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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708.1949 | Cold Dark Matter Substructure and Galactic Disks I: Morphological
Signatures of Hierarchical Satellite Accretion | (Abridged) We conduct a series of high-resolution, dissipationless N-body
simulations to investigate the cumulative effect of substructure mergers onto
thin disk galaxies in the context of the LCDM paradigm of structure formation.
Our simulation campaign is based on a hybrid approach. Substructure properties
are cull... | astro-ph | abridged we conduct a series of highresolution dissipationless nbody simulations to investigate the cumulative effect of substructure mergers onto thin disk galaxies in the context of the lcdm paradigm of structure formation our simulation campaign is based on a hybrid approach substructure properties are culled direct... | [['abridged', 'we', 'conduct', 'a', 'series', 'of', 'highresolution', 'dissipationless', 'nbody', 'simulations', 'to', 'investigate', 'the', 'cumulative', 'effect', 'of', 'substructure', 'mergers', 'onto', 'thin', 'disk', 'galaxies', 'in', 'the', 'context', 'of', 'the', 'lcdm', 'paradigm', 'of', 'structure', 'formation... | [-0.08566768411520387, 0.0683330492132114, -0.13693248539341493, 0.1493141187029358, -0.14662259722751753, 0.009417095967876538, -0.03646620342569043, 0.40364228722997036, -0.2131575187473441, -0.35016371270096347, 0.004869201634443957, -0.27689853860260105, -0.06518670242676376, 0.20170107291402303, 0.0001717517152428... |
708.195 | Kondo effect in an Antiferromagnetic metal | We study the fate of a spin-1/2 impurity in the itinerant antiferromagnetic
metallic phase via a renormalization group analysis and a variational
calculation. The local moment - conduction electron interaction hamiltonian in
an antiferromagnetic metal is spin non-conserving. We show that for a general
location of the... | cond-mat.str-el | we study the fate of a spin12 impurity in the itinerant antiferromagnetic metallic phase via a renormalization group analysis and a variational calculation the local moment conduction electron interaction hamiltonian in an antiferromagnetic metal is spin nonconserving we show that for a general location of the impurity... | [['we', 'study', 'the', 'fate', 'of', 'a', 'spin12', 'impurity', 'in', 'the', 'itinerant', 'antiferromagnetic', 'metallic', 'phase', 'via', 'a', 'renormalization', 'group', 'analysis', 'and', 'a', 'variational', 'calculation', 'the', 'local', 'moment', 'conduction', 'electron', 'interaction', 'hamiltonian', 'in', 'an',... | [-0.19739465571060846, 0.22669000538606218, -0.039917860946087076, 0.10133760001849836, -0.0272798775238307, -0.13756111278590338, 0.0919811596705526, 0.34856134810197714, -0.25852738818258186, -0.23303487551154864, 0.017300704209064353, -0.3466774466334381, -0.06751230920482183, 0.07800329193716572, 0.0911606051132222... |
708.1951 | On bilinear biquandles | We define a type of biquandle which is a generalization of symplectic
quandles. We use the extra structure of these bilinear biquandles to define new
knot and link invariants and give some examples.
| math.QA math.GT | we define a type of biquandle which is a generalization of symplectic quandles we use the extra structure of these bilinear biquandles to define new knot and link invariants and give some examples | [['we', 'define', 'a', 'type', 'of', 'biquandle', 'which', 'is', 'a', 'generalization', 'of', 'symplectic', 'quandles', 'we', 'use', 'the', 'extra', 'structure', 'of', 'these', 'bilinear', 'biquandles', 'to', 'define', 'new', 'knot', 'and', 'link', 'invariants', 'and', 'give', 'some', 'examples']] | [-0.2437405287655014, 0.05205171154529759, -0.09651799127459526, 0.14991194779180328, -0.22165975189118675, -0.1854176287059531, 0.06402542117531553, 0.3176960467614911, -0.3596795510613557, -0.2828597408352476, 0.07053748808914062, -0.20114164088260045, -0.27607377364554186, 0.13859138356973277, -0.19308866870899996, ... |
708.1952 | Spontaneous Breaking of Space-Time Symmetries | Kinematical and dynamical mechanisms leading to the spontaneous breaking of
space-time symmetries are described. The symmetries affected are space and time
translations, space rotations, scale and conformal transformations.
Applications are made to solidification, string theory compactifications, the
analysis of stab... | hep-th | kinematical and dynamical mechanisms leading to the spontaneous breaking of spacetime symmetries are described the symmetries affected are space and time translations space rotations scale and conformal transformations applications are made to solidification string theory compactifications the analysis of stable theori... | [['kinematical', 'and', 'dynamical', 'mechanisms', 'leading', 'to', 'the', 'spontaneous', 'breaking', 'of', 'spacetime', 'symmetries', 'are', 'described', 'the', 'symmetries', 'affected', 'are', 'space', 'and', 'time', 'translations', 'space', 'rotations', 'scale', 'and', 'conformal', 'transformations', 'applications',... | [-0.1864696193992961, 0.25768933551418677, -0.0626051697079419, 0.11418600486215662, -0.08664733661632788, -0.0875548456709734, -0.0009257198952693949, 0.3512739143742804, -0.24761069951611653, -0.2984628304185575, 0.1490655081232258, -0.24659427665500788, -0.07370463389445815, 0.07443561581404586, 0.007279000816899433... |
708.1953 | Linear Quantum Error Correction | We develop a generalized theory of quantum error correction (QEC) that
applies to any linear map, in particular maps that are not completely positive
(CP). This theory describes entanglement-assisted QEC for invertible noise
maps, which we use to provides an example of the physical implementation of
non-CP recovery m... | quant-ph | we develop a generalized theory of quantum error correction qec that applies to any linear map in particular maps that are not completely positive cp this theory describes entanglementassisted qec for invertible noise maps which we use to provides an example of the physical implementation of noncp recovery maps we argu... | [['we', 'develop', 'a', 'generalized', 'theory', 'of', 'quantum', 'error', 'correction', 'qec', 'that', 'applies', 'to', 'any', 'linear', 'map', 'in', 'particular', 'maps', 'that', 'are', 'not', 'completely', 'positive', 'cp', 'this', 'theory', 'describes', 'entanglementassisted', 'qec', 'for', 'invertible', 'noise', '... | [-0.13366444519563736, 0.07913683445737908, -0.08135888015536906, 0.08656801194762932, -0.006047710969850614, -0.23299121187830513, 0.07409517182031186, 0.3274879453147387, -0.27208891240033234, -0.200121260913355, 0.11363681425588423, -0.2306873810404984, -0.2206006029215581, 0.193002881261508, -0.14530707831651746, 0... |
708.1954 | Why Do Only Some Galaxy Clusters Have Cool Cores? | Flux-limited X-ray samples indicate that about half of rich galaxy clusters
have cool cores. Why do only some clusters have cool cores while others do not?
In this paper, cosmological N-body + Eulerian hydrodynamic simulations,
including radiative cooling and heating, are used to address this question as
we examine t... | astro-ph | fluxlimited xray samples indicate that about half of rich galaxy clusters have cool cores why do only some clusters have cool cores while others do not in this paper cosmological nbody eulerian hydrodynamic simulations including radiative cooling and heating are used to address this question as we examine the formation... | [['fluxlimited', 'xray', 'samples', 'indicate', 'that', 'about', 'half', 'of', 'rich', 'galaxy', 'clusters', 'have', 'cool', 'cores', 'why', 'do', 'only', 'some', 'clusters', 'have', 'cool', 'cores', 'while', 'others', 'do', 'not', 'in', 'this', 'paper', 'cosmological', 'nbody', 'eulerian', 'hydrodynamic', 'simulations... | [-0.06929218444994485, 0.11583850400057898, -0.07954172917092953, 0.15727681282393757, -0.02376940210361451, -0.035590040578634415, 0.07966289167336857, 0.4308136885954817, -0.194498691485646, -0.35783162032141974, 0.04250579764651081, -0.2818185043312547, -0.006649966966128943, 0.14575210317323967, 0.04082165461002667... |
708.1955 | Cofinement, entropy, and single-particle dynamics of equilibrium
hard-sphere mixtures | We use discontinuous molecular dynamics and grand-canonical transition-matrix
Monte Carlo simulations to explore how confinement between parallel hard walls
modifies the relationships between packing fraction, self-diffusivity, partial
molar excess entropy, and total excess entropy for binary hard-sphere mixtures.
To... | cond-mat.soft cond-mat.stat-mech | we use discontinuous molecular dynamics and grandcanonical transitionmatrix monte carlo simulations to explore how confinement between parallel hard walls modifies the relationships between packing fraction selfdiffusivity partial molar excess entropy and total excess entropy for binary hardsphere mixtures to accomplis... | [['we', 'use', 'discontinuous', 'molecular', 'dynamics', 'and', 'grandcanonical', 'transitionmatrix', 'monte', 'carlo', 'simulations', 'to', 'explore', 'how', 'confinement', 'between', 'parallel', 'hard', 'walls', 'modifies', 'the', 'relationships', 'between', 'packing', 'fraction', 'selfdiffusivity', 'partial', 'molar... | [-0.0651657344959138, 0.22721014238533638, -0.0875869498943447, 0.08857347198083695, 0.01223547794355478, -0.1229307189714325, 0.07538388525216566, 0.36991364050204356, -0.2718697373320906, -0.33199537039406035, 0.013129857454228221, -0.34903354491672417, -0.06264622850246684, 0.09106226173240282, -0.0151995312822229, ... |
708.1956 | Transforming squeezed light into a large amplitude coherent state
superposition | A quantum superposition of two coherent states of light with small amplitude
can be obtained by subtracting a photon from a squeezed vacuum state. In
experiments this preparation can be made conditioned on the detection of a
photon in the field from a squeezed light source. We propose and analyze an
extended measurem... | quant-ph | a quantum superposition of two coherent states of light with small amplitude can be obtained by subtracting a photon from a squeezed vacuum state in experiments this preparation can be made conditioned on the detection of a photon in the field from a squeezed light source we propose and analyze an extended measurement ... | [['a', 'quantum', 'superposition', 'of', 'two', 'coherent', 'states', 'of', 'light', 'with', 'small', 'amplitude', 'can', 'be', 'obtained', 'by', 'subtracting', 'a', 'photon', 'from', 'a', 'squeezed', 'vacuum', 'state', 'in', 'experiments', 'this', 'preparation', 'can', 'be', 'made', 'conditioned', 'on', 'the', 'detect... | [-0.11988600340290842, 0.28589577702862723, -0.14455433855905678, 0.026168601179961115, 0.027744894423945385, -0.1431138865141706, 0.07570767633671605, 0.3681051641928427, -0.2317475813059983, -0.2882050353130608, 0.07658252501366378, -0.23907368178995306, -0.031404465824986495, 0.25529104530472646, -0.0537595532227759... |
708.1957 | Spin torque contribution to the a.c. spin Hall conductivity | Using the recently proposed definition of a conserved spin-current operator
[J. Shi et al., Phys. Rev. Lett. 96, 076604 (2006)] we explore the frequency
dependent spin Hall conductivity for a two-dimensional electron gas with Rashba
and Dresselhaus spin-orbit interaction in response to an oscillating electric
field. ... | cond-mat.mes-hall | using the recently proposed definition of a conserved spincurrent operator j shi et al phys rev lett 96 076604 2006 we explore the frequency dependent spin hall conductivity for a twodimensional electron gas with rashba and dresselhaus spinorbit interaction in response to an oscillating electric field we show that the ... | [['using', 'the', 'recently', 'proposed', 'definition', 'of', 'a', 'conserved', 'spincurrent', 'operator', 'j', 'shi', 'et', 'al', 'phys', 'rev', 'lett', '96', '076604', '2006', 'we', 'explore', 'the', 'frequency', 'dependent', 'spin', 'hall', 'conductivity', 'for', 'a', 'twodimensional', 'electron', 'gas', 'with', 'ra... | [-0.19466079685824095, 0.1770499332648349, 0.010589546560945491, -0.07035331772677304, -0.1009347597654495, -0.10002680466185132, -0.008468909420087815, 0.3469197603666948, -0.24591181144609842, -0.30496105770506554, -0.03824832773534581, -0.2538250198048199, -0.17164921880300557, 0.2104022480133507, -0.024123605625290... |
708.1958 | Charge, geometry, and effective mass | Charge, like mass in Newtonian mechanics, is an irreducible element of
electromagnetic theory that must be introduced ab initio. Its origin is not
properly a part of the theory. Fields are then defined in terms of forces on
either masses--in the case of Newtonian mechanics, or charges in the case of
electromagnetism.... | gr-qc | charge like mass in newtonian mechanics is an irreducible element of electromagnetic theory that must be introduced ab initio its origin is not properly a part of the theory fields are then defined in terms of forces on either massesin the case of newtonian mechanics or charges in the case of electromagnetism general r... | [['charge', 'like', 'mass', 'in', 'newtonian', 'mechanics', 'is', 'an', 'irreducible', 'element', 'of', 'electromagnetic', 'theory', 'that', 'must', 'be', 'introduced', 'ab', 'initio', 'its', 'origin', 'is', 'not', 'properly', 'a', 'part', 'of', 'the', 'theory', 'fields', 'are', 'then', 'defined', 'in', 'terms', 'of', ... | [-0.13277358814430912, 0.1334785355612569, -0.14270805964867275, 0.04880829205004764, -0.09462015536569414, -0.0956136436512073, -0.06753244803819274, 0.3114445643011658, -0.24433016251950038, -0.26204972193532045, 0.037398880215117794, -0.2756405278685547, -0.1522560069004872, 0.15261004678683265, -0.07236770349332974... |
708.1959 | The zero-energy state in graphene in a high magnetic field | The fate of the charge-neutral Dirac point in graphene in a high magnetic
field $H$ has been investigated at low temperatures ($T\sim$ 0.3 K). In samples
with small $V_0$ (the gate voltage needed to access the Dirac point), the
resistance $R_0$ at the Dirac point diverges steeply with $H$, signalling a
crossover to a... | cond-mat.mes-hall cond-mat.mtrl-sci | the fate of the chargeneutral dirac point in graphene in a high magnetic field h has been investigated at low temperatures tsim 03 k in samples with small v_0 the gate voltage needed to access the dirac point the resistance r_0 at the dirac point diverges steeply with h signalling a crossover to an insulating state in ... | [['the', 'fate', 'of', 'the', 'chargeneutral', 'dirac', 'point', 'in', 'graphene', 'in', 'a', 'high', 'magnetic', 'field', 'h', 'has', 'been', 'investigated', 'at', 'low', 'temperatures', 'tsim', '03', 'k', 'in', 'samples', 'with', 'small', 'v_0', 'the', 'gate', 'voltage', 'needed', 'to', 'access', 'the', 'dirac', 'poi... | [-0.20574791383804733, 0.2559193993413631, -0.03849590467961179, -0.01354934208781564, 0.003978760764194825, -0.22755803394889862, 0.12318627863699935, 0.35817903792965655, -0.22264103757543968, -0.2825892108886205, -0.0019660239208720088, -0.37367524172073785, -0.012233264609864078, 0.11830501634742796, 0.008577491771... |
708.196 | Ultra-high energy neutrino scattering | Estimates are made of the ultra-high energy neutrino cross sections based on
an extrapolation to very small Bjorken x of the logarithmic Froissart
dependence in x shown previously to provide an excellent fit to the measured
proton structure function F_2^p(x,Q^2) over a broad range of the virtuality
Q^2. Expressions a... | hep-ph astro-ph | estimates are made of the ultrahigh energy neutrino cross sections based on an extrapolation to very small bjorken x of the logarithmic froissart dependence in x shown previously to provide an excellent fit to the measured proton structure function f_2pxq2 over a broad range of the virtuality q2 expressions are obtaine... | [['estimates', 'are', 'made', 'of', 'the', 'ultrahigh', 'energy', 'neutrino', 'cross', 'sections', 'based', 'on', 'an', 'extrapolation', 'to', 'very', 'small', 'bjorken', 'x', 'of', 'the', 'logarithmic', 'froissart', 'dependence', 'in', 'x', 'shown', 'previously', 'to', 'provide', 'an', 'excellent', 'fit', 'to', 'the',... | [-0.03437696891850001, 0.14022041996872328, -0.03378822260430821, 0.17071155898870444, -0.010147179472523759, -0.08018502312490523, 0.036034359356425794, 0.38913543747281126, -0.13751450650183097, -0.32688618177451406, 0.009974291621716166, -0.3082299370468014, 0.0635370318887685, 0.27620926676845214, 0.075876924077505... |
708.1961 | The jamming transition and new percolation universality classes in
particulate systems with attraction | We numerically study the jamming transition in particulate systems with
attraction by investigating their mechanical response at zero temperature. We
find three regimes of mechanical behavior separated by two critical
transitions--connectivity and rigidity percolation. The transitions belong to
different universality... | cond-mat.soft cond-mat.stat-mech | we numerically study the jamming transition in particulate systems with attraction by investigating their mechanical response at zero temperature we find three regimes of mechanical behavior separated by two critical transitionsconnectivity and rigidity percolation the transitions belong to different universality class... | [['we', 'numerically', 'study', 'the', 'jamming', 'transition', 'in', 'particulate', 'systems', 'with', 'attraction', 'by', 'investigating', 'their', 'mechanical', 'response', 'at', 'zero', 'temperature', 'we', 'find', 'three', 'regimes', 'of', 'mechanical', 'behavior', 'separated', 'by', 'two', 'critical', 'transition... | [-0.12363769002521122, 0.2934414556932072, -0.07774025081283033, 0.026525679942955013, 0.030480325258087734, -0.18930572353985528, 0.07448861976219735, 0.4145102447921961, -0.2300088904981672, -0.28971066415100033, 0.06638576695367589, -0.34555593489761083, -0.1759126904800954, 0.10277112733415315, 0.055896987626984924... |
708.1962 | Exact Cover with light | We suggest a new optical solution for solving the YES/NO version of the Exact
Cover problem by using the massive parallelism of light. The idea is to build
an optical device which can generate all possible solutions of the problem and
then to pick the correct one. In our case the device has a graph-like
representatio... | cs.AR cs.DC | we suggest a new optical solution for solving the yesno version of the exact cover problem by using the massive parallelism of light the idea is to build an optical device which can generate all possible solutions of the problem and then to pick the correct one in our case the device has a graphlike representation and ... | [['we', 'suggest', 'a', 'new', 'optical', 'solution', 'for', 'solving', 'the', 'yesno', 'version', 'of', 'the', 'exact', 'cover', 'problem', 'by', 'using', 'the', 'massive', 'parallelism', 'of', 'light', 'the', 'idea', 'is', 'to', 'build', 'an', 'optical', 'device', 'which', 'can', 'generate', 'all', 'possible', 'solut... | [-0.13216930725965412, 0.0866925187331191, -0.07975818095964533, 0.032362020346100286, -0.13927974530696113, -0.16539364845692356, 0.11320112887482583, 0.36022051900648805, -0.3160226049161033, -0.32613840082047296, 0.09567795179300677, -0.30104333894692736, -0.13223568266670255, 0.1851773265442705, -0.0655864525757305... |
708.1963 | Origin of the Non-Linear Pressure Effects in Perovskite Manganites:
Buckling of Mn-O-Mn Bonds and Jahn-Teller Distortion of the MnO6 Octahedra
Induced by Pressure | High-pressure resistivity and x-ray diffraction have been measured on
La0.85MnO3-d. At low pressures the metal-insulator transition temperature (TMI)
increases linearly with pressure up to a critical pressure, P* ~ 3.4 GPa, which
is followed by reduction of TMI with increasing pressure. Analysis of the bond
distances... | cond-mat.mtrl-sci | highpressure resistivity and xray diffraction have been measured on la085mno3d at low pressures the metalinsulator transition temperature tmi increases linearly with pressure up to a critical pressure p 34 gpa which is followed by reduction of tmi with increasing pressure analysis of the bond distances and bond angles ... | [['highpressure', 'resistivity', 'and', 'xray', 'diffraction', 'have', 'been', 'measured', 'on', 'la085mno3d', 'at', 'low', 'pressures', 'the', 'metalinsulator', 'transition', 'temperature', 'tmi', 'increases', 'linearly', 'with', 'pressure', 'up', 'to', 'a', 'critical', 'pressure', 'p', '34', 'gpa', 'which', 'is', 'fo... | [-0.15638870002980204, 0.2933997080243867, -0.014139413228793734, -0.06693892163925687, -0.0005942416061572302, -0.1360603311559421, 0.15429941562657384, 0.38215642747865325, -0.31238893762059594, -0.3032928145619045, 0.037787841472389366, -0.3895559972366211, -0.06857919348296763, 0.1425785073882033, 0.043854053142940... |
708.1964 | Solving the subset-sum problem with a light-based device | We propose a special computational device which uses light rays for solving
the subset-sum problem. The device has a graph-like representation and the
light is traversing it by following the routes given by the connections between
nodes. The nodes are connected by arcs in a special way which lets us to
generate all p... | cs.AR cs.AI cs.DC | we propose a special computational device which uses light rays for solving the subsetsum problem the device has a graphlike representation and the light is traversing it by following the routes given by the connections between nodes the nodes are connected by arcs in a special way which lets us to generate all possibl... | [['we', 'propose', 'a', 'special', 'computational', 'device', 'which', 'uses', 'light', 'rays', 'for', 'solving', 'the', 'subsetsum', 'problem', 'the', 'device', 'has', 'a', 'graphlike', 'representation', 'and', 'the', 'light', 'is', 'traversing', 'it', 'by', 'following', 'the', 'routes', 'given', 'by', 'the', 'connect... | [-0.16044869894176372, 0.12206143480318588, -0.0454256395023549, -0.013465877068483678, -0.11746856721947552, -0.15312523703869374, 0.14064093515207787, 0.3813429542860831, -0.3161550175427692, -0.3245073596772272, 0.07512274219698156, -0.32003458326471446, -0.10482311069972639, 0.1713490608635766, -0.06340702879970195... |
708.1965 | Tail Asymptotics and Estimation for Elliptical Distributions | Let (X,Y) be a bivariate elliptical random vector with associated random
radius in the Gumbel max-domain of attraction. In this paper we obtain a second
order asymptotic expansion of the joint survival probability P(X > x, Y> y) for
x,y large. Further, based on the asymptotic bounds we discuss some aspects of
the sta... | math.PR math.ST stat.TH | let xy be a bivariate elliptical random vector with associated random radius in the gumbel maxdomain of attraction in this paper we obtain a second order asymptotic expansion of the joint survival probability px x y y for xy large further based on the asymptotic bounds we discuss some aspects of the statistical modelli... | [['let', 'xy', 'be', 'a', 'bivariate', 'elliptical', 'random', 'vector', 'with', 'associated', 'random', 'radius', 'in', 'the', 'gumbel', 'maxdomain', 'of', 'attraction', 'in', 'this', 'paper', 'we', 'obtain', 'a', 'second', 'order', 'asymptotic', 'expansion', 'of', 'the', 'joint', 'survival', 'probability', 'px', 'x',... | [-0.10722616111161187, 0.10154510880238377, -0.13916084231459536, 0.11194398823681695, -0.017595094977878034, -0.10388085346494336, 0.0954707809160027, 0.34902293275808915, -0.22391034637621487, -0.16131155329640023, 0.035708688457816606, -0.28195346739084926, -0.1082018368615536, 0.08044823532327428, -0.10577635475783... |
708.1966 | Incompatibility of modulated checkerboard patterns with the neutron
scattering resonance peak in cuprate superconductors | Checkerboard patterns have been proposed in order to explain STM experiments
on the cuprates BSCCO and Na-CCOC. However the presence of these patterns has
not been confirmed by a bulk probe such as neutron scattering. In particular,
simple checkerboard patterns are inconsistent with neutron scattering data, in
that t... | cond-mat.supr-con cond-mat.str-el | checkerboard patterns have been proposed in order to explain stm experiments on the cuprates bscco and naccoc however the presence of these patterns has not been confirmed by a bulk probe such as neutron scattering in particular simple checkerboard patterns are inconsistent with neutron scattering data in that they hav... | [['checkerboard', 'patterns', 'have', 'been', 'proposed', 'in', 'order', 'to', 'explain', 'stm', 'experiments', 'on', 'the', 'cuprates', 'bscco', 'and', 'naccoc', 'however', 'the', 'presence', 'of', 'these', 'patterns', 'has', 'not', 'been', 'confirmed', 'by', 'a', 'bulk', 'probe', 'such', 'as', 'neutron', 'scattering'... | [-0.13511879641293106, 0.16273838920996672, -0.08601091937161982, 0.1040981738197029, -0.10963373101120324, -0.13175305798159617, 0.045587104232981804, 0.409752347559276, -0.23756556106045057, -0.29819920983925263, 0.06663377520714053, -0.3169535449362899, -0.1584322865844067, 0.1674455682042447, 0.004281131896239362, ... |
708.1967 | Solar System Constraints on Gauss-Bonnet Dark Energy | Quadratic curvature Gauss-Bonnet gravity may be the solution to the dark
energy problem, but a large coupling strength is required. This can lead to
conflict with laboratory and planetary tests of Newton's law, as well as light
bending. The corresponding constraints are derived. If applied directly to
cosmological sc... | hep-th | quadratic curvature gaussbonnet gravity may be the solution to the dark energy problem but a large coupling strength is required this can lead to conflict with laboratory and planetary tests of newtons law as well as light bending the corresponding constraints are derived if applied directly to cosmological scales the ... | [['quadratic', 'curvature', 'gaussbonnet', 'gravity', 'may', 'be', 'the', 'solution', 'to', 'the', 'dark', 'energy', 'problem', 'but', 'a', 'large', 'coupling', 'strength', 'is', 'required', 'this', 'can', 'lead', 'to', 'conflict', 'with', 'laboratory', 'and', 'planetary', 'tests', 'of', 'newtons', 'law', 'as', 'well',... | [-0.1491306128251987, 0.1574754510598723, -0.09696205257593343, 0.08779321729865236, -0.15937162820094575, -0.15738943602579336, -0.00836068787612021, 0.2723555233950416, -0.2842708062225332, -0.4135409539875885, 0.08949202731989013, -0.26011320917556685, -0.05535778878256679, 0.19610336935147643, -0.037159544369205835... |
708.1968 | Some quasinilpotent generators of the hyperfinite $\mathrm{II}_1$ factor | For each sequence $\{c_n\}_n$ in $l_{1}(\N)$ we define an operator $A$ in the
hyperfinite $\mathrm{II}_1$-factor $\mathcal{R}$. We prove that these operators
are quasinilpotent and they generate the whole hyperfinite
$\mathrm{II}_1$-factor. We show that they have non-trivial, closed, invariant
subspaces affiliated to... | math.OA math.FA | for each sequence c_n_n in l_1n we define an operator a in the hyperfinite mathrmii_1factor mathcalr we prove that these operators are quasinilpotent and they generate the whole hyperfinite mathrmii_1factor we show that they have nontrivial closed invariant subspaces affiliated to the von neumann algebra and we provide... | [['for', 'each', 'sequence', 'c_n_n', 'in', 'l_1n', 'we', 'define', 'an', 'operator', 'a', 'in', 'the', 'hyperfinite', 'mathrmii_1factor', 'mathcalr', 'we', 'prove', 'that', 'these', 'operators', 'are', 'quasinilpotent', 'and', 'they', 'generate', 'the', 'whole', 'hyperfinite', 'mathrmii_1factor', 'we', 'show', 'that',... | [-0.14494485907290164, 0.10389449404838898, -0.09659544229381592, 0.10231549830620622, -0.07708502400179838, -0.0913074085874869, -0.0024268483923462866, 0.42467470596091367, -0.31146658191809784, -0.20745079697588006, 0.12286209859696494, -0.2949590404929073, -0.18198813889322485, 0.19138992140656924, -0.0889846708013... |
708.1969 | Linear Algebraic Groups without the Normalizer Theorem | One can develop the basic structure theory of linear algebraic groups (the
root system, Bruhat decomposition, etc.) in a way that bypasses several major
steps in the standard development, including the self-normalizing property of
Borel subgroups.
| math.RT math.AG | one can develop the basic structure theory of linear algebraic groups the root system bruhat decomposition etc in a way that bypasses several major steps in the standard development including the selfnormalizing property of borel subgroups | [['one', 'can', 'develop', 'the', 'basic', 'structure', 'theory', 'of', 'linear', 'algebraic', 'groups', 'the', 'root', 'system', 'bruhat', 'decomposition', 'etc', 'in', 'a', 'way', 'that', 'bypasses', 'several', 'major', 'steps', 'in', 'the', 'standard', 'development', 'including', 'the', 'selfnormalizing', 'property'... | [-0.15828901406429294, 0.05487853930228286, -0.12032041602974965, 0.060173536029954754, -0.11629120017298394, -0.0864931855790524, 0.011967792081931192, 0.29234610847197473, -0.4087338542513963, -0.20408408783583176, 0.13729215927499658, -0.2231424670252535, -0.1681964008053506, 0.18721961684059352, -0.1162286718867512... |
708.197 | Pair creation supernovae at low and high redshift | Pair creation supernovae (PCSN) are thought to be produced from very massive
low metallicity stars. The spectacularly bright SN 2006gy does show signatures
expected from PCSNe. Here, we investigate the metallicity threshold below which
PCSN can form and estimate their occurrence rate. We perform stellar evolution
cal... | astro-ph | pair creation supernovae pcsn are thought to be produced from very massive low metallicity stars the spectacularly bright sn 2006gy does show signatures expected from pcsne here we investigate the metallicity threshold below which pcsn can form and estimate their occurrence rate we perform stellar evolution calculation... | [['pair', 'creation', 'supernovae', 'pcsn', 'are', 'thought', 'to', 'be', 'produced', 'from', 'very', 'massive', 'low', 'metallicity', 'stars', 'the', 'spectacularly', 'bright', 'sn', '2006gy', 'does', 'show', 'signatures', 'expected', 'from', 'pcsne', 'here', 'we', 'investigate', 'the', 'metallicity', 'threshold', 'be... | [-0.041220269937884996, 0.20953664432384353, -0.02477079468037196, 0.18010138626643682, -0.09479851848887838, -0.12758220512330293, 0.09657707762092671, 0.419820740739292, -0.14230241429279833, -0.3292685966978577, 0.03842086695323892, -0.27129356964257234, -0.00919904596393898, 0.2269261697304739, -0.05079391393398855... |
708.1971 | Nimesulide limits kainate-induced oxidative damage in the rat
hippocampus | Kainate induces a marked expression of cyclooxygenase-2 after its systemic
administration. Because cyclooxygenase-2 activity is associated to the
production of reactive oxygen species, we investigated the effects of
nimesulide, a selective cyclooxygenase-2 inhibitor, on kainate-induced in vivo
oxidative damage in the... | q-bio.TO | kainate induces a marked expression of cyclooxygenase2 after its systemic administration because cyclooxygenase2 activity is associated to the production of reactive oxygen species we investigated the effects of nimesulide a selective cyclooxygenase2 inhibitor on kainateinduced in vivo oxidative damage in the rat hippo... | [['kainate', 'induces', 'a', 'marked', 'expression', 'of', 'cyclooxygenase2', 'after', 'its', 'systemic', 'administration', 'because', 'cyclooxygenase2', 'activity', 'is', 'associated', 'to', 'the', 'production', 'of', 'reactive', 'oxygen', 'species', 'we', 'investigated', 'the', 'effects', 'of', 'nimesulide', 'a', 'se... | [-0.10585193724141062, 0.1741341474686855, 0.048768422143898676, 0.017568101677995596, 0.053773460669692644, -0.11576131093747836, 0.10607024856852655, 0.4041776703958659, -0.1754046882953994, -0.2578344856855128, 0.07104106802138087, -0.3090092336816579, -0.18705647208334245, 0.1330262318147903, -0.15306499458971845, ... |
708.1972 | The Qweak Experiment -- A search for new physics at the TeV Scale | A new precision measurement of the parity violating analyzing power in
longitudinally polarized electron scattering from the proton at very low Q^2 at
an incident energy of 1.16 GeV is in the final stages of preparation for
execution at Jefferson Laboratory (JLab). A 2200 hour measurement of the parity
violating asym... | nucl-ex | a new precision measurement of the parity violating analyzing power in longitudinally polarized electron scattering from the proton at very low q2 at an incident energy of 116 gev is in the final stages of preparation for execution at jefferson laboratory jlab a 2200 hour measurement of the parity violating asymmetry i... | [['a', 'new', 'precision', 'measurement', 'of', 'the', 'parity', 'violating', 'analyzing', 'power', 'in', 'longitudinally', 'polarized', 'electron', 'scattering', 'from', 'the', 'proton', 'at', 'very', 'low', 'q2', 'at', 'an', 'incident', 'energy', 'of', '116', 'gev', 'is', 'in', 'the', 'final', 'stages', 'of', 'prepar... | [-0.08288743141262482, 0.23231799210698884, -0.07739378579342654, 0.08780581518252031, -0.019253136290170184, -0.1595976411796024, 0.09140331844425853, 0.30661018440281756, -0.20717351778980916, -0.3516550703175567, 0.030419163784507226, -0.3156796136464838, 0.09549687224595498, 0.18643844910993804, 0.05100536003062787... |
708.1973 | Strong violations of Bell-type inequalities for Werner-like states | We investigate the violation of Bell-type inequalities for two-qubit
Werner-like states parametrized by the positive parameter 0<p<1. We use an
unbalanced homodyne detection scheme to obtain the quantum mechanical
probabilities. A violation of the Bell-Wigner and Janssens inequalities is
obtained for a large range of... | quant-ph | we investigate the violation of belltype inequalities for twoqubit wernerlike states parametrized by the positive parameter 0p1 we use an unbalanced homodyne detection scheme to obtain the quantum mechanical probabilities a violation of the bellwigner and janssens inequalities is obtained for a large range of the param... | [['we', 'investigate', 'the', 'violation', 'of', 'belltype', 'inequalities', 'for', 'twoqubit', 'wernerlike', 'states', 'parametrized', 'by', 'the', 'positive', 'parameter', '0p1', 'we', 'use', 'an', 'unbalanced', 'homodyne', 'detection', 'scheme', 'to', 'obtain', 'the', 'quantum', 'mechanical', 'probabilities', 'a', '... | [-0.12480392206220998, 0.15128572403633253, -0.0051419184321042045, 0.07322299350992939, -0.01643277278785175, -0.20571476527395735, 0.08817991531676177, 0.27463296780345636, -0.25072099312012075, -0.30265072276901217, 0.09464476761779825, -0.2601115492240893, -0.05187478069421075, 0.2448827945413666, -0.05180248631262... |
708.1974 | Isotopic composition of cosmic-ray sources | We use the GALPROP code and the Advanced Composition Explorer (ACE) data to
derive the cosmic ray (CR) isotopic composition at the sources. The composition
is derived for two propagation models, diffusive reacceleration and plain
diffusion. We show that the compositions derived assuming these two propagation
models a... | astro-ph | we use the galprop code and the advanced composition explorer ace data to derive the cosmic ray cr isotopic composition at the sources the composition is derived for two propagation models diffusive reacceleration and plain diffusion we show that the compositions derived assuming these two propagation models are differ... | [['we', 'use', 'the', 'galprop', 'code', 'and', 'the', 'advanced', 'composition', 'explorer', 'ace', 'data', 'to', 'derive', 'the', 'cosmic', 'ray', 'cr', 'isotopic', 'composition', 'at', 'the', 'sources', 'the', 'composition', 'is', 'derived', 'for', 'two', 'propagation', 'models', 'diffusive', 'reacceleration', 'and'... | [-0.05674423992131201, 0.18256344482494843, -0.015520548477532372, 0.14556235456950076, -0.028202649265054672, -0.023647206303264414, -0.025489535167931565, 0.45358834770463763, -0.3471382684554786, -0.32411815007291145, 0.029167751715119396, -0.3198180076858354, -0.03565099835395813, 0.20887122584122514, 0.07278042213... |
708.1975 | Spin relaxation in $n$-type GaAs quantum wells with transient spin
grating | By solving the kinetic spin Bloch equations, we study the time evolution of
the transient spin grating, whose spin polarization varies periodically in real
space, confined in (001) GaAs quantum wells. With this study we can investigate
the properties of both the spin transport and the spin relaxation at the same
time... | cond-mat.mtrl-sci | by solving the kinetic spin bloch equations we study the time evolution of the transient spin grating whose spin polarization varies periodically in real space confined in 001 gaas quantum wells with this study we can investigate the properties of both the spin transport and the spin relaxation at the same time the fou... | [['by', 'solving', 'the', 'kinetic', 'spin', 'bloch', 'equations', 'we', 'study', 'the', 'time', 'evolution', 'of', 'the', 'transient', 'spin', 'grating', 'whose', 'spin', 'polarization', 'varies', 'periodically', 'in', 'real', 'space', 'confined', 'in', '001', 'gaas', 'quantum', 'wells', 'with', 'this', 'study', 'we',... | [-0.15957645913666654, 0.20690978847972463, -0.018981920134929286, 0.00278323862774225, -0.03147535708640174, -0.12417709409739032, 0.0046217202675605425, 0.3800238593011788, -0.2791314480475501, -0.29512946693391995, 0.009854911443539512, -0.29142037670337695, -0.10742983927958326, 0.21844904801255954, 0.0550756023297... |
708.1976 | Preparation of Neutron-activated Xenon for Liquid Xenon Detector
Calibration | We report the preparation of neutron-activated xenon for the calibration of
liquid xenon (LXe) detectors. Gamma rays from the decay of xenon metastable
states, produced by fast neutron activation, were detected and their activities
measured in a LXe scintillation detector. Following a five-day activation of
natural x... | physics.ins-det astro-ph nucl-ex | we report the preparation of neutronactivated xenon for the calibration of liquid xenon lxe detectors gamma rays from the decay of xenon metastable states produced by fast neutron activation were detected and their activities measured in a lxe scintillation detector following a fiveday activation of natural xenon gas w... | [['we', 'report', 'the', 'preparation', 'of', 'neutronactivated', 'xenon', 'for', 'the', 'calibration', 'of', 'liquid', 'xenon', 'lxe', 'detectors', 'gamma', 'rays', 'from', 'the', 'decay', 'of', 'xenon', 'metastable', 'states', 'produced', 'by', 'fast', 'neutron', 'activation', 'were', 'detected', 'and', 'their', 'act... | [0.010241473493741002, 0.29797770469743123, -0.019506178997658396, 0.07141038129391435, 0.05896095417205009, -0.1440124906524009, 0.11574066986606733, 0.41516881009882634, -0.1771408876882413, -0.42455466100023137, 0.03807370922096107, -0.42827188342742556, 0.1159608023291504, 0.19830550316213588, 0.08851808720889191, ... |
708.1977 | Truly Minimal Left-Right Symmetry Model for Electroweak Interaction | By using two primary doublets and one induced bidoublet Higgs fields as a
result of the interactions of the two doublets, we evaluate the predictive
power of the left-right symmetry model based on $SU(2)_{L}\otimes
SU(2)_{R}\otimes U(1)$ gauge group to the gauge bosons masses, leptons masses,
and the structure of ele... | hep-ph | by using two primary doublets and one induced bidoublet higgs fields as a result of the interactions of the two doublets we evaluate the predictive power of the leftright symmetry model based on su2_lotimes su2_rotimes u1 gauge group to the gauge bosons masses leptons masses and the structure of electroweak interaction... | [['by', 'using', 'two', 'primary', 'doublets', 'and', 'one', 'induced', 'bidoublet', 'higgs', 'fields', 'as', 'a', 'result', 'of', 'the', 'interactions', 'of', 'the', 'two', 'doublets', 'we', 'evaluate', 'the', 'predictive', 'power', 'of', 'the', 'leftright', 'symmetry', 'model', 'based', 'on', 'su2_lotimes', 'su2_roti... | [-0.13640428928371806, 0.3358536587813153, 0.004205765221447039, 0.16787994601136932, -0.08573904272455435, -0.17310125736089854, 0.031100233293210086, 0.3199421811795149, -0.2143061238484314, -0.32135500710171, 0.01938906534666715, -0.2915590610140218, -0.010550674903564728, 0.06390374041377352, 0.08662828751481497, -... |
708.1978 | Parabolic equations with the second order Cauchy conditions on the
boundary | The paper studies some ill-posed boundary value problems on semi-plane for
parabolic equations with homogenuous Cauchy condition at initial time and with
the second order Cauchy condition on the boundary of the semi-plane. A class of
inputs that allows some regularity is suggested and described explicitly in
frequenc... | math.AP math-ph math.MP | the paper studies some illposed boundary value problems on semiplane for parabolic equations with homogenuous cauchy condition at initial time and with the second order cauchy condition on the boundary of the semiplane a class of inputs that allows some regularity is suggested and described explicitly in frequency doma... | [['the', 'paper', 'studies', 'some', 'illposed', 'boundary', 'value', 'problems', 'on', 'semiplane', 'for', 'parabolic', 'equations', 'with', 'homogenuous', 'cauchy', 'condition', 'at', 'initial', 'time', 'and', 'with', 'the', 'second', 'order', 'cauchy', 'condition', 'on', 'the', 'boundary', 'of', 'the', 'semiplane', ... | [-0.14114223930557243, 0.07576969983514215, -0.02471548496730259, 0.03852156020861241, -0.1225358342110622, -0.09807768712186667, -0.05263335547661867, 0.32345622776412086, -0.2931135976534398, -0.2012046950212756, 0.23454615165723763, -0.2486426453986377, -0.12154337557673943, 0.191736708654732, -0.0864667094724833, 0... |
708.1979 | Advances in Cardinal Arithmetic | If cf(kappa) = kappa, kappa^+< cf(lambda) = \lambda, then there is a
stationary subset S of {delta<lambda:cf(delta)=kappa} in I[lambda]. Moreover,
we can find <C_delta :delta in S>, C_delta a club of lambda,
otp(C_delta)=kappa, guessing clubs and for each alpha<lambda we have: {C_delta
\cap alpha: alpha \in nacc(C_de... | math.LO | if cfkappa kappa kappa cflambda lambda then there is a stationary subset s of deltalambdacfdeltakappa in ilambda moreover we can find c_delta delta in s c_delta a club of lambda otpc_deltakappa guessing clubs and for each alphalambda we have c_delta cap alpha alpha in naccc_delta has cardinality lambda also we prove th... | [['if', 'cfkappa', 'kappa', 'kappa', 'cflambda', 'lambda', 'then', 'there', 'is', 'a', 'stationary', 'subset', 's', 'of', 'deltalambdacfdeltakappa', 'in', 'ilambda', 'moreover', 'we', 'can', 'find', 'c_delta', 'delta', 'in', 's', 'c_delta', 'a', 'club', 'of', 'lambda', 'otpc_deltakappa', 'guessing', 'clubs', 'and', 'fo... | [-0.13226162116331308, 0.15546560843868815, -0.08319846947783048, 0.05572477587229889, -0.09243122935679156, -0.20463291192715316, 0.04999463360026939, 0.43468138437295695, -0.27658149327353104, -0.18570904804336041, 0.08074416785822586, -0.34103810061345396, -0.08599078350882862, 0.17007096548631942, -0.07687901240802... |
708.198 | The first almost free Whitehead group | Assume G.C.H. and kappa is the first uncountable cardinal such that there is
a kappa-free abelian group which is not a Whitehead (abelian) group. We prove
that kappa is necessarily an inaccessible cardinal
| math.LO | assume gch and kappa is the first uncountable cardinal such that there is a kappafree abelian group which is not a whitehead abelian group we prove that kappa is necessarily an inaccessible cardinal | [['assume', 'gch', 'and', 'kappa', 'is', 'the', 'first', 'uncountable', 'cardinal', 'such', 'that', 'there', 'is', 'a', 'kappafree', 'abelian', 'group', 'which', 'is', 'not', 'a', 'whitehead', 'abelian', 'group', 'we', 'prove', 'that', 'kappa', 'is', 'necessarily', 'an', 'inaccessible', 'cardinal']] | [-0.2735335172037594, 0.25271820133320944, -0.170003504230408, 0.13080195647489745, -0.2353125490481034, -0.1938262468611356, -0.019506712087604683, 0.38444770220667124, -0.2979073994792998, -0.07190929329954088, 0.13125027260684874, -0.29978291445877403, -0.07364656869322062, 0.1630161594512174, -0.11381209250248503, ... |
708.1981 | On some problems in general topology | We prove that Arhangelskii's problem has a consistent positive answer: if
V\models CH, then for some aleph_1-complete aleph_2-c.c. forcing notion P of
cardinality aleph_2 we have that P forces ``CH and there is a Lindelof regular
topological space of size aleph_2 with clopen basis with every point of
pseudo-character... | math.LO | we prove that arhangelskiis problem has a consistent positive answer if vmodels ch then for some aleph_1complete aleph_2cc forcing notion p of cardinality aleph_2 we have that p forces ch and there is a lindelof regular topological space of size aleph_2 with clopen basis with every point of pseudocharacter aleph_0 ie e... | [['we', 'prove', 'that', 'arhangelskiis', 'problem', 'has', 'a', 'consistent', 'positive', 'answer', 'if', 'vmodels', 'ch', 'then', 'for', 'some', 'aleph_1complete', 'aleph_2cc', 'forcing', 'notion', 'p', 'of', 'cardinality', 'aleph_2', 'we', 'have', 'that', 'p', 'forces', 'ch', 'and', 'there', 'is', 'a', 'lindelof', '... | [-0.1794945553965157, 0.17109907247746983, -0.05950247978658548, 0.08157758158493034, -0.07976957525880564, -0.20251372681065863, 0.07062627793805275, 0.3545477484253102, -0.2885814678766543, -0.1329288787618723, 0.08697546455853929, -0.3394028577243998, -0.05393237483111166, 0.13368699597638278, -0.11412061025649087, ... |
708.1982 | Abelian and non-abelian second cohomologies of quantized enveloping
algebras | For a class of pointed Hopf algebras including the quantized enveloping
algebras, we discuss cleft extensions, cocycle deformations and the second
cohomology. We present such a non-standard method of computing the abelian
second cohomology that derives information from the non-abelian second
cohomology classifying cl... | math.QA | for a class of pointed hopf algebras including the quantized enveloping algebras we discuss cleft extensions cocycle deformations and the second cohomology we present such a nonstandard method of computing the abelian second cohomology that derives information from the nonabelian second cohomology classifying cleft ext... | [['for', 'a', 'class', 'of', 'pointed', 'hopf', 'algebras', 'including', 'the', 'quantized', 'enveloping', 'algebras', 'we', 'discuss', 'cleft', 'extensions', 'cocycle', 'deformations', 'and', 'the', 'second', 'cohomology', 'we', 'present', 'such', 'a', 'nonstandard', 'method', 'of', 'computing', 'the', 'abelian', 'sec... | [-0.21862167880305503, 0.03287899013433117, -0.06988987847246596, 0.12950560082032606, -0.168935000743778, -0.16233124000737903, -0.020286687909335386, 0.2534536735505843, -0.41376193780757364, -0.17597577479652693, 0.15404759941729487, -0.18196880129990398, -0.2081347879816274, 0.21014062180870868, -0.1947890277489157... |
708.1983 | Two-component Duality and Strings | A phenomenologically successful two-component hadronic duality picture led to
Veneziano's amplitude, the fundamental first step to string theory. This
picture is briefly recalled and its two components are identified as the open
strings (mesons and baryons) and closed strings (Pomeron).
| hep-th hep-ph physics.hist-ph | a phenomenologically successful twocomponent hadronic duality picture led to venezianos amplitude the fundamental first step to string theory this picture is briefly recalled and its two components are identified as the open strings mesons and baryons and closed strings pomeron | [['a', 'phenomenologically', 'successful', 'twocomponent', 'hadronic', 'duality', 'picture', 'led', 'to', 'venezianos', 'amplitude', 'the', 'fundamental', 'first', 'step', 'to', 'string', 'theory', 'this', 'picture', 'is', 'briefly', 'recalled', 'and', 'its', 'two', 'components', 'are', 'identified', 'as', 'the', 'open... | [-0.15174493388039992, 0.25359763715823647, -0.1377503158058971, 0.22339723128825426, -0.10398253067396582, -0.16698211864568294, 0.050004468587576414, 0.3186703204642981, -0.22369052779395132, -0.21021376941353082, -0.002895535173593089, -0.26556151392869654, -0.08120640840497799, 0.08159631886519492, 0.01462338876444... |
708.1984 | Density is at most the spread of the square | We show the following result:
Assume B is an infinite Boolean Algebra and lambda=d(B). Then s(B*B)$, i.e.
s(uf(B)xuf(B))>= lambda$ (if lambda limit - obtained)
| math.LO | we show the following result assume b is an infinite boolean algebra and lambdadb then sbb ie sufbxufb lambda if lambda limit obtained | [['we', 'show', 'the', 'following', 'result', 'assume', 'b', 'is', 'an', 'infinite', 'boolean', 'algebra', 'and', 'lambdadb', 'then', 'sbb', 'ie', 'sufbxufb', 'lambda', 'if', 'lambda', 'limit', 'obtained']] | [-0.11810403565565745, 0.0964009966098404, -0.04606653098016977, 0.03265220537183008, -0.06855558768092167, -0.1741369787958406, 0.007454885613350641, 0.34712785411448704, -0.38635714245694025, -0.12711082802464566, 0.08200387876214725, -0.24107600553404718, -0.12923375481650942, 0.13235545118472405, -0.017366092313923... |
708.1985 | Relativistic ab initio study of forbidden transitions of singly ionized
Zinc using CCSD(T) | In this work, the {\it ab initio} calculations have been carried out to study
the oscillator strengths corresponding to `forbidden transitions' of
astrophysically important electromagnetic transitions of singly ionized zinc,
Zn II. Many important electron correlations are considered to all-orders using
the relativist... | physics.atom-ph physics.comp-ph | in this work the it ab initio calculations have been carried out to study the oscillator strengths corresponding to forbidden transitions of astrophysically important electromagnetic transitions of singly ionized zinc zn ii many important electron correlations are considered to allorders using the relativistic coupledc... | [['in', 'this', 'work', 'the', 'it', 'ab', 'initio', 'calculations', 'have', 'been', 'carried', 'out', 'to', 'study', 'the', 'oscillator', 'strengths', 'corresponding', 'to', 'forbidden', 'transitions', 'of', 'astrophysically', 'important', 'electromagnetic', 'transitions', 'of', 'singly', 'ionized', 'zinc', 'zn', 'ii'... | [-0.0661042144932654, 0.14496577696208793, 0.025846165157065937, 0.08819012499479477, 0.011751733580103485, -0.12545340094635243, 0.0185343044376882, 0.46948718686177526, -0.1566858071062754, -0.3183580807920906, 0.00243110088281013, -0.31397906911117524, -0.058806954812939446, 0.15720456211216827, 0.12798995270283633,... |
708.1986 | Duality and Recycling Computing in Quantum Computers | Quantum computer possesses quantum parallelism and offers great computing
power over classical computer \cite{er1,er2}. As is well-know, a moving quantum
object passing through a double-slit exhibits particle wave duality. A quantum
computer is static and lacks this duality property. The recently proposed
duality com... | quant-ph | quantum computer possesses quantum parallelism and offers great computing power over classical computer citeer1er2 as is wellknow a moving quantum object passing through a doubleslit exhibits particle wave duality a quantum computer is static and lacks this duality property the recently proposed duality computer has ex... | [['quantum', 'computer', 'possesses', 'quantum', 'parallelism', 'and', 'offers', 'great', 'computing', 'power', 'over', 'classical', 'computer', 'citeer1er2', 'as', 'is', 'wellknow', 'a', 'moving', 'quantum', 'object', 'passing', 'through', 'a', 'doubleslit', 'exhibits', 'particle', 'wave', 'duality', 'a', 'quantum', '... | [-0.1447449817943819, 0.11058205932691531, -0.1907935965612406, 0.057932839103368376, -0.10415441456415722, -0.2274425426079183, 0.03886937098794853, 0.3488886065995009, -0.32235430214447125, -0.29649569447994517, 0.06574573322938995, -0.20223762445000298, -0.20279509199863416, 0.25997226367677834, -0.07813693805816072... |
708.1987 | Environmental effect on the subhalo abundance -- a solution to the
missing dwarf problem | Recent high-resolution simulations of the formation of dark-matter halos have
shown that the distribution of subhalos is scale-free, in the sense that if
scaled by the velocity dispersion of the parent halo, the velocity distribution
function of galaxy-sized and cluster-sized halos are identical. For
cluster-sized ha... | astro-ph | recent highresolution simulations of the formation of darkmatter halos have shown that the distribution of subhalos is scalefree in the sense that if scaled by the velocity dispersion of the parent halo the velocity distribution function of galaxysized and clustersized halos are identical for clustersized halos simulat... | [['recent', 'highresolution', 'simulations', 'of', 'the', 'formation', 'of', 'darkmatter', 'halos', 'have', 'shown', 'that', 'the', 'distribution', 'of', 'subhalos', 'is', 'scalefree', 'in', 'the', 'sense', 'that', 'if', 'scaled', 'by', 'the', 'velocity', 'dispersion', 'of', 'the', 'parent', 'halo', 'the', 'velocity', ... | [-0.10184876412725852, 0.11553943428794662, -0.09918937623126513, 0.11152466641500611, -0.08046478320093621, 0.03347558693505788, -0.04004840808363551, 0.3954464508193817, -0.10496071333725131, -0.4105443069221158, 0.0033805960266846432, -0.30559889928540257, -0.04639916096114371, 0.1997242017145576, 0.0161003991848684... |
708.1988 | Electrically Small Supergain Arrays | The theory, computer simulations, and experimental measurements are presented
for electrically small two-element supergain arrays with near optimal endfire
gains of 7 dB. We show how the difficulties of narrow tolerances, large
mismatches, low radiation efficiencies, and reduced scattering of electrically
small paras... | physics.class-ph | the theory computer simulations and experimental measurements are presented for electrically small twoelement supergain arrays with near optimal endfire gains of 7 db we show how the difficulties of narrow tolerances large mismatches low radiation efficiencies and reduced scattering of electrically small parasitic elem... | [['the', 'theory', 'computer', 'simulations', 'and', 'experimental', 'measurements', 'are', 'presented', 'for', 'electrically', 'small', 'twoelement', 'supergain', 'arrays', 'with', 'near', 'optimal', 'endfire', 'gains', 'of', '7', 'db', 'we', 'show', 'how', 'the', 'difficulties', 'of', 'narrow', 'tolerances', 'large',... | [-0.17684814402218763, 0.24310315072216326, 0.114219406619668, -0.01518567470338894, -0.02352499166408961, -0.18670660787029192, 0.06796668147399032, 0.4231731084000785, -0.25418959905800875, -0.3417284180977731, 0.1091824705270028, -0.31148511330684414, -0.1258342973633262, 0.2345163767968188, -0.05313544535601977, 0.... |
708.1989 | Four-dimensional lattice chiral gauge theories with anomalous fermion
content | In continuum field theory, it has been discussed that chiral gauge theories
with Weyl fermions in anomalous gauge representations (anomalous gauge
theories) can consistently be quantized, provided that some of gauge bosons are
permitted to acquire mass. Such theories in four dimensions are inevitablly
non-renormaliza... | hep-lat hep-th | in continuum field theory it has been discussed that chiral gauge theories with weyl fermions in anomalous gauge representations anomalous gauge theories can consistently be quantized provided that some of gauge bosons are permitted to acquire mass such theories in four dimensions are inevitablly nonrenormalizable and ... | [['in', 'continuum', 'field', 'theory', 'it', 'has', 'been', 'discussed', 'that', 'chiral', 'gauge', 'theories', 'with', 'weyl', 'fermions', 'in', 'anomalous', 'gauge', 'representations', 'anomalous', 'gauge', 'theories', 'can', 'consistently', 'be', 'quantized', 'provided', 'that', 'some', 'of', 'gauge', 'bosons', 'ar... | [-0.12569830818215338, 0.23542001601331655, -0.10934924311288519, 0.11166562949145417, -0.11249462298185724, -0.181734856777461, 0.023827751923108292, 0.3616041302987624, -0.1553348825971891, -0.2881343571445053, 0.026833073230369424, -0.23459420452553142, -0.18203255848635397, 0.07263012834336245, -0.03450812790656417... |
708.199 | Rational singularities associated to pairs | In this paper we introduce a notion of rational singularities associated to
pairs $(X, \ba^t)$ where $X$ is a variety, $\ba$ is an ideal sheaf and $t$ is a
nonnegative real number. We prove that most standard results about rational
singularities extend to this context. We also show that some results commonly
associat... | math.AG math.AC | in this paper we introduce a notion of rational singularities associated to pairs x bat where x is a variety ba is an ideal sheaf and t is a nonnegative real number we prove that most standard results about rational singularities extend to this context we also show that some results commonly associated with log termina... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'notion', 'of', 'rational', 'singularities', 'associated', 'to', 'pairs', 'x', 'bat', 'where', 'x', 'is', 'a', 'variety', 'ba', 'is', 'an', 'ideal', 'sheaf', 'and', 't', 'is', 'a', 'nonnegative', 'real', 'number', 'we', 'prove', 'that', 'most', 'standard', 'results', 'ab... | [-0.16452491305858255, 0.02928406617436586, -0.06264391251985567, 0.10729448724655906, -0.09955835658271449, -0.12634526525276252, -0.003789582310794258, 0.35890895114785215, -0.30779525550806064, -0.20285323410328612, 0.05963011981683772, -0.2935884090881032, -0.21012291643229952, 0.2127482860786728, -0.14930356747235... |
708.1991 | Conditions for the Trivers-Willard hypothesis to be valid: A minimal
population-genetic model | The very insightful Trivers-Willard hypothesis, proposed in the early 1970s,
states that females in good physiological conditions are more likely to produce
male offspring, when the variance of reproductive success amongst males is
high. A number of studies, aimed at its experimental verification, have found
adequate... | q-bio.PE | the very insightful triverswillard hypothesis proposed in the early 1970s states that females in good physiological conditions are more likely to produce male offspring when the variance of reproductive success amongst males is high a number of studies aimed at its experimental verification have found adequate supporti... | [['the', 'very', 'insightful', 'triverswillard', 'hypothesis', 'proposed', 'in', 'the', 'early', '1970s', 'states', 'that', 'females', 'in', 'good', 'physiological', 'conditions', 'are', 'more', 'likely', 'to', 'produce', 'male', 'offspring', 'when', 'the', 'variance', 'of', 'reproductive', 'success', 'amongst', 'males... | [-0.08954097194684027, 0.15089581427033202, -0.08395224310044513, 0.11813931799375675, -0.06472121130488157, -0.18255083737681738, 0.09774583790526713, 0.3599411600784228, -0.21162736144008665, -0.3197056203424721, 0.08837794376173201, -0.2661631312254082, -0.12669397872695567, 0.1778561095676375, -0.10372442775037022,... |
708.1992 | Distance-regular graphs of $q$-Racah type and the $q$-tetrahedron
algebra | In this paper we discuss a relationship between the following two algebras:
(i) the subconstituent algebra $T$ of a distance-regular graph that has
$q$-Racah type; (ii) the $q$-tetrahedron algebra $\boxtimes_q$ which is a
$q$-deformation of the three-point $sl_2$ loop algebra. Assuming that every
irreducible $T$-modu... | math.CO math.RT | in this paper we discuss a relationship between the following two algebras i the subconstituent algebra t of a distanceregular graph that has qracah type ii the qtetrahedron algebra boxtimes_q which is a qdeformation of the threepoint sl_2 loop algebra assuming that every irreducible tmodule is thin we display an algeb... | [['in', 'this', 'paper', 'we', 'discuss', 'a', 'relationship', 'between', 'the', 'following', 'two', 'algebras', 'i', 'the', 'subconstituent', 'algebra', 't', 'of', 'a', 'distanceregular', 'graph', 'that', 'has', 'qracah', 'type', 'ii', 'the', 'qtetrahedron', 'algebra', 'boxtimes_q', 'which', 'is', 'a', 'qdeformation',... | [-0.173247307206371, 0.10070708838944224, -0.09504780936986208, -0.007554354209319821, -0.11447458696950759, -0.17425789647469564, -0.043715120105272426, 0.39640976004302503, -0.37953517759035876, -0.16738037815583603, 0.09068415821363618, -0.2979125734285584, -0.15603292514570058, 0.1512364820178066, -0.10099235869732... |
708.1993 | Dynamics of glucose-lactose diauxic growth in E. coli | We present a mathematical model of glucose-lactose diauxic growth in
Escherichia coli including both the postive and negative regulation mechanisms
of the lactose operon as well as the inducer exclusion. To validate this model,
we first calculated the time evolution of beta-galactosidase for only the
lactose nutrient... | q-bio.OT q-bio.CB | we present a mathematical model of glucoselactose diauxic growth in escherichia coli including both the postive and negative regulation mechanisms of the lactose operon as well as the inducer exclusion to validate this model we first calculated the time evolution of betagalactosidase for only the lactose nutrient and c... | [['we', 'present', 'a', 'mathematical', 'model', 'of', 'glucoselactose', 'diauxic', 'growth', 'in', 'escherichia', 'coli', 'including', 'both', 'the', 'postive', 'and', 'negative', 'regulation', 'mechanisms', 'of', 'the', 'lactose', 'operon', 'as', 'well', 'as', 'the', 'inducer', 'exclusion', 'to', 'validate', 'this', ... | [-0.05098041434559906, 0.08225178997555192, 0.005388302089270661, 0.03845888522469945, 0.026620588101969475, -0.11682188526008344, 0.0629996834098149, 0.35299867403840546, -0.20676053089514507, -0.26578315069670216, 0.08192345919291767, -0.3061768575081308, -0.19623271312172474, 0.22808952377945707, -0.0297589116942202... |
708.1994 | Hall Conductivity of Flavor Fields from AdS/CFT | We use the AdS/CFT correspondence to compute a conductivity associated with
massive N=2 supersymmetric hypermultiplet fields at finite baryon density,
propagating through an N=4 supersymmetric SU(Nc) Yang-Mills plasma in the large
Nc, large 't Hooft coupling limit. We do so by introducing external electric
and magnet... | hep-th | we use the adscft correspondence to compute a conductivity associated with massive n2 supersymmetric hypermultiplet fields at finite baryon density propagating through an n4 supersymmetric sunc yangmills plasma in the large nc large t hooft coupling limit we do so by introducing external electric and magnetic fields co... | [['we', 'use', 'the', 'adscft', 'correspondence', 'to', 'compute', 'a', 'conductivity', 'associated', 'with', 'massive', 'n2', 'supersymmetric', 'hypermultiplet', 'fields', 'at', 'finite', 'baryon', 'density', 'propagating', 'through', 'an', 'n4', 'supersymmetric', 'sunc', 'yangmills', 'plasma', 'in', 'the', 'large', '... | [-0.1495012461761885, 0.2335012494552331, -0.02510864824156831, 0.07968153785531043, -0.0821825204582154, -0.10061243497118165, -0.015064132571717005, 0.3053843220047464, -0.17820659778788214, -0.2825708480528261, 0.024583017763009744, -0.2970058289179696, -0.10861231579115213, 0.1003433983143761, -0.031434159186562595... |
708.1995 | Hybrid single-electron transistor as a source of quantized electric
current | The basis of synchronous manipulation of individual electrons in solid-state
devices was laid by the rise of single-electronics about two decades ago.
Ultra-small structures in a low temperature environment form an ideal domain of
addressing electrons one by one. A long-standing challenge in this field has
been the r... | cond-mat.mes-hall | the basis of synchronous manipulation of individual electrons in solidstate devices was laid by the rise of singleelectronics about two decades ago ultrasmall structures in a low temperature environment form an ideal domain of addressing electrons one by one a longstanding challenge in this field has been the realizati... | [['the', 'basis', 'of', 'synchronous', 'manipulation', 'of', 'individual', 'electrons', 'in', 'solidstate', 'devices', 'was', 'laid', 'by', 'the', 'rise', 'of', 'singleelectronics', 'about', 'two', 'decades', 'ago', 'ultrasmall', 'structures', 'in', 'a', 'low', 'temperature', 'environment', 'form', 'an', 'ideal', 'doma... | [-0.14263323845903675, 0.11065899490098342, -0.06923483968289061, 0.013058475154853226, -0.05266714501213898, -0.17415550659691592, 0.08020235676980339, 0.3613775957044799, -0.24465042407853405, -0.33228036662811905, 0.08477890471618023, -0.24417483502390894, -0.09846080453250526, 0.2752607121470977, -0.065875260708738... |
708.1996 | Effective free energy method for nematic liquid crystals in contact with
structured substrates | We study the phase behavior of a nematic liquid crystal confined between a
flat substrate with strong anchoring and a patterned substrate whose structure
and local anchoring strength we vary. By first evaluating an effective surface
free energy function characterizing the patterned substrate we derive an
expression f... | cond-mat.soft cond-mat.stat-mech | we study the phase behavior of a nematic liquid crystal confined between a flat substrate with strong anchoring and a patterned substrate whose structure and local anchoring strength we vary by first evaluating an effective surface free energy function characterizing the patterned substrate we derive an expression for ... | [['we', 'study', 'the', 'phase', 'behavior', 'of', 'a', 'nematic', 'liquid', 'crystal', 'confined', 'between', 'a', 'flat', 'substrate', 'with', 'strong', 'anchoring', 'and', 'a', 'patterned', 'substrate', 'whose', 'structure', 'and', 'local', 'anchoring', 'strength', 'we', 'vary', 'by', 'first', 'evaluating', 'an', 'e... | [-0.1671045530222457, 0.19822276290683108, -0.08943920395639096, 0.03003218121896655, -0.01834048656432109, -0.13331936058475058, 0.056548806109522294, 0.4146866835653782, -0.26736376231152414, -0.32199864480660195, 0.003040453138276683, -0.2459103911596931, -0.12903015158529318, 0.12640641513123252, 0.0459311130123112... |
708.1997 | Time and nonlocal realism: Consequences of the before-before experiment | It is argued that recent experiments refuting nonlocal realism, can also be
considered as experiments refuting time-ordered nonlocality and, hence,
confirming the result of the before-before experiment. However, the
before-before experiment provides a broader refutation because it also
falsifies the testable relativi... | quant-ph | it is argued that recent experiments refuting nonlocal realism can also be considered as experiments refuting timeordered nonlocality and hence confirming the result of the beforebefore experiment however the beforebefore experiment provides a broader refutation because it also falsifies the testable relativistic versi... | [['it', 'is', 'argued', 'that', 'recent', 'experiments', 'refuting', 'nonlocal', 'realism', 'can', 'also', 'be', 'considered', 'as', 'experiments', 'refuting', 'timeordered', 'nonlocality', 'and', 'hence', 'confirming', 'the', 'result', 'of', 'the', 'beforebefore', 'experiment', 'however', 'the', 'beforebefore', 'exper... | [-0.09054801846578928, 0.11278257267156118, -0.13918464133043734, 0.13998675714968375, -0.10293534901780142, -0.1878461687576393, 0.018253944473157466, 0.2198357840239162, -0.20737843532902253, -0.2991142707916213, 0.04713745239439984, -0.25820629125539685, -0.14679814261240018, 0.18820902411038923, -0.0554241246845520... |
708.1998 | Spectroscopy of the hot pulsating star Beta Cephei. Velocities and EWs
from C,N,O and Si lines | Frequencies in oscillating $\beta$ Cephei stars are usually inferred by means
of radial velocities measured from the SiIII triplet 4552-4574 A. These lines,
relatively insensitive to the variation of Teff through a pulsation cycle, show
small equivalent width variations. In this study we aimed to verify if the
behavi... | astro-ph | frequencies in oscillating beta cephei stars are usually inferred by means of radial velocities measured from the siiii triplet 45524574 a these lines relatively insensitive to the variation of teff through a pulsation cycle show small equivalent width variations in this study we aimed to verify if the behavior of radi... | [['frequencies', 'in', 'oscillating', 'beta', 'cephei', 'stars', 'are', 'usually', 'inferred', 'by', 'means', 'of', 'radial', 'velocities', 'measured', 'from', 'the', 'siiii', 'triplet', '45524574', 'a', 'these', 'lines', 'relatively', 'insensitive', 'to', 'the', 'variation', 'of', 'teff', 'through', 'a', 'pulsation', ... | [-0.04831150616981317, 0.10465143986701837, -0.010671456162557965, 0.04473292299940015, -0.07565570618885334, -0.11808735805927364, 0.05333910013355171, 0.4387180318200537, -0.19348126420273562, -0.3394718691726643, 0.05602485022973269, -0.30206645985409747, -0.02084194190646302, 0.2115822041086461, -0.0280684786189203... |
708.1999 | Bi-Legendrian manifolds and paracontact geometry | We study the interplays between paracontact geometry and the theory of
bi-Legendrian manifolds. We interpret the bi-Legendrian connection of a
bi-Legendrian manifold M as the paracontact connection of a canonical
paracontact structure induced on M and then we discuss many consequences of
this result both for bi-Legen... | math.DG | we study the interplays between paracontact geometry and the theory of bilegendrian manifolds we interpret the bilegendrian connection of a bilegendrian manifold m as the paracontact connection of a canonical paracontact structure induced on m and then we discuss many consequences of this result both for bilegendrian a... | [['we', 'study', 'the', 'interplays', 'between', 'paracontact', 'geometry', 'and', 'the', 'theory', 'of', 'bilegendrian', 'manifolds', 'we', 'interpret', 'the', 'bilegendrian', 'connection', 'of', 'a', 'bilegendrian', 'manifold', 'm', 'as', 'the', 'paracontact', 'connection', 'of', 'a', 'canonical', 'paracontact', 'str... | [-0.24634572354404896, 0.04052365331559396, -0.0629823902377584, 0.1676182124332418, -0.1159898857357072, -0.10701363663509732, -0.07544660880650225, 0.4410063955688574, -0.2339644614668166, -0.2611534464951666, 0.0739009789282792, -0.2854387265339982, -0.31972259686129995, 0.1726114503107965, -0.10262985050021747, -0.... |
708.2 | Leptogenesis within a generalized quark-lepton symmetry | Quark-lepton symmetry has been shown to be inconsistent with baryogenesis via
leptogenesis in natural schemes of the see-saw mechanism. Within the
phenomenological approach of textures, we relax this strict symmetry and
propose weaker conditions, namely models of the neutrino Dirac mass matrix
$M_D$ which have the sa... | hep-ph | quarklepton symmetry has been shown to be inconsistent with baryogenesis via leptogenesis in natural schemes of the seesaw mechanism within the phenomenological approach of textures we relax this strict symmetry and propose weaker conditions namely models of the neutrino dirac mass matrix m_d which have the same hierar... | [['quarklepton', 'symmetry', 'has', 'been', 'shown', 'to', 'be', 'inconsistent', 'with', 'baryogenesis', 'via', 'leptogenesis', 'in', 'natural', 'schemes', 'of', 'the', 'seesaw', 'mechanism', 'within', 'the', 'phenomenological', 'approach', 'of', 'textures', 'we', 'relax', 'this', 'strict', 'symmetry', 'and', 'propose'... | [-0.1298201589670498, 0.2585481052246439, -0.009450042691941444, 0.16599973755849837, -0.07305728882784024, -0.14468907585027269, 0.03293468146465528, 0.3579145711249648, -0.24135921832520324, -0.2790815347062352, 0.057790125150812596, -0.2308146365595838, -0.07227960609210034, 0.08804526653898975, 0.018101156590721354... |
708.2001 | Screening model for nanowire surface-charge sensors in liquid | The conductance change of nanowire field-effect transistors is considered a
highly sensitive probe for surface charge. However, Debye screening of relevant
physiological liquid environments challenge device performance due to competing
screening from the ionic liquid and nanowire charge carriers. We discuss this
effe... | cond-mat.soft cond-mat.mes-hall | the conductance change of nanowire fieldeffect transistors is considered a highly sensitive probe for surface charge however debye screening of relevant physiological liquid environments challenge device performance due to competing screening from the ionic liquid and nanowire charge carriers we discuss this effect wit... | [['the', 'conductance', 'change', 'of', 'nanowire', 'fieldeffect', 'transistors', 'is', 'considered', 'a', 'highly', 'sensitive', 'probe', 'for', 'surface', 'charge', 'however', 'debye', 'screening', 'of', 'relevant', 'physiological', 'liquid', 'environments', 'challenge', 'device', 'performance', 'due', 'to', 'competi... | [-0.12338725259061903, 0.1355941001046449, -0.04065142928622663, 0.05713376133702695, -0.001666651121340692, -0.19776462870649994, 0.05382302595418878, 0.3829080525971949, -0.1938814861490391, -0.30431158644147216, -0.012786098280921579, -0.29812625049613417, -0.12918946922582109, 0.1838936979137361, -0.009720430739689... |
708.2002 | Measuring the Broad-band X-Ray Spectrum from 400 eV to 40 keV in the
Southwest Part of the Supernova Remnant RX J1713.7-3946 | We report on results from Suzaku broadband X-ray observations of the
southwest part of the Galactic supernova remnant (SNR) RX J1713.7-3946 with an
energy coverage of 0.4-40 keV. The X-ray spectrum, presumably of synchrotron
origin, is known to be completely lineless, making this SNR ideally suited for
a detailed stu... | astro-ph | we report on results from suzaku broadband xray observations of the southwest part of the galactic supernova remnant snr rx j171373946 with an energy coverage of 0440 kev the xray spectrum presumably of synchrotron origin is known to be completely lineless making this snr ideally suited for a detailed study of the xray... | [['we', 'report', 'on', 'results', 'from', 'suzaku', 'broadband', 'xray', 'observations', 'of', 'the', 'southwest', 'part', 'of', 'the', 'galactic', 'supernova', 'remnant', 'snr', 'rx', 'j171373946', 'with', 'an', 'energy', 'coverage', 'of', '0440', 'kev', 'the', 'xray', 'spectrum', 'presumably', 'of', 'synchrotron', '... | [-0.011647103913963643, 0.12584072977096686, -0.07647338281949406, 0.12441231012177308, -0.10781688544368831, -0.148427372265841, 0.061815833333553956, 0.4596444119807884, -0.20105167311478422, -0.39548050616387564, 0.04447022544307793, -0.35114213412903217, 0.055762911148603184, 0.2331034156634533, 0.00501363549011888... |
708.2003 | The logarithmic Sobolev inequality along the Ricci flow in dimension 2 | In this paper we present our results on the logarithmic Sobolev inequality
along the Ricci flow in dimension 2.
| math.DG | in this paper we present our results on the logarithmic sobolev inequality along the ricci flow in dimension 2 | [['in', 'this', 'paper', 'we', 'present', 'our', 'results', 'on', 'the', 'logarithmic', 'sobolev', 'inequality', 'along', 'the', 'ricci', 'flow', 'in', 'dimension', '2']] | [-0.14294065613495677, 0.024640967358687992, -0.07487923985249118, 0.019316948625553203, -0.024690994478173946, -0.09218221824420125, -0.07743577972685575, 0.3480087871614255, -0.26867898475182683, -0.17853913848337374, 0.13032112742382052, -0.325611859167877, -0.1511762075518307, 0.19199934440027727, -0.14311500570099... |
708.2004 | Reply to `Can infrared gravitons screen $\Lambda$?' | We reply to the recent criticism by Garriga and Tanaka of our proposal that
quantum gravitational loop corrections may lead to a secular screening of the
effective cosmological constant. Their argument rests upon a renormalization
scheme in which the composite operator $(R \sqrt{-g} - 4 \Lambda \sqrt{-g}
)_{\rm ren}$... | hep-th astro-ph gr-qc | we reply to the recent criticism by garriga and tanaka of our proposal that quantum gravitational loop corrections may lead to a secular screening of the effective cosmological constant their argument rests upon a renormalization scheme in which the composite operator r sqrtg 4 lambda sqrtg _rm ren is defined to be the... | [['we', 'reply', 'to', 'the', 'recent', 'criticism', 'by', 'garriga', 'and', 'tanaka', 'of', 'our', 'proposal', 'that', 'quantum', 'gravitational', 'loop', 'corrections', 'may', 'lead', 'to', 'a', 'secular', 'screening', 'of', 'the', 'effective', 'cosmological', 'constant', 'their', 'argument', 'rests', 'upon', 'a', 'r... | [-0.16017500969936097, 0.16602425486780703, -0.1249226638404209, 0.11171319246336463, -0.10510186988172963, -0.16258740294281215, -0.016560369429533324, 0.31435064215745245, -0.20767201118315348, -0.26993929571250364, 0.07261406830511988, -0.23904304040063704, -0.1596769216193241, 0.14203353877001929, -0.05619916917916... |
708.2005 | The logarithmic Sobolev inequality along the Ricci flow: the case
$\lambda_0(g_0)=0$ | We extend our previous results on the logarithmic Sobolev inequality along
the Ricci flow in the case $\lambda_0(g_0)>0$ to the case $\lambda_0(g_0)=0$.
| math.DG | we extend our previous results on the logarithmic sobolev inequality along the ricci flow in the case lambda_0g_00 to the case lambda_0g_00 | [['we', 'extend', 'our', 'previous', 'results', 'on', 'the', 'logarithmic', 'sobolev', 'inequality', 'along', 'the', 'ricci', 'flow', 'in', 'the', 'case', 'lambda_0g_00', 'to', 'the', 'case', 'lambda_0g_00']] | [-0.13206210351464423, -0.02024392032233829, -0.061710740862922234, 0.04523259536786513, -0.08034089258448644, -0.08565001977099614, -0.0516405248609689, 0.32492582008919935, -0.24688995189287447, -0.15157885460013693, 0.10784501378657296, -0.36043607274239714, -0.07795519398694689, 0.23935467140241104, -0.136048291809... |
708.2006 | Search for B0 -> rho0rho0 and Non-Resonant B0 -> 4pi Decays | We search for the decay B0 -> rho0rho0 and other possible charmless modes
with a pi+pi-pi+pi- final state, including B0 -> rho0f0(980), B0 ->
f0(980)f0(980), B0 -> f0(980)pipi, B0 -> rho0pipi and non-resonant B0 -> 4pi.
These results are obtained from a data sample containing 520 x 10^6 BBar pairs
collected by the Be... | hep-ex | we search for the decay b0 rho0rho0 and other possible charmless modes with a pipipipi final state including b0 rho0f0980 b0 f0980f0980 b0 f0980pipi b0 rho0pipi and nonresonant b0 4pi these results are obtained from a data sample containing 520 x 106 bbar pairs collected by the belle detector at the kekb asymmetricener... | [['we', 'search', 'for', 'the', 'decay', 'b0', 'rho0rho0', 'and', 'other', 'possible', 'charmless', 'modes', 'with', 'a', 'pipipipi', 'final', 'state', 'including', 'b0', 'rho0f0980', 'b0', 'f0980f0980', 'b0', 'f0980pipi', 'b0', 'rho0pipi', 'and', 'nonresonant', 'b0', '4pi', 'these', 'results', 'are', 'obtained', 'from... | [-0.1391352611200801, 0.21834656958825477, -0.008575110087069134, 0.07268993490557378, -0.02263282202917776, -0.11066517558216743, 0.21162516622858327, 0.2520188083617042, -0.13304336776012834, -0.28704960353366316, 0.019073466425889158, -0.46739083811742804, 0.13513904718573727, 0.17419381597085715, 0.1009122993101761... |
708.2007 | Textures with two traceless submatrices of the neutrino mass matrix | We propose a new texture for the light neutrino mass matrix. The proposal is
based upon imposing zero-trace condition on the two by two sub-matrices of the
complex symmetric Majorana mass matrix in the flavor basis where the charged
lepton mass matrix is diagonal. Restricting the mass matrix to have two
traceless sub... | hep-ph | we propose a new texture for the light neutrino mass matrix the proposal is based upon imposing zerotrace condition on the two by two submatrices of the complex symmetric majorana mass matrix in the flavor basis where the charged lepton mass matrix is diagonal restricting the mass matrix to have two traceless submatric... | [['we', 'propose', 'a', 'new', 'texture', 'for', 'the', 'light', 'neutrino', 'mass', 'matrix', 'the', 'proposal', 'is', 'based', 'upon', 'imposing', 'zerotrace', 'condition', 'on', 'the', 'two', 'by', 'two', 'submatrices', 'of', 'the', 'complex', 'symmetric', 'majorana', 'mass', 'matrix', 'in', 'the', 'flavor', 'basis'... | [-0.11555036526885541, 0.18795259983333595, 0.0024122331729706597, 0.06828131980591398, -0.07449759438305217, -0.15315632637699736, -2.2729228743735483e-05, 0.36820370300727734, -0.17718577122534898, -0.28768624354373007, 0.15157282283283113, -0.2529233084443738, -0.08832273056237575, 0.14625263515421572, -0.0047780211... |
708.2008 | The Log Entropy Functional Along the Ricci Flow | In this paper we introduce the log entropy functional and establish its
monotonicity along the Ricci flow. One consequence of it is the monotonicity of
the logarithmic Sobolev constant along the Ricci flow.
| math.DG | in this paper we introduce the log entropy functional and establish its monotonicity along the ricci flow one consequence of it is the monotonicity of the logarithmic sobolev constant along the ricci flow | [['in', 'this', 'paper', 'we', 'introduce', 'the', 'log', 'entropy', 'functional', 'and', 'establish', 'its', 'monotonicity', 'along', 'the', 'ricci', 'flow', 'one', 'consequence', 'of', 'it', 'is', 'the', 'monotonicity', 'of', 'the', 'logarithmic', 'sobolev', 'constant', 'along', 'the', 'ricci', 'flow']] | [-0.21140086058188567, 0.043012664540473255, -0.1183215505020185, 0.07136306776241823, -0.09919001811155767, -0.1430502401128637, -0.03220603459031378, 0.3106233704496514, -0.368559852722242, -0.18551630786422527, 0.13985758195419543, -0.31792049222823343, -0.09752265759038203, 0.10375807140812729, -0.11729440330104395... |
708.2009 | Quantum condensation from a tailored exciton population in a microcavity | An experiment is proposed, on the coherent quantum dynamics of a
semiconductor microcavity containing quantum dots. Modeling the experiment
using a generalized Dicke model, we show that a tailored excitation pulse can
create an energy-dependent population of excitons, which subsequently evolves
to a quantum condensat... | cond-mat.str-el cond-mat.supr-con | an experiment is proposed on the coherent quantum dynamics of a semiconductor microcavity containing quantum dots modeling the experiment using a generalized dicke model we show that a tailored excitation pulse can create an energydependent population of excitons which subsequently evolves to a quantum condensate of ex... | [['an', 'experiment', 'is', 'proposed', 'on', 'the', 'coherent', 'quantum', 'dynamics', 'of', 'a', 'semiconductor', 'microcavity', 'containing', 'quantum', 'dots', 'modeling', 'the', 'experiment', 'using', 'a', 'generalized', 'dicke', 'model', 'we', 'show', 'that', 'a', 'tailored', 'excitation', 'pulse', 'can', 'create... | [-0.11276824922404355, 0.23119050328548635, -0.14421204932861859, 0.06571581822936423, 0.0041693662416138165, -0.15963652071109713, 0.050600248107609026, 0.3543886395216557, -0.2489458429109719, -0.24913352894751975, -0.009068761001496265, -0.26508172209853204, -0.11050964965155192, 0.20050436565846516, 0.0086660022918... |
708.201 | A search for solar-like oscillations in K giants in the globular cluster
M4 | To expand the range in the colour-magnitude diagram where asteroseismology
can be applied, we organized a photometry campaign to find evidence for
solar-like oscillations in giant stars in the globular cluster M4. The aim was
to detect the comb-like p-mode structure characteristic for solar-like
oscillations in the a... | astro-ph | to expand the range in the colourmagnitude diagram where asteroseismology can be applied we organized a photometry campaign to find evidence for solarlike oscillations in giant stars in the globular cluster m4 the aim was to detect the comblike pmode structure characteristic for solarlike oscillations in the amplitude ... | [['to', 'expand', 'the', 'range', 'in', 'the', 'colourmagnitude', 'diagram', 'where', 'asteroseismology', 'can', 'be', 'applied', 'we', 'organized', 'a', 'photometry', 'campaign', 'to', 'find', 'evidence', 'for', 'solarlike', 'oscillations', 'in', 'giant', 'stars', 'in', 'the', 'globular', 'cluster', 'm4', 'the', 'aim'... | [-0.09335630305084873, 0.17608927414574496, -0.0855270526919733, 0.13620501441148328, -0.1410242939087124, -0.055886177993242574, 0.08222247804480824, 0.41923330929678154, -0.14340158223036698, -0.38924076751230613, 0.039014629808233996, -0.33127248772036505, -0.05023309778120807, 0.2528907836188891, -0.100027668315734... |
708.2011 | Well-posedness and scattering for the KP-II equation in a critical space | The Cauchy problem for the Kadomtsev-Petviashvili-II equation
(u_t+u_{xxx}+uu_x)_x+u_{yy}=0 is considered. A small data global well-posedness
and scattering result in the scale invariant, non-isotropic, homogeneous
Sobolev space \dot H^{-1/2,0}(R^2) is derived. Additionally, it is proved that
for arbitrarily large in... | math.AP | the cauchy problem for the kadomtsevpetviashviliii equation u_tu_xxxuu_x_xu_yy0 is considered a small data global wellposedness and scattering result in the scale invariant nonisotropic homogeneous sobolev space dot h120r2 is derived additionally it is proved that for arbitrarily large initial data the cauchy problem i... | [['the', 'cauchy', 'problem', 'for', 'the', 'kadomtsevpetviashviliii', 'equation', 'u_tu_xxxuu_x_xu_yy0', 'is', 'considered', 'a', 'small', 'data', 'global', 'wellposedness', 'and', 'scattering', 'result', 'in', 'the', 'scale', 'invariant', 'nonisotropic', 'homogeneous', 'sobolev', 'space', 'dot', 'h120r2', 'is', 'deri... | [-0.1592587819001798, 0.13074534384389247, -0.0401187296475059, 0.148355234775628, -0.04335007455264186, -0.10657320591894075, -0.09092567783202334, 0.31699098209882604, -0.3447390241098815, -0.19939381173201676, 0.18447020404634934, -0.2605527395157722, -0.061237610908674786, 0.18354486014115914, -0.04707816871914788,... |
708.2012 | Relic Radiation from an Evaporating Black Hole | We present a non-string-theoretic calculation of the microcanonical entropy
of relic integer-spin Hawking radiation -- at fixed total energy $E$. The only
conserved macroscopic quantity is the total energy $E$ (the total energy of the
relic radiation). Data for a boundary-value approach, with massless,
integer-spin p... | hep-th | we present a nonstringtheoretic calculation of the microcanonical entropy of relic integerspin hawking radiation at fixed total energy e the only conserved macroscopic quantity is the total energy e the total energy of the relic radiation data for a boundaryvalue approach with massless integerspin perturbations are set... | [['we', 'present', 'a', 'nonstringtheoretic', 'calculation', 'of', 'the', 'microcanonical', 'entropy', 'of', 'relic', 'integerspin', 'hawking', 'radiation', 'at', 'fixed', 'total', 'energy', 'e', 'the', 'only', 'conserved', 'macroscopic', 'quantity', 'is', 'the', 'total', 'energy', 'e', 'the', 'total', 'energy', 'of', ... | [-0.145351549312832, 0.1701902426112958, -0.09565993188407151, 0.10537836421659685, -0.033253194757631215, -0.1262628079195151, 0.04351840651467749, 0.24874371683179605, -0.21895775224437808, -0.2889471267069864, 0.028192560140202504, -0.32717110881415323, -0.03183087195095614, 0.1363063023948088, -0.032061973522318814... |
708.2013 | Quantum amplitudes in black-hole evaporation: Spins 1 and 2 | Quantum amplitudes for $s=1$ at Maxwell fields and for $s=2$ linearised
gravitational wave perturbations of a spherically symmetric Einstein/massless
scalar background, describing gravitational collapse to a black hole, are
treated by analogy with a previous treatment of $s=0$ scalar-field
perturbations of gravitatio... | gr-qc | quantum amplitudes for s1 at maxwell fields and for s2 linearised gravitational wave perturbations of a spherically symmetric einsteinmassless scalar background describing gravitational collapse to a black hole are treated by analogy with a previous treatment of s0 scalarfield perturbations of gravitational collapse at... | [['quantum', 'amplitudes', 'for', 's1', 'at', 'maxwell', 'fields', 'and', 'for', 's2', 'linearised', 'gravitational', 'wave', 'perturbations', 'of', 'a', 'spherically', 'symmetric', 'einsteinmassless', 'scalar', 'background', 'describing', 'gravitational', 'collapse', 'to', 'a', 'black', 'hole', 'are', 'treated', 'by',... | [-0.17959448333829642, 0.15088626586199097, -0.05599905317882076, 0.09216788805206307, -0.09358657811535523, -0.13091029727365822, -0.07342805869411677, 0.3366786496154964, -0.1957887927268166, -0.22998293181415647, 0.11548535872425418, -0.2516561532195192, -0.05449188058730215, 0.17039744525449352, -0.0151541750272735... |
708.2014 | Measurement of the Slope Parameter for the eta->3pi0 Decay in the pp->pp
eta Reaction | The CELSIUS/WASA setup is used to measure the 3pi0 decay of eta mesons
produced in pp interactions with beam kinetic energies of 1.36 and 1.45 GeV.
The efficiency-corrected Dalitz plot and density distributions for this decay
are shown, together with a fit of the quadratic slope parameter alpha yielding
alpha = -0.02... | nucl-ex | the celsiuswasa setup is used to measure the 3pi0 decay of eta mesons produced in pp interactions with beam kinetic energies of 136 and 145 gev the efficiencycorrected dalitz plot and density distributions for this decay are shown together with a fit of the quadratic slope parameter alpha yielding alpha 0026 0010stat 0... | [['the', 'celsiuswasa', 'setup', 'is', 'used', 'to', 'measure', 'the', '3pi0', 'decay', 'of', 'eta', 'mesons', 'produced', 'in', 'pp', 'interactions', 'with', 'beam', 'kinetic', 'energies', 'of', '136', 'and', '145', 'gev', 'the', 'efficiencycorrected', 'dalitz', 'plot', 'and', 'density', 'distributions', 'for', 'this'... | [-0.04358043008505774, 0.19178358813223895, -0.13025795435987675, 0.10381123219849542, -0.013362768106162548, -0.15000379536650144, 0.03154729121888522, 0.329391411603865, -0.1691276313868002, -0.33460059500066563, -0.06374806072744832, -0.3773965079453774, 0.050146730929554906, 0.18853455495263916, 0.0647374013933586,... |
708.2015 | Motion in Brane World Models: The Bazanski Approach | Recently, path equations have been obtained for charged, spinning objects in
brane world models, using a modified Bazanski Lagrangian. In this study, path
deviation equations of extended objects are derived. The significance of moving
extended objects in brane world models is examined. Motion in non- symmetric
brane ... | gr-qc hep-th | recently path equations have been obtained for charged spinning objects in brane world models using a modified bazanski lagrangian in this study path deviation equations of extended objects are derived the significance of moving extended objects in brane world models is examined motion in non symmetric brane world mode... | [['recently', 'path', 'equations', 'have', 'been', 'obtained', 'for', 'charged', 'spinning', 'objects', 'in', 'brane', 'world', 'models', 'using', 'a', 'modified', 'bazanski', 'lagrangian', 'in', 'this', 'study', 'path', 'deviation', 'equations', 'of', 'extended', 'objects', 'are', 'derived', 'the', 'significance', 'of... | [-0.1172418758013429, 0.0981843030357805, -0.10979257939526668, 0.14319683490724017, -0.0879410351626575, -0.16726343017608786, -0.08266027380830984, 0.3487755822626731, -0.1564548420898903, -0.2999869539366605, 0.05864058817566659, -0.2631028788164258, -0.12652856530621648, 0.15577585644160324, -0.11397242909655549, 0... |
708.2016 | Higgs Particle: The Origin of Mass | The Higgs particle is a new elementary particle predicted in the Standard
Model of the elementary particle physics. It plays a special role in the theory
of mass generation of quarks, leptons, and gauge bosons. In this article,
theoretical issues on the Higgs mechanism are first discussed, and then
experimental prosp... | hep-ph | the higgs particle is a new elementary particle predicted in the standard model of the elementary particle physics it plays a special role in the theory of mass generation of quarks leptons and gauge bosons in this article theoretical issues on the higgs mechanism are first discussed and then experimental prospects on ... | [['the', 'higgs', 'particle', 'is', 'a', 'new', 'elementary', 'particle', 'predicted', 'in', 'the', 'standard', 'model', 'of', 'the', 'elementary', 'particle', 'physics', 'it', 'plays', 'a', 'special', 'role', 'in', 'the', 'theory', 'of', 'mass', 'generation', 'of', 'quarks', 'leptons', 'and', 'gauge', 'bosons', 'in', ... | [-0.04750835994879405, 0.2649286770638557, -0.07185700060023616, 0.16974785762140526, -0.09846624267391033, -0.17135883146483039, -0.015252050841485874, 0.29521249356783097, -0.22795381802651618, -0.29174094938466116, 0.026813329209107905, -0.26766264230375075, -0.06288026650824273, 0.17924024482231793, 0.0515687849062... |
708.2017 | Photoelectron spectra of anionic sodium clusters from time-dependent
density-functional theory in real-time | We calculate the excitation energies of small neutral sodium clusters in the
framework of time-dependent density-functional theory. In the presented
calculations, we extract these energies from the power spectra of the dipole
and quadrupole signals that result from a real-time and real-space propagation.
For comparis... | cond-mat.mtrl-sci | we calculate the excitation energies of small neutral sodium clusters in the framework of timedependent densityfunctional theory in the presented calculations we extract these energies from the power spectra of the dipole and quadrupole signals that result from a realtime and realspace propagation for comparison with m... | [['we', 'calculate', 'the', 'excitation', 'energies', 'of', 'small', 'neutral', 'sodium', 'clusters', 'in', 'the', 'framework', 'of', 'timedependent', 'densityfunctional', 'theory', 'in', 'the', 'presented', 'calculations', 'we', 'extract', 'these', 'energies', 'from', 'the', 'power', 'spectra', 'of', 'the', 'dipole', ... | [-0.02901578530971263, 0.08881770878105198, -0.07806406877746151, 0.06940498434611268, 0.06607268077031886, -0.05497457912015553, 0.045704113896873254, 0.4042893918986256, -0.18753601864886446, -0.31200488883297184, -0.06785867187962238, -0.3696026239242103, -0.09556058584083174, 0.1695523844792734, 0.08943497038421196... |
708.2018 | Quantum amplitudes in black-hole evaporation: coherent and squeezed
states | The quantum amplitude for processes involving the formation and evaporation
of black holes was previously calculated by means of a complex-time approach.
In that treatment, we followed Feynman's $+i\epsilon$ approach in quantum field
theory. The Lorentzian time interval $T$, measured at spatial infinity between
a pai... | gr-qc | the quantum amplitude for processes involving the formation and evaporation of black holes was previously calculated by means of a complextime approach in that treatment we followed feynmans iepsilon approach in quantum field theory the lorentzian time interval t measured at spatial infinity between a pair of asymptoti... | [['the', 'quantum', 'amplitude', 'for', 'processes', 'involving', 'the', 'formation', 'and', 'evaporation', 'of', 'black', 'holes', 'was', 'previously', 'calculated', 'by', 'means', 'of', 'a', 'complextime', 'approach', 'in', 'that', 'treatment', 'we', 'followed', 'feynmans', 'iepsilon', 'approach', 'in', 'quantum', 'f... | [-0.1348888066258101, 0.18673566232984026, -0.11784942104333193, 0.09548931100697335, -0.03768060809963113, -0.1412458495981121, 0.005771718710654406, 0.3041066648612652, -0.21167706658793875, -0.2559046790098432, 0.05182834636424363, -0.24331691663137803, -0.11128050839162876, 0.18741030992056618, -0.02237091286360312... |
708.2019 | Giant optical Faraday rotation induced by a single electron spin in a
quantum dot: Applications to entangling remote spins via a single photon | We propose a quantum non-demolition method - giant Faraday rotation - to
detect a single electron spin in a quantum dot inside a microcavity where
negatively-charged exciton strongly couples to the cavity mode. Left- and
right-circularly polarized light reflected from the cavity feels different
phase shifts due to ca... | quant-ph cond-mat.other | we propose a quantum nondemolition method giant faraday rotation to detect a single electron spin in a quantum dot inside a microcavity where negativelycharged exciton strongly couples to the cavity mode left and rightcircularly polarized light reflected from the cavity feels different phase shifts due to cavity quantu... | [['we', 'propose', 'a', 'quantum', 'nondemolition', 'method', 'giant', 'faraday', 'rotation', 'to', 'detect', 'a', 'single', 'electron', 'spin', 'in', 'a', 'quantum', 'dot', 'inside', 'a', 'microcavity', 'where', 'negativelycharged', 'exciton', 'strongly', 'couples', 'to', 'the', 'cavity', 'mode', 'left', 'and', 'right... | [-0.13202061542021845, 0.25357824798909284, -0.07715528571831161, -0.017445954412074857, -0.07610917769274429, -0.2517362535882153, 0.0647160065948571, 0.4444855241399062, -0.2542184998869504, -0.27395166033192686, -0.01424397821415608, -0.2472062497938934, -0.06972689262137895, 0.243388094995661, -0.006911394872555607... |
708.202 | Models with time-dependent parameters using transform methods:
application to Heston's model | This paper presents a methodology to introduce time-dependent parameters for
a wide family of models preserving their analytic tractability. This family
includes hybrid models with stochastic volatility, stochastic interest-rates,
jumps and their non-hybrid counterparts. The methodology is applied to Heston's
model. ... | q-fin.PR math.PR stat.ME | this paper presents a methodology to introduce timedependent parameters for a wide family of models preserving their analytic tractability this family includes hybrid models with stochastic volatility stochastic interestrates jumps and their nonhybrid counterparts the methodology is applied to hestons model a bootstrap... | [['this', 'paper', 'presents', 'a', 'methodology', 'to', 'introduce', 'timedependent', 'parameters', 'for', 'a', 'wide', 'family', 'of', 'models', 'preserving', 'their', 'analytic', 'tractability', 'this', 'family', 'includes', 'hybrid', 'models', 'with', 'stochastic', 'volatility', 'stochastic', 'interestrates', 'jump... | [-0.07063372965369906, -0.006204673317166007, -0.08308094090126379, 0.12889449238540765, -0.11534022237649377, -0.13973693853738356, 0.06747725052041553, 0.39472149662217315, -0.2868450781596558, -0.273694367176492, 0.10928866951441278, -0.22430191154838824, -0.1387588316194561, 0.2325489281496147, -0.09663611036554283... |
708.2021 | Who is the best connected EC researcher? Centrality analysis of the
complex network of authors in evolutionary computation | Co-authorship graphs (that is, the graph of authors linked by co-authorship
of papers) are complex networks, which expresses the dynamics of a complex
system. Only recently its study has started to draw interest from the EC
community, the first paper dealing with it having been published two years ago.
In this paper ... | cs.CY cs.NE | coauthorship graphs that is the graph of authors linked by coauthorship of papers are complex networks which expresses the dynamics of a complex system only recently its study has started to draw interest from the ec community the first paper dealing with it having been published two years ago in this paper we will stu... | [['coauthorship', 'graphs', 'that', 'is', 'the', 'graph', 'of', 'authors', 'linked', 'by', 'coauthorship', 'of', 'papers', 'are', 'complex', 'networks', 'which', 'expresses', 'the', 'dynamics', 'of', 'a', 'complex', 'system', 'only', 'recently', 'its', 'study', 'has', 'started', 'to', 'draw', 'interest', 'from', 'the',... | [-0.11453061788404628, 0.030274199870429144, -0.09356335190364695, 0.07365872111580701, -0.07781805963057911, -0.08510888333319488, 0.049553026383474585, 0.38351483236659656, -0.22717026335797555, -0.31152251861622615, 0.07642624134049666, -0.30234048835876765, -0.229979266454889, 0.17428665697066623, -0.06767073644864... |
708.2022 | p-adic Monodromy of the Universal Deformation of a HW-cyclic
Barsotti-Tate Group | Let k be an algebraically closed field of characteristic $p>0$, and $G_0$ be
a Barsotti-Tate group (or $p$-divisible group) over k. We denote by $S$ the
"algebraic" local moduli in characteristic p of $G_0$, by $G$ the universal
deformation of $G_0$ over $S$, and by $U\subset S$ the ordinary locus of $G$.
The etale p... | math.AG | let k be an algebraically closed field of characteristic p0 and g_0 be a barsottitate group or pdivisible group over k we denote by s the algebraic local moduli in characteristic p of g_0 by g the universal deformation of g_0 over s and by usubset s the ordinary locus of g the etale part of g over u gives rise to a mon... | [['let', 'k', 'be', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'p0', 'and', 'g_0', 'be', 'a', 'barsottitate', 'group', 'or', 'pdivisible', 'group', 'over', 'k', 'we', 'denote', 'by', 's', 'the', 'algebraic', 'local', 'moduli', 'in', 'characteristic', 'p', 'of', 'g_0', 'by', 'g', 'the', 'universal... | [-0.26929173650099864, 0.1160237930252474, -0.12327510460407563, -0.04658085533470336, -0.09255426654577135, -0.1493627294229584, 0.015148940259560702, 0.32709798849217836, -0.3517724200181903, -0.20844939438581106, 0.015517673449545738, -0.23197186130264233, -0.11873468639697099, 0.2224566456805464, -0.125167563985732... |
708.2023 | Nonantagonistic noisy duels of discrete type with an arbitrary number of
actions | We study a nonzero-sum game of two players which is a generalization of the
antagonistic noisy duel of discrete type. The game is considered from the point
of view of various criterions of optimality. We prove existence of
epsilon-equilibrium situations and show that the epsilon-equilibrium strategies
that we have fo... | math.OC cs.GT math.PR | we study a nonzerosum game of two players which is a generalization of the antagonistic noisy duel of discrete type the game is considered from the point of view of various criterions of optimality we prove existence of epsilonequilibrium situations and show that the epsilonequilibrium strategies that we have found are... | [['we', 'study', 'a', 'nonzerosum', 'game', 'of', 'two', 'players', 'which', 'is', 'a', 'generalization', 'of', 'the', 'antagonistic', 'noisy', 'duel', 'of', 'discrete', 'type', 'the', 'game', 'is', 'considered', 'from', 'the', 'point', 'of', 'view', 'of', 'various', 'criterions', 'of', 'optimality', 'we', 'prove', 'ex... | [-0.15346845331307696, 0.015755264915672963, -0.17403362718974486, 0.10250570539593402, -0.0320905703089298, -0.20418084889503293, 0.10945126046671678, 0.380495463963598, -0.2820581984951308, -0.2542221447648971, 0.13529939967281135, -0.2428372281750566, -0.21890672989875862, 0.08799803486142896, -0.1341515824100689, 0... |
708.2024 | Commentary on: "Unconventional elasticity in smectic-A elastomers" by O.
Stenull and T.C. Lubensky | The reorientation behaviour of a smectic-A (SmA) elastomer deformed parallel
to the smectic layer normal has been interpreted as a Sm-C like transition by
Stenull and Lubensky. Experiments, however, prove that such a transition does
not occur.
| cond-mat.soft cond-mat.mtrl-sci | the reorientation behaviour of a smectica sma elastomer deformed parallel to the smectic layer normal has been interpreted as a smc like transition by stenull and lubensky experiments however prove that such a transition does not occur | [['the', 'reorientation', 'behaviour', 'of', 'a', 'smectica', 'sma', 'elastomer', 'deformed', 'parallel', 'to', 'the', 'smectic', 'layer', 'normal', 'has', 'been', 'interpreted', 'as', 'a', 'smc', 'like', 'transition', 'by', 'stenull', 'and', 'lubensky', 'experiments', 'however', 'prove', 'that', 'such', 'a', 'transiti... | [-0.1382914975889631, 0.1995988785465424, -0.10846472418288121, -0.01075335272361298, -0.11212508909001544, -0.1580068430661954, 0.020056002546806593, 0.4118967010966829, -0.2405785841212885, -0.24214294358357988, 0.11091681126807187, -0.24403854446309442, -0.18253175758228107, 0.07763953466673156, -0.01113405577976860... |
708.2025 | Effects of selective dilution on the magnetic properties of
La_{0.7}Sr_{0.3}Mn_{1-x}M'_xO_3 (M' = Al, Ti) | The magnetic lattice of mixed-valence Mn ions in
La$_{0.7}$Sr$_{0.3}$MnO$_{3}$ is selectively diluted by partial substitution of
Al or Ti for Mn. The ferromagnetic transition temperature $T_\mathrm{c}$ and
the saturation magnetization $M_\mathrm{s}$ both decrease with substitution. By
presenting the data in terms of ... | cond-mat.mtrl-sci cond-mat.str-el | the magnetic lattice of mixedvalence mn ions in la_07sr_03mno_3 is selectively diluted by partial substitution of al or ti for mn the ferromagnetic transition temperature t_mathrmc and the saturation magnetization m_mathrms both decrease with substitution by presenting the data in terms of selective dilution t_mathrmc ... | [['the', 'magnetic', 'lattice', 'of', 'mixedvalence', 'mn', 'ions', 'in', 'la_07sr_03mno_3', 'is', 'selectively', 'diluted', 'by', 'partial', 'substitution', 'of', 'al', 'or', 'ti', 'for', 'mn', 'the', 'ferromagnetic', 'transition', 'temperature', 't_mathrmc', 'and', 'the', 'saturation', 'magnetization', 'm_mathrms', '... | [-0.10986838803716725, 0.21368782842276438, 0.06319939853358758, 0.009534511238246435, 0.0046510435528151935, -0.17361108849065437, 0.1092289290569287, 0.36064280195522214, -0.27578227778506137, -0.3070615638195792, 0.013565515734127632, -0.38086850141295264, -0.06931449714935414, 0.13092678915821918, 0.024432226209741... |
708.2026 | Derivative of BICM Mutual Information | In this letter we determine the derivative of the mutual information
corresponding to bit-interleaved coded modulation systems. The derivative
follows as a linear combination of minimum-mean-squared error functions of
coded modulation sets. The result finds applications to the analysis of
communications systems in th... | cs.IT math.IT | in this letter we determine the derivative of the mutual information corresponding to bitinterleaved coded modulation systems the derivative follows as a linear combination of minimummeansquared error functions of coded modulation sets the result finds applications to the analysis of communications systems in the wideb... | [['in', 'this', 'letter', 'we', 'determine', 'the', 'derivative', 'of', 'the', 'mutual', 'information', 'corresponding', 'to', 'bitinterleaved', 'coded', 'modulation', 'systems', 'the', 'derivative', 'follows', 'as', 'a', 'linear', 'combination', 'of', 'minimummeansquared', 'error', 'functions', 'of', 'coded', 'modulat... | [-0.28350013121221723, -0.01422556070822545, -0.05050312463109466, 0.015138559210622175, -0.04373501782220873, -0.1280081436630677, 0.09678334414281628, 0.3437228030779145, -0.34074423956600103, -0.2550018417648971, 0.12884836204095998, -0.2534169287166812, -0.2075009844011881, 0.21688209927894853, -0.11596076564693993... |
708.2027 | Optical Birefringence and Domain Structure of the as-grown
Rb2xTl2(1-x)Cd2(SO4)3 Solid Solutions at Phase Transitions | It is shown that the as-grown solid solutions Tl2xRb2(1-x)Cd2(SO4)3 possess a
residual optical birefringence in the cubic phase at room temperature. The
existence of both the residual birefringence and the residual domain structure
in the compound with x=0.8 at the room temperature, along with the domain walls
orient... | cond-mat.other | it is shown that the asgrown solid solutions tl2xrb21xcd2so43 possess a residual optical birefringence in the cubic phase at room temperature the existence of both the residual birefringence and the residual domain structure in the compound with x08 at the room temperature along with the domain walls orientation and th... | [['it', 'is', 'shown', 'that', 'the', 'asgrown', 'solid', 'solutions', 'tl2xrb21xcd2so43', 'possess', 'a', 'residual', 'optical', 'birefringence', 'in', 'the', 'cubic', 'phase', 'at', 'room', 'temperature', 'the', 'existence', 'of', 'both', 'the', 'residual', 'birefringence', 'and', 'the', 'residual', 'domain', 'struct... | [-0.1361728449647665, 0.19416265236213803, -0.05618401102933055, -0.0572911405709658, -0.040434675727118834, -0.0655485246138951, 0.07739745881672658, 0.4270121593503876, -0.2742734908502787, -0.2847750889969633, 0.12261494479706868, -0.31145705142659497, -0.0878874400353178, 0.13808745319512508, 0.04883180809015712, -... |
708.2028 | Studies of Optical Damage in Photorefractive Single LiNbO3 Crystals
using Imaging Polarimetry | The optical damage of photorefractive material, single LiNbO3 crystal, is
experimentally studied. The specimen has been illuminated with the radiation of
continuous Ar-laser (the wavelength of 488 nm) focused to 35?m spot. The
induced birefringence map is obtained by means of imaging polarimeter.
Promising resources ... | physics.gen-ph physics.optics | the optical damage of photorefractive material single linbo3 crystal is experimentally studied the specimen has been illuminated with the radiation of continuous arlaser the wavelength of 488 nm focused to 35m spot the induced birefringence map is obtained by means of imaging polarimeter promising resources of the expe... | [['the', 'optical', 'damage', 'of', 'photorefractive', 'material', 'single', 'linbo3', 'crystal', 'is', 'experimentally', 'studied', 'the', 'specimen', 'has', 'been', 'illuminated', 'with', 'the', 'radiation', 'of', 'continuous', 'arlaser', 'the', 'wavelength', 'of', '488', 'nm', 'focused', 'to', '35m', 'spot', 'the', ... | [-0.10222385277851126, 0.18073065810951225, -0.036817412945981086, -0.09091997659957167, -0.07231980325294692, -0.17386674207814953, -0.02729515799958455, 0.5261131499550844, -0.24676623744399925, -0.2872691888100745, 0.060195652512719106, -0.31364452159195616, -0.10324255935847759, 0.2680064473431884, -0.0286909265263... |
708.2029 | Curvature flows on four manifolds with boundary | Given a compact four dimensional smooth Riemannian manifold $(M,g)$ with
smooth boundary, we consider the evolution equation by $Q$-curvature in the
interior keeping the $T$-curvature and the mean curvature to be zero and the
evolution equation by $T$-curvature at the boundary with the condition that the
$Q$-curvatur... | math.AP math.DG | given a compact four dimensional smooth riemannian manifold mg with smooth boundary we consider the evolution equation by qcurvature in the interior keeping the tcurvature and the mean curvature to be zero and the evolution equation by tcurvature at the boundary with the condition that the qcurvature and the mean curva... | [['given', 'a', 'compact', 'four', 'dimensional', 'smooth', 'riemannian', 'manifold', 'mg', 'with', 'smooth', 'boundary', 'we', 'consider', 'the', 'evolution', 'equation', 'by', 'qcurvature', 'in', 'the', 'interior', 'keeping', 'the', 'tcurvature', 'and', 'the', 'mean', 'curvature', 'to', 'be', 'zero', 'and', 'the', 'e... | [-0.20899895820766687, 0.05416323205281515, -0.08037398703745566, 0.03914302862249315, -0.09955998559016735, -0.17508079490507952, -0.10566300253849477, 0.33212942408863455, -0.26208172985352574, -0.2119630101369694, 0.15205394108052134, -0.29077613572590055, -0.10931555106653831, 0.08674686177982949, -0.11594756195554... |
708.203 | Constraints on non-thermal Dark Matter from Planck lensing extraction | Distortions of CMB temperature and polarization anisotropy maps caused by
gravitational lensing, observable with high angular resolution and sensitivity,
can be used to constrain the sterile neutrino mass, offering several advantages
against the analysis based on the combination of CMB, LSS and Ly\alpha forest
power ... | astro-ph | distortions of cmb temperature and polarization anisotropy maps caused by gravitational lensing observable with high angular resolution and sensitivity can be used to constrain the sterile neutrino mass offering several advantages against the analysis based on the combination of cmb lss and lyalpha forest power spectra... | [['distortions', 'of', 'cmb', 'temperature', 'and', 'polarization', 'anisotropy', 'maps', 'caused', 'by', 'gravitational', 'lensing', 'observable', 'with', 'high', 'angular', 'resolution', 'and', 'sensitivity', 'can', 'be', 'used', 'to', 'constrain', 'the', 'sterile', 'neutrino', 'mass', 'offering', 'several', 'advanta... | [-0.07917450348705184, 0.14857580292054012, -0.05810135486150884, 0.16727520267994814, -0.10201118840866776, -0.094243102402942, 0.006820695177451823, 0.3206749032722971, -0.20450888238924225, -0.3423266248846781, 0.02334174531471554, -0.33543412127601335, -0.0009046919366791228, 0.22351291679684843, 0.0645158890988831... |
708.2031 | "Dark galaxies" and local very metal-poor gas-rich galaxies: possible
interrelations | There are only a few ``dark galaxy'' candidates discovered to date in the
local Universe. One of the most prominent of them is the SW component of a
merging system HI 1225+01. On the other hand, the number of known very
metal-poor gas-rich dwarfs similar to IZw18 and SBS 0335-052 E,W has grown
drastically during the ... | astro-ph | there are only a few dark galaxy candidates discovered to date in the local universe one of the most prominent of them is the sw component of a merging system hi 122501 on the other hand the number of known very metalpoor gasrich dwarfs similar to izw18 and sbs 0335052 ew has grown drastically during the last decade fr... | [['there', 'are', 'only', 'a', 'few', 'dark', 'galaxy', 'candidates', 'discovered', 'to', 'date', 'in', 'the', 'local', 'universe', 'one', 'of', 'the', 'most', 'prominent', 'of', 'them', 'is', 'the', 'sw', 'component', 'of', 'a', 'merging', 'system', 'hi', '122501', 'on', 'the', 'other', 'hand', 'the', 'number', 'of', ... | [-0.09468841497981094, 0.1047200970003538, -0.08848953912405637, 0.11486903842643043, -0.09537629453817853, -0.06086303673251576, 0.03876049617940786, 0.3969875890935693, -0.15201907551621097, -0.34468570119640396, 0.0776709658017591, -0.3171888957649826, -0.06839054565176055, 0.20272397540322565, 0.0013326524003957198... |
708.2032 | Influence of magnetic field offsets on the resistance of magnetic
barriers in two-dimensional electron gases | Magnetic barriers in two-dimensional electron gases are shifted in B space by
homogeneous, perpendicular magnetic fields. The magnetoresistance across the
barrier shows a characteristic asymmetric dip in the regime where the polarity
of the homogeneous magnetic field is opposite to that one of the magnetic
barrier. T... | cond-mat.mes-hall | magnetic barriers in twodimensional electron gases are shifted in b space by homogeneous perpendicular magnetic fields the magnetoresistance across the barrier shows a characteristic asymmetric dip in the regime where the polarity of the homogeneous magnetic field is opposite to that one of the magnetic barrier the mea... | [['magnetic', 'barriers', 'in', 'twodimensional', 'electron', 'gases', 'are', 'shifted', 'in', 'b', 'space', 'by', 'homogeneous', 'perpendicular', 'magnetic', 'fields', 'the', 'magnetoresistance', 'across', 'the', 'barrier', 'shows', 'a', 'characteristic', 'asymmetric', 'dip', 'in', 'the', 'regime', 'where', 'the', 'po... | [-0.20424580942076373, 0.19892848478293562, -0.040236324515103936, -0.006888233359443046, -0.017291315275816673, -0.12263380662055619, 0.000379867644150214, 0.3756704426269574, -0.30933225424174804, -0.29309172211327106, -0.0408749625126057, -0.2939557084275118, -0.10525110687117979, 0.20973408217710185, 0.061124845806... |
708.2033 | Ground-state triply and doubly heavy baryons in a relativistic
three-quark model | Mass spectra of the ground-state baryons consisting of three or two heavy (b
or c) and one light (u,d,s) quarks are calculated in the framework of the
relativistic quark model and the hyperspherical expansion. The predictions of
masses of the triply and doubly heavy baryons are obtained by employing the
perturbation ... | hep-ph | mass spectra of the groundstate baryons consisting of three or two heavy b or c and one light uds quarks are calculated in the framework of the relativistic quark model and the hyperspherical expansion the predictions of masses of the triply and doubly heavy baryons are obtained by employing the perturbation theory for... | [['mass', 'spectra', 'of', 'the', 'groundstate', 'baryons', 'consisting', 'of', 'three', 'or', 'two', 'heavy', 'b', 'or', 'c', 'and', 'one', 'light', 'uds', 'quarks', 'are', 'calculated', 'in', 'the', 'framework', 'of', 'the', 'relativistic', 'quark', 'model', 'and', 'the', 'hyperspherical', 'expansion', 'the', 'predic... | [-0.09477740460105481, 0.2511958046891396, -0.051330077822410294, 0.1037812812494174, 0.04557414283044636, -0.10840731728521566, 0.03443213303445748, 0.3010086116771544, -0.18029046431183815, -0.29048473303837163, -0.052597495451224066, -0.36743406500787507, 0.03860151109796378, 0.08111723216866414, 0.15961391220410023... |
708.2034 | Alignment and Precession of a Black Hole with a Warped Accretion Disc | We consider the shape of an accretion disc whose outer regions are misaligned
with the spin axis of a central black hole and calculate the steady state form
of the warped disc in the case where the viscosity and surface densities are
power laws in the distance from the central black hole. We discuss the shape of
the ... | astro-ph | we consider the shape of an accretion disc whose outer regions are misaligned with the spin axis of a central black hole and calculate the steady state form of the warped disc in the case where the viscosity and surface densities are power laws in the distance from the central black hole we discuss the shape of the res... | [['we', 'consider', 'the', 'shape', 'of', 'an', 'accretion', 'disc', 'whose', 'outer', 'regions', 'are', 'misaligned', 'with', 'the', 'spin', 'axis', 'of', 'a', 'central', 'black', 'hole', 'and', 'calculate', 'the', 'steady', 'state', 'form', 'of', 'the', 'warped', 'disc', 'in', 'the', 'case', 'where', 'the', 'viscosit... | [-0.14499727216213845, 0.11096315420363304, -0.09365197516817339, 0.07814091198216314, -0.06310999336763444, -0.05284771778128578, -0.008211940708521928, 0.3500082413521185, -0.23318922618606702, -0.27943758359371923, 0.11001797952300778, -0.23681999219899968, -0.06317251145723879, 0.20300185845904245, -0.0732314703754... |
708.2035 | Acoustooptic Diffraction in Borate Crystals | The efficiency of acoustooptic (AO) diffraction in a-BaB2O4 and Li2B4O7
crystals is studied experimentally. The crystals are shown to be quite good AO
materials. The efficiency of AO diffraction in a-BaB2O4 reaches h=30% at the
electric signal power of P=0.7W for the transverse acoustic wave and 15% at the
power of P... | physics.gen-ph physics.optics | the efficiency of acoustooptic ao diffraction in abab2o4 and li2b4o7 crystals is studied experimentally the crystals are shown to be quite good ao materials the efficiency of ao diffraction in abab2o4 reaches h30 at the electric signal power of p07w for the transverse acoustic wave and 15 at the power of p056w for the ... | [['the', 'efficiency', 'of', 'acoustooptic', 'ao', 'diffraction', 'in', 'abab2o4', 'and', 'li2b4o7', 'crystals', 'is', 'studied', 'experimentally', 'the', 'crystals', 'are', 'shown', 'to', 'be', 'quite', 'good', 'ao', 'materials', 'the', 'efficiency', 'of', 'ao', 'diffraction', 'in', 'abab2o4', 'reaches', 'h30', 'at', ... | [-0.12713758741111422, 0.1895509052161987, -0.020123131336787572, -0.0007520550629124045, -0.046964468950262434, -0.07951580420709574, -0.0023387390475433606, 0.3978389866076983, -0.242547739812961, -0.2748493295449477, 0.08004183106554243, -0.34235557744709344, -0.05721809915625132, 0.2974147523251864, 0.0323827467858... |
708.2036 | Pfaffian Expressions for Random Matrix Correlation Functions | It is well known that Pfaffian formulas for eigenvalue correlations are
useful in the analysis of real and quaternion random matrices. Moreover the
parametric correlations in the crossover to complex random matrices are
evaluated in the forms of Pfaffians. In this article, we review the
formulations and applications ... | math-ph math.MP | it is well known that pfaffian formulas for eigenvalue correlations are useful in the analysis of real and quaternion random matrices moreover the parametric correlations in the crossover to complex random matrices are evaluated in the forms of pfaffians in this article we review the formulations and applications of pf... | [['it', 'is', 'well', 'known', 'that', 'pfaffian', 'formulas', 'for', 'eigenvalue', 'correlations', 'are', 'useful', 'in', 'the', 'analysis', 'of', 'real', 'and', 'quaternion', 'random', 'matrices', 'moreover', 'the', 'parametric', 'correlations', 'in', 'the', 'crossover', 'to', 'complex', 'random', 'matrices', 'are', ... | [-0.11346922393708506, 0.08977175157582551, -0.05116589845509448, 0.14009797073627023, -0.07299834273739211, -0.12075678171720683, -0.010075455113812432, 0.3502680025831388, -0.2489744579754443, -0.21393954319258532, 0.11410970098171547, -0.2612715548459898, -0.28576610995489254, 0.19440614394516798, -0.039009108357340... |
708.2037 | Non--Localizability of Electric Coupling and Gravitational Binding of
Charged Objects | The energy--momentum tensor in general relativity contains only localized
contributions to the total energy--momentum. Here, we consider a static,
spherically symmetric object consisting of a charged perfect fluid. For this
object, the total gravitational mass contains a non--localizable contribution
of electric coup... | gr-qc | the energymomentum tensor in general relativity contains only localized contributions to the total energymomentum here we consider a static spherically symmetric object consisting of a charged perfect fluid for this object the total gravitational mass contains a nonlocalizable contribution of electric coupling ordinari... | [['the', 'energymomentum', 'tensor', 'in', 'general', 'relativity', 'contains', 'only', 'localized', 'contributions', 'to', 'the', 'total', 'energymomentum', 'here', 'we', 'consider', 'a', 'static', 'spherically', 'symmetric', 'object', 'consisting', 'of', 'a', 'charged', 'perfect', 'fluid', 'for', 'this', 'object', 't... | [-0.20779098107122146, 0.16976602925112888, -0.037959949757773864, 0.06183002604615637, -0.10453491970940038, -0.10042968169829353, -0.041277365304183126, 0.2867993169767392, -0.135547008546784, -0.3243246020662577, -0.022419087623982408, -0.25437263076107, -0.07977110997308046, 0.11350209448150857, -0.0056109144189936... |
708.2038 | Genome landscapes and bacteriophage codon usage | Across all kingdoms of biological life, protein-coding genes exhibit unequal
usage of synonmous codons. Although alternative theories abound, translational
selection has been accepted as an important mechanism that shapes the patterns
of codon usage in prokaryotes and simple eukaryotes. Here we analyze patterns
of co... | q-bio.GN | across all kingdoms of biological life proteincoding genes exhibit unequal usage of synonmous codons although alternative theories abound translational selection has been accepted as an important mechanism that shapes the patterns of codon usage in prokaryotes and simple eukaryotes here we analyze patterns of codon usa... | [['across', 'all', 'kingdoms', 'of', 'biological', 'life', 'proteincoding', 'genes', 'exhibit', 'unequal', 'usage', 'of', 'synonmous', 'codons', 'although', 'alternative', 'theories', 'abound', 'translational', 'selection', 'has', 'been', 'accepted', 'as', 'an', 'important', 'mechanism', 'that', 'shapes', 'the', 'patte... | [-0.11269863590987472, 0.15388262695259622, -0.03405623115588632, 0.1023390244818845, -0.05765273409637775, -0.16611049975936779, 0.13631413485539162, 0.4154785937592808, -0.24140841327870718, -0.28836045585741094, -0.009999178380884315, -0.23281387933187903, -0.22880103892257364, 0.14274169449262994, -0.09592866256670... |
708.2039 | A survey of the Wolf-Rayet population of the barred, spiral galaxy NGC
1313 | We present a VLT/FORS1 survey of Wolf-Rayet (WR) stars in the spiral galaxy
NGC 1313. In total, 94 WR candidate sources have been identified from
narrow-band imaging. Of these, 82 have been spectroscopically observed, for
which WR emission features are confirmed in 70 cases, one of which also
exhibits strong nebular ... | astro-ph | we present a vltfors1 survey of wolfrayet wr stars in the spiral galaxy ngc 1313 in total 94 wr candidate sources have been identified from narrowband imaging of these 82 have been spectroscopically observed for which wr emission features are confirmed in 70 cases one of which also exhibits strong nebular heii 4686 emi... | [['we', 'present', 'a', 'vltfors1', 'survey', 'of', 'wolfrayet', 'wr', 'stars', 'in', 'the', 'spiral', 'galaxy', 'ngc', '1313', 'in', 'total', '94', 'wr', 'candidate', 'sources', 'have', 'been', 'identified', 'from', 'narrowband', 'imaging', 'of', 'these', '82', 'have', 'been', 'spectroscopically', 'observed', 'for', '... | [-0.024731798882601738, 0.008423124597452225, -0.037395253225362725, 0.09449952710530765, -0.10823949260991954, -0.10074467666092374, 0.11180636602830851, 0.47264857695526663, -0.04683486889532235, -0.3342316455252114, -0.0036437299884190515, -0.3404984706480588, 0.0058536652253852, 0.17968804242555053, -0.051567549733... |
708.204 | Radiation Pressure Acceleration of Thin Foils with Circularly Polarized
Laser Pulses | A new regime is described for Radiation Pressure Acceleration of a thin foil
by an intense laser beam of above 10^20 W/cm^2. Highly monoenergetic proton
beams extending to GeV energies can be produced with very high efficiency using
circularly polarized light. The proton beams have a very small divergence angle
(less... | physics.plasm-ph | a new regime is described for radiation pressure acceleration of a thin foil by an intense laser beam of above 1020 wcm2 highly monoenergetic proton beams extending to gev energies can be produced with very high efficiency using circularly polarized light the proton beams have a very small divergence angle less than 4 ... | [['a', 'new', 'regime', 'is', 'described', 'for', 'radiation', 'pressure', 'acceleration', 'of', 'a', 'thin', 'foil', 'by', 'an', 'intense', 'laser', 'beam', 'of', 'above', '1020', 'wcm2', 'highly', 'monoenergetic', 'proton', 'beams', 'extending', 'to', 'gev', 'energies', 'can', 'be', 'produced', 'with', 'very', 'high'... | [-0.05295079188820507, 0.35148825644968645, -0.06158947992537703, 0.0961431502564145, -0.020527680843536344, -0.18214268956549598, -0.03398109723181863, 0.4901128941880805, -0.21167491198783475, -0.3445863371182765, -0.0618850107986613, -0.27892196035099914, 0.11795846571081452, 0.29276897200616075, 0.02004880572536162... |
708.2041 | Topological Andr\'e-Quillen homology for cellular commutative
$S$-algebras | Topological Andr\'e-Quillen homology for commutative $S$-algebras was
introduced by Basterra following work of Kriz, and has been intensively studied
by several authors. In this paper we discuss it as a homology theory on CW
$S$-algebras and apply it to obtain results on minimal atomic $p$-local
$S$-algebras which ge... | math.AT math.KT | topological andrequillen homology for commutative salgebras was introduced by basterra following work of kriz and has been intensively studied by several authors in this paper we discuss it as a homology theory on cw salgebras and apply it to obtain results on minimal atomic plocal salgebras which generalise those of b... | [['topological', 'andrequillen', 'homology', 'for', 'commutative', 'salgebras', 'was', 'introduced', 'by', 'basterra', 'following', 'work', 'of', 'kriz', 'and', 'has', 'been', 'intensively', 'studied', 'by', 'several', 'authors', 'in', 'this', 'paper', 'we', 'discuss', 'it', 'as', 'a', 'homology', 'theory', 'on', 'cw',... | [-0.10837205615141154, 0.09289140707594068, -0.08631083074792781, 0.11574701892780415, -0.07909905605072923, -0.154921882053125, -0.015682285600204897, 0.37506231768330667, -0.2693882086793618, -0.26043086466790344, 0.11554495492943234, -0.20866058953106403, -0.2138837163665277, 0.24008226278237998, -0.1995600486475536... |
708.2042 | The empirical metallicity dependence of the mass-loss rate of O- and
early B-type stars | [Abridged] We present a comprehensive study of the metallicity dependence of
the mass-loss rates in stationary stellar winds of hot massive stars. Assuming
a power-law dependence of mass loss on metallicity, Mdot \propto Z^{m}, and
adopting a theoretical relation between the terminal velocity and metallicity,
v_inf \... | astro-ph | abridged we present a comprehensive study of the metallicity dependence of the massloss rates in stationary stellar winds of hot massive stars assuming a powerlaw dependence of mass loss on metallicity mdot propto zm and adopting a theoretical relation between the terminal velocity and metallicity v_inf propto z013 lei... | [['abridged', 'we', 'present', 'a', 'comprehensive', 'study', 'of', 'the', 'metallicity', 'dependence', 'of', 'the', 'massloss', 'rates', 'in', 'stationary', 'stellar', 'winds', 'of', 'hot', 'massive', 'stars', 'assuming', 'a', 'powerlaw', 'dependence', 'of', 'mass', 'loss', 'on', 'metallicity', 'mdot', 'propto', 'zm',... | [-0.05102744028120837, 0.13680904398906352, -0.05243486474624815, 0.1425886391642246, -0.08119689192266223, -0.06064479006850656, 0.07887543118905593, 0.4234965337083695, -0.12830595413490417, -0.3681300786343661, 0.015060317198290154, -0.30110288123263323, 0.015378722105611194, 0.23174983766100227, -0.0775908988434821... |
708.2043 | The hamiltonian study of supersymmetric Yang-Mills quantum mechanics | The hamiltonian formulation of Supersymmetric Yang-Mills quantum mechanics
(SYMQM) is discussed. We focus on the Fock space formulation of the models
since it is convenient for the numerical analysis, however some novel
analytical results are also pointed out.
| hep-th | the hamiltonian formulation of supersymmetric yangmills quantum mechanics symqm is discussed we focus on the fock space formulation of the models since it is convenient for the numerical analysis however some novel analytical results are also pointed out | [['the', 'hamiltonian', 'formulation', 'of', 'supersymmetric', 'yangmills', 'quantum', 'mechanics', 'symqm', 'is', 'discussed', 'we', 'focus', 'on', 'the', 'fock', 'space', 'formulation', 'of', 'the', 'models', 'since', 'it', 'is', 'convenient', 'for', 'the', 'numerical', 'analysis', 'however', 'some', 'novel', 'analyt... | [-0.07911117458225865, 0.11547169803739771, -0.12128025210021358, 0.11551040987557683, -0.07250047230014675, -0.1628878974404774, -0.018406154005788267, 0.36208633259919126, -0.16342492048677645, -0.21074625891388246, 0.10772753092092707, -0.24776943513241254, -0.25777194433306394, 0.22854886346153522, -0.0538146916507... |
708.2044 | Density-Profile Processes Describing Biological Signaling Networks:
Almost Sure Convergence to Deterministic Trajectories | We introduce jump processes in R^k, called density-profile process, to model
biological signaling networks. They describe the macroscopic evolution of
finite-size spin-flip models with k types of spins interacting through a
non-reversible Glauber dynamics. We focus on the the k-dimensional
empirical-magnetization vec... | math.PR | we introduce jump processes in rk called densityprofile process to model biological signaling networks they describe the macroscopic evolution of finitesize spinflip models with k types of spins interacting through a nonreversible glauber dynamics we focus on the the kdimensional empiricalmagnetization vector in the th... | [['we', 'introduce', 'jump', 'processes', 'in', 'rk', 'called', 'densityprofile', 'process', 'to', 'model', 'biological', 'signaling', 'networks', 'they', 'describe', 'the', 'macroscopic', 'evolution', 'of', 'finitesize', 'spinflip', 'models', 'with', 'k', 'types', 'of', 'spins', 'interacting', 'through', 'a', 'nonreve... | [-0.17456294239292408, 0.17621727520912486, -0.09853577431316343, 0.05849838223753526, -0.03749785515879775, -0.18116434840266687, 0.09112986298934275, 0.3476208046003676, -0.31551424547679874, -0.185244741487073, 0.06965212732664428, -0.2769560142726506, -0.15331130067430337, 0.13808014012104364, -0.012247714678125594... |
708.2045 | Sustainability of multi-field inflation and bound on string scale | We study the effects of the interaction terms between the inflaton fields on
the inflationary dynamics in multi-field models. With power law type potential
and interactions, the total number of e-folds may get considerably reduced and
can lead to unacceptably short period of inflation. Also we point out that this
can... | hep-th astro-ph hep-ph | we study the effects of the interaction terms between the inflaton fields on the inflationary dynamics in multifield models with power law type potential and interactions the total number of efolds may get considerably reduced and can lead to unacceptably short period of inflation also we point out that this can place ... | [['we', 'study', 'the', 'effects', 'of', 'the', 'interaction', 'terms', 'between', 'the', 'inflaton', 'fields', 'on', 'the', 'inflationary', 'dynamics', 'in', 'multifield', 'models', 'with', 'power', 'law', 'type', 'potential', 'and', 'interactions', 'the', 'total', 'number', 'of', 'efolds', 'may', 'get', 'considerably... | [-0.1452795121163785, 0.211589582284892, -0.14415771727626733, 0.16712860822431988, -0.06182122939767746, -0.13242083593210266, 0.019848969580789844, 0.2544001259400949, -0.27105305364334975, -0.33255412806193907, 0.07015197775147569, -0.21033265112111202, -0.16933948175654143, 0.19081191999510258, -0.03988380754970341... |
708.2046 | Quelques courbes de Hecke se plongent dans l'espace de Colmez | Let p be a prime, C the p-adic Eigencurve (with tame level 1) and Z the
blow-up of the Fredholm hypersurface of the U_p - operator at the special
points. We show that for p = 2, 3, 5 and 7, the natural map C -> Z is a
rigid-analytic isomorphism.
| math.NT | let p be a prime c the padic eigencurve with tame level 1 and z the blowup of the fredholm hypersurface of the u_p operator at the special points we show that for p 2 3 5 and 7 the natural map c z is a rigidanalytic isomorphism | [['let', 'p', 'be', 'a', 'prime', 'c', 'the', 'padic', 'eigencurve', 'with', 'tame', 'level', '1', 'and', 'z', 'the', 'blowup', 'of', 'the', 'fredholm', 'hypersurface', 'of', 'the', 'u_p', 'operator', 'at', 'the', 'special', 'points', 'we', 'show', 'that', 'for', 'p', '2', '3', '5', 'and', '7', 'the', 'natural', 'map',... | [-0.19803678795384863, 0.07334267858338232, -0.09129159661824815, 0.07433754334973249, -0.009267114956552783, -0.22242436230105037, 0.0005282954468081394, 0.26979690433169407, -0.34980171103961766, -0.21613178557405868, 0.060118731179197006, -0.2946329970970207, -0.0706342371898548, 0.15140730736311525, -0.039914371174... |
708.2047 | Inflating branes inside topological defects and periodic structures | We study brane world models which contain local topological defects in the
bulk and a (3+1)-dimensional inflating brane. We put the emphasis on new types
of solutions that are periodic in the bulk radial coordinate and thus provide
examples of "naturally compactified" brane worlds.
| gr-qc | we study brane world models which contain local topological defects in the bulk and a 31dimensional inflating brane we put the emphasis on new types of solutions that are periodic in the bulk radial coordinate and thus provide examples of naturally compactified brane worlds | [['we', 'study', 'brane', 'world', 'models', 'which', 'contain', 'local', 'topological', 'defects', 'in', 'the', 'bulk', 'and', 'a', '31dimensional', 'inflating', 'brane', 'we', 'put', 'the', 'emphasis', 'on', 'new', 'types', 'of', 'solutions', 'that', 'are', 'periodic', 'in', 'the', 'bulk', 'radial', 'coordinate', 'an... | [-0.1473324873738668, 0.13616153472949835, -0.09188714204356074, 0.09857334273824976, -0.1260142810219391, -0.1546733546896245, -0.02014642428416251, 0.29640098818874155, -0.15737038603137163, -0.23814410117285495, 0.11592229780878617, -0.2772194901481271, -0.1335137059425258, 0.1511249866082587, -0.08767858560366387, ... |
708.2048 | Focus Point SUSY at the LHC Revisited | The estimation of the backgrounds for gluino signals in focus point
supersymmetry is extended by including the backgrounds from the production of
four third generation quarks in the analysis. We find that these backgrounds
are negligible if one uses the strong selection criteria proposed in the
literature (including ... | hep-ph hep-ex | the estimation of the backgrounds for gluino signals in focus point supersymmetry is extended by including the backgrounds from the production of four third generation quarks in the analysis we find that these backgrounds are negligible if one uses the strong selection criteria proposed in the literature including this... | [['the', 'estimation', 'of', 'the', 'backgrounds', 'for', 'gluino', 'signals', 'in', 'focus', 'point', 'supersymmetry', 'is', 'extended', 'by', 'including', 'the', 'backgrounds', 'from', 'the', 'production', 'of', 'four', 'third', 'generation', 'quarks', 'in', 'the', 'analysis', 'we', 'find', 'that', 'these', 'backgrou... | [-0.03993070660647109, 0.16996772721154807, -0.06308650306950744, 0.15373624486347595, -0.04710315239289539, -0.11227252306700282, 0.019693282933380966, 0.37954063557542217, -0.18030582270041334, -0.34241281730137046, 0.09207127290260197, -0.3017343531272889, 0.010061541914958791, 0.19698355476806875, 0.015071015887737... |
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