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 |
|---|---|---|---|---|---|---|
710.3253 | Two Paradoxes of the Existence of electric Charge | Electromagnetic waves propagate with the speed of light. The reason is that
electrostatic fields as well as magnetic fields propagate with this speed. Both
types of objects, waves as well as static fields contain and transport energy.
Consequently it is possible to calculate how much energy and how much energy
densit... | physics.gen-ph | electromagnetic waves propagate with the speed of light the reason is that electrostatic fields as well as magnetic fields propagate with this speed both types of objects waves as well as static fields contain and transport energy consequently it is possible to calculate how much energy and how much energy density a so... | [['electromagnetic', 'waves', 'propagate', 'with', 'the', 'speed', 'of', 'light', 'the', 'reason', 'is', 'that', 'electrostatic', 'fields', 'as', 'well', 'as', 'magnetic', 'fields', 'propagate', 'with', 'this', 'speed', 'both', 'types', 'of', 'objects', 'waves', 'as', 'well', 'as', 'static', 'fields', 'contain', 'and',... | [-0.10090043533973064, 0.18948243011857285, -0.08839157304228254, 0.06428480804022876, -0.08423680872181846, -0.07722079433548222, 0.029685658358992523, 0.36225242615576575, -0.27587366497416976, -0.33763973815900505, 0.0836907079803704, -0.26002000443411954, -0.08299613092428335, 0.18078857511993807, -0.01732479759557... |
710.3254 | Influence of hydrodynamic interactions on lane formation in oppositely
charged driven colloids | The influence of hydrodynamic interactions on lane formation of oppositely
charged driven colloidal suspensions is investigated using Brownian dynamics
computer simulations performed on the Rotne-Prager level of the mobility
tensor. Two cases are considered, namely sedimentation and electrophoresis. In
the latter cas... | cond-mat.soft | the influence of hydrodynamic interactions on lane formation of oppositely charged driven colloidal suspensions is investigated using brownian dynamics computer simulations performed on the rotneprager level of the mobility tensor two cases are considered namely sedimentation and electrophoresis in the latter case the ... | [['the', 'influence', 'of', 'hydrodynamic', 'interactions', 'on', 'lane', 'formation', 'of', 'oppositely', 'charged', 'driven', 'colloidal', 'suspensions', 'is', 'investigated', 'using', 'brownian', 'dynamics', 'computer', 'simulations', 'performed', 'on', 'the', 'rotneprager', 'level', 'of', 'the', 'mobility', 'tensor... | [-0.1468946498703683, 0.195557855049738, -0.08469122210769993, 0.03551400828256597, 0.00017367830185825565, -0.11980617979642408, -0.06147901709079293, 0.3703528598051922, -0.2557468864567443, -0.24698183605312762, 0.005763615197530128, -0.30231189547129067, -0.12678427701389575, 0.13678340696489877, -0.019067774790462... |
710.3255 | $B_s-\bar{B}_s$ mixing and $B_s \to KK$ decays within supersymmetry | We consider the constraint of $B_s-\bar{B}_s$ mass difference, $\Delta m_s$,
on an MSSM scenario with large flavor mixing. Even with this constraint, we
show that a large deviation from the SM in CP asymmetries of $B_s \to KK$
decays is still possible, making this channel promising in search for
supersymmetry.
| hep-ph | we consider the constraint of b_sbarb_s mass difference delta m_s on an mssm scenario with large flavor mixing even with this constraint we show that a large deviation from the sm in cp asymmetries of b_s to kk decays is still possible making this channel promising in search for supersymmetry | [['we', 'consider', 'the', 'constraint', 'of', 'b_sbarb_s', 'mass', 'difference', 'delta', 'm_s', 'on', 'an', 'mssm', 'scenario', 'with', 'large', 'flavor', 'mixing', 'even', 'with', 'this', 'constraint', 'we', 'show', 'that', 'a', 'large', 'deviation', 'from', 'the', 'sm', 'in', 'cp', 'asymmetries', 'of', 'b_s', 'to',... | [-0.15845270313322543, 0.25029009290301474, -0.0009374126233160496, 0.14713055758853444, -0.10433055986650289, -0.17254702954553067, 0.11717236002208666, 0.2785603888751939, -0.2637446904182434, -0.3102414041385055, 0.0406223029224202, -0.2709359349496663, -0.009665942266583443, 0.10681375421117992, -0.0032099439390003... |
710.3256 | Statistical physics of social dynamics | Statistical physics has proven to be a very fruitful framework to describe
phenomena outside the realm of traditional physics. The last years have
witnessed the attempt by physicists to study collective phenomena emerging from
the interactions of individuals as elementary units in social structures. Here
we review th... | physics.soc-ph cond-mat.stat-mech physics.comp-ph | statistical physics has proven to be a very fruitful framework to describe phenomena outside the realm of traditional physics the last years have witnessed the attempt by physicists to study collective phenomena emerging from the interactions of individuals as elementary units in social structures here we review the st... | [['statistical', 'physics', 'has', 'proven', 'to', 'be', 'a', 'very', 'fruitful', 'framework', 'to', 'describe', 'phenomena', 'outside', 'the', 'realm', 'of', 'traditional', 'physics', 'the', 'last', 'years', 'have', 'witnessed', 'the', 'attempt', 'by', 'physicists', 'to', 'study', 'collective', 'phenomena', 'emerging'... | [-0.036394607580621685, 0.0986017990303004, -0.11764488007618291, 0.11974365184349674, -0.12174396901169703, -0.11421695642528079, 0.052184711733744255, 0.34997187365467347, -0.3067300965211221, -0.3567998496859911, 0.06207407821923317, -0.31887523558522973, -0.22648771036294332, 0.2019945104185137, -0.0375236722818088... |
710.3257 | Acceleration of heavy and light particles in turbulence: comparison
between experiments and direct numerical simulations | We compare experimental data and numerical simulations for the dynamics of
inertial particles with finite density in turbulence. In the experiment,
bubbles and solid particles are optically tracked in a turbulent flow of water
using an Extended Laser Doppler Velocimetry technique. The probability density
functions (P... | nlin.CD physics.flu-dyn | we compare experimental data and numerical simulations for the dynamics of inertial particles with finite density in turbulence in the experiment bubbles and solid particles are optically tracked in a turbulent flow of water using an extended laser doppler velocimetry technique the probability density functions pdf of ... | [['we', 'compare', 'experimental', 'data', 'and', 'numerical', 'simulations', 'for', 'the', 'dynamics', 'of', 'inertial', 'particles', 'with', 'finite', 'density', 'in', 'turbulence', 'in', 'the', 'experiment', 'bubbles', 'and', 'solid', 'particles', 'are', 'optically', 'tracked', 'in', 'a', 'turbulent', 'flow', 'of', ... | [-0.10541793971704386, 0.20076782312740407, -0.13334652358706264, 0.0674618905344844, 0.04303820123694998, -0.038637853093552506, -0.030202133293772828, 0.3843770809739614, -0.23860468783100947, -0.29194303357424284, 0.0667927443500434, -0.279656828662528, -0.05274689561359102, 0.21081494024482375, 0.02183041051566172,... |
710.3258 | Worst-case optimal approximation algorithms for maximizing triplet
consistency within phylogenetic networks | This article concerns the following question arising in computational
evolutionary biology. For a given subclass of phylogenetic networks, what is
the maximum value of 0 <= p <= 1 such that for every input set T of rooted
triplets, there exists some network N(T) from the subclass such that at least
p|T| of the triple... | q-bio.PE | this article concerns the following question arising in computational evolutionary biology for a given subclass of phylogenetic networks what is the maximum value of 0 p 1 such that for every input set t of rooted triplets there exists some network nt from the subclass such that at least pt of the triplets are consiste... | [['this', 'article', 'concerns', 'the', 'following', 'question', 'arising', 'in', 'computational', 'evolutionary', 'biology', 'for', 'a', 'given', 'subclass', 'of', 'phylogenetic', 'networks', 'what', 'is', 'the', 'maximum', 'value', 'of', '0', 'p', '1', 'such', 'that', 'for', 'every', 'input', 'set', 't', 'of', 'roote... | [-0.12535826097036776, 0.11351489915893559, 0.014359029854626157, 0.0650752402228157, -0.018816472395312388, -0.13891313141103573, 0.060093162957855384, 0.357623319802156, -0.2898285950772291, -0.293286322699968, 0.04467828764253957, -0.26245602059481277, -0.15549003558035746, 0.16295838285356673, -0.05627813987277562,... |
710.3259 | Continuous variable quantum teleportation with sculptured and noisy
non-Gaussian resources | We investigate continuous variable (CV) quantum teleportation using relevant
classes of non-Gaussian states of the radiation field as entangled resources.
First, we introduce the class two-mode squeezed symmetric superposition of Fock
states, including finite truncations of twin-beam Gaussian states as special
realiz... | quant-ph | we investigate continuous variable cv quantum teleportation using relevant classes of nongaussian states of the radiation field as entangled resources first we introduce the class twomode squeezed symmetric superposition of fock states including finite truncations of twinbeam gaussian states as special realizations the... | [['we', 'investigate', 'continuous', 'variable', 'cv', 'quantum', 'teleportation', 'using', 'relevant', 'classes', 'of', 'nongaussian', 'states', 'of', 'the', 'radiation', 'field', 'as', 'entangled', 'resources', 'first', 'we', 'introduce', 'the', 'class', 'twomode', 'squeezed', 'symmetric', 'superposition', 'of', 'foc... | [-0.1214920027153406, 0.22989996393617135, -0.08893798263181515, 0.0658058151602745, 0.031573650178274716, -0.20850151239348383, 0.07750264376578532, 0.38671303537256757, -0.2625691587253923, -0.24148470008894318, 0.03992611989940934, -0.2173752305910778, -0.07387716917859005, 0.1977717672647298, -0.08439351430921495, ... |
710.326 | YbRh2Si2: Quantum tricritical behavior in itinerant electron systems | We propose that proximity of the first-order transition manifested by the
quantum tricritical point (QTCP) explains non-Fermi-liquid properties of
YbRh2Si2. Here, at the QTCP, a continuous phase transition changes into first
order at zero temperature. The non-Fermi-liquid behaviors of YbRh2Si2 are
puzzling in two asp... | cond-mat.str-el cond-mat.stat-mech | we propose that proximity of the firstorder transition manifested by the quantum tricritical point qtcp explains nonfermiliquid properties of ybrh2si2 here at the qtcp a continuous phase transition changes into first order at zero temperature the nonfermiliquid behaviors of ybrh2si2 are puzzling in two aspects divergin... | [['we', 'propose', 'that', 'proximity', 'of', 'the', 'firstorder', 'transition', 'manifested', 'by', 'the', 'quantum', 'tricritical', 'point', 'qtcp', 'explains', 'nonfermiliquid', 'properties', 'of', 'ybrh2si2', 'here', 'at', 'the', 'qtcp', 'a', 'continuous', 'phase', 'transition', 'changes', 'into', 'first', 'order',... | [-0.19375405131569623, 0.2615091509362269, -0.12364235408849229, 0.0853028736371351, -0.029164898573837587, -0.1778557101865054, 0.11453910836625207, 0.2836396760846439, -0.26085567104287055, -0.24214634145487493, -0.005505084878103317, -0.41484033076190635, -0.17709069381970421, 0.10628343116197932, 0.0838807669872614... |
710.3261 | Branching rules for unramified principal series representations of GL(3)
over a p-adic field | On restriction to the maximal compact subgroup $\mathrm{GL}(3,\mathscr{R})$,
an unramified principal series representation of the $p$-adic group
$\mathrm{GL}(3,F)$ decomposes into a direct sum of finite-dimensional
irreducibles each appearing with finite multiplicity. We describe a coarser
decomposition into componen... | math.RT | on restriction to the maximal compact subgroup mathrmgl3mathscrr an unramified principal series representation of the padic group mathrmgl3f decomposes into a direct sum of finitedimensional irreducibles each appearing with finite multiplicity we describe a coarser decomposition into components which although reducible... | [['on', 'restriction', 'to', 'the', 'maximal', 'compact', 'subgroup', 'mathrmgl3mathscrr', 'an', 'unramified', 'principal', 'series', 'representation', 'of', 'the', 'padic', 'group', 'mathrmgl3f', 'decomposes', 'into', 'a', 'direct', 'sum', 'of', 'finitedimensional', 'irreducibles', 'each', 'appearing', 'with', 'finite... | [-0.1528124968172051, 0.08841177843745147, -0.17828479168626168, 0.018603949652363855, -0.15696293076810738, -0.06816296031077702, -0.04403891608429452, 0.3040646671142895, -0.3810669512410338, -0.12294677559596796, 0.04890703277730305, -0.2101535149073849, -0.056123873859178275, 0.14321314956760034, -0.072868638439103... |
710.3262 | $L^1$ bounds in normal approximation | The zero bias distribution $W^*$ of $W$, defined though the characterizing
equation $\mathit{EW}f(W)=\sigma^2Ef'(W^*)$ for all smooth functions $f$,
exists for all $W$ with mean zero and finite variance $\sigma^2$. For $W$ and
$W^*$ defined on the same probability space, the $L^1$ distance between $F$,
the distributi... | math.PR | the zero bias distribution w of w defined though the characterizing equation mathitewfwsigma2efw for all smooth functions f exists for all w with mean zero and finite variance sigma2 for w and w defined on the same probability space the l1 distance between f the distribution function of w with mathitew0 and varw1 and t... | [['the', 'zero', 'bias', 'distribution', 'w', 'of', 'w', 'defined', 'though', 'the', 'characterizing', 'equation', 'mathitewfwsigma2efw', 'for', 'all', 'smooth', 'functions', 'f', 'exists', 'for', 'all', 'w', 'with', 'mean', 'zero', 'and', 'finite', 'variance', 'sigma2', 'for', 'w', 'and', 'w', 'defined', 'on', 'the', ... | [-0.11434914886384555, 0.1481325708673862, -0.0837170675083104, 0.0908784531056881, -0.032148304243531566, -0.1715075301978251, 0.0934036317086556, 0.33015821405443485, -0.2981086426374057, -0.2543397505828382, 0.06435239371216006, -0.2783194262807703, -0.027754121277805254, 0.21697444341185948, -0.03145623869647313, 0... |
710.3263 | Branching rules for ramified principal series representations of GL(3)
over a p-adic field | We decompose the restriction of ramified principal series representations of
the $p$-adic group $\mathrm{GL}(3,\mathrm{k})$ to its maximal compact subgroup
$K=\mathrm{GL}(3,\mathscr{R})$. Its decomposition is dependent on the degree of
ramification of the inducing characters and can be characterized in terms of
filtr... | math.RT | we decompose the restriction of ramified principal series representations of the padic group mathrmgl3mathrmk to its maximal compact subgroup kmathrmgl3mathscrr its decomposition is dependent on the degree of ramification of the inducing characters and can be characterized in terms of filtrations of the iwahori subgrou... | [['we', 'decompose', 'the', 'restriction', 'of', 'ramified', 'principal', 'series', 'representations', 'of', 'the', 'padic', 'group', 'mathrmgl3mathrmk', 'to', 'its', 'maximal', 'compact', 'subgroup', 'kmathrmgl3mathscrr', 'its', 'decomposition', 'is', 'dependent', 'on', 'the', 'degree', 'of', 'ramification', 'of', 'th... | [-0.21412216257630734, 0.06361947165829693, -0.17109224978393237, 0.0023802360458495585, -0.13617710811657863, -0.059472972184027494, 0.008987638572427003, 0.3426085112518386, -0.3937426495708917, -0.20361137533919854, 0.14888327051231867, -0.2201051601911323, -0.12826971543070517, 0.19712068546122233, -0.1377286436526... |
710.3264 | Nanodroplets on rough hydrophilic and hydrophobic surfaces | We present results of Molecular Dynamics (MD) calculations on the behavior of
liquid nanodroplets on rough hydrophobic and hydrophilic solid surfaces. On
hydrophobic surfaces, the contact angle for nanodroplets depends strongly on
the root mean square roughness amplitude, but it is nearly independent of the
fractal d... | cond-mat.soft | we present results of molecular dynamics md calculations on the behavior of liquid nanodroplets on rough hydrophobic and hydrophilic solid surfaces on hydrophobic surfaces the contact angle for nanodroplets depends strongly on the root mean square roughness amplitude but it is nearly independent of the fractal dimensio... | [['we', 'present', 'results', 'of', 'molecular', 'dynamics', 'md', 'calculations', 'on', 'the', 'behavior', 'of', 'liquid', 'nanodroplets', 'on', 'rough', 'hydrophobic', 'and', 'hydrophilic', 'solid', 'surfaces', 'on', 'hydrophobic', 'surfaces', 'the', 'contact', 'angle', 'for', 'nanodroplets', 'depends', 'strongly', '... | [-0.16150435627418452, 0.25172924670443253, -0.10729582874886495, 0.055233734415542385, -0.007870444247472875, -0.17965265481837722, 0.01836656704446642, 0.423691753822733, -0.25016259867042095, -0.25205083298956005, 0.047872310103422265, -0.2966742040064763, -0.18579632977128657, 0.22302274210345735, -0.05924540944069... |
710.3265 | Threshold Pion Electroproduction at Large Momentum Transfers | We consider pion electroproduction close to threshold for $Q^2$ in the region
1-10 GeV$^2$ on a nucleon target. The momentum transfer dependence of the
S-wave multipoles at threshold, $E_{0+}$ and $L_{0+}$, is calculated in the
chiral limit using light-cone sum rules. Predictions for the cross sections in
the thresho... | hep-ph nucl-th | we consider pion electroproduction close to threshold for q2 in the region 110 gev2 on a nucleon target the momentum transfer dependence of the swave multipoles at threshold e_0 and l_0 is calculated in the chiral limit using lightcone sum rules predictions for the cross sections in the threshold region are given takin... | [['we', 'consider', 'pion', 'electroproduction', 'close', 'to', 'threshold', 'for', 'q2', 'in', 'the', 'region', '110', 'gev2', 'on', 'a', 'nucleon', 'target', 'the', 'momentum', 'transfer', 'dependence', 'of', 'the', 'swave', 'multipoles', 'at', 'threshold', 'e_0', 'and', 'l_0', 'is', 'calculated', 'in', 'the', 'chira... | [-0.09505552352022599, 0.16195116824853947, -0.06328392783179879, 0.12486484480939586, -0.02118955653379945, -0.047854193289052036, 0.0867531522670213, 0.38042626004008684, -0.16184784132329857, -0.2229924044188331, -0.03757685001610833, -0.3530194777337944, 0.0021764686978285146, 0.1528216937858173, 0.0786196791063583... |
710.3266 | Stochastic theory of lineshape broadening in quasielastic He atom
scattering with interacting adsorbates | The activated surface diffusion of interacting adsorbates is described in
terms of the so-called interacting single adsorbate approximation, which is
applied to the diffusion of Na atoms on Cu(001) for coverages up to 20% in
quasielastic He atom scattering experiments. This approximation essentially
consists of solvi... | cond-mat.stat-mech cond-mat.mtrl-sci quant-ph | the activated surface diffusion of interacting adsorbates is described in terms of the socalled interacting single adsorbate approximation which is applied to the diffusion of na atoms on cu001 for coverages up to 20 in quasielastic he atom scattering experiments this approximation essentially consists of solving the s... | [['the', 'activated', 'surface', 'diffusion', 'of', 'interacting', 'adsorbates', 'is', 'described', 'in', 'terms', 'of', 'the', 'socalled', 'interacting', 'single', 'adsorbate', 'approximation', 'which', 'is', 'applied', 'to', 'the', 'diffusion', 'of', 'na', 'atoms', 'on', 'cu001', 'for', 'coverages', 'up', 'to', '20',... | [-0.0859993172749672, 0.2091370841799039, -0.050708846851260564, 0.04666478637234231, 0.03978710853998814, -0.17136693296851505, 0.05373412836983868, 0.36372532763031373, -0.2365302397194532, -0.31825955400089606, -0.024360999327212775, -0.3715821685730864, -0.06464337276021412, 0.17825458653766765, 0.02408319502351207... |
710.3267 | GAP Computations Concerning Probabilistic Generation of Finite Simple
Groups | This is a collection of examples showing how the GAP system can be used to
compute information about the probabilistic generation of finite almost simple
groups. It includes all examples that were needed for the computational results
in the paper "Probabilistic generation of finite simple groups, II" by Thomas
Breuer... | math.RT math.GR | this is a collection of examples showing how the gap system can be used to compute information about the probabilistic generation of finite almost simple groups it includes all examples that were needed for the computational results in the paper probabilistic generation of finite simple groups ii by thomas breuer rober... | [['this', 'is', 'a', 'collection', 'of', 'examples', 'showing', 'how', 'the', 'gap', 'system', 'can', 'be', 'used', 'to', 'compute', 'information', 'about', 'the', 'probabilistic', 'generation', 'of', 'finite', 'almost', 'simple', 'groups', 'it', 'includes', 'all', 'examples', 'that', 'were', 'needed', 'for', 'the', 'c... | [-0.08932055081448306, 0.06436213804639433, -0.07447099147161634, 0.10388462671359983, -0.10478954818929628, -0.13703133456759375, 0.018990826683515444, 0.3486003885414488, -0.24743924159003367, -0.31981769477081773, 0.1406761162561632, -0.2546842884419873, -0.14012962516102165, 0.27356815067959006, -0.1085921775936932... |
710.3268 | Googling Social Interactions: Web Search Engine Based Social Network
Construction | Social network analysis has long been an untiring topic of sociology.
However, until the era of information technology, the availability of data,
mainly collected by the traditional method of personal survey, was highly
limited and prevented large-scale analysis. Recently, the exploding amount of
automatically genera... | physics.soc-ph cond-mat.stat-mech | social network analysis has long been an untiring topic of sociology however until the era of information technology the availability of data mainly collected by the traditional method of personal survey was highly limited and prevented largescale analysis recently the exploding amount of automatically generated data h... | [['social', 'network', 'analysis', 'has', 'long', 'been', 'an', 'untiring', 'topic', 'of', 'sociology', 'however', 'until', 'the', 'era', 'of', 'information', 'technology', 'the', 'availability', 'of', 'data', 'mainly', 'collected', 'by', 'the', 'traditional', 'method', 'of', 'personal', 'survey', 'was', 'highly', 'lim... | [-0.08599623927851668, 0.06118967821688844, -0.05367000061752541, 0.0770499076582952, -0.11171998041374916, -0.1032950327895418, 0.04445733326732867, 0.33872793127711004, -0.2812481676465013, -0.35129515545770196, 0.1645016901432997, -0.32672873357212384, -0.1875879797281104, 0.24054106262225944, -0.06360605767554511, ... |
710.3269 | Differential equation approximations for Markov chains | We formulate some simple conditions under which a Markov chain may be
approximated by the solution to a differential equation, with quantifiable
error probabilities. The role of a choice of coordinate functions for the
Markov chain is emphasised. The general theory is illustrated in three
examples: the classical stoc... | math.PR | we formulate some simple conditions under which a markov chain may be approximated by the solution to a differential equation with quantifiable error probabilities the role of a choice of coordinate functions for the markov chain is emphasised the general theory is illustrated in three examples the classical stochastic... | [['we', 'formulate', 'some', 'simple', 'conditions', 'under', 'which', 'a', 'markov', 'chain', 'may', 'be', 'approximated', 'by', 'the', 'solution', 'to', 'a', 'differential', 'equation', 'with', 'quantifiable', 'error', 'probabilities', 'the', 'role', 'of', 'a', 'choice', 'of', 'coordinate', 'functions', 'for', 'the',... | [-0.11204308944825943, 0.10942926563035983, -0.067203411173362, 0.13421958189991037, -0.06111502771695646, -0.17749264870698636, 0.06451578517623532, 0.38118521705842934, -0.30522365058557344, -0.2291909495798441, 0.16331730637556086, -0.20870399651332544, -0.16720506098981086, 0.1865299246309755, -0.0717157461393911, ... |
710.327 | On the dynamics created by a time--dependent Aharonov-Bohm flux | We study the dynamics of classical and quantum particles moving in a
punctured plane under the influence of a homogeneous magnetic field and driven
by a time-dependent singular flux tube through the hole.
| math-ph math.MP | we study the dynamics of classical and quantum particles moving in a punctured plane under the influence of a homogeneous magnetic field and driven by a timedependent singular flux tube through the hole | [['we', 'study', 'the', 'dynamics', 'of', 'classical', 'and', 'quantum', 'particles', 'moving', 'in', 'a', 'punctured', 'plane', 'under', 'the', 'influence', 'of', 'a', 'homogeneous', 'magnetic', 'field', 'and', 'driven', 'by', 'a', 'timedependent', 'singular', 'flux', 'tube', 'through', 'the', 'hole']] | [-0.20360573669048873, 0.18659781464234446, -0.05550718465537736, 0.028215555248386932, -0.00910256120065848, -0.07724881066348065, 0.03893825978615716, 0.3281017887321385, -0.2473371818831021, -0.23403669397036234, 0.08482574384349088, -0.23749090403769957, -0.12326464305321376, 0.2173869482834231, 0.01288320245503476... |
710.3271 | Geometric properties derived from generic initial spaces | For a vector space V of homogeneous forms of the same degree in a polynomial
ring, we investigate what can be said about the generic initial ideal of the
ideal generated by V, from the form of the generic initial space gin(V) for the
revlex order. Our main result is a considerable generalisation of a previous
result ... | math.AC | for a vector space v of homogeneous forms of the same degree in a polynomial ring we investigate what can be said about the generic initial ideal of the ideal generated by v from the form of the generic initial space ginv for the revlex order our main result is a considerable generalisation of a previous result by the ... | [['for', 'a', 'vector', 'space', 'v', 'of', 'homogeneous', 'forms', 'of', 'the', 'same', 'degree', 'in', 'a', 'polynomial', 'ring', 'we', 'investigate', 'what', 'can', 'be', 'said', 'about', 'the', 'generic', 'initial', 'ideal', 'of', 'the', 'ideal', 'generated', 'by', 'v', 'from', 'the', 'form', 'of', 'the', 'generic'... | [-0.14795944017047682, 0.08409384797948102, -0.0722472862030069, 0.010828385946418469, -0.05721094910986722, -0.05481604891829193, -0.0148332670951883, 0.2845062254307171, -0.31447981633245947, -0.2273157404658074, 0.08989769116160459, -0.20367201181749503, -0.13201156800302366, 0.19108812995254992, -0.0333864251617342... |
710.3272 | The fermion spectrum in braneworld collisions | In braneworld collisions fermions originally localised on one brane can be
transferred to another brane, or to a space-time boundary. By modelling branes
as scalar field kinks we bounce them off boundaries and study resulting effects
according to a braneworld observer. Extending on our previous work, we
numerically c... | hep-th | in braneworld collisions fermions originally localised on one brane can be transferred to another brane or to a spacetime boundary by modelling branes as scalar field kinks we bounce them off boundaries and study resulting effects according to a braneworld observer extending on our previous work we numerically compute ... | [['in', 'braneworld', 'collisions', 'fermions', 'originally', 'localised', 'on', 'one', 'brane', 'can', 'be', 'transferred', 'to', 'another', 'brane', 'or', 'to', 'a', 'spacetime', 'boundary', 'by', 'modelling', 'branes', 'as', 'scalar', 'field', 'kinks', 'we', 'bounce', 'them', 'off', 'boundaries', 'and', 'study', 're... | [-0.15691724425295786, 0.22310060565835055, -0.130179284551485, 0.09458928051575714, -0.11201962583451247, -0.16502719105468416, -0.001326245730932878, 0.3193416059853471, -0.1713128721160928, -0.2406126643359965, 0.034364207977980225, -0.31539991423867797, -0.0508729693627137, 0.11980289139794376, -0.01967687539433186... |
710.3273 | Complex Fundamental Diagram of Traffic Flow in the Deep Lefortovo Tunnel
(Moscow) | The fundamental diagram for tunnel traffic is constructed based on the
empirical data collected during the last two years in the deep long branch of
the Lefortovo tunnel located on the 3$^\text{rd}$ circular highway of Moscow.
This tunnel of length 3 km is equipped with a dense system of stationary
radiodetetors dist... | physics.soc-ph physics.data-an | the fundamental diagram for tunnel traffic is constructed based on the empirical data collected during the last two years in the deep long branch of the lefortovo tunnel located on the 3textrd circular highway of moscow this tunnel of length 3 km is equipped with a dense system of stationary radiodetetors distributed u... | [['the', 'fundamental', 'diagram', 'for', 'tunnel', 'traffic', 'is', 'constructed', 'based', 'on', 'the', 'empirical', 'data', 'collected', 'during', 'the', 'last', 'two', 'years', 'in', 'the', 'deep', 'long', 'branch', 'of', 'the', 'lefortovo', 'tunnel', 'located', 'on', 'the', '3textrd', 'circular', 'highway', 'of', ... | [-0.1901247130349429, 0.10488067394856838, -0.06523477162159226, 0.008718893379960773, 0.017617798351560427, -0.12031876968897202, 0.05770821161238909, 0.3785497814115852, -0.2518761485945574, -0.31515115005613276, 0.10853015713633574, -0.31042514822323514, -0.04372712220958989, 0.2267619565157502, -0.03042203441939570... |
710.3274 | Dilepton measurements with HADES | HADES is the only operating dielectron spectrometer in the energy regime 1-2
AGeV. The physics program aims at a systematic investigation of dielectron
production in heavy ion as well as elementary and pion-induced reactions.
This contribution highlights recent results on electron pair production in
C12+C12 collisi... | nucl-ex | hades is the only operating dielectron spectrometer in the energy regime 12 agev the physics program aims at a systematic investigation of dielectron production in heavy ion as well as elementary and pioninduced reactions this contribution highlights recent results on electron pair production in c12c12 collisions at an... | [['hades', 'is', 'the', 'only', 'operating', 'dielectron', 'spectrometer', 'in', 'the', 'energy', 'regime', '12', 'agev', 'the', 'physics', 'program', 'aims', 'at', 'a', 'systematic', 'investigation', 'of', 'dielectron', 'production', 'in', 'heavy', 'ion', 'as', 'well', 'as', 'elementary', 'and', 'pioninduced', 'reacti... | [-0.03824509968947403, 0.23614871949552174, -0.10169946011223331, 0.10421117415999238, 0.037893843516518456, -0.09633183532666105, 0.02590195114127077, 0.3330919620567474, -0.19145322544500232, -0.3355485340040447, -0.08550335415571496, -0.39407585062186967, 0.10117934758908223, 0.19106802000137774, 0.08614619640929563... |
710.3275 | Search for single top production using multivariate analyses at CDF | This article reports on recent searches for single-top-quark production by
the CDF collaboration at the Tevatron using a data set that corresponds to an
integrated luminosity of 955 fb^-1. Three different analyses techniques are
employed, one using likelihood discriminants, one neural networks and one
matrix elements... | hep-ex | this article reports on recent searches for singletopquark production by the cdf collaboration at the tevatron using a data set that corresponds to an integrated luminosity of 955 fb1 three different analyses techniques are employed one using likelihood discriminants one neural networks and one matrix elements the sens... | [['this', 'article', 'reports', 'on', 'recent', 'searches', 'for', 'singletopquark', 'production', 'by', 'the', 'cdf', 'collaboration', 'at', 'the', 'tevatron', 'using', 'a', 'data', 'set', 'that', 'corresponds', 'to', 'an', 'integrated', 'luminosity', 'of', '955', 'fb1', 'three', 'different', 'analyses', 'techniques',... | [-0.0567310009928535, 0.1446061876710886, -0.021131956344028997, 0.10796191772120411, -0.016772653345874914, -0.10527397672782578, 0.09851659420779486, 0.29721568809530885, -0.18068581932032332, -0.3210136222948819, 0.021590350872739902, -0.37735774276239614, 0.025484272463123594, 0.17140193125431677, 0.066484392174824... |
710.3276 | Group field theory as the microscopic description of the quantum
spacetime fluid: a new perspective on the continuum in quantum gravity | We introduce the group field theory (GFT) formalism for non-perturbative
quantum gravity, and present it as a potential unifying framework for several
other quantum gravity approaches, i.e. loop quantum gravity and simplicial
quantum gravity ones. We then argue in favor of and present in detail what we
believe is a n... | gr-qc hep-th | we introduce the group field theory gft formalism for nonperturbative quantum gravity and present it as a potential unifying framework for several other quantum gravity approaches ie loop quantum gravity and simplicial quantum gravity ones we then argue in favor of and present in detail what we believe is a new gft per... | [['we', 'introduce', 'the', 'group', 'field', 'theory', 'gft', 'formalism', 'for', 'nonperturbative', 'quantum', 'gravity', 'and', 'present', 'it', 'as', 'a', 'potential', 'unifying', 'framework', 'for', 'several', 'other', 'quantum', 'gravity', 'approaches', 'ie', 'loop', 'quantum', 'gravity', 'and', 'simplicial', 'qu... | [-0.08332158010900736, 0.17520770158511229, -0.19238558728785182, 0.1227649101960616, -0.10293401556734283, -0.17150042085693432, 0.013123818579165695, 0.34197468750465376, -0.2037497370862044, -0.2551117791221119, 0.04736602183771678, -0.21375094609908185, -0.19845901334909005, 0.16473874586114948, -0.0700892282945390... |
710.3277 | Viscous hydrodynamics | We study the role of viscosity in the early stages of relativistic heavy ion
collisions. We investigate the role of viscosity on the chemical equilibration
of a parton gas. In the presence of viscosity the lifetime of the system is
increased. The temperature as well as the parton fugacities evolve more slowly
compare... | nucl-th | we study the role of viscosity in the early stages of relativistic heavy ion collisions we investigate the role of viscosity on the chemical equilibration of a parton gas in the presence of viscosity the lifetime of the system is increased the temperature as well as the parton fugacities evolve more slowly compared to ... | [['we', 'study', 'the', 'role', 'of', 'viscosity', 'in', 'the', 'early', 'stages', 'of', 'relativistic', 'heavy', 'ion', 'collisions', 'we', 'investigate', 'the', 'role', 'of', 'viscosity', 'on', 'the', 'chemical', 'equilibration', 'of', 'a', 'parton', 'gas', 'in', 'the', 'presence', 'of', 'viscosity', 'the', 'lifetime... | [-0.1321052320066695, 0.21798191543925424, -0.13628351174551864, 0.05450467560801591, 0.04978537119539647, -0.015080476894268188, -0.03654084251872424, 0.28704543334656746, -0.2498459856443364, -0.25812367401246367, 0.048182202747958744, -0.2732526922983856, 0.020755415380900276, 0.09250958748804085, 0.0444687921714423... |
710.3278 | Package models and the information crisis of prebiotic evolution | The coexistence between different types of templates has been the choice
solution to the information crisis of prebiotic evolution, triggered by the
finding that a single RNA-like template cannot carry enough information to code
for any useful replicase. In principle, confining $d$ distinct templates of
length $L$ in... | q-bio.PE | the coexistence between different types of templates has been the choice solution to the information crisis of prebiotic evolution triggered by the finding that a single rnalike template cannot carry enough information to code for any useful replicase in principle confining d distinct templates of length l in a package... | [['the', 'coexistence', 'between', 'different', 'types', 'of', 'templates', 'has', 'been', 'the', 'choice', 'solution', 'to', 'the', 'information', 'crisis', 'of', 'prebiotic', 'evolution', 'triggered', 'by', 'the', 'finding', 'that', 'a', 'single', 'rnalike', 'template', 'can', 'not', 'carry', 'enough', 'information',... | [-0.12002364361865653, 0.07808125837416607, -0.09638386622666278, 0.05489122312153793, -0.07095913940963025, -0.15518399936716176, 0.092364226041698, 0.3307724316087034, -0.26236330330268376, -0.3076825194604074, 0.10859243049506201, -0.24564958301165865, -0.11584001442921969, 0.13596953248424043, -0.07049832803911865,... |
710.3279 | Resource Allocation for Delay Differentiated Traffic in Multiuser OFDM
Systems | Most existing work on adaptive allocation of subcarriers and power in
multiuser orthogonal frequency division multiplexing (OFDM) systems has focused
on homogeneous traffic consisting solely of either delay-constrained data
(guaranteed service) or non-delay-constrained data (best-effort service). In
this paper, we in... | cs.NI cs.IT math.IT | most existing work on adaptive allocation of subcarriers and power in multiuser orthogonal frequency division multiplexing ofdm systems has focused on homogeneous traffic consisting solely of either delayconstrained data guaranteed service or nondelayconstrained data besteffort service in this paper we investigate the ... | [['most', 'existing', 'work', 'on', 'adaptive', 'allocation', 'of', 'subcarriers', 'and', 'power', 'in', 'multiuser', 'orthogonal', 'frequency', 'division', 'multiplexing', 'ofdm', 'systems', 'has', 'focused', 'on', 'homogeneous', 'traffic', 'consisting', 'solely', 'of', 'either', 'delayconstrained', 'data', 'guarantee... | [-0.2500134617962152, -0.036082241770915915, -0.024376795983550196, 0.007064122169715714, -0.11238639981828022, -0.2624071269481424, 0.16120677543221973, 0.40236356153095865, -0.27772972675346846, -0.2630617621269229, 0.10386411318548347, -0.2506120969275279, -0.16430868366400578, 0.17935693837768799, -0.14998632588670... |
710.328 | Generalized Entropy and Transport Coefficients of Hadronic Matter | We use the generalized entropy four-current of the Muller-Israel-Stewart
(MIS) theory of relativistic dissipative fluids to obtain information about
fluctuations around equilibrium. This allows one to compute the non-classical
coefficients of the entropy 4-flux in terms of the equilibrium distribution
functions. The ... | nucl-th | we use the generalized entropy fourcurrent of the mullerisraelstewart mis theory of relativistic dissipative fluids to obtain information about fluctuations around equilibrium this allows one to compute the nonclassical coefficients of the entropy 4flux in terms of the equilibrium distribution functions the greenkubo f... | [['we', 'use', 'the', 'generalized', 'entropy', 'fourcurrent', 'of', 'the', 'mullerisraelstewart', 'mis', 'theory', 'of', 'relativistic', 'dissipative', 'fluids', 'to', 'obtain', 'information', 'about', 'fluctuations', 'around', 'equilibrium', 'this', 'allows', 'one', 'to', 'compute', 'the', 'nonclassical', 'coefficien... | [-0.10712379676049515, 0.12807692314233846, -0.16171847429547098, 0.11183676998423893, -0.01321302005840886, -0.08683635360531268, -0.005487732223099878, 0.20804311765072447, -0.3162739654221842, -0.24501446514360367, 0.0369875202060587, -0.32370781473793847, -0.05952502928689243, 0.16394049397504498, -0.04125994563313... |
710.3281 | Probing deviation of tribimaximal mixing and reach of $\theta_{13}$
using neutrino factory at CERN and ICAL detector at INO | We investigate the deviation from tribimaximal mixing value and the reach of
$\theta_{13}$ using neutrino factory at CERN and ICAL detector at INO.
| hep-ph | we investigate the deviation from tribimaximal mixing value and the reach of theta_13 using neutrino factory at cern and ical detector at ino | [['we', 'investigate', 'the', 'deviation', 'from', 'tribimaximal', 'mixing', 'value', 'and', 'the', 'reach', 'of', 'theta_13', 'using', 'neutrino', 'factory', 'at', 'cern', 'and', 'ical', 'detector', 'at', 'ino']] | [0.016845654453272404, 0.29898115036928136, -0.008306200656553974, 0.13087941503719144, -0.00023503637994113177, -0.13927312393713256, 0.10321698953276096, 0.2652873835000007, -0.2656081978879545, -0.35393534584537795, 0.10639343530182606, -0.41953830396675545, 0.04284078413215668, 0.1677247266912752, 0.111295954000366... |
710.3282 | Condensation of cloud microdroplets in homogeneous isotropic turbulence | The growth by condensation of small water droplets in a three-dimensional
homogeneous isotropic turbulent flow is considered. Within a simple model of
advection and condensation, the dynamics and growth of millions of droplets are
integrated. A droplet-size spectra broadening is obtained and it is shown to
increase w... | nlin.CD physics.flu-dyn | the growth by condensation of small water droplets in a threedimensional homogeneous isotropic turbulent flow is considered within a simple model of advection and condensation the dynamics and growth of millions of droplets are integrated a dropletsize spectra broadening is obtained and it is shown to increase with the... | [['the', 'growth', 'by', 'condensation', 'of', 'small', 'water', 'droplets', 'in', 'a', 'threedimensional', 'homogeneous', 'isotropic', 'turbulent', 'flow', 'is', 'considered', 'within', 'a', 'simple', 'model', 'of', 'advection', 'and', 'condensation', 'the', 'dynamics', 'and', 'growth', 'of', 'millions', 'of', 'drople... | [-0.15249629040978, 0.1782920708071769, -0.0840721965630484, 0.050331574281239334, -0.03779943566358484, -0.04633326808894601, 0.026439400912974687, 0.2987980979111265, -0.22697323783752782, -0.3428536125623128, 0.07826362827532542, -0.24099700899027726, -0.06735703031368115, 0.2216332117684514, -0.01085229494215395, 0... |
710.3283 | Effects of Non-Identical Rayleigh Fading on Differential Unitary
Space-Time Modulation | This paper has been withdrawn by the author.
| cs.PF cs.IT math.IT | this paper has been withdrawn by the author | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author']] | [-0.11762839742004871, -0.04127746832091361, -0.17016396392136812, -0.1582642109860899, -0.18072871817275882, -0.04020218155346811, -0.09601712167204823, 0.33764172717928886, -0.2455208501778543, -0.3865965995937586, 0.12438089866191149, -0.3554150704294443, -0.17133164615370333, -0.03124168887734413, -0.36054937075823... |
710.3284 | Rigidity in the intersection of varieties does not imply rigidity in the
intersecting varieties | This paper has been withdrawn by the author due to a crucial error in
example.
| math.RA | this paper has been withdrawn by the author due to a crucial error in example | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'a', 'crucial', 'error', 'in', 'example']] | [-0.09723079738517602, -0.04242299584050973, -0.09025248636802037, 0.01122508281065772, -0.07706857882440091, -0.08662326755002141, 0.012278791090163091, 0.32468904852867125, -0.22993607024351756, -0.37868056322137517, 0.1545058767233665, -0.2466760369638602, -0.22330550365149976, 0.11764692763487498, -0.30574627437939... |
710.3285 | Nontraditional Scoring of C-tests | In C-tests the hypothesis of items local independence is violated, which
doesn't permit to consider them as real tests. It is suggested to determine the
distances between separate C-test items (blanks) and to combine items into
clusters. Weights, inversely proportional to the number of items in
corresponding clusters... | cs.CY cs.CL | in ctests the hypothesis of items local independence is violated which doesnt permit to consider them as real tests it is suggested to determine the distances between separate ctest items blanks and to combine items into clusters weights inversely proportional to the number of items in corresponding clusters are assign... | [['in', 'ctests', 'the', 'hypothesis', 'of', 'items', 'local', 'independence', 'is', 'violated', 'which', 'doesnt', 'permit', 'to', 'consider', 'them', 'as', 'real', 'tests', 'it', 'is', 'suggested', 'to', 'determine', 'the', 'distances', 'between', 'separate', 'ctest', 'items', 'blanks', 'and', 'to', 'combine', 'items... | [-0.08203165327579202, 0.10096290733002808, -0.06364468671381474, 0.11783825631358359, -0.13852780217855748, -0.1610329487544655, 0.1172389285720911, 0.3297205077300609, -0.3010911614745593, -0.358655488879328, 0.019806488763055647, -0.309048367126412, -0.040680080353820196, 0.09166847531434516, -0.057925112125739246, ... |
710.3286 | Lateral migration of a 2D vesicle in unbounded Poiseuille flow | The migration of a suspended vesicle in an unbounded Poiseuille flow is
investigated numerically in the low Reynolds number limit. We consider the
situation without viscosity contrast between the interior of the vesicle and
the exterior. Using the boundary integral method we solve the corresponding
hydrodynamic flow ... | cond-mat.soft | the migration of a suspended vesicle in an unbounded poiseuille flow is investigated numerically in the low reynolds number limit we consider the situation without viscosity contrast between the interior of the vesicle and the exterior using the boundary integral method we solve the corresponding hydrodynamic flow equa... | [['the', 'migration', 'of', 'a', 'suspended', 'vesicle', 'in', 'an', 'unbounded', 'poiseuille', 'flow', 'is', 'investigated', 'numerically', 'in', 'the', 'low', 'reynolds', 'number', 'limit', 'we', 'consider', 'the', 'situation', 'without', 'viscosity', 'contrast', 'between', 'the', 'interior', 'of', 'the', 'vesicle', ... | [-0.1715890139647645, 0.13382958095867178, -0.10392786963235208, -0.04083674209426471, -0.03278222248670371, -0.09159642474272632, -0.00011398362488869359, 0.28938703965594903, -0.3058633737908527, -0.28910675215569726, 0.06997680199148262, -0.23891530165020475, -0.12447854463897526, 0.13719612963119132, -0.05283099144... |
710.3287 | On the performance of FDR control: Constraints and a partial solution | The False Discovery Rate (FDR) paradigm aims to attain certain control on
Type I errors with relatively high power for multiple hypothesis testing. The
Benjamini--Hochberg (BH) procedure is a well-known FDR controlling procedure.
Under a random effects model, we show that, in general, unlike the FDR, the
positive FDR... | math.ST stat.TH | the false discovery rate fdr paradigm aims to attain certain control on type i errors with relatively high power for multiple hypothesis testing the benjaminihochberg bh procedure is a wellknown fdr controlling procedure under a random effects model we show that in general unlike the fdr the positive fdr pfdr of the bh... | [['the', 'false', 'discovery', 'rate', 'fdr', 'paradigm', 'aims', 'to', 'attain', 'certain', 'control', 'on', 'type', 'i', 'errors', 'with', 'relatively', 'high', 'power', 'for', 'multiple', 'hypothesis', 'testing', 'the', 'benjaminihochberg', 'bh', 'procedure', 'is', 'a', 'wellknown', 'fdr', 'controlling', 'procedure'... | [-0.1248479456894777, 0.08980502025444752, -0.07090047477095417, 0.08289319329443529, -0.05890940524157927, -0.22759816810827363, 0.1692199893846092, 0.31702623462135143, -0.23539281126224634, -0.3047750746323304, 0.1493200186922243, -0.20175798582477553, -0.13151084181259978, 0.22905393916069333, -0.10896836790489033,... |
710.3288 | Measurement of sigma_Total in e+e- Annihilations Below 10.56 GeV | Using the CLEO III detector, we measure absolute cross sections for e+e- ->
hadrons at seven center-of-mass energies between 6.964 and 10.538 GeV. R, the
ratio of hadronic and muon pair production cross sections, is measured at these
energies with a r.m.s. error <2% allowing determinations of the strong coupling
alph... | hep-ex hep-ph | using the cleo iii detector we measure absolute cross sections for ee hadrons at seven centerofmass energies between 6964 and 10538 gev r the ratio of hadronic and muon pair production cross sections is measured at these energies with a rms error 2 allowing determinations of the strong coupling alpha_s using the expect... | [['using', 'the', 'cleo', 'iii', 'detector', 'we', 'measure', 'absolute', 'cross', 'sections', 'for', 'ee', 'hadrons', 'at', 'seven', 'centerofmass', 'energies', 'between', '6964', 'and', '10538', 'gev', 'r', 'the', 'ratio', 'of', 'hadronic', 'and', 'muon', 'pair', 'production', 'cross', 'sections', 'is', 'measured', '... | [-0.06739176832695282, 0.18297572626221564, -0.05150355330307878, 0.12936413645060854, 0.05954767963022835, -0.10487345516711714, 0.018622318162552772, 0.37561762471112514, -0.1490099170365401, -0.3657325821658296, -0.08626142770592723, -0.41899253283777543, 0.17409811122342944, 0.1587914457552195, 0.15535799489777175,... |
710.3289 | Transient magnetotransport through a quantum wire | We consider an ideal parabolic quantum wire in a perpendicular magnetic
field. A simple Gaussian shaped scattering potential well or hill is flashed
softly on and off with its maximum at $t=0$, mimicking a temporary broadening
or narrowing of the wire. By an extension of the Lippmann-Schwinger formalism
to time-depen... | cond-mat.mes-hall | we consider an ideal parabolic quantum wire in a perpendicular magnetic field a simple gaussian shaped scattering potential well or hill is flashed softly on and off with its maximum at t0 mimicking a temporary broadening or narrowing of the wire by an extension of the lippmannschwinger formalism to timedependent scatt... | [['we', 'consider', 'an', 'ideal', 'parabolic', 'quantum', 'wire', 'in', 'a', 'perpendicular', 'magnetic', 'field', 'a', 'simple', 'gaussian', 'shaped', 'scattering', 'potential', 'well', 'or', 'hill', 'is', 'flashed', 'softly', 'on', 'and', 'off', 'with', 'its', 'maximum', 'at', 't0', 'mimicking', 'a', 'temporary', 'b... | [-0.14050654318998568, 0.16265794185922763, -0.07323407228492822, 0.06522721813305073, -0.08226075486163609, -0.14296378884561514, 0.040538381484414764, 0.3811344786857565, -0.3106975390886267, -0.25647503819588263, 0.021090054524393054, -0.28527263571353006, -0.12051924734745019, 0.16110070154536515, 0.004694757658095... |
710.329 | Smooth rationally connected threefolds contain all smooth curves | We show that if X is a smooth rationally connected threefold and C is a
smooth projective curve then C can be embedded in X. Furthermore, a version of
this property characterises rationally connected varieties of dimension at
least 3. We give some details about the toric case.
| math.AG | we show that if x is a smooth rationally connected threefold and c is a smooth projective curve then c can be embedded in x furthermore a version of this property characterises rationally connected varieties of dimension at least 3 we give some details about the toric case | [['we', 'show', 'that', 'if', 'x', 'is', 'a', 'smooth', 'rationally', 'connected', 'threefold', 'and', 'c', 'is', 'a', 'smooth', 'projective', 'curve', 'then', 'c', 'can', 'be', 'embedded', 'in', 'x', 'furthermore', 'a', 'version', 'of', 'this', 'property', 'characterises', 'rationally', 'connected', 'varieties', 'of',... | [-0.22488343781636408, 0.05437616351991892, -0.10475305690003249, 0.020794033065612894, -0.05838103154868198, -0.24154038138779774, -0.023080570274032652, 0.41825508850160986, -0.32431906345300376, -0.13095424500837302, 0.12040858490460475, -0.24009766633389518, -0.167686786968261, 0.1994550067562765, -0.20463325158925... |
710.3291 | Bounded modes to the rescue of optical transmission | This paper presents a brief survey of the evolution of knowledge about
diffraction gratings. After recalling some basic facts, historically and
physically, we introduce the concept of Wood anomalies. Next, we present some
recent works in order to introduce the role of bounded modes in transmission
gratings. The conse... | physics.optics physics.gen-ph | this paper presents a brief survey of the evolution of knowledge about diffraction gratings after recalling some basic facts historically and physically we introduce the concept of wood anomalies next we present some recent works in order to introduce the role of bounded modes in transmission gratings the consequences ... | [['this', 'paper', 'presents', 'a', 'brief', 'survey', 'of', 'the', 'evolution', 'of', 'knowledge', 'about', 'diffraction', 'gratings', 'after', 'recalling', 'some', 'basic', 'facts', 'historically', 'and', 'physically', 'we', 'introduce', 'the', 'concept', 'of', 'wood', 'anomalies', 'next', 'we', 'present', 'some', 'r... | [-0.12687746058439925, 0.09844715235244837, -0.08329601206683687, 0.018671906224751313, -0.13525281149140073, -0.07820996070014578, 0.02915254905764457, 0.3622262968371312, -0.1888930461968162, -0.3372776909132621, 0.14549815983489334, -0.31527552352331223, -0.21235455553756938, 0.151890165793399, -0.16164968128404802,... |
710.3292 | Continuous Abelian Sandpile Model in Two Dimensional Lattice | We define a new version of sandpile model which is very similar to Abelian
Sandpile Model (ASM), but the height variables are continuous ones. With the
toppling rule we define in our model, we show that the model can be mapped to
ASM, so the general properties of the two models are identical. Yet the new
model allows... | cond-mat.stat-mech | we define a new version of sandpile model which is very similar to abelian sandpile model asm but the height variables are continuous ones with the toppling rule we define in our model we show that the model can be mapped to asm so the general properties of the two models are identical yet the new model allows us to in... | [['we', 'define', 'a', 'new', 'version', 'of', 'sandpile', 'model', 'which', 'is', 'very', 'similar', 'to', 'abelian', 'sandpile', 'model', 'asm', 'but', 'the', 'height', 'variables', 'are', 'continuous', 'ones', 'with', 'the', 'toppling', 'rule', 'we', 'define', 'in', 'our', 'model', 'we', 'show', 'that', 'the', 'mode... | [-0.07755507782209091, 0.1543137073660126, -0.11320531754515684, 0.12193385266418307, -0.09688158359271117, -0.17620099441578183, 0.048896400610176034, 0.39337873606918716, -0.292129340975617, -0.29967799596488476, 0.11152898838880877, -0.2315172024389493, -0.16350259865896824, 0.18306070965869972, -0.08845234751247634... |
710.3293 | Electronic transitions in Rydberg Matter as the source of the
unidentified infrared bands (UIR) observed in interstellar space | Rydberg Matter (RM) theory is previously shown to give good agreement with
the unidentified infrared bands (UIR, UIB) that are observed in emission from
many objects in space. From stimulated emission studies in RM, a slightly
simpler theoretical model is found that describes the transitions giving the
UIR bands bett... | astro-ph | rydberg matter rm theory is previously shown to give good agreement with the unidentified infrared bands uir uib that are observed in emission from many objects in space from stimulated emission studies in rm a slightly simpler theoretical model is found that describes the transitions giving the uir bands better the ge... | [['rydberg', 'matter', 'rm', 'theory', 'is', 'previously', 'shown', 'to', 'give', 'good', 'agreement', 'with', 'the', 'unidentified', 'infrared', 'bands', 'uir', 'uib', 'that', 'are', 'observed', 'in', 'emission', 'from', 'many', 'objects', 'in', 'space', 'from', 'stimulated', 'emission', 'studies', 'in', 'rm', 'a', 's... | [-0.05355432801857003, 0.15373467874031954, -0.0158648586515429, 0.07911272444464083, 0.01628834786916638, -0.12337132206523856, 0.043756048129687974, 0.41278435157731247, -0.19214604873889185, -0.41087237260593423, 0.043740992469878254, -0.2986601365620059, -0.0670351439139581, 0.19529041006422504, -0.0187961529249903... |
710.3294 | Theories for the Fermi Scale | I give a short review of our present understanding of new theories of the
electroweak scale, with emphasis on recent progress. Plenary talk at the EPS
2007 Conference at Manchester.
| hep-ph | i give a short review of our present understanding of new theories of the electroweak scale with emphasis on recent progress plenary talk at the eps 2007 conference at manchester | [['i', 'give', 'a', 'short', 'review', 'of', 'our', 'present', 'understanding', 'of', 'new', 'theories', 'of', 'the', 'electroweak', 'scale', 'with', 'emphasis', 'on', 'recent', 'progress', 'plenary', 'talk', 'at', 'the', 'eps', '2007', 'conference', 'at', 'manchester']] | [-0.10854907693962255, 0.1362148108271261, -0.10441402851914366, -0.0008522470792134603, -0.10124983421216409, -0.12409850910771639, 0.004414626234211028, 0.2891632272551457, -0.10766966522981723, -0.3724277646591266, 0.1242858895411094, -0.2391099968769898, -0.1351363405585289, 0.1583192003890872, -0.06261903280392289... |
710.3295 | Phase control algorithms for focusing light through turbid media | Light propagation in materials with microscopic inhomogeneities is affected
by scattering. In scattering materials, such as powders, disordered
metamaterials or biological tissue, multiple scattering on sub-wavelength
particles makes light diffuse. Recently, we showed that it is possible to
construct a wavefront that... | cond-mat.dis-nn cond-mat.mes-hall | light propagation in materials with microscopic inhomogeneities is affected by scattering in scattering materials such as powders disordered metamaterials or biological tissue multiple scattering on subwavelength particles makes light diffuse recently we showed that it is possible to construct a wavefront that focuses ... | [['light', 'propagation', 'in', 'materials', 'with', 'microscopic', 'inhomogeneities', 'is', 'affected', 'by', 'scattering', 'in', 'scattering', 'materials', 'such', 'as', 'powders', 'disordered', 'metamaterials', 'or', 'biological', 'tissue', 'multiple', 'scattering', 'on', 'subwavelength', 'particles', 'makes', 'ligh... | [-0.08268231006004034, 0.20056139279809812, -0.09926736027678582, 0.033702261008879845, -0.07017284573595615, -0.13776800540352988, -0.004413195104178065, 0.46498639153162385, -0.24961635546023203, -0.28901539337791643, 0.08359664440774922, -0.2965066124489353, -0.2145575673532951, 0.20211376154285138, -0.0570786192013... |
710.3296 | One more approach to the convergence of the empirical process to the
Brownian bridge | A theorem of Donsker asserts that the empirical process converges in
distribution to the Brownian bridge. The aim of this paper is to provide a new
and simple proof of this fact.
| math.PR math.ST stat.TH | a theorem of donsker asserts that the empirical process converges in distribution to the brownian bridge the aim of this paper is to provide a new and simple proof of this fact | [['a', 'theorem', 'of', 'donsker', 'asserts', 'that', 'the', 'empirical', 'process', 'converges', 'in', 'distribution', 'to', 'the', 'brownian', 'bridge', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'provide', 'a', 'new', 'and', 'simple', 'proof', 'of', 'this', 'fact']] | [-0.06740198429906741, 0.03339505771873519, -0.2407784653478302, 0.06595830516590695, -0.07990852622606326, -0.06589148458442651, 0.10060129716657684, 0.29406559857307, -0.295887881424278, -0.24968801077920943, 0.04340402908201213, -0.2388511106837541, -0.20232921018032357, 0.18164411210455, -0.1965184253640473, 0.0091... |
710.3297 | Computing the optimal protocol for finite-time processes in stochastic
thermodynamics | Asking for the optimal protocol of an external control parameter that
minimizes the mean work required to drive a nano-scale system from one
equilibrium state to another in finite time, Schmiedl and Seifert ({\it Phys.
Rev. Lett.} {\bf 98}, 108301 (2007)) found the Euler-Lagrange equation to be a
non-local integro-di... | cond-mat.stat-mech | asking for the optimal protocol of an external control parameter that minimizes the mean work required to drive a nanoscale system from one equilibrium state to another in finite time schmiedl and seifert it phys rev lett bf 98 108301 2007 found the eulerlagrange equation to be a nonlocal integrodifferential equation o... | [['asking', 'for', 'the', 'optimal', 'protocol', 'of', 'an', 'external', 'control', 'parameter', 'that', 'minimizes', 'the', 'mean', 'work', 'required', 'to', 'drive', 'a', 'nanoscale', 'system', 'from', 'one', 'equilibrium', 'state', 'to', 'another', 'in', 'finite', 'time', 'schmiedl', 'and', 'seifert', 'it', 'phys', ... | [-0.15484456872602678, 0.10340794596839191, -0.0948584560427885, 0.033347223715127425, -0.06378808022775459, -0.20854438213139492, 0.050439013565785056, 0.38055631851355703, -0.27651597072264916, -0.3128048357694357, 0.052726408104271684, -0.25927310425432326, -0.21089218516465066, 0.22231460740473472, -0.0700010863343... |
710.3298 | Stability of monolayers and bilayers in a copolymer-homopolymer blend
model | We study the stability of layered structures in a variational model for
diblock copolymer-homopolymer blends. The main step consists of calculating the
first and second derivative of a sharp-interface Ohta-Kawasaki energy for
straight mono- and bilayers. By developing the interface perturbations in a
Fourier series w... | math-ph math.AP math.MP | we study the stability of layered structures in a variational model for diblock copolymerhomopolymer blends the main step consists of calculating the first and second derivative of a sharpinterface ohtakawasaki energy for straight mono and bilayers by developing the interface perturbations in a fourier series we fully ... | [['we', 'study', 'the', 'stability', 'of', 'layered', 'structures', 'in', 'a', 'variational', 'model', 'for', 'diblock', 'copolymerhomopolymer', 'blends', 'the', 'main', 'step', 'consists', 'of', 'calculating', 'the', 'first', 'and', 'second', 'derivative', 'of', 'a', 'sharpinterface', 'ohtakawasaki', 'energy', 'for', ... | [-0.12690506185489622, 0.04326590239493684, -0.09647847098610575, 0.05195954457899048, -0.01339075106873431, -0.047730214152993125, 0.024838655738593927, 0.34490403726654634, -0.2610920918364586, -0.27646276422522287, 0.09556332568701525, -0.23177485528338532, -0.17741437174580907, 0.16333261487042447, 0.00639273961794... |
710.3299 | Many body physics and the capacity of quantum channels with memory | In most studies of the capacity of quantum channels, it is assumed that the
errors in each use of the channel are independent. However, recent work has
begun to investigate the effects of memory or correlations in the error, and
has led to suggestions that there can be interesting non-analytic behaviour in
the capaci... | quant-ph | in most studies of the capacity of quantum channels it is assumed that the errors in each use of the channel are independent however recent work has begun to investigate the effects of memory or correlations in the error and has led to suggestions that there can be interesting nonanalytic behaviour in the capacity of s... | [['in', 'most', 'studies', 'of', 'the', 'capacity', 'of', 'quantum', 'channels', 'it', 'is', 'assumed', 'that', 'the', 'errors', 'in', 'each', 'use', 'of', 'the', 'channel', 'are', 'independent', 'however', 'recent', 'work', 'has', 'begun', 'to', 'investigate', 'the', 'effects', 'of', 'memory', 'or', 'correlations', 'i... | [-0.14149954203539383, 0.10112822874339286, -0.09207769672629303, 0.06834177097655625, -0.024725454853650946, -0.14452146017715706, 0.06692666123890151, 0.36032350090627346, -0.26888447854543535, -0.28281353819560007, 0.11307473399066106, -0.27910898407481566, -0.18769773360781417, 0.1987164422424267, -0.08117569297239... |
710.33 | Self-organization of irregular NEM vibrations in multi-mode shuttle
structures | We investigate theoretically multi-mode electromechanical "shuttle"
instabilities in DC voltage-biased nanoelectromechanical single-electron
tunneling (NEM-SET) devices. We show that initially irregular (quasi-periodic)
oscillations, that occur as a result of the simultaneous self-excitation of
several mechanical mod... | cond-mat.mes-hall | we investigate theoretically multimode electromechanical shuttle instabilities in dc voltagebiased nanoelectromechanical singleelectron tunneling nemset devices we show that initially irregular quasiperiodic oscillations that occur as a result of the simultaneous selfexcitation of several mechanical modes with incommen... | [['we', 'investigate', 'theoretically', 'multimode', 'electromechanical', 'shuttle', 'instabilities', 'in', 'dc', 'voltagebiased', 'nanoelectromechanical', 'singleelectron', 'tunneling', 'nemset', 'devices', 'we', 'show', 'that', 'initially', 'irregular', 'quasiperiodic', 'oscillations', 'that', 'occur', 'as', 'a', 're... | [-0.2931005700624415, 0.2367203802419161, -0.07127768763207963, 0.02286802509500246, -0.05475232781443213, -0.18485350271553866, 0.07918554217488105, 0.34388741510254994, -0.27951228194870054, -0.21983344424515963, 0.03028818739278774, -0.2360604206465983, -0.17951518821396997, 0.2521399246794837, -0.000362017950309174... |
710.3301 | Deleting a marked item from an unsorted database with a single query | In this Letter we present a quantum deletion algorithm that deletes a marked
state from an unsorted database of $N$ items with only a single query. This
algorithm achieves exponential speedup compared with classical algorithm where
O(N) number of query is required. General property of this deleting algorithm
is also ... | quant-ph | in this letter we present a quantum deletion algorithm that deletes a marked state from an unsorted database of n items with only a single query this algorithm achieves exponential speedup compared with classical algorithm where on number of query is required general property of this deleting algorithm is also studied | [['in', 'this', 'letter', 'we', 'present', 'a', 'quantum', 'deletion', 'algorithm', 'that', 'deletes', 'a', 'marked', 'state', 'from', 'an', 'unsorted', 'database', 'of', 'n', 'items', 'with', 'only', 'a', 'single', 'query', 'this', 'algorithm', 'achieves', 'exponential', 'speedup', 'compared', 'with', 'classical', 'al... | [-0.12910963174905263, 0.05138254203341728, -0.07603716815127899, -0.03761233222515633, -0.06749329908623122, -0.2213676812802898, 0.17986895683605006, 0.4008403756454879, -0.2949074155413637, -0.3516767873045276, 0.00876309558082664, -0.29763620383307043, -0.1606589093411743, 0.16506654002210674, -0.1295874444950445, ... |
710.3302 | On the Caudrey-Beals-Coifman System and the Gauge Group Action | The generalized Zakharov-Shabat systems with complex-valued Cartan elements
and the systems studied by Caudrey, Beals and Coifman (CBC systems) and their
gauge equivalent are studies. This includes: the properties of fundamental
analytical solutions (FAS) for the gauge-equivalent to CBC systems and the
minimal set of... | nlin.SI hep-th math-ph math.MP | the generalized zakharovshabat systems with complexvalued cartan elements and the systems studied by caudrey beals and coifman cbc systems and their gauge equivalent are studies this includes the properties of fundamental analytical solutions fas for the gaugeequivalent to cbc systems and the minimal set of scattering ... | [['the', 'generalized', 'zakharovshabat', 'systems', 'with', 'complexvalued', 'cartan', 'elements', 'and', 'the', 'systems', 'studied', 'by', 'caudrey', 'beals', 'and', 'coifman', 'cbc', 'systems', 'and', 'their', 'gauge', 'equivalent', 'are', 'studies', 'this', 'includes', 'the', 'properties', 'of', 'fundamental', 'an... | [-0.16777468592280875, 0.06664400661011806, -0.018460350564202747, 0.10342251407014005, -0.08791843877249472, -0.12660553665026217, -0.02518592175801058, 0.2885889679986379, -0.3187987208932739, -0.23992115467459568, 0.14604911739572984, -0.30028839690006665, -0.21514039700756454, 0.20933711302240152, 0.001272634496106... |
710.3303 | On a conjecture of Serre on abelian threefolds | In this article, we give a reformulation of a result from Howe, Leprevost and
Poonen on a three dimensional family of abelian threefolds. We also link their
result to a conjecture of Serre on a precise form of Torelli theorem for genus
3 curves.
| math.NT math.AG | in this article we give a reformulation of a result from howe leprevost and poonen on a three dimensional family of abelian threefolds we also link their result to a conjecture of serre on a precise form of torelli theorem for genus 3 curves | [['in', 'this', 'article', 'we', 'give', 'a', 'reformulation', 'of', 'a', 'result', 'from', 'howe', 'leprevost', 'and', 'poonen', 'on', 'a', 'three', 'dimensional', 'family', 'of', 'abelian', 'threefolds', 'we', 'also', 'link', 'their', 'result', 'to', 'a', 'conjecture', 'of', 'serre', 'on', 'a', 'precise', 'form', 'of... | [-0.190534547267651, 0.004345318884588778, -0.18125116946281528, 0.09681617894834331, -0.1010036411779848, -0.13431394086431034, 0.10006261945818551, 0.27513672005046497, -0.2380736846455627, -0.2739562206816944, 0.09794655631412752, -0.22020146794701842, -0.18676305308260702, 0.28263455361593515, -0.21979899520308457,... |
710.3304 | Measured quantum probability distribution functions for Brownian motion | The quantum analog of the joint probability distributions describing a
classical stochastic process is introduced. A prescription is given for
constructing the quantum distribution associated with a sequence of
measurements. For the case of quantum Brownian motion this prescription is
illustrated with a number of exp... | quant-ph | the quantum analog of the joint probability distributions describing a classical stochastic process is introduced a prescription is given for constructing the quantum distribution associated with a sequence of measurements for the case of quantum brownian motion this prescription is illustrated with a number of explici... | [['the', 'quantum', 'analog', 'of', 'the', 'joint', 'probability', 'distributions', 'describing', 'a', 'classical', 'stochastic', 'process', 'is', 'introduced', 'a', 'prescription', 'is', 'given', 'for', 'constructing', 'the', 'quantum', 'distribution', 'associated', 'with', 'a', 'sequence', 'of', 'measurements', 'for'... | [-0.09121422606777066, 0.16707340699548906, -0.13758458513527727, 0.06971446177799524, -0.02894661394515051, -0.13001519697718322, 0.018692794057409257, 0.31363365400093013, -0.22888366863704646, -0.26604388237524873, 0.05315677301498512, -0.24765815364364058, -0.1749151094028583, 0.22976598371184456, -0.07138042661767... |
710.3305 | Automatic Methods for Analyzing Non-Repudiation Protocols with an Active
Intruder | Non-repudiation protocols have an important role in many areas where secured
transactions with proofs of participation are necessary. Formal methods are
clever and without error, therefore using them for verifying such protocols is
crucial. In this purpose, we show how to partially represent non-repudiation as
a comb... | cs.LO cs.CR | nonrepudiation protocols have an important role in many areas where secured transactions with proofs of participation are necessary formal methods are clever and without error therefore using them for verifying such protocols is crucial in this purpose we show how to partially represent nonrepudiation as a combination ... | [['nonrepudiation', 'protocols', 'have', 'an', 'important', 'role', 'in', 'many', 'areas', 'where', 'secured', 'transactions', 'with', 'proofs', 'of', 'participation', 'are', 'necessary', 'formal', 'methods', 'are', 'clever', 'and', 'without', 'error', 'therefore', 'using', 'them', 'for', 'verifying', 'such', 'protocol... | [-0.11642328534339628, 0.007909423389145033, -0.10149675267625992, 0.10083627763072543, -0.0925713985956176, -0.21816339875620447, 0.07383616444330025, 0.3975169777618966, -0.24339334040537083, -0.3364192252660072, 0.11944320525110111, -0.2182577128160598, -0.14478225428626357, 0.26041361302946153, -0.13049831492734434... |
710.3306 | Light-mass Bragg cavity polaritons in planar quantum dot lattices | The exciton-polariton modes of a quantum dot lattice embedded in a planar
optical cavity are theoretically investigated. Umklapp terms, in which an
exciton interacts with many cavity modes differing by reciprocal lattice
vectors, appear in the Hamiltonian due to the periodicity of the dot lattice.
We focus on Bragg p... | cond-mat.mes-hall | the excitonpolariton modes of a quantum dot lattice embedded in a planar optical cavity are theoretically investigated umklapp terms in which an exciton interacts with many cavity modes differing by reciprocal lattice vectors appear in the hamiltonian due to the periodicity of the dot lattice we focus on bragg polarito... | [['the', 'excitonpolariton', 'modes', 'of', 'a', 'quantum', 'dot', 'lattice', 'embedded', 'in', 'a', 'planar', 'optical', 'cavity', 'are', 'theoretically', 'investigated', 'umklapp', 'terms', 'in', 'which', 'an', 'exciton', 'interacts', 'with', 'many', 'cavity', 'modes', 'differing', 'by', 'reciprocal', 'lattice', 'vec... | [-0.20145213472492554, 0.3170707839113873, -0.028010838758983032, 0.012683575768087317, -0.02542926582406048, -0.12763637819712856, 0.04277030097324589, 0.4302808448864037, -0.22686305681259192, -0.26349026911320683, 0.01552929897096102, -0.2897645975737011, -0.05176196345949874, 0.18559805619600817, 0.0294115934951403... |
710.3307 | The theory of the "0.7 anomaly" in quantum point contacts | The phenomenology of the "0.7 anomaly" in quantum point contacts is fully
explained in terms of a quasi-localized state, which forms as the point contact
opens up. Detailed numerical calculations within spin-density functional theory
indeed con rm the emergence of such a state. Quantitative calculations of the
conduc... | cond-mat.mes-hall cond-mat.str-el | the phenomenology of the 07 anomaly in quantum point contacts is fully explained in terms of a quasilocalized state which forms as the point contact opens up detailed numerical calculations within spindensity functional theory indeed con rm the emergence of such a state quantitative calculations of the conductance and ... | [['the', 'phenomenology', 'of', 'the', '07', 'anomaly', 'in', 'quantum', 'point', 'contacts', 'is', 'fully', 'explained', 'in', 'terms', 'of', 'a', 'quasilocalized', 'state', 'which', 'forms', 'as', 'the', 'point', 'contact', 'opens', 'up', 'detailed', 'numerical', 'calculations', 'within', 'spindensity', 'functional',... | [-0.15854637951765588, 0.09540977256129617, -0.10651937168533576, 0.049608026410156075, 0.008572663970129646, -0.09602406539319866, 0.08586791134945562, 0.3386799026064683, -0.21218805743948274, -0.318608107207262, 0.05455455201698224, -0.3503339748181727, -0.16861045208887832, 0.1873274421002176, 0.04427082180990365, ... |
710.3308 | Multicomponent solution in modified theory of gravity in the early
universe | We study the modified theory of gravity in Friedmann Robertson Walker
universe composed of several perfect fluids. We consider the power law
inflation and determine the equation of state parameters in terms of the
parameters of modified gravity's Lagrangian in the early universe. We also
discuss briefly the gravitati... | gr-qc astro-ph hep-th | we study the modified theory of gravity in friedmann robertson walker universe composed of several perfect fluids we consider the power law inflation and determine the equation of state parameters in terms of the parameters of modified gravitys lagrangian in the early universe we also discuss briefly the gravitational ... | [['we', 'study', 'the', 'modified', 'theory', 'of', 'gravity', 'in', 'friedmann', 'robertson', 'walker', 'universe', 'composed', 'of', 'several', 'perfect', 'fluids', 'we', 'consider', 'the', 'power', 'law', 'inflation', 'and', 'determine', 'the', 'equation', 'of', 'state', 'parameters', 'in', 'terms', 'of', 'the', 'pa... | [-0.1718498528759294, 0.14764740571098509, -0.1107736361863197, 0.11435736718209777, -0.07671945777563553, -0.12338299399136372, -0.05837522253156903, 0.2435146198730986, -0.21457906714025535, -0.2938468151919122, 0.023166895685893186, -0.2114387818717591, -0.13939163431894244, 0.09581670849935485, -0.06197721922313267... |
710.3309 | Radiative corrections to W-boson hadroproduction: higher-order
electroweak and supersymmetric effects | The high accuracy envisaged for future measurements of W-boson production at
hadron colliders has to be matched by precise theoretical predictions. We study
the impact of electroweak radiative corrections on W-boson production cross
sections and differential distributions at the Tevatron and at the LHC. In
particular... | hep-ph | the high accuracy envisaged for future measurements of wboson production at hadron colliders has to be matched by precise theoretical predictions we study the impact of electroweak radiative corrections on wboson production cross sections and differential distributions at the tevatron and at the lhc in particular we in... | [['the', 'high', 'accuracy', 'envisaged', 'for', 'future', 'measurements', 'of', 'wboson', 'production', 'at', 'hadron', 'colliders', 'has', 'to', 'be', 'matched', 'by', 'precise', 'theoretical', 'predictions', 'we', 'study', 'the', 'impact', 'of', 'electroweak', 'radiative', 'corrections', 'on', 'wboson', 'production'... | [0.006420523772016168, 0.209847891587764, -0.03757654956355691, 0.17313589699566365, -0.029873043425381184, -0.1052787666558288, 0.04117686035297811, 0.32575547888875006, -0.15233822260051966, -0.27755013122037053, -0.0371051551643759, -0.3684631997849792, 0.08557340357080102, 0.15033368938509376, 0.08096890308521688, ... |
710.331 | Two-parameter model predictions and theta-point crossover for
linear-polymer solutions | We consider the first few virial coefficients of the osmotic pressure, the
radius of gyration, the hydrodynamic radius, and the end-to-end distance for a
monodisperse polymer solution. We determine the corresponding two-parameter
model functions which parametrize the crossover between the good-solvent and
the ideal-c... | cond-mat.soft cond-mat.stat-mech | we consider the first few virial coefficients of the osmotic pressure the radius of gyration the hydrodynamic radius and the endtoend distance for a monodisperse polymer solution we determine the corresponding twoparameter model functions which parametrize the crossover between the goodsolvent and the idealchain behavi... | [['we', 'consider', 'the', 'first', 'few', 'virial', 'coefficients', 'of', 'the', 'osmotic', 'pressure', 'the', 'radius', 'of', 'gyration', 'the', 'hydrodynamic', 'radius', 'and', 'the', 'endtoend', 'distance', 'for', 'a', 'monodisperse', 'polymer', 'solution', 'we', 'determine', 'the', 'corresponding', 'twoparameter',... | [-0.09716178089434253, 0.14921194550992947, -0.09326729208122993, 0.016712986344498568, -0.00253230475726119, -0.10274090222420468, 0.03278362874002398, 0.32113273003125103, -0.2943312133041521, -0.24681594319121938, 0.03814108777399836, -0.28379551251081453, -0.09552787689735061, 0.13777441765093987, 0.031489535865451... |
710.3311 | Global firing induced by network disorder in ensembles of active
rotators | We study the influence of repulsive interactions on an ensemble of coupled
excitable rotators. We find that a moderate fraction of repulsive interactions
can trigger global firing of the ensemble. The regime of global firing,
however, is suppressed in sufficiently large systems if the network of
repulsive interaction... | cond-mat.soft cond-mat.stat-mech | we study the influence of repulsive interactions on an ensemble of coupled excitable rotators we find that a moderate fraction of repulsive interactions can trigger global firing of the ensemble the regime of global firing however is suppressed in sufficiently large systems if the network of repulsive interactions is f... | [['we', 'study', 'the', 'influence', 'of', 'repulsive', 'interactions', 'on', 'an', 'ensemble', 'of', 'coupled', 'excitable', 'rotators', 'we', 'find', 'that', 'a', 'moderate', 'fraction', 'of', 'repulsive', 'interactions', 'can', 'trigger', 'global', 'firing', 'of', 'the', 'ensemble', 'the', 'regime', 'of', 'global', ... | [-0.17061551381749185, 0.19624358719672522, -0.02472921045105481, 0.05590626791923899, 0.007724357070401311, -0.11951169390231371, 0.03161808554591103, 0.3409453024622053, -0.2679446906147694, -0.24502028958363967, 0.0242740971671248, -0.2703883090141145, -0.19617245525799015, 0.09692163084929978, -0.029415467965670607... |
710.3312 | On C-fibrations over projective curves | The goal of this paper is to present a modified version (GML) of ML invariant
which should take into account rulings over a projective base and allow further
stratification of smooth affine rational surfaces. We provide a non-trivial
example where GML invariant is computed for a smooth affine rational surface
admitti... | math.AG | the goal of this paper is to present a modified version gml of ml invariant which should take into account rulings over a projective base and allow further stratification of smooth affine rational surfaces we provide a nontrivial example where gml invariant is computed for a smooth affine rational surface admitting no ... | [['the', 'goal', 'of', 'this', 'paper', 'is', 'to', 'present', 'a', 'modified', 'version', 'gml', 'of', 'ml', 'invariant', 'which', 'should', 'take', 'into', 'account', 'rulings', 'over', 'a', 'projective', 'base', 'and', 'allow', 'further', 'stratification', 'of', 'smooth', 'affine', 'rational', 'surfaces', 'we', 'pro... | [-0.18552849934651303, 0.025074794974464635, -0.16292509564126914, 0.09107479178883995, -0.12818075735838366, -0.20501855683441345, 0.02461226790641936, 0.34534169816626953, -0.2692341360621727, -0.21656769821420313, 0.09547136436001613, -0.157502917956131, -0.19277733696194796, 0.19287742657157092, -0.1452114295997979... |
710.3313 | On the gamma-ray emission of Type Ia Supernovae | A multi-dimension, time-dependent Monte Carlo code is used to compute sample
gamma-ray spectra to explore whether unambiguous constraints could be obtained
from gamma-ray observations of Type Ia supernovae. Both spherical and
aspherical geometries are considered and it is shown that moderate departures
from sphericit... | astro-ph | a multidimension timedependent monte carlo code is used to compute sample gammaray spectra to explore whether unambiguous constraints could be obtained from gammaray observations of type ia supernovae both spherical and aspherical geometries are considered and it is shown that moderate departures from sphericity can pr... | [['a', 'multidimension', 'timedependent', 'monte', 'carlo', 'code', 'is', 'used', 'to', 'compute', 'sample', 'gammaray', 'spectra', 'to', 'explore', 'whether', 'unambiguous', 'constraints', 'could', 'be', 'obtained', 'from', 'gammaray', 'observations', 'of', 'type', 'ia', 'supernovae', 'both', 'spherical', 'and', 'asph... | [-0.04306972715899846, 0.1370380578850319, -0.07660339052260966, 0.19104467745452147, -0.1156728312480308, -0.16691590763723393, 0.026627433100703417, 0.43088338576304686, -0.22763078422715685, -0.3589460470114544, 0.11010707888357744, -0.28568265600438425, -0.027198083253850223, 0.2895027710789233, -0.0344322340694648... |
710.3314 | Pulsational pair instability as an explanation for the most luminous
supernovae | The extremely luminous supernova SN 2006gy challenges the traditional view
that the collapse of a stellar core is the only mechanism by which a massive
star makes a supernova, because it seems too luminous by more than a factor of
ten. Here we report that the brightest supernovae in the modern Universe arise
from col... | astro-ph | the extremely luminous supernova sn 2006gy challenges the traditional view that the collapse of a stellar core is the only mechanism by which a massive star makes a supernova because it seems too luminous by more than a factor of ten here we report that the brightest supernovae in the modern universe arise from collisi... | [['the', 'extremely', 'luminous', 'supernova', 'sn', '2006gy', 'challenges', 'the', 'traditional', 'view', 'that', 'the', 'collapse', 'of', 'a', 'stellar', 'core', 'is', 'the', 'only', 'mechanism', 'by', 'which', 'a', 'massive', 'star', 'makes', 'a', 'supernova', 'because', 'it', 'seems', 'too', 'luminous', 'by', 'more... | [-0.06609297660902921, 0.1852231444279587, -0.0696651885749004, 0.1415664236394078, -0.1253534969755338, -0.10073148886709984, 0.03981687924969352, 0.36769636834071856, -0.1733209729341969, -0.311378363193681, 0.06921263388358057, -0.32289389955500764, -0.030464977375889397, 0.2175216705828631, -0.025054393732161617, -... |
710.3315 | Can the Quantum Measurement Problem be resolved within the framework of
Schroedinger Dynamics and Quantum Probability? | We provide an affirmative answer to the question posed in the title. Our
argument is based on a treatment of the Schroedinger dynamics of the composite
of a quantum microsystem, S, and a macroscopic measuring apparatus, I,
consisting of N interacting particles. The pointer positions of this apparatus
are represented ... | quant-ph math-ph math.MP | we provide an affirmative answer to the question posed in the title our argument is based on a treatment of the schroedinger dynamics of the composite of a quantum microsystem s and a macroscopic measuring apparatus i consisting of n interacting particles the pointer positions of this apparatus are represented by ortho... | [['we', 'provide', 'an', 'affirmative', 'answer', 'to', 'the', 'question', 'posed', 'in', 'the', 'title', 'our', 'argument', 'is', 'based', 'on', 'a', 'treatment', 'of', 'the', 'schroedinger', 'dynamics', 'of', 'the', 'composite', 'of', 'a', 'quantum', 'microsystem', 's', 'and', 'a', 'macroscopic', 'measuring', 'appara... | [-0.14748718667330898, 0.15228434110681657, -0.08697055297141726, 0.022193469868260294, -0.013169996723511511, -0.14869947177287418, 0.05180460768028614, 0.30936177002943377, -0.2594187285073779, -0.2847741490201742, 0.03583113994770401, -0.26443065286289447, -0.09184240784750065, 0.15036612197008886, -0.02738899156578... |
710.3316 | Internal-state thermometry by depletion spectroscopy in a cold guided
beam of formaldehyde | We present measurements of the internal state distribution of
electrostatically guided formaldehyde. Upon excitation with continuous tunable
ultraviolet laser light the molecules dissociate, leading to a decrease in the
molecular flux. The population of individual guided states is measured by
addressing transitions o... | physics.chem-ph | we present measurements of the internal state distribution of electrostatically guided formaldehyde upon excitation with continuous tunable ultraviolet laser light the molecules dissociate leading to a decrease in the molecular flux the population of individual guided states is measured by addressing transitions origin... | [['we', 'present', 'measurements', 'of', 'the', 'internal', 'state', 'distribution', 'of', 'electrostatically', 'guided', 'formaldehyde', 'upon', 'excitation', 'with', 'continuous', 'tunable', 'ultraviolet', 'laser', 'light', 'the', 'molecules', 'dissociate', 'leading', 'to', 'a', 'decrease', 'in', 'the', 'molecular', ... | [-0.07212137485468628, 0.20183647619654435, -0.08179405372533383, -0.0074973519305896125, 0.051249426679046015, -0.10817140128200102, 0.13868085596701035, 0.40978032017521787, -0.2176373199079976, -0.35618720811349575, -0.003909421860089883, -0.3083075053162045, 0.015127963856840976, 0.18452598605859988, 0.037810585715... |
710.3317 | Surface effects in magnetic superconductors with a spiral magnetic
structure | We consider a magnetic superconductor MS with a spiral magnetic structure. On
the basis of generalized Eilenberger and Usadel equations we show that near the
boundary of the MS with an insulator or vacuum the condensate (Gor'kov's)
Green's functions are disturbed by boundary conditions and differ essentially
from the... | cond-mat.supr-con cond-mat.mes-hall | we consider a magnetic superconductor ms with a spiral magnetic structure on the basis of generalized eilenberger and usadel equations we show that near the boundary of the ms with an insulator or vacuum the condensate gorkovs greens functions are disturbed by boundary conditions and differ essentially from their value... | [['we', 'consider', 'a', 'magnetic', 'superconductor', 'ms', 'with', 'a', 'spiral', 'magnetic', 'structure', 'on', 'the', 'basis', 'of', 'generalized', 'eilenberger', 'and', 'usadel', 'equations', 'we', 'show', 'that', 'near', 'the', 'boundary', 'of', 'the', 'ms', 'with', 'an', 'insulator', 'or', 'vacuum', 'the', 'cond... | [-0.20623010980737647, 0.1709922569071802, -0.0684823779234515, 0.027856484350816505, -0.03960804008061021, -0.09132313519731407, 0.05693390827656277, 0.3306777351876585, -0.23726476876186284, -0.25435164735872084, -0.006158371656618225, -0.29924190851170723, -0.08596990465913422, 0.20843800905773915, 0.065742464910253... |
710.3318 | CP violation in chargino production in e+e- collisions | We present the analysis of CP-violating effects in non-diagonal chargino pair
production in e+e- collisions. These effects appear only at the one-loop level.
We show that CP-odd asymmetries in chargino production are sensitive to the
phases of mu and A_t parameters and can be of the order of a few %.
| hep-ph | we present the analysis of cpviolating effects in nondiagonal chargino pair production in ee collisions these effects appear only at the oneloop level we show that cpodd asymmetries in chargino production are sensitive to the phases of mu and a_t parameters and can be of the order of a few | [['we', 'present', 'the', 'analysis', 'of', 'cpviolating', 'effects', 'in', 'nondiagonal', 'chargino', 'pair', 'production', 'in', 'ee', 'collisions', 'these', 'effects', 'appear', 'only', 'at', 'the', 'oneloop', 'level', 'we', 'show', 'that', 'cpodd', 'asymmetries', 'in', 'chargino', 'production', 'are', 'sensitive', ... | [-0.15648374903015794, 0.28564993862062693, -0.035118115721270445, 0.14223609961569308, -0.008193524745292962, -0.11375499651767314, 0.03639797107316554, 0.32545295372605326, -0.23879694078117608, -0.26212524365633727, 0.017116480639670043, -0.34941190723329785, -0.014023583233356476, 0.1264411650598049, 0.081549043226... |
710.3319 | Correlations in connected random graphs | We study the properties of the giant connected component in random graphs
with arbitrary degree distribution. We concentrate on the degree-degree
correlations. We show that the adjoining nodes in the giant connected component
are correlated and derive analytic formulas for the joint nearest-neighbor
degree probabilit... | cond-mat.stat-mech cond-mat.other | we study the properties of the giant connected component in random graphs with arbitrary degree distribution we concentrate on the degreedegree correlations we show that the adjoining nodes in the giant connected component are correlated and derive analytic formulas for the joint nearestneighbor degree probability dist... | [['we', 'study', 'the', 'properties', 'of', 'the', 'giant', 'connected', 'component', 'in', 'random', 'graphs', 'with', 'arbitrary', 'degree', 'distribution', 'we', 'concentrate', 'on', 'the', 'degreedegree', 'correlations', 'we', 'show', 'that', 'the', 'adjoining', 'nodes', 'in', 'the', 'giant', 'connected', 'componen... | [-0.21083210177797204, 0.1553882554012489, -0.02778672882899021, 0.06634416172164492, -0.06081935699330643, -0.10642383915061752, 0.012618124385577781, 0.4542076109210029, -0.23557907936386377, -0.2570150465374657, 0.03711588604528515, -0.3455823862847562, -0.22334976767403228, 0.14083784169876404, -0.03166770298093979... |
710.332 | Complex Networks: Time-Dependent Connections and Silent Nodes | We studied, both analytically and numerically, complex excitable networks, in
which connections are time dependent and some of the nodes remain silent at
each time step. More specifically, (a) there is a heterogenous distribution of
connection weights and, depending on the current degree of order, some
connections ar... | cond-mat.dis-nn cond-mat.stat-mech | we studied both analytically and numerically complex excitable networks in which connections are time dependent and some of the nodes remain silent at each time step more specifically a there is a heterogenous distribution of connection weights and depending on the current degree of order some connections are reinforce... | [['we', 'studied', 'both', 'analytically', 'and', 'numerically', 'complex', 'excitable', 'networks', 'in', 'which', 'connections', 'are', 'time', 'dependent', 'and', 'some', 'of', 'the', 'nodes', 'remain', 'silent', 'at', 'each', 'time', 'step', 'more', 'specifically', 'a', 'there', 'is', 'a', 'heterogenous', 'distribu... | [-0.17959738490001687, 0.17998894586834763, -0.07132351702979106, 0.056808340168960934, -0.03423095931654817, -0.15932401116372327, 0.07964610060797271, 0.3619170851189266, -0.27354761110841075, -0.2632940740198985, 0.10510203414439653, -0.28106532457972655, -0.17576815725011186, 0.16148867037178677, -0.017248172679225... |
710.3321 | Efficient formalism for large scale ab initio molecular dynamics based
on time-dependent density functional theory | A new "on the fly" method to perform Born-Oppenheimer ab initio molecular
dynamics (AIMD) is presented. Inspired by Ehrenfest dynamics in time-dependent
density functional theory, the electronic orbitals are evolved by a
Schroedinger-like equation, where the orbital time derivative is multiplied by
a parameter. This ... | cond-mat.mtrl-sci physics.comp-ph | a new on the fly method to perform bornoppenheimer ab initio molecular dynamics aimd is presented inspired by ehrenfest dynamics in timedependent density functional theory the electronic orbitals are evolved by a schroedingerlike equation where the orbital time derivative is multiplied by a parameter this parameter con... | [['a', 'new', 'on', 'the', 'fly', 'method', 'to', 'perform', 'bornoppenheimer', 'ab', 'initio', 'molecular', 'dynamics', 'aimd', 'is', 'presented', 'inspired', 'by', 'ehrenfest', 'dynamics', 'in', 'timedependent', 'density', 'functional', 'theory', 'the', 'electronic', 'orbitals', 'are', 'evolved', 'by', 'a', 'schroedi... | [-0.12824922759819435, 0.14268240775482388, -0.11413144134360576, 0.06477644648878605, -0.05416635107950017, -0.09451818184786907, 0.04039829023437755, 0.3502019111227284, -0.32180397446838116, -0.29503690224874424, 0.03610725813014533, -0.23666829960320585, -0.15017071450429578, 0.14766373677099104, 0.0263972976895910... |
710.3322 | On the relation between Bell inequalities and nonlocal games | We investigate the relation between Bell inequalities and nonlocal games by
presenting a systematic method for their bilateral conversion. In particular,
we show that while to any nonlocal game there naturally corresponds a unique
Bell inequality, the converse is not true. As an illustration of the method we
present ... | quant-ph | we investigate the relation between bell inequalities and nonlocal games by presenting a systematic method for their bilateral conversion in particular we show that while to any nonlocal game there naturally corresponds a unique bell inequality the converse is not true as an illustration of the method we present a numb... | [['we', 'investigate', 'the', 'relation', 'between', 'bell', 'inequalities', 'and', 'nonlocal', 'games', 'by', 'presenting', 'a', 'systematic', 'method', 'for', 'their', 'bilateral', 'conversion', 'in', 'particular', 'we', 'show', 'that', 'while', 'to', 'any', 'nonlocal', 'game', 'there', 'naturally', 'corresponds', 'a... | [-0.0954604327589983, 0.045492300418406975, -0.11132030259995233, 0.13861670884089397, -0.05644964941200756, -0.2120190025940131, 0.0718116705483269, 0.3734101314164166, -0.24616552785012155, -0.2946753471143662, 0.05075315850701863, -0.24641484610499845, -0.20740196981009038, 0.1945226267423658, -0.09900754351641923, ... |
710.3323 | $D$ and $\bar{D}$ mesons in hot and dense matter | The $D$ and $\bar {D}$ mesons are studied in hot dense matter within a
self-consistent coupled-channel approach taking, as bare interaction, a broken
SU(4) s-wave Tomozawa-Weinberg interaction supplemented by an attractive
isoscalar-scalar term. The in-medium solution at finite temperature
incorporates Pauli blocking... | nucl-th hep-ph | the d and bar d mesons are studied in hot dense matter within a selfconsistent coupledchannel approach taking as bare interaction a broken su4 swave tomozawaweinberg interaction supplemented by an attractive isoscalarscalar term the inmedium solution at finite temperature incorporates pauli blocking effects baryon mean... | [['the', 'd', 'and', 'bar', 'd', 'mesons', 'are', 'studied', 'in', 'hot', 'dense', 'matter', 'within', 'a', 'selfconsistent', 'coupledchannel', 'approach', 'taking', 'as', 'bare', 'interaction', 'a', 'broken', 'su4', 'swave', 'tomozawaweinberg', 'interaction', 'supplemented', 'by', 'an', 'attractive', 'isoscalarscalar'... | [-0.13874280310119502, 0.23162887340970428, -0.10626682412839727, 0.1450513054842304, -0.029333049100387143, -0.17604424558521714, 0.0948106247051328, 0.3253620402319939, -0.19968359282756865, -0.22277915143058635, -0.09344252104892803, -0.34940494005422806, -0.010904872986429837, 0.03278651706932578, 0.097497444158349... |
710.3324 | Topology and Phases in Fermionic Systems | There can exist topological obstructions to continuously deforming a gapped
Hamiltonian for free fermions into a trivial form without closing the gap.
These topological obstructions are closely related to obstructions to the
existence of exponentially localized Wannier functions. We show that by taking
two copies of ... | quant-ph cond-mat.str-el | there can exist topological obstructions to continuously deforming a gapped hamiltonian for free fermions into a trivial form without closing the gap these topological obstructions are closely related to obstructions to the existence of exponentially localized wannier functions we show that by taking two copies of a ga... | [['there', 'can', 'exist', 'topological', 'obstructions', 'to', 'continuously', 'deforming', 'a', 'gapped', 'hamiltonian', 'for', 'free', 'fermions', 'into', 'a', 'trivial', 'form', 'without', 'closing', 'the', 'gap', 'these', 'topological', 'obstructions', 'are', 'closely', 'related', 'to', 'obstructions', 'to', 'the'... | [-0.1943437341083255, 0.22799979377563837, -0.0728384534115321, 0.07449001953937114, -0.09019400044603067, -0.1663293438497931, 0.057582455459568235, 0.35464713731133896, -0.298375806491822, -0.2615469958219263, 0.08127302487975814, -0.2771190055259568, -0.15847755392702917, 0.10212888090560833, -0.04300777776580718, 0... |
710.3325 | Testing CPT Symmetry with CMB Measurements | In this paper we study the possibility of testing \emph{CPT} symmetry with
Cosmic Microwave Background (CMB) measurements. Working with an effective
lagrangian of the photon with \emph{CPT} violation ${\cal L} \sim
p_{\mu}A_{\nu}\tilde F^{\mu\nu}$ which causes the polarization vectors of the
propagating CMB photons r... | hep-ph astro-ph gr-qc hep-th | in this paper we study the possibility of testing emphcpt symmetry with cosmic microwave background cmb measurements working with an effective lagrangian of the photon with emphcpt violation cal l sim p_mua_nutilde fmunu which causes the polarization vectors of the propagating cmb photons rotated we determine the rotat... | [['in', 'this', 'paper', 'we', 'study', 'the', 'possibility', 'of', 'testing', 'emphcpt', 'symmetry', 'with', 'cosmic', 'microwave', 'background', 'cmb', 'measurements', 'working', 'with', 'an', 'effective', 'lagrangian', 'of', 'the', 'photon', 'with', 'emphcpt', 'violation', 'cal', 'l', 'sim', 'p_mua_nutilde', 'fmunu'... | [-0.11354836840434251, 0.1526589728806308, -0.01581398005332999, 0.029274859979301942, -0.06434911853205916, -0.09157545458445973, 0.06565667185743616, 0.3079908598541609, -0.20175616628241827, -0.37434984707097346, 0.030420687951846048, -0.34425594064413345, -0.02552107603264016, 0.17888749872233617, -0.02233966930165... |
710.3326 | Narrow-Line Seyfert 1 Galaxies | I provide a short review of the properties of Narrow-line Seyfert 1 (NLS1)
galaxies across the electromagnetic spectrum and of the models to explain them.
Their continuum and emission-line properties manifest one extreme form of
Seyfert activity. As such, NLS1 galaxies may hold important clues to the key
parameters t... | astro-ph | i provide a short review of the properties of narrowline seyfert 1 nls1 galaxies across the electromagnetic spectrum and of the models to explain them their continuum and emissionline properties manifest one extreme form of seyfert activity as such nls1 galaxies may hold important clues to the key parameters that drive... | [['i', 'provide', 'a', 'short', 'review', 'of', 'the', 'properties', 'of', 'narrowline', 'seyfert', '1', 'nls1', 'galaxies', 'across', 'the', 'electromagnetic', 'spectrum', 'and', 'of', 'the', 'models', 'to', 'explain', 'them', 'their', 'continuum', 'and', 'emissionline', 'properties', 'manifest', 'one', 'extreme', 'fo... | [-0.04047257283673389, 0.06390612892028003, -0.028902328242111253, 0.22145825026927923, -0.1439067991086631, -0.16609362846065778, 0.06404068793563056, 0.476527016809996, -0.12006236307206564, -0.31779321220165, 0.03830202992503473, -0.2591191529536445, -0.013672160399437416, 0.20662975813320372, -0.032077662166557275,... |
710.3327 | A la Fock-Goncharov coordinates for PU(2,1) | We describe a set of coordinates on the PU(2,1)-representation variety of the
fundamental group of an oriented punctured surface $S$ with negative Euler
characteristic. The main technical tool we use is a set of geometric invariants
of a triple of flags in the complex hyperpolic plane. We establish a bijection
betwee... | math.DG | we describe a set of coordinates on the pu21representation variety of the fundamental group of an oriented punctured surface s with negative euler characteristic the main technical tool we use is a set of geometric invariants of a triple of flags in the complex hyperpolic plane we establish a bijection between a set of... | [['we', 'describe', 'a', 'set', 'of', 'coordinates', 'on', 'the', 'pu21representation', 'variety', 'of', 'the', 'fundamental', 'group', 'of', 'an', 'oriented', 'punctured', 'surface', 's', 'with', 'negative', 'euler', 'characteristic', 'the', 'main', 'technical', 'tool', 'we', 'use', 'is', 'a', 'set', 'of', 'geometric'... | [-0.23863345966336952, 0.020825939580707043, -0.09696206554392542, -0.00470131861579105, -0.08297167051637518, -0.0655670031176313, 0.042717077472395656, 0.3128524043637773, -0.32568664654441504, -0.25707612891910947, 0.05831788183844554, -0.24181910088974173, -0.1538144467479509, 0.2304811668244825, -0.124776242692293... |
710.3328 | Discussion of the Electromotive Force Terms in the Model of
Parker-unstable Galactic Disks with Cosmic Rays and Shear | We analyze the electromotive force (EMF) terms and basic assumptions of the
linear and nonlinear dynamo theories in our three-dimensional (3D) numerical
model of the Parker instability with cosmic rays and shear in a galactic disk.
We also apply the well known prescriptions of the EMF obtained by the nonlinear
dynamo... | astro-ph | we analyze the electromotive force emf terms and basic assumptions of the linear and nonlinear dynamo theories in our threedimensional 3d numerical model of the parker instability with cosmic rays and shear in a galactic disk we also apply the well known prescriptions of the emf obtained by the nonlinear dynamo theory ... | [['we', 'analyze', 'the', 'electromotive', 'force', 'emf', 'terms', 'and', 'basic', 'assumptions', 'of', 'the', 'linear', 'and', 'nonlinear', 'dynamo', 'theories', 'in', 'our', 'threedimensional', '3d', 'numerical', 'model', 'of', 'the', 'parker', 'instability', 'with', 'cosmic', 'rays', 'and', 'shear', 'in', 'a', 'gal... | [-0.0711988980022805, 0.08864288866230897, -0.06353334245946386, 0.11414271734598704, -0.08866028658090287, -0.04068306417421213, -0.029641665129898246, 0.31348314275965095, -0.2873092991207598, -0.3222875667270273, 0.05690154484031593, -0.20024805769709678, -0.18664857144628105, 0.2506195804533741, -0.0563074254414773... |
710.3329 | Universality and programmability of quantum computers | Manin, Feynman, and Deutsch have viewed quantum computing as a kind of
universal physical simulation procedure. Much of the writing about quantum
logic circuits and quantum Turing machines has shown how these machines can
simulate an arbitrary unitary transformation on a finite number of qubits. The
problem of univer... | quant-ph | manin feynman and deutsch have viewed quantum computing as a kind of universal physical simulation procedure much of the writing about quantum logic circuits and quantum turing machines has shown how these machines can simulate an arbitrary unitary transformation on a finite number of qubits the problem of universality... | [['manin', 'feynman', 'and', 'deutsch', 'have', 'viewed', 'quantum', 'computing', 'as', 'a', 'kind', 'of', 'universal', 'physical', 'simulation', 'procedure', 'much', 'of', 'the', 'writing', 'about', 'quantum', 'logic', 'circuits', 'and', 'quantum', 'turing', 'machines', 'has', 'shown', 'how', 'these', 'machines', 'can... | [-0.10116116911695715, 0.16112653273969618, -0.10004593437591675, 0.08523497435098176, -0.10128801205462357, -0.2120772759669749, 0.04438757757473824, 0.3044026116105287, -0.2848417288072309, -0.29691593840238995, 0.06388973370425904, -0.20206674844113706, -0.18475624420053777, 0.25195775260435344, -0.10752181561217147... |
710.333 | Astrophysics from data analysis of spherical gravitational wave
detectors | The direct detection of gravitational waves will provide valuable
astrophysical information about many celestial objects. Also, it will be an
important test to general relativity and other theories of gravitation. The
gravitational wave detector SCHENBERG has recently undergone its first test
run. It is expected to h... | astro-ph | the direct detection of gravitational waves will provide valuable astrophysical information about many celestial objects also it will be an important test to general relativity and other theories of gravitation the gravitational wave detector schenberg has recently undergone its first test run it is expected to have it... | [['the', 'direct', 'detection', 'of', 'gravitational', 'waves', 'will', 'provide', 'valuable', 'astrophysical', 'information', 'about', 'many', 'celestial', 'objects', 'also', 'it', 'will', 'be', 'an', 'important', 'test', 'to', 'general', 'relativity', 'and', 'other', 'theories', 'of', 'gravitation', 'the', 'gravitati... | [-0.1391059612526493, 0.11522726840127705, -0.12201557138509918, 0.07607254551176243, -0.1136749163392539, -0.07642452288500703, -0.048767643835673335, 0.3242570678090775, -0.21914319919316066, -0.32759837533363645, 0.13189632888973216, -0.2857109473593402, -0.13041220133176498, 0.2615436291068858, 0.013525320563706356... |
710.3331 | On a possible origin of a resonance-like structure in the two-photon
invariant mass spectrum of the reaction pp->ppgg | We show that the resonance-like structure found by the \emph{CELSIUS-WASA
Collaboration} in the two-photon invariant mass spectrum of the reaction $pp
\to pp \gamma \gamma$ is rather a signature of the $NN$-decoupled dibaryon
resonance $d^\star_1$(1956) that is produced in the radiative process $pp \to
\gamma d^\star... | hep-ph hep-ex nucl-ex nucl-th | we show that the resonancelike structure found by the emphcelsiuswasa collaboration in the twophoton invariant mass spectrum of the reaction pp to pp gamma gamma is rather a signature of the nndecoupled dibaryon resonance dstar_11956 that is produced in the radiative process pp to gamma dstar_1 and then undergoes radia... | [['we', 'show', 'that', 'the', 'resonancelike', 'structure', 'found', 'by', 'the', 'emphcelsiuswasa', 'collaboration', 'in', 'the', 'twophoton', 'invariant', 'mass', 'spectrum', 'of', 'the', 'reaction', 'pp', 'to', 'pp', 'gamma', 'gamma', 'is', 'rather', 'a', 'signature', 'of', 'the', 'nndecoupled', 'dibaryon', 'resona... | [-0.08417218408705492, 0.21904352617467632, -0.14757047819011002, 0.14459978202794788, -0.021692857339556487, -0.07699604092587559, 0.021420803844691517, 0.34984665256837066, -0.27971615399813876, -0.279381116386503, -0.13177687046227907, -0.32153000898729517, -0.03390515119888664, 0.1502180254209857, 0.124910307327672... |
710.3332 | Model and Program Repair via SAT Solving | We consider the following \emph{model repair problem}: given a finite Kripke
structure $M$ and a specification formula $\eta$ in some modal or temporal
logic, determine if $M$ contains a substructure $M'$ (with the same initial
state) that satisfies $\eta$. Thus, $M$ can be ``repaired'' to satisfy the
specification $... | cs.LO | we consider the following emphmodel repair problem given a finite kripke structure m and a specification formula eta in some modal or temporal logic determine if m contains a substructure m with the same initial state that satisfies eta thus m can be repaired to satisfy the specification eta by deleting some transition... | [['we', 'consider', 'the', 'following', 'emphmodel', 'repair', 'problem', 'given', 'a', 'finite', 'kripke', 'structure', 'm', 'and', 'a', 'specification', 'formula', 'eta', 'in', 'some', 'modal', 'or', 'temporal', 'logic', 'determine', 'if', 'm', 'contains', 'a', 'substructure', 'm', 'with', 'the', 'same', 'initial', '... | [-0.15724959183348025, 0.05761419319719496, -0.08741491943052629, 0.07996344853521938, -0.12120803923050805, -0.2471426631801012, 0.09502374810143942, 0.3645010030976065, -0.31609325632452967, -0.28695953473357894, 0.09442903002008524, -0.24115618119107152, -0.0914552163652133, 0.12327003332945269, -0.09532145155116734... |
710.3333 | Non-linear mechanical response of the Red Blood Cell | We measure the dynamical mechanical properties of human red blood cells.
Single cell response is measured with optical tweezers. We investigate both the
stress relaxation following a fast deformation, and the effect of varying the
strain rate. We find a power law decay of the stress as a function of time,
down to a p... | cond-mat.soft | we measure the dynamical mechanical properties of human red blood cells single cell response is measured with optical tweezers we investigate both the stress relaxation following a fast deformation and the effect of varying the strain rate we find a power law decay of the stress as a function of time down to a plateau ... | [['we', 'measure', 'the', 'dynamical', 'mechanical', 'properties', 'of', 'human', 'red', 'blood', 'cells', 'single', 'cell', 'response', 'is', 'measured', 'with', 'optical', 'tweezers', 'we', 'investigate', 'both', 'the', 'stress', 'relaxation', 'following', 'a', 'fast', 'deformation', 'and', 'the', 'effect', 'of', 'va... | [-0.12761385797670013, 0.18021344100308948, -0.10947659005729579, -0.0019478808419415529, -0.026856891149164813, -0.08804278734130908, 0.07939188573417548, 0.3444117085937729, -0.29107058344801007, -0.23245093579029535, 0.054587801888517695, -0.26440275487440984, -0.23375112390127278, 0.162017164572669, -0.068897327797... |
710.3334 | Speculations on Isolated Lepton Events at HERA | Speculations on mechanisms which might be responsible for events with an
isolated high p_T lepton, a hadron jet and missing energy, as observed in the
H1 experiment at HERA, are discussed.
| hep-ph | speculations on mechanisms which might be responsible for events with an isolated high p_t lepton a hadron jet and missing energy as observed in the h1 experiment at hera are discussed | [['speculations', 'on', 'mechanisms', 'which', 'might', 'be', 'responsible', 'for', 'events', 'with', 'an', 'isolated', 'high', 'p_t', 'lepton', 'a', 'hadron', 'jet', 'and', 'missing', 'energy', 'as', 'observed', 'in', 'the', 'h1', 'experiment', 'at', 'hera', 'are', 'discussed']] | [-0.06464971277502275, 0.2545600270203713, -0.10796487379458643, 0.24270170109887276, -0.024049709671207013, -0.12542809826517176, -0.07758401283213208, 0.3742552029509698, -0.153515309335724, -0.32570352531488866, 0.04970919738538684, -0.3394031360925686, 0.061011873065463955, 0.17902382616434367, 0.08564801048487425,... |
710.3335 | Non-linear numerical simulations of magneto-acoustic wave propagation in
small-scale flux tubes | We present results of non-linear, 2D, numerical simulations of
magneto-acoustic wave propagation in the photosphere and chromosphere of
small-scale flux tubes with internal structure. Waves with realistic periods of
three to five minutes are studied, after applying horizontal and vertical
oscillatory perturbations to... | astro-ph | we present results of nonlinear 2d numerical simulations of magnetoacoustic wave propagation in the photosphere and chromosphere of smallscale flux tubes with internal structure waves with realistic periods of three to five minutes are studied after applying horizontal and vertical oscillatory perturbations to the equi... | [['we', 'present', 'results', 'of', 'nonlinear', '2d', 'numerical', 'simulations', 'of', 'magnetoacoustic', 'wave', 'propagation', 'in', 'the', 'photosphere', 'and', 'chromosphere', 'of', 'smallscale', 'flux', 'tubes', 'with', 'internal', 'structure', 'waves', 'with', 'realistic', 'periods', 'of', 'three', 'to', 'five'... | [-0.16534295522641124, 0.21855435658653732, -0.03350733188978795, 0.07439560720428874, -0.08638462970079022, -0.07346911638991774, 0.0360484653855175, 0.3863866816183353, -0.27699223673179013, -0.30067914615418495, 0.11005852782026133, -0.23872596983151848, -0.08421982029696144, 0.22447127378109144, 0.02731664406331089... |
710.3336 | Potts Glass on Random Graphs | We solve the q-state Potts model with anti-ferromagnetic interactions on
large random lattices of finite coordination. Due to the frustration induced by
the large loops and to the local tree-like structure of the lattice this model
behaves as a mean field spin glass. We use the cavity method to compute the
temperatur... | cond-mat.dis-nn cond-mat.stat-mech | we solve the qstate potts model with antiferromagnetic interactions on large random lattices of finite coordination due to the frustration induced by the large loops and to the local treelike structure of the lattice this model behaves as a mean field spin glass we use the cavity method to compute the temperaturecoordi... | [['we', 'solve', 'the', 'qstate', 'potts', 'model', 'with', 'antiferromagnetic', 'interactions', 'on', 'large', 'random', 'lattices', 'of', 'finite', 'coordination', 'due', 'to', 'the', 'frustration', 'induced', 'by', 'the', 'large', 'loops', 'and', 'to', 'the', 'local', 'treelike', 'structure', 'of', 'the', 'lattice',... | [-0.15120294096414, 0.17856082766558284, -0.06802049442927388, 0.07344331125280372, -0.06548864539298746, -0.1311247184941614, 0.08039113964230098, 0.39243099518396235, -0.2565476043770711, -0.24782448645591676, 0.09594010831184548, -0.2795032873956694, -0.1749462789364366, 0.05091688967033945, 0.022139899082806853, 0.... |
710.3337 | Structure and properties of the vacuum of the Twisted Eguchi-Kawai model | We investigate numerically the phase structure of the Twisted Eguchi-Kawai
(TEK) model in four dimensions. In the numerical simulations of the zero
temperature TEK model (using a symmetric twist) we observe the existence of new
phases that break its centre symmetry at intermediate lattice couplings and for
large SU(N... | hep-lat hep-th | we investigate numerically the phase structure of the twisted eguchikawai tek model in four dimensions in the numerical simulations of the zero temperature tek model using a symmetric twist we observe the existence of new phases that break its centre symmetry at intermediate lattice couplings and for large sun gauge gr... | [['we', 'investigate', 'numerically', 'the', 'phase', 'structure', 'of', 'the', 'twisted', 'eguchikawai', 'tek', 'model', 'in', 'four', 'dimensions', 'in', 'the', 'numerical', 'simulations', 'of', 'the', 'zero', 'temperature', 'tek', 'model', 'using', 'a', 'symmetric', 'twist', 'we', 'observe', 'the', 'existence', 'of'... | [-0.1642469150318327, 0.22138324447869495, -0.055726303098448886, 0.07281772719520353, -0.018275496374093453, -0.11217222145606516, 0.02819978051619338, 0.35857562863324977, -0.23841899024959348, -0.2545828999837442, 0.07937071705355822, -0.24478953280628715, -0.1402919242937802, 0.09969990824263696, 0.0516340247985291... |
710.3338 | Search for Randall-Sundrum gravitons with 1 fb-1 of data from ppbar
collisions at sqrt(s)=1.96 TeV | Using 1 fb-1 of data from ppbar collisions at sqrt(s)=1.96 TeV at the
Fermilab Tevatron collider collected by the D0 detector, we search for decays
of Kaluza-Klein excitations of the graviton in the Randall-Sundrum model of
extra dimensions to e+e- and diphotons. We set 95% confidence level upper
limits on the produc... | hep-ex | using 1 fb1 of data from ppbar collisions at sqrts196 tev at the fermilab tevatron collider collected by the d0 detector we search for decays of kaluzaklein excitations of the graviton in the randallsundrum model of extra dimensions to ee and diphotons we set 95 confidence level upper limits on the production cross sec... | [['using', '1', 'fb1', 'of', 'data', 'from', 'ppbar', 'collisions', 'at', 'sqrts196', 'tev', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'collected', 'by', 'the', 'd0', 'detector', 'we', 'search', 'for', 'decays', 'of', 'kaluzaklein', 'excitations', 'of', 'the', 'graviton', 'in', 'the', 'randallsundrum', 'model', ... | [-0.0427276778535592, 0.23371288115270886, -0.03018784585846476, 0.14475099335660238, -0.013039708945406488, -0.1120677813663181, 0.09287750749380316, 0.27909091496784016, -0.1330912221357765, -0.36340744994266566, -0.008868434018994042, -0.4322092034797891, 0.18015076825956264, 0.17653307445201438, 0.15638915412352386... |
710.3339 | Investigation of the bottomonium ground state \eta_b via its inclusive
charm decays | Based on the non-relativistic QCD factorization formalism, we calculate the
bottomonium ground state, $\eta_b$, inclusive charm decays at the leading order
in the strong coupling constant $\alpha_s$ and quarkonium internal relative
velocity $v$. The inclusive charm pair production in $\eta_b$ decay is mainly
realized... | hep-ph hep-ex | based on the nonrelativistic qcd factorization formalism we calculate the bottomonium ground state eta_b inclusive charm decays at the leading order in the strong coupling constant alpha_s and quarkonium internal relative velocity v the inclusive charm pair production in eta_b decay is mainly realized through eta_b to ... | [['based', 'on', 'the', 'nonrelativistic', 'qcd', 'factorization', 'formalism', 'we', 'calculate', 'the', 'bottomonium', 'ground', 'state', 'eta_b', 'inclusive', 'charm', 'decays', 'at', 'the', 'leading', 'order', 'in', 'the', 'strong', 'coupling', 'constant', 'alpha_s', 'and', 'quarkonium', 'internal', 'relative', 've... | [-0.05660112616667328, 0.3054165687297651, -0.13564435507399603, 0.1602984119739503, -0.03999487305950504, -0.11769313640124573, 0.08112687325889342, 0.2942054849281384, -0.2236341100243296, -0.1631690723772504, -0.07181160583103631, -0.3579825881476465, 0.08473015047830383, 0.07002805481999785, 0.10033827864058446, 0.... |
710.334 | Distances to Galactic high-velocity clouds. Complex C | We report the first determination of a distance bracket for the high-velocity
cloud (HVC) complex C. Combined with previous measurements showing that this
cloud has a metallicity of 0.15 times solar, these results provide ample
evidence that complex C traces the continuing accretion of intergalactic gas
falling onto ... | astro-ph | we report the first determination of a distance bracket for the highvelocity cloud hvc complex c combined with previous measurements showing that this cloud has a metallicity of 015 times solar these results provide ample evidence that complex c traces the continuing accretion of intergalactic gas falling onto the milk... | [['we', 'report', 'the', 'first', 'determination', 'of', 'a', 'distance', 'bracket', 'for', 'the', 'highvelocity', 'cloud', 'hvc', 'complex', 'c', 'combined', 'with', 'previous', 'measurements', 'showing', 'that', 'this', 'cloud', 'has', 'a', 'metallicity', 'of', '015', 'times', 'solar', 'these', 'results', 'provide', ... | [-0.14080128690455945, 0.06512757180398013, -0.026886604301834188, 0.04113038309586874, -0.09169375203980677, -0.059130031536301586, 0.10128994285110005, 0.4079579455131779, -0.18274284615838698, -0.30611373938708786, 0.015369473305549853, -0.27862789510388153, -0.013021247268204583, 0.19017413804358263, -0.02958716076... |
710.3341 | Discrete, 3D distributed, linear imaging methods of electric neuronal
activity. Part 1: exact, zero error localization | This paper deals with the EEG/MEG neuroimaging problem: given measurements of
scalp electric potential differences (EEG: electroencephalogram) and
extracranial magnetic fields (MEG: magnetoencephalogram), find the 3D
distribution of the generating electric neuronal activity. This problem has no
unique solution. Only ... | math-ph math.MP physics.bio-ph q-bio.NC | this paper deals with the eegmeg neuroimaging problem given measurements of scalp electric potential differences eeg electroencephalogram and extracranial magnetic fields meg magnetoencephalogram find the 3d distribution of the generating electric neuronal activity this problem has no unique solution only particular so... | [['this', 'paper', 'deals', 'with', 'the', 'eegmeg', 'neuroimaging', 'problem', 'given', 'measurements', 'of', 'scalp', 'electric', 'potential', 'differences', 'eeg', 'electroencephalogram', 'and', 'extracranial', 'magnetic', 'fields', 'meg', 'magnetoencephalogram', 'find', 'the', '3d', 'distribution', 'of', 'the', 'ge... | [-0.0987364108518579, 0.05534901129318535, -0.036432026313020956, 0.07403440408997794, -0.06593350662710917, -0.16193938522615073, -0.037692726980791895, 0.378257945776809, -0.25828957073107484, -0.28516861553000317, 0.10589070355253376, -0.2906190192543011, -0.2255298444764555, 0.18128721500638853, -0.0998788556516252... |
710.3342 | The Conjugate Linearized Ricci Flow on Closed 3-Manifolds | We characterize the conjugate linearized Ricci flow and the associated
backward heat kernel on closed three--manifolds of bounded geometry. We discuss
their properties, and introduce the notion of Ricci flow conjugated constraint
sets which characterizes a way of Ricci flow averaging metric dependent
geometrical data... | math.DG math-ph math.MP | we characterize the conjugate linearized ricci flow and the associated backward heat kernel on closed threemanifolds of bounded geometry we discuss their properties and introduce the notion of ricci flow conjugated constraint sets which characterizes a way of ricci flow averaging metric dependent geometrical data we al... | [['we', 'characterize', 'the', 'conjugate', 'linearized', 'ricci', 'flow', 'and', 'the', 'associated', 'backward', 'heat', 'kernel', 'on', 'closed', 'threemanifolds', 'of', 'bounded', 'geometry', 'we', 'discuss', 'their', 'properties', 'and', 'introduce', 'the', 'notion', 'of', 'ricci', 'flow', 'conjugated', 'constrain... | [-0.20744613574987109, 0.0753920667987338, -0.1453457929363305, 0.0702585805809558, -0.18588923674189683, -0.14770422396579325, -0.0928728677887432, 0.3259469815576919, -0.34292265012709783, -0.1713843719817397, 0.14399280877327642, -0.2916920754512904, -0.13016981801789518, 0.16131423304628845, -0.08348139005667893, 0... |
710.3343 | Entanglement in the F-AF zig-zag Heisenberg chain | We present a study of the entanglement properties of the F-AF zig-zag
Heisenberg chain done by means of the Density Matrix Renormalization Group
method. In particular, we have selected the concurrence as measure of
entanglement and checked its capability to signal the presence of quantum phase
transitions within the ... | cond-mat.str-el cond-mat.soft | we present a study of the entanglement properties of the faf zigzag heisenberg chain done by means of the density matrix renormalization group method in particular we have selected the concurrence as measure of entanglement and checked its capability to signal the presence of quantum phase transitions within the previo... | [['we', 'present', 'a', 'study', 'of', 'the', 'entanglement', 'properties', 'of', 'the', 'faf', 'zigzag', 'heisenberg', 'chain', 'done', 'by', 'means', 'of', 'the', 'density', 'matrix', 'renormalization', 'group', 'method', 'in', 'particular', 'we', 'have', 'selected', 'the', 'concurrence', 'as', 'measure', 'of', 'enta... | [-0.16487668722519658, 0.13028100724782674, -0.08630269341501257, -0.0016234910431047601, 0.003241469370550476, -0.10355600650842872, 0.11294444525734551, 0.35324732450798396, -0.22016910545907223, -0.29206614163253575, 0.05764239562878145, -0.24981473622498132, -0.1465828273325197, 0.13856475625840586, 0.0072719469652... |
710.3344 | Description of Derivations on Measurable Operator Algebras of Type I | Given a type I von Neumann algebra $M$ with a faithful normal semi-finite
trace $\tau,$ let $L(M, \tau)$ be the algebra of all $\tau$-measurable
operators affiliated with $M.$ We give a complete description of all
derivations on the algebra $L(M, \tau).$ In particular, we prove that if $M$ is
of type I$_\infty$ then ... | math.OA math.FA | given a type i von neumann algebra m with a faithful normal semifinite trace tau let lm tau be the algebra of all taumeasurable operators affiliated with m we give a complete description of all derivations on the algebra lm tau in particular we prove that if m is of type i_infty then every derivation on lm tau is inner | [['given', 'a', 'type', 'i', 'von', 'neumann', 'algebra', 'm', 'with', 'a', 'faithful', 'normal', 'semifinite', 'trace', 'tau', 'let', 'lm', 'tau', 'be', 'the', 'algebra', 'of', 'all', 'taumeasurable', 'operators', 'affiliated', 'with', 'm', 'we', 'give', 'a', 'complete', 'description', 'of', 'all', 'derivations', 'on'... | [-0.14247671348663668, 0.13375193063014498, -0.06233718888834119, 0.01028199028611804, -0.13954366104444488, -0.20638347351923586, -0.04382819705060683, 0.3117318209842779, -0.2892074210025991, -0.1375044891455521, 0.1213651174271945, -0.2728011930982272, -0.06648004984793564, 0.18631825214639927, -0.10460609733127058,... |
710.3345 | The final spin from the coalescence of aligned-spin black-hole binaries | Determining the final spin of a black-hole (BH) binary is a question of key
importance in astrophysics. Modelling this quantity in general is made
difficult by the fact that it depends on the 7-dimensional space of parameters
characterizing the two initial black holes. However, in special cases, when
symmetries can b... | gr-qc astro-ph | determining the final spin of a blackhole bh binary is a question of key importance in astrophysics modelling this quantity in general is made difficult by the fact that it depends on the 7dimensional space of parameters characterizing the two initial black holes however in special cases when symmetries can be exploite... | [['determining', 'the', 'final', 'spin', 'of', 'a', 'blackhole', 'bh', 'binary', 'is', 'a', 'question', 'of', 'key', 'importance', 'in', 'astrophysics', 'modelling', 'this', 'quantity', 'in', 'general', 'is', 'made', 'difficult', 'by', 'the', 'fact', 'that', 'it', 'depends', 'on', 'the', '7dimensional', 'space', 'of', ... | [-0.11092230400670534, 0.13613745553790907, -0.061699244869837105, 0.12049606304879909, -0.09636183967478036, -0.1121380329288793, 0.0066216322190414826, 0.33315794350794303, -0.1835203709337153, -0.32437075686175376, 0.08313843332367608, -0.2599349804054677, -0.06344803838762275, 0.24012959882608043, -0.03098310531752... |
710.3346 | Associated charged Higgs and W boson production in the MSSM at the LHC | We investigate the associated production of charged Higgs bosons (H^\pm) and
W bosons at the CERN Large Hadron Collider, using the leptonic decay H^+ ->
tau^+ nu_tau and hadronic W decay, within different scenarios of the Minimal
Supersymmetric Standard Model (MSSM) with both real and complex parameters.
Performing a... | hep-ph | we investigate the associated production of charged higgs bosons hpm and w bosons at the cern large hadron collider using the leptonic decay h tau nu_tau and hadronic w decay within different scenarios of the minimal supersymmetric standard model mssm with both real and complex parameters performing a parton level stud... | [['we', 'investigate', 'the', 'associated', 'production', 'of', 'charged', 'higgs', 'bosons', 'hpm', 'and', 'w', 'bosons', 'at', 'the', 'cern', 'large', 'hadron', 'collider', 'using', 'the', 'leptonic', 'decay', 'h', 'tau', 'nu_tau', 'and', 'hadronic', 'w', 'decay', 'within', 'different', 'scenarios', 'of', 'the', 'min... | [-0.05210041000197331, 0.3159552627320712, 0.0009433781534122925, 0.15570417679846288, -0.03129369546853316, -0.2270722688602594, 0.04212170419438432, 0.31701388365666694, -0.2372024988833194, -0.2741091631818563, 0.0065284455039848885, -0.28763228240422906, 0.024581933739439895, 0.14068636962911113, 0.0959370479278732... |
710.3347 | The compact group--fossil group connection: observations of a massive
compact group at z=0.22 | It has been suggested that fossil groups could be the cannibalized remains of
compact groups, that lost energy through tidal friction. However, in the nearby
universe, compact groups which are close to the merging phase and display a
wealth of interacting features (such as HCG 31 and HCG 79) have very low
velocity di... | astro-ph | it has been suggested that fossil groups could be the cannibalized remains of compact groups that lost energy through tidal friction however in the nearby universe compact groups which are close to the merging phase and display a wealth of interacting features such as hcg 31 and hcg 79 have very low velocity dispersion... | [['it', 'has', 'been', 'suggested', 'that', 'fossil', 'groups', 'could', 'be', 'the', 'cannibalized', 'remains', 'of', 'compact', 'groups', 'that', 'lost', 'energy', 'through', 'tidal', 'friction', 'however', 'in', 'the', 'nearby', 'universe', 'compact', 'groups', 'which', 'are', 'close', 'to', 'the', 'merging', 'phase... | [-0.13292134667814418, 0.13223274405594374, -0.11083411233754016, 0.07910903699035522, -0.09556800401605468, -0.03495230026274411, 0.02280038866237019, 0.44326165613681406, -0.14989901108095177, -0.3434149578197281, 0.10979679416063025, -0.2769407079460731, -0.07416049929311097, 0.21558950293915846, -0.0441324050812741... |
710.3348 | Heavy Flavour Production in Deep--Inelastic Scattering - Two--Loop
Massive Operator Matrix Elements and Beyond | We calculate the O($\eps$)--term of the two--loop massive operator matrix
elements for twist 2--operators, which contribute to the heavy flavour Wilson
coefficients in unpolarized deep--inelastic scattering in the asymptotic limit
$Q^2 \gg m^2.$ Our calculation was performed in Mellin space using
Mellin--Barnes integ... | hep-ph | we calculate the oepsterm of the twoloop massive operator matrix elements for twist 2operators which contribute to the heavy flavour wilson coefficients in unpolarized deepinelastic scattering in the asymptotic limit q2 gg m2 our calculation was performed in mellin space using mellinbarnes integrals and generalized hyp... | [['we', 'calculate', 'the', 'oepsterm', 'of', 'the', 'twoloop', 'massive', 'operator', 'matrix', 'elements', 'for', 'twist', '2operators', 'which', 'contribute', 'to', 'the', 'heavy', 'flavour', 'wilson', 'coefficients', 'in', 'unpolarized', 'deepinelastic', 'scattering', 'in', 'the', 'asymptotic', 'limit', 'q2', 'gg',... | [-0.10426381680639987, 0.20736698284393773, -0.08200853368056552, 0.14352535894843485, -0.025119352312582843, -0.01399198090130428, 0.030799047230690154, 0.3085564419205459, -0.15252612812339134, -0.15055223584245397, -0.0021763015362732817, -0.36203502413799177, -0.09626494455239121, 0.12729592881393884, 0.07078120901... |
710.3349 | Determining Reheating Temperature at Colliders with Axino or Gravitino
Dark Matter | After a period of inflationary expansion, the
Universe reheated and reached full thermal equilibrium at the reheating
temperature T_R. In this work we point out that, in the context of effective
low-energy supersymmetric models, LHC measurements may allow one to determine
T_R as a function of the mass of the dark m... | hep-ph astro-ph | after a period of inflationary expansion the universe reheated and reached full thermal equilibrium at the reheating temperature t_r in this work we point out that in the context of effective lowenergy supersymmetric models lhc measurements may allow one to determine t_r as a function of the mass of the dark matter par... | [['after', 'a', 'period', 'of', 'inflationary', 'expansion', 'the', 'universe', 'reheated', 'and', 'reached', 'full', 'thermal', 'equilibrium', 'at', 'the', 'reheating', 'temperature', 't_r', 'in', 'this', 'work', 'we', 'point', 'out', 'that', 'in', 'the', 'context', 'of', 'effective', 'lowenergy', 'supersymmetric', 'm... | [-0.08796905629828365, 0.25457859403144945, -0.16975396248098049, 0.11820516693114769, -0.06248457725935926, -0.13147090220849755, 0.05660386083440648, 0.30192319186042166, -0.2343944178816552, -0.31429308495070374, 0.1152755331972407, -0.22463404159579012, 0.03147512854452038, 0.16827124653597517, 0.0184857851644564, ... |
710.335 | Fully Correlated Electronic Dynamics for Antiproton Impact Ionization of
Helium | We present total cross sections for single and double ionization of helium by
antiproton impact over a wide range of impact energies from 10 keV/amu to 1
MeV/amu. A non-perturbative time-dependent close-coupling method (TDCC) is
applied to fully treat the correlated dynamics of the ionized electrons.
Excellent agreem... | physics.atom-ph | we present total cross sections for single and double ionization of helium by antiproton impact over a wide range of impact energies from 10 kevamu to 1 mevamu a nonperturbative timedependent closecoupling method tdcc is applied to fully treat the correlated dynamics of the ionized electrons excellent agreement is obta... | [['we', 'present', 'total', 'cross', 'sections', 'for', 'single', 'and', 'double', 'ionization', 'of', 'helium', 'by', 'antiproton', 'impact', 'over', 'a', 'wide', 'range', 'of', 'impact', 'energies', 'from', '10', 'kevamu', 'to', '1', 'mevamu', 'a', 'nonperturbative', 'timedependent', 'closecoupling', 'method', 'tdcc'... | [-0.035819136269122094, 0.1511652040860861, -0.03549305828359515, 0.11906356647975642, 0.04459127432720207, -0.09393226912167545, 0.05730468491176227, 0.3788977706351796, -0.17359992681775946, -0.390392302812354, -0.06225112019324893, -0.33453514667748063, 0.0221693018107331, 0.2421043879239241, 0.07338151862364481, 0.... |
710.3351 | The Rich Mid-Infrared Environments of Two Highly-Obscured X-ray
Binaries: Spitzer Observations of IGR J16318-4848 and GX 301-2 | We present the results of Spitzer mid-infrared spectroscopic observations of
two highly-obscured massive X-ray binaries: IGR J16318-4848 and GX301-2. Our
observations reveal for the first time the extremely rich mid-infrared
environments of this type of source, including multiple continuum emission
components (a hot ... | astro-ph | we present the results of spitzer midinfrared spectroscopic observations of two highlyobscured massive xray binaries igr j163184848 and gx3012 our observations reveal for the first time the extremely rich midinfrared environments of this type of source including multiple continuum emission components a hot component wi... | [['we', 'present', 'the', 'results', 'of', 'spitzer', 'midinfrared', 'spectroscopic', 'observations', 'of', 'two', 'highlyobscured', 'massive', 'xray', 'binaries', 'igr', 'j163184848', 'and', 'gx3012', 'our', 'observations', 'reveal', 'for', 'the', 'first', 'time', 'the', 'extremely', 'rich', 'midinfrared', 'environmen... | [-0.052938000647057046, 0.13426442233865504, -0.04472894230367322, 0.07507574430691373, -0.094209949374444, -0.10380626824243289, 0.062351170220216245, 0.49315641931209125, -0.16181733463461953, -0.30528479207775827, 0.03988929797258032, -0.3323812589441475, -0.036386931873857976, 0.15682652179612455, -0.00973145373067... |
710.3352 | Applications of Level Curves to Some Problems on Algebraic Surfaces | In a previous work of the authors, a result to algorithmically compute the
topology types of the level curves of an algebraic surface, is given. From this
result, here we derive applications based on level curves to determine some
topological features of surfaces (reality, compactness, connectivity) and to
the proble... | math.AG | in a previous work of the authors a result to algorithmically compute the topology types of the level curves of an algebraic surface is given from this result here we derive applications based on level curves to determine some topological features of surfaces reality compactness connectivity and to the problem of plott... | [['in', 'a', 'previous', 'work', 'of', 'the', 'authors', 'a', 'result', 'to', 'algorithmically', 'compute', 'the', 'topology', 'types', 'of', 'the', 'level', 'curves', 'of', 'an', 'algebraic', 'surface', 'is', 'given', 'from', 'this', 'result', 'here', 'we', 'derive', 'applications', 'based', 'on', 'level', 'curves', '... | [-0.13540793693839356, 0.03547701333865497, -0.1562607895511274, 0.07748829104149571, -0.09311306841958028, -0.05959740859599641, 0.10451021702745213, 0.3317008964144267, -0.29080096523438653, -0.32672564667434645, 0.08739198898099577, -0.2512433359112877, -0.20548536743109042, 0.2441303967184817, -0.15509077318263456,... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.