new', 'even', 'in', 'the', 'classical', 'lo... | [-0.09481230354326409, 0.04107954723457264, -0.11354685803810351, 0.1797928763712556, -0.1047178550547552, -0.21169841165524408, 0.015631336854164336, 0.3790555357889727, -0.3161203805357218, -0.294962651783947, 0.16351195717457856, -0.2662051424362458, -0.1970029513373278, 0.23422606838433896, -0.1499513125610213, 0.1... |
709.3891 | A Description of Rotating Multicharged Black Holes in terms of Branes
and Antibranes | We describe rotating multicharge black holes as stacks of intersecting branes
and antibranes together with massless gases on them. Assuming the energies of
the gases to be equal, we find that their angular momentum parameters,
corresponding to black hole rotations, are also equal. The entropy S of this
model is given... | hep-th | we describe rotating multicharge black holes as stacks of intersecting branes and antibranes together with massless gases on them assuming the energies of the gases to be equal we find that their angular momentum parameters corresponding to black hole rotations are also equal the entropy s of this model is given by s x... | [['we', 'describe', 'rotating', 'multicharge', 'black', 'holes', 'as', 'stacks', 'of', 'intersecting', 'branes', 'and', 'antibranes', 'together', 'with', 'massless', 'gases', 'on', 'them', 'assuming', 'the', 'energies', 'of', 'the', 'gases', 'to', 'be', 'equal', 'we', 'find', 'that', 'their', 'angular', 'momentum', 'pa... | [-0.14367850460500145, 0.20764561801193782, -0.04903335220145959, 0.09516264173046997, -0.004421156706909338, -0.18974148539688301, 0.017004106179983526, 0.32647706892824285, -0.21023311622578789, -0.2792413754250716, 0.07177876566226284, -0.31389638787066493, -0.038888336148940855, 0.16435238143463654, -0.051721338437... |
709.3892 | AC conductivity of polymer composites: an efficient confirmatory tool
for qualifying crude multi-walled carbon nanotube-samples | The present communication highlights that ac conductivity measurement of the
multi-walled carbon nanotubes (MWNTs)-polymer composites is a very promising
characterizing tool for qualifying any crude MWNT-sample synthesized by
electric arc. It distinguishes graphite structures from that of the MWNTs and
reflects the r... | cond-mat.mtrl-sci | the present communication highlights that ac conductivity measurement of the multiwalled carbon nanotubes mwntspolymer composites is a very promising characterizing tool for qualifying any crude mwntsample synthesized by electric arc it distinguishes graphite structures from that of the mwnts and reflects the relative ... | [['the', 'present', 'communication', 'highlights', 'that', 'ac', 'conductivity', 'measurement', 'of', 'the', 'multiwalled', 'carbon', 'nanotubes', 'mwntspolymer', 'composites', 'is', 'a', 'very', 'promising', 'characterizing', 'tool', 'for', 'qualifying', 'any', 'crude', 'mwntsample', 'synthesized', 'by', 'electric', '... | [-0.1162928907041389, 0.14641134132091937, -0.06423246337002829, 0.01588624397378513, -0.030617470141059082, -0.1568990183945157, 0.10942572548642363, 0.3937934311302869, -0.2507330294110273, -0.327355316536207, 0.04427865507130168, -0.2576961044026049, -0.13421448866689675, 0.2378351700786305, -0.031050525108156236, 0... |
709.3893 | Linearization of skew-periodic loops and $\mathbb S^1$-cocycles | We discuss linearization of skew-periodic loops. We generalize the situation
to linearization of non-commutative loops and $\mathbb S^1$-cocycles.
| math.KT math.OA | we discuss linearization of skewperiodic loops we generalize the situation to linearization of noncommutative loops and mathbb s1cocycles | [['we', 'discuss', 'linearization', 'of', 'skewperiodic', 'loops', 'we', 'generalize', 'the', 'situation', 'to', 'linearization', 'of', 'noncommutative', 'loops', 'and', 'mathbb', 's1cocycles']] | [-0.25726174004375935, 0.08288884640205652, -0.014137294259853661, 0.10977127123624086, -0.16769641858991235, -0.11334024218376726, 0.021870383992791176, 0.37693393626250327, -0.273682723287493, -0.13118861301336437, 0.14599712059134617, -0.2563086766167544, -0.20238721324130893, 0.14888041792437434, -0.190901607275009... |
709.3894 | Electrically injected cavity polaritons | We have realised a semiconductor quantum structure that produces
electroluminescence while operating in the light-matter strong coupling regime.
The mid-infrared light emitting device is composed of a quantum cascade
structure embedded in a planar microcavity, based on the GaAs/AlGaAs material
system. At zero bias, t... | cond-mat.other quant-ph | we have realised a semiconductor quantum structure that produces electroluminescence while operating in the lightmatter strong coupling regime the midinfrared light emitting device is composed of a quantum cascade structure embedded in a planar microcavity based on the gaasalgaas material system at zero bias the struct... | [['we', 'have', 'realised', 'a', 'semiconductor', 'quantum', 'structure', 'that', 'produces', 'electroluminescence', 'while', 'operating', 'in', 'the', 'lightmatter', 'strong', 'coupling', 'regime', 'the', 'midinfrared', 'light', 'emitting', 'device', 'is', 'composed', 'of', 'a', 'quantum', 'cascade', 'structure', 'emb... | [-0.14733820200698183, 0.2608746079049524, -0.08458106927407373, -0.03865783978757723, 0.002022387455716463, -0.18945214261683369, 0.06101909559739787, 0.4331178661668673, -0.25747909363625304, -0.3054344949279247, -0.05101753001612711, -0.31700473800966783, -0.06261897990978989, 0.2639293743289142, 0.04584028526109510... |
709.3895 | Energy Extraction from Black Holes | In this lecture I give an introduction to the rotational energy extraction of
black holes by the electromagnetic Blandford-Znajek process and the generation
of relativistic jets. After some basic material on the electrodynamics of black
hole magnetospheres, we derive the most important results of Blandford and
Znajek... | astro-ph gr-qc hep-ph | in this lecture i give an introduction to the rotational energy extraction of black holes by the electromagnetic blandfordznajek process and the generation of relativistic jets after some basic material on the electrodynamics of black hole magnetospheres we derive the most important results of blandford and znajek by m... | [['in', 'this', 'lecture', 'i', 'give', 'an', 'introduction', 'to', 'the', 'rotational', 'energy', 'extraction', 'of', 'black', 'holes', 'by', 'the', 'electromagnetic', 'blandfordznajek', 'process', 'and', 'the', 'generation', 'of', 'relativistic', 'jets', 'after', 'some', 'basic', 'material', 'on', 'the', 'electrodyna... | [-0.1278435989052698, 0.11310567684322646, -0.03651316605648527, 0.1314677894385558, -0.10686626723436739, -0.07203628056211978, -0.03720019909963813, 0.33423191975922356, -0.161908218951305, -0.29345697476979227, 0.09845183354862515, -0.2674346752984259, -0.05403504084535344, 0.22491179933641306, -0.033450320963898016... |
709.3896 | Variations and estimators for the selfsimilarity order through Malliavin
calculus | Using multiple stochastic integrals and the Malliavin calculus, we analyze
the asymptotic behavior of quadratic variations for a specific non-Gaussian
self-similar process, the Rosenblatt process. We apply our results to the
design of strongly consistent statistical estimators for the self-similarity
parameter $H$. A... | math.PR math.ST stat.TH | using multiple stochastic integrals and the malliavin calculus we analyze the asymptotic behavior of quadratic variations for a specific nongaussian selfsimilar process the rosenblatt process we apply our results to the design of strongly consistent statistical estimators for the selfsimilarity parameter h although in ... | [['using', 'multiple', 'stochastic', 'integrals', 'and', 'the', 'malliavin', 'calculus', 'we', 'analyze', 'the', 'asymptotic', 'behavior', 'of', 'quadratic', 'variations', 'for', 'a', 'specific', 'nongaussian', 'selfsimilar', 'process', 'the', 'rosenblatt', 'process', 'we', 'apply', 'our', 'results', 'to', 'the', 'desi... | [-0.05766306604337262, 0.06244084688397237, -0.16500659216846147, 0.12753936777370248, -0.056896893582475114, -0.11317909562803176, 0.031444205442465935, 0.3624871148312666, -0.2953343561973916, -0.22568148404292493, 0.12793150935911135, -0.26147333295813885, -0.17383068847660738, 0.19657374723219728, -0.10104863031441... |
709.3897 | Microscopic Dynamics of Shape Coexistence Phenomena around 68Se and 72Kr | The adiabatic self-consistent collective coordinate (ASCC) method is applied
to the pairing-plus-quadrupole (P + Q) model Hamiltonian including the
quadrupole pairing, and the oblate-prolate shape coexistence phenomena in
proton-rich nuclei, 68Se and 72Kr, are investigated. It is shown that the
collective path connec... | nucl-th | the adiabatic selfconsistent collective coordinate ascc method is applied to the pairingplusquadrupole p q model hamiltonian including the quadrupole pairing and the oblateprolate shape coexistence phenomena in protonrich nuclei 68se and 72kr are investigated it is shown that the collective path connecting the oblate a... | [['the', 'adiabatic', 'selfconsistent', 'collective', 'coordinate', 'ascc', 'method', 'is', 'applied', 'to', 'the', 'pairingplusquadrupole', 'p', 'q', 'model', 'hamiltonian', 'including', 'the', 'quadrupole', 'pairing', 'and', 'the', 'oblateprolate', 'shape', 'coexistence', 'phenomena', 'in', 'protonrich', 'nuclei', '6... | [-0.1527626955949624, 0.18940875365321214, -0.09203022033228384, 0.1101803517783992, -0.011118742196898287, -0.08288156427054977, -0.024378973080699022, 0.38031389413711925, -0.219702830259727, -0.2638790496935447, -0.0508462646859698, -0.25876221398712007, -0.11579340885121686, 0.15067217285201576, 0.05264402957788358... |
709.3898 | Neutrinos from WIMP Annihilations Obtained Using a Full Three-Flavor
Monte Carlo Approach | Weakly Interacting Massive Particles (WIMPs) are one of the main candidates
for the dark matter in the Universe. If these particles make up the dark
matter, then they can be captured by the Sun or the Earth, sink to the
respective cores, annihilate, and produce neutrinos. Thus, these neutrinos can
be a striking dark ... | hep-ph astro-ph | weakly interacting massive particles wimps are one of the main candidates for the dark matter in the universe if these particles make up the dark matter then they can be captured by the sun or the earth sink to the respective cores annihilate and produce neutrinos thus these neutrinos can be a striking dark matter sign... | [['weakly', 'interacting', 'massive', 'particles', 'wimps', 'are', 'one', 'of', 'the', 'main', 'candidates', 'for', 'the', 'dark', 'matter', 'in', 'the', 'universe', 'if', 'these', 'particles', 'make', 'up', 'the', 'dark', 'matter', 'then', 'they', 'can', 'be', 'captured', 'by', 'the', 'sun', 'or', 'the', 'earth', 'sin... | [-0.059158835222013297, 0.2660354350713314, -0.06582345978403464, 0.18966413923865183, -0.06284820058755576, -0.09298653806932271, 0.03968986482033506, 0.3390589741168078, -0.22194634976796807, -0.3576092453338206, 0.04471652485337108, -0.32145740385353566, -0.0402193943914026, 0.22199085810710675, 0.05878081320251658,... |
709.3899 | On Third-Order Timelike Splitting Functions and Top-Mediated Higgs Decay
into Hadrons | We employ relations between spacelike and timelike deep-inelastic processes
in perturbative QCD to calculate the next-to-next-to-leading order (NNLO)
contributions to the timelike quark-quark and gluon-gluon splitting functions
for the evolution of flavour-singlet fragmentation distributions. We briefly
address the e... | hep-ph | we employ relations between spacelike and timelike deepinelastic processes in perturbative qcd to calculate the nexttonexttoleading order nnlo contributions to the timelike quarkquark and gluongluon splitting functions for the evolution of flavoursinglet fragmentation distributions we briefly address the endpoint behav... | [['we', 'employ', 'relations', 'between', 'spacelike', 'and', 'timelike', 'deepinelastic', 'processes', 'in', 'perturbative', 'qcd', 'to', 'calculate', 'the', 'nexttonexttoleading', 'order', 'nnlo', 'contributions', 'to', 'the', 'timelike', 'quarkquark', 'and', 'gluongluon', 'splitting', 'functions', 'for', 'the', 'evo... | [-0.11297612155898061, 0.18903525898559498, -0.11470660613849759, 0.17122307884838125, -0.031065726187080145, -0.02834916312113097, 0.04757116175227866, 0.325988956769093, -0.16214652021521145, -0.1798902182004501, -0.019560548866926163, -0.35276159801587614, 0.004896036397243284, 0.08758736564057697, 0.120568499122998... |
709.39 | Nonlinear tunneling in two-dimensional lattices | We present thorough analysis of the nonlinear tunneling of Bose-Einstein
condensates in static and accelerating two-dimensional lattices within the
framework of the mean-field approximation. We deal with nonseparable lattices
considering different initial atomic distributions in the highly symmetric
states. For analy... | cond-mat.other nlin.PS | we present thorough analysis of the nonlinear tunneling of boseeinstein condensates in static and accelerating twodimensional lattices within the framework of the meanfield approximation we deal with nonseparable lattices considering different initial atomic distributions in the highly symmetric states for analytical d... | [['we', 'present', 'thorough', 'analysis', 'of', 'the', 'nonlinear', 'tunneling', 'of', 'boseeinstein', 'condensates', 'in', 'static', 'and', 'accelerating', 'twodimensional', 'lattices', 'within', 'the', 'framework', 'of', 'the', 'meanfield', 'approximation', 'we', 'deal', 'with', 'nonseparable', 'lattices', 'consider... | [-0.15528152631583347, 0.1869486766443786, -0.0658283059357076, 0.11325412504114904, 0.009733205061762574, -0.16550119853816292, 0.03005955707247151, 0.3613241128227178, -0.23504133016599263, -0.262701171068871, 0.025539368569375352, -0.24906100686503316, -0.13291919063096352, 0.18341871113343006, 0.03789038126272684, ... |
709.3901 | Influence of Mn doping on the microstructure and optical property of ZnO | Undoped and Mn doped ZnO samples with different percentage of Mn content (1
mol%, 2 mol% and 3mol%) were synthesized by a simple solvo-thermal method. We
have studied the structural, chemical and optical properties of the samples by
using x-ray diffraction (XRD), scanning electron microscopy (SEM), energy
dispersive ... | cond-mat.mtrl-sci | undoped and mn doped zno samples with different percentage of mn content 1 mol 2 mol and 3mol were synthesized by a simple solvothermal method we have studied the structural chemical and optical properties of the samples by using xray diffraction xrd scanning electron microscopy sem energy dispersive xray edx analysis ... | [['undoped', 'and', 'mn', 'doped', 'zno', 'samples', 'with', 'different', 'percentage', 'of', 'mn', 'content', '1', 'mol', '2', 'mol', 'and', '3mol', 'were', 'synthesized', 'by', 'a', 'simple', 'solvothermal', 'method', 'we', 'have', 'studied', 'the', 'structural', 'chemical', 'and', 'optical', 'properties', 'of', 'the... | [-0.0210794644333936, 0.1780952014904148, 0.0038484913040080977, -0.014596438326808656, 0.0583732710348378, -0.161155046548309, 0.1282832565263781, 0.5302898437266463, -0.2528940774114995, -0.3251101002225588, -0.030581051543965166, -0.4660078557722014, -0.06998655018236102, 0.16021124863322697, 0.05231894648730241, 0.... |
709.3902 | Optical Stern Gerlach Effect beyond the rotating wave approximation | We show that the inclusion of counter rotating terms, usually dropped, in the
interaction Hamiltonian of the electric dipole of a two level atom with an
electromagnetic field leads to significant modification of the splitting of an
atomic beam known as Optical Stern Gerlach Effect which now acquires a fine
structure.... | physics.atom-ph physics.optics | we show that the inclusion of counter rotating terms usually dropped in the interaction hamiltonian of the electric dipole of a two level atom with an electromagnetic field leads to significant modification of the splitting of an atomic beam known as optical stern gerlach effect which now acquires a fine structure | [['we', 'show', 'that', 'the', 'inclusion', 'of', 'counter', 'rotating', 'terms', 'usually', 'dropped', 'in', 'the', 'interaction', 'hamiltonian', 'of', 'the', 'electric', 'dipole', 'of', 'a', 'two', 'level', 'atom', 'with', 'an', 'electromagnetic', 'field', 'leads', 'to', 'significant', 'modification', 'of', 'the', 's... | [-0.16992218872787906, 0.1639831492765213, -0.03728505607475253, 0.031706967153677754, -0.0643987885000659, -0.08321917069820213, 0.012581657300995407, 0.3586818960805734, -0.2584364695437983, -0.3412254798207797, -0.018161293669311584, -0.2448765681873934, -0.09194217005050649, 0.15342862195536203, 0.00780981245870683... |
709.3903 | Noncentral convergence of multiple integrals | Fix $\nu>0$, denote by $G(\nu/2)$ a Gamma random variable with parameter
$\nu/2$ and let $n\geq2$ be a fixed even integer. Consider a sequence
$\{F_k\}_{k\geq1}$ of square integrable random variables belonging to the $n$th
Wiener chaos of a given Gaussian process and with variance converging to
$2\nu$. As $k\to\infty... | math.PR | fix nu0 denote by gnu2 a gamma random variable with parameter nu2 and let ngeq2 be a fixed even integer consider a sequence f_k_kgeq1 of square integrable random variables belonging to the nth wiener chaos of a given gaussian process and with variance converging to 2nu as ktoinfty we prove that f_k converges in distrib... | [['fix', 'nu0', 'denote', 'by', 'gnu2', 'a', 'gamma', 'random', 'variable', 'with', 'parameter', 'nu2', 'and', 'let', 'ngeq2', 'be', 'a', 'fixed', 'even', 'integer', 'consider', 'a', 'sequence', 'f_k_kgeq1', 'of', 'square', 'integrable', 'random', 'variables', 'belonging', 'to', 'the', 'nth', 'wiener', 'chaos', 'of', '... | [-0.15407737585362688, 0.2298227904669555, -0.08937508283696811, -0.0021623806044866294, -0.048073487633293305, -0.24176222436001588, 0.06691204033117613, 0.31751913900069634, -0.3348805454784426, -0.16804221155250382, 0.12101874736354462, -0.2873719063555372, -0.12542565425673244, 0.10872153908913505, -0.0522279734482... |
709.3904 | An Eshelby model for the highly viscous flow | The shear flow and the dielectric alpha-process in molecular glass formers is
modeled in terms of local structural rearrangements which reverse a strong
local shear. Using Eshelby's solution of the corresponding elasticity theory
problem (J. D. Eshelby, Proc. Roy. Soc. A241, 376 (1957)), one can calculate
the recover... | cond-mat.dis-nn | the shear flow and the dielectric alphaprocess in molecular glass formers is modeled in terms of local structural rearrangements which reverse a strong local shear using eshelbys solution of the corresponding elasticity theory problem j d eshelby proc roy soc a241 376 1957 one can calculate the recoverable compliance a... | [['the', 'shear', 'flow', 'and', 'the', 'dielectric', 'alphaprocess', 'in', 'molecular', 'glass', 'formers', 'is', 'modeled', 'in', 'terms', 'of', 'local', 'structural', 'rearrangements', 'which', 'reverse', 'a', 'strong', 'local', 'shear', 'using', 'eshelbys', 'solution', 'of', 'the', 'corresponding', 'elasticity', 't... | [-0.13596403262004106, 0.14217157367951438, -0.09023455756180214, 0.020385226102595393, -0.021200429163685048, -0.09620804366928459, 0.006841616369924988, 0.3152192875630025, -0.37402098165881453, -0.26127646517742315, 0.06317980567491943, -0.23686462843959982, -0.15579659154349373, 0.08507321225573318, 0.0289463986151... |
709.3905 | On Voevodsky's algebraic K-theory spectrum BGL | Under a certain normalization assumption we prove that the $\Pro^1$-spectrum
$\mathrm{BGL}$ of Voevodsky which represents algebraic $K$-theory is unique
over $\Spec(\mathbb{Z})$. Following an idea of Voevodsky, we equip the
$\Pro^1$-spectrum $\mathrm{BGL}$ with the structure of a commutative
$\Pro^1$-ring spectrum in... | math.AG math.AT | under a certain normalization assumption we prove that the pro1spectrum mathrmbgl of voevodsky which represents algebraic ktheory is unique over specmathbbz following an idea of voevodsky we equip the pro1spectrum mathrmbgl with the structure of a commutative pro1ring spectrum in the motivic stable homotopy category fu... | [['under', 'a', 'certain', 'normalization', 'assumption', 'we', 'prove', 'that', 'the', 'pro1spectrum', 'mathrmbgl', 'of', 'voevodsky', 'which', 'represents', 'algebraic', 'ktheory', 'is', 'unique', 'over', 'specmathbbz', 'following', 'an', 'idea', 'of', 'voevodsky', 'we', 'equip', 'the', 'pro1spectrum', 'mathrmbgl', '... | [-0.18233101528037238, -0.02324977438023255, -0.1959743315337209, 0.09824530154399506, -0.09614470847336962, -0.14938311765037543, -0.011408661336948475, 0.34642189574167803, -0.3943708633567702, -0.15232493694838103, 0.06999314330761565, -0.13393012194963475, -0.12027194197835014, 0.1789573399173851, -0.19998004486331... |
709.3906 | Fast stable direct fitting and smoothness selection for Generalized
Additive Models | Existing computationally efficient methods for penalized likelihood GAM
fitting employ iterative smoothness selection on working linear models (or
working mixed models). Such schemes fail to converge for a non-negligible
proportion of models, with failure being particularly frequent in the presence
of concurvity. If ... | stat.ME stat.CO | existing computationally efficient methods for penalized likelihood gam fitting employ iterative smoothness selection on working linear models or working mixed models such schemes fail to converge for a nonnegligible proportion of models with failure being particularly frequent in the presence of concurvity if smoothne... | [['existing', 'computationally', 'efficient', 'methods', 'for', 'penalized', 'likelihood', 'gam', 'fitting', 'employ', 'iterative', 'smoothness', 'selection', 'on', 'working', 'linear', 'models', 'or', 'working', 'mixed', 'models', 'such', 'schemes', 'fail', 'to', 'converge', 'for', 'a', 'nonnegligible', 'proportion', ... | [-0.05197658495638858, 0.032729142416042814, -0.12049518143370126, 0.10978154005539237, -0.1284074587500513, -0.22658074279421603, 0.08454920184114158, 0.4334067414147836, -0.2538612712470984, -0.29351327444116276, 0.14219448394247924, -0.17133632352378106, -0.12861657103128504, 0.2068538977738089, -0.11127652907298673... |
709.3907 | Continuous Frequency Controllable Nano-electromechanical Systems Based
on Multiwalled Carbon Nanotubes | We demonstrate a class of model nano-electromechanical systems (NEMS) based
on multiwalled carbon nanotubes (MWNTs) which has longer inner cores coaxially
oscillating inside their respective shorter outer shell holders and can operate
at continuously controllable frequencies up to the gigahertz range when fuelled
by ... | cond-mat.mtrl-sci cond-mat.stat-mech | we demonstrate a class of model nanoelectromechanical systems nems based on multiwalled carbon nanotubes mwnts which has longer inner cores coaxially oscillating inside their respective shorter outer shell holders and can operate at continuously controllable frequencies up to the gigahertz range when fuelled by ac elec... | [['we', 'demonstrate', 'a', 'class', 'of', 'model', 'nanoelectromechanical', 'systems', 'nems', 'based', 'on', 'multiwalled', 'carbon', 'nanotubes', 'mwnts', 'which', 'has', 'longer', 'inner', 'cores', 'coaxially', 'oscillating', 'inside', 'their', 'respective', 'shorter', 'outer', 'shell', 'holders', 'and', 'can', 'op... | [-0.14902487098312017, 0.20986698047713714, 0.01338120780436071, -0.040066318423817505, -0.08910383642419961, -0.17985221211210634, 0.06882334149158592, 0.4238888992009856, -0.2168449263174272, -0.30708095373863237, 0.07627572761212825, -0.24255473484410672, -0.06606054626378818, 0.2855191873518605, -0.0142069085788457... |
709.3908 | Spin dynamics with non-abelian Berry gauge fields as a semiclassical
constrained hamiltonian system | The dynamics of observables which are matrices depending on \hbar and taking
values in classical phase space is defined retaining the terms up to the first
order in \hbar of the Moyal bracket. Within this semiclassical approach a first
order lagrangian involving gauge fields is studied as a constrained hamiltonian
sy... | cond-mat.mes-hall hep-th quant-ph | the dynamics of observables which are matrices depending on hbar and taking values in classical phase space is defined retaining the terms up to the first order in hbar of the moyal bracket within this semiclassical approach a first order lagrangian involving gauge fields is studied as a constrained hamiltonian system ... | [['the', 'dynamics', 'of', 'observables', 'which', 'are', 'matrices', 'depending', 'on', 'hbar', 'and', 'taking', 'values', 'in', 'classical', 'phase', 'space', 'is', 'defined', 'retaining', 'the', 'terms', 'up', 'to', 'the', 'first', 'order', 'in', 'hbar', 'of', 'the', 'moyal', 'bracket', 'within', 'this', 'semiclassi... | [-0.22629962099303844, 0.20398166659395459, -0.08370489122529255, 0.04710836101754676, -0.07273269058434201, -0.06378663002730912, -0.0011636046845404828, 0.3232703981921077, -0.24534813858202245, -0.2937857047463844, 0.009199463437906787, -0.21116749565956777, -0.1506248536237256, 0.188827703493174, -0.013588060670700... |
709.3909 | Bell's inequality: Physics meets Probability | We remind the viewpoint that violation of Bell's inequality might be
interpreted not only as an evidence of the alternative -- either nonlocality or
``death of reality'' (under the assumption the quantum mechanics is
incomplete). Violation of Bell's type inequalities is a well known sufficient
condition of incompatib... | quant-ph | we remind the viewpoint that violation of bells inequality might be interpreted not only as an evidence of the alternative either nonlocality or death of reality under the assumption the quantum mechanics is incomplete violation of bells type inequalities is a well known sufficient condition of incompatibility of rando... | [['we', 'remind', 'the', 'viewpoint', 'that', 'violation', 'of', 'bells', 'inequality', 'might', 'be', 'interpreted', 'not', 'only', 'as', 'an', 'evidence', 'of', 'the', 'alternative', 'either', 'nonlocality', 'or', 'death', 'of', 'reality', 'under', 'the', 'assumption', 'the', 'quantum', 'mechanics', 'is', 'incomplete... | [-0.1319467072794366, 0.13455826230214002, -0.11967254394141871, 0.1435708500234885, -0.10598127053916649, -0.23327415929255046, 0.08740870695975092, 0.29203495078908853, -0.2676433481304949, -0.29191374078733856, 0.07063679746009738, -0.23088794038935376, -0.10513314913526128, 0.17822237506971444, -0.11996824674770917... |
709.391 | Flavors in an expanding plasma | We consider the effect of an expanding plasma on probe matter by determining
time-dependent D7 embeddings in the holographic dual of an expanding viscous
plasma. We calculate the chiral condensate and meson spectra including
contributions of viscosity. The chiral condensate essentially confirms the
expectation from t... | hep-th | we consider the effect of an expanding plasma on probe matter by determining timedependent d7 embeddings in the holographic dual of an expanding viscous plasma we calculate the chiral condensate and meson spectra including contributions of viscosity the chiral condensate essentially confirms the expectation from the st... | [['we', 'consider', 'the', 'effect', 'of', 'an', 'expanding', 'plasma', 'on', 'probe', 'matter', 'by', 'determining', 'timedependent', 'd7', 'embeddings', 'in', 'the', 'holographic', 'dual', 'of', 'an', 'expanding', 'viscous', 'plasma', 'we', 'calculate', 'the', 'chiral', 'condensate', 'and', 'meson', 'spectra', 'inclu... | [-0.1236272639052683, 0.194419006207336, -0.1002636428780948, 0.07294062769800849, -0.015304813185070135, -0.05561255336491556, -0.011239128258032135, 0.2968857497259786, -0.19312255052831967, -0.21276698346379436, -0.004259924778620465, -0.32341285082924215, -0.03796769086200791, 0.10264552012085915, 0.041596792897657... |
709.3911 | Classical Exchange Algebra of the Superstring on S^5 with the AdS-time | A classical exchange algebra of the superstring on S^5 with the AdS-time is
shown on the light-like plane. To this end we use the geometrical method of
which consistency is guaranteed by the classical Yang-Baxter equation. The
Dirac method does not work, there being constraints which contain first-class
and second-cl... | hep-th | a classical exchange algebra of the superstring on s5 with the adstime is shown on the lightlike plane to this end we use the geometrical method of which consistency is guaranteed by the classical yangbaxter equation the dirac method does not work there being constraints which contain firstclass and secondclass and one... | [['a', 'classical', 'exchange', 'algebra', 'of', 'the', 'superstring', 'on', 's5', 'with', 'the', 'adstime', 'is', 'shown', 'on', 'the', 'lightlike', 'plane', 'to', 'this', 'end', 'we', 'use', 'the', 'geometrical', 'method', 'of', 'which', 'consistency', 'is', 'guaranteed', 'by', 'the', 'classical', 'yangbaxter', 'equa... | [-0.12963994427700526, 0.08323969396296889, -0.08262428324669599, 0.05202524039001825, -0.18848743674655755, -0.17564510500524194, 0.0015015284220377604, 0.3340547644533217, -0.2780029200250283, -0.27268133762603003, 0.10393724445796883, -0.2847630106844008, -0.1273422834579833, 0.14611933037328223, -0.0729926325021854... |
709.3912 | Scattering of Long Folded Strings and Mixed Correlators in the
Two-Matrix Model | We study the interactions of Maldacena's long folded strings in
two-dimensional string theory. We find the amplitude for a state containing two
long folded strings to come and go back to infinity. We calculate this
amplitude both in the worldsheet theory and in the dual matrix model, the
Matrix Quantum Mechanics. The... | hep-th | we study the interactions of maldacenas long folded strings in twodimensional string theory we find the amplitude for a state containing two long folded strings to come and go back to infinity we calculate this amplitude both in the worldsheet theory and in the dual matrix model the matrix quantum mechanics the matrix ... | [['we', 'study', 'the', 'interactions', 'of', 'maldacenas', 'long', 'folded', 'strings', 'in', 'twodimensional', 'string', 'theory', 'we', 'find', 'the', 'amplitude', 'for', 'a', 'state', 'containing', 'two', 'long', 'folded', 'strings', 'to', 'come', 'and', 'go', 'back', 'to', 'infinity', 'we', 'calculate', 'this', 'a... | [-0.14434153128038102, 0.18269673042471632, -0.09230350663287187, 0.13936797773931175, -0.013360543674612535, -0.12905741085687392, 0.004399061208897376, 0.31215048586077326, -0.2872520306595613, -0.2366009107496165, 0.0671699085343582, -0.28217988060746796, -0.17352993481002654, 0.09400938407965947, -0.001897781545036... |
709.3913 | Forward-Backward rapidity correlations at all rapidities | We discuss forward-bacward rapidity correlations in the general situation of
asymmetrical collisions, asymmetric rapidity windows, higher rapidities and
higher energy. We give predictions for RHIC and LHC.
| hep-ph | we discuss forwardbacward rapidity correlations in the general situation of asymmetrical collisions asymmetric rapidity windows higher rapidities and higher energy we give predictions for rhic and lhc | [['we', 'discuss', 'forwardbacward', 'rapidity', 'correlations', 'in', 'the', 'general', 'situation', 'of', 'asymmetrical', 'collisions', 'asymmetric', 'rapidity', 'windows', 'higher', 'rapidities', 'and', 'higher', 'energy', 'we', 'give', 'predictions', 'for', 'rhic', 'and', 'lhc']] | [-0.09689760172309783, 0.2656771076413301, -0.2390175111269435, 0.31069814843627125, 0.017303782801788587, -0.1858940657514792, -0.11736430514317292, 0.4542560333815905, -0.14684041532186362, -0.23325527767435864, -0.12000009949910097, -0.32494779418294245, 0.1594091502842135, 0.11391572654247284, 0.025299853788545497,... |
709.3914 | A Quiver Presentation for Solomon's Descent Algebra | The descent algebra $\Sigma(W)$ is a subalgebra of the group algebra $\Q W$
of a finite Coxeter group $W$, which supports a homomorphism with nilpotent
kernel and commutative image in the character ring of $W$. Thus $\Sigma(W)$ is
a basic algebra, and as such it has a presentation as a quiver with relations.
Here we ... | math.RT math.CO | the descent algebra sigmaw is a subalgebra of the group algebra q w of a finite coxeter group w which supports a homomorphism with nilpotent kernel and commutative image in the character ring of w thus sigmaw is a basic algebra and as such it has a presentation as a quiver with relations here we construct sigmaw as a q... | [['the', 'descent', 'algebra', 'sigmaw', 'is', 'a', 'subalgebra', 'of', 'the', 'group', 'algebra', 'q', 'w', 'of', 'a', 'finite', 'coxeter', 'group', 'w', 'which', 'supports', 'a', 'homomorphism', 'with', 'nilpotent', 'kernel', 'and', 'commutative', 'image', 'in', 'the', 'character', 'ring', 'of', 'w', 'thus', 'sigmaw'... | [-0.15698009407239372, 0.07829131326959259, -0.11431764118129113, 0.013182291475727727, -0.13489665631891884, -0.1551535762808301, 0.02641791202028694, 0.3389247432656464, -0.39220453204861916, -0.20374745023665858, 0.10598173061362849, -0.2332189604792683, -0.09730101016075274, 0.16588686132177588, -0.1361794883431103... |
709.3915 | Guessing Facets: Polytope Structure and Improved LP Decoding | In this paper we investigate the structure of the fundamental polytope used
in the Linear Programming decoding introduced by Feldman, Karger and
Wainwright. We begin by showing that for expander codes, every fractional
pseudocodeword always has at least a constant fraction of non-integral bits. We
then prove that for... | cs.IT math.IT | in this paper we investigate the structure of the fundamental polytope used in the linear programming decoding introduced by feldman karger and wainwright we begin by showing that for expander codes every fractional pseudocodeword always has at least a constant fraction of nonintegral bits we then prove that for expand... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'structure', 'of', 'the', 'fundamental', 'polytope', 'used', 'in', 'the', 'linear', 'programming', 'decoding', 'introduced', 'by', 'feldman', 'karger', 'and', 'wainwright', 'we', 'begin', 'by', 'showing', 'that', 'for', 'expander', 'codes', 'every', 'fractional', 'ps... | [-0.13152669042800413, 0.06036580323298683, -0.062393156336526374, 0.08827413832022094, -0.04985264813847313, -0.25522567818853814, 0.07700702215773006, 0.37702015675416195, -0.343695410619598, -0.27994999079965055, 0.12252043392873754, -0.2426399409658078, -0.1718931483960889, 0.16549435050480746, -0.1159781813715594,... |
709.3916 | Hawking Radiation, Effective Actions and Covariant Boundary Conditions | From appropriate expressions for effective actions, the Hawking radiation
from charged black holes is derived, using only covariant boundary conditions
at the event horizon. The connection of our approach with the Unruh vacuum and
the recent analysis \cite{Robwilczek,Isowilczek,shailesh} of Hawking radiation
using an... | hep-th gr-qc | from appropriate expressions for effective actions the hawking radiation from charged black holes is derived using only covariant boundary conditions at the event horizon the connection of our approach with the unruh vacuum and the recent analysis citerobwilczekisowilczekshailesh of hawking radiation using anomalies is... | [['from', 'appropriate', 'expressions', 'for', 'effective', 'actions', 'the', 'hawking', 'radiation', 'from', 'charged', 'black', 'holes', 'is', 'derived', 'using', 'only', 'covariant', 'boundary', 'conditions', 'at', 'the', 'event', 'horizon', 'the', 'connection', 'of', 'our', 'approach', 'with', 'the', 'unruh', 'vacu... | [-0.08962744968117807, 0.1411338708448139, -0.1498431631639092, 0.13524722660870545, -0.07433198188664392, -0.1308915237472816, 0.006120061882856217, 0.30197130122476, -0.1182852815836668, -0.2968125940639187, 0.10671910951549018, -0.34750198996202514, -0.10079051152041013, 0.1940953236242587, -0.05412806517613882, 0.0... |
709.3917 | Groebner bases for spaces of quadrics of codimension 3 | Let $R=\oplus_{i\geq 0} R_i$ be an Artinian standard graded $K$-algebra
defined by quadrics. Assume that $\dim R_2\leq 3$ and that $K$ is algebraically
closed of characteristic $\neq 2$. We show that $R$ is defined by a Gr\"obner
basis of quadrics with, essentially, one exception. The exception is given by
$K[x,y,z]/... | math.AC | let roplus_igeq 0 r_i be an artinian standard graded kalgebra defined by quadrics assume that dim r_2leq 3 and that k is algebraically closed of characteristic neq 2 we show that r is defined by a grobner basis of quadrics with essentially one exception the exception is given by kxyzi where i is a complete intersection... | [['let', 'roplus_igeq', '0', 'r_i', 'be', 'an', 'artinian', 'standard', 'graded', 'kalgebra', 'defined', 'by', 'quadrics', 'assume', 'that', 'dim', 'r_2leq', '3', 'and', 'that', 'k', 'is', 'algebraically', 'closed', 'of', 'characteristic', 'neq', '2', 'we', 'show', 'that', 'r', 'is', 'defined', 'by', 'a', 'grobner', 'b... | [-0.21266766953340266, 0.0805388608953308, -0.005178870458621532, -0.004670102229283657, -0.0446259612654103, -0.262703515625617, -0.11317920475266874, 0.32193351857131347, -0.3347257135028485, -0.15123206938733347, 0.0877539815774071, -0.2923372519799159, -0.11471309596890933, 0.15781032359518576, -0.07971164237824269... |
709.3918 | Nonthermal dark matter in mirage mediation | In mirage-mediation models there exists a modulus field whose mass is O(1000)
TeV and its late-decay may significantly change the standard thermal relic
scenario of the dark matter. We study nonthermal production of the dark matter
directly from the modulus decay, and find that for some parameter regions
non-thermall... | hep-ph | in miragemediation models there exists a modulus field whose mass is o1000 tev and its latedecay may significantly change the standard thermal relic scenario of the dark matter we study nonthermal production of the dark matter directly from the modulus decay and find that for some parameter regions nonthermally produce... | [['in', 'miragemediation', 'models', 'there', 'exists', 'a', 'modulus', 'field', 'whose', 'mass', 'is', 'o1000', 'tev', 'and', 'its', 'latedecay', 'may', 'significantly', 'change', 'the', 'standard', 'thermal', 'relic', 'scenario', 'of', 'the', 'dark', 'matter', 'we', 'study', 'nonthermal', 'production', 'of', 'the', '... | [-0.13212433527223766, 0.28606643885035404, -0.1609810255129229, 0.16514324812768874, -0.08301909339021553, -0.09995334018868479, -0.026997455063445325, 0.3083260123025287, -0.27605184235356073, -0.3617007636549798, 0.0332852831300856, -0.26302447549321434, 0.028942098282277583, 0.1659472288733179, 0.059891505996611985... |
709.3919 | Dynamics of the topological structures in inhomogeneous media | We present a general review of the dynamics of topological solitons in 1 and
2 dimensions and then discuss some recent work on the scattering of various
solitonic objects (such as kinks and breathers etc) on potential obstructions.
| hep-th | we present a general review of the dynamics of topological solitons in 1 and 2 dimensions and then discuss some recent work on the scattering of various solitonic objects such as kinks and breathers etc on potential obstructions | [['we', 'present', 'a', 'general', 'review', 'of', 'the', 'dynamics', 'of', 'topological', 'solitons', 'in', '1', 'and', '2', 'dimensions', 'and', 'then', 'discuss', 'some', 'recent', 'work', 'on', 'the', 'scattering', 'of', 'various', 'solitonic', 'objects', 'such', 'as', 'kinks', 'and', 'breathers', 'etc', 'on', 'pot... | [-0.1500836907346782, 0.11814704956486821, -0.05065879595809077, 0.11752603107475136, -0.04750987245260101, -0.08820534903114956, 0.006190262741017106, 0.3605400008198462, -0.201693865409317, -0.2589071935876028, 0.1654687340487726, -0.3091414148036979, -0.258637081047422, 0.1630511511374559, -0.03242609219772643, 0.06... |
709.392 | Blind Minimax Estimation | We consider the linear regression problem of estimating an unknown,
deterministic parameter vector based on measurements corrupted by colored
Gaussian noise. We present and analyze blind minimax estimators (BMEs), which
consist of a bounded parameter set minimax estimator, whose parameter set is
itself estimated from... | math.ST stat.ME stat.TH | we consider the linear regression problem of estimating an unknown deterministic parameter vector based on measurements corrupted by colored gaussian noise we present and analyze blind minimax estimators bmes which consist of a bounded parameter set minimax estimator whose parameter set is itself estimated from measure... | [['we', 'consider', 'the', 'linear', 'regression', 'problem', 'of', 'estimating', 'an', 'unknown', 'deterministic', 'parameter', 'vector', 'based', 'on', 'measurements', 'corrupted', 'by', 'colored', 'gaussian', 'noise', 'we', 'present', 'and', 'analyze', 'blind', 'minimax', 'estimators', 'bmes', 'which', 'consist', 'o... | [-0.030660332617711047, 0.03812758041457447, -0.11552004540199731, 0.08626453761964858, -0.09914787533078469, -0.2150194265714967, 0.07081838904604391, 0.37319696157359755, -0.29134464064188503, -0.2758229727267611, 0.17269975219878564, -0.2291389413353778, -0.17706914251467504, 0.21273803957468723, -0.1407703721213160... |
709.3921 | Geographic Gossip: Efficient Averaging for Sensor Networks | Gossip algorithms for distributed computation are attractive due to their
simplicity, distributed nature, and robustness in noisy and uncertain
environments. However, using standard gossip algorithms can lead to a
significant waste in energy by repeatedly recirculating redundant information.
For realistic sensor netw... | cs.IT cs.NI math.IT math.PR | gossip algorithms for distributed computation are attractive due to their simplicity distributed nature and robustness in noisy and uncertain environments however using standard gossip algorithms can lead to a significant waste in energy by repeatedly recirculating redundant information for realistic sensor network mod... | [['gossip', 'algorithms', 'for', 'distributed', 'computation', 'are', 'attractive', 'due', 'to', 'their', 'simplicity', 'distributed', 'nature', 'and', 'robustness', 'in', 'noisy', 'and', 'uncertain', 'environments', 'however', 'using', 'standard', 'gossip', 'algorithms', 'can', 'lead', 'to', 'a', 'significant', 'waste... | [-0.14803735410602564, 0.03683710254744908, -0.037430189807746705, 0.05750184460598344, -0.03849800879472477, -0.20631716727268604, 0.11399876892219409, 0.4595835982995518, -0.27042566734960694, -0.3537434695109641, 0.07561560331496521, -0.22384261019990942, -0.16496625675761936, 0.2046836164564889, -0.1252328659232514... |
709.3922 | Ambipolar blends of CuPc and C60: charge carrier mobility, electronic
structure and its implications for solar cell applications | Ambipolar transport has been realised in blends of the molecular hole
conductor Cu-phthalocyanine (CuPc) and the electron conducting fullerene C60.
Charge carrier mobilities and the occupied electronic levels have been analyzed
as a function of the mixing ratio using field-effect transistor measurements
and photoelec... | cond-mat.soft | ambipolar transport has been realised in blends of the molecular hole conductor cuphthalocyanine cupc and the electron conducting fullerene c60 charge carrier mobilities and the occupied electronic levels have been analyzed as a function of the mixing ratio using fieldeffect transistor measurements and photoelectron sp... | [['ambipolar', 'transport', 'has', 'been', 'realised', 'in', 'blends', 'of', 'the', 'molecular', 'hole', 'conductor', 'cuphthalocyanine', 'cupc', 'and', 'the', 'electron', 'conducting', 'fullerene', 'c60', 'charge', 'carrier', 'mobilities', 'and', 'the', 'occupied', 'electronic', 'levels', 'have', 'been', 'analyzed', '... | [-0.13645919099257425, 0.13627744001207936, 0.010442574701175607, -0.03286922849506011, 0.07998412450903962, -0.17771521752603867, 0.08419023160541687, 0.45746911599718293, -0.1953154937203588, -0.2869728003018375, -0.025329812771062655, -0.3325592897157988, -0.11867524226645715, 0.2052610109977681, -0.0097608048115567... |
709.3923 | On the star formation rate and turbulent dissipation in galactic models | We suggest a model for star formation function and a model for dissipation of
the turbulent energy of interstellar medium. Star formation function takes into
account the effect of turbulization of the ISM. It is shown that application of
mentioned relations to the hierarchical scenario of formation of galaxies
allows... | astro-ph | we suggest a model for star formation function and a model for dissipation of the turbulent energy of interstellar medium star formation function takes into account the effect of turbulization of the ism it is shown that application of mentioned relations to the hierarchical scenario of formation of galaxies allows to ... | [['we', 'suggest', 'a', 'model', 'for', 'star', 'formation', 'function', 'and', 'a', 'model', 'for', 'dissipation', 'of', 'the', 'turbulent', 'energy', 'of', 'interstellar', 'medium', 'star', 'formation', 'function', 'takes', 'into', 'account', 'the', 'effect', 'of', 'turbulization', 'of', 'the', 'ism', 'it', 'is', 'sh... | [-0.07934438768063194, 0.09302639134379255, -0.09225763888350008, 0.12097918025274584, -0.08184476166560843, 0.026986440593326413, 0.030789553892572184, 0.37693028781260995, -0.19594058177962498, -0.37341444116287137, -0.02493850834120216, -0.2030936225250165, -0.059283130223283895, 0.17848986794391797, -0.002329508585... |
709.3924 | The Hubble Constant | I review the current state of determinations of the Hubble constant, which
gives the length scale of the Universe by relating the expansion velocity of
objects to their distance. There are two broad categories of measurements. The
first uses individual astrophysical objects which have some property that
allows their ... | astro-ph | i review the current state of determinations of the hubble constant which gives the length scale of the universe by relating the expansion velocity of objects to their distance there are two broad categories of measurements the first uses individual astrophysical objects which have some property that allows their intri... | [['i', 'review', 'the', 'current', 'state', 'of', 'determinations', 'of', 'the', 'hubble', 'constant', 'which', 'gives', 'the', 'length', 'scale', 'of', 'the', 'universe', 'by', 'relating', 'the', 'expansion', 'velocity', 'of', 'objects', 'to', 'their', 'distance', 'there', 'are', 'two', 'broad', 'categories', 'of', 'm... | [-0.08856745114654878, 0.09938102428590492, -0.0754278059258073, 0.06336734557352995, -0.10143572977252023, -0.08878215340395537, 0.03218984786824121, 0.35525702798897224, -0.24960728290156936, -0.3709059752532685, 0.1159516945530722, -0.2699316302074157, -0.023899762257538242, 0.2315394927029287, -0.039724734491000904... |
709.3925 | Homotopy nilpotent groups | We study the connection between the Goodwillie tower of the identity and the
lower central series of the loop group on connected spaces. We define the
simplicial theory of homotopy n-nilpotent groups. This notion interpolates
between infinite loop spaces and loop spaces. We prove that the set-valued
algebraic theory ... | math.AT | we study the connection between the goodwillie tower of the identity and the lower central series of the loop group on connected spaces we define the simplicial theory of homotopy nnilpotent groups this notion interpolates between infinite loop spaces and loop spaces we prove that the setvalued algebraic theory obtaine... | [['we', 'study', 'the', 'connection', 'between', 'the', 'goodwillie', 'tower', 'of', 'the', 'identity', 'and', 'the', 'lower', 'central', 'series', 'of', 'the', 'loop', 'group', 'on', 'connected', 'spaces', 'we', 'define', 'the', 'simplicial', 'theory', 'of', 'homotopy', 'nnilpotent', 'groups', 'this', 'notion', 'inter... | [-0.20964181716950175, 0.12702275866127394, -0.12845404315343562, 0.14069943544776872, -0.07909808284107675, -0.08508627836968988, 0.03629991092268338, 0.34337500892975864, -0.3563407757814894, -0.20651327226152447, 0.0708385051037383, -0.21388859094734838, -0.16608087632785293, 0.15427917043772585, -0.1564752735331298... |
709.3926 | Radiation of photons in process of charge particle volume reflection in
bent single crystal | New type of radiation in crystals is predicted and investigated in computer
simulation. It is shown that process of volume reflection of electrons and
positrons in bent crystals is accomplished with high-power radiation of
photons. Volume reflection radiation has intensity comparable with known
channeling radiation, ... | physics.acc-ph | new type of radiation in crystals is predicted and investigated in computer simulation it is shown that process of volume reflection of electrons and positrons in bent crystals is accomplished with highpower radiation of photons volume reflection radiation has intensity comparable with known channeling radiation but it... | [['new', 'type', 'of', 'radiation', 'in', 'crystals', 'is', 'predicted', 'and', 'investigated', 'in', 'computer', 'simulation', 'it', 'is', 'shown', 'that', 'process', 'of', 'volume', 'reflection', 'of', 'electrons', 'and', 'positrons', 'in', 'bent', 'crystals', 'is', 'accomplished', 'with', 'highpower', 'radiation', '... | [-0.07256838329908222, 0.24968868603113376, -0.046888631296484434, 0.06994744077455337, -0.033056507907705764, -0.15238984609788206, -0.034900169803646124, 0.43964880694673486, -0.21266685259107448, -0.34722843814692267, 0.0020040997817525512, -0.3349422988009779, 0.006267548130493458, 0.27770327929844313, 0.0019049926... |
709.3927 | Exact relationship between the entanglement entropies of XY and quantum
Ising chains | We consider two prototypical quantum models, the spin-1/2 XY chain and the
quantum Ising chain and study their entanglement entropy, S(l,L), of blocks of
l spins in homogeneous or inhomogeneous systems of length L. By using two
different approaches, free-fermion techniques and perturbational expansion, an
exact relat... | cond-mat.stat-mech quant-ph | we consider two prototypical quantum models the spin12 xy chain and the quantum ising chain and study their entanglement entropy sll of blocks of l spins in homogeneous or inhomogeneous systems of length l by using two different approaches freefermion techniques and perturbational expansion an exact relationship betwee... | [['we', 'consider', 'two', 'prototypical', 'quantum', 'models', 'the', 'spin12', 'xy', 'chain', 'and', 'the', 'quantum', 'ising', 'chain', 'and', 'study', 'their', 'entanglement', 'entropy', 'sll', 'of', 'blocks', 'of', 'l', 'spins', 'in', 'homogeneous', 'or', 'inhomogeneous', 'systems', 'of', 'length', 'l', 'by', 'usi... | [-0.18021056494779056, 0.19594357631366519, -0.013756688270303939, 0.0850196425182124, 0.02387552858951191, -0.22339211020411717, 0.03095359183369308, 0.3532041709456179, -0.26876653513560694, -0.2294627057776476, 0.05409927442540518, -0.32430950610174075, -0.09944908986540718, 0.15206060322363757, 0.08647391364599268,... |
709.3928 | On tameness and growth conditions | We study discrete subsets of C^d, relating "tameness" with growth conditions.
| math.CV | we study discrete subsets of cd relating tameness with growth conditions | [['we', 'study', 'discrete', 'subsets', 'of', 'cd', 'relating', 'tameness', 'with', 'growth', 'conditions']] | [-0.13552648438648743, 0.04526902506635948, -0.10588478195396336, 0.01598846031860872, -0.08896033023484051, -0.10343182036145167, 0.0025109634681774132, 0.3682574741119011, -0.28790020739490335, -0.1748411191458052, 0.15421197076582097, -0.20751022682948547, -0.1372802569107576, 0.13204895256256516, -0.168646845119920... |
709.3929 | On Meromorphic Functions which are Brody Curves | We discuss meromorphic functions on the complex plane which are Brody curves
regarded as holomorphic maps to P_1, i.e., which have bounded spherical
derivative.
| math.CV | we discuss meromorphic functions on the complex plane which are brody curves regarded as holomorphic maps to p_1 ie which have bounded spherical derivative | [['we', 'discuss', 'meromorphic', 'functions', 'on', 'the', 'complex', 'plane', 'which', 'are', 'brody', 'curves', 'regarded', 'as', 'holomorphic', 'maps', 'to', 'p_1', 'ie', 'which', 'have', 'bounded', 'spherical', 'derivative']] | [-0.18832413076112667, 0.035789214074611664, -0.07845698601158801, 0.1415542347046236, -0.14488092749767625, -0.11052391538396478, -0.06868300610221922, 0.3840484047929446, -0.2954153019624452, -0.15253827441483736, 0.11116246027328695, -0.264162100191849, -0.20438900458005568, 0.27097917860373855, -0.08740017902406787... |
709.393 | On supersymmetric $D6$-$\bar D 6$ systems with magnetic fields | We study systems of $D6$ and $\bar D 6$ branes with non zero world-volume
magnetic fields in the weak coupling limit. We find two configurations for
which the conditions for absence of tachyons in the spectra coincide exactly
with those found in the low energy effective theory approach, for the systems
to preserve 1/... | hep-th | we study systems of d6 and bar d 6 branes with non zero worldvolume magnetic fields in the weak coupling limit we find two configurations for which the conditions for absence of tachyons in the spectra coincide exactly with those found in the low energy effective theory approach for the systems to preserve 18 of the su... | [['we', 'study', 'systems', 'of', 'd6', 'and', 'bar', 'd', '6', 'branes', 'with', 'non', 'zero', 'worldvolume', 'magnetic', 'fields', 'in', 'the', 'weak', 'coupling', 'limit', 'we', 'find', 'two', 'configurations', 'for', 'which', 'the', 'conditions', 'for', 'absence', 'of', 'tachyons', 'in', 'the', 'spectra', 'coincid... | [-0.1896134981178437, 0.12461320235161111, -0.03994242793716559, 0.09957444667816162, -0.0001095692450353117, -0.14033681737621212, 0.010625100268818508, 0.29191334009239517, -0.18527110536686248, -0.3173207426702397, 0.09327530949505874, -0.2703939180527986, -0.1376976101504018, 0.14267097446308644, 0.0056182650021380... |
709.3931 | Kernel methods for in silico chemogenomics | Predicting interactions between small molecules and proteins is a crucial
ingredient of the drug discovery process. In particular, accurate predictive
models are increasingly used to preselect potential lead compounds from large
molecule databases, or to screen for side-effects. While classical in silico
approaches f... | q-bio.QM | predicting interactions between small molecules and proteins is a crucial ingredient of the drug discovery process in particular accurate predictive models are increasingly used to preselect potential lead compounds from large molecule databases or to screen for sideeffects while classical in silico approaches focus on... | [['predicting', 'interactions', 'between', 'small', 'molecules', 'and', 'proteins', 'is', 'a', 'crucial', 'ingredient', 'of', 'the', 'drug', 'discovery', 'process', 'in', 'particular', 'accurate', 'predictive', 'models', 'are', 'increasingly', 'used', 'to', 'preselect', 'potential', 'lead', 'compounds', 'from', 'large'... | [-0.06661098000533398, 0.06110322170500313, -0.01858385756420302, 0.06646765140127289, -0.039487584272489676, -0.1738246268097071, 0.09558114898297185, 0.39264232406933464, -0.21567792080402856, -0.3226515029767348, 0.008244601250724725, -0.28661871787300053, -0.18345993754431425, 0.1845767227688714, -0.056820959059311... |
709.3932 | Coexisting stochastic and coherence resonance in a mean-field dynamo
model for Earth's magnetic field reversals | Using a spherical symmetric mean field alpha^2-dynamo model for Earth's
magnetic field reversals, we show the coexistence of the noise-induced
phenomena coherence resonance and stochastic resonance. Stochastic resonance
has been recently invoked to explain the 100 kyr periodicity in the
distribution of the residence ... | astro-ph nlin.CD physics.geo-ph | using a spherical symmetric mean field alpha2dynamo model for earths magnetic field reversals we show the coexistence of the noiseinduced phenomena coherence resonance and stochastic resonance stochastic resonance has been recently invoked to explain the 100 kyr periodicity in the distribution of the residence time bet... | [['using', 'a', 'spherical', 'symmetric', 'mean', 'field', 'alpha2dynamo', 'model', 'for', 'earths', 'magnetic', 'field', 'reversals', 'we', 'show', 'the', 'coexistence', 'of', 'the', 'noiseinduced', 'phenomena', 'coherence', 'resonance', 'and', 'stochastic', 'resonance', 'stochastic', 'resonance', 'has', 'been', 'rece... | [-0.12877033952036468, 0.20853965905616464, -0.09084530020355368, 0.11347168532918896, -0.06241746999971245, -0.06644613060432122, 0.019541491815091475, 0.34506568537377147, -0.26951032195685676, -0.3557312140777788, 0.08803712225736766, -0.22233738236236208, -0.06913401154135658, 0.19831816568330396, 0.020403294818369... |
709.3933 | Understanding the shape of the halo-mass and galaxy-mass
cross-correlation functions | We use the Millennium Simulation to measure the cross-correlation between
halo centres and mass (or equivalently the average density profiles of dark
haloes) in a LCDM cosmology. We present results for radii in the range 10 kpc/h
< r < 30 Mpc/h for halo masses in the range 4e10 Msol/h < M200 < 4e14 Msol/h.
Both at z=... | astro-ph | we use the millennium simulation to measure the crosscorrelation between halo centres and mass or equivalently the average density profiles of dark haloes in a lcdm cosmology we present results for radii in the range 10 kpch r 30 mpch for halo masses in the range 4e10 msolh m200 4e14 msolh both at z0 and at z076 these ... | [['we', 'use', 'the', 'millennium', 'simulation', 'to', 'measure', 'the', 'crosscorrelation', 'between', 'halo', 'centres', 'and', 'mass', 'or', 'equivalently', 'the', 'average', 'density', 'profiles', 'of', 'dark', 'haloes', 'in', 'a', 'lcdm', 'cosmology', 'we', 'present', 'results', 'for', 'radii', 'in', 'the', 'rang... | [-0.044548214720695783, 0.08478630483640652, -0.11359420543955416, 0.1504424439774354, -0.07340507622491836, -0.05474703882388664, -0.01734881596216424, 0.41601403095006373, -0.18064188713020685, -0.39577481208333487, 0.049310105524703184, -0.2972683322361924, -0.05291451554540456, 0.21225650921579825, 0.04504038196064... |
709.3934 | Electromagnetic Field Simulations of Isolated and Periodic 3D Photomask
Patterns | We present rigorous 3D EMF simulations of isolated features on photomasks
using a newly developed finite-element method. We report on the current status
of the finite-element solver JCMsuite, incorporating higher-order edge
elements, adaptive refinement methods, and fast solution algorithms. We
demonstrate that rigor... | physics.optics physics.comp-ph | we present rigorous 3d emf simulations of isolated features on photomasks using a newly developed finiteelement method we report on the current status of the finiteelement solver jcmsuite incorporating higherorder edge elements adaptive refinement methods and fast solution algorithms we demonstrate that rigorous and ac... | [['we', 'present', 'rigorous', '3d', 'emf', 'simulations', 'of', 'isolated', 'features', 'on', 'photomasks', 'using', 'a', 'newly', 'developed', 'finiteelement', 'method', 'we', 'report', 'on', 'the', 'current', 'status', 'of', 'the', 'finiteelement', 'solver', 'jcmsuite', 'incorporating', 'higherorder', 'edge', 'eleme... | [-0.08076805310722973, -0.016376145842618175, -0.11088466404138932, 0.04123604392765888, -0.07868156919721514, -0.11250307381020061, 0.07562147554542337, 0.443525009815182, -0.23553526843232767, -0.32901274733511465, 0.10112177493449832, -0.2870461201295257, -0.15370403569457786, 0.24798123529180885, -0.036579623003490... |
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