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 |
|---|---|---|---|---|---|---|
710.2853 | Exotic hadrons and SU(3) chiral dynamics | We explore a possibility to generate exotic hadrons dynamically in the
scattering of hadrons. The s-wave scattering amplitude of an arbitrary hadron
with the Nambu-Goldstone boson is constructed so as to satisfy the unitarity
condition and the chiral low energy theorem. We find that the chiral
interaction for the exo... | hep-ph nucl-th | we explore a possibility to generate exotic hadrons dynamically in the scattering of hadrons the swave scattering amplitude of an arbitrary hadron with the nambugoldstone boson is constructed so as to satisfy the unitarity condition and the chiral low energy theorem we find that the chiral interaction for the exotic ch... | [['we', 'explore', 'a', 'possibility', 'to', 'generate', 'exotic', 'hadrons', 'dynamically', 'in', 'the', 'scattering', 'of', 'hadrons', 'the', 'swave', 'scattering', 'amplitude', 'of', 'an', 'arbitrary', 'hadron', 'with', 'the', 'nambugoldstone', 'boson', 'is', 'constructed', 'so', 'as', 'to', 'satisfy', 'the', 'unita... | [-0.17689186547606908, 0.25919397511744235, -0.11591039833836947, 0.1506624154755156, -0.07734878490359902, -0.18313690251670778, 0.011338413805114451, 0.3332239344060697, -0.24432573018323941, -0.26402567811655225, 0.003364492159259195, -0.29359156853967794, -0.0980742642423138, 0.10194501372192193, 0.0741799612081161... |
710.2854 | Diffraction in low-energy electron scattering from DNA: bridging gas
phase and solid state theory | Using high-quality gas phase electron scattering calculations and multiple
scattering theory, we attempt to gain insights on the radiation damage to DNA
induced by secondary low-energy electrons in the condensed phase, and to bridge
the existing gap with the gas phase theory and experiments. The origin of
different r... | physics.chem-ph physics.bio-ph | using highquality gas phase electron scattering calculations and multiple scattering theory we attempt to gain insights on the radiation damage to dna induced by secondary lowenergy electrons in the condensed phase and to bridge the existing gap with the gas phase theory and experiments the origin of different resonant... | [['using', 'highquality', 'gas', 'phase', 'electron', 'scattering', 'calculations', 'and', 'multiple', 'scattering', 'theory', 'we', 'attempt', 'to', 'gain', 'insights', 'on', 'the', 'radiation', 'damage', 'to', 'dna', 'induced', 'by', 'secondary', 'lowenergy', 'electrons', 'in', 'the', 'condensed', 'phase', 'and', 'to... | [-0.07417667616813349, 0.181051433452513, -0.07221932082936383, 0.05474370840322766, -0.026330787108104298, -0.1043129298242106, 0.0844026069001605, 0.4151363177899865, -0.29744821765284607, -0.3246598335495893, 0.0162919235409008, -0.39481521002354397, -0.11653276273400347, 0.16762317567591326, 0.03856565718255613, 0.... |
710.2855 | Comparison between 2-D and 3-D codes in dynamical simulations of gas
flow in barred galaxies | Context: One of the ways to determine the contribution of the dark halo to
the gravitational potential of a galaxy is the study of non-circular
(streaming) motions and the associated gas shocks in the bar region. These
motions, determined by the potential in the inner parts, can break the
disk-halo degeneracy. Here, ... | astro-ph | context one of the ways to determine the contribution of the dark halo to the gravitational potential of a galaxy is the study of noncircular streaming motions and the associated gas shocks in the bar region these motions determined by the potential in the inner parts can break the diskhalo degeneracy here two main flu... | [['context', 'one', 'of', 'the', 'ways', 'to', 'determine', 'the', 'contribution', 'of', 'the', 'dark', 'halo', 'to', 'the', 'gravitational', 'potential', 'of', 'a', 'galaxy', 'is', 'the', 'study', 'of', 'noncircular', 'streaming', 'motions', 'and', 'the', 'associated', 'gas', 'shocks', 'in', 'the', 'bar', 'region', 't... | [-0.09531232311906787, 0.04468706104910859, -0.09416809348169176, 0.06440281752854798, -0.015553024378698944, -0.057769873348258484, -0.0363411506135548, 0.3628092283514272, -0.24104290308927703, -0.3227676528462228, 0.041567109372848084, -0.25429208969834866, -0.07852888291142256, 0.18657060390363303, -0.0069962872925... |
710.2856 | An asymptotic integral representation for Carleman orthogonal
polynomials | In this paper we investigate the asymptotic behavior of polynomials that are
orthonormal over the interior domain of an analytic Jordan curve L with respect
to area measure. We prove that, inside L, these polynomials behave
asymptotically like a sequence of certain integrals involving the canonical
conformal map of t... | math.CA math.CV | in this paper we investigate the asymptotic behavior of polynomials that are orthonormal over the interior domain of an analytic jordan curve l with respect to area measure we prove that inside l these polynomials behave asymptotically like a sequence of certain integrals involving the canonical conformal map of the ex... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'asymptotic', 'behavior', 'of', 'polynomials', 'that', 'are', 'orthonormal', 'over', 'the', 'interior', 'domain', 'of', 'an', 'analytic', 'jordan', 'curve', 'l', 'with', 'respect', 'to', 'area', 'measure', 'we', 'prove', 'that', 'inside', 'l', 'these', 'polynomials',... | [-0.1755088168481729, 0.04034409821622119, -0.11208529244492152, 0.05126707732005227, -0.09542163280784187, -0.08492802572961812, 0.03869308139848754, 0.3281763893923253, -0.2953942341737001, -0.2119711000823304, 0.12945005473946886, -0.25007272721268237, -0.1387961170727149, 0.20792725682958849, -0.08530831325311683, ... |
710.2857 | Renormalisable SO(10) models and neutrino masses and mixing | We discuss some recent developments in SUSY Grand Unified Theories based on
the gauge group SO(10). Considering renormalisable Yukawa couplings, we present
ways to accommodate quark and lepton masses and and mixings.
| hep-ph | we discuss some recent developments in susy grand unified theories based on the gauge group so10 considering renormalisable yukawa couplings we present ways to accommodate quark and lepton masses and and mixings | [['we', 'discuss', 'some', 'recent', 'developments', 'in', 'susy', 'grand', 'unified', 'theories', 'based', 'on', 'the', 'gauge', 'group', 'so10', 'considering', 'renormalisable', 'yukawa', 'couplings', 'we', 'present', 'ways', 'to', 'accommodate', 'quark', 'and', 'lepton', 'masses', 'and', 'and', 'mixings']] | [-0.11445477599045262, 0.30420528358081356, 0.009851672395598143, 0.22418550692964345, -0.1435494478791952, -0.19568557816091925, 0.07149649326311192, 0.3502468573860824, -0.078865741728805, -0.2984679061919451, -0.0059981528647767846, -0.19348528314731084, -0.1079665694905998, 0.016075405874289572, -0.0441602162318304... |
710.2858 | Observation of an unexpected hardening in the spectrum of GRB 021206 | GRB 021206 is one of the brightest GRBs ever observed. Its prompt emission,
as measured by RHESSI, shows an unexpected spectral feature. The spectrum has a
peak energy of about 700 keV and can be described by a Band function up to 4.5
MeV. Above 4.5 MeV, the spectrum hardens again, so that the Band function fails
to ... | astro-ph | grb 021206 is one of the brightest grbs ever observed its prompt emission as measured by rhessi shows an unexpected spectral feature the spectrum has a peak energy of about 700 kev and can be described by a band function up to 45 mev above 45 mev the spectrum hardens again so that the band function fails to fit the who... | [['grb', '021206', 'is', 'one', 'of', 'the', 'brightest', 'grbs', 'ever', 'observed', 'its', 'prompt', 'emission', 'as', 'measured', 'by', 'rhessi', 'shows', 'an', 'unexpected', 'spectral', 'feature', 'the', 'spectrum', 'has', 'a', 'peak', 'energy', 'of', 'about', '700', 'kev', 'and', 'can', 'be', 'described', 'by', 'a... | [-0.02351972027617979, 0.1421934680456865, -0.07649301981062258, 0.1796263791222049, -0.09171363612703105, -0.13546947210912325, 0.06755757705015067, 0.45206686941115826, -0.22308555262622565, -0.387160814016394, 0.02272458330804661, -0.3449620943172031, -0.03339152859702502, 0.21395324985656172, 0.005326188762659488, ... |
710.2859 | Nonequilibrium valley polarization in graphene nanoconstrictions | We recently shown, using tight-binding calculations, that nonequilibrium
valley polarization can be realized in graphene, when the current is injected
through "valley filter": a ballistic point contact with zigzag edges. Here we
demonstrate, that the effect is surprisingly robust against changing the
crystallographic... | cond-mat.mes-hall | we recently shown using tightbinding calculations that nonequilibrium valley polarization can be realized in graphene when the current is injected through valley filter a ballistic point contact with zigzag edges here we demonstrate that the effect is surprisingly robust against changing the crystallographic orientatio... | [['we', 'recently', 'shown', 'using', 'tightbinding', 'calculations', 'that', 'nonequilibrium', 'valley', 'polarization', 'can', 'be', 'realized', 'in', 'graphene', 'when', 'the', 'current', 'is', 'injected', 'through', 'valley', 'filter', 'a', 'ballistic', 'point', 'contact', 'with', 'zigzag', 'edges', 'here', 'we', '... | [-0.17653737859331564, 0.1747998317579105, -0.05463636008789763, -0.014772416492633056, -0.055371976879137544, -0.2310409141824089, 0.05822572827229225, 0.4734124241319175, -0.31041823801610413, -0.2745012441753513, 0.03548914360079733, -0.2725325664117311, -0.14011816641383726, 0.16970692240445512, 0.00917820315108504... |
710.286 | Universal derived equivalences of posets of cluster tilting objects | We show that for two quivers without oriented cycles related by a BGP
reflection, the posets of their cluster tilting objects are related by a simple
combinatorial construction, which we call a flip-flop.
We deduce that the posets of cluster tilting objects of derived equivalent
path algebras of quivers without ori... | math.RT math.CO | we show that for two quivers without oriented cycles related by a bgp reflection the posets of their cluster tilting objects are related by a simple combinatorial construction which we call a flipflop we deduce that the posets of cluster tilting objects of derived equivalent path algebras of quivers without oriented cy... | [['we', 'show', 'that', 'for', 'two', 'quivers', 'without', 'oriented', 'cycles', 'related', 'by', 'a', 'bgp', 'reflection', 'the', 'posets', 'of', 'their', 'cluster', 'tilting', 'objects', 'are', 'related', 'by', 'a', 'simple', 'combinatorial', 'construction', 'which', 'we', 'call', 'a', 'flipflop', 'we', 'deduce', 't... | [-0.18307820342481138, 0.15962801381169509, -0.02823823562512795, 0.12612242449074984, -0.10625225942581892, -0.13569540040567518, 0.02298345719774564, 0.4585245894889037, -0.3653285897274812, -0.23430484207347035, 0.09091764302769055, -0.15033601733545462, -0.15781566658057272, 0.18019219967226188, -0.1815558120235800... |
710.2861 | A Feynman-Kac-type formula for the deterministic and stochastic wave
equations | We establish a probabilistic representation for a wide class of linear
deterministic p.d.e.s with potential term, including the wave equation in
spatial dimensions 1 to 3. Our representation applies to the heat equation,
where it is related to the classical Feynman-Kac formula, as well as to the
telegraph and beam eq... | math.PR | we establish a probabilistic representation for a wide class of linear deterministic pdes with potential term including the wave equation in spatial dimensions 1 to 3 our representation applies to the heat equation where it is related to the classical feynmankac formula as well as to the telegraph and beam equations if... | [['we', 'establish', 'a', 'probabilistic', 'representation', 'for', 'a', 'wide', 'class', 'of', 'linear', 'deterministic', 'pdes', 'with', 'potential', 'term', 'including', 'the', 'wave', 'equation', 'in', 'spatial', 'dimensions', '1', 'to', '3', 'our', 'representation', 'applies', 'to', 'the', 'heat', 'equation', 'whe... | [-0.06220054555986378, 0.06447562870645826, -0.07560786476195161, 0.07135660197063526, -0.10804246356584937, -0.14958419475226184, -0.00926725656215756, 0.29724492686423093, -0.330153406371136, -0.2426217893969167, 0.0961366030419044, -0.2722571410893186, -0.17759860135816238, 0.19950021953145797, -0.03707842691172216,... |
710.2862 | Non-perturbative renormalisation of four-fermion operators in N_f=2 QCD | We present results for the non-perturbative renormalisation of four-fermion
operators with two flavours of dynamical quarks. We consider both fully
relativistic left current-left current operators, and a full basis for $\Delta
B=2$ operators with static heavy quarks. The renormalisation group running of
the operators... | hep-lat | we present results for the nonperturbative renormalisation of fourfermion operators with two flavours of dynamical quarks we consider both fully relativistic left currentleft current operators and a full basis for delta b2 operators with static heavy quarks the renormalisation group running of the operators to high ene... | [['we', 'present', 'results', 'for', 'the', 'nonperturbative', 'renormalisation', 'of', 'fourfermion', 'operators', 'with', 'two', 'flavours', 'of', 'dynamical', 'quarks', 'we', 'consider', 'both', 'fully', 'relativistic', 'left', 'currentleft', 'current', 'operators', 'and', 'a', 'full', 'basis', 'for', 'delta', 'b2',... | [-0.1492930402827644, 0.22000451050807052, -0.1031263759738744, 0.10846471860815315, -0.03835290960350269, -0.12326154020360433, 0.05194646813351726, 0.35437505215752957, -0.22609746601259292, -0.22142848084399172, 0.06337168626893355, -0.28458168478899226, -0.021022066067860917, 0.12119867541112525, 0.0367247782008679... |
710.2863 | First quenched results for the matrix elements of the B_{B_s} mixing
parameter in the static limit from tmQCD | We report on a non-perturbative study of the scale-dependent renormalization
factors of a multiplicatively renormalizable basis of Delta B=2 parity-odd
four-fermion operators in quenched lattice QCD. We also present some
preliminary results of the matrix elements related to the mixing parameter of
the B_s-meson. In o... | hep-lat | we report on a nonperturbative study of the scaledependent renormalization factors of a multiplicatively renormalizable basis of delta b2 parityodd fourfermion operators in quenched lattice qcd we also present some preliminary results of the matrix elements related to the mixing parameter of the b_smeson in our lattice... | [['we', 'report', 'on', 'a', 'nonperturbative', 'study', 'of', 'the', 'scaledependent', 'renormalization', 'factors', 'of', 'a', 'multiplicatively', 'renormalizable', 'basis', 'of', 'delta', 'b2', 'parityodd', 'fourfermion', 'operators', 'in', 'quenched', 'lattice', 'qcd', 'we', 'also', 'present', 'some', 'preliminary'... | [-0.15358855204875954, 0.24254420689599465, -0.052067446773939756, 0.07401472591135623, -0.05703289958012773, -0.10732799518622295, 0.05809385143900222, 0.3463925360871928, -0.22085988123214592, -0.20339895646855996, 0.015737036133463746, -0.30022457959878185, -0.10435807848702708, 0.07332271373198523, 0.06367902692775... |
710.2864 | The Outer Cut-Off of the Giant Planet Population and the 6pc-Survey | We present results from two high-contrast imaging surveys that exploit a
novel technique, L-band angular differential imaging. Our first survey targeted
21 young stars in the Beta Pic and Tuc-Hor moving groups with VLT/NACO reaching
typical sensitivities of <1 MJup at r > 20 AU. The statistical analysis of the
null r... | astro-ph | we present results from two highcontrast imaging surveys that exploit a novel technique lband angular differential imaging our first survey targeted 21 young stars in the beta pic and tuchor moving groups with vltnaco reaching typical sensitivities of 1 mjup at r 20 au the statistical analysis of the null result demons... | [['we', 'present', 'results', 'from', 'two', 'highcontrast', 'imaging', 'surveys', 'that', 'exploit', 'a', 'novel', 'technique', 'lband', 'angular', 'differential', 'imaging', 'our', 'first', 'survey', 'targeted', '21', 'young', 'stars', 'in', 'the', 'beta', 'pic', 'and', 'tuchor', 'moving', 'groups', 'with', 'vltnaco'... | [-0.08241147328263675, 0.0719703500971007, -0.07080644209526925, 0.0315595401230101, -0.11609844357356365, -0.0842044923024682, 0.08419833952261525, 0.3564804260754305, -0.16736508222917715, -0.37577589543966144, 0.10122679689407556, -0.29416793625170967, -0.07604235464818457, 0.2185316777630892, -0.04198966496305652, ... |
710.2865 | Individual complex Dirac eigenvalue distributions from random matrix
theory and comparison to quenched lattice QCD with a quark chemical potential | We analyze how individual eigenvalues of the QCD Dirac operator at nonzero
quark chemical potential are distributed in the complex plane. Exact and
approximate analytical results for both quenched and unquenched distributions
are derived from non-Hermitian random matrix theory. When comparing these to
quenched lattic... | hep-lat | we analyze how individual eigenvalues of the qcd dirac operator at nonzero quark chemical potential are distributed in the complex plane exact and approximate analytical results for both quenched and unquenched distributions are derived from nonhermitian random matrix theory when comparing these to quenched lattice qcd... | [['we', 'analyze', 'how', 'individual', 'eigenvalues', 'of', 'the', 'qcd', 'dirac', 'operator', 'at', 'nonzero', 'quark', 'chemical', 'potential', 'are', 'distributed', 'in', 'the', 'complex', 'plane', 'exact', 'and', 'approximate', 'analytical', 'results', 'for', 'both', 'quenched', 'and', 'unquenched', 'distributions... | [-0.09547342577141273, 0.17183820850002657, -0.07691282783466649, 0.10841165515117303, -0.039191435820546495, -0.12790772923638663, 0.07431293772786003, 0.4086887492876814, -0.200272155858307, -0.23920109235199102, 0.04518554458978126, -0.3249059546604214, -0.11941125751080284, 0.13864108839307923, 0.055511551303227984... |
710.2866 | Intersubband spin-orbit coupling and spin splitting in symmetric quantum
wells | In semiconductors with inversion asymmetry, spin-orbit coupling gives rise to
the well-known Dresselhaus and Rashba effects. If one considers quantum wells
with two or more conduction subbands, an additional, intersubband-induced
spin-orbit term appears whose strength is comparable to the Rashba coupling,
and which r... | cond-mat.mtrl-sci | in semiconductors with inversion asymmetry spinorbit coupling gives rise to the wellknown dresselhaus and rashba effects if one considers quantum wells with two or more conduction subbands an additional intersubbandinduced spinorbit term appears whose strength is comparable to the rashba coupling and which remains fini... | [['in', 'semiconductors', 'with', 'inversion', 'asymmetry', 'spinorbit', 'coupling', 'gives', 'rise', 'to', 'the', 'wellknown', 'dresselhaus', 'and', 'rashba', 'effects', 'if', 'one', 'considers', 'quantum', 'wells', 'with', 'two', 'or', 'more', 'conduction', 'subbands', 'an', 'additional', 'intersubbandinduced', 'spin... | [-0.26017154355899297, 0.19878733139006988, 0.07115866086844887, 0.06863889045115294, -0.08882548174421702, -0.29347691956375327, -0.010104645627351212, 0.4056956042136465, -0.3051739523985556, -0.2892282197518008, -0.10133005550430556, -0.2820654952632529, -0.13511240707510816, 0.18502992062629867, 0.04054781052150896... |
710.2867 | QED in arbitrary linear media: amplifying media | Recently, we have developed a unified approach to QED in arbitrary linearly
responding media in equilibrium--media that give rise to absorption [Phys. Rev.
A \textbf{75}, (2007) 053813]. In the present paper we show that, under
appropriate conditions, the theory can be quite naturally generalized to
amplifying media ... | quant-ph | recently we have developed a unified approach to qed in arbitrary linearly responding media in equilibriummedia that give rise to absorption phys rev a textbf75 2007 053813 in the present paper we show that under appropriate conditions the theory can be quite naturally generalized to amplifying media the effect of whic... | [['recently', 'we', 'have', 'developed', 'a', 'unified', 'approach', 'to', 'qed', 'in', 'arbitrary', 'linearly', 'responding', 'media', 'in', 'equilibriummedia', 'that', 'give', 'rise', 'to', 'absorption', 'phys', 'rev', 'a', 'textbf75', '2007', '053813', 'in', 'the', 'present', 'paper', 'we', 'show', 'that', 'under', ... | [-0.10395378965523233, 0.13454629647954602, -0.09796958186916102, 0.007227186123387906, -0.05850501244704927, -0.1176167271213136, 0.015015967713590607, 0.35473627399731533, -0.2227234722193435, -0.2638519662497652, 0.022890584386676273, -0.24484680346691998, -0.250428685122039, 0.19402759029556102, -0.0450612688632943... |
710.2868 | Maximally multipartite entangled states | We introduce the notion of maximally multipartite entangled states of n
qubits as a generalization of the bipartite case. These pure states have a
bipartite entanglement that does not depend on the bipartition and is maximal
for all possible bipartitions. They are solutions of a minimization problem.
Examples for sma... | quant-ph cond-mat.stat-mech | we introduce the notion of maximally multipartite entangled states of n qubits as a generalization of the bipartite case these pure states have a bipartite entanglement that does not depend on the bipartition and is maximal for all possible bipartitions they are solutions of a minimization problem examples for small n ... | [['we', 'introduce', 'the', 'notion', 'of', 'maximally', 'multipartite', 'entangled', 'states', 'of', 'n', 'qubits', 'as', 'a', 'generalization', 'of', 'the', 'bipartite', 'case', 'these', 'pure', 'states', 'have', 'a', 'bipartite', 'entanglement', 'that', 'does', 'not', 'depend', 'on', 'the', 'bipartition', 'and', 'is... | [-0.16755109933907525, 0.24074014761534177, -0.01454184692875858, 0.07354500864656936, 0.02913142453977152, -0.22077212128951623, 0.024685752953876528, 0.35816706821583866, -0.1961940569443661, -0.2506918734462376, 0.10376111900826034, -0.34217323092212737, -0.12541408870336518, 0.1511068138244905, -0.03641620744836696... |
710.2869 | Canonical extensions of local systems | A local system H on a complex manifold M can be viewed in two ways--either as
a locally free sheaf, or as a union of covering spaces T = T(H). When M is an
open set in a bigger manifold, the local system will generally not extend,
because of local monodromy. This paper proposes an extension of the local
system as an ... | math.AG | a local system h on a complex manifold m can be viewed in two wayseither as a locally free sheaf or as a union of covering spaces t th when m is an open set in a bigger manifold the local system will generally not extend because of local monodromy this paper proposes an extension of the local system as an analytic spac... | [['a', 'local', 'system', 'h', 'on', 'a', 'complex', 'manifold', 'm', 'can', 'be', 'viewed', 'in', 'two', 'wayseither', 'as', 'a', 'locally', 'free', 'sheaf', 'or', 'as', 'a', 'union', 'of', 'covering', 'spaces', 't', 'th', 'when', 'm', 'is', 'an', 'open', 'set', 'in', 'a', 'bigger', 'manifold', 'the', 'local', 'system... | [-0.20029233115669973, 0.07421053342964654, -0.09108948462516449, 0.049422535938763265, -0.08004529675137315, -0.10466799402798889, -0.0020062087046503387, 0.31183374081185816, -0.32704580647839326, -0.21198898197104366, 0.13414510676215038, -0.22407913401375634, -0.11265582694095891, 0.19888293824426956, -0.1204559642... |
710.287 | On the "pits effect" of Littlewood and Offord | Suppose that the moduli of the coefficients of a power series are 1/n!, while
the arguments are arbitrary. If an entire function f represented by such power
series decreases exponentially on some ray, then it has to be an exponential.
If the arguments of the coefficients are of the form 2pi n^2a, where a is
irrationa... | math.CV | suppose that the moduli of the coefficients of a power series are 1n while the arguments are arbitrary if an entire function f represented by such power series decreases exponentially on some ray then it has to be an exponential if the arguments of the coefficients are of the form 2pi n2a where a is irrational then the... | [['suppose', 'that', 'the', 'moduli', 'of', 'the', 'coefficients', 'of', 'a', 'power', 'series', 'are', '1n', 'while', 'the', 'arguments', 'are', 'arbitrary', 'if', 'an', 'entire', 'function', 'f', 'represented', 'by', 'such', 'power', 'series', 'decreases', 'exponentially', 'on', 'some', 'ray', 'then', 'it', 'has', 't... | [-0.1570924304273481, 0.1819252216601177, -0.11882670126700152, 0.026218956511002034, -0.061117835372734144, -0.12304797901127201, -0.005803568897625575, 0.3246732335000371, -0.320604269249508, -0.19766634635519809, 0.12052652852323192, -0.3095181560478149, -0.17954849799832281, 0.21842403904510996, -0.0296683793839735... |
710.2871 | High-Efficiency Resonant RF Spin Rotator with Broad Phase Space
Acceptance for Pulsed Polarized Cold Neutron Beams | We have developed a radio-frequency resonant spin rotator to reverse the
neutron polarization in a 9.5 cm x 9.5 cm pulsed cold neutron beam with high
efficiency over a broad cold neutron energy range. The effect of the spin
reversal by the rotator on the neutron beam phase space is compared
qualitatively to RF neutro... | nucl-ex | we have developed a radiofrequency resonant spin rotator to reverse the neutron polarization in a 95 cm x 95 cm pulsed cold neutron beam with high efficiency over a broad cold neutron energy range the effect of the spin reversal by the rotator on the neutron beam phase space is compared qualitatively to rf neutron spin... | [['we', 'have', 'developed', 'a', 'radiofrequency', 'resonant', 'spin', 'rotator', 'to', 'reverse', 'the', 'neutron', 'polarization', 'in', 'a', '95', 'cm', 'x', '95', 'cm', 'pulsed', 'cold', 'neutron', 'beam', 'with', 'high', 'efficiency', 'over', 'a', 'broad', 'cold', 'neutron', 'energy', 'range', 'the', 'effect', 'o... | [-0.09784899810962965, 0.2429565815592559, -0.03888364429024892, 0.0402008934548071, -0.05647249483209011, -0.08253105033764431, 0.06670131560912385, 0.3954430841694523, -0.221716375824025, -0.3148515345528722, 0.02085905568552306, -0.27502710892482424, 0.05678509437376682, 0.2595465779828678, 0.04017949717470411, 0.04... |
710.2872 | Geometrical constraints on dark energy models | This contribution intends to give a pedagogical introduction to the topic of
dark energy (the mysterious agent supposed to drive the observed late time
acceleration of the Universe) and to various observational tests which require
only assumptions on the geometry of the Universe. Those tests are the
supernovae lumino... | astro-ph | this contribution intends to give a pedagogical introduction to the topic of dark energy the mysterious agent supposed to drive the observed late time acceleration of the universe and to various observational tests which require only assumptions on the geometry of the universe those tests are the supernovae luminosity ... | [['this', 'contribution', 'intends', 'to', 'give', 'a', 'pedagogical', 'introduction', 'to', 'the', 'topic', 'of', 'dark', 'energy', 'the', 'mysterious', 'agent', 'supposed', 'to', 'drive', 'the', 'observed', 'late', 'time', 'acceleration', 'of', 'the', 'universe', 'and', 'to', 'various', 'observational', 'tests', 'whi... | [-0.08431694373450797, 0.09380099169496621, -0.103577852658363, 0.17775508300448306, -0.18848911104629737, -0.09260981741615316, -0.013328673200437216, 0.3233054084985545, -0.2049733105190851, -0.32213555017693174, 0.09797863804998648, -0.27639329760991543, -0.029363644177639724, 0.20655495364858648, -0.024868545628160... |
710.2873 | Sensitive multiplex spectroscopy in the molecular fingerprint 2.4 $\mu$m
region with a Cr^{2+}:ZnSe femtosecond laser | An ultrashort-pulse Cr^{2+}:ZnSe laser is a novel broadband source for
sensitive high resolution molecular spectroscopy. A 130-fs pulse allows
covering of up to 380 cm^-1 spectral domain around 2.4 $\mu$m which is analyzed
simultaneously with a 0.12 cm^-1 (3.6 GHz) resolution by a Fourier-transform
spectrometer. Reco... | physics.optics | an ultrashortpulse cr2znse laser is a novel broadband source for sensitive high resolution molecular spectroscopy a 130fs pulse allows covering of up to 380 cm1 spectral domain around 24 mum which is analyzed simultaneously with a 012 cm1 36 ghz resolution by a fouriertransform spectrometer recorded in 13 s from 70cm l... | [['an', 'ultrashortpulse', 'cr2znse', 'laser', 'is', 'a', 'novel', 'broadband', 'source', 'for', 'sensitive', 'high', 'resolution', 'molecular', 'spectroscopy', 'a', '130fs', 'pulse', 'allows', 'covering', 'of', 'up', 'to', '380', 'cm1', 'spectral', 'domain', 'around', '24', 'mum', 'which', 'is', 'analyzed', 'simultane... | [-0.042141290606765476, 0.11384232805850894, -0.03619503333868685, -0.01085862130683925, 0.023560187605287983, -0.20591244072366122, 0.05790589819227075, 0.47790748064589, -0.1901556911843472, -0.35444229629291135, 0.06334612489825933, -0.33030915415694034, 0.05822199505153243, 0.18811179826114433, -0.00339099764769513... |
710.2874 | Infrared frequency combs and supercontinua for multiplex high
sensitivity spectroscopy | An infrared high-brightness light source based on supercontinuum generation
through a SF6 photonic crystal fiber seeded by a Cr^4+:YAG femtosecond
oscillator is developed for high resolution multiplex spectroscopy in the 1.5
$\mu$m region. Moreover, a multiplex high resolution approach based on a
Cr^4+:YAG frequency ... | physics.optics | an infrared highbrightness light source based on supercontinuum generation through a sf6 photonic crystal fiber seeded by a cr4yag femtosecond oscillator is developed for high resolution multiplex spectroscopy in the 15 mum region moreover a multiplex high resolution approach based on a cr4yag frequency comb enables to... | [['an', 'infrared', 'highbrightness', 'light', 'source', 'based', 'on', 'supercontinuum', 'generation', 'through', 'a', 'sf6', 'photonic', 'crystal', 'fiber', 'seeded', 'by', 'a', 'cr4yag', 'femtosecond', 'oscillator', 'is', 'developed', 'for', 'high', 'resolution', 'multiplex', 'spectroscopy', 'in', 'the', '15', 'mum'... | [-0.07911863627690655, 0.13237377175033516, -0.057151732201785294, -0.03770614110816048, -0.058179760817438364, -0.17199688538241742, 0.042836288362046455, 0.524970551758115, -0.20770264166726995, -0.286902083403695, 0.09004340324126907, -0.258916234402959, -0.05484784525513316, 0.24598090568515682, -0.0065268815687072... |
710.2875 | What are the benefits of bound (protonation) states for the
electron-transfer kinetics? | We describe a model of electron transfer reactions affected by local binding
to the donor or acceptor sites of a particle in equilibrium with the solution.
The statistics of fluctuations of the donor-acceptor energy gap caused by
binding/unbinding events are non-Gaussian, and the resulting free energy
surfaces of ele... | physics.bio-ph physics.chem-ph | we describe a model of electron transfer reactions affected by local binding to the donor or acceptor sites of a particle in equilibrium with the solution the statistics of fluctuations of the donoracceptor energy gap caused by bindingunbinding events are nongaussian and the resulting free energy surfaces of electron t... | [['we', 'describe', 'a', 'model', 'of', 'electron', 'transfer', 'reactions', 'affected', 'by', 'local', 'binding', 'to', 'the', 'donor', 'or', 'acceptor', 'sites', 'of', 'a', 'particle', 'in', 'equilibrium', 'with', 'the', 'solution', 'the', 'statistics', 'of', 'fluctuations', 'of', 'the', 'donoracceptor', 'energy', 'g... | [-0.1069809458573524, 0.1800009205414093, -0.03140965142370303, 0.0928900790110341, 0.056997378218439546, -0.13269021504069908, 0.08275119615672617, 0.3481724166338987, -0.28656952635449645, -0.3419117363778376, -0.015575231960052532, -0.3253000424252731, -0.0883078068669996, 0.12702672123922829, 0.022485409761862, 0.0... |
710.2876 | Information, Inflation, and Interest | We propose a class of discrete-time stochastic models for the pricing of
inflation-linked assets. The paper begins with an axiomatic scheme for asset
pricing and interest rate theory in a discrete-time setting. The first axiom
introduces a "risk-free" asset, and the second axiom determines the
intertemporal pricing r... | q-fin.GN math.PR | we propose a class of discretetime stochastic models for the pricing of inflationlinked assets the paper begins with an axiomatic scheme for asset pricing and interest rate theory in a discretetime setting the first axiom introduces a riskfree asset and the second axiom determines the intertemporal pricing relations th... | [['we', 'propose', 'a', 'class', 'of', 'discretetime', 'stochastic', 'models', 'for', 'the', 'pricing', 'of', 'inflationlinked', 'assets', 'the', 'paper', 'begins', 'with', 'an', 'axiomatic', 'scheme', 'for', 'asset', 'pricing', 'and', 'interest', 'rate', 'theory', 'in', 'a', 'discretetime', 'setting', 'the', 'first', ... | [-0.1365652906193741, 0.027211198988324643, -0.07489019789193806, 0.10718829173339672, -0.09439064346155839, -0.1420537582623135, 0.15692569986230842, 0.36167761368284884, -0.3127305851955163, -0.246457553949011, 0.14496623414911722, -0.24818884596767787, -0.0837818907169429, 0.19840530388204283, -0.14495680707163716, ... |
710.2877 | Differential isospin-fractionation in dilute asymmetric nuclear matter | The differential isospin-fractionation (IsoF) during the liquid-gas phase
transition in dilute asymmetric nuclear matter is studied as a function of
nucleon momentum. Within a self-consistent thermal model it is shown that the
neutron/proton ratio of the gas phase becomes {\it smaller} than that of the
liquid phase f... | nucl-th nucl-ex | the differential isospinfractionation isof during the liquidgas phase transition in dilute asymmetric nuclear matter is studied as a function of nucleon momentum within a selfconsistent thermal model it is shown that the neutronproton ratio of the gas phase becomes it smaller than that of the liquid phase for energetic... | [['the', 'differential', 'isospinfractionation', 'isof', 'during', 'the', 'liquidgas', 'phase', 'transition', 'in', 'dilute', 'asymmetric', 'nuclear', 'matter', 'is', 'studied', 'as', 'a', 'function', 'of', 'nucleon', 'momentum', 'within', 'a', 'selfconsistent', 'thermal', 'model', 'it', 'is', 'shown', 'that', 'the', '... | [-0.08913574858917855, 0.2082486691325903, -0.14277038490399718, 0.12127019738662057, -0.039780158260837195, -0.10956855671945959, 0.01812655245885253, 0.32828588819131255, -0.19178643400984582, -0.2848729943658691, -0.015325967880198733, -0.33744775887578726, -0.04317377392668277, 0.14341504375683145, 0.08280714136082... |
710.2878 | Hydrogen Adsorption of Back Side of Graphene | We studied the interaction between a single hydrogen atom and a single
graphene using classical molecular dynamics simulation with modified Brenner
REBO potential. Three interactions, which are adsorption, reflection,
penetration, were observed. Overhang structure appears and creates an
adsorption site on the backsid... | cond-mat.mtrl-sci cond-mat.other | we studied the interaction between a single hydrogen atom and a single graphene using classical molecular dynamics simulation with modified brenner rebo potential three interactions which are adsorption reflection penetration were observed overhang structure appears and creates an adsorption site on the backside of the... | [['we', 'studied', 'the', 'interaction', 'between', 'a', 'single', 'hydrogen', 'atom', 'and', 'a', 'single', 'graphene', 'using', 'classical', 'molecular', 'dynamics', 'simulation', 'with', 'modified', 'brenner', 'rebo', 'potential', 'three', 'interactions', 'which', 'are', 'adsorption', 'reflection', 'penetration', 'w... | [-0.11951236880343893, 0.16069335555415515, -0.028509766291841425, 0.001153035252788885, 0.017483209152792736, -0.16271757325721523, 0.09231429933483556, 0.42076187535703924, -0.2612350602859851, -0.29176524515200103, -0.010077521855717305, -0.3211822354969401, -0.094270534963804, 0.1410390045378149, 0.0477549120926975... |
710.2879 | The Richness and Beauty of the Physics of Cosmological Recombination | The physical ingredients to describe the epoch of cosmological recombination
are amazingly simple and well-understood. This fact allows us to take into
account a very large variety of processes, still finding potentially measurable
consequences. In this contribution we highlight some of the detailed physics
that were... | astro-ph | the physical ingredients to describe the epoch of cosmological recombination are amazingly simple and wellunderstood this fact allows us to take into account a very large variety of processes still finding potentially measurable consequences in this contribution we highlight some of the detailed physics that were recen... | [['the', 'physical', 'ingredients', 'to', 'describe', 'the', 'epoch', 'of', 'cosmological', 'recombination', 'are', 'amazingly', 'simple', 'and', 'wellunderstood', 'this', 'fact', 'allows', 'us', 'to', 'take', 'into', 'account', 'a', 'very', 'large', 'variety', 'of', 'processes', 'still', 'finding', 'potentially', 'mea... | [-0.06833207820113583, 0.11644936335615379, -0.09415407983207069, 0.09911830612360321, -0.11114438042401097, -0.0757234489269126, 0.013521226972910222, 0.3550472999758095, -0.2530544368319411, -0.3247058195354565, 0.07239818396494906, -0.26820687378507646, -0.04160641791480305, 0.20994496633467652, -0.00824956513891837... |
710.288 | A determination of the B_s^0 and B_d^0 mixing parameters in 2+1 lattice
QCD | We report on the advances in our unquenched calculation of the matrix
elements relevant for the analysis of B^0-\bar B^0 mixing using the Asqtad
(light quark) and Fermilab (heavy quark) actions. We have calculated the
hadronic parameters for the mass and width differences in the neutral B meson
system. Preliminary re... | hep-lat | we report on the advances in our unquenched calculation of the matrix elements relevant for the analysis of b0bar b0 mixing using the asqtad light quark and fermilab heavy quark actions we have calculated the hadronic parameters for the mass and width differences in the neutral b meson system preliminary results are pr... | [['we', 'report', 'on', 'the', 'advances', 'in', 'our', 'unquenched', 'calculation', 'of', 'the', 'matrix', 'elements', 'relevant', 'for', 'the', 'analysis', 'of', 'b0bar', 'b0', 'mixing', 'using', 'the', 'asqtad', 'light', 'quark', 'and', 'fermilab', 'heavy', 'quark', 'actions', 'we', 'have', 'calculated', 'the', 'had... | [-0.029224740671775034, 0.2550561177288933, -0.02890347517771466, 0.07061298485214432, 0.011392362535961213, -0.06799757766026643, 0.11470445693140069, 0.36120159707723126, -0.12703495612367988, -0.252236801154551, 0.04493471682297006, -0.33848704812267133, -0.013630388627549814, 0.15863512949116768, 0.0717792440235855... |
710.2881 | On the Geometry of Supersymmetric Quantum Mechanical Systems | We consider some simple examples of supersymmetric quantum mechanical systems
and explore their possible geometric interpretation with the help of geometric
aspects of real Clifford algebras. This leads to natural extensions of the
considered systems to higher dimensions and more complicated potentials.
| hep-th math-ph math.MP | we consider some simple examples of supersymmetric quantum mechanical systems and explore their possible geometric interpretation with the help of geometric aspects of real clifford algebras this leads to natural extensions of the considered systems to higher dimensions and more complicated potentials | [['we', 'consider', 'some', 'simple', 'examples', 'of', 'supersymmetric', 'quantum', 'mechanical', 'systems', 'and', 'explore', 'their', 'possible', 'geometric', 'interpretation', 'with', 'the', 'help', 'of', 'geometric', 'aspects', 'of', 'real', 'clifford', 'algebras', 'this', 'leads', 'to', 'natural', 'extensions', '... | [-0.11758833000203595, 0.08826891335082196, -0.02981460475850673, 0.1396226798976949, -0.11605430199276834, -0.1987579587758297, -0.017625861970286462, 0.3327451280894734, -0.2527906646331151, -0.26624369785367025, 0.07047295011025631, -0.21681638132958186, -0.24949740862385147, 0.2275448830443479, -0.1679574783802742,... |
710.2882 | The Initial Mass Function of the Massive Star-forming Region NGC 3603
from Near-Infrared Adaptive Optics observations | We study the initial mass function (IMF) of one of the most massive Galactic
star-forming regions NGC 3603 to answer a fundamental question in current
astrophysics: is the IMF universal, or does it vary? Using our very deep, high
angular resolution JHKsL' images obtained with NAOS-CONICA at the VLT at ESO,
we have su... | astro-ph | we study the initial mass function imf of one of the most massive galactic starforming regions ngc 3603 to answer a fundamental question in current astrophysics is the imf universal or does it vary using our very deep high angular resolution jhksl images obtained with naosconica at the vlt at eso we have successfully r... | [['we', 'study', 'the', 'initial', 'mass', 'function', 'imf', 'of', 'one', 'of', 'the', 'most', 'massive', 'galactic', 'starforming', 'regions', 'ngc', '3603', 'to', 'answer', 'a', 'fundamental', 'question', 'in', 'current', 'astrophysics', 'is', 'the', 'imf', 'universal', 'or', 'does', 'it', 'vary', 'using', 'our', 'v... | [-0.05232541619049613, 0.12584729407619386, -0.09629579227863268, 0.12747890744509055, -0.06663981070172498, -0.035222000940769854, 0.05807424637509121, 0.4073865548205033, -0.1455025015044589, -0.41152007005130536, 0.00660255972150271, -0.21723561636306238, 0.03312212902497293, 0.18845294549535263, -0.0437167325164291... |
710.2883 | What rare K decays can tell about the MSSM | The supersymmetric contributions to the theoretically clean K+ --> pi+ nu nu
bar, KL --> pi0 nu nu bar, KL --> pi0 e+ e- and KL --> pi0 mu+ mu- decays are
briefly reviewed. Particular emphasis is laid on the information one could get
on the MSSM flavor sector from a combined study of the four modes.
| hep-ph | the supersymmetric contributions to the theoretically clean k pi nu nu bar kl pi0 nu nu bar kl pi0 e e and kl pi0 mu mu decays are briefly reviewed particular emphasis is laid on the information one could get on the mssm flavor sector from a combined study of the four modes | [['the', 'supersymmetric', 'contributions', 'to', 'the', 'theoretically', 'clean', 'k', 'pi', 'nu', 'nu', 'bar', 'kl', 'pi0', 'nu', 'nu', 'bar', 'kl', 'pi0', 'e', 'e', 'and', 'kl', 'pi0', 'mu', 'mu', 'decays', 'are', 'briefly', 'reviewed', 'particular', 'emphasis', 'is', 'laid', 'on', 'the', 'information', 'one', 'coul... | [-0.15089562534407344, 0.23979588870380847, -0.07807887946519088, 0.1452768277486716, -0.06722503865383705, -0.19224215290983612, 0.1320970001617306, 0.2254523728921447, -0.2186939684709288, -0.0924139576349056, -0.06348901208191407, -0.39976700587760444, 0.008353824779953598, 0.11097365178448974, 0.10759001638177994, ... |
710.2884 | The Urysohn sphere is oscillation stable | We solve the oscillation stability problem for the Urysohn sphere, an analog
of the distortion problem for the Hilbert space in the context of the Urysohn
universal metric space. This is achieved by solving a purely combinatorial
problem involving a family of countable homogeneous metric spaces with finitely
many dis... | math.MG math.CO | we solve the oscillation stability problem for the urysohn sphere an analog of the distortion problem for the hilbert space in the context of the urysohn universal metric space this is achieved by solving a purely combinatorial problem involving a family of countable homogeneous metric spaces with finitely many distanc... | [['we', 'solve', 'the', 'oscillation', 'stability', 'problem', 'for', 'the', 'urysohn', 'sphere', 'an', 'analog', 'of', 'the', 'distortion', 'problem', 'for', 'the', 'hilbert', 'space', 'in', 'the', 'context', 'of', 'the', 'urysohn', 'universal', 'metric', 'space', 'this', 'is', 'achieved', 'by', 'solving', 'a', 'purel... | [-0.1490567884594202, 0.07785979185515317, -0.07138107765465974, 0.10438003297895193, -0.12018255293369293, -0.05799916971474886, 0.017494561839848755, 0.3180112008517608, -0.40850153744220735, -0.20324887823313476, 0.15249933008803054, -0.2586971110850573, -0.14419591575860977, 0.24812218162347563, -0.1154891366511583... |
710.2885 | Partition properties of the dense local order and a colored version of
Milliken's theorem | We study the finite dimensional partition properties of the countable
homogeneous dense local order. Some of our results use ideas borrowed from the
partition calculus of the rationals and are obtained thanks to a strengthening
of Milliken's theorem on trees.
| math.CO math.LO | we study the finite dimensional partition properties of the countable homogeneous dense local order some of our results use ideas borrowed from the partition calculus of the rationals and are obtained thanks to a strengthening of millikens theorem on trees | [['we', 'study', 'the', 'finite', 'dimensional', 'partition', 'properties', 'of', 'the', 'countable', 'homogeneous', 'dense', 'local', 'order', 'some', 'of', 'our', 'results', 'use', 'ideas', 'borrowed', 'from', 'the', 'partition', 'calculus', 'of', 'the', 'rationals', 'and', 'are', 'obtained', 'thanks', 'to', 'a', 'st... | [-0.07025934087160306, 0.09318041753692505, -0.1383653744482077, 0.056959724316421226, -0.1058577925253373, 0.0009969747147690027, 0.08090432964933988, 0.30384771556903917, -0.32242819055532795, -0.20250633597756043, 0.127188139463751, -0.27716565027068824, -0.11914560571312904, 0.1990336867613503, -0.06924267024852526... |
710.2886 | $\kappa$-Minkowski space, scalar field, and the issue of Lorentz
invariance | We describe $\kappa$-Minkowski space and its relation to group theory. The
group theoretical picture makes it possible to analyze the symmetries of this
space. As an application of this analysis we analyze in detail free field
theory on $\kappa$-Minkowski space and the Noether charges associated with
deformed spaceti... | hep-th | we describe kappaminkowski space and its relation to group theory the group theoretical picture makes it possible to analyze the symmetries of this space as an application of this analysis we analyze in detail free field theory on kappaminkowski space and the noether charges associated with deformed spacetime symmetrie... | [['we', 'describe', 'kappaminkowski', 'space', 'and', 'its', 'relation', 'to', 'group', 'theory', 'the', 'group', 'theoretical', 'picture', 'makes', 'it', 'possible', 'to', 'analyze', 'the', 'symmetries', 'of', 'this', 'space', 'as', 'an', 'application', 'of', 'this', 'analysis', 'we', 'analyze', 'in', 'detail', 'free'... | [-0.138779657474738, 0.11180113589810445, -0.112572700973144, 0.1359082941032414, -0.15894481053157727, -0.046953156390892606, 0.013077259306054639, 0.3985322973101723, -0.2860518275779121, -0.26441451127412824, 0.06830093731904137, -0.25415990427516555, -0.1969457189457453, 0.11357681270764798, -0.12156640607103401, -... |
710.2887 | Implementation, Compilation, Optimization of Object-Oriented Languages,
Programs and Systems - Report on the Workshop ICOOOLPS'2006 at ECOOP'06 | ICOOOLPS'2006 was the first edition of ECOOP-ICOOOLPS workshop. It intended
to bring researchers and practitioners both from academia and industry
together, with a spirit of openness, to try and identify and begin to address
the numerous and very varied issues of optimization. This succeeded, as can be
seen from the ... | cs.PF cs.PL cs.SE | icooolps2006 was the first edition of ecoopicooolps workshop it intended to bring researchers and practitioners both from academia and industry together with a spirit of openness to try and identify and begin to address the numerous and very varied issues of optimization this succeeded as can be seen from the papers th... | [['icooolps2006', 'was', 'the', 'first', 'edition', 'of', 'ecoopicooolps', 'workshop', 'it', 'intended', 'to', 'bring', 'researchers', 'and', 'practitioners', 'both', 'from', 'academia', 'and', 'industry', 'together', 'with', 'a', 'spirit', 'of', 'openness', 'to', 'try', 'and', 'identify', 'and', 'begin', 'to', 'addres... | [-0.02206766763195065, 0.0778805574875385, -0.0846649470725923, 0.029698812412173158, -0.17618788020580164, -0.13969887637593334, 0.09857392613400495, 0.33885943092736265, -0.2364143636227856, -0.389363937921101, 0.16430325451637467, -0.32418414170763665, -0.1419496211963105, 0.17197128221525945, -0.10902480638375686, ... |
710.2888 | Pair-distribution functions of two-temperature two-mass systems:
Comparison of MD, HNC, CHNC, QMC and Kohn-Sham calculations for dense
hydrogen | Two-temperature, two-mass quasi-equilibrium plasmas may occur in electron-ion
plasmas,nuclear-matter, as well as in electron-hole condensed-matter systems.
Dense two-temperature hydrogen plasmas straddle the difficult partially -
degenerate regime of electron densities and temperatures which are important in
astrophy... | cond-mat.stat-mech astro-ph cond-mat.str-el physics.plasm-ph | twotemperature twomass quasiequilibrium plasmas may occur in electronion plasmasnuclearmatter as well as in electronhole condensedmatter systems dense twotemperature hydrogen plasmas straddle the difficult partially degenerate regime of electron densities and temperatures which are important in astrophysics in inertial... | [['twotemperature', 'twomass', 'quasiequilibrium', 'plasmas', 'may', 'occur', 'in', 'electronion', 'plasmasnuclearmatter', 'as', 'well', 'as', 'in', 'electronhole', 'condensedmatter', 'systems', 'dense', 'twotemperature', 'hydrogen', 'plasmas', 'straddle', 'the', 'difficult', 'partially', 'degenerate', 'regime', 'of', ... | [-0.02896945134168217, 0.15752715175382465, -0.04876353022015845, 0.14449469451039262, 0.06293478986481205, -0.12807307806660367, -0.019356869512942947, 0.3889212610802668, -0.18990034140091772, -0.2878913194667, 0.008013871070408426, -0.25946801175664674, -0.017198328336235136, 0.2222841121872668, 0.07658464848474764,... |
710.2889 | An efficient reduction of ranking to classification | This paper describes an efficient reduction of the learning problem of
ranking to binary classification. The reduction guarantees an average pairwise
misranking regret of at most that of the binary classifier regret, improving a
recent result of Balcan et al which only guarantees a factor of 2. Moreover,
our reductio... | cs.LG cs.IR | this paper describes an efficient reduction of the learning problem of ranking to binary classification the reduction guarantees an average pairwise misranking regret of at most that of the binary classifier regret improving a recent result of balcan et al which only guarantees a factor of 2 moreover our reduction appl... | [['this', 'paper', 'describes', 'an', 'efficient', 'reduction', 'of', 'the', 'learning', 'problem', 'of', 'ranking', 'to', 'binary', 'classification', 'the', 'reduction', 'guarantees', 'an', 'average', 'pairwise', 'misranking', 'regret', 'of', 'at', 'most', 'that', 'of', 'the', 'binary', 'classifier', 'regret', 'improv... | [-0.09470060005270202, 0.029289241812651832, -0.06008680059065299, 0.05101489892637752, -0.09645485364616357, -0.14724662047329135, 0.14275204479692072, 0.3437092666849127, -0.2298607575114165, -0.37074717879754127, 0.07299886228518991, -0.2790657117449004, -0.14732495204859822, 0.2426917338300797, -0.08744131341081095... |
710.289 | Model for a collimated spin wave beam generated by a single layer, spin
torque nanocontact | A model of spin torque induced magnetization dynamics based upon
semi-classical spin diffusion theory for a single layer nanocontact is
presented. The model incorporates effects due to the current induced Oersted
field and predicts the generation of a variety of spatially dependent,
coherent, precessional magnetic wa... | cond-mat.mtrl-sci | a model of spin torque induced magnetization dynamics based upon semiclassical spin diffusion theory for a single layer nanocontact is presented the model incorporates effects due to the current induced oersted field and predicts the generation of a variety of spatially dependent coherent precessional magnetic wave str... | [['a', 'model', 'of', 'spin', 'torque', 'induced', 'magnetization', 'dynamics', 'based', 'upon', 'semiclassical', 'spin', 'diffusion', 'theory', 'for', 'a', 'single', 'layer', 'nanocontact', 'is', 'presented', 'the', 'model', 'incorporates', 'effects', 'due', 'to', 'the', 'current', 'induced', 'oersted', 'field', 'and'... | [-0.25317673191428186, 0.28835867012283417, -0.019230208732187747, 0.03934247502940707, -0.1103734537307173, -0.07935740747023373, -0.04937657770351507, 0.40136645441874863, -0.3189442605897784, -0.24177674472332, 0.017980694685829805, -0.21610335409641265, -0.12628413408994674, 0.238511089743115, 0.10426805866416544, ... |
710.2891 | SUSY Model Building | I review some of the latest directions in supersymmetric model building,
focusing on SUSY breaking mechanisms in the minimal supersymmetric standard
model [MSSM], the "little" hierarchy and $\mu$ problems, etc. I then discuss
SUSY GUTs and UV completions in string theory.
| hep-ph | i review some of the latest directions in supersymmetric model building focusing on susy breaking mechanisms in the minimal supersymmetric standard model mssm the little hierarchy and mu problems etc i then discuss susy guts and uv completions in string theory | [['i', 'review', 'some', 'of', 'the', 'latest', 'directions', 'in', 'supersymmetric', 'model', 'building', 'focusing', 'on', 'susy', 'breaking', 'mechanisms', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'the', 'little', 'hierarchy', 'and', 'mu', 'problems', 'etc', 'i', 'then', 'discuss', 'sus... | [-0.05196031604938936, 0.18734560642255152, 0.04486026137885524, 0.23792601220037152, -0.10011868133414083, -0.2603837119006529, 0.014910591683895668, 0.3527234330341765, -0.22106876569550213, -0.26388197480814485, 0.1167296719902036, -0.26991767909877545, -0.13158486542723527, 0.07529328076350617, -0.08328116083057688... |
710.2892 | On the Diversity of the Taurus Transitional Disks: UX Tau A & Lk Ca 15 | The recently recognized class of "transitional disk" systems consists of
young starswith optically-thick outer disks but inner disks which are mostly
devoid of small dust. Here we introduce a further class of "pre-transitional
disks" with significant near-infrared excesses which indicate the presence of
an optically ... | astro-ph | the recently recognized class of transitional disk systems consists of young starswith opticallythick outer disks but inner disks which are mostly devoid of small dust here we introduce a further class of pretransitional disks with significant nearinfrared excesses which indicate the presence of an optically thick inne... | [['the', 'recently', 'recognized', 'class', 'of', 'transitional', 'disk', 'systems', 'consists', 'of', 'young', 'starswith', 'opticallythick', 'outer', 'disks', 'but', 'inner', 'disks', 'which', 'are', 'mostly', 'devoid', 'of', 'small', 'dust', 'here', 'we', 'introduce', 'a', 'further', 'class', 'of', 'pretransitional'... | [-0.08005313870783609, 0.09321234572688719, -0.0476898986089509, 0.003463630563231533, -0.0541012815025809, -0.04135510064712675, 0.008904048048502223, 0.41842086439194914, -0.22288710943290166, -0.34520676629208435, 0.06636140373942269, -0.2594114038862984, -0.02789305225091444, 0.12984329391178767, -0.072352365352684... |
710.2893 | On solutions of Rashevskii equation | The solutions of Rashevskii equation for gonometric family of plane curves
are considered. Their properties are studied. The connection with the theory of
duality for the second order ODE's is discussed.
| nlin.SI | the solutions of rashevskii equation for gonometric family of plane curves are considered their properties are studied the connection with the theory of duality for the second order odes is discussed | [['the', 'solutions', 'of', 'rashevskii', 'equation', 'for', 'gonometric', 'family', 'of', 'plane', 'curves', 'are', 'considered', 'their', 'properties', 'are', 'studied', 'the', 'connection', 'with', 'the', 'theory', 'of', 'duality', 'for', 'the', 'second', 'order', 'odes', 'is', 'discussed']] | [-0.221808438654989, 0.0596065689841735, -0.055285683849119936, 0.09204076882853204, -0.0819555321901009, -0.08307026827643657, -0.0590942906866107, 0.32945131243945197, -0.2759105934408204, -0.2734574249720779, 0.15817137850159457, -0.34057420386194154, -0.1596657452012958, 0.21852304452452168, 0.010358485939173863, 0... |
710.2894 | HAT-P-6b: A Hot Jupiter transiting a bright F star | In the ongoing HATNet survey we have detected a giant planet, with radius
1.33 +/- 0.06 RJup and mass 1.06 +/- 0.12 MJup, transiting the bright (V =
10.5) star GSC 03239-00992. The planet is in a circular orbit with period
3.852985 +/- 0.000005 days and mid-transit epoch 2,454,035.67575 +/- 0.00028
(HJD). The parent ... | astro-ph | in the ongoing hatnet survey we have detected a giant planet with radius 133 006 rjup and mass 106 012 mjup transiting the bright v 105 star gsc 0323900992 the planet is in a circular orbit with period 3852985 0000005 days and midtransit epoch 245403567575 000028 hjd the parent star is a late f star with mass 129 006 m... | [['in', 'the', 'ongoing', 'hatnet', 'survey', 'we', 'have', 'detected', 'a', 'giant', 'planet', 'with', 'radius', '133', '006', 'rjup', 'and', 'mass', '106', '012', 'mjup', 'transiting', 'the', 'bright', 'v', '105', 'star', 'gsc', '0323900992', 'the', 'planet', 'is', 'in', 'a', 'circular', 'orbit', 'with', 'period', '3... | [-0.13966417568296474, 0.18158469783177353, -0.06823400964626586, 0.0022384970765209422, -0.10418128921597633, -0.08803431115570073, 0.12480636480492803, 0.36876952821248266, -0.05933440783728828, -0.4296237092184008, 0.10803580194720472, -0.3618849994140273, 0.007692121127444618, 0.16178384504526994, -0.12589068955056... |
710.2895 | Quaternionic Analysis and the Algebrodynamics | We present the ``algebrodynamical'' approach to field-particle theory based
on a nonlinear generalization of the Cauchy-Riemann conditions to
non-commutative algebras of quaternion-like type. For complex quaternions the
theory is Lorentz invariant and naturally carries some gauge and twistor
structures. Point- and st... | math-ph gr-qc hep-th math.CV math.MP | we present the algebrodynamical approach to fieldparticle theory based on a nonlinear generalization of the cauchyriemann conditions to noncommutative algebras of quaternionlike type for complex quaternions the theory is lorentz invariant and naturally carries some gauge and twistor structures point and stringlike sing... | [['we', 'present', 'the', 'algebrodynamical', 'approach', 'to', 'fieldparticle', 'theory', 'based', 'on', 'a', 'nonlinear', 'generalization', 'of', 'the', 'cauchyriemann', 'conditions', 'to', 'noncommutative', 'algebras', 'of', 'quaternionlike', 'type', 'for', 'complex', 'quaternions', 'the', 'theory', 'is', 'lorentz',... | [-0.1955478639276915, 0.1368269603374566, -0.11990445826289266, 0.13324026198418767, -0.16059646709702996, -0.1053116298009923, -0.06896954885857223, 0.3388366808297199, -0.2654409289554974, -0.209946395317634, 0.06306426247668474, -0.22900013230351168, -0.2338277732000448, 0.12539312266203206, -0.09500569379130422, 0.... |
710.2896 | EasyNData: A simple tool to extract numerical values from published
plots | The comparison of numerical data with published plots is a frequently
occurring task. In this article I present a short computer program written in
Java(TM) helping in those cases where someone wants to get the numbers out of a
plot but is not able to read the plot with a decent accuracy and cannot contact
the author... | physics.comp-ph hep-ph physics.data-an | the comparison of numerical data with published plots is a frequently occurring task in this article i present a short computer program written in javatm helping in those cases where someone wants to get the numbers out of a plot but is not able to read the plot with a decent accuracy and cannot contact the author of t... | [['the', 'comparison', 'of', 'numerical', 'data', 'with', 'published', 'plots', 'is', 'a', 'frequently', 'occurring', 'task', 'in', 'this', 'article', 'i', 'present', 'a', 'short', 'computer', 'program', 'written', 'in', 'javatm', 'helping', 'in', 'those', 'cases', 'where', 'someone', 'wants', 'to', 'get', 'the', 'numb... | [-0.07508130102595757, 0.039607895467252956, -0.10178253632260575, 0.09128410922075134, -0.084872210309619, -0.147019297283675, 0.1137878586349654, 0.33534569550483, -0.23153622780616084, -0.3739674842472942, 0.10468659120545323, -0.30158871484787336, -0.10081735389928023, 0.25692646466195584, -0.0980657946318388, 0.02... |
710.2897 | Searches for Squarks and Gluinos with D0 Detector | Searches for supersymmetry in the framework of R-parity conserving models
have been performed in data collected by the D0 detector at the Tevatron
$p\bar{p}$ collider at a center-of-mass energy of 1.96 TeV. Topologies analyzed
consist of acoplanar-jets, multijets, and leptons with large missing transverse
energy in t... | hep-ex | searches for supersymmetry in the framework of rparity conserving models have been performed in data collected by the d0 detector at the tevatron pbarp collider at a centerofmass energy of 196 tev topologies analyzed consist of acoplanarjets multijets and leptons with large missing transverse energy in the final state ... | [['searches', 'for', 'supersymmetry', 'in', 'the', 'framework', 'of', 'rparity', 'conserving', 'models', 'have', 'been', 'performed', 'in', 'data', 'collected', 'by', 'the', 'd0', 'detector', 'at', 'the', 'tevatron', 'pbarp', 'collider', 'at', 'a', 'centerofmass', 'energy', 'of', '196', 'tev', 'topologies', 'analyzed',... | [-0.08135531965315286, 0.3323468307407825, 0.008092253639847597, 0.21900771418368367, -0.04429006141223264, -0.2181528247587648, 0.06873989153275906, 0.3329649528929761, -0.14678206537023522, -0.36114550952551966, 0.025487542672131616, -0.3236252621953351, 0.16652949991259264, 0.14458526585866743, 0.07339967775755049, ... |
710.2898 | Higher rank numerical ranges and low rank perturbations of quantum
channels | For a positive integer $k$, the rank-$k$ numerical range $\Lambda_k(A)$ of an
operator $A$ acting on a Hilbert space $\cH$ of dimension at least $k$ is the
set of scalars $\lambda$ such that $PAP = \lambda P$ for some rank $k$
orthogonal projection $P$. In this paper, a close connection between low rank
perturbation ... | math.FA quant-ph | for a positive integer k the rankk numerical range lambda_ka of an operator a acting on a hilbert space ch of dimension at least k is the set of scalars lambda such that pap lambda p for some rank k orthogonal projection p in this paper a close connection between low rank perturbation of an operator a and lambda_ka is ... | [['for', 'a', 'positive', 'integer', 'k', 'the', 'rankk', 'numerical', 'range', 'lambda_ka', 'of', 'an', 'operator', 'a', 'acting', 'on', 'a', 'hilbert', 'space', 'ch', 'of', 'dimension', 'at', 'least', 'k', 'is', 'the', 'set', 'of', 'scalars', 'lambda', 'such', 'that', 'pap', 'lambda', 'p', 'for', 'some', 'rank', 'k',... | [-0.1633140239957191, 0.12154531895480018, -0.05161212575639541, 0.03423319121374692, -0.02245256364888822, -0.1780294367803656, 0.005919163623206479, 0.34080888982862234, -0.2830833182317402, -0.1774148727894168, 0.11264117081979445, -0.2803052219352332, -0.11333369516686423, 0.19763540474002983, -0.04291999759858079,... |
710.2899 | Discovery of 21cm absorption in a $z_{\rm abs} =2.289$ DLA towards TXS
0311+430: The first low spin temperature absorber at z > 1 | We report the detection of HI 21 cm absorption from the $z=2.289$ damped
Lyman-$\alpha$ system (DLA) towards TXS 0311+430, with the Green Bank
Telescope. The 21 cm absorption has a velocity spread (between nulls) of $\sim
110$ km s$^{-1}$ and an integrated optical depth of $\int \tau {\rm d}V =
(0.818 \pm 0.085)$ km ... | astro-ph | we report the detection of hi 21 cm absorption from the z2289 damped lymanalpha system dla towards txs 0311430 with the green bank telescope the 21 cm absorption has a velocity spread between nulls of sim 110 km s1 and an integrated optical depth of int tau rm dv 0818 pm 0085 km s1 we also present new giant metrewave r... | [['we', 'report', 'the', 'detection', 'of', 'hi', '21', 'cm', 'absorption', 'from', 'the', 'z2289', 'damped', 'lymanalpha', 'system', 'dla', 'towards', 'txs', '0311430', 'with', 'the', 'green', 'bank', 'telescope', 'the', '21', 'cm', 'absorption', 'has', 'a', 'velocity', 'spread', 'between', 'nulls', 'of', 'sim', '110'... | [-0.11311555878675886, 0.1427058265427676, 0.036279967381504546, 0.01256301845046038, -0.036306561983860376, -0.09200862937059515, 0.04190488091900765, 0.4405792993656768, -0.12091984163781856, -0.3232122592203188, 0.03872971935912542, -0.334030426091008, 0.02497957877226566, 0.18329412293587666, 0.051339050509843796, ... |
710.29 | In Search of Possible Associations between Planetary Nebulae and Open
Clusters | We consider the possibility of cluster membership for 13 planetary nebulae
that are located in close proximity to open clusters lying in their lines of
sight. The short lifetimes and low sample size of intermediate-mass planetary
nebulae with respect to nearby open clusters conspire to reduce the probability
of obser... | astro-ph | we consider the possibility of cluster membership for 13 planetary nebulae that are located in close proximity to open clusters lying in their lines of sight the short lifetimes and low sample size of intermediatemass planetary nebulae with respect to nearby open clusters conspire to reduce the probability of observing... | [['we', 'consider', 'the', 'possibility', 'of', 'cluster', 'membership', 'for', '13', 'planetary', 'nebulae', 'that', 'are', 'located', 'in', 'close', 'proximity', 'to', 'open', 'clusters', 'lying', 'in', 'their', 'lines', 'of', 'sight', 'the', 'short', 'lifetimes', 'and', 'low', 'sample', 'size', 'of', 'intermediatema... | [-0.12626829902020595, 0.08483746416245898, -0.010818823079268137, 0.13008296510127063, -0.1047145891437928, -0.12854698759193223, 0.10661636387308439, 0.41870793086787067, -0.1413707285746932, -0.37589282865209195, 0.03464234081407388, -0.2673104655370116, -0.02320650697375337, 0.22057861351252844, -0.0321336725540459... |
710.2901 | Bulges versus disks: the evolution of angular momentum in cosmological
simulations of galaxy formation | We investigate the evolution of angular momentum in simulations of galaxy
formation in a cold dark matter universe. We analyse two model galaxies
generated in the N-body/hydrodynamic simulations of Okamoto et al. Starting
from identical initial conditions, but using different assumptions for the
baryonic physics, one... | astro-ph | we investigate the evolution of angular momentum in simulations of galaxy formation in a cold dark matter universe we analyse two model galaxies generated in the nbodyhydrodynamic simulations of okamoto et al starting from identical initial conditions but using different assumptions for the baryonic physics one of the ... | [['we', 'investigate', 'the', 'evolution', 'of', 'angular', 'momentum', 'in', 'simulations', 'of', 'galaxy', 'formation', 'in', 'a', 'cold', 'dark', 'matter', 'universe', 'we', 'analyse', 'two', 'model', 'galaxies', 'generated', 'in', 'the', 'nbodyhydrodynamic', 'simulations', 'of', 'okamoto', 'et', 'al', 'starting', '... | [-0.08903796601462238, 0.16149460713099167, -0.13824253248440516, 0.09886760830763743, -0.10591744310582223, -0.03734001006014887, -0.013441799925469861, 0.33435467152091547, -0.21393509239626327, -0.3408724047277668, 0.02551850376506828, -0.2622045425630016, -0.00945954529258112, 0.15536765693649043, 0.014610991552017... |
710.2902 | A Half-Megasecond Chandra Observation of the Oxygen-Rich Supernova
Remnant G292.0+1.8 | We report on our initial analysis of a deep 510 ks observation of the
Galactic oxygen-rich supernova remnant (SNR) G292.0+1.8 with the {\it Chandra
X-ray Observatory}. Our new {\it Chandra} ACIS-I observation has a larger field
of view and an order of magnitude deeper exposure than the previous {\it
Chandra} observat... | astro-ph | we report on our initial analysis of a deep 510 ks observation of the galactic oxygenrich supernova remnant snr g292018 with the it chandra xray observatory our new it chandra acisi observation has a larger field of view and an order of magnitude deeper exposure than the previous it chandra observation which allows us ... | [['we', 'report', 'on', 'our', 'initial', 'analysis', 'of', 'a', 'deep', '510', 'ks', 'observation', 'of', 'the', 'galactic', 'oxygenrich', 'supernova', 'remnant', 'snr', 'g292018', 'with', 'the', 'it', 'chandra', 'xray', 'observatory', 'our', 'new', 'it', 'chandra', 'acisi', 'observation', 'has', 'a', 'larger', 'field... | [-0.07468157917454538, 0.06450231512114736, -0.10812131566450175, 0.08576528392512146, -0.16744585060441178, -0.06630670704226208, 0.06997210974988388, 0.43827878293676636, -0.18304824989699708, -0.32193746778281684, 0.06535112402057201, -0.29803370446616173, -0.042313421955405495, 0.19235964626528498, -0.0033192409451... |
710.2903 | Non-LTE dust nucleation in sub-saturated vapors | We use the kinetic theory of nucleation to explore the properties of dust
nucleation in sub-saturated vapors. Due to radiation losses, the sub-critical
clusters have a smaller temperature compared to their vapor. This alters the
dynamical balance between attachment and detachment of monomers, allowing for
stable nucl... | astro-ph cond-mat.soft physics.chem-ph | we use the kinetic theory of nucleation to explore the properties of dust nucleation in subsaturated vapors due to radiation losses the subcritical clusters have a smaller temperature compared to their vapor this alters the dynamical balance between attachment and detachment of monomers allowing for stable nucleation o... | [['we', 'use', 'the', 'kinetic', 'theory', 'of', 'nucleation', 'to', 'explore', 'the', 'properties', 'of', 'dust', 'nucleation', 'in', 'subsaturated', 'vapors', 'due', 'to', 'radiation', 'losses', 'the', 'subcritical', 'clusters', 'have', 'a', 'smaller', 'temperature', 'compared', 'to', 'their', 'vapor', 'this', 'alter... | [-0.06034044609942402, 0.20005119171968172, -0.08382135780098346, 0.0721447346970821, -0.02941624343347473, -0.06611485497799152, 0.06556375958920958, 0.38832653970815817, -0.23463607363355082, -0.2553612969051569, 0.0792190445593009, -0.25355311749885096, -0.0787509374642888, 0.1624654140466681, -0.019406310668161425,... |
710.2904 | Planets Around Massive Subgiants | Compared to planets around Sun-like stars, relatively little is known about
the occurrence rate and orbital properties of planets around stars more massive
than 1.3 Msun. The apparent deficit of planets around massive stars is due to a
strong selection bias against early-type dwarfs in Doppler-based planet
searches. ... | astro-ph | compared to planets around sunlike stars relatively little is known about the occurrence rate and orbital properties of planets around stars more massive than 13 msun the apparent deficit of planets around massive stars is due to a strong selection bias against earlytype dwarfs in dopplerbased planet searches one metho... | [['compared', 'to', 'planets', 'around', 'sunlike', 'stars', 'relatively', 'little', 'is', 'known', 'about', 'the', 'occurrence', 'rate', 'and', 'orbital', 'properties', 'of', 'planets', 'around', 'stars', 'more', 'massive', 'than', '13', 'msun', 'the', 'apparent', 'deficit', 'of', 'planets', 'around', 'massive', 'star... | [-0.08344610425939952, 0.16469646359539844, -0.05363763264860168, 0.13564788074158554, -0.16651044925674796, -0.05503266948543376, 0.14112339685247702, 0.37377229270835716, -0.05885575777475341, -0.3881795081789746, 0.04145848337617336, -0.31573149175242043, -0.057071772926120146, 0.20177729505997954, -0.12439662185815... |
710.2905 | Chiral Random Two-Matrix Theory and QCD with imaginary chemical
potential | We summarise recent results for the chiral Random Two-Matrix Theory
constructed to describe QCD in the epsilon-regime with imaginary chemical
potential. The virtue of this theory is that unquenched Lattice simulations can
be used to determine both low energy constants Sigma and F in the leading order
chiral Lagrangia... | hep-th hep-lat | we summarise recent results for the chiral random twomatrix theory constructed to describe qcd in the epsilonregime with imaginary chemical potential the virtue of this theory is that unquenched lattice simulations can be used to determine both low energy constants sigma and f in the leading order chiral lagrangian due... | [['we', 'summarise', 'recent', 'results', 'for', 'the', 'chiral', 'random', 'twomatrix', 'theory', 'constructed', 'to', 'describe', 'qcd', 'in', 'the', 'epsilonregime', 'with', 'imaginary', 'chemical', 'potential', 'the', 'virtue', 'of', 'this', 'theory', 'is', 'that', 'unquenched', 'lattice', 'simulations', 'can', 'be... | [-0.10005995037320714, 0.1458799600923577, -0.08602597481714418, 0.0800192704021286, -0.05235305944135269, -0.10575720743061258, 0.027708342920344037, 0.3700146010861947, -0.24614094952837778, -0.220894993447627, 0.04457807248601547, -0.2767457662866666, -0.1647942933683785, 0.0720982567837032, 0.043423153786548374, 0.... |
710.2906 | The gl(1|1) super-current algebra: the role of twist and logarithmic
fields | A free field representation of the gl(1|1)_k current algebra at arbitrary
level k is given in terms of two scalar fields and a symplectic fermion. The
primary fields for all representations are explicitly constructed using the
twist and logarithmic fields in the symplectic fermion sector. A closed
operator algebra is... | hep-th math-ph math.MP | a free field representation of the gl11_k current algebra at arbitrary level k is given in terms of two scalar fields and a symplectic fermion the primary fields for all representations are explicitly constructed using the twist and logarithmic fields in the symplectic fermion sector a closed operator algebra is descri... | [['a', 'free', 'field', 'representation', 'of', 'the', 'gl11_k', 'current', 'algebra', 'at', 'arbitrary', 'level', 'k', 'is', 'given', 'in', 'terms', 'of', 'two', 'scalar', 'fields', 'and', 'a', 'symplectic', 'fermion', 'the', 'primary', 'fields', 'for', 'all', 'representations', 'are', 'explicitly', 'constructed', 'us... | [-0.18371544879113064, 0.21453660806702052, -0.06357627679578594, 0.09473397802050057, -0.08824126739589283, -0.1659356645751195, -0.031648785249448426, 0.2914530346170068, -0.28574490021975313, -0.248640870770867, 0.06717318522965261, -0.2535018579133588, -0.16491371573742908, 0.15168750722755175, -0.00699774448539905... |
710.2907 | Renormalization group approach to 2D Coulomb interacting Dirac fermions
with random gauge potential | We argue that massless Dirac particles in two spatial dimensions with $1/r$
Coulomb repulsion and quenched random gauge field are described by a manifold
of fixed points which can be accessed perturbatively in disorder and
interaction strength, thereby confirming and extending the results of
arXiv:0707.4171. At small... | cond-mat.mes-hall cond-mat.dis-nn | we argue that massless dirac particles in two spatial dimensions with 1r coulomb repulsion and quenched random gauge field are described by a manifold of fixed points which can be accessed perturbatively in disorder and interaction strength thereby confirming and extending the results of arxiv07074171 at small interact... | [['we', 'argue', 'that', 'massless', 'dirac', 'particles', 'in', 'two', 'spatial', 'dimensions', 'with', '1r', 'coulomb', 'repulsion', 'and', 'quenched', 'random', 'gauge', 'field', 'are', 'described', 'by', 'a', 'manifold', 'of', 'fixed', 'points', 'which', 'can', 'be', 'accessed', 'perturbatively', 'in', 'disorder', ... | [-0.18676648916247265, 0.28091652121855243, -0.08176087783407662, 0.06493988081770526, 0.008834714072230333, -0.2238343560829299, 0.05522611841571505, 0.35743666986946937, -0.2012640086014743, -0.22679913669292415, 0.02933612064603571, -0.31433658267964015, -0.1125396901995621, 0.10308125142806343, 0.04563310916547651,... |
710.2908 | A tour of theta dualities on moduli spaces of sheaves | The purpose of this paper is twofold. First, we survey known results about
theta dualities on moduli spaces of sheaves on curves and surfaces. Secondly,
we establish new such dualities in the surface case. Among others, the case of
elliptic K3 surfaces is studied in detail; we propose further conjectures which
are sh... | math.AG | the purpose of this paper is twofold first we survey known results about theta dualities on moduli spaces of sheaves on curves and surfaces secondly we establish new such dualities in the surface case among others the case of elliptic k3 surfaces is studied in detail we propose further conjectures which are shown to im... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'twofold', 'first', 'we', 'survey', 'known', 'results', 'about', 'theta', 'dualities', 'on', 'moduli', 'spaces', 'of', 'sheaves', 'on', 'curves', 'and', 'surfaces', 'secondly', 'we', 'establish', 'new', 'such', 'dualities', 'in', 'the', 'surface', 'case', 'among', 'other... | [-0.17317273529663094, 0.07987361325343188, -0.11597118892690592, 0.14528378234204037, -0.08840140523879152, -0.12763598316202038, 0.014651105945456055, 0.3741676534869169, -0.2648254297020143, -0.24259717572937933, 0.09211449325901636, -0.26738203630635615, -0.24736138773069047, 0.2289329999077477, -0.1995301433806225... |
710.2909 | Signal and Charge Transfer Efficiency of Few Electrons Clocked on
Microscopic Superfluid Helium Channels | Electrons floating on the surface of liquid helium are possible spin-qubits
for quantum information processing. Varying electric potentials are not
expected to modify spin states, which allows their transport on helium using a
charge-coupled device (CCD)-like array of underlying gates. This approach
depends upon effi... | cond-mat.other | electrons floating on the surface of liquid helium are possible spinqubits for quantum information processing varying electric potentials are not expected to modify spin states which allows their transport on helium using a chargecoupled device ccdlike array of underlying gates this approach depends upon efficient inte... | [['electrons', 'floating', 'on', 'the', 'surface', 'of', 'liquid', 'helium', 'are', 'possible', 'spinqubits', 'for', 'quantum', 'information', 'processing', 'varying', 'electric', 'potentials', 'are', 'not', 'expected', 'to', 'modify', 'spin', 'states', 'which', 'allows', 'their', 'transport', 'on', 'helium', 'using', ... | [-0.14308567647551468, 0.23831517828715054, -0.03155243535103753, 0.027510144146765735, -0.030615472732934843, -0.188043667544979, 0.11577960045001101, 0.4031201170021018, -0.25323753860280956, -0.334857756098689, 0.011024027089534198, -0.29143199628116806, -0.037783956520670896, 0.2524048102976278, -0.0138371989271755... |
710.291 | Generating dark solitons by single photons | We show that dark solitons in 1D bose systems may be excited by resonant
absorption of single quanta of an external ac field. The energy of the quantum
$\hbar\omega$ should be slightly blue-detuned from the energy of a soliton with
momentum $\hbar q$, where $q$ is the external field wavenumber $q$. We
calculate the a... | cond-mat.other cond-mat.stat-mech | we show that dark solitons in 1d bose systems may be excited by resonant absorption of single quanta of an external ac field the energy of the quantum hbaromega should be slightly bluedetuned from the energy of a soliton with momentum hbar q where q is the external field wavenumber q we calculate the absorption crossse... | [['we', 'show', 'that', 'dark', 'solitons', 'in', '1d', 'bose', 'systems', 'may', 'be', 'excited', 'by', 'resonant', 'absorption', 'of', 'single', 'quanta', 'of', 'an', 'external', 'ac', 'field', 'the', 'energy', 'of', 'the', 'quantum', 'hbaromega', 'should', 'be', 'slightly', 'bluedetuned', 'from', 'the', 'energy', 'o... | [-0.1939655466315647, 0.22709324973281278, -0.08844236671436756, 0.0355729048419995, -0.042429423630459324, -0.1487170465323808, 0.02393307811247983, 0.38702012115113793, -0.25617126035060556, -0.2629018452218069, -0.02552286241275613, -0.2829175813655768, -0.07534194152824403, 0.18415723369911402, 0.031153394258581102... |
710.2911 | Spectral isolation of bi-invariant metrics on compact Lie groups | We show that a bi-invariant metric on a compact connected Lie group $G$ is
spectrally isolated within the class of left-invariant metrics. In fact, we
prove that given a bi-invariant metric $g_0$ on $G$ there is a positive integer
$N$ such that, within a neighborhood of $g_0$ in the class of left-invariant
metrics of... | math.DG | we show that a biinvariant metric on a compact connected lie group g is spectrally isolated within the class of leftinvariant metrics in fact we prove that given a biinvariant metric g_0 on g there is a positive integer n such that within a neighborhood of g_0 in the class of leftinvariant metrics of at most the same v... | [['we', 'show', 'that', 'a', 'biinvariant', 'metric', 'on', 'a', 'compact', 'connected', 'lie', 'group', 'g', 'is', 'spectrally', 'isolated', 'within', 'the', 'class', 'of', 'leftinvariant', 'metrics', 'in', 'fact', 'we', 'prove', 'that', 'given', 'a', 'biinvariant', 'metric', 'g_0', 'on', 'g', 'there', 'is', 'a', 'pos... | [-0.23439781162678525, 0.11638414126747612, -0.04545003931781047, -0.011625337241782566, -0.12003253738845834, -0.12149733083657502, -0.03424842132443792, 0.44753829791639627, -0.24448033612289496, -0.2374069762908006, 0.04170473225106056, -0.31235068276775685, -0.1653881912522562, 0.1746695895713304, -0.08504861330592... |
710.2912 | Updating Probabilities: An Econometric Example | We demonstrate how information in the form of observable data and moment
constraints are introduced into the method of Maximum relative Entropy (ME). A
general example of updating with data and moments is shown. A specific
econometric example is solved in detail which can then be used as a template
for real world pro... | stat.ME stat.CO | we demonstrate how information in the form of observable data and moment constraints are introduced into the method of maximum relative entropy me a general example of updating with data and moments is shown a specific econometric example is solved in detail which can then be used as a template for real world problems ... | [['we', 'demonstrate', 'how', 'information', 'in', 'the', 'form', 'of', 'observable', 'data', 'and', 'moment', 'constraints', 'are', 'introduced', 'into', 'the', 'method', 'of', 'maximum', 'relative', 'entropy', 'me', 'a', 'general', 'example', 'of', 'updating', 'with', 'data', 'and', 'moments', 'is', 'shown', 'a', 'sp... | [-0.05773045449687571, 0.0324665023316, -0.11326914129627717, 0.10144490803233222, -0.10068320159838107, -0.12592195956716062, 0.02959857668768539, 0.35119108445438985, -0.2786352386874323, -0.3351698948095578, 0.16177157672889833, -0.2908175524223495, -0.17084106042779781, 0.23148868820705526, -0.05610001627104105, 0.... |
710.2913 | Tight closure does not commute with localization | We give an example showing that tight closure does not commute with
localization.
| math.AC math.AG | we give an example showing that tight closure does not commute with localization | [['we', 'give', 'an', 'example', 'showing', 'that', 'tight', 'closure', 'does', 'not', 'commute', 'with', 'localization']] | [-0.17911979298178965, 0.08550748677785472, -0.06725023257044646, 0.09481085578982647, -0.11003765026823832, -0.18960464573823488, -0.009141038386867596, 0.49629615533810395, -0.2267347717514405, -0.219360938295722, 0.023475579738330383, -0.21061215463739175, -0.23920674894291621, 0.23998485734829536, -0.22172123222396... |
710.2914 | Andreev-like reflections with cold atoms | We propose a setup in which Andreev-like reflections predicted for 1D
transport systems could be observed time-dependently using cold atoms in a 1D
optical lattice. Using time-dependent Density Matrix Renormalisation Group
methods we analyse the wavepacket dynamics as a density excitation propagates
across a boundary... | cond-mat.other | we propose a setup in which andreevlike reflections predicted for 1d transport systems could be observed timedependently using cold atoms in a 1d optical lattice using timedependent density matrix renormalisation group methods we analyse the wavepacket dynamics as a density excitation propagates across a boundary in th... | [['we', 'propose', 'a', 'setup', 'in', 'which', 'andreevlike', 'reflections', 'predicted', 'for', '1d', 'transport', 'systems', 'could', 'be', 'observed', 'timedependently', 'using', 'cold', 'atoms', 'in', 'a', '1d', 'optical', 'lattice', 'using', 'timedependent', 'density', 'matrix', 'renormalisation', 'group', 'metho... | [-0.12773452006355934, 0.17796110508434876, -0.10891435479090826, 0.05432181191202756, 0.02129245369468589, -0.17009980532315536, 0.02431828563881887, 0.4194781311812836, -0.2572427196176471, -0.277873496921431, 0.041286433038515716, -0.27212723490555546, -0.14288179122691824, 0.1575942818245322, 0.035066611605469845, ... |
710.2915 | The late-time tails in the Reissner-Nordstr\"{o}m spacetime revisited | We propose that the late-time tail problem in the Reissner-Nordstr\"{o}m (RN)
spacetime is dual to a tail problem in the Schwarzschild spacetime with a
different initial data set: at a fixed observation point the asymptotic decay
rate of the fields are equal. This duality is used to find the decay rate for
tails in R... | gr-qc | we propose that the latetime tail problem in the reissnernordstrom rn spacetime is dual to a tail problem in the schwarzschild spacetime with a different initial data set at a fixed observation point the asymptotic decay rate of the fields are equal this duality is used to find the decay rate for tails in rn this decay... | [['we', 'propose', 'that', 'the', 'latetime', 'tail', 'problem', 'in', 'the', 'reissnernordstrom', 'rn', 'spacetime', 'is', 'dual', 'to', 'a', 'tail', 'problem', 'in', 'the', 'schwarzschild', 'spacetime', 'with', 'a', 'different', 'initial', 'data', 'set', 'at', 'a', 'fixed', 'observation', 'point', 'the', 'asymptotic'... | [-0.12873873406492953, 0.08160103075373518, -0.09436703161614489, 0.10538906390768295, -0.027766470362974416, -0.12208478700772707, -0.027340649502046073, 0.3018211512200868, -0.2468833634108583, -0.19629556577610993, 0.13477875853527282, -0.33312985225955943, -0.04907231459588702, 0.1691752719317577, -0.03731741997371... |
710.2916 | Dissociation and ionization of small molecules steered by external noise | We show that ionization and dissociation can be influenced separately in a
molecule with appropriate external noise. Specifically we investigate the
hydrogen molecular ion under a stochastic force quantum mechanically beyond the
Born-Oppenheimer approximation. We find that up to 30% of dissociation without
ionization... | quant-ph | we show that ionization and dissociation can be influenced separately in a molecule with appropriate external noise specifically we investigate the hydrogen molecular ion under a stochastic force quantum mechanically beyond the bornoppenheimer approximation we find that up to 30 of dissociation without ionization can b... | [['we', 'show', 'that', 'ionization', 'and', 'dissociation', 'can', 'be', 'influenced', 'separately', 'in', 'a', 'molecule', 'with', 'appropriate', 'external', 'noise', 'specifically', 'we', 'investigate', 'the', 'hydrogen', 'molecular', 'ion', 'under', 'a', 'stochastic', 'force', 'quantum', 'mechanically', 'beyond', '... | [-0.08174212978063326, 0.19535461786853256, -0.061728532303054376, 0.06408905078006803, 0.05297552448486523, -0.16008419353725775, 0.1118386824799807, 0.44028363137874965, -0.30157610608862256, -0.31059257102743637, -0.02539054171032852, -0.20089753065258265, -0.08028393172008812, 0.14225042913601083, 0.005984792011385... |
710.2917 | Comparison of Boltzmann Kinetics with Quantum Dynamics for a Chiral
Yukawa Model Far From Equilibrium | Boltzmann equations are often used to describe the non-equilibrium
time-evolution of many-body systems in particle physics. Prominent examples are
the computation of the baryon asymmetry of the universe and the evolution of
the quark-gluon plasma after a relativistic heavy ion collision. However,
Boltzmann equations ... | hep-ph | boltzmann equations are often used to describe the nonequilibrium timeevolution of manybody systems in particle physics prominent examples are the computation of the baryon asymmetry of the universe and the evolution of the quarkgluon plasma after a relativistic heavy ion collision however boltzmann equations are only ... | [['boltzmann', 'equations', 'are', 'often', 'used', 'to', 'describe', 'the', 'nonequilibrium', 'timeevolution', 'of', 'manybody', 'systems', 'in', 'particle', 'physics', 'prominent', 'examples', 'are', 'the', 'computation', 'of', 'the', 'baryon', 'asymmetry', 'of', 'the', 'universe', 'and', 'the', 'evolution', 'of', 't... | [-0.10817736559317212, 0.165882450484947, -0.12915414333238603, 0.11565842269929807, -0.044858967987718164, -0.1117648762461453, -0.006142140992349116, 0.2680790488720759, -0.27910874970769, -0.26852373048090017, 0.01863293177806414, -0.2832908339230446, -0.07065279039318909, 0.15532391540422155, 0.042045709137340424, ... |
710.2918 | Twisted Yangians and finite W-algebras | We construct an explicit set of generators for the finite W-algebras
associated to nilpotent matrices in the symplectic or orthogonal Lie algebras
whose Jordan blocks are all of the same size. We use these generators to show
that such finite W-algebras are quotients of twisted Yangians.
| math.QA math.RA math.RT | we construct an explicit set of generators for the finite walgebras associated to nilpotent matrices in the symplectic or orthogonal lie algebras whose jordan blocks are all of the same size we use these generators to show that such finite walgebras are quotients of twisted yangians | [['we', 'construct', 'an', 'explicit', 'set', 'of', 'generators', 'for', 'the', 'finite', 'walgebras', 'associated', 'to', 'nilpotent', 'matrices', 'in', 'the', 'symplectic', 'or', 'orthogonal', 'lie', 'algebras', 'whose', 'jordan', 'blocks', 'are', 'all', 'of', 'the', 'same', 'size', 'we', 'use', 'these', 'generators'... | [-0.1852666243262913, 0.1282435542547635, 0.002161672581797061, 0.04001224694935524, -0.13927544551172658, -0.1139057676874749, -0.08284281595842913, 0.41407508079124533, -0.3578103346669156, -0.13594937657572978, 0.13403479007589023, -0.2652899299485042, -0.1148968453610154, 0.17915892177362644, -0.17097741805786348, ... |
710.2919 | Phase structure of twisted Eguchi-Kawai model | We study the phase structure of the four-dimensional twisted Eguchi-Kawai
model using numerical simulations. This model is an effective tool for studying
SU(N) gauge theory in the large-N limit and provides a nonperturbative
formulation of the gauge theory on noncommutative spaces. Recently it was found
that its Z_N^... | hep-lat hep-th | we study the phase structure of the fourdimensional twisted eguchikawai model using numerical simulations this model is an effective tool for studying sun gauge theory in the largen limit and provides a nonperturbative formulation of the gauge theory on noncommutative spaces recently it was found that its z_n4 symmetry... | [['we', 'study', 'the', 'phase', 'structure', 'of', 'the', 'fourdimensional', 'twisted', 'eguchikawai', 'model', 'using', 'numerical', 'simulations', 'this', 'model', 'is', 'an', 'effective', 'tool', 'for', 'studying', 'sun', 'gauge', 'theory', 'in', 'the', 'largen', 'limit', 'and', 'provides', 'a', 'nonperturbative', ... | [-0.12330070588405818, 0.1309344555423756, -0.14123498431380288, 0.10528739105211571, -0.032254658480908006, -0.0920513083345871, 0.02440801166503274, 0.3492102962522272, -0.23392950460076967, -0.2672179670548661, 0.0942729361159628, -0.210212570798405, -0.18494924029057963, 0.11186270694188932, -0.004619685608826756, ... |
710.292 | Continuum theory for the piezoelectric response of chiral nanotubes
under uniaxial and torsional stresses | We develop and solve a continuum theory for the piezoelectric response of
nanotubes under applied uniaxial and torsional stresses. We find that the
piezoelectric response is controlled by the chiral angle, the aspect ratio, and
two dimensionless parameters specifying the ratio of the strengths of the
electrostatic an... | cond-mat.mtrl-sci cond-mat.mes-hall | we develop and solve a continuum theory for the piezoelectric response of nanotubes under applied uniaxial and torsional stresses we find that the piezoelectric response is controlled by the chiral angle the aspect ratio and two dimensionless parameters specifying the ratio of the strengths of the electrostatic and ela... | [['we', 'develop', 'and', 'solve', 'a', 'continuum', 'theory', 'for', 'the', 'piezoelectric', 'response', 'of', 'nanotubes', 'under', 'applied', 'uniaxial', 'and', 'torsional', 'stresses', 'we', 'find', 'that', 'the', 'piezoelectric', 'response', 'is', 'controlled', 'by', 'the', 'chiral', 'angle', 'the', 'aspect', 'rat... | [-0.1759744791418378, 0.14783025165249047, -0.03382884553665745, 0.008662492164274165, -0.01209616827264685, -0.12867060426124854, 0.0023876149448212878, 0.398774696883328, -0.24889934269293887, -0.2890946041363099, 0.0495461555336329, -0.24014405349815457, -0.17346102013784573, 0.17922238816491104, 0.01132757612504065... |
710.2921 | Shock-Induced Flows through Packed Beds: Transient Regimes | The early stage of the transient regimes in the shock-induced flows within
solid-packed beds are investigated in the linear longwave and high-frequency
approximation. The transient resistance law is refined as the Duhameltime
integral that follows from the general concept of dynamic tortuosity and
compressibility of ... | physics.class-ph physics.gen-ph | the early stage of the transient regimes in the shockinduced flows within solidpacked beds are investigated in the linear longwave and highfrequency approximation the transient resistance law is refined as the duhameltime integral that follows from the general concept of dynamic tortuosity and compressibility of the pa... | [['the', 'early', 'stage', 'of', 'the', 'transient', 'regimes', 'in', 'the', 'shockinduced', 'flows', 'within', 'solidpacked', 'beds', 'are', 'investigated', 'in', 'the', 'linear', 'longwave', 'and', 'highfrequency', 'approximation', 'the', 'transient', 'resistance', 'law', 'is', 'refined', 'as', 'the', 'duhameltime', ... | [-0.1259641206272366, 0.11974769011861316, -0.12967456646368536, 0.06145463502657613, -0.024708912327465877, -0.09498215098799744, 0.00942615912177823, 0.3114814644705662, -0.26672749373484667, -0.2561501961981904, 0.15178139732238954, -0.2894007534208432, -0.15545885306848606, 0.21453659128869923, -0.03472250893311968... |
710.2922 | Experimental demonstration of phase measurement precision beating
standard quantum limit by projection measurement | We propose and demonstrate experimentally a projection scheme to measure the
quantum phase with a precision beating the standard quantum limit. The initial
input state is a twin Fock state $|N,N>$ proposed by Holland and Burnett [Phys.
Rev. Lett. {\bf 71}, 1355 (1993)] but the phase information is extracted by a
quan... | quant-ph | we propose and demonstrate experimentally a projection scheme to measure the quantum phase with a precision beating the standard quantum limit the initial input state is a twin fock state nn proposed by holland and burnett phys rev lett bf 71 1355 1993 but the phase information is extracted by a quantum state projectio... | [['we', 'propose', 'and', 'demonstrate', 'experimentally', 'a', 'projection', 'scheme', 'to', 'measure', 'the', 'quantum', 'phase', 'with', 'a', 'precision', 'beating', 'the', 'standard', 'quantum', 'limit', 'the', 'initial', 'input', 'state', 'is', 'a', 'twin', 'fock', 'state', 'nn', 'proposed', 'by', 'holland', 'and'... | [-0.0968035311636395, 0.21870936055455614, -0.0581240300607803, -0.0008044129359711073, 0.008916949392250269, -0.146047521225813, 0.13734033735155468, 0.3233355889050751, -0.20285738777774986, -0.30060356678348954, 0.031028947357254307, -0.2942205362556742, -0.06771723533482614, 0.17844600452220824, -0.0449736029011114... |
710.2923 | Looking for signals beyond the neutrino Standard Model | Any new neutrino physics at the TeV scale must include a suppression
mechanism to keep its contribution to light neutrino masses small enough. We
review some seesaw model examples with weakly broken lepton number, and comment
on the expected effects at large colliders and in neutrino oscillations.
| hep-ph | any new neutrino physics at the tev scale must include a suppression mechanism to keep its contribution to light neutrino masses small enough we review some seesaw model examples with weakly broken lepton number and comment on the expected effects at large colliders and in neutrino oscillations | [['any', 'new', 'neutrino', 'physics', 'at', 'the', 'tev', 'scale', 'must', 'include', 'a', 'suppression', 'mechanism', 'to', 'keep', 'its', 'contribution', 'to', 'light', 'neutrino', 'masses', 'small', 'enough', 'we', 'review', 'some', 'seesaw', 'model', 'examples', 'with', 'weakly', 'broken', 'lepton', 'number', 'and... | [-0.08089225258717829, 0.33838411315562245, 0.013727241691122664, 0.2530411819907579, -0.13453505810429442, -0.19377879307486434, 0.045677056803586004, 0.2863698254359212, -0.23973507461871238, -0.33886231941745637, 0.05295183549962066, -0.3352282207776257, -0.01586062328374766, 0.16797368212087832, 0.03955997092688971... |
710.2924 | Neutron Polarisabilities from Deuteron Compton Scattering in \chiEFT | Chiral Effective Field Theory is for photon energies up to 200 MeV the tool
to accurately determine the polarisabilities of the neutron from deuteron
Compton scattering. A multipole analysis reveals that dispersive effects from
an explicit Delta(1232) prove in particular indispensable to understand the
data at 95 MeV... | nucl-th | chiral effective field theory is for photon energies up to 200 mev the tool to accurately determine the polarisabilities of the neutron from deuteron compton scattering a multipole analysis reveals that dispersive effects from an explicit delta1232 prove in particular indispensable to understand the data at 95 mev meas... | [['chiral', 'effective', 'field', 'theory', 'is', 'for', 'photon', 'energies', 'up', 'to', '200', 'mev', 'the', 'tool', 'to', 'accurately', 'determine', 'the', 'polarisabilities', 'of', 'the', 'neutron', 'from', 'deuteron', 'compton', 'scattering', 'a', 'multipole', 'analysis', 'reveals', 'that', 'dispersive', 'effects... | [-0.0012346177807666806, 0.19589959572451926, -0.08143116554452313, 0.17857058063392234, -0.055418464640239015, -0.07744436402124567, 0.051831781855211236, 0.31656506086866826, -0.1725141191894873, -0.32452865460744273, -0.02342787566375879, -0.34348502282339793, 0.03652732383507567, 0.19348834925450575, 0.084103166725... |
710.2925 | Bridging over p-wave pi-production and weak processes in few-nucleon
systems with chiral perturbation theory | We focus on a powerful aspect of chiral perturbation theory (chi PT) which
provides us with a ``bridge'' over different reactions. For this purpose, we
study a contact operator which contributes p-wave pi-production and several
weak processes. We fix the unknown coupling of the contact operator using a
matrix element... | nucl-th hep-ph | we focus on a powerful aspect of chiral perturbation theory chi pt which provides us with a bridge over different reactions for this purpose we study a contact operator which contributes pwave piproduction and several weak processes we fix the unknown coupling of the contact operator using a matrix element of a lowener... | [['we', 'focus', 'on', 'a', 'powerful', 'aspect', 'of', 'chiral', 'perturbation', 'theory', 'chi', 'pt', 'which', 'provides', 'us', 'with', 'a', 'bridge', 'over', 'different', 'reactions', 'for', 'this', 'purpose', 'we', 'study', 'a', 'contact', 'operator', 'which', 'contributes', 'pwave', 'piproduction', 'and', 'sever... | [-0.12409808565178639, 0.13714596456565187, -0.08683508209936269, 0.07219346530596944, -0.07685615047584515, -0.1281765835633228, 0.037806400158963575, 0.33854008297976496, -0.23754546761356451, -0.2193338559823228, 0.03266670933511056, -0.2997538131121155, -0.1319474513784244, 0.13890618140568267, 0.043014812703289974... |
710.2926 | Long Baseline Neutrino Experiments with Two-Detector Setup | I discuss why and how powerful is the two-detector setting in neutrino
oscillation experiments. I cover three concrete examples: (1) reactor
\theta_{13} experiments, (2) T2KK, Tokai-to-Kamioka-Korea two-detector complex
for measuring CP violation, determining the neutrino mass hierarchy, and
resolving the eight-fold ... | hep-ph hep-ex | i discuss why and how powerful is the twodetector setting in neutrino oscillation experiments i cover three concrete examples 1 reactor theta_13 experiments 2 t2kk tokaitokamiokakorea twodetector complex for measuring cp violation determining the neutrino mass hierarchy and resolving the eightfold parameter degeneracy ... | [['i', 'discuss', 'why', 'and', 'how', 'powerful', 'is', 'the', 'twodetector', 'setting', 'in', 'neutrino', 'oscillation', 'experiments', 'i', 'cover', 'three', 'concrete', 'examples', '1', 'reactor', 'theta_13', 'experiments', '2', 't2kk', 'tokaitokamiokakorea', 'twodetector', 'complex', 'for', 'measuring', 'cp', 'vio... | [-0.11731500757124388, 0.2861910084770484, 0.08032862480401738, 0.2290411572144931, -0.08193479056441874, -0.22747376086331453, 0.06605346005579288, 0.27332716147330677, -0.21349468407976074, -0.3436906495780656, 0.09965949695712577, -0.33700322514315223, -0.02747713416024591, 0.20630913625725292, 0.07063382555674197, ... |
710.2927 | Renormalization group analysis of the chiral pion production operator
for NN\to d\pi | We are interested in the consistency between the cutoff, chiral symmetry, and
the power counting. For this purpose, we apply the Wilsonian renormalization
group (RG) to an operator and then decrease the Wilsonian cutoff. As an
example, we study the s-wave pion production operator for NN\to d\pi, derived
in chiral per... | nucl-th hep-ph | we are interested in the consistency between the cutoff chiral symmetry and the power counting for this purpose we apply the wilsonian renormalization group rg to an operator and then decrease the wilsonian cutoff as an example we study the swave pion production operator for nnto dpi derived in chiral perturbation theo... | [['we', 'are', 'interested', 'in', 'the', 'consistency', 'between', 'the', 'cutoff', 'chiral', 'symmetry', 'and', 'the', 'power', 'counting', 'for', 'this', 'purpose', 'we', 'apply', 'the', 'wilsonian', 'renormalization', 'group', 'rg', 'to', 'an', 'operator', 'and', 'then', 'decrease', 'the', 'wilsonian', 'cutoff', 'a... | [-0.10352320046372061, 0.14514573225870195, -0.10081203637030925, 0.09635013714884814, -0.0897257720183545, -0.10168121778632253, 0.02086039952983519, 0.3377637356085685, -0.2263552220447839, -0.2278206058669365, 0.040015363619319226, -0.33867949922795143, -0.11767295002033121, 0.09065212974849257, -0.03220762486018024... |
710.2928 | Embedding A4 into left-right flavor symmetry: Tribimaximal neutrino
mixing and fermion hierarchy | We address two fundamental aspects of flavor physics: the mass hierarchy and
the large lepton mixing angles. On one side, left-right flavor symmetry
realizes the democratic mass matrix patterns and explains why one family is
much heavier than the others. On the other side, discrete flavor symmetry such
as A4 leads to... | hep-ph | we address two fundamental aspects of flavor physics the mass hierarchy and the large lepton mixing angles on one side leftright flavor symmetry realizes the democratic mass matrix patterns and explains why one family is much heavier than the others on the other side discrete flavor symmetry such as a4 leads to the obs... | [['we', 'address', 'two', 'fundamental', 'aspects', 'of', 'flavor', 'physics', 'the', 'mass', 'hierarchy', 'and', 'the', 'large', 'lepton', 'mixing', 'angles', 'on', 'one', 'side', 'leftright', 'flavor', 'symmetry', 'realizes', 'the', 'democratic', 'mass', 'matrix', 'patterns', 'and', 'explains', 'why', 'one', 'family'... | [-0.09836977657723464, 0.33460949178908234, 0.020345159529223424, 0.21177088377866432, -0.1040123009453874, -0.18596766341847082, 0.05515406305097382, 0.32585068656062355, -0.2608851910807377, -0.27191156552227075, 0.044775225363540935, -0.27381694761743725, -0.05393897744919335, 0.04198074823414737, 0.0305440759186225... |
710.2929 | Quantum Barnes function as the partition function of the resolved
conifold | We suggest a new strategy for proving large $N$ duality by interpreting
Gromov-Witten, Donaldson-Thomas and Chern-Simons invariants of a Calabi-Yau
threefold as different characterizations of the same holomorphic function. For
the resolved conifold this function turns out to be the quantum Barnes
function, a natural ... | math.AG hep-th math.QA | we suggest a new strategy for proving large n duality by interpreting gromovwitten donaldsonthomas and chernsimons invariants of a calabiyau threefold as different characterizations of the same holomorphic function for the resolved conifold this function turns out to be the quantum barnes function a natural qdeformatio... | [['we', 'suggest', 'a', 'new', 'strategy', 'for', 'proving', 'large', 'n', 'duality', 'by', 'interpreting', 'gromovwitten', 'donaldsonthomas', 'and', 'chernsimons', 'invariants', 'of', 'a', 'calabiyau', 'threefold', 'as', 'different', 'characterizations', 'of', 'the', 'same', 'holomorphic', 'function', 'for', 'the', 'r... | [-0.14541276949099624, 0.02380295576623235, -0.161211375409785, 0.13916128430103597, -0.11002510695312268, -0.15832126973411784, 0.031202598412234623, 0.24827078266594654, -0.3099260448108021, -0.2444927615041916, 0.023855115964602776, -0.19631290461163586, -0.22981246479395898, 0.21704359693849723, -0.1299862940556919... |
710.293 | Atmospheric Circulation of Hot Jupiters: A Review of Current
Understanding | Hot Jupiters are new laboratories for the physics of giant planet
atmospheres. Subject to unusual forcing conditions, the circulation regime on
these planets may be unlike anything known in the Solar System. Characterizing
the atmospheric circulation of hot Jupiters is necessary for reliable
interpretation of the mul... | astro-ph | hot jupiters are new laboratories for the physics of giant planet atmospheres subject to unusual forcing conditions the circulation regime on these planets may be unlike anything known in the solar system characterizing the atmospheric circulation of hot jupiters is necessary for reliable interpretation of the multifac... | [['hot', 'jupiters', 'are', 'new', 'laboratories', 'for', 'the', 'physics', 'of', 'giant', 'planet', 'atmospheres', 'subject', 'to', 'unusual', 'forcing', 'conditions', 'the', 'circulation', 'regime', 'on', 'these', 'planets', 'may', 'be', 'unlike', 'anything', 'known', 'in', 'the', 'solar', 'system', 'characterizing',... | [-0.11896983055556391, 0.1645272478481081, -0.054907304540702556, 0.13402700312361318, -0.14260734763848495, -0.08760428664452852, 0.03789440482765674, 0.3253989660755751, -0.20949990629277965, -0.3408952494290598, 0.1321655401273908, -0.25915768227857, -0.12556212748143267, 0.246717136110516, -0.1360457908520673, 0.09... |
710.2931 | Exchange biasing of single-domain Ni nanoparticles spontaneously grown
in an antiferromagnetic MnO matrix | Exchange biased composites of ferromagnetic single-domain Ni nanoparticles
embedded within large grains of MnO have been prepared by reduction of
Ni$_x$Mn$_{1-x}$O$_4$ phases in flowing hydrogen. The Ni precipitates are 15-30
nm in extent, and the majority are completely encased within the MnO matrix.
The manner in w... | cond-mat.mtrl-sci | exchange biased composites of ferromagnetic singledomain ni nanoparticles embedded within large grains of mno have been prepared by reduction of ni_xmn_1xo_4 phases in flowing hydrogen the ni precipitates are 1530 nm in extent and the majority are completely encased within the mno matrix the manner in which the ni nano... | [['exchange', 'biased', 'composites', 'of', 'ferromagnetic', 'singledomain', 'ni', 'nanoparticles', 'embedded', 'within', 'large', 'grains', 'of', 'mno', 'have', 'been', 'prepared', 'by', 'reduction', 'of', 'ni_xmn_1xo_4', 'phases', 'in', 'flowing', 'hydrogen', 'the', 'ni', 'precipitates', 'are', '1530', 'nm', 'in', 'e... | [-0.15244544154453343, 0.24508096868866833, 0.035007408046621384, -0.001843971664962059, 0.008896274697351254, -0.12270651061987599, 0.060866271770140944, 0.43701988392335883, -0.2694086688610141, -0.36619436755476487, 0.010411751075742482, -0.3482513357648405, -0.013785386173906972, 0.08727728323300638, 0.062544133391... |
710.2932 | Total positivity for cominuscule Grassmannians | In this paper we explore the combinatorics of the non-negative part (G/P)+ of
a cominuscule Grassmannian. For each such Grassmannian we define Le-diagrams --
certain fillings of generalized Young diagrams which are in bijection with the
cells of (G/P)+. In the classical cases, we describe Le-diagrams explicitly in
te... | math.CO | in this paper we explore the combinatorics of the nonnegative part gp of a cominuscule grassmannian for each such grassmannian we define lediagrams certain fillings of generalized young diagrams which are in bijection with the cells of gp in the classical cases we describe lediagrams explicitly in terms of pattern avoi... | [['in', 'this', 'paper', 'we', 'explore', 'the', 'combinatorics', 'of', 'the', 'nonnegative', 'part', 'gp', 'of', 'a', 'cominuscule', 'grassmannian', 'for', 'each', 'such', 'grassmannian', 'we', 'define', 'lediagrams', 'certain', 'fillings', 'of', 'generalized', 'young', 'diagrams', 'which', 'are', 'in', 'bijection', '... | [-0.14650006874845448, 0.09379070344584761, -0.061001918867061085, 0.09225661054740406, -0.08938537636263803, -0.13083837266418744, 0.06633158118823881, 0.3549273234707388, -0.3130586457396434, -0.23388714985075323, 0.05518834754792889, -0.21976265454961155, -0.23901082573204555, 0.13612204231321812, -0.164073132846335... |
710.2933 | Alternative Derivation of Electromagnetic Cloaks and Concentrators | Beginning with a straightforward formulation of electromagnetic cloaking that
reduces to a boundary value problem involving a single Maxwell first-order
differential equation, explicit formulae for the relative
permittivity-permeability dyadic and fields of spherical and circular
cylindrical annular cloaks are derive... | physics.class-ph physics.optics | beginning with a straightforward formulation of electromagnetic cloaking that reduces to a boundary value problem involving a single maxwell firstorder differential equation explicit formulae for the relative permittivitypermeability dyadic and fields of spherical and circular cylindrical annular cloaks are derived in ... | [['beginning', 'with', 'a', 'straightforward', 'formulation', 'of', 'electromagnetic', 'cloaking', 'that', 'reduces', 'to', 'a', 'boundary', 'value', 'problem', 'involving', 'a', 'single', 'maxwell', 'firstorder', 'differential', 'equation', 'explicit', 'formulae', 'for', 'the', 'relative', 'permittivitypermeability', ... | [-0.1650174808786193, 0.1434248883145492, -0.05370207769229027, -0.013484912884226184, -0.1413871944065631, -0.13280987906664488, -0.0462919999572253, 0.4202190572395921, -0.2334851189142806, -0.27235572819632514, 0.08409606740587686, -0.2398324013197097, -0.09005339597179382, 0.20852052122297018, -0.03780342061566035,... |
710.2934 | A Tale Of Two Spicules: The Impact of Spicules on the Magnetic
Chromosphere | We use high-resolution observations of the Sun in Ca II H 3968 A from the
Solar Optical Telescope on Hinode to show that there are at least two types of
spicules that dominate the structure of the magnetic solar chromosphere. Both
types are tied to the relentless magnetoconvective driving in the photosphere,
but have... | astro-ph | we use highresolution observations of the sun in ca ii h 3968 a from the solar optical telescope on hinode to show that there are at least two types of spicules that dominate the structure of the magnetic solar chromosphere both types are tied to the relentless magnetoconvective driving in the photosphere but have very... | [['we', 'use', 'highresolution', 'observations', 'of', 'the', 'sun', 'in', 'ca', 'ii', 'h', '3968', 'a', 'from', 'the', 'solar', 'optical', 'telescope', 'on', 'hinode', 'to', 'show', 'that', 'there', 'are', 'at', 'least', 'two', 'types', 'of', 'spicules', 'that', 'dominate', 'the', 'structure', 'of', 'the', 'magnetic',... | [-0.12550029004047614, 0.24661257522955035, 0.04519199257416669, 0.09195933684815133, -0.08449456007795388, -0.10493077579728757, 0.02141687535586652, 0.4411655088750583, -0.23687984400659046, -0.3264162107370794, 0.09424456860019899, -0.27011726048429696, -0.0656633262778894, 0.23898378035493112, 0.009772335533464715,... |
710.2935 | Simulation Study of TenTen: A new Multi-TeV IACT array | TenTen is a proposed array of Imaging Atmospheric Cherenkov Telescopes (IACT)
optimized for the gamma ray energy regime of 10 TeV to 100 TeV, but with a
threshold of ~1 to a few TeV. It will offer a collecting area of 10 km2 above
energies of 10 TeV. In the initial phase, a cell of 3 to 5 modest-sized
telescopes, eac... | astro-ph | tenten is a proposed array of imaging atmospheric cherenkov telescopes iact optimized for the gamma ray energy regime of 10 tev to 100 tev but with a threshold of 1 to a few tev it will offer a collecting area of 10 km2 above energies of 10 tev in the initial phase a cell of 3 to 5 modestsized telescopes each with 1030... | [['tenten', 'is', 'a', 'proposed', 'array', 'of', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'iact', 'optimized', 'for', 'the', 'gamma', 'ray', 'energy', 'regime', 'of', '10', 'tev', 'to', '100', 'tev', 'but', 'with', 'a', 'threshold', 'of', '1', 'to', 'a', 'few', 'tev', 'it', 'will', 'offer', 'a', 'collectin... | [-0.12849278619098126, 0.19134115993679685, 0.01056247892859979, 0.0649419451678297, -0.05447604853910308, -0.1422421040029085, 0.019117510611457483, 0.4184816460273847, -0.17379411268869743, -0.43901994951194573, 0.1632592816330383, -0.3194255582624342, -0.059979623312741016, 0.25287176745341106, -0.005858204617094593... |
710.2936 | Optimal design problems in rough inhomogeneous media. Existence theory | This paper settles the existence question for a rather general class of
convex optimal design problems with a volume constraint. In low dimensions, we
prove the existence of an optimal configuration for general convex minimization
problems ruled by bounded measurable degenerate elliptic operators. Under a
mild contin... | math.AP | this paper settles the existence question for a rather general class of convex optimal design problems with a volume constraint in low dimensions we prove the existence of an optimal configuration for general convex minimization problems ruled by bounded measurable degenerate elliptic operators under a mild continuity ... | [['this', 'paper', 'settles', 'the', 'existence', 'question', 'for', 'a', 'rather', 'general', 'class', 'of', 'convex', 'optimal', 'design', 'problems', 'with', 'a', 'volume', 'constraint', 'in', 'low', 'dimensions', 'we', 'prove', 'the', 'existence', 'of', 'an', 'optimal', 'configuration', 'for', 'general', 'convex', ... | [-0.15717847894383483, 0.06108615886039909, -0.04879542768383062, 0.09173710251904474, -0.11057728581713984, -0.16935253128162528, 0.03081418789715607, 0.3192053781261286, -0.31195266480299544, -0.2289372761004481, 0.1885721578826589, -0.20074164905551686, -0.11546916565128479, 0.19782533501106572, -0.14293992372386785... |
710.2937 | A Search for SS Cyg Outburst Predictors | We report null results on a two year photometric search for outburst
predictors in SS Cyg. Observations in Johnson V and Cousins I were obtained
almost daily for multiple hours per night for two observing seasons. The
accumulated data are put through various statistical and visual analysis
techniques but fails to det... | astro-ph | we report null results on a two year photometric search for outburst predictors in ss cyg observations in johnson v and cousins i were obtained almost daily for multiple hours per night for two observing seasons the accumulated data are put through various statistical and visual analysis techniques but fails to detect ... | [['we', 'report', 'null', 'results', 'on', 'a', 'two', 'year', 'photometric', 'search', 'for', 'outburst', 'predictors', 'in', 'ss', 'cyg', 'observations', 'in', 'johnson', 'v', 'and', 'cousins', 'i', 'were', 'obtained', 'almost', 'daily', 'for', 'multiple', 'hours', 'per', 'night', 'for', 'two', 'observing', 'seasons'... | [-0.0922646822566296, 0.06870985824967243, -0.09291635213109355, 0.05951729336132606, -0.08470158106647432, -0.16513034186532927, 0.1065661066936122, 0.4383820313960314, -0.18884525444462066, -0.35828667206482756, 0.16171713921551903, -0.3941040735277865, -0.07376434918906953, 0.23611923205511023, -0.0960608535601447, ... |
710.2938 | The R(S^1)-graded equivariant homotopy of THH(F_p) | The main result of this paper is the computation of TR^n_{\alpha}(F_p;p) for
\alpha in R(S^1). These R(S^1)-graded TR-groups are the equivariant homotopy
groups naturally associated to the S^1-spectrum THH(F_p), the topological
Hochschild S^1-spectrum. This computation, which extends a partial result of
Hesselholt an... | math.AT math.KT | the main result of this paper is the computation of trn_alphaf_pp for alpha in rs1 these rs1graded trgroups are the equivariant homotopy groups naturally associated to the s1spectrum thhf_p the topological hochschild s1spectrum this computation which extends a partial result of hesselholt and madsen provides the first ... | [['the', 'main', 'result', 'of', 'this', 'paper', 'is', 'the', 'computation', 'of', 'trn_alphaf_pp', 'for', 'alpha', 'in', 'rs1', 'these', 'rs1graded', 'trgroups', 'are', 'the', 'equivariant', 'homotopy', 'groups', 'naturally', 'associated', 'to', 'the', 's1spectrum', 'thhf_p', 'the', 'topological', 'hochschild', 's1sp... | [-0.21870508445944223, 0.026937834478707776, -0.09414816898707715, 0.09625900142742062, -0.06658283799899639, -0.10725717620354974, -0.018451304121602636, 0.28545018362153013, -0.34651534049771726, -0.24822789744939655, 0.12225225133523862, -0.18876353172850535, -0.19131647439725283, 0.22357882460993198, -0.16463152918... |
710.2939 | Uncovering individual and collective human dynamics from mobile phone
records | Novel aspects of human dynamics and social interactions are investigated by
means of mobile phone data. Using extensive phone records resolved in both time
and space, we study the mean collective behavior at large scales and focus on
the occurrence of anomalous events. We discuss how these spatiotemporal
anomalies ca... | physics.soc-ph physics.data-an | novel aspects of human dynamics and social interactions are investigated by means of mobile phone data using extensive phone records resolved in both time and space we study the mean collective behavior at large scales and focus on the occurrence of anomalous events we discuss how these spatiotemporal anomalies can be ... | [['novel', 'aspects', 'of', 'human', 'dynamics', 'and', 'social', 'interactions', 'are', 'investigated', 'by', 'means', 'of', 'mobile', 'phone', 'data', 'using', 'extensive', 'phone', 'records', 'resolved', 'in', 'both', 'time', 'and', 'space', 'we', 'study', 'the', 'mean', 'collective', 'behavior', 'at', 'large', 'sca... | [-0.1393867725414791, 0.14764698889881078, -0.06550068924915839, 0.12625790176230786, -0.03952936886228842, -0.10109729624565432, 0.054405269940328405, 0.40560810339849185, -0.24234595274239187, -0.3263927618926852, 0.07977522442827352, -0.32916042715827426, -0.25572571728267884, 0.19410031519214724, -0.040568250295991... |
710.294 | Recent Advances in the Theory of Nuclear Forces and its Impact on
Microscopic Nuclear Structure | The theory of nuclear forces has made great progress since the turn of the
millenium using the framework of chiral effective field theory (ChEFT). The
advantage of this approach, which was originally proposed by Weinberg, is that
it has a firm basis in quantum-chromodynamics and allows for quantitative
calculations. ... | nucl-th | the theory of nuclear forces has made great progress since the turn of the millenium using the framework of chiral effective field theory cheft the advantage of this approach which was originally proposed by weinberg is that it has a firm basis in quantumchromodynamics and allows for quantitative calculations moreover ... | [['the', 'theory', 'of', 'nuclear', 'forces', 'has', 'made', 'great', 'progress', 'since', 'the', 'turn', 'of', 'the', 'millenium', 'using', 'the', 'framework', 'of', 'chiral', 'effective', 'field', 'theory', 'cheft', 'the', 'advantage', 'of', 'this', 'approach', 'which', 'was', 'originally', 'proposed', 'by', 'weinber... | [-0.07776846591510966, 0.09534113092860001, -0.17411375004567403, 0.05738215056449933, -0.07393251301770189, -0.07794519183555601, 0.03352038844064109, 0.3426294390408866, -0.16059074015150557, -0.2751268182378427, 0.03588601674027411, -0.25932806685365495, -0.19749246041117385, 0.17693439351221696, -0.0158145241459947... |
710.2941 | Why Is Supercritical Disk Accretion Feasible? | Although the occurrence of steady supercritical disk accretion onto a black
hole has been speculated about since the 1970s, it has not been accurately
verified so far. For the first time, we previously demonstrated it through
two-dimensional, long-term radiation-hydrodynamic simulations. To clarify why
this accretion... | astro-ph | although the occurrence of steady supercritical disk accretion onto a black hole has been speculated about since the 1970s it has not been accurately verified so far for the first time we previously demonstrated it through twodimensional longterm radiationhydrodynamic simulations to clarify why this accretion is possib... | [['although', 'the', 'occurrence', 'of', 'steady', 'supercritical', 'disk', 'accretion', 'onto', 'a', 'black', 'hole', 'has', 'been', 'speculated', 'about', 'since', 'the', '1970s', 'it', 'has', 'not', 'been', 'accurately', 'verified', 'so', 'far', 'for', 'the', 'first', 'time', 'we', 'previously', 'demonstrated', 'it'... | [-0.11496775965047196, 0.15050859668831468, -0.03664560534274407, 0.08423433690197873, -0.07349877883244654, -0.10553460125225134, 0.0033628648656199305, 0.38047755475444117, -0.24978950532846717, -0.3045425138188352, 0.09204232223414005, -0.2681356258656856, -0.017742951349489285, 0.21426684911389626, -0.0074199130122... |
710.2942 | Rapidity gap survival in the black-disk regime | We summarize how the approach to the black--disk regime (BDR) of strong
interactions at TeV energies influences rapidity gap survival in exclusive hard
diffraction pp--> p + H + p (H =dijet, \bar Q Q, Higgs). Employing a recently
developed partonic description of such processes, we discuss (a) the
suppression of diff... | hep-ph | we summarize how the approach to the blackdisk regime bdr of strong interactions at tev energies influences rapidity gap survival in exclusive hard diffraction pp p h p h dijet bar q q higgs employing a recently developed partonic description of such processes we discuss a the suppression of diffraction at small impact... | [['we', 'summarize', 'how', 'the', 'approach', 'to', 'the', 'blackdisk', 'regime', 'bdr', 'of', 'strong', 'interactions', 'at', 'tev', 'energies', 'influences', 'rapidity', 'gap', 'survival', 'in', 'exclusive', 'hard', 'diffraction', 'pp', 'p', 'h', 'p', 'h', 'dijet', 'bar', 'q', 'q', 'higgs', 'employing', 'a', 'recent... | [-0.08628489390426015, 0.2980129380051394, -0.14634042637771927, 0.21535159376749802, 0.003385858594487279, -0.0992029179277301, 0.035244414361856755, 0.3751178948994, -0.24717142655893024, -0.3037438887937026, -0.12879432582343786, -0.3337476393010594, 0.001406355050660796, 0.02759811641664197, 0.08287884248815225, 0.... |
710.2943 | Global quark polarization in non-central $A+A$ collisions | Partons produced in the early stage of non-central heavy-ion collisions can
develop a longitudinal fluid shear because of unequal local number densities of
participant target and projectile nucleons. Under such fluid shear, local
parton pairs with non-vanishing impact parameter have finite local relative
orbital angu... | nucl-th | partons produced in the early stage of noncentral heavyion collisions can develop a longitudinal fluid shear because of unequal local number densities of participant target and projectile nucleons under such fluid shear local parton pairs with nonvanishing impact parameter have finite local relative orbital angular mom... | [['partons', 'produced', 'in', 'the', 'early', 'stage', 'of', 'noncentral', 'heavyion', 'collisions', 'can', 'develop', 'a', 'longitudinal', 'fluid', 'shear', 'because', 'of', 'unequal', 'local', 'number', 'densities', 'of', 'participant', 'target', 'and', 'projectile', 'nucleons', 'under', 'such', 'fluid', 'shear', 'l... | [-0.14876155487050907, 0.30494491776099075, -0.14254315740437778, 0.08706841869531451, -0.048452461113196774, -0.051533262188722555, -0.028228323963294562, 0.34379321191594137, -0.26372226324091824, -0.26308028695072877, -0.08769214534471315, -0.2854363212722714, 0.08326320703611248, 0.10329298481349372, 0.093074331184... |
710.2944 | Gamow-Teller strength for the analog transitions to the first T=1/2,
J^pi=3/2- states in 13C and 13N and the implications for Type Ia supernovae | The Gamow-Teller strength for the transition from the ground state of 13C to
the T=1/2, J^pi=3/2- excited state at 3.51 MeV in 13N is extracted via the
13C(3He,t) reaction at 420 MeV. In contrast to results from earlier (p,n)
studies on 13C, a good agreement with shell-model calculations and the
empirical unit cross ... | nucl-ex | the gamowteller strength for the transition from the ground state of 13c to the t12 jpi32 excited state at 351 mev in 13n is extracted via the 13c3het reaction at 420 mev in contrast to results from earlier pn studies on 13c a good agreement with shellmodel calculations and the empirical unit cross section systematics ... | [['the', 'gamowteller', 'strength', 'for', 'the', 'transition', 'from', 'the', 'ground', 'state', 'of', '13c', 'to', 'the', 't12', 'jpi32', 'excited', 'state', 'at', '351', 'mev', 'in', '13n', 'is', 'extracted', 'via', 'the', '13c3het', 'reaction', 'at', '420', 'mev', 'in', 'contrast', 'to', 'results', 'from', 'earlier... | [-0.030763293909361798, 0.12169959493202426, -0.042064441029096844, 0.09402727106215149, 0.01787543072418499, -0.03629100990828948, 0.09845288913554938, 0.3482301289795787, -0.1924631606897939, -0.308985052472454, -0.0014715245254022086, -0.3483151331922765, -0.04123603061662387, 0.2065623385291073, 0.03703496659413065... |
710.2945 | Resonances of 7He in the complex scaling method | We study the resonance spectroscopy of 7He in the 4He+n+n+n cluster model,
where the motion of valence neutrons is described in the cluster orbital shell
model. Many-body resonances are treated on the correct boundary condition as
the Gamow states in the complex scaling method. We obtain five resonances and
investiga... | nucl-th | we study the resonance spectroscopy of 7he in the 4hennn cluster model where the motion of valence neutrons is described in the cluster orbital shell model manybody resonances are treated on the correct boundary condition as the gamow states in the complex scaling method we obtain five resonances and investigate their ... | [['we', 'study', 'the', 'resonance', 'spectroscopy', 'of', '7he', 'in', 'the', '4hennn', 'cluster', 'model', 'where', 'the', 'motion', 'of', 'valence', 'neutrons', 'is', 'described', 'in', 'the', 'cluster', 'orbital', 'shell', 'model', 'manybody', 'resonances', 'are', 'treated', 'on', 'the', 'correct', 'boundary', 'con... | [-0.1197336558600824, 0.16409966925111336, -0.08458135457327351, 0.07718473751571539, 0.014566064057533398, -0.06395203342390621, 0.06511465807118987, 0.3548007872051153, -0.19673332555043416, -0.3112262885890201, 0.025018048863738585, -0.2901647156661647, -0.061975208612588734, 0.13286681041821966, 0.03621733744238686... |
710.2946 | An universal algorithm of calculating terms of atomic many-body
perturbation theory | An algorithm, based on numerical description of the terms of many-body
perturbation theory (Goldstone diagrams), is presented. The algorithm allows
the use of the same piece of computer code to evaluate any particular diagram
in any specific order of the perturbation theory or to calculate similar terms
in other area... | physics.atom-ph physics.comp-ph | an algorithm based on numerical description of the terms of manybody perturbation theory goldstone diagrams is presented the algorithm allows the use of the same piece of computer code to evaluate any particular diagram in any specific order of the perturbation theory or to calculate similar terms in other areas of the... | [['an', 'algorithm', 'based', 'on', 'numerical', 'description', 'of', 'the', 'terms', 'of', 'manybody', 'perturbation', 'theory', 'goldstone', 'diagrams', 'is', 'presented', 'the', 'algorithm', 'allows', 'the', 'use', 'of', 'the', 'same', 'piece', 'of', 'computer', 'code', 'to', 'evaluate', 'any', 'particular', 'diagra... | [-0.08645456778834125, 0.09800210853521733, -0.05718041257932782, 0.05989683554205975, 0.00611188572279557, -0.08322158281656879, 0.022301297174568323, 0.287031846759082, -0.23514373296078434, -0.3046485141299113, 0.045490500775890216, -0.3198701630334889, -0.14295798843010776, 0.14978602100637983, 0.04094293245321347,... |
710.2947 | Average Path Length in Complex Networks: Patterns and Predictions | A simple and accurate relationship is demonstrated that links the average
shortest path, nodes, and edges in a complex network. This relationship takes
advantage of the concept of link density and shows a large improvement in
fitting networks of all scales over the typical random graph model. The
relationships herein... | physics.soc-ph | a simple and accurate relationship is demonstrated that links the average shortest path nodes and edges in a complex network this relationship takes advantage of the concept of link density and shows a large improvement in fitting networks of all scales over the typical random graph model the relationships herein can a... | [['a', 'simple', 'and', 'accurate', 'relationship', 'is', 'demonstrated', 'that', 'links', 'the', 'average', 'shortest', 'path', 'nodes', 'and', 'edges', 'in', 'a', 'complex', 'network', 'this', 'relationship', 'takes', 'advantage', 'of', 'the', 'concept', 'of', 'link', 'density', 'and', 'shows', 'a', 'large', 'improve... | [-0.1867731657022467, 0.0571205916814506, -0.0888448755758313, 0.08305223907988805, -0.1071290238473851, -0.11803336560439605, 0.09502136478057274, 0.43541016509899727, -0.2816442800112642, -0.33308029343875556, 0.02478759390875124, -0.2749800320714712, -0.2225515220600825, 0.1609259410152355, -0.04606132404162334, 0.0... |
710.2948 | Spectral Properties of Quarks in the Quark-Gluon Plasma | We analyze the spectral properties of the quark propagator above the critical
temperature for the deconfinement phase transition in quenched lattice QCD
using clover improved Wilson fermions. The bare quark mass dependence of the
quark spectral function is analyzed by varying the hopping parameter \kappa in
Landau ga... | hep-lat hep-ph | we analyze the spectral properties of the quark propagator above the critical temperature for the deconfinement phase transition in quenched lattice qcd using clover improved wilson fermions the bare quark mass dependence of the quark spectral function is analyzed by varying the hopping parameter kappa in landau gauge ... | [['we', 'analyze', 'the', 'spectral', 'properties', 'of', 'the', 'quark', 'propagator', 'above', 'the', 'critical', 'temperature', 'for', 'the', 'deconfinement', 'phase', 'transition', 'in', 'quenched', 'lattice', 'qcd', 'using', 'clover', 'improved', 'wilson', 'fermions', 'the', 'bare', 'quark', 'mass', 'dependence', ... | [-0.09490862641885707, 0.3044059897899966, -0.12688234045424246, 0.11069879084402187, -0.0429738473655148, -0.098399644641375, 0.0853362750008025, 0.3818546219813553, -0.1637133289932866, -0.2284316792152822, 0.008284543709702451, -0.2671668712219054, -0.06711454931223257, 0.07751736739142374, 0.06558661446906626, 0.08... |
710.2949 | L-functions of Symmetric Products of the Kloosterman Sheaf over Z | The classical $n$-variable Kloosterman sums over the finite field ${\bf F}_p$
give rise to a lisse $\bar {\bf Q}_l$-sheaf ${\rm Kl}_{n+1}$ on ${\bf G}_{m,
{\bf F}_p}={\bf P}^1_{{\bf F}_p}-\{0,\infty\}$, which we call the Kloosterman
sheaf. Let $L_p({\bf G}_{m,{\bf F}_p}, {\rm Sym}^k{\rm Kl}_{n+1}, s)$ be the
$L$-func... | math.AG math.NT | the classical nvariable kloosterman sums over the finite field bf f_p give rise to a lisse bar bf q_lsheaf rm kl_n1 on bf g_m bf f_pbf p1_bf f_p0infty which we call the kloosterman sheaf let l_pbf g_mbf f_p rm symkrm kl_n1 s be the lfunction of the kfold symmetric product of rm kl_n1 we construct an explicit virtual sc... | [['the', 'classical', 'nvariable', 'kloosterman', 'sums', 'over', 'the', 'finite', 'field', 'bf', 'f_p', 'give', 'rise', 'to', 'a', 'lisse', 'bar', 'bf', 'q_lsheaf', 'rm', 'kl_n1', 'on', 'bf', 'g_m', 'bf', 'f_pbf', 'p1_bf', 'f_p0infty', 'which', 'we', 'call', 'the', 'kloosterman', 'sheaf', 'let', 'l_pbf', 'g_mbf', 'f_p... | [-0.2651654643047115, 0.05227813076714444, -0.0587178304862312, 0.017813114105197397, -0.03779071715214978, -0.06712247523841064, -0.00543046458725534, 0.31458450736396987, -0.306285012776599, -0.1339197590587782, 0.004098893731640166, -0.2237113319468968, -0.04974422626116354, 0.2556700283033854, -0.0633395578732471, ... |
710.295 | Initial ideals of tangent cones to Schubert varieties in orthogonal
Grassmannians | We compute the initial ideals, with respect to certain conveniently chosen
term orders, of ideals of tangent cones at torus fixed points to Schubert
varieties in orthogonal Grassmannians. The initial ideals turn out to be
square-free monomial ideals and therefore Stanley-Reisner face rings of
simplicial complexes. We... | math.CO math.AC math.AG | we compute the initial ideals with respect to certain conveniently chosen term orders of ideals of tangent cones at torus fixed points to schubert varieties in orthogonal grassmannians the initial ideals turn out to be squarefree monomial ideals and therefore stanleyreisner face rings of simplicial complexes we describ... | [['we', 'compute', 'the', 'initial', 'ideals', 'with', 'respect', 'to', 'certain', 'conveniently', 'chosen', 'term', 'orders', 'of', 'ideals', 'of', 'tangent', 'cones', 'at', 'torus', 'fixed', 'points', 'to', 'schubert', 'varieties', 'in', 'orthogonal', 'grassmannians', 'the', 'initial', 'ideals', 'turn', 'out', 'to', ... | [-0.2325414622143384, 0.036884304010383194, -0.02075297578370997, 0.07185888245317434, -0.06247883509208877, -0.15008045656103935, -0.0559755235851284, 0.3752245104738644, -0.45933783929499367, -0.104301007720457, 0.08271034202438646, -0.2580603980348401, -0.05443405525551902, 0.0881085785379308, -0.20285934730181618, ... |
710.2951 | String Cosmology: A Review | We give an overview of the status of string cosmology. We explain the
motivation for the subject, outline the main problems, and assess some of the
proposed solutions. Our focus is on those aspects of cosmology that benefit
from the structure of an ultraviolet-complete theory.
| hep-th astro-ph hep-ph | we give an overview of the status of string cosmology we explain the motivation for the subject outline the main problems and assess some of the proposed solutions our focus is on those aspects of cosmology that benefit from the structure of an ultravioletcomplete theory | [['we', 'give', 'an', 'overview', 'of', 'the', 'status', 'of', 'string', 'cosmology', 'we', 'explain', 'the', 'motivation', 'for', 'the', 'subject', 'outline', 'the', 'main', 'problems', 'and', 'assess', 'some', 'of', 'the', 'proposed', 'solutions', 'our', 'focus', 'is', 'on', 'those', 'aspects', 'of', 'cosmology', 'th... | [-0.08181858074126971, 0.009434614977928706, -0.1036421574652195, 0.11061961946025904, -0.07746216592689355, -0.0598102141585615, -0.03189269481485502, 0.27802961746023763, -0.24649695861670706, -0.2808645790028903, 0.14905998017638922, -0.26065910421311855, -0.18783893254068162, 0.22731585966216195, -0.112735963892191... |
710.2952 | The "mean king's problem" with continuous variables | We present the solution to the "mean king's problem" in the continuous
variable setting. We show that in this setting, the outcome of a
randomly-selected projective measurement of any linear combination of the
canonical variables x and p can be ascertained with arbitrary precision.
Moreover, we show that the solution... | quant-ph | we present the solution to the mean kings problem in the continuous variable setting we show that in this setting the outcome of a randomlyselected projective measurement of any linear combination of the canonical variables x and p can be ascertained with arbitrary precision moreover we show that the solution is in tur... | [['we', 'present', 'the', 'solution', 'to', 'the', 'mean', 'kings', 'problem', 'in', 'the', 'continuous', 'variable', 'setting', 'we', 'show', 'that', 'in', 'this', 'setting', 'the', 'outcome', 'of', 'a', 'randomlyselected', 'projective', 'measurement', 'of', 'any', 'linear', 'combination', 'of', 'the', 'canonical', 'v... | [-0.14100266227045644, 0.042027277311559454, -0.08866622703878776, 0.00868493421433453, -0.06622136089667353, -0.11228295361481445, 0.08838830575215346, 0.34486968693849834, -0.3357161666145143, -0.270049957740728, 0.1014495364892671, -0.2495316006470998, -0.11305651969134646, 0.15979338947521604, -0.10376931599887979,... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.