id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.2935 | An Extension to an Algebraic Method for Linear Time-Invariant System and
Network Theory: The full AC-Calculus | Being inspired by phasor analysis in linear circuit theory, and its algebraic
counterpart - the AC-(operational)-calculus for sinusoids developed by W.
Marten and W. Mathis - we define a complex structure on several spaces of
real-valued elementary functions. This is used to algebraize inhomogeneous
linear ordinary d... | math.CA cs.SC | being inspired by phasor analysis in linear circuit theory and its algebraic counterpart the acoperationalcalculus for sinusoids developed by w marten and w mathis we define a complex structure on several spaces of realvalued elementary functions this is used to algebraize inhomogeneous linear ordinary differential equ... | [['being', 'inspired', 'by', 'phasor', 'analysis', 'in', 'linear', 'circuit', 'theory', 'and', 'its', 'algebraic', 'counterpart', 'the', 'acoperationalcalculus', 'for', 'sinusoids', 'developed', 'by', 'w', 'marten', 'and', 'w', 'mathis', 'we', 'define', 'a', 'complex', 'structure', 'on', 'several', 'spaces', 'of', 'rea... | [-0.11405011817618314, 0.0661162159341794, -0.09966854662842937, 0.09187835406289617, -0.11119931084520893, -0.12659000872926257, 0.004996896504229908, 0.314250924555001, -0.3422837548736316, -0.25666795062151415, 0.104468455923888, -0.2522480922348019, -0.20122802115841282, 0.23123514460427547, -0.05848077480305931, 0... |
709.2936 | Bayesian Classification and Regression with High Dimensional Features | This thesis responds to the challenges of using a large number, such as
thousands, of features in regression and classification problems.
There are two situations where such high dimensional features arise. One is
when high dimensional measurements are available, for example, gene expression
data produced by microa... | stat.ML | this thesis responds to the challenges of using a large number such as thousands of features in regression and classification problems there are two situations where such high dimensional features arise one is when high dimensional measurements are available for example gene expression data produced by microarray techn... | [['this', 'thesis', 'responds', 'to', 'the', 'challenges', 'of', 'using', 'a', 'large', 'number', 'such', 'as', 'thousands', 'of', 'features', 'in', 'regression', 'and', 'classification', 'problems', 'there', 'are', 'two', 'situations', 'where', 'such', 'high', 'dimensional', 'features', 'arise', 'one', 'is', 'when', '... | [-0.045990633284375866, 0.07383766776703773, -0.04864021662692044, 0.08701548172666275, -0.07444767479963126, -0.1654380426979921, 0.03297805670460567, 0.3900644363558039, -0.278416860279964, -0.3382420200715832, 0.13778840811833978, -0.3008889477382949, -0.17151514294240228, 0.20884422491765284, -0.0599540247839499, 0... |
709.2937 | Theory of current-driven magnetization dynamics in inhomogeneous
ferromagnets | We give a brief account of recent developments in the theoretical
understanding of the interaction between electric currents and inhomogeneous
ferromagnetic order parameters. We start by discussing the physical origin of
the spin torques responsible for this interaction and construct a
phenomenological description. W... | cond-mat.mes-hall | we give a brief account of recent developments in the theoretical understanding of the interaction between electric currents and inhomogeneous ferromagnetic order parameters we start by discussing the physical origin of the spin torques responsible for this interaction and construct a phenomenological description we th... | [['we', 'give', 'a', 'brief', 'account', 'of', 'recent', 'developments', 'in', 'the', 'theoretical', 'understanding', 'of', 'the', 'interaction', 'between', 'electric', 'currents', 'and', 'inhomogeneous', 'ferromagnetic', 'order', 'parameters', 'we', 'start', 'by', 'discussing', 'the', 'physical', 'origin', 'of', 'the'... | [-0.21012169769389577, 0.1856925814292195, -0.033062259645693086, 0.0428054020256118, -0.136738522501474, -0.06548420957739601, 0.006668791760889332, 0.33568717696274936, -0.24055582039016352, -0.26865987487011744, 0.024910008092018453, -0.21900397112718625, -0.14366161529225915, 0.18484097980015146, 0.0632754521878708... |
709.2938 | Near linear time algorithm to detect community structures in large-scale
networks | Community detection and analysis is an important methodology for
understanding the organization of various real-world networks and has
applications in problems as diverse as consensus formation in social
communities or the identification of functional modules in biochemical
networks. Currently used algorithms that id... | physics.soc-ph | community detection and analysis is an important methodology for understanding the organization of various realworld networks and has applications in problems as diverse as consensus formation in social communities or the identification of functional modules in biochemical networks currently used algorithms that identi... | [['community', 'detection', 'and', 'analysis', 'is', 'an', 'important', 'methodology', 'for', 'understanding', 'the', 'organization', 'of', 'various', 'realworld', 'networks', 'and', 'has', 'applications', 'in', 'problems', 'as', 'diverse', 'as', 'consensus', 'formation', 'in', 'social', 'communities', 'or', 'the', 'id... | [-0.10378823191453905, 0.013302922745029007, -0.05829000397858655, 0.07743716751117616, -0.12512639974264186, -0.14599950631173156, 0.05888884988709596, 0.45981578567348746, -0.28779269705853, -0.322663300761791, 0.11470700611117417, -0.24658862052392974, -0.24517461593875298, 0.14546133630210534, -0.04248998209874591,... |
709.2939 | NICMOS Observations of Shocked H_2 in Orion | HST NICMOS narrowband images of the shocked molecular hydrogen emission in
OMC-1 are analyzed to reveal new information on the BN/KL outflow. The
outstanding morphological feature of this region is the array of molecular
hydrogen ``fingers'' emanating from the general vicinity of IRc2 and the
presence of several Herb... | astro-ph | hst nicmos narrowband images of the shocked molecular hydrogen emission in omc1 are analyzed to reveal new information on the bnkl outflow the outstanding morphological feature of this region is the array of molecular hydrogen fingers emanating from the general vicinity of irc2 and the presence of several herbigharo ob... | [['hst', 'nicmos', 'narrowband', 'images', 'of', 'the', 'shocked', 'molecular', 'hydrogen', 'emission', 'in', 'omc1', 'are', 'analyzed', 'to', 'reveal', 'new', 'information', 'on', 'the', 'bnkl', 'outflow', 'the', 'outstanding', 'morphological', 'feature', 'of', 'this', 'region', 'is', 'the', 'array', 'of', 'molecular'... | [-0.03588331006765843, 0.06667417361377141, 0.0010509040708152147, 0.025948756463968985, -0.02699184266802592, -0.0854455568956044, 0.02019074871383894, 0.4651481942393077, -0.16388382192951842, -0.36814172138006257, 0.07320348518088651, -0.29629751438609303, 0.008388806535647466, 0.1765412569905703, 0.0293796184608557... |
709.294 | Spin-dependent tunneling and Coulomb blockade in ferromagnetic
nanoparticles | We review studies on spin-dependent tunneling phenomena in systems containing
ferromagnetic nanoparticles. We discuss preparation methods of assembling
nanoparticles as well as the mechanisms and results of spin-dependent transport
properties. The emphasis of this review is on characteristic spin-dependent
tunneling ... | cond-mat.mtrl-sci cond-mat.mes-hall | we review studies on spindependent tunneling phenomena in systems containing ferromagnetic nanoparticles we discuss preparation methods of assembling nanoparticles as well as the mechanisms and results of spindependent transport properties the emphasis of this review is on characteristic spindependent tunneling phenome... | [['we', 'review', 'studies', 'on', 'spindependent', 'tunneling', 'phenomena', 'in', 'systems', 'containing', 'ferromagnetic', 'nanoparticles', 'we', 'discuss', 'preparation', 'methods', 'of', 'assembling', 'nanoparticles', 'as', 'well', 'as', 'the', 'mechanisms', 'and', 'results', 'of', 'spindependent', 'transport', 'p... | [-0.20099290472510925, 0.14467389452785476, -0.002228109944444984, 0.07286766063727772, -0.023272967428219184, -0.14796451655730827, 0.06419506305898193, 0.3825944703795127, -0.2561364346531345, -0.3280033572618641, -0.041128793924199, -0.31346270179292607, -0.2023165154534934, 0.2537072154679405, -0.005440248920123523... |
709.2941 | The p-harmonic boundary for finitely generated groups and the first
reduced \ell_p-cohomology | Let $p$ be a real number greater than one and let $G$ be a finitely
generated, infinite group. In this paper we introduce the $p$-harmonic boundary
of $G$. We then characterize the vanishing of the first reduced
$\ell^p$-cohomology of $G$ in terms of the cardinality of this boundary. Some
properties of $p$-harmonic b... | math.FA math.GR | let p be a real number greater than one and let g be a finitely generated infinite group in this paper we introduce the pharmonic boundary of g we then characterize the vanishing of the first reduced ellpcohomology of g in terms of the cardinality of this boundary some properties of pharmonic boundaries that are preser... | [['let', 'p', 'be', 'a', 'real', 'number', 'greater', 'than', 'one', 'and', 'let', 'g', 'be', 'a', 'finitely', 'generated', 'infinite', 'group', 'in', 'this', 'paper', 'we', 'introduce', 'the', 'pharmonic', 'boundary', 'of', 'g', 'we', 'then', 'characterize', 'the', 'vanishing', 'of', 'the', 'first', 'reduced', 'ellpco... | [-0.18930937641210133, 0.14839504482675223, -0.09881569350999529, 0.013403111275145284, -0.08944025514547223, -0.0737671631648736, 0.0021115980444035383, 0.365396287968202, -0.32393568994537475, -0.24523235381811218, 0.10150119349090082, -0.2727565928712808, -0.13935131932138115, 0.18570675954888624, -0.115059695326753... |
709.2942 | Conformal Enhancement of Holographic Scaling in Black Hole
Thermodynamics: A Near-Horizon Heat-Kernel Framework | Standard thermodynamic treatments of quantum field theory in the presence of
black-hole backgrounds reproduce the black hole entropy by usually specializing
to the leading order of the heat-kernel or the high-temperature expansion. By
contrast, this work develops a hybrid framework centered on geometric spectral
asym... | hep-th gr-qc math-ph math.MP quant-ph | standard thermodynamic treatments of quantum field theory in the presence of blackhole backgrounds reproduce the black hole entropy by usually specializing to the leading order of the heatkernel or the hightemperature expansion by contrast this work develops a hybrid framework centered on geometric spectral asymptotics... | [['standard', 'thermodynamic', 'treatments', 'of', 'quantum', 'field', 'theory', 'in', 'the', 'presence', 'of', 'blackhole', 'backgrounds', 'reproduce', 'the', 'black', 'hole', 'entropy', 'by', 'usually', 'specializing', 'to', 'the', 'leading', 'order', 'of', 'the', 'heatkernel', 'or', 'the', 'hightemperature', 'expans... | [-0.099599242904956, 0.10202278295176083, -0.12929983599257938, 0.08888380001253302, -0.07023783970959066, -0.13710088992826222, 0.02325397489063986, 0.2367878874784775, -0.2070495197287855, -0.24929653836435148, 0.11505721901213813, -0.2949201910850707, -0.12168089394286613, 0.15468958999407006, -0.08841957688708318, ... |
709.2943 | On Birnbaum-Saunders Inference | The Birnbaum-Saunders distribution, also known as the fatigue-life
distribution, is frequently used in reliability studies. We obtain adjustments
to the Birnbaum--Saunders profile likelihood function. The modified versions of
the likelihood function were obtained for both the shape and scale parameters,
i.e., we take... | stat.ME math.ST stat.TH | the birnbaumsaunders distribution also known as the fatiguelife distribution is frequently used in reliability studies we obtain adjustments to the birnbaumsaunders profile likelihood function the modified versions of the likelihood function were obtained for both the shape and scale parameters ie we take the shape par... | [['the', 'birnbaumsaunders', 'distribution', 'also', 'known', 'as', 'the', 'fatiguelife', 'distribution', 'is', 'frequently', 'used', 'in', 'reliability', 'studies', 'we', 'obtain', 'adjustments', 'to', 'the', 'birnbaumsaunders', 'profile', 'likelihood', 'function', 'the', 'modified', 'versions', 'of', 'the', 'likeliho... | [-0.061697088378695725, 0.020935093124277573, -0.11848688730222975, 0.11426715864949327, -0.08187253806082641, -0.14227633457381855, 0.05134770415541542, 0.3986045176332647, -0.23235837603485918, -0.35314770169801424, 0.14100971998943185, -0.24632251410456224, -0.11644812474863972, 0.19477339253765855, -0.0592454042613... |
709.2944 | On the state space geometry of the Kuramoto-Sivashinsky flow in a
periodic domain | The continuous and discrete symmetries of the Kuramoto-Sivashinsky system
restricted to a spatially periodic domain play a prominent role in shaping the
invariant sets of its chaotic dynamics. The continuous spatial translation
symmetry leads to relative equilibrium (traveling wave) and relative periodic
orbit (modul... | nlin.CD | the continuous and discrete symmetries of the kuramotosivashinsky system restricted to a spatially periodic domain play a prominent role in shaping the invariant sets of its chaotic dynamics the continuous spatial translation symmetry leads to relative equilibrium traveling wave and relative periodic orbit modulated tr... | [['the', 'continuous', 'and', 'discrete', 'symmetries', 'of', 'the', 'kuramotosivashinsky', 'system', 'restricted', 'to', 'a', 'spatially', 'periodic', 'domain', 'play', 'a', 'prominent', 'role', 'in', 'shaping', 'the', 'invariant', 'sets', 'of', 'its', 'chaotic', 'dynamics', 'the', 'continuous', 'spatial', 'translatio... | [-0.2265843372560561, 0.13946560728973487, -0.10564431340234089, 0.07385406658743575, -0.06612252783850722, -0.12390526876177839, 0.01115657331857143, 0.3483496920671314, -0.3532540862160247, -0.21816362551735005, 0.1146249938749298, -0.21679789440739633, -0.19157789472679032, 0.1312028125366418, -0.04280530370860582, ... |
709.2945 | A Simple Model of Direct Gauge Mediation of Metastable Supersymmetry
Breaking | We construct a model of direct gauge mediation of metastable SUSY breaking by
simply deforming the Intriligator, Seiberg and Shih model in terms of a dual
meson superpotential mass term. No extra matter field is introduced. The
deformation explicitly breaks a U(1)_R symmetry and a pseudo moduli have a
nonzero VEV at ... | hep-ph | we construct a model of direct gauge mediation of metastable susy breaking by simply deforming the intriligator seiberg and shih model in terms of a dual meson superpotential mass term no extra matter field is introduced the deformation explicitly breaks a u1_r symmetry and a pseudo moduli have a nonzero vev at oneloop... | [['we', 'construct', 'a', 'model', 'of', 'direct', 'gauge', 'mediation', 'of', 'metastable', 'susy', 'breaking', 'by', 'simply', 'deforming', 'the', 'intriligator', 'seiberg', 'and', 'shih', 'model', 'in', 'terms', 'of', 'a', 'dual', 'meson', 'superpotential', 'mass', 'term', 'no', 'extra', 'matter', 'field', 'is', 'in... | [-0.15045090335583414, 0.2775567913028811, -0.07971893006054286, 0.1656147528078041, -0.1423121577328337, -0.18088672281841614, 0.016096479721974383, 0.3063380811425824, -0.22690416051773354, -0.28767107650803936, 0.07191797363962646, -0.20887543380792653, -0.13027137649727852, 0.03456699720741848, -0.03371401255883809... |
709.2946 | The relationships between Invertible Module Maps X and X_z | If $R$ and $M$ are Hilbert modules (in the sense of R. G. Douglas and V. I.
Paulsen), we study the relationship between invertible module maps $X:R\to{M}$
and $X_{z}:R/R_{z}\to{M/M_{z}}$. In particular, for quasi-free Hilbert modules
$R$ and $M$, we provide a condition of a module map $X:R\to{M}$, such that if
$X_{z}... | math.FA math.OA | if r and m are hilbert modules in the sense of r g douglas and v i paulsen we study the relationship between invertible module maps xrtom and x_zrr_ztomm_z in particular for quasifree hilbert modules r and m we provide a condition of a module map xrtom such that if x_zrr_ztomm_z is invertible for every z in a domain om... | [['if', 'r', 'and', 'm', 'are', 'hilbert', 'modules', 'in', 'the', 'sense', 'of', 'r', 'g', 'douglas', 'and', 'v', 'i', 'paulsen', 'we', 'study', 'the', 'relationship', 'between', 'invertible', 'module', 'maps', 'xrtom', 'and', 'x_zrr_ztomm_z', 'in', 'particular', 'for', 'quasifree', 'hilbert', 'modules', 'r', 'and', '... | [-0.18504483487743598, 0.0648160881541956, -0.055920556316582055, 0.016232885080031477, -0.037396005942271306, -0.20452048699013314, -0.016198656278160903, 0.4289864753301327, -0.35705956048690357, -0.13508850452131949, 0.1105259180570451, -0.25914557705131863, -0.17341813505269013, 0.16996980792878624, -0.090543430807... |
709.2947 | Sums of Products of Bernoulli numbers of the second kind | The Bernoulli numbers b_0,b_1,b_2,.... of the second kind are defined by
\sum_{n=0}^\infty b_nt^n=\frac{t}{\log(1+t)}. In this paper, we give an
explicit formula for the sum \sum_{j_1+j_2+...+j_N=n,
j_1,j_2,...,j_N>=0}b_{j_1}b_{j_2}...b_{j_N}. We also establish a q-analogue for
\sum_{k=0}^n b_kb_{n-k}=-(n-1)b_n-(n-2)... | math.NT math.CO | the bernoulli numbers b_0b_1b_2 of the second kind are defined by sum_n0infty b_ntnfractlog1t in this paper we give an explicit formula for the sum sum_j_1j_2j_nn j_1j_2j_n0b_j_1b_j_2b_j_n we also establish a qanalogue for sum_k0n b_kb_nkn1b_nn2b_n1 | [['the', 'bernoulli', 'numbers', 'b_0b_1b_2', 'of', 'the', 'second', 'kind', 'are', 'defined', 'by', 'sum_n0infty', 'b_ntnfractlog1t', 'in', 'this', 'paper', 'we', 'give', 'an', 'explicit', 'formula', 'for', 'the', 'sum', 'sum_j_1j_2j_nn', 'j_1j_2j_n0b_j_1b_j_2b_j_n', 'we', 'also', 'establish', 'a', 'qanalogue', 'for',... | [-0.19511889865429238, 0.07770504788465493, -0.05054355139747776, 0.08477451910409306, -0.07813265697291956, -0.06674739029579635, 0.06688124012474998, 0.27314305071044587, -0.2834490070055271, -0.21144243894979872, 0.05987979424715941, -0.24130560761189151, -0.2236042565441337, 0.24900634432661123, -0.1143847697831947... |
709.2948 | The Contribution of the Cosmological Constant to the Relativistic
Bending of Light Revisited | We study the effect of the cosmological constant $\Lambda$ on the bending of
light by a concentrated spherically symmetric mass. Contrarily to previous
claims, we show that when the Schwarzschild-de Sitter geometry is taken into
account, $\Lambda$ does indeed contribute to the bending.
| astro-ph gr-qc hep-th | we study the effect of the cosmological constant lambda on the bending of light by a concentrated spherically symmetric mass contrarily to previous claims we show that when the schwarzschildde sitter geometry is taken into account lambda does indeed contribute to the bending | [['we', 'study', 'the', 'effect', 'of', 'the', 'cosmological', 'constant', 'lambda', 'on', 'the', 'bending', 'of', 'light', 'by', 'a', 'concentrated', 'spherically', 'symmetric', 'mass', 'contrarily', 'to', 'previous', 'claims', 'we', 'show', 'that', 'when', 'the', 'schwarzschildde', 'sitter', 'geometry', 'is', 'taken'... | [-0.13459370923120267, 0.12851464250233285, -0.1081873019832338, 0.07945464509485159, -0.12828353102600507, -0.10761009172947947, -0.030538708404746165, 0.36744575644301813, -0.1767833124586316, -0.22794992805913436, 0.028616359955522905, -0.26736761231062023, -0.09654522197710913, 0.14681116753626008, -0.0467149388954... |
709.2949 | Metallicity and mean age across M33 | New wide-field near-infrared (NIR) imaging observations of M33 were obtained
from UKIRT. These show a large population of intermediate-age stars
considerably improving on previous NIR data. The spatial distribution of super
giant stars, carbon-rich (C-rich or C stars) and oxygen-rich (O-rich or M
stars) asymptotic gi... | astro-ph | new widefield nearinfrared nir imaging observations of m33 were obtained from ukirt these show a large population of intermediateage stars considerably improving on previous nir data the spatial distribution of super giant stars carbonrich crich or c stars and oxygenrich orich or m stars asymptotic giant branch agb sta... | [['new', 'widefield', 'nearinfrared', 'nir', 'imaging', 'observations', 'of', 'm33', 'were', 'obtained', 'from', 'ukirt', 'these', 'show', 'a', 'large', 'population', 'of', 'intermediateage', 'stars', 'considerably', 'improving', 'on', 'previous', 'nir', 'data', 'the', 'spatial', 'distribution', 'of', 'super', 'giant',... | [0.03377355438072321, 0.07634494610693912, -0.13785569015673774, 0.09719439682572387, -0.1474897611756311, -0.01735004722573903, 0.11956955334388239, 0.4777154313660292, -0.10554043398452598, -0.381826053173173, 0.027794053994638974, -0.2834116903805109, -0.001414088586475267, 0.1543701541079425, -0.12482617806025975, ... |
709.295 | Propagation of a quantum particle through two dimensional percolating
systems | We study quantum percolation which is described by a tight-binding
Hamiltonian containing only off-diagonal hopping terms that are generally in
quenched binary disorder (zero or one). In such a system, transmission of a
quantum particle is determined by the disorder and interference effects,
leading to interesting sh... | cond-mat.dis-nn cond-mat.stat-mech | we study quantum percolation which is described by a tightbinding hamiltonian containing only offdiagonal hopping terms that are generally in quenched binary disorder zero or one in such a system transmission of a quantum particle is determined by the disorder and interference effects leading to interesting sharp featu... | [['we', 'study', 'quantum', 'percolation', 'which', 'is', 'described', 'by', 'a', 'tightbinding', 'hamiltonian', 'containing', 'only', 'offdiagonal', 'hopping', 'terms', 'that', 'are', 'generally', 'in', 'quenched', 'binary', 'disorder', 'zero', 'or', 'one', 'in', 'such', 'a', 'system', 'transmission', 'of', 'a', 'quan... | [-0.15883544866561092, 0.1851737731533144, -0.08265788208370153, 0.0386111322928182, 0.005402236131533068, -0.15759575385505295, 0.07347781316267935, 0.35948659466313465, -0.247348695905518, -0.25917978893385785, 0.10881066666108233, -0.29442238156465167, -0.15659383680239053, 0.17949471913209203, 0.01046358865486192, ... |
709.2951 | The population of AM CVn stars from the Sloan Digital Sky Survey | The AM Canum Venaticorum stars are rare interacting white dwarf binaries,
whose formation and evolution are still poorly known. The Sloan Digital Sky
Survey provides, for the first time, a sample of 6 AM CVn stars (out of a total
population of 18) that is sufficiently homogeneous that we can start to study
the popula... | astro-ph | the am canum venaticorum stars are rare interacting white dwarf binaries whose formation and evolution are still poorly known the sloan digital sky survey provides for the first time a sample of 6 am cvn stars out of a total population of 18 that is sufficiently homogeneous that we can start to study the population in ... | [['the', 'am', 'canum', 'venaticorum', 'stars', 'are', 'rare', 'interacting', 'white', 'dwarf', 'binaries', 'whose', 'formation', 'and', 'evolution', 'are', 'still', 'poorly', 'known', 'the', 'sloan', 'digital', 'sky', 'survey', 'provides', 'for', 'the', 'first', 'time', 'a', 'sample', 'of', '6', 'am', 'cvn', 'stars', ... | [-0.05924621131413094, 0.16421962319210748, -0.04658831103053701, 0.1282784557069379, -0.10077243415653948, -0.1010713155033082, 0.07271939825230633, 0.3649959062657705, -0.18548122166496953, -0.3458521764240856, 0.10284015689020583, -0.28223993545170967, -0.08270684739090199, 0.22541735634137686, -0.06754317144272713,... |
709.2952 | Non-equilibrium microtubule fluctuations in a model cytoskeleton | Biological activity gives rise to non-equilibrium fluctuations in the
cytoplasm of cells; however, there are few methods to directly measure these
fluctuations. Using a reconstituted actin cytoskeleton, we show that the
bending dynamics of embedded microtubules can be used to probe local stress
fluctuations. We add m... | cond-mat.soft cond-mat.stat-mech q-bio.SC | biological activity gives rise to nonequilibrium fluctuations in the cytoplasm of cells however there are few methods to directly measure these fluctuations using a reconstituted actin cytoskeleton we show that the bending dynamics of embedded microtubules can be used to probe local stress fluctuations we add myosin mo... | [['biological', 'activity', 'gives', 'rise', 'to', 'nonequilibrium', 'fluctuations', 'in', 'the', 'cytoplasm', 'of', 'cells', 'however', 'there', 'are', 'few', 'methods', 'to', 'directly', 'measure', 'these', 'fluctuations', 'using', 'a', 'reconstituted', 'actin', 'cytoskeleton', 'we', 'show', 'that', 'the', 'bending',... | [-0.16046957525521002, 0.21759258217232477, -0.09007155428501382, 0.02976566030049761, -0.01620731629088692, -0.1145540839435811, -0.004269980188544797, 0.38826487720783415, -0.3228152674761997, -0.23136166226247262, -0.018361829593242413, -0.2632692914493596, -0.26578272326753055, 0.16873360206319513, -0.0420524862156... |
709.2953 | Quantum Entanglement Capacity with Classical Feedback | For any quantum discrete memoryless channel, we define a quantity called
quantum entanglement capacity with classical feedback ($E_B$), and we show that
this quantity lies between two other well-studied quantities. These two
quantities - namely the quantum capacity assisted by two-way classical
communication ($Q_2$) ... | quant-ph | for any quantum discrete memoryless channel we define a quantity called quantum entanglement capacity with classical feedback e_b and we show that this quantity lies between two other wellstudied quantities these two quantities namely the quantum capacity assisted by twoway classical communication q_2 and the quantum c... | [['for', 'any', 'quantum', 'discrete', 'memoryless', 'channel', 'we', 'define', 'a', 'quantity', 'called', 'quantum', 'entanglement', 'capacity', 'with', 'classical', 'feedback', 'e_b', 'and', 'we', 'show', 'that', 'this', 'quantity', 'lies', 'between', 'two', 'other', 'wellstudied', 'quantities', 'these', 'two', 'quan... | [-0.1502208870683599, 0.16323566899292286, -0.10389193318485056, 0.06397157926848303, -0.010696901932872658, -0.3142337666853413, 0.107229422960054, 0.3505821252540912, -0.30703049764119167, -0.24260296153358227, 0.07239725811641007, -0.21543186117890123, -0.12830382788317385, 0.25901571421888825, -0.10906832864015831,... |
709.2954 | The long-period AM CVn star SDSS J155252.48+320150.9 | The Sloan Digital Sky Survey has been instrumental in obtaining a homogeneous
sample of the rare AM CVn stars: mass-transferring binary white dwarfs. As part
of a campaign of spectroscopic follow-up on candidate AM CVn stars from the
Sloan Digital Sky Survey, we have obtained time-resolved spectra of the g=20.2
candi... | astro-ph | the sloan digital sky survey has been instrumental in obtaining a homogeneous sample of the rare am cvn stars masstransferring binary white dwarfs as part of a campaign of spectroscopic followup on candidate am cvn stars from the sloan digital sky survey we have obtained timeresolved spectra of the g202 candidate sdss ... | [['the', 'sloan', 'digital', 'sky', 'survey', 'has', 'been', 'instrumental', 'in', 'obtaining', 'a', 'homogeneous', 'sample', 'of', 'the', 'rare', 'am', 'cvn', 'stars', 'masstransferring', 'binary', 'white', 'dwarfs', 'as', 'part', 'of', 'a', 'campaign', 'of', 'spectroscopic', 'followup', 'on', 'candidate', 'am', 'cvn'... | [-0.09107468388350584, 0.12419601315263414, -0.047517375941340305, 0.03942684154986337, -0.1441650630272541, -0.08215213289301958, 0.1223126099272103, 0.3685331163308631, -0.13809278576164363, -0.3224073152547491, 0.07062675743831859, -0.3482504382527904, -0.028143234064888938, 0.232788083065522, -0.07655665404211308, ... |
709.2955 | Baryonic Acoustic Oscillations in 21cm Emission: A Probe of Dark Energy
out to High Redshifts | Low-frequency observatories are currently being constructed with the goal of
detecting redshifted 21cm emission from the epoch of reionization. These
observatories will also be able to detect intensity fluctuations in the
cumulative 21cm emission after reionization, from hydrogen in unresolved damped
Ly-alpha absorbe... | astro-ph | lowfrequency observatories are currently being constructed with the goal of detecting redshifted 21cm emission from the epoch of reionization these observatories will also be able to detect intensity fluctuations in the cumulative 21cm emission after reionization from hydrogen in unresolved damped lyalpha absorbers suc... | [['lowfrequency', 'observatories', 'are', 'currently', 'being', 'constructed', 'with', 'the', 'goal', 'of', 'detecting', 'redshifted', '21cm', 'emission', 'from', 'the', 'epoch', 'of', 'reionization', 'these', 'observatories', 'will', 'also', 'be', 'able', 'to', 'detect', 'intensity', 'fluctuations', 'in', 'the', 'cumu... | [-0.04886048982639888, 0.146402565372926, -0.0412993518790851, 0.0906655889061833, -0.12805248203727862, -0.06426924039387023, 0.007576373069584235, 0.4106365341855132, -0.21205456372674392, -0.3272825861957086, 0.10306502593279668, -0.3244934050784703, -0.009150786230853502, 0.23700635273775517, 0.052036888965749706, ... |
709.2956 | The Phase Behavior of Mixed Lipid Membranes in Presence of the Rippled
Phase | We propose a model describing liquid-solid phase coexistence in mixed lipid
membranes by including explicitly the occurrence of a rippled phase. For a
single component membrane, we employ a previous model in which the membrane
thickness is used as an order parameter. As function of temperature, this model
properly ac... | cond-mat.soft cond-mat.mtrl-sci | we propose a model describing liquidsolid phase coexistence in mixed lipid membranes by including explicitly the occurrence of a rippled phase for a single component membrane we employ a previous model in which the membrane thickness is used as an order parameter as function of temperature this model properly accounts ... | [['we', 'propose', 'a', 'model', 'describing', 'liquidsolid', 'phase', 'coexistence', 'in', 'mixed', 'lipid', 'membranes', 'by', 'including', 'explicitly', 'the', 'occurrence', 'of', 'a', 'rippled', 'phase', 'for', 'a', 'single', 'component', 'membrane', 'we', 'employ', 'a', 'previous', 'model', 'in', 'which', 'the', '... | [-0.12155078039584874, 0.19790816034407632, -0.07757014464105255, 0.011715071540775484, 0.014095722272157156, -0.12844313761412068, 0.054211574783227565, 0.3727442199396419, -0.233788466153281, -0.2814469117317991, 0.06827964727738711, -0.25564003310262645, -0.18819747322463784, 0.11912815207575352, -0.0154333817692280... |
709.2957 | Radio and gamma-ray emissions from pulsars: possible observational tests | Many models for the pulsar radio and $\gamma$-ray emissions have been
developed. The tests for these models using observational data are very
important. Tests for the pulsar radio emission models using frequency-altitude
relation are presented in this paper. In the radio band, the mean pulse
profiles evolve with obse... | astro-ph | many models for the pulsar radio and gammaray emissions have been developed the tests for these models using observational data are very important tests for the pulsar radio emission models using frequencyaltitude relation are presented in this paper in the radio band the mean pulse profiles evolve with observing frequ... | [['many', 'models', 'for', 'the', 'pulsar', 'radio', 'and', 'gammaray', 'emissions', 'have', 'been', 'developed', 'the', 'tests', 'for', 'these', 'models', 'using', 'observational', 'data', 'are', 'very', 'important', 'tests', 'for', 'the', 'pulsar', 'radio', 'emission', 'models', 'using', 'frequencyaltitude', 'relatio... | [-0.05493724442987094, 0.14140483204629653, -0.0663969391932299, 0.13151644999799408, -0.11372164749012043, -0.11064642864557055, -0.0017722200825049255, 0.44357427596472776, -0.20691762959289078, -0.3607363251951308, 0.07499151657975744, -0.26749867272267763, -0.09111000795383006, 0.295747677208755, -0.018682058858058... |
709.2958 | Denaturation transition of stretched DNA | We generalize the Poland-Scheraga model to consider DNA denaturation in the
presence of an external stretching force. We demonstrate the existence of a
force-induced DNA denaturation transition and obtain the temperature-force
phase diagram. The transition is determined by the loop exponent $c$ for which
we find the ... | cond-mat.soft cond-mat.stat-mech q-bio.BM | we generalize the polandscheraga model to consider dna denaturation in the presence of an external stretching force we demonstrate the existence of a forceinduced dna denaturation transition and obtain the temperatureforce phase diagram the transition is determined by the loop exponent c for which we find the new value... | [['we', 'generalize', 'the', 'polandscheraga', 'model', 'to', 'consider', 'dna', 'denaturation', 'in', 'the', 'presence', 'of', 'an', 'external', 'stretching', 'force', 'we', 'demonstrate', 'the', 'existence', 'of', 'a', 'forceinduced', 'dna', 'denaturation', 'transition', 'and', 'obtain', 'the', 'temperatureforce', 'p... | [-0.17611640983647325, 0.20331296052733328, -0.05051944130270674, 0.009515317648126766, -0.014501652138722242, -0.1545510845338335, 0.08926135775201567, 0.3648540260520105, -0.28357927653393367, -0.20710213595955837, -0.0006194855413036194, -0.2670843455849624, -0.1845388632585726, 0.14251388417182081, 0.02413857234187... |
709.2959 | Monte Carlo Simulation for the MAGIC-II System | Within the year 2007, MAGIC will be upgraded to a two telescope system at La
Palma. Its main goal is to improve the sensitivity in the
stereoscopic/coincident operational mode. At the same time it will lower the
analysis threshold of the currently running single MAGIC telescope. Results
from the Monte Carlo simulatio... | astro-ph | within the year 2007 magic will be upgraded to a two telescope system at la palma its main goal is to improve the sensitivity in the stereoscopiccoincident operational mode at the same time it will lower the analysis threshold of the currently running single magic telescope results from the monte carlo simulations of t... | [['within', 'the', 'year', '2007', 'magic', 'will', 'be', 'upgraded', 'to', 'a', 'two', 'telescope', 'system', 'at', 'la', 'palma', 'its', 'main', 'goal', 'is', 'to', 'improve', 'the', 'sensitivity', 'in', 'the', 'stereoscopiccoincident', 'operational', 'mode', 'at', 'the', 'same', 'time', 'it', 'will', 'lower', 'the',... | [-0.09412896589808031, 0.12038506675197418, -0.09966709807021432, 0.05863929103431573, -0.04014628160610256, -0.09937208718676345, 0.025270941117441797, 0.37293698979788514, -0.2051171827163682, -0.40533598081534167, 0.16662127862078507, -0.2921406786821513, -0.06356557584311588, 0.2536592458386019, -0.0470706580391894... |
709.296 | Exact Solvability of Two-Dimensional Real Singular Morse Potential | The supersymmetric approach in the form of second order intertwining
relations is used to prove the exact solvability of two-dimensional Schrodinger
equation with generalized two-dimensional Morse potential for $a_0=-1/2$. This
two-parametric model is not amenable to conventional separation of variables,
but it is co... | hep-th math-ph math.MP quant-ph | the supersymmetric approach in the form of second order intertwining relations is used to prove the exact solvability of twodimensional schrodinger equation with generalized twodimensional morse potential for a_012 this twoparametric model is not amenable to conventional separation of variables but it is completely int... | [['the', 'supersymmetric', 'approach', 'in', 'the', 'form', 'of', 'second', 'order', 'intertwining', 'relations', 'is', 'used', 'to', 'prove', 'the', 'exact', 'solvability', 'of', 'twodimensional', 'schrodinger', 'equation', 'with', 'generalized', 'twodimensional', 'morse', 'potential', 'for', 'a_012', 'this', 'twopara... | [-0.13546802414290782, 0.1521448137399812, -0.06811192856876405, 0.11044680625379372, -0.10207465899453222, -0.16489498488154714, -0.046835551488694255, 0.3332533416246156, -0.2730386739975394, -0.26660254760389474, 0.08137689760098091, -0.26757509279151825, -0.16433497724522436, 0.14592092815827537, 0.0289639690174506... |
709.2961 | Incremental Satisfiability and Implication for UTVPI Constraints | Unit two-variable-per-inequality (UTVPI) constraints form one of the largest
class of integer constraints which are polynomial time solvable (unless P=NP).
There is considerable interest in their use for constraint solving, abstract
interpretation, spatial databases, and theorem proving. In this paper we
develop a ne... | cs.DS cs.CG cs.LO | unit twovariableperinequality utvpi constraints form one of the largest class of integer constraints which are polynomial time solvable unless pnp there is considerable interest in their use for constraint solving abstract interpretation spatial databases and theorem proving in this paper we develop a new incremental a... | [['unit', 'twovariableperinequality', 'utvpi', 'constraints', 'form', 'one', 'of', 'the', 'largest', 'class', 'of', 'integer', 'constraints', 'which', 'are', 'polynomial', 'time', 'solvable', 'unless', 'pnp', 'there', 'is', 'considerable', 'interest', 'in', 'their', 'use', 'for', 'constraint', 'solving', 'abstract', 'i... | [-0.20302661336027086, 0.02592783820582554, -0.0480146003421396, 0.07297228100942448, -0.16392945307306944, -0.2192548914521467, 0.10893922835966804, 0.30488078681519254, -0.29538922758074476, -0.39913287790841423, 0.1295971391024068, -0.20955027699237688, -0.08078520396084059, 0.15384938383649568, -0.03528096411610022... |
709.2962 | Algebraic characterization of logically defined tree languages | We give an algebraic characterization of the tree languages that are defined
by logical formulas using certain Lindstr\"om quantifiers. An important
instance of our result concerns first-order definable tree languages. Our
characterization relies on the usage of preclones, an algebraic structure
introduced by the aut... | cs.LO math.LO | we give an algebraic characterization of the tree languages that are defined by logical formulas using certain lindstrom quantifiers an important instance of our result concerns firstorder definable tree languages our characterization relies on the usage of preclones an algebraic structure introduced by the authors in ... | [['we', 'give', 'an', 'algebraic', 'characterization', 'of', 'the', 'tree', 'languages', 'that', 'are', 'defined', 'by', 'logical', 'formulas', 'using', 'certain', 'lindstrom', 'quantifiers', 'an', 'important', 'instance', 'of', 'our', 'result', 'concerns', 'firstorder', 'definable', 'tree', 'languages', 'our', 'charac... | [-0.10890339416168306, 0.07108313084704011, -0.09471198442675498, 0.1150492331400291, -0.1569155846929947, -0.11579961241627841, 0.08175501099954684, 0.3691534820701117, -0.2958590984546944, -0.2499141432547375, 0.10384926068186558, -0.22223621200385463, -0.15808579829931463, 0.23842618910155422, -0.15403225772388396, ... |
709.2963 | Order 1 autoregressive process of finite length | The stochastic processes of finite length defined by recurrence relations
request additional relations specifying the first terms of the process
analogously to the initial conditions for the differential equations. As a
general rule, in time series theory one analyzes only stochastic processes of
infinite length whic... | physics.data-an | the stochastic processes of finite length defined by recurrence relations request additional relations specifying the first terms of the process analogously to the initial conditions for the differential equations as a general rule in time series theory one analyzes only stochastic processes of infinite length which ne... | [['the', 'stochastic', 'processes', 'of', 'finite', 'length', 'defined', 'by', 'recurrence', 'relations', 'request', 'additional', 'relations', 'specifying', 'the', 'first', 'terms', 'of', 'the', 'process', 'analogously', 'to', 'the', 'initial', 'conditions', 'for', 'the', 'differential', 'equations', 'as', 'a', 'gener... | [-0.12580092437270604, 0.17373636699317738, -0.09677360461482519, 0.10730848453854551, -0.06539681769872108, -0.10038396961326841, 0.014430375810995509, 0.376270349031385, -0.3357100517052827, -0.23749177135774702, 0.13657512319940318, -0.2620706198194736, -0.1558914540241225, 0.181230420612176, -0.026067571343170313, ... |
709.2964 | Variational formulation of ideal fluid flows according to gauge
principle | On the basis of the gauge principle of field theory, a new variational
formulation is presented for flows of an ideal fluid. The fluid is defined
thermodynamically by mass density and entropy density, and its flow fields are
characterized by symmetries of translation and rotation. The rotational
transformations are r... | nlin.CD | on the basis of the gauge principle of field theory a new variational formulation is presented for flows of an ideal fluid the fluid is defined thermodynamically by mass density and entropy density and its flow fields are characterized by symmetries of translation and rotation the rotational transformations are regarde... | [['on', 'the', 'basis', 'of', 'the', 'gauge', 'principle', 'of', 'field', 'theory', 'a', 'new', 'variational', 'formulation', 'is', 'presented', 'for', 'flows', 'of', 'an', 'ideal', 'fluid', 'the', 'fluid', 'is', 'defined', 'thermodynamically', 'by', 'mass', 'density', 'and', 'entropy', 'density', 'and', 'its', 'flow',... | [-0.18690019031591748, 0.15214169206072775, -0.09266296832946726, 0.047912368458086274, -0.07852305255697242, -0.07774899259192465, -0.035472323065988444, 0.296461636204839, -0.28746401441759917, -0.2674024129277825, 0.05571726460974397, -0.23988974921422482, -0.1019376570751573, 0.13805351146574085, -0.046581049973342... |
709.2965 | False Vacuum in the Supersymmetric Mass Varying Neutrinos Model | We present detailed analyses of the vacuum structure of the scalar potential
in a supersymmetric Mass Varying Neutrinos model. The observed dark energy
density is identified with false vacuum energy and the dark energy scale of
order $(10^{-3}eV)^4$ is understood by gravitationally suppressed supersymmetry
breaking s... | hep-ph | we present detailed analyses of the vacuum structure of the scalar potential in a supersymmetric mass varying neutrinos model the observed dark energy density is identified with false vacuum energy and the dark energy scale of order 103ev4 is understood by gravitationally suppressed supersymmetry breaking scale ftev2m_... | [['we', 'present', 'detailed', 'analyses', 'of', 'the', 'vacuum', 'structure', 'of', 'the', 'scalar', 'potential', 'in', 'a', 'supersymmetric', 'mass', 'varying', 'neutrinos', 'model', 'the', 'observed', 'dark', 'energy', 'density', 'is', 'identified', 'with', 'false', 'vacuum', 'energy', 'and', 'the', 'dark', 'energy'... | [-0.1349854921108654, 0.2886763535133457, -0.03220437658078308, 0.2135507123503551, -0.03696967656370488, -0.12417341808823845, -0.0038608116233320553, 0.3154796190984264, -0.18664724117032946, -0.3562554610020752, 0.04178789960031834, -0.24881199176741553, -0.015562953898989701, 0.09189148766469045, 0.0437093726300363... |
709.2966 | Spin-Orbit Correlations and Single-Spin Asymmetries | Several examples for the role of orbital angular momentum and spin-orbit
correlations in hadron structure are discussed.
| hep-ph | several examples for the role of orbital angular momentum and spinorbit correlations in hadron structure are discussed | [['several', 'examples', 'for', 'the', 'role', 'of', 'orbital', 'angular', 'momentum', 'and', 'spinorbit', 'correlations', 'in', 'hadron', 'structure', 'are', 'discussed']] | [-0.24008868579917095, 0.20949379179407568, -0.0420783483697211, 0.208085174946224, -0.0488174743950367, -0.03889257044476621, -0.11798383114749894, 0.4301013103960192, -0.23485995631884127, -0.2976713513626772, -0.018682382651604712, -0.3149322435150252, -0.056939583710011316, 0.24859450823243925, 0.12688512278392033,... |
709.2967 | Least squares volatility change point estimation for partially observed
diffusion processes | A one dimensional diffusion process $X=\{X_t, 0\leq t \leq T\}$, with drift
$b(x)$ and diffusion coefficient $\sigma(\theta, x)=\sqrt{\theta} \sigma(x)$
known up to $\theta>0$, is supposed to switch volatility regime at some point
$t^*\in (0,T)$. On the basis of discrete time observations from $X$, the
problem is the... | math.ST math.PR stat.AP stat.TH | a one dimensional diffusion process xx_t 0leq t leq t with drift bx and diffusion coefficient sigmatheta xsqrttheta sigmax known up to theta0 is supposed to switch volatility regime at some point tin 0t on the basis of discrete time observations from x the problem is the one of estimating the instant of change in the v... | [['a', 'one', 'dimensional', 'diffusion', 'process', 'xx_t', '0leq', 't', 'leq', 't', 'with', 'drift', 'bx', 'and', 'diffusion', 'coefficient', 'sigmatheta', 'xsqrttheta', 'sigmax', 'known', 'up', 'to', 'theta0', 'is', 'supposed', 'to', 'switch', 'volatility', 'regime', 'at', 'some', 'point', 'tin', '0t', 'on', 'the', ... | [-0.12009133138201213, 0.14494936721008422, -0.05424191939064126, 0.03207450599989713, -0.033643304641979434, -0.1755250909709898, 0.0733462939835221, 0.4272799809341845, -0.33372151849966875, -0.20833552286659024, 0.16398528692619604, -0.3038984259280066, -0.09109372197333183, 0.16481855641409376, -0.03452912020915444... |
709.2968 | Structure of the string link concordance group and Hirzebruch-type
invariants | We employ Hirzebruch-type invariants obtained from iterated p-covers to
investigate concordance of links and string links. We show that the invariants
naturally give various group homomorphisms of the string link concordance group
into L-groups over number fields. We also obtain homomorphisms of successive
quotients ... | math.GT | we employ hirzebruchtype invariants obtained from iterated pcovers to investigate concordance of links and string links we show that the invariants naturally give various group homomorphisms of the string link concordance group into lgroups over number fields we also obtain homomorphisms of successive quotients of the ... | [['we', 'employ', 'hirzebruchtype', 'invariants', 'obtained', 'from', 'iterated', 'pcovers', 'to', 'investigate', 'concordance', 'of', 'links', 'and', 'string', 'links', 'we', 'show', 'that', 'the', 'invariants', 'naturally', 'give', 'various', 'group', 'homomorphisms', 'of', 'the', 'string', 'link', 'concordance', 'gr... | [-0.2166677885921672, 0.0976694786449419, -0.09933710482825214, 0.09069153412419836, -0.09527973005315289, -0.11674651483384271, 0.019165782713874552, 0.3545774352833784, -0.3401663564145565, -0.2644720599676172, 0.10365640763096357, -0.24194174234289675, -0.17562131677016926, 0.2173812154874516, -0.1269165174647545, -... |
709.2969 | Double prism evanescent mode experiment: superluminal photons? | A critique on the interpretation of the double prism experiment on the
evanescent microwave modes (arXiv:0708.0681) is presented. It is argued that
these experiments do not give any evidence of superluminal photons. A physical
mechanism based on the inhomogeneous waves of classical electromagnetic fields
is proposed.... | quant-ph | a critique on the interpretation of the double prism experiment on the evanescent microwave modes arxiv07080681 is presented it is argued that these experiments do not give any evidence of superluminal photons a physical mechanism based on the inhomogeneous waves of classical electromagnetic fields is proposed | [['a', 'critique', 'on', 'the', 'interpretation', 'of', 'the', 'double', 'prism', 'experiment', 'on', 'the', 'evanescent', 'microwave', 'modes', 'arxiv07080681', 'is', 'presented', 'it', 'is', 'argued', 'that', 'these', 'experiments', 'do', 'not', 'give', 'any', 'evidence', 'of', 'superluminal', 'photons', 'a', 'physic... | [-0.18140310428829656, 0.17276390025185215, -0.1321815251890156, 0.08327129143548923, -0.1805889788808094, -0.11143082943227556, 0.008657289096704011, 0.3629391916924053, -0.14089436973962519, -0.2627892060412301, 0.03659368277682613, -0.2715300908105241, -0.17847454311947028, 0.26869880290339804, 0.013058941707842879,... |
709.297 | Local gating of a graphene Hall bar by graphene side gates | We have investigated the magnetotransport properties of a single-layer
graphene Hall bar with additional graphene side gates. The side gating in the
absence of a magnetic field can be modeled by considering two parallel
conducting channels within the Hall bar. This results in an average penetration
depth of the side ... | cond-mat.mes-hall | we have investigated the magnetotransport properties of a singlelayer graphene hall bar with additional graphene side gates the side gating in the absence of a magnetic field can be modeled by considering two parallel conducting channels within the hall bar this results in an average penetration depth of the side gate ... | [['we', 'have', 'investigated', 'the', 'magnetotransport', 'properties', 'of', 'a', 'singlelayer', 'graphene', 'hall', 'bar', 'with', 'additional', 'graphene', 'side', 'gates', 'the', 'side', 'gating', 'in', 'the', 'absence', 'of', 'a', 'magnetic', 'field', 'can', 'be', 'modeled', 'by', 'considering', 'two', 'parallel'... | [-0.20474907390579775, 0.2093682244509631, -0.0487175951288505, -0.049813028245063666, 0.003363237813018359, -0.20841941618445245, 0.07415378694543494, 0.39093670350584114, -0.29563393632506396, -0.2858168792052122, 0.021885420160984936, -0.27011914074711213, -0.11829563404445524, 0.21966478419671584, -0.00979794500480... |
709.2971 | New method for extracting quasi-bound states from the continuum | A new parameter-free method is proposed for treatment of single-particle
resonances in the real-energy continuum shell model. This method yields
quasi-bound states embedded in the continuum which provide a natural
generalization of weakly bound single-particle states.
| nucl-th | a new parameterfree method is proposed for treatment of singleparticle resonances in the realenergy continuum shell model this method yields quasibound states embedded in the continuum which provide a natural generalization of weakly bound singleparticle states | [['a', 'new', 'parameterfree', 'method', 'is', 'proposed', 'for', 'treatment', 'of', 'singleparticle', 'resonances', 'in', 'the', 'realenergy', 'continuum', 'shell', 'model', 'this', 'method', 'yields', 'quasibound', 'states', 'embedded', 'in', 'the', 'continuum', 'which', 'provide', 'a', 'natural', 'generalization', '... | [-0.03135035479337805, 0.09217910923891598, -0.16081108442611164, 0.12807843403425068, 0.021343407221138477, -0.1554258015886363, 0.08146802850791977, 0.31547800078988075, -0.15215876884758472, -0.2648203489888046, -0.09060748907763304, -0.2291289289585418, -0.14215661937163937, 0.11665867970764844, 0.00485055847093462... |
709.2972 | Double Fell bundles over discrete double groupoids with folding | In this paper we construct the notions of double Fell bundle and double
C*-category for possible future use as tools to describe noncommutative spaces,
in particular in finite dimensions. We identify the algebra of sections of a
double Fell line bundle over a discrete double groupoid with folding with the
convolution... | math-ph math.MP | in this paper we construct the notions of double fell bundle and double ccategory for possible future use as tools to describe noncommutative spaces in particular in finite dimensions we identify the algebra of sections of a double fell line bundle over a discrete double groupoid with folding with the convolution algeb... | [['in', 'this', 'paper', 'we', 'construct', 'the', 'notions', 'of', 'double', 'fell', 'bundle', 'and', 'double', 'ccategory', 'for', 'possible', 'future', 'use', 'as', 'tools', 'to', 'describe', 'noncommutative', 'spaces', 'in', 'particular', 'in', 'finite', 'dimensions', 'we', 'identify', 'the', 'algebra', 'of', 'sect... | [-0.11159176888855195, 0.0692015265493275, -0.0872297752648592, 0.11409900712801123, -0.13523947998400326, -0.1353663491228452, 0.02326412927896644, 0.37357035160555946, -0.37431108257682116, -0.16094286884641745, 0.08123619400686329, -0.20823243925614016, -0.16227172196402653, 0.19570126550292577, -0.17168797010166958... |
709.2973 | Cycle structures of autotopisms of the Latin squares of order up to 11 | The cycle structure of a Latin square autotopism
$\Theta=(\alpha,\beta,\gamma)$ is the triple
$(\mathbf{l}_{\alpha},\mathbf{l}_{\beta},\mathbf{l}_{\gamma})$, where
$\mathbf{l}_{\delta}$ is the cycle structure of $\delta$, for all
$\delta\in\{\alpha,\beta,\gamma\}$. In this paper we study some properties of
these cycl... | math.CO | the cycle structure of a latin square autotopism thetaalphabetagamma is the triple mathbfl_alphamathbfl_betamathbfl_gamma where mathbfl_delta is the cycle structure of delta for all deltainalphabetagamma in this paper we study some properties of these cycle structures and as a consequence we give a classification of al... | [['the', 'cycle', 'structure', 'of', 'a', 'latin', 'square', 'autotopism', 'thetaalphabetagamma', 'is', 'the', 'triple', 'mathbfl_alphamathbfl_betamathbfl_gamma', 'where', 'mathbfl_delta', 'is', 'the', 'cycle', 'structure', 'of', 'delta', 'for', 'all', 'deltainalphabetagamma', 'in', 'this', 'paper', 'we', 'study', 'som... | [-0.19544382510231992, 0.08933354026692755, -0.004536922948033202, 0.03010784976376111, -0.02653411992222947, -0.00897074504481519, 0.048500878464741014, 0.36233342154061093, -0.30201732469540016, -0.28357329570195255, 0.22072751879208155, -0.2945935282052732, -0.21326586724642446, 0.13848129813285434, -0.0597159341890... |
709.2974 | Outflow or galactic wind: The fate of ionized gas in the halos of dwarf
galaxies | Context: H\alpha images of star bursting irregular galaxies reveal a large
amount of extended ionized gas structures, in some cases at kpc-distance away
from any place of current star forming activity. A kinematic analysis of
especially the faint structures in the halo of dwarf galaxies allows insights
into the prope... | astro-ph | context halpha images of star bursting irregular galaxies reveal a large amount of extended ionized gas structures in some cases at kpcdistance away from any place of current star forming activity a kinematic analysis of especially the faint structures in the halo of dwarf galaxies allows insights into the properties a... | [['context', 'halpha', 'images', 'of', 'star', 'bursting', 'irregular', 'galaxies', 'reveal', 'a', 'large', 'amount', 'of', 'extended', 'ionized', 'gas', 'structures', 'in', 'some', 'cases', 'at', 'kpcdistance', 'away', 'from', 'any', 'place', 'of', 'current', 'star', 'forming', 'activity', 'a', 'kinematic', 'analysis'... | [-0.068078511290353, 0.07368193233726333, -0.07969248521097955, 0.10168879000812256, -0.08730518405994513, -0.06491210083586582, -0.000353560768905402, 0.4371494379194591, -0.15004372913835745, -0.35415898861001, 0.03903319396081712, -0.30476352677376034, -0.003644476785330764, 0.19237584375421635, 0.02446914627998067,... |
709.2975 | A Unified Approach to Stochastic Evolution Equations Using the Skorokhod
Integral | We study stochastic evolution equations driven by Gaussian noise. The key
features of the model are that the operators in the deterministic and
stochastic parts can have the same order and the noise can be time-only,
space-only, or space-time. Even the simplest equations of this kind do not have
a square-integrable s... | math.PR math.AP | we study stochastic evolution equations driven by gaussian noise the key features of the model are that the operators in the deterministic and stochastic parts can have the same order and the noise can be timeonly spaceonly or spacetime even the simplest equations of this kind do not have a squareintegrable solution an... | [['we', 'study', 'stochastic', 'evolution', 'equations', 'driven', 'by', 'gaussian', 'noise', 'the', 'key', 'features', 'of', 'the', 'model', 'are', 'that', 'the', 'operators', 'in', 'the', 'deterministic', 'and', 'stochastic', 'parts', 'can', 'have', 'the', 'same', 'order', 'and', 'the', 'noise', 'can', 'be', 'timeonl... | [-0.12030618775281168, 0.11578382717977677, -0.09001922208422218, 0.09751663650690932, -0.09577994572187197, -0.10599198721216194, -0.03117516372280772, 0.3346756382712296, -0.3264933132699558, -0.21509989526211507, 0.15989125569051663, -0.2343413493224597, -0.20097552859945045, 0.143303306625014, -0.1136085441602128, ... |
709.2976 | Molecular Dynamics Simulation of the Hydrogen Isotope Sputtering of
Graphite | We used a molecular dynamics simulation with the modified Brenner reactive
empirical bond order potential to investigate the erosion of a graphite surface
due to the incidence of hydrogen, deuterium, and tritium atoms. Incident
particles cause pressure on the graphite surface, and the chemical bond between
graphene l... | cond-mat.mtrl-sci cond-mat.other | we used a molecular dynamics simulation with the modified brenner reactive empirical bond order potential to investigate the erosion of a graphite surface due to the incidence of hydrogen deuterium and tritium atoms incident particles cause pressure on the graphite surface and the chemical bond between graphene layers ... | [['we', 'used', 'a', 'molecular', 'dynamics', 'simulation', 'with', 'the', 'modified', 'brenner', 'reactive', 'empirical', 'bond', 'order', 'potential', 'to', 'investigate', 'the', 'erosion', 'of', 'a', 'graphite', 'surface', 'due', 'to', 'the', 'incidence', 'of', 'hydrogen', 'deuterium', 'and', 'tritium', 'atoms', 'in... | [-0.06388394865467682, 0.24010235116302225, -0.054136437028415085, 0.03043616723893962, 0.04713965334021342, -0.08369814238499457, 0.09368129077899669, 0.37620310396279977, -0.26376005784486944, -0.31604373076444736, -0.015763731169375527, -0.31042858526712247, -0.03222626382889955, 0.1609236872472991, 0.02381804194561... |
709.2977 | Minimal surfaces in sub-Riemannian manifolds and structure of their
singular sets in the (2,3) case | We study minimal surfaces in generic sub-Riemannian manifolds with
sub-Riemannian structures of co-rank one. These surfaces can be defined as the
critical points of the so-called {\it horizontal} area functional associated to
the canonical {\it horizontal} area form. We derive the intrinsic equation in
the general ca... | math.AP math.DG | we study minimal surfaces in generic subriemannian manifolds with subriemannian structures of corank one these surfaces can be defined as the critical points of the socalled it horizontal area functional associated to the canonical it horizontal area form we derive the intrinsic equation in the general case and then co... | [['we', 'study', 'minimal', 'surfaces', 'in', 'generic', 'subriemannian', 'manifolds', 'with', 'subriemannian', 'structures', 'of', 'corank', 'one', 'these', 'surfaces', 'can', 'be', 'defined', 'as', 'the', 'critical', 'points', 'of', 'the', 'socalled', 'it', 'horizontal', 'area', 'functional', 'associated', 'to', 'the... | [-0.17218365492980656, 0.049341510841244364, -0.045437380648785976, 0.0993066675699793, -0.0653709547889487, -0.1166303555170695, -0.005785589189669951, 0.3671314118286156, -0.25990937873380393, -0.22796162033862458, 0.10158326633641784, -0.2763481511567848, -0.20582428428427718, 0.20791626287949824, -0.139411526660688... |
709.2978 | The Groebner basis of the ideal of vanishing polynomials | We construct an explicit minimal strong Groebner basis of the ideal of
vanishing polynomials in the polynomial ring over Z/m for m>=2. The proof is
done in a purely combinatorial way. It is a remarkable fact that the
constructed Groebner basis is independent of the monomial order and that the
set of leading terms of ... | math.AC math.AG | we construct an explicit minimal strong groebner basis of the ideal of vanishing polynomials in the polynomial ring over zm for m2 the proof is done in a purely combinatorial way it is a remarkable fact that the constructed groebner basis is independent of the monomial order and that the set of leading terms of the con... | [['we', 'construct', 'an', 'explicit', 'minimal', 'strong', 'groebner', 'basis', 'of', 'the', 'ideal', 'of', 'vanishing', 'polynomials', 'in', 'the', 'polynomial', 'ring', 'over', 'zm', 'for', 'm2', 'the', 'proof', 'is', 'done', 'in', 'a', 'purely', 'combinatorial', 'way', 'it', 'is', 'a', 'remarkable', 'fact', 'that',... | [-0.1603645061091441, 0.013527893801777173, -0.09876127699705756, 0.02777022551113771, -0.0971221009553489, -0.10075281285365129, 0.01895277968102719, 0.3305087730769952, -0.3166111284645937, -0.22853338625676678, 0.11316488519798316, -0.20560918378797102, -0.1481856442080274, 0.24435276680989032, -0.0601909441786613, ... |
709.2979 | Choice and Regularity: Common Consequences in Logic | It is well-known that Choice and Regularity are independent of each other but
have important common consequences of logical character (reflection principles,
representations of classes by sets, etc.). We explain this phenomenon by
isolating their "intersection", a principle (called here Best-Foundedness)
which is con... | math.LO | it is wellknown that choice and regularity are independent of each other but have important common consequences of logical character reflection principles representations of classes by sets etc we explain this phenomenon by isolating their intersection a principle called here bestfoundedness which is consistent with th... | [['it', 'is', 'wellknown', 'that', 'choice', 'and', 'regularity', 'are', 'independent', 'of', 'each', 'other', 'but', 'have', 'important', 'common', 'consequences', 'of', 'logical', 'character', 'reflection', 'principles', 'representations', 'of', 'classes', 'by', 'sets', 'etc', 'we', 'explain', 'this', 'phenomenon', '... | [-0.10383465396630209, 0.1078502826370992, -0.0747991785607409, 0.12840869344992908, -0.1198836756020048, -0.1154902895945016, 0.07991113027064996, 0.37593780160166845, -0.3081850208731931, -0.28388214781122323, 0.12575175167808614, -0.24888248884573924, -0.229383796177328, 0.19558141475846602, -0.10050281814873478, 0.... |
709.298 | H2 Double Ionization with Few-Cycle Laser Pulses | The temporal dynamics of double ionization of H2 has been investigated both
experimentally and theoretically with few-cycle laser pulses. The main
observables are the proton spectra associated to the H^+ + H^+ fragmentation
channel. The model is based on the time-dependent Schr\"odinger equation and
treats on the sam... | quant-ph | the temporal dynamics of double ionization of h2 has been investigated both experimentally and theoretically with fewcycle laser pulses the main observables are the proton spectra associated to the h h fragmentation channel the model is based on the timedependent schrodinger equation and treats on the same level the el... | [['the', 'temporal', 'dynamics', 'of', 'double', 'ionization', 'of', 'h2', 'has', 'been', 'investigated', 'both', 'experimentally', 'and', 'theoretically', 'with', 'fewcycle', 'laser', 'pulses', 'the', 'main', 'observables', 'are', 'the', 'proton', 'spectra', 'associated', 'to', 'the', 'h', 'h', 'fragmentation', 'chann... | [-0.0563474461206951, 0.18795714440174055, -0.07107419682076978, 0.1075288253530963, 0.01964619394681936, -0.11432449836500373, 0.040820260574027954, 0.4947708352613988, -0.22891932849224714, -0.3114350007697191, 0.016202803592937038, -0.25927787499706173, 0.005164937130245731, 0.2404249899718798, 0.026087529517373247,... |
709.2981 | The spectrum of closed loops of fundamental flux in D=2+1 SU(N) gauge
theories | We study the closed-string spectrum of SU(N) gauge theories in the
fundamental representation in 2+1 dimensions. We calculate the energies of the
lowest lying ~ 30 states using a large variety of operators characterised by
the quantum numbers of parity and longitudinal momentum. We find that our
results for the groun... | hep-lat hep-th | we study the closedstring spectrum of sun gauge theories in the fundamental representation in 21 dimensions we calculate the energies of the lowest lying 30 states using a large variety of operators characterised by the quantum numbers of parity and longitudinal momentum we find that our results for the ground state ar... | [['we', 'study', 'the', 'closedstring', 'spectrum', 'of', 'sun', 'gauge', 'theories', 'in', 'the', 'fundamental', 'representation', 'in', '21', 'dimensions', 'we', 'calculate', 'the', 'energies', 'of', 'the', 'lowest', 'lying', '30', 'states', 'using', 'a', 'large', 'variety', 'of', 'operators', 'characterised', 'by', ... | [-0.11246497312398708, 0.22180497472214958, -0.057741328557249685, 0.17215043788208909, -0.0032666607314477797, -0.10141233818848495, 0.0655568756972966, 0.33398603772663554, -0.17794155048449403, -0.32200700289205364, 0.04751655883155763, -0.2892191184927588, -0.1030722629542098, 0.18468498311450948, 0.018441137750430... |
709.2982 | Quasi-maximum likelihood estimation of periodic GARCH processes | This paper establishes the strong consistency and asymptotic normality of the
quasi-maximum likelihood estimator (QMLE) for a GARCH process with periodically
time-varying parameters. We first give a necessary and sufficient condition for
the existence of a strictly periodically stationary solution for the periodic
GA... | math.ST math.PR stat.ME stat.TH | this paper establishes the strong consistency and asymptotic normality of the quasimaximum likelihood estimator qmle for a garch process with periodically timevarying parameters we first give a necessary and sufficient condition for the existence of a strictly periodically stationary solution for the periodic garch pga... | [['this', 'paper', 'establishes', 'the', 'strong', 'consistency', 'and', 'asymptotic', 'normality', 'of', 'the', 'quasimaximum', 'likelihood', 'estimator', 'qmle', 'for', 'a', 'garch', 'process', 'with', 'periodically', 'timevarying', 'parameters', 'we', 'first', 'give', 'a', 'necessary', 'and', 'sufficient', 'conditio... | [-0.14762824340958902, 0.03791150837362315, -0.12524694591509491, 0.10912611703094902, -0.07298649289237147, -0.13601458438912803, 0.049335807885613626, 0.3284541385018089, -0.24187934528408425, -0.2188964652085907, 0.18397613900472945, -0.2218960543173585, -0.14471591194945105, 0.14543149572158798, -0.0666141924709918... |
709.2983 | On some probabilistic properties of periodic GARCH processes | This paper examines some probabilistic properties of the class of periodic
GARCH processes (PGARCH) which feature periodicity in conditional
heteroskedasticity. In these models, the parameters are allowed to switch
between different regimes, so that their structure shares many properties with
periodic ARMA process (P... | math.PR math.ST stat.TH | this paper examines some probabilistic properties of the class of periodic garch processes pgarch which feature periodicity in conditional heteroskedasticity in these models the parameters are allowed to switch between different regimes so that their structure shares many properties with periodic arma process parma we ... | [['this', 'paper', 'examines', 'some', 'probabilistic', 'properties', 'of', 'the', 'class', 'of', 'periodic', 'garch', 'processes', 'pgarch', 'which', 'feature', 'periodicity', 'in', 'conditional', 'heteroskedasticity', 'in', 'these', 'models', 'the', 'parameters', 'are', 'allowed', 'to', 'switch', 'between', 'differen... | [-0.11659613338085902, 0.0937735308768194, -0.07008156881678894, 0.1273773751751164, -0.11051033287174461, -0.11690991458269846, 0.0285246280535315, 0.4027850813378232, -0.33964384419013216, -0.24647792181875333, 0.1262273966301098, -0.22355468373700796, -0.1889454005847135, 0.1568629717628236, -0.06496633763189416, 0.... |
709.2984 | Precise dipole moment and quadrupole coupling constants of benzonitrile | We have performed Fourier transform microwave spectroscopy of benzonitrile,
without and with applied electric fields. From the field-free
hyperfine-resolved microwave transitions we simultaneously derive accurate
values for the rotational constants, centrifugal distortion constants, and
nitrogen nuclear quadrupole co... | physics.chem-ph | we have performed fourier transform microwave spectroscopy of benzonitrile without and with applied electric fields from the fieldfree hyperfineresolved microwave transitions we simultaneously derive accurate values for the rotational constants centrifugal distortion constants and nitrogen nuclear quadrupole coupling c... | [['we', 'have', 'performed', 'fourier', 'transform', 'microwave', 'spectroscopy', 'of', 'benzonitrile', 'without', 'and', 'with', 'applied', 'electric', 'fields', 'from', 'the', 'fieldfree', 'hyperfineresolved', 'microwave', 'transitions', 'we', 'simultaneously', 'derive', 'accurate', 'values', 'for', 'the', 'rotationa... | [-0.14565212665828037, 0.21952977266590126, 0.051755315379896125, -0.01001390020866863, -0.028461924738815574, -0.11529138604881334, 0.09699642901465327, 0.46214790503135655, -0.21757403710383738, -0.3224005054865704, -0.048108366226441546, -0.23889782989672462, 0.01622864704762326, 0.16690882419419215, 0.1205244933056... |
709.2985 | Chromomagnetic Instability and Gluonic Phase at Nonzero Temperature | We describe the results of recent studies of a chromomagnetic instability and
a gluonic phase in neutral two-flavor quark matter at nonzero temperature.
| hep-ph | we describe the results of recent studies of a chromomagnetic instability and a gluonic phase in neutral twoflavor quark matter at nonzero temperature | [['we', 'describe', 'the', 'results', 'of', 'recent', 'studies', 'of', 'a', 'chromomagnetic', 'instability', 'and', 'a', 'gluonic', 'phase', 'in', 'neutral', 'twoflavor', 'quark', 'matter', 'at', 'nonzero', 'temperature']] | [-0.17816771467661727, 0.40306294472564175, -0.10801690308701085, 0.04840438756281915, -0.010735360480359068, 0.0017391537194666655, 0.06414948687281298, 0.30309064410950826, -0.0694512054729073, -0.17822573269190994, -0.0004937249569870207, -0.2998439012014348, -0.06080490253541781, 0.03588659526861232, 0.086995373844... |
709.2986 | Blistering of viscoelastic filaments | When a dilute polymer solution experiences capillary thinning, it forms an
almost uniformly cylindrical thread, which we study experimentally. In the last
stages of thinning, when polymers have become fully stretched, the filament
becomes prone to instabilities, of which we describe two: A novel "breathing"
instabili... | physics.flu-dyn | when a dilute polymer solution experiences capillary thinning it forms an almost uniformly cylindrical thread which we study experimentally in the last stages of thinning when polymers have become fully stretched the filament becomes prone to instabilities of which we describe two a novel breathing instability originat... | [['when', 'a', 'dilute', 'polymer', 'solution', 'experiences', 'capillary', 'thinning', 'it', 'forms', 'an', 'almost', 'uniformly', 'cylindrical', 'thread', 'which', 'we', 'study', 'experimentally', 'in', 'the', 'last', 'stages', 'of', 'thinning', 'when', 'polymers', 'have', 'become', 'fully', 'stretched', 'the', 'fila... | [-0.16846982788504852, 0.25230812067797337, -0.09698196570388973, -0.0459483724355983, -0.01676086937227557, -0.15112617137891637, 0.0043350758271351935, 0.3694007001937397, -0.29172428009370643, -0.2088364478118057, 0.10996261041239655, -0.23729352398415007, -0.12875226326286793, 0.12926251287928842, -0.01385156413908... |
709.2987 | Hodge Theory for G2-manifolds: Intermediate Jacobians and Abel-Jacobi
maps | We study the moduli space of torsion-free G2-structures on a fixed compact
manifold, and define its associated universal intermediate Jacobian J. We
define the Yukawa coupling and relate it to a natural pseudo-Kahler structure
on J. We consider natural Chern-Simons type functionals, whose critical points
give associa... | math.DG math.SG | we study the moduli space of torsionfree g2structures on a fixed compact manifold and define its associated universal intermediate jacobian j we define the yukawa coupling and relate it to a natural pseudokahler structure on j we consider natural chernsimons type functionals whose critical points give associative and c... | [['we', 'study', 'the', 'moduli', 'space', 'of', 'torsionfree', 'g2structures', 'on', 'a', 'fixed', 'compact', 'manifold', 'and', 'define', 'its', 'associated', 'universal', 'intermediate', 'jacobian', 'j', 'we', 'define', 'the', 'yukawa', 'coupling', 'and', 'relate', 'it', 'to', 'a', 'natural', 'pseudokahler', 'struct... | [-0.2035923088526654, 0.13098676409572363, -0.053888097087421066, 0.10669659989000094, -0.10169295667068715, -0.15422128235762259, -0.008554102754981325, 0.3654938673305257, -0.3043946038659026, -0.20681244654796746, 0.08263833647474601, -0.22613843143690468, -0.24069528840482235, 0.1387050689919284, -0.141375565537955... |
709.2988 | Time reparameterization in Bianchi type I spinor cosmology | The problem of time reparameterization is addressed at both the classical and
quantum levels in a Bianchi-I universe in which the matter source is a massive
Dirac spinor field. We take the scale factors of the metric as the intrinsic
time and their conjugate momenta as the extrinsic time. A scalar character of
the sp... | gr-qc astro-ph hep-th | the problem of time reparameterization is addressed at both the classical and quantum levels in a bianchii universe in which the matter source is a massive dirac spinor field we take the scale factors of the metric as the intrinsic time and their conjugate momenta as the extrinsic time a scalar character of the spinor ... | [['the', 'problem', 'of', 'time', 'reparameterization', 'is', 'addressed', 'at', 'both', 'the', 'classical', 'and', 'quantum', 'levels', 'in', 'a', 'bianchii', 'universe', 'in', 'which', 'the', 'matter', 'source', 'is', 'a', 'massive', 'dirac', 'spinor', 'field', 'we', 'take', 'the', 'scale', 'factors', 'of', 'the', 'm... | [-0.17460600600612383, 0.13524381904992172, -0.1043019079801592, 0.06723458417238565, -0.060989952952325066, -0.11544930977807208, -0.004077378298259444, 0.3357512078989573, -0.24703194632160444, -0.32180571418117593, 0.09482628599787993, -0.21470034138635835, -0.10174323783980475, 0.1453104466695718, -0.00142530288064... |
709.2989 | Simulated Annealing: Rigorous finite-time guarantees for optimization on
continuous domains | Simulated annealing is a popular method for approaching the solution of a
global optimization problem. Existing results on its performance apply to
discrete combinatorial optimization where the optimization variables can assume
only a finite set of possible values. We introduce a new general formulation of
simulated ... | stat.ML | simulated annealing is a popular method for approaching the solution of a global optimization problem existing results on its performance apply to discrete combinatorial optimization where the optimization variables can assume only a finite set of possible values we introduce a new general formulation of simulated anne... | [['simulated', 'annealing', 'is', 'a', 'popular', 'method', 'for', 'approaching', 'the', 'solution', 'of', 'a', 'global', 'optimization', 'problem', 'existing', 'results', 'on', 'its', 'performance', 'apply', 'to', 'discrete', 'combinatorial', 'optimization', 'where', 'the', 'optimization', 'variables', 'can', 'assume'... | [-0.06560028605972944, 0.012275151398194873, -0.13122376493866678, 0.07795036314156555, -0.07291173289894409, -0.15792312839513886, 0.08766585245688001, 0.3900785842343517, -0.30129159285241497, -0.3067996324363934, 0.13858339665255145, -0.20943409870391327, -0.1457485925730156, 0.22169422526722368, -0.0926355286622824... |
709.299 | On the deduction of galaxy abundances with evolutionary neural networks | A growing number of indicators are now being used with some confidence to
measure the metallicity(Z) of photoionisation regions in planetary nebulae,
galactic HII regions(GHIIRs), extra-galactic HII regions(EGHIIRs) and HII
galaxies(HIIGs). However, a universal indicator valid also at high
metallicities has yet to be... | astro-ph | a growing number of indicators are now being used with some confidence to measure the metallicityz of photoionisation regions in planetary nebulae galactic hii regionsghiirs extragalactic hii regionseghiirs and hii galaxieshiigs however a universal indicator valid also at high metallicities has yet to be found here we ... | [['a', 'growing', 'number', 'of', 'indicators', 'are', 'now', 'being', 'used', 'with', 'some', 'confidence', 'to', 'measure', 'the', 'metallicityz', 'of', 'photoionisation', 'regions', 'in', 'planetary', 'nebulae', 'galactic', 'hii', 'regionsghiirs', 'extragalactic', 'hii', 'regionseghiirs', 'and', 'hii', 'galaxieshiig... | [-0.052304497671782246, 0.027829214423590605, -0.07114918885328866, 0.0951014187046059, -0.07532915966025686, -0.13316914981007255, 0.10065867734249569, 0.44207484387908064, -0.21051884238316393, -0.3230144506252407, 0.04301294047373463, -0.258004242404416, -0.12732894856546698, 0.22020214893895126, -0.0411494475581519... |
709.2991 | General Operator Solutions and BRST Quantization of Superstrings in the
pp-Wave with Torsion | We completely accomplish the canonically covariant quantization of
Ramond-Neveu-Schwarz (RNS) superstrings in the pp-wave background with a
non-zero flux of the NS-NS antisymmetric two-form field. Here this flux is
equivalent to a nonvanishing torsion. In this quantization, general operator
solutions, which satisfy t... | hep-th | we completely accomplish the canonically covariant quantization of ramondneveuschwarz rns superstrings in the ppwave background with a nonzero flux of the nsns antisymmetric twoform field here this flux is equivalent to a nonvanishing torsion in this quantization general operator solutions which satisfy the entire equa... | [['we', 'completely', 'accomplish', 'the', 'canonically', 'covariant', 'quantization', 'of', 'ramondneveuschwarz', 'rns', 'superstrings', 'in', 'the', 'ppwave', 'background', 'with', 'a', 'nonzero', 'flux', 'of', 'the', 'nsns', 'antisymmetric', 'twoform', 'field', 'here', 'this', 'flux', 'is', 'equivalent', 'to', 'a', ... | [-0.2019840799949386, 0.19363299080035756, -0.04494796472718008, 0.08507233989657834, -0.11150018707849085, -0.10297600819136608, -0.04222413334487514, 0.2848767029968175, -0.21556394795294512, -0.250788014174693, 0.02791765182363716, -0.24169008720412172, -0.1419074162629179, 0.06931689557704059, -0.061196272655136205... |
709.2992 | From matrix models' topological expansion to topological string
theories: counting surfaces with algebraic geometry | The 2-matrix model has been introduced to study Ising model on random
surfaces. Since then, the link between matrix models and combinatorics of
discrete surfaces has strongly tightened. This manuscript aims to investigate
these deep links and extend them beyond the matrix models, following my work's
evolution. First,... | hep-th | the 2matrix model has been introduced to study ising model on random surfaces since then the link between matrix models and combinatorics of discrete surfaces has strongly tightened this manuscript aims to investigate these deep links and extend them beyond the matrix models following my works evolution first i take ca... | [['the', '2matrix', 'model', 'has', 'been', 'introduced', 'to', 'study', 'ising', 'model', 'on', 'random', 'surfaces', 'since', 'then', 'the', 'link', 'between', 'matrix', 'models', 'and', 'combinatorics', 'of', 'discrete', 'surfaces', 'has', 'strongly', 'tightened', 'this', 'manuscript', 'aims', 'to', 'investigate', '... | [-0.11416195296797765, 0.07573892255245608, -0.1411880682809428, 0.0838213933673431, -0.10559300473600694, -0.1660524728182498, 0.0033196472886462755, 0.35062379090525553, -0.31480643462492236, -0.257278984660334, 0.10386348744788113, -0.24967230251806558, -0.2136392837151065, 0.16574067390560432, -0.09426974384178229,... |
709.2993 | The Astronomy and Science Behind the Myth | We show that many ancient Indian mythological legends are really allegorical
depictions of astronomical and other physical phenomena of which the composers
had a good idea. This detail enables us to also use techniques of astronomical
chronology for dating various events.
| physics.gen-ph | we show that many ancient indian mythological legends are really allegorical depictions of astronomical and other physical phenomena of which the composers had a good idea this detail enables us to also use techniques of astronomical chronology for dating various events | [['we', 'show', 'that', 'many', 'ancient', 'indian', 'mythological', 'legends', 'are', 'really', 'allegorical', 'depictions', 'of', 'astronomical', 'and', 'other', 'physical', 'phenomena', 'of', 'which', 'the', 'composers', 'had', 'a', 'good', 'idea', 'this', 'detail', 'enables', 'us', 'to', 'also', 'use', 'techniques'... | [-0.016474564257077873, 0.0743742691585794, -0.19006022985558957, 0.18154721384344158, -0.19217382655479015, -0.08600566386012361, 0.02569028255529702, 0.3493598414119333, -0.2114831586368382, -0.35636064456775784, 0.14897761587053537, -0.3152564232703298, -0.21621674257330598, 0.29121419549919664, -0.13377031073905526... |
709.2994 | CP violation at one loop in the polarization-independent chargino
production in e+e- collisions | Recently Osland and Vereshagin noticed, based on sample calculations of some
box diagrams, that in unpolarised e+e- collisions CP-odd effects in the
non-diagonal chargino-pair production process are generated at one-loop. Here
we perform a full one-loop analysis of these effects and point out that in some
cases the n... | hep-ph | recently osland and vereshagin noticed based on sample calculations of some box diagrams that in unpolarised ee collisions cpodd effects in the nondiagonal charginopair production process are generated at oneloop here we perform a full oneloop analysis of these effects and point out that in some cases the neglected ver... | [['recently', 'osland', 'and', 'vereshagin', 'noticed', 'based', 'on', 'sample', 'calculations', 'of', 'some', 'box', 'diagrams', 'that', 'in', 'unpolarised', 'ee', 'collisions', 'cpodd', 'effects', 'in', 'the', 'nondiagonal', 'charginopair', 'production', 'process', 'are', 'generated', 'at', 'oneloop', 'here', 'we', '... | [-0.11962518160587197, 0.2261936514523257, -0.06230526932860526, 0.14984213604060478, -0.05902725552323829, -0.12222797285472409, 0.09368898561276663, 0.3575747755220097, -0.21158705501597416, -0.2219666518961613, 0.04185901970335732, -0.33805700626454493, -0.09053836416536837, 0.14839007868954723, 0.073920197130882, 0... |
709.2995 | C*-pseudo-multiplicative unitaries | We introduce $C^*$-pseudo-multiplicative unitaries and (concrete) Hopf
$C^*$-bimodules, which are $C^*$-algebraic variants of the
pseudo-multiplicative unitaries on Hilbert spaces and the Hopf-von
Neumann-bimodules studied by Enock, Lesieur, Vallin. Moreover, we associate to
every regular $C^*$-pseudo-multiplicative ... | math.OA | we introduce cpseudomultiplicative unitaries and concrete hopf cbimodules which are calgebraic variants of the pseudomultiplicative unitaries on hilbert spaces and the hopfvon neumannbimodules studied by enock lesieur vallin moreover we associate to every regular cpseudomultiplicative unitary two hopfcbimodules and dis... | [['we', 'introduce', 'cpseudomultiplicative', 'unitaries', 'and', 'concrete', 'hopf', 'cbimodules', 'which', 'are', 'calgebraic', 'variants', 'of', 'the', 'pseudomultiplicative', 'unitaries', 'on', 'hilbert', 'spaces', 'and', 'the', 'hopfvon', 'neumannbimodules', 'studied', 'by', 'enock', 'lesieur', 'vallin', 'moreover... | [-0.11570818870413033, 0.15042108911174265, -0.03304716411300681, 0.12317777657881379, -0.06559596687227233, -0.2131101985208013, -0.008435267605818808, 0.43773758521472866, -0.3365900491110303, -0.09035045843285677, 0.13936124101746827, -0.2288956845983524, -0.16717700423164802, 0.20549285096455028, -0.229993085842579... |
709.2996 | Entanglement-free Heisenberg-limited phase estimation | Measurement underpins all quantitative science. A key example is the
measurement of optical phase, used in length metrology and many other
applications. Advances in precision measurement have consistently led to
important scientific discoveries. At the fundamental level, measurement
precision is limited by the number... | quant-ph | measurement underpins all quantitative science a key example is the measurement of optical phase used in length metrology and many other applications advances in precision measurement have consistently led to important scientific discoveries at the fundamental level measurement precision is limited by the number n of q... | [['measurement', 'underpins', 'all', 'quantitative', 'science', 'a', 'key', 'example', 'is', 'the', 'measurement', 'of', 'optical', 'phase', 'used', 'in', 'length', 'metrology', 'and', 'many', 'other', 'applications', 'advances', 'in', 'precision', 'measurement', 'have', 'consistently', 'led', 'to', 'important', 'scien... | [-0.08165906094063757, 0.1835504290943959, -0.06352244537265506, 0.053936444352984836, -0.010409252210365594, -0.19435316822637105, 0.08329424473186009, 0.36509682276664535, -0.23086425246947329, -0.364749667889555, 0.1035615530204268, -0.2742081506635259, -0.061447011455356915, 0.2551545851429182, -0.06809920139494352... |
709.2997 | Two polynomial representations of experimental design | In the context of algebraic statistics an experimental design is described by
a set of polynomials called the design ideal. This, in turn, is generated by
finite sets of polynomials. Two types of generating sets are mostly used in the
literature: Groebner bases and indicator functions. We briefly describe them
both, ... | stat.ME stat.CO | in the context of algebraic statistics an experimental design is described by a set of polynomials called the design ideal this in turn is generated by finite sets of polynomials two types of generating sets are mostly used in the literature groebner bases and indicator functions we briefly describe them both how they ... | [['in', 'the', 'context', 'of', 'algebraic', 'statistics', 'an', 'experimental', 'design', 'is', 'described', 'by', 'a', 'set', 'of', 'polynomials', 'called', 'the', 'design', 'ideal', 'this', 'in', 'turn', 'is', 'generated', 'by', 'finite', 'sets', 'of', 'polynomials', 'two', 'types', 'of', 'generating', 'sets', 'are'... | [-0.10412680860723794, 0.09685999061499095, -0.06786678261181087, 0.08538870828047992, -0.05332199653127679, -0.08727746243002238, 0.029402298611347324, 0.3820601883171885, -0.27817020539976195, -0.24865473315901596, 0.13756417810204036, -0.2572407228211056, -0.18279519763395743, 0.2636400467060782, -0.0653243003252111... |
709.2998 | Cavity-assisted spontaneous emission as a single-photon source: Pulse
shape and efficiency of one-photon Fock state preparation | Within the framework of exact quantum electrodynamics in dispersing and
absorbing media, we have studied the quantum state of the radiation emitted
from an initially in the upper state prepared two-level atom in a high-$Q$
cavity, including the regime where the emitted photon belongs to a wave packet
that simultaneou... | quant-ph | within the framework of exact quantum electrodynamics in dispersing and absorbing media we have studied the quantum state of the radiation emitted from an initially in the upper state prepared twolevel atom in a highq cavity including the regime where the emitted photon belongs to a wave packet that simultaneously cove... | [['within', 'the', 'framework', 'of', 'exact', 'quantum', 'electrodynamics', 'in', 'dispersing', 'and', 'absorbing', 'media', 'we', 'have', 'studied', 'the', 'quantum', 'state', 'of', 'the', 'radiation', 'emitted', 'from', 'an', 'initially', 'in', 'the', 'upper', 'state', 'prepared', 'twolevel', 'atom', 'in', 'a', 'hig... | [-0.16357610969884823, 0.23429525444886307, -0.04492642430302042, 0.0019380102162428487, 0.01908826484129979, -0.1415860132708286, 0.028072353336924257, 0.39075144360988184, -0.22638267687020394, -0.24415324590383813, 0.01889544438588648, -0.29684419873385476, -0.06685591004788875, 0.17043570398639601, 0.03599662370442... |
709.2999 | A Criterion for Precompactness in the Space of Hypermeasures | Let $Q$ denote the space of signed measures on the Borel $\sigma$-algebra of
a separable complete space $X$. We endow $Q$ with the norm $\|q\|=\sup|\int\phi
dq|$, where the supremum is taken over all Lipschitz with constant 1 functions
whose module does not exceed unity. This normed space is incomplete provided
$X$ i... | math.FA | let q denote the space of signed measures on the borel sigmaalgebra of a separable complete space x we endow q with the norm qsupintphi dq where the supremum is taken over all lipschitz with constant 1 functions whose module does not exceed unity this normed space is incomplete provided x is infinite and has at least o... | [['let', 'q', 'denote', 'the', 'space', 'of', 'signed', 'measures', 'on', 'the', 'borel', 'sigmaalgebra', 'of', 'a', 'separable', 'complete', 'space', 'x', 'we', 'endow', 'q', 'with', 'the', 'norm', 'qsupintphi', 'dq', 'where', 'the', 'supremum', 'is', 'taken', 'over', 'all', 'lipschitz', 'with', 'constant', '1', 'func... | [-0.13822608823766527, 0.12295299310885045, -0.08733637225795184, 0.07143583953755138, -0.06530077321930668, -0.11113586591091007, 0.02860127669713541, 0.37515540457452123, -0.2904703128354057, -0.16422238326429026, 0.13533351645784694, -0.29586067396904464, -0.048214497884897435, 0.18740389755238657, -0.13748398403454... |
709.3 | Cool carbon stars in the halo: new very red or distant objects | The goal of this paper is to present and analyse a new sample of cool carbon
(C)stars located in the halo. Twenty three new C stars were discovered. Spectra
are typical of N-type stars with C2 and CN bands and sometimes Halpha in
emission. ... Four objects are particularly red with J-K > 3, with 2 located at
more tha... | astro-ph | the goal of this paper is to present and analyse a new sample of cool carbon cstars located in the halo twenty three new c stars were discovered spectra are typical of ntype stars with c2 and cn bands and sometimes halpha in emission four objects are particularly red with jk 3 with 2 located at more than 5 kpc from the... | [['the', 'goal', 'of', 'this', 'paper', 'is', 'to', 'present', 'and', 'analyse', 'a', 'new', 'sample', 'of', 'cool', 'carbon', 'cstars', 'located', 'in', 'the', 'halo', 'twenty', 'three', 'new', 'c', 'stars', 'were', 'discovered', 'spectra', 'are', 'typical', 'of', 'ntype', 'stars', 'with', 'c2', 'and', 'cn', 'bands', ... | [-0.06255996778504283, 0.11956905137182335, -0.028027418769810717, 0.05040440365018053, -0.05866443059933265, -0.11509028364442563, 0.04963748707908796, 0.447630250954446, -0.13664428348020288, -0.41081178842382576, 0.04794531314054376, -0.33871269881910154, -0.014413782697569096, 0.19362592727535952, -0.05738048121277... |
709.3001 | Description of superdeformed bands in light N=Z nuclei using the cranked
HFB method | Superdeformed states in light $N=Z$ nuclei are studied by means of the
self-consistent cranking calculation (i.e., the P + QQ model based on the
cranked Hartree-Fock-Bogoliubov method). Analyses are given for two typical
cases of superdeformed bands in the $A \simeq 40$ mass region, that is, bands
where backbending i... | nucl-th | superdeformed states in light nz nuclei are studied by means of the selfconsistent cranking calculation ie the p qq model based on the cranked hartreefockbogoliubov method analyses are given for two typical cases of superdeformed bands in the a simeq 40 mass region that is bands where backbending is absent 40ca and pre... | [['superdeformed', 'states', 'in', 'light', 'nz', 'nuclei', 'are', 'studied', 'by', 'means', 'of', 'the', 'selfconsistent', 'cranking', 'calculation', 'ie', 'the', 'p', 'qq', 'model', 'based', 'on', 'the', 'cranked', 'hartreefockbogoliubov', 'method', 'analyses', 'are', 'given', 'for', 'two', 'typical', 'cases', 'of', ... | [-0.12243017374433987, 0.15062207423440951, -0.07077017536647218, 0.14598986521233073, 0.05579977994784713, -0.11118750009931103, 0.08327596735519667, 0.3605023706031422, -0.16013754055564922, -0.2406591668559779, -0.046530521803996173, -0.33118143502963326, -0.047972975018364124, 0.1412149115580745, 0.0931691467966659... |
709.3002 | A generalized Principle of Relativity | In this paper we bring to light an hitherto undisclosed richness of this
Theory, namely its admitting a consistent reformulation which is able to
provide a unified scenario for all kinds of particles, be they lightlike or
not. This result hinges on a "generalized" Principle of Relativity which is
{intrinsic} to Einst... | gr-qc | in this paper we bring to light an hitherto undisclosed richness of this theory namely its admitting a consistent reformulation which is able to provide a unified scenario for all kinds of particles be they lightlike or not this result hinges on a generalized principle of relativity which is intrinsic to einsteins theo... | [['in', 'this', 'paper', 'we', 'bring', 'to', 'light', 'an', 'hitherto', 'undisclosed', 'richness', 'of', 'this', 'theory', 'namely', 'its', 'admitting', 'a', 'consistent', 'reformulation', 'which', 'is', 'able', 'to', 'provide', 'a', 'unified', 'scenario', 'for', 'all', 'kinds', 'of', 'particles', 'be', 'they', 'light... | [-0.11301732707678186, 0.12380578581236448, -0.12527139768308887, 0.0522569073015364, -0.11519998369308618, -0.12900460576982642, 0.02413244361976003, 0.3402342335641505, -0.2789276458647268, -0.2920545456848043, 0.05203453216584859, -0.22262592501435213, -0.11408885582425606, 0.1704579264651145, -0.08262334051443007, ... |
709.3003 | Coherent backscattering of ultrasound without a source | Coherent backscattering is due to constructive interferences of reciprocal
paths and leads to an enhancement of the intensity of a multiply scattered
field near its source. To observe this enhancement an array of receivers is
conventionally placed close to the source. Our approach here is different. In a
first experi... | cond-mat.other cond-mat.stat-mech physics.class-ph physics.geo-ph | coherent backscattering is due to constructive interferences of reciprocal paths and leads to an enhancement of the intensity of a multiply scattered field near its source to observe this enhancement an array of receivers is conventionally placed close to the source our approach here is different in a first experiment ... | [['coherent', 'backscattering', 'is', 'due', 'to', 'constructive', 'interferences', 'of', 'reciprocal', 'paths', 'and', 'leads', 'to', 'an', 'enhancement', 'of', 'the', 'intensity', 'of', 'a', 'multiply', 'scattered', 'field', 'near', 'its', 'source', 'to', 'observe', 'this', 'enhancement', 'an', 'array', 'of', 'receiv... | [-0.1635467146813237, 0.11905002784267296, -0.0895357691937671, 0.035606924113861446, -0.04992994550123529, -0.08171148501986743, 0.05071515202377308, 0.41786172672368166, -0.2859778153218048, -0.28955198651320246, 0.0420537557439738, -0.3121855380452888, -0.10422289066614127, 0.18425042503776978, -0.004818651084963865... |
709.3004 | A FLAMINGOS Deep Near Infrared Imaging Survey of the Rosette Complex I:
Identification and Distribution of the Embedded Population | We present the results of a deep near-infrared imaging survey of the Rosette
Complex. We studied the distribution of young embedded sources using a
variation of the Nearest Neighbor Method applied to a carefully selected sample
of near-infrared excess (NIRX) stars which trace the latest episode of star
formation in t... | astro-ph | we present the results of a deep nearinfrared imaging survey of the rosette complex we studied the distribution of young embedded sources using a variation of the nearest neighbor method applied to a carefully selected sample of nearinfrared excess nirx stars which trace the latest episode of star formation in the comp... | [['we', 'present', 'the', 'results', 'of', 'a', 'deep', 'nearinfrared', 'imaging', 'survey', 'of', 'the', 'rosette', 'complex', 'we', 'studied', 'the', 'distribution', 'of', 'young', 'embedded', 'sources', 'using', 'a', 'variation', 'of', 'the', 'nearest', 'neighbor', 'method', 'applied', 'to', 'a', 'carefully', 'selec... | [-0.0849968157526156, 0.07295891544592843, -0.07783463659721451, 0.0698349709465244, -0.02264243294610768, 0.032261624947391654, 0.09153728221568304, 0.42160085968270494, -0.21276391408078976, -0.3533108408336301, 0.05206908289141752, -0.2675687787802638, -0.06976211093668197, 0.13897504421404083, 0.008360250040484086,... |
709.3005 | Feedback and efficiency in limit order markets | A consistency criterion for price impact functions in limit order markets is
proposed that prohibits chain arbitrage exploitation. Both the bid-ask spread
and the feedback of sequential market orders of the same kind onto both sides
of the order book are essential to ensure consistency at the smallest time
scale. All... | q-fin.TR cond-mat.stat-mech physics.soc-ph | a consistency criterion for price impact functions in limit order markets is proposed that prohibits chain arbitrage exploitation both the bidask spread and the feedback of sequential market orders of the same kind onto both sides of the order book are essential to ensure consistency at the smallest time scale all the ... | [['a', 'consistency', 'criterion', 'for', 'price', 'impact', 'functions', 'in', 'limit', 'order', 'markets', 'is', 'proposed', 'that', 'prohibits', 'chain', 'arbitrage', 'exploitation', 'both', 'the', 'bidask', 'spread', 'and', 'the', 'feedback', 'of', 'sequential', 'market', 'orders', 'of', 'the', 'same', 'kind', 'ont... | [-0.1411172022954339, 0.06456937418792337, -0.09526713832562404, 0.18821420230244892, -0.07272357383506402, -0.06880248543096795, 0.11762681111900343, 0.3984256816643571, -0.2576808501921949, -0.25419589900781236, 0.17361663997779408, -0.32191751294192816, -0.0772881026394547, 0.14575495875425756, -0.04446608290105822,... |
709.3006 | Soliton-like Spin State in the A-like Phase of 3He in Anisotropic
Aerogel | We have found a new stable spin state in the A-like phase of superfluid 3He
confined to intrinsically anisotropic aerogel. The state can be formed by
radiofrequency excitation applied while cooling through the superfluid
transition temperature and its NMR properties are different from the standard
A-like phase obtain... | cond-mat.dis-nn cond-mat.other | we have found a new stable spin state in the alike phase of superfluid 3he confined to intrinsically anisotropic aerogel the state can be formed by radiofrequency excitation applied while cooling through the superfluid transition temperature and its nmr properties are different from the standard alike phase obtained in... | [['we', 'have', 'found', 'a', 'new', 'stable', 'spin', 'state', 'in', 'the', 'alike', 'phase', 'of', 'superfluid', '3he', 'confined', 'to', 'intrinsically', 'anisotropic', 'aerogel', 'the', 'state', 'can', 'be', 'formed', 'by', 'radiofrequency', 'excitation', 'applied', 'while', 'cooling', 'through', 'the', 'superfluid... | [-0.09660541970597607, 0.3493850640296726, -0.10735445323688778, -0.0167186043969631, -0.019305218234133552, -0.1426669390819652, 0.0520866054346339, 0.3987035565406189, -0.25705764672233605, -0.24382706936186468, 0.06442140600591584, -0.24825535326356618, -0.04208721522189362, 0.14863768246182255, 0.0506155869503781, ... |
709.3007 | Mass loss predictions for hot stars | I present the results of radiation-driven mass-loss predictions for hot stars
of all mass. Mass loss is an important aspect for the evolution of massive
stars, the rotational properties of the progenitors of gamma-ray bursts, and is
essential in assessing whether the most massive stars explode as
pair-instability sup... | astro-ph | i present the results of radiationdriven massloss predictions for hot stars of all mass mass loss is an important aspect for the evolution of massive stars the rotational properties of the progenitors of gammaray bursts and is essential in assessing whether the most massive stars explode as pairinstability supernovae o... | [['i', 'present', 'the', 'results', 'of', 'radiationdriven', 'massloss', 'predictions', 'for', 'hot', 'stars', 'of', 'all', 'mass', 'mass', 'loss', 'is', 'an', 'important', 'aspect', 'for', 'the', 'evolution', 'of', 'massive', 'stars', 'the', 'rotational', 'properties', 'of', 'the', 'progenitors', 'of', 'gammaray', 'bu... | [-0.07013490502038723, 0.15466240832634626, -0.028863002248812705, 0.14310082869760535, -0.12366496106785546, -0.03090450086572266, 0.08157463359216657, 0.38729888992200906, -0.15184205366580233, -0.3246417140158323, 0.054134206521533224, -0.27907563605625835, -0.06932778272067906, 0.1999335341500043, -0.07888206895418... |
709.3008 | Magnetic flux emergence in fast rotating stars | Fast rotating cool stars are characterised by high magnetic activity levels
and frequently show dark spots up to polar latitudes. Their distinctive surface
distributions of magnetic flux are investigated in the context of the
solar-stellar connection by applying the solar flux eruption and surface flux
transport mode... | astro-ph | fast rotating cool stars are characterised by high magnetic activity levels and frequently show dark spots up to polar latitudes their distinctive surface distributions of magnetic flux are investigated in the context of the solarstellar connection by applying the solar flux eruption and surface flux transport models t... | [['fast', 'rotating', 'cool', 'stars', 'are', 'characterised', 'by', 'high', 'magnetic', 'activity', 'levels', 'and', 'frequently', 'show', 'dark', 'spots', 'up', 'to', 'polar', 'latitudes', 'their', 'distinctive', 'surface', 'distributions', 'of', 'magnetic', 'flux', 'are', 'investigated', 'in', 'the', 'context', 'of'... | [-0.15935432564832233, 0.26676280376094513, -0.0025592973097765715, 0.12049882205018315, -0.07447303192287534, -0.02844601526304181, 0.04113121423665574, 0.41799133873764593, -0.2113937017456371, -0.39483816420949586, 0.06499493431976187, -0.20624003595387067, -0.051024144447534975, 0.20400546927323293, -0.095281423970... |
709.3009 | ^{63,65}Cu NMR and NQR evidence for an unusual spin dynamics in PrCu_2
below 100 K | We report the results of a $^{63,65}$Cu NMR/NQR study probing the
intermetallic compound PrCu$_2$. The previously claimed onset of magnetic order
at 65 K, indicated in a $\mu$SR study, is not confirmed. Based on our data we
discuss different possible reasons for this apparent discrepancy, including a
non negligible i... | cond-mat.mtrl-sci | we report the results of a 6365cu nmrnqr study probing the intermetallic compound prcu_2 the previously claimed onset of magnetic order at 65 k indicated in a musr study is not confirmed based on our data we discuss different possible reasons for this apparent discrepancy including a non negligible influence of the imp... | [['we', 'report', 'the', 'results', 'of', 'a', '6365cu', 'nmrnqr', 'study', 'probing', 'the', 'intermetallic', 'compound', 'prcu_2', 'the', 'previously', 'claimed', 'onset', 'of', 'magnetic', 'order', 'at', '65', 'k', 'indicated', 'in', 'a', 'musr', 'study', 'is', 'not', 'confirmed', 'based', 'on', 'our', 'data', 'we',... | [-0.17507624128078925, 0.1528598317740886, -0.05496487684939882, 0.08469126008515823, -0.05344698472019238, -0.09844197048304626, 0.08618956809580515, 0.3540391320291954, -0.21163355511955068, -0.3420581331924547, 0.02649688426717597, -0.3322955442451035, -0.12361934676448096, 0.1835113737379979, 0.06303200690382266, -... |
709.301 | BFKL ansatz for BK equation in conformal basis | The BK equation in the conformal basis is considered and analyzed. It is
shown that at high energy a factorization of the coordinate and rapidity
dependence should hold. This allows to simplify significantly the from of the
equation under discussion. An analytical ansatz for the solution to the BK
equation at high en... | hep-ph | the bk equation in the conformal basis is considered and analyzed it is shown that at high energy a factorization of the coordinate and rapidity dependence should hold this allows to simplify significantly the from of the equation under discussion an analytical ansatz for the solution to the bk equation at high energie... | [['the', 'bk', 'equation', 'in', 'the', 'conformal', 'basis', 'is', 'considered', 'and', 'analyzed', 'it', 'is', 'shown', 'that', 'at', 'high', 'energy', 'a', 'factorization', 'of', 'the', 'coordinate', 'and', 'rapidity', 'dependence', 'should', 'hold', 'this', 'allows', 'to', 'simplify', 'significantly', 'the', 'from'... | [-0.10197783139773418, 0.1330090538098588, -0.14949625138998837, 0.10635551172812041, -0.04029744574254765, -0.11128012733198367, -0.008616267707668714, 0.3330848260199534, -0.20363074617863103, -0.27782262129256047, 0.07632733648013626, -0.2532378908621435, -0.013735952485050704, 0.15065064246825002, 0.007473816836896... |
709.3011 | Some extensions of the uncertainty principle | We study the formulation of the uncertainty principle in quantum mechanics in
terms of entropic inequalities, extending results recently derived by
Bialynicki-Birula [1] and Zozor et al. [2]. Those inequalities can be
considered as generalizations of the Heisenberg uncertainty principle, since
they measure the mutual... | math.PR | we study the formulation of the uncertainty principle in quantum mechanics in terms of entropic inequalities extending results recently derived by bialynickibirula 1 and zozor et al 2 those inequalities can be considered as generalizations of the heisenberg uncertainty principle since they measure the mutual uncertaint... | [['we', 'study', 'the', 'formulation', 'of', 'the', 'uncertainty', 'principle', 'in', 'quantum', 'mechanics', 'in', 'terms', 'of', 'entropic', 'inequalities', 'extending', 'results', 'recently', 'derived', 'by', 'bialynickibirula', '1', 'and', 'zozor', 'et', 'al', '2', 'those', 'inequalities', 'can', 'be', 'considered'... | [-0.06686142147929572, 0.1685322986665115, -0.06147078254177947, 0.07790966098186533, -0.007662753180792446, -0.1279737532227848, 0.038998549300766384, 0.3227833971134661, -0.2680497983819805, -0.27814887931762156, 0.11296118990525, -0.3032073952216545, -0.15071820855647436, 0.20619182792185764, -0.08224347774418728, 0... |
709.3012 | Construction of a stationary queue with impatient customers | In this paper, we study the stability of queues with impatient customers.
Under general stationary ergodic assumptions, we first provide some conditions
for such a queue to be regenerative (i.e. to empty a.s. an infinite number of
times). In the particular case of a single server operating in First in, First
out, we ... | math.PR | in this paper we study the stability of queues with impatient customers under general stationary ergodic assumptions we first provide some conditions for such a queue to be regenerative ie to empty as an infinite number of times in the particular case of a single server operating in first in first out we prove the exis... | [['in', 'this', 'paper', 'we', 'study', 'the', 'stability', 'of', 'queues', 'with', 'impatient', 'customers', 'under', 'general', 'stationary', 'ergodic', 'assumptions', 'we', 'first', 'provide', 'some', 'conditions', 'for', 'such', 'a', 'queue', 'to', 'be', 'regenerative', 'ie', 'to', 'empty', 'as', 'an', 'infinite', ... | [-0.17007262180347674, 0.07706453378705191, -0.08352367248153314, 0.060554354238609616, -0.014004434329267084, -0.12543756024785002, 0.12369151955433401, 0.3593588171484457, -0.26043227954704146, -0.200316817489114, 0.14869376069162338, -0.21170873803467574, -0.11890582731840285, 0.18033822791502727, -0.137690390950989... |
709.3013 | Supervised learning on graphs of spatio-temporal similarity in satellite
image sequences | High resolution satellite image sequences are multidimensional signals
composed of spatio-temporal patterns associated to numerous and various
phenomena. Bayesian methods have been previously proposed in (Heas and Datcu,
2005) to code the information contained in satellite image sequences in a graph
representation us... | cs.CV | high resolution satellite image sequences are multidimensional signals composed of spatiotemporal patterns associated to numerous and various phenomena bayesian methods have been previously proposed in heas and datcu 2005 to code the information contained in satellite image sequences in a graph representation using bay... | [['high', 'resolution', 'satellite', 'image', 'sequences', 'are', 'multidimensional', 'signals', 'composed', 'of', 'spatiotemporal', 'patterns', 'associated', 'to', 'numerous', 'and', 'various', 'phenomena', 'bayesian', 'methods', 'have', 'been', 'previously', 'proposed', 'in', 'heas', 'and', 'datcu', '2005', 'to', 'co... | [-0.0525637097235718, 0.04062476908026867, -0.10954946383714811, 0.11124333249113723, -0.12721473253363974, -0.1318593966459949, 0.04469763865262763, 0.4554652894111393, -0.3158108751846639, -0.3415851244218137, 0.05827618105715506, -0.27089852564670486, -0.20408367873041902, 0.18076300976657603, -0.12932869302296, 0.1... |
709.3014 | Future precision neutrino experiments and their theoretical implications | Future neutrino oscillation measurement focus, at first priority, on the
discovery of sin^2(2 theta_13) describing the coupling between solar and
atmospheric oscillations. In this talk, we briefly discuss the prospects to
measure sin^2(2 theta_13) by future reactor and beam experiments, and we
illustrate the usefulne... | hep-ph | future neutrino oscillation measurement focus at first priority on the discovery of sin22 theta_13 describing the coupling between solar and atmospheric oscillations in this talk we briefly discuss the prospects to measure sin22 theta_13 by future reactor and beam experiments and we illustrate the usefulness of these m... | [['future', 'neutrino', 'oscillation', 'measurement', 'focus', 'at', 'first', 'priority', 'on', 'the', 'discovery', 'of', 'sin22', 'theta_13', 'describing', 'the', 'coupling', 'between', 'solar', 'and', 'atmospheric', 'oscillations', 'in', 'this', 'talk', 'we', 'briefly', 'discuss', 'the', 'prospects', 'to', 'measure',... | [-0.11154635452354948, 0.2239696915205665, 0.023414557760891814, 0.061972374397252374, -0.057830980978906155, -0.10549784934458634, 0.152157429450502, 0.33249677658701937, -0.23643756872043015, -0.33772353604435923, 0.1320944808947388, -0.33080827275601526, -0.10831193211488425, 0.2559599582105875, 0.002456355226847033... |
709.3015 | Observational evidence for AGN feedback in early-type galaxies | A major amendment in recent models of hierarchical galaxy formation is the
inclusion of so-called AGN feedback. The energy input from an active central
massive black hole is invoked to suppress star formation in early-type galaxies
at later epochs. A major problem is that this process is poorly understood, and
compel... | astro-ph | a major amendment in recent models of hierarchical galaxy formation is the inclusion of socalled agn feedback the energy input from an active central massive black hole is invoked to suppress star formation in earlytype galaxies at later epochs a major problem is that this process is poorly understood and compelling ob... | [['a', 'major', 'amendment', 'in', 'recent', 'models', 'of', 'hierarchical', 'galaxy', 'formation', 'is', 'the', 'inclusion', 'of', 'socalled', 'agn', 'feedback', 'the', 'energy', 'input', 'from', 'an', 'active', 'central', 'massive', 'black', 'hole', 'is', 'invoked', 'to', 'suppress', 'star', 'formation', 'in', 'early... | [-0.044326370715987766, 0.10859520726227084, -0.08279515095574366, 0.11564448852560882, -0.10095337768279605, -0.04494941469931828, 0.0754012845430637, 0.4627338191829354, -0.15161012147055777, -0.354574544428975, 0.055597883499673026, -0.28835478318493357, -0.05729768464924674, 0.16580828844771467, -0.0760433908121445... |
709.3016 | On the ideal $(v^0)$ | The $\sigma$-ideal $(v^0)$ is associated with the Silver forcing, see
\cite{bre}. Also, it constitutes the family of all completely doughnut null
sets, see \cite{hal}. We introduce segments and $*$-segments topologies, to
state some resemblances of $(v^0)$ to the family of Ramsey null sets. To
describe $add(v^0)$ we ... | math.LO math.CO math.GN | the sigmaideal v0 is associated with the silver forcing see citebre also it constitutes the family of all completely doughnut null sets see citehal we introduce segments and segments topologies to state some resemblances of v0 to the family of ramsey null sets to describe addv0 we adopt a proof of base matrix lemma con... | [['the', 'sigmaideal', 'v0', 'is', 'associated', 'with', 'the', 'silver', 'forcing', 'see', 'citebre', 'also', 'it', 'constitutes', 'the', 'family', 'of', 'all', 'completely', 'doughnut', 'null', 'sets', 'see', 'citehal', 'we', 'introduce', 'segments', 'and', 'segments', 'topologies', 'to', 'state', 'some', 'resemblanc... | [-0.22326556254411117, 0.08394450521445833, -0.06000120483804494, 0.060472919317544435, -0.05161202032468282, -0.21975239518505987, 0.04893713118508458, 0.36987265998031943, -0.27049359044758603, -0.16298806237755342, 0.06702031491149682, -0.261929304205114, -0.07056304673897103, 0.13880741661705542, -0.096437437820713... |
709.3017 | Emergent Fermions and Anyons in the Kitaev Model | We study the gapped phase of the Kitaev model on the honeycomb lattice using
perturbative continuous unitary transformations. The effective low-energy
Hamiltonian is found to be an extended toric code with interacting anyons.
High-energy excitations are emerging free fermions which are composed of
hardcore bosons wit... | cond-mat.other quant-ph | we study the gapped phase of the kitaev model on the honeycomb lattice using perturbative continuous unitary transformations the effective lowenergy hamiltonian is found to be an extended toric code with interacting anyons highenergy excitations are emerging free fermions which are composed of hardcore bosons with an a... | [['we', 'study', 'the', 'gapped', 'phase', 'of', 'the', 'kitaev', 'model', 'on', 'the', 'honeycomb', 'lattice', 'using', 'perturbative', 'continuous', 'unitary', 'transformations', 'the', 'effective', 'lowenergy', 'hamiltonian', 'is', 'found', 'to', 'be', 'an', 'extended', 'toric', 'code', 'with', 'interacting', 'anyon... | [-0.13479820920016478, 0.22918040613903604, -0.08687596749169407, 0.07231352522676052, -0.026374172430088813, -0.17379715882189986, 0.0178739873334524, 0.3671397430718773, -0.2350758382084745, -0.23304606824745455, 0.015994109158378303, -0.2988373692130187, -0.11265693179599044, 0.1262683410777417, 0.054426463877057865... |
709.3018 | Nature and statistics of majority rankings in a dynamical model of
preference aggregation | We present numerical results on a complex dynamical model for the aggregation
of many individual rankings of S alternatives by the pairwise majority rule
under a deliberative scenario. Agents are assumed to interact when the Kemeny
distance between their rankings is smaller than a range R. The main object of
interest... | physics.soc-ph | we present numerical results on a complex dynamical model for the aggregation of many individual rankings of s alternatives by the pairwise majority rule under a deliberative scenario agents are assumed to interact when the kemeny distance between their rankings is smaller than a range r the main object of interest is ... | [['we', 'present', 'numerical', 'results', 'on', 'a', 'complex', 'dynamical', 'model', 'for', 'the', 'aggregation', 'of', 'many', 'individual', 'rankings', 'of', 's', 'alternatives', 'by', 'the', 'pairwise', 'majority', 'rule', 'under', 'a', 'deliberative', 'scenario', 'agents', 'are', 'assumed', 'to', 'interact', 'whe... | [-0.13407208993082384, 0.1296921574657231, -0.041971864461622856, 0.07283312734302685, -0.05358017887575207, -0.14414636348977822, 0.09218013793816444, 0.3683228623949819, -0.2554695781458307, -0.29650403667080727, 0.04439147324818704, -0.3066912291019603, -0.14232959751453664, 0.18354552742956137, -0.04008715700496126... |
709.3019 | Neutrino-induced coherent pion production | We have investigated the neutrino induced coherent pion production reaction
at the energies of interest for recent experiments like K2K and MiniBooNE. The
model includes pion, nucleon and the Delta(1232) resonance. Medium effects in
the production mechanism and the distortion of the pion wave function are taken
into ... | nucl-th hep-ex hep-ph nucl-ex | we have investigated the neutrino induced coherent pion production reaction at the energies of interest for recent experiments like k2k and miniboone the model includes pion nucleon and the delta1232 resonance medium effects in the production mechanism and the distortion of the pion wave function are taken into account... | [['we', 'have', 'investigated', 'the', 'neutrino', 'induced', 'coherent', 'pion', 'production', 'reaction', 'at', 'the', 'energies', 'of', 'interest', 'for', 'recent', 'experiments', 'like', 'k2k', 'and', 'miniboone', 'the', 'model', 'includes', 'pion', 'nucleon', 'and', 'the', 'delta1232', 'resonance', 'medium', 'effe... | [-0.0888283239380937, 0.22977399504049978, -0.039401568990371665, 0.1575117181996478, -0.001200016607788015, -0.017108783841707765, 0.05979400337673724, 0.3291394708435388, -0.18791265266035942, -0.22714222725877103, -0.0618304417733638, -0.38034134085706256, -0.027232974123685284, 0.1521946339684717, 0.120962726546728... |
709.302 | Transverse momentum dependence of semi-inclusive pion production | Cross sections for semi-inclusive electroproduction of charged pions
($\pi^{\pm}$) from both proton and deuteron targets were measured for
$0.2<x<0.5$, $2<Q^2<4$ GeV$^2$, $0.3<z<1$, and $P_t^2<0.2$ GeV$^2$. For
$P_t<0.1$ GeV, we find the azimuthal dependence to be small, as expected
theoretically. For both $\pi^+$ an... | hep-ph | cross sections for semiinclusive electroproduction of charged pions pipm from both proton and deuteron targets were measured for 02x05 2q24 gev2 03z1 and p_t202 gev2 for p_t01 gev we find the azimuthal dependence to be small as expected theoretically for both pi and pi the p_t dependence from the deuteron is found to b... | [['cross', 'sections', 'for', 'semiinclusive', 'electroproduction', 'of', 'charged', 'pions', 'pipm', 'from', 'both', 'proton', 'and', 'deuteron', 'targets', 'were', 'measured', 'for', '02x05', '2q24', 'gev2', '03z1', 'and', 'p_t202', 'gev2', 'for', 'p_t01', 'gev', 'we', 'find', 'the', 'azimuthal', 'dependence', 'to', ... | [-0.01792616227340668, 0.29091304614951813, -0.11125523925316755, 0.1878871089811766, -0.03502326398485839, -0.09433958999638568, -0.018867633150269587, 0.3615575115939583, -0.16018043381792277, -0.2321178342093422, -0.11783206444163101, -0.33347695648218645, 0.09246288877770756, 0.19661419753766043, 0.1064639182083986... |
709.3021 | Hankel hyperdeterminants, rectangular Jack polynomials and even powers
of the Vandermonde | We investigate the link between rectangular Jack polynomials and Hankel
hyperdeterminants. As an application we give an expression of the even power of
the Vandermonde in term of Jack polynomials.
| math.CO | we investigate the link between rectangular jack polynomials and hankel hyperdeterminants as an application we give an expression of the even power of the vandermonde in term of jack polynomials | [['we', 'investigate', 'the', 'link', 'between', 'rectangular', 'jack', 'polynomials', 'and', 'hankel', 'hyperdeterminants', 'as', 'an', 'application', 'we', 'give', 'an', 'expression', 'of', 'the', 'even', 'power', 'of', 'the', 'vandermonde', 'in', 'term', 'of', 'jack', 'polynomials']] | [-0.2503532334851722, 0.009401455995975994, -0.024611139359573524, 0.0688620057888329, -0.07271168970813353, -0.09832396411026517, 0.001772682617108027, 0.3296035224571824, -0.3038810345887517, -0.16850983115533988, 0.1426794102221417, -0.2722902201736967, -0.2706960057839751, 0.17593851573813785, -0.0785216536683341, ... |
709.3022 | BCB Based Packaging for Low Actuation Voltage RF MEMS Devices | This paper outlines the issues related to RF MEMS packaging and low actuation
voltage. An original approach is presented concerning the modeling of
capacitive contacts using multiphysics simulation and advanced
characterization. A similar approach is used concerning packaging development
where multi-physics simulatio... | physics.class-ph | this paper outlines the issues related to rf mems packaging and low actuation voltage an original approach is presented concerning the modeling of capacitive contacts using multiphysics simulation and advanced characterization a similar approach is used concerning packaging development where multiphysics simulations ar... | [['this', 'paper', 'outlines', 'the', 'issues', 'related', 'to', 'rf', 'mems', 'packaging', 'and', 'low', 'actuation', 'voltage', 'an', 'original', 'approach', 'is', 'presented', 'concerning', 'the', 'modeling', 'of', 'capacitive', 'contacts', 'using', 'multiphysics', 'simulation', 'and', 'advanced', 'characterization'... | [-0.11146471334896127, 0.023929893766524133, -0.008202770488245076, -0.03434753916345009, -0.09839290508725604, -0.20052930008864306, -0.05058568705171041, 0.3899529138427289, -0.23842514384171512, -0.335257978315969, 0.1211159930060633, -0.21674458075650646, -0.18576951511204243, 0.30344020871476074, -0.10855418846744... |
709.3023 | IGR J22517+2218=MG3 J225155+2217: a new gamma-ray lighthouse in the
distant Universe | We report on the identification of a new soft gamma ray source, namely IGR
J22517+2218, detected with IBIS/INTEGRAL. The source, which has an observed
20-100 keV flux of ~4 x10^-11 erg cm-2 s-1, is spatially coincident with MG3
J225155+2217, a quasar at z=3.668. The Swift/XRT 0.5-10 keV continuum is flat
(Gamma=1.5) ... | astro-ph | we report on the identification of a new soft gamma ray source namely igr j225172218 detected with ibisintegral the source which has an observed 20100 kev flux of 4 x1011 erg cm2 s1 is spatially coincident with mg3 j2251552217 a quasar at z3668 the swiftxrt 0510 kev continuum is flat gamma15 with evidence for a spectra... | [['we', 'report', 'on', 'the', 'identification', 'of', 'a', 'new', 'soft', 'gamma', 'ray', 'source', 'namely', 'igr', 'j225172218', 'detected', 'with', 'ibisintegral', 'the', 'source', 'which', 'has', 'an', 'observed', '20100', 'kev', 'flux', 'of', '4', 'x1011', 'erg', 'cm2', 's1', 'is', 'spatially', 'coincident', 'wit... | [-0.06442673642844579, 0.14272717894496784, -0.010819205102254998, 0.1179761009803826, -0.10572854781941356, -0.16115716936240465, 0.055464054781152176, 0.5149400810146502, -0.13373396284890318, -0.3712156370456796, 0.07565403340560495, -0.3696295281563321, 0.05128437155071125, 0.22435250085744757, 0.00434674867645987,... |
709.3024 | Non-linear self-consistent response of graphene in time domain | We study the non-linear electromagnetic response of graphene taking into
account the self-consistent-field effects. Response of the system to a strong
pulse excitation is calculated. It is shown that radiative decay in graphene
differs from that of conventional two-dimensional electron systems both
quantitatively and... | cond-mat.mes-hall | we study the nonlinear electromagnetic response of graphene taking into account the selfconsistentfield effects response of the system to a strong pulse excitation is calculated it is shown that radiative decay in graphene differs from that of conventional twodimensional electron systems both quantitatively and qualita... | [['we', 'study', 'the', 'nonlinear', 'electromagnetic', 'response', 'of', 'graphene', 'taking', 'into', 'account', 'the', 'selfconsistentfield', 'effects', 'response', 'of', 'the', 'system', 'to', 'a', 'strong', 'pulse', 'excitation', 'is', 'calculated', 'it', 'is', 'shown', 'that', 'radiative', 'decay', 'in', 'graphen... | [-0.11162177905046927, 0.15398498427058602, -0.05516716296752465, 0.08750514468531413, -0.008981495421251347, -0.10678334366369607, -0.02937702743079642, 0.3878968035609558, -0.24201776530465174, -0.24771832931658316, -0.01232684255730168, -0.30695724685210735, -0.17073040796797082, 0.2575975013575677, 0.06689560270450... |
709.3025 | Hard X-ray colours of Neutron Star and Black Hole Low Mass X-ray
Binaries with INTEGRAL | The X-ray spectra of Low Mass X-ray Binaries (LMXB) can change on short
time-scales, making it difficult to follow their spectral characteristics in
detail through model fitting. Colour-colour (C-C) diagrams are therefore often
used as alternative, model independent, tools to study the spectral variability
of these s... | astro-ph | the xray spectra of low mass xray binaries lmxb can change on short timescales making it difficult to follow their spectral characteristics in detail through model fitting colourcolour cc diagrams are therefore often used as alternative model independent tools to study the spectral variability of these sources the inte... | [['the', 'xray', 'spectra', 'of', 'low', 'mass', 'xray', 'binaries', 'lmxb', 'can', 'change', 'on', 'short', 'timescales', 'making', 'it', 'difficult', 'to', 'follow', 'their', 'spectral', 'characteristics', 'in', 'detail', 'through', 'model', 'fitting', 'colourcolour', 'cc', 'diagrams', 'are', 'therefore', 'often', 'u... | [-0.06935804501907634, 0.07670435367617756, -0.10135810342617332, 0.18358998897102927, -0.12201568222371861, -0.07603470712700593, 0.09188413960593088, 0.4577585659255939, -0.20126239883580377, -0.3890232342345241, 0.10882462075720209, -0.3221823160155119, -0.033397724100255544, 0.25815436925373175, -0.0410317495066140... |
709.3026 | Chern numbers and the geometry of partial flag manifolds | We calculate the Chern classes and Chern numbers for the natural almost
Hermitian structures of the partial flag manifolds F_n=SU(n+2)/S(U(n)\times
U(1)\times U(1)). For all n>1 there are two invariant complex algebraic
structures, which arise from the projectivizations of the holomorphic tangent
and cotangent bundle... | math.DG math.AG | we calculate the chern classes and chern numbers for the natural almost hermitian structures of the partial flag manifolds f_nsun2suntimes u1times u1 for all n1 there are two invariant complex algebraic structures which arise from the projectivizations of the holomorphic tangent and cotangent bundles of complex project... | [['we', 'calculate', 'the', 'chern', 'classes', 'and', 'chern', 'numbers', 'for', 'the', 'natural', 'almost', 'hermitian', 'structures', 'of', 'the', 'partial', 'flag', 'manifolds', 'f_nsun2suntimes', 'u1times', 'u1', 'for', 'all', 'n1', 'there', 'are', 'two', 'invariant', 'complex', 'algebraic', 'structures', 'which',... | [-0.2795073303606103, 0.12378943860280157, -0.037596884930487906, 0.1338544292191025, -0.14440349378337217, -0.11671401516506726, -0.07084146190877302, 0.37728017299334604, -0.3067397003311037, -0.16878357898480822, 0.07488382361958375, -0.23896841508437797, -0.23960415266527987, 0.15643374191275522, -0.106979672428183... |
709.3027 | Phase diagram of a two-component Fermi gas with resonant interactions | The pairing of fermions is at the heart of superconductivity and
superfluidity. The recent experimental realization of strongly interacting
atomic Fermi gases has opened a new, controllable way to study novel forms of
pairing and superfluidity. A major controversial issue has been the stability
of superfluidity again... | cond-mat.soft | the pairing of fermions is at the heart of superconductivity and superfluidity the recent experimental realization of strongly interacting atomic fermi gases has opened a new controllable way to study novel forms of pairing and superfluidity a major controversial issue has been the stability of superfluidity against an... | [['the', 'pairing', 'of', 'fermions', 'is', 'at', 'the', 'heart', 'of', 'superconductivity', 'and', 'superfluidity', 'the', 'recent', 'experimental', 'realization', 'of', 'strongly', 'interacting', 'atomic', 'fermi', 'gases', 'has', 'opened', 'a', 'new', 'controllable', 'way', 'to', 'study', 'novel', 'forms', 'of', 'pa... | [-0.18254143249054677, 0.2401003295446749, -0.11290297226372698, 0.02212679030078395, -0.009175360921157024, -0.15150049881918765, 0.12829077099421538, 0.32320069587539607, -0.24319307503245044, -0.22952832766842643, 0.0025095329009473507, -0.32739045982044646, -0.0821977221497857, 0.1278034201865766, 0.061699340826968... |
709.3028 | Emerging complexity in a simple model of the mechanical behaviour of
rocks | We propose a mechanical model for the behaviour of rocks based on progressive
damage at the elementary scale and elastic interaction. It allows us to
simulate several experimental observations: mechanical behaviour ranging from
brittle to ductile, fractal structure of the damage, powerlaw distribution of
the damage a... | physics.geo-ph | we propose a mechanical model for the behaviour of rocks based on progressive damage at the elementary scale and elastic interaction it allows us to simulate several experimental observations mechanical behaviour ranging from brittle to ductile fractal structure of the damage powerlaw distribution of the damage avalanc... | [['we', 'propose', 'a', 'mechanical', 'model', 'for', 'the', 'behaviour', 'of', 'rocks', 'based', 'on', 'progressive', 'damage', 'at', 'the', 'elementary', 'scale', 'and', 'elastic', 'interaction', 'it', 'allows', 'us', 'to', 'simulate', 'several', 'experimental', 'observations', 'mechanical', 'behaviour', 'ranging', '... | [-0.0775412512860973, 0.20133978351676726, -0.12350082726847819, 0.058231793924150066, -0.06936311078367426, -0.09223521109122564, 0.011842131754383445, 0.35844191501793615, -0.32531708764898426, -0.3123835316585267, 0.06230409573215772, -0.27910668629457874, -0.18385130895493443, 0.16322917593916988, -0.00554763492854... |
709.3029 | (Co)homology of quantum complete intersections | We construct a minimal projective bimodule resolution for every finite
dimensional quantum complete intersection of codimension two. Then we use this
resolution to compute both the Hochschild cohomology and homology for such an
algebra. In particular, we show that the cohomology vanishes in high degrees,
while the ho... | math.KT math.QA | we construct a minimal projective bimodule resolution for every finite dimensional quantum complete intersection of codimension two then we use this resolution to compute both the hochschild cohomology and homology for such an algebra in particular we show that the cohomology vanishes in high degrees while the homology... | [['we', 'construct', 'a', 'minimal', 'projective', 'bimodule', 'resolution', 'for', 'every', 'finite', 'dimensional', 'quantum', 'complete', 'intersection', 'of', 'codimension', 'two', 'then', 'we', 'use', 'this', 'resolution', 'to', 'compute', 'both', 'the', 'hochschild', 'cohomology', 'and', 'homology', 'for', 'such'... | [-0.22415777266609901, 0.06710681674674418, -0.06644598969860989, 0.058040143565877396, -0.05417788368375862, -0.14833360339752308, -0.08990641944932148, 0.35676654900296356, -0.3763514440141472, -0.15397030348871268, 0.11665556085405543, -0.22828106258941047, -0.14569961770857667, 0.11264122153321902, -0.1952595146939... |
709.303 | Recent results on (anti)nucleus and (anti)hyperon production in
nucleus-nucleus collisions at CERN SPS energies | The NA49 experiment has collected comprehensive data on particle production
in nucleus-nucleus collisions over the whole SPS beam energies range, the
critical energy domain where the expected phase transition to a deconfined
phase is expected to occur. The latest results from Pb+Pb collisions between
20$A$ GeV and 15... | nucl-ex | the na49 experiment has collected comprehensive data on particle production in nucleusnucleus collisions over the whole sps beam energies range the critical energy domain where the expected phase transition to a deconfined phase is expected to occur the latest results from pbpb collisions between 20a gev and 158a gev o... | [['the', 'na49', 'experiment', 'has', 'collected', 'comprehensive', 'data', 'on', 'particle', 'production', 'in', 'nucleusnucleus', 'collisions', 'over', 'the', 'whole', 'sps', 'beam', 'energies', 'range', 'the', 'critical', 'energy', 'domain', 'where', 'the', 'expected', 'phase', 'transition', 'to', 'a', 'deconfined',... | [-0.03713370203350981, 0.22571165857629644, -0.15004385591484606, 0.1553924245454578, 0.061398822199553255, -0.08889092791825533, -0.03545382024927272, 0.3319295035323335, -0.18082909811081158, -0.33147787338433166, -0.08229765561667995, -0.40375959294537705, 0.14402900704881177, 0.16806899013359927, 0.0842420371158772... |
709.3031 | On the origin of ultra high energy cosmic rays: Subluminal and
superluminal relativistic shocks | The flux of Ultra High Energy Cosmic Rays (UHECRs) at $E>10^{18.5}$ eV is
believed to arise in plasma shock environments in extragalactic sources. In
this paper, we present a systematic study of particle acceleration by
relativistic shocks, in particular concerning the dependence on bulk Lorentz
factor and the angle ... | astro-ph | the flux of ultra high energy cosmic rays uhecrs at e10185 ev is believed to arise in plasma shock environments in extragalactic sources in this paper we present a systematic study of particle acceleration by relativistic shocks in particular concerning the dependence on bulk lorentz factor and the angle between the ma... | [['the', 'flux', 'of', 'ultra', 'high', 'energy', 'cosmic', 'rays', 'uhecrs', 'at', 'e10185', 'ev', 'is', 'believed', 'to', 'arise', 'in', 'plasma', 'shock', 'environments', 'in', 'extragalactic', 'sources', 'in', 'this', 'paper', 'we', 'present', 'a', 'systematic', 'study', 'of', 'particle', 'acceleration', 'by', 'rel... | [-0.07451334253605456, 0.24305325879901649, -0.016257714999839662, 0.19778496848512442, -0.04695170739083551, -0.07747256690496579, 0.006779268138401676, 0.4567716510742903, -0.19530448000878095, -0.35931911173742265, -0.00945125792408362, -0.3093013103678823, 0.037872388523072, 0.25180052098771555, 0.03707032714784145... |
709.3032 | Erratum: algebraic spin liquid as the mother of many competing orders | We correct an error in our paper Phys. Rev. B 72, 104404 (2005)
[cond-mat/0502215]. We show that a particular fermion bilinear is not related
to the other ``competing orders'' of the algebraic spin liquid, and does not
possess their slowly decaying correlations. For the square lattice staggered
flux spin liquid (equi... | cond-mat.str-el | we correct an error in our paper phys rev b 72 104404 2005 condmat0502215 we show that a particular fermion bilinear is not related to the other competing orders of the algebraic spin liquid and does not possess their slowly decaying correlations for the square lattice staggered flux spin liquid equivalently dwave rvb ... | [['we', 'correct', 'an', 'error', 'in', 'our', 'paper', 'phys', 'rev', 'b', '72', '104404', '2005', 'condmat0502215', 'we', 'show', 'that', 'a', 'particular', 'fermion', 'bilinear', 'is', 'not', 'related', 'to', 'the', 'other', 'competing', 'orders', 'of', 'the', 'algebraic', 'spin', 'liquid', 'and', 'does', 'not', 'po... | [-0.15174649846740068, 0.2739135025634217, -0.0363512744816641, 0.034355952451005575, -0.10467732598384222, -0.1383705365859593, 0.06770950116721602, 0.3655537082348019, -0.2126075153471902, -0.25240065620358415, 0.008891717878092701, -0.28665492286284766, -0.08474239045754076, 0.10388994173457225, -0.03079649298451841... |
709.3033 | Comparison of quantization of charge transport in periodic and open
pumps | We compare the charges transported in two systems, a spatially periodic and
an open quantum pump, both depending periodically and adiabatically on time.
The charge transported in a cycle was computed by Thouless, respectively by
Buttiker et al. in the two cases. We show that the results agree in the limit
where the t... | math-ph cond-mat.mes-hall math.MP | we compare the charges transported in two systems a spatially periodic and an open quantum pump both depending periodically and adiabatically on time the charge transported in a cycle was computed by thouless respectively by buttiker et al in the two cases we show that the results agree in the limit where the two physi... | [['we', 'compare', 'the', 'charges', 'transported', 'in', 'two', 'systems', 'a', 'spatially', 'periodic', 'and', 'an', 'open', 'quantum', 'pump', 'both', 'depending', 'periodically', 'and', 'adiabatically', 'on', 'time', 'the', 'charge', 'transported', 'in', 'a', 'cycle', 'was', 'computed', 'by', 'thouless', 'respectiv... | [-0.16855749529504188, 0.22034494913466254, -0.03505536477843469, 0.021535993342033842, 0.0650429640271327, -0.14117660039725402, 0.05951668966956662, 0.3541123605700153, -0.24140676067944503, -0.2833708137499564, 0.08793169776485725, -0.26767149720002303, -0.09623594815617031, 0.2694599495805574, -0.05257730285291362,... |
709.3034 | Query Evaluation in P2P Systems of Taxonomy-based Sources: Algorithms,
Complexity, and Optimizations | In this study, we address the problem of answering queries over a
peer-to-peer system of taxonomy-based sources. A taxonomy states subsumption
relationships between negation-free DNF formulas on terms and negation-free
conjunctions of terms. To the end of laying the foundations of our study, we
first consider the cen... | cs.DB cs.DC cs.DS cs.LO | in this study we address the problem of answering queries over a peertopeer system of taxonomybased sources a taxonomy states subsumption relationships between negationfree dnf formulas on terms and negationfree conjunctions of terms to the end of laying the foundations of our study we first consider the centralized ca... | [['in', 'this', 'study', 'we', 'address', 'the', 'problem', 'of', 'answering', 'queries', 'over', 'a', 'peertopeer', 'system', 'of', 'taxonomybased', 'sources', 'a', 'taxonomy', 'states', 'subsumption', 'relationships', 'between', 'negationfree', 'dnf', 'formulas', 'on', 'terms', 'and', 'negationfree', 'conjunctions', ... | [-0.14232924103190372, -0.022914837999653374, -0.05531174794305116, 0.06988703773418416, -0.10228371089841756, -0.12591606393753965, 0.13097520804472473, 0.37678468217200134, -0.2772851572339682, -0.30375754840982455, 0.10085254338951523, -0.2543886601326651, -0.17208104841928515, 0.18479406801149403, -0.12320349215537... |
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