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 |
|---|---|---|---|---|---|---|
708.3049 | Photoabsorption in a plasma in a high magnetic field | Photo-absorption in fully ionized plasmas in high magnetic fields is
re-examined, using the methods of many-body quantum field theory. For
frequencies in the immediate vicinity of the electron cyclotron resonance the
rates we obtain disagree markedly from those in the literature. The new element
in our work that caus... | astro-ph | photoabsorption in fully ionized plasmas in high magnetic fields is reexamined using the methods of manybody quantum field theory for frequencies in the immediate vicinity of the electron cyclotron resonance the rates we obtain disagree markedly from those in the literature the new element in our work that causes most ... | [['photoabsorption', 'in', 'fully', 'ionized', 'plasmas', 'in', 'high', 'magnetic', 'fields', 'is', 'reexamined', 'using', 'the', 'methods', 'of', 'manybody', 'quantum', 'field', 'theory', 'for', 'frequencies', 'in', 'the', 'immediate', 'vicinity', 'of', 'the', 'electron', 'cyclotron', 'resonance', 'the', 'rates', 'we'... | [-0.09676882524777633, 0.1166726209787437, -0.032767228777699456, 0.04783357253584724, -0.024246348708402365, -0.03820554035561285, 0.04411780532525601, 0.33291766457617855, -0.1693095432139951, -0.2905508183623449, 0.03282965313253673, -0.3265196753021043, -0.0871660073977322, 0.23232009505031434, 0.001174016181511643... |
708.305 | Entangled-like Chain Dynamics in Non-entangled Polymer Blends with Large
Dynamic Asymmetry | We discuss simulations of a simple model for polymer blends in the framework
of the Rouse model. At odds with standard predictions, large dynamic asymmetry
between the two components induces strong non-exponentiality of the Rouse modes
for the fast component. Despite chains being much shorter than the entanglement
le... | cond-mat.soft | we discuss simulations of a simple model for polymer blends in the framework of the rouse model at odds with standard predictions large dynamic asymmetry between the two components induces strong nonexponentiality of the rouse modes for the fast component despite chains being much shorter than the entanglement length i... | [['we', 'discuss', 'simulations', 'of', 'a', 'simple', 'model', 'for', 'polymer', 'blends', 'in', 'the', 'framework', 'of', 'the', 'rouse', 'model', 'at', 'odds', 'with', 'standard', 'predictions', 'large', 'dynamic', 'asymmetry', 'between', 'the', 'two', 'components', 'induces', 'strong', 'nonexponentiality', 'of', 't... | [-0.15988584889377327, 0.19900285094794443, -0.09862853617717822, 0.08271979422833042, -0.061186264568789936, -0.189455383489358, 0.0012222269306430358, 0.3779989604720439, -0.3034059580886501, -0.24726497159264554, 0.04154079817315756, -0.2706664128164793, -0.09261141413683607, 0.14856147464771552, 0.06274721066563807... |
708.3051 | Topological Higher Gauge Theory - from BF to BFCG theory | We study generalizations of 3- and 4-dimensional BF-theory in the context of
higher gauge theory. First, we construct topological higher gauge theories as
discrete state sum models and explain how they are related to the state sums of
Yetter, Mackaay, and Porter. Under certain conditions, we can present their
corresp... | hep-th gr-qc | we study generalizations of 3 and 4dimensional bftheory in the context of higher gauge theory first we construct topological higher gauge theories as discrete state sum models and explain how they are related to the state sums of yetter mackaay and porter under certain conditions we can present their corresponding cont... | [['we', 'study', 'generalizations', 'of', '3', 'and', '4dimensional', 'bftheory', 'in', 'the', 'context', 'of', 'higher', 'gauge', 'theory', 'first', 'we', 'construct', 'topological', 'higher', 'gauge', 'theories', 'as', 'discrete', 'state', 'sum', 'models', 'and', 'explain', 'how', 'they', 'are', 'related', 'to', 'the... | [-0.10714600694158839, 0.1597466427147285, -0.08883892363972135, 0.118204463697556, -0.08312869739666995, -0.12398090145757629, -0.024341945235048318, 0.3415406082860298, -0.22042665744407308, -0.29307177336886525, 0.10059126107824139, -0.2635362462864982, -0.2079187986958358, 0.13225188378192898, -0.0849924246677094, ... |
708.3052 | Studying the MSSM Higgs sector by forward proton tagging at the LHC | We show that the use of forward proton detectors at the LHC installed at 220
m and 420 m distance around ATLAS and / or CMS can provide important
information on the Higgs sector of the MSSM. We analyse central exclusive
production of the neutral CP-even Higgs bosons h and H and their decays into
bottom quarks, tau le... | hep-ph | we show that the use of forward proton detectors at the lhc installed at 220 m and 420 m distance around atlas and or cms can provide important information on the higgs sector of the mssm we analyse central exclusive production of the neutral cpeven higgs bosons h and h and their decays into bottom quarks tau leptons a... | [['we', 'show', 'that', 'the', 'use', 'of', 'forward', 'proton', 'detectors', 'at', 'the', 'lhc', 'installed', 'at', '220', 'm', 'and', '420', 'm', 'distance', 'around', 'atlas', 'and', 'or', 'cms', 'can', 'provide', 'important', 'information', 'on', 'the', 'higgs', 'sector', 'of', 'the', 'mssm', 'we', 'analyse', 'cent... | [-0.0660867348853618, 0.27700011903802174, -0.030983993635835268, 0.18769652884787855, -0.06516439957209887, -0.21220240696707968, 0.06872819329220921, 0.3263971412058872, -0.19071396433103543, -0.260476212315739, -0.0068777496407841305, -0.3104445550841494, 0.0783256013229943, 0.1433093894395428, 0.08706511983062881, ... |
708.3053 | Stability conditions on generic complex tori | In this paper we describe a simply connected component of the complex
manifold of stability conditions on the bounded derived category of a generic
complex torus of any dimension. A torus is called generic if there are no
nontrivial integral (p,p)-classes. We give an explicit description of all
stability conditions i... | math.AG | in this paper we describe a simply connected component of the complex manifold of stability conditions on the bounded derived category of a generic complex torus of any dimension a torus is called generic if there are no nontrivial integral ppclasses we give an explicit description of all stability conditions in that c... | [['in', 'this', 'paper', 'we', 'describe', 'a', 'simply', 'connected', 'component', 'of', 'the', 'complex', 'manifold', 'of', 'stability', 'conditions', 'on', 'the', 'bounded', 'derived', 'category', 'of', 'a', 'generic', 'complex', 'torus', 'of', 'any', 'dimension', 'a', 'torus', 'is', 'called', 'generic', 'if', 'ther... | [-0.24600922934851557, 0.0727887341320484, -0.07358155833592392, 0.043306935596156795, -0.10719362914316216, -0.11759899459111522, -0.04064279657410774, 0.3642903752976431, -0.2383736680296935, -0.15151379610640262, 0.1535421610888937, -0.17902582970816852, -0.19860491434217625, 0.20604200583865057, -0.1071194527881606... |
708.3054 | Numerical Simulations of HH 555 | We present 3D gasdynamic simulations of the Herbig Haro object HH 555. HH 555
is a bipolar jet emerging from the tip of an elephant trunk entering the
Pelican Nebula from the adjacent molecular cloud. Both beams of HH 555 are
curved away from the center of the H II region. This indicates that they are
being deflected... | astro-ph | we present 3d gasdynamic simulations of the herbig haro object hh 555 hh 555 is a bipolar jet emerging from the tip of an elephant trunk entering the pelican nebula from the adjacent molecular cloud both beams of hh 555 are curved away from the center of the h ii region this indicates that they are being deflected by a... | [['we', 'present', '3d', 'gasdynamic', 'simulations', 'of', 'the', 'herbig', 'haro', 'object', 'hh', '555', 'hh', '555', 'is', 'a', 'bipolar', 'jet', 'emerging', 'from', 'the', 'tip', 'of', 'an', 'elephant', 'trunk', 'entering', 'the', 'pelican', 'nebula', 'from', 'the', 'adjacent', 'molecular', 'cloud', 'both', 'beams... | [-0.11003278867979183, 0.1462096017215902, -0.05637455814507948, 0.022378854338829458, -0.0558793771699313, -0.0858880559164049, 0.01526066613726533, 0.4202056902188418, -0.2408466366648595, -0.3073601498210127, 0.048209720010245524, -0.30731731925381595, -0.004007522626157971, 0.18326799027892401, -0.00984038607167359... |
708.3055 | Fourier transform on locally compact quantum groups | The notion of Fourier transform is among the more important tools in
analysis, which has been generalized in abstract harmonic analysis to the level
of abelian locally compact groups. The aim of this paper is to further
generalize the Fourier transform: Motivated by some recent works by Van Daele
in the multiplier Ho... | math.OA math.QA | the notion of fourier transform is among the more important tools in analysis which has been generalized in abstract harmonic analysis to the level of abelian locally compact groups the aim of this paper is to further generalize the fourier transform motivated by some recent works by van daele in the multiplier hopf al... | [['the', 'notion', 'of', 'fourier', 'transform', 'is', 'among', 'the', 'more', 'important', 'tools', 'in', 'analysis', 'which', 'has', 'been', 'generalized', 'in', 'abstract', 'harmonic', 'analysis', 'to', 'the', 'level', 'of', 'abelian', 'locally', 'compact', 'groups', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', ... | [-0.08073197437661599, 0.08415935227381821, -0.17991651775816284, 0.08547929613048821, -0.11258373331247258, -0.07550737955959655, 0.015554984934635837, 0.3570981839311724, -0.34177238380285996, -0.1839385265014878, 0.12904319959250474, -0.22721657360426517, -0.20933951331036432, 0.22781867374266898, -0.105254270077659... |
708.3056 | Schwinger-Dyson operator of Yang-Mills matrix models with ghosts and
derivations of the graded shuffle algebra | We consider large-N multi-matrix models whose action closely mimics that of
Yang-Mills theory, including gauge-fixing and ghost terms. We show that the
factorized Schwinger-Dyson loop equations, expressed in terms of the generating
series of gluon and ghost correlations G(xi), are quadratic equations S^i G = G
xi^i G... | hep-th | we consider largen multimatrix models whose action closely mimics that of yangmills theory including gaugefixing and ghost terms we show that the factorized schwingerdyson loop equations expressed in terms of the generating series of gluon and ghost correlations gxi are quadratic equations si g g xii g in concatenation... | [['we', 'consider', 'largen', 'multimatrix', 'models', 'whose', 'action', 'closely', 'mimics', 'that', 'of', 'yangmills', 'theory', 'including', 'gaugefixing', 'and', 'ghost', 'terms', 'we', 'show', 'that', 'the', 'factorized', 'schwingerdyson', 'loop', 'equations', 'expressed', 'in', 'terms', 'of', 'the', 'generating'... | [-0.15570767659080254, 0.1481444745956593, -0.10379525570855327, 0.08961863630323239, -0.10033424077770872, -0.10905760027618938, -0.012586817071326292, 0.2983484114977838, -0.31009853661943204, -0.19569583370577748, 0.060015134707179375, -0.27250980840993555, -0.15349080570235935, 0.13521064382929332, -0.0342773982926... |
708.3057 | Voice Service Support in Mobile Ad Hoc Networks | Mobile ad hoc networks are expected to support voice traffic. The requirement
for small delay and jitter of voice traffic poses a significant challenge for
medium access control (MAC) in such networks. User mobility makes it more
complex due to the associated dynamic path attenuation. In this paper, a MAC
scheme for ... | cs.IT cs.NI math.IT | mobile ad hoc networks are expected to support voice traffic the requirement for small delay and jitter of voice traffic poses a significant challenge for medium access control mac in such networks user mobility makes it more complex due to the associated dynamic path attenuation in this paper a mac scheme for mobile a... | [['mobile', 'ad', 'hoc', 'networks', 'are', 'expected', 'to', 'support', 'voice', 'traffic', 'the', 'requirement', 'for', 'small', 'delay', 'and', 'jitter', 'of', 'voice', 'traffic', 'poses', 'a', 'significant', 'challenge', 'for', 'medium', 'access', 'control', 'mac', 'in', 'such', 'networks', 'user', 'mobility', 'mak... | [-0.25967015157855877, 0.01486380628564141, -0.022286780449477107, 0.014597076490860094, -0.12125241356817158, -0.21312757841819388, 0.13432992661308327, 0.469325713457709, -0.2530324388295412, -0.32312398051673713, 0.05362202392637052, -0.19393098439851944, -0.19245894603769886, 0.2052177309481935, -0.1900827673052183... |
708.3058 | Explicit chiral symmetry breaking and the 1/N expansion in models with
multi-fermion interactions | Explicit chiral symmetry breaking is a natural feature of many QCD inspired
models with multi-quark interactions. To carry out the 1/N expansion of these
theories, one integrates over the quark fields. In the process of calculating
the one-loop fermion determinant which is not chiral invariant due to quark
masses, sp... | hep-th hep-ph | explicit chiral symmetry breaking is a natural feature of many qcd inspired models with multiquark interactions to carry out the 1n expansion of these theories one integrates over the quark fields in the process of calculating the oneloop fermion determinant which is not chiral invariant due to quark masses special car... | [['explicit', 'chiral', 'symmetry', 'breaking', 'is', 'a', 'natural', 'feature', 'of', 'many', 'qcd', 'inspired', 'models', 'with', 'multiquark', 'interactions', 'to', 'carry', 'out', 'the', '1n', 'expansion', 'of', 'these', 'theories', 'one', 'integrates', 'over', 'the', 'quark', 'fields', 'in', 'the', 'process', 'of'... | [-0.13358773883885225, 0.2188493654861845, -0.12067205120724425, 0.11010880357947384, -0.13176186722577424, -0.08787051123264875, 0.0057616642191754405, 0.3497485738449, -0.21741136412664847, -0.2463611412944423, 0.030550444124241335, -0.25168421299108684, -0.11486968249585983, 0.04190268419286538, -0.00366156710613821... |
708.3059 | Propagation of coherent waves in elastically scattering media | A general method for calculating statistical properties of speckle patterns
of coherent waves propagating in disordered media is developed. It allows one
to calculate speckle pattern correlations in space, as well as their
sensitivity to external parameters. This method, which is similar to the
Boltzmann-Langevin app... | cond-mat.dis-nn | a general method for calculating statistical properties of speckle patterns of coherent waves propagating in disordered media is developed it allows one to calculate speckle pattern correlations in space as well as their sensitivity to external parameters this method which is similar to the boltzmannlangevin approach f... | [['a', 'general', 'method', 'for', 'calculating', 'statistical', 'properties', 'of', 'speckle', 'patterns', 'of', 'coherent', 'waves', 'propagating', 'in', 'disordered', 'media', 'is', 'developed', 'it', 'allows', 'one', 'to', 'calculate', 'speckle', 'pattern', 'correlations', 'in', 'space', 'as', 'well', 'as', 'their'... | [-0.12609113711690487, 0.18430991104060365, -0.06132965598457543, 0.07541339218349362, -0.057725528706327196, -0.047971970607461625, 0.02403144336255022, 0.3757457818056262, -0.3082059877563643, -0.2744774421994654, 0.03965447641107752, -0.2912763690652891, -0.14355229308049, 0.23295999670675557, 0.05990644803906019, 0... |
708.306 | Single-Inclusive Hadron Production in Polarized pp Scattering at
Next-to-Leading Logarithmic Accuracy | We study the resummation of large logarithmic perturbative corrections to the
partonic cross sections relevant for the process pp-> h X at high transverse
momentum of the hadron h, when the initial protons are longitudinally
polarized. We perform the resummation to next-to-leading logarithmic accuracy.
We present num... | hep-ph | we study the resummation of large logarithmic perturbative corrections to the partonic cross sections relevant for the process pp h x at high transverse momentum of the hadron h when the initial protons are longitudinally polarized we perform the resummation to nexttoleading logarithmic accuracy we present numerical re... | [['we', 'study', 'the', 'resummation', 'of', 'large', 'logarithmic', 'perturbative', 'corrections', 'to', 'the', 'partonic', 'cross', 'sections', 'relevant', 'for', 'the', 'process', 'pp', 'h', 'x', 'at', 'high', 'transverse', 'momentum', 'of', 'the', 'hadron', 'h', 'when', 'the', 'initial', 'protons', 'are', 'longitud... | [-0.052587647208173834, 0.17017607796990958, -0.12540178518975154, 0.1422867975121125, -0.00936777814058587, -0.07715212735974301, -0.012814861829191124, 0.38057010685980247, -0.1765287924119128, -0.29442786124463266, -0.046284881724904366, -0.399182520663509, 0.08473995038702224, 0.18409796136144835, 0.091593664452935... |
708.3061 | Reliability of Coupled Oscillators I: Two-Oscillator Systems | This paper concerns the reliability of a pair of coupled oscillators in
response to fluctuating inputs. Reliability means that an input elicits
essentially identical responses upon repeated presentations regardless of the
network's initial condition. Our main result is that both reliable and
unreliable behaviors occu... | nlin.CD q-bio.NC | this paper concerns the reliability of a pair of coupled oscillators in response to fluctuating inputs reliability means that an input elicits essentially identical responses upon repeated presentations regardless of the networks initial condition our main result is that both reliable and unreliable behaviors occur in ... | [['this', 'paper', 'concerns', 'the', 'reliability', 'of', 'a', 'pair', 'of', 'coupled', 'oscillators', 'in', 'response', 'to', 'fluctuating', 'inputs', 'reliability', 'means', 'that', 'an', 'input', 'elicits', 'essentially', 'identical', 'responses', 'upon', 'repeated', 'presentations', 'regardless', 'of', 'the', 'net... | [-0.18548213836914426, 0.1717945220259988, -0.024228099552751743, 0.04863157324284966, -0.04269493946769429, -0.18659437780078608, 0.05527052028416611, 0.37124256501245556, -0.2308474298458076, -0.2839931880174209, 0.06563626049601844, -0.2605806496356008, -0.2027208906998496, 0.19318103419562566, -0.06864057729942995,... |
708.3062 | Quantum communication. Non-classical correlations and their applications | In the first part of this thesis Bell's theorem is revisited. It points at a
difference between the quantum and the classical world. This difference is
often behind the advantages of solutions using quantum mechanics. New and more
general versions of Bell inequalities are presented. These inequalities involve
multipl... | quant-ph | in the first part of this thesis bells theorem is revisited it points at a difference between the quantum and the classical world this difference is often behind the advantages of solutions using quantum mechanics new and more general versions of bell inequalities are presented these inequalities involve multiple setti... | [['in', 'the', 'first', 'part', 'of', 'this', 'thesis', 'bells', 'theorem', 'is', 'revisited', 'it', 'points', 'at', 'a', 'difference', 'between', 'the', 'quantum', 'and', 'the', 'classical', 'world', 'this', 'difference', 'is', 'often', 'behind', 'the', 'advantages', 'of', 'solutions', 'using', 'quantum', 'mechanics',... | [-0.09555042183278235, 0.09532892951367479, -0.09910062970272426, 0.11979817468191273, -0.059354337686993955, -0.2082508023689105, 0.028826974005165415, 0.2931467245664747, -0.26972851865540526, -0.29061775665259226, 0.07480203961196152, -0.27339287229610243, -0.17644480593374062, 0.24989271755919032, -0.10910184278377... |
708.3063 | Reliability of Coupled Oscillators II: Larger Networks | We study the reliability of phase oscillator networks in response to
fluctuating inputs. Reliability means that an input elicits essentially
identical responses upon repeated presentations, regardless of the network's
initial condition. In this paper, we extend previous results on two-cell
networks to larger systems.... | nlin.CD q-bio.NC | we study the reliability of phase oscillator networks in response to fluctuating inputs reliability means that an input elicits essentially identical responses upon repeated presentations regardless of the networks initial condition in this paper we extend previous results on twocell networks to larger systems the firs... | [['we', 'study', 'the', 'reliability', 'of', 'phase', 'oscillator', 'networks', 'in', 'response', 'to', 'fluctuating', 'inputs', 'reliability', 'means', 'that', 'an', 'input', 'elicits', 'essentially', 'identical', 'responses', 'upon', 'repeated', 'presentations', 'regardless', 'of', 'the', 'networks', 'initial', 'cond... | [-0.1689292588284551, 0.08008436192870524, -0.030901097735270448, 0.037193550984588784, -0.04386680643287821, -0.09415490651896241, 0.040548927647300885, 0.38960111928129687, -0.2874278754269311, -0.28145519673072417, 0.09001577471024058, -0.24342469045242995, -0.23377472652686299, 0.17201574992200513, -0.1321923692685... |
708.3064 | Synthesis and Analysis of Entangled Photonic Qubits in Spatial-Parity
Space | We present the novel embodiment of a photonic qubit that makes use of one
continuous spatial degree of freedom of a single photon and relies on the the
parity of the photon's transverse spatial distribution. Using optical
spontaneous parametric downconversion to produce photon pairs, we demonstrate
the controlled gen... | quant-ph | we present the novel embodiment of a photonic qubit that makes use of one continuous spatial degree of freedom of a single photon and relies on the the parity of the photons transverse spatial distribution using optical spontaneous parametric downconversion to produce photon pairs we demonstrate the controlled generati... | [['we', 'present', 'the', 'novel', 'embodiment', 'of', 'a', 'photonic', 'qubit', 'that', 'makes', 'use', 'of', 'one', 'continuous', 'spatial', 'degree', 'of', 'freedom', 'of', 'a', 'single', 'photon', 'and', 'relies', 'on', 'the', 'the', 'parity', 'of', 'the', 'photons', 'transverse', 'spatial', 'distribution', 'using'... | [-0.1475320458045508, 0.22348529917548235, -0.07770233355667883, 0.013103048836420049, -0.058665458853613205, -0.16515579891178434, 0.047291876453040976, 0.4213512529890368, -0.24266616608662206, -0.2661144110139489, 0.02541433601992161, -0.24682343656593186, -0.07066975962590631, 0.22217755944387416, -0.01610426296751... |
708.3065 | Notes on noncommutative supersymmetric gauge theory on the fuzzy
supersphere | In these notes we review Klimcik's construction of noncommutative gauge
theory on the fuzzy supersphere. This theory has an exact SUSY gauge symmetry
with a finite number of degrees of freedom and thus in principle it is amenable
to the methods of matrix models and Monte Carlo numerical simulations. We also
write dow... | hep-th | in these notes we review klimciks construction of noncommutative gauge theory on the fuzzy supersphere this theory has an exact susy gauge symmetry with a finite number of degrees of freedom and thus in principle it is amenable to the methods of matrix models and monte carlo numerical simulations we also write down in ... | [['in', 'these', 'notes', 'we', 'review', 'klimciks', 'construction', 'of', 'noncommutative', 'gauge', 'theory', 'on', 'the', 'fuzzy', 'supersphere', 'this', 'theory', 'has', 'an', 'exact', 'susy', 'gauge', 'symmetry', 'with', 'a', 'finite', 'number', 'of', 'degrees', 'of', 'freedom', 'and', 'thus', 'in', 'principle', ... | [-0.08886410291664876, 0.16940045569723364, -0.10278643164425515, 0.08783874603239103, -0.09343117017012376, -0.1056391862149422, 0.025869835411699918, 0.3545847882498772, -0.20930272532770267, -0.2747019842840158, 0.11141536415447123, -0.2630900875163766, -0.18667103118048264, 0.09883493775358566, -0.09046606111984987... |
708.3066 | A Proposal for a Non-Perturbative Regularization of {\cal N}=2 SUSY 4D
Gauge Theory | In this letter we show that supersymmetry like geometry can be approximated
using finite dimensional matrix models and fuzzy manifolds. In particular we
propose a non-perturbative regularization of {\cal N}=2 supersymmetric U(n)
gauge action in 4D. In some planar large N limits we recover exact SUSY
together with the... | hep-th | in this letter we show that supersymmetry like geometry can be approximated using finite dimensional matrix models and fuzzy manifolds in particular we propose a nonperturbative regularization of cal n2 supersymmetric un gauge action in 4d in some planar large n limits we recover exact susy together with the smooth geo... | [['in', 'this', 'letter', 'we', 'show', 'that', 'supersymmetry', 'like', 'geometry', 'can', 'be', 'approximated', 'using', 'finite', 'dimensional', 'matrix', 'models', 'and', 'fuzzy', 'manifolds', 'in', 'particular', 'we', 'propose', 'a', 'nonperturbative', 'regularization', 'of', 'cal', 'n2', 'supersymmetric', 'un', '... | [-0.08999569401539002, 0.16664588277658018, -0.04294914659112692, 0.09623062011311188, -0.05965214871013394, -0.17532733173217052, -0.05506655298030147, 0.38056090101599693, -0.17717445032814375, -0.2511826830987747, 0.10916905312422806, -0.2482337196572469, -0.23317228046765265, 0.055972294989400186, -0.15994292402711... |
708.3067 | On the regularity of weak solutions of the 3D Navier-Stokes equations in
$B^{-1}_{\infty,\infty}$ | We show that if a Leray-Hopf solution $u$ to the 3D Navier-Stokes equation
belongs to $C((0,T]; B^{-1}_{\infty,\infty})$ or its jumps in the
$B^{-1}_{\infty,\infty}$-norm do not exceed a constant multiple of viscosity,
then $u$ is regular on $(0,T]$. Our method uses frequency local estimates on
the nonlinear term, an... | math.AP | we show that if a lerayhopf solution u to the 3d navierstokes equation belongs to c0t b1_inftyinfty or its jumps in the b1_inftyinftynorm do not exceed a constant multiple of viscosity then u is regular on 0t our method uses frequency local estimates on the nonlinear term and yields an extension of the classical ladyzh... | [['we', 'show', 'that', 'if', 'a', 'lerayhopf', 'solution', 'u', 'to', 'the', '3d', 'navierstokes', 'equation', 'belongs', 'to', 'c0t', 'b1_inftyinfty', 'or', 'its', 'jumps', 'in', 'the', 'b1_inftyinftynorm', 'do', 'not', 'exceed', 'a', 'constant', 'multiple', 'of', 'viscosity', 'then', 'u', 'is', 'regular', 'on', '0t'... | [-0.1315515999258919, 0.008404820253913798, -0.08491538301618262, 0.036667386931367216, -0.11926686564799059, -0.14599009278992361, 0.00984106194227934, 0.306980943612077, -0.3433846266093579, -0.17034632353620097, 0.13711125673726202, -0.31676669256253676, -0.08379570827819408, 0.19371132472826338, -0.0770651901775801... |
708.3068 | On the structure of Thom polynomials of singularities | Thom polynomials of singularities express the cohomology classes dual to
singularity submanifolds. A stabilization property of Thom polynomials is known
classically, namely that trivial unfolding does not change the Thom polynomial.
In this paper we show that this is a special case of a product rule. The
product rule... | math.AG math.AT | thom polynomials of singularities express the cohomology classes dual to singularity submanifolds a stabilization property of thom polynomials is known classically namely that trivial unfolding does not change the thom polynomial in this paper we show that this is a special case of a product rule the product rule enabl... | [['thom', 'polynomials', 'of', 'singularities', 'express', 'the', 'cohomology', 'classes', 'dual', 'to', 'singularity', 'submanifolds', 'a', 'stabilization', 'property', 'of', 'thom', 'polynomials', 'is', 'known', 'classically', 'namely', 'that', 'trivial', 'unfolding', 'does', 'not', 'change', 'the', 'thom', 'polynomi... | [-0.20590300166660602, -0.0032675994627244837, -0.12589190026057195, 0.09270986857161194, -0.14288220893558082, -0.18521173789191084, -0.02201271997575925, 0.27668525203894656, -0.4243665714790155, -0.13243749368986166, 0.06940918208020194, -0.2005090353767144, -0.19962568378059176, 0.13698647648666626, -0.148318784659... |
708.3069 | Regge behavior of gluon scattering amplitudes in N=4 SYM theory | It is shown that the four-gluon scattering amplitude for N=4 supersymmetric
Yang-Mills theory in the planar limit can be written, in both the weak- and
strong-coupling limits, as a reggeized amplitude, with a parent trajectory and
an infinite number of daughter trajectories. This result relies crucially on
the fact t... | hep-th hep-ph | it is shown that the fourgluon scattering amplitude for n4 supersymmetric yangmills theory in the planar limit can be written in both the weak and strongcoupling limits as a reggeized amplitude with a parent trajectory and an infinite number of daughter trajectories this result relies crucially on the fact that the lea... | [['it', 'is', 'shown', 'that', 'the', 'fourgluon', 'scattering', 'amplitude', 'for', 'n4', 'supersymmetric', 'yangmills', 'theory', 'in', 'the', 'planar', 'limit', 'can', 'be', 'written', 'in', 'both', 'the', 'weak', 'and', 'strongcoupling', 'limits', 'as', 'a', 'reggeized', 'amplitude', 'with', 'a', 'parent', 'traject... | [-0.112806331548567, 0.1981967474215469, -0.13212310375100134, 0.09211987417868593, -0.03090025657185852, -0.07431693682729294, 0.03391329715653991, 0.2602091505747251, -0.19042424421823312, -0.2510811780494722, 0.06797575521532145, -0.2841274370486387, -0.1558384925051771, 0.17683840536387788, -0.03358366263258939, 0.... |
708.307 | Network Coding Capacity of Random Wireless Networks under a
Signal-to-Interference-and-Noise Model | In this paper, we study network coding capacity for random wireless networks.
Previous work on network coding capacity for wired and wireless networks have
focused on the case where the capacities of links in the network are
independent. In this paper, we consider a more realistic model, where wireless
networks are m... | cs.IT math.IT | in this paper we study network coding capacity for random wireless networks previous work on network coding capacity for wired and wireless networks have focused on the case where the capacities of links in the network are independent in this paper we consider a more realistic model where wireless networks are modeled ... | [['in', 'this', 'paper', 'we', 'study', 'network', 'coding', 'capacity', 'for', 'random', 'wireless', 'networks', 'previous', 'work', 'on', 'network', 'coding', 'capacity', 'for', 'wired', 'and', 'wireless', 'networks', 'have', 'focused', 'on', 'the', 'case', 'where', 'the', 'capacities', 'of', 'links', 'in', 'the', 'n... | [-0.21432878658022175, 0.047384116390824134, -0.0074584686937770855, 0.02554080425400102, -0.01109450442213218, -0.2153867752036739, 0.13445013328397543, 0.41684283429947655, -0.26783516209121355, -0.24074149360267086, 0.10977188444418705, -0.2700686139540504, -0.22221199599939243, 0.1677784494540845, -0.13610854086622... |
708.3071 | The double-slit and the EPR experiments: A paradox-free kinematic
description | The paradoxes of the double-slit and the EPR experiments with particles are
shown to originate in the implicit assumption that the particles are always
located in the classical space. It is demonstrated that there exists a natural
substitute for this assumption that provides a method of resolving the
paradoxes.
| quant-ph | the paradoxes of the doubleslit and the epr experiments with particles are shown to originate in the implicit assumption that the particles are always located in the classical space it is demonstrated that there exists a natural substitute for this assumption that provides a method of resolving the paradoxes | [['the', 'paradoxes', 'of', 'the', 'doubleslit', 'and', 'the', 'epr', 'experiments', 'with', 'particles', 'are', 'shown', 'to', 'originate', 'in', 'the', 'implicit', 'assumption', 'that', 'the', 'particles', 'are', 'always', 'located', 'in', 'the', 'classical', 'space', 'it', 'is', 'demonstrated', 'that', 'there', 'exi... | [-0.0927417729292255, 0.12550237402319908, -0.14281120056248442, 0.11096744646071172, -0.045725210626818696, -0.1599721092616721, -0.0074893921537666905, 0.35974892289662846, -0.2523883417704884, -0.2832832016354921, 0.029457872189410334, -0.31564946455538884, -0.13898725381919316, 0.1975318187733694, -0.05295030481885... |
708.3072 | On higher real and stable ranks for CCR C*-algebras | We calculate the real rank and stable rank of CCR algebras which either have
only finite dimensional irreducible representations or have finite topological
dimension. We show that either rank of A is determined in a good way by the
ranks of an ideal I and the quotient A/I in four cases: When A is CCR; when I
has only... | math.OA | we calculate the real rank and stable rank of ccr algebras which either have only finite dimensional irreducible representations or have finite topological dimension we show that either rank of a is determined in a good way by the ranks of an ideal i and the quotient ai in four cases when a is ccr when i has only finit... | [['we', 'calculate', 'the', 'real', 'rank', 'and', 'stable', 'rank', 'of', 'ccr', 'algebras', 'which', 'either', 'have', 'only', 'finite', 'dimensional', 'irreducible', 'representations', 'or', 'have', 'finite', 'topological', 'dimension', 'we', 'show', 'that', 'either', 'rank', 'of', 'a', 'is', 'determined', 'in', 'a'... | [-0.10129066129466371, 0.1520795128181196, -0.08533086949249818, 0.025925448574569254, -0.05903206932513664, -0.17926603060452237, -0.019425793445580417, 0.3892032651910706, -0.29250223095351385, -0.13363807358675533, 0.14823450596951362, -0.257675253874844, -0.13489421158807263, 0.1502368150330666, -0.0783162907372036... |
708.3073 | Spontaneous Resonances and the Coherent States of the Queuing Networks | We present an example of a highly connected closed network of servers, where
the time correlations do not go to zero in the infinite volume limit. This
phenomenon is similar to the continuous symmetry breaking at low temperatures
in statistical mechanics. The role of the inverse temperature is played by the
average l... | math-ph math.MP | we present an example of a highly connected closed network of servers where the time correlations do not go to zero in the infinite volume limit this phenomenon is similar to the continuous symmetry breaking at low temperatures in statistical mechanics the role of the inverse temperature is played by the average load | [['we', 'present', 'an', 'example', 'of', 'a', 'highly', 'connected', 'closed', 'network', 'of', 'servers', 'where', 'the', 'time', 'correlations', 'do', 'not', 'go', 'to', 'zero', 'in', 'the', 'infinite', 'volume', 'limit', 'this', 'phenomenon', 'is', 'similar', 'to', 'the', 'continuous', 'symmetry', 'breaking', 'at',... | [-0.1692395219403618, 0.19331297449979554, -0.09601876368078421, 0.06930841081380353, -0.030604291087859926, -0.10404512636750093, 0.07658743093510703, 0.35198891988762143, -0.2782143565281382, -0.26427538970590764, 0.10605740638994524, -0.2743357764732725, -0.09112565953038493, 0.11890753193644209, -0.0541079467039485... |
708.3074 | Phase-slip induced dissipation in an atomic Bose-Hubbard system | Phase slips play a primary role in dissipation across a wide spectrum of
bosonic systems, from determining the critical velocity of superfluid helium to
generating resistance in thin superconducting wires. This subject has also
inspired much technological interest, largely motivated by applications
involving nanoscal... | cond-mat.other | phase slips play a primary role in dissipation across a wide spectrum of bosonic systems from determining the critical velocity of superfluid helium to generating resistance in thin superconducting wires this subject has also inspired much technological interest largely motivated by applications involving nanoscale sup... | [['phase', 'slips', 'play', 'a', 'primary', 'role', 'in', 'dissipation', 'across', 'a', 'wide', 'spectrum', 'of', 'bosonic', 'systems', 'from', 'determining', 'the', 'critical', 'velocity', 'of', 'superfluid', 'helium', 'to', 'generating', 'resistance', 'in', 'thin', 'superconducting', 'wires', 'this', 'subject', 'has'... | [-0.19148700275497202, 0.2576208671599185, -0.04374865020702903, 0.020751434314782578, 0.005059213646867041, -0.15319154688040726, 0.07767245837167139, 0.3463137405846889, -0.24788932204052497, -0.258357872980802, 0.05076822849465922, -0.2893879936115506, -0.13978448515893735, 0.2394471962414779, -0.04778545612595432, ... |
708.3075 | Defining the integers in large rings of number fields using one
universal quantifier | Julia Robinson has given a first-order definition of the rational integers
$\mathbb Z$ in the rational numbers $\mathbb Q$ by a formula $(\forall \exists
\forall \exists)(F=0)$ where the $\forall$-quantifiers run over a total of 8
variables, and where F is a polynomial.
We show that for a large class of number fiel... | math.LO math.NT | julia robinson has given a firstorder definition of the rational integers mathbb z in the rational numbers mathbb q by a formula forall exists forall existsf0 where the forallquantifiers run over a total of 8 variables and where f is a polynomial we show that for a large class of number fields not including mathbb q fo... | [['julia', 'robinson', 'has', 'given', 'a', 'firstorder', 'definition', 'of', 'the', 'rational', 'integers', 'mathbb', 'z', 'in', 'the', 'rational', 'numbers', 'mathbb', 'q', 'by', 'a', 'formula', 'forall', 'exists', 'forall', 'existsf0', 'where', 'the', 'forallquantifiers', 'run', 'over', 'a', 'total', 'of', '8', 'var... | [-0.2517047281910339, 0.11287128234791577, -0.005476494741618124, -0.019251692794366844, -0.02044354146744451, -0.1910012960075759, 0.026490014955863103, 0.2793510931934047, -0.30851937753235936, -0.18709379226828998, 0.034553936450805865, -0.31251260249787927, -0.08994124870166247, 0.17931426755096921, -0.041186389310... |
708.3076 | Annihilation of the electron-positron pairs in polyelectrons | This paper has been withdrawn due to disagreement of suggested results and
methods between authors.
| hep-ph | this paper has been withdrawn due to disagreement of suggested results and methods between authors | [['this', 'paper', 'has', 'been', 'withdrawn', 'due', 'to', 'disagreement', 'of', 'suggested', 'results', 'and', 'methods', 'between', 'authors']] | [-0.04648124606659015, -0.08691756182039777, -0.14241849693159261, -0.02053842300083488, -0.12151742093265057, -0.06056763802965482, 0.03662305158407738, 0.41637521783510845, -0.2054200366139412, -0.41943285465240476, 0.035769740119576454, -0.34087974230448403, -0.20463877816994985, 0.13377958598236242, -0.264642774686... |
708.3077 | Chandra detection of diffuse hot gas in and around the M31 bulge | We report the detection of diffuse hot gas in M31, using archival Chandra
observations which allow us to map out a 30' by 30' field (covering a
galactocentric radius up to 4.5 kpc) and to detect sources in the galaxy down
to a 0.5-8 keV luminosity limit of ~10^35 ergs/s. We estimate the remaining
stellar contribution... | astro-ph | we report the detection of diffuse hot gas in m31 using archival chandra observations which allow us to map out a 30 by 30 field covering a galactocentric radius up to 45 kpc and to detect sources in the galaxy down to a 058 kev luminosity limit of 1035 ergss we estimate the remaining stellar contribution from fainter ... | [['we', 'report', 'the', 'detection', 'of', 'diffuse', 'hot', 'gas', 'in', 'm31', 'using', 'archival', 'chandra', 'observations', 'which', 'allow', 'us', 'to', 'map', 'out', 'a', '30', 'by', '30', 'field', 'covering', 'a', 'galactocentric', 'radius', 'up', 'to', '45', 'kpc', 'and', 'to', 'detect', 'sources', 'in', 'the... | [-0.009652478801730483, 0.10029181827666583, -0.06503881692391222, 0.13135493211263097, -0.11122820315450024, -0.02911149195571251, 0.07194554892920979, 0.4475286635706614, -0.1732122430691854, -0.3770896300993018, 0.03633825981231586, -0.3768419013307508, 0.029621136163129513, 0.2057742715455693, -0.02874121006208503,... |
708.3078 | Non-stable K-theory and extremally rich C*-algebras | We consider the properties weak cancellation, K_1-surjectivity, good index
theory, and K_1-injectivity for the class of extremally rich C*-algebras, and
for the smaller class of isometrically rich C*-algebras. We establish all four
properties for isometrically rich C*-algebras and for extremally rich
C*-algebras that... | math.OA | we consider the properties weak cancellation k_1surjectivity good index theory and k_1injectivity for the class of extremally rich calgebras and for the smaller class of isometrically rich calgebras we establish all four properties for isometrically rich calgebras and for extremally rich calgebras that are either purel... | [['we', 'consider', 'the', 'properties', 'weak', 'cancellation', 'k_1surjectivity', 'good', 'index', 'theory', 'and', 'k_1injectivity', 'for', 'the', 'class', 'of', 'extremally', 'rich', 'calgebras', 'and', 'for', 'the', 'smaller', 'class', 'of', 'isometrically', 'rich', 'calgebras', 'we', 'establish', 'all', 'four', '... | [-0.12719719239470104, 0.12534323106317416, -0.04605043170892674, 0.10781818704132963, -0.08399971444564669, -0.17056805886247237, -0.022374073145708637, 0.3869720755873815, -0.2813488438077595, -0.19499255555641393, 0.12173960440205005, -0.295265327896113, -0.14259503865816994, 0.17736071208694382, -0.0953463716675405... |
708.3079 | Feynman's Integral is About Mutually Unbiased Bases | The Feynman integral can be seen as an attempt to relate, under certain
circumstances, the quantum-information-theoretic separateness of mutually
unbiased bases to causal proximity of the measuring processes.
| quant-ph hep-th math-ph math.MP | the feynman integral can be seen as an attempt to relate under certain circumstances the quantuminformationtheoretic separateness of mutually unbiased bases to causal proximity of the measuring processes | [['the', 'feynman', 'integral', 'can', 'be', 'seen', 'as', 'an', 'attempt', 'to', 'relate', 'under', 'certain', 'circumstances', 'the', 'quantuminformationtheoretic', 'separateness', 'of', 'mutually', 'unbiased', 'bases', 'to', 'causal', 'proximity', 'of', 'the', 'measuring', 'processes']] | [-0.16802280735490577, 0.11341873954318414, -0.12804010922887496, 0.12674091064504214, -0.11919714578626943, -0.0647171913546377, 0.03847657411824912, 0.3827598236634263, -0.3197506011596748, -0.23074964492116123, 0.07799147811186101, -0.22395068380449498, -0.13187073715796163, 0.1882421402260661, -0.09864164383283683,... |
708.308 | Constraint from D - anti-D Mixing in Left-Right Symmetric Models | We study the constraint arising from the recently observed D - anti-D mixing
in the context of supersymmetric models with left-right symmetry. In these
models, the supersymmetric contributions in the mixing amplitudes of D -
anti-D, K - anti-K and B - anti-B are all correlated. We compare the constraint
from the D - ... | hep-ph | we study the constraint arising from the recently observed d antid mixing in the context of supersymmetric models with leftright symmetry in these models the supersymmetric contributions in the mixing amplitudes of d antid k antik and b antib are all correlated we compare the constraint from the d antid mixing with the... | [['we', 'study', 'the', 'constraint', 'arising', 'from', 'the', 'recently', 'observed', 'd', 'antid', 'mixing', 'in', 'the', 'context', 'of', 'supersymmetric', 'models', 'with', 'leftright', 'symmetry', 'in', 'these', 'models', 'the', 'supersymmetric', 'contributions', 'in', 'the', 'mixing', 'amplitudes', 'of', 'd', 'a... | [-0.14488252270876348, 0.3307527413284316, -0.02062388091773084, 0.07114092388090867, -0.02608533997034419, -0.16281242094011705, 0.06957338465314394, 0.23823689600651704, -0.2518975977035402, -0.25627315491076236, -0.013979647157135086, -0.3406886243650201, -0.0364377106567031, 0.05639188049487697, 0.07156608187711065... |
708.3081 | Transport in Graphene p-n Junctions in Magnetic Field | Ballistic transport in graphene p-n junctions in the presence of magnetic
field exhibits two distinct regimes: At low fields, transport is partially
suppressed by the field. When the field exceeds a certain critical value, the
junction is pinched off by the Landau level formation. Transmission and
conductance are fou... | cond-mat.mes-hall | ballistic transport in graphene pn junctions in the presence of magnetic field exhibits two distinct regimes at low fields transport is partially suppressed by the field when the field exceeds a certain critical value the junction is pinched off by the landau level formation transmission and conductance are found in th... | [['ballistic', 'transport', 'in', 'graphene', 'pn', 'junctions', 'in', 'the', 'presence', 'of', 'magnetic', 'field', 'exhibits', 'two', 'distinct', 'regimes', 'at', 'low', 'fields', 'transport', 'is', 'partially', 'suppressed', 'by', 'the', 'field', 'when', 'the', 'field', 'exceeds', 'a', 'certain', 'critical', 'value'... | [-0.27531503869787505, 0.1900597681817801, -0.02902780589242668, -8.786462105648673e-05, -0.00961266446089291, -0.1750660304263558, 0.050535706268704454, 0.38207407912806324, -0.25160232318322295, -0.2895178231532159, -0.02912824398878476, -0.2478412920933055, -0.13844152360385203, 0.19970977492630482, 0.03642156671570... |
708.3082 | Path Integral Approach for for Quantum Motion on Spaces of Non-constant
Curvature According to Koenigs: Three Dimensions | In this contribution a path integral approach for the quantum motion on
three-dimensional spaces according to Koenigs, for short``Koenigs-Spaces'', is
discussed. Their construction is simple: One takes a Hamiltonian from
three-dimensional flat space and divides it by a three-dimensional
superintegrable potential. Suc... | quant-ph | in this contribution a path integral approach for the quantum motion on threedimensional spaces according to koenigs for shortkoenigsspaces is discussed their construction is simple one takes a hamiltonian from threedimensional flat space and divides it by a threedimensional superintegrable potential such superintegrab... | [['in', 'this', 'contribution', 'a', 'path', 'integral', 'approach', 'for', 'the', 'quantum', 'motion', 'on', 'threedimensional', 'spaces', 'according', 'to', 'koenigs', 'for', 'shortkoenigsspaces', 'is', 'discussed', 'their', 'construction', 'is', 'simple', 'one', 'takes', 'a', 'hamiltonian', 'from', 'threedimensional... | [-0.14830696311987285, 0.1289602808238378, -0.07332580782658447, 0.07583210332255846, -0.08964937147277507, -0.14024126040523202, -0.04128274811969763, 0.3443263261533767, -0.2618097360969241, -0.21913940212079008, 0.05503666455161224, -0.29734833977067643, -0.15613876443889751, 0.1995617114527386, -0.03134012176628107... |
708.3083 | Dynamics around supermassive black holes | The dynamics of galactic nuclei reflects the presence of supermassive black
holes (SBHs) in many ways. Single SBHs act as sinks, destroying a mass in stars
equal to their own mass in roughly one relaxation time and forcing nuclei to
expand. Formation of binary SBHs displaces a mass in stars roughly equal to the
binar... | astro-ph | the dynamics of galactic nuclei reflects the presence of supermassive black holes sbhs in many ways single sbhs act as sinks destroying a mass in stars equal to their own mass in roughly one relaxation time and forcing nuclei to expand formation of binary sbhs displaces a mass in stars roughly equal to the binary mass ... | [['the', 'dynamics', 'of', 'galactic', 'nuclei', 'reflects', 'the', 'presence', 'of', 'supermassive', 'black', 'holes', 'sbhs', 'in', 'many', 'ways', 'single', 'sbhs', 'act', 'as', 'sinks', 'destroying', 'a', 'mass', 'in', 'stars', 'equal', 'to', 'their', 'own', 'mass', 'in', 'roughly', 'one', 'relaxation', 'time', 'an... | [-0.12401078722399214, 0.23825919778977075, -0.028455583257195743, 0.14940603513209877, -0.07890132406685987, -0.04232183744644989, 0.09300578873017398, 0.3364309253495025, -0.17647612653166542, -0.35294957747480465, -0.03417690416782811, -0.320298373101927, 0.006936487782260646, 0.19171759025598673, -0.051816203793429... |
708.3084 | Commensurate lock-in and incommensurate supersolid phases of hardcore
bosons on anisotropic triangular lattices | We investigate the interplay between commensurate lock-in and incommensurate
supersolid phases of the hardcore bosons at half-filling with anisotropic
nearest-neighbor hopping and repulsive interactions on triangular lattice. We
use numerical quantum and variational Monte Carlo as well as analytical
Schwinger boson m... | cond-mat.str-el cond-mat.mes-hall | we investigate the interplay between commensurate lockin and incommensurate supersolid phases of the hardcore bosons at halffilling with anisotropic nearestneighbor hopping and repulsive interactions on triangular lattice we use numerical quantum and variational monte carlo as well as analytical schwinger boson meanfie... | [['we', 'investigate', 'the', 'interplay', 'between', 'commensurate', 'lockin', 'and', 'incommensurate', 'supersolid', 'phases', 'of', 'the', 'hardcore', 'bosons', 'at', 'halffilling', 'with', 'anisotropic', 'nearestneighbor', 'hopping', 'and', 'repulsive', 'interactions', 'on', 'triangular', 'lattice', 'we', 'use', 'n... | [-0.21360062825634493, 0.3000403411959836, -0.05695326209608722, 0.09449540408234189, -0.0441048603778312, -0.1569959617587268, 0.12210448816580989, 0.4001463645847019, -0.2814675563809658, -0.2195128547967574, 0.03102155130488986, -0.3316166503782119, -0.11903454655559238, 0.08079188244434399, 0.11851615182961414, 0.0... |
708.3085 | A nonlinear theory of non-stationary low Mach number channel flows of
freely cooling nearly elastic granular gases | We use hydrodynamics to investigate non-stationary channel flows of freely
cooling dilute granular gases. We focus on the regime where the sound travel
time through the channel is much shorter than the characteristic cooling time
of the gas. As a result, the gas pressure rapidly becomes almost homogeneous,
while the ... | cond-mat.soft nlin.PS physics.flu-dyn | we use hydrodynamics to investigate nonstationary channel flows of freely cooling dilute granular gases we focus on the regime where the sound travel time through the channel is much shorter than the characteristic cooling time of the gas as a result the gas pressure rapidly becomes almost homogeneous while the typical... | [['we', 'use', 'hydrodynamics', 'to', 'investigate', 'nonstationary', 'channel', 'flows', 'of', 'freely', 'cooling', 'dilute', 'granular', 'gases', 'we', 'focus', 'on', 'the', 'regime', 'where', 'the', 'sound', 'travel', 'time', 'through', 'the', 'channel', 'is', 'much', 'shorter', 'than', 'the', 'characteristic', 'coo... | [-0.15629159016825725, 0.19424299713239937, -0.07675328625385494, 0.04260690754066066, -0.03683095750360129, -0.12637408626032992, 0.012227464070019779, 0.2825786676653176, -0.31133300254823554, -0.2403756603457926, 0.08628825844401339, -0.29075853116034217, -0.05209616625312871, 0.16604446124013825, 0.0300192542240968... |
708.3086 | Chemistry and cooling in metal-free and metal-poor gas | I summarize four of the most important areas of uncertainty in the study of
the chemistry and cooling of gas with zero or very low metallicity. These are:
i) the importance and effects of HD cooling in primordial gas; ii) the
importance of metal-line and dust cooling in low metallicity gas; iii) the
impact of the lar... | astro-ph | i summarize four of the most important areas of uncertainty in the study of the chemistry and cooling of gas with zero or very low metallicity these are i the importance and effects of hd cooling in primordial gas ii the importance of metalline and dust cooling in low metallicity gas iii the impact of the large uncerta... | [['i', 'summarize', 'four', 'of', 'the', 'most', 'important', 'areas', 'of', 'uncertainty', 'in', 'the', 'study', 'of', 'the', 'chemistry', 'and', 'cooling', 'of', 'gas', 'with', 'zero', 'or', 'very', 'low', 'metallicity', 'these', 'are', 'i', 'the', 'importance', 'and', 'effects', 'of', 'hd', 'cooling', 'in', 'primord... | [-0.057191242361852135, 0.14549167099244453, 0.006737686488229562, 0.04068827556774897, 0.028810714705682854, -0.06777343465124859, 0.046444443624247524, 0.35151704742627987, -0.1991063127800932, -0.30616059318623123, 0.08707207201240474, -0.24272806356277535, -0.03030890071600237, 0.19018993999754244, -0.0195759482462... |
708.3087 | The Tidal Evolution of Local Group Dwarf Spheroidals | (Abridged) We use N-body simulations to study the evolution of dwarf
spheroidal galaxies (dSphs) driven by galactic tides. We adopt a
cosmologically-motivated model where dSphs are approximated by a King model
embedded within an NFW halo. We find that these NFW-embedded King models are
extraordinarily resilient to ti... | astro-ph | abridged we use nbody simulations to study the evolution of dwarf spheroidal galaxies dsphs driven by galactic tides we adopt a cosmologicallymotivated model where dsphs are approximated by a king model embedded within an nfw halo we find that these nfwembedded king models are extraordinarily resilient to tides the ste... | [['abridged', 'we', 'use', 'nbody', 'simulations', 'to', 'study', 'the', 'evolution', 'of', 'dwarf', 'spheroidal', 'galaxies', 'dsphs', 'driven', 'by', 'galactic', 'tides', 'we', 'adopt', 'a', 'cosmologicallymotivated', 'model', 'where', 'dsphs', 'are', 'approximated', 'by', 'a', 'king', 'model', 'embedded', 'within', ... | [-0.09091996529518685, 0.11336789187590278, -0.1177063345749859, 0.16807570722305518, -0.13151222582539496, -0.06935698435672985, 0.02562906194242846, 0.3738329719932106, -0.13619095390548083, -0.40341995349742443, 0.011488886575602328, -0.2842907619378685, -0.05753278556941112, 0.20266728846086168, -0.0592627459288779... |
708.3088 | The Fourth Positive System of Carbon Monoxide in the Hubble Space
Telescope Spectra of Comets | The rich structure of the Fourth Positive System (A-X) of carbon monoxide
accounts for many of the spectral features seen in long slit HST-STIS
observations of comets 153P/Ikeya-Zhang, C/2001 Q4 (NEAT), and C/2000 WM1
(LINEAR), as well as in the HST-GHRS spectrum of comet C/1996 B2 Hyakutake. A
detailed CO fluorescen... | astro-ph | the rich structure of the fourth positive system ax of carbon monoxide accounts for many of the spectral features seen in long slit hststis observations of comets 153pikeyazhang c2001 q4 neat and c2000 wm1 linear as well as in the hstghrs spectrum of comet c1996 b2 hyakutake a detailed co fluorescence model is develope... | [['the', 'rich', 'structure', 'of', 'the', 'fourth', 'positive', 'system', 'ax', 'of', 'carbon', 'monoxide', 'accounts', 'for', 'many', 'of', 'the', 'spectral', 'features', 'seen', 'in', 'long', 'slit', 'hststis', 'observations', 'of', 'comets', '153pikeyazhang', 'c2001', 'q4', 'neat', 'and', 'c2000', 'wm1', 'linear', ... | [-0.026196750151929717, 0.06212162948644685, 0.010802661657589611, 0.03587669442856201, 0.011476636115244772, -0.11911854912186899, 0.04799267368097962, 0.4109989177218821, -0.19105324790093595, -0.3064748953495707, 0.053243849448066344, -0.29155861666883715, -0.03674898485938905, 0.1458192569605277, -0.007377071022462... |
708.3089 | Keck Hires Spectroscopy of Candidate Post T Tauri Stars | We use high-signal-to-noise ($\sim$150-450), high resolution
($R{\sim}45,000$) Keck HIRES spectroscopy of 13 candidate post T Tauri stars to
derive basic physical parameters, lithium abundances and radial velocities. We
place our stars in the M$_v$-T$_{eff}$ plane for use in determining approximate
ages from pre-main... | astro-ph | we use highsignaltonoise sim150450 high resolution rsim45000 keck hires spectroscopy of 13 candidate post t tauri stars to derive basic physical parameters lithium abundances and radial velocities we place our stars in the m_vt_eff plane for use in determining approximate ages from premain sequence isochrones and confi... | [['we', 'use', 'highsignaltonoise', 'sim150450', 'high', 'resolution', 'rsim45000', 'keck', 'hires', 'spectroscopy', 'of', '13', 'candidate', 'post', 't', 'tauri', 'stars', 'to', 'derive', 'basic', 'physical', 'parameters', 'lithium', 'abundances', 'and', 'radial', 'velocities', 'we', 'place', 'our', 'stars', 'in', 'th... | [0.0012429078770113302, 0.13054076512921545, -0.09769383815648826, 0.09124871891233241, -0.13110384448932913, -0.10992845615017631, 0.12570454322955446, 0.47093190946559677, -0.1431519068751462, -0.38136815643201954, 0.02402277818507692, -0.3122124131693531, -0.01051486410419287, 0.20773150337914661, -0.153933438359333... |
708.309 | Role of disorder in the size-scaling of material strength | We study the sample size dependence of the strength of disordered materials
with a flaw, by numerical simulations of lattice models for fracture. We find a
crossover between a regime controlled by the fluctuations due to disorder and
another controlled by stress-concentrations, ruled by continuum fracture
mechanics. ... | cond-mat.mtrl-sci | we study the sample size dependence of the strength of disordered materials with a flaw by numerical simulations of lattice models for fracture we find a crossover between a regime controlled by the fluctuations due to disorder and another controlled by stressconcentrations ruled by continuum fracture mechanics the res... | [['we', 'study', 'the', 'sample', 'size', 'dependence', 'of', 'the', 'strength', 'of', 'disordered', 'materials', 'with', 'a', 'flaw', 'by', 'numerical', 'simulations', 'of', 'lattice', 'models', 'for', 'fracture', 'we', 'find', 'a', 'crossover', 'between', 'a', 'regime', 'controlled', 'by', 'the', 'fluctuations', 'due... | [-0.10818035990220085, 0.15802485079714848, -0.09851711218105129, 0.008142267738852146, 0.018647549253317616, -0.11924009342547706, 0.10390067754578726, 0.35384232058159765, -0.2536809896669721, -0.29818864663441974, 0.07488606861912675, -0.30147114824703947, -0.16574711923397356, 0.20640808711409248, -0.00451850796979... |
708.3091 | Spin orbit interaction and zitterbewegung in symmetric wells | Recently, we have introduced a novel inter-subband-induced spin-orbit (s-o)
coupling [Phys. Rev. Lett. 99, 076603 (2007); cond-mat/0607218] arising in
\textit{symmetric} wells with at least two subbands. This new s-o coupling
gives rise to an usual zitterbewegung -- i.e. the semiconductor analog to the
relativistic t... | cond-mat.mes-hall | recently we have introduced a novel intersubbandinduced spinorbit so coupling phys rev lett 99 076603 2007 condmat0607218 arising in textitsymmetric wells with at least two subbands this new so coupling gives rise to an usual zitterbewegung ie the semiconductor analog to the relativistic trembling motion of electrons w... | [['recently', 'we', 'have', 'introduced', 'a', 'novel', 'intersubbandinduced', 'spinorbit', 'so', 'coupling', 'phys', 'rev', 'lett', '99', '076603', '2007', 'condmat0607218', 'arising', 'in', 'textitsymmetric', 'wells', 'with', 'at', 'least', 'two', 'subbands', 'this', 'new', 'so', 'coupling', 'gives', 'rise', 'to', 'a... | [-0.1524476913310697, 0.18541888752973618, -0.0042517192675458155, -0.03654544205603409, -0.12722272314268218, -0.1398034567383173, 0.035380483769318634, 0.3611391477444319, -0.19214877779321635, -0.33778348934891467, -0.09477537783095613, -0.25485617787960696, -0.1696170070208609, 0.20087628940724672, -0.0793666888134... |
708.3092 | The Molonglo Galactic Plane Survey (MGPS-2): Compact Source Catalogue | We present the first data release from the second epoch Molonglo Galactic
Plane Survey (MGPS-2). MGPS-2 was carried out with the Molonglo Observatory
Synthesis Telescope at a frequency of 843 MHz and with a restoring beam of 45
arcsec x 45 arcsec cosec(dec), making it the highest resolution large scale
radio survey o... | astro-ph | we present the first data release from the second epoch molonglo galactic plane survey mgps2 mgps2 was carried out with the molonglo observatory synthesis telescope at a frequency of 843 mhz and with a restoring beam of 45 arcsec x 45 arcsec cosecdec making it the highest resolution large scale radio survey of the sout... | [['we', 'present', 'the', 'first', 'data', 'release', 'from', 'the', 'second', 'epoch', 'molonglo', 'galactic', 'plane', 'survey', 'mgps2', 'mgps2', 'was', 'carried', 'out', 'with', 'the', 'molonglo', 'observatory', 'synthesis', 'telescope', 'at', 'a', 'frequency', 'of', '843', 'mhz', 'and', 'with', 'a', 'restoring', '... | [-0.08301262069489822, 0.037328140745952865, -0.009270708968786828, 0.02544053972528908, -0.12163192301291037, -0.018145969213613593, 0.0974022604286693, 0.4351562728021902, -0.16669447161628312, -0.421083570276183, 0.1328354829062422, -0.367917930058007, 0.04568131794537087, 0.20615141502715112, -0.012350722190096558,... |
708.3093 | Role of CuO chains in vortex core structure in YBa2Cu3O{7-delta} | The Bogoliubov-deGennes equations are solved for a proximity model for
YBa_2Cu_3O_{7-\delta} in a magnetic field. The model explicitly includes the
effects of the one-dimensional CuO chains, whose influence on the vortex core
structure is studied. The rapid vortex core contraction as a function of field
which is seen... | cond-mat.supr-con cond-mat.str-el | the bogoliubovdegennes equations are solved for a proximity model for yba_2cu_3o_7delta in a magnetic field the model explicitly includes the effects of the onedimensional cuo chains whose influence on the vortex core structure is studied the rapid vortex core contraction as a function of field which is seen experiment... | [['the', 'bogoliubovdegennes', 'equations', 'are', 'solved', 'for', 'a', 'proximity', 'model', 'for', 'yba_2cu_3o_7delta', 'in', 'a', 'magnetic', 'field', 'the', 'model', 'explicitly', 'includes', 'the', 'effects', 'of', 'the', 'onedimensional', 'cuo', 'chains', 'whose', 'influence', 'on', 'the', 'vortex', 'core', 'str... | [-0.20597921401983307, 0.18436117172842065, -0.019975199431721723, 0.08158775237050929, -0.027378678145337728, -0.08618637124046442, 0.0026812420110218227, 0.35547082215141984, -0.2902735174303093, -0.2774305905425741, 0.09290026851381446, -0.21626536926675227, -0.0961725638368197, 0.16808070087309687, 0.08620249974210... |
708.3094 | Brane Decay and Defect Formation | Topological defects are generically expected to form in models of brane
inflation. Brane-anti-brane annihilation provides a way to gracefully end
inflation, and the dynamics of the tachyon field results in defect formation.
The formation of defects has been studied mainly from the brane world-volume
point of view, bu... | hep-th | topological defects are generically expected to form in models of brane inflation braneantibrane annihilation provides a way to gracefully end inflation and the dynamics of the tachyon field results in defect formation the formation of defects has been studied mainly from the brane worldvolume point of view but the def... | [['topological', 'defects', 'are', 'generically', 'expected', 'to', 'form', 'in', 'models', 'of', 'brane', 'inflation', 'braneantibrane', 'annihilation', 'provides', 'a', 'way', 'to', 'gracefully', 'end', 'inflation', 'and', 'the', 'dynamics', 'of', 'the', 'tachyon', 'field', 'results', 'in', 'defect', 'formation', 'th... | [-0.1408803709089122, 0.16508351074505254, -0.11213431403854968, 0.11813473459316669, -0.05941623430666084, -0.09876753289767719, -0.008774003136163274, 0.36627390767374995, -0.2183489564489177, -0.295896997113864, 0.05443228846614031, -0.2702796463821585, -0.16345605260613275, 0.08809876690721073, -0.01590421162413578... |
708.3095 | Effect of Disorder and Notches on Crack Roughness | We analyze the effect of disorder and notches on crack roughness in two
dimensions. Our simulation results based on large system sizes and extensive
statistical sampling indicate that the crack surface exhibits a universal local
roughness of $\zeta_{loc} = 0.71$ and is independent of the initial notch size
and disord... | cond-mat.stat-mech cond-mat.mtrl-sci | we analyze the effect of disorder and notches on crack roughness in two dimensions our simulation results based on large system sizes and extensive statistical sampling indicate that the crack surface exhibits a universal local roughness of zeta_loc 071 and is independent of the initial notch size and disorder in break... | [['we', 'analyze', 'the', 'effect', 'of', 'disorder', 'and', 'notches', 'on', 'crack', 'roughness', 'in', 'two', 'dimensions', 'our', 'simulation', 'results', 'based', 'on', 'large', 'system', 'sizes', 'and', 'extensive', 'statistical', 'sampling', 'indicate', 'that', 'the', 'crack', 'surface', 'exhibits', 'a', 'univer... | [-0.1404507690099905, 0.18536269324690555, -0.16125488492914222, 0.05924569369961667, 0.014092541193340274, -0.1369038411754776, 0.032636602879548914, 0.3815712754925092, -0.2592378798684086, -0.2690376803899805, 0.08398154473538991, -0.2975502313312256, -0.15619143935842345, 0.17275945077452695, -0.0427375254644589, 0... |
708.3096 | Rectification of Swimming Bacteria and Self Driven Particle Systems by
Arrays of Asymmetric Barriers | We show that the recent experimental observation of the rectification of
swimming bacteria in a system with an array of asymmetric barriers occurs due
to the ballistic component of the bacteria trajectories introduced by the
bacterial "motor." Each bacteria selects a random direction for motion and then
moves in this... | cond-mat.soft cond-mat.stat-mech q-bio.CB | we show that the recent experimental observation of the rectification of swimming bacteria in a system with an array of asymmetric barriers occurs due to the ballistic component of the bacteria trajectories introduced by the bacterial motor each bacteria selects a random direction for motion and then moves in this dire... | [['we', 'show', 'that', 'the', 'recent', 'experimental', 'observation', 'of', 'the', 'rectification', 'of', 'swimming', 'bacteria', 'in', 'a', 'system', 'with', 'an', 'array', 'of', 'asymmetric', 'barriers', 'occurs', 'due', 'to', 'the', 'ballistic', 'component', 'of', 'the', 'bacteria', 'trajectories', 'introduced', '... | [-0.17015474066929012, 0.24114816829483662, -0.059621953170961826, -0.04477808388710057, -0.04200422614241757, -0.13084781852129074, 0.08322085089018384, 0.3908919231825561, -0.30704818621172375, -0.25474884618460286, 0.019888559468354116, -0.2597752155841522, -0.1945249227683921, 0.1483417391109298, -0.087909643674480... |
708.3097 | One loop superstring effective actions and N=8 supergravity | In a previous article we have shown the existence of a new independent R^4
term, at one loop, in the type IIA and heterotic effective actions, after
reduction to four dimensions, besides the usual square of the Bel-Robinson
tensor. It had been shown that such a term could not be directly
supersymmetrized, but we show... | hep-th | in a previous article we have shown the existence of a new independent r4 term at one loop in the type iia and heterotic effective actions after reduction to four dimensions besides the usual square of the belrobinson tensor it had been shown that such a term could not be directly supersymmetrized but we showed that wa... | [['in', 'a', 'previous', 'article', 'we', 'have', 'shown', 'the', 'existence', 'of', 'a', 'new', 'independent', 'r4', 'term', 'at', 'one', 'loop', 'in', 'the', 'type', 'iia', 'and', 'heterotic', 'effective', 'actions', 'after', 'reduction', 'to', 'four', 'dimensions', 'besides', 'the', 'usual', 'square', 'of', 'the', '... | [-0.11041694445446236, 0.1501057863280126, -0.0579577971804785, 0.0797273429821896, -0.09179839057758553, -0.1603932846146189, -0.032089922138591846, 0.3242699021078034, -0.18377579335276395, -0.25310808234395177, 0.11877460222075732, -0.26657519966670096, -0.1978544699640511, 0.09800960291942505, -0.10652728764697501,... |
708.3098 | CompostBin: A DNA composition-based algorithm for binning environmental
shotgun reads | A major hindrance to studies of microbial diversity has been that the vast
majority of microbes cannot be cultured in the laboratory and thus are not
amenable to traditional methods of characterization. Environmental shotgun
sequencing (ESS) overcomes this hurdle by sequencing the DNA from the organisms
present in a ... | q-bio.GN | a major hindrance to studies of microbial diversity has been that the vast majority of microbes cannot be cultured in the laboratory and thus are not amenable to traditional methods of characterization environmental shotgun sequencing ess overcomes this hurdle by sequencing the dna from the organisms present in a micro... | [['a', 'major', 'hindrance', 'to', 'studies', 'of', 'microbial', 'diversity', 'has', 'been', 'that', 'the', 'vast', 'majority', 'of', 'microbes', 'can', 'not', 'be', 'cultured', 'in', 'the', 'laboratory', 'and', 'thus', 'are', 'not', 'amenable', 'to', 'traditional', 'methods', 'of', 'characterization', 'environmental',... | [-0.04580540517855873, 0.06942595626836065, -0.06997188893431912, 0.057326092110348066, -0.08378627787971375, -0.09714222394823267, 0.07593087205124012, 0.4149253949218867, -0.27743684024103366, -0.33634983809137414, 0.10168134114925978, -0.27085441897376156, -0.11489556215338799, 0.21168570713097307, -0.11552057653779... |
708.3099 | A multicolor near-infrared study of the dwarf nova IP Peg | We report the analysis of $JHK_{s}$ light curves of the eclipsing dwarf nova
IP Peg in quiescence. The light curves are dominated by the ellipsoidal
variation of the mass-donor star, with additional contributions from the
accretion disc and anisotropic emission from the bright spot. A secondary
eclipse is visible in ... | astro-ph | we report the analysis of jhk_s light curves of the eclipsing dwarf nova ip peg in quiescence the light curves are dominated by the ellipsoidal variation of the massdonor star with additional contributions from the accretion disc and anisotropic emission from the bright spot a secondary eclipse is visible in the j and ... | [['we', 'report', 'the', 'analysis', 'of', 'jhk_s', 'light', 'curves', 'of', 'the', 'eclipsing', 'dwarf', 'nova', 'ip', 'peg', 'in', 'quiescence', 'the', 'light', 'curves', 'are', 'dominated', 'by', 'the', 'ellipsoidal', 'variation', 'of', 'the', 'massdonor', 'star', 'with', 'additional', 'contributions', 'from', 'the'... | [-0.11117184342960695, 0.11253556941249662, -0.08301883070118846, 0.05591966508914102, -0.05971314072390257, -0.11940252769602697, 0.07068771853673494, 0.41890564760257326, -0.22578365005824247, -0.3586695446695959, 0.07933628753436586, -0.3400692635890745, -0.02933192744602257, 0.19319891971620817, -0.0861697911335766... |
708.31 | Determining Spins of Metastable Sleptons at the Large Hadron Collider | We investigate models in minimal supergravity parameter space which contain
metastable sleptons. We find the luminosity required to determine the slepton
spin in these scenarios, and apply our analysis to two benchmark models. We
show that the spin of the slepton in one of the benchmark models can be
determined with ... | hep-ph | we investigate models in minimal supergravity parameter space which contain metastable sleptons we find the luminosity required to determine the slepton spin in these scenarios and apply our analysis to two benchmark models we show that the spin of the slepton in one of the benchmark models can be determined with less ... | [['we', 'investigate', 'models', 'in', 'minimal', 'supergravity', 'parameter', 'space', 'which', 'contain', 'metastable', 'sleptons', 'we', 'find', 'the', 'luminosity', 'required', 'to', 'determine', 'the', 'slepton', 'spin', 'in', 'these', 'scenarios', 'and', 'apply', 'our', 'analysis', 'to', 'two', 'benchmark', 'mode... | [-0.045741391368210316, 0.15077862722440236, -0.04590397694540259, 0.15571769790442072, -0.05483045943465345, -0.14613465976742046, 0.006161656247027088, 0.3751334687041348, -0.2300546635595853, -0.38348100710611205, 0.11351297382293922, -0.2779198512353264, -0.0314936635984116, 0.20474806772095658, -0.0070119275049747... |
708.3101 | Orbital Instabilities in a Triaxial Cusp Potential | This paper constructs an analytic form for a triaxial potential that
describes the dynamics of a wide variety of astrophysical systems, including
the inner portions of dark matter halos, the central regions of galactic
bulges, and young embedded star clusters. Specifically, this potential results
from a density profi... | astro-ph | this paper constructs an analytic form for a triaxial potential that describes the dynamics of a wide variety of astrophysical systems including the inner portions of dark matter halos the central regions of galactic bulges and young embedded star clusters specifically this potential results from a density profile of t... | [['this', 'paper', 'constructs', 'an', 'analytic', 'form', 'for', 'a', 'triaxial', 'potential', 'that', 'describes', 'the', 'dynamics', 'of', 'a', 'wide', 'variety', 'of', 'astrophysical', 'systems', 'including', 'the', 'inner', 'portions', 'of', 'dark', 'matter', 'halos', 'the', 'central', 'regions', 'of', 'galactic',... | [-0.17649743106780777, 0.11039829010228625, -0.11336942169564376, 0.09079601773340737, -0.0671961394746648, -0.02879815948210232, -0.02543413667961318, 0.3003750043689548, -0.22969754792537558, -0.29648661414653527, 0.06823345010139897, -0.22651303774035425, -0.12199053178309738, 0.19343247338212602, 0.0160678288793200... |
708.3102 | Spontaneous symmetry breaking in amnestically induced persistence | We investigate a recently proposed non-Markovian random walk model
characterized by loss of memories of the recent past and amnestically induced
persistence. We report numerical and analytical results showing the complete
phase diagram, consisting of 4 phases, for this system: (i) classical
nonpersistence, (ii) class... | cond-mat.stat-mech | we investigate a recently proposed nonmarkovian random walk model characterized by loss of memories of the recent past and amnestically induced persistence we report numerical and analytical results showing the complete phase diagram consisting of 4 phases for this system i classical nonpersistence ii classical persist... | [['we', 'investigate', 'a', 'recently', 'proposed', 'nonmarkovian', 'random', 'walk', 'model', 'characterized', 'by', 'loss', 'of', 'memories', 'of', 'the', 'recent', 'past', 'and', 'amnestically', 'induced', 'persistence', 'we', 'report', 'numerical', 'and', 'analytical', 'results', 'showing', 'the', 'complete', 'phas... | [-0.1712288331403397, 0.18839726151432842, -0.08735372122842819, 0.07538803674979136, -0.07172611808404326, -0.18661358882673085, 0.032892368588072714, 0.3716055510449223, -0.26323281672783194, -0.24776049477979542, 0.10634110015584156, -0.21151648355647923, -0.22995409006718545, 0.1216316259186715, -0.0175679974071681... |
708.3103 | Computer simulations on the sympatric speciation modes for the Midas
cichlid species complex | Cichlid fishes are one of the best model system for the study of evolution of
the species. Inspired by them, in this paper we simulated the splitting of a
single species into two separate ones via random mutations, with both
populations living together in sympatry, sharing the same habitat. We study the
ecological, m... | q-bio.PE | cichlid fishes are one of the best model system for the study of evolution of the species inspired by them in this paper we simulated the splitting of a single species into two separate ones via random mutations with both populations living together in sympatry sharing the same habitat we study the ecological mating an... | [['cichlid', 'fishes', 'are', 'one', 'of', 'the', 'best', 'model', 'system', 'for', 'the', 'study', 'of', 'evolution', 'of', 'the', 'species', 'inspired', 'by', 'them', 'in', 'this', 'paper', 'we', 'simulated', 'the', 'splitting', 'of', 'a', 'single', 'species', 'into', 'two', 'separate', 'ones', 'via', 'random', 'muta... | [-0.09915254549178783, 0.14757082500081095, -0.03072238482889675, 0.07070969469946754, -0.01785477369262408, -0.14516013602740943, 0.04446672156382914, 0.3568514174456516, -0.26890693468758686, -0.2821667769495102, 0.07907930241125295, -0.22229169469903268, -0.17448606178339335, 0.1369356623728804, -0.05939404533377716... |
708.3104 | Detecting a unique EBL signature with TeV gamma rays | We discuss prospects for detecting a spectral break in gamma-ray spectra of
blazars due to the extragalactic background light (EBL) density falling off
between the near and mid-IR. A measurable spectral change in the TeV spectra at
1 TeV could arise from a rapid or slow drop in the EBL density above ~1 micron.
This e... | astro-ph | we discuss prospects for detecting a spectral break in gammaray spectra of blazars due to the extragalactic background light ebl density falling off between the near and midir a measurable spectral change in the tev spectra at 1 tev could arise from a rapid or slow drop in the ebl density above 1 micron this effect is ... | [['we', 'discuss', 'prospects', 'for', 'detecting', 'a', 'spectral', 'break', 'in', 'gammaray', 'spectra', 'of', 'blazars', 'due', 'to', 'the', 'extragalactic', 'background', 'light', 'ebl', 'density', 'falling', 'off', 'between', 'the', 'near', 'and', 'midir', 'a', 'measurable', 'spectral', 'change', 'in', 'the', 'tev... | [-0.06090910392695991, 0.16432385180270723, -0.10364578049942977, 0.16097221736397063, -0.08705965938250057, -0.09619164978694014, 0.03443908254506395, 0.4517479848210551, -0.18196891410791846, -0.36585236988773867, 0.028654081669651724, -0.3186876634840204, 0.01467889325278459, 0.18591051957444796, -0.0012070986035303... |
708.3105 | Weak subintegral closure of ideals | We describe some basic facts about the weak subintegral closure of ideals in
both the algebraic and complex-analytic settings. We focus on the analogy
between results on the integral closure of ideals and modules and the weak
subintegral closure of an ideal. We start by giving a geometric interpretation
of the Reid-R... | math.AC math.AG math.CV | we describe some basic facts about the weak subintegral closure of ideals in both the algebraic and complexanalytic settings we focus on the analogy between results on the integral closure of ideals and modules and the weak subintegral closure of an ideal we start by giving a geometric interpretation of the reidroberts... | [['we', 'describe', 'some', 'basic', 'facts', 'about', 'the', 'weak', 'subintegral', 'closure', 'of', 'ideals', 'in', 'both', 'the', 'algebraic', 'and', 'complexanalytic', 'settings', 'we', 'focus', 'on', 'the', 'analogy', 'between', 'results', 'on', 'the', 'integral', 'closure', 'of', 'ideals', 'and', 'modules', 'and'... | [-0.17683642463119337, 0.04675893836789737, -0.07895975051580008, 0.04001691210160815, -0.05831409692102988, -0.09888250563161437, -0.017193642492439137, 0.316951230796572, -0.3508524090690902, -0.15378323396373011, 0.09636372592046681, -0.24306765005830125, -0.11757983654164351, 0.21985247353685622, -0.102118569464814... |
708.3106 | Rapidity gap survival in the black-disk regime | We summarize how the approach to the black-disk regime (BDR) of strong
interactions at TeV energies influences rapidity gap survival in exclusive hard
diffraction pp -> p + H + p (H = dijet, Qbar-Q, Higgs). Employing a recently
developed partonic description of such processes, we discuss (a) the
suppression of diffra... | hep-ph | we summarize how the approach to the blackdisk regime bdr of strong interactions at tev energies influences rapidity gap survival in exclusive hard diffraction pp p h p h dijet qbarq higgs employing a recently developed partonic description of such processes we discuss a the suppression of diffraction at small impact p... | [['we', 'summarize', 'how', 'the', 'approach', 'to', 'the', 'blackdisk', 'regime', 'bdr', 'of', 'strong', 'interactions', 'at', 'tev', 'energies', 'influences', 'rapidity', 'gap', 'survival', 'in', 'exclusive', 'hard', 'diffraction', 'pp', 'p', 'h', 'p', 'h', 'dijet', 'qbarq', 'higgs', 'employing', 'a', 'recently', 'de... | [-0.0775249961129937, 0.3051984951154511, -0.14350370119011374, 0.22563665299724364, -0.013491107823000741, -0.11315724295660008, 0.05668503425765744, 0.38049792867758764, -0.24102540692967392, -0.29534706614969164, -0.14668970228504083, -0.349091709999502, 0.014585898517026115, 0.029775798296767103, 0.0945426172231199... |
708.3107 | On the generalised Selberg integral of Richards and Zheng | In a recent paper Richards and Zheng compute the determinant of a matrix
whose entries are given by beta-type integrals, thereby generalising an earlier
result by Dixon and Varchenko. They then use their result to obtain a
generalisation of the famous Selberg integral.
In this note we point out that the Selberg-gen... | math.CA math.CO | in a recent paper richards and zheng compute the determinant of a matrix whose entries are given by betatype integrals thereby generalising an earlier result by dixon and varchenko they then use their result to obtain a generalisation of the famous selberg integral in this note we point out that the selberggeneralisati... | [['in', 'a', 'recent', 'paper', 'richards', 'and', 'zheng', 'compute', 'the', 'determinant', 'of', 'a', 'matrix', 'whose', 'entries', 'are', 'given', 'by', 'betatype', 'integrals', 'thereby', 'generalising', 'an', 'earlier', 'result', 'by', 'dixon', 'and', 'varchenko', 'they', 'then', 'use', 'their', 'result', 'to', 'o... | [-0.11630935463229737, 0.01715764523563242, -0.11565036522612597, 0.04842591750396726, -0.11043422680813819, -0.08081272217289855, 0.02795857888365087, 0.29533414032387856, -0.27027559518561856, -0.21214895070685694, 0.12483204454717149, -0.26002002185608336, -0.22914662439143285, 0.2299649317477209, -0.176711894435963... |
708.3108 | Plasmonic Bragg Reflectors for Subwavelength Hole Arrays in a Metal Film | We present plasmonic Bragg reflectors for increasing the extraordinary
optical transmission through periodic arrays of subwavelength apertures in a
metal film. The increase in transmission arises by preventing loss at the edges
of the array. The plasmonic Bragg reflectors have periodicity of half the usual
array's pe... | physics.optics | we present plasmonic bragg reflectors for increasing the extraordinary optical transmission through periodic arrays of subwavelength apertures in a metal film the increase in transmission arises by preventing loss at the edges of the array the plasmonic bragg reflectors have periodicity of half the usual arrays periodi... | [['we', 'present', 'plasmonic', 'bragg', 'reflectors', 'for', 'increasing', 'the', 'extraordinary', 'optical', 'transmission', 'through', 'periodic', 'arrays', 'of', 'subwavelength', 'apertures', 'in', 'a', 'metal', 'film', 'the', 'increase', 'in', 'transmission', 'arises', 'by', 'preventing', 'loss', 'at', 'the', 'edg... | [-0.23573926849731883, 0.14498330840203716, 0.007284313948874019, -0.03301587218639294, -0.03984279647518538, -0.17362703182612008, 0.04851141346826855, 0.5516370054285386, -0.2588087000185624, -0.3073970388228956, 0.09448724147698254, -0.3228937829967196, -0.18770576013546242, 0.21647447582922483, -0.01359504511530854... |
708.3109 | The reddest ISO-2MASS quasar | In the course of the NIR/MIR AGN search combining the 6.7 mu ISOCAM Parallel
Survey and 2MASS we have discovered 24 type-1 quasars about a third of which
are too red to be discriminated by optical/UV search techniques. Here we report
on a detailed case study of the reddest type-1 quasar of our sample (J2341) at
redsh... | astro-ph | in the course of the nirmir agn search combining the 67 mu isocam parallel survey and 2mass we have discovered 24 type1 quasars about a third of which are too red to be discriminated by opticaluv search techniques here we report on a detailed case study of the reddest type1 quasar of our sample j2341 at redshift z0236 ... | [['in', 'the', 'course', 'of', 'the', 'nirmir', 'agn', 'search', 'combining', 'the', '67', 'mu', 'isocam', 'parallel', 'survey', 'and', '2mass', 'we', 'have', 'discovered', '24', 'type1', 'quasars', 'about', 'a', 'third', 'of', 'which', 'are', 'too', 'red', 'to', 'be', 'discriminated', 'by', 'opticaluv', 'search', 'tec... | [0.006946574104069716, 0.060353651184939114, -0.06717986982040543, 0.08442594778573595, -0.09823612396403686, -0.13397049163772223, 0.06010735778840534, 0.4963228798813836, -0.11258390146112422, -0.32906021387076256, 0.05921347565105652, -0.33562244908864963, 0.003799207827806012, 0.1664014848387605, -0.031843551569594... |
708.311 | Rogers-Szego polynomials and Hall-Littlewood symmetric functions | We use Rogers-Szego polynomials to unify some well-known identities for
Hall-Littlewood symmetric functions due to Macdonald and Kawanaka.
| math.CO | we use rogersszego polynomials to unify some wellknown identities for halllittlewood symmetric functions due to macdonald and kawanaka | [['we', 'use', 'rogersszego', 'polynomials', 'to', 'unify', 'some', 'wellknown', 'identities', 'for', 'halllittlewood', 'symmetric', 'functions', 'due', 'to', 'macdonald', 'and', 'kawanaka']] | [-0.07289477106597689, 0.03737965593528417, -0.07355764435811175, 0.1693908376360519, -0.25039850485821563, -0.2078077888323201, -0.024221592272321384, 0.30989924797581303, -0.3681747176580959, -0.11419937304324573, 0.07722956244833767, -0.2482405122783449, -0.2782478007591433, 0.17414329325159392, -0.16343452584826285... |
708.3111 | Cohen-Macaulay, Shellable and unmixed clutters with a perfect matching
of K\"onig type | Let $\mathcal{C}$ be a clutter with a perfect matching $e_1,...,e_g$ of
K\"onig type and let $\Delta_\mathcal{C}$ be the Stanley-Reisner complex of the
edge ideal of $\mathcal{C}$. If all c-minors of $\mathcal{C}$ have a free
vertex and $\mathcal{C}$ is unmixed, we show that $\Delta_\mathcal{C}$ is pure
shellable. We... | math.AC math.CO | let mathcalc be a clutter with a perfect matching e_1e_g of konig type and let delta_mathcalc be the stanleyreisner complex of the edge ideal of mathcalc if all cminors of mathcalc have a free vertex and mathcalc is unmixed we show that delta_mathcalc is pure shellable we are able to describe in combinatorial and algeb... | [['let', 'mathcalc', 'be', 'a', 'clutter', 'with', 'a', 'perfect', 'matching', 'e_1e_g', 'of', 'konig', 'type', 'and', 'let', 'delta_mathcalc', 'be', 'the', 'stanleyreisner', 'complex', 'of', 'the', 'edge', 'ideal', 'of', 'mathcalc', 'if', 'all', 'cminors', 'of', 'mathcalc', 'have', 'a', 'free', 'vertex', 'and', 'mathc... | [-0.1570420459545254, 0.15639151223857917, -0.052982972475281186, 0.03317110316358165, -0.07115269724308111, -0.21452604082624496, -0.04842726971677557, 0.40547036592681857, -0.3264502445337521, -0.17289814531729927, 0.11145500109762799, -0.27606591862915125, -0.12876377341349704, 0.07509953401145, -0.16131629097157496... |
708.3112 | Near-infrared VLT adaptive optics imaging of evolved stars | The high angular resolution and dynamic range achieved by the NACO adaptive
optics system on the VLT is an excellent tool to study the morphology of
Planetary Nebulae (PNe). We observed four stars in different evolutionary
stages from the AGB to the PNe phase.
The images of the inner parts of the PN Hen 2-113 revea... | astro-ph | the high angular resolution and dynamic range achieved by the naco adaptive optics system on the vlt is an excellent tool to study the morphology of planetary nebulae pne we observed four stars in different evolutionary stages from the agb to the pne phase the images of the inner parts of the pn hen 2113 reveal the pre... | [['the', 'high', 'angular', 'resolution', 'and', 'dynamic', 'range', 'achieved', 'by', 'the', 'naco', 'adaptive', 'optics', 'system', 'on', 'the', 'vlt', 'is', 'an', 'excellent', 'tool', 'to', 'study', 'the', 'morphology', 'of', 'planetary', 'nebulae', 'pne', 'we', 'observed', 'four', 'stars', 'in', 'different', 'evolu... | [-0.08489277222042167, 0.034847012094186815, -0.11205788564456756, 0.014148183225459137, -0.12206300171741913, -0.06716501170032939, -0.014646337744455005, 0.4341287740441256, -0.1941141383809059, -0.3296866744315403, 0.07475989434846439, -0.2362130092825134, -0.0746003233416136, 0.16647167756806971, -0.086019959304275... |
708.3113 | The $J$-matrix inverse scattering approach for coupled channels with
different thresholds | The inverse scattering method within the $J$-matrix approach to the two
coupled-channel problem is discussed. We propose a generalization of the
procedure to the case with different thresholds.
| quant-ph | the inverse scattering method within the jmatrix approach to the two coupledchannel problem is discussed we propose a generalization of the procedure to the case with different thresholds | [['the', 'inverse', 'scattering', 'method', 'within', 'the', 'jmatrix', 'approach', 'to', 'the', 'two', 'coupledchannel', 'problem', 'is', 'discussed', 'we', 'propose', 'a', 'generalization', 'of', 'the', 'procedure', 'to', 'the', 'case', 'with', 'different', 'thresholds']] | [-0.03190796077251434, 0.0392244804450976, -0.10074631464002388, 0.10014530491233538, -0.031032994189964875, -0.10953034219398562, 0.04650568137211459, 0.38519853952207733, -0.3046715019403824, -0.2706127435501133, 0.028128282133755938, -0.25917024474724065, -0.20785553833203657, 0.15041606560615556, 0.0094092657174249... |
708.3114 | Differential Twisted K-theory and Applications | In this paper, we develop differential twisted K-theory and define a twisted
Chern character on twisted K-theory which depends on a choice of connection and
curving on the twisting gerbe. We also establish the general Riemann-Roch
theorem in twisted K-theory and find some applications in the study of twisted
K-theory... | math.KT math.DG | in this paper we develop differential twisted ktheory and define a twisted chern character on twisted ktheory which depends on a choice of connection and curving on the twisting gerbe we also establish the general riemannroch theorem in twisted ktheory and find some applications in the study of twisted ktheory of compa... | [['in', 'this', 'paper', 'we', 'develop', 'differential', 'twisted', 'ktheory', 'and', 'define', 'a', 'twisted', 'chern', 'character', 'on', 'twisted', 'ktheory', 'which', 'depends', 'on', 'a', 'choice', 'of', 'connection', 'and', 'curving', 'on', 'the', 'twisting', 'gerbe', 'we', 'also', 'establish', 'the', 'general',... | [-0.26424965042282234, 0.07549672942947258, -0.10735143792222847, 0.13472992716653442, -0.14675092670050535, -0.12430789255621759, 0.00640895168762654, 0.3864036311480132, -0.31838002320040354, -0.21816882565617562, 0.0897189948855984, -0.11608308086764406, -0.24714171004227617, 0.22552334144711494, -0.2422160571271722... |
708.3115 | Functional Time Evolution, Anomaly Potentials, and the Geometric Phase | A free quantum field in 1+1 dimensions admits unitary Schrodinger picture
dynamics along any foliation of spacetime by Cauchy curves. Kuchar showed that
the Schrodinger picture state vectors, viewed as functionals of spacelike
embeddings, satisfy a functional Schrodinger equation in which the generators
of time evolu... | hep-th gr-qc math-ph math.MP | a free quantum field in 11 dimensions admits unitary schrodinger picture dynamics along any foliation of spacetime by cauchy curves kuchar showed that the schrodinger picture state vectors viewed as functionals of spacelike embeddings satisfy a functional schrodinger equation in which the generators of time evolution a... | [['a', 'free', 'quantum', 'field', 'in', '11', 'dimensions', 'admits', 'unitary', 'schrodinger', 'picture', 'dynamics', 'along', 'any', 'foliation', 'of', 'spacetime', 'by', 'cauchy', 'curves', 'kuchar', 'showed', 'that', 'the', 'schrodinger', 'picture', 'state', 'vectors', 'viewed', 'as', 'functionals', 'of', 'spaceli... | [-0.19443124593662972, 0.141166010822039, -0.11409950206519649, 0.08534706807031706, -0.0838487949402292, -0.07061327257275735, -0.020359676419014948, 0.32375793158108196, -0.24130182841945674, -0.22206920134308544, 0.0426360303260485, -0.29645628662518975, -0.16478547330603796, 0.12725529263182972, -0.0359994156020671... |
708.3116 | Air fluorescence measurements in the spectral range 300-420 nm using a
28.5 GeV electron beam | Measurements are reported of the yield and spectrum of fluorescence, excited
by a 28.5 GeV electron beam, in air at a range of pressures of interest to
ultra-high energy cosmic ray detectors. The wavelength range was 300 - 420 nm.
System calibration has been performed using Rayleigh scattering of a nitrogen
laser bea... | astro-ph | measurements are reported of the yield and spectrum of fluorescence excited by a 285 gev electron beam in air at a range of pressures of interest to ultrahigh energy cosmic ray detectors the wavelength range was 300 420 nm system calibration has been performed using rayleigh scattering of a nitrogen laser beam in atmos... | [['measurements', 'are', 'reported', 'of', 'the', 'yield', 'and', 'spectrum', 'of', 'fluorescence', 'excited', 'by', 'a', '285', 'gev', 'electron', 'beam', 'in', 'air', 'at', 'a', 'range', 'of', 'pressures', 'of', 'interest', 'to', 'ultrahigh', 'energy', 'cosmic', 'ray', 'detectors', 'the', 'wavelength', 'range', 'was'... | [-0.07684568304787665, 0.3211560518727364, -0.034285491339259726, 0.006981715417864239, 0.0700515323153334, -0.0998318425639916, 0.03798342866973732, 0.4700923537945046, -0.16787030175328255, -0.4568931944120456, 0.026587479538969037, -0.3754244922550724, 0.14101280373356798, 0.2551960399518173, 0.060238764333703065, 0... |
708.3117 | Comments on the observation of quantum oscillations in cuprates | This paper comments on the recently reported quantum oscillations in
underdoped YBCO crystals. The implications to other experiments and some
hurdles to validating the proposed interpretation are discussed.
| cond-mat.str-el cond-mat.supr-con | this paper comments on the recently reported quantum oscillations in underdoped ybco crystals the implications to other experiments and some hurdles to validating the proposed interpretation are discussed | [['this', 'paper', 'comments', 'on', 'the', 'recently', 'reported', 'quantum', 'oscillations', 'in', 'underdoped', 'ybco', 'crystals', 'the', 'implications', 'to', 'other', 'experiments', 'and', 'some', 'hurdles', 'to', 'validating', 'the', 'proposed', 'interpretation', 'are', 'discussed']] | [-0.10565824397573513, 0.14397183127169097, -0.004653232604531305, 0.04081445308319027, -0.16834995137261494, -0.13827206487102167, 0.06668691043991462, 0.3416412184680147, -0.15164261763649328, -0.2881870931679649, 0.0926520816906954, -0.38073590620686965, -0.1973608528663005, 0.2862336365506053, -0.08926920339997325,... |
708.3118 | Phase Diffusion in Single-Walled Carbon Nanotube Josephson Transistors | We investigate electronic transport in Josephson junctions formed by
single-walled carbon nanotubes coupled to superconducting electrodes. We
observe enhanced zero-bias conductance (up to 10e^2/h) and pronounced
sub-harmonic gap structures in differential conductance, which arise from the
multiple Andreev reflections... | cond-mat.mes-hall cond-mat.supr-con | we investigate electronic transport in josephson junctions formed by singlewalled carbon nanotubes coupled to superconducting electrodes we observe enhanced zerobias conductance up to 10e2h and pronounced subharmonic gap structures in differential conductance which arise from the multiple andreev reflections at superco... | [['we', 'investigate', 'electronic', 'transport', 'in', 'josephson', 'junctions', 'formed', 'by', 'singlewalled', 'carbon', 'nanotubes', 'coupled', 'to', 'superconducting', 'electrodes', 'we', 'observe', 'enhanced', 'zerobias', 'conductance', 'up', 'to', '10e2h', 'and', 'pronounced', 'subharmonic', 'gap', 'structures',... | [-0.2273516783975445, 0.1294899746616447, -0.010570564749175492, -0.022210183484498793, -0.006909933558912302, -0.18644309057188885, 0.11656197525646385, 0.4129620106387123, -0.26445269402073773, -0.32431263767410906, -0.04945230924248772, -0.3237152111963654, -0.1413431619959218, 0.21625769372354736, -0.00922397865895... |
708.3119 | Detection of fidelity and multiparticle entanglement for arbitrary graph
states | withdrawn by the authors because of an error.
| quant-ph | withdrawn by the authors because of an error | [['withdrawn', 'by', 'the', 'authors', 'because', 'of', 'an', 'error']] | [-0.1120248157531023, -0.08911704183083202, -0.051461207680404186, -0.028530369279906154, -0.034761413000524044, -0.02113846456632018, 0.06282268709037453, 0.25568898022174835, -0.3380048223771155, -0.3927389325108379, 0.1172591750510037, -0.2983392346650362, -0.07453011628240347, 0.13353655044920743, -0.39491388550959... |
708.312 | Soliton Solution for the Spin Current in Ferromagnetic Nanowire | We investigate the interaction of a periodic solution and one-soliton
solution for the spin-polarized current in a uniaxial ferromagnetic nanowire.
The amplitude and wave number of the periodic solution for the spin current
have the different contribution to the width, velocity, and the amplitude of
soliton solution,... | cond-mat.other cond-mat.mtrl-sci | we investigate the interaction of a periodic solution and onesoliton solution for the spinpolarized current in a uniaxial ferromagnetic nanowire the amplitude and wave number of the periodic solution for the spin current have the different contribution to the width velocity and the amplitude of soliton solution respect... | [['we', 'investigate', 'the', 'interaction', 'of', 'a', 'periodic', 'solution', 'and', 'onesoliton', 'solution', 'for', 'the', 'spinpolarized', 'current', 'in', 'a', 'uniaxial', 'ferromagnetic', 'nanowire', 'the', 'amplitude', 'and', 'wave', 'number', 'of', 'the', 'periodic', 'solution', 'for', 'the', 'spin', 'current'... | [-0.23060693962240555, 0.09683041475608806, -0.039998509973357216, 0.04754670119243805, -0.06836102970780056, -0.096373514202641, 0.011437468056645349, 0.3722394345171541, -0.27329048365093417, -0.22521401581432776, 0.1420773574788663, -0.2711693139542242, -0.11623898568067038, 0.1928355920903176, 0.055118025418710415,... |
708.3121 | Holographic dark energy in a cyclic universe | In this paper we study the cosmological evolution of the holographic dark
energy in a cyclic universe, generalizing the model of holographic dark energy
proposed by Li. The holographic dark energy with $c<1$ can realize a quintom
behavior; namely, it evolves from a quintessence-like component to a
phantom-like one. T... | hep-th astro-ph gr-qc hep-ph | in this paper we study the cosmological evolution of the holographic dark energy in a cyclic universe generalizing the model of holographic dark energy proposed by li the holographic dark energy with c1 can realize a quintom behavior namely it evolves from a quintessencelike component to a phantomlike one the holograph... | [['in', 'this', 'paper', 'we', 'study', 'the', 'cosmological', 'evolution', 'of', 'the', 'holographic', 'dark', 'energy', 'in', 'a', 'cyclic', 'universe', 'generalizing', 'the', 'model', 'of', 'holographic', 'dark', 'energy', 'proposed', 'by', 'li', 'the', 'holographic', 'dark', 'energy', 'with', 'c1', 'can', 'realize'... | [-0.19696583995311004, 0.17397406130395313, -0.18143049970320943, 0.10784730520309596, -0.09019451357663558, -0.1496128144378114, -0.020508266759861726, 0.2561426555039361, -0.2251767657451435, -0.31324940036413157, 0.030549142192790493, -0.23440470347284442, -0.0691637274576351, 0.12401816725388118, -0.007124399300664... |
708.3122 | An analog of the Iwasawa conjecture for a complete hyperbolic threefold
of finite volume | For a unitary local system of rank one on a complete hyperbolic threefold of
finite volume which has only one cusp, we will compare the order of the
Alexander invariant at t=1 and one of Ruelle-Selberg L-function at s=0. Our
result may be considered as a geometric analog of the Iwasawa main conjecture
in the algebrai... | math.SP math.DG | for a unitary local system of rank one on a complete hyperbolic threefold of finite volume which has only one cusp we will compare the order of the alexander invariant at t1 and one of ruelleselberg lfunction at s0 our result may be considered as a geometric analog of the iwasawa main conjecture in the algebraic number... | [['for', 'a', 'unitary', 'local', 'system', 'of', 'rank', 'one', 'on', 'a', 'complete', 'hyperbolic', 'threefold', 'of', 'finite', 'volume', 'which', 'has', 'only', 'one', 'cusp', 'we', 'will', 'compare', 'the', 'order', 'of', 'the', 'alexander', 'invariant', 'at', 't1', 'and', 'one', 'of', 'ruelleselberg', 'lfunction'... | [-0.2017895922538612, 0.03849896233071361, -0.17115827027316155, 0.0740234377026035, -0.049185646134183594, -0.13567947695162474, -0.017507092326699773, 0.24616195094412224, -0.25359781282512767, -0.23394944785538604, 0.13514799104897274, -0.23546765917470971, -0.12617542632250933, 0.20672071494750285, -0.0922529435013... |
708.3123 | On a special value of the Ruelle L-function | For a unitary local system of rank one on a complete hyperbolic threefold of
finite volume which has only one cusp, the Ruelle L-function is defined. We
will show that if the first cohomology group of the local system vanishes its
value at s=0 is equal to the square of the Franz-Reidemeister torsion.
| math.DG math.SP | for a unitary local system of rank one on a complete hyperbolic threefold of finite volume which has only one cusp the ruelle lfunction is defined we will show that if the first cohomology group of the local system vanishes its value at s0 is equal to the square of the franzreidemeister torsion | [['for', 'a', 'unitary', 'local', 'system', 'of', 'rank', 'one', 'on', 'a', 'complete', 'hyperbolic', 'threefold', 'of', 'finite', 'volume', 'which', 'has', 'only', 'one', 'cusp', 'the', 'ruelle', 'lfunction', 'is', 'defined', 'we', 'will', 'show', 'that', 'if', 'the', 'first', 'cohomology', 'group', 'of', 'the', 'loca... | [-0.23714188305446163, 0.053904717322438955, -0.13441746867297646, 0.025737037967281558, -0.0628604612295301, -0.1269295826428928, -0.012261494429996954, 0.28360822116239714, -0.27817471081820816, -0.1576051436445246, 0.12285630744344626, -0.27917039351394546, -0.12661045343758395, 0.17230546666094318, -0.0690347249261... |
708.3124 | Asymptotic eigenvalue distribution of large Toeplitz matrices | We study the asymptotic eigenvalue distribution of Toeplitz matrices
generated by a singular symbol. It has been conjectured by Widom that, for a
generic symbol, the eigenvalues converge to the image of the symbol. In this
paper we ask how the eigenvalues converge to the image. For a given Toeplitz
matrix $T_n(a)$ of... | math-ph math.MP | we study the asymptotic eigenvalue distribution of toeplitz matrices generated by a singular symbol it has been conjectured by widom that for a generic symbol the eigenvalues converge to the image of the symbol in this paper we ask how the eigenvalues converge to the image for a given toeplitz matrix t_na of size n we ... | [['we', 'study', 'the', 'asymptotic', 'eigenvalue', 'distribution', 'of', 'toeplitz', 'matrices', 'generated', 'by', 'a', 'singular', 'symbol', 'it', 'has', 'been', 'conjectured', 'by', 'widom', 'that', 'for', 'a', 'generic', 'symbol', 'the', 'eigenvalues', 'converge', 'to', 'the', 'image', 'of', 'the', 'symbol', 'in',... | [-0.10440064148783716, 0.039138522424732036, -0.11123653589047294, 0.0657107153602472, -0.013270867287914836, -0.11541947183009665, 0.05069505539619718, 0.31467241375187854, -0.24170744908248296, -0.21315559394146621, 0.13041664054926352, -0.3064167828946086, -0.18847367897489628, 0.12947815578364957, -0.07189079233140... |
708.3125 | Control of spin coherence in semiconductor double quantum dots | We propose a scheme to manipulate the spin coherence in vertically coupled
GaAs double quantum dots. Up to {\em ten} orders of magnitude variation of the
spin relaxation and {\em two} orders of magnitude variation of the spin
dephasing can be achieved by a small gate voltage applied vertically on the
double dot. Spec... | cond-mat.mtrl-sci | we propose a scheme to manipulate the spin coherence in vertically coupled gaas double quantum dots up to em ten orders of magnitude variation of the spin relaxation and em two orders of magnitude variation of the spin dephasing can be achieved by a small gate voltage applied vertically on the double dot specially larg... | [['we', 'propose', 'a', 'scheme', 'to', 'manipulate', 'the', 'spin', 'coherence', 'in', 'vertically', 'coupled', 'gaas', 'double', 'quantum', 'dots', 'up', 'to', 'em', 'ten', 'orders', 'of', 'magnitude', 'variation', 'of', 'the', 'spin', 'relaxation', 'and', 'em', 'two', 'orders', 'of', 'magnitude', 'variation', 'of', ... | [-0.18069516815581269, 0.21546593865141608, 0.011706801449978039, 0.055932803139512544, -0.0005005559519885626, -0.14188872314849518, 0.01871088734141698, 0.3914447787070745, -0.31689004992183883, -0.2982162532529661, 0.01334326168263149, -0.26507162106664556, -0.05566827268724827, 0.19552471392080747, 0.07865458452737... |
708.3126 | Semilattice Structures of Spreading Models | Given a Banach space X, denote by SP_{w}(X) the set of equivalence classes of
spreading models of X generated by normalized weakly null sequences in X. It is
known that SP_{w}(X) is a semilattice, i.e., it is a partially ordered set in
which every pair of elements has a least upper bound. We show that every
countable... | math.FA | given a banach space x denote by sp_wx the set of equivalence classes of spreading models of x generated by normalized weakly null sequences in x it is known that sp_wx is a semilattice ie it is a partially ordered set in which every pair of elements has a least upper bound we show that every countable semilattice that... | [['given', 'a', 'banach', 'space', 'x', 'denote', 'by', 'sp_wx', 'the', 'set', 'of', 'equivalence', 'classes', 'of', 'spreading', 'models', 'of', 'x', 'generated', 'by', 'normalized', 'weakly', 'null', 'sequences', 'in', 'x', 'it', 'is', 'known', 'that', 'sp_wx', 'is', 'a', 'semilattice', 'ie', 'it', 'is', 'a', 'partia... | [-0.18701504042686581, 0.20927416448131378, -0.04256407686134244, 0.05548727940904073, -0.06635540652741956, -0.10624162134920041, 0.03985629461905254, 0.41066873805331333, -0.3392250072452929, -0.13872837312761452, 0.09656655867342148, -0.3293488714118282, -0.1017367248725775, 0.1771478485263122, -0.09767892838050551,... |
708.3127 | Question on Conditional Entropy | The problems of conditional entropy's definition and the formula to compute
conditional entropy are analyzed from various perspectives, and the corrected
computing formula is presented. Examples are given to prove the conclusion that
conditional entropy never be increased is not absolute, thus the representation
that... | cs.IT math.IT | the problems of conditional entropys definition and the formula to compute conditional entropy are analyzed from various perspectives and the corrected computing formula is presented examples are given to prove the conclusion that conditional entropy never be increased is not absolute thus the representation that infor... | [['the', 'problems', 'of', 'conditional', 'entropys', 'definition', 'and', 'the', 'formula', 'to', 'compute', 'conditional', 'entropy', 'are', 'analyzed', 'from', 'various', 'perspectives', 'and', 'the', 'corrected', 'computing', 'formula', 'is', 'presented', 'examples', 'are', 'given', 'to', 'prove', 'the', 'conclusio... | [-0.04446112529781126, 0.11516961436403, -0.15789583532171228, 0.14570111802274013, -0.083887954921288, -0.14312462085636996, 0.02420196316789015, 0.3422586775179637, -0.27999961641380344, -0.30595327399165956, 0.12862329646526693, -0.30686060437080215, -0.11036243126333012, 0.21132382171591585, -0.17400030116155996, 0... |
708.3128 | The u-invariant of the function fields of p-adic curves | The u-invariant of a field is the maximum dimension of ansiotropic quadratic
forms over the field. It is an open question whether the u-invariant of
function fields of p-aidc curves is 8. In this paper, we answer this question
in the affirmative for function fields of non-dyadic p-adic curves.
| math.NT | the uinvariant of a field is the maximum dimension of ansiotropic quadratic forms over the field it is an open question whether the uinvariant of function fields of paidc curves is 8 in this paper we answer this question in the affirmative for function fields of nondyadic padic curves | [['the', 'uinvariant', 'of', 'a', 'field', 'is', 'the', 'maximum', 'dimension', 'of', 'ansiotropic', 'quadratic', 'forms', 'over', 'the', 'field', 'it', 'is', 'an', 'open', 'question', 'whether', 'the', 'uinvariant', 'of', 'function', 'fields', 'of', 'paidc', 'curves', 'is', '8', 'in', 'this', 'paper', 'we', 'answer', ... | [-0.2234535469712379, 0.08051531070456501, -0.10397917387308553, 0.09313801398820942, -0.0721306809282396, -0.06341558965505101, 0.011284644892536258, 0.31201916133674484, -0.31528863155593473, -0.28009830781957135, 0.06948623401209868, -0.22774314826043943, -0.1728363528770084, 0.25959887421534705, -0.1110311583033762... |
708.3129 | Entanglement cost and distillable entanglement of symmetric states | We compute entanglement cost and distillable entanglement of states supported
on symmetric subspace. Not only giving general formula, we apply them to the
output states of optimal cloning machines. Surprisingly, under some settings,
the optimal n to m clone and true m copies are the same in entanglement
measures. How... | quant-ph | we compute entanglement cost and distillable entanglement of states supported on symmetric subspace not only giving general formula we apply them to the output states of optimal cloning machines surprisingly under some settings the optimal n to m clone and true m copies are the same in entanglement measures however the... | [['we', 'compute', 'entanglement', 'cost', 'and', 'distillable', 'entanglement', 'of', 'states', 'supported', 'on', 'symmetric', 'subspace', 'not', 'only', 'giving', 'general', 'formula', 'we', 'apply', 'them', 'to', 'the', 'output', 'states', 'of', 'optimal', 'cloning', 'machines', 'surprisingly', 'under', 'some', 'se... | [-0.15054954624093778, 0.1756981142203916, -0.0807654107376546, 0.11867565851108255, 0.009848534706344997, -0.2568612301951976, 0.11150302951429765, 0.36128583018268856, -0.2316436291756955, -0.21427953880062545, 0.09517701631472386, -0.2643440423968744, -0.08957480103708804, 0.1781559896824712, -0.13331451548819806, 0... |
708.313 | Equation of state for shock-compressed porous molybdenum from
first-principles mean-field potential calculations | The Hugoniot curves for shock-compressed molybdenum with initial porosities
of 1.0, 1.26, 1.83, and 2.31 are theoretically investigated. The method of
calculations combines the first-principles treatment for zero- and
finite-temperature electronic contribution and the mean-field-potential
approach for the ion-thermal... | cond-mat.mtrl-sci cond-mat.stat-mech | the hugoniot curves for shockcompressed molybdenum with initial porosities of 10 126 183 and 231 are theoretically investigated the method of calculations combines the firstprinciples treatment for zero and finitetemperature electronic contribution and the meanfieldpotential approach for the ionthermal contribution to ... | [['the', 'hugoniot', 'curves', 'for', 'shockcompressed', 'molybdenum', 'with', 'initial', 'porosities', 'of', '10', '126', '183', 'and', '231', 'are', 'theoretically', 'investigated', 'the', 'method', 'of', 'calculations', 'combines', 'the', 'firstprinciples', 'treatment', 'for', 'zero', 'and', 'finitetemperature', 'el... | [-0.028022538775401395, 0.1260704149485287, -0.05656241077970523, -2.6670164754954133e-05, 0.012026968791088374, -0.0693344960539826, 0.05709135527620568, 0.39979685388886144, -0.22531349024307118, -0.32519379818308963, 0.04667900871216952, -0.3492415841927167, -0.040324976020095354, 0.22381090303631432, 0.048486123915... |
708.3131 | Scattering of spin-polarized electron in an Aharonov--Bohm potential | The scattering of spin-polarized electrons in an Aharonov--Bohm vector
potential is considered. We solve the Pauli equation in 3+1 dimensions taking
into account explicitly the interaction between the three-dimensional spin
magnetic moment of electron and magnetic field. Expressions for the scattering
amplitude and t... | hep-th cond-mat.other math-ph math.MP quant-ph | the scattering of spinpolarized electrons in an aharonovbohm vector potential is considered we solve the pauli equation in 31 dimensions taking into account explicitly the interaction between the threedimensional spin magnetic moment of electron and magnetic field expressions for the scattering amplitude and the cross ... | [['the', 'scattering', 'of', 'spinpolarized', 'electrons', 'in', 'an', 'aharonovbohm', 'vector', 'potential', 'is', 'considered', 'we', 'solve', 'the', 'pauli', 'equation', 'in', '31', 'dimensions', 'taking', 'into', 'account', 'explicitly', 'the', 'interaction', 'between', 'the', 'threedimensional', 'spin', 'magnetic'... | [-0.1708645481762397, 0.21827723720606956, -0.03749690906323017, 0.13468219021067737, 0.019829020003213526, -0.10506013391460194, 0.014320695619817149, 0.3504816120133755, -0.22978059856339972, -0.2672734329714737, -0.0123359544024347, -0.29286600602790713, -0.08354034274816513, 0.2012371126973526, 0.058891834968582114... |
708.3132 | Casimir Forces in Trapped Dilute Bose Gas Between Two Slabs | We discuss a Casimir force due to zero-temperature quantum fluctuations in a
weakly interacting Bose-Einstein condensate (BEC) with a strong harmonic trap.
The results show that the presence of a strong harmonic trap changes the power
law behavior of Casimir force due to the dimensional reduction effect. At
finite te... | cond-mat.other | we discuss a casimir force due to zerotemperature quantum fluctuations in a weakly interacting boseeinstein condensate bec with a strong harmonic trap the results show that the presence of a strong harmonic trap changes the power law behavior of casimir force due to the dimensional reduction effect at finite temperatur... | [['we', 'discuss', 'a', 'casimir', 'force', 'due', 'to', 'zerotemperature', 'quantum', 'fluctuations', 'in', 'a', 'weakly', 'interacting', 'boseeinstein', 'condensate', 'bec', 'with', 'a', 'strong', 'harmonic', 'trap', 'the', 'results', 'show', 'that', 'the', 'presence', 'of', 'a', 'strong', 'harmonic', 'trap', 'change... | [-0.17700419855468413, 0.22986327540283502, -0.10963365813059842, 0.03131177732173134, -0.04427690032650443, -0.1225170829497716, 0.013289940444862142, 0.3239571031402139, -0.2361120666925083, -0.22970888334709932, 0.00020553499378044815, -0.321819616514532, -0.14714793338823845, 0.19225991249413174, 0.0149711565854137... |
708.3133 | Elliptical hole pockets in the Fermi surfaces of unhydrated and hydrated
sodium cobalt oxides | The surprise discovery of superconductivity below 5K in sodium cobalt oxides
when hydrated with water has caught the attention of experimentalists and
theorists alike. Most explanations for its occurence have focused heavily on
the properties of some small elliptically shaped pockets predicted to be the
electronicall... | cond-mat.supr-con cond-mat.str-el | the surprise discovery of superconductivity below 5k in sodium cobalt oxides when hydrated with water has caught the attention of experimentalists and theorists alike most explanations for its occurence have focused heavily on the properties of some small elliptically shaped pockets predicted to be the electronically d... | [['the', 'surprise', 'discovery', 'of', 'superconductivity', 'below', '5k', 'in', 'sodium', 'cobalt', 'oxides', 'when', 'hydrated', 'with', 'water', 'has', 'caught', 'the', 'attention', 'of', 'experimentalists', 'and', 'theorists', 'alike', 'most', 'explanations', 'for', 'its', 'occurence', 'have', 'focused', 'heavily'... | [-0.09554748350934943, 0.18334330858814776, -0.054488283201900065, 0.07583409183829719, -0.08451912374881913, -0.16387809713713217, 0.1112279974622652, 0.4255126226047168, -0.17692528437699515, -0.2924591274409346, 0.06004565589757142, -0.3636674998632195, -0.123684930750549, 0.19088560630382057, -0.0016599949971981803... |
708.3134 | Pseudoknot RNA Structures with Arc-Length $\ge 3$ | In this paper we study $k$-noncrossing RNA structures with arc-length $\ge
3$, i.e. RNA molecules in which for any $i$, the nucleotides labeled $i$ and
$i+j$ ($j=1,2$) cannot form a bond and in which there are at most $k-1$
mutually crossing arcs. Let ${\sf S}_{k,3}(n)$ denote their number. Based on a
novel functiona... | math.CO q-bio.BM | in this paper we study knoncrossing rna structures with arclength ge 3 ie rna molecules in which for any i the nucleotides labeled i and ij j12 cannot form a bond and in which there are at most k1 mutually crossing arcs let sf s_k3n denote their number based on a novel functional equation for the generating function su... | [['in', 'this', 'paper', 'we', 'study', 'knoncrossing', 'rna', 'structures', 'with', 'arclength', 'ge', '3', 'ie', 'rna', 'molecules', 'in', 'which', 'for', 'any', 'i', 'the', 'nucleotides', 'labeled', 'i', 'and', 'ij', 'j12', 'can', 'not', 'form', 'a', 'bond', 'and', 'in', 'which', 'there', 'are', 'at', 'most', 'k1', ... | [-0.17388674361241419, 0.1470445791519312, -0.013344244885280035, 0.03267520752757094, -0.033689395497488075, -0.167317945591369, 0.03239739830010072, 0.34239768940240667, -0.24098399605704904, -0.2539408345121977, 0.015265621208358383, -0.292438734084541, -0.16842238048394753, 0.13377980099514472, -0.01050207821170388... |
708.3135 | Mid-Infrared Instrumentation for the European Extremely Large Telescope | MIDIR is the proposed thermal/mid-IR imager and spectrograph for the European
Extremely Large Telescope (E-ELT). It will cover the wavelength range of 3 to
at least 20 microns. Designed for diffraction-limited performance over the
entire wavelength range, MIDIR will require an adaptive optics system; a
cryogenically ... | astro-ph | midir is the proposed thermalmidir imager and spectrograph for the european extremely large telescope eelt it will cover the wavelength range of 3 to at least 20 microns designed for diffractionlimited performance over the entire wavelength range midir will require an adaptive optics system a cryogenically cooled syste... | [['midir', 'is', 'the', 'proposed', 'thermalmidir', 'imager', 'and', 'spectrograph', 'for', 'the', 'european', 'extremely', 'large', 'telescope', 'eelt', 'it', 'will', 'cover', 'the', 'wavelength', 'range', 'of', '3', 'to', 'at', 'least', '20', 'microns', 'designed', 'for', 'diffractionlimited', 'performance', 'over', ... | [-0.09865364142808483, 0.0843615965547672, -0.07931664123429687, 0.009384098315351436, -0.10030063941421641, -0.12889567702440183, 0.020128220593399526, 0.4407497364785764, -0.2005587287501178, -0.34315708576544346, 0.17782431747537567, -0.2447572401240952, -0.12626920734243408, 0.2682188006235867, -0.08071695321674954... |
708.3136 | Atmospheric instability as a loss of a metastable equilibrium | General thermodynamic theory of metastable states is used in this short note
to try to understand better atmospheric instabilities. It is shown that not
only cooling of a cloud can lead to rain, but heating also, especially when
there are charged water drops in a cloud (in this case we have rain with
lightning). The ... | physics.ao-ph physics.chem-ph | general thermodynamic theory of metastable states is used in this short note to try to understand better atmospheric instabilities it is shown that not only cooling of a cloud can lead to rain but heating also especially when there are charged water drops in a cloud in this case we have rain with lightning the influenc... | [['general', 'thermodynamic', 'theory', 'of', 'metastable', 'states', 'is', 'used', 'in', 'this', 'short', 'note', 'to', 'try', 'to', 'understand', 'better', 'atmospheric', 'instabilities', 'it', 'is', 'shown', 'that', 'not', 'only', 'cooling', 'of', 'a', 'cloud', 'can', 'lead', 'to', 'rain', 'but', 'heating', 'also', ... | [-0.0861281197558128, 0.21311114165291656, -0.09806312649379834, 0.13979244273832592, -0.015280685871402966, -0.08958688174607232, 0.03542533605104836, 0.3938126649882179, -0.23091592398122884, -0.2623191513994243, 0.12814633159177902, -0.26507657144975383, -0.1508088305417914, 0.17252766503952444, -0.12802279625611845... |
708.3137 | Recent Developments on Kaon Condensation and Its Astrophysical
Implications | We discuss three different ways to arrive at kaon condensation at n_c = 3 n_0
where n_0 is nuclear matter density: (1) Fluctuating around the n=0 vacuum in
chiral perturbation theory, (2) fluctuating around n_VM near the chiral
restoration density n_chi where the vector manifestation of hidden local
symmetry is reach... | hep-ph astro-ph nucl-th | we discuss three different ways to arrive at kaon condensation at n_c 3 n_0 where n_0 is nuclear matter density 1 fluctuating around the n0 vacuum in chiral perturbation theory 2 fluctuating around n_vm near the chiral restoration density n_chi where the vector manifestation of hidden local symmetry is reached and 3 fl... | [['we', 'discuss', 'three', 'different', 'ways', 'to', 'arrive', 'at', 'kaon', 'condensation', 'at', 'n_c', '3', 'n_0', 'where', 'n_0', 'is', 'nuclear', 'matter', 'density', '1', 'fluctuating', 'around', 'the', 'n0', 'vacuum', 'in', 'chiral', 'perturbation', 'theory', '2', 'fluctuating', 'around', 'n_vm', 'near', 'the'... | [-0.10334127960523481, 0.24971111120543252, -0.10246779902381936, 0.12033912783294448, -0.03912422949587738, -0.11520582679960771, 0.07214880875935815, 0.3316090064130814, -0.14661451431862285, -0.28737997270456933, 0.04437790570972932, -0.33326635344108557, -0.009634325139390432, 0.1323950991335208, 0.0067773204059283... |
708.3138 | Dynamics of condensation of wetting layer in time-dependent
Ginzburg-Landau model | The dynamics of liquid condensation on a substrate or within a capillary is
studied when the wetting film grows via interface-limited growth. We use a
phenomenological time-dependent Ginzburg-Landau (TDGL)-type model with
long-range substrate potential. Using an order parameter, which does not
directly represent the ... | cond-mat.soft | the dynamics of liquid condensation on a substrate or within a capillary is studied when the wetting film grows via interfacelimited growth we use a phenomenological timedependent ginzburglandau tdgltype model with longrange substrate potential using an order parameter which does not directly represent the density we c... | [['the', 'dynamics', 'of', 'liquid', 'condensation', 'on', 'a', 'substrate', 'or', 'within', 'a', 'capillary', 'is', 'studied', 'when', 'the', 'wetting', 'film', 'grows', 'via', 'interfacelimited', 'growth', 'we', 'use', 'a', 'phenomenological', 'timedependent', 'ginzburglandau', 'tdgltype', 'model', 'with', 'longrange... | [-0.10899436701431993, 0.15383986767751145, -0.12899608367665127, 0.011927320763908818, -0.10217022108794241, -0.11465670174028683, 0.015927775536541018, 0.33813323025274405, -0.2649646336391855, -0.2614231883640309, 0.052453930131517924, -0.26649595655828384, -0.175147482554766, 0.16536251528976628, 0.0004099953361879... |
708.3139 | Baryon vector and axial content up to the 7Q component | We have used the light-cone formulation of Chiral-Quark Soliton Model to
investigate the vector and axial content of octet, decuplet and the
hypothetical antidecuplet in the flavor SU(3) symmetry limit. We have extended
previous works by computing the 7Q contribution to vector and axial charges for
the octet and anti... | hep-ph | we have used the lightcone formulation of chiralquark soliton model to investigate the vector and axial content of octet decuplet and the hypothetical antidecuplet in the flavor su3 symmetry limit we have extended previous works by computing the 7q contribution to vector and axial charges for the octet and antidecuplet... | [['we', 'have', 'used', 'the', 'lightcone', 'formulation', 'of', 'chiralquark', 'soliton', 'model', 'to', 'investigate', 'the', 'vector', 'and', 'axial', 'content', 'of', 'octet', 'decuplet', 'and', 'the', 'hypothetical', 'antidecuplet', 'in', 'the', 'flavor', 'su3', 'symmetry', 'limit', 'we', 'have', 'extended', 'prev... | [-0.07815547298649143, 0.21879627800765722, -0.06715465503671736, 0.13439966932249567, -0.09560772974129303, -0.08560678252670305, 0.09151448443793735, 0.3662366282462684, -0.14479026390358293, -0.29094502744356204, 0.03001141111865591, -0.2923387074203906, -0.022920103568668946, 0.07358979452949237, 0.0588802365052401... |
708.314 | Optical Identification of 15 Micron Sources in the AKARI Performance
Verification Field toward the North Ecliptic Pole | We present the results of optical identifications for 257 mid-infrared
sources detected with a deep 15um survey over approximately 80 arcmin^2 area in
the AKARI performance verification field near the North Ecliptic Pole. The 15um
fluxes of the sources range from 1 mJy down to 40 uJy, approximately a half of
which ar... | astro-ph | we present the results of optical identifications for 257 midinfrared sources detected with a deep 15um survey over approximately 80 arcmin2 area in the akari performance verification field near the north ecliptic pole the 15um fluxes of the sources range from 1 mjy down to 40 ujy approximately a half of which are belo... | [['we', 'present', 'the', 'results', 'of', 'optical', 'identifications', 'for', '257', 'midinfrared', 'sources', 'detected', 'with', 'a', 'deep', '15um', 'survey', 'over', 'approximately', '80', 'arcmin2', 'area', 'in', 'the', 'akari', 'performance', 'verification', 'field', 'near', 'the', 'north', 'ecliptic', 'pole', ... | [-0.01604399373471283, 0.055449431752211426, -0.07821296075753008, 0.08015362949222007, -0.08231013428228788, -0.037266188186720714, 0.06740061887719023, 0.5083204898341463, -0.08712039729202183, -0.3814486272465915, 0.09615280160151321, -0.3349965257395027, -0.004142876107018823, 0.23056492283711463, -0.04213514276800... |
708.3141 | On the universality of the Discrete Nonlinear Schroedinger Equation | We address the universal applicability of the discrete nonlinear Schroedinger
equation. By employing an original but general top-down/bottom-up procedure
based on symmetry analysis to the case of optical lattices, we derive the most
widely applicable and the simplest possible model, revealing that the discrete
nonlin... | physics.optics physics.gen-ph | we address the universal applicability of the discrete nonlinear schroedinger equation by employing an original but general topdownbottomup procedure based on symmetry analysis to the case of optical lattices we derive the most widely applicable and the simplest possible model revealing that the discrete nonlinear schr... | [['we', 'address', 'the', 'universal', 'applicability', 'of', 'the', 'discrete', 'nonlinear', 'schroedinger', 'equation', 'by', 'employing', 'an', 'original', 'but', 'general', 'topdownbottomup', 'procedure', 'based', 'on', 'symmetry', 'analysis', 'to', 'the', 'case', 'of', 'optical', 'lattices', 'we', 'derive', 'the',... | [-0.0718746189115758, 0.07062586596884353, -0.07011051951111227, 0.08940529869700634, -0.14059659382463366, -0.18653138421907806, -0.03554248118746108, 0.34576933982147684, -0.2722601976053303, -0.2284451177937613, 0.08368588226469423, -0.22193693542394086, -0.2127307269020357, 0.20114691637834345, -0.00772337537204873... |
708.3142 | Basic principle of superconductivity | The basic principle of superconductivity is suggested in this paper. There
have been two vital wrong suggestions on the basic principle, one is the
relation between superconductivity and the Bose-Einstein condensation (BEC),
and another is the relation between superconductivity and pseudogap.
| physics.gen-ph | the basic principle of superconductivity is suggested in this paper there have been two vital wrong suggestions on the basic principle one is the relation between superconductivity and the boseeinstein condensation bec and another is the relation between superconductivity and pseudogap | [['the', 'basic', 'principle', 'of', 'superconductivity', 'is', 'suggested', 'in', 'this', 'paper', 'there', 'have', 'been', 'two', 'vital', 'wrong', 'suggestions', 'on', 'the', 'basic', 'principle', 'one', 'is', 'the', 'relation', 'between', 'superconductivity', 'and', 'the', 'boseeinstein', 'condensation', 'bec', 'an... | [-0.16233718081763604, 0.18969737780961868, -0.09970244129256504, 0.14092282354036664, -0.10227194105888285, -0.17156050131633516, 0.09340225889563288, 0.3299035982387822, -0.23479068165690434, -0.2444257902481207, 0.00016275635159506303, -0.31376667893150956, -0.1609969627475593, 0.15884429889890114, -0.02088913525931... |
708.3143 | Statistical Approach to the Cosmological-Constant Problem on Brane
Worlds | We investigate the physically accepted solutions of general Braneworld
scenarios, scanning uniformly the associated parameter space. Without making
any further assumptions we find that solutions which give "small" Hubble
parameters on the physical brane, and therefore "small" effective cosmological
constants on the 4... | hep-th astro-ph | we investigate the physically accepted solutions of general braneworld scenarios scanning uniformly the associated parameter space without making any further assumptions we find that solutions which give small hubble parameters on the physical brane and therefore small effective cosmological constants on the 4d univers... | [['we', 'investigate', 'the', 'physically', 'accepted', 'solutions', 'of', 'general', 'braneworld', 'scenarios', 'scanning', 'uniformly', 'the', 'associated', 'parameter', 'space', 'without', 'making', 'any', 'further', 'assumptions', 'we', 'find', 'that', 'solutions', 'which', 'give', 'small', 'hubble', 'parameters', ... | [-0.1304731893003918, 0.15519559801157032, -0.05254855565061527, 0.12663571246500527, -0.1318883523810655, -0.13495654808357357, 0.04770882563399417, 0.3247457661665976, -0.2168741762638092, -0.2860350261858132, 0.10705531103137349, -0.2580238447790699, -0.07432416396747743, 0.19367933520781141, -0.03148556562539722, 0... |
708.3144 | Noether theorem for mu-symmetries | We give a version of Noether theorem adapted to the framework of
mu-symmetries; this extends to such case recent work by Muriel, Romero and
Olver in the framework of lambda-symmetries, and connects mu-symmetries of a
Lagrangian to a suitably modified conservation law. In some cases this
"mu-conservation law'' actuall... | math-ph math.MP | we give a version of noether theorem adapted to the framework of musymmetries this extends to such case recent work by muriel romero and olver in the framework of lambdasymmetries and connects musymmetries of a lagrangian to a suitably modified conservation law in some cases this muconservation law actually reduces to ... | [['we', 'give', 'a', 'version', 'of', 'noether', 'theorem', 'adapted', 'to', 'the', 'framework', 'of', 'musymmetries', 'this', 'extends', 'to', 'such', 'case', 'recent', 'work', 'by', 'muriel', 'romero', 'and', 'olver', 'in', 'the', 'framework', 'of', 'lambdasymmetries', 'and', 'connects', 'musymmetries', 'of', 'a', 'l... | [-0.1017093244840258, 0.04328424441960773, -0.10944790800567716, 0.1115945685367998, -0.11530403615324758, -0.1358113671178996, 0.027960756920427748, 0.2548366697405332, -0.2881817140816046, -0.3064999481939594, 0.06767962751577475, -0.23363542980847082, -0.1829765128204599, 0.15676370204684126, -0.17353738317823236, 0... |
708.3145 | Thermodynamics of regular black hole | We investigate thermodynamics for a magnetically charged regular black hole
(MCRBH), which comes from the action of general relativity and nonlinear
electromagnetics, comparing with the Reissner-Norstr\"om (RN) black hole in
both four and two dimensions after dimensional reduction. We find that there is
no thermodyna... | gr-qc | we investigate thermodynamics for a magnetically charged regular black hole mcrbh which comes from the action of general relativity and nonlinear electromagnetics comparing with the reissnernorstrom rn black hole in both four and two dimensions after dimensional reduction we find that there is no thermodynamic differen... | [['we', 'investigate', 'thermodynamics', 'for', 'a', 'magnetically', 'charged', 'regular', 'black', 'hole', 'mcrbh', 'which', 'comes', 'from', 'the', 'action', 'of', 'general', 'relativity', 'and', 'nonlinear', 'electromagnetics', 'comparing', 'with', 'the', 'reissnernorstrom', 'rn', 'black', 'hole', 'in', 'both', 'fou... | [-0.12948229183619556, 0.08453119756131057, -0.05528273937096329, 0.10905552819052614, -0.02887289295700101, -0.15519292097081216, 0.01635062304966707, 0.2698765220529024, -0.19150001326935334, -0.22908267362468077, 0.10397247094946929, -0.35496546687525615, -0.1214029346939928, 0.1545571828273272, -0.06770942602796774... |
708.3146 | Absorption cross section of RN black hole | The behavior of a charged scalar field in the RN black hole space time is
studied using WKB approximation. In the present work it is assumed that matter
waves can get reflected from the event horizon. Using this effect, the Hawking
temperature and the absorption cross section for RN black hole placed in a
charged sca... | gr-qc | the behavior of a charged scalar field in the rn black hole space time is studied using wkb approximation in the present work it is assumed that matter waves can get reflected from the event horizon using this effect the hawking temperature and the absorption cross section for rn black hole placed in a charged scalar f... | [['the', 'behavior', 'of', 'a', 'charged', 'scalar', 'field', 'in', 'the', 'rn', 'black', 'hole', 'space', 'time', 'is', 'studied', 'using', 'wkb', 'approximation', 'in', 'the', 'present', 'work', 'it', 'is', 'assumed', 'that', 'matter', 'waves', 'can', 'get', 'reflected', 'from', 'the', 'event', 'horizon', 'using', 't... | [-0.1335627041698899, 0.13320190398953854, -0.06861099710222333, 0.12676649055501912, -0.058416080730967226, -0.1310653028660454, -0.04760685048822779, 0.30574868319090454, -0.17738696494488976, -0.26432507620193063, 0.05469774470111588, -0.38835817001527173, -0.050015232886653396, 0.16181294121779502, 0.01354106492362... |
708.3147 | Controllability of Quantum Systems on the Lie Group SU(1,1) | This paper examines the controllability for quantum control systems with
SU(1,1) dynamical symmetry, namely, the ability to use some electromagnetic
field to redirect the quantum system toward a desired evolution. The problem is
formalized as the control of a right invariant bilinear system evolving on the
Lie group ... | math.OC math.QA | this paper examines the controllability for quantum control systems with su11 dynamical symmetry namely the ability to use some electromagnetic field to redirect the quantum system toward a desired evolution the problem is formalized as the control of a right invariant bilinear system evolving on the lie group su11 of ... | [['this', 'paper', 'examines', 'the', 'controllability', 'for', 'quantum', 'control', 'systems', 'with', 'su11', 'dynamical', 'symmetry', 'namely', 'the', 'ability', 'to', 'use', 'some', 'electromagnetic', 'field', 'to', 'redirect', 'the', 'quantum', 'system', 'toward', 'a', 'desired', 'evolution', 'the', 'problem', 'i... | [-0.21224864246323705, 0.09042178592147324, -0.04821891430030731, 0.05530229247247493, -0.08925039366167943, -0.14433585192886117, -0.029242354541230333, 0.35853315369018074, -0.27817059181702947, -0.24788308587124191, 0.16372133408971493, -0.20969770107083746, -0.14901805058284437, 0.19995449581499963, -0.059262824904... |
708.3148 | R-symmetry, supersymmetry breaking and metastable vacua in global and
local supersymmetric theories | We study N=1 global and local supersymmetric theories with a continuous
global $U(1)_R$ symmetry as models of dynamical supersymmetry (SUSY) breaking.
We introduce explicit R-symmetry breaking terms into such models, in particular
a generalized O'Raifeartaigh model. Such explicit R-symmetry breaking terms can
lead to... | hep-th hep-ph | we study n1 global and local supersymmetric theories with a continuous global u1_r symmetry as models of dynamical supersymmetry susy breaking we introduce explicit rsymmetry breaking terms into such models in particular a generalized oraifeartaigh model such explicit rsymmetry breaking terms can lead to a susy preserv... | [['we', 'study', 'n1', 'global', 'and', 'local', 'supersymmetric', 'theories', 'with', 'a', 'continuous', 'global', 'u1_r', 'symmetry', 'as', 'models', 'of', 'dynamical', 'supersymmetry', 'susy', 'breaking', 'we', 'introduce', 'explicit', 'rsymmetry', 'breaking', 'terms', 'into', 'such', 'models', 'in', 'particular', '... | [-0.14958072070217465, 0.19343700784009807, -0.03735512670603876, 0.1706036673453839, -0.1027473494155992, -0.18127299719258727, 0.0021600070371876777, 0.32494384397879844, -0.197371405980301, -0.27421213142712664, 0.1311093194768851, -0.20988938645951405, -0.16766284643132812, 0.06537855399471725, -0.05768674199602434... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.