id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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708.3649 | Relationship Between Bicomplex Generalized Analytic Functions and
Solutions of the Complexified Schr\"odinger Equation | Using three different representations of the bicomplex numbers $T\cong
Cl_{C}(1,0) \cong Cl_{C}(0,1)$, which is a commutative ring with zero divisors
defined by $T={w_0+w_1 {i_1}+w_2{i_2}+w_3 {j} | w_0,w_1,w_2,w_3 \in{R}}$ where
${i_1^{2}}=-1, {i_2^{2}}=-1, {j^{2}}=1 and {i_1}{i_2}={j}={i_2}{i_1}$, we
construct three... | math.CV | using three different representations of the bicomplex numbers tcong cl_c10 cong cl_c01 which is a commutative ring with zero divisors defined by tw_0w_1 i_1w_2i_2w_3 j w_0w_1w_2w_3 inr where i_121 i_221 j21 and i_1i_2ji_2i_1 we construct three classes of bicomplex pseudoanalytic functions in particular we obtain some ... | [['using', 'three', 'different', 'representations', 'of', 'the', 'bicomplex', 'numbers', 'tcong', 'cl_c10', 'cong', 'cl_c01', 'which', 'is', 'a', 'commutative', 'ring', 'with', 'zero', 'divisors', 'defined', 'by', 'tw_0w_1', 'i_1w_2i_2w_3', 'j', 'w_0w_1w_2w_3', 'inr', 'where', 'i_121', 'i_221', 'j21', 'and', 'i_1i_2ji_... | [-0.20856053634391478, 0.051048850275886556, -0.06251943844060102, 0.05832110123107365, -0.1249124603617626, -0.15273905892390757, -0.0717564585172416, 0.2829208302777261, -0.3002287958903859, -0.18468839285584787, 0.10600387161054338, -0.3064234192968191, -0.17872831779920187, 0.18383951513678767, -0.02378513435833156... |
708.365 | Improved Limits on the Lepton-Flavor Violating Decays tau- --> l-l+l- | A search for the neutrinoless, lepton-flavor violating decay of the tau
lepton into three charged leptons has been performed using 376 fb^{-1} of data
collected at an e^+e^- center-of-mass energy around 10.58 GeV with the BaBar
detector at the PEP-II storage rings. In all six decay modes considered, the
numbers of ev... | hep-ex | a search for the neutrinoless leptonflavor violating decay of the tau lepton into three charged leptons has been performed using 376 fb1 of data collected at an ee centerofmass energy around 1058 gev with the babar detector at the pepii storage rings in all six decay modes considered the numbers of events found in data... | [['a', 'search', 'for', 'the', 'neutrinoless', 'leptonflavor', 'violating', 'decay', 'of', 'the', 'tau', 'lepton', 'into', 'three', 'charged', 'leptons', 'has', 'been', 'performed', 'using', '376', 'fb1', 'of', 'data', 'collected', 'at', 'an', 'ee', 'centerofmass', 'energy', 'around', '1058', 'gev', 'with', 'the', 'bab... | [-0.11931884204570935, 0.21494034737443604, -0.0014638627961843828, 0.12014533925942983, 0.016658857694673766, -0.11035693231734293, 0.07172455711738218, 0.2820722444831759, -0.1411537030369892, -0.35505735744498196, 0.023367718606303104, -0.4412261484709533, 0.1732236822194691, 0.2028093692976274, 0.12528259305967182,... |
708.3651 | Magnetic and thermal properties of the S = 1/2 zig-zag spin-chain
compound In2VO5 | Static magnetic susceptibility \chi, ac susceptibility \chi_{ac} and specific
heat C versus temperature T measurements on polycrystalline samples of In2VO5
and \chi and C versus T measurements on the isostructural, nonmagnetic compound
In2TiO5 are reported. A Curie-Wiess fit to the \chi(T) data above 175 K for
In2VO5... | cond-mat.str-el cond-mat.mtrl-sci | static magnetic susceptibility chi ac susceptibility chi_ac and specific heat c versus temperature t measurements on polycrystalline samples of in2vo5 and chi and c versus t measurements on the isostructural nonmagnetic compound in2tio5 are reported a curiewiess fit to the chit data above 175 k for in2vo5 indicates fer... | [['static', 'magnetic', 'susceptibility', 'chi', 'ac', 'susceptibility', 'chi_ac', 'and', 'specific', 'heat', 'c', 'versus', 'temperature', 't', 'measurements', 'on', 'polycrystalline', 'samples', 'of', 'in2vo5', 'and', 'chi', 'and', 'c', 'versus', 't', 'measurements', 'on', 'the', 'isostructural', 'nonmagnetic', 'comp... | [-0.18216603482446844, 0.23812532797577687, -0.017773088037904294, 0.019031132115489992, -0.06068463256845923, -0.1736574775749008, 0.16421666304966073, 0.34129140886882836, -0.24718857414688897, -0.3516798146381116, 0.0360865736744703, -0.40675708377997133, 0.022823773381783, 0.2070337697883083, 0.08926024195050616, -... |
708.3652 | Extensions in FormCalc 5.3 | We present a new tool for editing Feynman diagrams as well as several
extensions in version 5.3 of the package FormCalc for the calculation of
Feynman diagrams.
| hep-ph | we present a new tool for editing feynman diagrams as well as several extensions in version 53 of the package formcalc for the calculation of feynman diagrams | [['we', 'present', 'a', 'new', 'tool', 'for', 'editing', 'feynman', 'diagrams', 'as', 'well', 'as', 'several', 'extensions', 'in', 'version', '53', 'of', 'the', 'package', 'formcalc', 'for', 'the', 'calculation', 'of', 'feynman', 'diagrams']] | [-0.02797894614438216, 0.046583409421145916, -0.12398328704552518, 0.18665111562478598, -0.10502097424533632, -0.07017629150370205, 0.06250002624087587, 0.35108992319416116, -0.19382225377140222, -0.392147783190012, 0.09521900630918229, -0.250965202520429, -0.17892403900623322, 0.30340538173913956, -0.01987205207761791... |
708.3653 | Thermonuclear Flame Spreading on Rapidly Spinning Neutron Stars:
Indications of the Coriolis Force? | Millisecond period brightness oscillations during the intensity rise of
thermonuclear X-ray bursts are likely caused by an azimuthally asymmetric,
expanding burning region on the stellar surface. The time evolution of the
oscillation amplitude during the intensity rise encodes information on how the
thermonuclear fla... | astro-ph | millisecond period brightness oscillations during the intensity rise of thermonuclear xray bursts are likely caused by an azimuthally asymmetric expanding burning region on the stellar surface the time evolution of the oscillation amplitude during the intensity rise encodes information on how the thermonuclear flames s... | [['millisecond', 'period', 'brightness', 'oscillations', 'during', 'the', 'intensity', 'rise', 'of', 'thermonuclear', 'xray', 'bursts', 'are', 'likely', 'caused', 'by', 'an', 'azimuthally', 'asymmetric', 'expanding', 'burning', 'region', 'on', 'the', 'stellar', 'surface', 'the', 'time', 'evolution', 'of', 'the', 'oscil... | [-0.08224343162634083, 0.20029918450077153, -0.11001491873852305, 0.10565731662072475, -0.084392348535963, -0.04989892753294191, 0.027973674575017916, 0.3892992421481255, -0.2542140059374474, -0.32358232479844545, 0.07190054957251492, -0.24414336355151356, -0.13947315769560314, 0.2616414665257105, -0.040117524315389126... |
708.3654 | Proof of Lemma 6.3 in ``The crossing number of $K_{4,n}$ on the torus
and the Klein bottle" | We found that Lemma 6.3 in the paper ``The crossing number of $K_{4,n}$ on
the torus and the Klein bottle" is wrong.
| math.CO | we found that lemma 63 in the paper the crossing number of k_4n on the torus and the klein bottle is wrong | [['we', 'found', 'that', 'lemma', '63', 'in', 'the', 'paper', 'the', 'crossing', 'number', 'of', 'k_4n', 'on', 'the', 'torus', 'and', 'the', 'klein', 'bottle', 'is', 'wrong']] | [-0.1702426690608263, 0.07341377851775005, -0.054563880676314944, 0.06932557607623971, -0.08914832362816447, -0.09072951706392425, 0.11069955646304325, 0.2813817762015831, -0.195253483773697, -0.36399129689449355, 0.1017863533093727, -0.2824182603619106, -0.198039175676448, 0.25360729314741637, -0.13700876021314234, -0... |
708.3655 | Gradient regularity for elliptic equations in the Heisenberg Group | We give dimension-free regularity conditions for a class of possibly
degenerate sub-elliptic equations in the Heisenberg group exhibiting
super-quadratic growth in the horizontal gradient; this solves an issue raised
by Manfredi & Mingione (Math. Ann. 2007) where only dimension dependent bounds
for the growth exponen... | math.AP math.DG | we give dimensionfree regularity conditions for a class of possibly degenerate subelliptic equations in the heisenberg group exhibiting superquadratic growth in the horizontal gradient this solves an issue raised by manfredi mingione math ann 2007 where only dimension dependent bounds for the growth exponent are given ... | [['we', 'give', 'dimensionfree', 'regularity', 'conditions', 'for', 'a', 'class', 'of', 'possibly', 'degenerate', 'subelliptic', 'equations', 'in', 'the', 'heisenberg', 'group', 'exhibiting', 'superquadratic', 'growth', 'in', 'the', 'horizontal', 'gradient', 'this', 'solves', 'an', 'issue', 'raised', 'by', 'manfredi', ... | [-0.09749449812562914, 0.04523559069430693, -0.04400990402547421, 0.07824043416291136, -0.13613947561715722, -0.14626734134565283, -0.004109352469685247, 0.2838342957576359, -0.28435135843440684, -0.2471272756143675, 0.17071350711524824, -0.2556477141765213, -0.12233763188123703, 0.2447992499422777, -0.1305081256749955... |
708.3656 | Memoirs of an Early String Theorist | I worked on String Theory over a period of five years during the First String
Era, the most intellectually satisfying years of my scientific life. One of the
early prospectors in the String Theory Mine, I was fortunate enough to
contribute to the birth of this subject, which retains after these many years,
its magica... | hep-th | i worked on string theory over a period of five years during the first string era the most intellectually satisfying years of my scientific life one of the early prospectors in the string theory mine i was fortunate enough to contribute to the birth of this subject which retains after these many years its magical hold ... | [['i', 'worked', 'on', 'string', 'theory', 'over', 'a', 'period', 'of', 'five', 'years', 'during', 'the', 'first', 'string', 'era', 'the', 'most', 'intellectually', 'satisfying', 'years', 'of', 'my', 'scientific', 'life', 'one', 'of', 'the', 'early', 'prospectors', 'in', 'the', 'string', 'theory', 'mine', 'i', 'was', '... | [-0.06670984220462012, 0.12368270104415104, -0.10690631572401425, 0.06826171310061253, -0.0861700781178279, -0.09777319030530873, 0.035040649581608956, 0.2944162615909352, -0.1854873125643668, -0.29889065828785055, 0.1454474169085352, -0.2847318688529681, -0.11109106251817258, 0.20954456577291253, -0.10862186103753868,... |
708.3657 | Hyperfine spectra of trapped Bosons in optical lattices | We calculate the interaction induced inhomogeneous broadening of spectral
lines in a trapped Bose gas as a function of the depth of a three-dimensional
cubic optical lattice. As observed in recent experiments, we find that the
terraced "wedding-cake" structure of Mott plateaus splits the spectrum into a
series of dis... | cond-mat.other | we calculate the interaction induced inhomogeneous broadening of spectral lines in a trapped bose gas as a function of the depth of a threedimensional cubic optical lattice as observed in recent experiments we find that the terraced weddingcake structure of mott plateaus splits the spectrum into a series of discrete pe... | [['we', 'calculate', 'the', 'interaction', 'induced', 'inhomogeneous', 'broadening', 'of', 'spectral', 'lines', 'in', 'a', 'trapped', 'bose', 'gas', 'as', 'a', 'function', 'of', 'the', 'depth', 'of', 'a', 'threedimensional', 'cubic', 'optical', 'lattice', 'as', 'observed', 'in', 'recent', 'experiments', 'we', 'find', '... | [-0.15427615755694346, 0.17389982152515307, -0.08319839119063452, 0.06429137501608914, 0.0094065255103394, -0.11775412275575292, 0.0253046583593226, 0.4191182143986225, -0.23558075558871794, -0.25875773853980577, 0.04321781947361066, -0.31349222163836926, -0.10350635658519772, 0.15485765177231187, 0.06216544102584848, ... |
708.3658 | Structured Near-Optimal Channel-Adapted Quantum Error Correction | We present a class of numerical algorithms which adapt a quantum error
correction scheme to a channel model. Given an encoding and a channel model, it
was previously shown that the quantum operation that maximizes the average
entanglement fidelity may be calculated by a semidefinite program (SDP), which
is a convex o... | quant-ph | we present a class of numerical algorithms which adapt a quantum error correction scheme to a channel model given an encoding and a channel model it was previously shown that the quantum operation that maximizes the average entanglement fidelity may be calculated by a semidefinite program sdp which is a convex optimiza... | [['we', 'present', 'a', 'class', 'of', 'numerical', 'algorithms', 'which', 'adapt', 'a', 'quantum', 'error', 'correction', 'scheme', 'to', 'a', 'channel', 'model', 'given', 'an', 'encoding', 'and', 'a', 'channel', 'model', 'it', 'was', 'previously', 'shown', 'that', 'the', 'quantum', 'operation', 'that', 'maximizes', '... | [-0.14081462860086413, 0.023389609283951455, -0.11232884151202843, 0.09051939029039997, -0.039266853089115226, -0.2611389420016256, 0.08391922425051548, 0.3900324176380733, -0.3097684480971132, -0.2793879693346028, 0.18996186981579863, -0.19385488387337305, -0.17240953144636637, 0.19141461964717654, -0.1299899434390709... |
708.3659 | Asymptotics of QCD traveling waves with fluctuations and running
coupling effects | Extending independently the Balitsky-Kovchegov (BK) equation to running
coupling or to fluctuation effects due to Pomeron loops is known to lead in
both cases to qualitative changes of the traveling-wave asymptotic solutions.
In this paper we study the extension of the forward BK equation, including both
running coup... | hep-ph | extending independently the balitskykovchegov bk equation to running coupling or to fluctuation effects due to pomeron loops is known to lead in both cases to qualitative changes of the travelingwave asymptotic solutions in this paper we study the extension of the forward bk equation including both running coupling and... | [['extending', 'independently', 'the', 'balitskykovchegov', 'bk', 'equation', 'to', 'running', 'coupling', 'or', 'to', 'fluctuation', 'effects', 'due', 'to', 'pomeron', 'loops', 'is', 'known', 'to', 'lead', 'in', 'both', 'cases', 'to', 'qualitative', 'changes', 'of', 'the', 'travelingwave', 'asymptotic', 'solutions', '... | [-0.1484236407244729, 0.06929348643894333, -0.15314744093228835, 0.10456684347544168, -0.10367163039454436, -0.09672248383946214, 0.0402136776781943, 0.2779754623770714, -0.25296218532477377, -0.3049249534268637, 0.08858016175784271, -0.28240250495287617, -0.10072881964073088, 0.13762364151409348, 0.031166647306039325,... |
708.366 | The nature of the dense core population in the Pipe Nebula: A survey of
NH3, CCS, and HC5N molecular line emission | Recent extinction studies of the Pipe Nebula (d=130 pc) reveal many cores
spanning a range in mass from 0.2 to 20.4 Msun. These dense cores were
identified via their high extinction and comprise a starless population in a
very early stage of development. Here we present a survey of NH3 (1,1), NH3
(2,2), CCS (2_1,1_0)... | astro-ph | recent extinction studies of the pipe nebula d130 pc reveal many cores spanning a range in mass from 02 to 204 msun these dense cores were identified via their high extinction and comprise a starless population in a very early stage of development here we present a survey of nh3 11 nh3 22 ccs 2_11_0 and hc5n 98 emissio... | [['recent', 'extinction', 'studies', 'of', 'the', 'pipe', 'nebula', 'd130', 'pc', 'reveal', 'many', 'cores', 'spanning', 'a', 'range', 'in', 'mass', 'from', '02', 'to', '204', 'msun', 'these', 'dense', 'cores', 'were', 'identified', 'via', 'their', 'high', 'extinction', 'and', 'comprise', 'a', 'starless', 'population',... | [-0.06927258125111523, 0.14064147206063493, 0.003343604768575855, 0.043026516202281324, -0.005191060765862985, -0.015944047874541838, 0.05971741808719153, 0.45673246545962587, -0.1308401509042822, -0.3643795653542345, 0.09956005708379455, -0.250658894769934, -0.003969536634891244, 0.11836738579197202, 0.015109569718249... |
708.3661 | On Kalai's conjectures concerning centrally symmetric polytopes | In 1989 Kalai stated the three conjectures A, B, C of increasing strength
concerning face numbers of centrally symmetric convex polytopes. The weakest
conjecture, A, became known as the ``$3^d$-conjecture''. It is well-known that
the three conjectures hold in dimensions d \leq 3. We show that in dimension 4
only conj... | math.CO math.MG | in 1989 kalai stated the three conjectures a b c of increasing strength concerning face numbers of centrally symmetric convex polytopes the weakest conjecture a became known as the 3dconjecture it is wellknown that the three conjectures hold in dimensions d leq 3 we show that in dimension 4 only conjectures a and b are... | [['in', '1989', 'kalai', 'stated', 'the', 'three', 'conjectures', 'a', 'b', 'c', 'of', 'increasing', 'strength', 'concerning', 'face', 'numbers', 'of', 'centrally', 'symmetric', 'convex', 'polytopes', 'the', 'weakest', 'conjecture', 'a', 'became', 'known', 'as', 'the', '3dconjecture', 'it', 'is', 'wellknown', 'that', '... | [-0.17841410095493, 0.10635004055996736, -0.009414524547755718, 0.07838383287967493, 0.01314243469387293, -0.2751886728219688, 0.007319691851735115, 0.32493974899252254, -0.2192661381388704, -0.2686752768481771, 0.11038954020167391, -0.26222999233131605, -0.15509552125508586, 0.17355168217482667, -0.10613783520956833, ... |
708.3662 | On a conjecture of Hacon and McKernan in dimension three | We prove that there exists a universal constant $r_3$ such that if $X$ is a
smooth projective threefold over $\mathbb{C}$ with non-negative Kodaira
dimension, then the linear system $|r K_X|$ admits a fibration that is
birational to the Iitaka fibration as soon as $r \geq r_3$ and sufficiently
divisible. This gives a... | math.AG | we prove that there exists a universal constant r_3 such that if x is a smooth projective threefold over mathbbc with nonnegative kodaira dimension then the linear system r k_x admits a fibration that is birational to the iitaka fibration as soon as r geq r_3 and sufficiently divisible this gives an affirmative answer ... | [['we', 'prove', 'that', 'there', 'exists', 'a', 'universal', 'constant', 'r_3', 'such', 'that', 'if', 'x', 'is', 'a', 'smooth', 'projective', 'threefold', 'over', 'mathbbc', 'with', 'nonnegative', 'kodaira', 'dimension', 'then', 'the', 'linear', 'system', 'r', 'k_x', 'admits', 'a', 'fibration', 'that', 'is', 'biration... | [-0.21274348975275642, 0.009666182236287568, -0.08075858363881708, 0.05187874354451196, -0.07745225533726625, -0.29531950161908754, -0.02559982478414895, 0.3476448573987, -0.3029112265678123, -0.148664150579134, 0.08144394130067667, -0.2759081020281883, -0.1652061217231676, 0.1979795023566112, -0.18298157039680518, -0.... |
708.3663 | How a liquid becomes a glass both on cooling and on heating | The onset of structural arrest and glass formation in a concentrated
suspension of silica nanoparticles in a water-lutidine binary mixture near its
consolute point is studied by exploiting the near-critical fluid degrees of
freedom to control the strength of an attraction between particles and
multispeckle x-ray phot... | cond-mat.soft | the onset of structural arrest and glass formation in a concentrated suspension of silica nanoparticles in a waterlutidine binary mixture near its consolute point is studied by exploiting the nearcritical fluid degrees of freedom to control the strength of an attraction between particles and multispeckle xray photon co... | [['the', 'onset', 'of', 'structural', 'arrest', 'and', 'glass', 'formation', 'in', 'a', 'concentrated', 'suspension', 'of', 'silica', 'nanoparticles', 'in', 'a', 'waterlutidine', 'binary', 'mixture', 'near', 'its', 'consolute', 'point', 'is', 'studied', 'by', 'exploiting', 'the', 'nearcritical', 'fluid', 'degrees', 'of... | [-0.12983789834681722, 0.25656890429769796, -0.11050494531269318, 0.02191596615372137, 0.02555787049766098, -0.14691186128627687, 0.05617185710580088, 0.38337207277571517, -0.22535831057244823, -0.2707330188048737, 0.05273589133728473, -0.33789107390191586, -0.12342845526568237, 0.07886679234382298, 0.03404913831147409... |
708.3664 | Commutator maps, measure preservation, and T-systems | Let G be a finite simple group. We show that the commutator map $a : G \times
G \to G$ is almost equidistributed as the order of G goes to infinity. This
somewhat surprising result has many applications. It shows that for a subset X
of G we have $a^{-1}(X)/|G|^2 = |X|/|G| + o(1)$, namely $a$ is almost measure
preserv... | math.GR | let g be a finite simple group we show that the commutator map a g times g to g is almost equidistributed as the order of g goes to infinity this somewhat surprising result has many applications it shows that for a subset x of g we have a1xg2 xg o1 namely a is almost measure preserving from this we deduce that almost a... | [['let', 'g', 'be', 'a', 'finite', 'simple', 'group', 'we', 'show', 'that', 'the', 'commutator', 'map', 'a', 'g', 'times', 'g', 'to', 'g', 'is', 'almost', 'equidistributed', 'as', 'the', 'order', 'of', 'g', 'goes', 'to', 'infinity', 'this', 'somewhat', 'surprising', 'result', 'has', 'many', 'applications', 'it', 'shows... | [-0.16513899022994347, 0.10695555700327862, -0.11749923195586437, 0.019259790241991103, -0.10195643690442949, -0.11947194073876047, 0.03392936972633117, 0.3652535533494871, -0.266564847412284, -0.28270205341966237, 0.06722038173507146, -0.2894898945773773, -0.1578503862703031, 0.2129581118134236, -0.12209814205539948, ... |
708.3665 | Symmetry of Lepton Mixing | Neutrino mixing is studied from a symmetry perspective, both bottom-up and
top-down. In the bottom-up approach, we start from the tri-bimaximal mixing, or
one of its three partial patterns, and construct a list of horizontal symmetry
groups capable of reproducing the mixng without adjustment of parameters. This
list,... | hep-ph | neutrino mixing is studied from a symmetry perspective both bottomup and topdown in the bottomup approach we start from the tribimaximal mixing or one of its three partial patterns and construct a list of horizontal symmetry groups capable of reproducing the mixng without adjustment of parameters this list labeled by a... | [['neutrino', 'mixing', 'is', 'studied', 'from', 'a', 'symmetry', 'perspective', 'both', 'bottomup', 'and', 'topdown', 'in', 'the', 'bottomup', 'approach', 'we', 'start', 'from', 'the', 'tribimaximal', 'mixing', 'or', 'one', 'of', 'its', 'three', 'partial', 'patterns', 'and', 'construct', 'a', 'list', 'of', 'horizontal... | [-0.08434613322561876, 0.20378343185900002, -0.07987055392182282, 0.04960877700168497, -0.09510846512804505, -0.15820418697877836, 0.07521260071204591, 0.3854760295562162, -0.2946353518583577, -0.2784034856381819, 0.08678496316100208, -0.24545469823940338, -0.15837975580934863, 0.11850539887437725, -0.01935073195331026... |
708.3666 | Jahn-Teller effect versus Hund's rule coupling in C60N- | We propose variational states for the ground state and the low-energy
collective rotator excitations in negatively charged C60N- ions (N=1...5). The
approach includes the linear electron-phonon coupling and the Coulomb
interaction on the same level. The electron-phonon coupling is treated within
the effective mode ap... | cond-mat.supr-con | we propose variational states for the ground state and the lowenergy collective rotator excitations in negatively charged c60n ions n15 the approach includes the linear electronphonon coupling and the coulomb interaction on the same level the electronphonon coupling is treated within the effective mode approximation em... | [['we', 'propose', 'variational', 'states', 'for', 'the', 'ground', 'state', 'and', 'the', 'lowenergy', 'collective', 'rotator', 'excitations', 'in', 'negatively', 'charged', 'c60n', 'ions', 'n15', 'the', 'approach', 'includes', 'the', 'linear', 'electronphonon', 'coupling', 'and', 'the', 'coulomb', 'interaction', 'on'... | [-0.15533072049233684, 0.1885832005759935, -0.015939769121663023, 0.09103459418111015, -0.03498838527917138, -0.13818736977366455, 0.09401094748776544, 0.3532514930702746, -0.23561223252046923, -0.2818869465220444, -0.02723312208965783, -0.28337998819410537, -0.06302317711136614, 0.11472837467401943, 0.0873717707420130... |
708.3667 | A note on the convergence of renewal and regenerative processes to a
Brownian bridge | The standard functional central limit theorem for a renewal process with
finite mean and variance, results in a Brownian motion limit. This note shows
how to obtain a Brownian bridge process by a direct procedure that does not
involve conditioning. Several examples are also considered.
| math.PR | the standard functional central limit theorem for a renewal process with finite mean and variance results in a brownian motion limit this note shows how to obtain a brownian bridge process by a direct procedure that does not involve conditioning several examples are also considered | [['the', 'standard', 'functional', 'central', 'limit', 'theorem', 'for', 'a', 'renewal', 'process', 'with', 'finite', 'mean', 'and', 'variance', 'results', 'in', 'a', 'brownian', 'motion', 'limit', 'this', 'note', 'shows', 'how', 'to', 'obtain', 'a', 'brownian', 'bridge', 'process', 'by', 'a', 'direct', 'procedure', 't... | [-0.030251331047879325, 0.11860821935244732, -0.16247628594024313, 0.09724519254887128, -0.06354469561742412, -0.08947443684770001, 0.11651235289819953, 0.3796036453710662, -0.27390589834087425, -0.25177410220106444, 0.12566530865668837, -0.2339750533302625, -0.16498677778161233, 0.23880980881965821, -0.153095399402081... |
708.3668 | A simple proof of the algebraic version of a conjecture by Vogan | In a recent manuscript, D.Vogan conjectures that four canonical
globalizations of Harish-Chandra modules commute with certain n-cohomology
groups. In this article we prove that Vogan's conjecture holds for one of the
globalizations if and only if it holds for the dual. Using a previously
published result of one of th... | math.RT math.SP | in a recent manuscript dvogan conjectures that four canonical globalizations of harishchandra modules commute with certain ncohomology groups in this article we prove that vogans conjecture holds for one of the globalizations if and only if it holds for the dual using a previously published result of one of the authors... | [['in', 'a', 'recent', 'manuscript', 'dvogan', 'conjectures', 'that', 'four', 'canonical', 'globalizations', 'of', 'harishchandra', 'modules', 'commute', 'with', 'certain', 'ncohomology', 'groups', 'in', 'this', 'article', 'we', 'prove', 'that', 'vogans', 'conjecture', 'holds', 'for', 'one', 'of', 'the', 'globalization... | [-0.16137270122656927, 0.06977285839178983, -0.1151248071623473, 0.07196355947149534, -0.05561262605410507, -0.15898656378061893, 0.00016768934095607083, 0.2925030079957865, -0.28507537487894297, -0.20561924196012757, 0.1008919549469069, -0.20356756264193201, -0.1782676813274841, 0.24057291437159567, -0.164463120471576... |
708.3669 | Band-Gap Engineering of Phononic Crystals: A Computational Survey of
Two-Dimensional Systems | We present graphic results with high-levels of abstraction to desribe the
basic principles and rules of thumb for acoustic or phononic band-gap
engineering. We use these rules for developing an improved machien mount for
damping acoustic vibrations, a phononic lens and a frequency selective filter
in the acoustic reg... | cond-mat.mtrl-sci | we present graphic results with highlevels of abstraction to desribe the basic principles and rules of thumb for acoustic or phononic bandgap engineering we use these rules for developing an improved machien mount for damping acoustic vibrations a phononic lens and a frequency selective filter in the acoustic regime | [['we', 'present', 'graphic', 'results', 'with', 'highlevels', 'of', 'abstraction', 'to', 'desribe', 'the', 'basic', 'principles', 'and', 'rules', 'of', 'thumb', 'for', 'acoustic', 'or', 'phononic', 'bandgap', 'engineering', 'we', 'use', 'these', 'rules', 'for', 'developing', 'an', 'improved', 'machien', 'mount', 'for'... | [-0.12366935114065807, 0.13482993532458445, -0.0390026372090991, -0.0018612181981249403, -0.20577382086776197, -0.14474710988967368, 0.150077062130246, 0.465557926800102, -0.2554254632559605, -0.21708418634564927, 0.09348912523879942, -0.2451475131480644, -0.2019374540783853, 0.252667248477034, -0.0020585418678820133, ... |
708.367 | A covariant entropy conjecture on cosmological dynamical horizon | We here propose a covariant entropy conjecture on cosmological dynamical
horizon. After the formulation of our conjecture, we test its validity in
adiabatically expanding universes with open, flat and closed spatial geometry,
where our conjecture can also be viewed as a cosmological version of the
generalized second ... | hep-th astro-ph gr-qc | we here propose a covariant entropy conjecture on cosmological dynamical horizon after the formulation of our conjecture we test its validity in adiabatically expanding universes with open flat and closed spatial geometry where our conjecture can also be viewed as a cosmological version of the generalized second law of... | [['we', 'here', 'propose', 'a', 'covariant', 'entropy', 'conjecture', 'on', 'cosmological', 'dynamical', 'horizon', 'after', 'the', 'formulation', 'of', 'our', 'conjecture', 'we', 'test', 'its', 'validity', 'in', 'adiabatically', 'expanding', 'universes', 'with', 'open', 'flat', 'and', 'closed', 'spatial', 'geometry', ... | [-0.12826335728212418, 0.10256229629212955, -0.17271208722706674, 0.07047262626155368, -0.07261413657424953, -0.16395478172201383, 0.00749032425184576, 0.2920315836046664, -0.2574008320159507, -0.2508664620086937, 0.10509848952697555, -0.1763917805565486, -0.12248172332479987, 0.17393756077958727, -0.10439735481445238,... |
708.3671 | A Multiwavelength Analysis of the Strong Lensing Cluster RCS
022434-0002.5 at z=0.778 | We present the results of two (101 ks total) Chandra observations of the
z=0.778 optically selected lensing cluster RCS022434-0002.5, along with weak
lensing and dynamical analyses of this object. An X-ray spectrum extracted
within R(2500) (362 h(70)^(-1) kpc) results in an integrated cluster
temperature of 5.1 (+0.9... | astro-ph | we present the results of two 101 ks total chandra observations of the z0778 optically selected lensing cluster rcs02243400025 along with weak lensing and dynamical analyses of this object an xray spectrum extracted within r2500 362 h701 kpc results in an integrated cluster temperature of 51 0905 kev the surface bright... | [['we', 'present', 'the', 'results', 'of', 'two', '101', 'ks', 'total', 'chandra', 'observations', 'of', 'the', 'z0778', 'optically', 'selected', 'lensing', 'cluster', 'rcs02243400025', 'along', 'with', 'weak', 'lensing', 'and', 'dynamical', 'analyses', 'of', 'this', 'object', 'an', 'xray', 'spectrum', 'extracted', 'wi... | [-0.07976533663233633, 0.08481107807525765, -0.10059775590481287, 0.07756611672471286, -0.04364971188945813, -0.05332127042578298, 0.06416600033497177, 0.4324675392158128, -0.16809773423943902, -0.3609154318492893, 0.0554086396765375, -0.32192450838146713, 0.0216514606032466, 0.20802042996804523, 0.01208249636640487, -... |
708.3672 | Reply to Comment: S. Das Sarma et al., arXiv:0708.3239 | The authors of the Comment ascribe us claims never made while moderating
their own previous unsubstantiated statements.
| cond-mat.mes-hall cond-mat.mtrl-sci | the authors of the comment ascribe us claims never made while moderating their own previous unsubstantiated statements | [['the', 'authors', 'of', 'the', 'comment', 'ascribe', 'us', 'claims', 'never', 'made', 'while', 'moderating', 'their', 'own', 'previous', 'unsubstantiated', 'statements']] | [-0.07775169545236756, -0.012714137706686468, -0.1340103080660543, 0.039566490347223246, -0.22058195105808623, -0.11459902515087057, 0.22489871588699958, 0.36576226222164493, -0.10146843020201606, -0.3112365656039294, 0.10569167575415443, -0.36962975035695467, -0.04498291468959959, 0.1353376966298503, -0.15766453480019... |
708.3673 | Exploiting scale dependence in cosmological averaging | We study the role of scale dependence in the Buchert averaging method, using
the flat Lemaitre-Tolman-Bondi model as a testing ground. Within this model, a
single averaging scale gives too coarse predictions, but by replacing it with
the distance of the objects R(z) for each redshift z, we find an O(1%)
precision at ... | astro-ph | we study the role of scale dependence in the buchert averaging method using the flat lemaitretolmanbondi model as a testing ground within this model a single averaging scale gives too coarse predictions but by replacing it with the distance of the objects rz for each redshift z we find an o1 precision at z2 in the aver... | [['we', 'study', 'the', 'role', 'of', 'scale', 'dependence', 'in', 'the', 'buchert', 'averaging', 'method', 'using', 'the', 'flat', 'lemaitretolmanbondi', 'model', 'as', 'a', 'testing', 'ground', 'within', 'this', 'model', 'a', 'single', 'averaging', 'scale', 'gives', 'too', 'coarse', 'predictions', 'but', 'by', 'repla... | [-0.06676625390370776, 0.09455457773645841, -0.11295230003805565, 0.12861461207919223, -0.041022214388275254, -0.10180661790904456, 0.0027218743759606567, 0.41948411324327545, -0.23945423123825874, -0.36539130026191874, 0.07510531333225247, -0.24713923380311045, -0.05137274661434016, 0.17358718453573863, 0.001961179666... |
708.3674 | Power-law expansion cosmology in Schr\"odinger-type formulation | We investigate non-linear Schr\"{o}dinger-type formulation of cosmology of
which our cosmological system is a general relativistic FRLW universe
containing canonical scalar field under arbitrary potential and a barotropic
fluid with arbitrary spatial curvatures. We extend the formulation to include
phantom field case... | gr-qc astro-ph hep-th quant-ph | we investigate nonlinear schrodingertype formulation of cosmology of which our cosmological system is a general relativistic frlw universe containing canonical scalar field under arbitrary potential and a barotropic fluid with arbitrary spatial curvatures we extend the formulation to include phantom field case and we h... | [['we', 'investigate', 'nonlinear', 'schrodingertype', 'formulation', 'of', 'cosmology', 'of', 'which', 'our', 'cosmological', 'system', 'is', 'a', 'general', 'relativistic', 'frlw', 'universe', 'containing', 'canonical', 'scalar', 'field', 'under', 'arbitrary', 'potential', 'and', 'a', 'barotropic', 'fluid', 'with', '... | [-0.1437874166191452, 0.09671727707997585, -0.09718311250520249, 0.09567339815483945, -0.10882323362036711, -0.1505405559980621, -0.12291616680514482, 0.33325210337837535, -0.21114836286805155, -0.28356290658315025, 0.023681171318619614, -0.2556290768707792, -0.16339668174429486, 0.13501779894447988, 0.0482598967901948... |
708.3675 | The Origin of Solar Activity in the Tachocline | Solar active regions, produced by the emergence of tubes of strong magnetic
field in the photosphere, are restricted to within 35 degrees of the solar
equator. The nature of the dynamo processes that create and renew these fields,
and are therefore responsible for solar magnetic phenomena, are not well
understood. We... | astro-ph | solar active regions produced by the emergence of tubes of strong magnetic field in the photosphere are restricted to within 35 degrees of the solar equator the nature of the dynamo processes that create and renew these fields and are therefore responsible for solar magnetic phenomena are not well understood we analyze... | [['solar', 'active', 'regions', 'produced', 'by', 'the', 'emergence', 'of', 'tubes', 'of', 'strong', 'magnetic', 'field', 'in', 'the', 'photosphere', 'are', 'restricted', 'to', 'within', '35', 'degrees', 'of', 'the', 'solar', 'equator', 'the', 'nature', 'of', 'the', 'dynamo', 'processes', 'that', 'create', 'and', 'rene... | [-0.187405279271385, 0.24486351720720745, 0.03138351625856682, 0.14611184277501385, -0.09044526664627274, -0.015815679737695043, 0.026654578329955072, 0.31515665610970783, -0.2721881502736762, -0.3472143499542483, 0.05067475856760879, -0.16562011825898998, -0.11530781721883862, 0.2194018928738639, -0.048094915032006545... |
708.3676 | On the Cauchy problem for higher-order nonlinear dispersive equations | We study a class of higher-order KdV equations. We show that the associated
initial value problem is well posed in weighted Besov and Sobolev spaces for
small initial data. We also prove ill-posedness results when in H^s(\R), for
any real s.
| math.AP | we study a class of higherorder kdv equations we show that the associated initial value problem is well posed in weighted besov and sobolev spaces for small initial data we also prove illposedness results when in hsr for any real s | [['we', 'study', 'a', 'class', 'of', 'higherorder', 'kdv', 'equations', 'we', 'show', 'that', 'the', 'associated', 'initial', 'value', 'problem', 'is', 'well', 'posed', 'in', 'weighted', 'besov', 'and', 'sobolev', 'spaces', 'for', 'small', 'initial', 'data', 'we', 'also', 'prove', 'illposedness', 'results', 'when', 'in... | [-0.14120223627584735, 0.07241701540287311, 0.012951350861751452, 0.1662061033208241, -0.09314156532651041, -0.09673650398078125, -0.05362953208159746, 0.33266354888314154, -0.33314798022733955, -0.21681913002053413, 0.18964133357129445, -0.27480896948496014, -0.16674130909690044, 0.2541829003134697, -0.141920076705878... |
708.3677 | Comment on "Limits on the Time Variation of the Electromagnetic
Fine-Structure Constant in the Low Energy Limit from Absorption Lines in the
Spectra of Distant Quasars" | In their Letter [Phys. Rev. Lett. 92, 121302 (2004)] (also [Astron.
Astrophys. 417, 853 (2004)]), Srianand et al. analysed optical spectra of
heavy-element species in 23 absorption systems along background quasar
sight-lines, reporting limits on relative variations in the fine-structure
constant: da/a=(-0.06+/-0.06) ... | astro-ph hep-th physics.atom-ph | in their letter phys rev lett 92 121302 2004 also astron astrophys 417 853 2004 srianand et al analysed optical spectra of heavyelement species in 23 absorption systems along background quasar sightlines reporting limits on relative variations in the finestructure constant daa006006 x 105 here we demonstrate basic flaw... | [['in', 'their', 'letter', 'phys', 'rev', 'lett', '92', '121302', '2004', 'also', 'astron', 'astrophys', '417', '853', '2004', 'srianand', 'et', 'al', 'analysed', 'optical', 'spectra', 'of', 'heavyelement', 'species', 'in', '23', 'absorption', 'systems', 'along', 'background', 'quasar', 'sightlines', 'reporting', 'limi... | [-0.06914100485600476, 0.036153306434725356, -0.04659995028872371, 0.031726845816592686, -0.07942532049577601, -0.10326397350838627, 0.16622551312492065, 0.3848096665529096, -0.12156097182956085, -0.39230730700279204, 0.04639562477121431, -0.3047721907564932, -0.12124534129329465, 0.1920835092656917, -0.139808387338074... |
708.3678 | A large population of mid-infrared selected, obscured active galaxies in
the Bootes field | We identify a population of 640 obscured and 839 unobscured AGNs at redshifts
0.7<z<~3 using multiwavelength observations of the 9 deg^2 NOAO Deep Wide-Field
Survey (NDWFS) region in Bootes. We select AGNs on the basis of Spitzer IRAC
colors obtained by the IRAC Shallow Survey. Redshifts are obtained from optical
spe... | astro-ph | we identify a population of 640 obscured and 839 unobscured agns at redshifts 07z3 using multiwavelength observations of the 9 deg2 noao deep widefield survey ndwfs region in bootes we select agns on the basis of spitzer irac colors obtained by the irac shallow survey redshifts are obtained from optical spectroscopy or... | [['we', 'identify', 'a', 'population', 'of', '640', 'obscured', 'and', '839', 'unobscured', 'agns', 'at', 'redshifts', '07z3', 'using', 'multiwavelength', 'observations', 'of', 'the', '9', 'deg2', 'noao', 'deep', 'widefield', 'survey', 'ndwfs', 'region', 'in', 'bootes', 'we', 'select', 'agns', 'on', 'the', 'basis', 'of... | [0.040313904870139514, 0.05752113148742153, -0.07357755963204672, 0.10739435686922187, -0.08940315357632125, -0.1005679442446031, 0.11200361046231473, 0.5680023961740991, -0.08488562310357457, -0.3556921056228811, 0.08496264226370208, -0.3699829959027145, -0.031197573325050104, 0.17845682213929134, -0.05335200676484458... |
708.3679 | Adiabatic cross-polarization | A scheme of adiabatic cross-polarization is described. It is based on
demagnetization - remagnetization, when the Zeeman order of abundant nuclei in
the laboratory frame is first adiabatically converted into the dipolar order,
and then, into the Zeeman order of rare nuclei. The scheme, implemented with
two low-power ... | cond-mat.other | a scheme of adiabatic crosspolarization is described it is based on demagnetization remagnetization when the zeeman order of abundant nuclei in the laboratory frame is first adiabatically converted into the dipolar order and then into the zeeman order of rare nuclei the scheme implemented with two lowpower frequencyswe... | [['a', 'scheme', 'of', 'adiabatic', 'crosspolarization', 'is', 'described', 'it', 'is', 'based', 'on', 'demagnetization', 'remagnetization', 'when', 'the', 'zeeman', 'order', 'of', 'abundant', 'nuclei', 'in', 'the', 'laboratory', 'frame', 'is', 'first', 'adiabatically', 'converted', 'into', 'the', 'dipolar', 'order', '... | [-0.10885783346436385, 0.20795676976420163, -0.0434711491044644, 0.04987776164558627, 0.003184791947811997, -0.15843883007099585, 0.032365925942680666, 0.45041971565002487, -0.21074037078679317, -0.27582098207702593, 0.014210858967133044, -0.25855797256476115, -0.03939527298955779, 0.2280274751108317, 0.047166424531800... |
708.368 | Black Holes, Entropy, and Information | Black holes are a continuing source of mystery. Although their classical
properties have been understood since the 1970's, their quantum properties
raise some of the deepest questions in theoretical physics. Some of these
questions have recently been answered using string theory. I will review these
fundamental quest... | astro-ph gr-qc | black holes are a continuing source of mystery although their classical properties have been understood since the 1970s their quantum properties raise some of the deepest questions in theoretical physics some of these questions have recently been answered using string theory i will review these fundamental questions an... | [['black', 'holes', 'are', 'a', 'continuing', 'source', 'of', 'mystery', 'although', 'their', 'classical', 'properties', 'have', 'been', 'understood', 'since', 'the', '1970s', 'their', 'quantum', 'properties', 'raise', 'some', 'of', 'the', 'deepest', 'questions', 'in', 'theoretical', 'physics', 'some', 'of', 'these', '... | [-0.049803893193228886, 0.1281555208986924, -0.09934271051100006, 0.17519394752718967, -0.12728960387822655, -0.16137725109648374, 0.043281772110703186, 0.3464981468141447, -0.27811719983080285, -0.33830801228544227, 0.1504840754751507, -0.30947625963592235, -0.1600311966842891, 0.22516407892840948, -0.1092573264843703... |
708.3681 | The family of analytic Poisson brackets for the Camassa--Holm hierarchy | We consider the integrable Camassa--Holm hierarchy on the line with positive
initial data rapidly decaying at infinity. It is known that flows of the
hierarchy can be formulated in a Hamiltonian form using two compatible Poisson
brackets. In this note we propose a new approach to Hamiltonian theory of the
CH equation... | math-ph math.AG math.MP | we consider the integrable camassaholm hierarchy on the line with positive initial data rapidly decaying at infinity it is known that flows of the hierarchy can be formulated in a hamiltonian form using two compatible poisson brackets in this note we propose a new approach to hamiltonian theory of the ch equation in te... | [['we', 'consider', 'the', 'integrable', 'camassaholm', 'hierarchy', 'on', 'the', 'line', 'with', 'positive', 'initial', 'data', 'rapidly', 'decaying', 'at', 'infinity', 'it', 'is', 'known', 'that', 'flows', 'of', 'the', 'hierarchy', 'can', 'be', 'formulated', 'in', 'a', 'hamiltonian', 'form', 'using', 'two', 'compatib... | [-0.17630670955175626, 0.05362305310521404, -0.05910754068487431, 0.08737555554243506, -0.13687209988425134, -0.16070549140424759, -0.012604670329057596, 0.2912479573813053, -0.32107411749416687, -0.23615953084997465, 0.0377974564135151, -0.2705866413221496, -0.18569461262754364, 0.18725470353879767, -0.041835582944885... |
708.3682 | Entanglement in Disordered Systems at Criticality | Entanglement is a physical resource of a quantum system just like mass,
charge or energy. Moreover it is an essential tool for many purposes of
nowadays quantum information processing, e.g. quantum teleportation, quantum
cryptography or quantum computation. In this work we investigate an extended
system of N qubits. ... | cond-mat.dis-nn quant-ph | entanglement is a physical resource of a quantum system just like mass charge or energy moreover it is an essential tool for many purposes of nowadays quantum information processing eg quantum teleportation quantum cryptography or quantum computation in this work we investigate an extended system of n qubits in our sys... | [['entanglement', 'is', 'a', 'physical', 'resource', 'of', 'a', 'quantum', 'system', 'just', 'like', 'mass', 'charge', 'or', 'energy', 'moreover', 'it', 'is', 'an', 'essential', 'tool', 'for', 'many', 'purposes', 'of', 'nowadays', 'quantum', 'information', 'processing', 'eg', 'quantum', 'teleportation', 'quantum', 'cry... | [-0.17392421222195542, 0.17712246893598008, -0.07281883415798175, 0.07302575278706078, 0.06899722011374503, -0.22044165675239316, 0.03940787043518804, 0.32857897808325703, -0.24752617779926495, -0.27293390092793207, 0.05131991127875216, -0.3128362429922382, -0.108804853006812, 0.20020433050933584, -0.011437835528089762... |
708.3683 | Formal equivalence between Tsallis and extended Boltzmann-Gibbs
statistics | A formal correspondence between the q-distribution obtained from the Tsallis
entropy and non-maxwellian distributions obtained from the Boltzmann-Gibbs
entropy is afforded.
| quant-ph | a formal correspondence between the qdistribution obtained from the tsallis entropy and nonmaxwellian distributions obtained from the boltzmanngibbs entropy is afforded | [['a', 'formal', 'correspondence', 'between', 'the', 'qdistribution', 'obtained', 'from', 'the', 'tsallis', 'entropy', 'and', 'nonmaxwellian', 'distributions', 'obtained', 'from', 'the', 'boltzmanngibbs', 'entropy', 'is', 'afforded']] | [0.01266553412590708, 0.12234473955773172, -0.29577960526304586, 0.16843028191942722, 0.03420853441847222, -0.1431628891178185, 0.06579897889778727, 0.21246392244384402, -0.31889988233645755, -0.21927376845408053, -0.10851491996574969, -0.40310681079115185, 0.01011217234744912, 0.23513522353910266, -0.11607050199416422... |
708.3684 | The influence of cluster emission and the symmetry energy on
neutron-proton spectral double ratios | Emissions of free neutrons and protons from the central collisions of
124Sn+124Sn and 112Sn+112Sn reactions are simulated using the Improved Quantum
Molecular Dynamics model with two different density dependence of the symmetry
energy in the nuclear equation of state. The constructed double ratios of the
neutron to p... | nucl-th nucl-ex | emissions of free neutrons and protons from the central collisions of 124sn124sn and 112sn112sn reactions are simulated using the improved quantum molecular dynamics model with two different density dependence of the symmetry energy in the nuclear equation of state the constructed double ratios of the neutron to proton... | [['emissions', 'of', 'free', 'neutrons', 'and', 'protons', 'from', 'the', 'central', 'collisions', 'of', '124sn124sn', 'and', '112sn112sn', 'reactions', 'are', 'simulated', 'using', 'the', 'improved', 'quantum', 'molecular', 'dynamics', 'model', 'with', 'two', 'different', 'density', 'dependence', 'of', 'the', 'symmetr... | [-0.06872415334815864, 0.185368353590964, -0.08768686804232705, 0.11591822693042238, 0.007630620815032045, -0.07807692360404894, 0.0026095070056382473, 0.3350076294903244, -0.24711507803783947, -0.3525758467520736, 0.03198826708146097, -0.30491055134965594, -0.0016342482153921067, 0.15873137815119778, 0.041621941270428... |
708.3685 | On representations of certain pseudo-Anosov maps of Riemann surfaces
with punctures | Let $S$ be a Riemann surface of type $(p,n)$ with $3p+n>4$ and $n\geq 1$. Let
$\alpha_1,\alpha_2\subset S$ be two simple closed geodesics such that
$\{\alpha_1, \alpha_2\}$ fills $S$. It was shown by Thurston that most maps
obtained through Dehn twists along $\alpha_1$ and $\alpha_2$ are pseudo-Anosov.
Let $a$ be a p... | math.CV math.GT | let s be a riemann surface of type pn with 3pn4 and ngeq 1 let alpha_1alpha_2subset s be two simple closed geodesics such that alpha_1 alpha_2 fills s it was shown by thurston that most maps obtained through dehn twists along alpha_1 and alpha_2 are pseudoanosov let a be a puncture in this paper we study the family mat... | [['let', 's', 'be', 'a', 'riemann', 'surface', 'of', 'type', 'pn', 'with', '3pn4', 'and', 'ngeq', '1', 'let', 'alpha_1alpha_2subset', 's', 'be', 'two', 'simple', 'closed', 'geodesics', 'such', 'that', 'alpha_1', 'alpha_2', 'fills', 's', 'it', 'was', 'shown', 'by', 'thurston', 'that', 'most', 'maps', 'obtained', 'throug... | [-0.1823377942178218, 0.17502226582963035, -0.07657729299558748, 0.0044794507159460935, -0.03558150948055329, -0.1785663289678914, -0.024186718348984518, 0.3963662569561312, -0.29030112102402433, -0.2132720746640717, 0.09108202812081624, -0.32597054131929915, -0.1397087739810588, 0.26165324443230226, -0.108446274185553... |
708.3686 | Accuracy of a teleported trapped field state inside a single bimodal
cavity | We propose a simplified scheme to teleport a superposition of coherent states
from one mode to another of the same bimodal lossy cavity. Based on current
experimental capabilities, we present a calculation of the fidelity that can be
achieved, demonstrating accurate teleportation if the mean photon number of
each mod... | quant-ph | we propose a simplified scheme to teleport a superposition of coherent states from one mode to another of the same bimodal lossy cavity based on current experimental capabilities we present a calculation of the fidelity that can be achieved demonstrating accurate teleportation if the mean photon number of each mode is ... | [['we', 'propose', 'a', 'simplified', 'scheme', 'to', 'teleport', 'a', 'superposition', 'of', 'coherent', 'states', 'from', 'one', 'mode', 'to', 'another', 'of', 'the', 'same', 'bimodal', 'lossy', 'cavity', 'based', 'on', 'current', 'experimental', 'capabilities', 'we', 'present', 'a', 'calculation', 'of', 'the', 'fide... | [-0.14430807106241228, 0.14384528662776574, -0.11101020614816141, -0.0120666709138147, -0.005125961554724546, -0.21716154817979605, 0.10523372920856457, 0.3790505674911574, -0.24467926662709077, -0.253363654438761, 0.060101773111715114, -0.23282783192449383, -0.053905014713693945, 0.2528890286117703, -0.048457445355043... |
708.3687 | Multiplicity in Supersymmetric Spin Chains | We discuss a simple procedure for obtaining new integrable spin chains from
old by replacing each single state of the original model by some collection of
states. This works whenever the Lax matrix of the chain has a certain form. The
simplest example is the su(n) XX model. We apply the techniques of the nested
algeb... | math-ph math.MP | we discuss a simple procedure for obtaining new integrable spin chains from old by replacing each single state of the original model by some collection of states this works whenever the lax matrix of the chain has a certain form the simplest example is the sun xx model we apply the techniques of the nested algebraic be... | [['we', 'discuss', 'a', 'simple', 'procedure', 'for', 'obtaining', 'new', 'integrable', 'spin', 'chains', 'from', 'old', 'by', 'replacing', 'each', 'single', 'state', 'of', 'the', 'original', 'model', 'by', 'some', 'collection', 'of', 'states', 'this', 'works', 'whenever', 'the', 'lax', 'matrix', 'of', 'the', 'chain', ... | [-0.1055283490979277, 0.10664289535078056, -0.037215466528269806, 0.1000691481783767, -0.056042651810190254, -0.20138430429677315, 0.03495386918075383, 0.31663094515747886, -0.27611265134970275, -0.2223844203262535, 0.11015671573284849, -0.27495077775743354, -0.14517487223972292, 0.17092275879044525, -0.011832948657684... |
708.3688 | Localization and delocalization errors in density functional theory and
implications for band-gap prediction | The band-gap problem and other systematic failures of approximate functionals
are explained from an analysis of total energy for fractional charges. The
deviation from the correct intrinsic linear behavior in finite systems leads to
delocalization and localization errors in large or bulk systems. Functionals
whose en... | cond-mat.mtrl-sci | the bandgap problem and other systematic failures of approximate functionals are explained from an analysis of total energy for fractional charges the deviation from the correct intrinsic linear behavior in finite systems leads to delocalization and localization errors in large or bulk systems functionals whose energy ... | [['the', 'bandgap', 'problem', 'and', 'other', 'systematic', 'failures', 'of', 'approximate', 'functionals', 'are', 'explained', 'from', 'an', 'analysis', 'of', 'total', 'energy', 'for', 'fractional', 'charges', 'the', 'deviation', 'from', 'the', 'correct', 'intrinsic', 'linear', 'behavior', 'in', 'finite', 'systems', ... | [-0.09102123256917428, 0.07107934847223184, -0.0917960470180633, 0.12587202612979753, -0.0234271191892404, -0.10591108861912801, 0.07463309996381619, 0.3406475839720478, -0.3150768646777119, -0.3375536803047634, 0.05010820345193582, -0.3215613425573678, -0.10312690770872913, 0.1505423647880518, -0.1347440618862572, 0.1... |
708.3689 | Arithmetic structures in smooth subsets of F_p | Fix integers a_1,...,a_d satisfying a_1 + ... + a_d = 0. Suppose that f : Z_N
-> [0,1], where N is prime. We show that if f is ``smooth enough'' then we can
bound from below the sum of f(x_1)...f(x_d) over all solutions (x_1,...,x_d) in
Z_N to a_1 x_1 + ... + a_d x_d == 0 (mod N). Note that d = 3 and a_1 = a_2 = 1
an... | math.NT math.CO | fix integers a_1a_d satisfying a_1 a_d 0 suppose that f z_n 01 where n is prime we show that if f is smooth enough then we can bound from below the sum of fx_1fx_d over all solutions x_1x_d in z_n to a_1 x_1 a_d x_d 0 mod n note that d 3 and a_1 a_2 1 and a_3 2 is the case where x_1x_2x_3 are in arithmetic progression ... | [['fix', 'integers', 'a_1a_d', 'satisfying', 'a_1', 'a_d', '0', 'suppose', 'that', 'f', 'z_n', '01', 'where', 'n', 'is', 'prime', 'we', 'show', 'that', 'if', 'f', 'is', 'smooth', 'enough', 'then', 'we', 'can', 'bound', 'from', 'below', 'the', 'sum', 'of', 'fx_1fx_d', 'over', 'all', 'solutions', 'x_1x_d', 'in', 'z_n', '... | [-0.17342325624876384, 0.14180477853387413, -0.07366993140270252, 0.0310304404048976, -0.0397085055063632, -0.16127551025597425, 0.010466477423395234, 0.33020456157420286, -0.30653886686692516, -0.2207706762824162, 0.09800661311672274, -0.29556416192449764, -0.16441916749051705, 0.18617968300709548, -0.1005601311874825... |
708.369 | Two-dimensional quantum-dot helium in a magnetic field: Variational
theory | A trial wave function for two-dimensional quantum dot helium in an arbitrary
perpendicular magnetic field (a system of two interacting electrons in a
two-dimensional parabolic confinement potential) is introduced. A key
ingredient of this trial wave function is a Jastrow pair correlation factor
that has a displaced G... | cond-mat.mes-hall cond-mat.str-el | a trial wave function for twodimensional quantum dot helium in an arbitrary perpendicular magnetic field a system of two interacting electrons in a twodimensional parabolic confinement potential is introduced a key ingredient of this trial wave function is a jastrow pair correlation factor that has a displaced gaussian... | [['a', 'trial', 'wave', 'function', 'for', 'twodimensional', 'quantum', 'dot', 'helium', 'in', 'an', 'arbitrary', 'perpendicular', 'magnetic', 'field', 'a', 'system', 'of', 'two', 'interacting', 'electrons', 'in', 'a', 'twodimensional', 'parabolic', 'confinement', 'potential', 'is', 'introduced', 'a', 'key', 'ingredien... | [-0.18870104439556598, 0.15638939048149042, -0.04287237574656804, 0.08096138854549888, -0.018457658220237743, -0.08247706127197792, 0.007700585393467918, 0.36979037057608366, -0.20731837606678408, -0.27065486716261755, 0.006870053826908891, -0.25326276252356666, -0.12425859226107908, 0.19571223239375587, 0.098411577730... |
708.3691 | Time dependent black holes and thermal equilibration | We study aspects of a recently proposed exact time dependent black hole
solution of IIB string theory using the AdS/CFT correspondence. The dual field
theory is a thermal system in which initially a vacuum density for a
non-conserved operator is turned on. We can see that in agreement with general
thermal field theor... | hep-th gr-qc | we study aspects of a recently proposed exact time dependent black hole solution of iib string theory using the adscft correspondence the dual field theory is a thermal system in which initially a vacuum density for a nonconserved operator is turned on we can see that in agreement with general thermal field theory expe... | [['we', 'study', 'aspects', 'of', 'a', 'recently', 'proposed', 'exact', 'time', 'dependent', 'black', 'hole', 'solution', 'of', 'iib', 'string', 'theory', 'using', 'the', 'adscft', 'correspondence', 'the', 'dual', 'field', 'theory', 'is', 'a', 'thermal', 'system', 'in', 'which', 'initially', 'a', 'vacuum', 'density', '... | [-0.13874511207578724, 0.1514193657785654, -0.12328841614047277, 0.10761485404533963, -0.020569190104520813, -0.14161315961193638, 0.018357176933744827, 0.2823836064907079, -0.20568598996242987, -0.2590493016405818, 0.08328652976215192, -0.2972534950102497, -0.1344125543423381, 0.1293908944449474, -0.055200728011730406... |
708.3692 | Influence of the N*(1440) and N*(1535) Resonances in Intermediate Energy
pp and np Scattering | Motivated by a recent measurement of proton-proton elastic scattering
observables up to 3.0 GeV, we investigate the description of those data within
models of the nucleon-nucleon (NN) interaction valid above the pion production
threshold. In addition to including the well known Delta resonance we
incorporate two low-... | nucl-th nucl-ex | motivated by a recent measurement of protonproton elastic scattering observables up to 30 gev we investigate the description of those data within models of the nucleonnucleon nn interaction valid above the pion production threshold in addition to including the well known delta resonance we incorporate two lowlying n re... | [['motivated', 'by', 'a', 'recent', 'measurement', 'of', 'protonproton', 'elastic', 'scattering', 'observables', 'up', 'to', '30', 'gev', 'we', 'investigate', 'the', 'description', 'of', 'those', 'data', 'within', 'models', 'of', 'the', 'nucleonnucleon', 'nn', 'interaction', 'valid', 'above', 'the', 'pion', 'production... | [-0.07118796887354822, 0.22852518916543987, -0.04424832004588097, 0.17096362744147578, 0.013487223564879969, -0.08587233934991269, 0.04465831024895629, 0.33018781475968556, -0.207767620191185, -0.34982771097889376, -0.10282166145205135, -0.36740124849085176, 0.02203666824627564, 0.12164407225403313, 0.1394099134841882,... |
708.3693 | An Ergodic Result | A rather general ergodic type scheme is presented on arbitrary sets X, as
they are generated by arbitrary mappings T : X \longrightarrow X. The
structures considered on X are given by suitable subsets of the set of all of
its finite partitions. Ergodicity is studied not with respect to subsets of X,
but with the {\it... | math.GM math.DS | a rather general ergodic type scheme is presented on arbitrary sets x as they are generated by arbitrary mappings t x longrightarrow x the structures considered on x are given by suitable subsets of the set of all of its finite partitions ergodicity is studied not with respect to subsets of x but with the it inverse li... | [['a', 'rather', 'general', 'ergodic', 'type', 'scheme', 'is', 'presented', 'on', 'arbitrary', 'sets', 'x', 'as', 'they', 'are', 'generated', 'by', 'arbitrary', 'mappings', 't', 'x', 'longrightarrow', 'x', 'the', 'structures', 'considered', 'on', 'x', 'are', 'given', 'by', 'suitable', 'subsets', 'of', 'the', 'set', 'of... | [-0.1871932328952151, 0.16432484950397222, -0.02569748295678033, 0.05498877475555572, -0.01038351908902682, -0.12909768600135096, 0.0801695295579968, 0.4042276293039322, -0.30597422635626226, -0.18378352097860198, 0.12533210124081326, -0.2798233009165242, -0.033040887690962306, 0.21507701520172376, -0.07179851692524694... |
708.3694 | Electronic, dynamical, and thermal properties of ultra-incompressible
superhard rhenium diboride: A combined first-principles and neutron
scattering study | Rhenium diboride is a recently recognized ultra-incompressible superhard
material. Here we report the electronic (e), phonon (p), e-p coupling and
thermal properties of ReB$_2$ from first-principles density-functional theory
(DFT) calculations and neutron scattering measurements. Our calculated elastic
constants ($c_... | cond-mat.mtrl-sci | rhenium diboride is a recently recognized ultraincompressible superhard material here we report the electronic e phonon p ep coupling and thermal properties of reb_2 from firstprinciples densityfunctional theory dft calculations and neutron scattering measurements our calculated elastic constants c_11 641 gpa c_12 159 ... | [['rhenium', 'diboride', 'is', 'a', 'recently', 'recognized', 'ultraincompressible', 'superhard', 'material', 'here', 'we', 'report', 'the', 'electronic', 'e', 'phonon', 'p', 'ep', 'coupling', 'and', 'thermal', 'properties', 'of', 'reb_2', 'from', 'firstprinciples', 'densityfunctional', 'theory', 'dft', 'calculations',... | [-0.081692374384913, 0.1778432813178944, -0.07419924060354549, -0.006139885399515104, -0.014317413919151908, -0.13462444791129152, 0.13872227974444334, 0.41974568256226025, -0.25966008642296257, -0.3148637428536619, -0.020765823123388386, -0.38241044029985605, -0.0989440351589828, 0.17215801569094, 0.09155074657587409,... |
708.3695 | Near-horizon geometries of supersymmetric AdS(5) black holes | We provide a classification of near-horizon geometries of supersymmetric,
asymptotically anti-de Sitter, black holes of five-dimensional U(1)^3-gauged
supergravity which admit two rotational symmetries. We find three
possibilities: a topologically spherical horizon, an S^1 \times S^2 horizon and
a toroidal horizon. T... | hep-th | we provide a classification of nearhorizon geometries of supersymmetric asymptotically antide sitter black holes of fivedimensional u13gauged supergravity which admit two rotational symmetries we find three possibilities a topologically spherical horizon an s1 times s2 horizon and a toroidal horizon the nearhorizon geo... | [['we', 'provide', 'a', 'classification', 'of', 'nearhorizon', 'geometries', 'of', 'supersymmetric', 'asymptotically', 'antide', 'sitter', 'black', 'holes', 'of', 'fivedimensional', 'u13gauged', 'supergravity', 'which', 'admit', 'two', 'rotational', 'symmetries', 'we', 'find', 'three', 'possibilities', 'a', 'topologica... | [-0.16979879775317386, 0.121236487256283, -0.04062763913275881, 0.1312816831810374, -0.10797615325039563, -0.20378643219656725, -0.06965632465693893, 0.31708860375349307, -0.09705098792538694, -0.19847945373557094, 0.15532238537060847, -0.26725675616439226, -0.13675342964577591, 0.13255061285275993, -0.1240925289708280... |
708.3696 | Relative-Error CUR Matrix Decompositions | Many data analysis applications deal with large matrices and involve
approximating the matrix using a small number of ``components.'' Typically,
these components are linear combinations of the rows and columns of the matrix,
and are thus difficult to interpret in terms of the original features of the
input data. In t... | cs.DS | many data analysis applications deal with large matrices and involve approximating the matrix using a small number of components typically these components are linear combinations of the rows and columns of the matrix and are thus difficult to interpret in terms of the original features of the input data in this paper ... | [['many', 'data', 'analysis', 'applications', 'deal', 'with', 'large', 'matrices', 'and', 'involve', 'approximating', 'the', 'matrix', 'using', 'a', 'small', 'number', 'of', 'components', 'typically', 'these', 'components', 'are', 'linear', 'combinations', 'of', 'the', 'rows', 'and', 'columns', 'of', 'the', 'matrix', '... | [-0.12942799800368693, 0.08380418780127892, -0.027595648200231346, 0.016641235929345778, -0.041461159331486266, -0.150309426962862, 0.04472410825208318, 0.38098224944349196, -0.29549629689881196, -0.27967434821003084, 0.14665405711832832, -0.27639900344252216, -0.15264041205093673, 0.1379137318729958, -0.04173225040732... |
708.3697 | Homotopy characterization of ANR mapping spaces | Let Y be an absolute neighborhood retract (ANR) for the class of metric
spaces and let X be a Hausdorff space. Let map(X,Y) denote the space of
continuous maps from X to Y with the compact open topology. It is shown that if
X is a CW complex then map(X,Y) is an ANR for the class of metric spaces if and
only if map(X,... | math.AT math.GN | let y be an absolute neighborhood retract anr for the class of metric spaces and let x be a hausdorff space let mapxy denote the space of continuous maps from x to y with the compact open topology it is shown that if x is a cw complex then mapxy is an anr for the class of metric spaces if and only if mapxy is metrizabl... | [['let', 'y', 'be', 'an', 'absolute', 'neighborhood', 'retract', 'anr', 'for', 'the', 'class', 'of', 'metric', 'spaces', 'and', 'let', 'x', 'be', 'a', 'hausdorff', 'space', 'let', 'mapxy', 'denote', 'the', 'space', 'of', 'continuous', 'maps', 'from', 'x', 'to', 'y', 'with', 'the', 'compact', 'open', 'topology', 'it', '... | [-0.14800474758908905, 0.13721381882583336, -0.09082611966036022, 0.04549094125197487, -0.09704369425456574, -0.12438041391841909, 0.004749110424296653, 0.42355421233050367, -0.33926776586536395, -0.12387807967458317, 0.10675795796262894, -0.2655078895845787, -0.09783473260641257, 0.2106674151851776, -0.168083388071031... |
708.3698 | Upper limit for circumstellar gas around the Type Ia SN 2000cx | The nature of the companion stars in Type Ia Supernova (SNe) progenitor
systems remains unclear. One possible way to discriminate between different
scenarios is the presence (or absence) of circumstellar material, the left
overs from the progenitor evolution that may be revealed by their interaction
with the SN. A ne... | astro-ph | the nature of the companion stars in type ia supernova sne progenitor systems remains unclear one possible way to discriminate between different scenarios is the presence or absence of circumstellar material the left overs from the progenitor evolution that may be revealed by their interaction with the sn a new method ... | [['the', 'nature', 'of', 'the', 'companion', 'stars', 'in', 'type', 'ia', 'supernova', 'sne', 'progenitor', 'systems', 'remains', 'unclear', 'one', 'possible', 'way', 'to', 'discriminate', 'between', 'different', 'scenarios', 'is', 'the', 'presence', 'or', 'absence', 'of', 'circumstellar', 'material', 'the', 'left', 'o... | [-0.07725678116109504, 0.036287896886450365, -0.044342822353531305, 0.07154911960846358, -0.14494268049130146, -0.1321121447759171, 0.06612705138571262, 0.4291530195579706, -0.2253591987515255, -0.27121973841232555, 0.05471625928228879, -0.28167981778728374, -0.042501287809397395, 0.15669337409012513, -0.05059538347735... |
708.3699 | Convolutional Entanglement Distillation | We develop a theory of entanglement distillation that exploits a
convolutional coding structure. We provide a method for converting an arbitrary
classical binary or quaternary convolutional code into a convolutional
entanglement distillation protocol. The imported classical convolutional code
does not have to be dual... | quant-ph cs.IT math.IT | we develop a theory of entanglement distillation that exploits a convolutional coding structure we provide a method for converting an arbitrary classical binary or quaternary convolutional code into a convolutional entanglement distillation protocol the imported classical convolutional code does not have to be dualcont... | [['we', 'develop', 'a', 'theory', 'of', 'entanglement', 'distillation', 'that', 'exploits', 'a', 'convolutional', 'coding', 'structure', 'we', 'provide', 'a', 'method', 'for', 'converting', 'an', 'arbitrary', 'classical', 'binary', 'or', 'quaternary', 'convolutional', 'code', 'into', 'a', 'convolutional', 'entanglement... | [-0.13747307797808908, 0.08745762793932291, -0.1258830952876159, 0.06512051977618277, 0.013166069019123585, -0.39106692050508884, 0.057633316604909994, 0.4230336415561011, -0.3112708968620231, -0.26052102800815563, 0.0703056202147727, -0.23877945278913978, -0.14663712351317823, 0.1776101527987116, -0.15140551997919696,... |
708.37 | Memory Effect and Fast Spinodal Decomposition | We consider the modification of the Cahn-Hilliard equation when a time delay
process through a memory function is taken into account. We then study the
process of spinodal decomposition in fast phase transitions associated with a
conserved order parameter. The introduced memory effect plays an important role
to obtai... | nucl-th cond-mat.soft hep-ph | we consider the modification of the cahnhilliard equation when a time delay process through a memory function is taken into account we then study the process of spinodal decomposition in fast phase transitions associated with a conserved order parameter the introduced memory effect plays an important role to obtain a f... | [['we', 'consider', 'the', 'modification', 'of', 'the', 'cahnhilliard', 'equation', 'when', 'a', 'time', 'delay', 'process', 'through', 'a', 'memory', 'function', 'is', 'taken', 'into', 'account', 'we', 'then', 'study', 'the', 'process', 'of', 'spinodal', 'decomposition', 'in', 'fast', 'phase', 'transitions', 'associat... | [-0.16544641719533587, 0.15768961552741942, -0.1271352247370161, 0.03685865469713394, -0.0737384139419586, -0.08058459142592016, 0.068019938707914, 0.3260517405600832, -0.30692024463963397, -0.25138442652335147, 0.10876137895272377, -0.21970261026279264, -0.12141554788598474, 0.13107374715530928, -0.008419254661003954,... |
708.3701 | Classical analogs for Rabi-oscillations, Ramsey-fringes, and spin-echo
in Josephson junctions | We investigate the results of recently published experiments on the quantum
behavior of Josephson circuits in terms of the classical modelling based on the
resistively and capacitively-shunted (RCSJ) junction model. Our analysis shows
evidence for a close analogy between the nonlinear behavior of a pulsed
microwave-d... | cond-mat.supr-con cond-mat.stat-mech | we investigate the results of recently published experiments on the quantum behavior of josephson circuits in terms of the classical modelling based on the resistively and capacitivelyshunted rcsj junction model our analysis shows evidence for a close analogy between the nonlinear behavior of a pulsed microwavedriven j... | [['we', 'investigate', 'the', 'results', 'of', 'recently', 'published', 'experiments', 'on', 'the', 'quantum', 'behavior', 'of', 'josephson', 'circuits', 'in', 'terms', 'of', 'the', 'classical', 'modelling', 'based', 'on', 'the', 'resistively', 'and', 'capacitivelyshunted', 'rcsj', 'junction', 'model', 'our', 'analysis... | [-0.17077500133903004, 0.13771889875856003, -0.06954240214590933, 0.0446840070204785, -0.05915252587398867, -0.15680994848519855, 0.05916353568641676, 0.3581159308771877, -0.22277694925653682, -0.29929382895770806, 0.05306875428414654, -0.2892491555090969, -0.17582512788133683, 0.30580037922044495, -0.00557775587890467... |
708.3702 | Measurements of Partial Branching Fractions for Bbar --> X_u ell nubar
and Determination of |V_{ub}| | We present partial branching fractions for inclusive charmless semileptonic B
decays Bbar --> X_u ell nubar, and the determination of the CKM matrix element
|V_{ub}|. The analysis is based on a sample of 383 million Y(4S) decays into B
Bbar pairs collected with the BaBar detector at the PEP-II e+ e- storage rings.
We... | hep-ex | we present partial branching fractions for inclusive charmless semileptonic b decays bbar x_u ell nubar and the determination of the ckm matrix element v_ub the analysis is based on a sample of 383 million y4s decays into b bbar pairs collected with the babar detector at the pepii e e storage rings we select events usi... | [['we', 'present', 'partial', 'branching', 'fractions', 'for', 'inclusive', 'charmless', 'semileptonic', 'b', 'decays', 'bbar', 'x_u', 'ell', 'nubar', 'and', 'the', 'determination', 'of', 'the', 'ckm', 'matrix', 'element', 'v_ub', 'the', 'analysis', 'is', 'based', 'on', 'a', 'sample', 'of', '383', 'million', 'y4s', 'de... | [-0.12324057241726288, 0.25888419131987955, 0.004793928669549633, 0.0629023506307799, -0.006006584779032088, -0.13678573344942127, 0.15164224006593283, 0.2790591051444357, -0.18525285824485446, -0.26264910713729, -0.05336073177370607, -0.43145665285460977, 0.1469566508759812, 0.11219411971029805, 0.08950042499202317, 0... |
708.3703 | Testing the evolution of the DB white dwarf GD 358: First results of a
new approach using asteroseismology | We present a new method that investigates the evolutionary history of the
pulsating DB white dwarf GD358 using asteroseismology. This is done considering
the internal C/O profile, which describes the relative abundances of carbon and
oxygen from the core of the star to its surface. Different evolutionary
channels lea... | astro-ph | we present a new method that investigates the evolutionary history of the pulsating db white dwarf gd358 using asteroseismology this is done considering the internal co profile which describes the relative abundances of carbon and oxygen from the core of the star to its surface different evolutionary channels lead to t... | [['we', 'present', 'a', 'new', 'method', 'that', 'investigates', 'the', 'evolutionary', 'history', 'of', 'the', 'pulsating', 'db', 'white', 'dwarf', 'gd358', 'using', 'asteroseismology', 'this', 'is', 'done', 'considering', 'the', 'internal', 'co', 'profile', 'which', 'describes', 'the', 'relative', 'abundances', 'of',... | [-0.06337065571780809, 0.1319868743901195, -0.07638373611063806, 0.09174452679522548, -0.05984017111393562, -0.08863650308311896, 0.09667000172997309, 0.4032714009024691, -0.21125756531107895, -0.36587282482485844, 0.04899678382499949, -0.2631138307590182, -0.08533806963640725, 0.18449527892491507, -0.04727205331335617... |
708.3704 | About Goldbach strong conjecture | In this work we use the number classification in families of the form 6n+1,
and 6n+5 with n integer (Such families contain all odd prime numbers greater
than 3 and other compound numbers related with primes). We will use this kind
of classification in order to attempt an approach to Goldbach strong
conjecture. By mea... | math.GM | in this work we use the number classification in families of the form 6n1 and 6n5 with n integer such families contain all odd prime numbers greater than 3 and other compound numbers related with primes we will use this kind of classification in order to attempt an approach to goldbach strong conjecture by means of a g... | [['in', 'this', 'work', 'we', 'use', 'the', 'number', 'classification', 'in', 'families', 'of', 'the', 'form', '6n1', 'and', '6n5', 'with', 'n', 'integer', 'such', 'families', 'contain', 'all', 'odd', 'prime', 'numbers', 'greater', 'than', '3', 'and', 'other', 'compound', 'numbers', 'related', 'with', 'primes', 'we', '... | [-0.19174317241840375, 0.09465219393702379, -0.06513508399327596, 0.07249846406591436, -0.07563807031139731, -0.11693183217197657, 0.04189440531656146, 0.2981498610725005, -0.25455730546886723, -0.37159303702414037, 0.04862732705504944, -0.27887863461859524, -0.18575844258380433, 0.20871935452024143, -0.080220145080238... |
708.3705 | Lattice QCD Calculation of the $\rho$ Meson Decay Width | We present a lattice QCD calculation of the $\rho$ meson decay width via the
$P$-wave scattering phase shift for the I=1 two-pion system. Our calculation
uses full QCD gauge configurations for $N_f=2$ flavors generated using a
renormalization group improved gauge action and an improved Wilson fermion
action on a $12^... | hep-lat | we present a lattice qcd calculation of the rho meson decay width via the pwave scattering phase shift for the i1 twopion system our calculation uses full qcd gauge configurations for n_f2 flavors generated using a renormalization group improved gauge action and an improved wilson fermion action on a 123times24 lattice... | [['we', 'present', 'a', 'lattice', 'qcd', 'calculation', 'of', 'the', 'rho', 'meson', 'decay', 'width', 'via', 'the', 'pwave', 'scattering', 'phase', 'shift', 'for', 'the', 'i1', 'twopion', 'system', 'our', 'calculation', 'uses', 'full', 'qcd', 'gauge', 'configurations', 'for', 'n_f2', 'flavors', 'generated', 'using', ... | [-0.11827424899903966, 0.2594111352238363, -0.11770416610658581, 0.07086520342320418, -0.025618857018015972, -0.0939783983650144, 0.10006127776229777, 0.3682755181932303, -0.16950863776881187, -0.20645617783741385, 0.020646703364632903, -0.31277518757603695, -0.00547932967215349, 0.11924691492935917, 0.0779248750692264... |
708.3706 | D3/D7 holographic Gauge theory and Chemical potential | N=2 supersymmetric Yang-Mills theory with flavor hypermultiplets at finite
temperature and in the dS${}_4$ are studied for finite quark number density
($n_b$) by a dual supergravity background with non-trivial dilaton and axion.
The quarks and its number density $n_b$ are introduced by embedding a probe D7
brane. We ... | hep-th | n2 supersymmetric yangmills theory with flavor hypermultiplets at finite temperature and in the ds_4 are studied for finite quark number density n_b by a dual supergravity background with nontrivial dilaton and axion the quarks and its number density n_b are introduced by embedding a probe d7 brane we find a critical v... | [['n2', 'supersymmetric', 'yangmills', 'theory', 'with', 'flavor', 'hypermultiplets', 'at', 'finite', 'temperature', 'and', 'in', 'the', 'ds_4', 'are', 'studied', 'for', 'finite', 'quark', 'number', 'density', 'n_b', 'by', 'a', 'dual', 'supergravity', 'background', 'with', 'nontrivial', 'dilaton', 'and', 'axion', 'the'... | [-0.11933142022998684, 0.26079060511639046, -0.0634968402032667, 0.04820138681756553, -0.007022358526132609, -0.12649863792313754, 0.07044773322214544, 0.32129210229093014, -0.16163624185872705, -0.29588579320912495, 0.06332071028469057, -0.2937184632755816, -0.08218669136802323, 0.07753294529270773, 0.0249025193625129... |
708.3707 | First order approach and index theorems for discrete and metric graphs | The aim of the present paper is to introduce the notion of first order
(supersymmetric) Dirac operators on discrete and metric (``quantum'') graphs.
In order to cover all self-adjoint boundary conditions for the associated
metric graph Laplacian, we develop systematically a new type of discrete graph
operators acting... | math.SP math-ph math.CO math.FA math.MP | the aim of the present paper is to introduce the notion of first order supersymmetric dirac operators on discrete and metric quantum graphs in order to cover all selfadjoint boundary conditions for the associated metric graph laplacian we develop systematically a new type of discrete graph operators acting on a decorat... | [['the', 'aim', 'of', 'the', 'present', 'paper', 'is', 'to', 'introduce', 'the', 'notion', 'of', 'first', 'order', 'supersymmetric', 'dirac', 'operators', 'on', 'discrete', 'and', 'metric', 'quantum', 'graphs', 'in', 'order', 'to', 'cover', 'all', 'selfadjoint', 'boundary', 'conditions', 'for', 'the', 'associated', 'me... | [-0.11986393147769074, 0.09827516010247767, -0.07379743245595212, 0.07337732544692699, -0.13907529360343082, -0.11402217317825286, 0.0041074053191955, 0.3291721952070172, -0.25659656858382124, -0.23836852815778306, 0.08559184321913765, -0.30547377718580215, -0.19502612770560923, 0.12402357201143685, -0.0827072369882241... |
708.3708 | Super-bicharacter construction of quantum vertex algebras | We extend the bicharacter construction of quantum vertex algebras first
proposed by Borcherds to the case of super Hopf algebras. We give a bicharacter
description of the charged free fermion super vertex algebra, which allows us
to construct different quantizations of it in the sense of $H_D$-quantum vertex
algebras... | math-ph math.MP math.QA | we extend the bicharacter construction of quantum vertex algebras first proposed by borcherds to the case of super hopf algebras we give a bicharacter description of the charged free fermion super vertex algebra which allows us to construct different quantizations of it in the sense of h_dquantum vertex algebras or spe... | [['we', 'extend', 'the', 'bicharacter', 'construction', 'of', 'quantum', 'vertex', 'algebras', 'first', 'proposed', 'by', 'borcherds', 'to', 'the', 'case', 'of', 'super', 'hopf', 'algebras', 'we', 'give', 'a', 'bicharacter', 'description', 'of', 'the', 'charged', 'free', 'fermion', 'super', 'vertex', 'algebra', 'which'... | [-0.13834856076573487, 0.10845863494323567, -0.07302243419981096, 0.06688911863602698, -0.14054615946952254, -0.12389599775779062, -0.011458073527319357, 0.30358488648198545, -0.30454871683032253, -0.1897815612144768, 0.07421939788910095, -0.23879035185400427, -0.16336801721772645, 0.13754803257470485, -0.0945300184472... |
708.3709 | An elementary sieve | In this paper we review the properties of families of numbers of the form
$6n\pm1$, with $n$ integer (in which there are all prime numbers greater than 3
and other compound numbers with particular properties) to later use them in a
new sieve that allows the separation of numbers $n$ that generate primes from
those th... | math.GM | in this paper we review the properties of families of numbers of the form 6npm1 with n integer in which there are all prime numbers greater than 3 and other compound numbers with particular properties to later use them in a new sieve that allows the separation of numbers n that generate primes from those that only gene... | [['in', 'this', 'paper', 'we', 'review', 'the', 'properties', 'of', 'families', 'of', 'numbers', 'of', 'the', 'form', '6npm1', 'with', 'n', 'integer', 'in', 'which', 'there', 'are', 'all', 'prime', 'numbers', 'greater', 'than', '3', 'and', 'other', 'compound', 'numbers', 'with', 'particular', 'properties', 'to', 'later... | [-0.1610041751690005, 0.18434508953941986, -0.08124648104421794, 0.04324908140260959, -0.05349144987412728, -0.11054635661421344, 0.04741850553109543, 0.3078888440039009, -0.28397611109539866, -0.3745171315036714, 0.032576889148913324, -0.2784424118262905, -0.12761452296399511, 0.2465490402537398, -0.031103335926309227... |
708.371 | Real World Interpretations of Quantum Theory | I propose a new class of interpretations, {\it real world interpretations},
of the quantum theory of closed systems. These interpretations postulate a
preferred factorization of Hilbert space and preferred projective measurements
on one factor. They give a mathematical characterisation of the different
possible world... | quant-ph | i propose a new class of interpretations it real world interpretations of the quantum theory of closed systems these interpretations postulate a preferred factorization of hilbert space and preferred projective measurements on one factor they give a mathematical characterisation of the different possible worlds arising... | [['i', 'propose', 'a', 'new', 'class', 'of', 'interpretations', 'it', 'real', 'world', 'interpretations', 'of', 'the', 'quantum', 'theory', 'of', 'closed', 'systems', 'these', 'interpretations', 'postulate', 'a', 'preferred', 'factorization', 'of', 'hilbert', 'space', 'and', 'preferred', 'projective', 'measurements', '... | [-0.10999964365630217, 0.1373276472906765, -0.12486088130243837, 0.1286085838219151, -0.10850313272760631, -0.15818253693129844, 0.03161817600616729, 0.3171125089327963, -0.2706021098595745, -0.30871131442744965, 0.06887674109524104, -0.2371284023612597, -0.14333693545206255, 0.1781517394581142, -0.09408112417327603, 0... |
708.3711 | Mean-field description of the nucleus-nucleus optical potential | A new finite-range representation of the JLM effective nucleon-nucleon
interaction is suggested based on the CDM3Y density dependent functional and
M3Y-Paris interaction. The density dependence has been carefully adjusted at
each energy so that the nucleon optical potential (OP) given by the new density
dependent int... | nucl-th nucl-ex | a new finiterange representation of the jlm effective nucleonnucleon interaction is suggested based on the cdm3y density dependent functional and m3yparis interaction the density dependence has been carefully adjusted at each energy so that the nucleon optical potential op given by the new density dependent interaction... | [['a', 'new', 'finiterange', 'representation', 'of', 'the', 'jlm', 'effective', 'nucleonnucleon', 'interaction', 'is', 'suggested', 'based', 'on', 'the', 'cdm3y', 'density', 'dependent', 'functional', 'and', 'm3yparis', 'interaction', 'the', 'density', 'dependence', 'has', 'been', 'carefully', 'adjusted', 'at', 'each',... | [-0.060721296326456856, 0.17145232827447, -0.12896998342624838, 0.11540566225829978, -0.025294731681545574, -0.08861453399904781, 0.0025856159516565854, 0.3479269664025023, -0.1961480611436335, -0.3051636972952457, -0.0747821220900819, -0.2945533942519909, -0.07607520646637395, 0.06846863272810533, 0.1255316810482847, ... |
708.3712 | Canonical Charmonium Interpretation for Y(4360) and Y(4660) | In this work, we consider the canonical charmonium assignments for Y(4360)
and Y(4660). Y(4660) is good candidate of $\rm 5 ^3S_1$ $c\bar{c}$ state, the
possibility of Y(4360) as a $\rm 3 ^3D_1$ $c\bar{c}$ state is studied, and the
charmonium hybrid interpretation of Y(4360) can not be excluded completely. We
evaluat... | hep-ph | in this work we consider the canonical charmonium assignments for y4360 and y4660 y4660 is good candidate of rm 5 3s_1 cbarc state the possibility of y4360 as a rm 3 3d_1 cbarc state is studied and the charmonium hybrid interpretation of y4360 can not be excluded completely we evaluate the ee leptonic widths e1 transit... | [['in', 'this', 'work', 'we', 'consider', 'the', 'canonical', 'charmonium', 'assignments', 'for', 'y4360', 'and', 'y4660', 'y4660', 'is', 'good', 'candidate', 'of', 'rm', '5', '3s_1', 'cbarc', 'state', 'the', 'possibility', 'of', 'y4360', 'as', 'a', 'rm', '3', '3d_1', 'cbarc', 'state', 'is', 'studied', 'and', 'the', 'c... | [-0.08982697849186431, 0.2543310774245152, -0.021959639283044164, 0.22745183778131736, -0.03427113658797584, -0.2012317221256365, 0.13049638133624716, 0.3667888923695213, -0.09589117441301871, -0.21718651053838825, -0.06683439939852658, -0.2993301555734912, 0.04625452569024147, 0.03320376898505186, 0.139981723108672, 0... |
708.3713 | A field theoretic approach to master equations and a variational method
beyond the Poisson ansatz | We develop a variational scheme in a field theoretic approach to a stochastic
process. While various stochastic processes can be expressed using master
equations, in general it is difficult to solve the master equations exactly,
and it is also hard to solve the master equations numerically because of the
curse of dim... | cond-mat.stat-mech | we develop a variational scheme in a field theoretic approach to a stochastic process while various stochastic processes can be expressed using master equations in general it is difficult to solve the master equations exactly and it is also hard to solve the master equations numerically because of the curse of dimensio... | [['we', 'develop', 'a', 'variational', 'scheme', 'in', 'a', 'field', 'theoretic', 'approach', 'to', 'a', 'stochastic', 'process', 'while', 'various', 'stochastic', 'processes', 'can', 'be', 'expressed', 'using', 'master', 'equations', 'in', 'general', 'it', 'is', 'difficult', 'to', 'solve', 'the', 'master', 'equations'... | [-0.06454943690445875, 0.004102717207736123, -0.1407407521764004, 0.11962007730072467, -0.12952814891859388, -0.15876096342659038, 0.03677409208510946, 0.3215246666097801, -0.3201511089233744, -0.2874053424011741, 0.05261996654315458, -0.20516838373353818, -0.20699519403716363, 0.1871727887766073, -0.07010346056343425,... |
708.3714 | Orbits of particles in noncommutative Schwarzschild spacetime | By considering particles as smeared objects, we investigate the effects of
space noncommutativity on the orbits of particles in Schwarzschild spacetime.
The effects of space noncommutativity on the value of the precession of the
perihelion of particle orbit and deflection of light ray in Schwarzschild
geometry are ca... | gr-qc | by considering particles as smeared objects we investigate the effects of space noncommutativity on the orbits of particles in schwarzschild spacetime the effects of space noncommutativity on the value of the precession of the perihelion of particle orbit and deflection of light ray in schwarzschild geometry are calcul... | [['by', 'considering', 'particles', 'as', 'smeared', 'objects', 'we', 'investigate', 'the', 'effects', 'of', 'space', 'noncommutativity', 'on', 'the', 'orbits', 'of', 'particles', 'in', 'schwarzschild', 'spacetime', 'the', 'effects', 'of', 'space', 'noncommutativity', 'on', 'the', 'value', 'of', 'the', 'precession', 'o... | [-0.20689415443588846, 0.19309130931339627, -0.09508663876580872, 0.10177509384603971, -0.03218622823312346, -0.020738581528088877, -0.024657323690397397, 0.30611373650442275, -0.1961156240431592, -0.2958640701004437, 0.052838141086145436, -0.2757306781630697, -0.05948814902720707, 0.21453072294700956, -0.1130054846206... |
708.3715 | Three String Junction and N=4 Dyon Spectrum | The exact spectrum of dyons in a class of N=4 supersymmetric string theories
gives us information about dyon spectrum in N=4 supersymmetric gauge theories.
This in turn can be translated into prediction about the BPS spectrum of three
string junctions on a configuration of three parallel D3-branes. We show that
this ... | hep-th | the exact spectrum of dyons in a class of n4 supersymmetric string theories gives us information about dyon spectrum in n4 supersymmetric gauge theories this in turn can be translated into prediction about the bps spectrum of three string junctions on a configuration of three parallel d3branes we show that this predict... | [['the', 'exact', 'spectrum', 'of', 'dyons', 'in', 'a', 'class', 'of', 'n4', 'supersymmetric', 'string', 'theories', 'gives', 'us', 'information', 'about', 'dyon', 'spectrum', 'in', 'n4', 'supersymmetric', 'gauge', 'theories', 'this', 'in', 'turn', 'can', 'be', 'translated', 'into', 'prediction', 'about', 'the', 'bps',... | [-0.1856105034805935, 0.1424403632110035, -0.07633573469403829, 0.12925955850467388, -0.029252193868160248, -0.1582492806420133, -0.013877757255466201, 0.31908283810559157, -0.15047721092186467, -0.30652959169064825, 0.048387498410758435, -0.2611967045341845, -0.08894405921770109, 0.14014451603430347, -0.06490120397427... |
708.3716 | The Impact of a Percolating IGM on Redshifted 21 cm Observations of
Quasar HII Regions | We assess the impact of inhomogeneous reionization on detection of HII
regions surrounding luminous high redshift quasars using planned low frequency
radio telescopes. Our approach is to implement a semi-numerical scheme to
calculate the 3-dimensional structure of ionized regions surrounding a massive
halo at high re... | astro-ph | we assess the impact of inhomogeneous reionization on detection of hii regions surrounding luminous high redshift quasars using planned low frequency radio telescopes our approach is to implement a seminumerical scheme to calculate the 3dimensional structure of ionized regions surrounding a massive halo at high redshif... | [['we', 'assess', 'the', 'impact', 'of', 'inhomogeneous', 'reionization', 'on', 'detection', 'of', 'hii', 'regions', 'surrounding', 'luminous', 'high', 'redshift', 'quasars', 'using', 'planned', 'low', 'frequency', 'radio', 'telescopes', 'our', 'approach', 'is', 'to', 'implement', 'a', 'seminumerical', 'scheme', 'to', ... | [-0.062376763962259114, 0.12798008584816542, 0.007540780134565596, 0.07429221066704486, -0.06907719676133378, -0.07985695893044717, 0.06404352955619938, 0.42679500696914535, -0.12316220692924357, -0.3540340817599956, 0.07322462686695091, -0.334278346830979, 0.012663819027615578, 0.1863435219289126, 0.029935521881082294... |
708.3717 | Evidence For The Production Of Slow Antiprotonic Hydrogen In Vacuum | We present evidence showing how antiprotonic hydrogen, the quasistable
antiproton-proton (pbar-p) bound system, has been synthesized following the
interaction of antiprotons with the hydrogen molecular ion (H2+) in a nested
Penning trap environment. From a careful analysis of the spatial distributions
of antiproton a... | hep-ex | we present evidence showing how antiprotonic hydrogen the quasistable antiprotonproton pbarp bound system has been synthesized following the interaction of antiprotons with the hydrogen molecular ion h2 in a nested penning trap environment from a careful analysis of the spatial distributions of antiproton annihilation ... | [['we', 'present', 'evidence', 'showing', 'how', 'antiprotonic', 'hydrogen', 'the', 'quasistable', 'antiprotonproton', 'pbarp', 'bound', 'system', 'has', 'been', 'synthesized', 'following', 'the', 'interaction', 'of', 'antiprotons', 'with', 'the', 'hydrogen', 'molecular', 'ion', 'h2', 'in', 'a', 'nested', 'penning', 't... | [-0.07353804210249923, 0.25056072731355306, -0.058760131035294184, 0.10008480526678461, 0.068646657761603, -0.1127355255946321, 0.041251570301890174, 0.4147569912632829, -0.16293188033159822, -0.3128449337397653, -0.07386230194242671, -0.3196889883225882, 0.08782032996072973, 0.15604559764707168, 0.11478382180518422, 0... |
708.3718 | Zero product preservers of C*-algebras | Let T be be a zero-product preserving bounded linear map between C*-algebras
A and B. Here neither A nor B is necessarily unital.
In this note, we investigate when T gives rise to a Jordan homomorphism. In
particular, we show that A and B are isomorphic as Jordan algebras if T is
bijective and sends zero products o... | math.OA math.FA | let t be be a zeroproduct preserving bounded linear map between calgebras a and b here neither a nor b is necessarily unital in this note we investigate when t gives rise to a jordan homomorphism in particular we show that a and b are isomorphic as jordan algebras if t is bijective and sends zero products of selfadjoin... | [['let', 't', 'be', 'be', 'a', 'zeroproduct', 'preserving', 'bounded', 'linear', 'map', 'between', 'calgebras', 'a', 'and', 'b', 'here', 'neither', 'a', 'nor', 'b', 'is', 'necessarily', 'unital', 'in', 'this', 'note', 'we', 'investigate', 'when', 't', 'gives', 'rise', 'to', 'a', 'jordan', 'homomorphism', 'in', 'particu... | [-0.15561238933020297, 0.17766313227371144, -0.07376672874371974, -0.0017645134939812124, -0.11584933111682916, -0.2351910838057311, -0.004543058096598356, 0.4041926442908171, -0.40131775710063106, -0.11999692181602885, 0.10460879406235062, -0.3029823863210204, -0.12070554914549948, 0.11770672761859038, -0.157322219531... |
708.3719 | Evolution of Star Clusters near the Galactic Center: Fully
Self-consistent N-body Simulations | We have performed fully self-consistent $N$-body simulations of star clusters
near the Galactic center (GC). Such simulations have not been performed because
it is difficult to perform fast and accurate simulations of such systems using
conventional methods. We used the Bridge code, which integrates the parent
galaxy... | astro-ph | we have performed fully selfconsistent nbody simulations of star clusters near the galactic center gc such simulations have not been performed because it is difficult to perform fast and accurate simulations of such systems using conventional methods we used the bridge code which integrates the parent galaxy using the ... | [['we', 'have', 'performed', 'fully', 'selfconsistent', 'nbody', 'simulations', 'of', 'star', 'clusters', 'near', 'the', 'galactic', 'center', 'gc', 'such', 'simulations', 'have', 'not', 'been', 'performed', 'because', 'it', 'is', 'difficult', 'to', 'perform', 'fast', 'and', 'accurate', 'simulations', 'of', 'such', 'sy... | [-0.07194222936844402, 0.08045856007552944, -0.12385038751345433, 0.09831955710418339, -0.06856323542617913, -0.04651840991032681, 0.03977326006257062, 0.40186843912872927, -0.21539148035627165, -0.35739405256253287, 0.069438651778552, -0.2468465082773613, -0.07364574088486003, 0.17357886022292687, 0.044984384976795626... |
708.372 | Dirac concentrations in Lotka-Volterra parabolic PDEs | We consider parabolic partial differential equations of Lotka-Volterra type,
with a non-local nonlinear term. This models, at the population level, the
darwinian evolution of a population; the Laplace term represents mutations and
the nonlinear birth/death term represents competition leading to selection.
Once rescal... | math.AP | we consider parabolic partial differential equations of lotkavolterra type with a nonlocal nonlinear term this models at the population level the darwinian evolution of a population the laplace term represents mutations and the nonlinear birthdeath term represents competition leading to selection once rescaled with a s... | [['we', 'consider', 'parabolic', 'partial', 'differential', 'equations', 'of', 'lotkavolterra', 'type', 'with', 'a', 'nonlocal', 'nonlinear', 'term', 'this', 'models', 'at', 'the', 'population', 'level', 'the', 'darwinian', 'evolution', 'of', 'a', 'population', 'the', 'laplace', 'term', 'represents', 'mutations', 'and'... | [-0.12688611765898875, 0.07521080553948088, -0.08390125641530818, 0.09373877267353237, -0.11266255781725597, -0.1656772919540184, 0.02832250603579964, 0.3069315793896642, -0.30162423182114523, -0.23486686279476784, 0.0965065139633439, -0.29287965795682636, -0.17628292099834653, 0.16945851829779499, -0.09168171383327503... |
708.3721 | Verified Real Number Calculations: A Library for Interval Arithmetic | Real number calculations on elementary functions are remarkably difficult to
handle in mechanical proofs. In this paper, we show how these calculations can
be performed within a theorem prover or proof assistant in a convenient and
highly automated as well as interactive way. First, we formally establish upper
and lo... | cs.MS cs.LO | real number calculations on elementary functions are remarkably difficult to handle in mechanical proofs in this paper we show how these calculations can be performed within a theorem prover or proof assistant in a convenient and highly automated as well as interactive way first we formally establish upper and lower bo... | [['real', 'number', 'calculations', 'on', 'elementary', 'functions', 'are', 'remarkably', 'difficult', 'to', 'handle', 'in', 'mechanical', 'proofs', 'in', 'this', 'paper', 'we', 'show', 'how', 'these', 'calculations', 'can', 'be', 'performed', 'within', 'a', 'theorem', 'prover', 'or', 'proof', 'assistant', 'in', 'a', '... | [-0.11311470818179953, 0.03370563518608044, -0.1516388047916385, 0.12616305798862026, -0.12610549256010176, -0.1315062822077189, 0.10462378278794744, 0.36690851118272316, -0.2339440701672664, -0.3251473317183294, 0.10442226340870496, -0.22404435313293725, -0.15925706790392188, 0.26533201913075793, -0.08046866119253104,... |
708.3722 | Formally Verified Argument Reduction with a Fused-Multiply-Add | Cody & Waite argument reduction technique works perfectly for reasonably
large arguments but as the input grows there are no bit left to approximate the
constant with enough accuracy. Under mild assumptions, we show that the result
computed with a fused-multiply-add provides a fully accurate result for many
possible ... | cs.MS cs.PF | cody waite argument reduction technique works perfectly for reasonably large arguments but as the input grows there are no bit left to approximate the constant with enough accuracy under mild assumptions we show that the result computed with a fusedmultiplyadd provides a fully accurate result for many possible values o... | [['cody', 'waite', 'argument', 'reduction', 'technique', 'works', 'perfectly', 'for', 'reasonably', 'large', 'arguments', 'but', 'as', 'the', 'input', 'grows', 'there', 'are', 'no', 'bit', 'left', 'to', 'approximate', 'the', 'constant', 'with', 'enough', 'accuracy', 'under', 'mild', 'assumptions', 'we', 'show', 'that',... | [-0.11647667072844715, 0.016869632556211624, -0.07808258984651831, 0.0935310687801132, -0.0661046594604213, -0.18774445249070215, 0.0954888945298158, 0.36909801447684437, -0.21616466849411511, -0.34468471720559984, 0.12653479032899037, -0.22442563919103745, -0.09847488106849293, 0.24264688526367784, -0.0873988748042502... |
708.3723 | Parametric Stiffness Analysis of the Orthoglide | This paper presents a parametric stiffness analysis of the Orthoglide, a
3-DOF translational Parallel Kinematic Machine. First, a compliant modeling of
the Orthoglide is conducted based on an existing method. Then stiffness matrix
is symbolically computed. This allows one to easily study the influence of the
geometri... | cs.RO | this paper presents a parametric stiffness analysis of the orthoglide a 3dof translational parallel kinematic machine first a compliant modeling of the orthoglide is conducted based on an existing method then stiffness matrix is symbolically computed this allows one to easily study the influence of the geometric design... | [['this', 'paper', 'presents', 'a', 'parametric', 'stiffness', 'analysis', 'of', 'the', 'orthoglide', 'a', '3dof', 'translational', 'parallel', 'kinematic', 'machine', 'first', 'a', 'compliant', 'modeling', 'of', 'the', 'orthoglide', 'is', 'conducted', 'based', 'on', 'an', 'existing', 'method', 'then', 'stiffness', 'ma... | [-0.14475431397001734, 0.10852741593560877, -0.10609321494325342, -0.032298376255774905, -0.14589043501601145, -0.1754294008735502, -0.021072102725922474, 0.4174572008155417, -0.31645970624920566, -0.28135591899780066, 0.1282054553619737, -0.190987661282921, -0.16851368922691204, 0.19891425323460185, -0.059833622390502... |
708.3724 | Compton telescope with coded aperture mask: Imaging with the
INTEGRAL/IBIS Compton mode | Compton telescopes provide a good sensitivity over a wide field of view in
the difficult energy range running from a few hundred keV to several MeV. Their
angular resolution is, however, poor and strongly energy dependent. We present
a novel experimental design associating a coded mask and a Compton detection
unit to... | astro-ph | compton telescopes provide a good sensitivity over a wide field of view in the difficult energy range running from a few hundred kev to several mev their angular resolution is however poor and strongly energy dependent we present a novel experimental design associating a coded mask and a compton detection unit to overc... | [['compton', 'telescopes', 'provide', 'a', 'good', 'sensitivity', 'over', 'a', 'wide', 'field', 'of', 'view', 'in', 'the', 'difficult', 'energy', 'range', 'running', 'from', 'a', 'few', 'hundred', 'kev', 'to', 'several', 'mev', 'their', 'angular', 'resolution', 'is', 'however', 'poor', 'and', 'strongly', 'energy', 'dep... | [-0.10348729277286906, 0.07678571781112994, -0.04312886392121404, 0.032339168559420255, -0.05546805101931764, -0.07770351280467276, 0.058674953045652796, 0.403104560552628, -0.23511430975924458, -0.4057089680116315, 0.1120042094944086, -0.2853510373745381, -0.04212888833186821, 0.23953903382335331, -0.04141350246603132... |
708.3725 | Temperature Dependent Polarity Reversal in Au/Nb:SrTiO3 Schottky
Junctions | We have observed temperature-dependent reversal of the rectifying polarity in
Au/Nb:SrTiO3 Schottky junctions. By simulating current-voltage characteristics
we have found that the permittivity of SrTiO3 near the interface exhibits
temperature dependence opposite to that observed in the bulk, significantly
reducing th... | cond-mat.str-el cond-mat.mtrl-sci | we have observed temperaturedependent reversal of the rectifying polarity in aunbsrtio3 schottky junctions by simulating currentvoltage characteristics we have found that the permittivity of srtio3 near the interface exhibits temperature dependence opposite to that observed in the bulk significantly reducing the barrie... | [['we', 'have', 'observed', 'temperaturedependent', 'reversal', 'of', 'the', 'rectifying', 'polarity', 'in', 'aunbsrtio3', 'schottky', 'junctions', 'by', 'simulating', 'currentvoltage', 'characteristics', 'we', 'have', 'found', 'that', 'the', 'permittivity', 'of', 'srtio3', 'near', 'the', 'interface', 'exhibits', 'temp... | [-0.19144109938317885, 0.17171575981131815, -0.04349556063942901, -0.008651209015447598, -0.05040752103056323, -0.1731849390916623, 0.05522537213000288, 0.42918631560229636, -0.2798951203366379, -0.32104383254206026, -0.060948379558523176, -0.2920954901870195, -0.12845907410812357, 0.22363124694675207, 0.01686828662097... |
708.3726 | Nonadiabatic factor accompanying magnetic translation of a charged
particle | The quantum adiabatic theorem incorporating the Berry phase phenomenon can be
characterized as a factorization of the time evolution operator into a
path-dependent geometric factor, a usual dynamical factor and a non-adiabatic
factor that approaches the identity in the adiabatic limit. We study a case
where all these... | quant-ph | the quantum adiabatic theorem incorporating the berry phase phenomenon can be characterized as a factorization of the time evolution operator into a pathdependent geometric factor a usual dynamical factor and a nonadiabatic factor that approaches the identity in the adiabatic limit we study a case where all these three... | [['the', 'quantum', 'adiabatic', 'theorem', 'incorporating', 'the', 'berry', 'phase', 'phenomenon', 'can', 'be', 'characterized', 'as', 'a', 'factorization', 'of', 'the', 'time', 'evolution', 'operator', 'into', 'a', 'pathdependent', 'geometric', 'factor', 'a', 'usual', 'dynamical', 'factor', 'and', 'a', 'nonadiabatic'... | [-0.1796597800459023, 0.20873503227154783, -0.0967073167996182, 0.07082179733293338, -0.01604736499764301, -0.11737520314528849, 0.05394386743298835, 0.3188106430073579, -0.285829041486629, -0.25112618328888475, 0.06937229059878047, -0.21189865266421326, -0.1613150840786136, 0.14869797510313398, 0.003440075387235409, 0... |
708.3727 | Galois cohomology of completed link groups | In this paper we compute the Galois cohomology of the pro-p completion of
primitive link groups. Here, a primitive link group is the fundamental group of
a tame link in the 3-sphere whose linking number diagram is irreducible modulo
p (e.g. none of the linking numbers is divisible by p).
The result is that (with Z/... | math.GR math.AG | in this paper we compute the galois cohomology of the prop completion of primitive link groups here a primitive link group is the fundamental group of a tame link in the 3sphere whose linking number diagram is irreducible modulo p eg none of the linking numbers is divisible by p the result is that with zpzcoefficients ... | [['in', 'this', 'paper', 'we', 'compute', 'the', 'galois', 'cohomology', 'of', 'the', 'prop', 'completion', 'of', 'primitive', 'link', 'groups', 'here', 'a', 'primitive', 'link', 'group', 'is', 'the', 'fundamental', 'group', 'of', 'a', 'tame', 'link', 'in', 'the', '3sphere', 'whose', 'linking', 'number', 'diagram', 'is... | [-0.22993721168066533, 0.12463259105658475, -0.1456955699074381, 0.0830308984078792, -0.12560084225820764, -0.13285779611225118, 0.006742954919694589, 0.314013526856214, -0.38718038706003494, -0.2568755574910989, 0.12397684649573112, -0.22556439810432494, -0.1773524279953288, 0.17615607986665982, -0.15605593363772025, ... |
708.3728 | Quasi-particle interference and superconducting gap in a
high-temperature superconductor Ca2-xNaxCuO2Cl2 | High-transition-temperature (high-Tc) superconductivity is ubiquitous in the
cuprates containing CuO2 planes but each cuprate has its own character. The
study of the material dependence of the d-wave superconducting gap (SG) should
provide important insights into the mechanism of high-Tc. However, because of
the 'pse... | cond-mat.supr-con cond-mat.str-el | hightransitiontemperature hightc superconductivity is ubiquitous in the cuprates containing cuo2 planes but each cuprate has its own character the study of the material dependence of the dwave superconducting gap sg should provide important insights into the mechanism of hightc however because of the pseudogap phenomen... | [['hightransitiontemperature', 'hightc', 'superconductivity', 'is', 'ubiquitous', 'in', 'the', 'cuprates', 'containing', 'cuo2', 'planes', 'but', 'each', 'cuprate', 'has', 'its', 'own', 'character', 'the', 'study', 'of', 'the', 'material', 'dependence', 'of', 'the', 'dwave', 'superconducting', 'gap', 'sg', 'should', 'p... | [-0.1647320528569467, 0.16862739456461415, -0.09570342698956237, 0.06415955607286271, -0.0731674873502925, -0.1499205149628003, 0.12020151295308845, 0.3783020445912638, -0.22494121244286788, -0.30128196003874214, -0.01775298683274099, -0.35780966934912345, -0.1312682752004441, 0.18501716905876117, 0.004595110957127284,... |
708.3729 | From Unruh temperature to generalized Bousso bound | In a classical spacetime satisfying Einstein's equation and the null
convergence condition, the same quantum mechanical effects that cause black
holes to have a temperature are found to imply, if joined to the macroscopic
nature of entropy, the covariant entropy bound in its generalized form. This is
obtained from th... | gr-qc | in a classical spacetime satisfying einsteins equation and the null convergence condition the same quantum mechanical effects that cause black holes to have a temperature are found to imply if joined to the macroscopic nature of entropy the covariant entropy bound in its generalized form this is obtained from thermodyn... | [['in', 'a', 'classical', 'spacetime', 'satisfying', 'einsteins', 'equation', 'and', 'the', 'null', 'convergence', 'condition', 'the', 'same', 'quantum', 'mechanical', 'effects', 'that', 'cause', 'black', 'holes', 'to', 'have', 'a', 'temperature', 'are', 'found', 'to', 'imply', 'if', 'joined', 'to', 'the', 'macroscopic... | [-0.17822463260736407, 0.1342600365510074, -0.15484717708626172, 0.09443265449528288, -0.08532193827828984, -0.1619911751335078, 0.01958265845811494, 0.23009613749184987, -0.24821752098547975, -0.2317278399416132, 0.018029811743805867, -0.30962820474921565, -0.08017708685975976, 0.15194144955887345, -0.0634095263780980... |
708.373 | Densities for Rough Differential Equations under Hoermander's Condition | We consider stochastic differential equations dY=V(Y)dX driven by a
multidimensional Gaussian process X in the rough path sense. Using Malliavin
Calculus we show that Y(t) admits a density for t in (0,T] provided (i) the
vector fields V=(V_1,...,V_d) satisfy Hoermander's condition and (ii) the
Gaussian driving signal... | math.PR | we consider stochastic differential equations dyvydx driven by a multidimensional gaussian process x in the rough path sense using malliavin calculus we show that yt admits a density for t in 0t provided i the vector fields vv_1v_d satisfy hoermanders condition and ii the gaussian driving signal x satisfies certain con... | [['we', 'consider', 'stochastic', 'differential', 'equations', 'dyvydx', 'driven', 'by', 'a', 'multidimensional', 'gaussian', 'process', 'x', 'in', 'the', 'rough', 'path', 'sense', 'using', 'malliavin', 'calculus', 'we', 'show', 'that', 'yt', 'admits', 'a', 'density', 'for', 't', 'in', '0t', 'provided', 'i', 'the', 've... | [-0.13489903285596017, 0.16058023170744246, -0.08525628137175699, 0.036363359183834855, -0.10840047784841846, -0.1760283251846763, 0.023528884680992044, 0.38298441422788576, -0.36890807812026627, -0.18733731453382485, 0.09025775163900107, -0.267717833983133, -0.13078299227699236, 0.17515045906593268, -0.110509971886671... |
708.3731 | Differences between charged-current coefficient functions | Second- and third-order results are presented for the structure functions of
charged-current deep-inelastic scattering in the framework of massless
perturbative QCD. We write down the two-loop differences between the
corresponding crossing-even and -odd coefficient functions, including those for
the longitudinal stru... | hep-ph | second and thirdorder results are presented for the structure functions of chargedcurrent deepinelastic scattering in the framework of massless perturbative qcd we write down the twoloop differences between the corresponding crossingeven and odd coefficient functions including those for the longitudinal structure funct... | [['second', 'and', 'thirdorder', 'results', 'are', 'presented', 'for', 'the', 'structure', 'functions', 'of', 'chargedcurrent', 'deepinelastic', 'scattering', 'in', 'the', 'framework', 'of', 'massless', 'perturbative', 'qcd', 'we', 'write', 'down', 'the', 'twoloop', 'differences', 'between', 'the', 'corresponding', 'cr... | [-0.09125261274930924, 0.14153577517909208, -0.050601029476679084, 0.14288311166890355, -0.04791478319927605, -0.027537156327335693, 0.019955470393509117, 0.3544636730950868, -0.2338887249421912, -0.26106554348327554, 0.0282605182763481, -0.3527353927840604, -0.11528719640371682, 0.16066172582952223, 0.1020840386438284... |
708.3732 | Evolution of the gaps through the cuprate phase-diagram | The actual physical origin of the gap at the antinodes, and a clear
identification of the superconducting gap are fundamental open issues in the
physics of high-$T_c$ superconductors. Here, we present a systematic electronic
Raman scattering study of a mercury-based single layer cuprate, as a function
of both doping ... | cond-mat.supr-con cond-mat.str-el | the actual physical origin of the gap at the antinodes and a clear identification of the superconducting gap are fundamental open issues in the physics of hight_c superconductors here we present a systematic electronic raman scattering study of a mercurybased single layer cuprate as a function of both doping level and ... | [['the', 'actual', 'physical', 'origin', 'of', 'the', 'gap', 'at', 'the', 'antinodes', 'and', 'a', 'clear', 'identification', 'of', 'the', 'superconducting', 'gap', 'are', 'fundamental', 'open', 'issues', 'in', 'the', 'physics', 'of', 'hight_c', 'superconductors', 'here', 'we', 'present', 'a', 'systematic', 'electronic... | [-0.18464720262451456, 0.16390371131976217, -0.08515140283934511, 0.05833569062228331, -0.0653370337717557, -0.14098217881595096, 0.19255504383615693, 0.3510073946560161, -0.2813214744671489, -0.24924084085796494, 0.02207903096068389, -0.3574964428451239, -0.10617084350240857, 0.15945536959426185, 0.009123678008204718,... |
708.3733 | Luminosity function, sizes and FR dichotomy of radio-loud AGN | The radio luminosity function (RLF) of radio galaxies and radio-loud quasars
is often modelled as a broken power-law. The break luminosity is close to the
dividing line between the two Fanaroff-Riley (FR) morphological classes for the
large-scale radio structure of these objects. We use an analytical model for
the lu... | astro-ph | the radio luminosity function rlf of radio galaxies and radioloud quasars is often modelled as a broken powerlaw the break luminosity is close to the dividing line between the two fanaroffriley fr morphological classes for the largescale radio structure of these objects we use an analytical model for the luminosity and... | [['the', 'radio', 'luminosity', 'function', 'rlf', 'of', 'radio', 'galaxies', 'and', 'radioloud', 'quasars', 'is', 'often', 'modelled', 'as', 'a', 'broken', 'powerlaw', 'the', 'break', 'luminosity', 'is', 'close', 'to', 'the', 'dividing', 'line', 'between', 'the', 'two', 'fanaroffriley', 'fr', 'morphological', 'classes... | [-0.06030077192157802, 0.09383189645356678, -0.07573530823010334, 0.13033319828894555, -0.09962273671379368, -0.08854112096850088, 0.015539355755415929, 0.4435216566308005, -0.1784762356575523, -0.324311929247757, 0.03866939555904321, -0.2647347922486168, -0.01840063258844179, 0.18015627201535914, 0.004251794720133121,... |
708.3734 | Searching for a dangerous host: randomized vs. deterministic | A Black Hole is an harmful host in a network that destroys incoming agents
without leaving any trace of such event. The problem of locating the black hole
in a network through a team of agent coordinated by a common protocol is
usually referred in literature as the Black Hole Search problem (or BHS for
brevity) and i... | cs.DC | a black hole is an harmful host in a network that destroys incoming agents without leaving any trace of such event the problem of locating the black hole in a network through a team of agent coordinated by a common protocol is usually referred in literature as the black hole search problem or bhs for brevity and it is ... | [['a', 'black', 'hole', 'is', 'an', 'harmful', 'host', 'in', 'a', 'network', 'that', 'destroys', 'incoming', 'agents', 'without', 'leaving', 'any', 'trace', 'of', 'such', 'event', 'the', 'problem', 'of', 'locating', 'the', 'black', 'hole', 'in', 'a', 'network', 'through', 'a', 'team', 'of', 'agent', 'coordinated', 'by'... | [-0.12014306970297976, 0.07946916654817518, -0.05270219276806727, 0.10627559358645969, -0.06990251038281137, -0.15768136601148192, 0.07848423063503762, 0.3394880756311635, -0.21883743236966358, -0.30098523303294683, 0.10878660078079781, -0.2894895991637823, -0.1336130892966256, 0.18307369808426663, -0.11020377531934686... |
708.3735 | Pattern formation in the damped Nikolaevskiy equation | The Nikolaevskiy equation has been proposed as a model for seismic waves,
electroconvection and weak turbulence; we show that it can also be used to
model transverse instabilities of fronts. This equation possesses a large-scale
"Goldstone" mode that significantly influences the stability of spatially
periodic steady... | nlin.PS | the nikolaevskiy equation has been proposed as a model for seismic waves electroconvection and weak turbulence we show that it can also be used to model transverse instabilities of fronts this equation possesses a largescale goldstone mode that significantly influences the stability of spatially periodic steady solutio... | [['the', 'nikolaevskiy', 'equation', 'has', 'been', 'proposed', 'as', 'a', 'model', 'for', 'seismic', 'waves', 'electroconvection', 'and', 'weak', 'turbulence', 'we', 'show', 'that', 'it', 'can', 'also', 'be', 'used', 'to', 'model', 'transverse', 'instabilities', 'of', 'fronts', 'this', 'equation', 'possesses', 'a', 'l... | [-0.20171219408996618, 0.1426204605932439, -0.09762204044654621, 0.06444719155868138, -0.07201146378284158, -0.11574607197130692, 0.001882827227041556, 0.28935508396088905, -0.2763632256645343, -0.2151316733697074, 0.14458832312025388, -0.2810608325923142, -0.1557030269436705, 0.19850813241869297, 0.030693742766911756,... |
708.3736 | A convergent finite difference method for a nonlinear variational wave
equation | We establish rigorously convergence of a semi-discrete upwind scheme for the
nonlinear variational wave equation $u_{tt} - c(u)(c(u) u_x)_x = 0$ with
$u|_{t=0}=u_0$ and $u_t|_{t=0}=v_0$. Introducing Riemann invariants $R=u_t+c
u_x$ and $S=u_t-c u_x$, the variational wave equation is equivalent to $R_t-c
R_x=\tilde c ... | math.AP math.NA | we establish rigorously convergence of a semidiscrete upwind scheme for the nonlinear variational wave equation u_tt cucu u_x_x 0 with u_t0u_0 and u_t_t0v_0 introducing riemann invariants ru_tc u_x and su_tc u_x the variational wave equation is equivalent to r_tc r_xtilde c r2s2 and s_tc s_xtilde c r2s2 with tilde cc4c... | [['we', 'establish', 'rigorously', 'convergence', 'of', 'a', 'semidiscrete', 'upwind', 'scheme', 'for', 'the', 'nonlinear', 'variational', 'wave', 'equation', 'u_tt', 'cucu', 'u_x_x', '0', 'with', 'u_t0u_0', 'and', 'u_t_t0v_0', 'introducing', 'riemann', 'invariants', 'ru_tc', 'u_x', 'and', 'su_tc', 'u_x', 'the', 'varia... | [-0.18273641037788377, 0.09224256274661369, -0.04934670073323861, 0.025300862908598978, -0.06671144315097706, -0.20989515698593425, -0.025895517622401196, 0.3543948187346918, -0.33358112475778684, -0.18547245143093619, 0.12971493019441882, -0.3413729502662388, -0.09667135665125876, 0.19311401414045368, -0.0038540460820... |
708.3737 | Joint deprojection of Sunyaev-Zeldovich and X-ray images of galaxy
clusters | We present two non-parametric deprojection methods aimed at recovering the
three-dimensional density and temperature profiles of galaxy clusters from
spatially resolved thermal Sunyaev-Zeldovich (tSZ) and X-ray surface brightness
maps, thus avoiding the use of X-ray spectroscopic data. In both methods,
clusters are a... | astro-ph | we present two nonparametric deprojection methods aimed at recovering the threedimensional density and temperature profiles of galaxy clusters from spatially resolved thermal sunyaevzeldovich tsz and xray surface brightness maps thus avoiding the use of xray spectroscopic data in both methods clusters are assumed to be... | [['we', 'present', 'two', 'nonparametric', 'deprojection', 'methods', 'aimed', 'at', 'recovering', 'the', 'threedimensional', 'density', 'and', 'temperature', 'profiles', 'of', 'galaxy', 'clusters', 'from', 'spatially', 'resolved', 'thermal', 'sunyaevzeldovich', 'tsz', 'and', 'xray', 'surface', 'brightness', 'maps', 't... | [-0.06802112858125905, 0.06796883519505004, -0.08227456914502437, 0.06016285938547096, -0.05456848946417234, -0.07171692724374157, 0.04467806387261522, 0.41294459545708917, -0.24056288759327596, -0.3344762951152882, 0.054241203672049945, -0.2931274212815441, -0.013621185852119837, 0.18405930414662214, 0.007562636410714... |
708.3738 | Killing superalgebra deformations of ten-dimensional supergravity
backgrounds | We explore Lie superalgebra deformations of the Killing superalgebras of some
ten-dimensional supergravity backgrounds. We prove the rigidity of the Poincare
superalgebras in types I, IIA and IIB, as well as of the Killing superalgebra
of the Freund-Rubin vacuum of type IIB supergravity. We also prove rigidity of
the... | hep-th | we explore lie superalgebra deformations of the killing superalgebras of some tendimensional supergravity backgrounds we prove the rigidity of the poincare superalgebras in types i iia and iib as well as of the killing superalgebra of the freundrubin vacuum of type iib supergravity we also prove rigidity of the killing... | [['we', 'explore', 'lie', 'superalgebra', 'deformations', 'of', 'the', 'killing', 'superalgebras', 'of', 'some', 'tendimensional', 'supergravity', 'backgrounds', 'we', 'prove', 'the', 'rigidity', 'of', 'the', 'poincare', 'superalgebras', 'in', 'types', 'i', 'iia', 'and', 'iib', 'as', 'well', 'as', 'of', 'the', 'killing... | [-0.16101985534623964, 0.08931346354256675, 0.020057030678799492, 0.12019013258941413, -0.13685754675680073, -0.23333424997326802, -0.06587313441377773, 0.2694272143635317, -0.1418438856198918, -0.19701591192097112, 0.12735519895068137, -0.2836483436403796, -0.18869928495405475, 0.05326761682954384, -0.1398246180760907... |
708.3739 | Exact Statistical Mechanical Investigation of a Finite Model Protein in
its environment: A Small System Paradigm | We consider a general incompressible finite model protein of size M in its
environment, which we represent by a semiflexible copolymer consisting of amino
acid residues classified into only two species (H and P, see text) following
Lau and Dill. We allow various interactions between chemically unbonded
residues in a ... | cond-mat.stat-mech q-bio.BM | we consider a general incompressible finite model protein of size m in its environment which we represent by a semiflexible copolymer consisting of amino acid residues classified into only two species h and p see text following lau and dill we allow various interactions between chemically unbonded residues in a given s... | [['we', 'consider', 'a', 'general', 'incompressible', 'finite', 'model', 'protein', 'of', 'size', 'm', 'in', 'its', 'environment', 'which', 'we', 'represent', 'by', 'a', 'semiflexible', 'copolymer', 'consisting', 'of', 'amino', 'acid', 'residues', 'classified', 'into', 'only', 'two', 'species', 'h', 'and', 'p', 'see', ... | [-0.10476785883336176, 0.17492146882038032, -0.09214789107147531, 0.10265875612549681, -0.02726652073706726, -0.14974835471533207, 0.060082818231738215, 0.39612759612008336, -0.24101939635855937, -0.2684257753308255, 0.029604587353158757, -0.26096205189235616, -0.13305414479229977, 0.13939261149424273, -0.0235609824949... |
708.374 | Plate-forme Magicien d'Oz pour l'\'etude de l'apport des ACAs \`a
l'interaction | In order to evaluate the contribution of Embodied (Animated) Conversational
Agents (ECAs) to the effectiveness and usability of human-computer interaction,
we developed a software platform meant to collect usage data. This platform,
which implements the wizard of Oz paradigm, makes it possible to simulate user
interf... | cs.HC | in order to evaluate the contribution of embodied animated conversational agents ecas to the effectiveness and usability of humancomputer interaction we developed a software platform meant to collect usage data this platform which implements the wizard of oz paradigm makes it possible to simulate user interfaces integr... | [['in', 'order', 'to', 'evaluate', 'the', 'contribution', 'of', 'embodied', 'animated', 'conversational', 'agents', 'ecas', 'to', 'the', 'effectiveness', 'and', 'usability', 'of', 'humancomputer', 'interaction', 'we', 'developed', 'a', 'software', 'platform', 'meant', 'to', 'collect', 'usage', 'data', 'this', 'platform... | [-0.07214891168450077, -0.00916405853170615, -0.10400013061410461, 0.08553054662188515, -0.190648719894055, -0.22637104497004587, 0.04444553059024307, 0.40786445069198424, -0.23015963511828047, -0.33746182464931807, 0.04336006362618019, -0.3130413914636637, -0.17060202713160275, 0.1819490062359434, -0.1252924291130442,... |
708.3741 | The correct relatively stable category for idempotent modules | We answer a question posed by Carlson, Peng, and Wheeler, and demonstrate
that in general Rickard modules in relatively stable categories are not
idempotent modules even if one localizes with respect to a tensor ideal
subcategory. We also show that there is a modification one can make so as to
recover the idempotent ... | math.RT | we answer a question posed by carlson peng and wheeler and demonstrate that in general rickard modules in relatively stable categories are not idempotent modules even if one localizes with respect to a tensor ideal subcategory we also show that there is a modification one can make so as to recover the idempotent behavi... | [['we', 'answer', 'a', 'question', 'posed', 'by', 'carlson', 'peng', 'and', 'wheeler', 'and', 'demonstrate', 'that', 'in', 'general', 'rickard', 'modules', 'in', 'relatively', 'stable', 'categories', 'are', 'not', 'idempotent', 'modules', 'even', 'if', 'one', 'localizes', 'with', 'respect', 'to', 'a', 'tensor', 'ideal'... | [-0.07836267670306067, 0.06296936438108484, -0.07528339790318299, 0.11806544898017482, -0.0991341056716111, -0.2189491388163771, -0.034458692047607015, 0.4069697940377174, -0.36479769857531347, -0.2159272719970128, 0.11576270932521394, -0.2658528510256912, -0.1772814360619695, 0.16797301366373343, -0.19229410528377802,... |
708.3742 | Interfaces adaptatives Adaptation dynamique \`a l'utilisateur courant | We present a survey of recent research studies of the implementation of
adaptive user models in human-computer interaction. A classification of
research directions on adaptive user interfaces is first proposed; it takes
account of the user characteristics that are modelled, the distribution of
initiative and control ... | cs.HC | we present a survey of recent research studies of the implementation of adaptive user models in humancomputer interaction a classification of research directions on adaptive user interfaces is first proposed it takes account of the user characteristics that are modelled the distribution of initiative and control of the... | [['we', 'present', 'a', 'survey', 'of', 'recent', 'research', 'studies', 'of', 'the', 'implementation', 'of', 'adaptive', 'user', 'models', 'in', 'humancomputer', 'interaction', 'a', 'classification', 'of', 'research', 'directions', 'on', 'adaptive', 'user', 'interfaces', 'is', 'first', 'proposed', 'it', 'takes', 'acco... | [-0.1496185559010849, -0.01283466140187186, -0.0603488568233809, 0.025898675704849192, -0.10979337815229816, -0.14939003672743975, 0.03529165791459726, 0.42173999913588717, -0.22596054894987633, -0.3327238566190418, 0.09758168159061353, -0.25854453051686976, -0.20391433816446267, 0.1986816604104307, -0.0746187557837132... |
708.3743 | The Universe expansion and Energy problems | In this paper we construct a physical modelization of the universe expansion.
The universe then reduces to a Riemannian space $0.2cm$ $(B(O,R(t)),g_t)$,
where $R(t) \sim t$ for $t \gg $0, and $g_t$ is a time - dependent Riemannian
metric which reflects and characterizes the dynamical matter - energy
distribution $E_t... | physics.gen-ph | in this paper we construct a physical modelization of the universe expansion the universe then reduces to a riemannian space 02cm bortg_t where rt sim t for t gg 0 and g_t is a time dependent riemannian metric which reflects and characterizes the dynamical matter energy distribution e_tx on bort according to the mach e... | [['in', 'this', 'paper', 'we', 'construct', 'a', 'physical', 'modelization', 'of', 'the', 'universe', 'expansion', 'the', 'universe', 'then', 'reduces', 'to', 'a', 'riemannian', 'space', '02cm', 'bortg_t', 'where', 'rt', 'sim', 't', 'for', 't', 'gg', '0', 'and', 'g_t', 'is', 'a', 'time', 'dependent', 'riemannian', 'met... | [-0.09957230787956181, 0.13978966035343823, -0.09739904722619208, 0.09892090285379904, -0.10566002459189192, -0.13630239888599888, 0.012893151203333491, 0.2834718996062802, -0.278270992042736, -0.3084974401713809, 0.0476496394144748, -0.23802817177404795, -0.09703075908149814, 0.18467868242960003, -0.046052799542010525... |
708.3744 | The Aharonov-Casher effect | The Aharonov-Casher effect, entry in the Compendium of Quantum Physics:
Concepts, Experiments, History and Philosophy, ed. F. Weinert, K. Hentschel, D.
Greenberger and B. Falkenburg (Springer), to appear
| quant-ph | the aharonovcasher effect entry in the compendium of quantum physics concepts experiments history and philosophy ed f weinert k hentschel d greenberger and b falkenburg springer to appear | [['the', 'aharonovcasher', 'effect', 'entry', 'in', 'the', 'compendium', 'of', 'quantum', 'physics', 'concepts', 'experiments', 'history', 'and', 'philosophy', 'ed', 'f', 'weinert', 'k', 'hentschel', 'd', 'greenberger', 'and', 'b', 'falkenburg', 'springer', 'to', 'appear']] | [-0.163638326106593, 0.1240095988448177, -0.12878226733300835, 0.0005851871932723693, -0.11255211842113308, -0.1968951397575438, 0.049432371834492575, 0.21032625134103, -0.29833718169746654, -0.33199539840487496, 0.008414441998216457, -0.291837135995073, -0.17364261685205357, 0.14028615990121449, -0.09002115058579616, ... |
708.3745 | Spectral Mapping Reconstruction of Extended Sources | Three dimensional spectroscopy of extended sources is typically performed
with dedicated integral field spectrographs. We describe a method of
reconstructing full spectral cubes, with two spatial and one spectral
dimension, from rastered spectral mapping observations employing a single slit
in a traditional slit spec... | astro-ph | three dimensional spectroscopy of extended sources is typically performed with dedicated integral field spectrographs we describe a method of reconstructing full spectral cubes with two spatial and one spectral dimension from rastered spectral mapping observations employing a single slit in a traditional slit spectrogr... | [['three', 'dimensional', 'spectroscopy', 'of', 'extended', 'sources', 'is', 'typically', 'performed', 'with', 'dedicated', 'integral', 'field', 'spectrographs', 'we', 'describe', 'a', 'method', 'of', 'reconstructing', 'full', 'spectral', 'cubes', 'with', 'two', 'spatial', 'and', 'one', 'spectral', 'dimension', 'from',... | [-0.07801732605774746, 0.039727586557891104, -0.10559933499263768, 0.07724728052077505, -0.11347526801171515, -0.18735761114988814, -0.011674776186489245, 0.4920380421434388, -0.23127622313966806, -0.3263010626418911, 0.14812768664242784, -0.23361935680661577, -0.07077768258044892, 0.249135038878938, -0.050357326786483... |
708.3746 | Energy-dependent tunnelling from few-electron dynamic quantum dots | We measure the electron escape-rate from surface-acoustic-wave dynamic
quantum dots (QDs) through a tunnel barrier. Rate-equations are used to extract
the tunnelling rates, which change by an order of magnitude with tunnel-barrier
gate voltage. We find that the tunnelling rates depend on the number of
electrons in ea... | cond-mat.mes-hall cond-mat.other | we measure the electron escaperate from surfaceacousticwave dynamic quantum dots qds through a tunnel barrier rateequations are used to extract the tunnelling rates which change by an order of magnitude with tunnelbarrier gate voltage we find that the tunnelling rates depend on the number of electrons in each dynamic q... | [['we', 'measure', 'the', 'electron', 'escaperate', 'from', 'surfaceacousticwave', 'dynamic', 'quantum', 'dots', 'qds', 'through', 'a', 'tunnel', 'barrier', 'rateequations', 'are', 'used', 'to', 'extract', 'the', 'tunnelling', 'rates', 'which', 'change', 'by', 'an', 'order', 'of', 'magnitude', 'with', 'tunnelbarrier', ... | [-0.0974498259421024, 0.17088028866839725, -0.011082337812210123, 0.08004152873117062, 0.038936750380930286, -0.17296892910316172, 0.07176566522878905, 0.3789669506355292, -0.25323126570114657, -0.35478382574187384, -0.010751328357340146, -0.30533593646768065, -0.057949618113020226, 0.2344486577151757, 0.01119347925608... |
708.3747 | Special correspondences and Chow traces of Landweber-Novikov operations | We prove that the function field of a variety which possesses a special
correspondence in the sense of M. Rost preserves the rationality of cycles of
small codimensions. This fact was proven by Vishik in the case of quadrics and
played the crucial role in his construction of fields with $u$-invariant
$2^r+1$. The mai... | math.AG | we prove that the function field of a variety which possesses a special correspondence in the sense of m rost preserves the rationality of cycles of small codimensions this fact was proven by vishik in the case of quadrics and played the crucial role in his construction of fields with uinvariant 2r1 the main technical ... | [['we', 'prove', 'that', 'the', 'function', 'field', 'of', 'a', 'variety', 'which', 'possesses', 'a', 'special', 'correspondence', 'in', 'the', 'sense', 'of', 'm', 'rost', 'preserves', 'the', 'rationality', 'of', 'cycles', 'of', 'small', 'codimensions', 'this', 'fact', 'was', 'proven', 'by', 'vishik', 'in', 'the', 'cas... | [-0.23714860242960806, 0.026446729321667754, -0.13335398100422358, 0.0901325069082139, -0.036053090954241765, -0.09309377256167037, -0.01118419200330126, 0.25755741698032414, -0.2783558840164915, -0.2643905774351548, 0.07828639206391844, -0.18058647379670714, -0.213795485408892, 0.23588244724669494, -0.1790773789927532... |
708.3748 | Unveiling the nature and interaction of the intermediate/high-mass YSOs
in IRAS 20343+4129 | In order to elucidate the nature of the brightest infrared sources associated
with IRAS 20343+4129, IRS1 and IRS3, we observed with the Submillimeter Array
(SMA) the 1.3 mm continuum and CO(2-1) emission of the region. Faint millimeter
dust continuum emission was detected toward IRS1, and we derived an associated
gas... | astro-ph | in order to elucidate the nature of the brightest infrared sources associated with iras 203434129 irs1 and irs3 we observed with the submillimeter array sma the 13 mm continuum and co21 emission of the region faint millimeter dust continuum emission was detected toward irs1 and we derived an associated gas mass of 08 m... | [['in', 'order', 'to', 'elucidate', 'the', 'nature', 'of', 'the', 'brightest', 'infrared', 'sources', 'associated', 'with', 'iras', '203434129', 'irs1', 'and', 'irs3', 'we', 'observed', 'with', 'the', 'submillimeter', 'array', 'sma', 'the', '13', 'mm', 'continuum', 'and', 'co21', 'emission', 'of', 'the', 'region', 'fai... | [-0.08342876568426212, 0.08396257789552589, 0.01901536362389542, 0.03919917310500987, -0.09440892353669052, -0.08884190776805598, -0.04519805792630158, 0.5215383325589866, -0.15577567481540894, -0.2686317072200733, 0.10039534407991507, -0.295504378816217, -0.009338627228649652, 0.1128306659698066, 0.026269998949170644,... |
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