id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.1514 | Electron and hole spin dynamics and decoherence in quantum dots | In this article we review our work on the dynamics and decoherence of
electron and hole spins in single and double quantum dots. The first part, on
electron spins, focuses on decoherence induced via the hyperfine interaction
while the second part covers decoherence and relaxation of heavy-hole spins due
to spin-orbit... | cond-mat.mes-hall | in this article we review our work on the dynamics and decoherence of electron and hole spins in single and double quantum dots the first part on electron spins focuses on decoherence induced via the hyperfine interaction while the second part covers decoherence and relaxation of heavyhole spins due to spinorbit intera... | [['in', 'this', 'article', 'we', 'review', 'our', 'work', 'on', 'the', 'dynamics', 'and', 'decoherence', 'of', 'electron', 'and', 'hole', 'spins', 'in', 'single', 'and', 'double', 'quantum', 'dots', 'the', 'first', 'part', 'on', 'electron', 'spins', 'focuses', 'on', 'decoherence', 'induced', 'via', 'the', 'hyperfine', ... | [-0.13766133836828745, 0.2069596651654977, 0.06083606528476454, 0.026065252769666796, 0.006666769775060507, -0.11456278665707662, 0.002497740602120757, 0.3818243928683492, -0.2322923020602992, -0.29210563104313153, -0.003603049385576294, -0.3066687411986865, -0.06994289417679493, 0.2039350076793478, 0.0733097362690247,... |
706.1515 | The generalized non-linear Schrodinger model on the interval | The generalized (1+1)-D non-linear Schrodinger (NLS) theory with particular
integrable boundary conditions is considered. More precisely, two distinct
types of boundary conditions, known as soliton preserving (SP) and soliton
non-preserving (SNP), are implemented into the classical $gl_N$ NLS model.
Based on this cho... | hep-th math-ph math.MP nlin.SI | the generalized 11d nonlinear schrodinger nls theory with particular integrable boundary conditions is considered more precisely two distinct types of boundary conditions known as soliton preserving sp and soliton nonpreserving snp are implemented into the classical gl_n nls model based on this choice of boundaries the... | [['the', 'generalized', '11d', 'nonlinear', 'schrodinger', 'nls', 'theory', 'with', 'particular', 'integrable', 'boundary', 'conditions', 'is', 'considered', 'more', 'precisely', 'two', 'distinct', 'types', 'of', 'boundary', 'conditions', 'known', 'as', 'soliton', 'preserving', 'sp', 'and', 'soliton', 'nonpreserving', ... | [-0.16828987829990646, 0.09675073853042927, -0.06929756327513226, 0.12117116315271326, -0.10387866882065654, -0.1982591461095655, -0.09676853688885173, 0.3241866643407515, -0.25968275561320536, -0.1760929458375488, 0.1577693037272963, -0.23166101538024994, -0.16525507540850692, 0.17763477732541458, 0.003781249879726341... |
706.1516 | Creating pseudo Kondo-resonances by field-induced diffusion of atomic
hydrogen | In low temperature scanning tunneling microscopy (STM) experiments a cerium
adatom on Ag(100) possesses two discrete states with significantly different
apparent heights. These atomic switches also exhibit a Kondo-like feature in
spectroscopy experiments. By extensive theoretical simulations we find that
this behavio... | cond-mat.mtrl-sci | in low temperature scanning tunneling microscopy stm experiments a cerium adatom on ag100 possesses two discrete states with significantly different apparent heights these atomic switches also exhibit a kondolike feature in spectroscopy experiments by extensive theoretical simulations we find that this behavior is due ... | [['in', 'low', 'temperature', 'scanning', 'tunneling', 'microscopy', 'stm', 'experiments', 'a', 'cerium', 'adatom', 'on', 'ag100', 'possesses', 'two', 'discrete', 'states', 'with', 'significantly', 'different', 'apparent', 'heights', 'these', 'atomic', 'switches', 'also', 'exhibit', 'a', 'kondolike', 'feature', 'in', '... | [-0.11092772719181948, 0.1944697375519801, -0.06560410371728999, 0.04289587429858807, 0.02741258013875113, -0.1688265933465781, 0.10425907164818007, 0.40912680051652556, -0.2657148232999242, -0.33734714905968155, -0.026375859158934426, -0.33940310867787415, -0.1053766079278568, 0.15729454633290485, 0.019478432581586352... |
706.1517 | Supersolid phase induced by correlated hopping in spin-1/2 frustrated
quantum magnets | We show that correlated hopping of triplets, which is often the dominant
source of kinetic energy in dimer-based frustrated quantum magnets, produces a
remarkably strong tendency to form supersolid phases in a magnetic field. These
phases are characterized by simultaneous modulation and ordering of the
longitudinal a... | cond-mat.str-el | we show that correlated hopping of triplets which is often the dominant source of kinetic energy in dimerbased frustrated quantum magnets produces a remarkably strong tendency to form supersolid phases in a magnetic field these phases are characterized by simultaneous modulation and ordering of the longitudinal and tra... | [['we', 'show', 'that', 'correlated', 'hopping', 'of', 'triplets', 'which', 'is', 'often', 'the', 'dominant', 'source', 'of', 'kinetic', 'energy', 'in', 'dimerbased', 'frustrated', 'quantum', 'magnets', 'produces', 'a', 'remarkably', 'strong', 'tendency', 'to', 'form', 'supersolid', 'phases', 'in', 'a', 'magnetic', 'fi... | [-0.19821009424358474, 0.3091900719979271, -0.04484863469863426, 0.09892651971751017, -0.036519589446550975, -0.19043374096200003, 0.054210205256886905, 0.42438155297288854, -0.24613876775137883, -0.22405584952670388, 0.033129447840351975, -0.3031549154640695, -0.10847740033559039, 0.15475053935872177, 0.08295746620711... |
706.1518 | GRB051022: physical parameters and extinction of a prototype dark burst | GRB051022 was undetected to deep limits in early optical observations, but
precise astrometry from radio and X-ray showed that it most likely originated
in a galaxy at z~0.8. We report radio, optical, near infra-red and X-ray
observations of GRB051022. Using the available X-ray and radio data, we model
the afterglow ... | astro-ph | grb051022 was undetected to deep limits in early optical observations but precise astrometry from radio and xray showed that it most likely originated in a galaxy at z08 we report radio optical near infrared and xray observations of grb051022 using the available xray and radio data we model the afterglow and calculate ... | [['grb051022', 'was', 'undetected', 'to', 'deep', 'limits', 'in', 'early', 'optical', 'observations', 'but', 'precise', 'astrometry', 'from', 'radio', 'and', 'xray', 'showed', 'that', 'it', 'most', 'likely', 'originated', 'in', 'a', 'galaxy', 'at', 'z08', 'we', 'report', 'radio', 'optical', 'near', 'infrared', 'and', '... | [-0.03754605864396137, 0.08475523225827535, -0.07262842104736171, 0.08729032687516315, -0.11830307162514456, -0.08828484947174196, 0.08748904383945756, 0.4816937030721797, -0.18757751576599618, -0.33318503672347927, 0.09827448978449399, -0.32781315188460614, -0.06614903409442888, 0.20736328150832845, -0.023885886677684... |
706.1519 | A novel method for evaluating the critical nucleus and the surface
tension in systems with first order phase transition | We introduce a novel method for calculating the size of the critical nucleus
and the value of the surface tension in systems with first order phase
transition. The method is based on classical nucleation theory, and it consists
in studying the thermodynamics of a sphere of given radius embedded in a frozen
metastable... | cond-mat.stat-mech | we introduce a novel method for calculating the size of the critical nucleus and the value of the surface tension in systems with first order phase transition the method is based on classical nucleation theory and it consists in studying the thermodynamics of a sphere of given radius embedded in a frozen metastable sur... | [['we', 'introduce', 'a', 'novel', 'method', 'for', 'calculating', 'the', 'size', 'of', 'the', 'critical', 'nucleus', 'and', 'the', 'value', 'of', 'the', 'surface', 'tension', 'in', 'systems', 'with', 'first', 'order', 'phase', 'transition', 'the', 'method', 'is', 'based', 'on', 'classical', 'nucleation', 'theory', 'an... | [-0.1195057938946162, 0.15030435603281625, -0.08537726054705161, 0.02531389212036595, -0.014769743318684438, -0.11830965090881694, 0.07033684743844709, 0.32788021902847575, -0.23036696492410438, -0.28588560473592206, 0.12048553496058831, -0.2753169565775337, -0.10942733543426954, 0.1964723635427554, -0.0114084018691926... |
706.152 | On dynamical bit sequences | Let X^{(k)}(t) = (X_1(t), ..., X_k(t)) denote a k-vector of i.i.d. random
variables, each taking the values 1 or 0 with respective probabilities p and
1-p. As a process indexed by non-negative t, $X^{(k)}(t)$ is
constructed--following Benjamini, Haggstrom, Peres, and Steif (2003)--so that
it is strong Markov with inv... | math.PR | let xkt x_1t x_kt denote a kvector of iid random variables each taking the values 1 or 0 with respective probabilities p and 1p as a process indexed by nonnegative t xkt is constructedfollowing benjamini haggstrom peres and steif 2003so that it is strong markov with invariant measure 1pdelta_0pdelta_1k we derive sharp ... | [['let', 'xkt', 'x_1t', 'x_kt', 'denote', 'a', 'kvector', 'of', 'iid', 'random', 'variables', 'each', 'taking', 'the', 'values', '1', 'or', '0', 'with', 'respective', 'probabilities', 'p', 'and', '1p', 'as', 'a', 'process', 'indexed', 'by', 'nonnegative', 't', 'xkt', 'is', 'constructedfollowing', 'benjamini', 'haggstro... | [-0.12895609515500395, 0.15962717529724946, -0.017896063893920545, 0.032293860454473994, -0.03758378694130277, -0.2218261492671445, 0.09668824080180263, 0.3541184745616082, -0.2570546690752081, -0.22770335963419217, 0.07093715127760361, -0.29094756456712884, -0.11726393405203425, 0.1487010909874119, -0.1011792391584480... |
706.1521 | $\nu$ masses in a SUSY SO(10) theory with spontaneous CP violation | We propose a possibility of spontaneous CP-violation (SCPV) at high scale in
a SUSY SO(10) theory. The model is L-R symmetric SUSY SO(10) with
\textbf{\noun{10}} and \textbf{126} dimensional Higgs generating fermion
masses, and the CP phase is generated through complex VEV of B-L breaking
\textbf{126} Higgs . The mod... | hep-ph | we propose a possibility of spontaneous cpviolation scpv at high scale in a susy so10 theory the model is lr symmetric susy so10 with textbfnoun10 and textbf126 dimensional higgs generating fermion masses and the cp phase is generated through complex vev of bl breaking textbf126 higgs the model can have potential appli... | [['we', 'propose', 'a', 'possibility', 'of', 'spontaneous', 'cpviolation', 'scpv', 'at', 'high', 'scale', 'in', 'a', 'susy', 'so10', 'theory', 'the', 'model', 'is', 'lr', 'symmetric', 'susy', 'so10', 'with', 'textbfnoun10', 'and', 'textbf126', 'dimensional', 'higgs', 'generating', 'fermion', 'masses', 'and', 'the', 'cp... | [-0.10903861642622485, 0.31095646371551117, 0.01822876438883872, 0.176186653291646, -0.12836264388571525, -0.23029086201307203, 0.02974721879882995, 0.3589006565703914, -0.17370848163384303, -0.2998200713331683, 0.07475235029364583, -0.19349143545721367, -0.08352264580477414, 0.051672875680479, 0.022208609120470697, 0.... |
706.1522 | Viscosity Information from Relativistic Nuclear Collisions: How Perfect
is the Fluid Observed at RHIC? | Relativistic viscous hydrodynamic fits to RHIC data on the centrality
dependence of multiplicity, transverse and elliptic flow for sqrt{s}=200 GeV
Au+Au collisions are presented. For Glauber-type initial conditions, while data
on integrated v_2 is consistent with a ratio of viscosity over entropy density
up to eta/s=... | nucl-th hep-ph hep-th | relativistic viscous hydrodynamic fits to rhic data on the centrality dependence of multiplicity transverse and elliptic flow for sqrts200 gev auau collisions are presented for glaubertype initial conditions while data on integrated v_2 is consistent with a ratio of viscosity over entropy density up to etas016 data on ... | [['relativistic', 'viscous', 'hydrodynamic', 'fits', 'to', 'rhic', 'data', 'on', 'the', 'centrality', 'dependence', 'of', 'multiplicity', 'transverse', 'and', 'elliptic', 'flow', 'for', 'sqrts200', 'gev', 'auau', 'collisions', 'are', 'presented', 'for', 'glaubertype', 'initial', 'conditions', 'while', 'data', 'on', 'in... | [-0.12076738388655153, 0.17816146687176582, -0.1946380330954452, 0.12036069735532275, -0.02833972358761506, -0.11598689341917634, -0.09118254409750572, 0.3277794757222354, -0.21064162826971025, -0.3044557790397792, 0.003343150409794337, -0.38313052424141586, 0.14375940401648246, 0.22992757375578624, -0.0167528136910216... |
706.1523 | Thom polynomials for maps of curves with isolated singularities | Thom (residual) polynomials in characteristic classes are used in the
analysis of geometry of functional spaces. They serve as a tool in description
of classes Poincar\'e dual to subvarieties of functions of prescribed types. We
give explicit universal expressions for residual polynomials in spaces of
functions on co... | math.AG | thom residual polynomials in characteristic classes are used in the analysis of geometry of functional spaces they serve as a tool in description of classes poincare dual to subvarieties of functions of prescribed types we give explicit universal expressions for residual polynomials in spaces of functions on complex cu... | [['thom', 'residual', 'polynomials', 'in', 'characteristic', 'classes', 'are', 'used', 'in', 'the', 'analysis', 'of', 'geometry', 'of', 'functional', 'spaces', 'they', 'serve', 'as', 'a', 'tool', 'in', 'description', 'of', 'classes', 'poincare', 'dual', 'to', 'subvarieties', 'of', 'functions', 'of', 'prescribed', 'type... | [-0.16873096606719332, 0.0266402729258344, -0.12262407420328944, 0.1665207647114388, -0.05150236697817171, -0.10447848637940714, -0.016204101442535583, 0.320571087602828, -0.27538019445145856, -0.23743962646285827, 0.062195291105544545, -0.20680507951466418, -0.19121455884935032, 0.2691065072132325, -0.1154018031760446... |
706.1524 | Helix, shadow boundary and minimal submanifolds | Inspired by a Blaschke's work about analytic convex surfaces, we study {\em
shadow boundaries} of Riemannian submanifolds $M$, which are defined by a
parallel vector field along $M$. Since a shadow boundary is just a closed
subset of $M$, first, we will give a condition that guarantee its smoothness.
It depends on th... | math.DG | inspired by a blaschkes work about analytic convex surfaces we study em shadow boundaries of riemannian submanifolds m which are defined by a parallel vector field along m since a shadow boundary is just a closed subset of m first we will give a condition that guarantee its smoothness it depends on the second fundament... | [['inspired', 'by', 'a', 'blaschkes', 'work', 'about', 'analytic', 'convex', 'surfaces', 'we', 'study', 'em', 'shadow', 'boundaries', 'of', 'riemannian', 'submanifolds', 'm', 'which', 'are', 'defined', 'by', 'a', 'parallel', 'vector', 'field', 'along', 'm', 'since', 'a', 'shadow', 'boundary', 'is', 'just', 'a', 'closed... | [-0.20091701789648944, 0.11605985337487792, -0.07176740637790131, 0.07372331340491811, -0.16618184448890788, -0.12809993414789117, 0.012175733293657022, 0.3637510374819319, -0.2600515031866649, -0.28661391950182374, 0.14786908037895438, -0.2476452670550795, -0.18723202130997613, 0.18687882901279515, -0.1572991880407977... |
706.1525 | Perturbative study of the transfer matrix on the string worldsheet in
AdS(5)xS(5) | Quantum non-local charges are central to the quantum integrability of a
sigma-model. In this paper we study the quantum consistency and UV finiteness
of non-local charges of string theory in AdS(5)xS(5). We use the pure spinor
formalism. We develop the near-flat space expansion of the transfer matrix and
calculate th... | hep-th | quantum nonlocal charges are central to the quantum integrability of a sigmamodel in this paper we study the quantum consistency and uv finiteness of nonlocal charges of string theory in ads5xs5 we use the pure spinor formalism we develop the nearflat space expansion of the transfer matrix and calculate the oneloop div... | [['quantum', 'nonlocal', 'charges', 'are', 'central', 'to', 'the', 'quantum', 'integrability', 'of', 'a', 'sigmamodel', 'in', 'this', 'paper', 'we', 'study', 'the', 'quantum', 'consistency', 'and', 'uv', 'finiteness', 'of', 'nonlocal', 'charges', 'of', 'string', 'theory', 'in', 'ads5xs5', 'we', 'use', 'the', 'pure', 's... | [-0.1491249315464413, 0.12875918902893912, -0.12156560563254265, 0.14437716335238776, -0.04786123831670883, -0.11417774141443018, 0.035051443015655256, 0.30857159128906775, -0.1892470296434298, -0.19846573705210027, 0.03901854321142012, -0.29965201832772215, -0.1629018337864961, 0.08080639864070988, -0.0480276769293206... |
706.1526 | On Colorings of Squares of Outerplanar Graphs | We study vertex colorings of the square $G^2$ of an outerplanar graph $G$. We
find the optimal bound of the inductiveness, chromatic number and the clique
number of $G^2$ as a function of the maximum degree $\Delta$ of $G$ for all
$\Delta\in \nats$. As a bonus, we obtain the optimal bound of the choosability
(or the ... | math.CO | we study vertex colorings of the square g2 of an outerplanar graph g we find the optimal bound of the inductiveness chromatic number and the clique number of g2 as a function of the maximum degree delta of g for all deltain nats as a bonus we obtain the optimal bound of the choosability or the listchromatic number of g... | [['we', 'study', 'vertex', 'colorings', 'of', 'the', 'square', 'g2', 'of', 'an', 'outerplanar', 'graph', 'g', 'we', 'find', 'the', 'optimal', 'bound', 'of', 'the', 'inductiveness', 'chromatic', 'number', 'and', 'the', 'clique', 'number', 'of', 'g2', 'as', 'a', 'function', 'of', 'the', 'maximum', 'degree', 'delta', 'of'... | [-0.2093518481976012, 0.13591638119148072, 0.015691402504538616, 0.05353505061598631, -0.09296934926178216, -0.12465629309824691, 0.09048017100771753, 0.33535346257920584, -0.2501888790781178, -0.41534650641516213, 0.08539819427078771, -0.3266870129126601, -0.13176797079660635, 0.13578136079865166, -0.08407012152871708... |
706.1527 | Surface waves in defocusing thermal nonlinear optical media | We predict that the interface of materials with defocusing thermal
nonlinearities support stable fundamental and higher-order surface waves when
the opposite edges of the medium are maintained at different temperatures. Such
surface waves exist due to the interplay between repulsion from the interface
and the defocus... | physics.optics nlin.PS | we predict that the interface of materials with defocusing thermal nonlinearities support stable fundamental and higherorder surface waves when the opposite edges of the medium are maintained at different temperatures such surface waves exist due to the interplay between repulsion from the interface and the defocusing ... | [['we', 'predict', 'that', 'the', 'interface', 'of', 'materials', 'with', 'defocusing', 'thermal', 'nonlinearities', 'support', 'stable', 'fundamental', 'and', 'higherorder', 'surface', 'waves', 'when', 'the', 'opposite', 'edges', 'of', 'the', 'medium', 'are', 'maintained', 'at', 'different', 'temperatures', 'such', 's... | [-0.15402656863825243, 0.21828286339086098, -0.07019010201462957, 0.04094132039024204, -0.07442030041921334, -0.14226150701249965, 0.003017224203489843, 0.3795762170777946, -0.32089081623393007, -0.2651077558393361, 0.059948165259766775, -0.35732473139880133, -0.12350947888125284, 0.13737780666436816, 0.069518874363103... |
706.1528 | $H_D$-Quantum Vertex Algebras and Bicharacters | We define a new class of quantum vertex algebras, based on the Hopf algebra
$H_D=\mathbb{C}[D]$ of "infinitesimal translations" generated by $D$. Besides
the braiding map describing the obstruction to commutativity of products of
vertex operators, $H_D$-quantum vertex algebras have as main new ingredient a
"translati... | math.QA math-ph math.MP | we define a new class of quantum vertex algebras based on the hopf algebra h_dmathbbcd of infinitesimal translations generated by d besides the braiding map describing the obstruction to commutativity of products of vertex operators h_dquantum vertex algebras have as main new ingredient a translation map that describes... | [['we', 'define', 'a', 'new', 'class', 'of', 'quantum', 'vertex', 'algebras', 'based', 'on', 'the', 'hopf', 'algebra', 'h_dmathbbcd', 'of', 'infinitesimal', 'translations', 'generated', 'by', 'd', 'besides', 'the', 'braiding', 'map', 'describing', 'the', 'obstruction', 'to', 'commutativity', 'of', 'products', 'of', 've... | [-0.15480579805417774, 0.09950976071382142, -0.05680002327085481, 0.0818562508374033, -0.14622990995737817, -0.17468774192840666, -0.014797057582040292, 0.28247690215908194, -0.3406174593345002, -0.2040509649275525, 0.07676488867025352, -0.26841054068089604, -0.19672917853621347, 0.1352940338437219, -0.1444305548998149... |
706.1529 | On multipartite posets | A poset $\mathbf{P} = (X,\preceq)$ is {\em $m$-partite} if $X$ has a
partition $X = X_1 \cup ... \cup X_m$ such that (1) each $X_i$ forms an
antichain in $\mathbf{P}$, and (2) $x\prec y$ implies $x\in X_i$ and $y\in X_j$
where $i<j$. In this article we derive a tight asymptotic upper bound on the
order dimension of $... | math.CO | a poset mathbfp xpreceq is em mpartite if x has a partition x x_1 cup cup x_m such that 1 each x_i forms an antichain in mathbfp and 2 xprec y implies xin x_i and yin x_j where ij in this article we derive a tight asymptotic upper bound on the order dimension of mpartite posets in terms of m and their bipartite subpose... | [['a', 'poset', 'mathbfp', 'xpreceq', 'is', 'em', 'mpartite', 'if', 'x', 'has', 'a', 'partition', 'x', 'x_1', 'cup', 'cup', 'x_m', 'such', 'that', '1', 'each', 'x_i', 'forms', 'an', 'antichain', 'in', 'mathbfp', 'and', '2', 'xprec', 'y', 'implies', 'xin', 'x_i', 'and', 'yin', 'x_j', 'where', 'ij', 'in', 'this', 'articl... | [-0.2330911765279977, 0.12631299423473125, -0.03241677666960311, 0.009996226084405098, -0.028806895982690046, -0.15859616469537866, 0.0699983471363405, 0.3535814541864438, -0.3203182561100339, -0.15366033801346665, 0.018447106613640917, -0.3621245362944361, -0.11421776592032984, 0.04798803433937871, -0.1391899232428683... |
706.153 | Randomly coloring planar graphs with fewer colors than the maximum
degree | We study Markov chains for randomly sampling $k$-colorings of a graph with
maximum degree $\Delta$. Our main result is a polynomial upper bound on the
mixing time of the single-site update chain known as the Glauber dynamics for
planar graphs when $k=\Omega(\Delta/\log{\Delta})$. Our results can be
partially extended... | math.PR math.CO | we study markov chains for randomly sampling kcolorings of a graph with maximum degree delta our main result is a polynomial upper bound on the mixing time of the singlesite update chain known as the glauber dynamics for planar graphs when komegadeltalogdelta our results can be partially extended to the more general ca... | [['we', 'study', 'markov', 'chains', 'for', 'randomly', 'sampling', 'kcolorings', 'of', 'a', 'graph', 'with', 'maximum', 'degree', 'delta', 'our', 'main', 'result', 'is', 'a', 'polynomial', 'upper', 'bound', 'on', 'the', 'mixing', 'time', 'of', 'the', 'singlesite', 'update', 'chain', 'known', 'as', 'the', 'glauber', 'd... | [-0.10621638118624757, 0.17488156547839406, -0.04441629502567838, 0.027133670295831927, -0.06399527893561537, -0.1447241305992174, 0.08101044092744367, 0.36849400591550036, -0.26909707502006736, -0.3015084228123914, 0.1188233512194841, -0.30498851730780147, -0.10039575723236177, 0.12458584003094862, -0.0386205421301967... |
706.1531 | Critical scaling and heterogeneous superdiffusion across the
jamming/rigidity transition of a granular glass | The dynamical properties of a dense horizontally vibrated bidisperse granular
monolayer are experimentally investigated. The quench protocol produces states
with a frozen structure of the assembly, but the remaining degrees of freedom
associated with contact dynamics control the appearance of macroscopic
rigidity. We... | cond-mat.soft | the dynamical properties of a dense horizontally vibrated bidisperse granular monolayer are experimentally investigated the quench protocol produces states with a frozen structure of the assembly but the remaining degrees of freedom associated with contact dynamics control the appearance of macroscopic rigidity we prov... | [['the', 'dynamical', 'properties', 'of', 'a', 'dense', 'horizontally', 'vibrated', 'bidisperse', 'granular', 'monolayer', 'are', 'experimentally', 'investigated', 'the', 'quench', 'protocol', 'produces', 'states', 'with', 'a', 'frozen', 'structure', 'of', 'the', 'assembly', 'but', 'the', 'remaining', 'degrees', 'of', ... | [-0.22750998869148606, 0.30687726534084014, -0.09252659712837616, 0.045656242213007195, 0.018958298502661657, -0.14475165237424933, 0.0119351066272468, 0.3441094931030104, -0.2678299153104742, -0.2686042224605244, 0.024158782955648786, -0.32995639816058653, -0.15073056457438738, 0.10047014628814414, 0.08191759976829198... |
706.1532 | Vector meson production in ultra-peripheral collisions at LHC | Vector meson production in ultra-peripheral collisions of heavy ions at LHC
is calculated in VDM and color dipole approaches.
| hep-ph | vector meson production in ultraperipheral collisions of heavy ions at lhc is calculated in vdm and color dipole approaches | [['vector', 'meson', 'production', 'in', 'ultraperipheral', 'collisions', 'of', 'heavy', 'ions', 'at', 'lhc', 'is', 'calculated', 'in', 'vdm', 'and', 'color', 'dipole', 'approaches']] | [0.0035770409127795382, 0.39613612486343636, -0.10452314169685308, 0.18491792338777727, 0.06405502322473024, -0.16189279309228846, -0.08601369953861362, 0.3930252694377774, -0.137415590254884, -0.14044995351057304, -0.2418047093271621, -0.44491660653760556, 0.23732472446404004, 0.010605418956593463, 0.16048692509924112... |
706.1533 | Renormalisation and the Batalin-Vilkovisky formalism | This paper gives a way to renormalise certain quantum field theories on
compact manifolds. Examples include Yang-Mills theory (in dimension 4 only),
Chern-Simons theory and holomorphic Chern-Simons theory. The method is within
the framework of the Batalin-Vilkovisky formalism. Chern-Simons theory is
renormalised in a... | math.QA hep-th | this paper gives a way to renormalise certain quantum field theories on compact manifolds examples include yangmills theory in dimension 4 only chernsimons theory and holomorphic chernsimons theory the method is within the framework of the batalinvilkovisky formalism chernsimons theory is renormalised in a way respecti... | [['this', 'paper', 'gives', 'a', 'way', 'to', 'renormalise', 'certain', 'quantum', 'field', 'theories', 'on', 'compact', 'manifolds', 'examples', 'include', 'yangmills', 'theory', 'in', 'dimension', '4', 'only', 'chernsimons', 'theory', 'and', 'holomorphic', 'chernsimons', 'theory', 'the', 'method', 'is', 'within', 'th... | [-0.2021607163672646, 0.10094416391681686, -0.12383856526797726, 0.08873116712424062, -0.12558823991345153, -0.1259819831133687, -0.047574926917496624, 0.3031708571971172, -0.2542623045654701, -0.2526008961722255, 0.032310076676020844, -0.20664718407871469, -0.23369930624695762, 0.12730855414632797, -0.1293378704188702... |
706.1534 | Coupling gauge theory to spinfoam 3d quantum gravity | We construct a spinfoam model for Yang-Mills theory coupled to quantum
gravity in three dimensional riemannian spacetime. We define the partition
function of the coupled system as a power series in g_0^2 G that can be
evaluated order by order using grasping rules and the recoupling theory. With
respect to previous at... | gr-qc hep-th | we construct a spinfoam model for yangmills theory coupled to quantum gravity in three dimensional riemannian spacetime we define the partition function of the coupled system as a power series in g_02 g that can be evaluated order by order using grasping rules and the recoupling theory with respect to previous attempts... | [['we', 'construct', 'a', 'spinfoam', 'model', 'for', 'yangmills', 'theory', 'coupled', 'to', 'quantum', 'gravity', 'in', 'three', 'dimensional', 'riemannian', 'spacetime', 'we', 'define', 'the', 'partition', 'function', 'of', 'the', 'coupled', 'system', 'as', 'a', 'power', 'series', 'in', 'g_02', 'g', 'that', 'can', '... | [-0.10926987654405886, 0.15420992172578663, -0.14140577550021421, 0.06305971664100457, -0.04279178633165043, -0.11468630054227975, 0.007820363192555321, 0.30545640423630194, -0.20423680089982804, -0.25797676392140656, 0.031070379661890652, -0.2777650337501437, -0.21378152987268645, 0.08332946429243393, -0.0676776524262... |
706.1535 | The initial conditions of star formation in the Ophiuchus main cloud:
Kinematics of the protocluster condensations | The earliest phases of clustered star formation and the origin of the stellar
initial mass function (IMF) are currently much debated. In order to constrain
the origin of the IMF, we investigated the internal and relative motions of
starless condensations and protostars previously detected by us in the dust
continuum ... | astro-ph | the earliest phases of clustered star formation and the origin of the stellar initial mass function imf are currently much debated in order to constrain the origin of the imf we investigated the internal and relative motions of starless condensations and protostars previously detected by us in the dust continuum at 12m... | [['the', 'earliest', 'phases', 'of', 'clustered', 'star', 'formation', 'and', 'the', 'origin', 'of', 'the', 'stellar', 'initial', 'mass', 'function', 'imf', 'are', 'currently', 'much', 'debated', 'in', 'order', 'to', 'constrain', 'the', 'origin', 'of', 'the', 'imf', 'we', 'investigated', 'the', 'internal', 'and', 'rela... | [-0.10256759392175505, 0.15576108509421227, -0.0853576990322786, 0.09397940382230954, -0.04487612796766169, -0.0131548842406607, 0.012539008326542199, 0.41796832312630483, -0.12896284802294977, -0.30940509111355946, 0.03093412655164716, -0.17776263776282392, 0.004407415470898383, 0.08963443368541055, 0.0388656961804089... |
706.1536 | Canonical forms, higher rank numerical range, convexity, totally
isotropic subspace, matrix equations | Results on matrix canonical forms are used to give a complete description of
the higher rank numerical range of matrices arising from the study of quantum
error correction. It is shown that the set can be obtained as the intersection
of closed half planes (of complex numbers). As a result, it is always a convex
set i... | math.FA quant-ph | results on matrix canonical forms are used to give a complete description of the higher rank numerical range of matrices arising from the study of quantum error correction it is shown that the set can be obtained as the intersection of closed half planes of complex numbers as a result it is always a convex set in mathc... | [['results', 'on', 'matrix', 'canonical', 'forms', 'are', 'used', 'to', 'give', 'a', 'complete', 'description', 'of', 'the', 'higher', 'rank', 'numerical', 'range', 'of', 'matrices', 'arising', 'from', 'the', 'study', 'of', 'quantum', 'error', 'correction', 'it', 'is', 'shown', 'that', 'the', 'set', 'can', 'be', 'obtai... | [-0.1256994007891044, 0.07350174779444933, -0.047018012065440415, 0.05818691531475633, -0.03430956353619695, -0.10661619920283556, 0.03029751849360764, 0.2917646582201123, -0.26032557607255874, -0.2538532893694937, 0.14292597129754722, -0.2570188702046871, -0.1827439924441278, 0.24093304786644876, -0.057282989099621776... |
706.1537 | Semi-Empirical Cepheid Period-Luminosity Relations in Sloan Magnitudes | In this paper we derive semi-empirical Cepheid period-luminosity (P-L)
relations in the Sloan ugriz magnitudes by combining the observed BVI mean
magnitudes from the Large Magellanic Cloud Cepheids (LMC) and theoretical
bolometric corrections. We also constructed empirical gr band P-L relations,
using the publicly av... | astro-ph | in this paper we derive semiempirical cepheid periodluminosity pl relations in the sloan ugriz magnitudes by combining the observed bvi mean magnitudes from the large magellanic cloud cepheids lmc and theoretical bolometric corrections we also constructed empirical gr band pl relations using the publicly available john... | [['in', 'this', 'paper', 'we', 'derive', 'semiempirical', 'cepheid', 'periodluminosity', 'pl', 'relations', 'in', 'the', 'sloan', 'ugriz', 'magnitudes', 'by', 'combining', 'the', 'observed', 'bvi', 'mean', 'magnitudes', 'from', 'the', 'large', 'magellanic', 'cloud', 'cepheids', 'lmc', 'and', 'theoretical', 'bolometric'... | [0.03211797336398652, 0.04187976226041263, -0.14288099841073607, 0.14856807612919842, -0.13739490563360354, -0.1056997305713594, 0.14668974262189516, 0.49262288935256726, -0.2586161719289411, -0.3526369607936817, -0.04826812730144328, -0.37845079352458316, -0.08184871853639682, 0.2980173417035434, -0.10602214833665075,... |
706.1538 | Superluminal motion and closed signal curves | We discuss some properties of Lorentz invariant theories which allow for
superluminal motion. We show that, if signals are always sent forward in time,
closed curves along which signals propagate can be formed. This leads to
problems with causality and with the second law of thermodynamics. Only if one
singles out on... | astro-ph gr-qc hep-th | we discuss some properties of lorentz invariant theories which allow for superluminal motion we show that if signals are always sent forward in time closed curves along which signals propagate can be formed this leads to problems with causality and with the second law of thermodynamics only if one singles out one frame... | [['we', 'discuss', 'some', 'properties', 'of', 'lorentz', 'invariant', 'theories', 'which', 'allow', 'for', 'superluminal', 'motion', 'we', 'show', 'that', 'if', 'signals', 'are', 'always', 'sent', 'forward', 'in', 'time', 'closed', 'curves', 'along', 'which', 'signals', 'propagate', 'can', 'be', 'formed', 'this', 'lea... | [-0.1513426150765498, 0.15278949830871152, -0.1164115183643417, 0.03313404023267177, -0.12522925462630785, -0.1665939439601284, 0.026380604664971507, 0.4133873731087969, -0.3058554288094901, -0.23355172508294048, 0.11326902146969105, -0.284201975237122, -0.06848754936458581, 0.21071587265611683, -0.055296946059069325, ... |
706.1539 | Vertex coloring acyclic digraphs and their corresponding hypergraphs | We consider vertex coloring of an acyclic digraph $\Gdag$ in such a way that
two vertices which have a common ancestor in $\Gdag$ receive distinct colors.
Such colorings arise in a natural way when bounding space for various genetic
data for efficient analysis. We discuss the corresponding {\em down-chromatic
number}... | math.CO | we consider vertex coloring of an acyclic digraph gdag in such a way that two vertices which have a common ancestor in gdag receive distinct colors such colorings arise in a natural way when bounding space for various genetic data for efficient analysis we discuss the corresponding em downchromatic number and derive an... | [['we', 'consider', 'vertex', 'coloring', 'of', 'an', 'acyclic', 'digraph', 'gdag', 'in', 'such', 'a', 'way', 'that', 'two', 'vertices', 'which', 'have', 'a', 'common', 'ancestor', 'in', 'gdag', 'receive', 'distinct', 'colors', 'such', 'colorings', 'arise', 'in', 'a', 'natural', 'way', 'when', 'bounding', 'space', 'for... | [-0.16861760355532168, 0.12154666253681123, -0.032537956202500745, 0.06465907419884676, -0.08888766536195027, -0.10495022670120785, 0.09859425521602756, 0.32504467673011517, -0.2498952111155775, -0.37273331519804503, 0.06599884362964842, -0.2985460985059801, -0.16686032828139633, 0.12186516695655883, -0.086506056268454... |
706.154 | Condition for the higher rank numerical range to be non-empty | It is shown that the rank-$k$ numerical range of every $n$-by-$n$ complex
matrix is non-empty if $n \ge 3k - 2$. The proof is based on a recent
characterization of the rank-$k$ numerical range by Li and Sze, the Helly's
theorem on compact convex sets, and some eigenvalue inequalities. In
particular, the result implie... | math.FA quant-ph | it is shown that the rankk numerical range of every nbyn complex matrix is nonempty if n ge 3k 2 the proof is based on a recent characterization of the rankk numerical range by li and sze the hellys theorem on compact convex sets and some eigenvalue inequalities in particular the result implies that lambda_2a is nonemp... | [['it', 'is', 'shown', 'that', 'the', 'rankk', 'numerical', 'range', 'of', 'every', 'nbyn', 'complex', 'matrix', 'is', 'nonempty', 'if', 'n', 'ge', '3k', '2', 'the', 'proof', 'is', 'based', 'on', 'a', 'recent', 'characterization', 'of', 'the', 'rankk', 'numerical', 'range', 'by', 'li', 'and', 'sze', 'the', 'hellys', 't... | [-0.12399615719799173, 0.12135886890833303, -0.013947776451045278, -0.00526182604538701, -0.05134106953259521, -0.11520711848936459, 0.003924523065290828, 0.3338398419246815, -0.25616492221528425, -0.21430225531561392, 0.11578579068455919, -0.29572693985831544, -0.18407094699450502, 0.21841196568987084, -0.094652249881... |
706.1541 | Noise induced forced synchronization of global variables in coupled
bistable systems | We analyze the noise induced synchronization between a collective variable
characterizing a complex system with a finite number of interacting bistable
units and time periodic driving forces. A random phase process associated to
the collective stochastic variable is defined. Its average phase frequency and
average ph... | cond-mat.stat-mech | we analyze the noise induced synchronization between a collective variable characterizing a complex system with a finite number of interacting bistable units and time periodic driving forces a random phase process associated to the collective stochastic variable is defined its average phase frequency and average phase ... | [['we', 'analyze', 'the', 'noise', 'induced', 'synchronization', 'between', 'a', 'collective', 'variable', 'characterizing', 'a', 'complex', 'system', 'with', 'a', 'finite', 'number', 'of', 'interacting', 'bistable', 'units', 'and', 'time', 'periodic', 'driving', 'forces', 'a', 'random', 'phase', 'process', 'associated... | [-0.2306337187469784, 0.18003334500305632, -0.09622625073890632, 0.021416901559669937, -0.059997647632358236, -0.11285963243763171, 0.0908316621841835, 0.35356144662668454, -0.30130985710047076, -0.24393119023584608, 0.09553051655139051, -0.26583680732926324, -0.19915525633980757, 0.18253673664502687, -0.01595479327796... |
706.1542 | Pulsar Physics and GLAST | Rotation-powered pulsars are excellent laboratories for study of particle
acceleration as well as fundamental physics of strong gravity, strong magnetic
fields, high densities and relativity. I will review the outstanding questions
in pulsar physics and the prospects for finding answers with GLAST LAT
observations. L... | astro-ph | rotationpowered pulsars are excellent laboratories for study of particle acceleration as well as fundamental physics of strong gravity strong magnetic fields high densities and relativity i will review the outstanding questions in pulsar physics and the prospects for finding answers with glast lat observations lat obse... | [['rotationpowered', 'pulsars', 'are', 'excellent', 'laboratories', 'for', 'study', 'of', 'particle', 'acceleration', 'as', 'well', 'as', 'fundamental', 'physics', 'of', 'strong', 'gravity', 'strong', 'magnetic', 'fields', 'high', 'densities', 'and', 'relativity', 'i', 'will', 'review', 'the', 'outstanding', 'questions... | [-0.05489144583716695, 0.19067317717085322, -0.08263809137654997, 0.19931125438471478, -0.17347228594168318, -0.14368443770378125, 0.018026127522136635, 0.4083491742104937, -0.14809156480927285, -0.4294355924380577, 0.02202721363883172, -0.30476299809350627, 0.01736183620908657, 0.3277455725868445, -0.00973451488805333... |
706.1543 | Structure of Vector Mesons in Holographic Model with Linear Confinement | Wave functions and form factors of vector mesons are investigated in the
holographic dual model of QCD with a smooth oscillator-like wall. We introduce
wave functions conjugate to solutions of the 5D equation of motion and develop
a formalism based on these wave functions, which are very similar to those of a
quantum... | hep-ph hep-th | wave functions and form factors of vector mesons are investigated in the holographic dual model of qcd with a smooth oscillatorlike wall we introduce wave functions conjugate to solutions of the 5d equation of motion and develop a formalism based on these wave functions which are very similar to those of a quantummecha... | [['wave', 'functions', 'and', 'form', 'factors', 'of', 'vector', 'mesons', 'are', 'investigated', 'in', 'the', 'holographic', 'dual', 'model', 'of', 'qcd', 'with', 'a', 'smooth', 'oscillatorlike', 'wall', 'we', 'introduce', 'wave', 'functions', 'conjugate', 'to', 'solutions', 'of', 'the', '5d', 'equation', 'of', 'motio... | [-0.11894738044016392, 0.19082264621190878, -0.08011380159201062, 0.08102803205561247, -0.05882522955385978, -0.12064884637868932, 0.003930940467002643, 0.353561563987513, -0.18981762123325852, -0.23536669700184748, -0.0014886331719149942, -0.3051056235230395, -0.10903791574045357, 0.12369336955863856, 0.05809646016889... |
706.1544 | Novel technique for monitoring the performance of the LAT instrument on
board the GLAST satellite | The Gamma-ray Large Area Space Telescope (GLAST) is an observatory designed
to perform gamma-ray astronomy in the energy range 20 MeV to 300 GeV, with
supporting measurements for gamma-ray bursts from 10 keV to 25 MeV. GLAST will
be launched at the end of 2007, opening a new and important window on a wide
variety of ... | astro-ph | the gammaray large area space telescope glast is an observatory designed to perform gammaray astronomy in the energy range 20 mev to 300 gev with supporting measurements for gammaray bursts from 10 kev to 25 mev glast will be launched at the end of 2007 opening a new and important window on a wide variety of high energ... | [['the', 'gammaray', 'large', 'area', 'space', 'telescope', 'glast', 'is', 'an', 'observatory', 'designed', 'to', 'perform', 'gammaray', 'astronomy', 'in', 'the', 'energy', 'range', '20', 'mev', 'to', '300', 'gev', 'with', 'supporting', 'measurements', 'for', 'gammaray', 'bursts', 'from', '10', 'kev', 'to', '25', 'mev'... | [-0.05903445025678815, 0.16371262759692887, -0.06300071958543324, 0.11898282557021736, -0.12066429508991948, -0.12123729146153825, 0.049869359293725435, 0.3898732374944701, -0.201573182533427, -0.42157930365604596, 0.08533151257533307, -0.335872231687351, -0.04961629561602888, 0.3154067326743133, -0.04056171294665191, ... |
706.1545 | Base-controlled mechanical systems and geometric phases | In this paper, we carry a detailed study of mechanical systems with
configuration space $Q\longrightarrow Q/G$ for which the base $Q/G$ variables
are being controlled. The overall system's motion is considered to be induced
from the base one due to the presence of general non-holonomic constraints. It
is shown that t... | math-ph math.DG math.MP | in this paper we carry a detailed study of mechanical systems with configuration space qlongrightarrow qg for which the base qg variables are being controlled the overall systems motion is considered to be induced from the base one due to the presence of general nonholonomic constraints it is shown that the solution ca... | [['in', 'this', 'paper', 'we', 'carry', 'a', 'detailed', 'study', 'of', 'mechanical', 'systems', 'with', 'configuration', 'space', 'qlongrightarrow', 'qg', 'for', 'which', 'the', 'base', 'qg', 'variables', 'are', 'being', 'controlled', 'the', 'overall', 'systems', 'motion', 'is', 'considered', 'to', 'be', 'induced', 'f... | [-0.14599648517905733, 0.09246912798043923, -0.15018971763551237, 0.04384968662634492, -0.07653299841564148, -0.10445075344061479, -0.01130942382500507, 0.3317964157089591, -0.29684607984963807, -0.27251914084423334, 0.11542415772913955, -0.20756218019872905, -0.17640424645505845, 0.19093078332021832, -0.06677324844757... |
706.1546 | On the dynamics of codimension one holomorphic foliations with ample
normal bundle | We investigate the accumulation to singular points of leaves of codimension
one foliations whose normal bundle is ample, with emphasis on the nonexistence
of Levi-flat hypersurfaces.
| math.CV | we investigate the accumulation to singular points of leaves of codimension one foliations whose normal bundle is ample with emphasis on the nonexistence of leviflat hypersurfaces | [['we', 'investigate', 'the', 'accumulation', 'to', 'singular', 'points', 'of', 'leaves', 'of', 'codimension', 'one', 'foliations', 'whose', 'normal', 'bundle', 'is', 'ample', 'with', 'emphasis', 'on', 'the', 'nonexistence', 'of', 'leviflat', 'hypersurfaces']] | [-0.3367127381766645, -0.017302647662850525, -0.05411887032767901, 0.05316744532095841, -0.1085342548501033, -0.1903858817755603, -0.056239966567283355, 0.30233120244856065, -0.20574201392726257, -0.08836708848293011, 0.15812601673846635, -0.3560788593469904, -0.10854673937249643, 0.15786378887983468, -0.19123458883796... |
706.1547 | Two-loop Corrections for Nuclear Matter in a Covariant Effective Field
Theory | Although one-loop calculations provide a realistic description of bulk and
single-particle nuclear properties, it is necessary to examine loop corrections
to develop a systematic finite-density power-counting scheme for the nuclear
many-body problem when loops are included. Moreover, it is imperative to study
exchang... | nucl-th | although oneloop calculations provide a realistic description of bulk and singleparticle nuclear properties it is necessary to examine loop corrections to develop a systematic finitedensity powercounting scheme for the nuclear manybody problem when loops are included moreover it is imperative to study exchange and corr... | [['although', 'oneloop', 'calculations', 'provide', 'a', 'realistic', 'description', 'of', 'bulk', 'and', 'singleparticle', 'nuclear', 'properties', 'it', 'is', 'necessary', 'to', 'examine', 'loop', 'corrections', 'to', 'develop', 'a', 'systematic', 'finitedensity', 'powercounting', 'scheme', 'for', 'the', 'nuclear', '... | [-0.07769544754583056, 0.16532373673335585, -0.10735120577276638, 0.1596713957012548, -0.06042239660775234, -0.11379982997423572, 0.012487456894083189, 0.3766324626262263, -0.24156853985640747, -0.2897051287778091, 0.06300887534634607, -0.2968297312105314, -0.09517515844338122, 0.13998250207301266, 0.04647046700119972,... |
706.1548 | Retaining Black Holes with Very Large Recoil Velocities | Recent numerical simulations of binary black hole mergers show the
possibility of producing very large recoil velocities (> 3000 km/s). Kicks of
this magnitude should be sufficient to eject the final black hole from
virtually any galactic potential. This result has been seen as a potential
contradiction with observat... | astro-ph | recent numerical simulations of binary black hole mergers show the possibility of producing very large recoil velocities 3000 kms kicks of this magnitude should be sufficient to eject the final black hole from virtually any galactic potential this result has been seen as a potential contradiction with observations of s... | [['recent', 'numerical', 'simulations', 'of', 'binary', 'black', 'hole', 'mergers', 'show', 'the', 'possibility', 'of', 'producing', 'very', 'large', 'recoil', 'velocities', '3000', 'kms', 'kicks', 'of', 'this', 'magnitude', 'should', 'be', 'sufficient', 'to', 'eject', 'the', 'final', 'black', 'hole', 'from', 'virtuall... | [-0.09822886580283322, 0.13082810924065486, -0.07931002507713146, 0.1445488415711003, -0.08244832733464313, -0.06389635616186552, 0.06899440825402896, 0.3537837852065156, -0.1682113678423154, -0.3637965746939455, 0.04670162619341437, -0.30632616247890926, -0.05486918995675075, 0.202801228735153, -0.027380223894241926, ... |
706.1549 | A Chain-Boson Model for the Decoherence and Relaxation of a Few Coupled
SQUIDs in a Phonon Bath | We develop a "chain-boson model" master equation, within the Born-Markov
approximation, for a few superconducting quantum interference devices (SQUIDs)
coupled into a chain and exchanging their angular momenta with a low
temperature phonon bath. Our master equation has four generators; we
concentrate on the damping a... | quant-ph cond-mat.mes-hall | we develop a chainboson model master equation within the bornmarkov approximation for a few superconducting quantum interference devices squids coupled into a chain and exchanging their angular momenta with a low temperature phonon bath our master equation has four generators we concentrate on the damping and diffusion... | [['we', 'develop', 'a', 'chainboson', 'model', 'master', 'equation', 'within', 'the', 'bornmarkov', 'approximation', 'for', 'a', 'few', 'superconducting', 'quantum', 'interference', 'devices', 'squids', 'coupled', 'into', 'a', 'chain', 'and', 'exchanging', 'their', 'angular', 'momenta', 'with', 'a', 'low', 'temperature... | [-0.2242786612725268, 0.26714652808154266, -0.05176304650735365, 0.058914793870564905, -0.026360405821110797, -0.2156492452239235, 0.08661866854885848, 0.3666225477976546, -0.25757393539462187, -0.26928803578580485, 0.010520865032784259, -0.32856802661402457, -0.0672644150940931, 0.17435584207582097, 0.0471154830246296... |
706.155 | Galactic disc warps due to intergalactic accretion flows onto the disc | The accretion of the intergalactic medium onto the gaseous disc is used to
explain the generation of galactic warps. A cup-shaped distortion is expected,
due to the transmission of the linear momentum; but, this effect is small for
most incident inflow angles and the predominant effect turns out to be the
transmissio... | astro-ph | the accretion of the intergalactic medium onto the gaseous disc is used to explain the generation of galactic warps a cupshaped distortion is expected due to the transmission of the linear momentum but this effect is small for most incident inflow angles and the predominant effect turns out to be the transmission of an... | [['the', 'accretion', 'of', 'the', 'intergalactic', 'medium', 'onto', 'the', 'gaseous', 'disc', 'is', 'used', 'to', 'explain', 'the', 'generation', 'of', 'galactic', 'warps', 'a', 'cupshaped', 'distortion', 'is', 'expected', 'due', 'to', 'the', 'transmission', 'of', 'the', 'linear', 'momentum', 'but', 'this', 'effect',... | [-0.12602755645670558, 0.12038845494555395, -0.1001876431319522, 0.08706100382316377, -0.1242433079888904, -0.061799033750953296, 0.01521956186018063, 0.3553427181116516, -0.251736130581678, -0.316613058219113, 0.027786633109308338, -0.23453272079237766, -0.04131675974756319, 0.1898579916131923, -0.04069553815411724, -... |
706.1551 | Study of the Flux and Spectral Variations in the VHE Emission from the
Blazar Markarian 501, with the MAGIC Telescope | The blazar Markarian 501 (Mrk 501) was observed above 100 GeV with the MAGIC
Telescope during May, June and July 2005. The high sensitivity of the
instrument made possible the detection of the source with high significance in
each of the observing nights. During this observational campaign, the emitted
gamma-ray flux... | astro-ph | the blazar markarian 501 mrk 501 was observed above 100 gev with the magic telescope during may june and july 2005 the high sensitivity of the instrument made possible the detection of the source with high significance in each of the observing nights during this observational campaign the emitted gammaray flux from mkn... | [['the', 'blazar', 'markarian', '501', 'mrk', '501', 'was', 'observed', 'above', '100', 'gev', 'with', 'the', 'magic', 'telescope', 'during', 'may', 'june', 'and', 'july', '2005', 'the', 'high', 'sensitivity', 'of', 'the', 'instrument', 'made', 'possible', 'the', 'detection', 'of', 'the', 'source', 'with', 'high', 'sig... | [-0.05560955064169861, 0.15334391982469242, -0.06844372366794159, 0.10099992373009603, -0.06790260128626549, -0.08271360386641242, 0.010720355266302422, 0.4747382144166811, -0.1255535132334665, -0.48571585347825613, 0.08819533024310462, -0.28795596796113093, -0.018450557814306906, 0.20719604258664656, -0.04968615597101... |
706.1552 | Fourier resolved spectroscopy of 4U 1728-34: New Insights into Spectral
and Temporal Properties of Low-Mass X-ray Binaries | Using archival RXTE data we derive the 2-16 keV Fourier-resolved spectra of
the Atoll source 4U 1728-34 in a sequence of its timing states as its low QPO
frequency spans the range between 6 and 94 Hz. The increase in the QPO
frequency accompanies a spectral transition of the source from its island to
its banana state... | astro-ph | using archival rxte data we derive the 216 kev fourierresolved spectra of the atoll source 4u 172834 in a sequence of its timing states as its low qpo frequency spans the range between 6 and 94 hz the increase in the qpo frequency accompanies a spectral transition of the source from its island to its banana states the ... | [['using', 'archival', 'rxte', 'data', 'we', 'derive', 'the', '216', 'kev', 'fourierresolved', 'spectra', 'of', 'the', 'atoll', 'source', '4u', '172834', 'in', 'a', 'sequence', 'of', 'its', 'timing', 'states', 'as', 'its', 'low', 'qpo', 'frequency', 'spans', 'the', 'range', 'between', '6', 'and', '94', 'hz', 'the', 'in... | [-0.07350563430167639, 0.12909766346324159, -0.08014038066443406, 0.07264298629055484, -0.046324692597875416, -0.12557274161272833, 0.07878539759345336, 0.43451622678524154, -0.20963921026589397, -0.3541965953544037, 0.0758576100686183, -0.3080340980962078, -0.009838281544602007, 0.2138709578385505, -0.0380136075153007... |
706.1553 | Absorption spectrum in the wings of the potassium second resonance
doublet broadened by helium | We have measured the reduced absorption coefficients occurring in the wings
of the potassium 4S-5P doublet lines at 404.414 nm and at 404.720 nm broadened
by helium gas at pressures of several hundred Torr. At the experimental
temperature of 900 K, we have detected a shoulder-like broadening feature on
the blue wing ... | physics.atom-ph astro-ph | we have measured the reduced absorption coefficients occurring in the wings of the potassium 4s5p doublet lines at 404414 nm and at 404720 nm broadened by helium gas at pressures of several hundred torr at the experimental temperature of 900 k we have detected a shoulderlike broadening feature on the blue wing of the d... | [['we', 'have', 'measured', 'the', 'reduced', 'absorption', 'coefficients', 'occurring', 'in', 'the', 'wings', 'of', 'the', 'potassium', '4s5p', 'doublet', 'lines', 'at', '404414', 'nm', 'and', 'at', '404720', 'nm', 'broadened', 'by', 'helium', 'gas', 'at', 'pressures', 'of', 'several', 'hundred', 'torr', 'at', 'the', ... | [-0.053170855260173934, 0.18141695776050595, -0.005056617193523858, -0.010271181489569845, 0.018670856546200182, -0.18864196278075923, 0.06012744098404517, 0.456741492784882, -0.18272338434659197, -0.29585721819973315, 0.019086398506414744, -0.34631547230785176, 0.05690585901187259, 0.13135807092846136, 0.0634882624055... |
706.1554 | Continuous Damage Fiber Bundle Model for Strongly Disordered Materials | We present an extension of the continuous damage fiber bundle model to
describe the gradual degradation of highly heterogeneous materials under an
increasing external load. Breaking of a fiber in the model is preceded by a
sequence of partial failure events occurring at random threshold values. In
order to capture th... | cond-mat.mtrl-sci cond-mat.stat-mech | we present an extension of the continuous damage fiber bundle model to describe the gradual degradation of highly heterogeneous materials under an increasing external load breaking of a fiber in the model is preceded by a sequence of partial failure events occurring at random threshold values in order to capture the su... | [['we', 'present', 'an', 'extension', 'of', 'the', 'continuous', 'damage', 'fiber', 'bundle', 'model', 'to', 'describe', 'the', 'gradual', 'degradation', 'of', 'highly', 'heterogeneous', 'materials', 'under', 'an', 'increasing', 'external', 'load', 'breaking', 'of', 'a', 'fiber', 'in', 'the', 'model', 'is', 'preceded',... | [-0.17094841940588382, 0.1719082484020429, -0.04997743857309742, -0.004796345395510614, -0.021731609267420893, -0.08459581297555173, 0.07133000795621165, 0.3727493902953529, -0.2834142842582723, -0.2675753927739092, 0.09197768926541068, -0.28430940960930995, -0.1728873944637373, 0.1504243609383558, -0.07141070223463945... |
706.1555 | High and Low Dimensions in The Black Hole Negative Mode | The negative mode of the Schwarzschild black hole is central to Euclidean
quantum gravity around hot flat space and for the Gregory-Laflamme black string
instability. We analyze the eigenvalue as a function of space-time dimension by
constructing two perturbative expansions: one for large d and the other for
small d-... | hep-th gr-qc | the negative mode of the schwarzschild black hole is central to euclidean quantum gravity around hot flat space and for the gregorylaflamme black string instability we analyze the eigenvalue as a function of spacetime dimension by constructing two perturbative expansions one for large d and the other for small d3 and d... | [['the', 'negative', 'mode', 'of', 'the', 'schwarzschild', 'black', 'hole', 'is', 'central', 'to', 'euclidean', 'quantum', 'gravity', 'around', 'hot', 'flat', 'space', 'and', 'for', 'the', 'gregorylaflamme', 'black', 'string', 'instability', 'we', 'analyze', 'the', 'eigenvalue', 'as', 'a', 'function', 'of', 'spacetime'... | [-0.12477532165015445, 0.10748201521705864, -0.048625282759723415, 0.13935572214232866, -0.07952155989649541, -0.15158699507112888, -0.01712544630281627, 0.2846417911569862, -0.19026446948101855, -0.26714503337108697, 0.12114417172201417, -0.3146854162695544, -0.10739517878083622, 0.19737301159869222, -0.00506034768460... |
706.1556 | Poisson Nernst-Planck Model of Ion Current Rectification through a
Nanofluidic Diode | We have investigated ion current rectification properties of a recently
prepared bipolar nanofluidic diode. This device is based on a single conically
shaped nanopore in a polymer film whose pore walls contain a sharp boundary
between positively and negatively charged regions. A semi-quantitative model
that employs P... | cond-mat.other | we have investigated ion current rectification properties of a recently prepared bipolar nanofluidic diode this device is based on a single conically shaped nanopore in a polymer film whose pore walls contain a sharp boundary between positively and negatively charged regions a semiquantitative model that employs poisso... | [['we', 'have', 'investigated', 'ion', 'current', 'rectification', 'properties', 'of', 'a', 'recently', 'prepared', 'bipolar', 'nanofluidic', 'diode', 'this', 'device', 'is', 'based', 'on', 'a', 'single', 'conically', 'shaped', 'nanopore', 'in', 'a', 'polymer', 'film', 'whose', 'pore', 'walls', 'contain', 'a', 'sharp',... | [-0.15105328210594246, 0.14668531990327843, -0.014425568783542874, -0.019308089941852923, 0.023235429609264953, -0.1924246635153946, 0.009392774340195694, 0.4426877417629867, -0.2579940286972983, -0.2863918545401909, 0.02128892162440796, -0.2509032488857029, -0.11153352888174016, 0.2208759042586087, -0.0520500394120586... |
706.1557 | The cosmological constant and dark energy in braneworlds | We review recent attempts to address the cosmological constant problem and
the late-time acceleration of the Universe based on braneworld models. In
braneworld models, the way in which the vacuum energy gravitates in the 4D
spacetime is radically different from conventional 4D physics. It is possible
that the vacuum ... | astro-ph gr-qc hep-th | we review recent attempts to address the cosmological constant problem and the latetime acceleration of the universe based on braneworld models in braneworld models the way in which the vacuum energy gravitates in the 4d spacetime is radically different from conventional 4d physics it is possible that the vacuum energy... | [['we', 'review', 'recent', 'attempts', 'to', 'address', 'the', 'cosmological', 'constant', 'problem', 'and', 'the', 'latetime', 'acceleration', 'of', 'the', 'universe', 'based', 'on', 'braneworld', 'models', 'in', 'braneworld', 'models', 'the', 'way', 'in', 'which', 'the', 'vacuum', 'energy', 'gravitates', 'in', 'the'... | [-0.07999686915920862, 0.08486041340619227, -0.12441749535254296, 0.13663969485517838, -0.13308538281858362, -0.15378017784003786, -0.029929150346148486, 0.3075303020455338, -0.21574119636357225, -0.30951735986063617, 0.04149547046735044, -0.23282119842702584, -0.14160894188684542, 0.14285405907804602, -0.0928157623425... |
706.1558 | Dynamical conductance in the two-channel Kondo regime of a double dot
system | We study finite-frequency transport properties of the double-dot system
recently constructed to observe the two-channel Kondo effect [R. M. Potok et
al., Nature 446, 167 (2007)]. We derive an analytical expression for the
frequency-dependent linear conductance of this device in the Kondo regime. We
show how the featu... | cond-mat.mes-hall cond-mat.str-el | we study finitefrequency transport properties of the doubledot system recently constructed to observe the twochannel kondo effect r m potok et al nature 446 167 2007 we derive an analytical expression for the frequencydependent linear conductance of this device in the kondo regime we show how the features characteristi... | [['we', 'study', 'finitefrequency', 'transport', 'properties', 'of', 'the', 'doubledot', 'system', 'recently', 'constructed', 'to', 'observe', 'the', 'twochannel', 'kondo', 'effect', 'r', 'm', 'potok', 'et', 'al', 'nature', '446', '167', '2007', 'we', 'derive', 'an', 'analytical', 'expression', 'for', 'the', 'frequency... | [-0.16714443281913796, 0.14021879051840802, -0.13700403822491866, 0.06241095946828901, -0.02338861542838541, -0.17444751087594965, 0.07172775097694624, 0.293641871779762, -0.27365736982013766, -0.28112733264387857, -0.011890439648237643, -0.29267640616932905, -0.224236490289596, 0.18678546150337266, -0.0024619122515573... |
706.1559 | Fractionalization in a square-lattice model with time-reversal symmetry | We propose a two-dimensional time-reversal invariant system of essentially
non-interacting electrons on a square lattice that exhibits configurations with
fractional charges e/2. These are vortex-like topological defects in the
dimerization order parameter describing spatial modulation in the electron
hopping amplitu... | cond-mat.str-el cond-mat.mes-hall | we propose a twodimensional timereversal invariant system of essentially noninteracting electrons on a square lattice that exhibits configurations with fractional charges e2 these are vortexlike topological defects in the dimerization order parameter describing spatial modulation in the electron hopping amplitudes char... | [['we', 'propose', 'a', 'twodimensional', 'timereversal', 'invariant', 'system', 'of', 'essentially', 'noninteracting', 'electrons', 'on', 'a', 'square', 'lattice', 'that', 'exhibits', 'configurations', 'with', 'fractional', 'charges', 'e2', 'these', 'are', 'vortexlike', 'topological', 'defects', 'in', 'the', 'dimeriza... | [-0.2390887379174891, 0.23427976635273942, -0.03451817357096315, 0.07454373584169159, -0.013041449503766166, -0.14384815059487283, 0.06288712991855716, 0.34752094009776174, -0.1948094740739943, -0.27347984204045783, 0.005561014157317487, -0.30964546813917015, -0.15702853359305013, 0.10271064909519972, 0.026250486451856... |
706.156 | Two gravitational shock waves on the AdS_3 brane | A gravitational shock wave is a solution to Einstein equations describing the
gravitational field of a massless particle. We obtain such a geometry for a
particle moving on a AdS_3 brane embedded in a AdS_4 bulk (the lower
dimensional version of the "locally localized gravity" model of Karch and
Randall). In order to... | hep-th | a gravitational shock wave is a solution to einstein equations describing the gravitational field of a massless particle we obtain such a geometry for a particle moving on a ads_3 brane embedded in a ads_4 bulk the lower dimensional version of the locally localized gravity model of karch and randall in order to do this... | [['a', 'gravitational', 'shock', 'wave', 'is', 'a', 'solution', 'to', 'einstein', 'equations', 'describing', 'the', 'gravitational', 'field', 'of', 'a', 'massless', 'particle', 'we', 'obtain', 'such', 'a', 'geometry', 'for', 'a', 'particle', 'moving', 'on', 'a', 'ads_3', 'brane', 'embedded', 'in', 'a', 'ads_4', 'bulk',... | [-0.15111073528972568, 0.11913966304763295, -0.09634796255971674, 0.09903162646127477, -0.11283682871663528, -0.12889675994021751, -0.02563138501722828, 0.2974723281955226, -0.17467180861113257, -0.2587251042035951, 0.08790747156256153, -0.29232987563842705, -0.1299074997509019, 0.16951754945916586, -0.0333656576167282... |
706.1561 | Characterization of separability and entanglement in $(2\times{D})$- and
$(3\times{D})$-dimensional systems by single-qubit and single-qutrit unitary
transformations | We investigate the geometric characterization of pure state bipartite
entanglement of $(2\times{D})$- and $(3\times{D})$-dimensional composite
quantum systems. To this aim, we analyze the relationship between states and
their images under the action of particular classes of local unitary
operations. We find that inva... | quant-ph cond-mat.other hep-th math-ph math.MP | we investigate the geometric characterization of pure state bipartite entanglement of 2timesd and 3timesddimensional composite quantum systems to this aim we analyze the relationship between states and their images under the action of particular classes of local unitary operations we find that invariance of states unde... | [['we', 'investigate', 'the', 'geometric', 'characterization', 'of', 'pure', 'state', 'bipartite', 'entanglement', 'of', '2timesd', 'and', '3timesddimensional', 'composite', 'quantum', 'systems', 'to', 'this', 'aim', 'we', 'analyze', 'the', 'relationship', 'between', 'states', 'and', 'their', 'images', 'under', 'the', ... | [-0.14055947729146048, 0.1557323732879013, -0.08750915046661131, 0.07238647221332235, 0.04508672178152107, -0.13567573838236352, 0.04693659414056568, 0.3487844805879098, -0.26538888724640974, -0.25703391245295926, 0.08357162427968315, -0.2753995191681409, -0.16033470116615775, 0.1782352900673305, -0.09021557059379355, ... |
706.1562 | Rapid Formation of Supermassive Black Hole Binaries in Galaxy Mergers
with Gas | Supermassive black holes (SMBHs) are a ubiquitous component of the nuclei of
galaxies. It is normally assumed that, following the merger of two massive
galaxies, a SMBH binary will form, shrink due to stellar or gas dynamical
processes and ultimately coalesce by emitting a burst of gravitational waves.
However, so fa... | astro-ph | supermassive black holes smbhs are a ubiquitous component of the nuclei of galaxies it is normally assumed that following the merger of two massive galaxies a smbh binary will form shrink due to stellar or gas dynamical processes and ultimately coalesce by emitting a burst of gravitational waves however so far it has n... | [['supermassive', 'black', 'holes', 'smbhs', 'are', 'a', 'ubiquitous', 'component', 'of', 'the', 'nuclei', 'of', 'galaxies', 'it', 'is', 'normally', 'assumed', 'that', 'following', 'the', 'merger', 'of', 'two', 'massive', 'galaxies', 'a', 'smbh', 'binary', 'will', 'form', 'shrink', 'due', 'to', 'stellar', 'or', 'gas', ... | [-0.1147059759720886, 0.14528198109483545, -0.08162593710680607, 0.11582591403595299, -0.10615309442277827, -0.03294069480376921, 0.002947357331031288, 0.35229147447187914, -0.1708908337198831, -0.31218579490638637, 0.054711391873889015, -0.3005116142977784, -0.06461176988546999, 0.22476145591483349, 0.0195922777726272... |
706.1563 | Optimal Choice of Threshold in Two Level Processor Sharing | We analyze the Two Level Processor Sharing (TLPS) scheduling discipline with
the hyper-exponential job size distribution and with the Poisson arrival
process. TLPS is a convenient model to study the benefit of the file size based
differentiation in TCP/IP networks. In the case of the hyper-exponential job
size distri... | cs.NI | we analyze the two level processor sharing tlps scheduling discipline with the hyperexponential job size distribution and with the poisson arrival process tlps is a convenient model to study the benefit of the file size based differentiation in tcpip networks in the case of the hyperexponential job size distribution wi... | [['we', 'analyze', 'the', 'two', 'level', 'processor', 'sharing', 'tlps', 'scheduling', 'discipline', 'with', 'the', 'hyperexponential', 'job', 'size', 'distribution', 'and', 'with', 'the', 'poisson', 'arrival', 'process', 'tlps', 'is', 'a', 'convenient', 'model', 'to', 'study', 'the', 'benefit', 'of', 'the', 'file', '... | [-0.14584194788378074, 0.09423332505059694, -0.09790457622476027, 0.0788564436481824, -0.03437252369591258, -0.12461281746206149, 0.13571326512905676, 0.3742479375091342, -0.2628496633104744, -0.3147808270214099, 0.09776377742519786, -0.2647285886817205, -0.07981153003687799, 0.17072709428120247, -0.05827859093264585, ... |
706.1564 | The First Survey of X-ray Flares from Gamma Ray Bursts Observed by
Swift: Spectral Properties and Energetics | Observations of gamma ray bursts (GRBs) with Swift produced the initially
surprising result that many bursts have large X-ray flares superimposed on the
underlying afterglow. The flares were sometimes intense, had rapid rise and
decay phases, and occurred late relative to the ``prompt'' phase. Some
remarkable flares ... | astro-ph | observations of gamma ray bursts grbs with swift produced the initially surprising result that many bursts have large xray flares superimposed on the underlying afterglow the flares were sometimes intense had rapid rise and decay phases and occurred late relative to the prompt phase some remarkable flares are observed ... | [['observations', 'of', 'gamma', 'ray', 'bursts', 'grbs', 'with', 'swift', 'produced', 'the', 'initially', 'surprising', 'result', 'that', 'many', 'bursts', 'have', 'large', 'xray', 'flares', 'superimposed', 'on', 'the', 'underlying', 'afterglow', 'the', 'flares', 'were', 'sometimes', 'intense', 'had', 'rapid', 'rise',... | [-0.022836768139873963, 0.18162261387533676, -0.06417232272650235, 0.1912321887421341, -0.0844242643052551, -0.09359573422057818, 0.013651555785941521, 0.5190827774341543, -0.1470854885346066, -0.356367393477359, 0.04340112488112609, -0.33152912822020303, -0.025343766042827322, 0.2593183534179176, -0.030517005900591355... |
706.1565 | The Beginning and Evolution of the Universe | We review the current standard model for the evolution of the Universe from
an early inflationary epoch to the complex hierarchy of structure seen today.
We summarize and provide key references for the following topics: observations
of the expanding Universe; the hot early Universe and nucleosynthesis; theory
and obs... | astro-ph gr-qc hep-ph hep-th physics.hist-ph | we review the current standard model for the evolution of the universe from an early inflationary epoch to the complex hierarchy of structure seen today we summarize and provide key references for the following topics observations of the expanding universe the hot early universe and nucleosynthesis theory and observati... | [['we', 'review', 'the', 'current', 'standard', 'model', 'for', 'the', 'evolution', 'of', 'the', 'universe', 'from', 'an', 'early', 'inflationary', 'epoch', 'to', 'the', 'complex', 'hierarchy', 'of', 'structure', 'seen', 'today', 'we', 'summarize', 'and', 'provide', 'key', 'references', 'for', 'the', 'following', 'topi... | [-0.08191253854555168, 0.10834907873504562, -0.12311077479558487, 0.1417126271032518, -0.13849870300093184, -0.07873885415028781, -0.04661831161525521, 0.32484966460164755, -0.22261346726407927, -0.3651448929562203, 0.0701893599489854, -0.26521161806369725, -0.0369707947510535, 0.14671861861021288, 0.009969644173378906... |
706.1566 | Murre's conjectures and explicit Chow--Kuenneth projectors for some
varieties | In this paper, we investigate Murre's conjectures on the structure of
rational Chow groups and exhibit explicit Chow--Kuenneth projectors for some
examples. More precisely, the examples we study are the varieties which have a
nef tangent bundle. For surfaces and threefolds which have a nef tangent bundle
explicit Cho... | math.AG math.AC | in this paper we investigate murres conjectures on the structure of rational chow groups and exhibit explicit chowkuenneth projectors for some examples more precisely the examples we study are the varieties which have a nef tangent bundle for surfaces and threefolds which have a nef tangent bundle explicit chowkuenneth... | [['in', 'this', 'paper', 'we', 'investigate', 'murres', 'conjectures', 'on', 'the', 'structure', 'of', 'rational', 'chow', 'groups', 'and', 'exhibit', 'explicit', 'chowkuenneth', 'projectors', 'for', 'some', 'examples', 'more', 'precisely', 'the', 'examples', 'we', 'study', 'are', 'the', 'varieties', 'which', 'have', '... | [-0.2251009520750813, -0.03389624954434112, -0.15451887334347703, 0.16709684197849128, -0.11749347878503613, -0.2146097945224028, -0.015584995242534205, 0.38517769175814465, -0.2635110603296198, -0.15512198710348457, 0.1324706832801894, -0.23226493403490167, -0.20625566456874367, 0.21632788720307872, -0.216615983386873... |
706.1567 | Equivalence of sparse circulants: the bipartite \'Ad\'am problem | We consider n-by-n circulant matrices having entries 0 and 1. Such matrices
can be identified with sets of residues mod n, corresponding to the columns in
which the top row contains an entry 1. Let A and B be two such matrices, and
suppose that the corresponding residue sets S_A and S_B have size at most 3. We
prove ... | math.CO math.NT | we consider nbyn circulant matrices having entries 0 and 1 such matrices can be identified with sets of residues mod n corresponding to the columns in which the top row contains an entry 1 let a and b be two such matrices and suppose that the corresponding residue sets s_a and s_b have size at most 3 we prove that the ... | [['we', 'consider', 'nbyn', 'circulant', 'matrices', 'having', 'entries', '0', 'and', '1', 'such', 'matrices', 'can', 'be', 'identified', 'with', 'sets', 'of', 'residues', 'mod', 'n', 'corresponding', 'to', 'the', 'columns', 'in', 'which', 'the', 'top', 'row', 'contains', 'an', 'entry', '1', 'let', 'a', 'and', 'b', 'be... | [-0.13866983885559925, 0.13869991381509156, 0.00255498459834295, 0.04882405828943269, -0.013660874748085108, -0.18204013348117265, 0.0082266205507848, 0.37472327871687916, -0.30866108530527625, -0.24531990984622906, 0.12467829939851072, -0.34652841607910684, -0.1752862127889077, 0.15397069196721228, -0.1017048008895168... |
706.1568 | Simulating non-small cell lung cancer with a multiscale agent-based
model | Background The epidermal growth factor receptor (EGFR) is frequently
overexpressed in many cancers, including non-small cell lung cancer (NSCLC). In
silcio modeling is considered to be an increasingly promising tool to add
useful insights into the dynamics of the EGFR signal transduction pathway.
However, most of the... | q-bio.CB | background the epidermal growth factor receptor egfr is frequently overexpressed in many cancers including nonsmall cell lung cancer nsclc in silcio modeling is considered to be an increasingly promising tool to add useful insights into the dynamics of the egfr signal transduction pathway however most of the previous m... | [['background', 'the', 'epidermal', 'growth', 'factor', 'receptor', 'egfr', 'is', 'frequently', 'overexpressed', 'in', 'many', 'cancers', 'including', 'nonsmall', 'cell', 'lung', 'cancer', 'nsclc', 'in', 'silcio', 'modeling', 'is', 'considered', 'to', 'be', 'an', 'increasingly', 'promising', 'tool', 'to', 'add', 'usefu... | [-0.07365027515093771, 0.117043596664748, -0.004375144576551308, 0.061162411995443575, -0.027461752109256266, -0.1424882601131685, 0.08182281145554703, 0.35013705059680916, -0.2619443289864031, -0.2425984014915046, 0.03318838881480362, -0.25231513878065714, -0.24640382683532602, 0.18036525959678745, -0.0478843408134774... |
706.1569 | Composition-sensitive parameters measured with the surface detector of
the Pierre Auger Observatory | A key step towards the understanding of the origin of ultra-high energy
cosmic rays is their mass composition. Primary photons and neutrinos produce
markedly different showers from nuclei, while showers of different nuclear
species are not easy to distinguish. To maximise the discrimination with the
Pierre Auger Obse... | astro-ph | a key step towards the understanding of the origin of ultrahigh energy cosmic rays is their mass composition primary photons and neutrinos produce markedly different showers from nuclei while showers of different nuclear species are not easy to distinguish to maximise the discrimination with the pierre auger observator... | [['a', 'key', 'step', 'towards', 'the', 'understanding', 'of', 'the', 'origin', 'of', 'ultrahigh', 'energy', 'cosmic', 'rays', 'is', 'their', 'mass', 'composition', 'primary', 'photons', 'and', 'neutrinos', 'produce', 'markedly', 'different', 'showers', 'from', 'nuclei', 'while', 'showers', 'of', 'different', 'nuclear'... | [-0.07991810482749513, 0.24022668157830712, -0.06524655287680418, 0.11818772634622925, -0.044668723087575614, -0.017505544450376994, -0.02415599631216458, 0.39485126029214135, -0.2133492509677561, -0.3843853901869253, 0.0562318053410348, -0.31451229946738435, 0.0016621150691365904, 0.17488590953238917, 0.01107951183331... |
706.157 | Lorentz spacetimes of constant curvature | This paper was first written in 1990, but was never published. In it, the
author presents a novel approach to the study of constant curvature spacetimes
in 2+1 dimensions. A parameterization of flat 2+1-dimensional domains of
dependence is given in terms of measured geodesic laminations. There is also an
interesting ... | math.DG math-ph math.GT math.MP | this paper was first written in 1990 but was never published in it the author presents a novel approach to the study of constant curvature spacetimes in 21 dimensions a parameterization of flat 21dimensional domains of dependence is given in terms of measured geodesic laminations there is also an interesting reinterpre... | [['this', 'paper', 'was', 'first', 'written', 'in', '1990', 'but', 'was', 'never', 'published', 'in', 'it', 'the', 'author', 'presents', 'a', 'novel', 'approach', 'to', 'the', 'study', 'of', 'constant', 'curvature', 'spacetimes', 'in', '21', 'dimensions', 'a', 'parameterization', 'of', 'flat', '21dimensional', 'domains... | [-0.13298936767218836, 0.07087816510934956, -0.10488466031018122, 0.0656503755560776, -0.11411363437393207, -0.09936897272305671, -0.006494073365614865, 0.33615131794729014, -0.17851158674837145, -0.3096772081994121, 0.1157532763390317, -0.3038545402059378, -0.13437255322625322, 0.16768357253148536, -0.1793127391325725... |
706.1571 | Connecting String/M Theory to the Electroweak Scale and to LHC Data | The Standard Model of particle physics explains (almost) all observed
non-gravitational microscopic phenomena but has many open theoretical
questions. We are on the threshold of unraveling the mysteries of the Standard
Model and discovering its extension. This could be achieved in the near future
with the help of man... | hep-ph hep-ex hep-th | the standard model of particle physics explains almost all observed nongravitational microscopic phenomena but has many open theoretical questions we are on the threshold of unraveling the mysteries of the standard model and discovering its extension this could be achieved in the near future with the help of many exper... | [['the', 'standard', 'model', 'of', 'particle', 'physics', 'explains', 'almost', 'all', 'observed', 'nongravitational', 'microscopic', 'phenomena', 'but', 'has', 'many', 'open', 'theoretical', 'questions', 'we', 'are', 'on', 'the', 'threshold', 'of', 'unraveling', 'the', 'mysteries', 'of', 'the', 'standard', 'model', '... | [-0.04479910670247985, 0.08144683013061715, -0.11374587250330787, 0.11157120160912494, -0.09064303699415177, -0.13242173871469104, 0.028850785288849743, 0.3148934462393715, -0.31214092443073826, -0.35559130402732875, 0.09181338316608792, -0.2602769162241868, -0.15502118654952451, 0.21473737865022757, -0.058748305766975... |
706.1572 | On Minkowskian Branching Structures | Contrary to its initial idea, Belnap's (1992) theory of Branching Space-Times
(BST) has models in which histories do not resemble relativistic space-times or
any other physical space-times. The aim of this paper is to define a certain
class of BST models, called "Minkowskian Branching Structures" (MBS), in which
hist... | math-ph math.MP | contrary to its initial idea belnaps 1992 theory of branching spacetimes bst has models in which histories do not resemble relativistic spacetimes or any other physical spacetimes the aim of this paper is to define a certain class of bst models called minkowskian branching structures mbs in which histories are isomorph... | [['contrary', 'to', 'its', 'initial', 'idea', 'belnaps', '1992', 'theory', 'of', 'branching', 'spacetimes', 'bst', 'has', 'models', 'in', 'which', 'histories', 'do', 'not', 'resemble', 'relativistic', 'spacetimes', 'or', 'any', 'other', 'physical', 'spacetimes', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'define'... | [-0.10521125841348682, 0.14332313702838256, -0.14039659341520602, 0.12234368856182543, -0.1666475688891098, -0.1750269472958649, 0.05636874011413443, 0.3713367676897214, -0.19604290685256814, -0.274892559510167, 0.09727760322742385, -0.22592204436659813, -0.14965240484435516, 0.17514499698046337, -0.12598614075617626, ... |
706.1573 | Thermal derivation of the Coleman-De Luccia tunneling prescription | We derive the rate for transitions between de Sitter vacua by treating the
field theory on the static patch as a thermal system. This reproduces the
Coleman-De Luccia formalism for calculating the rate, but leads to a modified
interpretation of the bounce solution and a different prediction for the
evolution of the s... | hep-th gr-qc | we derive the rate for transitions between de sitter vacua by treating the field theory on the static patch as a thermal system this reproduces the colemande luccia formalism for calculating the rate but leads to a modified interpretation of the bounce solution and a different prediction for the evolution of the system... | [['we', 'derive', 'the', 'rate', 'for', 'transitions', 'between', 'de', 'sitter', 'vacua', 'by', 'treating', 'the', 'field', 'theory', 'on', 'the', 'static', 'patch', 'as', 'a', 'thermal', 'system', 'this', 'reproduces', 'the', 'colemande', 'luccia', 'formalism', 'for', 'calculating', 'the', 'rate', 'but', 'leads', 'to... | [-0.13197576146133846, 0.09938701730061439, -0.1354305458227524, 0.12188814403937916, -0.025687921139857888, -0.1284989692188295, 0.042889634021776146, 0.2991253798827529, -0.20968877299674205, -0.2753624201771648, 0.09250907696332433, -0.2646481021341363, -0.09569133408513153, 0.18125540800125842, -0.03405312704489915... |
706.1574 | Wavelet transforms in a critical interface model for Barkhausen noise | We discuss the application of wavelet transforms to a critical interface
model, which is known to provide a good description of Barkhausen noise in soft
ferromagnets. The two-dimensional version of the model (one-dimensional
interface) is considered, mainly in the adiabatic limit of very slow driving.
On length scale... | cond-mat.stat-mech cond-mat.dis-nn | we discuss the application of wavelet transforms to a critical interface model which is known to provide a good description of barkhausen noise in soft ferromagnets the twodimensional version of the model onedimensional interface is considered mainly in the adiabatic limit of very slow driving on length scales shorter ... | [['we', 'discuss', 'the', 'application', 'of', 'wavelet', 'transforms', 'to', 'a', 'critical', 'interface', 'model', 'which', 'is', 'known', 'to', 'provide', 'a', 'good', 'description', 'of', 'barkhausen', 'noise', 'in', 'soft', 'ferromagnets', 'the', 'twodimensional', 'version', 'of', 'the', 'model', 'onedimensional',... | [-0.15333208345322752, 0.1969499704362431, -0.1449752652527384, 0.14829462950534358, -0.001608746141460921, -0.15381510116973182, 0.03340164615615258, 0.36261836166532946, -0.3069781935970548, -0.24461208980425564, 0.08776389742532456, -0.2738688988920587, -0.13764216420962147, 0.20444668265564603, 0.011462652736054865... |
706.1575 | Nilpotent normal form for divergence-free vector fields and
volume-preserving maps | We study the normal forms for incompressible flows and maps in the
neighborhood of an equilibrium or fixed point with a triple eigenvalue. We
prove that when a divergence free vector field in $\mathbb{R}^3$ has nilpotent
linearization with maximal Jordan block then, to arbitrary degree, coordinates
can be chosen so t... | nlin.CD | we study the normal forms for incompressible flows and maps in the neighborhood of an equilibrium or fixed point with a triple eigenvalue we prove that when a divergence free vector field in mathbbr3 has nilpotent linearization with maximal jordan block then to arbitrary degree coordinates can be chosen so that the non... | [['we', 'study', 'the', 'normal', 'forms', 'for', 'incompressible', 'flows', 'and', 'maps', 'in', 'the', 'neighborhood', 'of', 'an', 'equilibrium', 'or', 'fixed', 'point', 'with', 'a', 'triple', 'eigenvalue', 'we', 'prove', 'that', 'when', 'a', 'divergence', 'free', 'vector', 'field', 'in', 'mathbbr3', 'has', 'nilpoten... | [-0.16213323371302263, 0.10425545068559872, -0.09031949592206408, 0.0014963480449902515, -0.06917664969759975, -0.12236886535880759, -0.036553092486928125, 0.31413498981034055, -0.3405809661592631, -0.19956225235763864, 0.10329264157232554, -0.2703192669934794, -0.15235072073718423, 0.13819399116076894, -0.058395305210... |
706.1576 | A time frequency analysis of wave packet fractional revivals | We show that the time frequency analysis of the autocorrelation function is,
in many ways, a more appropriate tool to resolve fractional revivals of a wave
packet than the usual time domain analysis. This advantage is crucial in
reconstructing the initial state of the wave packet when its coherent structure
is short-... | quant-ph | we show that the time frequency analysis of the autocorrelation function is in many ways a more appropriate tool to resolve fractional revivals of a wave packet than the usual time domain analysis this advantage is crucial in reconstructing the initial state of the wave packet when its coherent structure is shortlived ... | [['we', 'show', 'that', 'the', 'time', 'frequency', 'analysis', 'of', 'the', 'autocorrelation', 'function', 'is', 'in', 'many', 'ways', 'a', 'more', 'appropriate', 'tool', 'to', 'resolve', 'fractional', 'revivals', 'of', 'a', 'wave', 'packet', 'than', 'the', 'usual', 'time', 'domain', 'analysis', 'this', 'advantage', '... | [-0.1774136054380094, 0.11092800918193907, -0.12378934537991881, 0.07276108874038811, -0.04617059134157761, -0.07190863716741146, 0.04175926973924638, 0.3667987172122834, -0.232926959707841, -0.23047448547100122, 0.11693746574170324, -0.2679762204028315, -0.15795173489418374, 0.2099627597688012, 0.03305324702084346, 0.... |
706.1577 | Cosmic string formation by flux trapping | We study the formation of cosmic strings by confining a stochastic magnetic
field into flux tubes in a numerical simulation. We use overdamped evolution in
a potential that is minimized when the flux through each face in the simulation
lattice is a multiple of the fundamental flux quantum. When the typical number
of ... | hep-th astro-ph cond-mat.supr-con hep-ph | we study the formation of cosmic strings by confining a stochastic magnetic field into flux tubes in a numerical simulation we use overdamped evolution in a potential that is minimized when the flux through each face in the simulation lattice is a multiple of the fundamental flux quantum when the typical number of flux... | [['we', 'study', 'the', 'formation', 'of', 'cosmic', 'strings', 'by', 'confining', 'a', 'stochastic', 'magnetic', 'field', 'into', 'flux', 'tubes', 'in', 'a', 'numerical', 'simulation', 'we', 'use', 'overdamped', 'evolution', 'in', 'a', 'potential', 'that', 'is', 'minimized', 'when', 'the', 'flux', 'through', 'each', '... | [-0.16280079892160193, 0.22136754176539225, -0.054066293886751826, 0.09700606081363124, 0.0008772332637038614, -0.10376414046844556, 0.03232522303975808, 0.38173323160126094, -0.24581690332741432, -0.2843206364306666, 0.07700376765292492, -0.28155360126956586, -0.08247317095880308, 0.16313057340795195, -0.0133908722354... |
706.1578 | The Origin of the Magellanic Stream and Its Leading Arm | We explore the Magellanic Stream (MS) using a Gaussian decomposition of the
HI velocity profiles in the Leiden-Argentine-Bonn (LAB) all-sky HI survey. This
decomposition exposes the MS to be composed of two filaments distinct both
spatially (as first pointed out by Putman et al.) and in velocity. Using the
velocity c... | astro-ph | we explore the magellanic stream ms using a gaussian decomposition of the hi velocity profiles in the leidenargentinebonn lab allsky hi survey this decomposition exposes the ms to be composed of two filaments distinct both spatially as first pointed out by putman et al and in velocity using the velocity coherence of th... | [['we', 'explore', 'the', 'magellanic', 'stream', 'ms', 'using', 'a', 'gaussian', 'decomposition', 'of', 'the', 'hi', 'velocity', 'profiles', 'in', 'the', 'leidenargentinebonn', 'lab', 'allsky', 'hi', 'survey', 'this', 'decomposition', 'exposes', 'the', 'ms', 'to', 'be', 'composed', 'of', 'two', 'filaments', 'distinct'... | [-0.11558237846167493, 0.0833404267741423, -0.10315043550567717, 0.05298453158172741, -0.08043640878759475, -0.018357371303775325, 0.052319654913778164, 0.3748122726498944, -0.2636418135053993, -0.31421664921089826, 0.03952611937155432, -0.261001507183764, -0.06034974756814365, 0.18162312322652074, -0.0474423440570784,... |
706.1579 | Integrable systems and complex geometry | In this paper, we discuss an interaction between complex geometry and
integrable systems. Section 1 reviews the classical results on integrable
systems. New examples of integrable systems, which have been discovered, are
based on the Lax representation of the equations of motion. These systems can
be realized as stra... | math.DS math.AG | in this paper we discuss an interaction between complex geometry and integrable systems section 1 reviews the classical results on integrable systems new examples of integrable systems which have been discovered are based on the lax representation of the equations of motion these systems can be realized as straight lin... | [['in', 'this', 'paper', 'we', 'discuss', 'an', 'interaction', 'between', 'complex', 'geometry', 'and', 'integrable', 'systems', 'section', '1', 'reviews', 'the', 'classical', 'results', 'on', 'integrable', 'systems', 'new', 'examples', 'of', 'integrable', 'systems', 'which', 'have', 'been', 'discovered', 'are', 'based... | [-0.17717046166241174, 0.041688104194830745, -0.08910568059002469, 0.08636441631792727, -0.07280794438486407, -0.11187168577645015, -0.04874573325147279, 0.3476353385434537, -0.28365252579941036, -0.2425198502106858, 0.14571470375925016, -0.2526092649498893, -0.20530784423821247, 0.238014101673808, -0.09830942931764114... |
706.158 | Empirical Photometric Redshifts of Luminous Red Galaxies and Clusters in
SDSS | In this work I discuss the necessary steps for deriving photometric redshifts
for luminous red galaxies (LRGs) and galaxy clusters through simple empirical
methods. The data used is from the Sloan Digital Sky Survey (SDSS). I show that
with three bands only ({\it gri}) it is possible to achieve results as accurate
as... | astro-ph | in this work i discuss the necessary steps for deriving photometric redshifts for luminous red galaxies lrgs and galaxy clusters through simple empirical methods the data used is from the sloan digital sky survey sdss i show that with three bands only it gri it is possible to achieve results as accurate as the ones obt... | [['in', 'this', 'work', 'i', 'discuss', 'the', 'necessary', 'steps', 'for', 'deriving', 'photometric', 'redshifts', 'for', 'luminous', 'red', 'galaxies', 'lrgs', 'and', 'galaxy', 'clusters', 'through', 'simple', 'empirical', 'methods', 'the', 'data', 'used', 'is', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'sd... | [-0.01181175808954215, 0.08126105116932981, -0.05264950352696059, 0.08742509446781314, -0.08190369661532847, -0.09926817471095095, 0.09580343268775245, 0.45057911360205494, -0.15481824910904535, -0.3358562534767803, 0.05996496922020002, -0.3455593560663221, 0.015924722891097087, 0.22921757866721218, -0.0211379918315592... |
706.1581 | Examples of Non-Rigid CAT(0) Groups from the Category of Knot Groups | C Croke and B Kleiner have constructed an example of a CAT(0) group with more
than one visual boundary. J Wilson has proven that this same group has
uncountably many distinct boundaries. In this article we prove that the knot
group of any connected sum of two non-trivial torus knots also has uncountably
many distinct... | math.GT math.GR | c croke and b kleiner have constructed an example of a cat0 group with more than one visual boundary j wilson has proven that this same group has uncountably many distinct boundaries in this article we prove that the knot group of any connected sum of two nontrivial torus knots also has uncountably many distinct cat0 b... | [['c', 'croke', 'and', 'b', 'kleiner', 'have', 'constructed', 'an', 'example', 'of', 'a', 'cat0', 'group', 'with', 'more', 'than', 'one', 'visual', 'boundary', 'j', 'wilson', 'has', 'proven', 'that', 'this', 'same', 'group', 'has', 'uncountably', 'many', 'distinct', 'boundaries', 'in', 'this', 'article', 'we', 'prove',... | [-0.2261916813256807, 0.12360370884013255, -0.1483439217411439, 0.014352998561470917, -0.10987294318252488, -0.2135871660144052, -0.012694829294719455, 0.45857519656419754, -0.23793368116674715, -0.2259169935591911, 0.11398452657005309, -0.2743027858485125, -0.1665628676123002, 0.18245817854869784, -0.165625874002121, ... |
706.1582 | Cavity Enhanced Optical Vernier Spectroscopy, Broad Band, High
Resolution, High Sensitivity | A femtosecond frequency comb provides a vast number of equidistantly spaced
narrow band laser modes that can be simultaneously tuned and frequency
calibrated with 15 digits accuracy. Our Vernier spectrometer utilizes all of
theses modes in a massively parallel manner to rapidly record both absorption
and dispersion s... | physics.optics physics.ins-det | a femtosecond frequency comb provides a vast number of equidistantly spaced narrow band laser modes that can be simultaneously tuned and frequency calibrated with 15 digits accuracy our vernier spectrometer utilizes all of theses modes in a massively parallel manner to rapidly record both absorption and dispersion spec... | [['a', 'femtosecond', 'frequency', 'comb', 'provides', 'a', 'vast', 'number', 'of', 'equidistantly', 'spaced', 'narrow', 'band', 'laser', 'modes', 'that', 'can', 'be', 'simultaneously', 'tuned', 'and', 'frequency', 'calibrated', 'with', '15', 'digits', 'accuracy', 'our', 'vernier', 'spectrometer', 'utilizes', 'all', 'o... | [-0.1396563019844945, 0.17453827467505578, -0.021437428535226687, -0.0720905637178846, -0.09616219926694478, -0.19756073515034384, 0.09507915648965189, 0.5295377960026172, -0.19689025276449773, -0.33641472672698675, 0.06317476799961662, -0.24634252051696365, -0.015653363360023057, 0.2631200411943374, -0.037001834574362... |
706.1583 | Evidence for Distinct Components of the Galactic Stellar Halo from 838
RR Lyrae Stars Discovered in the LONEOS-I Survey | We present 838 ab-type RR Lyrae stars from the Lowell Observatory Near Earth
Objects Survey Phase I (LONEOS-I). These objects cover 1430 deg^2 and span
distances ranging from 3-30 kpc from the Galactic Center. Object selection is
based on phased, photometric data with 28-50 epochs. We use this large sample
to explore... | astro-ph | we present 838 abtype rr lyrae stars from the lowell observatory near earth objects survey phase i loneosi these objects cover 1430 deg2 and span distances ranging from 330 kpc from the galactic center object selection is based on phased photometric data with 2850 epochs we use this large sample to explore the bulk pro... | [['we', 'present', '838', 'abtype', 'rr', 'lyrae', 'stars', 'from', 'the', 'lowell', 'observatory', 'near', 'earth', 'objects', 'survey', 'phase', 'i', 'loneosi', 'these', 'objects', 'cover', '1430', 'deg2', 'and', 'span', 'distances', 'ranging', 'from', '330', 'kpc', 'from', 'the', 'galactic', 'center', 'object', 'sel... | [-0.06520428747432168, 0.13322179341417695, -0.11591847310079012, 0.0785090895369649, -0.11485036018777138, -0.0660306796494093, 0.09492181520735317, 0.412257465857095, -0.16802434495358326, -0.38301885097440497, 0.03526751155297814, -0.3204277912754246, -0.046841420318389226, 0.20078462996144794, -0.056377042578394286... |
706.1584 | On the theory of flat spacetime | Special relativity turns out to be more than coordinate transformations in
which the constancy of the speed of light plays the central role between two
inertial reference frames. Special relativity, in essence, is a theory of
four-dimensional flat spacetime. Euclidian space spans three of the spacetime's
dimensions a... | physics.gen-ph | special relativity turns out to be more than coordinate transformations in which the constancy of the speed of light plays the central role between two inertial reference frames special relativity in essence is a theory of fourdimensional flat spacetime euclidian space spans three of the spacetimes dimensions and time ... | [['special', 'relativity', 'turns', 'out', 'to', 'be', 'more', 'than', 'coordinate', 'transformations', 'in', 'which', 'the', 'constancy', 'of', 'the', 'speed', 'of', 'light', 'plays', 'the', 'central', 'role', 'between', 'two', 'inertial', 'reference', 'frames', 'special', 'relativity', 'in', 'essence', 'is', 'a', 'th... | [-0.14034074363455426, 0.14724690722337422, -0.1518456514884467, 0.059763173273845144, -0.10841960300548145, -0.1399935784910877, -0.03804297833210932, 0.31758243430298394, -0.216361996350595, -0.2736489843216707, 0.043190254369759574, -0.20133108917686443, -0.15915425663115457, 0.21764968799946544, -0.1267436970150671... |
706.1585 | A method for the resolution of the Jacobi equation Y''+RY = 0 on the
manifold Sp(2)/SU(2) | In this paper a method for the resolution of the differential equation of the
Jacobi vector fields in the manifold V1 = Sp(2)/SU(2) is exposed. These results
are applied to determine areas and volumes of geodesic spheres and balls.
| math.DG | in this paper a method for the resolution of the differential equation of the jacobi vector fields in the manifold v1 sp2su2 is exposed these results are applied to determine areas and volumes of geodesic spheres and balls | [['in', 'this', 'paper', 'a', 'method', 'for', 'the', 'resolution', 'of', 'the', 'differential', 'equation', 'of', 'the', 'jacobi', 'vector', 'fields', 'in', 'the', 'manifold', 'v1', 'sp2su2', 'is', 'exposed', 'these', 'results', 'are', 'applied', 'to', 'determine', 'areas', 'and', 'volumes', 'of', 'geodesic', 'spheres... | [-0.12246238709603613, 0.07814942107762436, -0.07209223503800663, 0.06084576387562462, -0.02410157845431083, -0.04924992860823467, -0.05590249887176764, 0.37253593411800023, -0.27861847147043495, -0.2791239185309088, 0.13020279820429514, -0.31675946420511686, -0.1342260596921315, 0.18883608462842735, -0.119246336027375... |
706.1586 | 21-cm synthesis observations of VIRGOHI 21 - a possible dark galaxy in
the Virgo Cluster | Many observations indicate that dark matter dominates the extra-galactic
Universe, yet no totally dark structure of galactic proportions has ever been
convincingly identified. Previously we have suggested that VIRGOHI 21, a 21-cm
source we found in the Virgo Cluster using Jodrell Bank, was a possible dark
galaxy beca... | astro-ph | many observations indicate that dark matter dominates the extragalactic universe yet no totally dark structure of galactic proportions has ever been convincingly identified previously we have suggested that virgohi 21 a 21cm source we found in the virgo cluster using jodrell bank was a possible dark galaxy because of i... | [['many', 'observations', 'indicate', 'that', 'dark', 'matter', 'dominates', 'the', 'extragalactic', 'universe', 'yet', 'no', 'totally', 'dark', 'structure', 'of', 'galactic', 'proportions', 'has', 'ever', 'been', 'convincingly', 'identified', 'previously', 'we', 'have', 'suggested', 'that', 'virgohi', '21', 'a', '21cm... | [-0.09121834766004455, 0.0855112117757683, -0.082449385977009, 0.09474723965176243, -0.12995192083290383, -0.09292556335550207, -0.012354496207162, 0.42920310035495474, -0.12479719213592719, -0.36067227662384216, 0.07691212932666819, -0.26068366312371144, -0.06228785072960476, 0.19123618228697506, 0.006186139214285972,... |
706.1587 | Resonances of the Quantum $\delta$-Kicked Accelerator | We report the observation of high order resonances of the quantum
$\delta$-kicked accelerator using a BEC kicked by a standing wave of light. The
signature of these resonances is the existence of quantum accelerator modes.
For the first time quantum accelerator modes were seen near 1/4 and 1/3 of the
Talbot time. Usi... | physics.atom-ph | we report the observation of high order resonances of the quantum deltakicked accelerator using a bec kicked by a standing wave of light the signature of these resonances is the existence of quantum accelerator modes for the first time quantum accelerator modes were seen near 14 and 13 of the talbot time using a bec en... | [['we', 'report', 'the', 'observation', 'of', 'high', 'order', 'resonances', 'of', 'the', 'quantum', 'deltakicked', 'accelerator', 'using', 'a', 'bec', 'kicked', 'by', 'a', 'standing', 'wave', 'of', 'light', 'the', 'signature', 'of', 'these', 'resonances', 'is', 'the', 'existence', 'of', 'quantum', 'accelerator', 'mode... | [-0.16762272948696416, 0.1765652075162197, -0.1220830095476134, 0.0349524256456247, -0.05320806296027087, -0.11982062347035141, 0.031829922622257964, 0.2920405582544651, -0.23707399235919435, -0.2864688050566598, 0.08359667227821464, -0.2881900690436522, -0.13549862437425775, 0.22151931587289622, 0.07225193928411984, 0... |
706.1588 | Detection of Gauss-Markov Random Fields with Nearest-Neighbor Dependency | The problem of hypothesis testing against independence for a Gauss-Markov
random field (GMRF) is analyzed. Assuming an acyclic dependency graph, an
expression for the log-likelihood ratio of detection is derived. Assuming
random placement of nodes over a large region according to the Poisson or
uniform distribution a... | cs.IT math.IT | the problem of hypothesis testing against independence for a gaussmarkov random field gmrf is analyzed assuming an acyclic dependency graph an expression for the loglikelihood ratio of detection is derived assuming random placement of nodes over a large region according to the poisson or uniform distribution and neares... | [['the', 'problem', 'of', 'hypothesis', 'testing', 'against', 'independence', 'for', 'a', 'gaussmarkov', 'random', 'field', 'gmrf', 'is', 'analyzed', 'assuming', 'an', 'acyclic', 'dependency', 'graph', 'an', 'expression', 'for', 'the', 'loglikelihood', 'ratio', 'of', 'detection', 'is', 'derived', 'assuming', 'random', ... | [-0.16092105442658067, 0.10170480924358484, -0.07541528402182918, 0.10601132051446117, -0.01456523143972915, -0.15564138868537086, 0.07090237407918232, 0.32661436233096397, -0.2522856721618714, -0.29711013199367486, 0.08284024067151431, -0.26992473175498444, -0.11249146888641497, 0.16750243476663645, -0.044607779801187... |
706.1589 | Quasiparticle Energies and Band Gaps of Graphene Nanoribbons | We present calculations of the quasiparticle energies and band gaps of
graphene nanoribbons (GNRs) carried out using a first-principles many-electron
Green's function approach within the GW approximation. Because of the
quasi-one-dimension nature of a GNR, electron-electron interaction effects due
to the enhanced scr... | cond-mat.mes-hall | we present calculations of the quasiparticle energies and band gaps of graphene nanoribbons gnrs carried out using a firstprinciples manyelectron greens function approach within the gw approximation because of the quasionedimension nature of a gnr electronelectron interaction effects due to the enhanced screened coulom... | [['we', 'present', 'calculations', 'of', 'the', 'quasiparticle', 'energies', 'and', 'band', 'gaps', 'of', 'graphene', 'nanoribbons', 'gnrs', 'carried', 'out', 'using', 'a', 'firstprinciples', 'manyelectron', 'greens', 'function', 'approach', 'within', 'the', 'gw', 'approximation', 'because', 'of', 'the', 'quasionedimen... | [-0.15580755878155203, 0.11110769674097272, -0.06962623750494623, 0.08669589306227862, 0.021800368372880092, -0.12749988654289734, 0.13387801289156248, 0.49037052530541336, -0.23773223339072005, -0.30852466926655986, -0.10989836737386544, -0.3032836372964084, -0.1471228958149864, 0.11714226226957346, 0.1059875352075323... |
706.159 | Kolmogorov condition near hyperbolic singularities of integrable
Hamiltonian systems | In this paper we show that, if an integrable Hamiltonian system admits a
nondegenerate hyperbolic singularity then it will satisfy the Kolmogorov
condegeneracy condition near that singularity (under a mild additional
condition, which is trivial if the singularity contains a fixed point)
| math.DS | in this paper we show that if an integrable hamiltonian system admits a nondegenerate hyperbolic singularity then it will satisfy the kolmogorov condegeneracy condition near that singularity under a mild additional condition which is trivial if the singularity contains a fixed point | [['in', 'this', 'paper', 'we', 'show', 'that', 'if', 'an', 'integrable', 'hamiltonian', 'system', 'admits', 'a', 'nondegenerate', 'hyperbolic', 'singularity', 'then', 'it', 'will', 'satisfy', 'the', 'kolmogorov', 'condegeneracy', 'condition', 'near', 'that', 'singularity', 'under', 'a', 'mild', 'additional', 'condition... | [-0.22045443702216555, 0.08970728061884563, -0.19894033534134306, 0.0810800153625811, -0.11568443745760838, -0.2676875908495631, -0.026743121192472557, 0.2966198897579821, -0.3064895351303787, -0.08754560035630697, 0.1299369779909484, -0.2951765210345024, -0.21116196236959317, 0.13934858034296735, -0.11810849900016697,... |
706.1591 | Hard diffraction and the Color Glass Condensate | Following the Good-and-Walker picture, hard diffraction in the
high-energy/small-x limit of QCD can be described in terms of eigenstates of
the scattering matrix off a Color Glass Condensate. From the CGC non-linear
evolution equations, it is then possible to derive the behavior of diffractive
cross-sections at small... | hep-ph | following the goodandwalker picture hard diffraction in the highenergysmallx limit of qcd can be described in terms of eigenstates of the scattering matrix off a color glass condensate from the cgc nonlinear evolution equations it is then possible to derive the behavior of diffractive crosssections at small x i discuss... | [['following', 'the', 'goodandwalker', 'picture', 'hard', 'diffraction', 'in', 'the', 'highenergysmallx', 'limit', 'of', 'qcd', 'can', 'be', 'described', 'in', 'terms', 'of', 'eigenstates', 'of', 'the', 'scattering', 'matrix', 'off', 'a', 'color', 'glass', 'condensate', 'from', 'the', 'cgc', 'nonlinear', 'evolution', '... | [-0.06848571278036587, 0.19083304363968118, -0.15159511838906578, 0.08547791699501908, -0.002702129753454337, -0.030344006021521867, -0.0013932040892541409, 0.3527692084511121, -0.25112309081790346, -0.2082165881902689, 0.04808837023844558, -0.3156719318783236, -0.10412952351191687, 0.10101230771073864, 0.0021123701839... |
706.1592 | A novel method for the evaluation of uncertainty in dose volume
histogram computation | Dose volume histograms are a useful tool in state-of-the-art radiotherapy
planning, and it is essential to be aware of their limitations. Dose
distributions computed by treatment planning systems are affected by several
sources of uncertainty such as algorithm limitations, measurement uncertainty
in the data used to ... | physics.med-ph | dose volume histograms are a useful tool in stateoftheart radiotherapy planning and it is essential to be aware of their limitations dose distributions computed by treatment planning systems are affected by several sources of uncertainty such as algorithm limitations measurement uncertainty in the data used to model th... | [['dose', 'volume', 'histograms', 'are', 'a', 'useful', 'tool', 'in', 'stateoftheart', 'radiotherapy', 'planning', 'and', 'it', 'is', 'essential', 'to', 'be', 'aware', 'of', 'their', 'limitations', 'dose', 'distributions', 'computed', 'by', 'treatment', 'planning', 'systems', 'are', 'affected', 'by', 'several', 'source... | [0.004701253379984149, 0.07475504585092467, -0.06394954319823111, 0.10883275097697111, -0.011059454034353272, -0.10305504412550864, 0.06263281992439346, 0.4356588310392326, -0.18020691353887355, -0.33574686598564896, 0.08849378762103782, -0.2998478402329289, -0.07380727533907101, 0.2187170332602771, -0.1491792867558875... |
706.1593 | Groups of galaxies in the SDSS Data Release 5. A group-finder and a
catalogue | We extract groups of galaxies from the SDSS Data Release 5 with the purpose
of studying the supercluster-void network and environmental properties of
groups therein. We use a modified friends-of-friends (FoF) method with adopted
variable linking length in transverse and radial direction to eliminate
selection effects... | astro-ph | we extract groups of galaxies from the sdss data release 5 with the purpose of studying the superclustervoid network and environmental properties of groups therein we use a modified friendsoffriends fof method with adopted variable linking length in transverse and radial direction to eliminate selection effects and to ... | [['we', 'extract', 'groups', 'of', 'galaxies', 'from', 'the', 'sdss', 'data', 'release', '5', 'with', 'the', 'purpose', 'of', 'studying', 'the', 'superclustervoid', 'network', 'and', 'environmental', 'properties', 'of', 'groups', 'therein', 'we', 'use', 'a', 'modified', 'friendsoffriends', 'fof', 'method', 'with', 'ado... | [-0.08811107794270001, 0.10267312346367305, -0.08403754361855707, 0.0717105704722349, -0.11996839100297178, -0.050593429762227214, 0.08022686527976025, 0.4140395157436317, -0.232426926343232, -0.3648222783349652, 0.0729003004689569, -0.29528190622047473, -0.03084430040428992, 0.19857812192769045, -0.020456912147449907,... |
706.1594 | A uniform Sobolev inequality under Ricci flow | Let ${\bf M}$ be a compact Riemannian manifold and the metrics $g=g(t)$
evolve by the Ricci flow. We prove the following result. The Sobolev imbedding
by Aubin or Hebey, perturbed by a scalar curvature term and modulo sharpness of
constants, holds uniformly for $({\bf M}, g(t))$ for all time if the Ricci flow
exists ... | math.DG | let bf m be a compact riemannian manifold and the metrics ggt evolve by the ricci flow we prove the following result the sobolev imbedding by aubin or hebey perturbed by a scalar curvature term and modulo sharpness of constants holds uniformly for bf m gt for all time if the ricci flow exists for all time and if the ri... | [['let', 'bf', 'm', 'be', 'a', 'compact', 'riemannian', 'manifold', 'and', 'the', 'metrics', 'ggt', 'evolve', 'by', 'the', 'ricci', 'flow', 'we', 'prove', 'the', 'following', 'result', 'the', 'sobolev', 'imbedding', 'by', 'aubin', 'or', 'hebey', 'perturbed', 'by', 'a', 'scalar', 'curvature', 'term', 'and', 'modulo', 's... | [-0.18755940062304338, 0.11384364400804597, -0.10945771515724205, 0.04775553575960831, -0.08971116363203951, -0.18300311745898354, -0.09315868310541624, 0.32346816722835814, -0.2869614960337501, -0.18704222125843878, 0.15519481003173582, -0.24641025644682701, -0.07919867147824594, 0.18063482440608952, -0.10511627516576... |
706.1595 | Correlations between X-ray Spectral and Timing Characteristics in Cyg
X-2 | Correlations between the quasi-periodic oscillations (QPOs) and the spectral
power-law index have been reported for a number of black hole candidate sources
and for four neutron star (NS) sources, 4U 0614+09, 4U 1608-52, 4U 1728-34 and
Sco X-1. An examination of QPO frequencies and index relationship in Cyg X-2 is
re... | astro-ph | correlations between the quasiperiodic oscillations qpos and the spectral powerlaw index have been reported for a number of black hole candidate sources and for four neutron star ns sources 4u 061409 4u 160852 4u 172834 and sco x1 an examination of qpo frequencies and index relationship in cyg x2 is reported herein the... | [['correlations', 'between', 'the', 'quasiperiodic', 'oscillations', 'qpos', 'and', 'the', 'spectral', 'powerlaw', 'index', 'have', 'been', 'reported', 'for', 'a', 'number', 'of', 'black', 'hole', 'candidate', 'sources', 'and', 'for', 'four', 'neutron', 'star', 'ns', 'sources', '4u', '061409', '4u', '160852', '4u', '17... | [-0.0921283372512787, 0.17375177970890907, -0.03736328401925565, 0.12350763782314345, -0.08471164450409117, -0.16732680874201591, 0.09816264130529903, 0.43446557136084984, -0.18227966721711691, -0.3403214654446673, 0.05066285625336662, -0.35878508124579356, 0.006725791324343946, 0.2508974087229935, -0.01880787127982657... |
706.1596 | Large-Scale Structure of Short-Lived Lyman\alpha Emitters | Recently discovered large-scale structure of Ly\alpha Emitters (LAEs) raises
a novel challenge to the cold dark matter (CDM) cosmology. The structure is
extended over more than 50 Mpc at redshift z=3.1, and exhibits a considerably
weak angular correlation. Such properties of LAE distributions appear to be
incompatibl... | astro-ph | recently discovered largescale structure of lyalpha emitters laes raises a novel challenge to the cold dark matter cdm cosmology the structure is extended over more than 50 mpc at redshift z31 and exhibits a considerably weak angular correlation such properties of lae distributions appear to be incompatible with the st... | [['recently', 'discovered', 'largescale', 'structure', 'of', 'lyalpha', 'emitters', 'laes', 'raises', 'a', 'novel', 'challenge', 'to', 'the', 'cold', 'dark', 'matter', 'cdm', 'cosmology', 'the', 'structure', 'is', 'extended', 'over', 'more', 'than', '50', 'mpc', 'at', 'redshift', 'z31', 'and', 'exhibits', 'a', 'conside... | [-0.05832890624282654, 0.10842309443779835, -0.07531183007423108, 0.15933646032098317, -0.0675579201520943, -0.0862996427751169, 0.002755135886666433, 0.42262646610417015, -0.13424382467424814, -0.36493454580081675, -0.013465213498509512, -0.29043440906183293, -0.04665099156611576, 0.15989788066902447, 0.03736145015260... |
706.1597 | Graphene Spin Transistor | Graphitic nanostructures, e.g. carbon nanotubes (CNT) and graphene, have been
proposed as ideal materials for spin conduction[1-7]; they have long electronic
mean free paths[8] and small spin-orbit coupling[9], hence are expected to have
very long spin-scattering times. In addition, spin injection and detection in
gr... | cond-mat.mes-hall | graphitic nanostructures eg carbon nanotubes cnt and graphene have been proposed as ideal materials for spin conduction17 they have long electronic mean free paths8 and small spinorbit coupling9 hence are expected to have very long spinscattering times in addition spin injection and detection in graphene opens new oppo... | [['graphitic', 'nanostructures', 'eg', 'carbon', 'nanotubes', 'cnt', 'and', 'graphene', 'have', 'been', 'proposed', 'as', 'ideal', 'materials', 'for', 'spin', 'conduction17', 'they', 'have', 'long', 'electronic', 'mean', 'free', 'paths8', 'and', 'small', 'spinorbit', 'coupling9', 'hence', 'are', 'expected', 'to', 'have... | [-0.16613475677345926, 0.20468639583056067, 0.004270509716803671, -0.025839959469405895, -0.008362425910123188, -0.2251061995394845, 0.041629308359103, 0.45316952757590206, -0.26453161452639296, -0.33914423745838884, -0.002403803809598775, -0.33155098526840965, -0.10547039579643029, 0.19981986629208615, 0.0372815275439... |
706.1598 | Bounds on the multipartite entanglement of superpositions | We derive the lower and upper bounds on the entanglement of a given
multipartite superposition state in terms of the entanglement of the states
being superposed. The first entanglement measure we use is the geometric
measure, and the second is the q-squashed entanglement. These bounds allow us
to estimate the amount ... | quant-ph | we derive the lower and upper bounds on the entanglement of a given multipartite superposition state in terms of the entanglement of the states being superposed the first entanglement measure we use is the geometric measure and the second is the qsquashed entanglement these bounds allow us to estimate the amount of the... | [['we', 'derive', 'the', 'lower', 'and', 'upper', 'bounds', 'on', 'the', 'entanglement', 'of', 'a', 'given', 'multipartite', 'superposition', 'state', 'in', 'terms', 'of', 'the', 'entanglement', 'of', 'the', 'states', 'being', 'superposed', 'the', 'first', 'entanglement', 'measure', 'we', 'use', 'is', 'the', 'geometric... | [-0.13995280692745982, 0.1909983742271403, -0.1290623185310611, 0.08106299785370204, 0.014290495653097568, -0.13769932202749738, 0.06402414337437796, 0.30917734451788037, -0.2176379304789742, -0.2825987850266852, 0.10163069787085988, -0.2897963514061351, -0.05966765218870837, 0.17511291095319106, -0.05706784729600737, ... |
706.1599 | Thermodynamic Interpretation of the Field Equations of BTZ Charged Black
Hole near the Horizon | As is already known, a spacetime horizon acts like a boundary of a thermal
system an we can associate with it notions as temperature and entropy.
Following the work of M. Akbar, in this paper we will show how it is possible
to interpret the field equation of a charged BTZ black hole near horizon as a
thermodynamic id... | gr-qc | as is already known a spacetime horizon acts like a boundary of a thermal system an we can associate with it notions as temperature and entropy following the work of m akbar in this paper we will show how it is possible to interpret the field equation of a charged btz black hole near horizon as a thermodynamic identity... | [['as', 'is', 'already', 'known', 'a', 'spacetime', 'horizon', 'acts', 'like', 'a', 'boundary', 'of', 'a', 'thermal', 'system', 'an', 'we', 'can', 'associate', 'with', 'it', 'notions', 'as', 'temperature', 'and', 'entropy', 'following', 'the', 'work', 'of', 'm', 'akbar', 'in', 'this', 'paper', 'we', 'will', 'show', 'ho... | [-0.1605414550811533, 0.11750579349116437, -0.09756600394123985, 0.08179416600489609, -0.07952726407537378, -0.15364206096117375, -0.004332182997767563, 0.3007981122461378, -0.2089928570203483, -0.2834217161183015, 0.09548783234085247, -0.36642851656483066, -0.11986148938216189, 0.17964453850772671, -0.0780616004060032... |
706.16 | Measurement of the production of charged pions by protons on a tantalum
target | A measurement of the double-differential cross-section for the production of
charged pions in proton--tantalum collisions emitted at large angles from the
incoming beam direction is presented. The data were taken in 2002 with the HARP
detector in the T9 beam line of the CERN PS. The pions were produced by proton
beam... | hep-ex | a measurement of the doubledifferential crosssection for the production of charged pions in protontantalum collisions emitted at large angles from the incoming beam direction is presented the data were taken in 2002 with the harp detector in the t9 beam line of the cern ps the pions were produced by proton beams in a m... | [['a', 'measurement', 'of', 'the', 'doubledifferential', 'crosssection', 'for', 'the', 'production', 'of', 'charged', 'pions', 'in', 'protontantalum', 'collisions', 'emitted', 'at', 'large', 'angles', 'from', 'the', 'incoming', 'beam', 'direction', 'is', 'presented', 'the', 'data', 'were', 'taken', 'in', '2002', 'with'... | [-0.07341295510876733, 0.2648799412523254, -0.06727179978639843, 0.03337470928451313, 0.03867682895093806, -0.12131119925184494, -0.02591474101934423, 0.39664230497283304, -0.16254678409861034, -0.3564443158893249, -0.032366363717736595, -0.3694986778184071, 0.1405604078531918, 0.20227208099294153, 0.05811350741901268,... |
706.1601 | Discovery of 11 New T Dwarfs in the Two Micron All-Sky Survey, Including
a Possible L/T Transition Binary | We present the discovery of 11 new T dwarfs, found during the course of a
photometric survey for mid-to-late T dwarfs in the 2MASS Point Source Catalog
and from a proper motion selected sample of ultracool dwarfs in the 2MASS
Working Database. Using the NASA Infrared Telescope Facility SpeX spectrograph,
we obtained ... | astro-ph | we present the discovery of 11 new t dwarfs found during the course of a photometric survey for midtolate t dwarfs in the 2mass point source catalog and from a proper motion selected sample of ultracool dwarfs in the 2mass working database using the nasa infrared telescope facility spex spectrograph we obtained lowreso... | [['we', 'present', 'the', 'discovery', 'of', '11', 'new', 't', 'dwarfs', 'found', 'during', 'the', 'course', 'of', 'a', 'photometric', 'survey', 'for', 'midtolate', 't', 'dwarfs', 'in', 'the', '2mass', 'point', 'source', 'catalog', 'and', 'from', 'a', 'proper', 'motion', 'selected', 'sample', 'of', 'ultracool', 'dwarfs... | [-0.028180184642836566, 0.11860647741819516, -0.09464196342504488, 0.07238799468637919, -0.18039237650595985, -0.12201235144950297, 0.15027914293067607, 0.39719667597388736, -0.156531741675132, -0.4203458111091726, 0.038248283931111196, -0.343038009706533, -0.0006083104287928127, 0.21377255446313195, -0.090455399156186... |
706.1602 | The vanishing of the contact invariant in the presence of torsion | We prove that the Ozsvath-Szabo contact invariant of a closed contact
3-manifold with positive Giroux torsion vanishes.
| math.GT | we prove that the ozsvathszabo contact invariant of a closed contact 3manifold with positive giroux torsion vanishes | [['we', 'prove', 'that', 'the', 'ozsvathszabo', 'contact', 'invariant', 'of', 'a', 'closed', 'contact', '3manifold', 'with', 'positive', 'giroux', 'torsion', 'vanishes']] | [-0.48229142563307986, 0.15399165478918483, -0.15315562979701688, 0.09646013222963494, -0.16530224680900574, -0.3713551531545818, -0.04170155963476967, 0.3050706504898913, -0.28778255248770995, -0.1966844469527988, -0.08625999720328871, -0.2814564173493315, -0.24824468427173355, 0.1176635506836807, -0.1741222497623633,... |
706.1603 | Solutions of Bethe-Salpter equations in QED3 | To understand the mechanism of the fermion pair and fermion-antifermion pair
condensation,the solutions of Bethe-Salpeter equation in QED$_{3}$ is
examined.In the ladder appoximation our solution for the axial-scalar is
consistent with Ward-Takahashi-identity for the axial vector currents.Since the
massless scalar-ve... | hep-th | to understand the mechanism of the fermion pair and fermionantifermion pair condensationthe solutions of bethesalpeter equation in qed_3 is examinedin the ladder appoximation our solution for the axialscalar is consistent with wardtakahashiidentity for the axial vector currentssince the massless scalarvector sector is ... | [['to', 'understand', 'the', 'mechanism', 'of', 'the', 'fermion', 'pair', 'and', 'fermionantifermion', 'pair', 'condensationthe', 'solutions', 'of', 'bethesalpeter', 'equation', 'in', 'qed_3', 'is', 'examinedin', 'the', 'ladder', 'appoximation', 'our', 'solution', 'for', 'the', 'axialscalar', 'is', 'consistent', 'with'... | [-0.16524987583979964, 0.13978426025249063, -0.05770140221808106, 0.1024937250977382, -0.11371845203917473, -0.19740220697131008, -0.02866576666710898, 0.30657174591906367, -0.23685203047469258, -0.2650886170566082, 0.027435309548163787, -0.3153754891641438, -0.06990702548064291, 0.1216712218336761, 0.05905433637759415... |
706.1604 | Renormalized Newtonian Cosmic Evolution with Primordial Non-Gaussianity | We study Newtonian cosmological perturbation theory from a field theoretical
point of view. We derive a path integral representation for the cosmological
evolution of stochastic fluctuations. Our main result is the closed form of the
generating functional valid for any initial statistics. Moreover, we extend the
reno... | astro-ph gr-qc hep-th | we study newtonian cosmological perturbation theory from a field theoretical point of view we derive a path integral representation for the cosmological evolution of stochastic fluctuations our main result is the closed form of the generating functional valid for any initial statistics moreover we extend the renormaliz... | [['we', 'study', 'newtonian', 'cosmological', 'perturbation', 'theory', 'from', 'a', 'field', 'theoretical', 'point', 'of', 'view', 'we', 'derive', 'a', 'path', 'integral', 'representation', 'for', 'the', 'cosmological', 'evolution', 'of', 'stochastic', 'fluctuations', 'our', 'main', 'result', 'is', 'the', 'closed', 'f... | [-0.1528614738844335, 0.10808456315577496, -0.1585484393686056, 0.10971944358758629, -0.08737806109897793, -0.056835327494889495, -0.02312380371708423, 0.28864144878089426, -0.2389024570863694, -0.2449645152837038, 0.05494577652495354, -0.2615280035585165, -0.15855295066908, 0.18243944344110788, 0.0029736366854049264, ... |
706.1605 | Local Well-Posedness of Dynamics of Viscous Gaseous Stars | We establish the local in time well-posedness of strong solutions to the
vacuum free boundary problem of the compressible Navier-Stokes-Poisson system
in the spherically symmetric and isentropic motion. Our result captures the
physical vacuum boundary behavior of the Lane-Emden star configurations for all
adiabatic e... | math.AP math-ph math.MP | we establish the local in time wellposedness of strong solutions to the vacuum free boundary problem of the compressible navierstokespoisson system in the spherically symmetric and isentropic motion our result captures the physical vacuum boundary behavior of the laneemden star configurations for all adiabatic exponent... | [['we', 'establish', 'the', 'local', 'in', 'time', 'wellposedness', 'of', 'strong', 'solutions', 'to', 'the', 'vacuum', 'free', 'boundary', 'problem', 'of', 'the', 'compressible', 'navierstokespoisson', 'system', 'in', 'the', 'spherically', 'symmetric', 'and', 'isentropic', 'motion', 'our', 'result', 'captures', 'the',... | [-0.22186786838703684, 0.08946018303847975, -0.083486810238618, 0.04836116638034582, -0.02843543886103564, -0.09902961490054925, -0.05462595379600922, 0.2442260166345578, -0.26134225477774936, -0.22999622945984205, 0.12185311240351035, -0.22291416989432442, -0.04715528978655736, 0.13895493663019604, -0.0405825047236349... |
706.1606 | Quantum Dynamical Algebra SU(1,1) in One-Dimensional Exactly Solvable
Potentials | We mainly explore the linear algebraic structure like SU(2) or SU(1,1) of the
shift operators for some one-dimensional exactly solvable potentials in this
paper. During such process, a set of method based on original diagonalizing
technique is presented to construct those suitable operator elements, J0, J_\pm
that sa... | quant-ph | we mainly explore the linear algebraic structure like su2 or su11 of the shift operators for some onedimensional exactly solvable potentials in this paper during such process a set of method based on original diagonalizing technique is presented to construct those suitable operator elements j0 j_pm that satisfy su2 or ... | [['we', 'mainly', 'explore', 'the', 'linear', 'algebraic', 'structure', 'like', 'su2', 'or', 'su11', 'of', 'the', 'shift', 'operators', 'for', 'some', 'onedimensional', 'exactly', 'solvable', 'potentials', 'in', 'this', 'paper', 'during', 'such', 'process', 'a', 'set', 'of', 'method', 'based', 'on', 'original', 'diagon... | [-0.08117814888749775, 0.09554649409963875, -0.05483683309048993, 0.06630534718589991, -0.12484883902456008, -0.1623076578237217, -0.0009015828883904662, 0.405932101244862, -0.3040405086971618, -0.21656482863063747, 0.08268993480974254, -0.2725401905591826, -0.15634497708792017, 0.15203925751376193, -0.0228899413077915... |
706.1607 | Partitions with independent iterates in random dynamical systems | Consider an invertible measure-preserving transformation of a probability
space. A finite partition of the space is called weakly independent if there
are infinitely many images of this partition under powers of the transformation
that are jointly independent. Krengel proved that a transformation is weakly
mixing if ... | math.DS math.AC math.AG math.AP | consider an invertible measurepreserving transformation of a probability space a finite partition of the space is called weakly independent if there are infinitely many images of this partition under powers of the transformation that are jointly independent krengel proved that a transformation is weakly mixing if and o... | [['consider', 'an', 'invertible', 'measurepreserving', 'transformation', 'of', 'a', 'probability', 'space', 'a', 'finite', 'partition', 'of', 'the', 'space', 'is', 'called', 'weakly', 'independent', 'if', 'there', 'are', 'infinitely', 'many', 'images', 'of', 'this', 'partition', 'under', 'powers', 'of', 'the', 'transfo... | [-0.1397888742565633, 0.2508082377114098, -0.07640540819773649, 0.05836784292354268, -0.045440606411269055, -0.15493518892958008, 0.00911174663045305, 0.34658360536745253, -0.31002172748459145, -0.17339867411894686, 0.13130488001340207, -0.2821377693437674, -0.14919939135112106, 0.17579620800902473, -0.0616167293405754... |
706.1608 | Magneto-optical Trapping of Cadmium | We report the laser-cooling and confinement of Cd atoms in a magneto-optical
trap, and characterize the loading process from the background Cd vapor. The
trapping laser drives the 1S0-1P1 transition at 229 nm in this two-electron
atom and also photoionizes atoms directly from the 1P1 state. This
photoionization overw... | physics.atom-ph | we report the lasercooling and confinement of cd atoms in a magnetooptical trap and characterize the loading process from the background cd vapor the trapping laser drives the 1s01p1 transition at 229 nm in this twoelectron atom and also photoionizes atoms directly from the 1p1 state this photoionization overwhelms the... | [['we', 'report', 'the', 'lasercooling', 'and', 'confinement', 'of', 'cd', 'atoms', 'in', 'a', 'magnetooptical', 'trap', 'and', 'characterize', 'the', 'loading', 'process', 'from', 'the', 'background', 'cd', 'vapor', 'the', 'trapping', 'laser', 'drives', 'the', '1s01p1', 'transition', 'at', '229', 'nm', 'in', 'this', '... | [-0.014875335899251763, 0.21468033907955053, 0.007973171682322337, -0.029907548765589136, 0.07716426940294363, -0.1706251955180559, 0.1182046823443905, 0.43935386055419523, -0.24249033750690802, -0.254605656269417, -0.04215360678086478, -0.3294338125321496, 0.007391074031431188, 0.1447215593690353, 0.04654861641021305,... |
706.1609 | Phase transitions in coupled two dimensional XY systems with spatial
anisotropy | We study phase transitions of coupled two dimensional XY systems with spatial
anisotropy and $U(1) \times \mathbb{Z}_2$ symmetry, motivated by spinless
bosonic atoms trapped in square optical lattice on the metastable first excited
$p-$level orbitals with anisotropic hopping amplitudes. The phase transitions
of the s... | cond-mat.str-el cond-mat.soft | we study phase transitions of coupled two dimensional xy systems with spatial anisotropy and u1 times mathbbz_2 symmetry motivated by spinless bosonic atoms trapped in square optical lattice on the metastable first excited plevel orbitals with anisotropic hopping amplitudes the phase transitions of the system are gener... | [['we', 'study', 'phase', 'transitions', 'of', 'coupled', 'two', 'dimensional', 'xy', 'systems', 'with', 'spatial', 'anisotropy', 'and', 'u1', 'times', 'mathbbz_2', 'symmetry', 'motivated', 'by', 'spinless', 'bosonic', 'atoms', 'trapped', 'in', 'square', 'optical', 'lattice', 'on', 'the', 'metastable', 'first', 'excite... | [-0.1776133957164428, 0.3364026489642096, -0.015812608160993363, 0.027490007506288893, -0.00024287288427097666, -0.19377007828283627, 0.06535983307130502, 0.3648221178796241, -0.22953854429337764, -0.22950979397195367, 0.06455978502125884, -0.3287619700494626, -0.07551104206987451, 0.08145910000173062, 0.09596185966763... |
706.161 | Complex ferromagnetic state and magnetocaloric effect in single
crystalline Nd_{0.7}Sr_{0.3}MnO_{3} | The magnetocaloric effect in single crystalline Nd_{0.7}Sr_{0.3}MnO_{3} is
investigated by measuring the field-induced adiabatic change in temperature
which reveals a single negative peak around 130 K well below the Curie
temperature (T_C=203 K). In order to understand this unusual magnetocaloric
effect, we invoke th... | cond-mat.mtrl-sci | the magnetocaloric effect in single crystalline nd_07sr_03mno_3 is investigated by measuring the fieldinduced adiabatic change in temperature which reveals a single negative peak around 130 k well below the curie temperature t_c203 k in order to understand this unusual magnetocaloric effect we invoke the reported 55mn ... | [['the', 'magnetocaloric', 'effect', 'in', 'single', 'crystalline', 'nd_07sr_03mno_3', 'is', 'investigated', 'by', 'measuring', 'the', 'fieldinduced', 'adiabatic', 'change', 'in', 'temperature', 'which', 'reveals', 'a', 'single', 'negative', 'peak', 'around', '130', 'k', 'well', 'below', 'the', 'curie', 'temperature', ... | [-0.18191841294948788, 0.2390173202687908, -0.06730877722633614, 0.02224285068516385, -0.06236040999898486, -0.10222829282685793, 0.08638501138821673, 0.35141171813815186, -0.2679048832371938, -0.3203173667299662, 0.011005335429636427, -0.3231804793660375, -0.10536558369322004, 0.15920723081573093, 0.07901159653828728,... |
706.1611 | Calcium and synaptic dynamics underlying reverberatory activity in
neuronal networks | Persistent activity is postulated to drive neural network plasticity and
learning. To investigate its underlying cellular mechanisms, we developed a
biophysically tractable model that explains the emergence, sustenance, and
eventual termination of short-term persistent activity. Using the model, we
reproduced the fea... | q-bio.NC q-bio.PE | persistent activity is postulated to drive neural network plasticity and learning to investigate its underlying cellular mechanisms we developed a biophysically tractable model that explains the emergence sustenance and eventual termination of shortterm persistent activity using the model we reproduced the features of ... | [['persistent', 'activity', 'is', 'postulated', 'to', 'drive', 'neural', 'network', 'plasticity', 'and', 'learning', 'to', 'investigate', 'its', 'underlying', 'cellular', 'mechanisms', 'we', 'developed', 'a', 'biophysically', 'tractable', 'model', 'that', 'explains', 'the', 'emergence', 'sustenance', 'and', 'eventual',... | [-0.15134586476349304, 0.15301731579054575, -0.017534949911334356, 0.08460137047599808, -0.037769060365981155, -0.1496120482379175, 0.0702770475480329, 0.4192905551971086, -0.26283959075422486, -0.27135627210101626, 0.0712362692089404, -0.2105663680070963, -0.2665811557723258, 0.1701868043402982, -0.0642855850499548, -... |
706.1612 | Nonlocal effect on the magnetic penetration depth in multigapped
superconductors | A brief discussion is given on the nonlocal effect in multigapped
superconductivity. It is pointed out that the effective magnetic penetration
depth at lower external fields may be reduced by the nonlocal effect associated
with the presence of small energy gap. A crude estimation of the effect in
double gap system is... | cond-mat.supr-con | a brief discussion is given on the nonlocal effect in multigapped superconductivity it is pointed out that the effective magnetic penetration depth at lower external fields may be reduced by the nonlocal effect associated with the presence of small energy gap a crude estimation of the effect in double gap system is pro... | [['a', 'brief', 'discussion', 'is', 'given', 'on', 'the', 'nonlocal', 'effect', 'in', 'multigapped', 'superconductivity', 'it', 'is', 'pointed', 'out', 'that', 'the', 'effective', 'magnetic', 'penetration', 'depth', 'at', 'lower', 'external', 'fields', 'may', 'be', 'reduced', 'by', 'the', 'nonlocal', 'effect', 'associa... | [-0.14529725761404114, 0.1571887050097483, -0.05022732410875578, 0.0762201420231057, -0.06238053147754972, -0.11630410463031796, 0.07296511015692164, 0.3326429130420798, -0.24974439594717252, -0.3359255589663036, 0.08481590270382604, -0.30420240068009924, -0.09045634070588719, 0.22171987291602863, -0.02620460053107568,... |
706.1613 | Supersymmetric Construction of three-dimensional isospectral systems | Three-dimensional isospectral systems are constructed using the framework of
supersymmetric quantum mechanics. In case the supercharge of first order in
momentum is used, it is proved that the constructed systems reduce to a trivial
generalization of one-dimensional systems. In case the second order supercharge
is us... | quant-ph hep-th math-ph math.MP | threedimensional isospectral systems are constructed using the framework of supersymmetric quantum mechanics in case the supercharge of first order in momentum is used it is proved that the constructed systems reduce to a trivial generalization of onedimensional systems in case the second order supercharge is used nont... | [['threedimensional', 'isospectral', 'systems', 'are', 'constructed', 'using', 'the', 'framework', 'of', 'supersymmetric', 'quantum', 'mechanics', 'in', 'case', 'the', 'supercharge', 'of', 'first', 'order', 'in', 'momentum', 'is', 'used', 'it', 'is', 'proved', 'that', 'the', 'constructed', 'systems', 'reduce', 'to', 'a... | [-0.14396989864941973, 0.09354954751996467, -0.026325509740182988, 0.09294556066743098, -0.023809662626053277, -0.1628768445762734, -0.09923802359620683, 0.3127968943355462, -0.21845622117129657, -0.24176153250468466, 0.09112913562477423, -0.27546779668101895, -0.20427700318396091, 0.21928015236671156, -0.0748281041339... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.