id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.143 | On the Derivatives of Central Loops | The right(left) derivative, $a^{-1},e-$ and $e,a^{-1}-$ isotopes of a C-loop
are shown to be C-loops. Furthermore, for a central loop $(L,F)$, it is shown
that $\big\{F,F^{a^{-1}},F_{a^{-1},e}\big\}$ and
$\big\{F,F_{a^{-1}},F_{e,a^{-1}}\big\}$ are systems of isotopic C-loops that
obey a form of generalized distributi... | math.GM | the rightleft derivative a1e and ea1 isotopes of a cloop are shown to be cloops furthermore for a central loop lf it is shown that bigffa1f_a1ebig and bigff_a1f_ea1big are systems of isotopic cloops that obey a form of generalized distributive law quasigroup isotopes lotimes and lominus of a loop ltheta and its parastr... | [['the', 'rightleft', 'derivative', 'a1e', 'and', 'ea1', 'isotopes', 'of', 'a', 'cloop', 'are', 'shown', 'to', 'be', 'cloops', 'furthermore', 'for', 'a', 'central', 'loop', 'lf', 'it', 'is', 'shown', 'that', 'bigffa1f_a1ebig', 'and', 'bigff_a1f_ea1big', 'are', 'systems', 'of', 'isotopic', 'cloops', 'that', 'obey', 'a',... | [-0.12602641674207657, 0.18591890568911498, -0.06727697446123264, 0.07959772343123664, -0.014847083178340523, -0.19104471425193228, -0.015170273861648249, 0.3973261466848531, -0.27639523380535785, -0.1710521591012366, 0.12263417029004943, -0.2990468083963996, -0.11389517743633146, 0.17880040202622435, -0.06941207358613... |
707.1431 | Gravitational Field of Spherical Branes | The warped solution of Einstein's equations corresponding to the spherical
brane in five-dimensional AdS is considered. This metric represents interiors
of black holes on both sides of the brane and can provide gravitational
trapping of physical fields on the shell. It is found the analytic form of the
coordinate tra... | gr-qc astro-ph hep-th | the warped solution of einsteins equations corresponding to the spherical brane in fivedimensional ads is considered this metric represents interiors of black holes on both sides of the brane and can provide gravitational trapping of physical fields on the shell it is found the analytic form of the coordinate transform... | [['the', 'warped', 'solution', 'of', 'einsteins', 'equations', 'corresponding', 'to', 'the', 'spherical', 'brane', 'in', 'fivedimensional', 'ads', 'is', 'considered', 'this', 'metric', 'represents', 'interiors', 'of', 'black', 'holes', 'on', 'both', 'sides', 'of', 'the', 'brane', 'and', 'can', 'provide', 'gravitational... | [-0.16698773362113978, 0.1024567880209933, -0.06625607937477591, 0.09393527357593137, -0.09859094667782108, -0.1120851416287295, -0.06823259971910313, 0.3211649926170037, -0.1331835871227504, -0.24918772234173303, 0.061104921795417336, -0.29744270416709145, -0.11179553118293707, 0.15648208042277087, -0.0453021620253749... |
707.1432 | Sequential products in effect categories | A new categorical framework is provided for dealing with multiple arguments
in a programming language with effects, for example in a language with
imperative features. Like related frameworks (Monads, Arrows, Freyd
categories), we distinguish two kinds of functions. In addition, we also
distinguish two kinds of equat... | math.CT cs.PL | a new categorical framework is provided for dealing with multiple arguments in a programming language with effects for example in a language with imperative features like related frameworks monads arrows freyd categories we distinguish two kinds of functions in addition we also distinguish two kinds of equations then w... | [['a', 'new', 'categorical', 'framework', 'is', 'provided', 'for', 'dealing', 'with', 'multiple', 'arguments', 'in', 'a', 'programming', 'language', 'with', 'effects', 'for', 'example', 'in', 'a', 'language', 'with', 'imperative', 'features', 'like', 'related', 'frameworks', 'monads', 'arrows', 'freyd', 'categories', '... | [-0.0669926926003475, 0.043091066347092, -0.1185026420157795, 0.17909321010014728, -0.12252520446322467, -0.18618184101988414, -0.011438280294992421, 0.34701047225022, -0.31904373078386444, -0.2880325072175382, 0.054843884581810255, -0.2643028747663361, -0.17777471141399523, 0.23140643406536823, -0.10832479679466862, -... |
707.1433 | Population III stars: hidden or disappeared ? | A PopIII/Pop II transition from massive to normal stars is predicted to occur
when the metallicity of the star forming gas crosses the critical range Z_cr =
10^(-5 +/- 1) Z_sun. To investigate the cosmic implications of such process we
use numerical simulations which follow the evolution, metal enrichment and
energy ... | astro-ph | a popiiipop ii transition from massive to normal stars is predicted to occur when the metallicity of the star forming gas crosses the critical range z_cr 105 1 z_sun to investigate the cosmic implications of such process we use numerical simulations which follow the evolution metal enrichment and energy deposition of b... | [['a', 'popiiipop', 'ii', 'transition', 'from', 'massive', 'to', 'normal', 'stars', 'is', 'predicted', 'to', 'occur', 'when', 'the', 'metallicity', 'of', 'the', 'star', 'forming', 'gas', 'crosses', 'the', 'critical', 'range', 'z_cr', '105', '1', 'z_sun', 'to', 'investigate', 'the', 'cosmic', 'implications', 'of', 'such... | [-0.06266231978993526, 0.21544683896140643, 0.013107270965257944, 0.12493198319168448, -0.053275287327603935, -0.09299071007644978, 0.12359100447357291, 0.37373457244718394, -0.19900065348983484, -0.32648428798900486, 0.05711230625711529, -0.26505156900565335, 0.006240814184969933, 0.1233845364807521, 0.024963601934986... |
707.1434 | Spectroscopy, upconversion dynamics, and applications of Er3+-doped
low-phonon materials | In this work I summarize some of the recent work carried out by our group on
the upconversion dynamics of Er3+-doped potassium lead halide crystals, which
possess very small phonons and present very efficient blue and green
upconversion. Furthermore, a non-conventional application of these RE-doped
low-phonon materia... | cond-mat.other cond-mat.mtrl-sci | in this work i summarize some of the recent work carried out by our group on the upconversion dynamics of er3doped potassium lead halide crystals which possess very small phonons and present very efficient blue and green upconversion furthermore a nonconventional application of these redoped lowphonon materials in opti... | [['in', 'this', 'work', 'i', 'summarize', 'some', 'of', 'the', 'recent', 'work', 'carried', 'out', 'by', 'our', 'group', 'on', 'the', 'upconversion', 'dynamics', 'of', 'er3doped', 'potassium', 'lead', 'halide', 'crystals', 'which', 'possess', 'very', 'small', 'phonons', 'and', 'present', 'very', 'efficient', 'blue', 'a... | [-0.07246374841913795, 0.17182130520590222, -0.05044335487540453, -0.012105799661814952, -0.04945257217640084, -0.1690041161581086, 0.10049292131533058, 0.45711734838998663, -0.21069977071154147, -0.23124497450995618, 0.06794275846466637, -0.27472171234862447, -0.18281024766754575, 0.24266497866035655, -0.0206929286874... |
707.1435 | On Isotopic Characterization of Central Loops | The representation sets of central loops are investigated and the results
obtained are used to construct a finite C-loop. It is shown that for certain
types of isotopisms, the central identities are isotopic invariant.
| math.GM | the representation sets of central loops are investigated and the results obtained are used to construct a finite cloop it is shown that for certain types of isotopisms the central identities are isotopic invariant | [['the', 'representation', 'sets', 'of', 'central', 'loops', 'are', 'investigated', 'and', 'the', 'results', 'obtained', 'are', 'used', 'to', 'construct', 'a', 'finite', 'cloop', 'it', 'is', 'shown', 'that', 'for', 'certain', 'types', 'of', 'isotopisms', 'the', 'central', 'identities', 'are', 'isotopic', 'invariant']] | [-0.14793747175580768, 0.13168836441164947, -0.07315795496106148, 0.14298903297372711, 0.005710803684504593, -0.11164487716194023, -0.04507623564944986, 0.3855248309178826, -0.24432357751271305, -0.22162236217135453, 0.1297949641559492, -0.27283082803820863, -0.11546098303926342, 0.2349208208376213, -0.0558785691254717... |
707.1436 | The collective dynamics of self-propelled particles | We have proposed a method for the dynamic simulation of a collection of
self-propelled particles in a viscous Newtonian fluid. We restrict attention to
particles whose size and velocity are small enough that the fluid motion is in
the creeping flow regime. We have proposed a simple model for a self-propelled
particle... | cond-mat.soft cond-mat.stat-mech | we have proposed a method for the dynamic simulation of a collection of selfpropelled particles in a viscous newtonian fluid we restrict attention to particles whose size and velocity are small enough that the fluid motion is in the creeping flow regime we have proposed a simple model for a selfpropelled particle and e... | [['we', 'have', 'proposed', 'a', 'method', 'for', 'the', 'dynamic', 'simulation', 'of', 'a', 'collection', 'of', 'selfpropelled', 'particles', 'in', 'a', 'viscous', 'newtonian', 'fluid', 'we', 'restrict', 'attention', 'to', 'particles', 'whose', 'size', 'and', 'velocity', 'are', 'small', 'enough', 'that', 'the', 'fluid... | [-0.12205849082458245, 0.1953213124758656, -0.12475045882300799, -0.0035141328782882803, -0.04617324040249683, -0.11206665310012394, -0.012211147969761907, 0.35419613452151766, -0.27464892136712754, -0.3163112584501505, 0.029060707847197907, -0.28546629083277875, -0.10638322663428479, 0.157716077198491, -0.003477538710... |
707.1437 | Detrended Fluctuation Analysis of Autoregressive Processes | Autoregressive processes (AR) have typical short-range memory. Detrended
Fluctuation Analysis (DFA) was basically designed to reveal long range
correlation in non stationary processes. However DFA can also be regarded as a
suitable method to investigate both long-range and short range correlation in
non-stationary an... | physics.bio-ph physics.data-an | autoregressive processes ar have typical shortrange memory detrended fluctuation analysis dfa was basically designed to reveal long range correlation in non stationary processes however dfa can also be regarded as a suitable method to investigate both longrange and short range correlation in nonstationary and stationar... | [['autoregressive', 'processes', 'ar', 'have', 'typical', 'shortrange', 'memory', 'detrended', 'fluctuation', 'analysis', 'dfa', 'was', 'basically', 'designed', 'to', 'reveal', 'long', 'range', 'correlation', 'in', 'non', 'stationary', 'processes', 'however', 'dfa', 'can', 'also', 'be', 'regarded', 'as', 'a', 'suitable... | [-0.11382145872865353, 0.1434180173236327, -0.07652687415560727, 0.17298481838216864, 0.0008004555601992154, -0.16618848258319, 0.033543127989496595, 0.3959622268554985, -0.28132748101106897, -0.30950268966982003, 0.07884347618567528, -0.32339319175419706, -0.13093921319535096, 0.1680487018661894, 0.061453796244697066,... |
707.1438 | On Some Autotopisms Of Non-Steiner Central Loops | An algebraic process for the construction of an autotopism for a non-Steiner
C-loop is described and this is demonstrated with an example using a known
finite C-loop. In every C-loop, two of its parastrophes are not
equivalent(equal) it, if and only if both the first and second components of
the constructed autotopis... | math.GM | an algebraic process for the construction of an autotopism for a nonsteiner cloop is described and this is demonstrated with an example using a known finite cloop in every cloop two of its parastrophes are not equivalentequal it if and only if both the first and second components of the constructed autotopism and its i... | [['an', 'algebraic', 'process', 'for', 'the', 'construction', 'of', 'an', 'autotopism', 'for', 'a', 'nonsteiner', 'cloop', 'is', 'described', 'and', 'this', 'is', 'demonstrated', 'with', 'an', 'example', 'using', 'a', 'known', 'finite', 'cloop', 'in', 'every', 'cloop', 'two', 'of', 'its', 'parastrophes', 'are', 'not', ... | [-0.13782678181899988, 0.09694074470710203, -0.061842186148575645, 0.028898457493209632, -0.05644836946529277, -0.14985827312487712, 0.006432778746920063, 0.3459310250535132, -0.3096251515473457, -0.2104655966915666, 0.17076989310233795, -0.30029893710099637, -0.17002641999142917, 0.214679289951009, -0.0616718497414617... |
707.1439 | Using a phase space cross section to study large complex systems | For large coupled nonlinear systems, it is difficult to visualize the
high-dimensional phase space, which has been thoroughly studied in smaller
systems with regards to phenomena such as riddled basins. Here we propose a
method to reduce the phase space by defining a phase space cross section. The
method is applied t... | cond-mat.stat-mech math.DS | for large coupled nonlinear systems it is difficult to visualize the highdimensional phase space which has been thoroughly studied in smaller systems with regards to phenomena such as riddled basins here we propose a method to reduce the phase space by defining a phase space cross section the method is applied to a sys... | [['for', 'large', 'coupled', 'nonlinear', 'systems', 'it', 'is', 'difficult', 'to', 'visualize', 'the', 'highdimensional', 'phase', 'space', 'which', 'has', 'been', 'thoroughly', 'studied', 'in', 'smaller', 'systems', 'with', 'regards', 'to', 'phenomena', 'such', 'as', 'riddled', 'basins', 'here', 'we', 'propose', 'a',... | [-0.10990621361162255, 0.1543127985966235, -0.05480310083874086, -0.017908185217898377, -0.04597014233027354, -0.11372078242561881, 0.06447366838306558, 0.3622642517790641, -0.20847980567429325, -0.3180951695787803, 0.037492162305953924, -0.24317186294898097, -0.24191140735724775, 0.19775320501020638, -0.13154079045842... |
707.144 | Stability of Salpeter Solutions | In the framework of instantaneous approximations to the Bethe-Salpeter
formalism for the description of bound states within quantum field theories,
depending on the Lorentz structure of the Bethe-Salpeter interaction kernel the
solutions of the full Salpeter equation with some confining interaction may
exhibit certai... | hep-ph | in the framework of instantaneous approximations to the bethesalpeter formalism for the description of bound states within quantum field theories depending on the lorentz structure of the bethesalpeter interaction kernel the solutions of the full salpeter equation with some confining interaction may exhibit certain ins... | [['in', 'the', 'framework', 'of', 'instantaneous', 'approximations', 'to', 'the', 'bethesalpeter', 'formalism', 'for', 'the', 'description', 'of', 'bound', 'states', 'within', 'quantum', 'field', 'theories', 'depending', 'on', 'the', 'lorentz', 'structure', 'of', 'the', 'bethesalpeter', 'interaction', 'kernel', 'the', ... | [-0.11456195537771907, 0.10618551509383915, -0.1236003868531848, 0.10927242137392464, -0.11399860544221811, -0.16693944822935786, 0.026008677742662814, 0.29823213415932864, -0.27382354734241554, -0.3013170904535902, 0.06041463273335655, -0.2717104384960617, -0.09940145463845565, 0.16423471191455227, 0.01999777066012427... |
707.1441 | On central loops and the central square property | The representation sets of a central square C-loop are investigated. Isotopes
of central square C-loops of exponent 4 are shown to be both C-loops and
A-loops.
| math.GM | the representation sets of a central square cloop are investigated isotopes of central square cloops of exponent 4 are shown to be both cloops and aloops | [['the', 'representation', 'sets', 'of', 'a', 'central', 'square', 'cloop', 'are', 'investigated', 'isotopes', 'of', 'central', 'square', 'cloops', 'of', 'exponent', '4', 'are', 'shown', 'to', 'be', 'both', 'cloops', 'and', 'aloops']] | [-0.1348532477635532, 0.12731518732527128, -0.012503198885287229, 0.11511289643553588, 0.0738291694814017, -0.15759129182865414, -0.03164515775055266, 0.3886578925527059, -0.267127020463634, -0.1928278007544577, 0.16960108033023202, -0.3325874007378633, -0.09270698290604812, 0.17766799511781967, -0.04436246782111434, 0... |
707.1442 | Embedded metal cluster in strong laser fields | We discuss microscopic mechanisms of the violent dynamics following strong
laser excitation of a metal cluster embedded in a rare gas matrix, taking as
test case Na$_8$@Ar$_434$. This covers at least two aspects : first, it
represents the typical experimental situation of metal clusters handled in
raregas matrices or... | cond-mat.other | we discuss microscopic mechanisms of the violent dynamics following strong laser excitation of a metal cluster embedded in a rare gas matrix taking as test case na_8ar_434 this covers at least two aspects first it represents the typical experimental situation of metal clusters handled in raregas matrices or a finite dr... | [['we', 'discuss', 'microscopic', 'mechanisms', 'of', 'the', 'violent', 'dynamics', 'following', 'strong', 'laser', 'excitation', 'of', 'a', 'metal', 'cluster', 'embedded', 'in', 'a', 'rare', 'gas', 'matrix', 'taking', 'as', 'test', 'case', 'na_8ar_434', 'this', 'covers', 'at', 'least', 'two', 'aspects', 'first', 'it',... | [-0.09091722990317151, 0.18081516665027497, -0.028776617314623193, 0.06344502392063754, 0.010679954767151367, -0.15939197616738288, 0.06526346007215812, 0.3886293750797767, -0.2717350782924007, -0.29479216362064065, 0.04377630194459587, -0.2898395512128509, -0.052800352039454546, 0.17046122641172692, 0.0429547670470593... |
707.1443 | Jet Tomography at RHIC | The status of the use of hard probes in heavy ion collisions at RHIC is
reviewed. The discovery of strong jet quenching at RHIC is a major success.
However, in order to make full use of this new phenomenon for full jet emission
tomography of the properties of the collision zone further development is
needed, both exp... | nucl-ex | the status of the use of hard probes in heavy ion collisions at rhic is reviewed the discovery of strong jet quenching at rhic is a major success however in order to make full use of this new phenomenon for full jet emission tomography of the properties of the collision zone further development is needed both experimen... | [['the', 'status', 'of', 'the', 'use', 'of', 'hard', 'probes', 'in', 'heavy', 'ion', 'collisions', 'at', 'rhic', 'is', 'reviewed', 'the', 'discovery', 'of', 'strong', 'jet', 'quenching', 'at', 'rhic', 'is', 'a', 'major', 'success', 'however', 'in', 'order', 'to', 'make', 'full', 'use', 'of', 'this', 'new', 'phenomenon'... | [-0.05403947893340709, 0.15005699813492218, -0.11078300689725931, 0.09439122797210969, -0.05822053021293575, -0.0699364979498846, -0.020752243445081225, 0.3942543966537815, -0.2441402478774978, -0.2623203998526274, 0.06319072602269382, -0.28132550121616506, 0.010481430043987298, 0.17280997719489416, 0.03130570922236321... |
707.1444 | Algebraic properties of some varieties of central loops | Isotopes of C-loops with unique non-identity squares are shown to be both
C-loops and A-loops. The relationship between C-loops and Steiner loops is
further studied. Central loops with the weak and cross inverse properties are
also investigated. C-loops are found to be Osborn loops if every element in
them are square... | math.GM | isotopes of cloops with unique nonidentity squares are shown to be both cloops and aloops the relationship between cloops and steiner loops is further studied central loops with the weak and cross inverse properties are also investigated cloops are found to be osborn loops if every element in them are squares | [['isotopes', 'of', 'cloops', 'with', 'unique', 'nonidentity', 'squares', 'are', 'shown', 'to', 'be', 'both', 'cloops', 'and', 'aloops', 'the', 'relationship', 'between', 'cloops', 'and', 'steiner', 'loops', 'is', 'further', 'studied', 'central', 'loops', 'with', 'the', 'weak', 'and', 'cross', 'inverse', 'properties', ... | [-0.114173909628709, 0.16289461774331535, -0.0016522830279142248, 0.124900020980824, -0.030091698441252698, -0.19564439915120602, -0.025130590615684494, 0.5003102543015107, -0.3047325725064558, -0.23042605635618754, 0.1326105917185344, -0.37063580619938236, -0.1355784489389728, 0.15466798012893573, -0.02757128837573178... |
707.1445 | Invariant measure for a three dimensional nonlinear wave equation | We study the long time behavior of the subcritical (subcubic) defocussing
nonlinear wave equation on the three dimensional ball, for random data of low
regularity. We prove that for a large set of radial initial data in
$\cap_{s<1/2} H^s(B(0,1))$ the equation is (globally in time) well posed and we
construct an invar... | math.AP math.DS | we study the long time behavior of the subcritical subcubic defocussing nonlinear wave equation on the three dimensional ball for random data of low regularity we prove that for a large set of radial initial data in cap_s12 hsb01 the equation is globally in time well posed and we construct an invariant measure | [['we', 'study', 'the', 'long', 'time', 'behavior', 'of', 'the', 'subcritical', 'subcubic', 'defocussing', 'nonlinear', 'wave', 'equation', 'on', 'the', 'three', 'dimensional', 'ball', 'for', 'random', 'data', 'of', 'low', 'regularity', 'we', 'prove', 'that', 'for', 'a', 'large', 'set', 'of', 'radial', 'initial', 'data... | [-0.16719260247533813, 0.10573056513042983, -0.061645531734707305, 0.08310161022168092, -0.06191467605622522, -0.08645785909474772, -0.03517583667245858, 0.3339138365551537, -0.2894326027701883, -0.2415055398482318, 0.17647673956155047, -0.27607802853134333, -0.10571772468221538, 0.19601006206928515, -0.031064699732643... |
707.1446 | Excitations and superfluidity in non-equilibrium Bose-Einstein
condensates of exciton-polaritons | We present a generic model for the description of non-equilibrium
Bose-Einstein condensates, suited for the modelling of non-resonantly pumped
polariton condensates in a semiconductor microcavity. The excitation spectrum
and scattering of the non-equilibrium condensate with a defect are discussed.
| cond-mat.mes-hall | we present a generic model for the description of nonequilibrium boseeinstein condensates suited for the modelling of nonresonantly pumped polariton condensates in a semiconductor microcavity the excitation spectrum and scattering of the nonequilibrium condensate with a defect are discussed | [['we', 'present', 'a', 'generic', 'model', 'for', 'the', 'description', 'of', 'nonequilibrium', 'boseeinstein', 'condensates', 'suited', 'for', 'the', 'modelling', 'of', 'nonresonantly', 'pumped', 'polariton', 'condensates', 'in', 'a', 'semiconductor', 'microcavity', 'the', 'excitation', 'spectrum', 'and', 'scattering... | [-0.14987812836009723, 0.24562587610517556, -0.08236062378646472, 0.05576024085092239, 0.09402804043239509, -0.17249865210256898, -0.016383731848178193, 0.4040691623559747, -0.12506720377132297, -0.17796793699455568, -0.032006154174152285, -0.2595238194394952, -0.05653696115582417, 0.17833889634587252, 0.10063897825490... |
707.1447 | Random data Cauchy theory for supercritical wave equations I: Local
theory | We study the local existence of strong solutions for the cubic nonlinear wave
equation with data in $H^s(M)$, $s<1/2$, where $M$ is a three dimensional
compact riemannian manifold. This problem is supercritical and can be shown to
be strongly ill-posed (in the Hadamard sense). However, after a suitable
randomization,... | math.AP | we study the local existence of strong solutions for the cubic nonlinear wave equation with data in hsm s12 where m is a three dimensional compact riemannian manifold this problem is supercritical and can be shown to be strongly illposed in the hadamard sense however after a suitable randomization we are able to constr... | [['we', 'study', 'the', 'local', 'existence', 'of', 'strong', 'solutions', 'for', 'the', 'cubic', 'nonlinear', 'wave', 'equation', 'with', 'data', 'in', 'hsm', 's12', 'where', 'm', 'is', 'a', 'three', 'dimensional', 'compact', 'riemannian', 'manifold', 'this', 'problem', 'is', 'supercritical', 'and', 'can', 'be', 'show... | [-0.15418237188317685, 0.07585946199039674, -0.028324633752080528, 0.060674732422657224, -0.08650261170061474, -0.16919375989395616, -0.03263912884920666, 0.3484782487450337, -0.2583260332996195, -0.24417798629623244, 0.2094628136983374, -0.2733629860132086, -0.11229033954441547, 0.1757953464164695, -0.0488322566961869... |
707.1448 | Random data Cauchy theory for supercritical wave equations II : A global
existence result | We prove that the subquartic wave equation on the three dimensional ball
$\Theta$, with Dirichlet boundary conditions admits global strong solutions for
a large set of random supercritical initial data in $\cap_{s<1/2} H^s(\Theta)$.
We obtain this result as a consequence of a general random data Cauchy theory
for sup... | math.AP | we prove that the subquartic wave equation on the three dimensional ball theta with dirichlet boundary conditions admits global strong solutions for a large set of random supercritical initial data in cap_s12 hstheta we obtain this result as a consequence of a general random data cauchy theory for supercritical wave eq... | [['we', 'prove', 'that', 'the', 'subquartic', 'wave', 'equation', 'on', 'the', 'three', 'dimensional', 'ball', 'theta', 'with', 'dirichlet', 'boundary', 'conditions', 'admits', 'global', 'strong', 'solutions', 'for', 'a', 'large', 'set', 'of', 'random', 'supercritical', 'initial', 'data', 'in', 'cap_s12', 'hstheta', 'w... | [-0.1358638925723628, 0.07829669333295897, -0.12375634274859396, 0.07636382661520555, -0.10607093743035673, -0.11560902429078447, 0.03633517291261038, 0.2689015489175088, -0.24400971391393492, -0.23290842750834095, 0.17015563571476378, -0.2473025297642582, -0.12811362060407797, 0.19036146272749951, -0.02198864925594534... |
707.1449 | Abstract homotopical methods for theoretical computer science | The purpose of this paper is to collect the homotopical methods used in the
development of the theory of flows initialized by author's paper ``A model
category for the homotopy theory of concurrency''. It is presented
generalizations of the classical Whitehead theorem inverting weak homotopy
equivalences between CW-c... | math.AT math.CT | the purpose of this paper is to collect the homotopical methods used in the development of the theory of flows initialized by authors paper a model category for the homotopy theory of concurrency it is presented generalizations of the classical whitehead theorem inverting weak homotopy equivalences between cwcomplexes ... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'collect', 'the', 'homotopical', 'methods', 'used', 'in', 'the', 'development', 'of', 'the', 'theory', 'of', 'flows', 'initialized', 'by', 'authors', 'paper', 'a', 'model', 'category', 'for', 'the', 'homotopy', 'theory', 'of', 'concurrency', 'it', 'is', 'presented'... | [-0.1087741247102828, -0.015598049852997065, -0.1036632287539017, 0.1671952049962809, -0.07960018237501802, -0.15431024923159833, 0.003627062591553574, 0.35089485900817624, -0.38250695983551336, -0.2197482645327986, 0.06324938585011053, -0.18891524533990403, -0.14709043228657734, 0.15580237510246814, -0.199495951382731... |
707.145 | Critical Kauffman networks under deterministic asynchronous update | We investigate the influence of a deterministic but non-synchronous update on
Random Boolean Networks, with a focus on critical networks. Knowing that
``relevant components'' determine the number and length of attractors, we focus
on such relevant components and calculate how the length and number of
attractors on th... | cond-mat.dis-nn cond-mat.stat-mech | we investigate the influence of a deterministic but nonsynchronous update on random boolean networks with a focus on critical networks knowing that relevant components determine the number and length of attractors we focus on such relevant components and calculate how the length and number of attractors on these compon... | [['we', 'investigate', 'the', 'influence', 'of', 'a', 'deterministic', 'but', 'nonsynchronous', 'update', 'on', 'random', 'boolean', 'networks', 'with', 'a', 'focus', 'on', 'critical', 'networks', 'knowing', 'that', 'relevant', 'components', 'determine', 'the', 'number', 'and', 'length', 'of', 'attractors', 'we', 'focu... | [-0.19955786507473225, 0.19976377262630396, -0.006379627627837989, 0.07722283850113551, -0.041850558316542046, -0.17439000970787472, 0.05786880869418383, 0.38850144969506395, -0.2557362038228247, -0.26992228356086545, 0.15800512803899538, -0.27622413587814665, -0.1866224047727883, 0.21867278319421327, -0.04139053028387... |
707.1451 | BFKL equation at finite temperature | We consider the Color Glass Condensate (CGC) at finite temperature, which
would be relevant to the initial condition of relativistic heavy ion collisions
and the energy loss of energetic partons in the quark-gluon plasma. In the weak
source approximation, we derive the thermal BFKL equation. We find that the
thermal ... | hep-ph | we consider the color glass condensate cgc at finite temperature which would be relevant to the initial condition of relativistic heavy ion collisions and the energy loss of energetic partons in the quarkgluon plasma in the weak source approximation we derive the thermal bfkl equation we find that the thermal effect sh... | [['we', 'consider', 'the', 'color', 'glass', 'condensate', 'cgc', 'at', 'finite', 'temperature', 'which', 'would', 'be', 'relevant', 'to', 'the', 'initial', 'condition', 'of', 'relativistic', 'heavy', 'ion', 'collisions', 'and', 'the', 'energy', 'loss', 'of', 'energetic', 'partons', 'in', 'the', 'quarkgluon', 'plasma',... | [-0.06557195559195192, 0.28192023084765033, -0.18510014102743058, 0.12985704818760957, -0.016047893808438227, -0.07026916049973486, -0.01245187445042225, 0.3742745793373375, -0.20202646023532436, -0.2422432353065073, -0.004891763711194662, -0.2864794642510977, 0.04658631022487368, 0.08466212011638333, 0.018661500706982... |
707.1452 | Clusters, Graphs, and Networks for Analysing Internet-Web-Supported
Communication within a Virtual Community | The proposal is to use clusters, graphs and networks as models in order to
analyse the Web structure. Clusters, graphs and networks provide knowledge
representation and organization. Clusters were generated by co-site analysis.
The sample is a set of academic Web sites from the countries belonging to the
European Uni... | cs.AI cs.LG | the proposal is to use clusters graphs and networks as models in order to analyse the web structure clusters graphs and networks provide knowledge representation and organization clusters were generated by cosite analysis the sample is a set of academic web sites from the countries belonging to the european union these... | [['the', 'proposal', 'is', 'to', 'use', 'clusters', 'graphs', 'and', 'networks', 'as', 'models', 'in', 'order', 'to', 'analyse', 'the', 'web', 'structure', 'clusters', 'graphs', 'and', 'networks', 'provide', 'knowledge', 'representation', 'and', 'organization', 'clusters', 'were', 'generated', 'by', 'cosite', 'analysis... | [-0.09977008955849503, 0.017107113720571346, -0.07537082186018144, 0.0922957007124117, -0.11193232442945539, -0.06722951511443226, 0.09924368018982932, 0.4306784546792959, -0.2745747753969309, -0.33713929298083356, 0.0896439109593771, -0.33698771110820497, -0.21388076987711951, 0.14362685593324853, -0.0372304288973806,... |
707.1453 | A matrix formulation for small-x singlet evolution | We propose a matrix evolution equation in (x,kt)-space for flavour singlet,
unintegrated quark and gluon densities, which generalizes DGLAP and BFKL
equations in the relevant limits. The matrix evolution kernel is constructed so
as to satisfy renormalization group constraints in both the ordered and
antiordered regio... | hep-ph | we propose a matrix evolution equation in xktspace for flavour singlet unintegrated quark and gluon densities which generalizes dglap and bfkl equations in the relevant limits the matrix evolution kernel is constructed so as to satisfy renormalization group constraints in both the ordered and antiordered regions of exc... | [['we', 'propose', 'a', 'matrix', 'evolution', 'equation', 'in', 'xktspace', 'for', 'flavour', 'singlet', 'unintegrated', 'quark', 'and', 'gluon', 'densities', 'which', 'generalizes', 'dglap', 'and', 'bfkl', 'equations', 'in', 'the', 'relevant', 'limits', 'the', 'matrix', 'evolution', 'kernel', 'is', 'constructed', 'so... | [-0.0703869403702431, 0.11453615106742451, -0.14005903634419548, 0.16154245997534453, -0.0628059325475228, -0.1253831334893969, 0.011468186432236358, 0.35220296211729324, -0.19942546137195977, -0.2411363958322172, 0.026691753243367318, -0.27908786467594815, -0.08001613130504147, 0.09891310583835444, 0.038157706143028, ... |
707.1454 | Algorithms for entanglement renormalization | We describe an iterative method to optimize the multi-scale entanglement
renormalization ansatz (MERA) for the low-energy subspace of local Hamiltonians
on a D-dimensional lattice. For translation invariant systems the cost of this
optimization is logarithmic in the linear system size. Specialized algorithms
for the ... | cond-mat.str-el cond-mat.other quant-ph | we describe an iterative method to optimize the multiscale entanglement renormalization ansatz mera for the lowenergy subspace of local hamiltonians on a ddimensional lattice for translation invariant systems the cost of this optimization is logarithmic in the linear system size specialized algorithms for the treatment... | [['we', 'describe', 'an', 'iterative', 'method', 'to', 'optimize', 'the', 'multiscale', 'entanglement', 'renormalization', 'ansatz', 'mera', 'for', 'the', 'lowenergy', 'subspace', 'of', 'local', 'hamiltonians', 'on', 'a', 'ddimensional', 'lattice', 'for', 'translation', 'invariant', 'systems', 'the', 'cost', 'of', 'thi... | [-0.15111349523067474, 0.08640251923064907, -0.07059700838899949, 0.10766945038838978, 0.006752738584986045, -0.18614930472159313, -0.025648512437848176, 0.36170450265940635, -0.25225029109666747, -0.23440730663216008, 0.08179328347960975, -0.27431190404708367, -0.11637126693745986, 0.20816178372617633, 0.0263933120849... |
707.1455 | Supersymmetry Searches at the Tevatron | CDF and DO detectors have already collected 1.3 fb^{-1} of data delivered by
the Tevatron collider at 1.96 TeV center-of-mass energy. We present here the
various analyses that are currently testing the possibility of a supersymmetric
extension of the Standard Model. No evidence for such processes have been found
in l... | hep-ex | cdf and do detectors have already collected 13 fb1 of data delivered by the tevatron collider at 196 tev centerofmass energy we present here the various analyses that are currently testing the possibility of a supersymmetric extension of the standard model no evidence for such processes have been found in luminosities ... | [['cdf', 'and', 'do', 'detectors', 'have', 'already', 'collected', '13', 'fb1', 'of', 'data', 'delivered', 'by', 'the', 'tevatron', 'collider', 'at', '196', 'tev', 'centerofmass', 'energy', 'we', 'present', 'here', 'the', 'various', 'analyses', 'that', 'are', 'currently', 'testing', 'the', 'possibility', 'of', 'a', 'su... | [-0.0057923453614899985, 0.16075669442254462, -0.07161105582245479, 0.12881773908769614, -0.08439593794020384, -0.10351973170978263, -0.005212082077234395, 0.38496884134579695, -0.17483735341872825, -0.4354686758628017, 0.11474091449207136, -0.41012824080443305, 0.05835769756844169, 0.23951064649276974, 0.1048798936045... |
707.1456 | The UV Continuum of Quasars: Models and SDSS Spectral Slopes | We measure long (2200-4000 ang) and short (1450-2200 ang) wavelength spectral
slopes \alpha (F_\nu proportional to \nu^\alpha) for quasar spectra from the
Sloan Digital Sky Survey. The long and short wavelength slopes are computed
from 3646 and 2706 quasars with redshifts in the z=0.76-1.26 and z=1.67-2.07
ranges, re... | astro-ph | we measure long 22004000 ang and short 14502200 ang wavelength spectral slopes alpha f_nu proportional to nualpha for quasar spectra from the sloan digital sky survey the long and short wavelength slopes are computed from 3646 and 2706 quasars with redshifts in the z076126 and z167207 ranges respectively we calculate m... | [['we', 'measure', 'long', '22004000', 'ang', 'and', 'short', '14502200', 'ang', 'wavelength', 'spectral', 'slopes', 'alpha', 'f_nu', 'proportional', 'to', 'nualpha', 'for', 'quasar', 'spectra', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'the', 'long', 'and', 'short', 'wavelength', 'slopes', 'are', 'computed',... | [0.016210977832357726, 0.13964545522833727, -0.08910742814704362, 0.18521585706157903, -0.06662069261505234, -0.11202316708362627, 0.007923659699304995, 0.5315135900897009, -0.11799887744200532, -0.3674614904879558, 0.04115184197683077, -0.3578289944324987, 0.03331908707170644, 0.22680538837448694, -0.05179471046991508... |
707.1457 | Visibility Fringe Reduction Due to Noise-Induced Effects: Microscopic
Approach to Interference Experiments | Decoherence is the main process behind the quantum to classical transition.
It is a purely quantum mechanical effect by which the system looses its ability
to exhibit coherent behavior. The recent experimental observation of
diffraction and interference patterns for large molecules raises some
interesting questions. ... | quant-ph cond-mat.other hep-ph | decoherence is the main process behind the quantum to classical transition it is a purely quantum mechanical effect by which the system looses its ability to exhibit coherent behavior the recent experimental observation of diffraction and interference patterns for large molecules raises some interesting questions in th... | [['decoherence', 'is', 'the', 'main', 'process', 'behind', 'the', 'quantum', 'to', 'classical', 'transition', 'it', 'is', 'a', 'purely', 'quantum', 'mechanical', 'effect', 'by', 'which', 'the', 'system', 'looses', 'its', 'ability', 'to', 'exhibit', 'coherent', 'behavior', 'the', 'recent', 'experimental', 'observation',... | [-0.13699655739341196, 0.16418316680307804, -0.11815089464011624, 0.09344562441878597, -0.06935035796674686, -0.10849103046669148, 0.07751660334958335, 0.35963771157846675, -0.2645874119796387, -0.2996373727778339, 0.06434946468532614, -0.2839974723884645, -0.17010133537669175, 0.170360102833388, -0.05202647453122662, ... |
707.1458 | Explicit computations of all finite index bimodules for a family of II_1
factors | We study II_1 factors M and N associated with good generalized Bernoulli
actions of groups having an infinite almost normal subgroup with the relative
property (T). We prove the following rigidity result: every finite index
M-N-bimodule (in particular, every isomorphism between M and N) is described by
a commensurabi... | math.OA | we study ii_1 factors m and n associated with good generalized bernoulli actions of groups having an infinite almost normal subgroup with the relative property t we prove the following rigidity result every finite index mnbimodule in particular every isomorphism between m and n is described by a commensurability of the... | [['we', 'study', 'ii_1', 'factors', 'm', 'and', 'n', 'associated', 'with', 'good', 'generalized', 'bernoulli', 'actions', 'of', 'groups', 'having', 'an', 'infinite', 'almost', 'normal', 'subgroup', 'with', 'the', 'relative', 'property', 't', 'we', 'prove', 'the', 'following', 'rigidity', 'result', 'every', 'finite', 'i... | [-0.19129414252597385, 0.16583836005775424, -0.062475058319760815, 0.018200339603664302, -0.06965670085329319, -0.17194599950703504, 0.03855264159006493, 0.38286462969312046, -0.3175029869617842, -0.2380468667284629, 0.09348346247929627, -0.23799074658793268, -0.11960897283524136, 0.1589064918084192, -0.137217695223141... |
707.1459 | Standard Relations of Multiple Polylogarithm Values at Roots of Unity | Let $N$ be a positive integer. In this paper we shall study the special
values of multiple polylogarithms at $N$th roots of unity, called multiple
polylogarithm values (MPVs) of level $N$. These objects are generalizations of
multiple zeta values and alternating Euler sums, which was studied by Euler,
and more recent... | math.NT | let n be a positive integer in this paper we shall study the special values of multiple polylogarithms at nth roots of unity called multiple polylogarithm values mpvs of level n these objects are generalizations of multiple zeta values and alternating euler sums which was studied by euler and more recently many mathema... | [['let', 'n', 'be', 'a', 'positive', 'integer', 'in', 'this', 'paper', 'we', 'shall', 'study', 'the', 'special', 'values', 'of', 'multiple', 'polylogarithms', 'at', 'nth', 'roots', 'of', 'unity', 'called', 'multiple', 'polylogarithm', 'values', 'mpvs', 'of', 'level', 'n', 'these', 'objects', 'are', 'generalizations', '... | [-0.1270195356668577, 0.13714520757234652, -0.08382575041088412, 0.09981587990070206, -0.08048181364577747, -0.15738170438107088, 0.05182719839859567, 0.3150336297699465, -0.27842898634125995, -0.3182133962575611, 0.09272978917859245, -0.276540244551508, -0.1580363329437612, 0.23008166385471635, -0.05598821105419904, 0... |
707.146 | Structure and Evolution of Giant Cells in Global Models of Solar
Convection | The global scales of solar convection are studied through three-dimensional
simulations of compressible convection carried out in spherical shells of
rotating fluid which extend from the base of the convection zone to within 15
Mm of the photosphere. Such modelling at the highest spatial resolution to date
allows stu... | astro-ph | the global scales of solar convection are studied through threedimensional simulations of compressible convection carried out in spherical shells of rotating fluid which extend from the base of the convection zone to within 15 mm of the photosphere such modelling at the highest spatial resolution to date allows study o... | [['the', 'global', 'scales', 'of', 'solar', 'convection', 'are', 'studied', 'through', 'threedimensional', 'simulations', 'of', 'compressible', 'convection', 'carried', 'out', 'in', 'spherical', 'shells', 'of', 'rotating', 'fluid', 'which', 'extend', 'from', 'the', 'base', 'of', 'the', 'convection', 'zone', 'to', 'with... | [-0.1307831647415592, 0.19544033812679595, -0.06309839546657549, 0.08750040589242059, -0.06589489694509167, -0.06363052561245554, -0.004294289907700092, 0.37801310623095175, -0.2947957130610851, -0.31515438835991577, 0.10164741877863398, -0.24783152028958583, -0.12689127555197166, 0.2020165856620373, -0.039870038646231... |
707.1461 | Conditional large and moderate deviations for sums of discrete random
variables. Combinatoric applications | We prove large and moderate deviation principles for the distribution of an
empirical mean conditioned by the value of the sum of discrete i.i.d. random
variables. Some applications for combinatoric problems are discussed.
| math.PR | we prove large and moderate deviation principles for the distribution of an empirical mean conditioned by the value of the sum of discrete iid random variables some applications for combinatoric problems are discussed | [['we', 'prove', 'large', 'and', 'moderate', 'deviation', 'principles', 'for', 'the', 'distribution', 'of', 'an', 'empirical', 'mean', 'conditioned', 'by', 'the', 'value', 'of', 'the', 'sum', 'of', 'discrete', 'iid', 'random', 'variables', 'some', 'applications', 'for', 'combinatoric', 'problems', 'are', 'discussed']] | [-0.07858168559544014, 0.14881787860146936, -0.0606830646989472, 0.11694117962862506, -0.045339068129771586, -0.08197942387425539, 0.07759958849937627, 0.3558214038723346, -0.333812526794094, -0.25950200494491693, 0.15592622735791586, -0.2818826717239889, -0.1218327305484281, 0.19292133084187904, -0.11576597223227675, ... |
707.1462 | Non-Uniqueness of Gibbs measures relative to Brownian motion | We consider Gibbs measures relative to Brownian motion of Feynman-Kac type,
with single site potential V. We show that for a large class of V, including
the Coulomb potential, there exist infinitely many infinite volume Gibbs
measures.
| math.PR math-ph math.MP | we consider gibbs measures relative to brownian motion of feynmankac type with single site potential v we show that for a large class of v including the coulomb potential there exist infinitely many infinite volume gibbs measures | [['we', 'consider', 'gibbs', 'measures', 'relative', 'to', 'brownian', 'motion', 'of', 'feynmankac', 'type', 'with', 'single', 'site', 'potential', 'v', 'we', 'show', 'that', 'for', 'a', 'large', 'class', 'of', 'v', 'including', 'the', 'coulomb', 'potential', 'there', 'exist', 'infinitely', 'many', 'infinite', 'volume'... | [-0.10450786734754974, 0.1781881172209978, -0.036330538097064234, 0.0970054236869957, 0.013796322425273625, -0.18304340154989748, 0.053977077675832284, 0.4149002543575055, -0.31545491722991337, -0.21695746169299693, 0.0013655642034939013, -0.3306391305617384, -0.10641284417864438, 0.18901768356964394, -0.08930680737201... |
707.1463 | Continuously Crossing u=z in the H3+ Boundary CFT | For AdS boundary conditions, we give a solution of the H3+ two point function
involving degenerate field with SL(2)-label b^{-2}/2, which is defined on the
full (u,z) unit square. It consists of two patches, one for z<u and one for
u<z. Along the u=z "singularity", the solutions from both patches are shown to
have fi... | hep-th | for ads boundary conditions we give a solution of the h3 two point function involving degenerate field with sl2label b22 which is defined on the full uz unit square it consists of two patches one for zu and one for uz along the uz singularity the solutions from both patches are shown to have finite limits and are merge... | [['for', 'ads', 'boundary', 'conditions', 'we', 'give', 'a', 'solution', 'of', 'the', 'h3', 'two', 'point', 'function', 'involving', 'degenerate', 'field', 'with', 'sl2label', 'b22', 'which', 'is', 'defined', 'on', 'the', 'full', 'uz', 'unit', 'square', 'it', 'consists', 'of', 'two', 'patches', 'one', 'for', 'zu', 'and... | [-0.11169743820872748, 0.08780178190716127, -0.07086702185397101, 0.04725057606257978, -0.07592846745265519, -0.14700362399349562, -0.010535606754814634, 0.3487164921837278, -0.23160718154567894, -0.22640031200861283, 0.1791617602598623, -0.303352937812336, -0.1268503352778383, 0.19776119782570933, -0.05291763516972855... |
707.1464 | The Attractor Mechanism in Gauss-Bonnet Gravity | We study extremal black hole solutions of D=5 Gauss-Bonnet gravity coupled to
a system of gauge and scalar fields. As in Einstein gravity, we find that the
values of the scalar fields on the horizon must extremize a certain effective
potential that depends on the black hole charges. If the matrix of second
derivative... | hep-th | we study extremal black hole solutions of d5 gaussbonnet gravity coupled to a system of gauge and scalar fields as in einstein gravity we find that the values of the scalar fields on the horizon must extremize a certain effective potential that depends on the black hole charges if the matrix of second derivatives of th... | [['we', 'study', 'extremal', 'black', 'hole', 'solutions', 'of', 'd5', 'gaussbonnet', 'gravity', 'coupled', 'to', 'a', 'system', 'of', 'gauge', 'and', 'scalar', 'fields', 'as', 'in', 'einstein', 'gravity', 'we', 'find', 'that', 'the', 'values', 'of', 'the', 'scalar', 'fields', 'on', 'the', 'horizon', 'must', 'extremize... | [-0.17579596944825543, 0.09565201627188608, -0.10767706207706965, 0.11327779775352351, -0.0955480409057853, -0.17389161063050082, 0.011296348765324381, 0.2823622969812469, -0.17066389382545508, -0.23955254003237514, 0.09982868747547605, -0.2875014759698196, -0.16043575815296263, 0.16381832821245648, -0.0284418999104755... |
707.1465 | Resonant superradiant backward-scattering as a source for many-particle
entanglement | We investigate the atom pair production by superradiant backward-scattering
from a Bose-Einstein condensate. By driving the superradiant process with two
frequencies we can extend both the range of pulse duration and intensity by two
orders of magnitude and obtain full control over the number of scattered atoms
in fo... | cond-mat.other | we investigate the atom pair production by superradiant backwardscattering from a boseeinstein condensate by driving the superradiant process with two frequencies we can extend both the range of pulse duration and intensity by two orders of magnitude and obtain full control over the number of scattered atoms in forward... | [['we', 'investigate', 'the', 'atom', 'pair', 'production', 'by', 'superradiant', 'backwardscattering', 'from', 'a', 'boseeinstein', 'condensate', 'by', 'driving', 'the', 'superradiant', 'process', 'with', 'two', 'frequencies', 'we', 'can', 'extend', 'both', 'the', 'range', 'of', 'pulse', 'duration', 'and', 'intensity'... | [-0.13873872200379195, 0.26969131026644166, -0.02345978950786336, 0.03000419369410094, -0.005026220801150109, -0.1220611498986439, 0.055265142681735865, 0.44302471681702427, -0.28020720749457434, -0.22489446022252485, -0.039132096479567356, -0.3044221214694539, -0.027546149746673864, 0.23202812835778586, 0.047577239039... |
707.1466 | Coherent systems of genus 0, III: Computation of flips for k=1 | In this paper we continue the investigation of coherent systems of type
$(n,d,k)$ on the projective line which are stable with respect to some value of
a parameter $\alpha$. We consider the case $k=1$ and study the variation of the
moduli spaces with $\alpha$. We determine inductively the first and last moduli
spaces... | math.AG | in this paper we continue the investigation of coherent systems of type ndk on the projective line which are stable with respect to some value of a parameter alpha we consider the case k1 and study the variation of the moduli spaces with alpha we determine inductively the first and last moduli spaces and the flip loci ... | [['in', 'this', 'paper', 'we', 'continue', 'the', 'investigation', 'of', 'coherent', 'systems', 'of', 'type', 'ndk', 'on', 'the', 'projective', 'line', 'which', 'are', 'stable', 'with', 'respect', 'to', 'some', 'value', 'of', 'a', 'parameter', 'alpha', 'we', 'consider', 'the', 'case', 'k1', 'and', 'study', 'the', 'vari... | [-0.146699852699977, 0.11287895478135608, -0.014665715851236221, 0.07542998268848372, -0.0269973291203293, -0.1148145388497776, 0.03657454835131851, 0.36269119499944324, -0.25948580234246543, -0.25603053090500993, 0.15654477665233318, -0.2224070187387338, -0.15847770812336442, 0.1945866129556021, -0.07786556521192366, ... |
707.1467 | Electron-phonon coupling and electron self-energy in electron-doped
graphene: calculation of angular resolved photoemission spectra | We obtain analytical expressions for the electron self-energy and the
electron-phonon coupling in electron-doped graphene using electron-phonon
matrix elements extracted from density functional theory simulations. From the
electron self-energies we calculate angle resolved photoemission spectra. We
demonstrate that t... | cond-mat.supr-con cond-mat.mes-hall cond-mat.mtrl-sci | we obtain analytical expressions for the electron selfenergy and the electronphonon coupling in electrondoped graphene using electronphonon matrix elements extracted from density functional theory simulations from the electron selfenergies we calculate angle resolved photoemission spectra we demonstrate that the measur... | [['we', 'obtain', 'analytical', 'expressions', 'for', 'the', 'electron', 'selfenergy', 'and', 'the', 'electronphonon', 'coupling', 'in', 'electrondoped', 'graphene', 'using', 'electronphonon', 'matrix', 'elements', 'extracted', 'from', 'density', 'functional', 'theory', 'simulations', 'from', 'the', 'electron', 'selfen... | [-0.09667041199512337, 0.18602526912207504, -0.0467456969833647, 0.0798535801459906, 0.006513348764435637, -0.13336407117278196, 0.08015123918067, 0.37574314961836924, -0.25967350887425134, -0.327768444955017, -0.020497487900008698, -0.38821870688865384, -0.046312201106552, 0.20586469984932637, 0.0794854843620174, -0.0... |
707.1468 | Stable curves and screens on fatgraphs | The mapping class group invariant ideal cell decomposition of the
Teichmueller space of a punctured surface times an open simplex has been used
in a number of computations. This paper answers a question about the
asymptotics of this decomposition, namely, in a given cell of the
decomposition, which curves can be shor... | math.GT math.AG | the mapping class group invariant ideal cell decomposition of the teichmueller space of a punctured surface times an open simplex has been used in a number of computations this paper answers a question about the asymptotics of this decomposition namely in a given cell of the decomposition which curves can be short scre... | [['the', 'mapping', 'class', 'group', 'invariant', 'ideal', 'cell', 'decomposition', 'of', 'the', 'teichmueller', 'space', 'of', 'a', 'punctured', 'surface', 'times', 'an', 'open', 'simplex', 'has', 'been', 'used', 'in', 'a', 'number', 'of', 'computations', 'this', 'paper', 'answers', 'a', 'question', 'about', 'the', '... | [-0.14429084477187307, 0.07719795851153322, -0.124644421150241, 0.05591088174238663, -0.08492506481707096, -0.1044158479285047, 0.04619262325088781, 0.31096044139085727, -0.3337738245357702, -0.23608681817113616, 0.13895302063521045, -0.22642206284504982, -0.16095223452573942, 0.21158039496268755, -0.12627973279306365,... |
707.1469 | Coarse and synthetic Weil-Petersson geometry: quasi-flats, geodesics,
and relative hyperbolicity | We analyze the coarse geometry of the Weil-Petersson metric on Teichm\"uller
space, focusing on applications to its synthetic geometry (in particular the
behavior of geodesics). We settle the question of the strong relative
hyperbolicity of the Weil-Petersson metric via consideration of its coarse
quasi-isometric mod... | math.GT | we analyze the coarse geometry of the weilpetersson metric on teichmuller space focusing on applications to its synthetic geometry in particular the behavior of geodesics we settle the question of the strong relative hyperbolicity of the weilpetersson metric via consideration of its coarse quasiisometric model the pant... | [['we', 'analyze', 'the', 'coarse', 'geometry', 'of', 'the', 'weilpetersson', 'metric', 'on', 'teichmuller', 'space', 'focusing', 'on', 'applications', 'to', 'its', 'synthetic', 'geometry', 'in', 'particular', 'the', 'behavior', 'of', 'geodesics', 'we', 'settle', 'the', 'question', 'of', 'the', 'strong', 'relative', 'h... | [-0.15206269011264895, 0.12029453031236033, -0.08605628146608246, 0.0606246323079132, -0.06794615651242344, -0.09235429194494628, 0.012857543707757099, 0.3564700084502763, -0.2878424150488771, -0.23781876186854434, 0.10204341160644573, -0.274772129363555, -0.14994819330693246, 0.18858696160576782, -0.11571561100199909,... |
707.147 | Secrecy Capacity Region of Fading Broadcast Channels | The fading broadcast channel with confidential messages (BCC) is
investigated, where a source node has common information for two receivers
(receivers 1 and 2), and has confidential information intended only for
receiver 1. The confidential information needs to be kept as secret as possible
from receiver 2. The chann... | cs.IT math.IT | the fading broadcast channel with confidential messages bcc is investigated where a source node has common information for two receivers receivers 1 and 2 and has confidential information intended only for receiver 1 the confidential information needs to be kept as secret as possible from receiver 2 the channel state i... | [['the', 'fading', 'broadcast', 'channel', 'with', 'confidential', 'messages', 'bcc', 'is', 'investigated', 'where', 'a', 'source', 'node', 'has', 'common', 'information', 'for', 'two', 'receivers', 'receivers', '1', 'and', '2', 'and', 'has', 'confidential', 'information', 'intended', 'only', 'for', 'receiver', '1', 't... | [-0.2403923005113029, 0.005622906395728933, -0.007233418498799438, 0.03796298855377245, -0.062380967025092104, -0.35201931451956625, 0.15230376618274022, 0.3874234123795759, -0.30118351030978374, -0.18449119327124208, 0.17625837280047563, -0.32549418800044805, -0.052281958329331246, 0.07205007987613499, -0.104327849135... |
707.1471 | On strict inclusions in hierarchies of convex bodies | Let $\mathcal I_k$ be the class of convex $k$-intersection bodies in
$\mathbb{R}^n$ (in the sense of Koldobsky) and $\mathcal I_k^m$ be the class of
convex origin-symmetric bodies all of whose $m$-dimensional central sections
are $k$-intersection bodies. We show that 1) $\mathcal I_k^m\not\subset
\mathcal I_k^{m+1}$,... | math.MG math.FA | let mathcal i_k be the class of convex kintersection bodies in mathbbrn in the sense of koldobsky and mathcal i_km be the class of convex originsymmetric bodies all of whose mdimensional central sections are kintersection bodies we show that 1 mathcal i_kmnotsubset mathcal i_km1 k3le mn and 2 mathcal i_l notsubset math... | [['let', 'mathcal', 'i_k', 'be', 'the', 'class', 'of', 'convex', 'kintersection', 'bodies', 'in', 'mathbbrn', 'in', 'the', 'sense', 'of', 'koldobsky', 'and', 'mathcal', 'i_km', 'be', 'the', 'class', 'of', 'convex', 'originsymmetric', 'bodies', 'all', 'of', 'whose', 'mdimensional', 'central', 'sections', 'are', 'kinters... | [-0.19117954920959443, 0.12985029800508457, 0.06721602494900043, -0.025511387932615783, 0.01880317162991, -0.18962476406103143, -0.10535472368848367, 0.3041595541872084, -0.33386641783783066, -0.0929247577352306, 0.05994545718063959, -0.386243985607647, -0.10680190086937867, 0.12471937474149924, -0.19289585876350218, 0... |
707.1472 | Extra Current and Integer Quantum Hall Conductance in the Spin-Orbit
Coupling System | We study the extra term of particle current in a 2D k-cubic Rashba spin-orbit
coupling system and the integer quantization of the Hall conductance in this
system. We provide a correct formula of charge current in this system and the
careful consideration of extra currents provides a stronger theoretical basis
for the... | cond-mat.mes-hall | we study the extra term of particle current in a 2d kcubic rashba spinorbit coupling system and the integer quantization of the hall conductance in this system we provide a correct formula of charge current in this system and the careful consideration of extra currents provides a stronger theoretical basis for the theo... | [['we', 'study', 'the', 'extra', 'term', 'of', 'particle', 'current', 'in', 'a', '2d', 'kcubic', 'rashba', 'spinorbit', 'coupling', 'system', 'and', 'the', 'integer', 'quantization', 'of', 'the', 'hall', 'conductance', 'in', 'this', 'system', 'we', 'provide', 'a', 'correct', 'formula', 'of', 'charge', 'current', 'in', ... | [-0.2103724231560444, 0.12282182353984324, -0.07567606532886144, 0.037285971510667176, -0.06109652165023069, -0.155423836741266, 0.021559715909402696, 0.2900071129683525, -0.26078344888294175, -0.2890155795030296, 0.03650809390725748, -0.2659782733138737, -0.14672520552431384, 0.17674806053307088, -0.016442412118081964... |
707.1473 | On l^p norms of weighted mean matrices | We study $l^{p}$ operator norms of weighted mean matrices using the
approaches of Kaluza-Szeg\"o and Redheffer. As an application, we prove a
conjecture of Bennett.
| math.FA | we study lp operator norms of weighted mean matrices using the approaches of kaluzaszego and redheffer as an application we prove a conjecture of bennett | [['we', 'study', 'lp', 'operator', 'norms', 'of', 'weighted', 'mean', 'matrices', 'using', 'the', 'approaches', 'of', 'kaluzaszego', 'and', 'redheffer', 'as', 'an', 'application', 'we', 'prove', 'a', 'conjecture', 'of', 'bennett']] | [-0.09914047294296324, 0.01626468029341292, -0.1046351376377667, 0.1098910579457879, 0.016628027195110917, -0.07237292878562585, 0.045677768997848034, 0.3376850700005889, -0.32392765026694786, -0.21194116463690685, 0.15828875463921577, -0.27027146688002784, -0.22077395549664894, 0.19215344497933984, -0.1423575285201271... |
707.1474 | Integrable operators and squares of Hankel Matrices | In this note, we find sufficient conditions for an operator with kernel of
the form $A(x)B(y)-A(x)B(y)/(x-y)$ (which we call a Tracy-Widom type operator)
to be the square of a Hankel operator. We consider two contexts: infinite
matrices on $\ell^2$, and integral operators on the Hardy space
$H^2(\mathbb{T})$. The res... | math.FA | in this note we find sufficient conditions for an operator with kernel of the form axbyaxbyxy which we call a tracywidom type operator to be the square of a hankel operator we consider two contexts infinite matrices on ell2 and integral operators on the hardy space h2mathbbt the results can be applied to the discrete b... | [['in', 'this', 'note', 'we', 'find', 'sufficient', 'conditions', 'for', 'an', 'operator', 'with', 'kernel', 'of', 'the', 'form', 'axbyaxbyxy', 'which', 'we', 'call', 'a', 'tracywidom', 'type', 'operator', 'to', 'be', 'the', 'square', 'of', 'a', 'hankel', 'operator', 'we', 'consider', 'two', 'contexts', 'infinite', 'ma... | [-0.09541996548162593, 0.12380677000680496, -0.09313468818342494, 0.11220227025689618, -0.08923341381934381, -0.07797928729785546, -0.019021130611954797, 0.3921238395775999, -0.30322051384756643, -0.13352744690623256, 0.1741574753954586, -0.27823346202832555, -0.21161510821642174, 0.1653482157797102, -0.088780586788010... |
707.1475 | Dynamical laws of superenergy in General Relativity | The Bel and Bel-Robinson tensors were introduced nearly fifty years ago in an
attempt to generalize to gravitation the energy-momentum tensor of
electromagnetism. This generalization was successful from the mathematical
point of view because these tensors share mathematical properties which are
remarkably similar to ... | gr-qc | the bel and belrobinson tensors were introduced nearly fifty years ago in an attempt to generalize to gravitation the energymomentum tensor of electromagnetism this generalization was successful from the mathematical point of view because these tensors share mathematical properties which are remarkably similar to those... | [['the', 'bel', 'and', 'belrobinson', 'tensors', 'were', 'introduced', 'nearly', 'fifty', 'years', 'ago', 'in', 'an', 'attempt', 'to', 'generalize', 'to', 'gravitation', 'the', 'energymomentum', 'tensor', 'of', 'electromagnetism', 'this', 'generalization', 'was', 'successful', 'from', 'the', 'mathematical', 'point', 'o... | [-0.12709145957534468, 0.1131546024629071, -0.11295913084378016, 0.09974040103259128, -0.16987054577539765, -0.07423253233278691, -0.041116899054700874, 0.3363002259409148, -0.23668236615871333, -0.3080085781741873, 0.02743191412120158, -0.23682010246412222, -0.15658813599011792, 0.12744525034994, -0.026425286594036097... |
707.1476 | Modified Shephard's problem on projections of convex bodies | We disprove a conjecture of A. Koldobsky asking whether it is enough to
compare $(n-2)$-derivatives of the projection functions of two symmetric convex
bodies in the Shephard problem in order to get a positive answer in all
dimensions.
| math.MG | we disprove a conjecture of a koldobsky asking whether it is enough to compare n2derivatives of the projection functions of two symmetric convex bodies in the shephard problem in order to get a positive answer in all dimensions | [['we', 'disprove', 'a', 'conjecture', 'of', 'a', 'koldobsky', 'asking', 'whether', 'it', 'is', 'enough', 'to', 'compare', 'n2derivatives', 'of', 'the', 'projection', 'functions', 'of', 'two', 'symmetric', 'convex', 'bodies', 'in', 'the', 'shephard', 'problem', 'in', 'order', 'to', 'get', 'a', 'positive', 'answer', 'in... | [-0.10861757745009822, 0.06762878725154174, -0.09466787880739651, 0.12769057630951441, -0.08429603564326425, -0.15607744411288485, 0.019704539530180597, 0.32584830992729275, -0.2617796750084774, -0.23418123144153002, 0.11880175428578278, -0.30027077769281696, -0.15000251861842903, 0.13598723795164275, -0.11033346058448... |
707.1477 | Integration of iron in natural and synthetic Al-pyrophyllites: an
infrared spectroscopic study | Numerous studies focus on the relationships between chemical composition and
OHband positions in the infrared (IR) spectra of micaceous minerals. These
studies are based on the coexistence, in dioctahedral micas or smectites, of
several cationic pairs around the hydroxyl group which each produce a
characteristic band... | physics.geo-ph | numerous studies focus on the relationships between chemical composition and ohband positions in the infrared ir spectra of micaceous minerals these studies are based on the coexistence in dioctahedral micas or smectites of several cationic pairs around the hydroxyl group which each produce a characteristic band in the... | [['numerous', 'studies', 'focus', 'on', 'the', 'relationships', 'between', 'chemical', 'composition', 'and', 'ohband', 'positions', 'in', 'the', 'infrared', 'ir', 'spectra', 'of', 'micaceous', 'minerals', 'these', 'studies', 'are', 'based', 'on', 'the', 'coexistence', 'in', 'dioctahedral', 'micas', 'or', 'smectites', '... | [-0.04778636502591257, 0.14061261038001202, -0.04826731043268498, 0.0357075865534704, -0.013433474294825571, -0.09018233197029947, 0.09105576507900429, 0.46365364715221186, -0.25477611737027134, -0.3081893707087208, 0.058639619350610184, -0.3360450158783781, -0.09088227918513025, 0.13906102800419562, 0.0070051908137410... |
707.1478 | A Dipole Vortex Model of Obscuring Tori in Active Galaxy Nuclei | The torus concept as an essential structural component of active galactic
nuclei (AGN) is generally accepted. Here, the situation is discussed when the
torus "twisting" by the radiation or wind transforms it into a dipole toroidal
vortex which in turn can be a source of matter replenishing the accretion disk.
Thus em... | astro-ph | the torus concept as an essential structural component of active galactic nuclei agn is generally accepted here the situation is discussed when the torus twisting by the radiation or wind transforms it into a dipole toroidal vortex which in turn can be a source of matter replenishing the accretion disk thus emerging in... | [['the', 'torus', 'concept', 'as', 'an', 'essential', 'structural', 'component', 'of', 'active', 'galactic', 'nuclei', 'agn', 'is', 'generally', 'accepted', 'here', 'the', 'situation', 'is', 'discussed', 'when', 'the', 'torus', 'twisting', 'by', 'the', 'radiation', 'or', 'wind', 'transforms', 'it', 'into', 'a', 'dipole... | [-0.08563460696649809, 0.17154181156729464, -0.046737148345877916, 0.16262106324295297, -0.11040032531421345, -0.09983957632301518, -0.014669331954792142, 0.4019391506444663, -0.20431932506079858, -0.29358627169858664, 0.10455442330679104, -0.22445459790805428, -0.06441306368707536, 0.23731187279246604, -0.029708445887... |
707.1479 | Dark matter in low mass surface density galaxies | Low mass surface density spiral and irregular galaxies like low surface
brightness (LSB) and dwarf galaxies are unique laboratories to study the
dynamical properties of Dark Matter halos because their mass is generally
dominated by dark matter at all galactocentric radii. We present results from
the largest sample ev... | astro-ph | low mass surface density spiral and irregular galaxies like low surface brightness lsb and dwarf galaxies are unique laboratories to study the dynamical properties of dark matter halos because their mass is generally dominated by dark matter at all galactocentric radii we present results from the largest sample ever as... | [['low', 'mass', 'surface', 'density', 'spiral', 'and', 'irregular', 'galaxies', 'like', 'low', 'surface', 'brightness', 'lsb', 'and', 'dwarf', 'galaxies', 'are', 'unique', 'laboratories', 'to', 'study', 'the', 'dynamical', 'properties', 'of', 'dark', 'matter', 'halos', 'because', 'their', 'mass', 'is', 'generally', 'd... | [-0.07957041747046306, 0.13256280706948875, -0.14043499123277692, 0.15577002927859532, -0.11128611955791712, -0.0006297698130177142, -0.037939763439627475, 0.4256525024333421, -0.09573876234593198, -0.42872396253925915, 0.023221373240470283, -0.2920542756533798, -0.0020530806196963087, 0.18854730844716816, -0.031773843... |
707.148 | IRVO: an Interaction Model for designing Collaborative Mixed Reality
systems | This paper presents an interaction model adapted to mixed reality
environments known as IRVO (Interacting with Real and Virtual Objects). IRVO
aims at modeling the interaction between one or more users and the Mixed
Reality system by representing explicitly the objects and tools involved and
their relationship. IRVO ... | cs.HC | this paper presents an interaction model adapted to mixed reality environments known as irvo interacting with real and virtual objects irvo aims at modeling the interaction between one or more users and the mixed reality system by representing explicitly the objects and tools involved and their relationship irvo covers... | [['this', 'paper', 'presents', 'an', 'interaction', 'model', 'adapted', 'to', 'mixed', 'reality', 'environments', 'known', 'as', 'irvo', 'interacting', 'with', 'real', 'and', 'virtual', 'objects', 'irvo', 'aims', 'at', 'modeling', 'the', 'interaction', 'between', 'one', 'or', 'more', 'users', 'and', 'the', 'mixed', 're... | [-0.0872469537804598, 0.06117281711224692, -0.0725720299940024, 0.06918291421329957, -0.06980344128336698, -0.11945270491202199, 0.006444698444471532, 0.36978117396522847, -0.25372374362297473, -0.32911650296891964, 0.10336438614490723, -0.25318462028360317, -0.22671675517053771, 0.17818338364096625, -0.082289041622379... |
707.1481 | Measurement of Nuclear Transparency for the A(e,e' pi^+) Reaction | We have measured the nuclear transparency of the A(e,e' pi^+) process in
^{2}H,^{12}C, ^{27}Al, ^{63}Cu and ^{197}Au targets. These measurements were
performed at the Jefferson Laboratory over a four momentum transfer squared
range Q^2 = 1.1 - 4.7 (GeV/c)^2. The nuclear transparency was extracted as the
super-ratio o... | nucl-ex hep-ph nucl-th | we have measured the nuclear transparency of the aee pi process in 2h12c 27al 63cu and 197au targets these measurements were performed at the jefferson laboratory over a four momentum transfer squared range q2 11 47 gevc2 the nuclear transparency was extracted as the superratio of sigma_asigma_h from data to a model of... | [['we', 'have', 'measured', 'the', 'nuclear', 'transparency', 'of', 'the', 'aee', 'pi', 'process', 'in', '2h12c', '27al', '63cu', 'and', '197au', 'targets', 'these', 'measurements', 'were', 'performed', 'at', 'the', 'jefferson', 'laboratory', 'over', 'a', 'four', 'momentum', 'transfer', 'squared', 'range', 'q2', '11', ... | [-0.014103412060325757, 0.21439870128201113, -0.11770362769990848, 0.08714914064566984, 0.027547077741473913, -0.06304603677967356, 0.054068661923520264, 0.3825663165085845, -0.20917086204410426, -0.3393212847204672, -0.015143634545772026, -0.36570393509334986, 0.050060383313231996, 0.18886834838841524, 0.0755519183352... |
707.1482 | The effect of baryon cooling on the statistics of giant arcs and
multiple quasars | The statistics of giant arcs and large separation lensed quasars provide
powerful constraints for the parameters of the underlying cosmological model.
So far, most investigations have been carried out using pure dark matter
simulations. Here we present a recipe for including the effects of baryon
cooling (i.e. large ... | astro-ph | the statistics of giant arcs and large separation lensed quasars provide powerful constraints for the parameters of the underlying cosmological model so far most investigations have been carried out using pure dark matter simulations here we present a recipe for including the effects of baryon cooling ie large galaxy f... | [['the', 'statistics', 'of', 'giant', 'arcs', 'and', 'large', 'separation', 'lensed', 'quasars', 'provide', 'powerful', 'constraints', 'for', 'the', 'parameters', 'of', 'the', 'underlying', 'cosmological', 'model', 'so', 'far', 'most', 'investigations', 'have', 'been', 'carried', 'out', 'using', 'pure', 'dark', 'matter... | [-0.08214631801015361, 0.13514955620552208, -0.051979096472620015, 0.11120187341820131, -0.09674164319926119, -0.08609781298020207, 0.04669203683040402, 0.32800000287750936, -0.1376348591734926, -0.4010837948055449, 0.028611593532164626, -0.31756078417194966, -0.01717533780829915, 0.20125547973009764, 0.048259167343292... |
707.1483 | On the YM and QCD spectra from five dimensional strings | We consider a non-critical five dimensional string setup which could provide
a dual description of QCD in the limit of large number of colors and flavors.
The model corresponds to N_c color D3-branes and N_f D4/anti D4-brane pairs
supporting flavor degrees of freedom. The matching of the string model spectrum
with th... | hep-th hep-lat hep-ph | we consider a noncritical five dimensional string setup which could provide a dual description of qcd in the limit of large number of colors and flavors the model corresponds to n_c color d3branes and n_f d4anti d4brane pairs supporting flavor degrees of freedom the matching of the string model spectrum with the dual f... | [['we', 'consider', 'a', 'noncritical', 'five', 'dimensional', 'string', 'setup', 'which', 'could', 'provide', 'a', 'dual', 'description', 'of', 'qcd', 'in', 'the', 'limit', 'of', 'large', 'number', 'of', 'colors', 'and', 'flavors', 'the', 'model', 'corresponds', 'to', 'n_c', 'color', 'd3branes', 'and', 'n_f', 'd4anti'... | [-0.15840408678299614, 0.21176268604384468, -0.12189420361426614, 0.0740474062941281, -0.03879632151109122, -0.12531827262137085, 0.03818709229900768, 0.2853981672586607, -0.12079429334317822, -0.2745135947230405, 0.0629325152493991, -0.2907615636719302, -0.08714641762586932, 0.04276909698576977, -0.0532101085021471, 0... |
707.1484 | Instability of reconstruction of the low CMB multipoles | We discuss the problem of the bias of the Internal Linear Combination (ILC)
CMB map and show that it is closely related to the coefficient of
cross-correlation K(l) of the true CMB and the foreground for each multipole l.
We present analysis of the cross-correlation for the WMAP ILC quadrupole and
octupole from the f... | astro-ph | we discuss the problem of the bias of the internal linear combination ilc cmb map and show that it is closely related to the coefficient of crosscorrelation kl of the true cmb and the foreground for each multipole l we present analysis of the crosscorrelation for the wmap ilc quadrupole and octupole from the first ilci... | [['we', 'discuss', 'the', 'problem', 'of', 'the', 'bias', 'of', 'the', 'internal', 'linear', 'combination', 'ilc', 'cmb', 'map', 'and', 'show', 'that', 'it', 'is', 'closely', 'related', 'to', 'the', 'coefficient', 'of', 'crosscorrelation', 'kl', 'of', 'the', 'true', 'cmb', 'and', 'the', 'foreground', 'for', 'each', 'mu... | [-0.10452235935132621, 0.08493678602116073, -0.0595949902495383, 0.07653696694840476, -0.06731379440729963, -0.07507846192958965, -0.008801519150352653, 0.34859289180706526, -0.28055767826827277, -0.2807551682883344, 0.07256615833087149, -0.32773864565818916, -0.10828156591228702, 0.19054264361769252, 0.033278676482629... |
707.1485 | Descent on Elliptic Curves and Hilbert's Tenth Problem | Descent via an isogeny on an elliptic curve is used to construct two subrings
of the field of rational numbers, which are complementary in a strong sense,
and for which Hilbert's Tenth Problem is undecidable. This method further
develops that of Poonen, who used elliptic divisibility sequences to obtain
undecidabilit... | math.NT math.LO | descent via an isogeny on an elliptic curve is used to construct two subrings of the field of rational numbers which are complementary in a strong sense and for which hilberts tenth problem is undecidable this method further develops that of poonen who used elliptic divisibility sequences to obtain undecidability resul... | [['descent', 'via', 'an', 'isogeny', 'on', 'an', 'elliptic', 'curve', 'is', 'used', 'to', 'construct', 'two', 'subrings', 'of', 'the', 'field', 'of', 'rational', 'numbers', 'which', 'are', 'complementary', 'in', 'a', 'strong', 'sense', 'and', 'for', 'which', 'hilberts', 'tenth', 'problem', 'is', 'undecidable', 'this', ... | [-0.1774235617179992, 0.03276391364920143, -0.15816003822926747, 0.11815603637191767, -0.10990429877982301, -0.14865655578294043, -0.03023103043689566, 0.28574016437692157, -0.4030589802285372, -0.26836946142553275, 0.11125562878885954, -0.256296378165736, -0.1056529943341926, 0.302347460351253, -0.16659546196776426, 0... |
707.1486 | The modulus of continuity of Wegner estimates for random Schr\"odinger
operators on metric graphs | We consider an alloy type potential on an infinite metric graph. We assume a
covering condition on the single site potentials. For random Schr\"odingers
operator associated with the alloy type potential restricted to finite volume
subgraphs we prove a Wegner estimate which reproduces the modulus of continuity
of the ... | math.SP math-ph math.MP | we consider an alloy type potential on an infinite metric graph we assume a covering condition on the single site potentials for random schrodingers operator associated with the alloy type potential restricted to finite volume subgraphs we prove a wegner estimate which reproduces the modulus of continuity of the single... | [['we', 'consider', 'an', 'alloy', 'type', 'potential', 'on', 'an', 'infinite', 'metric', 'graph', 'we', 'assume', 'a', 'covering', 'condition', 'on', 'the', 'single', 'site', 'potentials', 'for', 'random', 'schrodingers', 'operator', 'associated', 'with', 'the', 'alloy', 'type', 'potential', 'restricted', 'to', 'finit... | [-0.12754310966759433, 0.11488460848674743, -0.05671715069959154, 0.06454965311339217, -0.055813671036272265, -0.12634603558566238, 0.07335858072963405, 0.36330076813942097, -0.3019228261269507, -0.20401148775928332, 0.06585746358499908, -0.31344309546908394, -0.07078356049729695, 0.13345004718170547, -0.07398307280706... |
707.1487 | Traversable wormholes: minimum violation of null energy condition
revisited | It was argued in literature that traversable wormholes can exist with
arbitrarily small violation of null energy conditions. We show that if the
amount of exotic material near the wormhole throat tends to zero, either this
leads to a horn instead of a wormhole or the throat approaches the horizon in
such a way that i... | gr-qc astro-ph hep-th | it was argued in literature that traversable wormholes can exist with arbitrarily small violation of null energy conditions we show that if the amount of exotic material near the wormhole throat tends to zero either this leads to a horn instead of a wormhole or the throat approaches the horizon in such a way that infni... | [['it', 'was', 'argued', 'in', 'literature', 'that', 'traversable', 'wormholes', 'can', 'exist', 'with', 'arbitrarily', 'small', 'violation', 'of', 'null', 'energy', 'conditions', 'we', 'show', 'that', 'if', 'the', 'amount', 'of', 'exotic', 'material', 'near', 'the', 'wormhole', 'throat', 'tends', 'to', 'zero', 'either... | [-0.19875185456006758, 0.10969680618314494, -0.14308565103208587, 0.10137748071405615, -0.1302566052707393, -0.1868858142500563, 0.020170476214374386, 0.3086186885353058, -0.18554924514084573, -0.29130344738763186, 0.1022132251734635, -0.2892462230858303, -0.09908609020508706, 0.10858781226805501, -0.10067891461808505,... |
707.1488 | First Results from the DRIFT-IIa Dark Matter Detector | Data from the DRIFT-IIa directional dark matter experiment are presented,
collected during a near continuous 6 month running period. A detailed
calibration analysis comparing data from gamma-ray, x-ray and neutron sources
to a GEANT4 Monte Carlo simulations reveals an efficiency for detection of
neutron induced recoi... | hep-ex | data from the driftiia directional dark matter experiment are presented collected during a near continuous 6 month running period a detailed calibration analysis comparing data from gammaray xray and neutron sources to a geant4 monte carlo simulations reveals an efficiency for detection of neutron induced recoils of 94... | [['data', 'from', 'the', 'driftiia', 'directional', 'dark', 'matter', 'experiment', 'are', 'presented', 'collected', 'during', 'a', 'near', 'continuous', '6', 'month', 'running', 'period', 'a', 'detailed', 'calibration', 'analysis', 'comparing', 'data', 'from', 'gammaray', 'xray', 'and', 'neutron', 'sources', 'to', 'a'... | [-0.009216304796528282, 0.16093118133887505, -0.10303633855050051, 0.13737135203517367, -0.04373933418419182, -0.09221826610723283, 0.05976591963979711, 0.3927740513733247, -0.16129045473881126, -0.37625470182411674, 0.04997280356190281, -0.39325239351852154, 0.04931991097585457, 0.2666144108899483, -0.0116008691256865... |
707.1489 | Is there an eta-3He quasi--bound state ? | The observed variation of the total cross section for the dp -> 3He eta
reaction near threshold means that the magnitude of the s--wave amplitude falls
very rapidly with the eta centre--of--mass momentum. It is shown here that
recent measurements of the momentum dependence of the angular distribution
imply a strong v... | nucl-ex nucl-th | the observed variation of the total cross section for the dp 3he eta reaction near threshold means that the magnitude of the swave amplitude falls very rapidly with the eta centreofmass momentum it is shown here that recent measurements of the momentum dependence of the angular distribution imply a strong variation als... | [['the', 'observed', 'variation', 'of', 'the', 'total', 'cross', 'section', 'for', 'the', 'dp', '3he', 'eta', 'reaction', 'near', 'threshold', 'means', 'that', 'the', 'magnitude', 'of', 'the', 'swave', 'amplitude', 'falls', 'very', 'rapidly', 'with', 'the', 'eta', 'centreofmass', 'momentum', 'it', 'is', 'shown', 'here'... | [-0.13872148332600112, 0.21907432392154905, -0.1287157470866408, 0.08021143612859305, -0.022354201710020952, -0.05107526802550472, 0.0679020768888718, 0.3064920436432162, -0.24930133362597023, -0.2880822822493924, -0.0014316366247261283, -0.3090183887715367, -0.05861962409372526, 0.1834385121950287, 0.07364969439169561... |
707.149 | Fast computing of velocity field for flows in industrial burners and
pumps | In this work we present a technique of fast numerical computation for
solutions of Navier-Stokes equations in the case of flows of industrial
interest. At first the partial differential equations are translated into a set
of nonlinear ordinary differential equations using the geometrical shape of the
domain where the... | math.NA cs.MS | in this work we present a technique of fast numerical computation for solutions of navierstokes equations in the case of flows of industrial interest at first the partial differential equations are translated into a set of nonlinear ordinary differential equations using the geometrical shape of the domain where the flo... | [['in', 'this', 'work', 'we', 'present', 'a', 'technique', 'of', 'fast', 'numerical', 'computation', 'for', 'solutions', 'of', 'navierstokes', 'equations', 'in', 'the', 'case', 'of', 'flows', 'of', 'industrial', 'interest', 'at', 'first', 'the', 'partial', 'differential', 'equations', 'are', 'translated', 'into', 'a', ... | [-0.17135748346853588, 0.0130030588984179, -0.0821761199247299, -0.023201965958449162, -0.0705336953772025, -0.11993386648181412, -0.016546659880421227, 0.3366074780623118, -0.29039066167444816, -0.3048680010665622, 0.15015513559855106, -0.2527188263574822, -0.13364334384807283, 0.25940434539030927, -0.0047276094449140... |
707.1491 | Secondary Baryon Asymmetry in pi(+-)p Collisions | The process of secondary baryon production in pi(+-)p collisions at high
energies in the central and forward fragmentation regions is considered in the
framework of the Quark-Gluon String Model. The contribution of the
string-junction mechanism to the baryon production is analysed. The results of
numerical calculatio... | hep-ph | the process of secondary baryon production in pip collisions at high energies in the central and forward fragmentation regions is considered in the framework of the quarkgluon string model the contribution of the stringjunction mechanism to the baryon production is analysed the results of numerical calculations are in ... | [['the', 'process', 'of', 'secondary', 'baryon', 'production', 'in', 'pip', 'collisions', 'at', 'high', 'energies', 'in', 'the', 'central', 'and', 'forward', 'fragmentation', 'regions', 'is', 'considered', 'in', 'the', 'framework', 'of', 'the', 'quarkgluon', 'string', 'model', 'the', 'contribution', 'of', 'the', 'strin... | [-0.09304388460392753, 0.17001349482840547, -0.1106063761205102, 0.13253698674297992, 0.02851252881810069, -0.03643746000404159, 0.037673077856500946, 0.30414771996438505, -0.18254859251125405, -0.24966241015742222, -0.02918579299778988, -0.37157129449769855, 0.04992557317018509, 0.13899461164837704, 0.0724635183811187... |
707.1492 | Electronic structure of heavily-doped graphene: the role of foreign atom
states | Using density functional theory calculations we investigate the electronic
structure of graphene doped by deposition of foreign atoms. We demonstrate
that, as the charge transfer to the graphene layer increases, the band
structure of the pristine graphene sheet is substantially affected. This is
particularly relevant... | cond-mat.mtrl-sci cond-mat.mes-hall cond-mat.supr-con | using density functional theory calculations we investigate the electronic structure of graphene doped by deposition of foreign atoms we demonstrate that as the charge transfer to the graphene layer increases the band structure of the pristine graphene sheet is substantially affected this is particularly relevant when ... | [['using', 'density', 'functional', 'theory', 'calculations', 'we', 'investigate', 'the', 'electronic', 'structure', 'of', 'graphene', 'doped', 'by', 'deposition', 'of', 'foreign', 'atoms', 'we', 'demonstrate', 'that', 'as', 'the', 'charge', 'transfer', 'to', 'the', 'graphene', 'layer', 'increases', 'the', 'band', 'str... | [-0.1414786816086972, 0.19549999270390161, 0.012228743641593267, 0.0442303897974294, 0.02202707352199203, -0.16494395430969794, 0.1294228263578825, 0.40642687222209034, -0.2949899162283153, -0.2641483470797539, -0.08054214406769547, -0.37015147952318894, -0.11999930688510026, 0.13582061050417576, 0.0421737114161869, -0... |
707.1493 | The Role of Exploding QSOs in Explosive Models of Evolution, Formation
and End of Galaxies | In this work we analise the role and evidence of exploding BAL + IR + Fe II
QSOs, and their relation with new -and previous- explosive models for
evolution, formation and end of galaxies.
| astro-ph | in this work we analise the role and evidence of exploding bal ir fe ii qsos and their relation with new and previous explosive models for evolution formation and end of galaxies | [['in', 'this', 'work', 'we', 'analise', 'the', 'role', 'and', 'evidence', 'of', 'exploding', 'bal', 'ir', 'fe', 'ii', 'qsos', 'and', 'their', 'relation', 'with', 'new', 'and', 'previous', 'explosive', 'models', 'for', 'evolution', 'formation', 'and', 'end', 'of', 'galaxies']] | [-0.007897698669694364, 0.05406472718459554, 0.006178681389428675, 0.11456400538372691, -0.0906659762840718, -0.08298967318842188, 0.08390911424066871, 0.46778422011993825, -0.09751986163610127, -0.3426910947309807, 0.05970504547804012, -0.3049560794606805, -0.10911059158388525, 0.10633964149747044, -0.0156170823320280... |
707.1494 | Heisenberg Uncertainty Principle for the q-Bessel Fourier transform | In this paper we uses an I.I. Hirschman-W. Beckner entropy argument to give
an uncertainty inequality for the $q$-Bessel Fourier transform: $$
\mathcal{F}_{q,v}f(x)=c_{q,v}\int_{0}^{\infty}f(t)j_{v}(xt,q^{2})t^{2v
+1}d_{q}t, $$ where $j_v(x,q)$ is the normalized Hahn-Exton $q$-Bessel
function.
| math.CA | in this paper we uses an ii hirschmanw beckner entropy argument to give an uncertainty inequality for the qbessel fourier transform mathcalf_qvfxc_qvint_0inftyftj_vxtq2t2v 1d_qt where j_vxq is the normalized hahnexton qbessel function | [['in', 'this', 'paper', 'we', 'uses', 'an', 'ii', 'hirschmanw', 'beckner', 'entropy', 'argument', 'to', 'give', 'an', 'uncertainty', 'inequality', 'for', 'the', 'qbessel', 'fourier', 'transform', 'mathcalf_qvfxc_qvint_0inftyftj_vxtq2t2v', '1d_qt', 'where', 'j_vxq', 'is', 'the', 'normalized', 'hahnexton', 'qbessel', 'f... | [-0.06862376202587728, 0.0057927258582182095, -0.17732012023528418, 0.14850517900453675, -0.09794890706392902, -0.10974523680353607, -0.00315757526550442, 0.31363453026171084, -0.3280990017509019, -0.17212458672346892, 0.0834989460762935, -0.3501826550949503, -0.17657704761734716, 0.21634157747030258, -0.19570105902298... |
707.1495 | Sterile neutrinos as subdominant warm dark matter | In light of recent findings which seem to disfavor a scenario with (warm)
dark matter entirely constituted of sterile neutrinos produced via the
Dodelson-Widrow (DW) mechanism, we investigate the constraints attainable for
this mechanism by relaxing the usual hypothesis that the relic neutrino
abundance must necessar... | astro-ph hep-ph | in light of recent findings which seem to disfavor a scenario with warm dark matter entirely constituted of sterile neutrinos produced via the dodelsonwidrow dw mechanism we investigate the constraints attainable for this mechanism by relaxing the usual hypothesis that the relic neutrino abundance must necessarily acco... | [['in', 'light', 'of', 'recent', 'findings', 'which', 'seem', 'to', 'disfavor', 'a', 'scenario', 'with', 'warm', 'dark', 'matter', 'entirely', 'constituted', 'of', 'sterile', 'neutrinos', 'produced', 'via', 'the', 'dodelsonwidrow', 'dw', 'mechanism', 'we', 'investigate', 'the', 'constraints', 'attainable', 'for', 'this... | [-0.09398231393537454, 0.22118805856293727, -0.06675967957764384, 0.14487812990968627, -0.09635385044234535, -0.10602601346589866, 0.09374332990978033, 0.30980801241652617, -0.23372948633566978, -0.3507188792009988, 0.027029090634577216, -0.27807384180205486, -0.01849858234486272, 0.1797139000913669, 0.0497748759034420... |
707.1496 | Subsets of F_p^n without three term arithmetic progressions have several
large Fourier coefficients | Suppose that f : F_p^n -> [0,1] has expected value t in [p^(-n/9),1] (so, the
density t can be quite low!). Furthermore, suppose that support(f) has no
three-term arithmetic progressions. Then, we develop non-trivial lower bounds
for f_j, which is the jth largest Fourier coefficient of f.
This result is similar in ... | math.CO math.NT | suppose that f f_pn 01 has expected value t in pn91 so the density t can be quite low furthermore suppose that supportf has no threeterm arithmetic progressions then we develop nontrivial lower bounds for f_j which is the jth largest fourier coefficient of f this result is similar in spirit to that appearing in an earl... | [['suppose', 'that', 'f', 'f_pn', '01', 'has', 'expected', 'value', 't', 'in', 'pn91', 'so', 'the', 'density', 't', 'can', 'be', 'quite', 'low', 'furthermore', 'suppose', 'that', 'supportf', 'has', 'no', 'threeterm', 'arithmetic', 'progressions', 'then', 'we', 'develop', 'nontrivial', 'lower', 'bounds', 'for', 'f_j', '... | [-0.1314433638646733, 0.14642530637458548, -0.11600853702984751, 0.02865933607565239, -0.08785947617376223, -0.10402264512144029, -0.004194868442136794, 0.32167503917589785, -0.2335315586492652, -0.24958755570463836, 0.11289846922853031, -0.2798127625323832, -0.18046115464298054, 0.22441599123179912, -0.096664252062328... |
707.1497 | Polaritonic characteristics of insulator and superfluid phases in a
coupled-cavity array | Recent studies of quantum phase transitions in coupled atom-cavity arrays
have focused on the similarities between such systems and the Bose-Hubbard
model. However, the bipartite nature of the atom-cavity systems that make up
the array introduces some differences. In order to examine the unique features
of the couple... | quant-ph | recent studies of quantum phase transitions in coupled atomcavity arrays have focused on the similarities between such systems and the bosehubbard model however the bipartite nature of the atomcavity systems that make up the array introduces some differences in order to examine the unique features of the coupledcavity ... | [['recent', 'studies', 'of', 'quantum', 'phase', 'transitions', 'in', 'coupled', 'atomcavity', 'arrays', 'have', 'focused', 'on', 'the', 'similarities', 'between', 'such', 'systems', 'and', 'the', 'bosehubbard', 'model', 'however', 'the', 'bipartite', 'nature', 'of', 'the', 'atomcavity', 'systems', 'that', 'make', 'up'... | [-0.20352257005474034, 0.1708835470355475, -0.04602473054794555, 0.01287946736742247, 0.008223008701300367, -0.18389951824606893, 0.05129488781243166, 0.38098051158235746, -0.23297467765378507, -0.28026794157724116, 0.05763463573988547, -0.30758668263343736, -0.1389976444163736, 0.19187177512844272, 0.04725670611901961... |
707.1498 | Hysteresis and re-entrant melting of a self-organized system of
classical particles confined in a parabolic trap | A self-organized system composed of classical particles confined in a
two-dimensional parabolic trap and interacting through a potential with a
short-range attractive part and long-range repulsive part is studied as
function of temperature. The influence of the competition between the
short-range attractive part of t... | cond-mat.soft | a selforganized system composed of classical particles confined in a twodimensional parabolic trap and interacting through a potential with a shortrange attractive part and longrange repulsive part is studied as function of temperature the influence of the competition between the shortrange attractive part of the inter... | [['a', 'selforganized', 'system', 'composed', 'of', 'classical', 'particles', 'confined', 'in', 'a', 'twodimensional', 'parabolic', 'trap', 'and', 'interacting', 'through', 'a', 'potential', 'with', 'a', 'shortrange', 'attractive', 'part', 'and', 'longrange', 'repulsive', 'part', 'is', 'studied', 'as', 'function', 'of'... | [-0.19030022069219818, 0.19368173296079616, -0.07476889172229598, 0.04286014853594031, 0.0012888851135160573, -0.1466459470093539, 0.03686171782730046, 0.3236964311479598, -0.2616722724046703, -0.27210343565589695, 0.0181568289606998, -0.3057075579787872, -0.1603812943681959, 0.12573974729333318, 0.08301689331902573, -... |
707.1499 | Polarization anisotropy in the optical properties of silicon ellipsoids | A new real space quantum mechanical approach with local field effects
included is applied to the calculation of the optical properties of silicon
nanocrystals. Silicon ellipsoids are studied and the role of surface
polarization is discussed in details. In particular, surface polarization is
shown to be responsible fo... | cond-mat.mtrl-sci | a new real space quantum mechanical approach with local field effects included is applied to the calculation of the optical properties of silicon nanocrystals silicon ellipsoids are studied and the role of surface polarization is discussed in details in particular surface polarization is shown to be responsible for a s... | [['a', 'new', 'real', 'space', 'quantum', 'mechanical', 'approach', 'with', 'local', 'field', 'effects', 'included', 'is', 'applied', 'to', 'the', 'calculation', 'of', 'the', 'optical', 'properties', 'of', 'silicon', 'nanocrystals', 'silicon', 'ellipsoids', 'are', 'studied', 'and', 'the', 'role', 'of', 'surface', 'pola... | [-0.10571234626695514, 0.12357753531874291, -0.05453931625622014, 0.048105124247423005, -0.03311151104964434, -0.15315136487276057, -0.05184089979766646, 0.4571241009832611, -0.2192766223960216, -0.28107989705694353, 0.058944617709448, -0.2668867852716219, -0.14276430449662877, 0.22785870156930907, 0.009247034802914613... |
707.15 | On the Correlation of Subevents in the ATLAS and CMS/Totem Experiments | We analyze the problem of correlating pp interaction data from the central
detectors with a subevent measured in an independent system of leading proton
detectors using FP420 as an example.
FP420 is an R&D project conducted by a collaboration formed by members of
ATLAS and CMS to investigate the possibility of dete... | hep-ex hep-ph | we analyze the problem of correlating pp interaction data from the central detectors with a subevent measured in an independent system of leading proton detectors using fp420 as an example fp420 is an rd project conducted by a collaboration formed by members of atlas and cms to investigate the possibility of detecting ... | [['we', 'analyze', 'the', 'problem', 'of', 'correlating', 'pp', 'interaction', 'data', 'from', 'the', 'central', 'detectors', 'with', 'a', 'subevent', 'measured', 'in', 'an', 'independent', 'system', 'of', 'leading', 'proton', 'detectors', 'using', 'fp420', 'as', 'an', 'example', 'fp420', 'is', 'an', 'rd', 'project', '... | [-0.10657279246230746, 0.17960228999130012, -0.10482240727508975, 0.08680518521595071, 0.006725467044359062, -0.14383009221637622, 0.029147565348498654, 0.3034814179177826, -0.25549610250776533, -0.3147311382736379, 0.03203513679279788, -0.31432011724335324, 0.023634046771936663, 0.18067685425709062, 0.0246158235798976... |
707.1501 | Random subgroups and analysis of the length-based and quotient attacks | In this paper we discuss generic properties of "random subgroups" of a given
group G. It turns out that in many groups G (even in most exotic of them) the
random subgroups have a simple algebraic structure and they "sit" inside G in a
very particular way. This gives a strong mathematical foundation for
cryptanalysis ... | math.GR cs.CR | in this paper we discuss generic properties of random subgroups of a given group g it turns out that in many groups g even in most exotic of them the random subgroups have a simple algebraic structure and they sit inside g in a very particular way this gives a strong mathematical foundation for cryptanalysis of several... | [['in', 'this', 'paper', 'we', 'discuss', 'generic', 'properties', 'of', 'random', 'subgroups', 'of', 'a', 'given', 'group', 'g', 'it', 'turns', 'out', 'that', 'in', 'many', 'groups', 'g', 'even', 'in', 'most', 'exotic', 'of', 'them', 'the', 'random', 'subgroups', 'have', 'a', 'simple', 'algebraic', 'structure', 'and',... | [-0.1501536894866149, 0.013234783691586927, -0.1594801482751791, 0.10428923707331705, -0.1199815278960159, -0.1982215061907482, 0.10870205849005288, 0.37599090645380784, -0.267337428483188, -0.2684657604986569, 0.10578541061931901, -0.2433065901423106, -0.2264485562700429, 0.2206288603010762, -0.1502605340538139, 0.011... |
707.1502 | Quasi-isometries Between Tubular Groups | We give a method of constructing maps between tubular groups inductively
according to a set of strategies. This map will be a quasi-isometry exactly
when the set of strategies is consistent. Conversely, if there exists a
quasi-isometry between tubular groups, then there is a consistent set of
strategies for them.
T... | math.GR math.GT | we give a method of constructing maps between tubular groups inductively according to a set of strategies this map will be a quasiisometry exactly when the set of strategies is consistent conversely if there exists a quasiisometry between tubular groups then there is a consistent set of strategies for them there is an ... | [['we', 'give', 'a', 'method', 'of', 'constructing', 'maps', 'between', 'tubular', 'groups', 'inductively', 'according', 'to', 'a', 'set', 'of', 'strategies', 'this', 'map', 'will', 'be', 'a', 'quasiisometry', 'exactly', 'when', 'the', 'set', 'of', 'strategies', 'is', 'consistent', 'conversely', 'if', 'there', 'exists'... | [-0.11830049889638673, 0.1307200993112421, -0.12939278878878022, 0.06717917991959121, -0.08669872499655845, -0.1867638558939879, 0.12534350327887508, 0.4757891489669334, -0.2968399348387191, -0.225002704134081, 0.1138818480093357, -0.2612495968865534, -0.1426495186453902, 0.21366458939020197, -0.12797561598140314, -0.0... |
707.1503 | ProbCD: enrichment analysis accounting for categorization uncertainty | As in many other areas of science, systems biology makes extensive use of
statistical association and significance estimates in contingency tables, a
type of categorical data analysis known in this field as enrichment (also
over-representation or enhancement) analysis. In spite of efforts to create
probabilistic anno... | q-bio.QM q-bio.GN | as in many other areas of science systems biology makes extensive use of statistical association and significance estimates in contingency tables a type of categorical data analysis known in this field as enrichment also overrepresentation or enhancement analysis in spite of efforts to create probabilistic annotations ... | [['as', 'in', 'many', 'other', 'areas', 'of', 'science', 'systems', 'biology', 'makes', 'extensive', 'use', 'of', 'statistical', 'association', 'and', 'significance', 'estimates', 'in', 'contingency', 'tables', 'a', 'type', 'of', 'categorical', 'data', 'analysis', 'known', 'in', 'this', 'field', 'as', 'enrichment', 'al... | [-0.05308465065507825, -0.0017662601853005346, -0.05306098885373788, 0.12003964134608273, -0.11730710900875248, -0.12857964345819076, 0.09038474699979376, 0.3836222158737083, -0.26953163816334597, -0.3329242010799687, 0.13032689199552694, -0.2701000746868824, -0.12000025409074981, 0.1752374280280737, -0.130639154647131... |
707.1504 | Perfect Fluidity in Atomic Physics | Experimental results obtained at the Relativistic Heavy Ion Collider (RHIC)
have been interpreted in terms of a strongly interacting quark gluon plasma.
The strongly interacting plasma is characterized by ``perfect fluidity'', i.e.
a ratio of shear viscosity to entropy density that saturates a proposed lower
bound. I... | nucl-th | experimental results obtained at the relativistic heavy ion collider rhic have been interpreted in terms of a strongly interacting quark gluon plasma the strongly interacting plasma is characterized by perfect fluidity ie a ratio of shear viscosity to entropy density that saturates a proposed lower bound in this contri... | [['experimental', 'results', 'obtained', 'at', 'the', 'relativistic', 'heavy', 'ion', 'collider', 'rhic', 'have', 'been', 'interpreted', 'in', 'terms', 'of', 'a', 'strongly', 'interacting', 'quark', 'gluon', 'plasma', 'the', 'strongly', 'interacting', 'plasma', 'is', 'characterized', 'by', 'perfect', 'fluidity', 'ie', ... | [-0.15655834055445217, 0.3208529064371311, -0.14235990210859614, 0.06867570929114356, 0.009717019129689638, -0.14812806970137474, -0.014702975390140306, 0.28101801742835864, -0.20794789997449556, -0.244570250852735, -0.044715941762672615, -0.3013444443463118, -0.02298828293327484, 0.15457424964126829, 0.053579622070764... |
707.1505 | Variation of Periods Modulo p in Arithmetic Dynamics | Let F : V --> V be a self-morphism of a quasiprojective variety defined over
a number field K and let P be a point in V(K) with infinite orbit under
iteration of F. For each prime ideal p of good reduction, let m_p(F,P) be the
size of the F-orbit of the reduction of P modulo p. Fix any e > 0. We show that
for almost ... | math.NT math.DS | let f v v be a selfmorphism of a quasiprojective variety defined over a number field k and let p be a point in vk with infinite orbit under iteration of f for each prime ideal p of good reduction let m_pfp be the size of the forbit of the reduction of p modulo p fix any e 0 we show that for almost all primes p in the s... | [['let', 'f', 'v', 'v', 'be', 'a', 'selfmorphism', 'of', 'a', 'quasiprojective', 'variety', 'defined', 'over', 'a', 'number', 'field', 'k', 'and', 'let', 'p', 'be', 'a', 'point', 'in', 'vk', 'with', 'infinite', 'orbit', 'under', 'iteration', 'of', 'f', 'for', 'each', 'prime', 'ideal', 'p', 'of', 'good', 'reduction', 'l... | [-0.2330232365699164, 0.1119121980007695, -0.1266510069785752, -0.03508496965046159, -0.0073249213311864046, -0.18493725847581338, 0.031414266408089246, 0.27081765232329397, -0.31821273413925677, -0.23796229818889378, -0.007177818820801103, -0.24482735195036592, -0.02077362246426015, 0.2040162355392829, -0.061016168959... |
707.1506 | Global Analysis of Fragmentation Functions for Protons and Charged
Hadrons | We present new sets of fragmentation functions for protons and inclusive
charged hadrons obtained in combined NLO QCD analyses of single-inclusive
hadron production in electron-positron annihilation, proton-proton collisions,
and deep-inelastic lepton-proton scattering. These analyses complement previous
results for ... | hep-ph | we present new sets of fragmentation functions for protons and inclusive charged hadrons obtained in combined nlo qcd analyses of singleinclusive hadron production in electronpositron annihilation protonproton collisions and deepinelastic leptonproton scattering these analyses complement previous results for pion and k... | [['we', 'present', 'new', 'sets', 'of', 'fragmentation', 'functions', 'for', 'protons', 'and', 'inclusive', 'charged', 'hadrons', 'obtained', 'in', 'combined', 'nlo', 'qcd', 'analyses', 'of', 'singleinclusive', 'hadron', 'production', 'in', 'electronpositron', 'annihilation', 'protonproton', 'collisions', 'and', 'deepi... | [-0.007263346023939769, 0.19953479587018272, -0.15511602612541003, 0.2048873405523516, 0.0030093917294460185, -0.013217723585993928, 0.0025090283049982696, 0.31975895870367393, -0.16623853509286968, -0.15468453826821027, -0.09967696265940663, -0.39097121210001845, 0.11770345971864812, 0.1469265581930385, 0.128244666163... |
707.1507 | Diffractive Neutral Pion Production, Chiral Symmetry and the Odderon | We discuss the diffractive photo- and electroproduction of a single neutral
pion at high energies where it can occur due to odderon exchange. We show that
this process is dynamically suppressed as a consequence of chiral symmetry. Our
result reconciles earlier theoretical expectations with the non-observation of
this... | hep-ph | we discuss the diffractive photo and electroproduction of a single neutral pion at high energies where it can occur due to odderon exchange we show that this process is dynamically suppressed as a consequence of chiral symmetry our result reconciles earlier theoretical expectations with the nonobservation of this react... | [['we', 'discuss', 'the', 'diffractive', 'photo', 'and', 'electroproduction', 'of', 'a', 'single', 'neutral', 'pion', 'at', 'high', 'energies', 'where', 'it', 'can', 'occur', 'due', 'to', 'odderon', 'exchange', 'we', 'show', 'that', 'this', 'process', 'is', 'dynamically', 'suppressed', 'as', 'a', 'consequence', 'of', '... | [-0.07674923658772718, 0.23136842550308095, -0.0993219750674268, 0.10091296171983641, -0.043740831215080676, -0.08995144758327846, 0.07322534683215268, 0.3704919143780774, -0.23219597495763616, -0.24617828899884925, -0.04150731443409242, -0.31540881654284164, -0.0775215533315478, 0.10919584016151287, 0.0447339376836430... |
707.1508 | How important are next-to-leading order models in predicting strange
particle spectra in p+p collisions at STAR ? | STAR has measured a variety of strange particle species in p + p collisions
at $\sqrt{s}$ = 200 GeV. These high statistics data are ideal for comparing to
existing leading- and next-to-leading order perturbative QCD (pQCD) models.
Next-to-leading (NLO) models have been successful in describing inclusive
hadron produc... | hep-ex | star has measured a variety of strange particle species in p p collisions at sqrts 200 gev these high statistics data are ideal for comparing to existing leading and nexttoleading order perturbative qcd pqcd models nexttoleading nlo models have been successful in describing inclusive hadron production using parameteriz... | [['star', 'has', 'measured', 'a', 'variety', 'of', 'strange', 'particle', 'species', 'in', 'p', 'p', 'collisions', 'at', 'sqrts', '200', 'gev', 'these', 'high', 'statistics', 'data', 'are', 'ideal', 'for', 'comparing', 'to', 'existing', 'leading', 'and', 'nexttoleading', 'order', 'perturbative', 'qcd', 'pqcd', 'models'... | [-0.016846861389591992, 0.16751543753932524, -0.15486405107038254, 0.14116495674775548, -0.017578637756257502, -0.08508619139364092, -0.041146850501229265, 0.39513563704513127, -0.1480563388313705, -0.3063271520425327, -0.04608787519239526, -0.338505621933982, 0.06299460118053096, 0.11455138820637692, 0.065744035809427... |
707.1509 | Bs Properties at the Tevatron | Results on Bs properties obtained by the CDF and D0 collaborations using the
data samples collected at the Tevatron Collider in the period 2002-2006 were
presented at the Hadron Collider Physics Symposium 2006 (Duke University,
Durham). The measurements of Bs mass and width differences are discussed in
details.
Pro... | hep-ex | results on bs properties obtained by the cdf and d0 collaborations using the data samples collected at the tevatron collider in the period 20022006 were presented at the hadron collider physics symposium 2006 duke university durham the measurements of bs mass and width differences are discussed in details prospects on ... | [['results', 'on', 'bs', 'properties', 'obtained', 'by', 'the', 'cdf', 'and', 'd0', 'collaborations', 'using', 'the', 'data', 'samples', 'collected', 'at', 'the', 'tevatron', 'collider', 'in', 'the', 'period', '20022006', 'were', 'presented', 'at', 'the', 'hadron', 'collider', 'physics', 'symposium', '2006', 'duke', 'u... | [-0.09517395253277432, 0.14388901996820913, -0.10503912232500517, 0.05961550006611367, -0.0694554023073702, -0.13576886026579413, 0.08820122663499945, 0.2809647802358209, -0.14918490061418044, -0.3583516389510389, 0.09775775645354415, -0.4053405345717477, 0.04095308910423921, 0.19449857909674362, 0.05318605644782311, 0... |
707.151 | STAR identifed particle measurements at high transverse momentum in p+p
$\sqrt{s}$ = 200 GeV | We present the STAR measurement of transverse momentum spectra at
mid-rapidity for identified particles in p+p collisions at $\sqrt{s}$ = 200
GeV. These high statistics data are ideal for comparing to existing leading-
and next-to-leading order (NLO) perturbative QCD calculations. Next-to-leading
models have been suc... | hep-ex | we present the star measurement of transverse momentum spectra at midrapidity for identified particles in pp collisions at sqrts 200 gev these high statistics data are ideal for comparing to existing leading and nexttoleading order nlo perturbative qcd calculations nexttoleading models have been successful in describin... | [['we', 'present', 'the', 'star', 'measurement', 'of', 'transverse', 'momentum', 'spectra', 'at', 'midrapidity', 'for', 'identified', 'particles', 'in', 'pp', 'collisions', 'at', 'sqrts', '200', 'gev', 'these', 'high', 'statistics', 'data', 'are', 'ideal', 'for', 'comparing', 'to', 'existing', 'leading', 'and', 'nextto... | [-0.01567970043218408, 0.19807297571969684, -0.1458062451879064, 0.13576484491820268, 9.865247501203648e-05, -0.08137513133876312, -0.04567728209076449, 0.38657715511418733, -0.1363998183962674, -0.30800954766499883, -0.06598562375942353, -0.3781442769731467, 0.1391898537090478, 0.11995714248041622, 0.12194410740630701... |
707.1511 | Distilling entanglement from cascades with partial "Which Path"
ambiguity | We develop a framework to calculate the density matrix of a pair of photons
emitted in a decay cascade with partial "which path" ambiguity. We describe an
appropriate entanglement distillation scheme which works also for certain
random cascades. The qualitative features of the distilled entanglement are
presented in ... | quant-ph cond-mat.str-el | we develop a framework to calculate the density matrix of a pair of photons emitted in a decay cascade with partial which path ambiguity we describe an appropriate entanglement distillation scheme which works also for certain random cascades the qualitative features of the distilled entanglement are presented in a two ... | [['we', 'develop', 'a', 'framework', 'to', 'calculate', 'the', 'density', 'matrix', 'of', 'a', 'pair', 'of', 'photons', 'emitted', 'in', 'a', 'decay', 'cascade', 'with', 'partial', 'which', 'path', 'ambiguity', 'we', 'describe', 'an', 'appropriate', 'entanglement', 'distillation', 'scheme', 'which', 'works', 'also', 'f... | [-0.11554698862780172, 0.20522867223917274, -0.11810773739722581, 0.08895890328261512, 0.04135342359912988, -0.1614726909633296, 0.02955559498887175, 0.3737054651316542, -0.25831319942162967, -0.24448134785947892, 0.017773383937310427, -0.2896225064372023, -0.11753733593445176, 0.17463112042213863, 0.016780832065985754... |
707.1512 | Mirror Duality in a Joyce Manifold | Previously the two of the authors defined a notion of dual Calabi-Yau
manifolds in a G_2 manifold, and described a process to obtain them. Here we
apply this process to a compact G_2 manifold, constructed by Joyce, and as a
result we obtain a pair of Borcea-Voisin Calabi-Yau manifolds, which are known
to be mirror du... | math.GT hep-th math.DG | previously the two of the authors defined a notion of dual calabiyau manifolds in a g_2 manifold and described a process to obtain them here we apply this process to a compact g_2 manifold constructed by joyce and as a result we obtain a pair of borceavoisin calabiyau manifolds which are known to be mirror duals of eac... | [['previously', 'the', 'two', 'of', 'the', 'authors', 'defined', 'a', 'notion', 'of', 'dual', 'calabiyau', 'manifolds', 'in', 'a', 'g_2', 'manifold', 'and', 'described', 'a', 'process', 'to', 'obtain', 'them', 'here', 'we', 'apply', 'this', 'process', 'to', 'a', 'compact', 'g_2', 'manifold', 'constructed', 'by', 'joyce... | [-0.15934065723065602, 0.049152066631211064, -0.10822402742707123, 0.13921299403153756, -0.13430471156755366, -0.17310627444126345, -0.0058079438947014886, 0.37304291362732145, -0.239741194803836, -0.2674081437684343, 0.13506668063188446, -0.2226310240546778, -0.17982156173783845, 0.16466501183113305, -0.15449140920950... |
707.1513 | Group velocity of gravitational waves in an expanding universe | The group velocity of gravitational waves in a flat Friedman-Robertson-Walker
universe is investigated. For plane waves with wavelength well inside the
horizon, and a universe filled with an ideal fluid with the pressure to density
ratio less than 1/3, the group velocity is greater than the velocity of light.
As a re... | gr-qc | the group velocity of gravitational waves in a flat friedmanrobertsonwalker universe is investigated for plane waves with wavelength well inside the horizon and a universe filled with an ideal fluid with the pressure to density ratio less than 13 the group velocity is greater than the velocity of light as a result a pl... | [['the', 'group', 'velocity', 'of', 'gravitational', 'waves', 'in', 'a', 'flat', 'friedmanrobertsonwalker', 'universe', 'is', 'investigated', 'for', 'plane', 'waves', 'with', 'wavelength', 'well', 'inside', 'the', 'horizon', 'and', 'a', 'universe', 'filled', 'with', 'an', 'ideal', 'fluid', 'with', 'the', 'pressure', 't... | [-0.19109110560976958, 0.2314557459961831, -0.07635848507680724, 0.045464370915598226, -0.08972886620930075, -0.05772586956061835, -0.0344993411357292, 0.33770743531661224, -0.21334736926926184, -0.29224302015057146, 0.07840854995492516, -0.3115554859766951, -0.00697873411205622, 0.20133668313676542, 0.0587138146748713... |
707.1514 | Effect of Two Level System Saturation on Charge Noise in Josephson
Junction Qubits | We show that charge noise $S_Q$ in Josephson qubits can be produced by
fluctuating two level systems (TLS) with electric dipole moments in the
substrate using a flat density of states. At high frequencies the frequency and
temperature dependence of the charge noise depends on the ratio $J/J_c$ of the
electromagnetic ... | cond-mat.mes-hall | we show that charge noise s_q in josephson qubits can be produced by fluctuating two level systems tls with electric dipole moments in the substrate using a flat density of states at high frequencies the frequency and temperature dependence of the charge noise depends on the ratio jj_c of the electromagnetic flux j to ... | [['we', 'show', 'that', 'charge', 'noise', 's_q', 'in', 'josephson', 'qubits', 'can', 'be', 'produced', 'by', 'fluctuating', 'two', 'level', 'systems', 'tls', 'with', 'electric', 'dipole', 'moments', 'in', 'the', 'substrate', 'using', 'a', 'flat', 'density', 'of', 'states', 'at', 'high', 'frequencies', 'the', 'frequenc... | [-0.17105386512981646, 0.256967023192176, -0.002828925250745986, 0.019624695481742612, 0.023594251474487068, -0.15844820069311105, 0.0494610130250373, 0.3867172270446368, -0.18287234475998126, -0.3106020938481063, 0.03513250647380989, -0.30913151379512704, -0.06167775917413604, 0.2198246281047392, -0.01437155779896547,... |
707.1515 | Properties of polynomial bases used in a line-surface intersection
algorithm | In [5], Srijuntongsiri and Vavasis propose the "Kantorovich-Test Subdivision
algorithm", or KTS, which is an algorithm for finding all zeros of a polynomial
system in a bounded region of the plane. This algorithm can be used to find the
intersections between a line and a surface. The main features of KTS are that
it ... | cs.NA cs.CG | in 5 srijuntongsiri and vavasis propose the kantorovichtest subdivision algorithm or kts which is an algorithm for finding all zeros of a polynomial system in a bounded region of the plane this algorithm can be used to find the intersections between a line and a surface the main features of kts are that it can operate ... | [['in', '5', 'srijuntongsiri', 'and', 'vavasis', 'propose', 'the', 'kantorovichtest', 'subdivision', 'algorithm', 'or', 'kts', 'which', 'is', 'an', 'algorithm', 'for', 'finding', 'all', 'zeros', 'of', 'a', 'polynomial', 'system', 'in', 'a', 'bounded', 'region', 'of', 'the', 'plane', 'this', 'algorithm', 'can', 'be', 'u... | [-0.155162453311641, 0.052733589707531794, -0.09338364515133435, 0.03515142392061534, -0.0607822726960876, -0.09548608901095576, 0.039741359284380454, 0.35451941166975304, -0.25751626477576794, -0.2852692508837208, 0.12563621391236665, -0.22778108780039474, -0.16267088072927435, 0.23897896202324773, -0.0299115131887447... |
707.1516 | Benchmark calculations for 3H, 4He, 16O and 40Ca with ab-initio
coupled-cluster theory | We present ab-initio calculations for 3H, 4He, 16O, and 40Ca based on
two-nucleon low-momentum interactions Vlowk within coupled-cluster theory. For
3H and 4He, our results are within 70 keV and 10 keV of the corresponding
Faddeev and Faddeev-Yakubovsky energies. We study in detail the convergence
with respect to the... | nucl-th | we present abinitio calculations for 3h 4he 16o and 40ca based on twonucleon lowmomentum interactions vlowk within coupledcluster theory for 3h and 4he our results are within 70 kev and 10 kev of the corresponding faddeev and faddeevyakubovsky energies we study in detail the convergence with respect to the size of the ... | [['we', 'present', 'abinitio', 'calculations', 'for', '3h', '4he', '16o', 'and', '40ca', 'based', 'on', 'twonucleon', 'lowmomentum', 'interactions', 'vlowk', 'within', 'coupledcluster', 'theory', 'for', '3h', 'and', '4he', 'our', 'results', 'are', 'within', '70', 'kev', 'and', '10', 'kev', 'of', 'the', 'corresponding',... | [0.053458421503844326, 0.19181522475523644, -0.05730342695709598, 0.12858288827007763, 0.08180031247360453, -0.08332508607218934, 0.04917385974063296, 0.4273888317944661, -0.12017061294069233, -0.2894415351386433, -0.12071755305347225, -0.39150704212537774, 0.00046558952922231124, 0.12988392745259486, 0.157820382799749... |
707.1517 | Environmental dependence of AGN activity in the supercluster A901/2 | We present XMM data for the supercluster A901/2, at z ~ 0.17, which is
combined with deep imaging and 17-band photometric redshifts (from the COMBO-17
survey), 2dF spectra and Spitzer 24um data, to identify AGN in the
supercluster. The 90ksec XMM image contains 139 point sources, of which 11 are
identified as supercl... | astro-ph | we present xmm data for the supercluster a9012 at z 017 which is combined with deep imaging and 17band photometric redshifts from the combo17 survey 2df spectra and spitzer 24um data to identify agn in the supercluster the 90ksec xmm image contains 139 point sources of which 11 are identified as supercluster agn with l... | [['we', 'present', 'xmm', 'data', 'for', 'the', 'supercluster', 'a9012', 'at', 'z', '017', 'which', 'is', 'combined', 'with', 'deep', 'imaging', 'and', '17band', 'photometric', 'redshifts', 'from', 'the', 'combo17', 'survey', '2df', 'spectra', 'and', 'spitzer', '24um', 'data', 'to', 'identify', 'agn', 'in', 'the', 'sup... | [-0.03133500636710475, 0.06182680844510388, -0.04098133504390716, 0.10542391231542246, -0.1003275128826499, -0.0651579329578413, 0.07370423690208958, 0.4867550907863511, -0.08699010373817549, -0.37131232269108294, 0.06743321234825998, -0.358965484092219, 0.020387211156388124, 0.17877366941215264, -0.010119302761999684,... |
707.1518 | Gluino Axion, Neutrino Seesaw, Dynamical Gaugino Mass, and A = 0
Supersymmetry | In the axionic solution of the strong CP problem, fermions which transform
under quantum chromodynamics (QCD) are required. In supersymmetry, by equating
U(1)_{PQ} with U(1)_R, the natural candidates are the gluinos, as pointed out
some years ago. A new specific implementation of this idea is proposed, linking
the gl... | hep-ph | in the axionic solution of the strong cp problem fermions which transform under quantum chromodynamics qcd are required in supersymmetry by equating u1_pq with u1_r the natural candidates are the gluinos as pointed out some years ago a new specific implementation of this idea is proposed linking the gluino axion scale ... | [['in', 'the', 'axionic', 'solution', 'of', 'the', 'strong', 'cp', 'problem', 'fermions', 'which', 'transform', 'under', 'quantum', 'chromodynamics', 'qcd', 'are', 'required', 'in', 'supersymmetry', 'by', 'equating', 'u1_pq', 'with', 'u1_r', 'the', 'natural', 'candidates', 'are', 'the', 'gluinos', 'as', 'pointed', 'out... | [-0.13907984870175522, 0.26178503361841043, -0.06488587225476901, 0.1901376646834736, -0.14011603775123754, -0.17244147701499363, 0.04472758777750035, 0.3302186504006386, -0.23474509567022322, -0.30584427538017434, 0.08477665827920039, -0.21761334180211028, -0.07955896362041434, 0.14848824940621852, -0.0197988490263621... |
707.1519 | Deformation Quantization of Almost Kahler Models and Lagrange-Finsler
Spaces | Finsler and Lagrange spaces can be equivalently represented as almost Kahler
manifolds enabled with a metric compatible canonical distinguished connection
structure generalizing the Levi Civita connection. The goal of this paper is to
perform a natural Fedosov-type deformation quantization of such geometries. All
con... | gr-qc hep-th math-ph math.MP math.SG | finsler and lagrange spaces can be equivalently represented as almost kahler manifolds enabled with a metric compatible canonical distinguished connection structure generalizing the levi civita connection the goal of this paper is to perform a natural fedosovtype deformation quantization of such geometries all construc... | [['finsler', 'and', 'lagrange', 'spaces', 'can', 'be', 'equivalently', 'represented', 'as', 'almost', 'kahler', 'manifolds', 'enabled', 'with', 'a', 'metric', 'compatible', 'canonical', 'distinguished', 'connection', 'structure', 'generalizing', 'the', 'levi', 'civita', 'connection', 'the', 'goal', 'of', 'this', 'paper... | [-0.20042383510684758, 0.0625292378990388, -0.05179095328703784, 0.12522406295236005, -0.21826013117995963, -0.17758127906474105, -0.07686143116249393, 0.38184031282077757, -0.30411625457437413, -0.2135707094546473, 0.062331661810739, -0.19804943895392252, -0.2286815752455017, 0.1709002055546367, -0.16564592172538764, ... |
707.152 | Shear viscosity of a superfluid Fermi gas in the unitarity limit | We compute the shear viscosity of a superfluid atomic Fermi gas in the
unitarity limit. The unitarity limit is characterized by a divergent scattering
length between the atoms, and it has been argued that this will result in a
very small viscosity. We show that in the low temperature T limit the shear
viscosity scale... | cond-mat.other hep-ph nucl-th | we compute the shear viscosity of a superfluid atomic fermi gas in the unitarity limit the unitarity limit is characterized by a divergent scattering length between the atoms and it has been argued that this will result in a very small viscosity we show that in the low temperature t limit the shear viscosity scales as ... | [['we', 'compute', 'the', 'shear', 'viscosity', 'of', 'a', 'superfluid', 'atomic', 'fermi', 'gas', 'in', 'the', 'unitarity', 'limit', 'the', 'unitarity', 'limit', 'is', 'characterized', 'by', 'a', 'divergent', 'scattering', 'length', 'between', 'the', 'atoms', 'and', 'it', 'has', 'been', 'argued', 'that', 'this', 'will... | [-0.17436209385807633, 0.22383012356448587, -0.1337083497281542, 0.023788813014166445, 0.01397736722838164, -0.08759111374601479, 0.11073682711807996, 0.23654294720797883, -0.2611207081216986, -0.2581568143171508, 0.04115319191534981, -0.3065283179919167, -0.057682250232655344, 0.16556096775078677, 0.008961688040006088... |
707.1521 | Reexamination of entanglement of superpositions | We find tight lower and upper bounds on the entanglement of a superposition
of two bipartite states in terms of the entanglement of the two states
constituting the superposition. Our upper bound is dramatically tighter than
the one presented in Phys. Rev. Lett 97, 100502 (2006) and our lower bound can
be used to prov... | quant-ph | we find tight lower and upper bounds on the entanglement of a superposition of two bipartite states in terms of the entanglement of the two states constituting the superposition our upper bound is dramatically tighter than the one presented in phys rev lett 97 100502 2006 and our lower bound can be used to provide lowe... | [['we', 'find', 'tight', 'lower', 'and', 'upper', 'bounds', 'on', 'the', 'entanglement', 'of', 'a', 'superposition', 'of', 'two', 'bipartite', 'states', 'in', 'terms', 'of', 'the', 'entanglement', 'of', 'the', 'two', 'states', 'constituting', 'the', 'superposition', 'our', 'upper', 'bound', 'is', 'dramatically', 'tight... | [-0.13686690330082044, 0.1902300086041743, -0.08031712381846526, 0.041861795292193575, 0.06080631668764082, -0.10683472481217574, 0.07428710674867034, 0.26726126803762534, -0.1794293504599905, -0.3191258947618983, 0.055168017838150264, -0.26493289992530744, -0.11114611022851684, 0.23086492776532064, -0.0372129290491681... |
707.1522 | Superexchange induced canted ferromagnetism in dilute magnets | We argue, in contrast to recent studies, that the antiferromagnetic
superexchange coupling between nearest neighbour spins does not fully destroy
the ferromagnetism in dilute magnets with long-ranged ferromagnetic couplings.
Above a critical coupling, we find a \textit{canted} ferromagnetic phase with
unsaturated mom... | cond-mat.dis-nn cond-mat.str-el | we argue in contrast to recent studies that the antiferromagnetic superexchange coupling between nearest neighbour spins does not fully destroy the ferromagnetism in dilute magnets with longranged ferromagnetic couplings above a critical coupling we find a textitcanted ferromagnetic phase with unsaturated moment we hav... | [['we', 'argue', 'in', 'contrast', 'to', 'recent', 'studies', 'that', 'the', 'antiferromagnetic', 'superexchange', 'coupling', 'between', 'nearest', 'neighbour', 'spins', 'does', 'not', 'fully', 'destroy', 'the', 'ferromagnetism', 'in', 'dilute', 'magnets', 'with', 'longranged', 'ferromagnetic', 'couplings', 'above', '... | [-0.1734551030836772, 0.1944968422710627, -0.00962436138758905, 0.07249732056049672, -0.0537495260901806, -0.16752089073398072, 0.0934821177502376, 0.4084858985347602, -0.23045792016165176, -0.28248078757648193, -0.004610155166112569, -0.32219034628349424, -0.10995184449578514, 0.11002326585025392, 0.08895114524368168,... |
707.1523 | Ages and Abundances of Red Sequence Galaxies as a Function of LINER
Emission Line Strength | Although the spectrum of a prototypical early-type galaxy is assumed to lack
emission lines, a substantial fraction (likely as high as 30%) of nearby red
sequence galaxy spectra contain emission lines with line ratios characteristic
of low ionization nuclear emission-line regions (LINERs). We use spectra of
~6000 gal... | astro-ph | although the spectrum of a prototypical earlytype galaxy is assumed to lack emission lines a substantial fraction likely as high as 30 of nearby red sequence galaxy spectra contain emission lines with line ratios characteristic of low ionization nuclear emissionline regions liners we use spectra of 6000 galaxies from t... | [['although', 'the', 'spectrum', 'of', 'a', 'prototypical', 'earlytype', 'galaxy', 'is', 'assumed', 'to', 'lack', 'emission', 'lines', 'a', 'substantial', 'fraction', 'likely', 'as', 'high', 'as', '30', 'of', 'nearby', 'red', 'sequence', 'galaxy', 'spectra', 'contain', 'emission', 'lines', 'with', 'line', 'ratios', 'ch... | [0.0031152599903038775, 0.11871857123275054, -0.044369172363308264, 0.10488654158645833, -0.10689575052439824, -0.07781761852779474, 0.04085666777550306, 0.543512576129807, -0.07913416181041663, -0.38255312536431263, -0.06991222520234561, -0.3354287661604613, 0.054912080367715416, 0.1920315703197171, -0.056290403837746... |
707.1524 | Finsler-Lagrange Geometries and Standard Theories in Physics: New
Methods in Einstein and String Gravity | In this article, we review the current status of Finsler-Lagrange geometry
and generalizations. The goal is to aid non-experts on Finsler spaces, but
physicists and geometers skilled in general relativity and particle theories,
to understand the crucial importance of such geometric methods for applications
in modern ... | gr-qc hep-th math-ph math.MP math.SG | in this article we review the current status of finslerlagrange geometry and generalizations the goal is to aid nonexperts on finsler spaces but physicists and geometers skilled in general relativity and particle theories to understand the crucial importance of such geometric methods for applications in modern physics ... | [['in', 'this', 'article', 'we', 'review', 'the', 'current', 'status', 'of', 'finslerlagrange', 'geometry', 'and', 'generalizations', 'the', 'goal', 'is', 'to', 'aid', 'nonexperts', 'on', 'finsler', 'spaces', 'but', 'physicists', 'and', 'geometers', 'skilled', 'in', 'general', 'relativity', 'and', 'particle', 'theories... | [-0.10828644208685678, 0.10751552368901296, -0.08758665332729873, 0.15538277665131256, -0.17134146959098995, -0.16327420488581, -0.0566660756884296, 0.37157556345153, -0.26135648590409094, -0.27563962603732145, 0.11088200243146151, -0.2344943353105048, -0.19122107087686244, 0.1764007066262082, -0.15002200366037652, 0.0... |
707.1525 | The patch topology and the ultrafilter topology on the prime spectrum of
a commutative ring | Let R be a commutative ring and let Spec(R) denote the collection of prime
ideals of R. We define a topology on Spec(R) by using ultrafilters and
demonstrate that this topology is identical to the well known patch or
constructible topology. The proof is accomplished by use of a von Neumann
regular ring canonically as... | math.AC math.AG | let r be a commutative ring and let specr denote the collection of prime ideals of r we define a topology on specr by using ultrafilters and demonstrate that this topology is identical to the well known patch or constructible topology the proof is accomplished by use of a von neumann regular ring canonically associated... | [['let', 'r', 'be', 'a', 'commutative', 'ring', 'and', 'let', 'specr', 'denote', 'the', 'collection', 'of', 'prime', 'ideals', 'of', 'r', 'we', 'define', 'a', 'topology', 'on', 'specr', 'by', 'using', 'ultrafilters', 'and', 'demonstrate', 'that', 'this', 'topology', 'is', 'identical', 'to', 'the', 'well', 'known', 'pat... | [-0.21239922881910675, 0.06916757177953657, -0.0871667885139846, -0.013102821178587251, -0.07988101822373114, -0.21516173307604172, -0.06669742146735652, 0.2931426202085915, -0.3926956135322127, -0.14544102340413814, 0.09819037892055094, -0.2469118912622594, -0.06513250624483223, 0.171729317943876, -0.17471005140166534... |
707.1526 | Generalized Lagrange Transforms: Finsler Geometry Methods and
Deformation Quantization of Gravity | We propose a natural Fedosov type quantization of generalized Lagrange models
and gravity theories with metrics lifted on tangent bundle, or extended to
higher dimension, following some stated geometric/ physical conditions (for
instance, nonholonomic and/or conformal transforms to some physically important
metrics o... | gr-qc hep-th math-ph math.MP math.SG | we propose a natural fedosov type quantization of generalized lagrange models and gravity theories with metrics lifted on tangent bundle or extended to higher dimension following some stated geometric physical conditions for instance nonholonomic andor conformal transforms to some physically important metrics or mappin... | [['we', 'propose', 'a', 'natural', 'fedosov', 'type', 'quantization', 'of', 'generalized', 'lagrange', 'models', 'and', 'gravity', 'theories', 'with', 'metrics', 'lifted', 'on', 'tangent', 'bundle', 'or', 'extended', 'to', 'higher', 'dimension', 'following', 'some', 'stated', 'geometric', 'physical', 'conditions', 'for... | [-0.15471234447465335, 0.06470245594035226, -0.07198302118981979, 0.14443114274466523, -0.18737971853246266, -0.23989797259528875, -0.04104190191244517, 0.3700835312887722, -0.3027261429732399, -0.24713043475105445, 0.0807984954694153, -0.1672621009424709, -0.2738135634037685, 0.12861092007072755, -0.1363726843015424, ... |
707.1527 | Programming Telepathy: Implementing Quantum Non-Locality Games | Quantum pseudo-telepathy is an intriguing phenomenon which results from the
application of quantum information theory to communication complexity. To
demonstrate this phenomenon researchers in the field of quantum communication
complexity devised a number of quantum non-locality games. The setting of these
games is a... | quant-ph cs.PL | quantum pseudotelepathy is an intriguing phenomenon which results from the application of quantum information theory to communication complexity to demonstrate this phenomenon researchers in the field of quantum communication complexity devised a number of quantum nonlocality games the setting of these games is as foll... | [['quantum', 'pseudotelepathy', 'is', 'an', 'intriguing', 'phenomenon', 'which', 'results', 'from', 'the', 'application', 'of', 'quantum', 'information', 'theory', 'to', 'communication', 'complexity', 'to', 'demonstrate', 'this', 'phenomenon', 'researchers', 'in', 'the', 'field', 'of', 'quantum', 'communication', 'comp... | [-0.1669797007960302, 0.12993242553870746, -0.1648872062563896, 0.10717159896330149, -0.10300614671367737, -0.250386090066146, 0.0744507575666325, 0.36144358311538344, -0.2837947023204631, -0.31879514774514567, 0.04842794960002518, -0.25881824044303764, -0.18613097959163563, 0.16636170253019641, -0.15668636390732393, 0... |
707.1528 | Simplified motional heating rate measurements of trapped ions | We have measured motional heating rates of trapped atomic ions, a factor that
can influence multi-ion quantum logic gate fidelities. Two simplified
techniques were developed for this purpose: one relies on Raman sideband
detection implemented with a single laser source, while the second is even
simpler and is based o... | quant-ph physics.atom-ph | we have measured motional heating rates of trapped atomic ions a factor that can influence multiion quantum logic gate fidelities two simplified techniques were developed for this purpose one relies on raman sideband detection implemented with a single laser source while the second is even simpler and is based on timer... | [['we', 'have', 'measured', 'motional', 'heating', 'rates', 'of', 'trapped', 'atomic', 'ions', 'a', 'factor', 'that', 'can', 'influence', 'multiion', 'quantum', 'logic', 'gate', 'fidelities', 'two', 'simplified', 'techniques', 'were', 'developed', 'for', 'this', 'purpose', 'one', 'relies', 'on', 'raman', 'sideband', 'd... | [-0.05856603987031263, 0.19378923967502318, 0.0026719438818160646, 0.017018670451740714, 0.032801833294346466, -0.1990499305656151, 0.09111647595752521, 0.4478300813325616, -0.19695481626937786, -0.3331505450629449, 0.048941776589598765, -0.2735516272896771, 0.015484452101423643, 0.3003122945760138, -0.0328952101422040... |
707.1529 | Radiation Due to Josephson Oscillations in Layered Superconductors | We derive the power of direct radiation into free space induced by Josephson
oscillations in intrinsic Josephson junctions of highly anisotropic layered
superconductors. We consider the super-radiation regime for a crystal cut in
the form of a thin slice parallel to the c-axis. We find that the radiation
correction t... | cond-mat.supr-con cond-mat.mtrl-sci | we derive the power of direct radiation into free space induced by josephson oscillations in intrinsic josephson junctions of highly anisotropic layered superconductors we consider the superradiation regime for a crystal cut in the form of a thin slice parallel to the caxis we find that the radiation correction to the ... | [['we', 'derive', 'the', 'power', 'of', 'direct', 'radiation', 'into', 'free', 'space', 'induced', 'by', 'josephson', 'oscillations', 'in', 'intrinsic', 'josephson', 'junctions', 'of', 'highly', 'anisotropic', 'layered', 'superconductors', 'we', 'consider', 'the', 'superradiation', 'regime', 'for', 'a', 'crystal', 'cut... | [-0.21267208333450313, 0.18140504937809038, -0.009333127033326546, 0.00832321240485893, -0.09702360386751135, -0.1177114698256613, 0.0806782636934017, 0.42145554059926343, -0.2635545714886631, -0.28277674269843467, -0.009375110287599417, -0.26147008464880744, -0.060159389604339183, 0.26913959542717025, 0.00862276130260... |
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