id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.1953 | Strong Reduction of the Field-Dependent Microwave Surface Resistance in
YBCO with BaZrO_3 Inclusions | We present measurements of the magnetic field dependent microwave surface
resistance in laser-ablated YBa$_2$Cu$_3$O$_{7-\delta}$ films on SrTiO$_3$
substrates. BaZrO$_3$ crystallites were included in the films using composite
targets containing BaZrO$_3$ inclusions with mean grain size smaller than 1
$\mu$m. X-ray d... | cond-mat.supr-con cond-mat.mtrl-sci | we present measurements of the magnetic field dependent microwave surface resistance in laserablated yba_2cu_3o_7delta films on srtio_3 substrates bazro_3 crystallites were included in the films using composite targets containing bazro_3 inclusions with mean grain size smaller than 1 mum xray diffraction showed single ... | [['we', 'present', 'measurements', 'of', 'the', 'magnetic', 'field', 'dependent', 'microwave', 'surface', 'resistance', 'in', 'laserablated', 'yba_2cu_3o_7delta', 'films', 'on', 'srtio_3', 'substrates', 'bazro_3', 'crystallites', 'were', 'included', 'in', 'the', 'films', 'using', 'composite', 'targets', 'containing', '... | [-0.12164111960702008, 0.2116136322893442, -0.027791254387078124, -0.032535668996321716, -0.000360770596804597, -0.15760818538085625, 0.08936215407998023, 0.4370220000287745, -0.1900127432536243, -0.36167159950269795, 0.015612630356084015, -0.33666716242867817, -0.05393884740855045, 0.21313240282555543, 0.0014839262656... |
710.1954 | Prospects for the Determination of Higgs Boson Properties at the LHC | The prospects for the determination of the properties of a hypothetical boson
discovered at the Large Hadron Collider using measurements to be performed with
the ATLAS and CMS detectors are summarized. The properties that are discussed
are the mass of the boson, its width, the strength of its couplings to
fermions, t... | hep-ph | the prospects for the determination of the properties of a hypothetical boson discovered at the large hadron collider using measurements to be performed with the atlas and cms detectors are summarized the properties that are discussed are the mass of the boson its width the strength of its couplings to fermions the str... | [['the', 'prospects', 'for', 'the', 'determination', 'of', 'the', 'properties', 'of', 'a', 'hypothetical', 'boson', 'discovered', 'at', 'the', 'large', 'hadron', 'collider', 'using', 'measurements', 'to', 'be', 'performed', 'with', 'the', 'atlas', 'and', 'cms', 'detectors', 'are', 'summarized', 'the', 'properties', 'th... | [-0.1301262577831307, 0.26619417642188425, -0.045533597613136995, 0.07265996082466752, -0.06521311837851125, -0.12435686538297244, 0.03127807683845544, 0.32741064444074736, -0.2466484693098156, -0.30189469503238797, 0.07982316725503873, -0.3168611228671473, -0.003775988397298052, 0.180161674726097, 0.1321472887031953, ... |
710.1955 | Renormalization, Wilson lines, and transverse-momentum dependent parton
distribution functions | We perform an analysis of transverse-momentum dependent parton distribution
functions, making use of their renormalization properties in terms of their
leading-order anomalous dimensions. We show that the appropriate Wilson line in
the light-cone gauge, associated with such quantities, is a cusped one. To
cancel the ... | hep-ph | we perform an analysis of transversemomentum dependent parton distribution functions making use of their renormalization properties in terms of their leadingorder anomalous dimensions we show that the appropriate wilson line in the lightcone gauge associated with such quantities is a cusped one to cancel the ensuing cu... | [['we', 'perform', 'an', 'analysis', 'of', 'transversemomentum', 'dependent', 'parton', 'distribution', 'functions', 'making', 'use', 'of', 'their', 'renormalization', 'properties', 'in', 'terms', 'of', 'their', 'leadingorder', 'anomalous', 'dimensions', 'we', 'show', 'that', 'the', 'appropriate', 'wilson', 'line', 'in... | [-0.14091865260801886, 0.20164776106447907, -0.15389364141889889, 0.1248756428818603, -0.10160910061803526, -0.04380198824725559, -0.01148434473282617, 0.4099969235451325, -0.20876863748645005, -0.21042627653957385, -0.0001052223720446067, -0.29410145249541686, -0.13642206117156488, 0.10565987232510689, -0.008934635410... |
710.1956 | Particular boundary condition ensures that a fermion in d=1+5,
compactified on a finite disk, manifests in d=1+3 as massless spinor with a
charge 1/2, mass protected and chirally coupled to the gauge field | The genuine Kaluza-Klein-like theories--with no fields in addition to
gravity--have difficulties with the existence of massless spinors after the
compactification of some space dimensions \cite{witten}. We proposed in
previous paper a boundary condition for spinors in d=(1+5) compactified on a
flat disk that ensures ... | hep-th | the genuine kaluzakleinlike theorieswith no fields in addition to gravityhave difficulties with the existence of massless spinors after the compactification of some space dimensions citewitten we proposed in previous paper a boundary condition for spinors in d15 compactified on a flat disk that ensures masslessness of ... | [['the', 'genuine', 'kaluzakleinlike', 'theorieswith', 'no', 'fields', 'in', 'addition', 'to', 'gravityhave', 'difficulties', 'with', 'the', 'existence', 'of', 'massless', 'spinors', 'after', 'the', 'compactification', 'of', 'some', 'space', 'dimensions', 'citewitten', 'we', 'proposed', 'in', 'previous', 'paper', 'a', ... | [-0.17546861639290345, 0.1795216244012924, -0.05058130166515356, 0.058504626384980274, -0.12232261006793696, -0.12819645304863495, -0.025723330814054046, 0.33073846363521175, -0.16263608892235581, -0.2717029365287419, 0.08313632503749553, -0.23497096604601606, -0.11295154140748846, 0.10717702457703299, -0.0311408723726... |
710.1957 | Determination of the Discovery Potential for Higgs Bosons in MSSM | The CMS and ATLAS collaborations have performed detailed studies of the
discovery potential for the Higgs boson in MSSM. Different benchmarks scenarios
have been studied both for the CP-conserving case and for the CP-violating one.
Results are presented of the discovery potential in the parameter space of
MSSM.
| hep-ex | the cms and atlas collaborations have performed detailed studies of the discovery potential for the higgs boson in mssm different benchmarks scenarios have been studied both for the cpconserving case and for the cpviolating one results are presented of the discovery potential in the parameter space of mssm | [['the', 'cms', 'and', 'atlas', 'collaborations', 'have', 'performed', 'detailed', 'studies', 'of', 'the', 'discovery', 'potential', 'for', 'the', 'higgs', 'boson', 'in', 'mssm', 'different', 'benchmarks', 'scenarios', 'have', 'been', 'studied', 'both', 'for', 'the', 'cpconserving', 'case', 'and', 'for', 'the', 'cpviol... | [-0.0983754090751366, 0.13935050027794205, -0.030212181465079386, 0.11367825818403314, -0.06637247461670388, -0.16267487268972522, 0.014435219306809207, 0.3425389726956685, -0.12250202769064344, -0.30999263701960444, 0.08796562029601773, -0.2919310858317961, -0.029353674831024062, 0.21938761034592366, 0.058288588188588... |
710.1958 | Reconstructing the properties of dark energy from recent observations | We explore the properties of dark energy from recent observational data,
including the Gold Sne Ia, the baryonic acoustic oscillation peak from SDSS,
the CMB shift parameter from WMAP3, the X-ray gas mass fraction in cluster and
the Hubble parameter versus redshift. The $\Lambda CDM$ model with curvature
and two para... | astro-ph | we explore the properties of dark energy from recent observational data including the gold sne ia the baryonic acoustic oscillation peak from sdss the cmb shift parameter from wmap3 the xray gas mass fraction in cluster and the hubble parameter versus redshift the lambda cdm model with curvature and two parameterized d... | [['we', 'explore', 'the', 'properties', 'of', 'dark', 'energy', 'from', 'recent', 'observational', 'data', 'including', 'the', 'gold', 'sne', 'ia', 'the', 'baryonic', 'acoustic', 'oscillation', 'peak', 'from', 'sdss', 'the', 'cmb', 'shift', 'parameter', 'from', 'wmap3', 'the', 'xray', 'gas', 'mass', 'fraction', 'in', '... | [-0.07022959683961341, 0.13461767463424537, -0.08898241339493117, 0.1279341839982609, -0.12380582151067165, -0.08361305663262615, 0.0371275921156701, 0.3447762335871012, -0.20165126522619078, -0.3639884023200223, 0.01195720337661879, -0.3256551255223178, 0.02672409328084638, 0.20087050361814732, 0.03615706519202422, 0.... |
710.1959 | Nonlinear Neumann boundary stabilization of the wave equation using
rotated multipliers | The rotated multipliers method is performed in the case of the boundary
stabilization by means of a(linear or non-linear) Neumann feedback. this method
leads to new geometrical cases concerning the "active" part of the boundary
where the feedback is apllied. Due to mixed boundary conditions, these cases
generate sing... | math.OC math.AP | the rotated multipliers method is performed in the case of the boundary stabilization by means of alinear or nonlinear neumann feedback this method leads to new geometrical cases concerning the active part of the boundary where the feedback is apllied due to mixed boundary conditions these cases generate singularities ... | [['the', 'rotated', 'multipliers', 'method', 'is', 'performed', 'in', 'the', 'case', 'of', 'the', 'boundary', 'stabilization', 'by', 'means', 'of', 'alinear', 'or', 'nonlinear', 'neumann', 'feedback', 'this', 'method', 'leads', 'to', 'new', 'geometrical', 'cases', 'concerning', 'the', 'active', 'part', 'of', 'the', 'bo... | [-0.1517423997958593, 0.07434365319116323, -0.06716132676228881, 0.005848816819982885, -0.09807588350888567, -0.1504601175741603, 0.007601209501665311, 0.3347582089764094, -0.2841947438463456, -0.237122513523156, 0.1886053469462433, -0.18094895424490626, -0.14406050458395234, 0.21028339938669832, -0.1364830768751827, 0... |
710.196 | Three manifolds as geometric branched coverings of the three sphere | One method for obtaining every closed orientable 3-manifold is as branched
covering of the 3-sphere over a link. There is a classical topological result
showing that the minimun possible number of sheets in the covering is three. In
this paper we obtain a geometric version of this result. The interest is given
by the... | math.GT | one method for obtaining every closed orientable 3manifold is as branched covering of the 3sphere over a link there is a classical topological result showing that the minimun possible number of sheets in the covering is three in this paper we obtain a geometric version of this result the interest is given by the growin... | [['one', 'method', 'for', 'obtaining', 'every', 'closed', 'orientable', '3manifold', 'is', 'as', 'branched', 'covering', 'of', 'the', '3sphere', 'over', 'a', 'link', 'there', 'is', 'a', 'classical', 'topological', 'result', 'showing', 'that', 'the', 'minimun', 'possible', 'number', 'of', 'sheets', 'in', 'the', 'coverin... | [-0.21547638595134752, 0.10231696867735171, -0.09112876317784434, 0.049068037359440916, -0.04590923386458002, -0.10656591691840135, 0.02199416964498089, 0.3188548681252735, -0.2677032982045021, -0.3038277558860232, 0.0959133667543103, -0.24671624713867416, -0.20458912358382625, 0.2512163623602542, -0.15741217162337948,... |
710.1961 | Modeling interaction of relativistic and nonrelativistic winds in binary
system PSR 1259-63/SS2883. I.Hydrodynamical limit | In this paper, we present a detailed hydrodynamical study of the properties
of the flow produced by the collision of a pulsar wind with the surrounding in
a binary system. This work is the first attempt to simulate interaction of the
ultrarelativistic flow (pulsar wind) with the nonrelativistic stellar wind.
Obtained... | astro-ph | in this paper we present a detailed hydrodynamical study of the properties of the flow produced by the collision of a pulsar wind with the surrounding in a binary system this work is the first attempt to simulate interaction of the ultrarelativistic flow pulsar wind with the nonrelativistic stellar wind obtained result... | [['in', 'this', 'paper', 'we', 'present', 'a', 'detailed', 'hydrodynamical', 'study', 'of', 'the', 'properties', 'of', 'the', 'flow', 'produced', 'by', 'the', 'collision', 'of', 'a', 'pulsar', 'wind', 'with', 'the', 'surrounding', 'in', 'a', 'binary', 'system', 'this', 'work', 'is', 'the', 'first', 'attempt', 'to', 'si... | [-0.1511407118631955, 0.15156024622505673, -0.07004424954203438, 0.07904810182134164, -0.10548982644303245, -0.05606984368797322, -0.017642924296727508, 0.3645520971289703, -0.26359924974833954, -0.30448521949026897, 0.040236890757086204, -0.2432451715854847, -0.01561213314377049, 0.24300415901153027, -0.00272080080272... |
710.1962 | Stanford Matrix Considered Harmful | This note argues about the validity of web-graph data used in the literature.
| cs.IR | this note argues about the validity of webgraph data used in the literature | [['this', 'note', 'argues', 'about', 'the', 'validity', 'of', 'webgraph', 'data', 'used', 'in', 'the', 'literature']] | [-0.09091673444849081, -0.09210960652965766, -0.12947106647949952, 0.1585881339941317, -0.08812405570195271, 0.019354913025521316, 0.09362933297569935, 0.2869215337559581, -0.19309866772248194, -0.31003185304311603, 0.10619008185592695, -0.2443112521790541, -0.08809232869400428, 0.17376615164371637, -0.1807199119088741... |
710.1963 | On the scaling behaviour of cross-tie domain wall structures in
patterned NiFe elements | The cross-tie domain wall structure in micrometre and sub-micrometre wide
patterned elements of NiFe, and a thickness range of 30 to 70nm, has been
studied by Lorentz microscopy. Whilst the basic geometry of the cross-tie
repeat units remains unchanged, their density increases when the cross-tie
length is constrained... | cond-mat.mtrl-sci | the crosstie domain wall structure in micrometre and submicrometre wide patterned elements of nife and a thickness range of 30 to 70nm has been studied by lorentz microscopy whilst the basic geometry of the crosstie repeat units remains unchanged their density increases when the crosstie length is constrained to be sma... | [['the', 'crosstie', 'domain', 'wall', 'structure', 'in', 'micrometre', 'and', 'submicrometre', 'wide', 'patterned', 'elements', 'of', 'nife', 'and', 'a', 'thickness', 'range', 'of', '30', 'to', '70nm', 'has', 'been', 'studied', 'by', 'lorentz', 'microscopy', 'whilst', 'the', 'basic', 'geometry', 'of', 'the', 'crosstie... | [-0.12167633412671941, 0.2016354459332693, -0.03818849653471261, 0.003731430745184688, -0.06036589081631973, -0.11326294489803591, 0.03639605266133523, 0.42732429802417754, -0.31555709107280044, -0.29745758712690856, 0.08423254852922192, -0.26349877550798867, -0.055164995312225074, 0.16253130614391662, -0.0114521063830... |
710.1964 | CDF Searches for New Physics with Photons | We present results of searches for new physics in final states with photons
at CDF in approximately 1 fb-1 of ppbar collisions at 1.96 TeV. We give an
overview of the data-driven photon background estimation techniques used for
the analyses. We report on a search for diphoton peaks and signature-based
searches for di... | hep-ex | we present results of searches for new physics in final states with photons at cdf in approximately 1 fb1 of ppbar collisions at 196 tev we give an overview of the datadriven photon background estimation techniques used for the analyses we report on a search for diphoton peaks and signaturebased searches for diphotonx ... | [['we', 'present', 'results', 'of', 'searches', 'for', 'new', 'physics', 'in', 'final', 'states', 'with', 'photons', 'at', 'cdf', 'in', 'approximately', '1', 'fb1', 'of', 'ppbar', 'collisions', 'at', '196', 'tev', 'we', 'give', 'an', 'overview', 'of', 'the', 'datadriven', 'photon', 'background', 'estimation', 'techniqu... | [-0.03444199804235708, 0.18035368024601534, -0.09031265261812044, 0.15753124938842641, -0.02816403635823336, -0.12859217192763922, 0.025760538719563943, 0.3658318811508476, -0.1332043494846, -0.3905532013502766, -0.010391085068924262, -0.3941544990864445, 0.0933214616274736, 0.1957672743668749, 0.07493301592461887, 0.1... |
710.1965 | Sestieri of Venice | We have investigated space syntax of Venice by means of random walks. Random
walks being defined on an undirected graph establish the Euclidean space in
which distances and angles between nodes acquire the clear statistical
interpretation. The properties of nodes with respect to random walks allow
partitioning the ci... | physics.soc-ph physics.data-an | we have investigated space syntax of venice by means of random walks random walks being defined on an undirected graph establish the euclidean space in which distances and angles between nodes acquire the clear statistical interpretation the properties of nodes with respect to random walks allow partitioning the city c... | [['we', 'have', 'investigated', 'space', 'syntax', 'of', 'venice', 'by', 'means', 'of', 'random', 'walks', 'random', 'walks', 'being', 'defined', 'on', 'an', 'undirected', 'graph', 'establish', 'the', 'euclidean', 'space', 'in', 'which', 'distances', 'and', 'angles', 'between', 'nodes', 'acquire', 'the', 'clear', 'stat... | [-0.13584770087304954, 0.16438310306290918, -0.09144940972328186, 0.04642098154156254, -0.07836689105114111, -0.13851737136451098, 0.11161570023888578, 0.41930290059401437, -0.27958543199213004, -0.28434821473022637, 0.06571770101033438, -0.26332606810789844, -0.14271366245184952, 0.10192485239643317, -0.09373255459448... |
710.1966 | Hadron Spectrum in a Two-Colour Baryon-Rich Medium | The hadron spectrum of SU(2) lattice gauge theory with two flavours of Wilson
quark is studied on an 8^3x16 lattice using all-to-all propagators, with
particular emphasis on the dependence on quark chemical potential mu. As mu is
increased from zero the diquark states with non-zero baryon number B respond as
expected... | hep-lat hep-ph nucl-th | the hadron spectrum of su2 lattice gauge theory with two flavours of wilson quark is studied on an 83x16 lattice using alltoall propagators with particular emphasis on the dependence on quark chemical potential mu as mu is increased from zero the diquark states with nonzero baryon number b respond as expected while sta... | [['the', 'hadron', 'spectrum', 'of', 'su2', 'lattice', 'gauge', 'theory', 'with', 'two', 'flavours', 'of', 'wilson', 'quark', 'is', 'studied', 'on', 'an', '83x16', 'lattice', 'using', 'alltoall', 'propagators', 'with', 'particular', 'emphasis', 'on', 'the', 'dependence', 'on', 'quark', 'chemical', 'potential', 'mu', 'a... | [-0.12993083052663473, 0.35065207396056947, -0.07463774749207018, 0.0756153685446951, -0.0303217544471913, -0.13740679027893357, 0.10911687385855093, 0.29270868407168094, -0.14884062668131867, -0.24367345769610935, -0.01088025979527755, -0.3338304056656839, -0.027690857410070616, 0.04324454500129188, 0.0858240875238756... |
710.1967 | Synchronization and bistability of qubit coupled to a driven dissipative
oscillator | We study numerically the behavior of qubit coupled to a quantum dissipative
driven oscillator (resonator). Above a critical coupling strength the qubit
rotations become synchronized with the oscillator phase. In the synchronized
regime, at certain parameters, the qubit exhibits tunneling between two
orientations with... | cond-mat.supr-con cond-mat.other nlin.CD quant-ph | we study numerically the behavior of qubit coupled to a quantum dissipative driven oscillator resonator above a critical coupling strength the qubit rotations become synchronized with the oscillator phase in the synchronized regime at certain parameters the qubit exhibits tunneling between two orientations with a macro... | [['we', 'study', 'numerically', 'the', 'behavior', 'of', 'qubit', 'coupled', 'to', 'a', 'quantum', 'dissipative', 'driven', 'oscillator', 'resonator', 'above', 'a', 'critical', 'coupling', 'strength', 'the', 'qubit', 'rotations', 'become', 'synchronized', 'with', 'the', 'oscillator', 'phase', 'in', 'the', 'synchronized... | [-0.20037419782602228, 0.24596518635977796, 0.005645090240207651, -0.06123712653303907, 0.0030107640729208165, -0.20480108187196797, 0.08627625920901967, 0.37267867562089424, -0.21186919841178073, -0.3318992703376959, -0.02155909616825132, -0.2703720039280597, -0.10670837770643023, 0.19033510140919438, -0.0334153889489... |
710.1968 | The Landau gauge gluon and ghost propagators in 4D SU(3) gluodynamics in
large lattice volumes | We present recent results of the Landau gauge gluon and ghost propagators in
SU(3) pure gauge theory at Wilson \beta=5.7 for lattice sizes up to 80^4
corresponding to physical volumes up to (13.2 fm)^4. In particular, we focus on
finite-volume and Gribov copy effects. We employ a gauge fixing method that
combines a s... | hep-lat | we present recent results of the landau gauge gluon and ghost propagators in su3 pure gauge theory at wilson beta57 for lattice sizes up to 804 corresponding to physical volumes up to 132 fm4 in particular we focus on finitevolume and gribov copy effects we employ a gauge fixing method that combines a simulated anneali... | [['we', 'present', 'recent', 'results', 'of', 'the', 'landau', 'gauge', 'gluon', 'and', 'ghost', 'propagators', 'in', 'su3', 'pure', 'gauge', 'theory', 'at', 'wilson', 'beta57', 'for', 'lattice', 'sizes', 'up', 'to', '804', 'corresponding', 'to', 'physical', 'volumes', 'up', 'to', '132', 'fm4', 'in', 'particular', 'we'... | [-0.07366620077906798, 0.22699194335857303, -0.14265033694122126, 0.1179362886371867, -0.05369400017015222, -0.09613542172074732, 0.10645415085579131, 0.42350639275240676, -0.09827891544679275, -0.2610878804299756, 0.04719096172225869, -0.28961713712110565, -0.061025978436831524, 0.11107438185286743, -0.017078457830781... |
710.1969 | Pfaffian Systems from Twistor Fibrations | Canonical twistor fibrations lead to Pfaffian systems by means of their
superhorizontal distribution. The aim of this note is to identify explicitly
the Pfaffian systems of five or less variables that arise in this way in terms
of the classification given by A.Awane and M.Goze.
| math.DG | canonical twistor fibrations lead to pfaffian systems by means of their superhorizontal distribution the aim of this note is to identify explicitly the pfaffian systems of five or less variables that arise in this way in terms of the classification given by aawane and mgoze | [['canonical', 'twistor', 'fibrations', 'lead', 'to', 'pfaffian', 'systems', 'by', 'means', 'of', 'their', 'superhorizontal', 'distribution', 'the', 'aim', 'of', 'this', 'note', 'is', 'to', 'identify', 'explicitly', 'the', 'pfaffian', 'systems', 'of', 'five', 'or', 'less', 'variables', 'that', 'arise', 'in', 'this', 'w... | [-0.16082063453545425, 0.07526046241265397, -0.07873242192490157, 0.09717544582726564, -0.030421136228670907, -0.06471318470010924, 0.03071791920161178, 0.3143100828625435, -0.2696053601454857, -0.3315835508496262, 0.07843687997719404, -0.23260282733759216, -0.22097392849689132, 0.16103025477617805, -0.1167112844021514... |
710.197 | Zeta functions of 3-dimensional p-adic Lie algebras | We give an explicit formula for the subalgebra zeta function of a general
3-dimensional Lie algebra over the p-adic integers $\mathbb{Z}_p$. To this end,
we associate to such a Lie algebra a ternary quadratic form over
$\mathbb{Z}_p$. The formula for the zeta function is given in terms of Igusa's
local zeta function ... | math.GR | we give an explicit formula for the subalgebra zeta function of a general 3dimensional lie algebra over the padic integers mathbbz_p to this end we associate to such a lie algebra a ternary quadratic form over mathbbz_p the formula for the zeta function is given in terms of igusas local zeta function associated to this... | [['we', 'give', 'an', 'explicit', 'formula', 'for', 'the', 'subalgebra', 'zeta', 'function', 'of', 'a', 'general', '3dimensional', 'lie', 'algebra', 'over', 'the', 'padic', 'integers', 'mathbbz_p', 'to', 'this', 'end', 'we', 'associate', 'to', 'such', 'a', 'lie', 'algebra', 'a', 'ternary', 'quadratic', 'form', 'over', ... | [-0.25953658144654973, -0.015029470442251685, -0.15673867115817433, 0.08448784098852359, -0.1693993255362979, -0.08176453927964238, 0.007892190961034171, 0.29771802824689075, -0.3602188494322555, -0.1859740228163511, 0.020551508481730707, -0.18367049760750628, -0.19247266241083189, 0.22866599085474654, -0.0665901391850... |
710.1971 | Hydrogen on graphene: Electronic structure, total energy, structural
distortions, and magnetism from first-principles calculations | Density functional calculations of electronic structure, total energy,
structural distortions, and magnetism for hydrogenated single-layer, bilayer,
and multi-layer graphene are performed. It is found that hydrogen-induced
magnetism can survives only at very low concentrations of hydrogen (single-atom
regime) whereas... | cond-mat.mtrl-sci | density functional calculations of electronic structure total energy structural distortions and magnetism for hydrogenated singlelayer bilayer and multilayer graphene are performed it is found that hydrogeninduced magnetism can survives only at very low concentrations of hydrogen singleatom regime whereas hydrogen pair... | [['density', 'functional', 'calculations', 'of', 'electronic', 'structure', 'total', 'energy', 'structural', 'distortions', 'and', 'magnetism', 'for', 'hydrogenated', 'singlelayer', 'bilayer', 'and', 'multilayer', 'graphene', 'are', 'performed', 'it', 'is', 'found', 'that', 'hydrogeninduced', 'magnetism', 'can', 'survi... | [-0.10937108943601036, 0.17099186074919998, 0.03497547757190963, 0.05977595021508427, 0.05464651705438478, -0.15623323722328578, 0.09847923800763157, 0.4822082751741012, -0.2803679702286091, -0.35273444113425084, -0.03295887682535168, -0.33120546720715033, -0.12791134983482252, 0.13186286550480872, 0.08820489842134217,... |
710.1972 | Combinatorial Gelfand models for some semigroups and q-rook monoid
algebras | Inspired by the results of [R. Adin, A. Postnikov, Y. Roichman, Combinatorial
Gelfand model, preprint math.RT arXiv:0709.3962], we propose combinatorial
Gelfand models for semigroup algebras of some finite semigroups, which include
the symmetric inverse semigroup, the dual symmetric inverse semigroup, the
maximal fac... | math.RT | inspired by the results of r adin a postnikov y roichman combinatorial gelfand model preprint mathrt arxiv07093962 we propose combinatorial gelfand models for semigroup algebras of some finite semigroups which include the symmetric inverse semigroup the dual symmetric inverse semigroup the maximal factorizable subsemig... | [['inspired', 'by', 'the', 'results', 'of', 'r', 'adin', 'a', 'postnikov', 'y', 'roichman', 'combinatorial', 'gelfand', 'model', 'preprint', 'mathrt', 'arxiv07093962', 'we', 'propose', 'combinatorial', 'gelfand', 'models', 'for', 'semigroup', 'algebras', 'of', 'some', 'finite', 'semigroups', 'which', 'include', 'the', ... | [-0.041787070923565345, 0.07406357208404828, -0.04246091150483231, 0.17975504772254713, -0.18032200829942285, -0.13751245997731149, -0.020018244093215024, 0.32133030689057007, -0.4348286209329043, -0.06777220739074695, 0.12994072908667825, -0.29398780693242577, -0.11885713912362669, 0.1550911708108299, -0.1313685359732... |
710.1973 | The 0^{-+} and 0^{++} glueballs and the multiplets including them | The properties of the $0^{++}$ and $0^{-+}$ meson multiplets are discussed.
Quoted are the $0^{++}$ and $0^{-+}$ glueball masses determined from data fit.
| hep-ph | the properties of the 0 and 0 meson multiplets are discussed quoted are the 0 and 0 glueball masses determined from data fit | [['the', 'properties', 'of', 'the', '0', 'and', '0', 'meson', 'multiplets', 'are', 'discussed', 'quoted', 'are', 'the', '0', 'and', '0', 'glueball', 'masses', 'determined', 'from', 'data', 'fit']] | [-0.08987826562446097, 0.24603277226181133, -0.003154252696296443, 0.16473627774773733, -0.02611785884136739, -0.18355038567729617, 0.02467381508777971, 0.3625224773650584, -0.22134407204778297, -0.23843908050785895, 0.07472858966692635, -0.3871294327647142, 0.058595322801367096, 0.06035046287528847, 0.1213543182643859... |
710.1974 | Microwave photovoltage and photoresistance effects in ferromagnetic
microstrips | We investigate the dc electric response induced by ferromagnetic resonance in
ferromagnetic Permalloy (Ni80Fe20) microstrips. The resulting magnetization
precession alters the angle of the magnetization with respect to both dc and rf
current. Consequently the time averaged anisotropic magnetoresistance (AMR)
changes ... | cond-mat.str-el | we investigate the dc electric response induced by ferromagnetic resonance in ferromagnetic permalloy ni80fe20 microstrips the resulting magnetization precession alters the angle of the magnetization with respect to both dc and rf current consequently the time averaged anisotropic magnetoresistance amr changes photores... | [['we', 'investigate', 'the', 'dc', 'electric', 'response', 'induced', 'by', 'ferromagnetic', 'resonance', 'in', 'ferromagnetic', 'permalloy', 'ni80fe20', 'microstrips', 'the', 'resulting', 'magnetization', 'precession', 'alters', 'the', 'angle', 'of', 'the', 'magnetization', 'with', 'respect', 'to', 'both', 'dc', 'and... | [-0.21867037160103922, 0.16975577226168737, 0.013927512294570874, -0.04292790857374433, -0.08770184280971687, -0.1316313242355177, 0.01913529094350566, 0.4156070094857667, -0.25192063813609583, -0.3010106553215542, -0.011565180845676107, -0.27369750349421623, -0.07201702806779796, 0.2749183930473419, 0.0464474665470891... |
710.1975 | The Levy-Gromov Isoperimetric Inequality in Convex Manifolds with
Boundary | We observe after Bayle and Rosales that the Levy-Gromov isoperimetric
inequality generalizes to convex manifolds with boundary.
| math.DG math.MG | we observe after bayle and rosales that the levygromov isoperimetric inequality generalizes to convex manifolds with boundary | [['we', 'observe', 'after', 'bayle', 'and', 'rosales', 'that', 'the', 'levygromov', 'isoperimetric', 'inequality', 'generalizes', 'to', 'convex', 'manifolds', 'with', 'boundary']] | [-0.0966649993788451, 0.019694747927132994, -0.10794565031392267, 0.04975100373849273, -0.0996377378469333, -0.2793603370664641, -0.005192684286157601, 0.3416990523110144, -0.27286354737589136, -0.24465884023811668, 0.16178772141574882, -0.31668186699971557, -0.18046328285709023, 0.16894711647182703, -0.280854466836899... |
710.1976 | Solving Infinite Kolam in Knot Theory | In south India, there are traditional patterns of line-drawings encircling
dots, called ``Kolam'', among which one-line drawings or the ``infinite Kolam''
provide very interesting questions in mathematics. For example, we address the
following simple question: how many patterns of infinite Kolam can we draw for
a giv... | cs.DM cond-mat.stat-mech | in south india there are traditional patterns of linedrawings encircling dots called kolam among which oneline drawings or the infinite kolam provide very interesting questions in mathematics for example we address the following simple question how many patterns of infinite kolam can we draw for a given grid pattern of... | [['in', 'south', 'india', 'there', 'are', 'traditional', 'patterns', 'of', 'linedrawings', 'encircling', 'dots', 'called', 'kolam', 'among', 'which', 'oneline', 'drawings', 'or', 'the', 'infinite', 'kolam', 'provide', 'very', 'interesting', 'questions', 'in', 'mathematics', 'for', 'example', 'we', 'address', 'the', 'fo... | [-0.10057191595948045, 0.12010190424600455, -0.106490020910143, 0.1114541595064414, -0.10928853222614397, -0.15925860840935205, 0.05748879940643826, 0.3711839514190628, -0.261955100816904, -0.28341816784814, 0.11731942488720802, -0.28190724646159704, -0.1765259388088505, 0.1919048554744855, -0.11438642085219423, -0.030... |
710.1977 | Coulomb-Blocked Transport Through a Quantum Dot with Spin-Split Level:
Increase of Differential Conductance Peaks by Spin Relaxation | Non-equilibrium transport through a quantum dot with one spin-split
single-particle level is studied in the cotunneling regime at low temperatures.
The Coulomb diamond can be subdivided into parts differing in at least one of
two respects: what kind of tunneling processes (i) determine the
single-particle occupations... | cond-mat.mes-hall | nonequilibrium transport through a quantum dot with one spinsplit singleparticle level is studied in the cotunneling regime at low temperatures the coulomb diamond can be subdivided into parts differing in at least one of two respects what kind of tunneling processes i determine the singleparticle occupations and ii ma... | [['nonequilibrium', 'transport', 'through', 'a', 'quantum', 'dot', 'with', 'one', 'spinsplit', 'singleparticle', 'level', 'is', 'studied', 'in', 'the', 'cotunneling', 'regime', 'at', 'low', 'temperatures', 'the', 'coulomb', 'diamond', 'can', 'be', 'subdivided', 'into', 'parts', 'differing', 'in', 'at', 'least', 'one', ... | [-0.11127829165467652, 0.170972509980546, -0.0754228890447582, 0.09042346746364052, 0.013060514915950323, -0.15265526673926905, 0.040975264583078284, 0.3646601862955566, -0.29220333665314063, -0.2683339638169855, 0.03870494203448931, -0.3024507954364597, -0.11166083708507712, 0.17879600590946743, 0.011428268225444765, ... |
710.1978 | The Role of Lepton Flavours in Thermal Leptogenesis | Thermal leptogenesis, that can be viewed as a consequence of the seesaw
model, is a very natural mechanism to explain the matter anti-matter asymmetry
of the Universe. Recently, lepton flavours have been included in the Boltzmann
equations, modifying significantly the evaluation of the efficiency of
leptogenesis to e... | hep-ph | thermal leptogenesis that can be viewed as a consequence of the seesaw model is a very natural mechanism to explain the matter antimatter asymmetry of the universe recently lepton flavours have been included in the boltzmann equations modifying significantly the evaluation of the efficiency of leptogenesis to explain t... | [['thermal', 'leptogenesis', 'that', 'can', 'be', 'viewed', 'as', 'a', 'consequence', 'of', 'the', 'seesaw', 'model', 'is', 'a', 'very', 'natural', 'mechanism', 'to', 'explain', 'the', 'matter', 'antimatter', 'asymmetry', 'of', 'the', 'universe', 'recently', 'lepton', 'flavours', 'have', 'been', 'included', 'in', 'the'... | [-0.08161033291029386, 0.21050835891555136, -0.12717905139120725, 0.2021461020944676, -0.11005187131321201, -0.13368434310317612, 0.021887682217101637, 0.2570710200816393, -0.2597039079007048, -0.3265185396034772, -0.0012261046548911298, -0.22397242203498116, -0.009774688452195663, 0.12643248476356697, 0.00308079039677... |
710.1979 | Groups with the Minimal Conditions for Subgroups and for Nonabelian
Subgroups | For some very wide classes $\mathfrak{D}$ and
$\mathfrak{B}\subset\mathfrak{D}$ of groups, the author proves that an
arbitrary (nonabelian) group $G\in \mathfrak{D}$ (respectively $G\in
\mathfrak{B}$) satisfies the minimal condition for (nonabelian) subgroups iff
it is Chernikov
| math.GR | for some very wide classes mathfrakd and mathfrakbsubsetmathfrakd of groups the author proves that an arbitrary nonabelian group gin mathfrakd respectively gin mathfrakb satisfies the minimal condition for nonabelian subgroups iff it is chernikov | [['for', 'some', 'very', 'wide', 'classes', 'mathfrakd', 'and', 'mathfrakbsubsetmathfrakd', 'of', 'groups', 'the', 'author', 'proves', 'that', 'an', 'arbitrary', 'nonabelian', 'group', 'gin', 'mathfrakd', 'respectively', 'gin', 'mathfrakb', 'satisfies', 'the', 'minimal', 'condition', 'for', 'nonabelian', 'subgroups', '... | [-0.2539758083382339, 0.1687883723877321, -0.06715636141598225, 0.06360140783274829, -0.1480230607769706, -0.2059782613068819, -0.051997387471298374, 0.3824777938778315, -0.2794025869983615, -0.16409558514979752, 0.07659941039288021, -0.2640960972869035, -0.08520669728573976, 0.22334051072936167, -0.17425370357479109, ... |
710.198 | The critical behavior of 3D Ising glass models: universality and scaling
corrections | We perform high-statistics Monte Carlo simulations of three three-dimensional
Ising spin-glass models: the +-J Ising model for two values of the disorder
parameter p, p=1/2 and p=0.7, and the bond-diluted +-J model for
bond-occupation probability p_b = 0.45. A finite-size scaling analysis of the
quartic cumulants at ... | cond-mat.dis-nn cond-mat.stat-mech | we perform highstatistics monte carlo simulations of three threedimensional ising spinglass models the j ising model for two values of the disorder parameter p p12 and p07 and the bonddiluted j model for bondoccupation probability p_b 045 a finitesize scaling analysis of the quartic cumulants at the critical point show... | [['we', 'perform', 'highstatistics', 'monte', 'carlo', 'simulations', 'of', 'three', 'threedimensional', 'ising', 'spinglass', 'models', 'the', 'j', 'ising', 'model', 'for', 'two', 'values', 'of', 'the', 'disorder', 'parameter', 'p', 'p12', 'and', 'p07', 'and', 'the', 'bonddiluted', 'j', 'model', 'for', 'bondoccupation... | [-0.11422543482773978, 0.15940706711262465, -0.09738326697539457, 0.10764908866511415, -0.01108489452124796, -0.20655836697931038, 0.0934966892287459, 0.2908122803492006, -0.19678889849709105, -0.2667284023279891, 0.025820934803366825, -0.3450739452966208, -0.08847894813959062, 0.1625366721988109, 0.10591206872714279, ... |
710.1981 | Oriented matroids and Ky Fan's theorem | L. Lovasz has shown that Sperner's combinatorial lemma admits a
generalization involving a matroid defined on the set of vertices of the
associated triangulation. Inspired by this result we prove that classical Ky
Fan's theorem admits an oriented matroid generalization of similar nature. Ky
Fan's theorem is obtained ... | math.CO math.AT | l lovasz has shown that sperners combinatorial lemma admits a generalization involving a matroid defined on the set of vertices of the associated triangulation inspired by this result we prove that classical ky fans theorem admits an oriented matroid generalization of similar nature ky fans theorem is obtained as a cor... | [['l', 'lovasz', 'has', 'shown', 'that', 'sperners', 'combinatorial', 'lemma', 'admits', 'a', 'generalization', 'involving', 'a', 'matroid', 'defined', 'on', 'the', 'set', 'of', 'vertices', 'of', 'the', 'associated', 'triangulation', 'inspired', 'by', 'this', 'result', 'we', 'prove', 'that', 'classical', 'ky', 'fans', ... | [-0.18934388250454504, 0.029859127864483526, -0.10092223578249104, 0.10108904273693042, -0.17913555543054827, -0.13346388958234456, 0.04798544850200415, 0.29631865335977636, -0.39304203359643, -0.25202291694586165, 0.07901610612680088, -0.21783429987772251, -0.22450183602632023, 0.16339794345549308, -0.2406191382469842... |
710.1982 | Comparing SU(2) to SU(3) gluodynamics on large lattices | We study the SU(2) gluon and ghost propagators in Landau gauge on lattices up
to a size of 112^4. A comparison with the SU(3) case is made and finite-volume
effects are then investigated. We find that for a large range of momenta the
SU(2) and SU(3) propagators are remarkably alike. In the low-momentum region we
comp... | hep-lat | we study the su2 gluon and ghost propagators in landau gauge on lattices up to a size of 1124 a comparison with the su3 case is made and finitevolume effects are then investigated we find that for a large range of momenta the su2 and su3 propagators are remarkably alike in the lowmomentum region we compare with recent ... | [['we', 'study', 'the', 'su2', 'gluon', 'and', 'ghost', 'propagators', 'in', 'landau', 'gauge', 'on', 'lattices', 'up', 'to', 'a', 'size', 'of', '1124', 'a', 'comparison', 'with', 'the', 'su3', 'case', 'is', 'made', 'and', 'finitevolume', 'effects', 'are', 'then', 'investigated', 'we', 'find', 'that', 'for', 'a', 'larg... | [-0.10977292891986894, 0.21371800770672658, -0.11543878309682688, 0.09988421469284786, -0.04184436798095703, -0.05936104529113932, 0.030486232565828796, 0.4443569469237418, -0.08475293422816321, -0.22621192266656595, 0.06609871911738689, -0.30254793725202256, -0.08655682685926105, 0.1345238326202062, 0.0275147986332850... |
710.1983 | The quantum-classical crossover of a field mode | We explore the quantum-classical crossover in the behaviour of a quantum
field mode. The quantum behaviour of a two-state system - a qubit - coupled to
the field is used as a probe. Collapse and revival of the qubit inversion form
the signature for quantum behaviour of the field and continuous Rabi
oscillations form ... | quant-ph | we explore the quantumclassical crossover in the behaviour of a quantum field mode the quantum behaviour of a twostate system a qubit coupled to the field is used as a probe collapse and revival of the qubit inversion form the signature for quantum behaviour of the field and continuous rabi oscillations form the signat... | [['we', 'explore', 'the', 'quantumclassical', 'crossover', 'in', 'the', 'behaviour', 'of', 'a', 'quantum', 'field', 'mode', 'the', 'quantum', 'behaviour', 'of', 'a', 'twostate', 'system', 'a', 'qubit', 'coupled', 'to', 'the', 'field', 'is', 'used', 'as', 'a', 'probe', 'collapse', 'and', 'revival', 'of', 'the', 'qubit',... | [-0.180113384169009, 0.1719930579057998, -0.07026712868052225, 0.043505982999017256, -0.0077872212665776415, -0.15863434824471673, 0.053631685925130214, 0.3062587856211596, -0.22719124238938093, -0.2562249239378919, 0.05128835490775398, -0.21959446602397495, -0.11597669008705351, 0.22031204907171842, 0.0537312014752792... |
710.1984 | Density modulations in an elongated Bose-Einstein condensate released
from a disordered potential | We observe large density modulations in time-of-flight images of elongated
Bose-Einstein condensates, initially confined in a harmonic trap and in the
presence of weak disorder. The development of these modulations during the
time-of-flight and their dependence with the disorder are investigated. We
render an account... | cond-mat.other quant-ph | we observe large density modulations in timeofflight images of elongated boseeinstein condensates initially confined in a harmonic trap and in the presence of weak disorder the development of these modulations during the timeofflight and their dependence with the disorder are investigated we render an account of this e... | [['we', 'observe', 'large', 'density', 'modulations', 'in', 'timeofflight', 'images', 'of', 'elongated', 'boseeinstein', 'condensates', 'initially', 'confined', 'in', 'a', 'harmonic', 'trap', 'and', 'in', 'the', 'presence', 'of', 'weak', 'disorder', 'the', 'development', 'of', 'these', 'modulations', 'during', 'the', '... | [-0.1700205348006645, 0.27214906162479574, -0.09464820620408397, 0.06970361381464488, 0.04379596784250972, -0.0849224679045563, 0.0025455481027839362, 0.3799839013336617, -0.23505188295916643, -0.2821516209960352, 0.061445360860994294, -0.29200438662995526, -0.13602462782593513, 0.12176731349555431, 0.03835738642302192... |
710.1985 | Dynamics of Mandelbrot Cascades | Mandelbrot multiplicative cascades provide a construction of a dynamical
system on a set of probability measures defined by inequalities on moments. To
be more specific, beyond the first iteration, the trajectories take values in
the set of fixed points of smoothing transformations (i.e., some generalized
stable laws... | math.PR math.DS | mandelbrot multiplicative cascades provide a construction of a dynamical system on a set of probability measures defined by inequalities on moments to be more specific beyond the first iteration the trajectories take values in the set of fixed points of smoothing transformations ie some generalized stable laws studying... | [['mandelbrot', 'multiplicative', 'cascades', 'provide', 'a', 'construction', 'of', 'a', 'dynamical', 'system', 'on', 'a', 'set', 'of', 'probability', 'measures', 'defined', 'by', 'inequalities', 'on', 'moments', 'to', 'be', 'more', 'specific', 'beyond', 'the', 'first', 'iteration', 'the', 'trajectories', 'take', 'valu... | [-0.1246949804613744, 0.0920358365712926, -0.14909153945649725, 0.09248118737614967, -0.02073586877447235, -0.11008255599992044, 0.12699090271651792, 0.25299689588667473, -0.3079593281579923, -0.23697801095822565, 0.10592389905300652, -0.2534603002817146, -0.11974424037705117, 0.22351424478560308, -0.08075500981546231,... |
710.1986 | A dual eigenvector condition for strong lumpability of Markov chains | Necessary and sufficient conditions for identifying strong lumpability in
Markov chains are presented. We show that the states in a lump necessarily
correspond to identical elements in eigenvectors of the dual transition matrix.
If there exist as many dual eigenvectors that respect the necessary condition
as there ar... | math.PR | necessary and sufficient conditions for identifying strong lumpability in markov chains are presented we show that the states in a lump necessarily correspond to identical elements in eigenvectors of the dual transition matrix if there exist as many dual eigenvectors that respect the necessary condition as there are lu... | [['necessary', 'and', 'sufficient', 'conditions', 'for', 'identifying', 'strong', 'lumpability', 'in', 'markov', 'chains', 'are', 'presented', 'we', 'show', 'that', 'the', 'states', 'in', 'a', 'lump', 'necessarily', 'correspond', 'to', 'identical', 'elements', 'in', 'eigenvectors', 'of', 'the', 'dual', 'transition', 'm... | [-0.12885002855380828, 0.1749857607100046, -0.02503293151543899, 0.10438450313328455, -0.02102420162621208, -0.1709664460539705, -0.027312908723781056, 0.42092001161566284, -0.23430161830037832, -0.20249257592050443, 0.16023835672460723, -0.24466663965898933, -0.20049513232978908, 0.13234988997944377, -0.04043269704914... |
710.1987 | Resonances in twisted quantum waveguides | In this paper we consider embedded eigenvalues of a Schroedinger Hamiltonian
in a waveguide induced by a symmetric perturbation. It is shown that these
eigenvalues become unstable and turn into resonances after twisting of the
waveguide. The perturbative expansion of the resonance width is calculated for
weakly twist... | math-ph math.MP | in this paper we consider embedded eigenvalues of a schroedinger hamiltonian in a waveguide induced by a symmetric perturbation it is shown that these eigenvalues become unstable and turn into resonances after twisting of the waveguide the perturbative expansion of the resonance width is calculated for weakly twisted w... | [['in', 'this', 'paper', 'we', 'consider', 'embedded', 'eigenvalues', 'of', 'a', 'schroedinger', 'hamiltonian', 'in', 'a', 'waveguide', 'induced', 'by', 'a', 'symmetric', 'perturbation', 'it', 'is', 'shown', 'that', 'these', 'eigenvalues', 'become', 'unstable', 'and', 'turn', 'into', 'resonances', 'after', 'twisting', ... | [-0.18237562908683547, 0.18436625849169033, -0.057202510678997405, 0.057717549016412635, -0.020968964667274402, -0.10581225355943809, -0.038680385151663076, 0.4110119999887852, -0.20943528067034026, -0.19122674152828179, 0.07111241364350113, -0.27813106105089763, -0.16972413373967776, 0.14840196468867362, 0.01966067555... |
710.1988 | Deflated BiCGStab for linear equations in QCD problems | The large systems of complex linear equations that are generated in QCD
problems often have multiple right-hand sides (for multiple sources) and
multiple shifts (for multiple masses). Deflated GMRES methods have previously
been developed for solving multiple right-hand sides. Eigenvectors are
generated during solutio... | hep-lat | the large systems of complex linear equations that are generated in qcd problems often have multiple righthand sides for multiple sources and multiple shifts for multiple masses deflated gmres methods have previously been developed for solving multiple righthand sides eigenvectors are generated during solution of the f... | [['the', 'large', 'systems', 'of', 'complex', 'linear', 'equations', 'that', 'are', 'generated', 'in', 'qcd', 'problems', 'often', 'have', 'multiple', 'righthand', 'sides', 'for', 'multiple', 'sources', 'and', 'multiple', 'shifts', 'for', 'multiple', 'masses', 'deflated', 'gmres', 'methods', 'have', 'previously', 'been... | [-0.09031922471951004, 0.09313694858089244, -0.03372211493206797, 0.03809457022300059, -0.11347124724200479, -0.19539361155971333, -0.020115873452138017, 0.40877364245415837, -0.32381012771899503, -0.23809759981447348, 0.1873994815154691, -0.3220696965508439, -0.1007595710111437, 0.22551560884134636, -0.026163269358652... |
710.1989 | Banach algebras of pseudodifferential operators and their almost
diagonalization | We define new symbol classes for pseudodifferntial operators and investigate
their pseudodifferential calculus. The symbol classes are parametrized by
commutative convolution algebras. To every solid convolution algebra over a
lattice we associate a symbol class. Then every operator with such a symbol is
almost diago... | math.FA math.OA | we define new symbol classes for pseudodifferntial operators and investigate their pseudodifferential calculus the symbol classes are parametrized by commutative convolution algebras to every solid convolution algebra over a lattice we associate a symbol class then every operator with such a symbol is almost diagonal w... | [['we', 'define', 'new', 'symbol', 'classes', 'for', 'pseudodifferntial', 'operators', 'and', 'investigate', 'their', 'pseudodifferential', 'calculus', 'the', 'symbol', 'classes', 'are', 'parametrized', 'by', 'commutative', 'convolution', 'algebras', 'to', 'every', 'solid', 'convolution', 'algebra', 'over', 'a', 'latti... | [-0.15821071570077777, 0.07865657082774029, -0.047684264558272946, 0.1011053252445561, -0.1220423868364668, -0.14337017415496317, -0.010898200036667666, 0.3331011151962414, -0.369341550340903, -0.14121872730227525, 0.16258729970001656, -0.2727490318213603, -0.1566623773044515, 0.194853618840579, -0.13800982493178351, 0... |
710.199 | Non-compact Gepner Models, Landau-Ginzburg Orbifolds and Mirror Symmetry | We study non-compact Gepner models that preserve sixteen or eight
supercharges in type II string theories. In particular, we develop an
orbifolded Landau-Ginzburg description of these models analogous to the
Landau-Ginzburg formulation of compact Gepner models. The Landau-Ginzburg
description provides an easy and dir... | hep-th | we study noncompact gepner models that preserve sixteen or eight supercharges in type ii string theories in particular we develop an orbifolded landauginzburg description of these models analogous to the landauginzburg formulation of compact gepner models the landauginzburg description provides an easy and direct acces... | [['we', 'study', 'noncompact', 'gepner', 'models', 'that', 'preserve', 'sixteen', 'or', 'eight', 'supercharges', 'in', 'type', 'ii', 'string', 'theories', 'in', 'particular', 'we', 'develop', 'an', 'orbifolded', 'landauginzburg', 'description', 'of', 'these', 'models', 'analogous', 'to', 'the', 'landauginzburg', 'formu... | [-0.11606515544950019, 0.06943884110651082, -0.11294795702435548, 0.14982858984775346, -0.1043832311951968, -0.17877459691106518, -0.026114227462418472, 0.3102556668705295, -0.19499078443674725, -0.25551611324403833, 0.08403413754495898, -0.23241681872301181, -0.15759879158061185, 0.13913151497150994, -0.14233411503425... |
710.1991 | Large spin expansion of the long-range Baxter equation in the sl(2)
sector of N=4 SYM | Recently, several multi-loop conjectures have been proposed for the spin
dependence of anomalous dimensions of twist-2 and 3 operators in the sl(2)
sector of N=4 SYM. Currently, these conjectures are not proven, although
several consistency checks have been performed on their large spin expansion.
In this paper, we s... | hep-th | recently several multiloop conjectures have been proposed for the spin dependence of anomalous dimensions of twist2 and 3 operators in the sl2 sector of n4 sym currently these conjectures are not proven although several consistency checks have been performed on their large spin expansion in this paper we show how these... | [['recently', 'several', 'multiloop', 'conjectures', 'have', 'been', 'proposed', 'for', 'the', 'spin', 'dependence', 'of', 'anomalous', 'dimensions', 'of', 'twist2', 'and', '3', 'operators', 'in', 'the', 'sl2', 'sector', 'of', 'n4', 'sym', 'currently', 'these', 'conjectures', 'are', 'not', 'proven', 'although', 'severa... | [-0.12452512478200406, 0.12020911734584158, -0.08168312488947954, 0.09896986834103225, -0.07502443074100379, -0.09811390353834454, -0.031530901092203516, 0.3788865694726727, -0.19232268101098923, -0.2925541204507504, 0.13310672448375221, -0.2722501709245442, -0.1545538054531918, 0.1613862778933768, 0.007112123550171346... |
710.1992 | Self-consistent Mean Field theory in weakly ionized media | We present a self-consistent mean field theory of the dynamo in 3D and
turbulent diffusion in 2D in weakly ionized gas. We find that in 3D, the
backreaction does not alter the beta effect while it suppresses the alpha
effect when the strength of a mean magnetic field exceeds a critical value.
These results suggest th... | astro-ph | we present a selfconsistent mean field theory of the dynamo in 3d and turbulent diffusion in 2d in weakly ionized gas we find that in 3d the backreaction does not alter the beta effect while it suppresses the alpha effect when the strength of a mean magnetic field exceeds a critical value these results suggest that a m... | [['we', 'present', 'a', 'selfconsistent', 'mean', 'field', 'theory', 'of', 'the', 'dynamo', 'in', '3d', 'and', 'turbulent', 'diffusion', 'in', '2d', 'in', 'weakly', 'ionized', 'gas', 'we', 'find', 'that', 'in', '3d', 'the', 'backreaction', 'does', 'not', 'alter', 'the', 'beta', 'effect', 'while', 'it', 'suppresses', 't... | [-0.10896651282255015, 0.2160509078183391, -0.010387258888314184, 0.07537040462321193, -0.02626956310613375, -0.07588667337570273, 0.010642133180354313, 0.3448051332757531, -0.24902136164733715, -0.2864781403914094, 0.016554667665459738, -0.23464715725889332, -0.1119142609154152, 0.20684390073936237, 0.0260508262977134... |
710.1993 | A turbulent model of torque in von Karman swirling flow | A stochastic model is derived to predict the turbulent torque produced by a
swirling flow. It is a simple Langevin process, with a colored noise. Using the
unified colored noise approximation, we derive analytically the PDF of the
fluctuations of injected power in two forcing regimes: constant angular
velocity or con... | physics.flu-dyn cond-mat.other | a stochastic model is derived to predict the turbulent torque produced by a swirling flow it is a simple langevin process with a colored noise using the unified colored noise approximation we derive analytically the pdf of the fluctuations of injected power in two forcing regimes constant angular velocity or constant a... | [['a', 'stochastic', 'model', 'is', 'derived', 'to', 'predict', 'the', 'turbulent', 'torque', 'produced', 'by', 'a', 'swirling', 'flow', 'it', 'is', 'a', 'simple', 'langevin', 'process', 'with', 'a', 'colored', 'noise', 'using', 'the', 'unified', 'colored', 'noise', 'approximation', 'we', 'derive', 'analytically', 'the... | [-0.17083064928738168, 0.16284026896270612, -0.10284627498509104, 0.03741656985672156, -0.038345513887987986, -0.14014749226043932, 0.0035366432760686926, 0.288163245552116, -0.2897196436258835, -0.27623741102999905, 0.05215688956377562, -0.26353333379099947, -0.08347062766066908, 0.20514377156764063, -0.02494960492185... |
710.1994 | Metric Dichotomies | These are notes from talks given at ICMS, Edinburgh, 4/2007 ("Geometry and
Algorithms workshop") and at Bernoulli Center, Lausanne 5/2007 ("Limits of
graphs in group theory and computer science"). We survey the following type of
dichotomies exhibited by certain classes X of finite metric spaces: For every
host space ... | math.MG | these are notes from talks given at icms edinburgh 42007 geometry and algorithms workshop and at bernoulli center lausanne 52007 limits of graphs in group theory and computer science we survey the following type of dichotomies exhibited by certain classes x of finite metric spaces for every host space h either all metr... | [['these', 'are', 'notes', 'from', 'talks', 'given', 'at', 'icms', 'edinburgh', '42007', 'geometry', 'and', 'algorithms', 'workshop', 'and', 'at', 'bernoulli', 'center', 'lausanne', '52007', 'limits', 'of', 'graphs', 'in', 'group', 'theory', 'and', 'computer', 'science', 'we', 'survey', 'the', 'following', 'type', 'of'... | [-0.11756021373341201, 0.10675542060823613, -0.044730703628451475, 0.037076915058464756, -0.058964161877848316, -0.15386897879718264, 0.02131943113964156, 0.4117820711780182, -0.2718276684795519, -0.30092482827603817, 0.15838877810821148, -0.3304905154361901, -0.11991949931679058, 0.19000548518813726, -0.13418467348756... |
710.1995 | Influence of corruption on economic growth rate and foreign investments | In order to investigate whether government regulations against corruption can
affect the economic growth of a country, we analyze the dependence between
Gross Domestic Product (GDP) per capita growth rates and changes in the
Corruption Perceptions Index (CPI). For the period 1999-2004 on average for all
countries in ... | q-fin.GN physics.data-an physics.soc-ph | in order to investigate whether government regulations against corruption can affect the economic growth of a country we analyze the dependence between gross domestic product gdp per capita growth rates and changes in the corruption perceptions index cpi for the period 19992004 on average for all countries in the world... | [['in', 'order', 'to', 'investigate', 'whether', 'government', 'regulations', 'against', 'corruption', 'can', 'affect', 'the', 'economic', 'growth', 'of', 'a', 'country', 'we', 'analyze', 'the', 'dependence', 'between', 'gross', 'domestic', 'product', 'gdp', 'per', 'capita', 'growth', 'rates', 'and', 'changes', 'in', '... | [-0.06089941049357513, 0.12025862859199943, -0.008822450257063685, 0.1287623191276541, 0.0192624713012997, -0.06872647375400577, 0.17715653828451072, 0.3291956284446279, -0.24341208688527732, -0.3557464086281305, 0.07709709405611789, -0.3573662372027802, -0.13995944694676377, 0.18680535611853777, -0.15535436840629652, ... |
710.1996 | Radius stabilization in 5D SUGRA models on orbifold | We study a four-dimensional effective theory of the five-dimensional (5D)
gauged supergravity with a universal hypermultiplet and perturbative
superpotential terms at the orbifold fixed points. The class of models we
consider includes the 5D heterotic M-theory and the supersymmetric
Randall-Sundrum model as special l... | hep-th hep-ph | we study a fourdimensional effective theory of the fivedimensional 5d gauged supergravity with a universal hypermultiplet and perturbative superpotential terms at the orbifold fixed points the class of models we consider includes the 5d heterotic mtheory and the supersymmetric randallsundrum model as special limits of ... | [['we', 'study', 'a', 'fourdimensional', 'effective', 'theory', 'of', 'the', 'fivedimensional', '5d', 'gauged', 'supergravity', 'with', 'a', 'universal', 'hypermultiplet', 'and', 'perturbative', 'superpotential', 'terms', 'at', 'the', 'orbifold', 'fixed', 'points', 'the', 'class', 'of', 'models', 'we', 'consider', 'inc... | [-0.12429367756204945, 0.11791834659608347, -0.007552551963765706, 0.1289581895273711, -0.08423489093173495, -0.1472089202409344, 0.010799360524729958, 0.2294706974910306, -0.15027832541880862, -0.2653655205055007, 0.0792330211361072, -0.25468577613854515, -0.19328981273408447, 0.06960995194302606, -0.09327087246679834... |
710.1997 | Roles of Higgs decay into two pseudoscalar bosons in the search of
intermediate-mass Higgs Boson | The dominance of $h\to \eta \eta$ decay mode for the intermediate mass Higgs
boson is highly motivated to solve the little hierarchy problem and to ease the
tension with the precision data. However, the discovery modes for $m_h \alt
150$ GeV, $h \to \gamma\gamma$ and $W/Z h \to (\ell\nu/\ell \bar \ell) (b\bar
b)$, wi... | hep-ph | the dominance of hto eta eta decay mode for the intermediate mass higgs boson is highly motivated to solve the little hierarchy problem and to ease the tension with the precision data however the discovery modes for m_h alt 150 gev h to gammagamma and wz h to ellnuell bar ell bbar b will be substantially affected we sh... | [['the', 'dominance', 'of', 'hto', 'eta', 'eta', 'decay', 'mode', 'for', 'the', 'intermediate', 'mass', 'higgs', 'boson', 'is', 'highly', 'motivated', 'to', 'solve', 'the', 'little', 'hierarchy', 'problem', 'and', 'to', 'ease', 'the', 'tension', 'with', 'the', 'precision', 'data', 'however', 'the', 'discovery', 'modes'... | [-0.045269886103467015, 0.239158027346379, -0.012760095105373433, 0.1725617165053596, -0.11273944417812995, -0.22674699749997151, 0.06210531523018809, 0.3339009735201086, -0.24244018208701162, -0.29702578515612654, 0.030743413349513762, -0.2804986846200856, 0.03877863349126918, 0.14615101096652713, 0.05190585537680558,... |
710.1998 | Entropy radiated by a braneworld black hole | The concept of black hole entropy is one of the most important enigmas of
theoretical physics. It relates thermodynamics to gravity and allows
substantial hints toward a quantum theory of gravitation. Although Bekenstein
conjecture -assuming the black hole entropy to be a measure of the number of
precollapse configur... | hep-th astro-ph gr-qc hep-ph | the concept of black hole entropy is one of the most important enigmas of theoretical physics it relates thermodynamics to gravity and allows substantial hints toward a quantum theory of gravitation although bekenstein conjecture assuming the black hole entropy to be a measure of the number of precollapse configuration... | [['the', 'concept', 'of', 'black', 'hole', 'entropy', 'is', 'one', 'of', 'the', 'most', 'important', 'enigmas', 'of', 'theoretical', 'physics', 'it', 'relates', 'thermodynamics', 'to', 'gravity', 'and', 'allows', 'substantial', 'hints', 'toward', 'a', 'quantum', 'theory', 'of', 'gravitation', 'although', 'bekenstein', ... | [-0.1158597066859938, 0.10491320964772531, -0.14240468849143215, 0.16749714082547415, -0.08246435483240268, -0.1793292105228694, 0.04639811951701706, 0.21812006587947697, -0.186388507636441, -0.32315789810420315, 0.0628001003252912, -0.2836545185006295, -0.08602286638184027, 0.1919844981883306, -0.09292439100417224, 0.... |
710.1999 | Non Linear Gauge Fixing for FeynArts | We review the non-linear gauge-fixing for the Standard Model, proposed by F.
Boudjema and E. Chopin, and present our implementation of this non-linear
gauge-fixing to the Standard Model and to the minimal supersymmetric Standard
Model in FeynArts.
| hep-ph | we review the nonlinear gaugefixing for the standard model proposed by f boudjema and e chopin and present our implementation of this nonlinear gaugefixing to the standard model and to the minimal supersymmetric standard model in feynarts | [['we', 'review', 'the', 'nonlinear', 'gaugefixing', 'for', 'the', 'standard', 'model', 'proposed', 'by', 'f', 'boudjema', 'and', 'e', 'chopin', 'and', 'present', 'our', 'implementation', 'of', 'this', 'nonlinear', 'gaugefixing', 'to', 'the', 'standard', 'model', 'and', 'to', 'the', 'minimal', 'supersymmetric', 'standa... | [-0.023076428048726585, 0.03415719583992743, -0.014317021963910924, 0.0449941705155652, -0.07511704394386874, -0.16902998741716146, 0.017063869803678244, 0.315430511888634, -0.23339568727209958, -0.317694617021415, 0.06548877782511732, -0.22836881544854906, -0.15669916477054358, 0.13387536415959606, -0.0839969590823683... |
710.2 | Atomic Hydrogen Properties of AGN Host Galaxies: HI in 16 NUclei of
GAlaxies (NUGA) Sources | We present a comprehensive spectroscopic imaging survey of the distribution
and kinematics of atomic hydrogen (HI) in 16 nearby spiral galaxies hosting low
luminosity AGN, observed with high spectral and spatial resolution (resolution:
~20 arcsec, 5 km/s) using the NRAO Very Large Array (VLA). The sample contains
a r... | astro-ph | we present a comprehensive spectroscopic imaging survey of the distribution and kinematics of atomic hydrogen hi in 16 nearby spiral galaxies hosting low luminosity agn observed with high spectral and spatial resolution resolution 20 arcsec 5 kms using the nrao very large array vla the sample contains a range of nuclea... | [['we', 'present', 'a', 'comprehensive', 'spectroscopic', 'imaging', 'survey', 'of', 'the', 'distribution', 'and', 'kinematics', 'of', 'atomic', 'hydrogen', 'hi', 'in', '16', 'nearby', 'spiral', 'galaxies', 'hosting', 'low', 'luminosity', 'agn', 'observed', 'with', 'high', 'spectral', 'and', 'spatial', 'resolution', 'r... | [-0.046579251892075665, 0.03542258580300431, -0.028836833263523185, 0.12312593510392213, -0.09351627497515572, -0.064515717055959, 0.005016294690668238, 0.5095858591354314, -0.09226934918357681, -0.3354090410112231, 0.04091691990766709, -0.2962738468699239, -0.011215371229843219, 0.15286103498941953, 0.0191656164674053... |
710.2001 | Time evolution and decoherence of a spin-1/2 particle coupled to a spin
bath in thermal equilibrium | The time evolution of a spin-1/2 particle under the influence of a locally
applied external magnetic field, and interacting with anisotropic spin
environment in thermal equilibrium at temperature $T$ is studied. The exact
analytical form of the reduced density matrix of the central spin is calculated
explicitly for f... | quant-ph | the time evolution of a spin12 particle under the influence of a locally applied external magnetic field and interacting with anisotropic spin environment in thermal equilibrium at temperature t is studied the exact analytical form of the reduced density matrix of the central spin is calculated explicitly for finite nu... | [['the', 'time', 'evolution', 'of', 'a', 'spin12', 'particle', 'under', 'the', 'influence', 'of', 'a', 'locally', 'applied', 'external', 'magnetic', 'field', 'and', 'interacting', 'with', 'anisotropic', 'spin', 'environment', 'in', 'thermal', 'equilibrium', 'at', 'temperature', 't', 'is', 'studied', 'the', 'exact', 'an... | [-0.18678396465817004, 0.23326851537941756, -0.06261280220906999, 0.04502259875311607, 0.013246905112891156, -0.06943595848445382, 0.01633737130874866, 0.3358858288790947, -0.2440216839506074, -0.24843422221054876, 0.05642979045020402, -0.27807100997411444, -0.04123225600521704, 0.14684757838792456, 0.08327361761550314... |
710.2002 | Transverse-momentum, threshold and joint resummations for slepton pair
production at hadron colliders | We present precision calculations of the transverse-momentum spectrum and the
invariant-mass distribution for slepton pair production at hadron colliders. We
implement the transverse-momentum, threshold and joint resummation formalisms
at the next-to-leading logarithmic accuracy and consistently match the obtained
re... | hep-ph | we present precision calculations of the transversemomentum spectrum and the invariantmass distribution for slepton pair production at hadron colliders we implement the transversemomentum threshold and joint resummation formalisms at the nexttoleading logarithmic accuracy and consistently match the obtained result with... | [['we', 'present', 'precision', 'calculations', 'of', 'the', 'transversemomentum', 'spectrum', 'and', 'the', 'invariantmass', 'distribution', 'for', 'slepton', 'pair', 'production', 'at', 'hadron', 'colliders', 'we', 'implement', 'the', 'transversemomentum', 'threshold', 'and', 'joint', 'resummation', 'formalisms', 'at... | [-0.05364002887076006, 0.13172113904371285, -0.09491423012402195, 0.14620287427439904, 0.010830738122025743, -0.1011552266128815, 0.00011595459065388124, 0.36927651301121867, -0.17288091618758747, -0.2836975666622703, -0.05817157446961993, -0.3605100500564545, 0.07040287079647757, 0.11541657329787715, 0.104406733627025... |
710.2003 | CMB Anisotropies and Inflation from Non-Standard Spinors | The apparent alignment of the cosmic microwave background multipoles on large
scales challenges the standard cosmological model. Scalar field inflation is
isotropic and cannot account for the observed alignment. We explore the
imprints, a non-standard spinor driven inflation would leave on the cosmic
microwave backgr... | astro-ph gr-qc hep-ph hep-th | the apparent alignment of the cosmic microwave background multipoles on large scales challenges the standard cosmological model scalar field inflation is isotropic and cannot account for the observed alignment we explore the imprints a nonstandard spinor driven inflation would leave on the cosmic microwave background a... | [['the', 'apparent', 'alignment', 'of', 'the', 'cosmic', 'microwave', 'background', 'multipoles', 'on', 'large', 'scales', 'challenges', 'the', 'standard', 'cosmological', 'model', 'scalar', 'field', 'inflation', 'is', 'isotropic', 'and', 'can', 'not', 'account', 'for', 'the', 'observed', 'alignment', 'we', 'explore', ... | [-0.18212099683781466, 0.1969736866164891, -0.09626106303934565, 0.14057107067709768, -0.1308531544851032, -0.06062547108907809, -0.12001237396322105, 0.2967376299416539, -0.25727366981492644, -0.2895497442490753, 0.017545887220907826, -0.26334619615226984, -0.05630732928242149, 0.16606060743342613, 0.05406874224500752... |
710.2004 | Optimality of private quantum channels | We addressed the question of optimality of private quantum channels. We have
shown that the Shannon entropy of the classical key necessary to securely
transfer the quantum information is lower bounded by the entropy exchange of
the private quantum channel $\cal E$ and von Neumann entropy of the ciphertext
state $\var... | quant-ph | we addressed the question of optimality of private quantum channels we have shown that the shannon entropy of the classical key necessary to securely transfer the quantum information is lower bounded by the entropy exchange of the private quantum channel cal e and von neumann entropy of the ciphertext state varrho0 bas... | [['we', 'addressed', 'the', 'question', 'of', 'optimality', 'of', 'private', 'quantum', 'channels', 'we', 'have', 'shown', 'that', 'the', 'shannon', 'entropy', 'of', 'the', 'classical', 'key', 'necessary', 'to', 'securely', 'transfer', 'the', 'quantum', 'information', 'is', 'lower', 'bounded', 'by', 'the', 'entropy', '... | [-0.18113800950483477, 0.1333508201142526, -0.0487772830888445, 0.050864896828302954, 0.025464279680616327, -0.24656518968397084, 0.10606031330951984, 0.3166262436856481, -0.269870941216747, -0.22903252372311222, 0.08546290217530857, -0.2899551012633759, -0.06703055420614502, 0.20659250488366793, -0.08357755306326313, ... |
710.2005 | Hidden Fermion in Stueckelberg Z' Models as Milli-charged Dark Matter | The hidden Stueckelberg Z' model is augmented by a pair of Dirac fermions. If
the Z' has a coupling strength comparable to weak scale coupling, one can show
that this hidden fermion-antifermion pair could be a milli-charged dark matter
candidate with a viable relic density. Monochromatic photon flux coming from
the G... | hep-ph | the hidden stueckelberg z model is augmented by a pair of dirac fermions if the z has a coupling strength comparable to weak scale coupling one can show that this hidden fermionantifermion pair could be a millicharged dark matter candidate with a viable relic density monochromatic photon flux coming from the galactic c... | [['the', 'hidden', 'stueckelberg', 'z', 'model', 'is', 'augmented', 'by', 'a', 'pair', 'of', 'dirac', 'fermions', 'if', 'the', 'z', 'has', 'a', 'coupling', 'strength', 'comparable', 'to', 'weak', 'scale', 'coupling', 'one', 'can', 'show', 'that', 'this', 'hidden', 'fermionantifermion', 'pair', 'could', 'be', 'a', 'mill... | [-0.11701944870934501, 0.292859530493874, -0.05585929188588313, 0.14333695169751018, -0.12188883040678399, -0.18507471421516725, 0.009998443002555648, 0.3437518504175261, -0.25810383167117834, -0.2848405158227502, -0.03703424749606899, -0.30107394267066284, 0.03626659497265415, 0.12861814071897995, 0.13726468457928698,... |
710.2006 | Hyperflares of SGRs as an engine for millisecond extragalactic radio
bursts | We propose that the strong millisecond extragalactic radio burst (mERB)
discovered by Lorimer et al. (2007) may be related to a hyperflare from an
extragalactic soft gamma-ray repeater. The expected rate of such hyperflares,
$\sim$ 20 - 100 d$^{-1}$ Gpc$^{-3}$, is in good correspondence with the value
estimated by Lo... | astro-ph | we propose that the strong millisecond extragalactic radio burst merb discovered by lorimer et al 2007 may be related to a hyperflare from an extragalactic soft gammaray repeater the expected rate of such hyperflares sim 20 100 d1 gpc3 is in good correspondence with the value estimated by lorimer et al the possible mec... | [['we', 'propose', 'that', 'the', 'strong', 'millisecond', 'extragalactic', 'radio', 'burst', 'merb', 'discovered', 'by', 'lorimer', 'et', 'al', '2007', 'may', 'be', 'related', 'to', 'a', 'hyperflare', 'from', 'an', 'extragalactic', 'soft', 'gammaray', 'repeater', 'the', 'expected', 'rate', 'of', 'such', 'hyperflares',... | [-0.07851511429180391, 0.17738967632385538, -0.011949863522507561, 0.13484314514425932, -0.13059601324736528, -0.061700911304797046, 0.08400535331262897, 0.37269928787524503, -0.2062427921652367, -0.3911866931982028, 0.05460348490790542, -0.26793031705892645, -0.07401679702646409, 0.2646854350847813, -0.066956245015414... |
710.2007 | The wave equation on singular space-times | We prove local unique solvability of the wave equation for a large class of
weakly singular, locally bounded space-time metrics in a suitable space of
generalised functions.
| math-ph gr-qc math.AP math.MP | we prove local unique solvability of the wave equation for a large class of weakly singular locally bounded spacetime metrics in a suitable space of generalised functions | [['we', 'prove', 'local', 'unique', 'solvability', 'of', 'the', 'wave', 'equation', 'for', 'a', 'large', 'class', 'of', 'weakly', 'singular', 'locally', 'bounded', 'spacetime', 'metrics', 'in', 'a', 'suitable', 'space', 'of', 'generalised', 'functions']] | [-0.21521129217688684, 0.08601969525355983, -0.05324549821239931, 0.11366663424781075, -0.12950474803370457, -0.1187139424253945, -0.04965929233434575, 0.27172951207116797, -0.3469397905800078, -0.10934153716597292, 0.10505533922265319, -0.22656476025090175, -0.15965637426685403, 0.20072847218425185, -0.025237090333744... |
710.2008 | Statistical Relaxation in Closed Quantum Systems and the Van Hove-Limit | We analyze the dynamics of occupation probabilities for a certain type of
design models by the use of two different methods. On the one hand we present
some numerical calculations for two concrete interactions which point out that
the occurrence of statistical dynamics depends on the interaction structure.
Furthermor... | cond-mat.stat-mech | we analyze the dynamics of occupation probabilities for a certain type of design models by the use of two different methods on the one hand we present some numerical calculations for two concrete interactions which point out that the occurrence of statistical dynamics depends on the interaction structure furthermore we... | [['we', 'analyze', 'the', 'dynamics', 'of', 'occupation', 'probabilities', 'for', 'a', 'certain', 'type', 'of', 'design', 'models', 'by', 'the', 'use', 'of', 'two', 'different', 'methods', 'on', 'the', 'one', 'hand', 'we', 'present', 'some', 'numerical', 'calculations', 'for', 'two', 'concrete', 'interactions', 'which'... | [-0.1408461836116338, 0.07144033378092383, -0.11565891962743842, 0.08528440886151951, 0.0009029359128829595, -0.07767792412935681, 0.0594642949180451, 0.34451085361777933, -0.24131955080539794, -0.2670839701754016, 0.07465849123184091, -0.2837489570516187, -0.18015494424144965, 0.23295769881696213, 0.04218125170902223,... |
710.2009 | DBI Inflation using a One-Parameter Family of Throat Geometries | We demonstrate the possibility of examining cosmological signatures in the
DBI inflation setup using the BGMPZ solution, a one-parameter family of
geometries for the warped throat which interpolate between the Maldacena-Nunez
and Klebanov-Strassler solutions. The warp factor is determined numerically and
subsequently... | hep-th astro-ph hep-ph | we demonstrate the possibility of examining cosmological signatures in the dbi inflation setup using the bgmpz solution a oneparameter family of geometries for the warped throat which interpolate between the maldacenanunez and klebanovstrassler solutions the warp factor is determined numerically and subsequently used t... | [['we', 'demonstrate', 'the', 'possibility', 'of', 'examining', 'cosmological', 'signatures', 'in', 'the', 'dbi', 'inflation', 'setup', 'using', 'the', 'bgmpz', 'solution', 'a', 'oneparameter', 'family', 'of', 'geometries', 'for', 'the', 'warped', 'throat', 'which', 'interpolate', 'between', 'the', 'maldacenanunez', 'a... | [-0.10658861303005603, 0.091066387897307, -0.10993447234205952, 0.10955525011973674, -0.06925035917477028, -0.1448240939586482, -0.0030192061367251715, 0.3095413196815161, -0.24430881472522611, -0.3006330636279607, 0.09906369478542458, -0.26261696784111027, -0.12101568247669854, 0.19055289007368842, -0.0068249229324964... |
710.201 | NLO Event Simulation for Chargino Production at the ILC | We present an extension of the Monte Carlo Event Generator Whizard which
includes chargino production at the ILC at NLO. We include photons using both a
fixed order and a resummation approach. While the fixed order approach suffers
from negative event weights, the resummation method solves this problem and
automatica... | hep-ph | we present an extension of the monte carlo event generator whizard which includes chargino production at the ilc at nlo we include photons using both a fixed order and a resummation approach while the fixed order approach suffers from negative event weights the resummation method solves this problem and automatically i... | [['we', 'present', 'an', 'extension', 'of', 'the', 'monte', 'carlo', 'event', 'generator', 'whizard', 'which', 'includes', 'chargino', 'production', 'at', 'the', 'ilc', 'at', 'nlo', 'we', 'include', 'photons', 'using', 'both', 'a', 'fixed', 'order', 'and', 'a', 'resummation', 'approach', 'while', 'the', 'fixed', 'order... | [-0.03680427932751275, 0.07898950188871978, -0.09605578801804973, 0.1445917574656246, -0.03291331435383488, -0.06606031963301282, 0.04180183046827874, 0.38125089952041225, -0.21599881165731016, -0.31913504206765725, 0.06885179146117862, -0.36982439330188177, -0.034068274286685775, 0.16762602020816136, 0.003080741655061... |
710.2011 | The spatial string tension and dimensional reduction in QCD | The spatial string tension for 3+1 dimensional QCD at finite temperature is
measured. The gauge configurations we re generated with two light and one
heavier strange quark on lattices of size $16^3 4$ and $24^3 6$. This spatial
string tension is compared with the string tension of the 3 dimensional pure
gauge theory ... | hep-lat | the spatial string tension for 31 dimensional qcd at finite temperature is measured the gauge configurations we re generated with two light and one heavier strange quark on lattices of size 163 4 and 243 6 this spatial string tension is compared with the string tension of the 3 dimensional pure gauge theory together wi... | [['the', 'spatial', 'string', 'tension', 'for', '31', 'dimensional', 'qcd', 'at', 'finite', 'temperature', 'is', 'measured', 'the', 'gauge', 'configurations', 'we', 're', 'generated', 'with', 'two', 'light', 'and', 'one', 'heavier', 'strange', 'quark', 'on', 'lattices', 'of', 'size', '163', '4', 'and', '243', '6', 'thi... | [-0.08062418536024375, 0.30842310465717065, -0.04510244483632656, 0.06710940784735915, -0.021917998570845358, -0.1733013335097995, 0.048114704800860233, 0.34484182458577883, -0.1504713088248132, -0.31775125912908053, 0.06746497236761367, -0.3181156017300155, -0.004798625880438421, 0.10368817546340223, 0.038274607776353... |
710.2012 | Hamiltonian systems of hydrodynamic type in 2 + 1 dimensions | We investigate multi-dimensional Hamiltonian systems associated with constant
Poisson brackets of hydrodynamic type. A complete list of two- and
three-component integrable Hamiltonians is obtained. All our examples possess
dispersionless Lax pairs and an infinity of hydrodynamic reductions.
| nlin.SI math-ph math.DG math.MP | we investigate multidimensional hamiltonian systems associated with constant poisson brackets of hydrodynamic type a complete list of two and threecomponent integrable hamiltonians is obtained all our examples possess dispersionless lax pairs and an infinity of hydrodynamic reductions | [['we', 'investigate', 'multidimensional', 'hamiltonian', 'systems', 'associated', 'with', 'constant', 'poisson', 'brackets', 'of', 'hydrodynamic', 'type', 'a', 'complete', 'list', 'of', 'two', 'and', 'threecomponent', 'integrable', 'hamiltonians', 'is', 'obtained', 'all', 'our', 'examples', 'possess', 'dispersionless'... | [-0.22978341169151906, 0.05587179829544275, 0.022998695639339654, 0.11089095686298064, -0.09476473538607762, -0.1950259824484788, -0.07339099600810457, 0.32511030540272995, -0.28974123812607816, -0.21669074324135845, 0.01085680812546933, -0.3190438203714989, -0.16729781587885037, 0.17513447280067043, 0.0088059850842566... |
710.2013 | Sub-leading contributions to the black hole entropy in the brick wall
approach | [Abridged] We compute the canonical entropy of a quantum scalar field around
static and spherically symmetric black holes through the brick wall approach at
the higher orders (in fact, up to the sixth order in \hbar) in the WKB
approximation. We explicitly show that the brick wall model generally predicts
corrections... | gr-qc hep-th | abridged we compute the canonical entropy of a quantum scalar field around static and spherically symmetric black holes through the brick wall approach at the higher orders in fact up to the sixth order in hbar in the wkb approximation we explicitly show that the brick wall model generally predicts corrections to the b... | [['abridged', 'we', 'compute', 'the', 'canonical', 'entropy', 'of', 'a', 'quantum', 'scalar', 'field', 'around', 'static', 'and', 'spherically', 'symmetric', 'black', 'holes', 'through', 'the', 'brick', 'wall', 'approach', 'at', 'the', 'higher', 'orders', 'in', 'fact', 'up', 'to', 'the', 'sixth', 'order', 'in', 'hbar',... | [-0.10198647341200413, 0.09538407829782983, -0.08079473555571477, 0.09936065486639396, 0.003694219688906242, -0.09459157162239305, 0.003516122277555916, 0.2781343074046246, -0.17101200149600743, -0.29422454921997915, 0.06173381746750154, -0.3842580749774138, -0.09801292371978798, 0.16620932731649463, -0.065037229005958... |
710.2014 | Quantum Effects for the Dirac Field in Reissner-Nordstrom-AdS Black Hole
Background | The behavior of a charged massive Dirac field on a Reissner-Nordstrom-AdS
black hole background is investigated. The essential self-adjointness of the
Dirac Hamiltonian is studied. Then, an analysis of the discharge problem is
carried out in analogy with the standard Reissner-Nordstrom black hole case.
| gr-qc | the behavior of a charged massive dirac field on a reissnernordstromads black hole background is investigated the essential selfadjointness of the dirac hamiltonian is studied then an analysis of the discharge problem is carried out in analogy with the standard reissnernordstrom black hole case | [['the', 'behavior', 'of', 'a', 'charged', 'massive', 'dirac', 'field', 'on', 'a', 'reissnernordstromads', 'black', 'hole', 'background', 'is', 'investigated', 'the', 'essential', 'selfadjointness', 'of', 'the', 'dirac', 'hamiltonian', 'is', 'studied', 'then', 'an', 'analysis', 'of', 'the', 'discharge', 'problem', 'is'... | [-0.19414770534918221, 0.07075362747028438, -0.03604960610920733, 0.1319056610677349, -0.03423295881260525, -0.15434698072600772, -0.029654323049312967, 0.26861763643947517, -0.1211038865995678, -0.2520312131594189, 0.06985987850665962, -0.38872420466081664, -0.12169696305963126, 0.16335277140817858, -0.018023762375709... |
710.2015 | Structure and f-dependence of the a.c.i.m. for a unimodal map f of
Misiurewicz type | By using a suitable Banach space on which we let the transfer operator act,
we make a detailed study of the ergodic theory of a unimodal map $f$ of the
interval in the Misiurewicz case. We show in particular that the absolutely
continuous invariant measure $\rho$ can be written as the sum of 1/square root
spikes alon... | math.DS | by using a suitable banach space on which we let the transfer operator act we make a detailed study of the ergodic theory of a unimodal map f of the interval in the misiurewicz case we show in particular that the absolutely continuous invariant measure rho can be written as the sum of 1square root spikes along the crit... | [['by', 'using', 'a', 'suitable', 'banach', 'space', 'on', 'which', 'we', 'let', 'the', 'transfer', 'operator', 'act', 'we', 'make', 'a', 'detailed', 'study', 'of', 'the', 'ergodic', 'theory', 'of', 'a', 'unimodal', 'map', 'f', 'of', 'the', 'interval', 'in', 'the', 'misiurewicz', 'case', 'we', 'show', 'in', 'particular... | [-0.14577133849991533, 0.11224867610069804, -0.11651517801846449, 0.06435173766639753, -0.026163975660426494, -0.08811795847036709, 0.052071620243040316, 0.3697453379296722, -0.30756156175182414, -0.17700748893026358, 0.1341512016310261, -0.2635360382965957, -0.17143472310645172, 0.18629092960737836, -0.091654495276415... |
710.2016 | Decomposition of residue currents | Given a submodule $J\subset \mathcal O_0^{\oplus r}$ and a free resolution of
$J$ one can define a certain vector valued residue current whose annihilator is
$J$. We make a decomposition of the current with respect to Ass$(J)$ that
correspond to a primary decomposition of $J$. As a tool we introduce a class of
curren... | math.CV math.AC | given a submodule jsubset mathcal o_0oplus r and a free resolution of j one can define a certain vector valued residue current whose annihilator is j we make a decomposition of the current with respect to assj that correspond to a primary decomposition of j as a tool we introduce a class of currents that includes usual... | [['given', 'a', 'submodule', 'jsubset', 'mathcal', 'o_0oplus', 'r', 'and', 'a', 'free', 'resolution', 'of', 'j', 'one', 'can', 'define', 'a', 'certain', 'vector', 'valued', 'residue', 'current', 'whose', 'annihilator', 'is', 'j', 'we', 'make', 'a', 'decomposition', 'of', 'the', 'current', 'with', 'respect', 'to', 'assj... | [-0.18350372914242546, 0.08762834614873687, -0.06983812961468025, 0.029283037675910076, -0.1215943538265515, -0.14939410580157103, -0.007681969077255624, 0.3221673760798913, -0.30932438939432555, -0.18382595209891117, 0.08515791066987086, -0.21455200061885804, -0.1041702559288544, 0.1739673103807093, -0.098361955672691... |
710.2017 | Discovery of very high energy gamma-ray emission in the W 28 (G6.4-0.1)
region, and multiwavelength comparisons | H.E.S.S. observations of the old-age (>10^4yr; ~0.5deg diameter) composite
supernova remnant (SNR) W 28 reveal very high energy (VHE) gamma-ray emission
situated at its northeastern and southern boundaries. The northeastern VHE
source (HESS J1801-233) is in an area where W 28 is interacting with a dense
molecular clo... | astro-ph | hess observations of the oldage 104yr 05deg diameter composite supernova remnant snr w 28 reveal very high energy vhe gammaray emission situated at its northeastern and southern boundaries the northeastern vhe source hess j1801233 is in an area where w 28 is interacting with a dense molecular cloud containing oh masers... | [['hess', 'observations', 'of', 'the', 'oldage', '104yr', '05deg', 'diameter', 'composite', 'supernova', 'remnant', 'snr', 'w', '28', 'reveal', 'very', 'high', 'energy', 'vhe', 'gammaray', 'emission', 'situated', 'at', 'its', 'northeastern', 'and', 'southern', 'boundaries', 'the', 'northeastern', 'vhe', 'source', 'hess... | [-0.0882903513355324, 0.07292027861931119, 0.014883011889954409, 0.058652701832425706, -0.12036702817536764, -0.09298620244058278, 0.07319357024871895, 0.4600095141074087, -0.15096495123818898, -0.32849751320532244, 0.01804806003307239, -0.34587360678129214, 0.05569637189101842, 0.1605385888933053, 0.039597668781534284... |
710.2018 | Cognitive Interference Channels with Confidential Messages | The cognitive interference channel with confidential messages is studied.
Similarly to the classical two-user interference channel, the cognitive
interference channel consists of two transmitters whose signals interfere at
the two receivers. It is assumed that there is a common message source (message
1) known to bot... | cs.IT math.IT | the cognitive interference channel with confidential messages is studied similarly to the classical twouser interference channel the cognitive interference channel consists of two transmitters whose signals interfere at the two receivers it is assumed that there is a common message source message 1 known to both transm... | [['the', 'cognitive', 'interference', 'channel', 'with', 'confidential', 'messages', 'is', 'studied', 'similarly', 'to', 'the', 'classical', 'twouser', 'interference', 'channel', 'the', 'cognitive', 'interference', 'channel', 'consists', 'of', 'two', 'transmitters', 'whose', 'signals', 'interfere', 'at', 'the', 'two', ... | [-0.28304962017856417, 0.015949804481351748, -0.04836050485060113, 0.08322474829214548, -0.10406707189411171, -0.4032011591335398, 0.1469837749481088, 0.3528265195039425, -0.31740620883068493, -0.2283246340538833, 0.10411797003570986, -0.2720426210351494, -0.10174473022748794, 0.07310969211696261, -0.1260113507507302, ... |
710.2019 | MagnetoResistance of graphene-based spin valves | We study the magnetoresistance of spin-valve devices using graphene as a
non-magnetic material to connect ferromagnetic leads. As a preliminary step we
first study the conductivity of a graphene strip connected to metallic contacts
for a variety of lead parameters, and demonstrate that the resulting
conductivity is r... | cond-mat.mes-hall cond-mat.mtrl-sci | we study the magnetoresistance of spinvalve devices using graphene as a nonmagnetic material to connect ferromagnetic leads as a preliminary step we first study the conductivity of a graphene strip connected to metallic contacts for a variety of lead parameters and demonstrate that the resulting conductivity is rather ... | [['we', 'study', 'the', 'magnetoresistance', 'of', 'spinvalve', 'devices', 'using', 'graphene', 'as', 'a', 'nonmagnetic', 'material', 'to', 'connect', 'ferromagnetic', 'leads', 'as', 'a', 'preliminary', 'step', 'we', 'first', 'study', 'the', 'conductivity', 'of', 'a', 'graphene', 'strip', 'connected', 'to', 'metallic',... | [-0.17909445546724848, 0.10511951638530352, -0.05922007664192048, -0.03320002167905405, -0.07967286068834627, -0.1434816862436005, 0.045180596330475296, 0.39147825184947166, -0.25469683169741447, -0.2745625080580128, 0.02736684079790278, -0.28539533552411994, -0.17811738317143697, 0.25766862919685285, -0.01699623255662... |
710.202 | Valiron's construction in higher dimension | We consider holomorphic self-maps $\v$ of the unit ball $\B^N$ in $\C^N$
($N=1,2,3,...$). In the one-dimensional case, when $\v$ has no fixed points in
$\D\defeq \B^1$ and is of hyperbolic type, there is a classical renormalization
procedure due to Valiron which allows to semi-linearize the map $\phi$, and
therefore,... | math.CV math.DS | we consider holomorphic selfmaps v of the unit ball bn in cn n123 in the onedimensional case when v has no fixed points in ddefeq b1 and is of hyperbolic type there is a classical renormalization procedure due to valiron which allows to semilinearize the map phi and therefore in this case the dynamical properties of ph... | [['we', 'consider', 'holomorphic', 'selfmaps', 'v', 'of', 'the', 'unit', 'ball', 'bn', 'in', 'cn', 'n123', 'in', 'the', 'onedimensional', 'case', 'when', 'v', 'has', 'no', 'fixed', 'points', 'in', 'ddefeq', 'b1', 'and', 'is', 'of', 'hyperbolic', 'type', 'there', 'is', 'a', 'classical', 'renormalization', 'procedure', '... | [-0.1390464982487322, 0.06681748583337398, -0.052778988357300195, 0.038005290948596546, -0.04596208663452871, -0.15507172274959796, 0.04351470133335125, 0.3435291904441225, -0.31140592168426007, -0.1610335495201795, 0.09665405590037959, -0.31028269034655614, -0.13600168534652973, 0.1578129754904317, -0.0663956890821578... |
710.2021 | Non-linear QCD | In this talk I give the mini-review on recent development in the non-linear
QCD (at low $x$).
| hep-ph | in this talk i give the minireview on recent development in the nonlinear qcd at low x | [['in', 'this', 'talk', 'i', 'give', 'the', 'minireview', 'on', 'recent', 'development', 'in', 'the', 'nonlinear', 'qcd', 'at', 'low', 'x']] | [-0.09688161505276666, 0.14055330634993665, -0.07089562694925595, -0.03749625523821177, -0.048078824889243525, -0.07796941456549308, -0.0032004979165161356, 0.33243026803521547, -0.17364755070165677, -0.18993760618340114, 0.10413394861525911, -0.28684533891432423, -0.11990941222757101, 0.10131751411758802, -0.089160872... |
710.2022 | Short distance modifications to Newton's law in SUSY braneworld
scenarios | In braneworld models coming from string theory one generally encounters
massless scalar degrees of freedom -moduli- parameterizing the volume of small
compact extra-dimensions. Here we discuss the effects of such moduli on
Newton's law for a fairly general 5-D supersymmetric braneworld scenario with a
bulk scalar fie... | hep-ph gr-qc hep-th | in braneworld models coming from string theory one generally encounters massless scalar degrees of freedom moduli parameterizing the volume of small compact extradimensions here we discuss the effects of such moduli on newtons law for a fairly general 5d supersymmetric braneworld scenario with a bulk scalar field phi w... | [['in', 'braneworld', 'models', 'coming', 'from', 'string', 'theory', 'one', 'generally', 'encounters', 'massless', 'scalar', 'degrees', 'of', 'freedom', 'moduli', 'parameterizing', 'the', 'volume', 'of', 'small', 'compact', 'extradimensions', 'here', 'we', 'discuss', 'the', 'effects', 'of', 'such', 'moduli', 'on', 'ne... | [-0.1941780532520693, 0.18320283095096856, -0.060387650203882856, 0.12724440028083273, -0.10280756730935536, -0.16803912895080525, -0.03010265837656334, 0.2574880996191528, -0.20792023085090702, -0.24124258387405262, -0.0063741679614475735, -0.28533176391228904, -0.159860152069199, 0.1371226441197559, -0.05000549380923... |
710.2023 | Model of World; her cities, languages and countries | The time evolution of Earth with her cities, languages and countries is
considered in terms of the multiplicative noise and the fragmentation-
processes, where the related families, size distributions, lifetimes,
bilinguals, etc. are studied. Earlier we treated the cities and the languages
differently (and as connect... | physics.soc-ph | the time evolution of earth with her cities languages and countries is considered in terms of the multiplicative noise and the fragmentation processes where the related families size distributions lifetimes bilinguals etc are studied earlier we treated the cities and the languages differently and as connected languages... | [['the', 'time', 'evolution', 'of', 'earth', 'with', 'her', 'cities', 'languages', 'and', 'countries', 'is', 'considered', 'in', 'terms', 'of', 'the', 'multiplicative', 'noise', 'and', 'the', 'fragmentation', 'processes', 'where', 'the', 'related', 'families', 'size', 'distributions', 'lifetimes', 'bilinguals', 'etc', ... | [-0.0816497930664156, 0.1118878657195035, -0.054309628507069926, 0.11465127373353617, 0.0018298294752652586, -0.06924416925626951, 0.06254703372972689, 0.3725676853209734, -0.26052646039867067, -0.31634225216235073, 0.08591950507129503, -0.29471460422894485, -0.07240478761336754, 0.21041131333749688, -0.065429523639490... |
710.2024 | Ratios: A short guide to confidence limits and proper use | Researchers often calculate ratios of measured quantities. Specifying
confidence limits for ratios is difficult and the appropriate methods are often
unknown. Appropriate methods are described (Fieller, Taylor, special bootstrap
methods). For the Fieller method a simple geometrical interpretation is given.
Monte Carl... | stat.AP stat.ME | researchers often calculate ratios of measured quantities specifying confidence limits for ratios is difficult and the appropriate methods are often unknown appropriate methods are described fieller taylor special bootstrap methods for the fieller method a simple geometrical interpretation is given monte carlo simulati... | [['researchers', 'often', 'calculate', 'ratios', 'of', 'measured', 'quantities', 'specifying', 'confidence', 'limits', 'for', 'ratios', 'is', 'difficult', 'and', 'the', 'appropriate', 'methods', 'are', 'often', 'unknown', 'appropriate', 'methods', 'are', 'described', 'fieller', 'taylor', 'special', 'bootstrap', 'method... | [-0.02214296758017045, 0.06302247642871422, -0.10235287399836264, 0.1951297744122034, -0.08751106751546012, -0.18600128050025364, 0.0475522055551094, 0.44120218472208006, -0.2387545191163939, -0.3291950613512831, 0.14593290004847667, -0.2576273508809933, -0.13241527856611726, 0.2339597507912697, -0.1060418708395939, 0.... |
710.2025 | Mechanisms of exchange bias with multiferroic BiFeO3 epitaxial thin
films | We have combined neutron scattering and piezoresponse force microscopy to
study the relation between the exchange bias observed in CoFeB/BiFeO3
heterostructures and the multiferroic domain structure of the BiFeO3 films. We
show that the exchange field scales with the inverse of the ferroelectric and
antiferromagnetic... | cond-mat.mtrl-sci cond-mat.str-el | we have combined neutron scattering and piezoresponse force microscopy to study the relation between the exchange bias observed in cofebbifeo3 heterostructures and the multiferroic domain structure of the bifeo3 films we show that the exchange field scales with the inverse of the ferroelectric and antiferromagnetic dom... | [['we', 'have', 'combined', 'neutron', 'scattering', 'and', 'piezoresponse', 'force', 'microscopy', 'to', 'study', 'the', 'relation', 'between', 'the', 'exchange', 'bias', 'observed', 'in', 'cofebbifeo3', 'heterostructures', 'and', 'the', 'multiferroic', 'domain', 'structure', 'of', 'the', 'bifeo3', 'films', 'we', 'sho... | [-0.17418544770845648, 0.15377097249126695, -0.05016645495019549, 0.008720263306583678, -0.09643682816579026, -0.07377719927617178, 0.09656119247725024, 0.4752822450685258, -0.3241601589763043, -0.3025760466460975, 0.013204842046787011, -0.3125859277265869, -0.10062820880616806, 0.20535087616572498, 0.08598736062531873... |
710.2026 | Concerning the Strauss conjecture and almost global existence for
nonlinear Dirichlet-wave equations in 4-dimensions | We show the obstacle version of the Strauss conjecture holds when the spatial
dimension is equal to 4. We also show that an almost global existence theorem
of H\"ormander for (4+1)-dimensional Minkowski space holds in the obstacle
setting. We use weighed space-time variants of the energy inequality and a
variant of t... | math.AP | we show the obstacle version of the strauss conjecture holds when the spatial dimension is equal to 4 we also show that an almost global existence theorem of hormander for 41dimensional minkowski space holds in the obstacle setting we use weighed spacetime variants of the energy inequality and a variant of the classica... | [['we', 'show', 'the', 'obstacle', 'version', 'of', 'the', 'strauss', 'conjecture', 'holds', 'when', 'the', 'spatial', 'dimension', 'is', 'equal', 'to', '4', 'we', 'also', 'show', 'that', 'an', 'almost', 'global', 'existence', 'theorem', 'of', 'hormander', 'for', '41dimensional', 'minkowski', 'space', 'holds', 'in', 't... | [-0.1467321775853634, 0.05831295443428892, -0.09523739901117304, 0.14282307862939145, -0.03948556166988882, -0.13037514208223333, -0.018953847495669668, 0.2847018803046508, -0.2715608357197859, -0.21885317245667632, 0.12260157806290821, -0.25493550471199505, -0.13138716424053365, 0.1952469484245574, -0.1343417956747792... |
710.2027 | TenTen: A New Array of Multi-TeV Imaging Cherenkov Telescopes | The exciting results from H.E.S.S. point to a new population of gamma-ray
sources at energies E > 10 TeV, paving the way for future studies and new
discoveries in the multi-TeV energy range. Connected with these energies is the
search for sources of PeV cosmic-rays (CRs) and the study of multi-TeV
gamma-ray productio... | astro-ph | the exciting results from hess point to a new population of gammaray sources at energies e 10 tev paving the way for future studies and new discoveries in the multitev energy range connected with these energies is the search for sources of pev cosmicrays crs and the study of multitev gammaray production in a growing nu... | [['the', 'exciting', 'results', 'from', 'hess', 'point', 'to', 'a', 'new', 'population', 'of', 'gammaray', 'sources', 'at', 'energies', 'e', '10', 'tev', 'paving', 'the', 'way', 'for', 'future', 'studies', 'and', 'new', 'discoveries', 'in', 'the', 'multitev', 'energy', 'range', 'connected', 'with', 'these', 'energies',... | [-0.07836229816178379, 0.20598121803956676, 0.023575581247597687, 0.11342283985081328, -0.0759935346584706, -0.07508403756350401, 0.0059246671019641105, 0.4014000278211974, -0.20149196782454726, -0.44483266329988225, 0.05149771990617127, -0.32218843729036756, 0.01744865575713701, 0.2848774211034637, 0.02483033179734894... |
710.2028 | Higher string functions, higher-level Appell functions, and the
logarithmic ^sl(2)_k/u(1) CFT model | We generalize the string functions C_{n,r}(tau) associated with the coset
^sl(2)_k/u(1) to higher string functions A_{n,r}(tau) and B_{n,r}(tau)
associated with the coset W(k)/u(1) of the W-algebra of the logarithmically
extended ^sl(2)_k conformal field model with positive integer k. The higher
string functions occu... | math.QA hep-th math-ph math.CO math.MP | we generalize the string functions c_nrtau associated with the coset sl2_ku1 to higher string functions a_nrtau and b_nrtau associated with the coset wku1 of the walgebra of the logarithmically extended sl2_k conformal field model with positive integer k the higher string functions occur in decomposing wk characters wi... | [['we', 'generalize', 'the', 'string', 'functions', 'c_nrtau', 'associated', 'with', 'the', 'coset', 'sl2_ku1', 'to', 'higher', 'string', 'functions', 'a_nrtau', 'and', 'b_nrtau', 'associated', 'with', 'the', 'coset', 'wku1', 'of', 'the', 'walgebra', 'of', 'the', 'logarithmically', 'extended', 'sl2_k', 'conformal', 'fi... | [-0.14063310590803835, 0.11759480040195128, -0.07496560218327857, 0.08291314916143604, -0.1261504484036713, -0.1403521281099013, -0.020298409993605066, 0.33114003189277985, -0.314344428347569, -0.2102421482220781, 0.08462423588733803, -0.2751782579704168, -0.18276025972276239, 0.15310422659699693, -0.0348899466107791, ... |
710.2029 | Volume Weighting in the No Boundary Proposal | It has been suggested that the no boundary proposal would predict little or
no slow roll inflation leading to an empty deSitter universe. However it is
argued that the probability for the whole universe should be multiplied by a
zero mode factor $e^{3N}$ which counts the number of Hubble volumes in the
universe. This... | hep-th | it has been suggested that the no boundary proposal would predict little or no slow roll inflation leading to an empty desitter universe however it is argued that the probability for the whole universe should be multiplied by a zero mode factor e3n which counts the number of hubble volumes in the universe this volume w... | [['it', 'has', 'been', 'suggested', 'that', 'the', 'no', 'boundary', 'proposal', 'would', 'predict', 'little', 'or', 'no', 'slow', 'roll', 'inflation', 'leading', 'to', 'an', 'empty', 'desitter', 'universe', 'however', 'it', 'is', 'argued', 'that', 'the', 'probability', 'for', 'the', 'whole', 'universe', 'should', 'be'... | [-0.12374293158895203, 0.1835695848722525, -0.1754430980590469, 0.13489026621439504, -0.07122990206538976, -0.13185103638814047, 0.015808704616194897, 0.3252412408365162, -0.18975515397531645, -0.25423592477422824, 0.09831442010133518, -0.2248284623518095, -0.12960737475173567, 0.13910319576050145, -0.08262320982476512... |
710.203 | FSR0190 - Another old distant galactic cluster | We are conducting a large program to classify newly discovered Milky Way star
cluster candidates from Froebrich et al. (2007). Here we present NIR follow-up
observations of FSR0190 (RA=20h05m31.3s, DEC=33deg34'09" J2000). The cluster is
situated close to the Galactic Plane (l=70.7302deg, b=+0.9498deg). It shows a
cir... | astro-ph | we are conducting a large program to classify newly discovered milky way star cluster candidates from froebrich et al 2007 here we present nir followup observations of fsr0190 ra20h05m313s dec33deg3409 j2000 the cluster is situated close to the galactic plane l707302deg b09498deg it shows a circular shape a relatively ... | [['we', 'are', 'conducting', 'a', 'large', 'program', 'to', 'classify', 'newly', 'discovered', 'milky', 'way', 'star', 'cluster', 'candidates', 'from', 'froebrich', 'et', 'al', '2007', 'here', 'we', 'present', 'nir', 'followup', 'observations', 'of', 'fsr0190', 'ra20h05m313s', 'dec33deg3409', 'j2000', 'the', 'cluster',... | [-0.0721886756312745, 0.10011388166561368, -0.12054345114282806, 0.06703994467553674, -0.11040420928121075, -0.03559513881803074, 0.06614866381947908, 0.4122138323171674, -0.19515022040196423, -0.3739276784183705, 0.04857060551824691, -0.31473346823513243, -0.03599490096743128, 0.19170927586223502, -0.06534230429679155... |
710.2031 | Modeling a Schottky-barrier carbon nanotube field-effect transistor with
ferromagnetic contacts | In this study, a model of a Schottky-barrier carbon nanotube field- effect
transistor (CNT-FET), with ferromagnetic contacts, has been developed. The
emphasis is put on analysis of current-voltage characteristics as well as shot
(and thermal) noise. The method is based on the tight-binding model and the
non- equilibr... | cond-mat.mes-hall cond-mat.mtrl-sci | in this study a model of a schottkybarrier carbon nanotube field effect transistor cntfet with ferromagnetic contacts has been developed the emphasis is put on analysis of currentvoltage characteristics as well as shot and thermal noise the method is based on the tightbinding model and the non equilibrium greens functi... | [['in', 'this', 'study', 'a', 'model', 'of', 'a', 'schottkybarrier', 'carbon', 'nanotube', 'field', 'effect', 'transistor', 'cntfet', 'with', 'ferromagnetic', 'contacts', 'has', 'been', 'developed', 'the', 'emphasis', 'is', 'put', 'on', 'analysis', 'of', 'currentvoltage', 'characteristics', 'as', 'well', 'as', 'shot', ... | [-0.14922557705203476, 0.10750066240965996, -0.06864561027563784, -0.01041758122610981, 0.008208817421742107, -0.22745068990018058, 0.08678562168295131, 0.4083481670073841, -0.21062102615833284, -0.3117431446585966, 0.02049142927154089, -0.3072576793609187, -0.13237344307177093, 0.24607118148883075, -0.0300779077206718... |
710.2032 | Construction of a Penrose Diagram for a Spatially Coherent Evaporating
Black Hole | A Penrose diagram is constructed for an example black hole that evaporates at
a steady rate as measured by a distant observer, until the mass vanishes,
yielding a final state Minkowski space-time. Coordinate dependencies of
significant features, such as the horizon and coordinate anomalies, are clearly
demonstrated o... | gr-qc | a penrose diagram is constructed for an example black hole that evaporates at a steady rate as measured by a distant observer until the mass vanishes yielding a final state minkowski spacetime coordinate dependencies of significant features such as the horizon and coordinate anomalies are clearly demonstrated on the di... | [['a', 'penrose', 'diagram', 'is', 'constructed', 'for', 'an', 'example', 'black', 'hole', 'that', 'evaporates', 'at', 'a', 'steady', 'rate', 'as', 'measured', 'by', 'a', 'distant', 'observer', 'until', 'the', 'mass', 'vanishes', 'yielding', 'a', 'final', 'state', 'minkowski', 'spacetime', 'coordinate', 'dependencies',... | [-0.17439300281306108, 0.13225537594238024, -0.09545655825641006, 0.11871921650987739, -0.05896402283882101, -0.12176097240298986, 0.01716537803489094, 0.31728053002928697, -0.22394445165991783, -0.24945659121343244, 0.13735879729501904, -0.3013166846736567, -0.10655372817224512, 0.17440056985554594, -0.017190004815347... |
710.2033 | Ricci curvature and conformality of Riemannian manifolds to spheres | In this paper we give bounds for the first eigenvalue of the conformal
Laplacian and the Yamabe invariant of a compact Riemannian manifold, by using
conditions on the Ricci curvature and the diameter and deduce certain
conditions on the manifold to be conformal to a sphere.
| math.DG | in this paper we give bounds for the first eigenvalue of the conformal laplacian and the yamabe invariant of a compact riemannian manifold by using conditions on the ricci curvature and the diameter and deduce certain conditions on the manifold to be conformal to a sphere | [['in', 'this', 'paper', 'we', 'give', 'bounds', 'for', 'the', 'first', 'eigenvalue', 'of', 'the', 'conformal', 'laplacian', 'and', 'the', 'yamabe', 'invariant', 'of', 'a', 'compact', 'riemannian', 'manifold', 'by', 'using', 'conditions', 'on', 'the', 'ricci', 'curvature', 'and', 'the', 'diameter', 'and', 'deduce', 'ce... | [-0.15780998677339242, 0.06616483181310089, -0.11896250012290219, 0.045794175763148814, -0.15261232540132882, -0.11924716293730814, -0.09294671417244346, 0.3314162643383379, -0.2171124242570089, -0.24635872236736442, 0.20978262548527235, -0.24662726194314336, -0.16598609021014493, 0.14539664596035753, -0.10736181412863... |
710.2034 | R-Parity violating minimal supergravity at the LHC | We consider the case where supersymmetry with broken R-parity is embedded in
the minimal supergravity model (mSUGRA). This alters the standard mSUGRA
spectrum and opens a wide range in parameter space, where the scalar tau is the
lightest supersymmetric particle, instead of the lightest neutralino. We study
the resul... | hep-ph | we consider the case where supersymmetry with broken rparity is embedded in the minimal supergravity model msugra this alters the standard msugra spectrum and opens a wide range in parameter space where the scalar tau is the lightest supersymmetric particle instead of the lightest neutralino we study the resulting lhc ... | [['we', 'consider', 'the', 'case', 'where', 'supersymmetry', 'with', 'broken', 'rparity', 'is', 'embedded', 'in', 'the', 'minimal', 'supergravity', 'model', 'msugra', 'this', 'alters', 'the', 'standard', 'msugra', 'spectrum', 'and', 'opens', 'a', 'wide', 'range', 'in', 'parameter', 'space', 'where', 'the', 'scalar', 't... | [-0.09537362388380051, 0.2676311737215371, 0.009008660578696304, 0.1955746752357234, -0.06143931559208466, -0.1973715619722673, -0.009130767448324884, 0.28445213048505674, -0.21200050934251533, -0.29135086369442653, 0.012440174756324794, -0.28126735502786665, -0.02324112118305975, 0.09901861890768969, 0.005680133790585... |
710.2035 | Electroweak Contributions to Squark Pair Production | We compute electroweak contributions to the production of squark pairs at
hadron colliders. These include the exchange of electroweak gauge bosons in the
$s-$channel as well as electroweak gaugino exchange in the $t-$ and/or
$u-$channel. In many cases these can interfere with the dominant QCD
contributions. As a resu... | hep-ph | we compute electroweak contributions to the production of squark pairs at hadron colliders these include the exchange of electroweak gauge bosons in the schannel as well as electroweak gaugino exchange in the t andor uchannel in many cases these can interfere with the dominant qcd contributions as a result we find siza... | [['we', 'compute', 'electroweak', 'contributions', 'to', 'the', 'production', 'of', 'squark', 'pairs', 'at', 'hadron', 'colliders', 'these', 'include', 'the', 'exchange', 'of', 'electroweak', 'gauge', 'bosons', 'in', 'the', 'schannel', 'as', 'well', 'as', 'electroweak', 'gaugino', 'exchange', 'in', 'the', 't', 'andor',... | [-0.10130507721874767, 0.31165322669428486, 0.011368979824353653, 0.20293817568494105, -0.06623358314993374, -0.1431974029050064, 0.044526839147097076, 0.3318579544570169, -0.2092298080799459, -0.3300576199263591, 0.011585134005270385, -0.3378120399369248, 0.05359114531291135, 0.12137389780977613, 0.07181464552734818, ... |
710.2036 | Cutoff effects for Wilson twisted mass fermions at tree-level of
perturbation theory | We study cutoff effects at tree-level of perturbation theory for standard
Wilson and Wilson twisted mass fermionic lattice actions with Nf=2 flavour
degenerate quarks. The discretization effects are investigated by computing the
mass spectrum and decay amplitudes for different hadron interpolating fields
and the scal... | hep-lat | we study cutoff effects at treelevel of perturbation theory for standard wilson and wilson twisted mass fermionic lattice actions with nf2 flavour degenerate quarks the discretization effects are investigated by computing the mass spectrum and decay amplitudes for different hadron interpolating fields and the scaling b... | [['we', 'study', 'cutoff', 'effects', 'at', 'treelevel', 'of', 'perturbation', 'theory', 'for', 'standard', 'wilson', 'and', 'wilson', 'twisted', 'mass', 'fermionic', 'lattice', 'actions', 'with', 'nf2', 'flavour', 'degenerate', 'quarks', 'the', 'discretization', 'effects', 'are', 'investigated', 'by', 'computing', 'th... | [-0.14158511148629052, 0.24123751777252125, -0.059017716801005926, 0.09539007777236626, -0.009890774475455194, -0.1371956810544797, 0.057183859998800844, 0.4277961558500628, -0.14529789591063105, -0.2515559388787491, 0.10144633362432216, -0.2731188960752623, -0.06484398441277668, 0.1494387396915208, -0.0207083092858858... |
710.2037 | An Affinity Propagation Based method for Vector Quantization Codebook
Design | In this paper, we firstly modify a parameter in affinity propagation (AP) to
improve its convergence ability, and then, we apply it to vector quantization
(VQ) codebook design problem. In order to improve the quality of the resulted
codebook, we combine the improved AP (IAP) with the conventional LBG algorithm
to gen... | cs.CV | in this paper we firstly modify a parameter in affinity propagation ap to improve its convergence ability and then we apply it to vector quantization vq codebook design problem in order to improve the quality of the resulted codebook we combine the improved ap iap with the conventional lbg algorithm to generate an effe... | [['in', 'this', 'paper', 'we', 'firstly', 'modify', 'a', 'parameter', 'in', 'affinity', 'propagation', 'ap', 'to', 'improve', 'its', 'convergence', 'ability', 'and', 'then', 'we', 'apply', 'it', 'to', 'vector', 'quantization', 'vq', 'codebook', 'design', 'problem', 'in', 'order', 'to', 'improve', 'the', 'quality', 'of'... | [-0.022267193286452533, 0.005833775976498146, -0.10667601139171094, 0.05754960527098397, -0.15498589033760676, -0.17396994120236942, 0.11476629314427378, 0.4565693040537398, -0.2519472227204682, -0.29814093809279546, 0.02362172894049209, -0.20959010045612003, -0.1961369842387418, 0.15507354391965925, -0.131744010762947... |
710.2038 | The Minimal Flavor Violating MSSM: application to meson mixings | We provide a short account of the effects one expects on meson-antimeson
oscillations in the context of the Minimal Supersymmetric Standard Model
(MSSM). This issue is largely dependent on the assumptions made on the MSSM
parameter space. In this respect, we consider in closer detail the cases of the
general MSSM, wi... | hep-ph | we provide a short account of the effects one expects on mesonantimeson oscillations in the context of the minimal supersymmetric standard model mssm this issue is largely dependent on the assumptions made on the mssm parameter space in this respect we consider in closer detail the cases of the general mssm with comple... | [['we', 'provide', 'a', 'short', 'account', 'of', 'the', 'effects', 'one', 'expects', 'on', 'mesonantimeson', 'oscillations', 'in', 'the', 'context', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'this', 'issue', 'is', 'largely', 'dependent', 'on', 'the', 'assumptions', 'made', 'on', 'the', 'ms... | [-0.10334558056513216, 0.18972917507147893, -0.00715530518691536, 0.14991193305579412, -0.05982040569696362, -0.1527984972693216, 0.0686539515925595, 0.292460417369778, -0.23104594160571315, -0.25412500740932065, 0.06326764558774128, -0.25990122101999297, -0.11504298067135606, 0.1371192702353238, -0.07574350283344745, ... |
710.2039 | A method of moments estimator of tail dependence | In the world of multivariate extremes, estimation of the dependence structure
still presents a challenge and an interesting problem. A procedure for the
bivariate case is presented that opens the road to a similar way of handling
the problem in a truly multivariate setting. We consider a semi-parametric
model in whic... | math.ST stat.TH | in the world of multivariate extremes estimation of the dependence structure still presents a challenge and an interesting problem a procedure for the bivariate case is presented that opens the road to a similar way of handling the problem in a truly multivariate setting we consider a semiparametric model in which the ... | [['in', 'the', 'world', 'of', 'multivariate', 'extremes', 'estimation', 'of', 'the', 'dependence', 'structure', 'still', 'presents', 'a', 'challenge', 'and', 'an', 'interesting', 'problem', 'a', 'procedure', 'for', 'the', 'bivariate', 'case', 'is', 'presented', 'that', 'opens', 'the', 'road', 'to', 'a', 'similar', 'way... | [-0.06603558357781336, 0.023440806621420566, -0.17525995197826943, 0.1321785356658695, -0.06768665418402413, -0.14958054590332295, 0.0482409725256401, 0.3694045196976618, -0.25424759030535676, -0.2686023865116097, 0.11039722676252114, -0.23226401660233567, -0.14557647038649735, 0.20451520591590153, -0.08638467403433922... |
710.204 | $B \to K^* \ell^+ \ell^-$ as a probe of Universal Extra Dimensions | We study some rare B decays induced by $b \to s$ transition within the
Standard Model and in the Appelquist-Cheng-Dobrescu model, which is a New
Physics scenario with a single universal extra dimension. In particular, we
discuss the dependence on the radius $R$ of the compactified extra-dimension of
the branching rat... | hep-ph | we study some rare b decays induced by b to s transition within the standard model and in the appelquistchengdobrescu model which is a new physics scenario with a single universal extra dimension in particular we discuss the dependence on the radius r of the compactified extradimension of the branching ratio the forwar... | [['we', 'study', 'some', 'rare', 'b', 'decays', 'induced', 'by', 'b', 'to', 's', 'transition', 'within', 'the', 'standard', 'model', 'and', 'in', 'the', 'appelquistchengdobrescu', 'model', 'which', 'is', 'a', 'new', 'physics', 'scenario', 'with', 'a', 'single', 'universal', 'extra', 'dimension', 'in', 'particular', 'we... | [-0.15640616971026006, 0.21752076346920915, -0.04205038312104452, 0.05119376383435699, -0.03560664747695787, -0.20184104637164307, 0.0816640664938366, 0.2807852496555726, -0.29076543962021906, -0.2482417166367712, -0.0011226121919700898, -0.2812674284901425, -0.004749005890440151, 0.09945319967725909, 0.085830995709220... |
710.2041 | Thin-shell wormholes supported by ordinary matter in
Einstein--Gauss--Bonnet gravity | The generalized Darmois--Israel formalism for Einstein--Gauss--Bonnet theory
is applied to construct thin-shell Lorentzian wormholes with spherical
symmetry. We calculate the energy localized on the shell, and we find that for
certain values of the parameters wormholes could be supported by matter not
violating the e... | gr-qc astro-ph hep-th | the generalized darmoisisrael formalism for einsteingaussbonnet theory is applied to construct thinshell lorentzian wormholes with spherical symmetry we calculate the energy localized on the shell and we find that for certain values of the parameters wormholes could be supported by matter not violating the energy condi... | [['the', 'generalized', 'darmoisisrael', 'formalism', 'for', 'einsteingaussbonnet', 'theory', 'is', 'applied', 'to', 'construct', 'thinshell', 'lorentzian', 'wormholes', 'with', 'spherical', 'symmetry', 'we', 'calculate', 'the', 'energy', 'localized', 'on', 'the', 'shell', 'and', 'we', 'find', 'that', 'for', 'certain',... | [-0.1428089585944848, 0.1448278250577657, -0.11106380020551708, 0.17205989030037966, -0.0921658871077892, -0.14152275667647304, -0.04323662820768178, 0.31811024301239976, -0.12799934255283163, -0.28978421865031123, 0.049716334506545376, -0.20190124231917056, -0.10338763190109444, 0.13159186992308367, -0.036375427994441... |
710.2042 | Gravitomagnetism in superconductors and compact stars | There are three experimentally observed effects in rotating superconductors
that are so far unexplained. Some authors have tried to interpret such a
phenomena as possible new gravitational properties of coherent quantum systems:
in particular, they suggest that the gravitomagnetic field of that kind of
matter may be ... | gr-qc | there are three experimentally observed effects in rotating superconductors that are so far unexplained some authors have tried to interpret such a phenomena as possible new gravitational properties of coherent quantum systems in particular they suggest that the gravitomagnetic field of that kind of matter may be many ... | [['there', 'are', 'three', 'experimentally', 'observed', 'effects', 'in', 'rotating', 'superconductors', 'that', 'are', 'so', 'far', 'unexplained', 'some', 'authors', 'have', 'tried', 'to', 'interpret', 'such', 'a', 'phenomena', 'as', 'possible', 'new', 'gravitational', 'properties', 'of', 'coherent', 'quantum', 'syste... | [-0.11248455803049193, 0.23551624356073209, -0.1025428345062952, 0.1412252556230209, -0.0913205949225645, -0.09849917802467258, 0.011981939245283004, 0.3719179428600032, -0.23450935720305505, -0.29698944807684197, 0.017951970574735052, -0.30515129711671635, -0.14238497967585578, 0.2206377794259581, -0.0423480953603726,... |
710.2043 | Roots, symmetries and conjugacy of pseudo-Anosov mapping classes | An algorithm is proposed that solves two decision problems for pseudo-Anosov
elements in the mapping class group of a surface with at least one marked fixed
point. The first problem is the root problem: decide if the element is a power
and in this case compute the roots. The second problem is the symmetry problem:
de... | math.DS math.GT | an algorithm is proposed that solves two decision problems for pseudoanosov elements in the mapping class group of a surface with at least one marked fixed point the first problem is the root problem decide if the element is a power and in this case compute the roots the second problem is the symmetry problem decide if... | [['an', 'algorithm', 'is', 'proposed', 'that', 'solves', 'two', 'decision', 'problems', 'for', 'pseudoanosov', 'elements', 'in', 'the', 'mapping', 'class', 'group', 'of', 'a', 'surface', 'with', 'at', 'least', 'one', 'marked', 'fixed', 'point', 'the', 'first', 'problem', 'is', 'the', 'root', 'problem', 'decide', 'if', ... | [-0.12241808849179911, 0.04473073709798175, -0.0992453304067668, 0.012826120797803419, -0.10493689484428614, -0.13189240613331396, 0.03467070394092136, 0.3318032642515997, -0.3683425735268328, -0.23260945540128483, 0.1445680276167372, -0.30581239950325756, -0.1514072990251912, 0.16819474414094454, -0.07896321264819967,... |
710.2044 | Estimation of Gaussian graphs by model selection | We investigate in this paper the estimation of Gaussian graphs by model
selection from a non-asymptotic point of view. We start from a n-sample of a
Gaussian law P_C in R^p and focus on the disadvantageous case where n is
smaller than p. To estimate the graph of conditional dependences of P_C, we
introduce a collecti... | math.ST stat.TH | we investigate in this paper the estimation of gaussian graphs by model selection from a nonasymptotic point of view we start from a nsample of a gaussian law p_c in rp and focus on the disadvantageous case where n is smaller than p to estimate the graph of conditional dependences of p_c we introduce a collection of ca... | [['we', 'investigate', 'in', 'this', 'paper', 'the', 'estimation', 'of', 'gaussian', 'graphs', 'by', 'model', 'selection', 'from', 'a', 'nonasymptotic', 'point', 'of', 'view', 'we', 'start', 'from', 'a', 'nsample', 'of', 'a', 'gaussian', 'law', 'p_c', 'in', 'rp', 'and', 'focus', 'on', 'the', 'disadvantageous', 'case', ... | [-0.07821163024172323, 0.06106394077352154, -0.10409258192815228, 0.07540968388058417, -0.05465176305947227, -0.1587945879949684, 0.13063841585791883, 0.35273601162597673, -0.2343032245156825, -0.2768528410361721, 0.0902865559873043, -0.28829804855962754, -0.15814450419125567, 0.1486667782674894, -0.1265545190192349, 0... |
710.2045 | Purity distribution for bipartite random pure states | Analytic expressions for the probability density distribution of the linear
entropy and the purity are derived for bipartite pure random quantum states.
The explicit distributions for a state belonging to a product of Hilbert spaces
of dimensions p and q are given for p=3 and any q>=3, as well as for p=q=4.
| quant-ph | analytic expressions for the probability density distribution of the linear entropy and the purity are derived for bipartite pure random quantum states the explicit distributions for a state belonging to a product of hilbert spaces of dimensions p and q are given for p3 and any q3 as well as for pq4 | [['analytic', 'expressions', 'for', 'the', 'probability', 'density', 'distribution', 'of', 'the', 'linear', 'entropy', 'and', 'the', 'purity', 'are', 'derived', 'for', 'bipartite', 'pure', 'random', 'quantum', 'states', 'the', 'explicit', 'distributions', 'for', 'a', 'state', 'belonging', 'to', 'a', 'product', 'of', 'h... | [-0.09180361505311269, 0.16385383492049116, -0.0712725494388276, 0.10417486879473123, 0.049555851898800865, -0.14184028119780123, 0.028709296741558667, 0.31391631030979067, -0.20014591527601275, -0.2392325283637127, 0.0974017102092218, -0.27016435045068365, -0.057433438809731834, 0.19230916859725347, 0.0039660812427218... |
710.2046 | Quark model: recent issues | In the first part I briefly survey recent issues in constituent quark models
raised by the observation of unusual hadronic states. In particular I discuss
the role of higher Fock components in the wave function of baryons and the
possible interpretation of open charm and of new charmonium-type resonances as
tetraquar... | hep-ph | in the first part i briefly survey recent issues in constituent quark models raised by the observation of unusual hadronic states in particular i discuss the role of higher fock components in the wave function of baryons and the possible interpretation of open charm and of new charmoniumtype resonances as tetraquarks i... | [['in', 'the', 'first', 'part', 'i', 'briefly', 'survey', 'recent', 'issues', 'in', 'constituent', 'quark', 'models', 'raised', 'by', 'the', 'observation', 'of', 'unusual', 'hadronic', 'states', 'in', 'particular', 'i', 'discuss', 'the', 'role', 'of', 'higher', 'fock', 'components', 'in', 'the', 'wave', 'function', 'of... | [-0.07295347760165376, 0.1730448792375336, -0.08899659736614142, 0.07868505464977629, -0.04757765687203833, -0.05712640361439082, 0.06532512754867119, 0.2911462087649852, -0.21790058156918912, -0.2405706013641542, 0.025434202660107985, -0.26874232002800064, -0.10381109212037354, 0.09526267443184874, 0.02616642846814578... |
710.2047 | Theory of cooling neutron stars versus observations | We review current state of neutron star cooling theory and discuss the
prospects to constrain the equation of state, neutrino emission and superfluid
properties of neutron star cores by comparing the cooling theory with
observations of thermal radiation from isolated neutron stars.
| astro-ph | we review current state of neutron star cooling theory and discuss the prospects to constrain the equation of state neutrino emission and superfluid properties of neutron star cores by comparing the cooling theory with observations of thermal radiation from isolated neutron stars | [['we', 'review', 'current', 'state', 'of', 'neutron', 'star', 'cooling', 'theory', 'and', 'discuss', 'the', 'prospects', 'to', 'constrain', 'the', 'equation', 'of', 'state', 'neutrino', 'emission', 'and', 'superfluid', 'properties', 'of', 'neutron', 'star', 'cores', 'by', 'comparing', 'the', 'cooling', 'theory', 'with... | [-0.02454129252804532, 0.25563619004207705, -0.06903198457855199, 0.08295005282741927, -0.1222914308753042, -0.01801329491926091, 0.0978419378599418, 0.31214138572769506, -0.18795179203152657, -0.3274443270195098, 0.03752378191399787, -0.34667708358860444, 0.07441208813162077, 0.2098522441506031, 0.07495199205974738, 0... |
710.2048 | Longitudinal double-spin asymmetry for inclusive jet production in p+p
collisions at sqrt(s)=200 GeV | We report a new STAR measurement of the longitudinal double-spin asymmetry
A_LL for inclusive jet production at mid-rapidity in polarized p+p collisions
at a center-of-mass energy of sqrt(s) = 200 GeV. The data, which cover jet
transverse momenta 5 < p_T < 30 GeV/c, are substantially more precise than
previous measur... | hep-ex | we report a new star measurement of the longitudinal doublespin asymmetry a_ll for inclusive jet production at midrapidity in polarized pp collisions at a centerofmass energy of sqrts 200 gev the data which cover jet transverse momenta 5 p_t 30 gevc are substantially more precise than previous measurements they provide... | [['we', 'report', 'a', 'new', 'star', 'measurement', 'of', 'the', 'longitudinal', 'doublespin', 'asymmetry', 'a_ll', 'for', 'inclusive', 'jet', 'production', 'at', 'midrapidity', 'in', 'polarized', 'pp', 'collisions', 'at', 'a', 'centerofmass', 'energy', 'of', 'sqrts', '200', 'gev', 'the', 'data', 'which', 'cover', 'je... | [-0.052234540670783584, 0.24347100360319018, -0.1588175921374327, 0.1334190196660045, -0.06411728375083343, -0.09271592628694587, -0.03785775940526615, 0.375542666457666, -0.18780993572254848, -0.29430175604081, -0.10400351925674439, -0.38941468318392125, 0.21192308858811082, 0.20211338967858972, 0.1220125619007589, 0.... |
710.2049 | The volume and Chern-Simons invariant of a representation | We give an efficient simplicial formula for the volume and Chern-Simons
invariant of a boundary-parabolic PSL(2,C)-representation of a tame 3-manifold.
If the representation is the geometric representation of a hyperbolic
3-manifold, our formula computes the volume and Chern-Simons invariant directly
from an ideal tr... | math.GT | we give an efficient simplicial formula for the volume and chernsimons invariant of a boundaryparabolic psl2crepresentation of a tame 3manifold if the representation is the geometric representation of a hyperbolic 3manifold our formula computes the volume and chernsimons invariant directly from an ideal triangulation w... | [['we', 'give', 'an', 'efficient', 'simplicial', 'formula', 'for', 'the', 'volume', 'and', 'chernsimons', 'invariant', 'of', 'a', 'boundaryparabolic', 'psl2crepresentation', 'of', 'a', 'tame', '3manifold', 'if', 'the', 'representation', 'is', 'the', 'geometric', 'representation', 'of', 'a', 'hyperbolic', '3manifold', '... | [-0.16751635309663557, 0.10409627736976651, -0.14668825185961193, 0.1027509105088751, -0.1295303629326915, -0.12695605447515845, -0.024199118453358846, 0.279441484146648, -0.2863693498666324, -0.282013841002943, 0.09391226291856063, -0.23316961988097146, -0.22133831599993364, 0.15728797710367612, -0.16414326419019037, ... |
710.205 | The control of iron oxidation state during FeO and olivine crystal
growth | Crystal growth experiments (micro-pulling down or Czochralski methods,
respectively) and DTA/TG measurements with Fe2+ containing olivines
(fayalite--forsterite solid solution) and with FeO (wustite) are performed. For
both substances the oxygen partial pressure p_O2 of the growth atmosphere had
to be adjusted within... | cond-mat.mtrl-sci physics.chem-ph | crystal growth experiments micropulling down or czochralski methods respectively and dtatg measurements with fe2 containing olivines fayaliteforsterite solid solution and with feo wustite are performed for both substances the oxygen partial pressure p_o2 of the growth atmosphere had to be adjusted within the stability ... | [['crystal', 'growth', 'experiments', 'micropulling', 'down', 'or', 'czochralski', 'methods', 'respectively', 'and', 'dtatg', 'measurements', 'with', 'fe2', 'containing', 'olivines', 'fayaliteforsterite', 'solid', 'solution', 'and', 'with', 'feo', 'wustite', 'are', 'performed', 'for', 'both', 'substances', 'the', 'oxyg... | [-0.010280361239685966, 0.20412639409458216, -0.01901371314286672, -0.04997019755798553, 0.04984030910639157, -0.154335049086989, 0.10889104763688198, 0.40686881241894424, -0.22729395670366698, -0.3085269652680365, 0.08820677747676985, -0.32489751876685125, 0.01998235313542958, 0.11050249640508715, 0.01571815993681004,... |
710.2051 | Lecture Notes on Quantum Teichmuller Theory | These notes are based on a lecture course by L. Chekhov held at the
University of Manchester in May 2006 and February-March 2007. They are
divulgative in character, and instead of containing rigorous mathematical
proofs, they illustrate statements giving an intuitive insight. We
intentionally remove most bibliographi... | math.AG math-ph math.MP | these notes are based on a lecture course by l chekhov held at the university of manchester in may 2006 and februarymarch 2007 they are divulgative in character and instead of containing rigorous mathematical proofs they illustrate statements giving an intuitive insight we intentionally remove most bibliographic refere... | [['these', 'notes', 'are', 'based', 'on', 'a', 'lecture', 'course', 'by', 'l', 'chekhov', 'held', 'at', 'the', 'university', 'of', 'manchester', 'in', 'may', '2006', 'and', 'februarymarch', '2007', 'they', 'are', 'divulgative', 'in', 'character', 'and', 'instead', 'of', 'containing', 'rigorous', 'mathematical', 'proofs... | [-0.05262778741289918, 0.06761590347146425, -0.14100414484908635, 0.06322687980718911, -0.13740298634917109, -0.11460940362038938, 0.05604317982568208, 0.31458154982520325, -0.18916049067312005, -0.33699745168401435, 0.12534562878621122, -0.33241528136105364, -0.126732277881467, 0.2083640112365229, -0.16049624440457785... |
710.2052 | Boltzmann, Gibbs and the Concept of Equilibrium | The Boltzmann and Gibbs approaches to statistical mechanics have very
different definitions of equilibrium and entropy. The problems associated with
this are discussed and it is suggested that they can be resolved, to produce a
version of statistical mechanics incorporating both approaches, by redefining
equilibrium ... | cond-mat.stat-mech | the boltzmann and gibbs approaches to statistical mechanics have very different definitions of equilibrium and entropy the problems associated with this are discussed and it is suggested that they can be resolved to produce a version of statistical mechanics incorporating both approaches by redefining equilibrium not a... | [['the', 'boltzmann', 'and', 'gibbs', 'approaches', 'to', 'statistical', 'mechanics', 'have', 'very', 'different', 'definitions', 'of', 'equilibrium', 'and', 'entropy', 'the', 'problems', 'associated', 'with', 'this', 'are', 'discussed', 'and', 'it', 'is', 'suggested', 'that', 'they', 'can', 'be', 'resolved', 'to', 'pr... | [-0.029506749726811443, 0.14040290179120626, -0.18267203747182265, 0.09261241193558857, -0.02453295832274707, -0.18271596329082007, 0.01855582078141007, 0.3273169298011523, -0.32375545075142775, -0.2793962036638142, 0.10520800671176883, -0.27565456600348043, -0.0804178972452224, 0.15369789758863459, -0.0508517246631966... |
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