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 |
|---|---|---|---|---|---|---|
706.3614 | Nuclear vector polarizability correction to hyperfine splitting | The interaction of orbital electrons with the charge and magnetic moment of
the nucleus polarizes it, and the detailed description requires a careful
treatment of the nuclear vector polarizability. We present a complete and
closed form expression for the resulting contribution to hyperfine splitting in
light atomic s... | physics.atom-ph nucl-th | the interaction of orbital electrons with the charge and magnetic moment of the nucleus polarizes it and the detailed description requires a careful treatment of the nuclear vector polarizability we present a complete and closed form expression for the resulting contribution to hyperfine splitting in light atomic syste... | [['the', 'interaction', 'of', 'orbital', 'electrons', 'with', 'the', 'charge', 'and', 'magnetic', 'moment', 'of', 'the', 'nucleus', 'polarizes', 'it', 'and', 'the', 'detailed', 'description', 'requires', 'a', 'careful', 'treatment', 'of', 'the', 'nuclear', 'vector', 'polarizability', 'we', 'present', 'a', 'complete', '... | [-0.1500864993625631, 0.13125290537330633, -0.03628051451717814, 0.059795872861286625, -0.03859423481238385, -0.042779415127976485, 0.07754300179779723, 0.36673499550670385, -0.19469177285403325, -0.302063786269476, -0.048855729364731815, -0.2715085018814231, -0.05155583320690008, 0.1369327256688848, 0.0886912665252263... |
706.3615 | CO adsorption on metal surfaces: a hybrid functional study with plane
wave basis set | We present a detailed study of the adsorption of CO on Cu, Rh, and Pt (111)
surfaces in top and hollow sites. The study has been performed using the local
density approximation, the gradient corrected functional PBE, and the hybrid
Hartree-Fock density functionals PBE0 and HSE03 within the framework of
generalized Ko... | cond-mat.mtrl-sci | we present a detailed study of the adsorption of co on cu rh and pt 111 surfaces in top and hollow sites the study has been performed using the local density approximation the gradient corrected functional pbe and the hybrid hartreefock density functionals pbe0 and hse03 within the framework of generalized kohnsham den... | [['we', 'present', 'a', 'detailed', 'study', 'of', 'the', 'adsorption', 'of', 'co', 'on', 'cu', 'rh', 'and', 'pt', '111', 'surfaces', 'in', 'top', 'and', 'hollow', 'sites', 'the', 'study', 'has', 'been', 'performed', 'using', 'the', 'local', 'density', 'approximation', 'the', 'gradient', 'corrected', 'functional', 'pbe... | [-0.058650765555922864, 0.056935556010020344, -0.0708483030608335, 0.11627883319296971, 0.06814840668566713, -0.11941262294368987, 0.10972994649117547, 0.39428064032373106, -0.21656318060077073, -0.31113459519412995, -0.015220578311634092, -0.34676633728668094, -0.09134976311840794, 0.0807538358902849, 0.07052791379422... |
706.3616 | Generation of potential/surface density pairs in flat disks Power law
distributions | We report a simple method to generate potential/surface density pairs in flat
axially symmetric finite size disks. Potential/surface density pairs consist of
a ``homogeneous'' pair (a closed form expression) corresponding to a uniform
disk, and a ``residual'' pair. This residual component is converted into an
infinit... | astro-ph | we report a simple method to generate potentialsurface density pairs in flat axially symmetric finite size disks potentialsurface density pairs consist of a homogeneous pair a closed form expression corresponding to a uniform disk and a residual pair this residual component is converted into an infinite series of integ... | [['we', 'report', 'a', 'simple', 'method', 'to', 'generate', 'potentialsurface', 'density', 'pairs', 'in', 'flat', 'axially', 'symmetric', 'finite', 'size', 'disks', 'potentialsurface', 'density', 'pairs', 'consist', 'of', 'a', 'homogeneous', 'pair', 'a', 'closed', 'form', 'expression', 'corresponding', 'to', 'a', 'uni... | [-0.1207132330157661, 0.08292017826419656, -0.0890596158403371, 0.054467805814929306, -0.05143102426347988, -0.07411313271549132, 0.00437827393346067, 0.3560706749345575, -0.26826402817254086, -0.2657459919310973, 0.09807986070535013, -0.2570169940910169, -0.06912739485103105, 0.20184485801695182, -0.022580721388970104... |
706.3617 | On microscopic theory of spin-S Bose-Einstein condensate in a magnetic
field | The Bogoliubov model for weakly interacting Bose gas is extended to
Bose-Einstein condensation (BEC) of spin-S atoms in a magnetic field. Equation
for the vectorial order parameter valid at temperature $T\to 0$ is derived and
its particular solution is found. This solution corresponds to the formation of
BEC of atoms... | cond-mat.stat-mech | the bogoliubov model for weakly interacting bose gas is extended to boseeinstein condensation bec of spins atoms in a magnetic field equation for the vectorial order parameter valid at temperature tto 0 is derived and its particular solution is found this solution corresponds to the formation of bec of atoms with a def... | [['the', 'bogoliubov', 'model', 'for', 'weakly', 'interacting', 'bose', 'gas', 'is', 'extended', 'to', 'boseeinstein', 'condensation', 'bec', 'of', 'spins', 'atoms', 'in', 'a', 'magnetic', 'field', 'equation', 'for', 'the', 'vectorial', 'order', 'parameter', 'valid', 'at', 'temperature', 'tto', '0', 'is', 'derived', 'a... | [-0.16734889524060492, 0.19382568321023613, -0.04865166385514805, 0.03269020840824128, -0.010211928198352838, -0.14409643799687424, 0.02259852421971468, 0.3173981292459827, -0.21520550090533036, -0.19788208587142903, 0.011251605896410556, -0.29170283909218436, -0.025448586355942566, 0.12310807514661111, 0.1112028863878... |
706.3618 | Low Regularity local well-posedness for the 1+3 dimensional
Dirac-Klein-Gordon system | We prove that the Cauchy problem for the Dirac-Klein-Gordon system of
equations in 1+3 dimensions is locally well-posed in a range of Sobolev spaces
for the Dirac spinor and the meson field. The result contains and extends the
earlier known results for the same problem. Our proof relies on the null
structure in the s... | math.AP | we prove that the cauchy problem for the dirackleingordon system of equations in 13 dimensions is locally wellposed in a range of sobolev spaces for the dirac spinor and the meson field the result contains and extends the earlier known results for the same problem our proof relies on the null structure in the system an... | [['we', 'prove', 'that', 'the', 'cauchy', 'problem', 'for', 'the', 'dirackleingordon', 'system', 'of', 'equations', 'in', '13', 'dimensions', 'is', 'locally', 'wellposed', 'in', 'a', 'range', 'of', 'sobolev', 'spaces', 'for', 'the', 'dirac', 'spinor', 'and', 'the', 'meson', 'field', 'the', 'result', 'contains', 'and', ... | [-0.15150297249877645, 0.06680744124347374, -0.05760400979629447, 0.08802209667778844, -0.06443004847894754, -0.07644956996814618, -0.025903198267182997, 0.2546968120000055, -0.23608106461864325, -0.22250499806156562, 0.1239044304144749, -0.2680197856689413, -0.11740073826043837, 0.22652458196746245, -0.056351539393466... |
706.3619 | Almost Everywhere Convergence of Inverse Dunkl Transform on the Real
Line | In this paper, we will first show that the maximal operator $S_*^\alpha$ of
spherical partial sums $S_R^\alpha$, associated to Dunkl transform on
$\mathbb{R}$ is bounded on $L^p(\mathbb{R}, |x|^{2\alpha+1} dx)$ functions when
$\frac{4(\alpha+1)}{2\alpha+3}<p<\frac{4(\alpha+1)}{2\alpha+1}$, and it implies
that, for ev... | math.CA | in this paper we will first show that the maximal operator s_alpha of spherical partial sums s_ralpha associated to dunkl transform on mathbbr is bounded on lpmathbbr x2alpha1 dx functions when frac4alpha12alpha3pfrac4alpha12alpha1 and it implies that for every lpmathbbr x2alpha1 dx function fx s_ralpha fx converges to... | [['in', 'this', 'paper', 'we', 'will', 'first', 'show', 'that', 'the', 'maximal', 'operator', 's_alpha', 'of', 'spherical', 'partial', 'sums', 's_ralpha', 'associated', 'to', 'dunkl', 'transform', 'on', 'mathbbr', 'is', 'bounded', 'on', 'lpmathbbr', 'x2alpha1', 'dx', 'functions', 'when', 'frac4alpha12alpha3pfrac4alpha1... | [-0.10211128846276551, 0.09052826008583242, -0.06521523667096689, 0.054886263954088195, -0.04486923966229566, -0.13707966397113697, -0.029181127309031482, 0.3775943073167189, -0.3676655501555148, -0.05121977229577464, 0.14313748076627333, -0.36048669623513074, -0.15640507687537655, 0.22844251539759539, -0.0911848048901... |
706.362 | Hypergroups with Unique Alpha-Means | Let $K$ be a commutative hypergroup and $\alpha\in \hat{K}$. We show that $K$
is $\alpha$-amenable with the unique $\alpha$-mean $m_\alpha$ if and only if
$m_\alpha\in L^1(K)\cap L^2(K)$ and $\alpha$ is isolated in $\hat{K}$. In
contrast to the case of amenable noncompact locally compact groups, examples of
polynomia... | math.GR | let k be a commutative hypergroup and alphain hatk we show that k is alphaamenable with the unique alphamean m_alpha if and only if m_alphain l1kcap l2k and alpha is isolated in hatk in contrast to the case of amenable noncompact locally compact groups examples of polynomial hypergroups with unique alphameans alphanot1... | [['let', 'k', 'be', 'a', 'commutative', 'hypergroup', 'and', 'alphain', 'hatk', 'we', 'show', 'that', 'k', 'is', 'alphaamenable', 'with', 'the', 'unique', 'alphamean', 'm_alpha', 'if', 'and', 'only', 'if', 'm_alphain', 'l1kcap', 'l2k', 'and', 'alpha', 'is', 'isolated', 'in', 'hatk', 'in', 'contrast', 'to', 'the', 'case... | [-0.14364771407319984, 0.13362762985691087, -0.1046040312790159, 0.009417701001737767, -0.10938220294609444, -0.17483898736675507, -0.0001264338854199915, 0.4115016388136949, -0.3015127085955508, -0.14132046159495837, 0.12943055756119037, -0.3181475278740721, -0.14787278458503866, 0.23064570397194198, -0.13110414522686... |
706.3621 | Climate Change: The Sun's Role | The sun's role in the earth's recent warming remains controversial even
though there is a good deal of evidence to support the thesis that solar
variations are a very significant factor in driving climate change both
currently and in the past. This precis lays out the background and data needed
to understand the basi... | physics.gen-ph | the suns role in the earths recent warming remains controversial even though there is a good deal of evidence to support the thesis that solar variations are a very significant factor in driving climate change both currently and in the past this precis lays out the background and data needed to understand the basic sci... | [['the', 'suns', 'role', 'in', 'the', 'earths', 'recent', 'warming', 'remains', 'controversial', 'even', 'though', 'there', 'is', 'a', 'good', 'deal', 'of', 'evidence', 'to', 'support', 'the', 'thesis', 'that', 'solar', 'variations', 'are', 'a', 'very', 'significant', 'factor', 'in', 'driving', 'climate', 'change', 'bo... | [-0.09890876475559629, 0.11822918406687677, -0.0702209768148706, 0.12887334082093413, -0.07758299662205188, -0.052507039974443614, 0.07567115754911515, 0.3578738227243657, -0.20596565042986817, -0.3321915374684107, 0.11770260772217349, -0.24161743681432438, -0.18372337434582575, 0.21540204107346336, -0.1362592780395694... |
706.3622 | Comments on the Unified approach to the construction of Classical
confidence intervals | The paper comments on properties of the so-called "Unified approach to the
construction of classical confidence intervals", in which confidence intervals
are computed in a Neyman construction using the likelihood ratio as ordering
quantity. In particular, two of the main results of a paper by Feldman and
Cousins (F&C... | physics.data-an astro-ph | the paper comments on properties of the socalled unified approach to the construction of classical confidence intervals in which confidence intervals are computed in a neyman construction using the likelihood ratio as ordering quantity in particular two of the main results of a paper by feldman and cousins fc are discu... | [['the', 'paper', 'comments', 'on', 'properties', 'of', 'the', 'socalled', 'unified', 'approach', 'to', 'the', 'construction', 'of', 'classical', 'confidence', 'intervals', 'in', 'which', 'confidence', 'intervals', 'are', 'computed', 'in', 'a', 'neyman', 'construction', 'using', 'the', 'likelihood', 'ratio', 'as', 'ord... | [-0.11686118030097307, 0.10140144740397991, -0.09508507003646499, 0.09892952200441406, -0.0627064953466077, -0.11926247561775404, 0.1614300381784423, 0.32212262997269175, -0.21856092911270295, -0.30972740212774097, 0.15641792166841786, -0.2520393197090071, -0.09752548972548414, 0.18718729650658403, -0.07793955461869279... |
706.3623 | On a class of $\mathrm{II}_1$ factors with at most one Cartan subalgebra | We prove that the normalizer of any diffuse amenable subalgebra of a free
group factor $L(\Bbb F_r)$ generates an amenable von Neumann subalgebra.
Moreover, any II$_1$ factor of the form $Q \vt L(\Bbb F_r) $, with $Q$ an
arbitrary subfactor of a tensor product of free group factors, has no Cartan
subalgebras. We also... | math.OA math.GR | we prove that the normalizer of any diffuse amenable subalgebra of a free group factor lbbb f_r generates an amenable von neumann subalgebra moreover any ii_1 factor of the form q vt lbbb f_r with q an arbitrary subfactor of a tensor product of free group factors has no cartan subalgebras we also prove that if a free e... | [['we', 'prove', 'that', 'the', 'normalizer', 'of', 'any', 'diffuse', 'amenable', 'subalgebra', 'of', 'a', 'free', 'group', 'factor', 'lbbb', 'f_r', 'generates', 'an', 'amenable', 'von', 'neumann', 'subalgebra', 'moreover', 'any', 'ii_1', 'factor', 'of', 'the', 'form', 'q', 'vt', 'lbbb', 'f_r', 'with', 'q', 'an', 'arbi... | [-0.19439791405671522, 0.163072704526559, -0.06300791639246439, -0.016055535367003788, -0.10863700657439614, -0.16206779678989397, -0.033342528073607304, 0.3918610325940934, -0.3411026822501107, -0.08308936094767169, 0.07198596653026088, -0.28911038460700134, -0.028881501891699277, 0.19040484651678094, -0.1335138203355... |
706.3624 | Absorption line-strengths of 18 late-type spiral galaxies observed with
SAURON | We present absorption line-strength maps for a sample of 18 Sb-Sd galaxies
observed using the integral-field spectrograph SAURON. The SAURON spectral
range allows the measurement of the Lick/IDS indices Hbeta, Fe5015 and Mgb,
which can be used to estimate the stellar population parameters. We present
here the two-dim... | astro-ph | we present absorption linestrength maps for a sample of 18 sbsd galaxies observed using the integralfield spectrograph sauron the sauron spectral range allows the measurement of the lickids indices hbeta fe5015 and mgb which can be used to estimate the stellar population parameters we present here the twodimensional li... | [['we', 'present', 'absorption', 'linestrength', 'maps', 'for', 'a', 'sample', 'of', '18', 'sbsd', 'galaxies', 'observed', 'using', 'the', 'integralfield', 'spectrograph', 'sauron', 'the', 'sauron', 'spectral', 'range', 'allows', 'the', 'measurement', 'of', 'the', 'lickids', 'indices', 'hbeta', 'fe5015', 'and', 'mgb', ... | [-0.006059011019101571, 0.07704965187900605, -0.09517963890269293, 0.13759411019297785, -0.07637934616928124, -0.09885509580031511, 0.02799400574833734, 0.48334227069264585, -0.12992029490067405, -0.345689401869718, 0.02896516474849107, -0.28901968768131614, -0.06903684958907617, 0.19298724587940916, -0.032395065855173... |
706.3625 | Two-dimensional cavity grid for scalable quantum computation with
superconducting circuits | Superconducting circuits are among the leading contenders for quantum
information processing. This promising avenue has been strengthened with the
advent of circuit quantum electrodynamics, underlined by recent experiments
coupling on-chip microwave resonators to superconducting qubits. However,
moving towards more q... | cond-mat.mes-hall quant-ph | superconducting circuits are among the leading contenders for quantum information processing this promising avenue has been strengthened with the advent of circuit quantum electrodynamics underlined by recent experiments coupling onchip microwave resonators to superconducting qubits however moving towards more qubits w... | [['superconducting', 'circuits', 'are', 'among', 'the', 'leading', 'contenders', 'for', 'quantum', 'information', 'processing', 'this', 'promising', 'avenue', 'has', 'been', 'strengthened', 'with', 'the', 'advent', 'of', 'circuit', 'quantum', 'electrodynamics', 'underlined', 'by', 'recent', 'experiments', 'coupling', '... | [-0.18414384233447045, 0.17519627231863752, 0.005375928620693924, -0.05408894379996768, -0.03672273249680297, -0.28899704288396477, 0.06747240197016496, 0.43496697757178715, -0.21913864288693494, -0.2920483992294335, 0.01552142635642772, -0.28891515957114955, -0.10617374347124195, 0.2541365651773932, -0.037144176440404... |
706.3626 | A Problem in Last-Passage Percolation | Let $\{X(v), v \in \Bbb Z^d \times \Bbb Z_+\}$ be an i.i.d. family of random
variables such that $P\{X(v)= e^b\}=1-P\{X(v)= 1\} = p$ for some $b>0$. We
consider paths $\pi \subset \Bbb Z^d \times \Bbb Z_+$ starting at the origin
and with the last coordinate increasing along the path, and of length $n$.
Define for suc... | math.PR math-ph math.MP | let xv v in bbb zd times bbb z_ be an iid family of random variables such that pxv eb1pxv 1 p for some b0 we consider paths pi subset bbb zd times bbb z_ starting at the origin and with the last coordinate increasing along the path and of length n define for such paths wpi textnumber of vertices pi_i 1 le i le n withxp... | [['let', 'xv', 'v', 'in', 'bbb', 'zd', 'times', 'bbb', 'z_', 'be', 'an', 'iid', 'family', 'of', 'random', 'variables', 'such', 'that', 'pxv', 'eb1pxv', '1', 'p', 'for', 'some', 'b0', 'we', 'consider', 'paths', 'pi', 'subset', 'bbb', 'zd', 'times', 'bbb', 'z_', 'starting', 'at', 'the', 'origin', 'and', 'with', 'the', 'l... | [-0.19800010517800368, 0.24019751508150033, 0.008690652407465442, -0.059573432701008934, 0.04900016307189901, -0.19089012637093503, 0.02445770613849163, 0.3581215184462327, -0.30850504044323196, -0.13554825727897946, 0.0023398432838079588, -0.40650855235114536, -0.044411535571349324, 0.09939840559657383, -0.01461210213... |
706.3627 | Familles fuchsiennes d'\'equations aux (q-)diff\'erences et confluence | In a first part, we give a method for solving a family of fuchsian systems of
operators of pseudo-derivations associated to a family of homographies with two
parameters which unify and generalize the differential, the difference and the
$q$-difference cases. In a second part, we study the problems of confluence
relat... | math.CA | in a first part we give a method for solving a family of fuchsian systems of operators of pseudoderivations associated to a family of homographies with two parameters which unify and generalize the differential the difference and the qdifference cases in a second part we study the problems of confluence related to thes... | [['in', 'a', 'first', 'part', 'we', 'give', 'a', 'method', 'for', 'solving', 'a', 'family', 'of', 'fuchsian', 'systems', 'of', 'operators', 'of', 'pseudoderivations', 'associated', 'to', 'a', 'family', 'of', 'homographies', 'with', 'two', 'parameters', 'which', 'unify', 'and', 'generalize', 'the', 'differential', 'the'... | [-0.15303724988674125, 0.0039899290272000214, -0.06871859211565202, 0.04812303357930095, -0.08268612502918889, -0.07380824088532892, -0.008747622284486337, 0.26310203331350174, -0.3170720910118824, -0.2781997871826644, 0.1303229182915486, -0.298690147490965, -0.18409666443174635, 0.2525057341489527, -0.0828729183585555... |
706.3628 | B->eta(') Form Factors in QCD | We calculate the semileptonic form factors $f_+^{B\to \eta}(q^2)$ and
$f_+^{B\to \eta'}(q^2)$ from QCD sum rules on the light-cone (LCSRs), to NLO in
QCD, and for small to moderate q^2, $0\leq q^2\leq 16 {\rm
GeV}^2$. We include in particular the so-called singlet contribution, i.e.\
weak annihilation of the B meso... | hep-ph | we calculate the semileptonic form factors f_bto etaq2 and f_bto etaq2 from qcd sum rules on the lightcone lcsrs to nlo in qcd and for small to moderate q2 0leq q2leq 16 rm gev2 we include in particular the socalled singlet contribution ie weak annihilation of the b meson with the emission of two gluons which thanks to... | [['we', 'calculate', 'the', 'semileptonic', 'form', 'factors', 'f_bto', 'etaq2', 'and', 'f_bto', 'etaq2', 'from', 'qcd', 'sum', 'rules', 'on', 'the', 'lightcone', 'lcsrs', 'to', 'nlo', 'in', 'qcd', 'and', 'for', 'small', 'to', 'moderate', 'q2', '0leq', 'q2leq', '16', 'rm', 'gev2', 'we', 'include', 'in', 'particular', '... | [-0.06654852523420499, 0.2019891432034509, -0.06179555828695062, 0.09959121367565411, -0.0674876315461006, -0.06895787316470352, 0.07460108880460371, 0.33231495279709206, -0.19742486636524142, -0.24650869865710026, -0.029987696290310638, -0.33945076822248454, -0.01903237951131921, 0.10640368726864621, 0.042171281496206... |
706.3629 | Critical fluctuations of time-dependent magnetization in a random-field
Ising model | Cooperative behaviors near the disorder-induced critical point in a random
field Ising model are numerically investigated by analyzing time-dependent
magnetization in ordering processes from a special initial condition. We find
that the intensity of fluctuations of time-dependent magnetization, $\chi(t)$,
attains a m... | cond-mat.stat-mech cond-mat.dis-nn | cooperative behaviors near the disorderinduced critical point in a random field ising model are numerically investigated by analyzing timedependent magnetization in ordering processes from a special initial condition we find that the intensity of fluctuations of timedependent magnetization chit attains a maximum value ... | [['cooperative', 'behaviors', 'near', 'the', 'disorderinduced', 'critical', 'point', 'in', 'a', 'random', 'field', 'ising', 'model', 'are', 'numerically', 'investigated', 'by', 'analyzing', 'timedependent', 'magnetization', 'in', 'ordering', 'processes', 'from', 'a', 'special', 'initial', 'condition', 'we', 'find', 'th... | [-0.18150757119990885, 0.22644075956195592, -0.1203778590192087, 0.09586958352010697, 0.027863557536620648, -0.172653377011884, 0.11932787776691839, 0.3484237880783621, -0.25211715781129895, -0.22798797465860843, 0.07383299854700454, -0.32366173930699005, -0.16936765673395712, 0.18198719735024496, 0.06591241337358951, ... |
706.363 | Orbit-counting for nilpotent group shifts | We study the asymptotic behaviour of the orbit-counting function and a
dynamical Mertens' theorem for the full $G$-shift for a finitely-generated
torsion-free nilpotent group $G$. Using bounds for the M{\"o}bius function on
the lattice of subgroups of finite index and known subgroup growth estimates,
we find a single... | math.DS math.GR | we study the asymptotic behaviour of the orbitcounting function and a dynamical mertens theorem for the full gshift for a finitelygenerated torsionfree nilpotent group g using bounds for the mobius function on the lattice of subgroups of finite index and known subgroup growth estimates we find a single asymptotic of th... | [['we', 'study', 'the', 'asymptotic', 'behaviour', 'of', 'the', 'orbitcounting', 'function', 'and', 'a', 'dynamical', 'mertens', 'theorem', 'for', 'the', 'full', 'gshift', 'for', 'a', 'finitelygenerated', 'torsionfree', 'nilpotent', 'group', 'g', 'using', 'bounds', 'for', 'the', 'mobius', 'function', 'on', 'the', 'latt... | [-0.16529459888503575, 0.11985568508195381, -0.14231117069236157, 0.09438719419267727, -0.07665256059165888, -0.08915291337689268, 0.09040725999511778, 0.3409818559885025, -0.25471579836448655, -0.2408044520270778, 0.10793132556985559, -0.2578907103500872, -0.11809616514619847, 0.22737851653558513, -0.05594167768140323... |
706.3631 | Gas stripping in galaxy clusters: a new SPH simulation approach | The influence of a time-varying ram pressure on spiral galaxies in clusters
is explored with a new simulation method based on the N-body SPH/tree code
GADGET. We have adapted the code to describe the interaction of two different
gas phases, the diffuse hot intracluster medium (ICM) and the denser and colder
interstel... | astro-ph | the influence of a timevarying ram pressure on spiral galaxies in clusters is explored with a new simulation method based on the nbody sphtree code gadget we have adapted the code to describe the interaction of two different gas phases the diffuse hot intracluster medium icm and the denser and colder interstellar mediu... | [['the', 'influence', 'of', 'a', 'timevarying', 'ram', 'pressure', 'on', 'spiral', 'galaxies', 'in', 'clusters', 'is', 'explored', 'with', 'a', 'new', 'simulation', 'method', 'based', 'on', 'the', 'nbody', 'sphtree', 'code', 'gadget', 'we', 'have', 'adapted', 'the', 'code', 'to', 'describe', 'the', 'interaction', 'of',... | [-0.08895518699518486, 0.13358534866400307, -0.10883711213788506, 0.0907799561549819, -0.10579460793179324, -0.007879328441543921, 0.02397490884358226, 0.4149410655288008, -0.21392043402364241, -0.31481488507910116, 0.025025141412432946, -0.26544445741795075, -0.024528753622751504, 0.17772076231454617, 0.02214303811180... |
706.3632 | Revised instability domains of SPB and beta Cephei stars | The excitation of pulsation modes in beta Cephei and Slowly Pulsating B stars
is known to be very sensitive to opacity changes in the stellar interior where
T~2 10^5 K. In this region differences in opacity up to ~50% can be induced by
the choice between OPAL and OP opacity tables, and between two different metal
mix... | astro-ph | the excitation of pulsation modes in beta cephei and slowly pulsating b stars is known to be very sensitive to opacity changes in the stellar interior where t2 105 k in this region differences in opacity up to 50 can be induced by the choice between opal and op opacity tables and between two different metal mixtures gr... | [['the', 'excitation', 'of', 'pulsation', 'modes', 'in', 'beta', 'cephei', 'and', 'slowly', 'pulsating', 'b', 'stars', 'is', 'known', 'to', 'be', 'very', 'sensitive', 'to', 'opacity', 'changes', 'in', 'the', 'stellar', 'interior', 'where', 't2', '105', 'k', 'in', 'this', 'region', 'differences', 'in', 'opacity', 'up', ... | [-0.04220467092123179, 0.21491552136047223, -0.026203511464121067, 0.04749407569787144, -0.06182312155636934, -0.08293638178106166, 0.11947485069183847, 0.4022417487164514, -0.19011857077083757, -0.3917568815641303, 0.03558709978669948, -0.2609631781161359, -0.07493288369295063, 0.1858642062716252, -0.06812868947833192... |
706.3633 | Phase Diffusion in Quantum Dissipative Systems | We study the dynamics of the quantum phase distribution associated with the
reduced density matrix of a system for a number of situations of practical
importance, as the system evolves under the influence of its environment,
interacting via a quantum nondemoliton type of coupling, such that there is
decoherence witho... | quant-ph cond-mat.stat-mech | we study the dynamics of the quantum phase distribution associated with the reduced density matrix of a system for a number of situations of practical importance as the system evolves under the influence of its environment interacting via a quantum nondemoliton type of coupling such that there is decoherence without di... | [['we', 'study', 'the', 'dynamics', 'of', 'the', 'quantum', 'phase', 'distribution', 'associated', 'with', 'the', 'reduced', 'density', 'matrix', 'of', 'a', 'system', 'for', 'a', 'number', 'of', 'situations', 'of', 'practical', 'importance', 'as', 'the', 'system', 'evolves', 'under', 'the', 'influence', 'of', 'its', 'e... | [-0.1564803369947486, 0.1914503173936906, -0.10540985213717723, 0.02749462212601384, 0.013760418631136417, -0.123126116623594, 0.061665737962981394, 0.33310709286227147, -0.2737841104111088, -0.26339812597071305, 0.07674865450128944, -0.2809161917568177, -0.12809434316259585, 0.19534752643975037, 0.00869146552252437, 0... |
706.3634 | Cohomology of Congruence Subgroups of SL(4,\Z) II | In a previous paper [3] we computed cohomology groups H^5 (Gamma_0 (N), \C),
where Gamma_0 (N) is a certain congruence subgroup of SL (4, \Z), for a range
of levels N. In this note we update this earlier work by extending the range of
levels and describe cuspidal cohomology classes and additional boundary
phenomena f... | math.NT | in a previous paper 3 we computed cohomology groups h5 gamma_0 n c where gamma_0 n is a certain congruence subgroup of sl 4 z for a range of levels n in this note we update this earlier work by extending the range of levels and describe cuspidal cohomology classes and additional boundary phenomena found since the publi... | [['in', 'a', 'previous', 'paper', '3', 'we', 'computed', 'cohomology', 'groups', 'h5', 'gamma_0', 'n', 'c', 'where', 'gamma_0', 'n', 'is', 'a', 'certain', 'congruence', 'subgroup', 'of', 'sl', '4', 'z', 'for', 'a', 'range', 'of', 'levels', 'n', 'in', 'this', 'note', 'we', 'update', 'this', 'earlier', 'work', 'by', 'ext... | [-0.21624651420861482, 0.10568076423369348, -0.048245072865393014, 0.028980822450830602, -0.036079840635647994, -0.11438427479588427, 0.02622814103087876, 0.30238299516495315, -0.2855302714800928, -0.3226777605013922, 0.05522447649855167, -0.21508151427842676, -0.1238302848272724, 0.16435119951202068, -0.10648060113890... |
706.3635 | Comparison of relative cohomology theories with respect to semidualizing
modules | We compare and contrast various relative cohomology theories that arise from
resolutions involving semidualizing modules. We prove a general balance result
for relative cohomology over a Cohen-Macaulay ring with a dualizing module, and
we demonstrate the failure of the naive version of balance one might expect for
th... | math.AC | we compare and contrast various relative cohomology theories that arise from resolutions involving semidualizing modules we prove a general balance result for relative cohomology over a cohenmacaulay ring with a dualizing module and we demonstrate the failure of the naive version of balance one might expect for these f... | [['we', 'compare', 'and', 'contrast', 'various', 'relative', 'cohomology', 'theories', 'that', 'arise', 'from', 'resolutions', 'involving', 'semidualizing', 'modules', 'we', 'prove', 'a', 'general', 'balance', 'result', 'for', 'relative', 'cohomology', 'over', 'a', 'cohenmacaulay', 'ring', 'with', 'a', 'dualizing', 'mo... | [-0.18418561004494366, -0.00022800994154654051, -0.09677524930846534, 0.10939010878730761, -0.03233808368248375, -0.1454944794752488, -0.03809078442619035, 0.3734069795200699, -0.4005016920205794, -0.23358343498487222, 0.05663860048240933, -0.2014679030478491, -0.17460100674315504, 0.1920675665532288, -0.21199026068819... |
706.3636 | alpha'-Corrections to Heterotic Superstring Effective Action Revisited | In this letter we establish that the supersymmetric R^2 effective action for
the heterotic string, obtained from the supersymmetrisation of the Lorentz
Chern-Simons term, is to order $\alpha'$ equivalent modulo field redefinitions
to heterotic string effective actions computed by different methods.
| hep-th | in this letter we establish that the supersymmetric r2 effective action for the heterotic string obtained from the supersymmetrisation of the lorentz chernsimons term is to order alpha equivalent modulo field redefinitions to heterotic string effective actions computed by different methods | [['in', 'this', 'letter', 'we', 'establish', 'that', 'the', 'supersymmetric', 'r2', 'effective', 'action', 'for', 'the', 'heterotic', 'string', 'obtained', 'from', 'the', 'supersymmetrisation', 'of', 'the', 'lorentz', 'chernsimons', 'term', 'is', 'to', 'order', 'alpha', 'equivalent', 'modulo', 'field', 'redefinitions',... | [-0.143327813550103, 0.15874540028957332, -0.025356927046143427, 0.14783944539362337, -0.09942289489525848, -0.18318780313995553, 0.0026551500735122985, 0.2997633377771552, -0.19465578953939966, -0.27975640447083405, 0.028454972706485268, -0.23460396742675363, -0.17098135082619037, 0.09982718196811109, -0.1077231787054... |
706.3637 | Translation-invariance of two-dimensional Gibbsian point processes | The conservation of translation as a symmetry in two-dimensional systems with
interaction is a classical subject of statistical mechanics. Here we establish
such a result for Gibbsian particle systems with two-body interaction, where
the interesting cases of singular, hard-core and discontinuous interaction are
inclu... | math.PR math-ph math.MP | the conservation of translation as a symmetry in twodimensional systems with interaction is a classical subject of statistical mechanics here we establish such a result for gibbsian particle systems with twobody interaction where the interesting cases of singular hardcore and discontinuous interaction are included we s... | [['the', 'conservation', 'of', 'translation', 'as', 'a', 'symmetry', 'in', 'twodimensional', 'systems', 'with', 'interaction', 'is', 'a', 'classical', 'subject', 'of', 'statistical', 'mechanics', 'here', 'we', 'establish', 'such', 'a', 'result', 'for', 'gibbsian', 'particle', 'systems', 'with', 'twobody', 'interaction'... | [-0.11587287760763006, 0.15108590175143696, -0.048078069145875896, 0.09474327562863684, -0.0317772610860905, -0.18539791066679312, 0.009224096567116001, 0.3346930614700823, -0.272945924415112, -0.2723359194104419, 0.052623064112567314, -0.28590071720960125, -0.1342708716084334, 0.09675922208980685, -0.00977525085380131... |
706.3638 | Singularity categories, Schur Functors and Triangular Matrix Rings | We study certain Schur functors which preserve singularity categories of
rings and we apply them to study the singularity category of triangular matrix
rings. In particular, combining these results with Buchweitz-Happel's theorem,
we can describe singularity categories of certain non-Gorenstein rings via the
stable c... | math.RT math.RA | we study certain schur functors which preserve singularity categories of rings and we apply them to study the singularity category of triangular matrix rings in particular combining these results with buchweitzhappels theorem we can describe singularity categories of certain nongorenstein rings via the stable category ... | [['we', 'study', 'certain', 'schur', 'functors', 'which', 'preserve', 'singularity', 'categories', 'of', 'rings', 'and', 'we', 'apply', 'them', 'to', 'study', 'the', 'singularity', 'category', 'of', 'triangular', 'matrix', 'rings', 'in', 'particular', 'combining', 'these', 'results', 'with', 'buchweitzhappels', 'theore... | [-0.18192842976785586, -0.056071653756022945, -0.07296402349335249, 0.1247106714662714, -0.07241362699719726, -0.20927455751072677, -0.1201567378841707, 0.3852118419819191, -0.41743226636384356, -0.11737043400615697, 0.15353950941897013, -0.22032258885561443, -0.13716106654190627, 0.13975785831447507, -0.18818901561689... |
706.3639 | A Collection of Definitions of Intelligence | This paper is a survey of a large number of informal definitions of
``intelligence'' that the authors have collected over the years. Naturally,
compiling a complete list would be impossible as many definitions of
intelligence are buried deep inside articles and books. Nevertheless, the
70-odd definitions presented he... | cs.AI | this paper is a survey of a large number of informal definitions of intelligence that the authors have collected over the years naturally compiling a complete list would be impossible as many definitions of intelligence are buried deep inside articles and books nevertheless the 70odd definitions presented here are to t... | [['this', 'paper', 'is', 'a', 'survey', 'of', 'a', 'large', 'number', 'of', 'informal', 'definitions', 'of', 'intelligence', 'that', 'the', 'authors', 'have', 'collected', 'over', 'the', 'years', 'naturally', 'compiling', 'a', 'complete', 'list', 'would', 'be', 'impossible', 'as', 'many', 'definitions', 'of', 'intellig... | [-0.10334973647946218, 0.09062120016114633, -0.06007770688624167, 0.07192161507698418, -0.164996563075263, -0.053850450759112344, 0.029457478755397996, 0.3657406498181832, -0.23205953191337939, -0.3827505995382051, 0.12778641074346225, -0.36279631955701797, -0.14487743089128224, 0.23214134100641384, -0.1345056231347386... |
706.364 | Can Protostellar Jets Drive Supersonic Turbulence in Molecular Clouds? | Jets and outflows from young stellar objects are proposed candidates to drive
supersonic turbulence in molecular clouds. Here, we present the results from
multi-dimensional jet simulations where we investigate in detail the energy and
momentum deposition from jets into their surrounding environment and quantify
the c... | astro-ph | jets and outflows from young stellar objects are proposed candidates to drive supersonic turbulence in molecular clouds here we present the results from multidimensional jet simulations where we investigate in detail the energy and momentum deposition from jets into their surrounding environment and quantify the charac... | [['jets', 'and', 'outflows', 'from', 'young', 'stellar', 'objects', 'are', 'proposed', 'candidates', 'to', 'drive', 'supersonic', 'turbulence', 'in', 'molecular', 'clouds', 'here', 'we', 'present', 'the', 'results', 'from', 'multidimensional', 'jet', 'simulations', 'where', 'we', 'investigate', 'in', 'detail', 'the', '... | [-0.10851773557362038, 0.2244481866840612, -0.07885562505439989, 0.11981988544863129, -0.08125967186174125, -0.038497907947144146, -0.021217523301443594, 0.4324834553174094, -0.2481159845513727, -0.27784434467245667, 0.01194638742871776, -0.24342661367898638, 0.009738332874673818, 0.16424450568564528, 0.027872363631553... |
706.3641 | Leapover lengths and first passage time statistics for L\'evy flights | Exact results for the first passage time and leapover statistics of symmetric
and one-sided Levy flights (LFs) are derived. LFs with stable index alpha are
shown to have leapover lengths, that are asymptotically power-law distributed
with index alpha for one-sided LFs and, surprisingly, with index alpha/2 for
symmetr... | cond-mat.stat-mech | exact results for the first passage time and leapover statistics of symmetric and onesided levy flights lfs are derived lfs with stable index alpha are shown to have leapover lengths that are asymptotically powerlaw distributed with index alpha for onesided lfs and surprisingly with index alpha2 for symmetric lfs the f... | [['exact', 'results', 'for', 'the', 'first', 'passage', 'time', 'and', 'leapover', 'statistics', 'of', 'symmetric', 'and', 'onesided', 'levy', 'flights', 'lfs', 'are', 'derived', 'lfs', 'with', 'stable', 'index', 'alpha', 'are', 'shown', 'to', 'have', 'leapover', 'lengths', 'that', 'are', 'asymptotically', 'powerlaw', ... | [-0.05678041934184116, 0.16777572587419015, -0.12678412296860428, 0.09532250568352557, -0.0023439343798659987, -0.18109601745791323, -0.010336887951080617, 0.522875853302469, -0.16801824845414567, -0.2939694348395198, 0.12649377713947055, -0.2511248844010489, -0.08336444561379952, 0.1985391386385475, 0.0355394747886028... |
706.3642 | Nearly Tight Frames and Space-Frequency Analysis on Compact Manifolds | Let $\bf M$ be a smooth compact oriented Riemannian manifold, and let
$\Delta$ be the Laplace-Beltrami operator on ${\bf M}$. Say $0 \neq f \in
\mathcal{S}(\RR^+)$, and that $f(0) = 0$. For $t > 0$, let $K_t(x,y)$ denote
the kernel of $f(t^2 \Delta)$. Suppose $f$ satisfies Daubechies' criterion, and
$b > 0$. For each... | math.CA math.FA | let bf m be a smooth compact oriented riemannian manifold and let delta be the laplacebeltrami operator on bf m say 0 neq f in mathcalsrr and that f0 0 for t 0 let k_txy denote the kernel of ft2 delta suppose f satisfies daubechies criterion and b 0 for each j write bf m as a disjoint union of measurable sets e_jk with... | [['let', 'bf', 'm', 'be', 'a', 'smooth', 'compact', 'oriented', 'riemannian', 'manifold', 'and', 'let', 'delta', 'be', 'the', 'laplacebeltrami', 'operator', 'on', 'bf', 'm', 'say', '0', 'neq', 'f', 'in', 'mathcalsrr', 'and', 'that', 'f0', '0', 'for', 't', '0', 'let', 'k_txy', 'denote', 'the', 'kernel', 'of', 'ft2', 'de... | [-0.1357691191640401, 0.1596788792805963, -0.048630472308957895, 0.029520225381774668, -0.05253866537340534, -0.1799089605071719, 0.01105458020456424, 0.3626518175944455, -0.28980712347723503, -0.20757625754342807, 0.09069603705794962, -0.27480596902350674, -0.1080084161989954, 0.184103392394866, -0.056271542810062, -0... |
706.3643 | Partition function for two-dimensional nearest neighbour Ising model in
the presence of external magnetic field | The partition function for two-dimensional nearest neighbour Ising models in
the presence of a magnetic field is derived . A comparison with the partition
functions predicted by Onsager is carried out. The critical temperature
estimated by two different methods yields good agreement with the result of
Yang and Lee.
| physics.chem-ph | the partition function for twodimensional nearest neighbour ising models in the presence of a magnetic field is derived a comparison with the partition functions predicted by onsager is carried out the critical temperature estimated by two different methods yields good agreement with the result of yang and lee | [['the', 'partition', 'function', 'for', 'twodimensional', 'nearest', 'neighbour', 'ising', 'models', 'in', 'the', 'presence', 'of', 'a', 'magnetic', 'field', 'is', 'derived', 'a', 'comparison', 'with', 'the', 'partition', 'functions', 'predicted', 'by', 'onsager', 'is', 'carried', 'out', 'the', 'critical', 'temperatur... | [-0.12048932457886015, 0.07451225418481044, -0.021492947154911235, 0.08172718923015054, 0.018546143158649404, -0.1425126877729781, 0.059435481283192836, 0.34307118334497017, -0.16758372619127235, -0.3243308859722068, 0.035534162081603426, -0.2837208939405779, -0.14391670007413873, 0.17962935524216542, 0.088968200492672... |
706.3644 | Dilatation structures with the Radon-Nikodym property | In this paper I explain what is a pair of dilatation structures, one looking
down to another. Such a pair of dilatation structures leads to the intrinsic
definition of a distribution as a field of topological filters.
To any pair of dilatation structures there is an associated notion of
differentiability which gene... | math.MG | in this paper i explain what is a pair of dilatation structures one looking down to another such a pair of dilatation structures leads to the intrinsic definition of a distribution as a field of topological filters to any pair of dilatation structures there is an associated notion of differentiability which generalizes... | [['in', 'this', 'paper', 'i', 'explain', 'what', 'is', 'a', 'pair', 'of', 'dilatation', 'structures', 'one', 'looking', 'down', 'to', 'another', 'such', 'a', 'pair', 'of', 'dilatation', 'structures', 'leads', 'to', 'the', 'intrinsic', 'definition', 'of', 'a', 'distribution', 'as', 'a', 'field', 'of', 'topological', 'fi... | [-0.14943945267031655, 0.09378819894699592, -0.13131724376948659, 0.12211445705756417, -0.11630128652001892, -0.08373147331381581, -0.014665905194860166, 0.38683533347907595, -0.335829016514358, -0.17743848663240927, 0.09735883437913317, -0.2774402996774893, -0.15637153630739015, 0.1768271249528953, -0.1339952183295919... |
706.3645 | Multi-black hole configurations on the cylinder | We construct the metric of new multi-black hole configurations on a
d-dimensional cylinder R^{d-1} x S^1, in the limit of small total mass (or
equivalently in the limit of a large cylinder). These solutions are valid to
first order in the total mass and describe configurations with several small
black holes located a... | hep-th gr-qc | we construct the metric of new multiblack hole configurations on a ddimensional cylinder rd1 x s1 in the limit of small total mass or equivalently in the limit of a large cylinder these solutions are valid to first order in the total mass and describe configurations with several small black holes located at different p... | [['we', 'construct', 'the', 'metric', 'of', 'new', 'multiblack', 'hole', 'configurations', 'on', 'a', 'ddimensional', 'cylinder', 'rd1', 'x', 's1', 'in', 'the', 'limit', 'of', 'small', 'total', 'mass', 'or', 'equivalently', 'in', 'the', 'limit', 'of', 'a', 'large', 'cylinder', 'these', 'solutions', 'are', 'valid', 'to'... | [-0.1849101623674618, 0.10986448751597856, -0.054309188931130736, 0.12181022557177844, -0.04061209516810737, -0.09689425257194108, 0.05052603747006197, 0.29991912275027915, -0.1903903237518273, -0.27515370851043014, 0.11592897475576183, -0.2980967941771143, -0.09144837684924226, 0.1798724408315505, -0.04948209845769677... |
706.3646 | Symmetries and Dynamics of Discrete Systems | We consider discrete dynamical systems and lattice models in statistical
mechanics from the point of view of their symmetry groups. We describe a C
program for symmetry analysis of discrete systems. Among other features, the
program constructs and investigates phase portraits of discrete dynamical
systems modulo grou... | math-ph math.DS math.MP nlin.PS | we consider discrete dynamical systems and lattice models in statistical mechanics from the point of view of their symmetry groups we describe a c program for symmetry analysis of discrete systems among other features the program constructs and investigates phase portraits of discrete dynamical systems modulo groups of... | [['we', 'consider', 'discrete', 'dynamical', 'systems', 'and', 'lattice', 'models', 'in', 'statistical', 'mechanics', 'from', 'the', 'point', 'of', 'view', 'of', 'their', 'symmetry', 'groups', 'we', 'describe', 'a', 'c', 'program', 'for', 'symmetry', 'analysis', 'of', 'discrete', 'systems', 'among', 'other', 'features'... | [-0.2030423018815262, 0.11743556804044152, -0.12756956366637906, 0.09268909039815049, -0.038743646252531926, -0.1572972474463673, 0.05767626958166167, 0.36734203062951565, -0.2989458643056063, -0.2716865852516104, 0.08905295571977538, -0.2772251762050603, -0.1711754537888567, 0.14103042326642426, -0.029647878023212428,... |
706.3647 | Epidemic modeling in metapopulation systems with heterogeneous coupling
pattern: theory and simulations | The spatial structure of populations is a key element in the understanding of
the large scale spreading of epidemics. Motivated by the recent empirical
evidence on the heterogeneous properties of transportation and commuting
patterns among urban areas, we present a thorough analysis of the behavior of
infectious dise... | q-bio.PE physics.soc-ph | the spatial structure of populations is a key element in the understanding of the large scale spreading of epidemics motivated by the recent empirical evidence on the heterogeneous properties of transportation and commuting patterns among urban areas we present a thorough analysis of the behavior of infectious diseases... | [['the', 'spatial', 'structure', 'of', 'populations', 'is', 'a', 'key', 'element', 'in', 'the', 'understanding', 'of', 'the', 'large', 'scale', 'spreading', 'of', 'epidemics', 'motivated', 'by', 'the', 'recent', 'empirical', 'evidence', 'on', 'the', 'heterogeneous', 'properties', 'of', 'transportation', 'and', 'commuti... | [-0.15216817172366834, 0.09488545878181415, -0.07499828493345237, 0.09091033595363968, -0.04045537281759876, -0.11415908470033158, 0.0896095419532539, 0.33254168513269305, -0.24742220247110713, -0.28904713982325275, 0.0677013954659349, -0.27434584088131275, -0.24290236805224555, 0.13202226080130708, -0.0426141498725355... |
706.3648 | Flare magnetic reconnection and relativistic particles in the 2003
October 28 event | An X17.2 solar flare occurred on 2003 October 28, accompanied by
multi-wavelength emissions and a high flux of relativistic particles observed
at 1AU. We present the analytic results of the TRACE, SOHO, RHESSI, ACE, GOES,
hard X-ray (INTEGRAL satellite), radio (Onderejov radio telescope), and neutron
monitor data. It... | astro-ph | an x172 solar flare occurred on 2003 october 28 accompanied by multiwavelength emissions and a high flux of relativistic particles observed at 1au we present the analytic results of the trace soho rhessi ace goes hard xray integral satellite radio onderejov radio telescope and neutron monitor data it is found that the ... | [['an', 'x172', 'solar', 'flare', 'occurred', 'on', '2003', 'october', '28', 'accompanied', 'by', 'multiwavelength', 'emissions', 'and', 'a', 'high', 'flux', 'of', 'relativistic', 'particles', 'observed', 'at', '1au', 'we', 'present', 'the', 'analytic', 'results', 'of', 'the', 'trace', 'soho', 'rhessi', 'ace', 'goes', ... | [-0.09566687132464721, 0.26589123331796144, -0.024016056306780748, 0.18453617489659727, -0.09823896374062835, -0.06123640795038747, 0.026387749592374478, 0.43006530738036547, -0.1998204234521836, -0.41037873842620426, 0.011581608705455437, -0.3073245247360319, -0.03368012626721923, 0.2169590665634522, -0.00622041965169... |
706.3649 | Vacuum Rabi splitting and intracavity dark state in a cavity-atoms
system | We report experimental measurements of the transmission spectrum of an
optical cavity coupled with cold Rb atoms. We observe the multi-atom vacuum
Rabi splitting of a composite cavity and atom system. When a coupling field is
applied to the atoms and induces the resonant two-photon Raman transition with
the cavity fi... | physics.optics physics.atom-ph | we report experimental measurements of the transmission spectrum of an optical cavity coupled with cold rb atoms we observe the multiatom vacuum rabi splitting of a composite cavity and atom system when a coupling field is applied to the atoms and induces the resonant twophoton raman transition with the cavity field in... | [['we', 'report', 'experimental', 'measurements', 'of', 'the', 'transmission', 'spectrum', 'of', 'an', 'optical', 'cavity', 'coupled', 'with', 'cold', 'rb', 'atoms', 'we', 'observe', 'the', 'multiatom', 'vacuum', 'rabi', 'splitting', 'of', 'a', 'composite', 'cavity', 'and', 'atom', 'system', 'when', 'a', 'coupling', 'f... | [-0.19674791138619185, 0.2292557193945686, -0.022003285833634437, -0.0538143344654236, 0.007563137710094452, -0.20221483600325882, 0.08214723062817939, 0.4333733041677624, -0.21325156275881454, -0.2584831691719592, -0.022616004842566328, -0.2795501988194883, -0.01754762450233102, 0.17132268494926392, 0.0323223309498280... |
706.365 | The Weyl-Heisenberg Group on the Noncommutative Two-Torus: A Zoo of
Representations | In order to assess possible observable effects of noncommutativity in
deformations of quantum mechanics, all irreducible representations of the
noncommutative Heisenberg algebra and Weyl-Heisenberg group on the two-torus
are constructed. This analysis extends the well known situation for the
noncommutative torus base... | hep-th | in order to assess possible observable effects of noncommutativity in deformations of quantum mechanics all irreducible representations of the noncommutative heisenberg algebra and weylheisenberg group on the twotorus are constructed this analysis extends the well known situation for the noncommutative torus based on t... | [['in', 'order', 'to', 'assess', 'possible', 'observable', 'effects', 'of', 'noncommutativity', 'in', 'deformations', 'of', 'quantum', 'mechanics', 'all', 'irreducible', 'representations', 'of', 'the', 'noncommutative', 'heisenberg', 'algebra', 'and', 'weylheisenberg', 'group', 'on', 'the', 'twotorus', 'are', 'construc... | [-0.16550619832964408, 0.14859586232341826, -0.07898292046997489, 0.09699259769533658, -0.09841226492426358, -0.09229898682355674, -0.0507317310904101, 0.3178702603456461, -0.2967163882373522, -0.2364735903360674, 0.10941042577097607, -0.24368793087261212, -0.11978497495874763, 0.1943092507572146, -0.09138620423618704,... |
706.3651 | Super strong nuclear force caused by migrating Kbar mesons - Revival of
the Heitler-London-Heisenberg scheme in kaonic nuclear clusters | We have studied the structure of K- pp comprehensively by solving this
three-body system in a variational method, starting from the Ansatz that the
Lambda(1405) resonance (~ Lambda*) is a K-p bound state. The structure of K-pp
reveals a molecular feature, namely, the K- in Lambda* as an "atomic center"
plays a key ro... | nucl-th | we have studied the structure of k pp comprehensively by solving this threebody system in a variational method starting from the ansatz that the lambda1405 resonance lambda is a kp bound state the structure of kpp reveals a molecular feature namely the k in lambda as an atomic center plays a key role in producing stron... | [['we', 'have', 'studied', 'the', 'structure', 'of', 'k', 'pp', 'comprehensively', 'by', 'solving', 'this', 'threebody', 'system', 'in', 'a', 'variational', 'method', 'starting', 'from', 'the', 'ansatz', 'that', 'the', 'lambda1405', 'resonance', 'lambda', 'is', 'a', 'kp', 'bound', 'state', 'the', 'structure', 'of', 'kp... | [-0.16956800574867836, 0.21323321066960785, -0.10312992238401864, 0.06594427744824782, -0.014547853655106312, -0.15620863710677982, 0.05260206985277929, 0.3069836454752304, -0.2619625000421562, -0.2583226423924537, -0.05198050504298629, -0.27945983777376443, -0.10680400710466406, 0.11514518263347044, 0.106841906562221,... |
706.3652 | Continuous breakdown of Purcell's scallop theorem with inertia | Purcell's scallop theorem defines the type of motions of a solid body -
reciprocal motions - which cannot propel the body in a viscous fluid with zero
Reynolds number. For example, the flapping of a wing is reciprocal and, as was
recently shown, can lead to directed motion only if its frequency Reynolds
number, Re_f,... | cond-mat.soft physics.bio-ph physics.flu-dyn | purcells scallop theorem defines the type of motions of a solid body reciprocal motions which cannot propel the body in a viscous fluid with zero reynolds number for example the flapping of a wing is reciprocal and as was recently shown can lead to directed motion only if its frequency reynolds number re_f is above a c... | [['purcells', 'scallop', 'theorem', 'defines', 'the', 'type', 'of', 'motions', 'of', 'a', 'solid', 'body', 'reciprocal', 'motions', 'which', 'can', 'not', 'propel', 'the', 'body', 'in', 'a', 'viscous', 'fluid', 'with', 'zero', 'reynolds', 'number', 'for', 'example', 'the', 'flapping', 'of', 'a', 'wing', 'is', 'reciproc... | [-0.21453628325364732, 0.2462698523214875, -0.08690178067011473, -0.022050966225483883, -0.11899205243053775, -0.10013460021358557, 0.021703119967311908, 0.2936137722661862, -0.28194042419692356, -0.28829452982441023, 0.07213298181550971, -0.21084796924752972, -0.14688900790161613, 0.22293475791453743, -0.0807268548037... |
706.3653 | Lower bound of minimal time evolution in quantum mechanics | We show that the total time of evolution from the initial quantum state to
final quantum state and then back to the initial state, i.e., making a round
trip along the great circle over S^2, must have a lower bound in quantum
mechanics, if the difference between two eigenstates of the 2\times 2
Hamiltonian is kept fix... | quant-ph hep-th | we show that the total time of evolution from the initial quantum state to final quantum state and then back to the initial state ie making a round trip along the great circle over s2 must have a lower bound in quantum mechanics if the difference between two eigenstates of the 2times 2 hamiltonian is kept fixed even th... | [['we', 'show', 'that', 'the', 'total', 'time', 'of', 'evolution', 'from', 'the', 'initial', 'quantum', 'state', 'to', 'final', 'quantum', 'state', 'and', 'then', 'back', 'to', 'the', 'initial', 'state', 'ie', 'making', 'a', 'round', 'trip', 'along', 'the', 'great', 'circle', 'over', 's2', 'must', 'have', 'a', 'lower',... | [-0.1569264802354336, 0.2194844808990587, -0.07780426059797499, 0.039757755877137736, -0.025600260755579387, -0.17560894909656102, 0.006060645519321935, 0.33083879287638096, -0.28933187700252727, -0.28382983126370986, 0.0887976181512606, -0.25655912214554616, -0.12802833755448553, 0.1481184116951537, -0.031636726333519... |
706.3654 | Catalytic Conversion Probabilities for Bipartite Pure States | For two given bipartite-entangled pure states, an expression is obtained for
the least upper bound of conversion probabilities using catalysis. The
attainability of the upper bound can also be decided if that bound is less than
one.
| quant-ph | for two given bipartiteentangled pure states an expression is obtained for the least upper bound of conversion probabilities using catalysis the attainability of the upper bound can also be decided if that bound is less than one | [['for', 'two', 'given', 'bipartiteentangled', 'pure', 'states', 'an', 'expression', 'is', 'obtained', 'for', 'the', 'least', 'upper', 'bound', 'of', 'conversion', 'probabilities', 'using', 'catalysis', 'the', 'attainability', 'of', 'the', 'upper', 'bound', 'can', 'also', 'be', 'decided', 'if', 'that', 'bound', 'is', '... | [-0.105127168668283, 0.2277034061895589, -0.08590921706746558, 0.10383392079431261, -0.016727438121027238, -0.1880752089861277, 0.12318038874985399, 0.2642525616227775, -0.1846314114644318, -0.3458077246071519, 0.13727183045970426, -0.2643176645443246, -0.11037240846938379, 0.29509073460625634, 0.02777302949815183, -0.... |
706.3655 | Curvature Fields, Topology, and the Dynamics of Spatiotemporal Chaos | The curvature field is measured from tracer particle trajectories in a
two-dimensional fluid flow that exhibits spatiotemporal chaos, and is used to
extract the hyperbolic and elliptic points of the flow. These special points
are pinned to the forcing when the driving is weak, but wander over the domain
and interact ... | physics.flu-dyn | the curvature field is measured from tracer particle trajectories in a twodimensional fluid flow that exhibits spatiotemporal chaos and is used to extract the hyperbolic and elliptic points of the flow these special points are pinned to the forcing when the driving is weak but wander over the domain and interact in pai... | [['the', 'curvature', 'field', 'is', 'measured', 'from', 'tracer', 'particle', 'trajectories', 'in', 'a', 'twodimensional', 'fluid', 'flow', 'that', 'exhibits', 'spatiotemporal', 'chaos', 'and', 'is', 'used', 'to', 'extract', 'the', 'hyperbolic', 'and', 'elliptic', 'points', 'of', 'the', 'flow', 'these', 'special', 'po... | [-0.1950497222318187, 0.18705396787729775, -0.12745847186306491, 0.0511506291579942, -0.05483872776808725, -0.10943926290333779, -0.006524056151234122, 0.3542792947581885, -0.34704631325704133, -0.2547713537086648, 0.06874442370132204, -0.2873430762529923, -0.14823849049968307, 0.15348074182640464, -0.04311436005148359... |
706.3656 | Betti numbers of Springer fibers in type A | We determine the Betti numbers of the Springer fibers in type A. To do this,
we construct a cell decomposition of the Springer fibers. The codimension of
the cells is given by an analogue of the Coxeter length. This makes our cell
decomposition well suited for the calculation of Betti numbers.
| math.AG | we determine the betti numbers of the springer fibers in type a to do this we construct a cell decomposition of the springer fibers the codimension of the cells is given by an analogue of the coxeter length this makes our cell decomposition well suited for the calculation of betti numbers | [['we', 'determine', 'the', 'betti', 'numbers', 'of', 'the', 'springer', 'fibers', 'in', 'type', 'a', 'to', 'do', 'this', 'we', 'construct', 'a', 'cell', 'decomposition', 'of', 'the', 'springer', 'fibers', 'the', 'codimension', 'of', 'the', 'cells', 'is', 'given', 'by', 'an', 'analogue', 'of', 'the', 'coxeter', 'length... | [-0.1889035598758389, 0.08279181064783331, -0.07877155239967738, 0.02884839290488219, -0.06672299879730917, -0.05381663108938465, 0.04332138722141584, 0.27810217242907076, -0.3180103450283116, -0.19831916927268692, 0.08363673765458823, -0.20115768697624112, -0.19201060808172413, 0.1898649613961906, -0.20481173927877463... |
706.3657 | Coloring complexes and arrangements | Steingrimsson's coloring complex and Jonsson's unipolar complex are
interpreted in terms of hyperplane arrangements. This viewpoint leads to short
proofs that all coloring complexes and a large class of unipolar complexes have
convex ear decompositions. These convex ear decompositions impose strong new
restrictions o... | math.CO | steingrimssons coloring complex and jonssons unipolar complex are interpreted in terms of hyperplane arrangements this viewpoint leads to short proofs that all coloring complexes and a large class of unipolar complexes have convex ear decompositions these convex ear decompositions impose strong new restrictions on the ... | [['steingrimssons', 'coloring', 'complex', 'and', 'jonssons', 'unipolar', 'complex', 'are', 'interpreted', 'in', 'terms', 'of', 'hyperplane', 'arrangements', 'this', 'viewpoint', 'leads', 'to', 'short', 'proofs', 'that', 'all', 'coloring', 'complexes', 'and', 'a', 'large', 'class', 'of', 'unipolar', 'complexes', 'have'... | [-0.2063873216966241, 0.06262962071461574, -0.045271638588654614, 0.0866161823690322, -0.1419991364643451, -0.14564182791888478, -0.04071663033830682, 0.3899281836513962, -0.3145963291800211, -0.2335253344287002, 0.08366096071669803, -0.21676720986290585, -0.17034166607828366, 0.18331305320478147, -0.18328739349390305,... |
706.3658 | Field theory on $\kappa$--Minkowski space revisited: Noether charges and
breaking of Lorentz symmetry | This paper is devoted to detailed investigations of free scalar field theory
on $\kappa$-Minkowski space. After reviewing necessary mathematical tools we
discuss in depth the Lagrangian and solutions of field equations. We analyze
the spacetime symmetries of the model and construct the conserved charges
associated wi... | hep-th | this paper is devoted to detailed investigations of free scalar field theory on kappaminkowski space after reviewing necessary mathematical tools we discuss in depth the lagrangian and solutions of field equations we analyze the spacetime symmetries of the model and construct the conserved charges associated with trans... | [['this', 'paper', 'is', 'devoted', 'to', 'detailed', 'investigations', 'of', 'free', 'scalar', 'field', 'theory', 'on', 'kappaminkowski', 'space', 'after', 'reviewing', 'necessary', 'mathematical', 'tools', 'we', 'discuss', 'in', 'depth', 'the', 'lagrangian', 'and', 'solutions', 'of', 'field', 'equations', 'we', 'anal... | [-0.18475388228537493, 0.1732092537015305, -0.07022087543344732, 0.09202181607788282, -0.10772172541598256, -0.10927390848192271, -0.04618066683374973, 0.33236150440414636, -0.23099380119944388, -0.25868209087279403, 0.07052411079626489, -0.23823377864142314, -0.17100143234841944, 0.10647158843486078, -0.07110552914084... |
706.3659 | Duality Symmetries and G^{+++} Theories | We show that the non-linear realisations of all the very extended algebras
G^{+++}, except the B and C series which we do not consider, contain fields
corresponding to all possible duality symmetries of the on-shell degrees of
freedom of these theories. This result also holds for G_2^{+++} and we argue
that the non-l... | hep-th | we show that the nonlinear realisations of all the very extended algebras g except the b and c series which we do not consider contain fields corresponding to all possible duality symmetries of the onshell degrees of freedom of these theories this result also holds for g_2 and we argue that the nonlinear realisation of... | [['we', 'show', 'that', 'the', 'nonlinear', 'realisations', 'of', 'all', 'the', 'very', 'extended', 'algebras', 'g', 'except', 'the', 'b', 'and', 'c', 'series', 'which', 'we', 'do', 'not', 'consider', 'contain', 'fields', 'corresponding', 'to', 'all', 'possible', 'duality', 'symmetries', 'of', 'the', 'onshell', 'degree... | [-0.16467542809927288, 0.11918897241737475, -0.06540820324683891, 0.0755789003417115, -0.10350840963861521, -0.12260782267240918, -0.014111922701875515, 0.35122007497531527, -0.25026097843313916, -0.2513539011206697, 0.08222712973981877, -0.2124786501421648, -0.18165233410237466, 0.15451091996476274, -0.046656048363622... |
706.366 | Polarization of Lambda0 and antiLambda0 inclusively produced by 610GeV/c
Sigma- and 525GeV/c proton beams | We have measured the polarization of Lambda0 and antiLambda0 inclusively
produced by 610GeV/c Sigma- and 525GeV/c proton beams in the experiment SELEX
during the 1996/7 fixed target run at Fermilab. The polarization was measured
as a function of the Lambda longitudinal momentum fraction xF and transverse
momentum pt.... | hep-ex | we have measured the polarization of lambda0 and antilambda0 inclusively produced by 610gevc sigma and 525gevc proton beams in the experiment selex during the 19967 fixed target run at fermilab the polarization was measured as a function of the lambda longitudinal momentum fraction xf and transverse momentum pt for the... | [['we', 'have', 'measured', 'the', 'polarization', 'of', 'lambda0', 'and', 'antilambda0', 'inclusively', 'produced', 'by', '610gevc', 'sigma', 'and', '525gevc', 'proton', 'beams', 'in', 'the', 'experiment', 'selex', 'during', 'the', '19967', 'fixed', 'target', 'run', 'at', 'fermilab', 'the', 'polarization', 'was', 'mea... | [-0.09096863073664868, 0.20633540659647195, -0.09417043881671082, 0.06967681420933185, 0.00121375308334527, -0.12203675860655494, -0.0017965903595810937, 0.4080493619004565, -0.20586719327876646, -0.3034510190388368, -0.016769232770105103, -0.35221601216753406, 0.044850772539634376, 0.1683863705482274, 0.06968241833871... |
706.3661 | Thermodynamic properties of magneto-anisotropic nanoparticles | The purpose of this paper is to study the thermodynamic equilibrium
properties of a collection of non-interacting three-dimensional (3D)
magnetically anisotropic nanoparticles in the light of classical statistical
physics. Pertaining to the angular dependence ($\alpha$) of the magnetic field
with the anisotropy axis,... | cond-mat.stat-mech | the purpose of this paper is to study the thermodynamic equilibrium properties of a collection of noninteracting threedimensional 3d magnetically anisotropic nanoparticles in the light of classical statistical physics pertaining to the angular dependence alpha of the magnetic field with the anisotropy axis energy lands... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'study', 'the', 'thermodynamic', 'equilibrium', 'properties', 'of', 'a', 'collection', 'of', 'noninteracting', 'threedimensional', '3d', 'magnetically', 'anisotropic', 'nanoparticles', 'in', 'the', 'light', 'of', 'classical', 'statistical', 'physics', 'pertaining',... | [-0.16362828859679499, 0.14982466283101148, -0.0672582704788319, 0.015054894507078356, -0.04760284050931468, -0.1097246245312578, 0.030306982506820197, 0.33797067379284845, -0.2525926404571357, -0.32674552687737896, 0.024439987152857754, -0.2998564164828215, -0.10965957157742723, 0.18587400158254527, 0.0796839834901651... |
706.3662 | Numerical experiments with p F- and q D-strings: the formation of (p,q)
bound states | We investigate the behaviour of (p,q) string networks, focusing on two
aspects: (1) modelling more realistic (p,q) string networks than the Z_N
networks used so far and (2) investigating the effect of long-range
interactions on the evolution of the network. We model the network with no
long-range interactions using t... | hep-th astro-ph hep-ph | we investigate the behaviour of pq string networks focusing on two aspects 1 modelling more realistic pq string networks than the z_n networks used so far and 2 investigating the effect of longrange interactions on the evolution of the network we model the network with no longrange interactions using two sets of fields... | [['we', 'investigate', 'the', 'behaviour', 'of', 'pq', 'string', 'networks', 'focusing', 'on', 'two', 'aspects', '1', 'modelling', 'more', 'realistic', 'pq', 'string', 'networks', 'than', 'the', 'z_n', 'networks', 'used', 'so', 'far', 'and', '2', 'investigating', 'the', 'effect', 'of', 'longrange', 'interactions', 'on'... | [-0.2040115925788641, 0.1694531634779329, -0.05662584022324953, 0.13146970089647078, -0.004284003195807156, -0.12283182696711908, 0.0035956106219645137, 0.35850371624536176, -0.22527956536675736, -0.30616016181401634, 0.0544816782100342, -0.31298626015791897, -0.16959448008820777, 0.11197887696950447, 0.061917559859888... |
706.3663 | Wilson-t'Hooft Loops in Finite-Temperature Non-commutative Dipole Field
Theory from Dual Supergravity | We first study the temporal Wilson loop in the finite-temperature
non-commutative dipole field theory from the string/gauge correspondence. The
associated dual supergravity background is constructed from the near-horizon
geometry of near-extremal D-branes, after applying T-duality and smeared twist.
We investigate th... | hep-th | we first study the temporal wilson loop in the finitetemperature noncommutative dipole field theory from the stringgauge correspondence the associated dual supergravity background is constructed from the nearhorizon geometry of nearextremal dbranes after applying tduality and smeared twist we investigate the string con... | [['we', 'first', 'study', 'the', 'temporal', 'wilson', 'loop', 'in', 'the', 'finitetemperature', 'noncommutative', 'dipole', 'field', 'theory', 'from', 'the', 'stringgauge', 'correspondence', 'the', 'associated', 'dual', 'supergravity', 'background', 'is', 'constructed', 'from', 'the', 'nearhorizon', 'geometry', 'of', ... | [-0.15162835941677952, 0.206211588434903, -0.06522529330824066, 0.11799173596536924, -0.05393659904431312, -0.1305701530302671, 0.021981528874230872, 0.36342211461390167, -0.2100010571397777, -0.25749555585782, 0.030644368841972344, -0.27036386700706805, -0.11558517909213069, 0.11283152383380438, -0.00520133646373695, ... |
706.3664 | Long time behavior of quasi-stationary states of the Hamiltonian
Mean-Field model | The Hamiltonian Mean-Field model has been investigated, since its
introduction about a decade ago, to study the equilibrium and dynamical
properties of long-range interacting systems. Here we study the long-time
behavior of long-lived, out-of-equilibrium, quasi-stationary dynamical states,
whose lifetime diverges in ... | cond-mat.stat-mech | the hamiltonian meanfield model has been investigated since its introduction about a decade ago to study the equilibrium and dynamical properties of longrange interacting systems here we study the longtime behavior of longlived outofequilibrium quasistationary dynamical states whose lifetime diverges in the thermodynam... | [['the', 'hamiltonian', 'meanfield', 'model', 'has', 'been', 'investigated', 'since', 'its', 'introduction', 'about', 'a', 'decade', 'ago', 'to', 'study', 'the', 'equilibrium', 'and', 'dynamical', 'properties', 'of', 'longrange', 'interacting', 'systems', 'here', 'we', 'study', 'the', 'longtime', 'behavior', 'of', 'lon... | [-0.1378047550199612, 0.21047882133005363, -0.1389903401217933, 0.06722160830212254, 0.013701945105450426, -0.08344279149541362, 0.04581379091715639, 0.33917991826955063, -0.25360974400310116, -0.2763235746888713, 0.11454793713099481, -0.25092042815057364, -0.11764116746478907, 0.1693541892810063, 0.028900760307954916,... |
706.3665 | Multiwavelength optical observations of chromospherically active binary
systems V. FF UMa (2RE J0933+624): a system with orbital period variation | This is the fifth paper in a series aimed at studying the chromospheres of
active binary systems using several optical spectroscopic indicators to obtain
or improve orbital solution and fundamental stellar parameters. We present here
the study of FF UMa (2RE J0933+624), a recently discovered, X-ray/EUV selected,
acti... | astro-ph | this is the fifth paper in a series aimed at studying the chromospheres of active binary systems using several optical spectroscopic indicators to obtain or improve orbital solution and fundamental stellar parameters we present here the study of ff uma 2re j0933624 a recently discovered xrayeuv selected active binary w... | [['this', 'is', 'the', 'fifth', 'paper', 'in', 'a', 'series', 'aimed', 'at', 'studying', 'the', 'chromospheres', 'of', 'active', 'binary', 'systems', 'using', 'several', 'optical', 'spectroscopic', 'indicators', 'to', 'obtain', 'or', 'improve', 'orbital', 'solution', 'and', 'fundamental', 'stellar', 'parameters', 'we',... | [-0.11322889516778877, 0.08574287647664615, -0.08251393043736087, 0.0332096890670209, -0.09199573321608924, -0.11081073799760043, 0.07278378223658065, 0.42509688741147295, -0.20831058105568956, -0.34337542389523, 0.0570797505226049, -0.25550734332138286, -0.07489256742619647, 0.2069288275164486, -0.029172243498098313, ... |
706.3666 | Propagation of Ultra-high-energy Protons in Cosmic Magnetic Fields | We simulate the arrival distribution of ultra-high-energy (UHE) protons by
following their propagation processes in several strengths of a structured
extragalactic magnetic field (EGMF). Comparing our result to observational one
by Akeno Giant Air Shower Array, we constrain the number density of UHE cosmic
ray source... | astro-ph | we simulate the arrival distribution of ultrahighenergy uhe protons by following their propagation processes in several strengths of a structured extragalactic magnetic field egmf comparing our result to observational one by akeno giant air shower array we constrain the number density of uhe cosmic ray sources with the... | [['we', 'simulate', 'the', 'arrival', 'distribution', 'of', 'ultrahighenergy', 'uhe', 'protons', 'by', 'following', 'their', 'propagation', 'processes', 'in', 'several', 'strengths', 'of', 'a', 'structured', 'extragalactic', 'magnetic', 'field', 'egmf', 'comparing', 'our', 'result', 'to', 'observational', 'one', 'by', ... | [-0.11800957247883512, 0.24090453969737818, 0.02571476551059347, 0.15409714913783737, -0.07012585589948755, 0.039607810472639705, -0.015816922784926225, 0.3901489531478057, -0.17421355624325, -0.44369080607564404, 0.006451642902818723, -0.33291387176857545, 0.0027735610367157137, 0.2435062419766417, 0.06339033368276432... |
706.3667 | Affine equation of state from quintessence and k-essence fields | We explore the possibility that a scalar field with appropriate Lagrangian
can mimic a perfect fluid with an affine barotropic equation of state. The
latter can be thought of as a generic cosmological dark component evolving as
an effective cosmological constant plus a generalized dark matter. As such, it
can be used... | astro-ph gr-qc hep-th | we explore the possibility that a scalar field with appropriate lagrangian can mimic a perfect fluid with an affine barotropic equation of state the latter can be thought of as a generic cosmological dark component evolving as an effective cosmological constant plus a generalized dark matter as such it can be used as a... | [['we', 'explore', 'the', 'possibility', 'that', 'a', 'scalar', 'field', 'with', 'appropriate', 'lagrangian', 'can', 'mimic', 'a', 'perfect', 'fluid', 'with', 'an', 'affine', 'barotropic', 'equation', 'of', 'state', 'the', 'latter', 'can', 'be', 'thought', 'of', 'as', 'a', 'generic', 'cosmological', 'dark', 'component'... | [-0.13878281359801758, 0.13529016638286184, -0.15683755319617637, 0.1149050291640671, -0.13298830726644728, -0.14945682767987042, -0.05846365089235189, 0.2971980085635519, -0.26629668512622584, -0.3578307475972842, 0.04994604524169638, -0.23544065621714075, -0.09731591847006572, 0.13568402445953262, 0.03746170018167866... |
706.3668 | The Sunyaev-Zel'dovich temperature of the intracluster medium | The relativistic Sunyaev-Zel'dovich (SZ) effect offers a method, independent
of X-ray, for measuring the temperature of the intracluster medium (ICM) in the
hottest systems. Here, using N-body/hydrodynamic simulations of three galaxy
clusters, we compare the two quantities for a non-radiative ICM, and for one
that is... | astro-ph | the relativistic sunyaevzeldovich sz effect offers a method independent of xray for measuring the temperature of the intracluster medium icm in the hottest systems here using nbodyhydrodynamic simulations of three galaxy clusters we compare the two quantities for a nonradiative icm and for one that is subject both to r... | [['the', 'relativistic', 'sunyaevzeldovich', 'sz', 'effect', 'offers', 'a', 'method', 'independent', 'of', 'xray', 'for', 'measuring', 'the', 'temperature', 'of', 'the', 'intracluster', 'medium', 'icm', 'in', 'the', 'hottest', 'systems', 'here', 'using', 'nbodyhydrodynamic', 'simulations', 'of', 'three', 'galaxy', 'clu... | [-0.04779620089043216, 0.1672432754295552, -0.08378901743407177, 0.09466595774231727, -0.07641359701586567, -0.05104241170772132, 0.07515105685652204, 0.39655629369863277, -0.1904535943399047, -0.3240079988909375, 0.0631156173122418, -0.35139895018166417, 0.020908570390159063, 0.27685252570244634, 0.0638062678674009, -... |
706.3669 | The wave equation on asymptotically de Sitter-like spaces | In this paper we obtain the asymptotic behavior of solutions of the
Klein-Gordon equation on Lorentzian manifolds $(X^\circ,g)$ which are de
Sitter-like at infinity. Such manifolds are Lorentzian analogues of the
so-called Riemannian conformally compact (or asymptotically hyperbolic) spaces.
Under global assumptions ... | math.AP math.DG | in this paper we obtain the asymptotic behavior of solutions of the kleingordon equation on lorentzian manifolds xcircg which are de sitterlike at infinity such manifolds are lorentzian analogues of the socalled riemannian conformally compact or asymptotically hyperbolic spaces under global assumptions on the nullbicha... | [['in', 'this', 'paper', 'we', 'obtain', 'the', 'asymptotic', 'behavior', 'of', 'solutions', 'of', 'the', 'kleingordon', 'equation', 'on', 'lorentzian', 'manifolds', 'xcircg', 'which', 'are', 'de', 'sitterlike', 'at', 'infinity', 'such', 'manifolds', 'are', 'lorentzian', 'analogues', 'of', 'the', 'socalled', 'riemannia... | [-0.1587921339590339, 0.09880000090826366, -0.12781537047555766, 0.09837155072985343, -0.10557475196734323, -0.15930266233981918, -0.034722398957671693, 0.33094376355204413, -0.2782818215851814, -0.19045923475641757, 0.15680992438643382, -0.3575565794924811, -0.10767863044649426, 0.14759551749714667, -0.113604856958865... |
706.367 | Construction of eigenvarieties in small cohomological dimensions for
semi-simple, simply connected groups | We study low order terms of Emerton's spectral sequence for simply connected,
simple groups. As a result, for real rank 1 groups, we show that Emerton's
method for constructing eigenvarieties is successful in cohomological dimension
1. For real rank 2 groups, we show that a slight modification of Emerton's
method all... | math.NT | we study low order terms of emertons spectral sequence for simply connected simple groups as a result for real rank 1 groups we show that emertons method for constructing eigenvarieties is successful in cohomological dimension 1 for real rank 2 groups we show that a slight modification of emertons method allows one to ... | [['we', 'study', 'low', 'order', 'terms', 'of', 'emertons', 'spectral', 'sequence', 'for', 'simply', 'connected', 'simple', 'groups', 'as', 'a', 'result', 'for', 'real', 'rank', '1', 'groups', 'we', 'show', 'that', 'emertons', 'method', 'for', 'constructing', 'eigenvarieties', 'is', 'successful', 'in', 'cohomological',... | [-0.13082553796722726, 0.04935002507507738, -0.10019535823898801, 0.11573881849496609, -0.07803725358493374, -0.15753867923897708, -0.023089147597093577, 0.3825892422158839, -0.2514655893131838, -0.27721306125996475, 0.08258215377849164, -0.18291614164023115, -0.21988329433409845, 0.22494630302476176, -0.14521602951621... |
706.3671 | Validity of the Brunet-Derrida formula for the speed of pulled fronts
with a cutoff | We establish rigorous upper and lower bounds for the speed of pulled fronts
with a cutoff. We show that the Brunet-Derrida formula corresponds to the
leading order expansion in the cut-off parameter of both the upper and lower
bounds. For sufficiently large cut-off parameter the Brunet-Derrida formula
lies outside th... | nlin.PS | we establish rigorous upper and lower bounds for the speed of pulled fronts with a cutoff we show that the brunetderrida formula corresponds to the leading order expansion in the cutoff parameter of both the upper and lower bounds for sufficiently large cutoff parameter the brunetderrida formula lies outside the allowe... | [['we', 'establish', 'rigorous', 'upper', 'and', 'lower', 'bounds', 'for', 'the', 'speed', 'of', 'pulled', 'fronts', 'with', 'a', 'cutoff', 'we', 'show', 'that', 'the', 'brunetderrida', 'formula', 'corresponds', 'to', 'the', 'leading', 'order', 'expansion', 'in', 'the', 'cutoff', 'parameter', 'of', 'both', 'the', 'uppe... | [-0.143506951465071, 0.16954119029584563, -0.07049043565587718, 0.1094872471935387, -0.10248070124748952, -0.12480051956387071, 0.13872577763999563, 0.28643885364496635, -0.18748273537788965, -0.32891849560450903, 0.1356695009368955, -0.2617930259697045, -0.05672982585015176, 0.27163567936307265, 0.017167806002028475, ... |
706.3672 | Bootstrap and the physical values of $\pi N$ resonance parameters | This is the 6th paper in the series developing the formalism to manage the
effective scattering theory of strong interactions. Relying on the theoretical
scheme suggested in our previous publications we concentrate here on the
practical aspect and apply our technique to the elastic pion-nucleon scattering
amplitude. ... | hep-ph hep-th | this is the 6th paper in the series developing the formalism to manage the effective scattering theory of strong interactions relying on the theoretical scheme suggested in our previous publications we concentrate here on the practical aspect and apply our technique to the elastic pionnucleon scattering amplitude we te... | [['this', 'is', 'the', '6th', 'paper', 'in', 'the', 'series', 'developing', 'the', 'formalism', 'to', 'manage', 'the', 'effective', 'scattering', 'theory', 'of', 'strong', 'interactions', 'relying', 'on', 'the', 'theoretical', 'scheme', 'suggested', 'in', 'our', 'previous', 'publications', 'we', 'concentrate', 'here', ... | [-0.08264023015245554, 0.07156170545626551, -0.1417051837502626, 0.0822690820420957, -0.08913478926162145, -0.07720107167598701, 0.08888097803649161, 0.36177718236802087, -0.25785235700858455, -0.2896203162156106, 0.054577552552913286, -0.26445214164202974, -0.1899751899824966, 0.18360543944272062, -0.00382952769512250... |
706.3673 | Systematic study of carrier correlations in the electron-hole
recombination dynamics of quantum dots | The ground state carrier dynamics in self-assembled (In,Ga)As/GaAs quantum
dots has been studied using time-resolved photoluminescence and transmission.
By varying the dot design with respect to confinement and doping, the dynamics
is shown to follow in general a non-exponential decay. Only for specific
conditions in... | cond-mat.other | the ground state carrier dynamics in selfassembled ingaasgaas quantum dots has been studied using timeresolved photoluminescence and transmission by varying the dot design with respect to confinement and doping the dynamics is shown to follow in general a nonexponential decay only for specific conditions in regard to o... | [['the', 'ground', 'state', 'carrier', 'dynamics', 'in', 'selfassembled', 'ingaasgaas', 'quantum', 'dots', 'has', 'been', 'studied', 'using', 'timeresolved', 'photoluminescence', 'and', 'transmission', 'by', 'varying', 'the', 'dot', 'design', 'with', 'respect', 'to', 'confinement', 'and', 'doping', 'the', 'dynamics', '... | [-0.09176123264977443, 0.1864035427437297, -0.06512388439760322, 0.06530344949015195, 0.029799610378575467, -0.20244084303489043, 0.027319464110769333, 0.42343349621764254, -0.24387068634941464, -0.2587576187243463, 0.039040662737430204, -0.29085713206302555, -0.08573315172855343, 0.21458828640835625, 0.013034579885147... |
706.3674 | Conjugate varieties with distinct real cohomology algebras | Using constructions of Voisin, we exhibit a smooth projective variety defined
over a number field k and two complex embeddings of k, such that the two
complex manifolds induced by these embeddings have non isomorphic cohomology
algebras with real coefficients. This contrasts with the fact that the
cohomology algebras... | math.AG | using constructions of voisin we exhibit a smooth projective variety defined over a number field k and two complex embeddings of k such that the two complex manifolds induced by these embeddings have non isomorphic cohomology algebras with real coefficients this contrasts with the fact that the cohomology algebras with... | [['using', 'constructions', 'of', 'voisin', 'we', 'exhibit', 'a', 'smooth', 'projective', 'variety', 'defined', 'over', 'a', 'number', 'field', 'k', 'and', 'two', 'complex', 'embeddings', 'of', 'k', 'such', 'that', 'the', 'two', 'complex', 'manifolds', 'induced', 'by', 'these', 'embeddings', 'have', 'non', 'isomorphic'... | [-0.2358494413819051, 0.08333311829659523, -0.053293147406569034, 0.02640620448316137, -0.12471825361364719, -0.17227863911962646, -0.08128985748132408, 0.3626818941680319, -0.36888258370824833, -0.25682818409845687, 0.06460538840231796, -0.2515069845866299, -0.18342173215227597, 0.22702469401569528, -0.138904796779212... |
706.3675 | Phase-field crystal modeling of equilibrium bcc-liquid interfaces | We investigate the equilibrium properties of bcc-liquid interfaces modeled
with a continuum phase-field crystal (PFC) approach [K. R. Elder and M. Grant,
Phys. Rev. E 70, 051605 (2004)]. A multiscale analysis of the PFC model is
carried out which exploits the fact that the amplitudes of crystal density
waves decay sl... | cond-mat.mtrl-sci | we investigate the equilibrium properties of bccliquid interfaces modeled with a continuum phasefield crystal pfc approach k r elder and m grant phys rev e 70 051605 2004 a multiscale analysis of the pfc model is carried out which exploits the fact that the amplitudes of crystal density waves decay slowly into the liqu... | [['we', 'investigate', 'the', 'equilibrium', 'properties', 'of', 'bccliquid', 'interfaces', 'modeled', 'with', 'a', 'continuum', 'phasefield', 'crystal', 'pfc', 'approach', 'k', 'r', 'elder', 'and', 'm', 'grant', 'phys', 'rev', 'e', '70', '051605', '2004', 'a', 'multiscale', 'analysis', 'of', 'the', 'pfc', 'model', 'is... | [-0.11606350916748245, 0.12387908355199866, -0.07813105696280087, -0.01756685527119165, -0.040838395121196906, -0.09839130118128932, 0.038540231972001494, 0.3024522026690344, -0.21722044898030748, -0.32528621510247746, 0.00878042326574879, -0.2815605685447476, -0.16299479637472403, 0.15158025205933623, 0.04345942592203... |
706.3676 | On the Gompertzian dynamics of growth and self-organization | Comment on the Waliszewski's article "A principle of fractal-sto-chastic
dualism and Gompertzian dynamics of growth and self-organization" (BioSystems
82 (2005)61-73) is presented. It has been proved that the main idea of this
work that Gompertzian dynamics is governed by the Schr\"{o}dinger-like equation
including a... | q-bio.OT q-bio.QM | comment on the waliszewskis article a principle of fractalstochastic dualism and gompertzian dynamics of growth and selforganization biosystems 82 20056173 is presented it has been proved that the main idea of this work that gompertzian dynamics is governed by the schrodingerlike equation including anharmonic morse pot... | [['comment', 'on', 'the', 'waliszewskis', 'article', 'a', 'principle', 'of', 'fractalstochastic', 'dualism', 'and', 'gompertzian', 'dynamics', 'of', 'growth', 'and', 'selforganization', 'biosystems', '82', '20056173', 'is', 'presented', 'it', 'has', 'been', 'proved', 'that', 'the', 'main', 'idea', 'of', 'this', 'work',... | [-0.09631972612133102, 0.0907291408687357, -0.13418020465825167, 0.06110068188337166, -0.05816981157967969, -0.11731335159302467, 0.011687595958984087, 0.3029524611885704, -0.22980740925829327, -0.2757326342638523, 0.10356553310217957, -0.27176885720017174, -0.25530013008900576, 0.19504637661064783, -0.0979723328990595... |
706.3677 | Bubbles Unbound II: AdS and the Single Bubble | I present further analytic time symmetric initial data for five dimensions
describing ``bubbles of nothing'' which have no Kaluza-Klein circle
asymptotically. The new solutions consist of a large family of single bubbles
in both asymptotically flat and asymptotically AdS space. I also numerically
construct gravitatio... | hep-th gr-qc | i present further analytic time symmetric initial data for five dimensions describing bubbles of nothing which have no kaluzaklein circle asymptotically the new solutions consist of a large family of single bubbles in both asymptotically flat and asymptotically ads space i also numerically construct gravitational solit... | [['i', 'present', 'further', 'analytic', 'time', 'symmetric', 'initial', 'data', 'for', 'five', 'dimensions', 'describing', 'bubbles', 'of', 'nothing', 'which', 'have', 'no', 'kaluzaklein', 'circle', 'asymptotically', 'the', 'new', 'solutions', 'consist', 'of', 'a', 'large', 'family', 'of', 'single', 'bubbles', 'in', '... | [-0.16058265392933332, 0.168243699054252, -0.08631457482902881, 0.13479678618593835, -0.1000848516191849, -0.19270379487972925, 0.005480626273863748, 0.313417031429708, -0.17324963361755305, -0.20264385482090908, 0.1584316817929457, -0.28118018890895385, -0.14363758603804835, 0.13591897536260897, -0.02368344578380678, ... |
706.3678 | Experimental confirmation of tissue liquidity based on the exact
solution of the Laplace equation | The notion of tissue surface tension has provided a physical understanding of
morphogenetic phenomena such as tissue spreading or cell sorting. The
measurement of tissue surface tension so far relied on strong approximations on
the geometric profile of a spherical droplet compressed between parallel
plates. We solved... | physics.bio-ph physics.flu-dyn q-bio.TO | the notion of tissue surface tension has provided a physical understanding of morphogenetic phenomena such as tissue spreading or cell sorting the measurement of tissue surface tension so far relied on strong approximations on the geometric profile of a spherical droplet compressed between parallel plates we solved the... | [['the', 'notion', 'of', 'tissue', 'surface', 'tension', 'has', 'provided', 'a', 'physical', 'understanding', 'of', 'morphogenetic', 'phenomena', 'such', 'as', 'tissue', 'spreading', 'or', 'cell', 'sorting', 'the', 'measurement', 'of', 'tissue', 'surface', 'tension', 'so', 'far', 'relied', 'on', 'strong', 'approximatio... | [-0.08011209484445111, 0.15179243443661458, -0.09898129991075445, 0.06285047398001377, -0.04860319112307362, -0.11504479018866175, 0.00469257200377122, 0.34063791467117205, -0.27610882506104967, -0.27610059773489354, 0.1131363038955662, -0.24895911190974257, -0.20936282300728284, 0.1880141965305102, -0.0606093385088775... |
706.3679 | Scale-sensitive Psi-dimensions: the Capacity Measures for Classifiers
Taking Values in R^Q | Bounds on the risk play a crucial role in statistical learning theory. They
usually involve as capacity measure of the model studied the VC dimension or
one of its extensions. In classification, such "VC dimensions" exist for models
taking values in {0, 1}, {1,..., Q} and R. We introduce the generalizations
appropria... | cs.LG | bounds on the risk play a crucial role in statistical learning theory they usually involve as capacity measure of the model studied the vc dimension or one of its extensions in classification such vc dimensions exist for models taking values in 0 1 1 q and r we introduce the generalizations appropriate for the missing ... | [['bounds', 'on', 'the', 'risk', 'play', 'a', 'crucial', 'role', 'in', 'statistical', 'learning', 'theory', 'they', 'usually', 'involve', 'as', 'capacity', 'measure', 'of', 'the', 'model', 'studied', 'the', 'vc', 'dimension', 'or', 'one', 'of', 'its', 'extensions', 'in', 'classification', 'such', 'vc', 'dimensions', 'e... | [-0.08379434157783787, 0.05864331679257714, -0.04105533008682139, 0.1197856987444224, -0.019298452171094625, -0.20013478695541437, 0.03659357670205933, 0.32218014963983016, -0.24050515171508363, -0.27297202368729667, 0.1278089434253397, -0.27399211404500184, -0.10559360714583302, 0.20221997770469313, -0.081383781007456... |
706.368 | The Universal sl_2 Link Homology Theory | We explore the complex associated to a link in the geometric formalism of
Khovanov's (n=2) link homology theory, determine its exact underlying algebraic
structure and find its precise universality properties for link homology
functors. We present new methods of extracting all known link homology theories
directly fr... | math.GT math.QA | we explore the complex associated to a link in the geometric formalism of khovanovs n2 link homology theory determine its exact underlying algebraic structure and find its precise universality properties for link homology functors we present new methods of extracting all known link homology theories directly from this ... | [['we', 'explore', 'the', 'complex', 'associated', 'to', 'a', 'link', 'in', 'the', 'geometric', 'formalism', 'of', 'khovanovs', 'n2', 'link', 'homology', 'theory', 'determine', 'its', 'exact', 'underlying', 'algebraic', 'structure', 'and', 'find', 'its', 'precise', 'universality', 'properties', 'for', 'link', 'homology... | [-0.14127650518471804, 0.06274648556270851, -0.12164370424803704, 0.14955647990528423, -0.11820547440572857, -0.16927512485820514, 0.035031849933931464, 0.3351501348571709, -0.3529294997955171, -0.3219631012099294, 0.07604119431254311, -0.1987548618085454, -0.2355700843895857, 0.18709137693602734, -0.11342829355092432,... |
706.3681 | On the Classification Scheme for Phenomenological Universalities in
Growth Problems in Physics and Other Sciences | Comment on "Classification Scheme for Phenomenological Universalities in
Growth Problems in Physics and Other Sciences" by P. Castorina, P. P. Delsanto
and C. Guiot, Phys. Rev. Lett. {\bf 96}, 188701 (2006) is presented. It has
been proved that the West-like function of growth derived by the authors is
incorrect and ... | q-bio.OT q-bio.QM | comment on classification scheme for phenomenological universalities in growth problems in physics and other sciences by p castorina p p delsanto and c guiot phys rev lett bf 96 188701 2006 is presented it has been proved that the westlike function of growth derived by the authors is incorrect and the approach does not... | [['comment', 'on', 'classification', 'scheme', 'for', 'phenomenological', 'universalities', 'in', 'growth', 'problems', 'in', 'physics', 'and', 'other', 'sciences', 'by', 'p', 'castorina', 'p', 'p', 'delsanto', 'and', 'c', 'guiot', 'phys', 'rev', 'lett', 'bf', '96', '188701', '2006', 'is', 'presented', 'it', 'has', 'be... | [-0.07662067263801065, 0.0647723065663336, -0.09954816607447962, -0.010260077655160179, -0.08796929247263405, -0.1551092504989356, 0.048761351534631105, 0.3030586068932381, -0.20762080120362547, -0.29982528034597633, 0.035710167010418244, -0.24785656375137882, -0.2173223508780615, 0.20565199801543108, -0.11389802866874... |
706.3682 | Orthogonal Set of Basis Functions over the Binocular Pupil | Sets of orthogonal basis functions over two-dimensional circular areas--most
often representing pupils in optical applications--are known in the literature
for the full circle (Zernike or Jacobi polynomials) and the annulus. This work
proposes an orthogonal set if the area is two non-overlapping circular pupils
of sa... | physics.optics | sets of orthogonal basis functions over twodimensional circular areasmost often representing pupils in optical applicationsare known in the literature for the full circle zernike or jacobi polynomials and the annulus this work proposes an orthogonal set if the area is two nonoverlapping circular pupils of same size the... | [['sets', 'of', 'orthogonal', 'basis', 'functions', 'over', 'twodimensional', 'circular', 'areasmost', 'often', 'representing', 'pupils', 'in', 'optical', 'applicationsare', 'known', 'in', 'the', 'literature', 'for', 'the', 'full', 'circle', 'zernike', 'or', 'jacobi', 'polynomials', 'and', 'the', 'annulus', 'this', 'wo... | [-0.14940032231370134, 0.08281204690299798, -0.06652501430584207, 0.02659375283179716, -0.054334935301633934, -0.06863685396854721, -0.0064887723826345, 0.38396845507391153, -0.29431381999766304, -0.2311447016591768, 0.10886817833174035, -0.26509995643596446, -0.12031199877327751, 0.22002235868583536, -0.04438626947664... |
706.3683 | Pipeline Reduction of Binary Light Curves from Large-Scale Surveys | One of the most important changes in observational astronomy of the 21st
Century is a rapid shift from classical object-by-object observations to
extensive automatic surveys. As CCD detectors are getting better and their
prices are getting lower, more and more small and medium-size observatories are
refocusing their ... | astro-ph | one of the most important changes in observational astronomy of the 21st century is a rapid shift from classical objectbyobject observations to extensive automatic surveys as ccd detectors are getting better and their prices are getting lower more and more small and mediumsize observatories are refocusing their attenti... | [['one', 'of', 'the', 'most', 'important', 'changes', 'in', 'observational', 'astronomy', 'of', 'the', '21st', 'century', 'is', 'a', 'rapid', 'shift', 'from', 'classical', 'objectbyobject', 'observations', 'to', 'extensive', 'automatic', 'surveys', 'as', 'ccd', 'detectors', 'are', 'getting', 'better', 'and', 'their', '... | [-0.0757088219197884, 0.05777636202358043, -0.07983962680903536, 0.11686544249328765, -0.17171229126826115, -0.11613525035767931, 0.06963140534559052, 0.44224953203837375, -0.20462598391798145, -0.35622633754539845, 0.16236670063785394, -0.35152969968074294, -0.11513946283451137, 0.2641685205090105, -0.1138402176812402... |
706.3684 | Stability in generic mitochondrial models | In this paper, we use a variety of mathematical techniques to explore
existence, local stability, and global stability of equilibria in abstract
models of mitochondrial metabolism. The class of models constructed is defined
by the biological description of the system, with minimal mathematical
assumptions. The key fe... | q-bio.QM q-bio.SC | in this paper we use a variety of mathematical techniques to explore existence local stability and global stability of equilibria in abstract models of mitochondrial metabolism the class of models constructed is defined by the biological description of the system with minimal mathematical assumptions the key features a... | [['in', 'this', 'paper', 'we', 'use', 'a', 'variety', 'of', 'mathematical', 'techniques', 'to', 'explore', 'existence', 'local', 'stability', 'and', 'global', 'stability', 'of', 'equilibria', 'in', 'abstract', 'models', 'of', 'mitochondrial', 'metabolism', 'the', 'class', 'of', 'models', 'constructed', 'is', 'defined',... | [-0.14105276027076774, 0.11802501094652831, -0.08793526761824401, 0.07365983189337628, -0.01183716779597467, -0.1693307222321448, 0.023863903190741862, 0.37884152173802893, -0.27233989794295643, -0.2631620211759582, 0.11232767940574133, -0.22142092266301738, -0.1236886500250321, 0.15615622045702254, -0.044591494732985,... |
706.3685 | Exclusive Double Charmonium Production from $\Upsilon$ Decay | The exclusive decay of $\Upsilon$ to a vector plus pseudoscalar charmonium is
studied in perturbative QCD. The corresponding branching ratios are predicted
to be of order $10^{-6}$ for first three $\Upsilon$ resonances, and we expect
these decay modes should be discovered in the prospective high-luminosity
$e^+e^-$ f... | hep-ph hep-ex | the exclusive decay of upsilon to a vector plus pseudoscalar charmonium is studied in perturbative qcd the corresponding branching ratios are predicted to be of order 106 for first three upsilon resonances and we expect these decay modes should be discovered in the prospective highluminosity ee facilities such as super... | [['the', 'exclusive', 'decay', 'of', 'upsilon', 'to', 'a', 'vector', 'plus', 'pseudoscalar', 'charmonium', 'is', 'studied', 'in', 'perturbative', 'qcd', 'the', 'corresponding', 'branching', 'ratios', 'are', 'predicted', 'to', 'be', 'of', 'order', '106', 'for', 'first', 'three', 'upsilon', 'resonances', 'and', 'we', 'ex... | [-0.13771342085857652, 0.24876225794799178, -0.08941466080162812, 0.1597009586316913, -0.050663007496580204, -0.13798797833388327, 0.03846285487007764, 0.34136411518341414, -0.20126886950391862, -0.22320357511785846, -0.01232747953165219, -0.311618211579992, -0.04358417811562066, 0.15842971358344787, 0.1105857657708434... |
706.3686 | Spontaneous rotating vortex lattices in a pumped decaying condensate | Injection and decay of particles in an inhomogeneous quantum condensate can
significantly change its behaviour. We model trapped, pumped, decaying
condensates by a complex Gross-Pitaevskii equation and analyse the density and
currents in the steady state. With homogeneous pumping, rotationally symmetric
solutions are... | cond-mat.other | injection and decay of particles in an inhomogeneous quantum condensate can significantly change its behaviour we model trapped pumped decaying condensates by a complex grosspitaevskii equation and analyse the density and currents in the steady state with homogeneous pumping rotationally symmetric solutions are unstabl... | [['injection', 'and', 'decay', 'of', 'particles', 'in', 'an', 'inhomogeneous', 'quantum', 'condensate', 'can', 'significantly', 'change', 'its', 'behaviour', 'we', 'model', 'trapped', 'pumped', 'decaying', 'condensates', 'by', 'a', 'complex', 'grosspitaevskii', 'equation', 'and', 'analyse', 'the', 'density', 'and', 'cu... | [-0.1908993473701665, 0.2904604963375238, -0.05824911787741534, 0.0482098610993252, -0.005676728187371855, -0.18920543770123596, -0.025602688868631325, 0.37068219143775816, -0.2463435161271659, -0.21471920109394452, 0.1363390032455082, -0.25274711741013045, -0.009463128127643595, 0.09578365527609688, 0.0298684670415241... |
706.3687 | Stabilizing unstable periodic orbits in the Lorenz equations using
time-delayed feedback control | For many years it was believed that an unstable periodic orbit with an odd
number of real Floquet multipliers greater than unity cannot be stabilized by
the time-delayed feedback control mechanism of Pyragus. A recent paper by
Fiedler et al uses the normal form of a subcritical Hopf bifurcation to give a
counterexamp... | nlin.CD | for many years it was believed that an unstable periodic orbit with an odd number of real floquet multipliers greater than unity cannot be stabilized by the timedelayed feedback control mechanism of pyragus a recent paper by fiedler et al uses the normal form of a subcritical hopf bifurcation to give a counterexample t... | [['for', 'many', 'years', 'it', 'was', 'believed', 'that', 'an', 'unstable', 'periodic', 'orbit', 'with', 'an', 'odd', 'number', 'of', 'real', 'floquet', 'multipliers', 'greater', 'than', 'unity', 'can', 'not', 'be', 'stabilized', 'by', 'the', 'timedelayed', 'feedback', 'control', 'mechanism', 'of', 'pyragus', 'a', 're... | [-0.18300639787098258, 0.1190311518346567, -0.07877453418403137, 0.04846386634176824, -0.10867122097122596, -0.15576560126628908, 0.05323717496982526, 0.2911128098826583, -0.2815820599338267, -0.2557086243703053, 0.11682276926060184, -0.210806937683828, -0.26036116591677433, 0.23879356481839062, -0.10397197949904494, 0... |
706.3688 | Why the Standard Model | The Standard Model is based on the gauge invariance principle with gauge
group U(1)xSU(2)xSU(3) and suitable representations for fermions and bosons,
which are begging for a conceptual understanding. We propose a purely
gravitational explanation: space-time has a fine structure given as a product
of a four dimensiona... | hep-th math.OA | the standard model is based on the gauge invariance principle with gauge group u1xsu2xsu3 and suitable representations for fermions and bosons which are begging for a conceptual understanding we propose a purely gravitational explanation spacetime has a fine structure given as a product of a four dimensional continuum ... | [['the', 'standard', 'model', 'is', 'based', 'on', 'the', 'gauge', 'invariance', 'principle', 'with', 'gauge', 'group', 'u1xsu2xsu3', 'and', 'suitable', 'representations', 'for', 'fermions', 'and', 'bosons', 'which', 'are', 'begging', 'for', 'a', 'conceptual', 'understanding', 'we', 'propose', 'a', 'purely', 'gravitati... | [-0.142669366235101, 0.14681495974829104, -0.08112045536567801, 0.09311980586702116, -0.08591523741515691, -0.1536709471924493, -0.017851008544519743, 0.3057959424331784, -0.24283183848285336, -0.2712161427601272, 0.08473865745039094, -0.2295779246030588, -0.11828063780773156, 0.16653986953373923, -0.05010204077166999,... |
706.3689 | Space-frequency correlation of classical waves in disordered media:
high-frequency and small scale asymptotics | Two-frequency radiative transfer (2f-RT) theory is developed for geometrical
optics in random media. The space-frequency correlation is described by the
two-frequency Wigner distribution (2f-WD) which satisfies a closed form
equation, the two-frequency Wigner-Moyal equation. In the RT regime it is
proved rigorously t... | physics.optics physics.gen-ph | twofrequency radiative transfer 2frt theory is developed for geometrical optics in random media the spacefrequency correlation is described by the twofrequency wigner distribution 2fwd which satisfies a closed form equation the twofrequency wignermoyal equation in the rt regime it is proved rigorously that 2fwd satisfi... | [['twofrequency', 'radiative', 'transfer', '2frt', 'theory', 'is', 'developed', 'for', 'geometrical', 'optics', 'in', 'random', 'media', 'the', 'spacefrequency', 'correlation', 'is', 'described', 'by', 'the', 'twofrequency', 'wigner', 'distribution', '2fwd', 'which', 'satisfies', 'a', 'closed', 'form', 'equation', 'the... | [-0.16265530855750687, 0.14381311709333336, -0.13201807495311238, 0.07944723222341933, -0.06456254334110516, -0.17271558340283089, -0.046895570023602735, 0.30963319036167825, -0.27478196873758615, -0.18243671124905683, 0.03530216669752734, -0.2688325643317062, -0.1570648631039128, 0.20586859267414287, 0.052449581998117... |
706.369 | Conceptual Explanation for the Algebra in the Noncommutative Approach to
the Standard Model | The purpose of this letter is to remove the arbitrariness of the ad hoc
choice of the algebra and its representation in the noncommutative approach to
the Standard Model, which was begging for a conceptual explanation. We assume
as before that space-time is the product of a four-dimensional manifold by a
finite nonco... | hep-th hep-ph | the purpose of this letter is to remove the arbitrariness of the ad hoc choice of the algebra and its representation in the noncommutative approach to the standard model which was begging for a conceptual explanation we assume as before that spacetime is the product of a fourdimensional manifold by a finite noncommmuta... | [['the', 'purpose', 'of', 'this', 'letter', 'is', 'to', 'remove', 'the', 'arbitrariness', 'of', 'the', 'ad', 'hoc', 'choice', 'of', 'the', 'algebra', 'and', 'its', 'representation', 'in', 'the', 'noncommutative', 'approach', 'to', 'the', 'standard', 'model', 'which', 'was', 'begging', 'for', 'a', 'conceptual', 'explana... | [-0.11360454159055619, 0.16148559317745745, -0.05831972504965961, 0.08296311007951326, -0.11556689883780448, -0.11878109851708397, 0.05510352142749632, 0.329353546699945, -0.23494253076929994, -0.33006650597015597, 0.07737036770546532, -0.24063136234007618, -0.06977602200622254, 0.12426360961089426, -0.0418847348223975... |
706.3691 | Slow crack growth in polycarbonate films | We study experimentally the slow growth of a single crack in polycarbonate
films submitted to uniaxial and constant imposed stress. The specificity of
fracture in polycarbonate films is the appearance of flame shaped macroscopic
process zones at the tips of the crack. Supported by an experimental study of
the mechani... | cond-mat.mtrl-sci physics.class-ph | we study experimentally the slow growth of a single crack in polycarbonate films submitted to uniaxial and constant imposed stress the specificity of fracture in polycarbonate films is the appearance of flame shaped macroscopic process zones at the tips of the crack supported by an experimental study of the mechanical ... | [['we', 'study', 'experimentally', 'the', 'slow', 'growth', 'of', 'a', 'single', 'crack', 'in', 'polycarbonate', 'films', 'submitted', 'to', 'uniaxial', 'and', 'constant', 'imposed', 'stress', 'the', 'specificity', 'of', 'fracture', 'in', 'polycarbonate', 'films', 'is', 'the', 'appearance', 'of', 'flame', 'shaped', 'ma... | [-0.13153523964272743, 0.14620273857171587, -0.10487950700894123, -0.05042572386259457, -0.023142626655667468, -0.07043139291151117, 0.034903694103747884, 0.391820991601519, -0.30658713949136046, -0.23776328072158825, 0.05751232392180504, -0.2645775844618954, -0.156554170414219, 0.20404955014991746, -0.0219599203361819... |
706.3692 | Next-to-Leading Order Shear Viscosity in lambda phi^4 Theory | We show that the shear viscosity of lambda phi^4 theory is sensitive at
next-to-leading order to soft physics, which gives rise to subleading
corrections suppressed by only a half power of the coupling, eta = [3033.54 +
1548.3 m_{th}/T] N T^3]/[ (N+2)/3 lambda^2], with m^2_th=(N+2)/72 lambda T^2.
The series appears t... | hep-ph | we show that the shear viscosity of lambda phi4 theory is sensitive at nexttoleading order to soft physics which gives rise to subleading corrections suppressed by only a half power of the coupling eta 303354 15483 m_tht n t3 n23 lambda2 with m2_thn272 lambda t2 the series appears to converge about as well or badly as ... | [['we', 'show', 'that', 'the', 'shear', 'viscosity', 'of', 'lambda', 'phi4', 'theory', 'is', 'sensitive', 'at', 'nexttoleading', 'order', 'to', 'soft', 'physics', 'which', 'gives', 'rise', 'to', 'subleading', 'corrections', 'suppressed', 'by', 'only', 'a', 'half', 'power', 'of', 'the', 'coupling', 'eta', '303354', '154... | [-0.14086116790738806, 0.1846954814370787, -0.07312115722156146, 0.07382039050367382, -0.07077595137321112, -0.17086071670545558, -0.024921253043749744, 0.2685595156396167, -0.2728654271432836, -0.2645935700029919, 0.05777409420299687, -0.35666617574660403, -0.0698571530734434, 0.13232735615926222, 0.035026156915384424... |
706.3693 | Relating Biophysical Properties Across Scales | A distinguishing feature of a multicellular living system is that it operates
at various scales, from the intracellular to organismal. Very little is known
at present on how tissue level properties are related to cell and subcellular
properties. Modern measurement techniques provide quantitative results at both
the i... | physics.bio-ph physics.comp-ph q-bio.CB q-bio.TO | a distinguishing feature of a multicellular living system is that it operates at various scales from the intracellular to organismal very little is known at present on how tissue level properties are related to cell and subcellular properties modern measurement techniques provide quantitative results at both the intrac... | [['a', 'distinguishing', 'feature', 'of', 'a', 'multicellular', 'living', 'system', 'is', 'that', 'it', 'operates', 'at', 'various', 'scales', 'from', 'the', 'intracellular', 'to', 'organismal', 'very', 'little', 'is', 'known', 'at', 'present', 'on', 'how', 'tissue', 'level', 'properties', 'are', 'related', 'to', 'cell... | [-0.04108600861736242, 0.12877370625876394, -0.09492746257291591, 0.07132405175160152, -0.03383816632417183, -0.10706335303273662, 0.020153072790247993, 0.3739609159529209, -0.2835480471741471, -0.27987084274659046, 0.0657763665451242, -0.2256820227866624, -0.24331741929343653, 0.17847251409130688, -0.04508751100665853... |
706.3694 | Status of the H1 Very Forward Proton Spectrometer | The Very Forward Proton Spectrometer (VFPS) of the H1 experiment at HERA is
collecting data since 2005. The fiber detectors in the Roman pots located at
218 and 222m downstream from the H1 interaction point, tag and measure
diffractively scattered protons with a high acceptance in the $\xpom$ range
[0.01, 0.025]. The... | physics.ins-det | the very forward proton spectrometer vfps of the h1 experiment at hera is collecting data since 2005 the fiber detectors in the roman pots located at 218 and 222m downstream from the h1 interaction point tag and measure diffractively scattered protons with a high acceptance in the xpom range 001 0025 the experimental s... | [['the', 'very', 'forward', 'proton', 'spectrometer', 'vfps', 'of', 'the', 'h1', 'experiment', 'at', 'hera', 'is', 'collecting', 'data', 'since', '2005', 'the', 'fiber', 'detectors', 'in', 'the', 'roman', 'pots', 'located', 'at', '218', 'and', '222m', 'downstream', 'from', 'the', 'h1', 'interaction', 'point', 'tag', 'a... | [-0.022309544212792232, 0.19015177649756274, -0.10719351136409071, 0.06919561024161353, -0.00953222049292231, -0.07906240629170602, 0.027804408654354622, 0.39325762432122574, -0.18327950942161345, -0.3855696408536987, 0.044100426542370216, -0.4349255200299988, 0.08888795048646304, 0.1960627365236481, 0.0341094928942080... |
706.3695 | Magnetism and local distortions near carbon impurity in $\gamma$-iron | Local perturbations of crystal and magnetic structure of $\gamma$-iron near
carbon interstitial impurity is investigated by {\it ab initio} electronic
structure calculations. It is shown that the carbon impurity creates locally a
region of ferromagnetic ordering with substantial tetragonal distortions.
Exchange integ... | cond-mat.mtrl-sci | local perturbations of crystal and magnetic structure of gammairon near carbon interstitial impurity is investigated by it ab initio electronic structure calculations it is shown that the carbon impurity creates locally a region of ferromagnetic ordering with substantial tetragonal distortions exchange integrals and so... | [['local', 'perturbations', 'of', 'crystal', 'and', 'magnetic', 'structure', 'of', 'gammairon', 'near', 'carbon', 'interstitial', 'impurity', 'is', 'investigated', 'by', 'it', 'ab', 'initio', 'electronic', 'structure', 'calculations', 'it', 'is', 'shown', 'that', 'the', 'carbon', 'impurity', 'creates', 'locally', 'a', ... | [-0.17903707586851916, 0.16818774446622062, -0.028510149382218773, 0.07365613746043609, -0.014070392127188159, -0.10086352051511197, 0.07351344657904456, 0.4598819332223543, -0.27828057042100063, -0.2638705285187338, 0.001514918220058923, -0.36170300779680553, -0.11407197523914592, 0.09563395124860108, 0.09775731212444... |
706.3696 | The Mellin transform and spectral properties of toric varieties | In this article we apply results of \cite{W} on the twisted Mellin transform
to problems in toric geometry. In particular we use these results to describe
the asymptotics of probability densities associated with the monomial
eigenstates, $z^k$, $k \in \ZZ^d$, in Bargmann space and prove an "upstairs"
version of the s... | math.SG | in this article we apply results of citew on the twisted mellin transform to problems in toric geometry in particular we use these results to describe the asymptotics of probability densities associated with the monomial eigenstates zk k in zzd in bargmann space and prove an upstairs version of the spectral density the... | [['in', 'this', 'article', 'we', 'apply', 'results', 'of', 'citew', 'on', 'the', 'twisted', 'mellin', 'transform', 'to', 'problems', 'in', 'toric', 'geometry', 'in', 'particular', 'we', 'use', 'these', 'results', 'to', 'describe', 'the', 'asymptotics', 'of', 'probability', 'densities', 'associated', 'with', 'the', 'mon... | [-0.10176594008066475, 0.05191084283443123, -0.11545551429528182, 0.09529643021492058, -0.014398857070873045, -0.04616354705689296, -0.005330835762497497, 0.3518119009645426, -0.24003985354498233, -0.19788907429407518, 0.08505247241007291, -0.2547889370471239, -0.1474389993674951, 0.2135053751001466, -0.146881436316730... |
706.3697 | Thermal electric effects and heat generation in polypyrrole coated PET
fabrics | Polypyrrole chemically synthesized on PET gives rise to textiles with a high
electric conductivity, suitable for several applications from antistatics to
electromagnetic interference shielding devices. Here, we discuss investigations
on thermal electric performances of the polypyrrole coated PET in a wide range
of te... | cond-mat.mtrl-sci | polypyrrole chemically synthesized on pet gives rise to textiles with a high electric conductivity suitable for several applications from antistatics to electromagnetic interference shielding devices here we discuss investigations on thermal electric performances of the polypyrrole coated pet in a wide range of tempera... | [['polypyrrole', 'chemically', 'synthesized', 'on', 'pet', 'gives', 'rise', 'to', 'textiles', 'with', 'a', 'high', 'electric', 'conductivity', 'suitable', 'for', 'several', 'applications', 'from', 'antistatics', 'to', 'electromagnetic', 'interference', 'shielding', 'devices', 'here', 'we', 'discuss', 'investigations', ... | [-0.10403932161660542, 0.15577367567927397, -0.01681876891794113, -0.07426263017091864, -0.07200742509807102, -0.18782479096598065, 0.050524807324668825, 0.4366179285570979, -0.24619853177752632, -0.2999534065870998, 0.021047949664464865, -0.34190534447463083, -0.08689689839061779, 0.32939542674172956, -0.0282226260796... |
706.3698 | On the nature of QPO in the tail of SGR giant flares | A model is presented for the quasiperiodic component of magnetar emission
during the tail phase of giant flares. The model invokes modulation of the
particle number density in the magnetosphere. The magnetospheric currents are
modulated by torsional motion of the surface and we calculate that the
amplitude of neutron... | astro-ph | a model is presented for the quasiperiodic component of magnetar emission during the tail phase of giant flares the model invokes modulation of the particle number density in the magnetosphere the magnetospheric currents are modulated by torsional motion of the surface and we calculate that the amplitude of neutron sta... | [['a', 'model', 'is', 'presented', 'for', 'the', 'quasiperiodic', 'component', 'of', 'magnetar', 'emission', 'during', 'the', 'tail', 'phase', 'of', 'giant', 'flares', 'the', 'model', 'invokes', 'modulation', 'of', 'the', 'particle', 'number', 'density', 'in', 'the', 'magnetosphere', 'the', 'magnetospheric', 'currents'... | [-0.14861682874515006, 0.19957199866058425, -0.07430580552343441, 0.09816811286905051, -0.0709412075660151, -0.04822909331921002, -0.01305933141797457, 0.3856265286712543, -0.2558665818413315, -0.30949583941989617, 0.06523790461638862, -0.24859612464256908, -0.060691338826132854, 0.23049234844561992, 0.0076897536282954... |
706.3699 | Inflation after WMAP3 | I discuss the current status of inflationary cosmology in light of the recent
WMAP 3-year data release. The basic predictions of inflation are all supported
by the data. Inflation also makes predictions which have not been well tested
by current data but can be by future experiments, most notably a deviation from
a s... | astro-ph hep-ph | i discuss the current status of inflationary cosmology in light of the recent wmap 3year data release the basic predictions of inflation are all supported by the data inflation also makes predictions which have not been well tested by current data but can be by future experiments most notably a deviation from a scalein... | [['i', 'discuss', 'the', 'current', 'status', 'of', 'inflationary', 'cosmology', 'in', 'light', 'of', 'the', 'recent', 'wmap', '3year', 'data', 'release', 'the', 'basic', 'predictions', 'of', 'inflation', 'are', 'all', 'supported', 'by', 'the', 'data', 'inflation', 'also', 'makes', 'predictions', 'which', 'have', 'not'... | [-0.14185591655656357, 0.1884020339836504, -0.0647138943916864, 0.1104261037279767, -0.11698098300786858, -0.14442648339847272, -0.026773522387851367, 0.2906148937107487, -0.2131543687089685, -0.3117207288869064, 0.1471793246063912, -0.28826113679361615, -0.0675178168468516, 0.22532401914411987, -0.008069118072109466, ... |
706.37 | Probing white dwarf interiors with LISA: periastron precession in double
white dwarfs | In globular clusters, dynamical interactions give rise to a population of
eccentric double white dwarfs detectable by the Laser Interferometer Space
Antenna (LISA) up to the Large Magellanic Cloud. In this Letter, we explore the
detectability of periastron precession in these systems with LISA. Unlike
previous invest... | astro-ph gr-qc | in globular clusters dynamical interactions give rise to a population of eccentric double white dwarfs detectable by the laser interferometer space antenna lisa up to the large magellanic cloud in this letter we explore the detectability of periastron precession in these systems with lisa unlike previous investigations... | [['in', 'globular', 'clusters', 'dynamical', 'interactions', 'give', 'rise', 'to', 'a', 'population', 'of', 'eccentric', 'double', 'white', 'dwarfs', 'detectable', 'by', 'the', 'laser', 'interferometer', 'space', 'antenna', 'lisa', 'up', 'to', 'the', 'large', 'magellanic', 'cloud', 'in', 'this', 'letter', 'we', 'explor... | [-0.18418930001629918, 0.16982366625840464, -0.05307303490767749, 0.08884223644945807, -0.12060666082235162, -0.02740206201583622, 0.09072394898234337, 0.3629078958183527, -0.2283855081243696, -0.31884933715028796, 0.00861668006879935, -0.2722016588200395, -0.10342310926895223, 0.2130275472551219, -0.06012327096187601,... |
706.3701 | Continuous variable quantum teleportation with non-Gaussian resources | We investigate continuous variable quantum teleportation using non-Gaussian
states of the radiation field as entangled resources. We compare the
performance of different classes of degaussified resources, including two-mode
photon-added and two-mode photon-subtracted squeezed states. We then introduce
a class of two-... | quant-ph | we investigate continuous variable quantum teleportation using nongaussian states of the radiation field as entangled resources we compare the performance of different classes of degaussified resources including twomode photonadded and twomode photonsubtracted squeezed states we then introduce a class of twomode squeez... | [['we', 'investigate', 'continuous', 'variable', 'quantum', 'teleportation', 'using', 'nongaussian', 'states', 'of', 'the', 'radiation', 'field', 'as', 'entangled', 'resources', 'we', 'compare', 'the', 'performance', 'of', 'different', 'classes', 'of', 'degaussified', 'resources', 'including', 'twomode', 'photonadded',... | [-0.125222380889037, 0.22307142258922416, -0.0862687290727489, 0.07882155376068485, 0.03792722174883124, -0.2249817738940162, 0.04527056618138972, 0.39794995764813085, -0.2327489352163558, -0.266392110502274, 0.013162350381988533, -0.24517493782286334, -0.06607309040268809, 0.22544843701675066, -0.05786815347648629, 0.... |
706.3702 | From Massive Cores to Massive Stars | The similarity between the mass and spatial distributions of pre-stellar gas
cores in star-forming clouds and young stars in clusters provides strong
circumstantial evidence that these gas cores are the direct progenitors of
individual stars. Here I describe a physical model for the evolution of massive
cores into st... | astro-ph | the similarity between the mass and spatial distributions of prestellar gas cores in starforming clouds and young stars in clusters provides strong circumstantial evidence that these gas cores are the direct progenitors of individual stars here i describe a physical model for the evolution of massive cores into stars s... | [['the', 'similarity', 'between', 'the', 'mass', 'and', 'spatial', 'distributions', 'of', 'prestellar', 'gas', 'cores', 'in', 'starforming', 'clouds', 'and', 'young', 'stars', 'in', 'clusters', 'provides', 'strong', 'circumstantial', 'evidence', 'that', 'these', 'gas', 'cores', 'are', 'the', 'direct', 'progenitors', 'o... | [-0.08352003817750557, 0.16051952794871546, -0.10437027896823715, 0.10227692862279898, -0.09202754099984184, 0.02168249092180251, 0.09730449451272152, 0.3963989940556613, -0.1697771724867673, -0.34231936266599605, 0.0077932770922010345, -0.22014848549462074, -0.03779592225712932, 0.13717996807430277, 0.0472823301857445... |
706.3703 | Loss of mass and stability of galaxies in MOND | The self-binding energy and stability of a galaxy in MOND-based gravity are
curiously decreasing functions of its center of mass acceleration towards
neighbouring mass concentrations. A tentative indication of this breaking of
the Strong Equivalence Principle in field galaxies is the RAVE-observed escape
speed in the... | astro-ph | the selfbinding energy and stability of a galaxy in mondbased gravity are curiously decreasing functions of its center of mass acceleration towards neighbouring mass concentrations a tentative indication of this breaking of the strong equivalence principle in field galaxies is the raveobserved escape speed in the milky... | [['the', 'selfbinding', 'energy', 'and', 'stability', 'of', 'a', 'galaxy', 'in', 'mondbased', 'gravity', 'are', 'curiously', 'decreasing', 'functions', 'of', 'its', 'center', 'of', 'mass', 'acceleration', 'towards', 'neighbouring', 'mass', 'concentrations', 'a', 'tentative', 'indication', 'of', 'this', 'breaking', 'of'... | [-0.15557389701551536, 0.15406502224255175, -0.08467741057089072, 0.1225011906770767, -0.10460323276721052, -0.09246584741961655, 0.03220286184692505, 0.39233083646299677, -0.14901373327584633, -0.3070792465456831, 0.033651715082832295, -0.27664517501626273, -0.01687473851019767, 0.19672375356208588, -0.043792227960286... |
706.3704 | Detectability of Exoplanetary Transits from Radial Velocity Surveys | Of the known transiting extra-solar planets, a few have been detected through
photometric follow-up observations of radial velocity planets. Perhaps the best
known of these is the transiting exoplanet HD 209458b. For hot Jupiters
(periods less than ~5 days), the a priori information that 10% of these planets
will tra... | astro-ph | of the known transiting extrasolar planets a few have been detected through photometric followup observations of radial velocity planets perhaps the best known of these is the transiting exoplanet hd 209458b for hot jupiters periods less than 5 days the a priori information that 10 of these planets will transit their p... | [['of', 'the', 'known', 'transiting', 'extrasolar', 'planets', 'a', 'few', 'have', 'been', 'detected', 'through', 'photometric', 'followup', 'observations', 'of', 'radial', 'velocity', 'planets', 'perhaps', 'the', 'best', 'known', 'of', 'these', 'is', 'the', 'transiting', 'exoplanet', 'hd', '209458b', 'for', 'hot', 'ju... | [-0.09265887886329302, 0.12304785035707809, -0.1243062805657484, 0.05157871280631451, -0.16854877667566848, -0.12257838177181363, 0.07141805689392403, 0.3776100931697847, -0.1809162498020924, -0.3455768106396475, 0.12933076799370644, -0.282472291496331, -0.07049149038649825, 0.24666884716460916, -0.11419293089338935, 0... |
706.3705 | A coverage independent method to analyze large scale anisotropies | The arrival time distribution of cosmic ray events is well suited to extract
information regarding sky anisotropies. For an experiment with nearly constant
exposure, the frequency resolution one can achieve is given by the inverse of
the time $T$ during which the data was recorded. For $T$ larger than one
calendar ye... | astro-ph | the arrival time distribution of cosmic ray events is well suited to extract information regarding sky anisotropies for an experiment with nearly constant exposure the frequency resolution one can achieve is given by the inverse of the time t during which the data was recorded for t larger than one calendar year the re... | [['the', 'arrival', 'time', 'distribution', 'of', 'cosmic', 'ray', 'events', 'is', 'well', 'suited', 'to', 'extract', 'information', 'regarding', 'sky', 'anisotropies', 'for', 'an', 'experiment', 'with', 'nearly', 'constant', 'exposure', 'the', 'frequency', 'resolution', 'one', 'can', 'achieve', 'is', 'given', 'by', 't... | [-0.10645663527210648, 0.12885468990815496, -0.11052599768393123, 0.09923988261233227, -0.09009930474582152, -0.07146266323382942, 0.022751456810137592, 0.38482337541734946, -0.2495214933087715, -0.330494054294645, 0.11510066218892089, -0.2629997123180007, -0.08333047576702367, 0.22562638574088803, -0.02951271738745093... |
706.3706 | Modeling the Dust Properties of z ~ 6 Quasars with ART^2 --
All-wavelength Radiative Transfer with Adaptive Refinement Tree | The detection of large quantities of dust in z ~ 6 quasars by infrared and
radio surveys presents puzzles for the formation and evolution of dust in these
early systems. Previously (Li et al. 2007), we showed that luminous quasars at
z > 6 can form through hierarchical mergers of gas-rich galaxies. Here, we
calculate... | astro-ph | the detection of large quantities of dust in z 6 quasars by infrared and radio surveys presents puzzles for the formation and evolution of dust in these early systems previously li et al 2007 we showed that luminous quasars at z 6 can form through hierarchical mergers of gasrich galaxies here we calculate the dust prop... | [['the', 'detection', 'of', 'large', 'quantities', 'of', 'dust', 'in', 'z', '6', 'quasars', 'by', 'infrared', 'and', 'radio', 'surveys', 'presents', 'puzzles', 'for', 'the', 'formation', 'and', 'evolution', 'of', 'dust', 'in', 'these', 'early', 'systems', 'previously', 'li', 'et', 'al', '2007', 'we', 'showed', 'that', ... | [-0.013091943373437972, 0.08500207202458114, -0.06701283069145575, 0.1303738937835442, -0.08569764970336109, -0.05188644565874711, 0.030733322895830497, 0.4514951319806278, -0.12286775378859602, -0.3323787303315476, 0.04778648646606598, -0.28884886897169054, -0.04758258118388767, 0.1572501100273439, 0.01232093289960175... |
706.3707 | Comparing powers and symbolic powers of ideals | We develop tools to study the problem of containment of symbolic powers
$I^{(m)}$ in powers $I^r$ for a homogeneous ideal $I$ in a polynomial ring
$k[{\bf P}^N]$ in $N+1$ variables over an algebraically closed field $k$. We
obtain results on the structure of the set of pairs $(r,m)$ such that
$I^{(m)}\subseteq I^r$. ... | math.AG math.AC | we develop tools to study the problem of containment of symbolic powers im in powers ir for a homogeneous ideal i in a polynomial ring kbf pn in n1 variables over an algebraically closed field k we obtain results on the structure of the set of pairs rm such that imsubseteq ir as corollaries we show that i2 contains i3 ... | [['we', 'develop', 'tools', 'to', 'study', 'the', 'problem', 'of', 'containment', 'of', 'symbolic', 'powers', 'im', 'in', 'powers', 'ir', 'for', 'a', 'homogeneous', 'ideal', 'i', 'in', 'a', 'polynomial', 'ring', 'kbf', 'pn', 'in', 'n1', 'variables', 'over', 'an', 'algebraically', 'closed', 'field', 'k', 'we', 'obtain',... | [-0.19519876363216945, 0.03864152576283916, -0.03830887567215037, 0.03329870291630562, -0.03196402508903774, -0.13240681632449575, 0.031165429676818377, 0.34181237217997856, -0.2827420803801258, -0.17409533077371445, 0.0820598711149011, -0.2877039527474432, -0.12219537748023868, 0.20500748603152905, -0.0688536760286603... |
706.3708 | The Bergman kernel and projection on non-smooth worm domains | This paper provides a precise asymptotic expansion for the Bergman kernel on
the non-smooth worm domains of Christer Kiselman in complex 2-space.
Applications are given to the failure of Condition R, to deviant boundary
behavior of the kernel, and to L^p mapping properties of the kernel.
| math.CV math.AP | this paper provides a precise asymptotic expansion for the bergman kernel on the nonsmooth worm domains of christer kiselman in complex 2space applications are given to the failure of condition r to deviant boundary behavior of the kernel and to lp mapping properties of the kernel | [['this', 'paper', 'provides', 'a', 'precise', 'asymptotic', 'expansion', 'for', 'the', 'bergman', 'kernel', 'on', 'the', 'nonsmooth', 'worm', 'domains', 'of', 'christer', 'kiselman', 'in', 'complex', '2space', 'applications', 'are', 'given', 'to', 'the', 'failure', 'of', 'condition', 'r', 'to', 'deviant', 'boundary', ... | [-0.14392838448933934, -0.012236264078756389, -0.1136081694908764, 0.08108026931902555, -0.1623652361576324, -0.08985207332095699, 0.01003477773780975, 0.3654648316619189, -0.285298343292316, -0.14854066750115674, 0.1834891590001264, -0.26433011731537787, -0.1739948448198645, 0.2113660122267902, -0.1071737952651861, 0.... |
706.3709 | The H-alpha stellar and interstellar emission in the open cluster NGC
6910 | We verify the nature of emission-line stars in the field of the open cluster
NGC 6910. % Spectroscopy in the H-alpha region was obtained. Raw CCD frames of
spectra of all stars fainter than V = 9 mag observed by us are significantly
affected by nebular emission originating in the surrounding HII region IC 1318.
After... | astro-ph | we verify the nature of emissionline stars in the field of the open cluster ngc 6910 spectroscopy in the halpha region was obtained raw ccd frames of spectra of all stars fainter than v 9 mag observed by us are significantly affected by nebular emission originating in the surrounding hii region ic 1318 after careful da... | [['we', 'verify', 'the', 'nature', 'of', 'emissionline', 'stars', 'in', 'the', 'field', 'of', 'the', 'open', 'cluster', 'ngc', '6910', 'spectroscopy', 'in', 'the', 'halpha', 'region', 'was', 'obtained', 'raw', 'ccd', 'frames', 'of', 'spectra', 'of', 'all', 'stars', 'fainter', 'than', 'v', '9', 'mag', 'observed', 'by', ... | [-0.027797640689338248, 0.028760469321791732, -0.08167293668368164, 0.05176086078992941, -0.10308720442512428, -0.10232084256274925, 0.06241767887848165, 0.4896201107214079, -0.11468116895088719, -0.30137903383468784, 0.023376574656454686, -0.3122098929950117, -0.02724168669535882, 0.2004163837998841, -0.10676217590563... |
706.371 | Optimal Constellations for the Low SNR Noncoherent MIMO Block Rayleigh
Fading Channel | Reliable communication over the discrete-input/continuous-output noncoherent
multiple-input multiple-output (MIMO) Rayleigh block fading channel is
considered when the signal-to-noise ratio (SNR) per degree of freedom is low.
Two key problems are posed and solved to obtain the optimum discrete input. In
both problems... | cs.IT math.IT | reliable communication over the discreteinputcontinuousoutput noncoherent multipleinput multipleoutput mimo rayleigh block fading channel is considered when the signaltonoise ratio snr per degree of freedom is low two key problems are posed and solved to obtain the optimum discrete input in both problems the average an... | [['reliable', 'communication', 'over', 'the', 'discreteinputcontinuousoutput', 'noncoherent', 'multipleinput', 'multipleoutput', 'mimo', 'rayleigh', 'block', 'fading', 'channel', 'is', 'considered', 'when', 'the', 'signaltonoise', 'ratio', 'snr', 'per', 'degree', 'of', 'freedom', 'is', 'low', 'two', 'key', 'problems', ... | [-0.20457699116008976, 0.06385561875610923, -0.011751451459195879, 0.05761845963230978, -0.055617307972990804, -0.18412680637091397, 0.04610209145376252, 0.36503299589372346, -0.30368069079394144, -0.3041470604845219, 0.1429606344587066, -0.27437196655923296, -0.1499343485550748, 0.1653549772252639, -0.0970010121497843... |
706.3711 | Point counting on reductions of CM elliptic curves | We give explicit formulas for the number of points on reductions of elliptic
curves with complex multiplication by any imaginary quadratic field. We also
find models for CM $\mathbf{Q}$-curves in certain cases. This generalizes
earlier results of Gross, Stark, and others.
| math.NT | we give explicit formulas for the number of points on reductions of elliptic curves with complex multiplication by any imaginary quadratic field we also find models for cm mathbfqcurves in certain cases this generalizes earlier results of gross stark and others | [['we', 'give', 'explicit', 'formulas', 'for', 'the', 'number', 'of', 'points', 'on', 'reductions', 'of', 'elliptic', 'curves', 'with', 'complex', 'multiplication', 'by', 'any', 'imaginary', 'quadratic', 'field', 'we', 'also', 'find', 'models', 'for', 'cm', 'mathbfqcurves', 'in', 'certain', 'cases', 'this', 'generalize... | [-0.1709340889705345, 0.048817965330090377, -0.058029495063237846, 0.06009116152708884, -0.063764952076599, -0.13507928429171442, 0.042214625730412084, 0.32802767110988496, -0.1898531740065664, -0.3080776478163898, 0.0526490197138628, -0.24038813161278086, -0.19619006984867154, 0.31834370009601115, -0.12158063234346628... |
706.3712 | Resonant and Near-Resonant Internal Wave Interactions | We report evaluations of a resonant kinetic equation that suggest the slow
time evolution of the Garrett and Munk spectrum is {\em not}, in fact, slow.
Instead nonlinear transfers lead to evolution time scales that are smaller than
one wave period at high vertical wavenumber. Such values of the transfer rates
are inc... | physics.flu-dyn physics.ao-ph | we report evaluations of a resonant kinetic equation that suggest the slow time evolution of the garrett and munk spectrum is em not in fact slow instead nonlinear transfers lead to evolution time scales that are smaller than one wave period at high vertical wavenumber such values of the transfer rates are inconsistent... | [['we', 'report', 'evaluations', 'of', 'a', 'resonant', 'kinetic', 'equation', 'that', 'suggest', 'the', 'slow', 'time', 'evolution', 'of', 'the', 'garrett', 'and', 'munk', 'spectrum', 'is', 'em', 'not', 'in', 'fact', 'slow', 'instead', 'nonlinear', 'transfers', 'lead', 'to', 'evolution', 'time', 'scales', 'that', 'are... | [-0.16286243782919232, 0.13785436515081528, -0.08413994065995212, 0.10116189055198836, -0.07455659722576716, -0.10010064485582656, 0.03278655331502835, 0.3105773113035996, -0.27812577000752625, -0.30183445181631086, 0.06068897122479809, -0.2885825459462857, -0.0761827894686056, 0.18313552918646434, -0.00493847540097444... |
706.3713 | Lubrication effects on the flow of wet granular materials | We investigate the dynamics of a partially saturated grain-liquid mixture
with a rotating drum apparatus. The drum is partially filled with the mixture
and then rotated about its horizontal axis. We focus on the continous
avalanching regime and measure the impact of volume fraction and viscosity of
the liquid on the ... | cond-mat.soft | we investigate the dynamics of a partially saturated grainliquid mixture with a rotating drum apparatus the drum is partially filled with the mixture and then rotated about its horizontal axis we focus on the continous avalanching regime and measure the impact of volume fraction and viscosity of the liquid on the dynam... | [['we', 'investigate', 'the', 'dynamics', 'of', 'a', 'partially', 'saturated', 'grainliquid', 'mixture', 'with', 'a', 'rotating', 'drum', 'apparatus', 'the', 'drum', 'is', 'partially', 'filled', 'with', 'the', 'mixture', 'and', 'then', 'rotated', 'about', 'its', 'horizontal', 'axis', 'we', 'focus', 'on', 'the', 'contin... | [-0.13190257753250978, 0.21757050623711505, -0.0661029301485733, -0.015949203340712478, -0.03720983136200199, -0.08227524031579973, 0.06114163897163643, 0.3585833815629022, -0.2841527900054005, -0.3305182563663836, 0.11513407430706861, -0.2919113143232831, -0.0755796714615055, 0.16870175361087306, -0.06370341759011672,... |
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