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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706.3114 | Polynomial rate convergence to an invariant measure for the continuum
time limit of the Minority Game | In this paper we show that the continuum time version of the Minority Game
satisfies the criteria for the application of a theorem on the existence of an
invariant measure. We consider the special case of a game with "sufficiently"
asymmetric initial condition where the number of possible choices for each
individual ... | math.PR | in this paper we show that the continuum time version of the minority game satisfies the criteria for the application of a theorem on the existence of an invariant measure we consider the special case of a game with sufficiently asymmetric initial condition where the number of possible choices for each individual is s2... | [['in', 'this', 'paper', 'we', 'show', 'that', 'the', 'continuum', 'time', 'version', 'of', 'the', 'minority', 'game', 'satisfies', 'the', 'criteria', 'for', 'the', 'application', 'of', 'a', 'theorem', 'on', 'the', 'existence', 'of', 'an', 'invariant', 'measure', 'we', 'consider', 'the', 'special', 'case', 'of', 'a', '... | [-0.1508707488067897, 0.10938016314891234, -0.10443332809842674, 0.05922314591554319, -0.015758976873279696, -0.1337192169199866, 0.08381126664090811, 0.3110787693876773, -0.22920549173940377, -0.27945546939385585, 0.13117114681587835, -0.2514206046289035, -0.10212616396910813, 0.15428369759346347, -0.0603621950126197,... |
706.3115 | Finite jet determination of CR mappings | We prove the following finite jet determination result for CR mappings: Given
a smooth generic submanifold M of C^N, N >= 2, which is essentially finite and
of finite type at each of its points, for every point p on M there exists an
integer l(p), depending upper-semicontinuously on p, such that for every smooth
gene... | math.CV | we prove the following finite jet determination result for cr mappings given a smooth generic submanifold m of cn n 2 which is essentially finite and of finite type at each of its points for every point p on m there exists an integer lp depending uppersemicontinuously on p such that for every smooth generic submanifold... | [['we', 'prove', 'the', 'following', 'finite', 'jet', 'determination', 'result', 'for', 'cr', 'mappings', 'given', 'a', 'smooth', 'generic', 'submanifold', 'm', 'of', 'cn', 'n', '2', 'which', 'is', 'essentially', 'finite', 'and', 'of', 'finite', 'type', 'at', 'each', 'of', 'its', 'points', 'for', 'every', 'point', 'p',... | [-0.21094597504620818, 0.09832835734481772, -0.052251078261717876, 0.0017289927670423855, -0.0637819862954698, -0.19780817398741082, -0.00685612224171766, 0.36746179060665546, -0.2974520521410913, -0.16031944865567815, 0.06325623129857748, -0.2820511770572651, -0.05249978590829953, 0.17462372386082145, -0.0370063804848... |
706.3116 | Series expansion for the density of states of the Ising and Potts models | An approximation of the density of states for the Ising and Potts models
based on the high- and low-temperature series are developed.
| cond-mat.str-el cond-mat.stat-mech | an approximation of the density of states for the ising and potts models based on the high and lowtemperature series are developed | [['an', 'approximation', 'of', 'the', 'density', 'of', 'states', 'for', 'the', 'ising', 'and', 'potts', 'models', 'based', 'on', 'the', 'high', 'and', 'lowtemperature', 'series', 'are', 'developed']] | [-0.07066728056154468, 0.13237114401536845, -0.07763509537008675, 0.042039907833730635, 0.02737455154684457, -0.09112352268262343, 0.011496288193897768, 0.32939977977763524, -0.1544423527930948, -0.27629386438903486, 0.12417420050637289, -0.293396609750661, -0.10264384213157675, 0.1763929402117025, 0.08895697360011665,... |
706.3117 | How do methanol masers manage to appear in the youngest star vicinities
and isolated molecular clumps? | General characteristics of methanol (CH3OH) maser emission are summarized. It
is shown that methanol maser sources are concentrated in the spiral arms. Most
of the methanol maser sources from the Perseus arm are associated with embedded
stellar clusters and a considerable portion is situated close to compact HII
regi... | astro-ph | general characteristics of methanol ch3oh maser emission are summarized it is shown that methanol maser sources are concentrated in the spiral arms most of the methanol maser sources from the perseus arm are associated with embedded stellar clusters and a considerable portion is situated close to compact hii regions al... | [['general', 'characteristics', 'of', 'methanol', 'ch3oh', 'maser', 'emission', 'are', 'summarized', 'it', 'is', 'shown', 'that', 'methanol', 'maser', 'sources', 'are', 'concentrated', 'in', 'the', 'spiral', 'arms', 'most', 'of', 'the', 'methanol', 'maser', 'sources', 'from', 'the', 'perseus', 'arm', 'are', 'associated... | [-0.07646490942199742, 0.08785768960897103, 0.009649251613558995, 0.016363356890579803, -0.0840885266323343, -0.06544472795759892, 0.03124465680289138, 0.44442165309451837, -0.1649665880583139, -0.30361975563897026, 0.05553141586794956, -0.22729936089681593, -0.03276649417761618, 0.17760096397847894, -0.022477182365767... |
706.3118 | The structural and magnetic properties of (In1-xFex)2O3 (0.0 <= x <=
0.25) system : prepared by gel combustion method | (In1-xFex)2O3 polycrystalline samples with x = (0.0, 0.05, 0.10, 0.15, 0.20
and 0.25) have been synthesized by a gel combustion method. Reitveld refinement
analysis of X raydiffraction data indicated the formation of single phase cubic
bixbyite structure without any parasitic phases. This observation is further
confi... | cond-mat.mtrl-sci | in1xfex2o3 polycrystalline samples with x 00 005 010 015 020 and 025 have been synthesized by a gel combustion method reitveld refinement analysis of x raydiffraction data indicated the formation of single phase cubic bixbyite structure without any parasitic phases this observation is further confirmed by high resoluti... | [['in1xfex2o3', 'polycrystalline', 'samples', 'with', 'x', '00', '005', '010', '015', '020', 'and', '025', 'have', 'been', 'synthesized', 'by', 'a', 'gel', 'combustion', 'method', 'reitveld', 'refinement', 'analysis', 'of', 'x', 'raydiffraction', 'data', 'indicated', 'the', 'formation', 'of', 'single', 'phase', 'cubic'... | [-0.09816041065972637, 0.2011980906642169, -0.0634487689927813, -0.04610040952684358, -0.021468502035449175, -0.16024748936284927, 0.1598261908769597, 0.49432201429524203, -0.26782408242367883, -0.3458763655613769, 0.05483303547556385, -0.4165493948067623, -0.03680526996454732, 0.18898140450685538, 0.04898327638776126,... |
706.3119 | G2 Hitchin functionals at one loop | We consider the quantization of the effective target space description of
topological M-theory in terms of the Hitchin functional whose critical points
describe seven-manifolds with G2 structure. The one-loop partition function for
this theory is calculated and an extended version of it, that is related to
generalize... | hep-th | we consider the quantization of the effective target space description of topological mtheory in terms of the hitchin functional whose critical points describe sevenmanifolds with g2 structure the oneloop partition function for this theory is calculated and an extended version of it that is related to generalized g2 ge... | [['we', 'consider', 'the', 'quantization', 'of', 'the', 'effective', 'target', 'space', 'description', 'of', 'topological', 'mtheory', 'in', 'terms', 'of', 'the', 'hitchin', 'functional', 'whose', 'critical', 'points', 'describe', 'sevenmanifolds', 'with', 'g2', 'structure', 'the', 'oneloop', 'partition', 'function', '... | [-0.1322836579908569, 0.1075042889721406, -0.08789595461344903, 0.13181691913332635, -0.05276664897569062, -0.08070320042675917, -0.012287393909610193, 0.26768191811657444, -0.2199242554086539, -0.2710795178145324, 0.04598627138412414, -0.27371846016534823, -0.20765476495257973, 0.14153055275415943, -0.0722706811022512... |
706.312 | Some Thermodynamic Aspects of Pure Glue, Fuzzy Bags and Gauge/String
Duality | The thermodynamic properties of a SU(3) gauge theory without quarks are
calculated using a string formulation for 1.2T_c < T < 3T_c. The results are in
good agreement with the lattice data. We also comment on SU(N) gauge theories.
| hep-ph hep-lat hep-th nucl-th | the thermodynamic properties of a su3 gauge theory without quarks are calculated using a string formulation for 12t_c t 3t_c the results are in good agreement with the lattice data we also comment on sun gauge theories | [['the', 'thermodynamic', 'properties', 'of', 'a', 'su3', 'gauge', 'theory', 'without', 'quarks', 'are', 'calculated', 'using', 'a', 'string', 'formulation', 'for', '12t_c', 't', '3t_c', 'the', 'results', 'are', 'in', 'good', 'agreement', 'with', 'the', 'lattice', 'data', 'we', 'also', 'comment', 'on', 'sun', 'gauge', ... | [-0.10677441668923239, 0.23936608674105359, -0.10435884713857572, 0.12532937810504557, -0.049930334846312936, -0.10969540957562826, 0.08362805990288286, 0.4043595825598852, -0.09081850749616688, -0.25695177545217246, 0.04067039066560667, -0.3252177764284047, -0.07800665553155783, 0.12759265162654826, 0.0035298228565905... |
706.3121 | Multi-triangulations as complexes of star polygons | Maximal $(k+1)$-crossing-free graphs on a planar point set in convex
position, that is, $k$-triangulations, have received attention in recent
literature, with motivation coming from several interpretations of them.
We introduce a new way of looking at $k$-triangulations, namely as complexes
of star polygons. With t... | math.CO | maximal k1crossingfree graphs on a planar point set in convex position that is ktriangulations have received attention in recent literature with motivation coming from several interpretations of them we introduce a new way of looking at ktriangulations namely as complexes of star polygons with this tool we give new dir... | [['maximal', 'k1crossingfree', 'graphs', 'on', 'a', 'planar', 'point', 'set', 'in', 'convex', 'position', 'that', 'is', 'ktriangulations', 'have', 'received', 'attention', 'in', 'recent', 'literature', 'with', 'motivation', 'coming', 'from', 'several', 'interpretations', 'of', 'them', 'we', 'introduce', 'a', 'new', 'wa... | [-0.07963609533870998, 0.06532606138035846, -0.08540247644235094, 0.04234502309760174, -0.13550487621567953, -0.10287814030949122, 0.05816393436338657, 0.3927122277613634, -0.2791227769488708, -0.2737911431930768, 0.09825936443536566, -0.2494365540989794, -0.21361578562302896, 0.25904415497699607, -0.10795572791726162,... |
706.3122 | Effects of payoff functions and preference distributions in an adaptive
population | Adaptive populations such as those in financial markets and distributed
control can be modeled by the Minority Game. We consider how their dynamics
depends on the agents' initial preferences of strategies, when the agents use
linear or quadratic payoff functions to evaluate their strategies. We find that
the fluctuat... | q-fin.ST physics.soc-ph | adaptive populations such as those in financial markets and distributed control can be modeled by the minority game we consider how their dynamics depends on the agents initial preferences of strategies when the agents use linear or quadratic payoff functions to evaluate their strategies we find that the fluctuations o... | [['adaptive', 'populations', 'such', 'as', 'those', 'in', 'financial', 'markets', 'and', 'distributed', 'control', 'can', 'be', 'modeled', 'by', 'the', 'minority', 'game', 'we', 'consider', 'how', 'their', 'dynamics', 'depends', 'on', 'the', 'agents', 'initial', 'preferences', 'of', 'strategies', 'when', 'the', 'agents... | [-0.14428633754650239, 0.158464619180061, -0.1045151621315773, 0.11596223661049893, -0.055531740169384454, -0.14125638255268536, 0.09026917515862823, 0.3872598921563657, -0.2698717634871747, -0.2589927979437544, 0.10017674404210004, -0.2949308042778426, -0.1317993841649404, 0.12954763163873492, -0.07649342776095332, -0... |
706.3123 | Comparative study of the inial spikes of SGR giant flares in 1998 and
2004 observed with GEOTAIL: Do magnetospheric instabilities trigger large
scale fracturing of magnetar's crust? | We present the unsaturated peak profile of SGR 1900+14 giant flare on 1998
August 27. This was obtained by particle counters of the Low Energy Particle
instrument onboard the GEOTAIL spacecraft. The observed peak profile revealed
four characteristic structures: initial steep rise, intermediate rise to the
peak, expon... | astro-ph | we present the unsaturated peak profile of sgr 190014 giant flare on 1998 august 27 this was obtained by particle counters of the low energy particle instrument onboard the geotail spacecraft the observed peak profile revealed four characteristic structures initial steep rise intermediate rise to the peak exponential d... | [['we', 'present', 'the', 'unsaturated', 'peak', 'profile', 'of', 'sgr', '190014', 'giant', 'flare', 'on', '1998', 'august', '27', 'this', 'was', 'obtained', 'by', 'particle', 'counters', 'of', 'the', 'low', 'energy', 'particle', 'instrument', 'onboard', 'the', 'geotail', 'spacecraft', 'the', 'observed', 'peak', 'profi... | [-0.09005161646084908, 0.1642964464113809, -0.09412515404132696, 0.13163471162969914, -0.09082613847791575, -0.09070172312024694, 0.04258719481265125, 0.428044815428364, -0.15459389222833592, -0.38495522897021894, 0.05568463328616837, -0.3140844897581981, -0.030364848262606523, 0.23376592027190596, -0.01789969395105846... |
706.3124 | The Non-Trapping Degree of Scattering | We consider classical potential scattering. If no orbit is trapped at energy
E, the Hamiltonian dynamics defines an integer-valued topological degree. This
can be calculated explicitly and be used for symbolic dynamics of
multi-obstacle scattering.
If the potential is bounded, then in the non-trapping case the boun... | math-ph math.MP | we consider classical potential scattering if no orbit is trapped at energy e the hamiltonian dynamics defines an integervalued topological degree this can be calculated explicitly and be used for symbolic dynamics of multiobstacle scattering if the potential is bounded then in the nontrapping case the boundary of hill... | [['we', 'consider', 'classical', 'potential', 'scattering', 'if', 'no', 'orbit', 'is', 'trapped', 'at', 'energy', 'e', 'the', 'hamiltonian', 'dynamics', 'defines', 'an', 'integervalued', 'topological', 'degree', 'this', 'can', 'be', 'calculated', 'explicitly', 'and', 'be', 'used', 'for', 'symbolic', 'dynamics', 'of', '... | [-0.17432994953083708, 0.1409643701394423, -0.07688166489075313, 0.06557696875273089, -0.04256808832448361, -0.15610512609904012, -0.034369952774649465, 0.3454612285626688, -0.2885552269122938, -0.20916095907510868, 0.07519439140457831, -0.2878634284635813, -0.14174945128214514, 0.16854527420578416, -0.0494139944888977... |
706.3125 | Spatial string tension in $N_f=2$ lattice QCD at finite temperature | The spatial string tension across a crossover from the low temperature phase
to the high temperature phase is computed in QCD with two flavors of
non-perturbatively improved Wilson fermions at small lattice spacing a \sim
0.12fm. We find that in the low temperature phase spatial string tension agrees
well with zero t... | hep-lat | the spatial string tension across a crossover from the low temperature phase to the high temperature phase is computed in qcd with two flavors of nonperturbatively improved wilson fermions at small lattice spacing a sim 012fm we find that in the low temperature phase spatial string tension agrees well with zero tempera... | [['the', 'spatial', 'string', 'tension', 'across', 'a', 'crossover', 'from', 'the', 'low', 'temperature', 'phase', 'to', 'the', 'high', 'temperature', 'phase', 'is', 'computed', 'in', 'qcd', 'with', 'two', 'flavors', 'of', 'nonperturbatively', 'improved', 'wilson', 'fermions', 'at', 'small', 'lattice', 'spacing', 'a', ... | [-0.11141724629590335, 0.3159572745983799, -0.06299094887426457, 0.060261086448847964, 0.000397018270376019, -0.1597128284211533, 0.12527928244059858, 0.3961144646581931, -0.17699724114619386, -0.30585167673416436, 0.04565960047945667, -0.3128985620270937, -0.011282326438679146, 0.14208072073494968, -0.0071860429090567... |
706.3126 | On the structure of relativistic collisionless shocks in electron-ion
plasmas | Relativistic collisionless shocks in electron-ion plasma are thought to occur
in the afterglow phase of Gamma-Ray Bursts (GRBs), and in other environments
where relativistic flows interact with the interstellar medium. A particular
regime of shocks in an unmagnetized plasma has generated much interest for GRB
applica... | astro-ph | relativistic collisionless shocks in electronion plasma are thought to occur in the afterglow phase of gammaray bursts grbs and in other environments where relativistic flows interact with the interstellar medium a particular regime of shocks in an unmagnetized plasma has generated much interest for grb applications in... | [['relativistic', 'collisionless', 'shocks', 'in', 'electronion', 'plasma', 'are', 'thought', 'to', 'occur', 'in', 'the', 'afterglow', 'phase', 'of', 'gammaray', 'bursts', 'grbs', 'and', 'in', 'other', 'environments', 'where', 'relativistic', 'flows', 'interact', 'with', 'the', 'interstellar', 'medium', 'a', 'particula... | [-0.10878401728335857, 0.2614101318420234, -0.015202250317781277, 0.12956215942505792, -0.024630020835112582, -0.09492584567383996, -0.01979342847854631, 0.42313484231098775, -0.231607380873313, -0.3127987440578484, -0.03532886327524293, -0.29551568953320384, 0.08839932247203597, 0.20244133324983218, 0.1196018500763568... |
706.3127 | Brane-Worlds Pseudo-Goldstinos | We consider a space-time with extra dimensions containing sectors, branes and
bulk, that communicate only through gravitational interactions. In each sector,
if considered separately, supersymmetry could be spontaneously broken, leading
to the appearance of Goldstinos. However, when taken all together, only certain
c... | hep-th hep-ph | we consider a spacetime with extra dimensions containing sectors branes and bulk that communicate only through gravitational interactions in each sector if considered separately supersymmetry could be spontaneously broken leading to the appearance of goldstinos however when taken all together only certain combinations ... | [['we', 'consider', 'a', 'spacetime', 'with', 'extra', 'dimensions', 'containing', 'sectors', 'branes', 'and', 'bulk', 'that', 'communicate', 'only', 'through', 'gravitational', 'interactions', 'in', 'each', 'sector', 'if', 'considered', 'separately', 'supersymmetry', 'could', 'be', 'spontaneously', 'broken', 'leading'... | [-0.14876438345933377, 0.22012149877632192, -0.051554303936620464, 0.11145699858262073, -0.1106642535264972, -0.18474548417624076, 0.0005027789569752247, 0.31809239968424663, -0.21175771508484992, -0.25857922571797876, 0.0973138180608742, -0.23078759734224066, -0.11327688025207756, 0.09124266110403939, -0.0486703992829... |
706.3128 | Gamma-delayed deuteron emission of the 6Li (0+;T=1) halo state | M1 transitions from the $^6$Li($0^+;T=1$) state at 3.563 MeV to the
$^6$Li($1^+$) ground state and to the $\alpha+d$ continuum are studied in a
three-body model. The bound states are described as an $\alpha+n+p$ system in
hyperspherical coordinates on a Lagrange mesh. The ground-state magnetic moment
and the gamma wi... | nucl-th | m1 transitions from the 6li0t1 state at 3563 mev to the 6li1 ground state and to the alphad continuum are studied in a threebody model the bound states are described as an alphanp system in hyperspherical coordinates on a lagrange mesh the groundstate magnetic moment and the gamma width of the 6li0 resonance are well r... | [['m1', 'transitions', 'from', 'the', '6li0t1', 'state', 'at', '3563', 'mev', 'to', 'the', '6li1', 'ground', 'state', 'and', 'to', 'the', 'alphad', 'continuum', 'are', 'studied', 'in', 'a', 'threebody', 'model', 'the', 'bound', 'states', 'are', 'described', 'as', 'an', 'alphanp', 'system', 'in', 'hyperspherical', 'coor... | [-0.10739523914302342, 0.19546806840951067, -0.056710787946854295, 0.11462654922909749, 0.004656721409010706, -0.10342034206797297, 0.049849634663926536, 0.3652153151363311, -0.2082599077990951, -0.30191517060280904, -0.003905026332376051, -0.31544566840848187, -0.007101948080259271, 0.12272405740529431, 0.091374735191... |
706.3129 | Closed-Form Density of States and Localization Length for a
Non-Hermitian Disordered System | We calculate the Lyapunov exponent for the non-Hermitian Zakharov-Shabat
eigenvalue problem corresponding to the attractive non-linear Schroedinger
equation with a Gaussian random pulse as initial value function. Using an
extension of the Thouless formula to non-Hermitian random operators, we
calculate the correspond... | cond-mat.dis-nn cond-mat.stat-mech cs.IT math.IT nlin.SI | we calculate the lyapunov exponent for the nonhermitian zakharovshabat eigenvalue problem corresponding to the attractive nonlinear schroedinger equation with a gaussian random pulse as initial value function using an extension of the thouless formula to nonhermitian random operators we calculate the corresponding aver... | [['we', 'calculate', 'the', 'lyapunov', 'exponent', 'for', 'the', 'nonhermitian', 'zakharovshabat', 'eigenvalue', 'problem', 'corresponding', 'to', 'the', 'attractive', 'nonlinear', 'schroedinger', 'equation', 'with', 'a', 'gaussian', 'random', 'pulse', 'as', 'initial', 'value', 'function', 'using', 'an', 'extension', ... | [-0.12530639213568803, 0.11719355469770712, -0.08080666885958819, 0.0752284907311484, -0.05108379718296442, -0.1822197700355532, -0.009999789108958426, 0.4058711126069479, -0.2749002017493395, -0.1936948471525802, 0.08431899174311068, -0.30005154715367605, -0.20056759329111892, 0.19035489202913228, 0.01729337819498268,... |
706.313 | Abelian Magnetic Monopoles and Topologically Massive Vector Bosons in
Scalar-Tensor Gravity with Torsion Potential | A Lagrangian formulation describing the electromagnetic interaction -
mediated by topologically massive vector bosons - between charged, spin-(1/2)
fermions with an abelian magnetic monopole in a curved spacetime with
non-minimal coupling and torsion potential is presented. The covariant field
equations are obtained.... | gr-qc hep-th | a lagrangian formulation describing the electromagnetic interaction mediated by topologically massive vector bosons between charged spin12 fermions with an abelian magnetic monopole in a curved spacetime with nonminimal coupling and torsion potential is presented the covariant field equations are obtained the issue of ... | [['a', 'lagrangian', 'formulation', 'describing', 'the', 'electromagnetic', 'interaction', 'mediated', 'by', 'topologically', 'massive', 'vector', 'bosons', 'between', 'charged', 'spin12', 'fermions', 'with', 'an', 'abelian', 'magnetic', 'monopole', 'in', 'a', 'curved', 'spacetime', 'with', 'nonminimal', 'coupling', 'a... | [-0.25082781163113627, 0.28842288537704547, -0.0019737189794157414, 0.10806471296150158, -0.10217030574270386, -0.16928605119539228, -0.08786968685602373, 0.3402140632549182, -0.1498131606173008, -0.32447917355927935, -0.0845998632845449, -0.2778041026297402, -0.1257213183698502, 0.08545859933810983, 0.0530698714837273... |
706.3131 | A nilpotent quotient algorithm for L-presented groups | The main part of this paper contains a description of a nilpotent quotient
algorithm for L-presented groups and a report on applications of its
implementation in the computer algebra system GAP. The appendix introduces two
new infinite series of L-presented groups. Apart from being of interest in
their own right, the... | math.GR | the main part of this paper contains a description of a nilpotent quotient algorithm for lpresented groups and a report on applications of its implementation in the computer algebra system gap the appendix introduces two new infinite series of lpresented groups apart from being of interest in their own right these new ... | [['the', 'main', 'part', 'of', 'this', 'paper', 'contains', 'a', 'description', 'of', 'a', 'nilpotent', 'quotient', 'algorithm', 'for', 'lpresented', 'groups', 'and', 'a', 'report', 'on', 'applications', 'of', 'its', 'implementation', 'in', 'the', 'computer', 'algebra', 'system', 'gap', 'the', 'appendix', 'introduces',... | [-0.16524281821330078, 0.0209401318907112, -0.10463960435299668, 0.009799286859561107, -0.11511744410381652, -0.12274485306988936, 0.010346101395043661, 0.36513945600017905, -0.32054988087475067, -0.26934876205632463, 0.1695536288425501, -0.2481847173476126, -0.16608072716917377, 0.2869786373266834, -0.1466970931942341... |
706.3132 | EasyVoice: Integrating voice synthesis with Skype | This paper presents EasyVoice, a system that integrates voice synthesis with
Skype. EasyVoice allows a person with voice disabilities to talk with another
person located anywhere in the world, removing an important obstacle that
affect these people during a phone or VoIP-based conversation.
| cs.CY cs.HC | this paper presents easyvoice a system that integrates voice synthesis with skype easyvoice allows a person with voice disabilities to talk with another person located anywhere in the world removing an important obstacle that affect these people during a phone or voipbased conversation | [['this', 'paper', 'presents', 'easyvoice', 'a', 'system', 'that', 'integrates', 'voice', 'synthesis', 'with', 'skype', 'easyvoice', 'allows', 'a', 'person', 'with', 'voice', 'disabilities', 'to', 'talk', 'with', 'another', 'person', 'located', 'anywhere', 'in', 'the', 'world', 'removing', 'an', 'important', 'obstacle'... | [-0.14109719558618963, 0.056989517473630256, -0.08186796377412975, -0.016738777249702252, -0.20459082978777587, -0.2588874720851891, 0.08425396497186739, 0.39527867436409, -0.20582704846165142, -0.3326379875652492, 0.04936023704649415, -0.35057379576064707, -0.2008825905562844, 0.17937516758101993, -0.2407886120257899,... |
706.3133 | Tunable photonic band gaps with coherently driven atoms in optical
lattices | Optical lattice loaded with cold atoms can exhibit a tunable photonic band
gap for a weak probe field under the conditions of electromagnetically induced
transparency. This system possesses a number of advantageous properties,
including reduced relaxation of Raman coherence and the associated probe
absorption, and si... | quant-ph | optical lattice loaded with cold atoms can exhibit a tunable photonic band gap for a weak probe field under the conditions of electromagnetically induced transparency this system possesses a number of advantageous properties including reduced relaxation of raman coherence and the associated probe absorption and simulta... | [['optical', 'lattice', 'loaded', 'with', 'cold', 'atoms', 'can', 'exhibit', 'a', 'tunable', 'photonic', 'band', 'gap', 'for', 'a', 'weak', 'probe', 'field', 'under', 'the', 'conditions', 'of', 'electromagnetically', 'induced', 'transparency', 'this', 'system', 'possesses', 'a', 'number', 'of', 'advantageous', 'propert... | [-0.17820885347089532, 0.17092633118730677, -0.0658878552529848, 0.009080839117593838, -0.027533501007998683, -0.19298523441521506, 0.06928688145449592, 0.44164901467585804, -0.29654611980147433, -0.2987561128854827, 0.05891572130900441, -0.23171707637833827, -0.11503202892896353, 0.2286386245842835, 0.0369433819814914... |
706.3134 | Triadophilia: A Special Corner in the Landscape | It is well known that there are a great many apparently consistent vacua of
string theory. We draw attention to the fact that there appear to be very few
Calabi--Yau manifolds with the Hodge numbers h^{11} and h^{21} both small. Of
these, the case (h^{11}, h^{21})=(3,3) corresponds to a manifold on which a
three gene... | hep-th astro-ph hep-ph math.AG | it is well known that there are a great many apparently consistent vacua of string theory we draw attention to the fact that there appear to be very few calabiyau manifolds with the hodge numbers h11 and h21 both small of these the case h11 h2133 corresponds to a manifold on which a three generation heterotic model has... | [['it', 'is', 'well', 'known', 'that', 'there', 'are', 'a', 'great', 'many', 'apparently', 'consistent', 'vacua', 'of', 'string', 'theory', 'we', 'draw', 'attention', 'to', 'the', 'fact', 'that', 'there', 'appear', 'to', 'be', 'very', 'few', 'calabiyau', 'manifolds', 'with', 'the', 'hodge', 'numbers', 'h11', 'and', 'h2... | [-0.12424433133306188, 0.12581443469082135, -0.08526156986546185, 0.12985436790040694, -0.09183068042750367, -0.1503459142624504, 0.02785802583093755, 0.37083404601887904, -0.220015383620436, -0.3131438359737836, 0.1201077437817326, -0.2868311640812964, -0.20706215564730682, 0.18935509595450842, -0.13514676162869566, -... |
706.3135 | Excited $(70,L^+)$ baryon resonances in the relativistic quark model | The masses of positive parity $(70,0^+)$ and $(70,2^+)$ nonstrange and
strange baryons are calculated in the relativistic quark model. The
relativistic three-quark equations of the $(70,L^+)$ multiplets are found in
the framework of the dispersion relation technique. The approximate solutions
of these equations using... | hep-ph | the masses of positive parity 700 and 702 nonstrange and strange baryons are calculated in the relativistic quark model the relativistic threequark equations of the 70l multiplets are found in the framework of the dispersion relation technique the approximate solutions of these equations using the method based on the e... | [['the', 'masses', 'of', 'positive', 'parity', '700', 'and', '702', 'nonstrange', 'and', 'strange', 'baryons', 'are', 'calculated', 'in', 'the', 'relativistic', 'quark', 'model', 'the', 'relativistic', 'threequark', 'equations', 'of', 'the', '70l', 'multiplets', 'are', 'found', 'in', 'the', 'framework', 'of', 'the', 'd... | [-0.10713157235846124, 0.15478089184978525, -0.0959574673985559, 0.12253127292402692, -0.007839538811429127, -0.09628448737281803, -0.0027169390153643246, 0.30554644484072924, -0.14119423626893754, -0.3163439315819257, 0.00248682450005986, -0.33303076335908594, -0.027499504019254568, 0.15482697763316636, 0.076967340894... |
706.3136 | Broad distribution of stick-slip events in Slowly Sheared Granular
Media: Table-top production of a Gutenberg-Richter-like distribution | We monitor the stick-slip displacements of a very slowly driven moveable
perforated top plate which interacts via shearing with a packing of identical
glass beads confined in a tray. When driven at a constant stress rate, the
distributions of large event displacements and energies triggered by the
stick-slip instabil... | cond-mat.stat-mech cond-mat.soft | we monitor the stickslip displacements of a very slowly driven moveable perforated top plate which interacts via shearing with a packing of identical glass beads confined in a tray when driven at a constant stress rate the distributions of large event displacements and energies triggered by the stickslip instabilities ... | [['we', 'monitor', 'the', 'stickslip', 'displacements', 'of', 'a', 'very', 'slowly', 'driven', 'moveable', 'perforated', 'top', 'plate', 'which', 'interacts', 'via', 'shearing', 'with', 'a', 'packing', 'of', 'identical', 'glass', 'beads', 'confined', 'in', 'a', 'tray', 'when', 'driven', 'at', 'a', 'constant', 'stress',... | [-0.16561675368165465, 0.3234142846440975, -0.08882124091065685, 0.02132335553785235, -0.03421435473670422, -0.17424363097254658, 0.038187479423227866, 0.31599821727460536, -0.28599090561349416, -0.24246883650743206, 0.045032555747344355, -0.34712348450762287, -0.1220148149418684, 0.16971073068783316, -0.03521423468130... |
706.3137 | Asymptotic Enumeration of RNA Structures with Pseudoknots | In this paper we present the asymptotic enumeration of RNA structures with
pseudoknots. We develop a general framework for the computation of exponential
growth rate and the sub exponential factors for $k$-noncrossing RNA structures.
Our results are based on the generating function for the number of
$k$-noncrossing R... | q-bio.BM math.CO | in this paper we present the asymptotic enumeration of rna structures with pseudoknots we develop a general framework for the computation of exponential growth rate and the sub exponential factors for knoncrossing rna structures our results are based on the generating function for the number of knoncrossing rna pseudok... | [['in', 'this', 'paper', 'we', 'present', 'the', 'asymptotic', 'enumeration', 'of', 'rna', 'structures', 'with', 'pseudoknots', 'we', 'develop', 'a', 'general', 'framework', 'for', 'the', 'computation', 'of', 'exponential', 'growth', 'rate', 'and', 'the', 'sub', 'exponential', 'factors', 'for', 'knoncrossing', 'rna', '... | [-0.18113296689029704, 0.06557269007997944, -0.08931895092473174, 0.11245932211151598, -0.03919895892592926, -0.08486805413684524, 0.05477953760501605, 0.30494205961136, -0.24065091356417126, -0.23385111478665935, 0.06528292928660513, -0.25469517997129165, -0.22163294060882313, 0.19960626809369006, -0.00382764470339950... |
706.3138 | Insights and puzzles in light quark physics | Recent work in light flavour hadron physics is reviewed. In particular, I
discuss the significance of the progress achieved with light dynamical quarks
on the lattice for the effective low energy theory of QCD. Also, I draw
attention to some puzzling results from NA48 and KTeV concerning the scalar
form factor releva... | hep-ph | recent work in light flavour hadron physics is reviewed in particular i discuss the significance of the progress achieved with light dynamical quarks on the lattice for the effective low energy theory of qcd also i draw attention to some puzzling results from na48 and ktev concerning the scalar form factor relevant for... | [['recent', 'work', 'in', 'light', 'flavour', 'hadron', 'physics', 'is', 'reviewed', 'in', 'particular', 'i', 'discuss', 'the', 'significance', 'of', 'the', 'progress', 'achieved', 'with', 'light', 'dynamical', 'quarks', 'on', 'the', 'lattice', 'for', 'the', 'effective', 'low', 'energy', 'theory', 'of', 'qcd', 'also', ... | [-0.0052919905195294905, 0.17462475175235534, -0.07012479443272407, 0.09514080041095219, -0.06523740040420582, -0.16939942303261804, 0.06429111613772076, 0.3229214801650607, -0.19607518574533364, -0.27202059667218814, 0.05604772270431347, -0.3173055373781333, -0.07716752968333436, 0.18209957851760203, 0.001456803811544... |
706.3139 | Exclusive Meson Production at NLO | We report on numerical studies of the NLO corrections to exclusive meson
electroproduction, both in collider and fixed-target kinematics. Corrections
are found to be huge at small xB and sizeable at intermediate or large xB.
| hep-ph | we report on numerical studies of the nlo corrections to exclusive meson electroproduction both in collider and fixedtarget kinematics corrections are found to be huge at small xb and sizeable at intermediate or large xb | [['we', 'report', 'on', 'numerical', 'studies', 'of', 'the', 'nlo', 'corrections', 'to', 'exclusive', 'meson', 'electroproduction', 'both', 'in', 'collider', 'and', 'fixedtarget', 'kinematics', 'corrections', 'are', 'found', 'to', 'be', 'huge', 'at', 'small', 'xb', 'and', 'sizeable', 'at', 'intermediate', 'or', 'large'... | [-0.09153634038354669, 0.18506885524839162, -0.10244348738342524, 0.17693876592176302, -0.050293669131185326, -0.1322964119325791, 0.04916229571348855, 0.3965187312236854, -0.17349275909364223, -0.22027299723454885, -0.006777339059460376, -0.42175068163446017, 0.07081735041325114, 0.1703244121944798, 0.1349017477993454... |
706.314 | Saffman-Taylor instability in a non-Brownian suspension: finger
selection and destabilization | We study the Saffman-Taylor instability in a non-Brownian suspension by
injection of air. We find that flow structuration in the Hele-Shaw cell can be
described by an effective viscosity depending on the volume fraction. When this
viscosity is used to define the control parameter of the instability, the
classical fin... | cond-mat.soft | we study the saffmantaylor instability in a nonbrownian suspension by injection of air we find that flow structuration in the heleshaw cell can be described by an effective viscosity depending on the volume fraction when this viscosity is used to define the control parameter of the instability the classical finger sele... | [['we', 'study', 'the', 'saffmantaylor', 'instability', 'in', 'a', 'nonbrownian', 'suspension', 'by', 'injection', 'of', 'air', 'we', 'find', 'that', 'flow', 'structuration', 'in', 'the', 'heleshaw', 'cell', 'can', 'be', 'described', 'by', 'an', 'effective', 'viscosity', 'depending', 'on', 'the', 'volume', 'fraction', ... | [-0.12475940974150533, 0.19628684416875994, -0.08598461204011293, 0.028657020963592468, -0.04243950118874981, -0.07962981135971899, 0.04541992711542297, 0.28287463284430714, -0.29435188956150826, -0.3040039515714195, 0.09653176649908678, -0.20848304565401535, -0.12250208152784374, 0.1358488864319766, -0.079706224742053... |
706.3141 | Higher-Order Calculus of Variations on Time Scales | We prove a version of the Euler-Lagrange equations for certain problems of
the calculus of variations on time scales with higher-order delta derivatives.
| math.OC math.CA math.FA | we prove a version of the eulerlagrange equations for certain problems of the calculus of variations on time scales with higherorder delta derivatives | [['we', 'prove', 'a', 'version', 'of', 'the', 'eulerlagrange', 'equations', 'for', 'certain', 'problems', 'of', 'the', 'calculus', 'of', 'variations', 'on', 'time', 'scales', 'with', 'higherorder', 'delta', 'derivatives']] | [-0.19470541835155175, 0.03600323366244202, -0.10044738974260248, 0.10789539669032978, -0.11492909806901994, -0.05817824035235073, -0.0519455187022686, 0.25217662362948706, -0.36572217325801437, -0.3099445456881886, 0.14007510965609032, -0.2531996298095454, -0.11573240322911221, 0.18199949096078458, -0.0863824495337093... |
706.3142 | Three-point correlations for quantum star graphs | We compute the three point correlation function for the eigenvalues of the
Laplacian on quantum star graphs in the limit where the number of edges tends
to infinity. This extends a work by Berkolaiko and Keating, where they get the
2-point correlation function and show that it follows neither Poisson, nor
random matr... | math-ph math.MP | we compute the three point correlation function for the eigenvalues of the laplacian on quantum star graphs in the limit where the number of edges tends to infinity this extends a work by berkolaiko and keating where they get the 2point correlation function and show that it follows neither poisson nor random matrix sta... | [['we', 'compute', 'the', 'three', 'point', 'correlation', 'function', 'for', 'the', 'eigenvalues', 'of', 'the', 'laplacian', 'on', 'quantum', 'star', 'graphs', 'in', 'the', 'limit', 'where', 'the', 'number', 'of', 'edges', 'tends', 'to', 'infinity', 'this', 'extends', 'a', 'work', 'by', 'berkolaiko', 'and', 'keating',... | [-0.07827475394879002, 0.07001641782699153, -0.11835434450767934, 0.10775207217920979, -0.07281836417678278, -0.09634574175288435, 0.052042388917470817, 0.3160628766345326, -0.2509143842107733, -0.26789962594921235, 0.08554067345721705, -0.327132100937888, -0.21797846064146142, 0.119856803357834, -0.023954828102432657,... |
706.3143 | First Order Superfluid to Bose Metal Transition in Systems with Resonant
Pairing | Systems showing resonant superfluidity, driven by an exchange coupling of
strength $g$ between uncorrelated pairs of itinerant fermions and tightly bound
ones, undergo a first order phase transition as $g$ increases beyond some
critical value $g_c$. The superfluid phase for $g \leq g_c$ is characterized by
a gap in t... | cond-mat.supr-con cond-mat.str-el | systems showing resonant superfluidity driven by an exchange coupling of strength g between uncorrelated pairs of itinerant fermions and tightly bound ones undergo a first order phase transition as g increases beyond some critical value g_c the superfluid phase for g leq g_c is characterized by a gap in the fermionic s... | [['systems', 'showing', 'resonant', 'superfluidity', 'driven', 'by', 'an', 'exchange', 'coupling', 'of', 'strength', 'g', 'between', 'uncorrelated', 'pairs', 'of', 'itinerant', 'fermions', 'and', 'tightly', 'bound', 'ones', 'undergo', 'a', 'first', 'order', 'phase', 'transition', 'as', 'g', 'increases', 'beyond', 'some... | [-0.2353854249935424, 0.35255620412584016, -0.03687743001162659, 0.02854428290210794, -0.035503995453202444, -0.18445983838809785, 0.11978116487207022, 0.32183824070231165, -0.2343593193867872, -0.2834610359250503, -0.05340833895498627, -0.34273459207873014, -0.09177465724412265, 0.1269239612251282, 0.07009422614477402... |
706.3144 | Comment on the paper "Weyssenhoff fluid dynamics in a 1+3 covariant
approach" (arXiv:0706.2367) | Few comments are given to clarify some issues of Weyssenhoff fluid in the
Einstein-Cartan gravity.
| astro-ph gr-qc | few comments are given to clarify some issues of weyssenhoff fluid in the einsteincartan gravity | [['few', 'comments', 'are', 'given', 'to', 'clarify', 'some', 'issues', 'of', 'weyssenhoff', 'fluid', 'in', 'the', 'einsteincartan', 'gravity']] | [-0.2593390095978975, 0.13865451862414677, -0.038383806496858595, 0.11908253853519758, -0.23261945694684982, -0.2143740553408861, -0.10052803568542004, 0.25494282618165015, -0.233952305590113, -0.3763389671842257, 0.07343196424189954, -0.3562878593802452, -0.09374934807419777, 0.057937026023864746, -0.21116775584717593... |
706.3145 | Revisiting Signature of Minimal Gauge Mediation | We revisit phenomenology of the minimal gauge-mediated model. This model is
motivated from the SUSY CP and flavor problems. A specific feature of this
model is that \tan\beta is naturally large, since the B term in the Higgs
potential is zero at the messenger scale. This leads to significant SUSY
contributions to var... | hep-ph | we revisit phenomenology of the minimal gaugemediated model this model is motivated from the susy cp and flavor problems a specific feature of this model is that tanbeta is naturally large since the b term in the higgs potential is zero at the messenger scale this leads to significant susy contributions to various lowe... | [['we', 'revisit', 'phenomenology', 'of', 'the', 'minimal', 'gaugemediated', 'model', 'this', 'model', 'is', 'motivated', 'from', 'the', 'susy', 'cp', 'and', 'flavor', 'problems', 'a', 'specific', 'feature', 'of', 'this', 'model', 'is', 'that', 'tanbeta', 'is', 'naturally', 'large', 'since', 'the', 'b', 'term', 'in', '... | [-0.1007622322291494, 0.2673259095951485, -0.006490918847087484, 0.15145364471066455, -0.07115563582091664, -0.16091364725636176, 0.05259699064011399, 0.29589573796659424, -0.24602021120775205, -0.2931907780181903, 0.024063666825755857, -0.30571659286506475, -0.03894836494269279, 0.13577023113432984, 0.0325717814195041... |
706.3146 | WiFi Epidemiology: Can Your Neighbors' Router Make Yours Sick? | In densely populated urban areas WiFi routers form a tightly interconnected
proximity network that can be exploited as a substrate for the spreading of
malware able to launch massive fraudulent attack and affect entire urban areas
WiFi networks. In this paper we consider several scenarios for the deployment
of malwar... | cs.CR physics.soc-ph | in densely populated urban areas wifi routers form a tightly interconnected proximity network that can be exploited as a substrate for the spreading of malware able to launch massive fraudulent attack and affect entire urban areas wifi networks in this paper we consider several scenarios for the deployment of malware t... | [['in', 'densely', 'populated', 'urban', 'areas', 'wifi', 'routers', 'form', 'a', 'tightly', 'interconnected', 'proximity', 'network', 'that', 'can', 'be', 'exploited', 'as', 'a', 'substrate', 'for', 'the', 'spreading', 'of', 'malware', 'able', 'to', 'launch', 'massive', 'fraudulent', 'attack', 'and', 'affect', 'entire... | [-0.18773366613435297, 0.04218802848405485, 0.004462831490825302, 0.08132723073955941, -0.035923846333829404, -0.15125885972862735, 0.12313016499560082, 0.3823719308315928, -0.23127405906744375, -0.29341866429042973, 0.1312738294740591, -0.3169474736800694, -0.2036402836924014, 0.20848151402444476, -0.13301177165932113... |
706.3147 | Half-Supersymmetric Solutions in Five-Dimensional Supergravity | We present a systematic classification of half-supersymmetric solutions of
gauged N=2, D=5 supergravity coupled to an arbitrary number of abelian vector
multiplets for which at least one of the Killing spinors generate a time-like
Killing vector.
| hep-th | we present a systematic classification of halfsupersymmetric solutions of gauged n2 d5 supergravity coupled to an arbitrary number of abelian vector multiplets for which at least one of the killing spinors generate a timelike killing vector | [['we', 'present', 'a', 'systematic', 'classification', 'of', 'halfsupersymmetric', 'solutions', 'of', 'gauged', 'n2', 'd5', 'supergravity', 'coupled', 'to', 'an', 'arbitrary', 'number', 'of', 'abelian', 'vector', 'multiplets', 'for', 'which', 'at', 'least', 'one', 'of', 'the', 'killing', 'spinors', 'generate', 'a', 't... | [-0.20965657701405385, 0.1800293971225781, 0.05819211184926745, 0.03752477513626218, -0.1679948288688643, -0.22680460995373627, -0.06384514301316813, 0.2910444321654116, -0.10930992246398495, -0.23298773723137048, 0.08149318164052805, -0.3191063097781605, -0.10125515551771969, 0.01908254400930471, -0.014817522321310308... |
706.3148 | Finite size effects on surface excess quantities: application to crystal
growth and surface melting of epitaxial layers | From a macroscopic point of view phase transitions as surface melting or two
dimensional (2D) towards three dimensional (3D) growth mode (Stranski-Krastanov
transition) can be described in terms of Gibbs excess quantity duly amended by
size effects (since usual Gibbs excess quantities are only well defined for
semi-i... | cond-mat.mtrl-sci | from a macroscopic point of view phase transitions as surface melting or two dimensional 2d towards three dimensional 3d growth mode stranskikrastanov transition can be described in terms of gibbs excess quantity duly amended by size effects since usual gibbs excess quantities are only well defined for semiinfinite sys... | [['from', 'a', 'macroscopic', 'point', 'of', 'view', 'phase', 'transitions', 'as', 'surface', 'melting', 'or', 'two', 'dimensional', '2d', 'towards', 'three', 'dimensional', '3d', 'growth', 'mode', 'stranskikrastanov', 'transition', 'can', 'be', 'described', 'in', 'terms', 'of', 'gibbs', 'excess', 'quantity', 'duly', '... | [-0.09011421410123939, 0.20200391316219515, -0.0649107356717729, 0.024904577466456787, -0.0182637057064668, -0.13658521272161084, 0.07412401029192235, 0.32946539455619844, -0.3086777961488975, -0.26987574703576367, 0.09771815486879938, -0.28710554365445756, -0.11303001180412653, 0.09825076952212207, -0.0188868240609735... |
706.3149 | Probing the truncation of galaxy dark matter halos in high density
environments from hydrodynamical N-body simulations | We analyze high resolution, N-body hydrodynamical simulations of fiducial
galaxy clusters to probe tidal stripping of the dark matter subhalos. These
simulations include a prescription for star formation allowing us to track the
fate of the stellar component as well. We investigate the effect of tidal
stripping on cl... | astro-ph | we analyze high resolution nbody hydrodynamical simulations of fiducial galaxy clusters to probe tidal stripping of the dark matter subhalos these simulations include a prescription for star formation allowing us to track the fate of the stellar component as well we investigate the effect of tidal stripping on cluster ... | [['we', 'analyze', 'high', 'resolution', 'nbody', 'hydrodynamical', 'simulations', 'of', 'fiducial', 'galaxy', 'clusters', 'to', 'probe', 'tidal', 'stripping', 'of', 'the', 'dark', 'matter', 'subhalos', 'these', 'simulations', 'include', 'a', 'prescription', 'for', 'star', 'formation', 'allowing', 'us', 'to', 'track', ... | [-0.07008953249676393, 0.09256052787488002, -0.1086063629287916, 0.1457245307736395, -0.09202113645468754, 0.0009341153076313661, -0.009634238807131735, 0.41716056189563294, -0.13863585392501784, -0.3857178281865675, 0.006238183057796436, -0.3116633751584838, -0.0011960390177343718, 0.17648463436599934, 0.0201951224942... |
706.315 | Measurement of the Cross Section for open b-Quark Production in
Two-Photon Interactions at LEP | Inclusive beauty-quark production in two-photon collisions has been measured
at LEP using an integrated luminosity of 698 pb-1 collected by the ALEPH
detector with sqrt(s) between 130 and 209 GeV. The b quarks were identified
using lifetime information. The cross section is found to be sigma(e+ e- --> e+
e- b \bar{b}... | hep-ex | inclusive beautyquark production in twophoton collisions has been measured at lep using an integrated luminosity of 698 pb1 collected by the aleph detector with sqrts between 130 and 209 gev the b quarks were identified using lifetime information the cross section is found to be sigmae e e e b barb x 54 08 stat 08 syst... | [['inclusive', 'beautyquark', 'production', 'in', 'twophoton', 'collisions', 'has', 'been', 'measured', 'at', 'lep', 'using', 'an', 'integrated', 'luminosity', 'of', '698', 'pb1', 'collected', 'by', 'the', 'aleph', 'detector', 'with', 'sqrts', 'between', '130', 'and', '209', 'gev', 'the', 'b', 'quarks', 'were', 'identi... | [-0.020681923710239622, 0.19996933700145186, -0.08711436617259796, 0.05859246988637516, 0.03836415156435508, -0.12972874642851262, -0.00024628141680015965, 0.36583158588753295, -0.1308477626182139, -0.3966275847875155, -0.09593449807546746, -0.4763651143759489, 0.2393405333447915, 0.11592208684708637, 0.069639275180032... |
706.3151 | Meta-stable A_n quiver gauge theories | We study metastable dynamical breaking of supersymmetry in A_n quiver gauge
theories. We present a general analysis and criteria for the perturbative
existence of metastable vacua in quivers of any length. Different mechanisms of
gauge mediation can be realized.
| hep-th | we study metastable dynamical breaking of supersymmetry in a_n quiver gauge theories we present a general analysis and criteria for the perturbative existence of metastable vacua in quivers of any length different mechanisms of gauge mediation can be realized | [['we', 'study', 'metastable', 'dynamical', 'breaking', 'of', 'supersymmetry', 'in', 'a_n', 'quiver', 'gauge', 'theories', 'we', 'present', 'a', 'general', 'analysis', 'and', 'criteria', 'for', 'the', 'perturbative', 'existence', 'of', 'metastable', 'vacua', 'in', 'quivers', 'of', 'any', 'length', 'different', 'mechani... | [-0.21734250284349307, 0.26632703271193, -0.11766701260915934, 0.16380632974398443, -0.06374698700025104, -0.20615272785429484, 0.017965620311980065, 0.350064081307023, -0.20931069911099398, -0.22477001854433462, 0.062467369507663906, -0.15084650981216094, -0.133798614048805, 0.01654449076606677, -0.06618901779158758, ... |
706.3152 | Remarks on the calculus of variations on time scales | The calculus of variations is a classical subject which has gain throughout
the last three hundred years a level of rigor and elegance that only time can
give. In this note we show that, contrary to the classical field, available
formulations and results on the recent calculus of variations on time scales
are still a... | math.OC math.CA | the calculus of variations is a classical subject which has gain throughout the last three hundred years a level of rigor and elegance that only time can give in this note we show that contrary to the classical field available formulations and results on the recent calculus of variations on time scales are still at the... | [['the', 'calculus', 'of', 'variations', 'is', 'a', 'classical', 'subject', 'which', 'has', 'gain', 'throughout', 'the', 'last', 'three', 'hundred', 'years', 'a', 'level', 'of', 'rigor', 'and', 'elegance', 'that', 'only', 'time', 'can', 'give', 'in', 'this', 'note', 'we', 'show', 'that', 'contrary', 'to', 'the', 'class... | [-0.09377034869173477, 0.07421637397933879, -0.12940257828650548, 0.053808137292748894, -0.05779842778654962, -0.07869739046095517, 0.03763448212552687, 0.3714436335681841, -0.2754078296751812, -0.3261585121267828, 0.15630420669311143, -0.2521123664276996, -0.13763093819905972, 0.20648037146873258, -0.12408199082610422... |
706.3153 | Connections between Romanovski and other polynomials | A connection between Romanovski polynomials and those polynomials that solve
the one-dimensional Schr\"odinger equation with the trigonometric Rosen-Morse
and hyperbolic Scarf potential is established. The map is constructed by
reworking the Rodrigues formula in an elementary and natural way. The
generating function ... | math.CA | a connection between romanovski polynomials and those polynomials that solve the onedimensional schrodinger equation with the trigonometric rosenmorse and hyperbolic scarf potential is established the map is constructed by reworking the rodrigues formula in an elementary and natural way the generating function is summe... | [['a', 'connection', 'between', 'romanovski', 'polynomials', 'and', 'those', 'polynomials', 'that', 'solve', 'the', 'onedimensional', 'schrodinger', 'equation', 'with', 'the', 'trigonometric', 'rosenmorse', 'and', 'hyperbolic', 'scarf', 'potential', 'is', 'established', 'the', 'map', 'is', 'constructed', 'by', 'reworki... | [-0.13106956547274004, 0.06617410644350226, -0.10374815401340289, 0.12849284434092365, -0.14631415282686552, -0.1815549962680846, -0.0031003267578189335, 0.3027722490064445, -0.3361969770686257, -0.23765875993385202, 0.05760308272863132, -0.3032675451406884, -0.21658910541251922, 0.23134959274015965, -0.040664595640486... |
706.3154 | M31 and Local Group QSO's | Previous analyses have shown companion galaxies aligned along the minor axis
of M31. The alignment includes some galaxies of higher redshift than
conventionally accepted for Local Group members. Here we look at the
distribution of all high redshift objects listed in a 10 x 10 deg. area around
M31. We find not only ga... | astro-ph | previous analyses have shown companion galaxies aligned along the minor axis of m31 the alignment includes some galaxies of higher redshift than conventionally accepted for local group members here we look at the distribution of all high redshift objects listed in a 10 x 10 deg area around m31 we find not only galaxies... | [['previous', 'analyses', 'have', 'shown', 'companion', 'galaxies', 'aligned', 'along', 'the', 'minor', 'axis', 'of', 'm31', 'the', 'alignment', 'includes', 'some', 'galaxies', 'of', 'higher', 'redshift', 'than', 'conventionally', 'accepted', 'for', 'local', 'group', 'members', 'here', 'we', 'look', 'at', 'the', 'distr... | [-0.1322128413918403, 0.08007602107505049, -0.051665670520899744, 0.08143574564963126, -0.1578411962874737, -0.06724436187210518, 0.003815341755949162, 0.5204807271224421, -0.15709814779661796, -0.28795897453469604, 0.04469992828781943, -0.2964694228199487, -0.01797521046387988, 0.20076445089401426, -0.0534653227637849... |
706.3155 | Collider Phenomenology of Unparticle Physics | Low energy phenomenology of the unparticle physics associated with an exact
scale invariant sector possessing a non-trivial infrared fixed point at a
higher energy scale is explored for both electron-positron and hadronic
colliders. Feynman rules for a spin 0, 1 or 2 unparticle coupled to a variety
of standard model ... | hep-ph hep-th | low energy phenomenology of the unparticle physics associated with an exact scale invariant sector possessing a nontrivial infrared fixed point at a higher energy scale is explored for both electronpositron and hadronic colliders feynman rules for a spin 0 1 or 2 unparticle coupled to a variety of standard model gauge ... | [['low', 'energy', 'phenomenology', 'of', 'the', 'unparticle', 'physics', 'associated', 'with', 'an', 'exact', 'scale', 'invariant', 'sector', 'possessing', 'a', 'nontrivial', 'infrared', 'fixed', 'point', 'at', 'a', 'higher', 'energy', 'scale', 'is', 'explored', 'for', 'both', 'electronpositron', 'and', 'hadronic', 'c... | [-0.11250150641112515, 0.27884751707044025, -0.0872433518527393, 0.21614312768366964, -0.10170954551498933, -0.16559892453053576, -0.018088058623910816, 0.3065582172359141, -0.2173099105807949, -0.28595344864585426, 0.002462057834090002, -0.3199228582213099, -0.05201439879841628, 0.1465252938659422, 0.1102669966086215,... |
706.3156 | Interfaces and the edge percolation map of random directed networks | The traditional node percolation map of directed networks is reanalyzed in
terms of edges. In the percolated phase, edges can mainly organize into five
distinct giant connected components, interfaces bridging the communication of
nodes in the strongly connected component and those in the in- and
out-components. Forma... | cond-mat.dis-nn physics.soc-ph | the traditional node percolation map of directed networks is reanalyzed in terms of edges in the percolated phase edges can mainly organize into five distinct giant connected components interfaces bridging the communication of nodes in the strongly connected component and those in the in and outcomponents formal equati... | [['the', 'traditional', 'node', 'percolation', 'map', 'of', 'directed', 'networks', 'is', 'reanalyzed', 'in', 'terms', 'of', 'edges', 'in', 'the', 'percolated', 'phase', 'edges', 'can', 'mainly', 'organize', 'into', 'five', 'distinct', 'giant', 'connected', 'components', 'interfaces', 'bridging', 'the', 'communication'... | [-0.17233670492447456, 0.1268507422093139, -0.06250586138315956, 0.04882918755590383, -0.0425298946124001, -0.13630074872096784, 0.031415026751643864, 0.4024706769253121, -0.2649092530787346, -0.3107001116549989, 0.03246288411683549, -0.32554655637652263, -0.16860652700554402, 0.08324740808393781, -0.014293198171230096... |
706.3157 | Power corrections for jets at hadron colliders | We discuss non-perturbative QCD corrections to jet distributions in hadron
collisions, focussing on hadronisation and underlying event contributions.
Using soft gluon resummation and Monte-Carlo modelling we show that
hadronisation dominates at small values of the jet radius R, behaving as 1/R,
while underlying event... | hep-ph | we discuss nonperturbative qcd corrections to jet distributions in hadron collisions focussing on hadronisation and underlying event contributions using soft gluon resummation and montecarlo modelling we show that hadronisation dominates at small values of the jet radius r behaving as 1r while underlying event correcti... | [['we', 'discuss', 'nonperturbative', 'qcd', 'corrections', 'to', 'jet', 'distributions', 'in', 'hadron', 'collisions', 'focussing', 'on', 'hadronisation', 'and', 'underlying', 'event', 'contributions', 'using', 'soft', 'gluon', 'resummation', 'and', 'montecarlo', 'modelling', 'we', 'show', 'that', 'hadronisation', 'do... | [-0.06759515789350214, 0.17667330950115845, -0.17815748264866382, 0.18427980949819942, -0.0915582593249744, -0.10438163355248023, -0.02396538591471641, 0.3762828000910478, -0.1957355283251772, -0.24687805472018376, 0.0001134003595487304, -0.3235755198035542, 0.021506291342108217, 0.11681701378794769, 0.0212141977087275... |
706.3158 | On contact tops and integrable tops | In this paper, we introduce a geometric structure called top, which is a
trivialized bundle of plane pencils over a Riemannian 3-manifold, defined as
the set of kernels of a circle of 1-forms (e.g. of contact and integrable
forms) with particular properties with respect to the metric. We classify the
manifolds which ... | math.DG math.GT | in this paper we introduce a geometric structure called top which is a trivialized bundle of plane pencils over a riemannian 3manifold defined as the set of kernels of a circle of 1forms eg of contact and integrable forms with particular properties with respect to the metric we classify the manifolds which admit tops a... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'geometric', 'structure', 'called', 'top', 'which', 'is', 'a', 'trivialized', 'bundle', 'of', 'plane', 'pencils', 'over', 'a', 'riemannian', '3manifold', 'defined', 'as', 'the', 'set', 'of', 'kernels', 'of', 'a', 'circle', 'of', '1forms', 'eg', 'of', 'contact', 'and', 'i... | [-0.207773783026884, 0.030344201294550052, -0.07178318273896972, 0.0508648412146916, -0.12865024305259187, -0.13563934589425722, -0.03889277227960217, 0.3811640347043673, -0.2835018699367841, -0.22551346476830075, 0.11898928244869846, -0.2823991139108936, -0.22568374682062617, 0.16926100172568112, -0.12645889547032615,... |
706.3159 | Une s\'emantique observationnelle du mod\`ele des bo\^ites pour la
r\'esolution de programmes logiques (version \'etendue) | This report specifies an observational semantics and gives an original
presentation of the Byrd's box model. The approach accounts for the semantics
of Prolog tracers independently of a particular implementation. Traces are, in
general, considered as rather obscure and difficult to use. The proposed formal
presentati... | cs.PL cs.SE | this report specifies an observational semantics and gives an original presentation of the byrds box model the approach accounts for the semantics of prolog tracers independently of a particular implementation traces are in general considered as rather obscure and difficult to use the proposed formal presentation of a ... | [['this', 'report', 'specifies', 'an', 'observational', 'semantics', 'and', 'gives', 'an', 'original', 'presentation', 'of', 'the', 'byrds', 'box', 'model', 'the', 'approach', 'accounts', 'for', 'the', 'semantics', 'of', 'prolog', 'tracers', 'independently', 'of', 'a', 'particular', 'implementation', 'traces', 'are', '... | [-0.05226827560354171, 0.0008468279803836547, -0.09497319355508999, 0.09177539407206543, -0.12808676557860485, -0.1376132139611352, 0.059936982249813524, 0.3576518350930296, -0.2685307439808783, -0.3087038545881545, 0.08905679980326615, -0.24303639957705805, -0.12003050021073584, 0.18756753307005916, -0.070230122220604... |
706.316 | Spin pumping by a field-driven domain wall | We calculate the charge current in a metallic ferromagnet to first order in
the time derivative of the magnetization direction. Irrespective of the
microscopic details, the result can be expressed in terms of the conductivities
of the majority and minority electrons and the non-adiabatic spin transfer
torque paramete... | cond-mat.mes-hall | we calculate the charge current in a metallic ferromagnet to first order in the time derivative of the magnetization direction irrespective of the microscopic details the result can be expressed in terms of the conductivities of the majority and minority electrons and the nonadiabatic spin transfer torque parameter bet... | [['we', 'calculate', 'the', 'charge', 'current', 'in', 'a', 'metallic', 'ferromagnet', 'to', 'first', 'order', 'in', 'the', 'time', 'derivative', 'of', 'the', 'magnetization', 'direction', 'irrespective', 'of', 'the', 'microscopic', 'details', 'the', 'result', 'can', 'be', 'expressed', 'in', 'terms', 'of', 'the', 'cond... | [-0.1669012354475192, 0.1591010212798596, -0.00849853878290477, 0.016052296027691676, -0.07950085373077956, -0.07431680420495927, 0.03640383905307813, 0.34260651965936023, -0.2500979183147652, -0.28456779354901024, 0.05753915524992132, -0.22036118534478275, -0.11331607018493944, 0.228485216671187, 0.019013952068758732,... |
706.3161 | Euler Walk on a Cayley Tree | We show that the Euler walk on a Cayley tree exhibits two regimes (dynamic
phases): a condensed phase and a low-density phase. In the condensed phase the
self-organized area grows as a compact domain. In the low-density phase the
proportion of self-organized (visited) nodes decreases rapidly from one
generation of th... | cond-mat.stat-mech math.PR | we show that the euler walk on a cayley tree exhibits two regimes dynamic phases a condensed phase and a lowdensity phase in the condensed phase the selforganized area grows as a compact domain in the lowdensity phase the proportion of selforganized visited nodes decreases rapidly from one generation of the tree to the... | [['we', 'show', 'that', 'the', 'euler', 'walk', 'on', 'a', 'cayley', 'tree', 'exhibits', 'two', 'regimes', 'dynamic', 'phases', 'a', 'condensed', 'phase', 'and', 'a', 'lowdensity', 'phase', 'in', 'the', 'condensed', 'phase', 'the', 'selforganized', 'area', 'grows', 'as', 'a', 'compact', 'domain', 'in', 'the', 'lowdensi... | [-0.19529866516352334, 0.24100904789891966, -0.09948046484149675, 0.04424775800013796, -0.007829802031529711, -0.08625396246219331, 0.09309806891697202, 0.3117921844154517, -0.3032456384773584, -0.20923893568366073, 0.12300748586099833, -0.30201497051042525, -0.18339290276189593, 0.12327849914498151, -0.008821747880032... |
706.3162 | Remarks on the density of the law of the occupation time for Bessel
bridges and stable excursions | Smoothness and asymptotic behaviors are studied for the densities of the law
of the occupation time on the positive line for Bessel bridges and the
normalized excursion of strictly stable processes. The key role is played by
these properties for functions defined by Riemann--Liouville fractional
integrals.
| math.PR | smoothness and asymptotic behaviors are studied for the densities of the law of the occupation time on the positive line for bessel bridges and the normalized excursion of strictly stable processes the key role is played by these properties for functions defined by riemannliouville fractional integrals | [['smoothness', 'and', 'asymptotic', 'behaviors', 'are', 'studied', 'for', 'the', 'densities', 'of', 'the', 'law', 'of', 'the', 'occupation', 'time', 'on', 'the', 'positive', 'line', 'for', 'bessel', 'bridges', 'and', 'the', 'normalized', 'excursion', 'of', 'strictly', 'stable', 'processes', 'the', 'key', 'role', 'is',... | [-0.14269885186956305, 0.16325018453695203, -0.09654179235677356, 0.12996905057377223, -0.0038491901334213176, -0.04955016679899848, 0.016035118464218533, 0.34543358431129373, -0.24942144468102767, -0.23339361430186292, 0.11099764696605828, -0.27848962856375653, -0.12998792946176685, 0.20771831205195707, -0.00779828267... |
706.3163 | Verhulst's logistic curve | We observe that the elementary logistic differential equation dP/dt=(1-P/M)kP
may be solved by first changing the variable to R=(M-P)/P. This reduces the
logistic differential equation to the simple linear differential equation
dR/dt=-kR, which can be solved without using the customary but slightly more
elaborate met... | math.HO math.CA | we observe that the elementary logistic differential equation dpdt1pmkp may be solved by first changing the variable to rmpp this reduces the logistic differential equation to the simple linear differential equation drdtkr which can be solved without using the customary but slightly more elaborate methods applied to th... | [['we', 'observe', 'that', 'the', 'elementary', 'logistic', 'differential', 'equation', 'dpdt1pmkp', 'may', 'be', 'solved', 'by', 'first', 'changing', 'the', 'variable', 'to', 'rmpp', 'this', 'reduces', 'the', 'logistic', 'differential', 'equation', 'to', 'the', 'simple', 'linear', 'differential', 'equation', 'drdtkr',... | [-0.06540770806471068, 0.07245219329091827, -0.11782332864153174, 0.09844899907568058, -0.15211059263520008, -0.1940405545550176, 0.002795001708251317, 0.2952535474813024, -0.34290469726300343, -0.2577406939003715, 0.09721629689365163, -0.21797476477294633, -0.21361778193386272, 0.238817428354075, -0.09538697547782048,... |
706.3164 | Poisson sigma model on the sphere | We evaluate the path integral of the Poisson sigma model on sphere and study
the correlators of quantum observables. We argue that for the path integral to
be well-defined the corresponding
Poisson structure should be unimodular. The construction of the finite
dimensional BV theory is presented and we argue that it... | hep-th math.SG | we evaluate the path integral of the poisson sigma model on sphere and study the correlators of quantum observables we argue that for the path integral to be welldefined the corresponding poisson structure should be unimodular the construction of the finite dimensional bv theory is presented and we argue that it is res... | [['we', 'evaluate', 'the', 'path', 'integral', 'of', 'the', 'poisson', 'sigma', 'model', 'on', 'sphere', 'and', 'study', 'the', 'correlators', 'of', 'quantum', 'observables', 'we', 'argue', 'that', 'for', 'the', 'path', 'integral', 'to', 'be', 'welldefined', 'the', 'corresponding', 'poisson', 'structure', 'should', 'be... | [-0.12946088136439876, 0.11473622439519446, -0.1267259035031406, 0.12549222479170494, -0.07637417691104038, -0.08893036230809379, -0.012600677032071185, 0.36001009024603636, -0.27456722237473846, -0.17173410411353926, 0.06115036405033755, -0.23253954906130628, -0.21507407033017703, 0.17306727172369707, -0.0470886202814... |
706.3165 | A solution for actors' viewpoints representation with collaborative
product development | As product complexity and marketing competition increase, a collaborative
product development is necessary for companies which develop high quality
products in short lead-times. To support product actors from different fields,
disciplines, and locations, wishing to exchange and share information, the
representation o... | cs.HC | as product complexity and marketing competition increase a collaborative product development is necessary for companies which develop high quality products in short leadtimes to support product actors from different fields disciplines and locations wishing to exchange and share information the representation of the act... | [['as', 'product', 'complexity', 'and', 'marketing', 'competition', 'increase', 'a', 'collaborative', 'product', 'development', 'is', 'necessary', 'for', 'companies', 'which', 'develop', 'high', 'quality', 'products', 'in', 'short', 'leadtimes', 'to', 'support', 'product', 'actors', 'from', 'different', 'fields', 'disc... | [-0.10094253954576803, 0.05849724849739412, -0.07159383290794474, 0.06758678006943594, -0.13941340006821784, -0.0940611247309434, 0.036765376915301046, 0.38272568633567716, -0.2801856934671571, -0.33530888903731776, 0.12172659789349817, -0.2767085761697026, -0.15401594334188298, 0.13629804238106658, -0.1071183471472041... |
706.3166 | The Equations of Motion of a Charged Particle in the Five-Dimensional
Model of the General Relativity Theory with the Four-Dimensional Nonholonomic
Velocity Space | We consider the four-dimensional nonholonomic distribution defined by the
4-potential of the electromagnetic field on the manifold. This distribution has
a metric tensor with the Lorentzian signature $(+,-,-,-)$, therefore, the
causal structure appears as in the general relativity theory. By means of the
Pontryagin's... | math.DG gr-qc math.MG math.OC physics.class-ph | we consider the fourdimensional nonholonomic distribution defined by the 4potential of the electromagnetic field on the manifold this distribution has a metric tensor with the lorentzian signature therefore the causal structure appears as in the general relativity theory by means of the pontryagins maximum principle we... | [['we', 'consider', 'the', 'fourdimensional', 'nonholonomic', 'distribution', 'defined', 'by', 'the', '4potential', 'of', 'the', 'electromagnetic', 'field', 'on', 'the', 'manifold', 'this', 'distribution', 'has', 'a', 'metric', 'tensor', 'with', 'the', 'lorentzian', 'signature', 'therefore', 'the', 'causal', 'structure... | [-0.16284235751827403, 0.11069035693209552, -0.12058744200411634, 0.0991138686865469, -0.10915959811598591, -0.10379117326645633, -0.03585363794724352, 0.2968779470297624, -0.30344705948242423, -0.27845221625354427, 0.0939706098191859, -0.24334754745101214, -0.1612417101639615, 0.1560877536915342, -0.08931949258556027,... |
706.3167 | Production of a sterile species via active-sterile mixing: an exactly
solvable model | The production of a sterile species via active-sterile mixing in a thermal
medium is studied in an exactly solvable model. The \emph{exact} time evolution
of the sterile distribution function is determined by the dispersion relations
and damping rates $\Gamma_{1,2}$ for the quasiparticle modes. These depend on
$\wtg ... | hep-ph | the production of a sterile species via activesterile mixing in a thermal medium is studied in an exactly solvable model the emphexact time evolution of the sterile distribution function is determined by the dispersion relations and damping rates gamma_12 for the quasiparticle modes these depend on wtg gamma_aa2delta e... | [['the', 'production', 'of', 'a', 'sterile', 'species', 'via', 'activesterile', 'mixing', 'in', 'a', 'thermal', 'medium', 'is', 'studied', 'in', 'an', 'exactly', 'solvable', 'model', 'the', 'emphexact', 'time', 'evolution', 'of', 'the', 'sterile', 'distribution', 'function', 'is', 'determined', 'by', 'the', 'dispersion... | [-0.17064979741406658, 0.3041665272416515, -0.001733317555031114, 0.11103565263028471, -0.0345315182463489, -0.16469039880351422, 0.07148724280630059, 0.2903167663946608, -0.2433981975286919, -0.2595371831986756, 0.0128582375071628, -0.3020224331182913, -0.004608293089079955, 0.18106611548079082, 0.07372884886741568, 0... |
706.3168 | Fluctuations and the clustering of color sources | We present our results on multiplicity and $p_T$ fluctuations at LHC energies
in the framework of the clustering of color sources. In this approach,
elementary color sources -strings- overlap forming clusters, so the number of
effective sources is modified. We find that the fluctuations are proportional
to the number... | hep-ph | we present our results on multiplicity and p_t fluctuations at lhc energies in the framework of the clustering of color sources in this approach elementary color sources strings overlap forming clusters so the number of effective sources is modified we find that the fluctuations are proportional to the number of those ... | [['we', 'present', 'our', 'results', 'on', 'multiplicity', 'and', 'p_t', 'fluctuations', 'at', 'lhc', 'energies', 'in', 'the', 'framework', 'of', 'the', 'clustering', 'of', 'color', 'sources', 'in', 'this', 'approach', 'elementary', 'color', 'sources', 'strings', 'overlap', 'forming', 'clusters', 'so', 'the', 'number',... | [-0.09257455428059284, 0.20438549124026814, -0.1406278511097368, 0.1326335913125569, 0.0051207357677272875, -0.0070280386493183095, 0.009855590433849452, 0.4002433996289395, -0.19574319885578007, -0.36432403007235664, -0.02521512725014383, -0.36832382802206737, -0.0395073654866652, 0.11497614285550438, -0.0066254677680... |
706.3169 | N=1* model superpotential revisited (IR behaviour of N=4 limit) | The one-loop contribution to the superpotential, in particular the
Veneziano-Yankielowicz potential in N=1 supersymmetric Yang-Mills model is
discussed from an elementary field theory method and the matrix model point of
view. Both approaches are based on the Renormalization Group variation of the
superconformal N=4 ... | hep-th | the oneloop contribution to the superpotential in particular the venezianoyankielowicz potential in n1 supersymmetric yangmills model is discussed from an elementary field theory method and the matrix model point of view both approaches are based on the renormalization group variation of the superconformal n4 supersymm... | [['the', 'oneloop', 'contribution', 'to', 'the', 'superpotential', 'in', 'particular', 'the', 'venezianoyankielowicz', 'potential', 'in', 'n1', 'supersymmetric', 'yangmills', 'model', 'is', 'discussed', 'from', 'an', 'elementary', 'field', 'theory', 'method', 'and', 'the', 'matrix', 'model', 'point', 'of', 'view', 'bot... | [-0.04897921756801612, 0.1462547031576136, -0.09409902649039918, 0.09416951228458276, -0.022602243883971203, -0.1546578106886529, -0.03185544084965628, 0.32122808429313465, -0.15867537682123006, -0.25434459416948735, 0.06071784817415508, -0.3325080765173473, -0.2566620664723079, 0.06559410796778158, -0.0317973290035065... |
706.317 | Asymptotic Analysis of General Multiuser Detectors in MIMO DS-CDMA
Channels | We analyze a MIMO DS-CDMA channel with a general multiuser detector including
a nonlinear multiuser detector, using the replica method. In the many-user,
limit the MIMO DS-CDMA channel with the multiuser detector is decoupled into a
bank of single-user SIMO Gaussian channels if a spatial spreading scheme is
employed.... | cs.IT math.IT | we analyze a mimo dscdma channel with a general multiuser detector including a nonlinear multiuser detector using the replica method in the manyuser limit the mimo dscdma channel with the multiuser detector is decoupled into a bank of singleuser simo gaussian channels if a spatial spreading scheme is employed on the ot... | [['we', 'analyze', 'a', 'mimo', 'dscdma', 'channel', 'with', 'a', 'general', 'multiuser', 'detector', 'including', 'a', 'nonlinear', 'multiuser', 'detector', 'using', 'the', 'replica', 'method', 'in', 'the', 'manyuser', 'limit', 'the', 'mimo', 'dscdma', 'channel', 'with', 'the', 'multiuser', 'detector', 'is', 'decouple... | [-0.25284823620928587, 0.038120404382455626, -0.07912689064583067, 0.005521143954478781, -0.025675060483498387, -0.2790205475426593, 0.05199432380250475, 0.3631155433246444, -0.23677537570455373, -0.18707372896400284, 0.1059638208990083, -0.25328771123911503, -0.1905895075902281, 0.13870114170513964, -0.062377531367009... |
706.3171 | Comment to the article "Possible Systematic Effects in Fomblin Coated
Storage Cell Neutron Lifetime Measurements", Steve K. Lamoreaux [1] | The author of article discusses the possible systematic effects in our
experiment using reference and picture from allegedly our publication. First of
all this publication does not exist. The assumption of author about the
probability of lower energy upscattering is in a rough contradiction (300
times) with our exper... | nucl-ex | the author of article discusses the possible systematic effects in our experiment using reference and picture from allegedly our publication first of all this publication does not exist the assumption of author about the probability of lower energy upscattering is in a rough contradiction 300 times with our experimenta... | [['the', 'author', 'of', 'article', 'discusses', 'the', 'possible', 'systematic', 'effects', 'in', 'our', 'experiment', 'using', 'reference', 'and', 'picture', 'from', 'allegedly', 'our', 'publication', 'first', 'of', 'all', 'this', 'publication', 'does', 'not', 'exist', 'the', 'assumption', 'of', 'author', 'about', 't... | [-0.07100518367812038, 0.08842895702272653, -0.09893014133302495, 0.07478777501173317, -0.08874824271723628, -0.054633565874304624, 0.07654069028049708, 0.34815567829459904, -0.185126711221179, -0.37650166526064277, 0.06565966915152967, -0.31533978378772737, -0.07715041556023061, 0.2199492842592299, -0.1147456833608448... |
706.3172 | Switching of the vortex polarity in a magnetic nanodisk by a DC current | We study the dynamics of a vortex state nanodisk due to a dc spin current,
perpendicular to the disk plane. The irreversible switching of the vortex
polarity takes place above some threshold current. The detailed description of
these processes is obtained by spin-lattice simulations.
| cond-mat.str-el | we study the dynamics of a vortex state nanodisk due to a dc spin current perpendicular to the disk plane the irreversible switching of the vortex polarity takes place above some threshold current the detailed description of these processes is obtained by spinlattice simulations | [['we', 'study', 'the', 'dynamics', 'of', 'a', 'vortex', 'state', 'nanodisk', 'due', 'to', 'a', 'dc', 'spin', 'current', 'perpendicular', 'to', 'the', 'disk', 'plane', 'the', 'irreversible', 'switching', 'of', 'the', 'vortex', 'polarity', 'takes', 'place', 'above', 'some', 'threshold', 'current', 'the', 'detailed', 'de... | [-0.23213391625110738, 0.14493732458636674, -0.014896592950787057, 0.02359362474949607, -0.09096309906718406, -0.046389157460494476, 0.08738516044633632, 0.3690062779933214, -0.2890478958989578, -0.2515497829087756, 0.06277396489696746, -0.2181525841270658, -0.059828981418501244, 0.21740595509552144, 0.0734682898672128... |
706.3173 | Sine-Gordon solitons, auxiliary fields, and singular limit of a double
pendulums chain | We consider the continuum version of an elastic chain supporting topological
and non-topological degrees of freedom; this generalizes a model for the
dynamics of DNA recently proposed and investigated by ourselves. In a certain
limit, the non-topological degrees of freedom are frozen, and the model reduces
to the sin... | math-ph math.MP nlin.PS | we consider the continuum version of an elastic chain supporting topological and nontopological degrees of freedom this generalizes a model for the dynamics of dna recently proposed and investigated by ourselves in a certain limit the nontopological degrees of freedom are frozen and the model reduces to the sinegordon ... | [['we', 'consider', 'the', 'continuum', 'version', 'of', 'an', 'elastic', 'chain', 'supporting', 'topological', 'and', 'nontopological', 'degrees', 'of', 'freedom', 'this', 'generalizes', 'a', 'model', 'for', 'the', 'dynamics', 'of', 'dna', 'recently', 'proposed', 'and', 'investigated', 'by', 'ourselves', 'in', 'a', 'c... | [-0.17187224473991233, 0.12643231604982527, -0.0704857070424308, 0.06657068817381286, -0.044732875755335404, -0.11895085388325213, 0.025315067417347643, 0.2694324185387928, -0.2516855309556026, -0.24217198099794351, 0.06233559400448209, -0.25059236340796737, -0.17664254907019963, 0.12771272972614806, -0.050183390586189... |
706.3174 | NGC4438 and its environment at radio wavelengths | We present multi-frequency, radio-continuum and HI observations of NGC4438,
the highly-disturbed, active galaxy in the Virgo cluster, with the VLA and the
GMRT. High-resolution observations with the VLA at 4860 and 8460 MHz show the
presence of an inverted-spectrum radio nucleus located between the highly
asymmetric ... | astro-ph | we present multifrequency radiocontinuum and hi observations of ngc4438 the highlydisturbed active galaxy in the virgo cluster with the vla and the gmrt highresolution observations with the vla at 4860 and 8460 mhz show the presence of an invertedspectrum radio nucleus located between the highly asymmetric lobes of rad... | [['we', 'present', 'multifrequency', 'radiocontinuum', 'and', 'hi', 'observations', 'of', 'ngc4438', 'the', 'highlydisturbed', 'active', 'galaxy', 'in', 'the', 'virgo', 'cluster', 'with', 'the', 'vla', 'and', 'the', 'gmrt', 'highresolution', 'observations', 'with', 'the', 'vla', 'at', '4860', 'and', '8460', 'mhz', 'sho... | [-0.05494853984712409, 0.07566226644584892, -0.08043989306879079, 0.059947471498162486, -0.10106106184708376, -0.05432085740763033, 0.016249402303665485, 0.4686255676281308, -0.1579467189242883, -0.28240015690830805, 0.07086329341297143, -0.28841280464398406, -0.03343057299160489, 0.1721953978281348, 0.0112262696721304... |
706.3175 | Unveiling new systematics in the self-assembly of atomic chains on
Si(111) | Self-assembled arrays of atomic chains on Si(111) represent a fascinating
family of nanostructures with quasi-one-dimensional electronic properties.
These surface reconstructions are stabilized by a variety of adsorbates ranging
from alkali and alkaline earth metals to noble and rare earth metals. Combining
the compl... | cond-mat.other | selfassembled arrays of atomic chains on si111 represent a fascinating family of nanostructures with quasionedimensional electronic properties these surface reconstructions are stabilized by a variety of adsorbates ranging from alkali and alkaline earth metals to noble and rare earth metals combining the complementary ... | [['selfassembled', 'arrays', 'of', 'atomic', 'chains', 'on', 'si111', 'represent', 'a', 'fascinating', 'family', 'of', 'nanostructures', 'with', 'quasionedimensional', 'electronic', 'properties', 'these', 'surface', 'reconstructions', 'are', 'stabilized', 'by', 'a', 'variety', 'of', 'adsorbates', 'ranging', 'from', 'al... | [-0.13181895733433813, 0.2789616238033353, -0.0038892725994425616, 0.03852589814074642, 0.016179877454568902, -0.21676215076961455, 0.09078896313295738, 0.45098747000914097, -0.29871792278217907, -0.2745031764623055, -0.012205535699882784, -0.38523316665067653, -0.15137042724411964, 0.1592824724156502, 0.06974108350147... |
706.3176 | Properties of noncommutative axionic electrodynamics | Using the gauge-invariant but path-dependent variables formalism, we compute
the static quantum potential for noncommutative axionic electrodynamics, and
find a radically different result than the corresponding commutative case. We
explicitly show that the static potential profile is analogous to that
encountered in ... | hep-th | using the gaugeinvariant but pathdependent variables formalism we compute the static quantum potential for noncommutative axionic electrodynamics and find a radically different result than the corresponding commutative case we explicitly show that the static potential profile is analogous to that encountered in both no... | [['using', 'the', 'gaugeinvariant', 'but', 'pathdependent', 'variables', 'formalism', 'we', 'compute', 'the', 'static', 'quantum', 'potential', 'for', 'noncommutative', 'axionic', 'electrodynamics', 'and', 'find', 'a', 'radically', 'different', 'result', 'than', 'the', 'corresponding', 'commutative', 'case', 'we', 'exp... | [-0.13811365175551096, 0.1840248437855687, -0.09237677974855169, 0.13497336615048544, -0.1085147970650149, -0.1681391592014973, -0.029577158912281066, 0.3280029469087981, -0.2089484188248191, -0.2753481843688509, 0.021235064256184717, -0.24146201130688974, -0.21516845041984006, 0.11378522491768787, -0.02447222374183567... |
706.3177 | Role of homeostasis in learning sparse representations | Neurons in the input layer of primary visual cortex in primates develop
edge-like receptive fields. One approach to understanding the emergence of this
response is to state that neural activity has to efficiently represent sensory
data with respect to the statistics of natural scenes. Furthermore, it is
believed that... | q-bio.NC | neurons in the input layer of primary visual cortex in primates develop edgelike receptive fields one approach to understanding the emergence of this response is to state that neural activity has to efficiently represent sensory data with respect to the statistics of natural scenes furthermore it is believed that such ... | [['neurons', 'in', 'the', 'input', 'layer', 'of', 'primary', 'visual', 'cortex', 'in', 'primates', 'develop', 'edgelike', 'receptive', 'fields', 'one', 'approach', 'to', 'understanding', 'the', 'emergence', 'of', 'this', 'response', 'is', 'to', 'state', 'that', 'neural', 'activity', 'has', 'to', 'efficiently', 'represe... | [-0.06938039924098442, 0.10723098003281284, -0.06404840800317779, 0.06803485414371785, -0.06257569281779955, -0.18538501183090286, 0.03721441804076982, 0.4197193516904604, -0.2937591244555202, -0.3055310224616113, 0.05051710789938729, -0.22480850018338358, -0.2710721564759393, 0.141502625314082, -0.14233330064618022, 0... |
706.3178 | Representing a product system representation as a contractive semigroup
and applications to regular isometric dilations | In this paper we propose a new technical tool for analyzing representations
of Hilbert $C^*$-product systems. Using this tool, we give a new proof that
every doubly commuting representation over $\mathbb{N}^k$ has a regular
isometric dilation, and we also prove sufficient conditions for the existence
of a regular iso... | math.OA | in this paper we propose a new technical tool for analyzing representations of hilbert cproduct systems using this tool we give a new proof that every doubly commuting representation over mathbbnk has a regular isometric dilation and we also prove sufficient conditions for the existence of a regular isometric dilation ... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'new', 'technical', 'tool', 'for', 'analyzing', 'representations', 'of', 'hilbert', 'cproduct', 'systems', 'using', 'this', 'tool', 'we', 'give', 'a', 'new', 'proof', 'that', 'every', 'doubly', 'commuting', 'representation', 'over', 'mathbbnk', 'has', 'a', 'regular', 'isom... | [-0.11341819003116273, 0.08605580949058224, -0.14609059287301665, 0.06843969795902792, -0.07983258070141476, -0.12485204178041645, -0.017003891740127335, 0.373456272329869, -0.2800848259191428, -0.15680453189997934, 0.1369055851973826, -0.22431023886227713, -0.20826968866666512, 0.23049858824482986, -0.1428558090701699... |
706.3179 | Supernova remnants with magnetars: clues to magnetar formation | I discuss the lack of observational evidence that magnetars are formed as
rapidly rotating neutron stars. Supernova remnants containing magnetars do not
show the excess of kinetic energy expected for such a formation scenario, nor
is there any evidence for a relic pulsar wind nebula. However, it could be that
magneta... | astro-ph | i discuss the lack of observational evidence that magnetars are formed as rapidly rotating neutron stars supernova remnants containing magnetars do not show the excess of kinetic energy expected for such a formation scenario nor is there any evidence for a relic pulsar wind nebula however it could be that magnetars are... | [['i', 'discuss', 'the', 'lack', 'of', 'observational', 'evidence', 'that', 'magnetars', 'are', 'formed', 'as', 'rapidly', 'rotating', 'neutron', 'stars', 'supernova', 'remnants', 'containing', 'magnetars', 'do', 'not', 'show', 'the', 'excess', 'of', 'kinetic', 'energy', 'expected', 'for', 'such', 'a', 'formation', 'sc... | [-0.1074109658474472, 0.1917284650551716, -0.0802221394027112, 0.16778136223464118, -0.153127207499005, -0.08700736146797294, 0.07346916938886831, 0.3833150689147021, -0.20072358626465084, -0.328444010101123, 0.0934764476415705, -0.24904295148741293, -0.0017045288703023543, 0.2454646861492675, -0.03265616105333172, -0.... |
706.318 | The Emerging Features of Bipolar Magnetic Regions during Solar Minima | Solar magnetic synoptic charts obtained by NSO/Kitt Peak and SOHO/MDI are
analyzed for studying the appearance of bipolar magnetic regions (BMRs) during
solar minima. As a result, we find the emergence of long-lived BMRs has three
typical features. (1) BMRs' emerging rates of the new cycles increase about 3
times fas... | astro-ph | solar magnetic synoptic charts obtained by nsokitt peak and sohomdi are analyzed for studying the appearance of bipolar magnetic regions bmrs during solar minima as a result we find the emergence of longlived bmrs has three typical features 1 bmrs emerging rates of the new cycles increase about 3 times faster than thos... | [['solar', 'magnetic', 'synoptic', 'charts', 'obtained', 'by', 'nsokitt', 'peak', 'and', 'sohomdi', 'are', 'analyzed', 'for', 'studying', 'the', 'appearance', 'of', 'bipolar', 'magnetic', 'regions', 'bmrs', 'during', 'solar', 'minima', 'as', 'a', 'result', 'we', 'find', 'the', 'emergence', 'of', 'longlived', 'bmrs', 'h... | [-0.20062707206234337, 0.2382211825270054, 0.006589090442704891, 0.12655317896632884, 0.013229982044709765, -0.06721359848490228, 0.04134994207516961, 0.3672314872884232, -0.20481549202585997, -0.39590878067133217, 0.11075171190718917, -0.24966731227063776, -0.10304500437949014, 0.21592979028659023, -0.0741669627230452... |
706.3181 | Simulation of the Single- and Double-Slit Experiments with Quantum
Walkers | We employ the broken-link model to create a barrier with slits in a
two-dimensional lattice. The diffraction and interference patterns of the
probability distribution of quantum walkers passing through the slits are
analyzed. Simulations were performed using the main types of coins, and display
diffraction and interf... | quant-ph | we employ the brokenlink model to create a barrier with slits in a twodimensional lattice the diffraction and interference patterns of the probability distribution of quantum walkers passing through the slits are analyzed simulations were performed using the main types of coins and display diffraction and interference ... | [['we', 'employ', 'the', 'brokenlink', 'model', 'to', 'create', 'a', 'barrier', 'with', 'slits', 'in', 'a', 'twodimensional', 'lattice', 'the', 'diffraction', 'and', 'interference', 'patterns', 'of', 'the', 'probability', 'distribution', 'of', 'quantum', 'walkers', 'passing', 'through', 'the', 'slits', 'are', 'analyzed... | [-0.14284161578311963, 0.16063884564640898, -0.1571130414182941, 0.04366095488270124, -0.0033650454823617583, -0.16075979968256973, 0.12366337095887435, 0.4274576498126542, -0.24645036660863465, -0.30329322992582564, 0.043586088497519354, -0.33327472682490394, -0.14583432839976418, 0.15913657443511678, -0.0034070812207... |
706.3182 | Flux Densities and Radio Polarization Characteristics of Two Vela-like
Pulsars | We report on dual-frequency radio polarimetry observations of two young,
energetic pulsars, PSRs J0940-5428 and J1301-6305. These were among the first
Vela-like pulsars discovered in the Parkes Multibeam survey. We conducted
observations of these pulsars with the Australia Telescope Compact Array (ATCA)
at center fre... | astro-ph | we report on dualfrequency radio polarimetry observations of two young energetic pulsars psrs j09405428 and j13016305 these were among the first velalike pulsars discovered in the parkes multibeam survey we conducted observations of these pulsars with the australia telescope compact array atca at center frequencies of ... | [['we', 'report', 'on', 'dualfrequency', 'radio', 'polarimetry', 'observations', 'of', 'two', 'young', 'energetic', 'pulsars', 'psrs', 'j09405428', 'and', 'j13016305', 'these', 'were', 'among', 'the', 'first', 'velalike', 'pulsars', 'discovered', 'in', 'the', 'parkes', 'multibeam', 'survey', 'we', 'conducted', 'observa... | [-0.10032708418150084, 0.1297788295964552, -0.00977734652772343, 0.07812593948511014, -0.13933635538849395, -0.10744359243192336, 0.06264332334707383, 0.5060129296414706, -0.14173249216737593, -0.3518745233874996, 0.12516584592557758, -0.30426950764931027, -0.03538019647885139, 0.31992442537769106, 0.012963987703175367... |
706.3183 | Entanglement Production in Non-Equilibrium Thermodynamics | We define and analyse the concept of entanglement production during the
evolution of a general quantum mechanical dissipative system. While it is
important to minimise entropy production in order to achieve thermodynamical
efficiency, maximising the rate of change of entanglement is important in
quantum information p... | quant-ph | we define and analyse the concept of entanglement production during the evolution of a general quantum mechanical dissipative system while it is important to minimise entropy production in order to achieve thermodynamical efficiency maximising the rate of change of entanglement is important in quantum information proce... | [['we', 'define', 'and', 'analyse', 'the', 'concept', 'of', 'entanglement', 'production', 'during', 'the', 'evolution', 'of', 'a', 'general', 'quantum', 'mechanical', 'dissipative', 'system', 'while', 'it', 'is', 'important', 'to', 'minimise', 'entropy', 'production', 'in', 'order', 'to', 'achieve', 'thermodynamical', ... | [-0.11050902332551778, 0.15435387160768732, -0.07497251299768687, 0.11458802257385105, 0.004158938068896532, -0.16252901244536042, 0.01639744767174125, 0.32318282714486124, -0.25129207837954165, -0.29670626144483686, 0.07995699707698077, -0.30709854840300976, -0.11341071772947907, 0.20740548160672187, -0.03451183914765... |
706.3184 | Late-time behaviour of the tilted Bianchi type VI$_{-1/9}$ models | We study tilted perfect fluid cosmological models with a constant equation of
state parameter in spatially homogeneous models of Bianchi type VI$_{-1/9}$
using dynamical systems methods and numerical simulations. We study models with
and without vorticity, with an emphasis on their future asymptotic evolution.
We sho... | gr-qc astro-ph math-ph math.MP | we study tilted perfect fluid cosmological models with a constant equation of state parameter in spatially homogeneous models of bianchi type vi_19 using dynamical systems methods and numerical simulations we study models with and without vorticity with an emphasis on their future asymptotic evolution we show that for ... | [['we', 'study', 'tilted', 'perfect', 'fluid', 'cosmological', 'models', 'with', 'a', 'constant', 'equation', 'of', 'state', 'parameter', 'in', 'spatially', 'homogeneous', 'models', 'of', 'bianchi', 'type', 'vi_19', 'using', 'dynamical', 'systems', 'methods', 'and', 'numerical', 'simulations', 'we', 'study', 'models', ... | [-0.17978788882663305, 0.09609406043014271, -0.08687549015986874, 0.01067857833748514, -0.05757635972942367, -0.15337409591478662, -0.014336392544492177, 0.3787402333691716, -0.23900467702046488, -0.23765079683454876, 0.1124025255505165, -0.2368929021229798, -0.13493532702594882, 0.21283946062127748, 0.0149240729105341... |
706.3185 | Resistivity effects in surface superconductivity of thin films in strong
magnetic fields | Phase slips creation in the thin film in perpendicular magnetic filed with
edge superconductivity is studied. These centers are due to thermal activation
of the order parameter below superconducting temperature transition leading to
the suppression of the superconductivity. The corresponding resistance is
calculated.... | cond-mat.supr-con | phase slips creation in the thin film in perpendicular magnetic filed with edge superconductivity is studied these centers are due to thermal activation of the order parameter below superconducting temperature transition leading to the suppression of the superconductivity the corresponding resistance is calculated the ... | [['phase', 'slips', 'creation', 'in', 'the', 'thin', 'film', 'in', 'perpendicular', 'magnetic', 'filed', 'with', 'edge', 'superconductivity', 'is', 'studied', 'these', 'centers', 'are', 'due', 'to', 'thermal', 'activation', 'of', 'the', 'order', 'parameter', 'below', 'superconducting', 'temperature', 'transition', 'lea... | [-0.22607578841753576, 0.2533843589693921, -0.013223446474024436, 0.01246946489455451, -0.027136001128294483, -0.1288370240945369, 0.05397157594220849, 0.33883608892423717, -0.2711240027735873, -0.27926268782920954, 0.0459913838237365, -0.29566272686621764, -0.08326057284479825, 0.17440645415591438, 0.01952669136055813... |
706.3186 | Precision spectroscopy with two correlated atoms | We discuss techniques that allow for long coherence times in laser
spectroscopy experiments with two trapped ions. We show that for this purpose
not only entangled ions prepared in decoherence-free subspaces can be used but
also a pair of ions that are not entangled but subject to the same kind of
phase noise. We app... | quant-ph physics.atom-ph | we discuss techniques that allow for long coherence times in laser spectroscopy experiments with two trapped ions we show that for this purpose not only entangled ions prepared in decoherencefree subspaces can be used but also a pair of ions that are not entangled but subject to the same kind of phase noise we apply th... | [['we', 'discuss', 'techniques', 'that', 'allow', 'for', 'long', 'coherence', 'times', 'in', 'laser', 'spectroscopy', 'experiments', 'with', 'two', 'trapped', 'ions', 'we', 'show', 'that', 'for', 'this', 'purpose', 'not', 'only', 'entangled', 'ions', 'prepared', 'in', 'decoherencefree', 'subspaces', 'can', 'be', 'used'... | [-0.10158172451231755, 0.23965943103091755, -0.04471448813094182, 0.010818579482709926, 0.04979450222146645, -0.1854906351922938, 0.044120656727326596, 0.4535423783438929, -0.22354011267706167, -0.237396358407699, 0.007553970538016953, -0.2726833569932352, -0.010030569843529315, 0.21851131022813614, -0.0045212895172553... |
706.3187 | Simulations of the Poynting--Robertson Cosmic Battery in Resistive
Accretion Disks | We describe the results of numerical "2.5--dimensional" MHD simulations of an
initially unmagnetized disk model orbiting a central point--mass and responding
to the continual generation of poloidal magnetic field due to a secular source
that emulates the Poynting--Robertson (PR) drag on electrons in the vicinity of
a... | astro-ph | we describe the results of numerical 25dimensional mhd simulations of an initially unmagnetized disk model orbiting a central pointmass and responding to the continual generation of poloidal magnetic field due to a secular source that emulates the poyntingrobertson pr drag on electrons in the vicinity of a luminous ste... | [['we', 'describe', 'the', 'results', 'of', 'numerical', '25dimensional', 'mhd', 'simulations', 'of', 'an', 'initially', 'unmagnetized', 'disk', 'model', 'orbiting', 'a', 'central', 'pointmass', 'and', 'responding', 'to', 'the', 'continual', 'generation', 'of', 'poloidal', 'magnetic', 'field', 'due', 'to', 'a', 'secula... | [-0.14572562653039553, 0.18610477804667402, -0.05069900188299449, 0.04521700785790948, -0.07877177609299205, -0.04816849075445314, -0.051254817880626524, 0.36077749084541416, -0.28032758986774464, -0.2938315875036801, 0.08005386957963896, -0.2447147716620779, -0.011661912137388217, 0.2161971675965981, -0.01894179624817... |
706.3188 | A tutorial on conformal prediction | Conformal prediction uses past experience to determine precise levels of
confidence in new predictions. Given an error probability $\epsilon$, together
with a method that makes a prediction $\hat{y}$ of a label $y$, it produces a
set of labels, typically containing $\hat{y}$, that also contains $y$ with
probability $... | cs.LG stat.ML | conformal prediction uses past experience to determine precise levels of confidence in new predictions given an error probability epsilon together with a method that makes a prediction haty of a label y it produces a set of labels typically containing haty that also contains y with probability 1epsilon conformal predic... | [['conformal', 'prediction', 'uses', 'past', 'experience', 'to', 'determine', 'precise', 'levels', 'of', 'confidence', 'in', 'new', 'predictions', 'given', 'an', 'error', 'probability', 'epsilon', 'together', 'with', 'a', 'method', 'that', 'makes', 'a', 'prediction', 'haty', 'of', 'a', 'label', 'y', 'it', 'produces', '... | [-0.048543071181552905, 0.08141455305392913, -0.0956998819601722, 0.07318519593989652, -0.09548090891539172, -0.20020831264511524, 0.04073349825482166, 0.4069041695691786, -0.24407008180959272, -0.28083300896709396, 0.0956072243746537, -0.28773845921991004, -0.14718723417488191, 0.20056833837945717, -0.0985130371464381... |
706.3189 | Exponentially Expanding Radiation Dominated and Dust Dominated Universes
in Brans-Dicke Theory | The Brans-Dicke Theory of Gravity is one of the most promising alternatives
to the Einstein's Theory of General Relativity. We have examined an action term
with wrong signs for both the kinetic and mass terms for the scalar field and
have found solutions for both the scale factor of the universe and the
Brans-Dicke s... | gr-qc | the bransdicke theory of gravity is one of the most promising alternatives to the einsteins theory of general relativity we have examined an action term with wrong signs for both the kinetic and mass terms for the scalar field and have found solutions for both the scale factor of the universe and the bransdicke scalar ... | [['the', 'bransdicke', 'theory', 'of', 'gravity', 'is', 'one', 'of', 'the', 'most', 'promising', 'alternatives', 'to', 'the', 'einsteins', 'theory', 'of', 'general', 'relativity', 'we', 'have', 'examined', 'an', 'action', 'term', 'with', 'wrong', 'signs', 'for', 'both', 'the', 'kinetic', 'and', 'mass', 'terms', 'for', ... | [-0.1427716403955319, 0.10988098850352575, -0.07977615168592969, 0.10960038734283145, -0.07827404358225767, -0.1429146559504395, -0.0769751155176429, 0.27086581011134825, -0.1855679856952982, -0.3260629174345341, 0.059384868287511904, -0.24162037969856967, -0.11499058036897027, 0.16257750978273508, 0.01092755796815284,... |
706.319 | Equilibrium nano-shape changes induced by epitaxial stress (generalised
Wulf-Kaishew theorem) | A generalised Wulf-Kaishew theorem is given describing the equilibrium shape
(ES) of an isolated 3D crystal A deposited coherently onto a lattice mismatched
planar substrate. For this purpose a free polyhedral crystal is formed then
homogeneously strained to be accommodated onto the lattice mismatched
substrate. Duri... | cond-mat.mtrl-sci | a generalised wulfkaishew theorem is given describing the equilibrium shape es of an isolated 3d crystal a deposited coherently onto a lattice mismatched planar substrate for this purpose a free polyhedral crystal is formed then homogeneously strained to be accommodated onto the lattice mismatched substrate during its ... | [['a', 'generalised', 'wulfkaishew', 'theorem', 'is', 'given', 'describing', 'the', 'equilibrium', 'shape', 'es', 'of', 'an', 'isolated', '3d', 'crystal', 'a', 'deposited', 'coherently', 'onto', 'a', 'lattice', 'mismatched', 'planar', 'substrate', 'for', 'this', 'purpose', 'a', 'free', 'polyhedral', 'crystal', 'is', 'f... | [-0.10951059238955213, 0.20574689911521965, -0.05928868826912107, 0.02242359516526674, -0.032558448478985244, -0.1383629456937018, 0.02713388850679621, 0.4059382158764961, -0.30423232240344183, -0.25407057977973085, 0.05721595677279747, -0.28211885535776027, -0.122889367047476, 0.14704216840892503, -0.04310314382869049... |
706.3191 | Spinar Paradigm and Gamma Ray Bursts Central Engine | A spinar is a quasi-equilibrium collapsing object whose equilibrium is
maintained by the balance of centrifugal and gravitational forces and whose
evolution is determined by its magnetic field. The spinar quasi equilibrium
model recently discussed as the course for extralong X-ray plateu in GRB
(Lipunov & Gorbovskoy,... | astro-ph | a spinar is a quasiequilibrium collapsing object whose equilibrium is maintained by the balance of centrifugal and gravitational forces and whose evolution is determined by its magnetic field the spinar quasi equilibrium model recently discussed as the course for extralong xray plateu in grb lipunov gorbovskoy 2007 we ... | [['a', 'spinar', 'is', 'a', 'quasiequilibrium', 'collapsing', 'object', 'whose', 'equilibrium', 'is', 'maintained', 'by', 'the', 'balance', 'of', 'centrifugal', 'and', 'gravitational', 'forces', 'and', 'whose', 'evolution', 'is', 'determined', 'by', 'its', 'magnetic', 'field', 'the', 'spinar', 'quasi', 'equilibrium', '... | [-0.13396847175360826, 0.1429119813542703, -0.08112107498588776, 0.1063656368117385, -0.07377544293418674, -0.06208969435191213, 0.005577192140291239, 0.34356587095727475, -0.23492257973968322, -0.3400812839167055, 0.033006318548941996, -0.24043458982910146, -0.08233334179371228, 0.1938135361337915, 0.00499483945967602... |
706.3192 | Hankel determinant and orthogonal polynomials for the Gaussian weight
with a jump | We obtain asymptotics in n for the n-dimensional Hankel determinant whose
symbol is the Gaussian multiplied by a step-like function. We use
Riemann-Hilbert analysis of the related system of orthogonal polynomials to
obtain our results.
| math.FA math-ph math.MP | we obtain asymptotics in n for the ndimensional hankel determinant whose symbol is the gaussian multiplied by a steplike function we use riemannhilbert analysis of the related system of orthogonal polynomials to obtain our results | [['we', 'obtain', 'asymptotics', 'in', 'n', 'for', 'the', 'ndimensional', 'hankel', 'determinant', 'whose', 'symbol', 'is', 'the', 'gaussian', 'multiplied', 'by', 'a', 'steplike', 'function', 'we', 'use', 'riemannhilbert', 'analysis', 'of', 'the', 'related', 'system', 'of', 'orthogonal', 'polynomials', 'to', 'obtain', ... | [-0.16403073317238262, 0.006600767546998603, -0.07841398492455483, 0.03815620573836246, -0.05012555194220373, -0.13465792157554202, -0.0074323263385200075, 0.3121035579858082, -0.25220814964600974, -0.18686006713126388, 0.14186479341172215, -0.2769643363143717, -0.2764174082516027, 0.1648847512235599, -0.04719893652945... |
706.3193 | Crossing the Wall: Branes vs. Bundles | We test a recently proposed wall-crossing formula for the change of the
Hilbert space of BPS states in d=4,N=2 theories. We study decays of D4D2D0
systems into pairs of D4D2D0 systems and we show how the wall-crossing formula
reproduces results of Goettsche and Yoshioka on wall-crossing behavior of the
moduli of slop... | hep-th | we test a recently proposed wallcrossing formula for the change of the hilbert space of bps states in d4n2 theories we study decays of d4d2d0 systems into pairs of d4d2d0 systems and we show how the wallcrossing formula reproduces results of goettsche and yoshioka on wallcrossing behavior of the moduli of slopestable h... | [['we', 'test', 'a', 'recently', 'proposed', 'wallcrossing', 'formula', 'for', 'the', 'change', 'of', 'the', 'hilbert', 'space', 'of', 'bps', 'states', 'in', 'd4n2', 'theories', 'we', 'study', 'decays', 'of', 'd4d2d0', 'systems', 'into', 'pairs', 'of', 'd4d2d0', 'systems', 'and', 'we', 'show', 'how', 'the', 'wallcrossi... | [-0.18288535019382834, 0.09506484669438864, -0.14955956459599584, 0.1492792638374708, -0.05203336435716507, -0.1163590675112137, 0.012245266759875884, 0.29196881071071734, -0.23661696305883326, -0.2274582143064804, 0.05601666928249727, -0.21791603204155388, -0.20987209504901255, 0.24476973687814288, -0.1437161071072063... |
706.3194 | Phase resolved spectroscopy of the Vela pulsar with XMM-Newton | The ~10^4 y old Vela Pulsar represents the bridge between the young Crab-like
and the middle-aged rotation powered pulsars. Its multiwavelength behaviour is
due to the superposition of different spectral components. We take advantage of
the unprecedented harvest of photons collected by XMM-Newton to assess the Vela
P... | astro-ph | the 104 y old vela pulsar represents the bridge between the young crablike and the middleaged rotation powered pulsars its multiwavelength behaviour is due to the superposition of different spectral components we take advantage of the unprecedented harvest of photons collected by xmmnewton to assess the vela pulsar spe... | [['the', '104', 'y', 'old', 'vela', 'pulsar', 'represents', 'the', 'bridge', 'between', 'the', 'young', 'crablike', 'and', 'the', 'middleaged', 'rotation', 'powered', 'pulsars', 'its', 'multiwavelength', 'behaviour', 'is', 'due', 'to', 'the', 'superposition', 'of', 'different', 'spectral', 'components', 'we', 'take', '... | [-0.1360636859921352, 0.17790596346471915, -0.08511945293899977, 0.06458227477994097, -0.1343270470998865, -0.11372927960781556, 0.0551082341606676, 0.39664405198627206, -0.23485781334621728, -0.3276817617709485, 0.04889912833898978, -0.3032198644247574, -0.0017696883538210729, 0.24125899884867358, -0.02105018364865209... |
706.3195 | Genetic Transferability of Anomalous Irradiation Alterations of
Antibiotic Activity | It previously has been discovered that visible light irradiation of
crystalline substrates can lead to enhancement of subsequent enzymatic reaction
rates as sharply peaked oscillatory functions of irradiation time. The
particular activating irradiation times can vary with source of a given enzyme
and thus, presumably... | q-bio.BM | it previously has been discovered that visible light irradiation of crystalline substrates can lead to enhancement of subsequent enzymatic reaction rates as sharply peaked oscillatory functions of irradiation time the particular activating irradiation times can vary with source of a given enzyme and thus presumably its... | [['it', 'previously', 'has', 'been', 'discovered', 'that', 'visible', 'light', 'irradiation', 'of', 'crystalline', 'substrates', 'can', 'lead', 'to', 'enhancement', 'of', 'subsequent', 'enzymatic', 'reaction', 'rates', 'as', 'sharply', 'peaked', 'oscillatory', 'functions', 'of', 'irradiation', 'time', 'the', 'particula... | [-0.09976718927481475, 0.20566990213643616, 0.005780354911109011, 0.006595926006833987, 0.025658725176870987, -0.18156790714042045, 0.07387877832609357, 0.37398571062071545, -0.24868113859376526, -0.29427548724828667, 0.037064217775802835, -0.2925086425725391, -0.14133676118731953, 0.2097039781240695, -0.03676277588672... |
706.3196 | Super Heavy Dark Matter and UHECR Anisotropy at Low Energy | Super Heavy quasi-stable particles are naturally produced in the early
universe and could represent a substantial fraction of the Dark Matter: the
so-called Super Heavy Dark Matter (SHDM). The decay of SHDM represents also a
possible source of Ultra High Energy Cosmic Rays (UHECR), with a reliably
calculated spectrum... | astro-ph | super heavy quasistable particles are naturally produced in the early universe and could represent a substantial fraction of the dark matter the socalled super heavy dark matter shdm the decay of shdm represents also a possible source of ultra high energy cosmic rays uhecr with a reliably calculated spectrum of the par... | [['super', 'heavy', 'quasistable', 'particles', 'are', 'naturally', 'produced', 'in', 'the', 'early', 'universe', 'and', 'could', 'represent', 'a', 'substantial', 'fraction', 'of', 'the', 'dark', 'matter', 'the', 'socalled', 'super', 'heavy', 'dark', 'matter', 'shdm', 'the', 'decay', 'of', 'shdm', 'represents', 'also',... | [-0.08492981755849102, 0.24413340813731213, -0.08799924786234724, 0.21011045881193774, -0.025018744857917573, -0.027865246468191517, -0.008656365462932093, 0.32718862976782537, -0.23449709616473008, -0.35509823129416024, -0.022221218386729216, -0.3474721620758546, -0.012234868992376944, 0.16293107323380637, 0.055857736... |
706.3197 | An HI study of three long-tailed irregular galaxies in the cluster
Abell1367 | We present the results on the distribution and kinematics of H$\sc{i}$ gas
with higher sensitivity and in one case of higher spectral resolution as well
than reported earlier, of three irregular galaxies CGCG 097073, 097079 and
097087 (UGC 06697) in the cluster Abell 1367. These galaxies are known to
exhibit long (50... | astro-ph | we present the results on the distribution and kinematics of hsci gas with higher sensitivity and in one case of higher spectral resolution as well than reported earlier of three irregular galaxies cgcg 097073 097079 and 097087 ugc 06697 in the cluster abell 1367 these galaxies are known to exhibit long 5075 kpc tails ... | [['we', 'present', 'the', 'results', 'on', 'the', 'distribution', 'and', 'kinematics', 'of', 'hsci', 'gas', 'with', 'higher', 'sensitivity', 'and', 'in', 'one', 'case', 'of', 'higher', 'spectral', 'resolution', 'as', 'well', 'than', 'reported', 'earlier', 'of', 'three', 'irregular', 'galaxies', 'cgcg', '097073', '09707... | [-0.04470172041824712, 0.07680903789746067, -0.047769388435302644, 0.0771092065187986, -0.06333917635955996, -0.06586554892022502, 0.002926093265572986, 0.459032242059369, -0.16904098519907249, -0.2934637355078435, 0.07806098244459876, -0.3246686305448582, -0.011428786683774722, 0.16728320979084607, 0.00090799510838802... |
706.3198 | Overspinning a nearly extreme charged black hole via a quantum tunneling
process | We examine a nearly extreme macroscopic Reissner-Nordstrom black hole in the
context of semi-classical gravity. The absorption rate associated with the
quantum tunneling process of scalar particles whereby this black hole can
acquire enough angular momentum to violate the weak cosmic censorship
conjecture is shown to... | gr-qc hep-th | we examine a nearly extreme macroscopic reissnernordstrom black hole in the context of semiclassical gravity the absorption rate associated with the quantum tunneling process of scalar particles whereby this black hole can acquire enough angular momentum to violate the weak cosmic censorship conjecture is shown to be n... | [['we', 'examine', 'a', 'nearly', 'extreme', 'macroscopic', 'reissnernordstrom', 'black', 'hole', 'in', 'the', 'context', 'of', 'semiclassical', 'gravity', 'the', 'absorption', 'rate', 'associated', 'with', 'the', 'quantum', 'tunneling', 'process', 'of', 'scalar', 'particles', 'whereby', 'this', 'black', 'hole', 'can',... | [-0.19748341115337098, 0.16539295737554008, -0.07162355546218653, 0.17643262614384034, -0.08325566134105127, -0.1874585910603249, -0.028278735917410813, 0.26054122031200677, -0.199152176171386, -0.28352936355319497, 0.0040993490620166995, -0.31325939382562257, -0.049096112294743456, 0.1511532556420813, -0.0716885481961... |
706.3199 | Scattering of twist fields from D-branes and orientifolds | We compute the two-point function for Z_N orbifold twist fields on the disk
and RP2. We apply this to a computation of the O(g_s) correction to the Kahler
potential for (the symmetric combination of) blow-up modes in type I string
theory on T^6/Z_3. This is related by supersymmetry to the one-loop field
dependent cor... | hep-th | we compute the twopoint function for z_n orbifold twist fields on the disk and rp2 we apply this to a computation of the og_s correction to the kahler potential for the symmetric combination of blowup modes in type i string theory on t6z_3 this is related by supersymmetry to the oneloop field dependent correction to th... | [['we', 'compute', 'the', 'twopoint', 'function', 'for', 'z_n', 'orbifold', 'twist', 'fields', 'on', 'the', 'disk', 'and', 'rp2', 'we', 'apply', 'this', 'to', 'a', 'computation', 'of', 'the', 'og_s', 'correction', 'to', 'the', 'kahler', 'potential', 'for', 'the', 'symmetric', 'combination', 'of', 'blowup', 'modes', 'in... | [-0.15174161781308343, 0.09943225351162255, -0.07264607159949436, 0.1345494581430496, -0.09728433851253342, -0.1345872939690142, 0.020043706482062367, 0.31928908847574444, -0.2446271066327353, -0.22198804600692884, 0.10395610264999591, -0.2576528747842924, -0.1469437127863686, 0.11339999277245354, -0.08431892367130982,... |
706.32 | Vortex generation in protoplanetary disks with an embedded giant planet | Vortices in protoplanetary disks can capture solid particles and form
planetary cores within shorter timescales than those involved in the standard
core-accretion model. We investigate vortex generation in thin unmagnetized
protoplanetary disks with an embedded giant planet with planet to star mass
ratio $10^{-4}$ an... | astro-ph | vortices in protoplanetary disks can capture solid particles and form planetary cores within shorter timescales than those involved in the standard coreaccretion model we investigate vortex generation in thin unmagnetized protoplanetary disks with an embedded giant planet with planet to star mass ratio 104 and 103 twod... | [['vortices', 'in', 'protoplanetary', 'disks', 'can', 'capture', 'solid', 'particles', 'and', 'form', 'planetary', 'cores', 'within', 'shorter', 'timescales', 'than', 'those', 'involved', 'in', 'the', 'standard', 'coreaccretion', 'model', 'we', 'investigate', 'vortex', 'generation', 'in', 'thin', 'unmagnetized', 'proto... | [-0.17854142022426742, 0.16389671916173876, -0.059808501163015206, 0.0409489832804594, -0.06693300790806483, -0.04734442217564915, -0.04262515868209173, 0.3500663418159542, -0.1997956813487458, -0.30608499918478094, 0.06792909120380196, -0.23846603632430116, -0.03747640949230088, 0.18955143486414905, -0.014793096147793... |
706.3201 | Volume Weighted Measures of Eternal Inflation in the Bousso-Polchinski
Landscape | We consider the cosmological dynamics associated with volume weighted
measures of eternal inflation, in the Bousso-Polchinski model of the string
theory landscape. We find that this measure predicts that observers are most
likely to find themselves in low energy vacua with one flux considerably larger
than the rest. ... | hep-th astro-ph gr-qc | we consider the cosmological dynamics associated with volume weighted measures of eternal inflation in the boussopolchinski model of the string theory landscape we find that this measure predicts that observers are most likely to find themselves in low energy vacua with one flux considerably larger than the rest furthe... | [['we', 'consider', 'the', 'cosmological', 'dynamics', 'associated', 'with', 'volume', 'weighted', 'measures', 'of', 'eternal', 'inflation', 'in', 'the', 'boussopolchinski', 'model', 'of', 'the', 'string', 'theory', 'landscape', 'we', 'find', 'that', 'this', 'measure', 'predicts', 'that', 'observers', 'are', 'most', 'l... | [-0.12510143042786595, 0.1826708305814712, -0.09494590263967838, 0.1373373179946919, -0.05677447394173083, -0.1554536547096406, 0.0615687061916943, 0.36414858121123406, -0.2156655669200616, -0.37384628012052756, 0.0954351346728747, -0.25989206083189687, -0.03786822332055877, 0.155380575333072, -0.06762999231699292, 0.0... |
706.3202 | Source Matching in the SDSS and RASS: Which Galaxies are Really X-ray
Sources? | The current view of galaxy formation holds that all massive galaxies harbor a
massive black hole at their center, but that these black holes are not always
in an actively accreting phase. X-ray emission is often used to identify
accreting sources, but for galaxies that are not harboring quasars
(low-luminosity active... | astro-ph | the current view of galaxy formation holds that all massive galaxies harbor a massive black hole at their center but that these black holes are not always in an actively accreting phase xray emission is often used to identify accreting sources but for galaxies that are not harboring quasars lowluminosity active galaxie... | [['the', 'current', 'view', 'of', 'galaxy', 'formation', 'holds', 'that', 'all', 'massive', 'galaxies', 'harbor', 'a', 'massive', 'black', 'hole', 'at', 'their', 'center', 'but', 'that', 'these', 'black', 'holes', 'are', 'not', 'always', 'in', 'an', 'actively', 'accreting', 'phase', 'xray', 'emission', 'is', 'often', '... | [-0.04350586355848678, 0.05524401296378257, -0.03906042870837939, 0.15621264201219243, -0.1595793044166142, -0.0636119437030737, 0.07997049141732109, 0.4463780242416524, -0.08785679189662471, -0.36550741179540525, 0.07591197352131246, -0.37664633885276805, -0.0022906453512210882, 0.236759468672694, -0.05571245071158268... |
706.3203 | Detecting Axion-Like Particles With Gamma Ray Telescopes | We propose that axion-like particles (ALPs) with a two-photon vertex,
consistent with all astrophysical and laboratory bounds, may lead to a
detectable signature in the spectra of high-energy gamma ray sources. This
occurs as a result of gamma rays being converted into ALPs in the magnetic
fields of efficient astroph... | hep-ph astro-ph | we propose that axionlike particles alps with a twophoton vertex consistent with all astrophysical and laboratory bounds may lead to a detectable signature in the spectra of highenergy gamma ray sources this occurs as a result of gamma rays being converted into alps in the magnetic fields of efficient astrophysical acc... | [['we', 'propose', 'that', 'axionlike', 'particles', 'alps', 'with', 'a', 'twophoton', 'vertex', 'consistent', 'with', 'all', 'astrophysical', 'and', 'laboratory', 'bounds', 'may', 'lead', 'to', 'a', 'detectable', 'signature', 'in', 'the', 'spectra', 'of', 'highenergy', 'gamma', 'ray', 'sources', 'this', 'occurs', 'as'... | [-0.08295949206344391, 0.2981671784675104, -0.04148205599110377, 0.17265183301642537, -0.11745819297962283, -0.07179278165200038, 0.03922631504798406, 0.3928406489522834, -0.20259848652701629, -0.3854608570078486, -0.009730589541753655, -0.2920946608052442, 0.016405103794348085, 0.280604773482896, 0.05572748941026236, ... |
706.3204 | Optimal purifications and fidelity for displaced thermal states | We evaluate the Uhlmann fidelity between two one-mode displaced thermal
states as the maximal probability transition between appropriate purifications
of the given states. The optimal purifications defining the fidelity are proved
to be two-mode displaced Gaussian states.
| quant-ph | we evaluate the uhlmann fidelity between two onemode displaced thermal states as the maximal probability transition between appropriate purifications of the given states the optimal purifications defining the fidelity are proved to be twomode displaced gaussian states | [['we', 'evaluate', 'the', 'uhlmann', 'fidelity', 'between', 'two', 'onemode', 'displaced', 'thermal', 'states', 'as', 'the', 'maximal', 'probability', 'transition', 'between', 'appropriate', 'purifications', 'of', 'the', 'given', 'states', 'the', 'optimal', 'purifications', 'defining', 'the', 'fidelity', 'are', 'prove... | [-0.13182508454003647, 0.2713454224018229, -0.07647071985175481, 0.09941249486763735, 0.06640133233992634, -0.21036044201134024, 0.10506263002753258, 0.37543156914211606, -0.246882637106889, -0.22883537454480254, 0.02565744290178692, -0.2901052960471527, -0.08136866886068035, 0.14798932381578395, -0.05141746136989143, ... |
706.3205 | Exact Solutions of the Isothermal Lane--Emden Equation with Rotation and
Implications for the Formation of Planets and Satellites | We have derived exact solutions of the isothermal Lane--Emden equation with
and without rotation in a cylindrical geometry. The corresponding hydrostatic
equilibria are most relevant to the dynamics of the protosolar nebula before
and during the stages of planet and satellite formation. The nonrotating
solution for t... | astro-ph | we have derived exact solutions of the isothermal laneemden equation with and without rotation in a cylindrical geometry the corresponding hydrostatic equilibria are most relevant to the dynamics of the protosolar nebula before and during the stages of planet and satellite formation the nonrotating solution for the mas... | [['we', 'have', 'derived', 'exact', 'solutions', 'of', 'the', 'isothermal', 'laneemden', 'equation', 'with', 'and', 'without', 'rotation', 'in', 'a', 'cylindrical', 'geometry', 'the', 'corresponding', 'hydrostatic', 'equilibria', 'are', 'most', 'relevant', 'to', 'the', 'dynamics', 'of', 'the', 'protosolar', 'nebula', '... | [-0.12206784709241213, 0.10691270333325154, -0.0862877118675798, 0.07147681477972372, -0.06460202522684148, -0.11411191335547166, 0.002974934702582997, 0.3469582308587337, -0.24399558142551345, -0.3085181247406863, 0.1635999178799057, -0.271187074007304, -0.07964119795699019, 0.17020977375750942, -0.02865538009814196, ... |
706.3206 | A Spectroscopic Study of Mass Outflows in the Interacting Binary RY
Scuti | The massive interacting binary RY Scuti is an important representative of an
active mass-transferring system that is changing before our eyes and which may
be an example of the formation of a Wolf-Rayet star through tidal stripping.
Utilizing new and previously published spectra, we present examples of how a
number o... | astro-ph | the massive interacting binary ry scuti is an important representative of an active masstransferring system that is changing before our eyes and which may be an example of the formation of a wolfrayet star through tidal stripping utilizing new and previously published spectra we present examples of how a number of illu... | [['the', 'massive', 'interacting', 'binary', 'ry', 'scuti', 'is', 'an', 'important', 'representative', 'of', 'an', 'active', 'masstransferring', 'system', 'that', 'is', 'changing', 'before', 'our', 'eyes', 'and', 'which', 'may', 'be', 'an', 'example', 'of', 'the', 'formation', 'of', 'a', 'wolfrayet', 'star', 'through',... | [-0.09882100860533469, 0.09810179603615524, -0.04444201655114586, 0.05768878736920623, -0.1108417311612861, -0.09979456616369929, 0.03503832148931952, 0.3673974575510076, -0.20679801751804702, -0.32512863114194457, 0.08232227338775366, -0.307884837647493, -0.08163560691931356, 0.1679338601363056, -0.048746113848462586,... |
706.3207 | Mirror symmetry and T-duality in the complement of an anticanonical
divisor | We study the geometry of complexified moduli spaces of special Lagrangian
submanifolds in the complement of an anticanonical divisor in a compact Kahler
manifold. In particular, we explore the connections between T-duality and
mirror symmetry in concrete examples, and show how quantum corrections arise in
this contex... | math.SG math.AG math.DG | we study the geometry of complexified moduli spaces of special lagrangian submanifolds in the complement of an anticanonical divisor in a compact kahler manifold in particular we explore the connections between tduality and mirror symmetry in concrete examples and show how quantum corrections arise in this context | [['we', 'study', 'the', 'geometry', 'of', 'complexified', 'moduli', 'spaces', 'of', 'special', 'lagrangian', 'submanifolds', 'in', 'the', 'complement', 'of', 'an', 'anticanonical', 'divisor', 'in', 'a', 'compact', 'kahler', 'manifold', 'in', 'particular', 'we', 'explore', 'the', 'connections', 'between', 'tduality', 'a... | [-0.216124245025059, 0.05892764819826822, -0.05844275316500917, 0.15179455763551386, -0.12246879709369325, -0.12049130285951368, -0.026093945387711235, 0.37040859730319775, -0.26869406878076335, -0.19789712535257034, 0.059690264288950315, -0.23688391065522235, -0.274955652337125, 0.1592606415456914, -0.2293825444190743... |
706.3208 | The chiral condensate in a constant electromagnetic field | We study the shift of the chiral condensate in a constant electromagnetic
field in the context of chiral perturbation theory. Using the Schwinger
proper-time formalism, we derive a one-loop expression correct to all orders in
$m_{\pi}^2 / eH$. Our result correctly reproduces a previously derived
``low-energy theorem'... | hep-ph | we study the shift of the chiral condensate in a constant electromagnetic field in the context of chiral perturbation theory using the schwinger propertime formalism we derive a oneloop expression correct to all orders in m_pi2 eh our result correctly reproduces a previously derived lowenergy theorem for m_pi 0 we show... | [['we', 'study', 'the', 'shift', 'of', 'the', 'chiral', 'condensate', 'in', 'a', 'constant', 'electromagnetic', 'field', 'in', 'the', 'context', 'of', 'chiral', 'perturbation', 'theory', 'using', 'the', 'schwinger', 'propertime', 'formalism', 'we', 'derive', 'a', 'oneloop', 'expression', 'correct', 'to', 'all', 'orders... | [-0.13884280379978986, 0.1306354251716867, -0.09530998134453382, 0.11135487727226079, -0.034498315889529195, -0.061524220836200134, 0.04421525217980115, 0.3325267667185609, -0.17537862156956074, -0.27848066088250456, 0.01192693751962746, -0.24207585084275537, -0.1263256994263903, 0.17101174345075645, -0.011132356468118... |
706.3209 | GRB060218 and GRBs associated with Supernovae Ib/c | We plan to fit the complete gamma- and X-ray light curves of the long
duration GRB060218, including the prompt emission, in order to clarify the
nature of the progenitors and the astrophysical scenario of the class of GRBs
associated to SNe Ib/c. The initial total energy of the electron-positron
plasma E_{e^\pm}^{tot... | astro-ph | we plan to fit the complete gamma and xray light curves of the long duration grb060218 including the prompt emission in order to clarify the nature of the progenitors and the astrophysical scenario of the class of grbs associated to sne ibc the initial total energy of the electronpositron plasma e_epmtot232times 1050 e... | [['we', 'plan', 'to', 'fit', 'the', 'complete', 'gamma', 'and', 'xray', 'light', 'curves', 'of', 'the', 'long', 'duration', 'grb060218', 'including', 'the', 'prompt', 'emission', 'in', 'order', 'to', 'clarify', 'the', 'nature', 'of', 'the', 'progenitors', 'and', 'the', 'astrophysical', 'scenario', 'of', 'the', 'class',... | [-0.0843622751075865, 0.1429514626615708, -0.06082417137981185, 0.16787231212334805, -0.07649185241912661, -0.07216012420044149, 0.05960091233709714, 0.3657742523011348, -0.1860820822038797, -0.3071116983974428, 0.048636127554581535, -0.30968979136596025, -0.02850958676292346, 0.19866997264005123, -0.009323920408897252... |
706.321 | Self-interaction correction with Wannier functions | We describe the behavior of the Perdew-Zunger self-interaction-corrected
local density approximation (SIC-LDA) functional when implemented in a
plane-wave pseudopotential formalism with Wannier functions. Prototypical
semiconductors and wide-bandgap oxides show a large overcorrection of the LDA
bandgap. Application t... | cond-mat.other | we describe the behavior of the perdewzunger selfinteractioncorrected local density approximation siclda functional when implemented in a planewave pseudopotential formalism with wannier functions prototypical semiconductors and widebandgap oxides show a large overcorrection of the lda bandgap application to transition... | [['we', 'describe', 'the', 'behavior', 'of', 'the', 'perdewzunger', 'selfinteractioncorrected', 'local', 'density', 'approximation', 'siclda', 'functional', 'when', 'implemented', 'in', 'a', 'planewave', 'pseudopotential', 'formalism', 'with', 'wannier', 'functions', 'prototypical', 'semiconductors', 'and', 'widebandga... | [-0.10392612112564562, 0.12120670162687969, -0.04542786137481807, 0.1176243380810458, -0.004391189156708803, -0.14862385586552, 0.055579158852038825, 0.4014935892318254, -0.21985101119777106, -0.2321685048164395, -0.0012304901535136869, -0.27603187685346475, -0.1510702942487905, 0.12153207645852766, 0.00855407599516658... |
706.3211 | Path probability density functions for semi-Markovian random walks | In random walks, the path representation of the Green's function is an
infinite sum over the length of path probability density functions (PDFs). Here
we derive and solve, in Laplace space, the recursion relation for the n order
path PDF for any arbitrarily inhomogeneous semi-Markovian random walk in a
one-dimensiona... | math-ph math.MP physics.bio-ph q-bio.OT | in random walks the path representation of the greens function is an infinite sum over the length of path probability density functions pdfs here we derive and solve in laplace space the recursion relation for the n order path pdf for any arbitrarily inhomogeneous semimarkovian random walk in a onedimensional 1d chain ... | [['in', 'random', 'walks', 'the', 'path', 'representation', 'of', 'the', 'greens', 'function', 'is', 'an', 'infinite', 'sum', 'over', 'the', 'length', 'of', 'path', 'probability', 'density', 'functions', 'pdfs', 'here', 'we', 'derive', 'and', 'solve', 'in', 'laplace', 'space', 'the', 'recursion', 'relation', 'for', 'th... | [-0.15645056044616337, 0.19100777544361855, -0.1529011090552168, 0.08883686497824134, -0.05984116497316531, -0.12996670021010295, 0.05450178986149175, 0.37542957328259946, -0.26320975982068506, -0.1954660535723503, 0.034000019818943523, -0.2785163523463, -0.1301900384016335, 0.1589099956310487, 0.0272275647843214, 0.11... |
706.3212 | Linear Stability of Closed Timelike Geodesics | The linear stability of closed timelike geodesics (CTGs) is analyzed in two
spacetimes with cylindrical sources, an infinite rotating dust cylinder, and a
cylindrical cloud of static cosmic strings with a central spinning string. We
also study the existence and linear stability of closed timelike curves in
spacetimes... | gr-qc | the linear stability of closed timelike geodesics ctgs is analyzed in two spacetimes with cylindrical sources an infinite rotating dust cylinder and a cylindrical cloud of static cosmic strings with a central spinning string we also study the existence and linear stability of closed timelike curves in spacetimes that s... | [['the', 'linear', 'stability', 'of', 'closed', 'timelike', 'geodesics', 'ctgs', 'is', 'analyzed', 'in', 'two', 'spacetimes', 'with', 'cylindrical', 'sources', 'an', 'infinite', 'rotating', 'dust', 'cylinder', 'and', 'a', 'cylindrical', 'cloud', 'of', 'static', 'cosmic', 'strings', 'with', 'a', 'central', 'spinning', '... | [-0.24551451646833009, 0.10400349753348642, -0.06803442226342296, 0.09441913985797475, -0.10677276145146099, -0.13449550546725753, -0.08428267900261187, 0.3210284985521788, -0.16121042872308403, -0.16717928241417612, 0.09873602574350693, -0.3054736128817963, -0.0583085147213311, 0.1478818005253811, -0.05288476804371483... |
706.3213 | A Spitzer IRAC Census of the Asymptotic Giant Branch Populations in
Local Group Dwarfs. II. IC 1613 | We present Spitzer Space Telescope IRAC photometry of the Local Group dwarf
irregular galaxy IC 1613. We compare our 3.6, 4.5, 5.8, and 8.0 micron
photometry with broadband optical photometry and find that the optical data do
not detect 43% and misidentify an additional 11% of the total AGB population,
likely because... | astro-ph | we present spitzer space telescope irac photometry of the local group dwarf irregular galaxy ic 1613 we compare our 36 45 58 and 80 micron photometry with broadband optical photometry and find that the optical data do not detect 43 and misidentify an additional 11 of the total agb population likely because of extinctio... | [['we', 'present', 'spitzer', 'space', 'telescope', 'irac', 'photometry', 'of', 'the', 'local', 'group', 'dwarf', 'irregular', 'galaxy', 'ic', '1613', 'we', 'compare', 'our', '36', '45', '58', 'and', '80', 'micron', 'photometry', 'with', 'broadband', 'optical', 'photometry', 'and', 'find', 'that', 'the', 'optical', 'da... | [-0.037945183767921505, 0.07621712935680279, -0.04778331674340113, 0.09552858114276626, -0.08740498725234008, -0.060259265333936524, 0.11698639631646163, 0.4800324221823092, -0.13130512357570184, -0.37388650314291805, 0.055961033173910595, -0.30518556327740776, -0.028055809594395503, 0.185473367174315, -0.1144585377542... |
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