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 |
|---|---|---|---|---|---|---|
710.3953 | Strategy for early SUSY searches at ATLAS | The CERN Large Hadron Collider (LHC) is scheduled to commence operation in
2008 and inclusive searches for supersymmetry (SUSY) will be one of our primary
tasks in the first days of LHC operation. It is certain that the final state of
multijets + missing transverse energy will provide a superior performance in
SUSY s... | hep-ex | the cern large hadron collider lhc is scheduled to commence operation in 2008 and inclusive searches for supersymmetry susy will be one of our primary tasks in the first days of lhc operation it is certain that the final state of multijets missing transverse energy will provide a superior performance in susy searches s... | [['the', 'cern', 'large', 'hadron', 'collider', 'lhc', 'is', 'scheduled', 'to', 'commence', 'operation', 'in', '2008', 'and', 'inclusive', 'searches', 'for', 'supersymmetry', 'susy', 'will', 'be', 'one', 'of', 'our', 'primary', 'tasks', 'in', 'the', 'first', 'days', 'of', 'lhc', 'operation', 'it', 'is', 'certain', 'tha... | [-0.03812727331312309, 0.16465819574070087, -0.10880763702704732, 0.14595841175017493, -0.0970323470271602, -0.15439403511921007, -0.022748020533793444, 0.3552350218022435, -0.19148415569035368, -0.33789281135852495, 0.12415544927955188, -0.30786228485822936, 0.004185338506619607, 0.19463565773611632, -0.02334422579613... |
710.3954 | Seiberg-Witten map for the 4D noncommutative BF theory | We describe the Seiberg-Witten map for the 4D noncommutative BF theory
(NCBF). We establish the existence of a map taking the abelian NCBF into its
commutative version, in agreement with the hypothesis that such maps are
available for any noncommutative theory with Schwarz type topological sectors.
| hep-th | we describe the seibergwitten map for the 4d noncommutative bf theory ncbf we establish the existence of a map taking the abelian ncbf into its commutative version in agreement with the hypothesis that such maps are available for any noncommutative theory with schwarz type topological sectors | [['we', 'describe', 'the', 'seibergwitten', 'map', 'for', 'the', '4d', 'noncommutative', 'bf', 'theory', 'ncbf', 'we', 'establish', 'the', 'existence', 'of', 'a', 'map', 'taking', 'the', 'abelian', 'ncbf', 'into', 'its', 'commutative', 'version', 'in', 'agreement', 'with', 'the', 'hypothesis', 'that', 'such', 'maps', '... | [-0.1317146166270091, 0.06048595871437679, -0.1038369029675695, 0.12022807931696827, -0.0367915672250092, -0.15453057759441435, -0.03123157319549302, 0.3014483878981661, -0.29819784783334896, -0.2072108210572465, 0.10488742007609372, -0.26304968425326725, -0.16805223587223075, 0.16259449508718468, -0.11396113597914916,... |
710.3955 | On the Behavior of the Distributed Coordination Function of IEEE 802.11
with Multirate Capability under General Transmission Conditions | The aim of this paper is threefold. First, it presents a multi-dimensional
Markovian state transition model characterizing the behavior of the IEEE 802.11
protocol at the Medium Access Control layer which accounts for packet
transmission failures due to channel errors modeling both saturated and
non-saturated traffic... | cs.NI cs.PF | the aim of this paper is threefold first it presents a multidimensional markovian state transition model characterizing the behavior of the ieee 80211 protocol at the medium access control layer which accounts for packet transmission failures due to channel errors modeling both saturated and nonsaturated traffic condit... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'threefold', 'first', 'it', 'presents', 'a', 'multidimensional', 'markovian', 'state', 'transition', 'model', 'characterizing', 'the', 'behavior', 'of', 'the', 'ieee', '80211', 'protocol', 'at', 'the', 'medium', 'access', 'control', 'layer', 'which', 'accounts', 'for', 'pack... | [-0.24831513712591627, 0.015903765038513627, -0.06575536731342206, 0.00814632406782996, -0.009429709439006584, -0.19759104550681322, 0.12063043908366174, 0.3444523280118837, -0.25250315557135955, -0.259037376589779, 0.10033137757272925, -0.23879468899011905, -0.1482770876088915, 0.16422381550288073, -0.0742200677371951... |
710.3956 | The solution of a memorable problem by a special artifice of calculation | E731 in the Enestrom index. Originally published as "Solutio problematis ob
singularia calculi artificia memorabilis", Memoires de l'academie des sciences
de St-Petersbourg 2 (1810), 3-9.
For $z$ the distance from the origin, and $v$ a given function of $z$, Euler
wants to find a curve $s$ such that the integral of... | math.HO math.CA | e731 in the enestrom index originally published as solutio problematis ob singularia calculi artificia memorabilis memoires de lacademie des sciences de stpetersbourg 2 1810 39 for z the distance from the origin and v a given function of z euler wants to find a curve s such that the integral of z over s is a maximum or... | [['e731', 'in', 'the', 'enestrom', 'index', 'originally', 'published', 'as', 'solutio', 'problematis', 'ob', 'singularia', 'calculi', 'artificia', 'memorabilis', 'memoires', 'de', 'lacademie', 'des', 'sciences', 'de', 'stpetersbourg', '2', '1810', '39', 'for', 'z', 'the', 'distance', 'from', 'the', 'origin', 'and', 'v'... | [-0.14284259202363697, 0.05738284813149063, -0.1354452293548409, 0.04645805233799299, -0.11570391616365616, -0.14848426218563016, 0.04035443979301962, 0.27154310392064, -0.24867134878708833, -0.3215859500772279, 0.04653799353484604, -0.31779200775022415, -0.07650697276171675, 0.17205162395966117, -0.08704623572555358, ... |
710.3957 | Non-archimedean equidistribution on elliptic curves with global
applications | Let $E$ be an elliptic curve over an algebraically closed, complete,
non-archimedean field $K$, and let ${\mathsf E}$ denote the Berkovich analytic
space associated to $E/K$. We study the $\mu$-equidistribution of finite
subsets of $E(K)$, where $\mu$ is a certain canonical unit Borel measure on
${\mathsf E}$. Our ma... | math.NT math.AG | let e be an elliptic curve over an algebraically closed complete nonarchimedean field k and let mathsf e denote the berkovich analytic space associated to ek we study the muequidistribution of finite subsets of ek where mu is a certain canonical unit borel measure on mathsf e our main result is an inequality bounding t... | [['let', 'e', 'be', 'an', 'elliptic', 'curve', 'over', 'an', 'algebraically', 'closed', 'complete', 'nonarchimedean', 'field', 'k', 'and', 'let', 'mathsf', 'e', 'denote', 'the', 'berkovich', 'analytic', 'space', 'associated', 'to', 'ek', 'we', 'study', 'the', 'muequidistribution', 'of', 'finite', 'subsets', 'of', 'ek',... | [-0.23519392288684593, 0.0601434463518425, -0.12602897916162797, 0.0674756427603316, -0.0761060206164306, -0.10208125367871154, 0.026624216118006635, 0.28482388173845613, -0.3049869555072322, -0.19699901406321738, 0.03838967691053305, -0.28354893419575894, -0.09872194807739708, 0.30055083378644315, -0.15110920368835834... |
710.3958 | The problem of gauge invariance and the functional Schroedinger approach | Quantum field theory is assumed to be gauge invariant. However it is well
known that when certain quantities, such as the vacuum current, are calculated
the results are not gauge invariant. The non-gauge invariant terms have to be
removed in order to obtain a physically correct result. It has been shown in
Ref. [3] a... | quant-ph | quantum field theory is assumed to be gauge invariant however it is well known that when certain quantities such as the vacuum current are calculated the results are not gauge invariant the nongauge invariant terms have to be removed in order to obtain a physically correct result it has been shown in ref 3 and 4 that t... | [['quantum', 'field', 'theory', 'is', 'assumed', 'to', 'be', 'gauge', 'invariant', 'however', 'it', 'is', 'well', 'known', 'that', 'when', 'certain', 'quantities', 'such', 'as', 'the', 'vacuum', 'current', 'are', 'calculated', 'the', 'results', 'are', 'not', 'gauge', 'invariant', 'the', 'nongauge', 'invariant', 'terms'... | [-0.06435677021213379, 0.145989824357255, -0.14726049752558568, 0.10565168301053789, -0.07881135020464186, -0.11586490708831994, -0.06982849816891498, 0.36475488389029154, -0.24298020866551687, -0.2968937198941906, 0.0801257400326283, -0.21711675161569718, -0.22897424219390525, 0.15539218545410902, -0.11281561074290603... |
710.3959 | The t copula with Multiple Parameters of Degrees of Freedom: Bivariate
Characteristics and Application to Risk Management | The t copula is often used in risk management as it allows for modelling tail
dependence between risks and it is simple to simulate and calibrate. However,
the use of a standard t copula is often criticized due to its restriction of
having a single parameter for the degrees of freedom (dof) that may limit its
capabil... | math.PR q-fin.CP q-fin.RM | the t copula is often used in risk management as it allows for modelling tail dependence between risks and it is simple to simulate and calibrate however the use of a standard t copula is often criticized due to its restriction of having a single parameter for the degrees of freedom dof that may limit its capability to... | [['the', 't', 'copula', 'is', 'often', 'used', 'in', 'risk', 'management', 'as', 'it', 'allows', 'for', 'modelling', 'tail', 'dependence', 'between', 'risks', 'and', 'it', 'is', 'simple', 'to', 'simulate', 'and', 'calibrate', 'however', 'the', 'use', 'of', 'a', 'standard', 't', 'copula', 'is', 'often', 'criticized', 'd... | [-0.04694196125444937, 0.05268193961938425, -0.1345927242869131, 0.11656606919666733, -0.1019759936524289, -0.1554853740903758, 0.07311978133345422, 0.401297694452259, -0.26563499508691685, -0.27697261232806714, 0.0974657347940184, -0.26238034008083, -0.0998204502749865, 0.12523632806521479, -0.11753581990060226, 0.067... |
710.396 | A Kruskal-Katona Type Theorem for Graphs | A bound on consecutive clique numbers of graphs is established. This bound is
evaluated and shown to often be much better than the bound of the
Kruskal-Katona theorem. A bound on non-consecutive clique numbers is also
proven.
| math.CO | a bound on consecutive clique numbers of graphs is established this bound is evaluated and shown to often be much better than the bound of the kruskalkatona theorem a bound on nonconsecutive clique numbers is also proven | [['a', 'bound', 'on', 'consecutive', 'clique', 'numbers', 'of', 'graphs', 'is', 'established', 'this', 'bound', 'is', 'evaluated', 'and', 'shown', 'to', 'often', 'be', 'much', 'better', 'than', 'the', 'bound', 'of', 'the', 'kruskalkatona', 'theorem', 'a', 'bound', 'on', 'nonconsecutive', 'clique', 'numbers', 'is', 'als... | [-0.1914266409774034, 0.1424078886976113, -0.14045984162068045, 0.16691276378854103, -0.06840946449822671, -0.16846325391953862, 0.11568906820203001, 0.27214784462105585, -0.21159400790929794, -0.3847345558775438, 0.11963828698404737, -0.25022426972518097, -0.1457702525501215, 0.24426156081057884, -0.10187892096016456,... |
710.3961 | On a New Type of Information Processing for Efficient Management of
Complex Systems | It is a challenge to manage complex systems efficiently without confronting
NP-hard problems. To address the situation we suggest to use self-organization
processes of prime integer relations for information processing.
Self-organization processes of prime integer relations define correlation
structures of a complex ... | cs.CC | it is a challenge to manage complex systems efficiently without confronting nphard problems to address the situation we suggest to use selforganization processes of prime integer relations for information processing selforganization processes of prime integer relations define correlation structures of a complex system ... | [['it', 'is', 'a', 'challenge', 'to', 'manage', 'complex', 'systems', 'efficiently', 'without', 'confronting', 'nphard', 'problems', 'to', 'address', 'the', 'situation', 'we', 'suggest', 'to', 'use', 'selforganization', 'processes', 'of', 'prime', 'integer', 'relations', 'for', 'information', 'processing', 'selforganiz... | [-0.18148138353643645, 0.060060106854378195, -0.10279598669503547, 0.08576113293077418, -0.09638918053387159, -0.1362942891776902, 0.06497522634052232, 0.3246971826934194, -0.3720047652064279, -0.33571907336147605, 0.1317686216071305, -0.22784247499214588, -0.19748820698474945, 0.20871190377392895, -0.06843564509258128... |
710.3962 | d+id'-wave Superconducting States in Graphene | We show that effective superconducting orders generally emerge at low energy
in the superconducting state of graphene with conventionally defined pairing
symmetry .
We study such a particular interesting example, the $d_{x^2-y^2}+id'_{xy}$
spin singlet pairing superconducting state in graphene, which can be generat... | cond-mat.mes-hall cond-mat.supr-con | we show that effective superconducting orders generally emerge at low energy in the superconducting state of graphene with conventionally defined pairing symmetry we study such a particular interesting example the d_x2y2id_xy spin singlet pairing superconducting state in graphene which can be generated by electronic co... | [['we', 'show', 'that', 'effective', 'superconducting', 'orders', 'generally', 'emerge', 'at', 'low', 'energy', 'in', 'the', 'superconducting', 'state', 'of', 'graphene', 'with', 'conventionally', 'defined', 'pairing', 'symmetry', 'we', 'study', 'such', 'a', 'particular', 'interesting', 'example', 'the', 'd_x2y2id_xy',... | [-0.22133647439707266, 0.2470317096853825, -0.07823823941381354, 0.09706909757499632, -0.05692069734887857, -0.18453816041644466, 0.07345337444842842, 0.3538861105512632, -0.2573099422366603, -0.30846208161429356, -0.05818574176856169, -0.32169325096826806, -0.13196988983177824, 0.1357522658023395, 0.08386997371225764,... |
710.3963 | Including nonlocality in exchange-correlation kernel from time-dependent
current density functional theory: Application to the stopping power of
electron liquids | We develop a scheme for building the scalar exchange-correlation (xc) kernel
of time-dependent density functional theory (TDDFT) from the tensorial kernel
of time-dependent {\em current} density functional theory (TDCDFT) and the
Kohn-Sham current density response function. Resorting to the local
approximation to the... | cond-mat.mtrl-sci | we develop a scheme for building the scalar exchangecorrelation xc kernel of timedependent density functional theory tddft from the tensorial kernel of timedependent em current density functional theory tdcdft and the kohnsham current density response function resorting to the local approximation to the kernel of tdcdf... | [['we', 'develop', 'a', 'scheme', 'for', 'building', 'the', 'scalar', 'exchangecorrelation', 'xc', 'kernel', 'of', 'timedependent', 'density', 'functional', 'theory', 'tddft', 'from', 'the', 'tensorial', 'kernel', 'of', 'timedependent', 'em', 'current', 'density', 'functional', 'theory', 'tdcdft', 'and', 'the', 'kohnsh... | [-0.03934994300602582, -0.0052447057566715905, -0.1556877493256189, 0.13469110824296188, 0.004464567462303515, -0.10402994148999228, 0.04911831288461991, 0.3422343850232147, -0.2413706515417916, -0.27865220803028806, -0.023460497364104757, -0.30904019489113627, -0.14440535644775834, 0.14014442833461638, 0.0242813369761... |
710.3964 | A note on a curious formula for Euler's constant | In this short note we will use the residue theorem to establish a formula for
Euler's constant. In particular, we offer a slightly generalized version of an
interesting infinite series due to Flajolet, Gourdon, and Dumas.
| math.NT | in this short note we will use the residue theorem to establish a formula for eulers constant in particular we offer a slightly generalized version of an interesting infinite series due to flajolet gourdon and dumas | [['in', 'this', 'short', 'note', 'we', 'will', 'use', 'the', 'residue', 'theorem', 'to', 'establish', 'a', 'formula', 'for', 'eulers', 'constant', 'in', 'particular', 'we', 'offer', 'a', 'slightly', 'generalized', 'version', 'of', 'an', 'interesting', 'infinite', 'series', 'due', 'to', 'flajolet', 'gourdon', 'and', 'du... | [-0.1516606703452352, 0.05000735073351987, -0.17791029805731443, 0.13994180290481179, -0.13207715842872858, -0.13031040833124685, 0.06900516850873828, 0.28374310882969034, -0.2841971448312203, -0.22813774578066337, 0.0822948393243779, -0.22502297714042166, -0.17567729432549742, 0.23842489222685495, -0.18421151434692243... |
710.3965 | Quasisymmetric functions and Kazhdan-Lusztig polynomials | We associate a quasisymmetric function to any Bruhat interval in a general
Coxeter group. This association can be seen to be a morphism of Hopf algebras
to the subalgebra of all peak functions, leading to an extension of the
cd-index of convex polytopes. We show how the Kazhdan-Lusztig polynomial of the
Bruhat interv... | math.CO math.RT | we associate a quasisymmetric function to any bruhat interval in a general coxeter group this association can be seen to be a morphism of hopf algebras to the subalgebra of all peak functions leading to an extension of the cdindex of convex polytopes we show how the kazhdanlusztig polynomial of the bruhat interval can ... | [['we', 'associate', 'a', 'quasisymmetric', 'function', 'to', 'any', 'bruhat', 'interval', 'in', 'a', 'general', 'coxeter', 'group', 'this', 'association', 'can', 'be', 'seen', 'to', 'be', 'a', 'morphism', 'of', 'hopf', 'algebras', 'to', 'the', 'subalgebra', 'of', 'all', 'peak', 'functions', 'leading', 'to', 'an', 'ext... | [-0.1712563540238668, 0.025760316964656606, -0.07775802944293793, 0.09397585322970853, -0.14523945561993648, -0.11249448621426435, 0.01903522653395639, 0.3437506185077569, -0.41172845979385514, -0.16156524587559568, 0.08082236699102556, -0.19055733150966903, -0.16055899410892058, 0.16751736428807765, -0.195057301319149... |
710.3966 | Overview of progress in neutrino scattering measurements | Recent progress in neutrino scattering experiments with few GeV neutrino
beams is reviewed, focusing on new experimental input since the beginning of
the NuInt workshop series in 2001. Progress in neutrino quasi-elastic
scattering, resonance production, coherent pion production, scattering in the
transition region be... | hep-ex | recent progress in neutrino scattering experiments with few gev neutrino beams is reviewed focusing on new experimental input since the beginning of the nuint workshop series in 2001 progress in neutrino quasielastic scattering resonance production coherent pion production scattering in the transition region between th... | [['recent', 'progress', 'in', 'neutrino', 'scattering', 'experiments', 'with', 'few', 'gev', 'neutrino', 'beams', 'is', 'reviewed', 'focusing', 'on', 'new', 'experimental', 'input', 'since', 'the', 'beginning', 'of', 'the', 'nuint', 'workshop', 'series', 'in', '2001', 'progress', 'in', 'neutrino', 'quasielastic', 'scat... | [-0.04970557905995009, 0.2788292067615609, -0.02948574078056896, 0.1591801057986327, -0.04914101089040438, -0.07506206781979192, 0.0014765993365200988, 0.39124928284109683, -0.22175651615518227, -0.22959221379929468, -0.012211736399892783, -0.38350617741806464, -0.06384094019436784, 0.2123466053520117, 0.11937312249517... |
710.3967 | Associahedra, Cyclohedra and a Topological solution to the
A_{\infty}--Deligne conjecture | We give a topological solution to the $\Ainf$ Deligne conjecture using
associahedra and cyclohedra. For this we construct three CW complexes whose
cells are indexed by products of polytopes. Giving new explicit realizations of
the polytopes in terms of different types of trees, we are able to show that
the CW complex... | math.AT math.QA | we give a topological solution to the ainf deligne conjecture using associahedra and cyclohedra for this we construct three cw complexes whose cells are indexed by products of polytopes giving new explicit realizations of the polytopes in terms of different types of trees we are able to show that the cw complexes are c... | [['we', 'give', 'a', 'topological', 'solution', 'to', 'the', 'ainf', 'deligne', 'conjecture', 'using', 'associahedra', 'and', 'cyclohedra', 'for', 'this', 'we', 'construct', 'three', 'cw', 'complexes', 'whose', 'cells', 'are', 'indexed', 'by', 'products', 'of', 'polytopes', 'giving', 'new', 'explicit', 'realizations', ... | [-0.13329921669383596, 0.07466103898859867, -0.07274120659318589, 0.07817948572622001, -0.09490652753480973, -0.10656352372633876, 0.02249084279840485, 0.3614680677668355, -0.3377492206725683, -0.23030923801751538, 0.12229560001198743, -0.225940024497997, -0.1799797679489578, 0.2118660298652435, -0.12783054151849552, -... |
710.3968 | Gromov-Witten invariants of blow-ups along submanifolds with convex
normal bundles | Given a submanifold Z inside X, let Y be the blow-up of X along Z. When the
normal bundle of Z in X is convex with a minor assumption, we prove that
genus-zero GW-invariants of Y with cohomology insertions from X, are identical
to GW-invariants of X. Under the same hypothesis, a vanishing theorem is also
proved. An e... | math.AG | given a submanifold z inside x let y be the blowup of x along z when the normal bundle of z in x is convex with a minor assumption we prove that genuszero gwinvariants of y with cohomology insertions from x are identical to gwinvariants of x under the same hypothesis a vanishing theorem is also proved an example to whi... | [['given', 'a', 'submanifold', 'z', 'inside', 'x', 'let', 'y', 'be', 'the', 'blowup', 'of', 'x', 'along', 'z', 'when', 'the', 'normal', 'bundle', 'of', 'z', 'in', 'x', 'is', 'convex', 'with', 'a', 'minor', 'assumption', 'we', 'prove', 'that', 'genuszero', 'gwinvariants', 'of', 'y', 'with', 'cohomology', 'insertions', '... | [-0.1818249071137247, 0.09852136364563112, -0.09682783841291505, 0.07600157836117269, -0.02122865684246749, -0.20623392972237106, 0.009828952517820878, 0.3830794097248758, -0.2768827797321791, -0.1789360360054069, 0.09043680984144925, -0.26934075479008507, -0.08691393373157369, 0.18910652538369085, -0.1370178930817193,... |
710.3969 | Primordial Mass Segregation in Starburst Stellar Clusters | We present a model to explain the mass segregation and shallow mass functions
observed in the central parts of dense and young starburst stellar clusters.
The model assumes that the initial pre-stellar cores mass function resulting
from the turbulent fragmentation of the proto-cluster cloud is significantly
altered b... | astro-ph | we present a model to explain the mass segregation and shallow mass functions observed in the central parts of dense and young starburst stellar clusters the model assumes that the initial prestellar cores mass function resulting from the turbulent fragmentation of the protocluster cloud is significantly altered by the... | [['we', 'present', 'a', 'model', 'to', 'explain', 'the', 'mass', 'segregation', 'and', 'shallow', 'mass', 'functions', 'observed', 'in', 'the', 'central', 'parts', 'of', 'dense', 'and', 'young', 'starburst', 'stellar', 'clusters', 'the', 'model', 'assumes', 'that', 'the', 'initial', 'prestellar', 'cores', 'mass', 'func... | [-0.08223803512728176, 0.16011359635024117, -0.058584212867590864, 0.14606073566937994, -0.031008114748132917, -0.03032794370053288, 0.061975664595285286, 0.34023189921027575, -0.15640688569117814, -0.3921146892345487, 0.05216247549352165, -0.2315989008030066, -0.004113222013872403, 0.13818101310290587, 0.0014134654458... |
710.397 | An Overview of the SPACE Mission Proposal | SPACE (SPectroscopic All-sky Cosmic Explorer) is a class-M mission proposed
to ESA for the Cosmic Vision 2015-2025 call and recently promoted to the next
assessment study phase. SPACE will produce the first all-sky spectroscopic
survey of the Universe, taking spectra of more than 500 million galaxies over a
wide rang... | astro-ph | space spectroscopic allsky cosmic explorer is a classm mission proposed to esa for the cosmic vision 20152025 call and recently promoted to the next assessment study phase space will produce the first allsky spectroscopic survey of the universe taking spectra of more than 500 million galaxies over a wide range of redsh... | [['space', 'spectroscopic', 'allsky', 'cosmic', 'explorer', 'is', 'a', 'classm', 'mission', 'proposed', 'to', 'esa', 'for', 'the', 'cosmic', 'vision', '20152025', 'call', 'and', 'recently', 'promoted', 'to', 'the', 'next', 'assessment', 'study', 'phase', 'space', 'will', 'produce', 'the', 'first', 'allsky', 'spectrosco... | [-0.0882952431099478, 0.09804693358652916, -0.06902981773094248, 0.0843477339647816, -0.156118452772385, -0.017000659969390222, 0.04835920808610585, 0.37024494894753823, -0.2175448969688063, -0.36193567128882176, 0.11842194575696678, -0.3206227023818112, -0.018390492929206022, 0.23978779823194965, 0.017055915925003256,... |
710.3971 | Spontaneous Supersymmetry Breaking by Large-N Matrices | Motivated by supersymmetry breaking in matrix model formulations of
superstrings, we present some concrete models, in which the supersymmetry is
preserved for any finite $N$, but gets broken at infinite $N$, where $N$ is the
rank of matrix variables. The models are defined as supersymmetric field
theories coupled to ... | hep-th hep-ph | motivated by supersymmetry breaking in matrix model formulations of superstrings we present some concrete models in which the supersymmetry is preserved for any finite n but gets broken at infinite n where n is the rank of matrix variables the models are defined as supersymmetric field theories coupled to some matrix m... | [['motivated', 'by', 'supersymmetry', 'breaking', 'in', 'matrix', 'model', 'formulations', 'of', 'superstrings', 'we', 'present', 'some', 'concrete', 'models', 'in', 'which', 'the', 'supersymmetry', 'is', 'preserved', 'for', 'any', 'finite', 'n', 'but', 'gets', 'broken', 'at', 'infinite', 'n', 'where', 'n', 'is', 'the'... | [-0.13851655060330367, 0.21566909296298717, -0.028840082707073614, 0.08503983804059602, -0.026801050697662393, -0.17904290978537024, -0.007364163332029569, 0.30168341139496185, -0.2265647805999128, -0.28298414386111964, 0.12512616751965794, -0.2551424001109134, -0.13353795987010622, 0.07243004108804474, -0.024367509175... |
710.3972 | Centrality measures and thermodynamic formalism for complex networks | In the study of small and large networks it is customary to perform a simple
random walk, where the random walker jumps from one node to one of its
neighbours with uniform probability. The properties of this random walk are
intimately related to the combinatorial properties of the network. In this
paper we propose to... | physics.data-an cond-mat.stat-mech physics.soc-ph | in the study of small and large networks it is customary to perform a simple random walk where the random walker jumps from one node to one of its neighbours with uniform probability the properties of this random walk are intimately related to the combinatorial properties of the network in this paper we propose to use ... | [['in', 'the', 'study', 'of', 'small', 'and', 'large', 'networks', 'it', 'is', 'customary', 'to', 'perform', 'a', 'simple', 'random', 'walk', 'where', 'the', 'random', 'walker', 'jumps', 'from', 'one', 'node', 'to', 'one', 'of', 'its', 'neighbours', 'with', 'uniform', 'probability', 'the', 'properties', 'of', 'this', '... | [-0.08214580212398749, 0.1221917218532785, -0.07955217494819204, 0.10569550535750115, -0.07215024011200565, -0.16325909430607566, 0.06164818359493703, 0.3992978897379729, -0.2729324315746939, -0.25417769703114385, 0.08457669494357141, -0.3131109153856388, -0.15874050585134858, 0.13337099146396283, -0.09598212079958791,... |
710.3973 | Diffusion in the Continuous-Imaginary-Time Quantum World-Line Monte
Carlo Simulations with Extended Ensembles | The dynamics of samples in the continuous-imaginary-time quantum world-line
Monte Carlo simulations with extended ensembles are investigated. In the case
of a conventional flat ensemble on the one-dimensional quantum S=1 bi-quadratic
model, the asymmetric behavior of Monte Carlo samples appears in the diffusion
proce... | cond-mat.stat-mech cond-mat.str-el | the dynamics of samples in the continuousimaginarytime quantum worldline monte carlo simulations with extended ensembles are investigated in the case of a conventional flat ensemble on the onedimensional quantum s1 biquadratic model the asymmetric behavior of monte carlo samples appears in the diffusion process in the ... | [['the', 'dynamics', 'of', 'samples', 'in', 'the', 'continuousimaginarytime', 'quantum', 'worldline', 'monte', 'carlo', 'simulations', 'with', 'extended', 'ensembles', 'are', 'investigated', 'in', 'the', 'case', 'of', 'a', 'conventional', 'flat', 'ensemble', 'on', 'the', 'onedimensional', 'quantum', 's1', 'biquadratic'... | [-0.1542490721216396, 0.15584025558143375, -0.06386032562673562, 0.04540768595590033, 0.023951346787998058, -0.09943154579996476, 0.021428466684690964, 0.3847044839516399, -0.2394696948683168, -0.2615319703811941, 0.04990298036342912, -0.3188961570877142, -0.14383738970303336, 0.13824424349636896, 0.015375769601797495,... |
710.3974 | Distributed source coding in dense sensor networks | We study the problem of the reconstruction of a Gaussian field defined in
[0,1] using N sensors deployed at regular intervals. The goal is to quantify
the total data rate required for the reconstruction of the field with a given
mean square distortion. We consider a class of two-stage mechanisms which a)
send informa... | cs.IT math.IT | we study the problem of the reconstruction of a gaussian field defined in 01 using n sensors deployed at regular intervals the goal is to quantify the total data rate required for the reconstruction of the field with a given mean square distortion we consider a class of twostage mechanisms which a send information to a... | [['we', 'study', 'the', 'problem', 'of', 'the', 'reconstruction', 'of', 'a', 'gaussian', 'field', 'defined', 'in', '01', 'using', 'n', 'sensors', 'deployed', 'at', 'regular', 'intervals', 'the', 'goal', 'is', 'to', 'quantify', 'the', 'total', 'data', 'rate', 'required', 'for', 'the', 'reconstruction', 'of', 'the', 'fie... | [-0.1593786801746551, 0.066544095314841, -0.05169766934172429, 0.011688628023430864, -0.015212900602714496, -0.14542098349118804, 0.08819897955362783, 0.3655252865337311, -0.280034835914031, -0.3050022012930601, 0.12350832343824762, -0.24408862754662938, -0.10860314728380081, 0.1877784016244906, -0.08452389704836334, 0... |
710.3975 | Homotopy nilpotency in p-compact groups | A p-compact group is a mod p homotopy theoretical analogue of a compact Lie
group. It is determined the homotopy nilpotency class of a p-compact group
having the homotopy type of the $p$-completion of the direct product of
spheres.
| math.AT | a pcompact group is a mod p homotopy theoretical analogue of a compact lie group it is determined the homotopy nilpotency class of a pcompact group having the homotopy type of the pcompletion of the direct product of spheres | [['a', 'pcompact', 'group', 'is', 'a', 'mod', 'p', 'homotopy', 'theoretical', 'analogue', 'of', 'a', 'compact', 'lie', 'group', 'it', 'is', 'determined', 'the', 'homotopy', 'nilpotency', 'class', 'of', 'a', 'pcompact', 'group', 'having', 'the', 'homotopy', 'type', 'of', 'the', 'pcompletion', 'of', 'the', 'direct', 'pro... | [-0.26654957994245565, 0.05940139766495962, -0.13497821690562445, 0.06527007350292152, -0.15296925098086014, -0.10461937063015424, 0.028240710210341673, 0.3445831381190473, -0.3322595323746403, -0.19847852946856084, 0.09803851066419902, -0.198084940130894, -0.08636704717691128, 0.16048854981095362, -0.1422416144170058,... |
710.3976 | An attempt to control a manmade nuclear fusion | A detailed simple model is applied to study a high temperature hydrogen
plasma ball. It is assumed that the ions and delocalized electrons are
distributed randomly throughout the charged plasma ball (extra/missing charge
is assumed to be found in a thin layer on the surface of a ball). The energy of
the microscopic e... | physics.plasm-ph hep-ph physics.chem-ph | a detailed simple model is applied to study a high temperature hydrogen plasma ball it is assumed that the ions and delocalized electrons are distributed randomly throughout the charged plasma ball extramissing charge is assumed to be found in a thin layer on the surface of a ball the energy of the microscopic electros... | [['a', 'detailed', 'simple', 'model', 'is', 'applied', 'to', 'study', 'a', 'high', 'temperature', 'hydrogen', 'plasma', 'ball', 'it', 'is', 'assumed', 'that', 'the', 'ions', 'and', 'delocalized', 'electrons', 'are', 'distributed', 'randomly', 'throughout', 'the', 'charged', 'plasma', 'ball', 'extramissing', 'charge', '... | [-0.07109096050049296, 0.22230779054299207, -0.0854935206466315, 0.06882053860676357, 0.030255912101342226, -0.14413861927746888, 0.02482475831770194, 0.3843478967606182, -0.25904676071892846, -0.24745704744234157, 0.05517658209231433, -0.2842576474600642, 0.005515315386296158, 0.11951497263311159, -0.03297531640183338... |
710.3977 | Reconstruction of the Berger measure when the core is of tensor form | Let $\mathfrak{H}_{0}$ denote the class of commuting pairs of subnormal
operators on Hilbert space, and let $\mathcal{TC}:=\{\mathbf{T}\in \mathfrak{%
H}_{0}:c(\mathbf{T)}$ is of tensor form$\}$, where $c(\mathbf{T})$ is the core
of $\mathbf{T}$. We obtain a concrete necessary and sufficient condition for
the subnorm... | math.FA | let mathfrakh_0 denote the class of commuting pairs of subnormal operators on hilbert space and let mathcaltcmathbftin mathfrak h_0cmathbft is of tensor form where cmathbft is the core of mathbft we obtain a concrete necessary and sufficient condition for the subnormality of mathbftequiv t_1t_2in mathcaltc in terms of ... | [['let', 'mathfrakh_0', 'denote', 'the', 'class', 'of', 'commuting', 'pairs', 'of', 'subnormal', 'operators', 'on', 'hilbert', 'space', 'and', 'let', 'mathcaltcmathbftin', 'mathfrak', 'h_0cmathbft', 'is', 'of', 'tensor', 'form', 'where', 'cmathbft', 'is', 'the', 'core', 'of', 'mathbft', 'we', 'obtain', 'a', 'concrete',... | [-0.17110907174646856, 0.19374922651120208, -0.0066777320409362965, 0.0050266524480486454, -0.05289700586264107, -0.09737372265451334, -0.01237390263598751, 0.3136542460457845, -0.2756686520170082, -0.15743812714195388, 0.09050484341992573, -0.2679260731251402, -0.052446457845243544, 0.15881146348335526, -0.09597901554... |
710.3978 | Dielectric anomaly at T_N in LaMnO3 | We observe a distinct anomaly in dielectric permittivity (epsilon') as well
as relaxation time (tao_0) versus temperature (T) pattern at the
antiferromagnetic transition point (T_N) in single crystal of LaMnO3. The
equivalent circuit analysis of the impedance spectra across T_N reveals clear
anomaly in the capacitive... | cond-mat.str-el | we observe a distinct anomaly in dielectric permittivity epsilon as well as relaxation time tao_0 versus temperature t pattern at the antiferromagnetic transition point t_n in single crystal of lamno3 the equivalent circuit analysis of the impedance spectra across t_n reveals clear anomaly in the capacitive component c... | [['we', 'observe', 'a', 'distinct', 'anomaly', 'in', 'dielectric', 'permittivity', 'epsilon', 'as', 'well', 'as', 'relaxation', 'time', 'tao_0', 'versus', 'temperature', 't', 'pattern', 'at', 'the', 'antiferromagnetic', 'transition', 'point', 't_n', 'in', 'single', 'crystal', 'of', 'lamno3', 'the', 'equivalent', 'circu... | [-0.20675370704939033, 0.22673164102454463, -0.0005547602081901164, -0.06067572401038238, -0.032867212489537605, -0.1302035616819638, 0.12692151275802066, 0.4445577408489469, -0.2800477443337773, -0.2803828231325107, 0.014847668713486343, -0.37513275826712705, -0.13078775948711804, 0.11092532087456096, 0.08247516012762... |
710.3979 | Toward Trusted Sharing of Network Packet Traces Using Anonymization:
Single-Field Privacy/Analysis Tradeoffs | Network data needs to be shared for distributed security analysis.
Anonymization of network data for sharing sets up a fundamental tradeoff
between privacy protection versus security analysis capability. This
privacy/analysis tradeoff has been acknowledged by many researchers but this is
the first paper to provide em... | cs.CR cs.NI | network data needs to be shared for distributed security analysis anonymization of network data for sharing sets up a fundamental tradeoff between privacy protection versus security analysis capability this privacyanalysis tradeoff has been acknowledged by many researchers but this is the first paper to provide empiric... | [['network', 'data', 'needs', 'to', 'be', 'shared', 'for', 'distributed', 'security', 'analysis', 'anonymization', 'of', 'network', 'data', 'for', 'sharing', 'sets', 'up', 'a', 'fundamental', 'tradeoff', 'between', 'privacy', 'protection', 'versus', 'security', 'analysis', 'capability', 'this', 'privacyanalysis', 'trad... | [-0.15283858555654484, -0.03184037128237598, -0.08813582254468554, 0.09421313361024423, -0.0778986533480366, -0.23708771253305097, 0.12330949410980177, 0.3887735878628108, -0.2687444829029001, -0.3584421698807649, 0.14620590658629343, -0.32214770323386593, -0.1470588542250616, 0.20766950716384716, -0.1283186545892198, ... |
710.398 | Some properties of minimizers for the Chan-Esedoglu L1TV functional | We present two results characterizing minimizers of the Chan-Esedoglu L1TV
functional $F(u) \equiv \int |\nabla u | dx + \lambda \int |u - f| dx $;
$u,f:\Bbb{R}^n \to \Bbb{R}$. If we restrict to $u = \chi_{\Sigma}$ and $f =
\chi_{\Omega}$, $\Sigma, \Omega \in \Bbb{R}^n$, the $L^1$TV functional reduces
to $E(\Sigma) =... | math.OC math.AP math.CA | we present two results characterizing minimizers of the chanesedoglu l1tv functional fu equiv int nabla u dx lambda int u f dx ufbbbrn to bbbr if we restrict to u chi_sigma and f chi_omega sigma omega in bbbrn the l1tv functional reduces to esigma persigma lambda sigmavartriangle omega we show that there is a minimizer... | [['we', 'present', 'two', 'results', 'characterizing', 'minimizers', 'of', 'the', 'chanesedoglu', 'l1tv', 'functional', 'fu', 'equiv', 'int', 'nabla', 'u', 'dx', 'lambda', 'int', 'u', 'f', 'dx', 'ufbbbrn', 'to', 'bbbr', 'if', 'we', 'restrict', 'to', 'u', 'chi_sigma', 'and', 'f', 'chi_omega', 'sigma', 'omega', 'in', 'bb... | [-0.18270356788080397, 0.03799362947153518, -0.0591223273630731, 0.03424729334618291, -0.05422574299864653, -0.11800057872584681, 0.038687771267628644, 0.35886547712957473, -0.29461852709452313, -0.1708096607353508, 0.05829224150961008, -0.378906031752505, -0.09510960728280261, 0.13856291273851098, -0.12592846423016513... |
710.3981 | The importance of the Selberg integral | It has been remarked that a fair measure of the impact of Atle Selberg's work
is the number of mathematical terms which bear his name. One of these is the
Selberg integral, an n-dimensional generalization of the Euler beta integral.
We trace its sudden rise to prominence, initiated by a question to Selberg from
Enric... | math.CA math-ph math.CO math.MP math.QA | it has been remarked that a fair measure of the impact of atle selbergs work is the number of mathematical terms which bear his name one of these is the selberg integral an ndimensional generalization of the euler beta integral we trace its sudden rise to prominence initiated by a question to selberg from enrico bombie... | [['it', 'has', 'been', 'remarked', 'that', 'a', 'fair', 'measure', 'of', 'the', 'impact', 'of', 'atle', 'selbergs', 'work', 'is', 'the', 'number', 'of', 'mathematical', 'terms', 'which', 'bear', 'his', 'name', 'one', 'of', 'these', 'is', 'the', 'selberg', 'integral', 'an', 'ndimensional', 'generalization', 'of', 'the',... | [-0.12494471564683925, 0.08416616196119497, -0.1322332032914482, 0.08926653817779065, -0.08622290751438087, -0.12059013582001538, -0.004326158537661462, 0.2692169207843271, -0.26885954671497664, -0.250910933112114, 0.08939922306644939, -0.2547839536494923, -0.22358996955566665, 0.22103253619939978, -0.11564721948981507... |
710.3982 | Covariant differentiation of spinors for a general affine connection | We show that the covariant derivative of a spinor for a general affine
connection, not restricted to be metric compatible, is given by the
Fock-Ivanenko coefficients with the antisymmetric part of the Lorentz
connection. The projective invariance of the spinor connection allows to
introduce gauge fields interacting w... | gr-qc math-ph math.MP | we show that the covariant derivative of a spinor for a general affine connection not restricted to be metric compatible is given by the fockivanenko coefficients with the antisymmetric part of the lorentz connection the projective invariance of the spinor connection allows to introduce gauge fields interacting with sp... | [['we', 'show', 'that', 'the', 'covariant', 'derivative', 'of', 'a', 'spinor', 'for', 'a', 'general', 'affine', 'connection', 'not', 'restricted', 'to', 'be', 'metric', 'compatible', 'is', 'given', 'by', 'the', 'fockivanenko', 'coefficients', 'with', 'the', 'antisymmetric', 'part', 'of', 'the', 'lorentz', 'connection',... | [-0.19835618557408452, 0.157185585163957, -0.07684796318150774, 0.0730559820058812, -0.19782780350722146, -0.13182205769628513, -0.04970322154236562, 0.35607129696643713, -0.22895751462783664, -0.2042869385331869, 0.03194529291552802, -0.19344985001446208, -0.2162310111576296, 0.09827050778690274, -0.013767652566347158... |
710.3983 | Long time simulation of a beam in a periodic focusing channel via a
two-scale PIC-method | We study the two-scale asymptotics for a charged beam under the action of a
rapidly oscillating external electric field. After proving the convergence to
the correct asymptotic state, we develop a numerical method for solving the
limit model involving two time scales and validate its efficiency for the
simulation of ... | math.NA | we study the twoscale asymptotics for a charged beam under the action of a rapidly oscillating external electric field after proving the convergence to the correct asymptotic state we develop a numerical method for solving the limit model involving two time scales and validate its efficiency for the simulation of long ... | [['we', 'study', 'the', 'twoscale', 'asymptotics', 'for', 'a', 'charged', 'beam', 'under', 'the', 'action', 'of', 'a', 'rapidly', 'oscillating', 'external', 'electric', 'field', 'after', 'proving', 'the', 'convergence', 'to', 'the', 'correct', 'asymptotic', 'state', 'we', 'develop', 'a', 'numerical', 'method', 'for', '... | [-0.15079650573898107, 0.10039290754745404, -0.1323693544017496, 0.06895030282989696, -0.00013952050358057022, -0.10086499969474971, 0.058557147367133036, 0.3610135969636893, -0.244728931122356, -0.2956030909316959, 0.1342590412521666, -0.22186375706008188, -0.050276870744440844, 0.20227038002728173, 0.0416979616663108... |
710.3984 | A model for giant flares in soft gamma repeaters | We argue that giant flares in SGRs can be associated to the core conversion
of an isolated neutron star having a subcritical magnetic field $\sim 10^{12}$
G and a fallback disk around it. We show that, in a timescale of $\lesssim
10^5$ yrs, accretion from the fallback disk can increase the mass of the
central object ... | astro-ph | we argue that giant flares in sgrs can be associated to the core conversion of an isolated neutron star having a subcritical magnetic field sim 1012 g and a fallback disk around it we show that in a timescale of lesssim 105 yrs accretion from the fallback disk can increase the mass of the central object up to the criti... | [['we', 'argue', 'that', 'giant', 'flares', 'in', 'sgrs', 'can', 'be', 'associated', 'to', 'the', 'core', 'conversion', 'of', 'an', 'isolated', 'neutron', 'star', 'having', 'a', 'subcritical', 'magnetic', 'field', 'sim', '1012', 'g', 'and', 'a', 'fallback', 'disk', 'around', 'it', 'we', 'show', 'that', 'in', 'a', 'time... | [-0.10046203133846525, 0.2098076141188531, -0.06993182699614185, 0.10972794461805298, -0.08510038151475442, -0.003344484872571161, 0.08684226459361055, 0.3613155951001206, -0.21683830251207664, -0.3478959060217045, 0.04145600445106068, -0.2920022452421182, 0.009873316198790155, 0.21873964271096347, -0.00252084245550490... |
710.3985 | Antiproton-deuteron atoms in models of realistic potentials | The antiproton-deuteron atoms are studied in models of various realistic,
popular nucleon-antinucleon potentials. The small energy shifts and decay
widths of the atoms, which stem from the short-ranged strong interactions
between the antiproton and deuteron, are evaluated in a well-established,
accurate approach base... | physics.atom-ph | the antiprotondeuteron atoms are studied in models of various realistic popular nucleonantinucleon potentials the small energy shifts and decay widths of the atoms which stem from the shortranged strong interactions between the antiproton and deuteron are evaluated in a wellestablished accurate approach based on the st... | [['the', 'antiprotondeuteron', 'atoms', 'are', 'studied', 'in', 'models', 'of', 'various', 'realistic', 'popular', 'nucleonantinucleon', 'potentials', 'the', 'small', 'energy', 'shifts', 'and', 'decay', 'widths', 'of', 'the', 'atoms', 'which', 'stem', 'from', 'the', 'shortranged', 'strong', 'interactions', 'between', '... | [-0.0781039491580599, 0.16268601100737892, -0.06582187026188793, 0.18553131412953322, 0.0171733210902384, -0.14108215143888697, 0.044735087984249244, 0.3681364073610503, -0.2175094248526845, -0.2758971135293649, -0.04812896816629516, -0.3444807310704111, -0.034160998988197154, 0.16293031314372525, 0.10702868435947487, ... |
710.3986 | Microwave band on-chip coil technique for single electron spin resonance
in a quantum dot | Microwave band on-chip microcoils are developed for the application to single
electron spin resonance measurement with a single quantum dot. Basic properties
such as characteristic impedance and electromagnetic field distribution are
examined for various coil designs by means of experiment and simulation. The
combine... | cond-mat.mes-hall | microwave band onchip microcoils are developed for the application to single electron spin resonance measurement with a single quantum dot basic properties such as characteristic impedance and electromagnetic field distribution are examined for various coil designs by means of experiment and simulation the combined set... | [['microwave', 'band', 'onchip', 'microcoils', 'are', 'developed', 'for', 'the', 'application', 'to', 'single', 'electron', 'spin', 'resonance', 'measurement', 'with', 'a', 'single', 'quantum', 'dot', 'basic', 'properties', 'such', 'as', 'characteristic', 'impedance', 'and', 'electromagnetic', 'field', 'distribution', ... | [-0.16303156488502282, 0.20259976374994343, -0.01990606882997478, 0.03403531840983002, -0.03496508540993091, -0.2100278556967775, 0.05544524418219225, 0.39282027669639014, -0.22758614025078713, -0.33214232564593354, -0.005248232857047697, -0.2817208408766116, -0.08508711868780665, 0.27672846951754765, 0.020483045788326... |
710.3987 | Nonequilibrium electron charging in carbon-nanotube-based molecular
bridges | We evidence the importance of electron charging under nonequilibrium
conditions for carbon-nanotube-based molecular bridges, using a self-consistent
Green's function method with an extended Huckel Hamiltonian and a
three-dimensional Poisson solver. Our analysis demonstrates that such feature
is highly dependent on th... | cond-mat.mes-hall cond-mat.mtrl-sci | we evidence the importance of electron charging under nonequilibrium conditions for carbonnanotubebased molecular bridges using a selfconsistent greens function method with an extended huckel hamiltonian and a threedimensional poisson solver our analysis demonstrates that such feature is highly dependent on the chirali... | [['we', 'evidence', 'the', 'importance', 'of', 'electron', 'charging', 'under', 'nonequilibrium', 'conditions', 'for', 'carbonnanotubebased', 'molecular', 'bridges', 'using', 'a', 'selfconsistent', 'greens', 'function', 'method', 'with', 'an', 'extended', 'huckel', 'hamiltonian', 'and', 'a', 'threedimensional', 'poisso... | [-0.12102042085501136, 0.06887300801166128, -0.08339450057716138, 0.03173178834189731, -0.00106705077773621, -0.13119476865376195, 0.08986686636763876, 0.41743436886338137, -0.20812787315858308, -0.2639042406633336, 0.0136477719937321, -0.27907053749727945, -0.18943734955723568, 0.22626143933514192, 0.02676431633912587... |
710.3988 | Sexual reproduction from the male (men) point of view | To counterbalance the views presented here by Suzana Moss de Oliveira, we
explain here the truth: How men are oppressed by Mother Nature, who may have
made an error inventing us, and by living women, who could get rid of most of
us. Why do women live longer than us? Why is the Y chromosome for men so small?
What are ... | q-bio.PE | to counterbalance the views presented here by suzana moss de oliveira we explain here the truth how men are oppressed by mother nature who may have made an error inventing us and by living women who could get rid of most of us why do women live longer than us why is the y chromosome for men so small what are the danger... | [['to', 'counterbalance', 'the', 'views', 'presented', 'here', 'by', 'suzana', 'moss', 'de', 'oliveira', 'we', 'explain', 'here', 'the', 'truth', 'how', 'men', 'are', 'oppressed', 'by', 'mother', 'nature', 'who', 'may', 'have', 'made', 'an', 'error', 'inventing', 'us', 'and', 'by', 'living', 'women', 'who', 'could', 'g... | [-0.04539660294399967, 0.16781738936004834, -0.09023400780980487, 0.1693769358841882, -0.17416982715163964, -0.16193625122218966, 0.11154534186921027, 0.397560836186251, -0.176059316626346, -0.35787551269406476, 0.08653786778309752, -0.3083728561304083, -0.16674682585500092, 0.16835073257813296, -0.25023489518382824, -... |
710.3989 | C1-generic conservative diffeomorphisms have trivial centralizer | We prove that the spaces of C1 symplectomorphisms and of C1 volume-preserving
diffeomorphisms of connected manifolds both contain residual subsets of
diffeomorphisms whose centralizers are trivial. (Les diff\'eomorphismes
conservatifs C1-g\'en\'eriques ont un centralisateur trivial. Nous montrons que
l'espace des sym... | math.DS | we prove that the spaces of c1 symplectomorphisms and of c1 volumepreserving diffeomorphisms of connected manifolds both contain residual subsets of diffeomorphisms whose centralizers are trivial les diffeomorphismes conservatifs c1generiques ont un centralisateur trivial nous montrons que lespace des symplectomorphism... | [['we', 'prove', 'that', 'the', 'spaces', 'of', 'c1', 'symplectomorphisms', 'and', 'of', 'c1', 'volumepreserving', 'diffeomorphisms', 'of', 'connected', 'manifolds', 'both', 'contain', 'residual', 'subsets', 'of', 'diffeomorphisms', 'whose', 'centralizers', 'are', 'trivial', 'les', 'diffeomorphismes', 'conservatifs', '... | [-0.375244690105319, 0.038117960824941594, -0.1762257742113434, 0.06230470680942138, -0.09129895409569144, -0.15884419458452612, -0.28182827748629885, 0.08443818705078836, -0.14337237342260778, -0.18521096274877588, 0.08684309082260976, -0.4119010508681337, -0.17483276166021824, 0.13566045234232055, -0.4038277741676817... |
710.399 | Scattering of Low-Frequency Radiation by a Gyrating Electron | The scattering of electromagnetic radiation by the particle gyrating in an
external magnetic field is considered. Particular attention is paid to the
low-frequency case, when the frequencies of incident radiation are much less
than the electron gyrofrequency. The spectral and polarization features of the
scattering c... | astro-ph | the scattering of electromagnetic radiation by the particle gyrating in an external magnetic field is considered particular attention is paid to the lowfrequency case when the frequencies of incident radiation are much less than the electron gyrofrequency the spectral and polarization features of the scattering crossse... | [['the', 'scattering', 'of', 'electromagnetic', 'radiation', 'by', 'the', 'particle', 'gyrating', 'in', 'an', 'external', 'magnetic', 'field', 'is', 'considered', 'particular', 'attention', 'is', 'paid', 'to', 'the', 'lowfrequency', 'case', 'when', 'the', 'frequencies', 'of', 'incident', 'radiation', 'are', 'much', 'le... | [-0.09599005830629419, 0.2340725081971934, -0.02886248074903868, 0.12037351261655652, -0.08158680063037985, -0.05277195863272761, -0.03198853946304408, 0.404439196512463, -0.25185615411208234, -0.2882775233851539, 0.032464739134319236, -0.3184670355611881, -0.040633924237951854, 0.23152154276219472, 0.08073767167032395... |
710.3991 | Dirichlet Duality and the Nonlinear Dirichlet Problem | We study the Dirichlet problem for fully nonlinear, degenerate elliptic
equations of the form f(Hess, u)=0 on a smoothly bounded domain D in R^n. In
our approach the equation is replaced by a subset F of the space of symmetric
nxn-matrices, with bdy(F) contined in the set {f=0}. We establish the existence
and uniquen... | math.AP math.CV math.DG | we study the dirichlet problem for fully nonlinear degenerate elliptic equations of the form fhess u0 on a smoothly bounded domain d in rn in our approach the equation is replaced by a subset f of the space of symmetric nxnmatrices with bdyf contined in the set f0 we establish the existence and uniqueness of continuous... | [['we', 'study', 'the', 'dirichlet', 'problem', 'for', 'fully', 'nonlinear', 'degenerate', 'elliptic', 'equations', 'of', 'the', 'form', 'fhess', 'u0', 'on', 'a', 'smoothly', 'bounded', 'domain', 'd', 'in', 'rn', 'in', 'our', 'approach', 'the', 'equation', 'is', 'replaced', 'by', 'a', 'subset', 'f', 'of', 'the', 'space... | [-0.17241387606272238, 0.046658939599880336, -0.07408163120478467, 0.05977862014324135, -0.09515424329978958, -0.12959057415083883, -0.02061551305474855, 0.3034616417882652, -0.3046433015107201, -0.21652822916013031, 0.1259268344525333, -0.2702449021877503, -0.15062168400101175, 0.19470502049922186, -0.0625990920246290... |
710.3992 | Zero modes for the magnetic Pauli operator in even-dimensional Euclidean
space | We study the ground state of the Pauli Hamiltonian with a magnetic field in
R^(2d). We consider the case where a scalar potential W is present and the
magnetic field B is given by $B=2i\partial\bar\partial W$. The main result is
that there are no zero modes if the magnetic field decays faster than
quadratically at in... | math.SP | we study the ground state of the pauli hamiltonian with a magnetic field in r2d we consider the case where a scalar potential w is present and the magnetic field b is given by b2ipartialbarpartial w the main result is that there are no zero modes if the magnetic field decays faster than quadratically at infinity if the... | [['we', 'study', 'the', 'ground', 'state', 'of', 'the', 'pauli', 'hamiltonian', 'with', 'a', 'magnetic', 'field', 'in', 'r2d', 'we', 'consider', 'the', 'case', 'where', 'a', 'scalar', 'potential', 'w', 'is', 'present', 'and', 'the', 'magnetic', 'field', 'b', 'is', 'given', 'by', 'b2ipartialbarpartial', 'w', 'the', 'mai... | [-0.17509224268884122, 0.23315588311691368, -0.048002540886115566, 0.038429811845052536, -0.0595955065308282, -0.13443417711551864, 0.04052054468839133, 0.30464938600742064, -0.22029496420297648, -0.2738623518271597, 0.06459547390593318, -0.28445294624255907, -0.12126206105145124, 0.17001200905376737, -0.01035138921668... |
710.3993 | A Study of the Radiative Ke3 Decay and Search for Direct Photon Emission
with the KLOE Detector | We present a measurement of the ratio R =
\Gamma(\keg;\Estar>30\mev,\qstar>20^\circ)$/$\Gamma(\kegf)$ and a first
measurement of the direct emission contribution in KL semileptonic decays. The
measurement is done at the DAFNE phi-factory selecting phi->KL KS decays with
the KLOE detector. We use 328 pb^{-1}$ of data ... | hep-ex | we present a measurement of the ratio r gammakegestar30mevqstar20circgammakegf and a first measurement of the direct emission contribution in kl semileptonic decays the measurement is done at the dafne phifactory selecting phikl ks decays with the kloe detector we use 328 pb1 of data corresponding to about 35 million k... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'ratio', 'r', 'gammakegestar30mevqstar20circgammakegf', 'and', 'a', 'first', 'measurement', 'of', 'the', 'direct', 'emission', 'contribution', 'in', 'kl', 'semileptonic', 'decays', 'the', 'measurement', 'is', 'done', 'at', 'the', 'dafne', 'phifactory', 'selecting', 'p... | [-0.06770465931359967, 0.11138827533913698, -0.051883743531529754, 0.06415806564831988, -0.05312812018116385, -0.0994038235291209, 0.10374002292437452, 0.3011868975164605, -0.16619653380672697, -0.3416327285214695, 0.027900166355375147, -0.42595789933078726, 0.09049180096251444, 0.1691906863305403, 0.09270608476297536,... |
710.3994 | Accelerating Universe and Pioneer anomaly as manifestation of conformal
time inhomogeneity | The description of the cosmological expansion and its possible local
manifestations via treating the proper conformal transformations as a
coordinate transformation from a comoving Lorentz reference frame (RF) to an
uniformly accelerated RF is given. The explicit form of the conformal
deformation of time is establish... | gr-qc | the description of the cosmological expansion and its possible local manifestations via treating the proper conformal transformations as a coordinate transformation from a comoving lorentz reference frame rf to an uniformly accelerated rf is given the explicit form of the conformal deformation of time is established th... | [['the', 'description', 'of', 'the', 'cosmological', 'expansion', 'and', 'its', 'possible', 'local', 'manifestations', 'via', 'treating', 'the', 'proper', 'conformal', 'transformations', 'as', 'a', 'coordinate', 'transformation', 'from', 'a', 'comoving', 'lorentz', 'reference', 'frame', 'rf', 'to', 'an', 'uniformly', '... | [-0.13774451211709796, 0.1094002390837586, -0.09718197638655758, 0.04700968296681508, -0.09789876917457324, -0.11188049609527777, 0.0014006539511674811, 0.319584453853881, -0.280870600258174, -0.2615183214322802, 0.05101994968534104, -0.23158288679785277, -0.10542579119319445, 0.19204995218156415, 0.0010500122797474907... |
710.3995 | The Hubble constant and dark energy from cosmological distance measures | We study how the determination of the Hubble constant from cosmological
distance measures is affected by models of dark energy and vice versa. For this
purpose, constraints on the Hubble constant and dark energy are investigated
using the cosmological observations of cosmic microwave background, baryon
acoustic oscil... | astro-ph | we study how the determination of the hubble constant from cosmological distance measures is affected by models of dark energy and vice versa for this purpose constraints on the hubble constant and dark energy are investigated using the cosmological observations of cosmic microwave background baryon acoustic oscillatio... | [['we', 'study', 'how', 'the', 'determination', 'of', 'the', 'hubble', 'constant', 'from', 'cosmological', 'distance', 'measures', 'is', 'affected', 'by', 'models', 'of', 'dark', 'energy', 'and', 'vice', 'versa', 'for', 'this', 'purpose', 'constraints', 'on', 'the', 'hubble', 'constant', 'and', 'dark', 'energy', 'are',... | [-0.13450484553036923, 0.15059905313418723, -0.0832038879329663, 0.14413368617895694, -0.16593068268205693, -0.12144120349849931, 0.015807698232895552, 0.34600301572487724, -0.25758670282953267, -0.3390820277825841, 0.10192823565486281, -0.22112159962436898, -0.05025100972693395, 0.20284523979693522, -0.014588767871149... |
710.3996 | Universal quantum computation with electronic qubits in decoherence-free
subspace | We investigate how to carry out universal quantum computation
deterministically with free electrons in decoherence-free subspace by using
polarizing beam splitters, charge detectors, and single-spin rotations. Quantum
information in our case is encoded in spin degrees of freedom of the
electron-pairs which construct ... | quant-ph | we investigate how to carry out universal quantum computation deterministically with free electrons in decoherencefree subspace by using polarizing beam splitters charge detectors and singlespin rotations quantum information in our case is encoded in spin degrees of freedom of the electronpairs which construct a decohe... | [['we', 'investigate', 'how', 'to', 'carry', 'out', 'universal', 'quantum', 'computation', 'deterministically', 'with', 'free', 'electrons', 'in', 'decoherencefree', 'subspace', 'by', 'using', 'polarizing', 'beam', 'splitters', 'charge', 'detectors', 'and', 'singlespin', 'rotations', 'quantum', 'information', 'in', 'ou... | [-0.17739045662404615, 0.21896809194519928, -0.06829068489679241, -0.010021164211668546, -0.010486844974228098, -0.24792250978489278, 0.06533469223782798, 0.4160246467099914, -0.2750287095108364, -0.23148133056356182, 0.03603411176465923, -0.21895992079207413, -0.10492095533283899, 0.22363823232582852, -0.0477894264198... |
710.3997 | Reversibility in the group of homeomorphisms of the circle | We identify those elements of the homeomorphism group of the circle that can
be expressed as a composite of two involutions.
| math.DS | we identify those elements of the homeomorphism group of the circle that can be expressed as a composite of two involutions | [['we', 'identify', 'those', 'elements', 'of', 'the', 'homeomorphism', 'group', 'of', 'the', 'circle', 'that', 'can', 'be', 'expressed', 'as', 'a', 'composite', 'of', 'two', 'involutions']] | [-0.23359875611606098, 0.14047326285037257, -0.09425300271028564, 0.04978129507175514, -0.04451075342616865, -0.08230272935526002, 0.03565917714011101, 0.3652025354760034, -0.34655676569257465, -0.29539880498001975, 0.13465923627483703, -0.3070669863373041, -0.1571305560923758, 0.1879484240586559, -0.11855378511938311,... |
710.3998 | Charged Lepton Flavour Violation in Littlest Higgs model with T-parity | The Little Higgs model with T-parity (LHT) belongs to the non-minimal flavour
violating model. This model has new sources of flavour and CP violation both in
quark and leptonic sectors. These new sources of flavour violation originates
by the interaction of Standard Model (SM) fermions with heavy gauge bosons and
hea... | hep-ph | the little higgs model with tparity lht belongs to the nonminimal flavour violating model this model has new sources of flavour and cp violation both in quark and leptonic sectors these new sources of flavour violation originates by the interaction of standard model sm fermions with heavy gauge bosons and heavy or mirr... | [['the', 'little', 'higgs', 'model', 'with', 'tparity', 'lht', 'belongs', 'to', 'the', 'nonminimal', 'flavour', 'violating', 'model', 'this', 'model', 'has', 'new', 'sources', 'of', 'flavour', 'and', 'cp', 'violation', 'both', 'in', 'quark', 'and', 'leptonic', 'sectors', 'these', 'new', 'sources', 'of', 'flavour', 'vio... | [-0.09567761548954111, 0.32466311610034226, 0.003188640988235803, 0.1806956979685071, -0.14035701955129443, -0.2831639325687368, 0.10536701540695503, 0.2754123662843516, -0.18640926841793484, -0.2853013342246413, -0.04079688927863332, -0.30691708205880497, 0.0055471622403466, -0.004429461584598022, 0.029218504327888552... |
710.3999 | WD0433+270: an old Hyades stream member or an Fe-core white dwarf? | G39-27/289 is a common proper motion pair formed by a white dwarf
(WD0433+270) and a main-sequence star (BD+26 730) that apparently has been
classified as a member of the Hyades open cluster. Previous studies of the
white dwarf component yielded a cooling time of ~4 Gyr. Although it has not
been pointed out before ex... | astro-ph | g3927289 is a common proper motion pair formed by a white dwarf wd0433270 and a mainsequence star bd26 730 that apparently has been classified as a member of the hyades open cluster previous studies of the white dwarf component yielded a cooling time of 4 gyr although it has not been pointed out before explicitly this ... | [['g3927289', 'is', 'a', 'common', 'proper', 'motion', 'pair', 'formed', 'by', 'a', 'white', 'dwarf', 'wd0433270', 'and', 'a', 'mainsequence', 'star', 'bd26', '730', 'that', 'apparently', 'has', 'been', 'classified', 'as', 'a', 'member', 'of', 'the', 'hyades', 'open', 'cluster', 'previous', 'studies', 'of', 'the', 'whi... | [-0.06061432043659604, 0.14058832706472862, -0.12395461171917203, 0.08456294606396653, -0.12166027213722744, -0.10027476249918066, 0.09933831688033899, 0.40346527603213433, -0.18195017261853166, -0.3406332441088226, 0.05340613194189414, -0.2766134758553192, -0.05658968069625121, 0.1926268355325899, -0.08478980318527815... |
710.4 | Exact Solutions of Diffusion-Convection Equations | In the presented paper known (up to the beginning of 2008) Lie- and non-Lie
exact solutions of different $(1+1)$-dimensional diffusion-convection equations
of form $f(x)u_t=(g(x)A(u)u_x)_x+h(x)B(u)u_x$ are collected.
| math-ph math.MP | in the presented paper known up to the beginning of 2008 lie and nonlie exact solutions of different 11dimensional diffusionconvection equations of form fxu_tgxauu_x_xhxbuu_x are collected | [['in', 'the', 'presented', 'paper', 'known', 'up', 'to', 'the', 'beginning', 'of', '2008', 'lie', 'and', 'nonlie', 'exact', 'solutions', 'of', 'different', '11dimensional', 'diffusionconvection', 'equations', 'of', 'form', 'fxu_tgxauu_x_xhxbuu_x', 'are', 'collected']] | [-0.1464884400439377, 0.04226459928143483, -0.03250127486311472, 0.01574489212809847, -0.12189253118748848, -0.11199879689285389, -0.06228473393443542, 0.2530453456644094, -0.21268242619072014, -0.3472910365806176, 0.12453688617992717, -0.29131787241651463, -0.14782422322493333, 0.19028515529890472, -0.0265443390235304... |
710.4001 | Fluctuation induces evolutionary branching in a modeled microbial
ecosystem | The impact of environmental fluctuation on species diversity is studied with
a model of the evolutionary ecology of microorganisms. We show that
environmental fluctuation induces evolutionary branching and assures the
consequential coexistence of multiple species. Pairwise invasibility analysis
is applied to illustra... | q-bio.PE | the impact of environmental fluctuation on species diversity is studied with a model of the evolutionary ecology of microorganisms we show that environmental fluctuation induces evolutionary branching and assures the consequential coexistence of multiple species pairwise invasibility analysis is applied to illustrate t... | [['the', 'impact', 'of', 'environmental', 'fluctuation', 'on', 'species', 'diversity', 'is', 'studied', 'with', 'a', 'model', 'of', 'the', 'evolutionary', 'ecology', 'of', 'microorganisms', 'we', 'show', 'that', 'environmental', 'fluctuation', 'induces', 'evolutionary', 'branching', 'and', 'assures', 'the', 'consequent... | [-0.14193662420850914, 0.19368395269057662, -0.13038079999387264, 0.14527647658641793, -0.0012093738846059114, -0.075649969552134, 0.08500197513977874, 0.3437002723649988, -0.272203442693319, -0.2655510149614991, 0.00871270663052235, -0.2380344912515215, -0.22235603363446468, 0.08860479229248462, -0.06589698413703239, ... |
710.4002 | Chow--Kuenneth decomposition for special varieties | In this paper we investigate Murre's conjecture on the Chow--K\"unneth
decomposition for two classes of examples. We look at the universal families of
smooth curves over spaces which dominate the moduli space $\cM_g$, in genus at
most 8 and show existence of a Chow--K\"unneth decomposition. The second class
of exampl... | math.AG math.AC | in this paper we investigate murres conjecture on the chowkunneth decomposition for two classes of examples we look at the universal families of smooth curves over spaces which dominate the moduli space cm_g in genus at most 8 and show existence of a chowkunneth decomposition the second class of examples include the re... | [['in', 'this', 'paper', 'we', 'investigate', 'murres', 'conjecture', 'on', 'the', 'chowkunneth', 'decomposition', 'for', 'two', 'classes', 'of', 'examples', 'we', 'look', 'at', 'the', 'universal', 'families', 'of', 'smooth', 'curves', 'over', 'spaces', 'which', 'dominate', 'the', 'moduli', 'space', 'cm_g', 'in', 'genu... | [-0.1863718237138436, 0.03731279127606297, -0.13957750935201782, 0.08961295055172441, -0.06256931390660474, -0.09202230905618848, -0.028193172325285835, 0.32537847687785004, -0.3475755859310798, -0.22350217903598765, 0.11921594986733332, -0.21469561294416745, -0.17043950243652622, 0.24512198491941525, -0.16350167579477... |
710.4003 | YREC: The Yale Rotating Stellar Evolution Code | The stellar evolution code YREC is outlined with emphasis on its applications
to helio- and asteroseismology. The procedure for calculating calibrated solar
and stellar models is described. Other features of the code such as a non-local
treatment of convective core overshoot, and the implementation of a
parametrized ... | astro-ph | the stellar evolution code yrec is outlined with emphasis on its applications to helio and asteroseismology the procedure for calculating calibrated solar and stellar models is described other features of the code such as a nonlocal treatment of convective core overshoot and the implementation of a parametrized descrip... | [['the', 'stellar', 'evolution', 'code', 'yrec', 'is', 'outlined', 'with', 'emphasis', 'on', 'its', 'applications', 'to', 'helio', 'and', 'asteroseismology', 'the', 'procedure', 'for', 'calculating', 'calibrated', 'solar', 'and', 'stellar', 'models', 'is', 'described', 'other', 'features', 'of', 'the', 'code', 'such', ... | [-0.039177992340410125, 0.11430277060717345, -0.041648672852898014, 0.14149125510302837, -0.06691194996237755, -0.11288334972341545, -0.046304079914989416, 0.37471559215337036, -0.21272408406366594, -0.3411462270189077, 0.1459011985018151, -0.22607862642034887, -0.10473106340505182, 0.28824767988116945, -0.046955606091... |
710.4004 | The N-Vortex Problem on a Symmetric Ellipsoid: A Perturbation Approach | We consider the N-vortex problem on a ellipsoid of revolution. Applying
standard techniques of classical perturbation theory we construct a sequence of
conformal transformations from the ellipsoid into the complex plane. Using
these transformations the equations of motion for the N-vortex problem on the
ellipsoid are... | math.DS | we consider the nvortex problem on a ellipsoid of revolution applying standard techniques of classical perturbation theory we construct a sequence of conformal transformations from the ellipsoid into the complex plane using these transformations the equations of motion for the nvortex problem on the ellipsoid are writt... | [['we', 'consider', 'the', 'nvortex', 'problem', 'on', 'a', 'ellipsoid', 'of', 'revolution', 'applying', 'standard', 'techniques', 'of', 'classical', 'perturbation', 'theory', 'we', 'construct', 'a', 'sequence', 'of', 'conformal', 'transformations', 'from', 'the', 'ellipsoid', 'into', 'the', 'complex', 'plane', 'using'... | [-0.16216003387066794, 0.01679045319871371, -0.10079668442079101, 0.04688394629166473, -0.060791792942727185, -0.035380304504904043, -0.05450916547799505, 0.3363987907587764, -0.2874549116310944, -0.24736875134060182, 0.1508641451364383, -0.28092469885406723, -0.17260473451565905, 0.2199084164956248, -0.048825251735208... |
710.4005 | Dynamo quenching due to shear flow | We provide a theory of dynamo ($\alpha$ effect) and momentum transport in
three-dimensional magnetohydrodynamics. For the first time, we show that the
$\alpha$ effect is severely reduced by the shear even in the absence of
magnetic field. The $\alpha$ effect is further suppressed by magnetic fields
well below equipar... | physics.flu-dyn astro-ph | we provide a theory of dynamo alpha effect and momentum transport in threedimensional magnetohydrodynamics for the first time we show that the alpha effect is severely reduced by the shear even in the absence of magnetic field the alpha effect is further suppressed by magnetic fields well below equipartition with the l... | [['we', 'provide', 'a', 'theory', 'of', 'dynamo', 'alpha', 'effect', 'and', 'momentum', 'transport', 'in', 'threedimensional', 'magnetohydrodynamics', 'for', 'the', 'first', 'time', 'we', 'show', 'that', 'the', 'alpha', 'effect', 'is', 'severely', 'reduced', 'by', 'the', 'shear', 'even', 'in', 'the', 'absence', 'of', '... | [-0.1552198455447994, 0.24570866051856113, -0.029596894560801064, 0.04927146517557202, -0.04052761029767788, -0.0350169448450334, -0.025242585749010223, 0.31807275645245436, -0.27709247467060716, -0.3500195907239439, 0.06260812426108267, -0.17873776183311701, -0.11213516711920374, 0.2505078717782083, 0.0494752232048471... |
710.4006 | Critical Temperature for Bose-Einstein condensation in quartic
potentials | The quartic confining potential has emerged as a key ingredient to obtain
fast rotating vortices in BEC as well as observation of quantum phase
transitions in optical lattices. We calculate the critical temperature $T_c$ of
bosons at which normal to BEC transition occurs for the quartic confining
potential. Further m... | physics.atom-ph cond-mat.other cond-mat.stat-mech | the quartic confining potential has emerged as a key ingredient to obtain fast rotating vortices in bec as well as observation of quantum phase transitions in optical lattices we calculate the critical temperature t_c of bosons at which normal to bec transition occurs for the quartic confining potential further more we... | [['the', 'quartic', 'confining', 'potential', 'has', 'emerged', 'as', 'a', 'key', 'ingredient', 'to', 'obtain', 'fast', 'rotating', 'vortices', 'in', 'bec', 'as', 'well', 'as', 'observation', 'of', 'quantum', 'phase', 'transitions', 'in', 'optical', 'lattices', 'we', 'calculate', 'the', 'critical', 'temperature', 't_c'... | [-0.144673018456872, 0.24919109857317223, -0.03210864684281304, 0.04399560935385323, -0.03773441073565703, -0.19290947414549958, 0.05647223342321408, 0.31376429064118344, -0.20503040295823113, -0.2761303934410376, 0.01119750918967285, -0.3014496894674781, -0.12015776174223941, 0.19875231415220618, 0.0331053510282958, 0... |
710.4007 | Dynamics of horizontal-like maps in higher dimension | We study the regularity of the Green currents and of the equilibrium measure
associated to a horizontal-like map in C^k, under a natural assumption on the
dynamical degrees. We estimate the speed of convergence towards the Green
currents, the decay of correlations for the equilibrium measure and the
Lyapounov exponen... | math.DS math.CV | we study the regularity of the green currents and of the equilibrium measure associated to a horizontallike map in ck under a natural assumption on the dynamical degrees we estimate the speed of convergence towards the green currents the decay of correlations for the equilibrium measure and the lyapounov exponents we s... | [['we', 'study', 'the', 'regularity', 'of', 'the', 'green', 'currents', 'and', 'of', 'the', 'equilibrium', 'measure', 'associated', 'to', 'a', 'horizontallike', 'map', 'in', 'ck', 'under', 'a', 'natural', 'assumption', 'on', 'the', 'dynamical', 'degrees', 'we', 'estimate', 'the', 'speed', 'of', 'convergence', 'towards'... | [-0.17807311607818854, 0.1032097418498444, -0.09489648957785807, 0.10895445770951674, 0.0035602330548786805, -0.04669375728056031, 0.0339718487554867, 0.3612858899881279, -0.2950105625547861, -0.16393586426581208, 0.12770556208836895, -0.27465652593068385, -0.1484762348914764, 0.1757288072552336, -0.03784990364520605, ... |
710.4008 | Scale-free networks resistant to intentional attacks | We study the detailed mechanism of the failure of scale-free networks under
intentional attacks. Although it is generally accepted that such networks are
very sensitive to targeted attacks, we show that for a particular type of
structure such networks surprisingly remain very robust even under removal of a
large frac... | physics.soc-ph | we study the detailed mechanism of the failure of scalefree networks under intentional attacks although it is generally accepted that such networks are very sensitive to targeted attacks we show that for a particular type of structure such networks surprisingly remain very robust even under removal of a large fraction ... | [['we', 'study', 'the', 'detailed', 'mechanism', 'of', 'the', 'failure', 'of', 'scalefree', 'networks', 'under', 'intentional', 'attacks', 'although', 'it', 'is', 'generally', 'accepted', 'that', 'such', 'networks', 'are', 'very', 'sensitive', 'to', 'targeted', 'attacks', 'we', 'show', 'that', 'for', 'a', 'particular',... | [-0.12718691070424928, 0.10014892851628748, -0.0625350711513953, 0.06548865723768892, -0.02990109134925765, -0.15780427721436083, 0.057230339765591526, 0.38581684330242805, -0.27113838965640585, -0.32336746887892653, 0.08430464006826581, -0.289394135706678, -0.22842019847353343, 0.1719278216458343, -0.02446012735238363... |
710.4009 | The congruence kernel of an arithmetic lattice in a rank one algebraic
group over a local field | Let k be a global field and let k_v be the completion of k with respect to v,
a non-archimedean place of k. Let \mathbf{G} be a connected, simply-connected
algebraic group over k, which is absolutely almost simple of k_v-rank 1. Let
G=\mathbf{G}(k_v). Let \Gamma be an arithmetic lattice in G and let C=C(\Gamma)
be it... | math.GR math.NT | let k be a global field and let k_v be the completion of k with respect to v a nonarchimedean place of k let mathbfg be a connected simplyconnected algebraic group over k which is absolutely almost simple of k_vrank 1 let gmathbfgk_v let gamma be an arithmetic lattice in g and let ccgamma be its congruence kernel lubot... | [['let', 'k', 'be', 'a', 'global', 'field', 'and', 'let', 'k_v', 'be', 'the', 'completion', 'of', 'k', 'with', 'respect', 'to', 'v', 'a', 'nonarchimedean', 'place', 'of', 'k', 'let', 'mathbfg', 'be', 'a', 'connected', 'simplyconnected', 'algebraic', 'group', 'over', 'k', 'which', 'is', 'absolutely', 'almost', 'simple',... | [-0.188602431822801, 0.10648901033761436, -0.1275054676989752, -0.027814875217507397, -0.09753021803411721, -0.14240034591321918, 0.004822899525129058, 0.32988282548019077, -0.31772449963392146, -0.22801489603260033, 0.09837297525437963, -0.2569089793515476, -0.09807538568286808, 0.22817289151458275, -0.084290824607108... |
710.401 | A stochastic theory for temporal fluctuations in self-organized critical
systems | A stochastic theory for the toppling activity in sandpile models is
developed, based on a simple mean-field assumption about the toppling process.
The theory describes the process as an anti-persistent Gaussian walk, where the
diffusion coefficient is proportional to the activity. It is formulated as a
generalization... | q-fin.ST nlin.AO nlin.CG | a stochastic theory for the toppling activity in sandpile models is developed based on a simple meanfield assumption about the toppling process the theory describes the process as an antipersistent gaussian walk where the diffusion coefficient is proportional to the activity it is formulated as a generalization of the ... | [['a', 'stochastic', 'theory', 'for', 'the', 'toppling', 'activity', 'in', 'sandpile', 'models', 'is', 'developed', 'based', 'on', 'a', 'simple', 'meanfield', 'assumption', 'about', 'the', 'toppling', 'process', 'the', 'theory', 'describes', 'the', 'process', 'as', 'an', 'antipersistent', 'gaussian', 'walk', 'where', '... | [-0.07201005202767095, 0.11559073615154423, -0.11361242944472714, 0.07676177884198918, -0.05296533945947886, -0.12126792956229397, 0.03198135139445137, 0.3197923016783438, -0.32281251006612655, -0.21687312157530533, 0.10189614298655407, -0.2795750896593458, -0.19258373599303397, 0.1415229940198754, -0.07057155756966065... |
710.4011 | Counting BPS Solitons and Applications | We propose a novel and simple method of computing the volume of the moduli
space of BPS solitons in supersymmetric gauge theory. We use a D-brane
realization of vortices and T-duality relation to domain walls. We there use a
special limit where domain walls reduce to gas of hard (soft) one-dimensional
rods for the Ab... | hep-th | we propose a novel and simple method of computing the volume of the moduli space of bps solitons in supersymmetric gauge theory we use a dbrane realization of vortices and tduality relation to domain walls we there use a special limit where domain walls reduce to gas of hard soft onedimensional rods for the abelian non... | [['we', 'propose', 'a', 'novel', 'and', 'simple', 'method', 'of', 'computing', 'the', 'volume', 'of', 'the', 'moduli', 'space', 'of', 'bps', 'solitons', 'in', 'supersymmetric', 'gauge', 'theory', 'we', 'use', 'a', 'dbrane', 'realization', 'of', 'vortices', 'and', 'tduality', 'relation', 'to', 'domain', 'walls', 'we', '... | [-0.1459946871206931, 0.11931250249378171, -0.06918835116005471, 0.0541025721943196, -0.09635945503935725, -0.08819648089064729, 0.05996733285458188, 0.3459168182635287, -0.21082182182315864, -0.2539897572825707, 0.10955926782505422, -0.23992583734224088, -0.14114419301357248, 0.1731294814503568, -0.07160509622902894, ... |
710.4012 | Experimental and First principle calculation of Co_xNi_{(1-x)}Si solid
solution structural stability | We report the investigation of the structural stability of
Co$_{(1-x)}$Ni$_x$Si monosilicides for $0<x<1$. As CoSi crystallizes in the
FeSi-type structure (B20) and NiSi is stable in the MnP-type structure (B31), a
complete set of samples has been synthesized and a systematic study of phase
formation under different ... | cond-mat.mtrl-sci cond-mat.other | we report the investigation of the structural stability of co_1xni_xsi monosilicides for 0x1 as cosi crystallizes in the fesitype structure b20 and nisi is stable in the mnptype structure b31 a complete set of samples has been synthesized and a systematic study of phase formation under different annealing conditions we... | [['we', 'report', 'the', 'investigation', 'of', 'the', 'structural', 'stability', 'of', 'co_1xni_xsi', 'monosilicides', 'for', '0x1', 'as', 'cosi', 'crystallizes', 'in', 'the', 'fesitype', 'structure', 'b20', 'and', 'nisi', 'is', 'stable', 'in', 'the', 'mnptype', 'structure', 'b31', 'a', 'complete', 'set', 'of', 'sampl... | [-0.1262811766017206, 0.10472989404674418, -0.09226850949752027, 0.0008715915258048091, -0.00765067057734255, -0.03909192210855241, 0.09802666901886842, 0.39453473815437917, -0.23360343036885947, -0.31964522949838176, 0.0895967452381152, -0.30319298984494036, -0.12567209058112191, 0.127953107056102, 0.07623115236017697... |
710.4013 | Screened Coulomb interaction in the maximally localized Wannier basis | We discuss a maximally localized Wannier function approach for constructing
lattice models from first-principles electronic structure calculations, where
the effective Coulomb interactions are calculated in the constrained
random-phase-approximation. The method is applied to the 3d transition metals
and a perovskite ... | cond-mat.str-el | we discuss a maximally localized wannier function approach for constructing lattice models from firstprinciples electronic structure calculations where the effective coulomb interactions are calculated in the constrained randomphaseapproximation the method is applied to the 3d transition metals and a perovskite srvo_3 ... | [['we', 'discuss', 'a', 'maximally', 'localized', 'wannier', 'function', 'approach', 'for', 'constructing', 'lattice', 'models', 'from', 'firstprinciples', 'electronic', 'structure', 'calculations', 'where', 'the', 'effective', 'coulomb', 'interactions', 'are', 'calculated', 'in', 'the', 'constrained', 'randomphaseappr... | [-0.07446778645472867, 0.15943577638162035, -0.0670541559254551, 0.14204125753936492, 0.0015432244698916162, -0.15968050393941147, 0.10810861589520106, 0.4517287194196667, -0.2741873840668372, -0.20537362404699835, -0.009771290582804276, -0.3254348013550043, -0.2261881044666682, 0.11473029275491302, 0.07892789226690573... |
710.4014 | Dynamic Control of Laser Produced Proton Beams | The emission characteristics of intense laser driven protons are controlled
using ultra-strong (of the order of 10^9 V/m) electrostatic fields varying on a
few ps timescale. The field structures are achieved by exploiting the high
potential of the target (reaching multi-MV during the laser interaction).
Suitably shap... | physics.plasm-ph physics.acc-ph | the emission characteristics of intense laser driven protons are controlled using ultrastrong of the order of 109 vm electrostatic fields varying on a few ps timescale the field structures are achieved by exploiting the high potential of the target reaching multimv during the laser interaction suitably shaped targets r... | [['the', 'emission', 'characteristics', 'of', 'intense', 'laser', 'driven', 'protons', 'are', 'controlled', 'using', 'ultrastrong', 'of', 'the', 'order', 'of', '109', 'vm', 'electrostatic', 'fields', 'varying', 'on', 'a', 'few', 'ps', 'timescale', 'the', 'field', 'structures', 'are', 'achieved', 'by', 'exploiting', 'th... | [-0.1325864512188013, 0.18767935081054662, -0.03508286714079041, 0.047384038951028794, -0.019760118350021394, -0.10492572632924124, -0.0010751713633391203, 0.4474129163313146, -0.23157115382891075, -0.3655540737159112, 0.03663522354897806, -0.24889725910536215, 0.0017386961125713937, 0.22453286653092386, -0.01819202647... |
710.4015 | A new extended KP hierarchy | A method is proposed to construct a new extended KP hierarchy, which includes
two types of KP equation with self-consistent sources and admits reductions to
k-constrained KP hierarchy and to Gelfand-Dickey hierarchy with sources. It
provides a general way to construct soliton equations with sources and their
Lax repr... | nlin.SI | a method is proposed to construct a new extended kp hierarchy which includes two types of kp equation with selfconsistent sources and admits reductions to kconstrained kp hierarchy and to gelfanddickey hierarchy with sources it provides a general way to construct soliton equations with sources and their lax representat... | [['a', 'method', 'is', 'proposed', 'to', 'construct', 'a', 'new', 'extended', 'kp', 'hierarchy', 'which', 'includes', 'two', 'types', 'of', 'kp', 'equation', 'with', 'selfconsistent', 'sources', 'and', 'admits', 'reductions', 'to', 'kconstrained', 'kp', 'hierarchy', 'and', 'to', 'gelfanddickey', 'hierarchy', 'with', 's... | [-0.11930357451949801, 0.00556288139742552, -0.10767392205948732, 0.15578132270293651, -0.1748068093569303, -0.1922184374202423, 0.006470211610502126, 0.31834028068245673, -0.3086261945795648, -0.3503774697227137, 0.02908531203866005, -0.28911497276656484, -0.14811154743846583, 0.1610266412323227, 0.028282569322202886,... |
710.4016 | Equicontinuous Geodesic Flows | The author shows that equicontinuous geodesic flows on surfaces are periodic.
A similar result for flows on 3-manifolds is also proven. The idea of the proof
is to show that the return map is recurrent and therefore periodic.
| math.DS math.DG | the author shows that equicontinuous geodesic flows on surfaces are periodic a similar result for flows on 3manifolds is also proven the idea of the proof is to show that the return map is recurrent and therefore periodic | [['the', 'author', 'shows', 'that', 'equicontinuous', 'geodesic', 'flows', 'on', 'surfaces', 'are', 'periodic', 'a', 'similar', 'result', 'for', 'flows', 'on', '3manifolds', 'is', 'also', 'proven', 'the', 'idea', 'of', 'the', 'proof', 'is', 'to', 'show', 'that', 'the', 'return', 'map', 'is', 'recurrent', 'and', 'theref... | [-0.20621652107097602, 0.09997769026085734, -0.1405423216423706, 0.12394931823885265, -0.06912118929291242, -0.12260163633005791, -0.020460515319810885, 0.38555798326667984, -0.2713788245853625, -0.1815334224191151, 0.1636478628865198, -0.3119826656521151, -0.21735512099755733, 0.3019334621433365, -0.1792256590224018, ... |
710.4017 | Eta and Eta' physics | This talk describes the reasons why $\eta$ and $\eta^\prime$ decays are an
interesting topic of study for both theory and experiment. The main part
discusses the results of the recent calculation of $\eta\to3\pi$ at two-loop
order in ChPT. Some puzzling aspects of the results compared to earlier
dispersive calculatio... | nucl-th hep-ph | this talk describes the reasons why eta and etaprime decays are an interesting topic of study for both theory and experiment the main part discusses the results of the recent calculation of etato3pi at twoloop order in chpt some puzzling aspects of the results compared to earlier dispersive calculations are highlighted... | [['this', 'talk', 'describes', 'the', 'reasons', 'why', 'eta', 'and', 'etaprime', 'decays', 'are', 'an', 'interesting', 'topic', 'of', 'study', 'for', 'both', 'theory', 'and', 'experiment', 'the', 'main', 'part', 'discusses', 'the', 'results', 'of', 'the', 'recent', 'calculation', 'of', 'etato3pi', 'at', 'twoloop', 'or... | [-0.07973786027702902, 0.12890591891004338, -0.10397943888175568, 0.1247073672029988, -0.08491576372512749, -0.10654295020337616, 0.02110589718213305, 0.2818736596032977, -0.16673884193712313, -0.24333508139742271, 0.041426691018776704, -0.3830136035169874, -0.17199189734778234, 0.1645115014340263, -0.00151663799104946... |
710.4018 | Correcting \alpha_3(M_Z) in the NMSGUT | We show that superheavy threshold corrections in the New Minimal
Supersymmetric GUT based on the SO(10) Higgs system ${\bf{210\oplus 126\oplus
{\bar {126}}\oplus 10 \oplus 120}} $ can comfortably correct the prediction for
the value of $\alpha_3(M_Z)$ from the relatively large value predicted by the
two loop RG equat... | hep-ph | we show that superheavy threshold corrections in the new minimal supersymmetric gut based on the so10 higgs system bf210oplus 126oplus bar 126oplus 10 oplus 120 can comfortably correct the prediction for the value of alpha_3m_z from the relatively large value predicted by the two loop rg equations to the central value ... | [['we', 'show', 'that', 'superheavy', 'threshold', 'corrections', 'in', 'the', 'new', 'minimal', 'supersymmetric', 'gut', 'based', 'on', 'the', 'so10', 'higgs', 'system', 'bf210oplus', '126oplus', 'bar', '126oplus', '10', 'oplus', '120', 'can', 'comfortably', 'correct', 'the', 'prediction', 'for', 'the', 'value', 'of',... | [-0.10909459487379838, 0.18371598946551482, -0.002523062778636813, 0.11857365688464294, -0.05236335491761565, -0.14040491943868497, 0.06614096719150742, 0.28457642608011763, -0.21018627328177295, -0.3322310632963975, 0.1175632216486459, -0.22440982790042957, -0.019955430272966625, 0.17191379251579444, -0.03436973178138... |
710.4019 | A principal component analysis approach to the morphology of Planetary
Nebulae | Principal Component Analysis (PCA) is a well-known technique used to
decorrelate a set of vectors. It has been applied to explore the star formation
history of galaxies or to determine distances of mass-lossing stars. Here we
apply PCA to the optical data of Planetary Nebulae (PNe) with the aim of
extracting informat... | astro-ph | principal component analysis pca is a wellknown technique used to decorrelate a set of vectors it has been applied to explore the star formation history of galaxies or to determine distances of masslossing stars here we apply pca to the optical data of planetary nebulae pne with the aim of extracting information about ... | [['principal', 'component', 'analysis', 'pca', 'is', 'a', 'wellknown', 'technique', 'used', 'to', 'decorrelate', 'a', 'set', 'of', 'vectors', 'it', 'has', 'been', 'applied', 'to', 'explore', 'the', 'star', 'formation', 'history', 'of', 'galaxies', 'or', 'to', 'determine', 'distances', 'of', 'masslossing', 'stars', 'her... | [-0.04899846600719838, 0.06531337079631759, -0.0883216995951104, 0.05683171708320299, -0.06444118912567304, -0.10362665794254083, 0.03666444679809008, 0.4198536494602765, -0.16987577825784683, -0.34580426567068356, 0.04487479010930332, -0.2852697572808997, -0.0454904626457068, 0.1851449897493062, -0.05514135912368548, ... |
710.402 | Dice and Pulsars | The pulse sequence is interpreted as a realization of a random electron
discharge process in a vacuum gap over the polar cap (PC) - the open magnetic
force line region on the neutron star surface. This point of view is
illustrated by an example based on the dice. The generators of the random
numbers are a cube and a ... | astro-ph | the pulse sequence is interpreted as a realization of a random electron discharge process in a vacuum gap over the polar cap pc the open magnetic force line region on the neutron star surface this point of view is illustrated by an example based on the dice the generators of the random numbers are a cube and a coin thr... | [['the', 'pulse', 'sequence', 'is', 'interpreted', 'as', 'a', 'realization', 'of', 'a', 'random', 'electron', 'discharge', 'process', 'in', 'a', 'vacuum', 'gap', 'over', 'the', 'polar', 'cap', 'pc', 'the', 'open', 'magnetic', 'force', 'line', 'region', 'on', 'the', 'neutron', 'star', 'surface', 'this', 'point', 'of', '... | [-0.1293421562002077, 0.16710817508638276, -0.10380994554931723, 0.03202433315503393, -0.033279594972612354, -0.11192833411133313, 0.10656183127288187, 0.38414633708206686, -0.2441201086236736, -0.28030803452033226, 0.11979046471116286, -0.2692061085858947, -0.05050930945481372, 0.22331070252712523, -0.0589596705869166... |
710.4021 | Flat-brane Compactifications in Supergravity Induced by Scalars | We discuss flat compactifications of supergravities in diverse dimensions in
the presence of branes. The compactification is induced by the scalar fields of
supergravity and it is such that there is no relic cosmological constant on the
brane, rendering this way the latter flat. We discuss in particular the D=4,
$N=2... | hep-th | we discuss flat compactifications of supergravities in diverse dimensions in the presence of branes the compactification is induced by the scalar fields of supergravity and it is such that there is no relic cosmological constant on the brane rendering this way the latter flat we discuss in particular the d4 n24 and d8 ... | [['we', 'discuss', 'flat', 'compactifications', 'of', 'supergravities', 'in', 'diverse', 'dimensions', 'in', 'the', 'presence', 'of', 'branes', 'the', 'compactification', 'is', 'induced', 'by', 'the', 'scalar', 'fields', 'of', 'supergravity', 'and', 'it', 'is', 'such', 'that', 'there', 'is', 'no', 'relic', 'cosmologica... | [-0.20105977495671204, 0.19618888049026822, 0.00936061449090738, 0.10032688935015277, -0.10052746048861064, -0.1620592295219845, -0.06740834809480106, 0.30530452254772333, -0.13886548346369573, -0.24436186240654034, 0.1194862254288988, -0.29013852213537045, -0.1343596480454844, 0.08575861940695213, -0.08756936906484224... |
710.4022 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume I | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4023 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume II(a) | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4024 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume II(b) | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4025 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume III | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4026 | Scalar Field with Robin Boundary Conditions in the Worldline Formalism | The worldline formalism has been widely used to compute physical quantities
in quantum field theory. However, applications of this formalism to quantum
fields in the presence of boundaries have been studied only recently. In this
article we show how to compute in the worldline approach the heat kernel
expansion for a... | hep-th | the worldline formalism has been widely used to compute physical quantities in quantum field theory however applications of this formalism to quantum fields in the presence of boundaries have been studied only recently in this article we show how to compute in the worldline approach the heat kernel expansion for a scal... | [['the', 'worldline', 'formalism', 'has', 'been', 'widely', 'used', 'to', 'compute', 'physical', 'quantities', 'in', 'quantum', 'field', 'theory', 'however', 'applications', 'of', 'this', 'formalism', 'to', 'quantum', 'fields', 'in', 'the', 'presence', 'of', 'boundaries', 'have', 'been', 'studied', 'only', 'recently', ... | [-0.12075218663925362, 0.10268718051272877, -0.10272409221800716, 0.04542460278775927, -0.10428885133821786, -0.09868577588349581, -0.029805009624171888, 0.36069660858471986, -0.2288091429269191, -0.23667298253510416, 0.09882958366213962, -0.23520406487292236, -0.18020805683150196, 0.17161564259626663, -0.0301714591662... |
710.4027 | Ultra-Peripheral Collisions at RHIC | This presentation summarizes the results on ultra-peripheral collisions
obtained at RHIC. It also discusses some aspects of the corresponding
electromagnetic interactions in pp and pbarp collisions.
| hep-ph | this presentation summarizes the results on ultraperipheral collisions obtained at rhic it also discusses some aspects of the corresponding electromagnetic interactions in pp and pbarp collisions | [['this', 'presentation', 'summarizes', 'the', 'results', 'on', 'ultraperipheral', 'collisions', 'obtained', 'at', 'rhic', 'it', 'also', 'discusses', 'some', 'aspects', 'of', 'the', 'corresponding', 'electromagnetic', 'interactions', 'in', 'pp', 'and', 'pbarp', 'collisions']] | [-0.09247781468841892, 0.19086565277449644, -0.1893422200922102, 0.14616807866752005, 0.004822162356084356, -0.027975382892271645, -0.1444490414399367, 0.3234455487601316, -0.18189662508666515, -0.21302907111553046, -0.10283082056020458, -0.4252568834389632, 0.017338490686737575, 0.1849841191791571, 0.08562022297141644... |
710.4028 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume IV | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4029 | An analytical model of surface mass densities of cold dark matter haloes
- with an application to MACHO microlensing optical depths | The cold dark matter (CDM) scenario generically predicts the existence of
triaxial dark matter haloes which contain notable amounts of substructure.
However, analytical halo models with smooth, spherically symmetric density
profiles are routinely adopted in the modelling of light propagation effects
through such obje... | astro-ph | the cold dark matter cdm scenario generically predicts the existence of triaxial dark matter haloes which contain notable amounts of substructure however analytical halo models with smooth spherically symmetric density profiles are routinely adopted in the modelling of light propagation effects through such objects in ... | [['the', 'cold', 'dark', 'matter', 'cdm', 'scenario', 'generically', 'predicts', 'the', 'existence', 'of', 'triaxial', 'dark', 'matter', 'haloes', 'which', 'contain', 'notable', 'amounts', 'of', 'substructure', 'however', 'analytical', 'halo', 'models', 'with', 'smooth', 'spherically', 'symmetric', 'density', 'profiles... | [-0.06696361318033943, 0.0996561241637767, -0.11281833112344987, 0.1358445686867438, -0.0725324644365408, -0.037033604225613206, 0.006137815152478945, 0.39077985996470577, -0.1361158717078187, -0.44402933237893927, -0.011438857474375607, -0.2916014143716424, -0.044207350345283385, 0.18081850494397053, -0.03159822073611... |
710.403 | From DNA sequence analysis to modeling replication in the human genome | We explore the large-scale behavior of nucleotide compositional strand
asymmetries along human chromosomes. As we observe for 7 of 9 origins of
replication experimentally identified so far, the (TA+GC) skew displays rather
sharp upward jumps, with a linear decreasing profile in between two successive
jumps. We presen... | q-bio.GN | we explore the largescale behavior of nucleotide compositional strand asymmetries along human chromosomes as we observe for 7 of 9 origins of replication experimentally identified so far the tagc skew displays rather sharp upward jumps with a linear decreasing profile in between two successive jumps we present a model ... | [['we', 'explore', 'the', 'largescale', 'behavior', 'of', 'nucleotide', 'compositional', 'strand', 'asymmetries', 'along', 'human', 'chromosomes', 'as', 'we', 'observe', 'for', '7', 'of', '9', 'origins', 'of', 'replication', 'experimentally', 'identified', 'so', 'far', 'the', 'tagc', 'skew', 'displays', 'rather', 'shar... | [-0.16173762257622676, 0.1879370653953595, -0.021461374790373224, 0.10127205076019487, -0.012580078349586713, -0.16921245276979688, 0.08512716637751847, 0.44063496912174205, -0.2911686137301364, -0.27479186472138045, 0.04721511723861719, -0.2813348089171254, -0.15483965612603007, 0.12056407594354823, -0.036229630212161... |
710.4031 | On the critical exponent of generalized Thue-Morse words | For certain generalized Thue-Morse words t, we compute the "critical
exponent", i.e., the supremum of the set of rational numbers that are exponents
of powers in t, and determine exactly the occurrences of powers realizing it.
| math.CO cs.DM | for certain generalized thuemorse words t we compute the critical exponent ie the supremum of the set of rational numbers that are exponents of powers in t and determine exactly the occurrences of powers realizing it | [['for', 'certain', 'generalized', 'thuemorse', 'words', 't', 'we', 'compute', 'the', 'critical', 'exponent', 'ie', 'the', 'supremum', 'of', 'the', 'set', 'of', 'rational', 'numbers', 'that', 'are', 'exponents', 'of', 'powers', 'in', 't', 'and', 'determine', 'exactly', 'the', 'occurrences', 'of', 'powers', 'realizing',... | [-0.21816534507605764, 0.21007405764733753, -0.010129031472994635, 0.0774942964522375, -0.02833085619204212, -0.12820656494134003, 0.1082792602893379, 0.25503859507605536, -0.3440806187637564, -0.20849790484903175, 0.056831210421579376, -0.3227798822077198, -0.14737232650319734, 0.2279628457310739, 0.009092390437015437... |
710.4032 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume VI | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4033 | Application of Groebner bases to the cup-length of oriented Grassmann
manifolds | We determine the cup-length of some oriented Grassmann manifolds by finding a
Groebner basis associated with a certain subring of the cohomology of them. As
its applications, we provide not only a lower but also an upper bound for the
LS-category of some oriented Grassmann manifolds. We also study the immersion
probl... | math.AT | we determine the cuplength of some oriented grassmann manifolds by finding a groebner basis associated with a certain subring of the cohomology of them as its applications we provide not only a lower but also an upper bound for the lscategory of some oriented grassmann manifolds we also study the immersion problem of t... | [['we', 'determine', 'the', 'cuplength', 'of', 'some', 'oriented', 'grassmann', 'manifolds', 'by', 'finding', 'a', 'groebner', 'basis', 'associated', 'with', 'a', 'certain', 'subring', 'of', 'the', 'cohomology', 'of', 'them', 'as', 'its', 'applications', 'we', 'provide', 'not', 'only', 'a', 'lower', 'but', 'also', 'an'... | [-0.2081488138883961, 0.051927424228105576, -0.07682666757695929, 0.08935850796600182, -0.10750813420896453, -0.11610314115467998, 0.04374732430679379, 0.3725081806554011, -0.2963197443772245, -0.27020790572795605, 0.16723321258366383, -0.2274184264242649, -0.1822793522366771, 0.2290392900230708, -0.11459981725999603, ... |
710.4034 | On the stability of AdS black strings | We explore via linearized perturbation theory the Gregory-Laflamme
instability of the black string solutions of Einstein's equations with negative
cosmological constant recently discussed in literature. Our results indicate
that the black strings whose conformal infinity is the product of time and
$S^{d-3}\times S^1$... | hep-th | we explore via linearized perturbation theory the gregorylaflamme instability of the black string solutions of einsteins equations with negative cosmological constant recently discussed in literature our results indicate that the black strings whose conformal infinity is the product of time and sd3times s1 are stable f... | [['we', 'explore', 'via', 'linearized', 'perturbation', 'theory', 'the', 'gregorylaflamme', 'instability', 'of', 'the', 'black', 'string', 'solutions', 'of', 'einsteins', 'equations', 'with', 'negative', 'cosmological', 'constant', 'recently', 'discussed', 'in', 'literature', 'our', 'results', 'indicate', 'that', 'the'... | [-0.20686776057676706, 0.14470818041913908, -0.08398690754675293, 0.11584806110556811, -0.08925938531628823, -0.13868792213448514, -0.038336579738924764, 0.27569027326694906, -0.19663797858273227, -0.2337441073654041, 0.13724803606092878, -0.2935284380641549, -0.13617232393422354, 0.176632869715981, -0.0329496284168570... |
710.4035 | Pairs of commuting Hamiltonians quadratic in momenta | In the case of two degree system the pairs of quadratic in momenta
Hamiltonians commuting according the standard Poisson bracket are considered.
The new many-parametrical families of such pairs are founded. The universal
method of constructing the full solution of Hamilton - Jacobi equation in terms
of integrals on s... | nlin.SI | in the case of two degree system the pairs of quadratic in momenta hamiltonians commuting according the standard poisson bracket are considered the new manyparametrical families of such pairs are founded the universal method of constructing the full solution of hamilton jacobi equation in terms of integrals on some alg... | [['in', 'the', 'case', 'of', 'two', 'degree', 'system', 'the', 'pairs', 'of', 'quadratic', 'in', 'momenta', 'hamiltonians', 'commuting', 'according', 'the', 'standard', 'poisson', 'bracket', 'are', 'considered', 'the', 'new', 'manyparametrical', 'families', 'of', 'such', 'pairs', 'are', 'founded', 'the', 'universal', '... | [-0.22943422447133344, 0.041493339056614786, -0.09186025775852613, 0.06849405621505866, -0.0797274302385631, -0.11926328286062926, -0.04593604507681448, 0.3041876385686919, -0.2983533770311624, -0.2541323861805722, 0.04966033339042042, -0.29762775351991877, -0.15723505188361742, 0.300112916942453, -0.10675861841446022,... |
710.4036 | A SINFONI view of Galaxy Centers: Morphology and Kinematics of five
Nuclear Star Formation Rings | We present near-infrared (H- and K-band) integral-field observations of the
circumnuclear star formation rings in five nearby spiral galaxies. The data,
obtained at the Very Large Telescope with the SINFONI spectrograph, are used to
construct maps of various emission lines that reveal the individual star
forming regi... | astro-ph | we present nearinfrared h and kband integralfield observations of the circumnuclear star formation rings in five nearby spiral galaxies the data obtained at the very large telescope with the sinfoni spectrograph are used to construct maps of various emission lines that reveal the individual star forming regions hot spo... | [['we', 'present', 'nearinfrared', 'h', 'and', 'kband', 'integralfield', 'observations', 'of', 'the', 'circumnuclear', 'star', 'formation', 'rings', 'in', 'five', 'nearby', 'spiral', 'galaxies', 'the', 'data', 'obtained', 'at', 'the', 'very', 'large', 'telescope', 'with', 'the', 'sinfoni', 'spectrograph', 'are', 'used'... | [-0.08353427825455458, 0.048489208612591025, -0.06475932876226204, 0.06462531266412859, -0.08581459689564232, -0.08485399457658159, 0.0159179612432189, 0.45022497308151477, -0.17806495934692693, -0.27478787708577923, 0.05699827415499322, -0.2747605298549451, -0.0076797758967712005, 0.18000316954667456, -0.0089300581177... |
710.4037 | Cross Section Constrained Top Quark Mass Measurement from Dilepton
Events at the Tevatron | We report the first top quark mass measurement that uses a cross section
constraint to improve the mass determination. This measurement is made with a
dilepton $t\bar{t}$ event sample collected with the CDF II detector. From a
data sample corresponding to an integrated luminosity of 1.2 fb$^{-1}$, we
measure a top qu... | hep-ex | we report the first top quark mass measurement that uses a cross section constraint to improve the mass determination this measurement is made with a dilepton tbart event sample collected with the cdf ii detector from a data sample corresponding to an integrated luminosity of 12 fb1 we measure a top quark mass of rm170... | [['we', 'report', 'the', 'first', 'top', 'quark', 'mass', 'measurement', 'that', 'uses', 'a', 'cross', 'section', 'constraint', 'to', 'improve', 'the', 'mass', 'determination', 'this', 'measurement', 'is', 'made', 'with', 'a', 'dilepton', 'tbart', 'event', 'sample', 'collected', 'with', 'the', 'cdf', 'ii', 'detector', ... | [-0.0285237489733845, 0.12706493555507384, -0.10651709826882272, 0.06799506176920499, -0.08034143396242358, -0.06329909411450739, 0.09374248682904769, 0.32341191052075696, -0.13170819413190818, -0.3754038336577223, 0.010658670208238833, -0.3802909559214159, 0.13156282625106328, 0.150016309642096, 0.0353419862632804, 0.... |
710.4038 | Charged Higgs production in the flavored MSSM | In the Minimal Supersymmetric Standard Model squark mixing can significantly
change the pattern of charged-Higgs production. We find that non-minimal flavor
structures can have a sizeable impact on the charged-Higgs production cross
section, whereas charged-Higgs searches may be able to probe flavor structures
not ac... | hep-ph | in the minimal supersymmetric standard model squark mixing can significantly change the pattern of chargedhiggs production we find that nonminimal flavor structures can have a sizeable impact on the chargedhiggs production cross section whereas chargedhiggs searches may be able to probe flavor structures not accessible... | [['in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'squark', 'mixing', 'can', 'significantly', 'change', 'the', 'pattern', 'of', 'chargedhiggs', 'production', 'we', 'find', 'that', 'nonminimal', 'flavor', 'structures', 'can', 'have', 'a', 'sizeable', 'impact', 'on', 'the', 'chargedhiggs', 'production', 'c... | [-0.08567567501736224, 0.3273925806441512, -0.04918113024141945, 0.21365029799950416, -0.12820323272684558, -0.18596125384181983, 0.09502078672168685, 0.29114342354176964, -0.2154359234283205, -0.2911865482809114, 0.0005789151067891326, -0.30075273189510476, 0.0043760235669457765, 0.11594458283917582, 0.042284859756587... |
710.4039 | SAXJ1712.6-3739: a persistent hard X-ray source as monitored with
INTEGRAL | The X-ray source SAXJ1712.6-3739 is a very weak Low Mass X-ray Binary
discovered in 1999 with BeppoSAX and located in the Galactic Center. This
region has been deeply investigated by the INTEGRAL satellite with an
unprecedented exposure time, giving us an unique opportunity to study the hard
X-ray behavior also for w... | astro-ph | the xray source saxj171263739 is a very weak low mass xray binary discovered in 1999 with bepposax and located in the galactic center this region has been deeply investigated by the integral satellite with an unprecedented exposure time giving us an unique opportunity to study the hard xray behavior also for weak objec... | [['the', 'xray', 'source', 'saxj171263739', 'is', 'a', 'very', 'weak', 'low', 'mass', 'xray', 'binary', 'discovered', 'in', '1999', 'with', 'bepposax', 'and', 'located', 'in', 'the', 'galactic', 'center', 'this', 'region', 'has', 'been', 'deeply', 'investigated', 'by', 'the', 'integral', 'satellite', 'with', 'an', 'unp... | [-0.09842303528957629, 0.10482172562571039, -0.07256264488558184, 0.10101235035518316, -0.10018908853222891, -0.08609951511156601, 0.05582560496535939, 0.44027260365620463, -0.2214995080117626, -0.371715280419749, 0.12156340266668626, -0.2988863787438913, 0.004180263800048073, 0.23177411656350141, -0.03509951324531144,... |
710.404 | Elastic Nd scattering at intermediate energies as a tool for probing the
short-range deuteron structure | A calculation of the deuteron polarization observables $A^d_y$, $A_{yy}$,
$A_{xx}$, $A_{xz}$ and the differential cross-section for elastic
nucleon-deuteron scattering at incident deuteron energies 270 and 880 MeV in
lab is presented. A comparison of the calculations with two different deuteron
wave-functions derived... | nucl-th | a calculation of the deuteron polarization observables ad_y a_yy a_xx a_xz and the differential crosssection for elastic nucleondeuteron scattering at incident deuteron energies 270 and 880 mev in lab is presented a comparison of the calculations with two different deuteron wavefunctions derived from the bonncd nnpoten... | [['a', 'calculation', 'of', 'the', 'deuteron', 'polarization', 'observables', 'ad_y', 'a_yy', 'a_xx', 'a_xz', 'and', 'the', 'differential', 'crosssection', 'for', 'elastic', 'nucleondeuteron', 'scattering', 'at', 'incident', 'deuteron', 'energies', '270', 'and', '880', 'mev', 'in', 'lab', 'is', 'presented', 'a', 'compa... | [-0.048821252262037575, 0.17038030243803287, -0.14678149044250502, 0.11732877205308202, -0.03146994052329556, -0.07277033096381827, 0.03440429133352945, 0.36917360260596743, -0.17032005374178127, -0.2505571462780885, -0.08183631461756506, -0.3209727114957312, 0.008824892048521535, 0.1597623311757596, 0.1278662700509733... |
710.4041 | Area limit laws for symmetry classes of staircase polygons | We derive area limit laws for the various symmetry classes of staircase
polygons on the square lattice, in a uniform ensemble where, for fixed
perimeter, each polygon occurs with the same probability. This complements a
previous study by Leroux and Rassart, where explicit expressions for the area
and perimeter genera... | math.CO math.PR | we derive area limit laws for the various symmetry classes of staircase polygons on the square lattice in a uniform ensemble where for fixed perimeter each polygon occurs with the same probability this complements a previous study by leroux and rassart where explicit expressions for the area and perimeter generating fu... | [['we', 'derive', 'area', 'limit', 'laws', 'for', 'the', 'various', 'symmetry', 'classes', 'of', 'staircase', 'polygons', 'on', 'the', 'square', 'lattice', 'in', 'a', 'uniform', 'ensemble', 'where', 'for', 'fixed', 'perimeter', 'each', 'polygon', 'occurs', 'with', 'the', 'same', 'probability', 'this', 'complements', 'a... | [-0.12912889207447215, 0.09521339309867471, -0.03594732058367559, 0.057534074034525214, -0.022429232539642335, -0.10783345737893667, 0.08310748723202518, 0.3509166726310338, -0.21592020788479463, -0.25558909968822263, 0.12295511850347143, -0.2723750055052473, -0.127032466831484, 0.18355092370100984, -0.0878154561006730... |
710.4042 | Physics from HBT radii | An approximate formula connecting the true and the HBT homogeneity regions in
multiparticle production processes is derived. It implies that when calculating
the HBT radii one should use the ceter of mass systems of the pairs rather than
the now popular LCMS system. A discussion of several examples clarifies the
pote... | hep-ph | an approximate formula connecting the true and the hbt homogeneity regions in multiparticle production processes is derived it implies that when calculating the hbt radii one should use the ceter of mass systems of the pairs rather than the now popular lcms system a discussion of several examples clarifies the potentia... | [['an', 'approximate', 'formula', 'connecting', 'the', 'true', 'and', 'the', 'hbt', 'homogeneity', 'regions', 'in', 'multiparticle', 'production', 'processes', 'is', 'derived', 'it', 'implies', 'that', 'when', 'calculating', 'the', 'hbt', 'radii', 'one', 'should', 'use', 'the', 'ceter', 'of', 'mass', 'systems', 'of', '... | [-0.11395419609161223, 0.12983090656542676, -0.14270484907896083, 0.15053450337399055, -0.008207908250612787, -0.11293741857337922, -0.0471627379324988, 0.3287073396478254, -0.22524504328958025, -0.2791166841836259, 0.05235705236295736, -0.3072313129219531, -0.05045330654691425, 0.2114231377692506, -0.01125275004582507... |
710.4043 | Observation of magnetization reversal and negative magnetization in a
double perovskite compound Sr2YbRuO6 | Detailed magnetic properties of the compound Sr2YbRuO6 are presented here.
The compound belongs to the family of double perovskites forming a monoclinic
structure. Magnetization meas-urements reveal clear evidence for two components
of magnetic ordering aligned opposite to each other, leading to a magnetization
rever... | cond-mat.str-el cond-mat.mtrl-sci | detailed magnetic properties of the compound sr2ybruo6 are presented here the compound belongs to the family of double perovskites forming a monoclinic structure magnetization measurements reveal clear evidence for two components of magnetic ordering aligned opposite to each other leading to a magnetization reversal co... | [['detailed', 'magnetic', 'properties', 'of', 'the', 'compound', 'sr2ybruo6', 'are', 'presented', 'here', 'the', 'compound', 'belongs', 'to', 'the', 'family', 'of', 'double', 'perovskites', 'forming', 'a', 'monoclinic', 'structure', 'magnetization', 'measurements', 'reveal', 'clear', 'evidence', 'for', 'two', 'componen... | [-0.20056079920748768, 0.24363166509842782, -0.0008157588265120324, 0.04860672335849986, -0.08184202864835811, -0.11430176014245368, 0.08842840378622518, 0.3924981798773923, -0.2673696410494974, -0.3529390004292435, 0.0360196794622394, -0.3038994450736664, -0.0525372608780202, 0.1432083012444303, 0.08849426707867407, -... |
710.4044 | Compactified Jacobians, Abel maps and Theta divisors | This is an expository paper about the topics listed in the title.
| math.AG | this is an expository paper about the topics listed in the title | [['this', 'is', 'an', 'expository', 'paper', 'about', 'the', 'topics', 'listed', 'in', 'the', 'title']] | [-0.11976149662708242, 0.04377265597698473, -0.04058115929365158, 0.11684245647241671, -0.17135288783659539, 0.07137525950868924, -0.01938171629444696, 0.3362434655427933, -0.30587771721184254, -0.2972278295395275, 0.08170640308526345, -0.3613065608466665, -0.18327017834720513, 0.1504794651409611, -0.24853443478544554,... |
710.4045 | A new formulation of the relativistic many-body theory of electric
dipole moments of closed shell atoms | The electric dipole moments of closed-shell atoms are sensitive to the parity
and time-reversal violating phenomena in the nucleus. The nuclear Schiff moment
is one such property, it arises from the parity and time reversal violating
quark-quark interactions and the quark-chromo electric dipole moments. We
calculate ... | physics.atom-ph | the electric dipole moments of closedshell atoms are sensitive to the parity and timereversal violating phenomena in the nucleus the nuclear schiff moment is one such property it arises from the parity and time reversal violating quarkquark interactions and the quarkchromo electric dipole moments we calculate the elect... | [['the', 'electric', 'dipole', 'moments', 'of', 'closedshell', 'atoms', 'are', 'sensitive', 'to', 'the', 'parity', 'and', 'timereversal', 'violating', 'phenomena', 'in', 'the', 'nucleus', 'the', 'nuclear', 'schiff', 'moment', 'is', 'one', 'such', 'property', 'it', 'arises', 'from', 'the', 'parity', 'and', 'time', 'reve... | [-0.09631878415061461, 0.21512547115621677, -0.03216104113380425, 0.12369314653570053, -0.03465535752159559, -0.07290826405998382, 0.040042791195446625, 0.2969511519580827, -0.2459726365316675, -0.29439078808083374, -0.05193409605752835, -0.3353112890243025, -0.03335226752639401, 0.09726176628649583, 0.1214071016154899... |
710.4046 | Bit-interleaved coded modulation in the wideband regime | The wideband regime of bit-interleaved coded modulation (BICM) in Gaussian
channels is studied. The Taylor expansion of the coded modulation capacity for
generic signal constellations at low signal-to-noise ratio (SNR) is derived and
used to determine the corresponding expansion for the BICM capacity. Simple
formulas... | cs.IT math.IT | the wideband regime of bitinterleaved coded modulation bicm in gaussian channels is studied the taylor expansion of the coded modulation capacity for generic signal constellations at low signaltonoise ratio snr is derived and used to determine the corresponding expansion for the bicm capacity simple formulas for the mi... | [['the', 'wideband', 'regime', 'of', 'bitinterleaved', 'coded', 'modulation', 'bicm', 'in', 'gaussian', 'channels', 'is', 'studied', 'the', 'taylor', 'expansion', 'of', 'the', 'coded', 'modulation', 'capacity', 'for', 'generic', 'signal', 'constellations', 'at', 'low', 'signaltonoise', 'ratio', 'snr', 'is', 'derived', ... | [-0.1967582422510301, 0.07971117654520178, -0.03441641634841725, 0.08741352670952271, -0.023631279497787778, -0.2222520280334259, 0.13531700838488384, 0.37993320245066214, -0.27838008315630364, -0.2834852457663018, 0.10352499951677345, -0.2288739737123251, -0.12385781277397412, 0.23858165134131437, -0.14682623560646546... |
710.4047 | Some series and integrals involving the Riemann zeta function, binomial
coefficients and the harmonic numbers. Volume V | In this series of seven papers, predominantly by means of elementary
analysis, we establish a number of identities related to the Riemann zeta
function. Whilst this paper is mainly expository, some of the formulae reported
in it are believed to be new, and the paper may also be of interest
specifically due to the fac... | math.HO | in this series of seven papers predominantly by means of elementary analysis we establish a number of identities related to the riemann zeta function whilst this paper is mainly expository some of the formulae reported in it are believed to be new and the paper may also be of interest specifically due to the fact that ... | [['in', 'this', 'series', 'of', 'seven', 'papers', 'predominantly', 'by', 'means', 'of', 'elementary', 'analysis', 'we', 'establish', 'a', 'number', 'of', 'identities', 'related', 'to', 'the', 'riemann', 'zeta', 'function', 'whilst', 'this', 'paper', 'is', 'mainly', 'expository', 'some', 'of', 'the', 'formulae', 'repor... | [-0.11530844273554759, 0.09796234634724435, -0.11181551533570486, 0.08285223662596085, -0.10019141775486406, -0.07045825119755829, 0.001738097848815482, 0.31895867048470833, -0.26462381259267176, -0.33202195352415986, 0.14744018157596575, -0.2559475443923651, -0.22675369485496863, 0.2414655297883411, -0.077032941699361... |
710.4048 | Evidence for a Type 1/Type 2 dichotomy in the correlation between quasar
optical polarization and host galaxy/extended emission position angles | For Seyfert galaxies, the AGN unification model provides a simple and well
established explanation of the Type 1/Type 2 dichotomy through orientation
based effects. The generalization of this unification model to the higher
luminosity AGNs that are the quasars remains a key question. The recent
detection of Type 2 Ra... | astro-ph | for seyfert galaxies the agn unification model provides a simple and well established explanation of the type 1type 2 dichotomy through orientation based effects the generalization of this unification model to the higher luminosity agns that are the quasars remains a key question the recent detection of type 2 radioqui... | [['for', 'seyfert', 'galaxies', 'the', 'agn', 'unification', 'model', 'provides', 'a', 'simple', 'and', 'well', 'established', 'explanation', 'of', 'the', 'type', '1type', '2', 'dichotomy', 'through', 'orientation', 'based', 'effects', 'the', 'generalization', 'of', 'this', 'unification', 'model', 'to', 'the', 'higher'... | [-0.08703529864878339, 0.0630278197382245, -0.037689451456946486, 0.09709495372756287, -0.124505252008457, -0.11434811285941343, 0.018414000230440996, 0.44513402848053574, -0.19631591946206886, -0.30565652676027827, 0.050674107804898665, -0.2731510875788749, -0.04878902277588945, 0.17459966531929422, -0.022255370126851... |
710.4049 | Parity violating cylindrical shell in the framework of QED | We present calculations of Casimir energy (CE) in a system of quantized
electromagnetic (EM) field interacting with an infinite circular cylindrical
shell (which we call `the defect'). Interaction is described in the only
QFT-consistent way by Chern-Simon action concentrated on the defect, with a
single coupling cons... | hep-th cond-mat.stat-mech quant-ph | we present calculations of casimir energy ce in a system of quantized electromagnetic em field interacting with an infinite circular cylindrical shell which we call the defect interaction is described in the only qftconsistent way by chernsimon action concentrated on the defect with a single coupling constant a for reg... | [['we', 'present', 'calculations', 'of', 'casimir', 'energy', 'ce', 'in', 'a', 'system', 'of', 'quantized', 'electromagnetic', 'em', 'field', 'interacting', 'with', 'an', 'infinite', 'circular', 'cylindrical', 'shell', 'which', 'we', 'call', 'the', 'defect', 'interaction', 'is', 'described', 'in', 'the', 'only', 'qftco... | [-0.1633262579100177, 0.1402910135517549, -0.07448661689543062, 0.059622219204717865, -0.05399145217730649, -0.11897190680934323, 0.0025619659323378335, 0.3670927788175288, -0.21685258455071893, -0.27437102924367146, 0.036734152527984294, -0.281090127939861, -0.1438797091442601, 0.1505763845791715, -0.01498709688524878... |
710.405 | Pseudo-goldstone higgs from five dimensions | I discuss radiative generation of the higgs potential in 5D models of
gauge-higgs unification.
| hep-ph | i discuss radiative generation of the higgs potential in 5d models of gaugehiggs unification | [['i', 'discuss', 'radiative', 'generation', 'of', 'the', 'higgs', 'potential', 'in', '5d', 'models', 'of', 'gaugehiggs', 'unification']] | [-0.08614252680646521, 0.1803387991551842, 0.14141477052388446, 0.24218782423330204, -0.04536095919632187, -0.25459255810294834, -0.043761754142386575, 0.37032270963702885, -0.16824220090971462, -0.26414814478318605, -0.02174460582734485, -0.1494729522216533, -0.04483859377380993, 0.01830194577840822, 0.060293540358543... |
710.4051 | On the capacity achieving covariance matrix for Rician MIMO channels: an
asymptotic approach | The capacity-achieving input covariance matrices for coherent block-fading
correlated MIMO Rician channels are determined. In this case, no closed-form
expressions for the eigenvectors of the optimum input covariance matrix are
available. An approximation of the average mutual information is evaluated in
this paper i... | math.PR cs.IT math.IT | the capacityachieving input covariance matrices for coherent blockfading correlated mimo rician channels are determined in this case no closedform expressions for the eigenvectors of the optimum input covariance matrix are available an approximation of the average mutual information is evaluated in this paper in the as... | [['the', 'capacityachieving', 'input', 'covariance', 'matrices', 'for', 'coherent', 'blockfading', 'correlated', 'mimo', 'rician', 'channels', 'are', 'determined', 'in', 'this', 'case', 'no', 'closedform', 'expressions', 'for', 'the', 'eigenvectors', 'of', 'the', 'optimum', 'input', 'covariance', 'matrix', 'are', 'avai... | [-0.1682320499218934, 0.03804450963954358, -0.0439773315630321, 0.07937352577074697, -0.04225635238523994, -0.20204420724018876, 0.05437145142599807, 0.3767768297610538, -0.23001140973397663, -0.2750328879570588, 0.08373892208910547, -0.2926098932911243, -0.1866471820693862, 0.16419914372132294, -0.060144493999957506, ... |
710.4052 | Metastable Feshbach Molecules in High Rotational States | We experimentally demonstrate Cs2 Feshbach molecules well above the
dissociation threshold, which are stable against spontaneous decay on the
timescale of one second. An optically trapped sample of ultracold dimers is
prepared in an l-wave state and magnetically tuned into a region with negative
binding energy. The m... | cond-mat.other | we experimentally demonstrate cs2 feshbach molecules well above the dissociation threshold which are stable against spontaneous decay on the timescale of one second an optically trapped sample of ultracold dimers is prepared in an lwave state and magnetically tuned into a region with negative binding energy the metasta... | [['we', 'experimentally', 'demonstrate', 'cs2', 'feshbach', 'molecules', 'well', 'above', 'the', 'dissociation', 'threshold', 'which', 'are', 'stable', 'against', 'spontaneous', 'decay', 'on', 'the', 'timescale', 'of', 'one', 'second', 'an', 'optically', 'trapped', 'sample', 'of', 'ultracold', 'dimers', 'is', 'prepared... | [-0.13199661837507395, 0.2820527362616643, 0.008122730341674102, 0.021603986524478203, 0.02565488212440878, -0.15701842419520923, 0.08925352874917514, 0.3947465873859597, -0.24580928297581697, -0.29831333618347694, -0.016274392139166594, -0.27619797228412196, -0.0018767408022393633, 0.14405868825211068, 0.0549512088467... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.