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710.2753 | Effects of anharmonic vibration on large-angle quasi-elastic scattering
of 16O+144Sm | We study the effects of double octupole and quadrupole phonon excitations in
the 144Sm nucleus on quasi-elastic 16O+144Sm scattering at backward angles. To
this end, we use the coupled-channels framework, taking into account explicitly
the anharmonicities of the vibrations. We use the same coupling scheme as that
pre... | nucl-th | we study the effects of double octupole and quadrupole phonon excitations in the 144sm nucleus on quasielastic 16o144sm scattering at backward angles to this end we use the coupledchannels framework taking into account explicitly the anharmonicities of the vibrations we use the same coupling scheme as that previously e... | [['we', 'study', 'the', 'effects', 'of', 'double', 'octupole', 'and', 'quadrupole', 'phonon', 'excitations', 'in', 'the', '144sm', 'nucleus', 'on', 'quasielastic', '16o144sm', 'scattering', 'at', 'backward', 'angles', 'to', 'this', 'end', 'we', 'use', 'the', 'coupledchannels', 'framework', 'taking', 'into', 'account', ... | [-0.04655036579878715, 0.13233474792231106, -0.11425659520361219, 0.1453462973471568, -0.0018438105352467646, -0.07989418181806572, 0.04952260433784584, 0.3988514721230434, -0.24131411122307725, -0.23826218725447237, -0.05805220433432663, -0.3234964136075038, -0.07671987718093569, 0.16579846208439256, 0.036066702157462... |
710.2754 | A comparison between detailed and configuration-averaged
collisional-radiative codes applied to non-local thermal equilibrium plasma | A collisional-radiative model describing nonlocal-thermodynamic-equilibrium
plasmas is developed. It is based on the HULLAC (Hebrew University Lawrence
Livermore Atomic Code) suite for the transitions rates, in the zero-temperature
radiation field hypothesis. Two variants of the model are presented: the first
one is ... | physics.plasm-ph | a collisionalradiative model describing nonlocalthermodynamicequilibrium plasmas is developed it is based on the hullac hebrew university lawrence livermore atomic code suite for the transitions rates in the zerotemperature radiation field hypothesis two variants of the model are presented the first one is configuratio... | [['a', 'collisionalradiative', 'model', 'describing', 'nonlocalthermodynamicequilibrium', 'plasmas', 'is', 'developed', 'it', 'is', 'based', 'on', 'the', 'hullac', 'hebrew', 'university', 'lawrence', 'livermore', 'atomic', 'code', 'suite', 'for', 'the', 'transitions', 'rates', 'in', 'the', 'zerotemperature', 'radiation... | [-0.09576456714003252, 0.12359520898440722, -0.09705335949687008, 0.11438310883652061, -0.016548812355913087, -0.1504654063910112, 0.028518196666602068, 0.35928863785536347, -0.18752010766427943, -0.2835138031019422, 0.0657126385931896, -0.26146438683266054, -0.0678203451533629, 0.21999863819023985, -0.0022261193186646... |
710.2755 | Reduced branching processes with very heavy tails | The reduced Markov branching process is a stochastic model for the genealogy
of an unstructured biological population. Its limit behavior in the critical
case is well studied for the Zolotarev-Slack regularity parameter
$\alpha\in(0,1]$. We turn to the case of very heavy tailed reproduction
distribution $\alpha=0$ as... | math.PR | the reduced markov branching process is a stochastic model for the genealogy of an unstructured biological population its limit behavior in the critical case is well studied for the zolotarevslack regularity parameter alphain01 we turn to the case of very heavy tailed reproduction distribution alpha0 assuming zubkovs r... | [['the', 'reduced', 'markov', 'branching', 'process', 'is', 'a', 'stochastic', 'model', 'for', 'the', 'genealogy', 'of', 'an', 'unstructured', 'biological', 'population', 'its', 'limit', 'behavior', 'in', 'the', 'critical', 'case', 'is', 'well', 'studied', 'for', 'the', 'zolotarevslack', 'regularity', 'parameter', 'alp... | [-0.0980768222050269, 0.16503581018568325, -0.09302195337351779, 0.11220980495810681, -0.0510328688304609, -0.1162978793350114, 0.10045808943932955, 0.32974900147864517, -0.27758627342925946, -0.21963927629862873, 0.12996683689326205, -0.2327123392852102, -0.0700565450693625, 0.16979184478823042, -0.07420924150476783, ... |
710.2756 | From Holonomy of the Ising Model Form Factors to n-Fold Integrals and
the Theory of Elliptic Curve | We recall the form factors $ f^{(j)}_{N,N}$ corresponding to the
$\lambda$-extension $C(N,N; \lambda)$ of the two-point diagonal correlation
function of the Ising model on the square lattice and their associated linear
differential equations which exhibit both a ``Russian-doll'' nesting, and a
decomposition of the li... | math-ph cond-mat.stat-mech hep-th math.CA math.MP | we recall the form factors fj_nn corresponding to the lambdaextension cnn lambda of the twopoint diagonal correlation function of the ising model on the square lattice and their associated linear differential equations which exhibit both a russiandoll nesting and a decomposition of the linear differential operators as ... | [['we', 'recall', 'the', 'form', 'factors', 'fj_nn', 'corresponding', 'to', 'the', 'lambdaextension', 'cnn', 'lambda', 'of', 'the', 'twopoint', 'diagonal', 'correlation', 'function', 'of', 'the', 'ising', 'model', 'on', 'the', 'square', 'lattice', 'and', 'their', 'associated', 'linear', 'differential', 'equations', 'wh... | [-0.19428173731573206, 0.06853908734358027, -0.05486475004274222, 0.10149207674611196, -0.10563326600657881, -0.11916880196241557, -0.0027080434433084987, 0.2769941240607661, -0.3069917405399043, -0.2293829873010938, 0.10808317137533599, -0.3303126618383253, -0.14057119902803228, 0.1538107022965245, 0.02338121911955985... |
710.2757 | Future plan for observation of cosmic gamma rays in the 100 TeV energy
region with the Tibet air shower array : physics goal and overview | The Tibet air shower array, which has an effective area of 37,000 square
meters and is located at 4300 m in altitude, has been observing air showers
induced by cosmic rays with energies above a few TeV. We are planning to add a
large muon detector array to it for the purpose of increasing its sensitivity
to cosmic ga... | astro-ph | the tibet air shower array which has an effective area of 37000 square meters and is located at 4300 m in altitude has been observing air showers induced by cosmic rays with energies above a few tev we are planning to add a large muon detector array to it for the purpose of increasing its sensitivity to cosmic gamma ra... | [['the', 'tibet', 'air', 'shower', 'array', 'which', 'has', 'an', 'effective', 'area', 'of', '37000', 'square', 'meters', 'and', 'is', 'located', 'at', '4300', 'm', 'in', 'altitude', 'has', 'been', 'observing', 'air', 'showers', 'induced', 'by', 'cosmic', 'rays', 'with', 'energies', 'above', 'a', 'few', 'tev', 'we', 'a... | [-0.0736947102117789, 0.25341205202175443, -0.01973161103401696, 0.10761556699068442, -0.015674194288069168, 0.0002772568692082325, -0.013963832989730666, 0.4418472915360358, -0.21097013030399, -0.45753055891697914, 0.052121625487915185, -0.37901345831630506, 0.051932582335002656, 0.2219634529417463, 0.0616753958201703... |
710.2758 | The fundamental theorem of asset pricing under proportional transaction
costs | We extend the fundamental theorem of asset pricing to a model where the risky
stock is subject to proportional transaction costs in the form of bid-ask
spreads and the bank account has different interest rates for borrowing and
lending. We show that such a model is free of arbitrage if and only if one can
embed in it... | q-fin.PR math.PR | we extend the fundamental theorem of asset pricing to a model where the risky stock is subject to proportional transaction costs in the form of bidask spreads and the bank account has different interest rates for borrowing and lending we show that such a model is free of arbitrage if and only if one can embed in it a f... | [['we', 'extend', 'the', 'fundamental', 'theorem', 'of', 'asset', 'pricing', 'to', 'a', 'model', 'where', 'the', 'risky', 'stock', 'is', 'subject', 'to', 'proportional', 'transaction', 'costs', 'in', 'the', 'form', 'of', 'bidask', 'spreads', 'and', 'the', 'bank', 'account', 'has', 'different', 'interest', 'rates', 'for... | [-0.07803107900033909, 0.0950881164996933, -0.10692710838871212, 0.10773099943888866, -0.08802180011222911, -0.15859644773995457, 0.16419595662822448, 0.38023270723387237, -0.3234625824942912, -0.19808844004462406, 0.15500502736114602, -0.2673813248530212, -0.1382689985394103, 0.20552272040101632, -0.147742514813705, -... |
710.2759 | Structural anomalies, spin transitions and charge disproportionation in
LnCoO3 | The diamagnetic-paramagnetic and insulator-metal transitions in LnCoO3
perovskites (Ln = La, Y, rare earths) are reinterpreted and modeled as a
two-level excitation process. In distinction to previous models, the present
approach can be characterized as a LS-HS-IS (low-high-intermediate spin)
scenario. The first leve... | cond-mat.mtrl-sci | the diamagneticparamagnetic and insulatormetal transitions in lncoo3 perovskites ln la y rare earths are reinterpreted and modeled as a twolevel excitation process in distinction to previous models the present approach can be characterized as a lshsis lowhighintermediate spin scenario the first level is the local excit... | [['the', 'diamagneticparamagnetic', 'and', 'insulatormetal', 'transitions', 'in', 'lncoo3', 'perovskites', 'ln', 'la', 'y', 'rare', 'earths', 'are', 'reinterpreted', 'and', 'modeled', 'as', 'a', 'twolevel', 'excitation', 'process', 'in', 'distinction', 'to', 'previous', 'models', 'the', 'present', 'approach', 'can', 'b... | [-0.12012120633386075, 0.20281967133283615, -0.03321231994405389, 0.04920374547650863, 0.012900295631960034, -0.12550827484205365, 0.08004428454861044, 0.37360445711761714, -0.2665396349281073, -0.2727494805455208, 0.03120850556436926, -0.34353463268280027, -0.07591462979465723, 0.1280325227715075, 0.05006763198040426,... |
710.276 | A quantitative study of quasiparticle traps using the
single-Cooper-pair-transistor | We use radio-frequency reflectometry to measure quasiparticle tunneling rates
in the single-Cooper-pair-transistor. Devices with and without quasiparticle
traps in proximity to the island are studied. A $10^2$ to $10^3$-fold reduction
in the quasiparticle tunneling rate onto the island is observed in the case of
quas... | cond-mat.supr-con cond-mat.mes-hall | we use radiofrequency reflectometry to measure quasiparticle tunneling rates in the singlecooperpairtransistor devices with and without quasiparticle traps in proximity to the island are studied a 102 to 103fold reduction in the quasiparticle tunneling rate onto the island is observed in the case of quasiparticle traps... | [['we', 'use', 'radiofrequency', 'reflectometry', 'to', 'measure', 'quasiparticle', 'tunneling', 'rates', 'in', 'the', 'singlecooperpairtransistor', 'devices', 'with', 'and', 'without', 'quasiparticle', 'traps', 'in', 'proximity', 'to', 'the', 'island', 'are', 'studied', 'a', '102', 'to', '103fold', 'reduction', 'in', ... | [-0.15886415829438538, 0.20910413702210737, -0.0726411057310918, 0.11805507075965464, 0.05231294189653699, -0.12921757287981492, 0.2020507806705104, 0.37173855860554983, -0.20449740964446275, -0.26132323575161753, -0.052021446900205714, -0.37033847639603273, -0.04603855915012814, 0.1870473191319477, -0.0449337034471451... |
710.2761 | VLT-VIMOS integral field spectroscopy of luminous and ultraluminous
infrared galaxies. I. The sample and first results | (Ultra)Luminous Infrared Galaxies [(U)LIRGs] are much more numerous at
cosmological distances than locally, and are likely precursors of elliptical
galaxies. Our goal is to carry out an integral field spectroscopic survey of a
representative sample of low redshift (z < 0.26) (U)LIRGs, covering different
morphologies ... | astro-ph | ultraluminous infrared galaxies ulirgs are much more numerous at cosmological distances than locally and are likely precursors of elliptical galaxies our goal is to carry out an integral field spectroscopic survey of a representative sample of low redshift z 026 ulirgs covering different morphologies from spirals to me... | [['ultraluminous', 'infrared', 'galaxies', 'ulirgs', 'are', 'much', 'more', 'numerous', 'at', 'cosmological', 'distances', 'than', 'locally', 'and', 'are', 'likely', 'precursors', 'of', 'elliptical', 'galaxies', 'our', 'goal', 'is', 'to', 'carry', 'out', 'an', 'integral', 'field', 'spectroscopic', 'survey', 'of', 'a', ... | [-0.09788635851610011, 0.0943370550224882, -0.05531862890806166, 0.06267043290701951, -0.034579509443889454, -0.06079027307307802, -0.013426882865670042, 0.4371201531066904, -0.1369823207721246, -0.30001887689366585, 0.06223087441762836, -0.31306174861296543, -0.022277019039808412, 0.18051855594623745, 0.03425687227093... |
710.2762 | Valence and spin states in perovskites LaCo0.95M0.05O3 (M = Mg, Ga, Ti) | The samples LaCoO3 with dilute substitutions on cobalt sites have been
studied using the resistivity, thermopower and magnetic susceptibility
measurements over the temperature range up to ~900 K. The Co-site substitution
does not affect the magnetic transition at ~100 K and the onset of massive
population of hole car... | cond-mat.mtrl-sci | the samples lacoo3 with dilute substitutions on cobalt sites have been studied using the resistivity thermopower and magnetic susceptibility measurements over the temperature range up to 900 k the cosite substitution does not affect the magnetic transition at 100 k and the onset of massive population of hole carriers a... | [['the', 'samples', 'lacoo3', 'with', 'dilute', 'substitutions', 'on', 'cobalt', 'sites', 'have', 'been', 'studied', 'using', 'the', 'resistivity', 'thermopower', 'and', 'magnetic', 'susceptibility', 'measurements', 'over', 'the', 'temperature', 'range', 'up', 'to', '900', 'k', 'the', 'cosite', 'substitution', 'does', ... | [-0.10460040222775811, 0.26812635248837374, 0.07134557594157134, -0.0021605091586631413, 0.02646125179308001, -0.18252002562318617, 0.1322326904395595, 0.4063502087568243, -0.22097508843968777, -0.3503883203986334, -0.026203766150865705, -0.4543622962664813, 0.0027246115379966794, 0.1418292652912593, 0.0666955128855382... |
710.2763 | Threefolds with big and nef anticanonical bundles II | In continuation of our paper in Math. Ann. 333 we classify smooth complex
projective threefolds X with -K_X big and nef but not ample and Picard number
2, whose anticanonical map is small. We assume also that the Mori contraction
of X and of its flop are not both birational.
| math.AG | in continuation of our paper in math ann 333 we classify smooth complex projective threefolds x with k_x big and nef but not ample and picard number 2 whose anticanonical map is small we assume also that the mori contraction of x and of its flop are not both birational | [['in', 'continuation', 'of', 'our', 'paper', 'in', 'math', 'ann', '333', 'we', 'classify', 'smooth', 'complex', 'projective', 'threefolds', 'x', 'with', 'k_x', 'big', 'and', 'nef', 'but', 'not', 'ample', 'and', 'picard', 'number', '2', 'whose', 'anticanonical', 'map', 'is', 'small', 'we', 'assume', 'also', 'that', 'th... | [-0.14852286542300136, -0.002851395234465599, -0.028868508953601123, 0.037038721714634446, -0.09692643117159605, -0.21407413962297142, 0.01996542825596407, 0.40951457304880023, -0.3156335652898997, -0.1802629943192005, 0.09064651801483706, -0.2615110003389418, -0.18778987298719585, 0.1926820918172598, -0.23951525002717... |
710.2764 | On the Equivalent Theory of the Generalized \tau^{(2)}-model and the
Chiral Potts Model with two Alternating Vertical Rapidities | By the Baxter's $Q_{72}$-operator method, we demonstrate the equivalent
theory between the generalized $\tau^{(2)}$-model (other than two special cases
with a pseudovacuum state) and the $N$-state chiral Potts model with two
alternating vertical rapidities, where the degenerate models are included. As a
consequence, ... | cond-mat.stat-mech hep-th math-ph math.AG math.MP nlin.SI | by the baxters q_72operator method we demonstrate the equivalent theory between the generalized tau2model other than two special cases with a pseudovacuum state and the nstate chiral potts model with two alternating vertical rapidities where the degenerate models are included as a consequence the theory of the xxz chai... | [['by', 'the', 'baxters', 'q_72operator', 'method', 'we', 'demonstrate', 'the', 'equivalent', 'theory', 'between', 'the', 'generalized', 'tau2model', 'other', 'than', 'two', 'special', 'cases', 'with', 'a', 'pseudovacuum', 'state', 'and', 'the', 'nstate', 'chiral', 'potts', 'model', 'with', 'two', 'alternating', 'verti... | [-0.13239163278650715, 0.19044110252184848, -0.0011550744912072794, 0.07372312874397707, -0.033889071791738605, -0.23171092847139754, -0.02639469521210543, 0.33122684158829613, -0.24408371635684883, -0.24547726700235326, 0.06151469246616392, -0.3075558516255983, -0.11832686217237653, 0.1272037233340679, 0.0883159419632... |
710.2765 | Note on the existence theorem in ``Emergent Quantum Mechanics and
Emergent Symmetries'' | Recently 't Hooft demonstrated that ``For any quantum system there exists at
least one deterministic model that reproduces all its dynamics after
prequantization''. An extension is presented here which covers quantum systems
that are characterized by a complete set of mutually commuting Hermitian
operators (``beables... | quant-ph gr-qc hep-th | recently t hooft demonstrated that for any quantum system there exists at least one deterministic model that reproduces all its dynamics after prequantization an extension is presented here which covers quantum systems that are characterized by a complete set of mutually commuting hermitian operators beables we introdu... | [['recently', 't', 'hooft', 'demonstrated', 'that', 'for', 'any', 'quantum', 'system', 'there', 'exists', 'at', 'least', 'one', 'deterministic', 'model', 'that', 'reproduces', 'all', 'its', 'dynamics', 'after', 'prequantization', 'an', 'extension', 'is', 'presented', 'here', 'which', 'covers', 'quantum', 'systems', 'th... | [-0.15632676429532724, 0.1423022273722444, -0.07560073751715365, 0.05503456121017546, -0.06428213005259248, -0.17242022173013538, -0.006640143566042313, 0.3189192720977911, -0.2474528339627231, -0.25680003946261676, 0.09664724309374739, -0.24889842613503851, -0.14916638000707688, 0.17089869938028077, -0.038497783606952... |
710.2766 | Thermodynamic properties of Holstein polarons and the effects of
disorder | The ground state and finite temperature properties of polarons are studied
considering a two-site and a four-site Holstein model by exact diagonalization
of the Hamiltonian. The kinetic energy, Drude weight, correlation functions
involving charge and lattice deformations, and the specific heat have been
evaluated as ... | cond-mat.str-el | the ground state and finite temperature properties of polarons are studied considering a twosite and a foursite holstein model by exact diagonalization of the hamiltonian the kinetic energy drude weight correlation functions involving charge and lattice deformations and the specific heat have been evaluated as a functi... | [['the', 'ground', 'state', 'and', 'finite', 'temperature', 'properties', 'of', 'polarons', 'are', 'studied', 'considering', 'a', 'twosite', 'and', 'a', 'foursite', 'holstein', 'model', 'by', 'exact', 'diagonalization', 'of', 'the', 'hamiltonian', 'the', 'kinetic', 'energy', 'drude', 'weight', 'correlation', 'functions... | [-0.15109234801819846, 0.2202642886086729, -0.014297872864801412, 0.09650389249154788, -0.015583862924272088, -0.1261767300978825, 0.05903752906853037, 0.3573951670176284, -0.2868652752226895, -0.23198131236965489, -0.010005312606953322, -0.313362827405903, -0.07086491682952281, 0.1231521634180336, 0.11127144671608782,... |
710.2767 | Irreducible polynomials with prescribed trace and restricted norm | Let GF(q), q=p^r, be a finite field with a primitive element g. In this paper
we use exponential sums and Jacobi sums to compute the number of the
irreducible polynomials of degree m over GF(q) with trace fixed and norm
restricted to a coset of a subgroup <g^s>, s|(q-1). We give the number
explicitly for s=2, 3, 4 wh... | math.NT | let gfq qpr be a finite field with a primitive element g in this paper we use exponential sums and jacobi sums to compute the number of the irreducible polynomials of degree m over gfq with trace fixed and norm restricted to a coset of a subgroup gs sq1 we give the number explicitly for s2 3 4 when qp and for spe1 when... | [['let', 'gfq', 'qpr', 'be', 'a', 'finite', 'field', 'with', 'a', 'primitive', 'element', 'g', 'in', 'this', 'paper', 'we', 'use', 'exponential', 'sums', 'and', 'jacobi', 'sums', 'to', 'compute', 'the', 'number', 'of', 'the', 'irreducible', 'polynomials', 'of', 'degree', 'm', 'over', 'gfq', 'with', 'trace', 'fixed', 'a... | [-0.18914858288154368, 0.13234896340207608, -0.036413568850725934, 0.025393095081842437, -0.05678980785603749, -0.14910891821335365, 0.014860651514027268, 0.3427707688860232, -0.3013614172842808, -0.27363831827008145, 0.12309164523073222, -0.24991420940950332, -0.09655292298099617, 0.1867588193967893, -0.06766098226908... |
710.2768 | On a problem of Juhasz and van Mill | A 27 years old and still open problem of Juhasz and van Mill asks whether
there exists a cardinal kappa such that every regular dense in itself countably
compact space has a dense in itself subset of cardinality at most kappa. We
give a negative answer for the analogous question where_regular_ is weakened
to_Hausdorf... | math.GN | a 27 years old and still open problem of juhasz and van mill asks whether there exists a cardinal kappa such that every regular dense in itself countably compact space has a dense in itself subset of cardinality at most kappa we give a negative answer for the analogous question where_regular_ is weakened to_hausdorff_ ... | [['a', '27', 'years', 'old', 'and', 'still', 'open', 'problem', 'of', 'juhasz', 'and', 'van', 'mill', 'asks', 'whether', 'there', 'exists', 'a', 'cardinal', 'kappa', 'such', 'that', 'every', 'regular', 'dense', 'in', 'itself', 'countably', 'compact', 'space', 'has', 'a', 'dense', 'in', 'itself', 'subset', 'of', 'cardin... | [-0.18334740361509225, 0.15568914774943282, -0.07498844279217776, 0.1113328673850952, -0.11044020112603903, -0.18505183503859574, 0.09691600594885165, 0.336118786190464, -0.2944512980821956, -0.2046936923224065, 0.11492016246214647, -0.30398940084786674, -0.1118036827624396, 0.20997341318676868, -0.131439232258816, -0.... |
710.2769 | Renormalization of the vacuum angle in quantum mechanics, Berry phase
and continuous measurements | The vacuum angle $\theta$ renormalization is studied for a toy model of a
quantum particle moving around a ring, threaded by a magnetic flux $\theta$.
Different renormalization group (RG) procedures lead to the same generic RG
flow diagram, similar to that of the quantum Hall effect. We argue that the
renormalized va... | hep-th cond-mat.mes-hall | the vacuum angle theta renormalization is studied for a toy model of a quantum particle moving around a ring threaded by a magnetic flux theta different renormalization group rg procedures lead to the same generic rg flow diagram similar to that of the quantum hall effect we argue that the renormalized value of the vac... | [['the', 'vacuum', 'angle', 'theta', 'renormalization', 'is', 'studied', 'for', 'a', 'toy', 'model', 'of', 'a', 'quantum', 'particle', 'moving', 'around', 'a', 'ring', 'threaded', 'by', 'a', 'magnetic', 'flux', 'theta', 'different', 'renormalization', 'group', 'rg', 'procedures', 'lead', 'to', 'the', 'same', 'generic',... | [-0.19855190225077413, 0.2437289352405124, -0.12088157559654354, 0.041685938505472336, -0.06097255918337444, -0.1732642465493584, 0.012194101559358806, 0.3421264235012695, -0.2870410346071673, -0.2832992325611083, 0.062179472541593145, -0.2379690669476986, -0.0740076672013816, 0.15254847538983038, -0.03250073315987809,... |
710.277 | Renormalizing the Schrodinger Equation for NN scattering | The renormalization of the Schr"odinger equation with regular One Boson
Exchange and singular chiral potentials including One and Two-Pion exchanges is
analyzed within the context of NN scattering.
| nucl-th | the renormalization of the schrodinger equation with regular one boson exchange and singular chiral potentials including one and twopion exchanges is analyzed within the context of nn scattering | [['the', 'renormalization', 'of', 'the', 'schrodinger', 'equation', 'with', 'regular', 'one', 'boson', 'exchange', 'and', 'singular', 'chiral', 'potentials', 'including', 'one', 'and', 'twopion', 'exchanges', 'is', 'analyzed', 'within', 'the', 'context', 'of', 'nn', 'scattering']] | [-0.15710297147078173, 0.18617753272077867, -0.09074024756305984, 0.1184059402980243, -0.039779130568993945, -0.19889410059633, -0.049001717806926796, 0.2859759280192001, -0.2579895320148872, -0.14906854794493743, 0.00903872327346887, -0.4300821500032076, -0.0928916500415653, 0.08298843360639044, 0.17296408245705866, 0... |
710.2771 | Hard exclusive scattering at Jlab | The various factorization schemes for hard exclusive processes and the status
of their applications is briefly reviewed.
| hep-ph | the various factorization schemes for hard exclusive processes and the status of their applications is briefly reviewed | [['the', 'various', 'factorization', 'schemes', 'for', 'hard', 'exclusive', 'processes', 'and', 'the', 'status', 'of', 'their', 'applications', 'is', 'briefly', 'reviewed']] | [-0.10070622821941096, 0.15492245313875816, -0.06234886491780772, 0.19606754274847096, -0.05478721353061059, -0.12776882190476446, 0.038677333141951, 0.4550396098810084, -0.28529080156894293, -0.13818662525976405, 0.21922882602495306, -0.2487731470781214, -0.12459516388309352, 0.19159463661558487, 0.008168907562161194,... |
710.2772 | Significant g-factor values of a two-electron ground state in quantum
dots with spin-orbit coupling | The magnetization of semiconductor quantum dots in the presence of spin-orbit
coupling and interactions is investigated numerically. When the dot is occupied
by two electrons we find that a level crossing between the two lowest many-body
eigenstates may occur as a function of the spin-orbit coupling strength. This
le... | cond-mat.str-el cond-mat.mes-hall | the magnetization of semiconductor quantum dots in the presence of spinorbit coupling and interactions is investigated numerically when the dot is occupied by two electrons we find that a level crossing between the two lowest manybody eigenstates may occur as a function of the spinorbit coupling strength this level cro... | [['the', 'magnetization', 'of', 'semiconductor', 'quantum', 'dots', 'in', 'the', 'presence', 'of', 'spinorbit', 'coupling', 'and', 'interactions', 'is', 'investigated', 'numerically', 'when', 'the', 'dot', 'is', 'occupied', 'by', 'two', 'electrons', 'we', 'find', 'that', 'a', 'level', 'crossing', 'between', 'the', 'two... | [-0.20325573030227828, 0.2117397784448073, -0.03454286454075758, 0.05840022862253521, -0.011260694427557795, -0.12490604382197736, 0.05018130069602502, 0.36190289603072706, -0.25892676443050977, -0.3496605483420446, 0.0038621749450705187, -0.28616725823889344, -0.16953538710219881, 0.15930099506720397, 0.07036830358388... |
710.2773 | Ramond-Ramond Fields, Fractional Branes and Orbifold Differential
K-Theory | We study D-branes and Ramond-Ramond fields on global orbifolds of Type II
string theory with vanishing H-flux using methods of equivariant K-theory and
K-homology. We illustrate how Bredon equivariant cohomology naturally realizes
stringy orbifold cohomology. We emphasize its role as the correct cohomological
tool wh... | hep-th math.KT | we study dbranes and ramondramond fields on global orbifolds of type ii string theory with vanishing hflux using methods of equivariant ktheory and khomology we illustrate how bredon equivariant cohomology naturally realizes stringy orbifold cohomology we emphasize its role as the correct cohomological tool which captu... | [['we', 'study', 'dbranes', 'and', 'ramondramond', 'fields', 'on', 'global', 'orbifolds', 'of', 'type', 'ii', 'string', 'theory', 'with', 'vanishing', 'hflux', 'using', 'methods', 'of', 'equivariant', 'ktheory', 'and', 'khomology', 'we', 'illustrate', 'how', 'bredon', 'equivariant', 'cohomology', 'naturally', 'realizes... | [-0.2054723338301604, 0.049361850499311306, -0.0977935742509241, 0.21326953374858323, -0.1522619630889191, -0.20246131499685968, -0.0002605316248567154, 0.31538988189810574, -0.2596732507440417, -0.24367784732700482, 0.04005572827688108, -0.1968916200698004, -0.2046269091583478, 0.14212456975947135, -0.2626364851991336... |
710.2774 | Final state interaction and \Delta I=1/2 rule | Contrary to wide-spread opinion that the final state interaction (FSI)
enhances the amplitude <2\pi;I=0|K^0>, we argue that FSI does not increase the
absolute value of this amplitude.
| hep-ph | contrary to widespread opinion that the final state interaction fsi enhances the amplitude 2pii0k0 we argue that fsi does not increase the absolute value of this amplitude | [['contrary', 'to', 'widespread', 'opinion', 'that', 'the', 'final', 'state', 'interaction', 'fsi', 'enhances', 'the', 'amplitude', '2pii0k0', 'we', 'argue', 'that', 'fsi', 'does', 'not', 'increase', 'the', 'absolute', 'value', 'of', 'this', 'amplitude']] | [-0.13694209426354903, 0.16274008459339923, -0.10788702602999714, 0.06081446960049037, -0.1273130250091736, -0.06172083167789074, 0.052763821163143106, 0.3669574696284074, -0.22602563279752547, -0.23222268759631193, 0.017047731975953166, -0.27067659250818765, -0.11971429276924866, 0.06960352101864722, -0.05704380220805... |
710.2775 | Dam Rain and Cumulative Gain | We consider a financial contract that delivers a single cash flow given by
the terminal value of a cumulative gains process. The problem of modelling and
pricing such an asset and associated derivatives is important, for example, in
the determination of optimal insurance claims reserve policies, and in the
pricing of... | q-fin.PR math.PR | we consider a financial contract that delivers a single cash flow given by the terminal value of a cumulative gains process the problem of modelling and pricing such an asset and associated derivatives is important for example in the determination of optimal insurance claims reserve policies and in the pricing of reins... | [['we', 'consider', 'a', 'financial', 'contract', 'that', 'delivers', 'a', 'single', 'cash', 'flow', 'given', 'by', 'the', 'terminal', 'value', 'of', 'a', 'cumulative', 'gains', 'process', 'the', 'problem', 'of', 'modelling', 'and', 'pricing', 'such', 'an', 'asset', 'and', 'associated', 'derivatives', 'is', 'important'... | [-0.11766840796458897, -0.005873250091170864, -0.0853011412557508, 0.11101913879175465, -0.07357240090229242, -0.07184726278311367, 0.14339993657828698, 0.39096736737292975, -0.27699158108091265, -0.24288322096644657, 0.18016251764062957, -0.2933059083366666, -0.09331543570421086, 0.22711367452181097, -0.13914301299737... |
710.2776 | New constraints on the membership of the T dwarf S Ori 70 in the sigma
Orionis cluster | (Abridged) The nature of S Ori 70, a faint mid-T type object found towards
the direction of the young sigma Orionis cluster, is still under debate. We
intend to disentangle whether it is a field brown dwarf or a 3-Myr old
planetary-mass member of the cluster. We report on near-infrared JHK_s and
mid-infrared [3.6] an... | astro-ph | abridged the nature of s ori 70 a faint midt type object found towards the direction of the young sigma orionis cluster is still under debate we intend to disentangle whether it is a field brown dwarf or a 3myr old planetarymass member of the cluster we report on nearinfrared jhk_s and midinfrared 36 and 45 iracspitzer... | [['abridged', 'the', 'nature', 'of', 's', 'ori', '70', 'a', 'faint', 'midt', 'type', 'object', 'found', 'towards', 'the', 'direction', 'of', 'the', 'young', 'sigma', 'orionis', 'cluster', 'is', 'still', 'under', 'debate', 'we', 'intend', 'to', 'disentangle', 'whether', 'it', 'is', 'a', 'field', 'brown', 'dwarf', 'or', ... | [-0.040352607061239804, 0.11348107408845651, -0.10073740808105078, 0.0601788547390959, -0.15520094367064008, -0.10294367915790792, 0.12422449915667506, 0.40656542794007544, -0.17175810343545928, -0.3803084969021982, 0.05512253329336568, -0.26208168595166165, -0.018503252331742482, 0.16151293205047929, -0.13435220110522... |
710.2777 | Teleportation of two-mode squeezed states | We consider two-mode squeezed states which are parametrized by the squeezing
parameter and the phase. We present a scheme for teleporting such entangled
states of continuous variables from Alice to Bob. Our protocol is
operationalized through the creation of a four-mode entangled state shared by
Alice and Bob using l... | quant-ph | we consider twomode squeezed states which are parametrized by the squeezing parameter and the phase we present a scheme for teleporting such entangled states of continuous variables from alice to bob our protocol is operationalized through the creation of a fourmode entangled state shared by alice and bob using linear ... | [['we', 'consider', 'twomode', 'squeezed', 'states', 'which', 'are', 'parametrized', 'by', 'the', 'squeezing', 'parameter', 'and', 'the', 'phase', 'we', 'present', 'a', 'scheme', 'for', 'teleporting', 'such', 'entangled', 'states', 'of', 'continuous', 'variables', 'from', 'alice', 'to', 'bob', 'our', 'protocol', 'is', ... | [-0.1810024186408007, 0.2538662776350975, -0.12892739775074866, -0.022216109649693814, 0.07805595785299296, -0.2891787361724162, 0.1247596161675349, 0.37415878910330996, -0.26957143751043144, -0.2717456615940538, 0.024208854514634816, -0.27389589798266206, -0.038071861210209064, 0.17005251008536545, -0.0379675421012585... |
710.2778 | Determining the crystal-field ground state in rare earth Heavy Fermion
materials using soft-x-ray absorption spectroscopy | We infer that soft-x-ray absorption spectroscopy is a versatile method for
the determination of the crystal-field ground state symmetry of rare earth
Heavy Fermion systems, complementing neutron scattering. Using realistic and
universal parameters, we provide a theoretical mapping between the polarization
dependence ... | cond-mat.str-el | we infer that softxray absorption spectroscopy is a versatile method for the determination of the crystalfield ground state symmetry of rare earth heavy fermion systems complementing neutron scattering using realistic and universal parameters we provide a theoretical mapping between the polarization dependence of ce m_... | [['we', 'infer', 'that', 'softxray', 'absorption', 'spectroscopy', 'is', 'a', 'versatile', 'method', 'for', 'the', 'determination', 'of', 'the', 'crystalfield', 'ground', 'state', 'symmetry', 'of', 'rare', 'earth', 'heavy', 'fermion', 'systems', 'complementing', 'neutron', 'scattering', 'using', 'realistic', 'and', 'un... | [-0.1125927091849482, 0.16851672537908916, -0.05624621033506549, 0.09148543065985786, -0.05176770126285112, -0.08512475131504724, 0.09800034679938108, 0.3763365718819525, -0.2498974311367973, -0.32272286229240504, -0.013612060681106928, -0.3341246525068646, -0.02107238015362426, 0.16523046238833797, 0.0756523378962732,... |
710.2779 | Quantum degenerate two-species Fermi-Fermi mixture coexisting with a
Bose-Einstein condensate | We report on the generation of a quantum degenerate Fermi-Fermi mixture of
two different atomic species. The quantum degenerate mixture is realized
employing sympathetic cooling of fermionic Li-6 and K-40 gases by an
evaporatively cooled bosonic Rb-87 gas. We describe the combination of trapping
and cooling methods t... | cond-mat.other | we report on the generation of a quantum degenerate fermifermi mixture of two different atomic species the quantum degenerate mixture is realized employing sympathetic cooling of fermionic li6 and k40 gases by an evaporatively cooled bosonic rb87 gas we describe the combination of trapping and cooling methods that prov... | [['we', 'report', 'on', 'the', 'generation', 'of', 'a', 'quantum', 'degenerate', 'fermifermi', 'mixture', 'of', 'two', 'different', 'atomic', 'species', 'the', 'quantum', 'degenerate', 'mixture', 'is', 'realized', 'employing', 'sympathetic', 'cooling', 'of', 'fermionic', 'li6', 'and', 'k40', 'gases', 'by', 'an', 'evapo... | [-0.07077469906034535, 0.26659634296702567, 0.0052910852044322125, -0.01584126780766755, 0.06277071143405175, -0.1452755490977933, 0.07457627665698821, 0.34563345025022196, -0.2351662635099231, -0.26662688175817645, 0.037926924010687396, -0.24651432461215286, -0.01744592110223071, 0.21570988798763338, 0.031843105353063... |
710.278 | The Optical Gravitational Lensing Experiment. Period-Luminosity
Relations of Variable Red Giant Stars | Period-luminosity (PL) relations of variable red giants in the Large (LMC)
and Small Magellanic Clouds (SMC) are presented. The PL diagrams are plotted in
three planes: logP-K_S, logP-W_{JK}, and logP-W_I. Fourteen PL sequences are
distinguishable, and some of them consist of three closely spaced ridges. Each
of the ... | astro-ph | periodluminosity pl relations of variable red giants in the large lmc and small magellanic clouds smc are presented the pl diagrams are plotted in three planes logpk_s logpw_jk and logpw_i fourteen pl sequences are distinguishable and some of them consist of three closely spaced ridges each of the sequences is fitted w... | [['periodluminosity', 'pl', 'relations', 'of', 'variable', 'red', 'giants', 'in', 'the', 'large', 'lmc', 'and', 'small', 'magellanic', 'clouds', 'smc', 'are', 'presented', 'the', 'pl', 'diagrams', 'are', 'plotted', 'in', 'three', 'planes', 'logpk_s', 'logpw_jk', 'and', 'logpw_i', 'fourteen', 'pl', 'sequences', 'are', '... | [-0.11298915540205322, 0.15977404127278202, -0.11960680596316592, 0.15469991965603258, -0.10319587666754974, -0.11294347416662935, 0.10194429581213782, 0.43798739962466726, -0.2072346609846879, -0.3434184505220329, 0.014372615409450852, -0.28599798030534584, -0.0848829296991683, 0.2342832634649084, -0.10003316695017467... |
710.2781 | Rhombus Filtrations and Rauzy Algebras | Peach introduced rhombal algebras associated to quivers given by tilings of
the plane by rhombi. We develop general techniques to analyse rhombal algebras,
including a filtration by what we call rhombus modules.
We introduce a way to relate the infinite-dimensional rhombal algebra
corresponding to a complete tiling... | math.RT math.DS | peach introduced rhombal algebras associated to quivers given by tilings of the plane by rhombi we develop general techniques to analyse rhombal algebras including a filtration by what we call rhombus modules we introduce a way to relate the infinitedimensional rhombal algebra corresponding to a complete tiling of the ... | [['peach', 'introduced', 'rhombal', 'algebras', 'associated', 'to', 'quivers', 'given', 'by', 'tilings', 'of', 'the', 'plane', 'by', 'rhombi', 'we', 'develop', 'general', 'techniques', 'to', 'analyse', 'rhombal', 'algebras', 'including', 'a', 'filtration', 'by', 'what', 'we', 'call', 'rhombus', 'modules', 'we', 'introd... | [-0.11065542880753311, 0.06548329299102738, -0.07941168998880739, 0.10767312018081136, -0.1680234539143126, -0.11304226784684926, 0.005872468763125052, 0.35640412758728235, -0.38994352751915606, -0.19637601896522378, 0.12961203022005566, -0.19895764856843318, -0.18809299082537995, 0.13363181446772923, -0.17707164689830... |
710.2782 | Effective linkage learning using low-order statistics and clustering | The adoption of probabilistic models for the best individuals found so far is
a powerful approach for evolutionary computation. Increasingly more complex
models have been used by estimation of distribution algorithms (EDAs), which
often result better effectiveness on finding the global optima for hard
optimization pr... | cs.NE cs.AI | the adoption of probabilistic models for the best individuals found so far is a powerful approach for evolutionary computation increasingly more complex models have been used by estimation of distribution algorithms edas which often result better effectiveness on finding the global optima for hard optimization problems... | [['the', 'adoption', 'of', 'probabilistic', 'models', 'for', 'the', 'best', 'individuals', 'found', 'so', 'far', 'is', 'a', 'powerful', 'approach', 'for', 'evolutionary', 'computation', 'increasingly', 'more', 'complex', 'models', 'have', 'been', 'used', 'by', 'estimation', 'of', 'distribution', 'algorithms', 'edas', '... | [-0.014225695569402012, -0.011669386547751001, -0.1302244696090789, 0.1478282778393421, -0.11840701123968844, -0.1769152809304735, 0.022148523392037947, 0.40395299548350544, -0.26580011186818314, -0.37637834252049046, 0.12157352892569749, -0.21162369357660785, -0.18171314921802337, 0.2097006020338151, -0.07611318830529... |
710.2783 | Void Statistics and Void Galaxies in the 2dFGRS | For the 2dFGRS we study the properties of voids and of fainter galaxies
within voids that are defined by brighter galaxies. Our results are compared
with simulated galaxy catalogues from the Millenium simulation coupled with a
semianalytical galaxy formation recipe. We derive the void size distribution
and discuss it... | astro-ph | for the 2dfgrs we study the properties of voids and of fainter galaxies within voids that are defined by brighter galaxies our results are compared with simulated galaxy catalogues from the millenium simulation coupled with a semianalytical galaxy formation recipe we derive the void size distribution and discuss its de... | [['for', 'the', '2dfgrs', 'we', 'study', 'the', 'properties', 'of', 'voids', 'and', 'of', 'fainter', 'galaxies', 'within', 'voids', 'that', 'are', 'defined', 'by', 'brighter', 'galaxies', 'our', 'results', 'are', 'compared', 'with', 'simulated', 'galaxy', 'catalogues', 'from', 'the', 'millenium', 'simulation', 'coupled... | [-0.04736958285444929, 0.06843152329678769, -0.08174071750410787, 0.12513799578903267, -0.07482847580655441, 0.019351516364117683, 0.028125559525986894, 0.4454619265510188, -0.08687300937820025, -0.36821102942565725, 0.0022677805850134613, -0.30929465086859886, -0.048488232003533104, 0.17277842906246266, -0.00113115709... |
710.2784 | Routes to thermodynamic limit on scale-free networks | We show that there are two classes of finite size effects for dynamic models
taking place on a scale-free topology. Some models in finite networks show a
behavior that depends only on the system size N. Others present an additional
distinct dependence on the upper cutoff k_c of the degree distribution. Since
the infi... | cond-mat.stat-mech | we show that there are two classes of finite size effects for dynamic models taking place on a scalefree topology some models in finite networks show a behavior that depends only on the system size n others present an additional distinct dependence on the upper cutoff k_c of the degree distribution since the infinite n... | [['we', 'show', 'that', 'there', 'are', 'two', 'classes', 'of', 'finite', 'size', 'effects', 'for', 'dynamic', 'models', 'taking', 'place', 'on', 'a', 'scalefree', 'topology', 'some', 'models', 'in', 'finite', 'networks', 'show', 'a', 'behavior', 'that', 'depends', 'only', 'on', 'the', 'system', 'size', 'n', 'others', ... | [-0.15699811375234277, 0.13942867898367695, -0.09850471204457184, 0.05272615421231421, -0.021601129602640868, -0.12299996162376677, 0.07302319246906942, 0.3459310527890921, -0.24998748155776412, -0.30014319163747133, 0.0543421099166153, -0.27800673499392964, -0.16302364333338726, 0.19294895744727303, -0.016474289796315... |
710.2785 | Monte Carlo Generators for the LHC | The status of two Monte Carlo generators, HELAC-PHEGAS, a program for
multi-jet processes and VBFNLO, a parton level program for vector boson fusion
processes at NLO QCD, is briefly presented. The aim of these tools is the
simulation of events within the Standard Model at current and future high
energy experiments, i... | hep-ph | the status of two monte carlo generators helacphegas a program for multijet processes and vbfnlo a parton level program for vector boson fusion processes at nlo qcd is briefly presented the aim of these tools is the simulation of events within the standard model at current and future high energy experiments in particul... | [['the', 'status', 'of', 'two', 'monte', 'carlo', 'generators', 'helacphegas', 'a', 'program', 'for', 'multijet', 'processes', 'and', 'vbfnlo', 'a', 'parton', 'level', 'program', 'for', 'vector', 'boson', 'fusion', 'processes', 'at', 'nlo', 'qcd', 'is', 'briefly', 'presented', 'the', 'aim', 'of', 'these', 'tools', 'is'... | [-0.029572877463963355, 0.20228423618278663, -0.10195176397830667, 0.1860296731900004, -0.006815513123718786, -0.06711105745233281, 0.0024946679715329495, 0.3576576757493993, -0.22370281403648182, -0.2645912432295441, 0.08306336747056109, -0.3394878995539227, 0.00944031512653324, 0.17938773412401723, 0.0767238702670946... |
710.2786 | Higgsless electroweak symmetry breaking at the LHC | While the Higgs model is the best studied scenario of electroweak symmetry
breaking, a number strongly-coupled models exist, predicting new signatures.
Recent studies of WW and WZ final states at the ATLAS and CMS experiments are
summarized and expected sensitivities are presented within the frameworks of
the technic... | hep-ex | while the higgs model is the best studied scenario of electroweak symmetry breaking a number stronglycoupled models exist predicting new signatures recent studies of ww and wz final states at the atlas and cms experiments are summarized and expected sensitivities are presented within the frameworks of the technicolor s... | [['while', 'the', 'higgs', 'model', 'is', 'the', 'best', 'studied', 'scenario', 'of', 'electroweak', 'symmetry', 'breaking', 'a', 'number', 'stronglycoupled', 'models', 'exist', 'predicting', 'new', 'signatures', 'recent', 'studies', 'of', 'ww', 'and', 'wz', 'final', 'states', 'at', 'the', 'atlas', 'and', 'cms', 'exper... | [-0.09158364659683271, 0.22671288109638474, -0.042869276460260154, 0.13284440559800714, -0.0578076883695427, -0.19721200179139323, -0.02075625603002581, 0.31647001735188746, -0.16907229764725673, -0.32402518515221096, 0.056018669293685396, -0.30778969058936295, -0.07074632407589392, 0.0906205494295467, 0.06877049933695... |
710.2787 | The shuffle Hopf algebra and quasiplanar Wick products | The operator valued distributions which arise in quantum field theory on the
noncommutative Minkowski space can be symbolized by a generalization of chord
diagrams, the dotted chord diagrams. In this framework, the combinatorial
aspects of quasiplanar Wick products are understood in terms of the shuffle
Hopf algebra ... | math.QA hep-th | the operator valued distributions which arise in quantum field theory on the noncommutative minkowski space can be symbolized by a generalization of chord diagrams the dotted chord diagrams in this framework the combinatorial aspects of quasiplanar wick products are understood in terms of the shuffle hopf algebra of do... | [['the', 'operator', 'valued', 'distributions', 'which', 'arise', 'in', 'quantum', 'field', 'theory', 'on', 'the', 'noncommutative', 'minkowski', 'space', 'can', 'be', 'symbolized', 'by', 'a', 'generalization', 'of', 'chord', 'diagrams', 'the', 'dotted', 'chord', 'diagrams', 'in', 'this', 'framework', 'the', 'combinato... | [-0.16952330823260126, 0.16283999844035862, -0.13823719460051506, 0.1391289894701913, -0.09710810935430345, -0.07885214060661383, 0.024081663812103214, 0.34655635259114204, -0.3434991860762239, -0.2319781734375283, 0.10140617143042618, -0.21540782802621833, -0.24469620548188686, 0.18581376641013775, -0.1599965089815668... |
710.2788 | Exploring the QCD vacuum - (some) recent developments in confinement and
topology | I start by giving a brief overview over new developments in the area of
confinement and topology. As an example for the interrelations between
topological objects, instantons at finite temperature are discussed. Then I
focus on new insights into the structure of the QCD vacuum obtained through
filtering methods, in p... | hep-lat hep-ph hep-th | i start by giving a brief overview over new developments in the area of confinement and topology as an example for the interrelations between topological objects instantons at finite temperature are discussed then i focus on new insights into the structure of the qcd vacuum obtained through filtering methods in particu... | [['i', 'start', 'by', 'giving', 'a', 'brief', 'overview', 'over', 'new', 'developments', 'in', 'the', 'area', 'of', 'confinement', 'and', 'topology', 'as', 'an', 'example', 'for', 'the', 'interrelations', 'between', 'topological', 'objects', 'instantons', 'at', 'finite', 'temperature', 'are', 'discussed', 'then', 'i', ... | [-0.0919540087885127, 0.15692886112258841, -0.09752079885420871, 0.058875589840242576, -0.06818781060905292, -0.09075661818496883, 0.019754369799368853, 0.37613212240153343, -0.21823372474293515, -0.24459118961260237, 0.11749072656725887, -0.271309696186077, -0.1548789861001845, 0.2125661555709767, -0.04179171765833322... |
710.2789 | SGR 1806-20 about two years after the giant flare: Suzaku, XMM-Newton
and INTEGRAL observations | In December 2004, the soft gamma-ray repeater SGR 1806-20 emitted the most
powerful giant flare ever observed. This probably involved a large-scale
rearrangement of the magnetosphere leading to observable variations in the
properties of its X-ray emission. Here we present the results of the first
Suzaku observation o... | astro-ph | in december 2004 the soft gammaray repeater sgr 180620 emitted the most powerful giant flare ever observed this probably involved a largescale rearrangement of the magnetosphere leading to observable variations in the properties of its xray emission here we present the results of the first suzaku observation of sgr 180... | [['in', 'december', '2004', 'the', 'soft', 'gammaray', 'repeater', 'sgr', '180620', 'emitted', 'the', 'most', 'powerful', 'giant', 'flare', 'ever', 'observed', 'this', 'probably', 'involved', 'a', 'largescale', 'rearrangement', 'of', 'the', 'magnetosphere', 'leading', 'to', 'observable', 'variations', 'in', 'the', 'pro... | [-0.09670283541382446, 0.13009543634312104, -0.07750585092653106, 0.11369247464050987, -0.12760133482175914, -0.059959620174469194, 0.08751945137420167, 0.46112312214707374, -0.18993438402085436, -0.369884102680061, 0.0823227857361908, -0.27761686089691656, -0.05624060745752097, 0.23054177162278253, -0.0535044794265745... |
710.279 | PNJL model with a Van der Monde term | We extend the Polyakov-Nambu-Jona-Lasinio (PNJL) model for two degenerate
flavours by including the effect of the SU(3) measure with a Van der Monde
(VdM) term. This ensures that the Polyakov loop always remains in the domain
[0,1]. The pressure, energy density, specific heat, speed of sound and
conformal measure sho... | hep-ph hep-lat nucl-th | we extend the polyakovnambujonalasinio pnjl model for two degenerate flavours by including the effect of the su3 measure with a van der monde vdm term this ensures that the polyakov loop always remains in the domain 01 the pressure energy density specific heat speed of sound and conformal measure show small or negligib... | [['we', 'extend', 'the', 'polyakovnambujonalasinio', 'pnjl', 'model', 'for', 'two', 'degenerate', 'flavours', 'by', 'including', 'the', 'effect', 'of', 'the', 'su3', 'measure', 'with', 'a', 'van', 'der', 'monde', 'vdm', 'term', 'this', 'ensures', 'that', 'the', 'polyakov', 'loop', 'always', 'remains', 'in', 'the', 'dom... | [-0.08957878313542876, 0.17944357889153215, -0.071017572694287, 0.07450870721249328, -0.05082708974939068, -0.13244707707543762, 0.06717317036533614, 0.36090082975522597, -0.195477137427625, -0.2549683857253011, 0.04407763070835523, -0.33623065886905, -0.06750276255925015, 0.12356379833690138, 0.02437938588234235, 0.07... |
710.2791 | Drift instability and tunneling of lattice solitons | We derive an analytic formula for the lateral dynamics of solitons in a
general inhomogeneous nonlinear media, and show that it can be valid over tens
of diffraction lengths. In particular, we show that solitons centered at a
lattice maximum can be ``mathematically unstable'' but ``physically stable''.
We also derive... | nlin.PS | we derive an analytic formula for the lateral dynamics of solitons in a general inhomogeneous nonlinear media and show that it can be valid over tens of diffraction lengths in particular we show that solitons centered at a lattice maximum can be mathematically unstable but physically stable we also derive an analytic u... | [['we', 'derive', 'an', 'analytic', 'formula', 'for', 'the', 'lateral', 'dynamics', 'of', 'solitons', 'in', 'a', 'general', 'inhomogeneous', 'nonlinear', 'media', 'and', 'show', 'that', 'it', 'can', 'be', 'valid', 'over', 'tens', 'of', 'diffraction', 'lengths', 'in', 'particular', 'we', 'show', 'that', 'solitons', 'cen... | [-0.13778810181759926, 0.1454390607758681, -0.12370436447082271, 0.12195124469113759, -0.05304798950821581, -0.15997902995211558, 0.025187317196699515, 0.39410949373801407, -0.24607727047659353, -0.2128656442132844, 0.09559612192908748, -0.21767548975390447, -0.1681445340402949, 0.26585918823650606, 0.00299446745267347... |
710.2792 | Market completion using options | Mathematical models for financial asset prices which include, for example,
stochastic volatility or jumps are incomplete in that derivative securities are
generally not replicable by trading in the underlying. In earlier work (2004)
the first author provided a geometric condition under which trading in the
underlying... | q-fin.PR math.PR | mathematical models for financial asset prices which include for example stochastic volatility or jumps are incomplete in that derivative securities are generally not replicable by trading in the underlying in earlier work 2004 the first author provided a geometric condition under which trading in the underlying and a ... | [['mathematical', 'models', 'for', 'financial', 'asset', 'prices', 'which', 'include', 'for', 'example', 'stochastic', 'volatility', 'or', 'jumps', 'are', 'incomplete', 'in', 'that', 'derivative', 'securities', 'are', 'generally', 'not', 'replicable', 'by', 'trading', 'in', 'the', 'underlying', 'in', 'earlier', 'work',... | [-0.08382595786641009, 0.06258181075492375, -0.1038371859337387, 0.15436696380799586, -0.14386335681315118, -0.1497357089721941, 0.06986538425170645, 0.41983257741115887, -0.27722489296789526, -0.2205708550326036, 0.18862324063497668, -0.22332489759796054, -0.17458547067699806, 0.2099986826713001, -0.14789441995641314,... |
710.2793 | The SGR 1806-20 magnetar signature on the Earth's magnetic field | SGRs denote ``soft $\gamma$-ray repeaters'', a small class of slowly spinning
neutron stars with strong magnetic fields. On 27 December 2004, a giant flare
was detected from magnetar SGR 1806-20. The initial spike was followed by a
hard-X-ray tail persisting for 380 s with a modulation period of 7.56 s. This
event ha... | astro-ph | sgrs denote soft gammaray repeaters a small class of slowly spinning neutron stars with strong magnetic fields on 27 december 2004 a giant flare was detected from magnetar sgr 180620 the initial spike was followed by a hardxray tail persisting for 380 s with a modulation period of 756 s this event has received consider... | [['sgrs', 'denote', 'soft', 'gammaray', 'repeaters', 'a', 'small', 'class', 'of', 'slowly', 'spinning', 'neutron', 'stars', 'with', 'strong', 'magnetic', 'fields', 'on', '27', 'december', '2004', 'a', 'giant', 'flare', 'was', 'detected', 'from', 'magnetar', 'sgr', '180620', 'the', 'initial', 'spike', 'was', 'followed',... | [-0.14162019276060164, 0.1934997340114205, -0.05509456980042159, 0.10232305970430995, -0.11924895099674662, -0.0464089338031287, 0.05312620922923088, 0.38592614906219147, -0.17252066956212123, -0.3876203661908706, 0.09279847400495783, -0.2987423484430959, -0.0711208027228713, 0.25933457107283175, -0.05964063046344866, ... |
710.2794 | Fermion loop simulations in 2--d lattice theories -- results and
limitations | We review our results for the simulation of the 2--d lattice Gross--Neveu
model in a fermion loop representation. Possible extensions of our techniques
to other models and higher dimensions are discussed, as well as the limitations
of loop--type representations.
| hep-lat | we review our results for the simulation of the 2d lattice grossneveu model in a fermion loop representation possible extensions of our techniques to other models and higher dimensions are discussed as well as the limitations of looptype representations | [['we', 'review', 'our', 'results', 'for', 'the', 'simulation', 'of', 'the', '2d', 'lattice', 'grossneveu', 'model', 'in', 'a', 'fermion', 'loop', 'representation', 'possible', 'extensions', 'of', 'our', 'techniques', 'to', 'other', 'models', 'and', 'higher', 'dimensions', 'are', 'discussed', 'as', 'well', 'as', 'the',... | [-0.028273712557095747, 0.10172170824490678, -0.019048960646614432, 0.08884888619948657, -0.05586954523833134, -0.1293170194571408, 0.01716591341373248, 0.3660781184832255, -0.19856046073329756, -0.26092852680728984, 0.1370235610818968, -0.29396515107976323, -0.19956513236348444, 0.2214745225277371, -0.0132872756713858... |
710.2795 | Charmonium properties in the quark-gluon plasma | We present results for charmonium correlators and spectral functions in
2-flavour CD on anisotropic lattices. Our results indicate that the S-waves
(J/psi and eta_c) survive up to temperatures close to 2T_c, while the P-waves
(chi_c0 and chi_c1) melt away below 1.2T_c.
| hep-lat | we present results for charmonium correlators and spectral functions in 2flavour cd on anisotropic lattices our results indicate that the swaves jpsi and eta_c survive up to temperatures close to 2t_c while the pwaves chi_c0 and chi_c1 melt away below 12t_c | [['we', 'present', 'results', 'for', 'charmonium', 'correlators', 'and', 'spectral', 'functions', 'in', '2flavour', 'cd', 'on', 'anisotropic', 'lattices', 'our', 'results', 'indicate', 'that', 'the', 'swaves', 'jpsi', 'and', 'eta_c', 'survive', 'up', 'to', 'temperatures', 'close', 'to', '2t_c', 'while', 'the', 'pwaves'... | [-0.0029580333701721053, 0.2630902227559468, -0.10444012896453099, 0.10343069937534449, 0.017686603045681627, -0.11494959345678003, 0.12599646615250626, 0.3734473251942091, -0.12159039002911347, -0.12100290457104765, -0.05400313841599244, -0.40768277004542874, 0.014633609345409929, 0.14732428876365103, 0.12599459899271... |
710.2796 | On the Limitations of the Color Dipole Picture | We discuss two aspects of the color dipole picture of high energy
photon-proton scattering. First we present bounds on various ratios of deep
inelastic structure functions resulting from the dipole picture that, together
with the measured data, can be used to restrict the kinematical range of its
applicability. The s... | hep-ph | we discuss two aspects of the color dipole picture of high energy photonproton scattering first we present bounds on various ratios of deep inelastic structure functions resulting from the dipole picture that together with the measured data can be used to restrict the kinematical range of its applicability the second i... | [['we', 'discuss', 'two', 'aspects', 'of', 'the', 'color', 'dipole', 'picture', 'of', 'high', 'energy', 'photonproton', 'scattering', 'first', 'we', 'present', 'bounds', 'on', 'various', 'ratios', 'of', 'deep', 'inelastic', 'structure', 'functions', 'resulting', 'from', 'the', 'dipole', 'picture', 'that', 'together', '... | [-0.08863372455995816, 0.09498919419084605, -0.09057101395267707, 0.11116477289201263, -0.06316829481377051, -0.0314046613800411, 0.030564679803613288, 0.3985864197835326, -0.2458461864063373, -0.3133537958161189, 0.015749040516451575, -0.2760014691318457, -0.06636154978321149, 0.1759536342623715, 0.012734327264703237,... |
710.2797 | Unparticles and holography | We construct the holographic dual theory of unparticles. The Randall-Sundrum
type hard wall model is shown to produce deconstructing particles, whose
spectrum has a finite mass gap proportional to the inverse of the fifth
direction segment. The introduction of new scale corresponds to setting a brane
in ${\rm AdS}_5$... | hep-ph astro-ph hep-th | we construct the holographic dual theory of unparticles the randallsundrum type hard wall model is shown to produce deconstructing particles whose spectrum has a finite mass gap proportional to the inverse of the fifth direction segment the introduction of new scale corresponds to setting a brane in rm ads_5 the broken... | [['we', 'construct', 'the', 'holographic', 'dual', 'theory', 'of', 'unparticles', 'the', 'randallsundrum', 'type', 'hard', 'wall', 'model', 'is', 'shown', 'to', 'produce', 'deconstructing', 'particles', 'whose', 'spectrum', 'has', 'a', 'finite', 'mass', 'gap', 'proportional', 'to', 'the', 'inverse', 'of', 'the', 'fifth... | [-0.1070110441170012, 0.247573319086999, -0.09855700594062607, 0.1293019999967267, -0.15766433102389177, -0.19056662782095374, -0.048602182157337664, 0.29297689395646254, -0.2605293531964223, -0.2413626838102937, 0.07688315585410843, -0.28359077258656423, -0.07787758430155615, 0.04090598462459942, -0.055084429184595746... |
710.2798 | A common integrable structure in the hermitian matrix model and
Hele-Shaw flows | It is proved that the system of string equations of the dispersionless 2-Toda
hierarchy which arises in the planar limit of the hermitian matrix model also
underlies certain processes in Hele-Shaw flows.
| nlin.SI | it is proved that the system of string equations of the dispersionless 2toda hierarchy which arises in the planar limit of the hermitian matrix model also underlies certain processes in heleshaw flows | [['it', 'is', 'proved', 'that', 'the', 'system', 'of', 'string', 'equations', 'of', 'the', 'dispersionless', '2toda', 'hierarchy', 'which', 'arises', 'in', 'the', 'planar', 'limit', 'of', 'the', 'hermitian', 'matrix', 'model', 'also', 'underlies', 'certain', 'processes', 'in', 'heleshaw', 'flows']] | [-0.19583954359404743, 0.13915247085969895, -0.040852469857782125, 0.09110065612549079, -0.017835607868619263, -0.14113646850455552, -0.027879515138920397, 0.22031476208940148, -0.364147636690177, -0.19114755117334425, 0.10131941550207557, -0.2566545819863677, -0.24703158455668017, 0.14511668518389342, -0.0585580319893... |
710.2799 | Study of the topological vacuum structure of SU(2) gluodynamics at T > 0
with overlap fermions and improved action | We study SU(2) gluodynamics at finite temperature near the deconfining phase
transition. We create the lattice ensembles using the tadpole improved
Luscher-Weisz action. The overlap Dirac operator is used to determine the
following three aspects of vacuum structure: (i) The topological susceptibility
is evaluated at ... | hep-lat | we study su2 gluodynamics at finite temperature near the deconfining phase transition we create the lattice ensembles using the tadpole improved luscherweisz action the overlap dirac operator is used to determine the following three aspects of vacuum structure i the topological susceptibility is evaluated at various te... | [['we', 'study', 'su2', 'gluodynamics', 'at', 'finite', 'temperature', 'near', 'the', 'deconfining', 'phase', 'transition', 'we', 'create', 'the', 'lattice', 'ensembles', 'using', 'the', 'tadpole', 'improved', 'luscherweisz', 'action', 'the', 'overlap', 'dirac', 'operator', 'is', 'used', 'to', 'determine', 'the', 'foll... | [-0.13822173966790538, 0.26188538663218314, -0.06257257554455693, 0.07310081448220838, -0.012003936588831515, -0.10186198277466268, 0.0665305253645652, 0.4110794481204217, -0.17456189119425344, -0.25028821879840757, 0.09727838157440524, -0.30168618528868063, -0.11054970272985029, 0.04858833684933832, 0.0615023646660777... |
710.28 | A weight two phenomenon for the moduli of rank one local systems on open
varieties | The twistor space of representations on an open variety maps to a weight two
space of local monodromy transformations around a divisor component at infinty.
The space of $\sigma$-invariant sections of this slope-two bundle over the
twistor line is a real 3 dimensional space whose parameters correspond to the
complex ... | math.AG | the twistor space of representations on an open variety maps to a weight two space of local monodromy transformations around a divisor component at infinty the space of sigmainvariant sections of this slopetwo bundle over the twistor line is a real 3 dimensional space whose parameters correspond to the complex residue ... | [['the', 'twistor', 'space', 'of', 'representations', 'on', 'an', 'open', 'variety', 'maps', 'to', 'a', 'weight', 'two', 'space', 'of', 'local', 'monodromy', 'transformations', 'around', 'a', 'divisor', 'component', 'at', 'infinty', 'the', 'space', 'of', 'sigmainvariant', 'sections', 'of', 'this', 'slopetwo', 'bundle',... | [-0.19469794830412515, 0.08510767119291666, -0.06410522345123032, 0.03728809985782831, -0.12178501066180968, -0.06759904171790808, -0.01669389586858151, 0.3672422841191292, -0.3146384511548545, -0.1788211011237675, 0.07993751609577768, -0.23454915047172578, -0.14686006626054163, 0.199372191192402, -0.05121825722556922,... |
710.2801 | Multi-Gap Superconductivity in MgB2: Magneto-Raman Spectroscopy | Electronic Raman scattering studies on MgB2 single crystals as a function of
excitation and polarization have revealed three distinct superconducting
features: a clean gap below 37 cm-1 and two coherence peaks at 109 cm-1 and 78
cm-1 which we identify as the superconducting gaps in \pi- and \sigma-bands and
as the Le... | cond-mat.supr-con | electronic raman scattering studies on mgb2 single crystals as a function of excitation and polarization have revealed three distinct superconducting features a clean gap below 37 cm1 and two coherence peaks at 109 cm1 and 78 cm1 which we identify as the superconducting gaps in pi and sigmabands and as the leggetts col... | [['electronic', 'raman', 'scattering', 'studies', 'on', 'mgb2', 'single', 'crystals', 'as', 'a', 'function', 'of', 'excitation', 'and', 'polarization', 'have', 'revealed', 'three', 'distinct', 'superconducting', 'features', 'a', 'clean', 'gap', 'below', '37', 'cm1', 'and', 'two', 'coherence', 'peaks', 'at', '109', 'cm1... | [-0.17714366276129723, 0.24807565421430547, -0.04616163600848554, -0.0051332377303991315, -0.026529631548727006, -0.1388545353061277, 0.11309236374824014, 0.3996839245704755, -0.24603052076417953, -0.25358582247520656, -0.021301716202487275, -0.37219819089729494, -0.07839522391361542, 0.18044652919961165, 0.11499727745... |
710.2802 | Investigation of Strongly Correlated Electron Systems with Cellular
Dynamical Mean Field Theory | In this thesis we study the strongly-correlated-electron physics of the
longstanding H-Tc-superconductivity problem using a non-perturbative method,
the Dynamical Mean Field Theory (DMFT), capable to go beyond standard
perturbation-theory techniques. DMFT is by construction a local theory which
neglects spatial corre... | cond-mat.str-el | in this thesis we study the stronglycorrelatedelectron physics of the longstanding htcsuperconductivity problem using a nonperturbative method the dynamical mean field theory dmft capable to go beyond standard perturbationtheory techniques dmft is by construction a local theory which neglects spatial correlation experi... | [['in', 'this', 'thesis', 'we', 'study', 'the', 'stronglycorrelatedelectron', 'physics', 'of', 'the', 'longstanding', 'htcsuperconductivity', 'problem', 'using', 'a', 'nonperturbative', 'method', 'the', 'dynamical', 'mean', 'field', 'theory', 'dmft', 'capable', 'to', 'go', 'beyond', 'standard', 'perturbationtheory', 't... | [-0.11614862028451171, 0.11589405077807896, -0.10843840743182227, 0.10634742302878294, -0.011763757620938122, -0.15116514864959754, 0.08616361202904954, 0.3491519520012662, -0.25318229276221244, -0.22861956541775727, 0.011872988762333989, -0.2949610576580744, -0.20625911965849808, 0.12444465325097553, 0.038142410675063... |
710.2803 | Observation of Leggett's collective mode in a multi-band MgB2
superconductor | We report observation of Leggett's collective mode in a multi-band MgB2
superconductor with T_c=39K arising from the fluctuations in the relative phase
between two superconducting condensates. The novel mode is observed by Raman
spectroscopy at 9.4 meV in the fully symmetric scattering channel. The observed
mode freq... | cond-mat.supr-con | we report observation of leggetts collective mode in a multiband mgb2 superconductor with t_c39k arising from the fluctuations in the relative phase between two superconducting condensates the novel mode is observed by raman spectroscopy at 94 mev in the fully symmetric scattering channel the observed mode frequency is... | [['we', 'report', 'observation', 'of', 'leggetts', 'collective', 'mode', 'in', 'a', 'multiband', 'mgb2', 'superconductor', 'with', 't_c39k', 'arising', 'from', 'the', 'fluctuations', 'in', 'the', 'relative', 'phase', 'between', 'two', 'superconducting', 'condensates', 'the', 'novel', 'mode', 'is', 'observed', 'by', 'ra... | [-0.16667089792654702, 0.22457622544709266, -0.09472160888509008, -0.029165599981257527, -0.055299411493602714, -0.1409119823539074, 0.13947437285331257, 0.3764629662036896, -0.2201998458946483, -0.27227817874467164, 0.015113963249237522, -0.30958608616339534, -0.09466347626099984, 0.18242834934866742, 0.03353117594266... |
710.2804 | Inelastic soliton processes generated by the perturbed KdV equation | Perturbations commonly added to the KdV equation contain terms that represent
inelastic interac-tions among KdV solitons in multiple-soliton solutions. These
terms trigger the emergence of new waves in the first-order correction to the
solution of the perturbed equation. The new waves can represent
soliton-anti-solit... | nlin.PS | perturbations commonly added to the kdv equation contain terms that represent inelastic interactions among kdv solitons in multiplesoliton solutions these terms trigger the emergence of new waves in the firstorder correction to the solution of the perturbed equation the new waves can represent solitonantisoliton creati... | [['perturbations', 'commonly', 'added', 'to', 'the', 'kdv', 'equation', 'contain', 'terms', 'that', 'represent', 'inelastic', 'interactions', 'among', 'kdv', 'solitons', 'in', 'multiplesoliton', 'solutions', 'these', 'terms', 'trigger', 'the', 'emergence', 'of', 'new', 'waves', 'in', 'the', 'firstorder', 'correction', ... | [-0.18279331772854285, 0.15967829678473727, -0.065566028244835, 0.14651154643589898, -0.13115833947501546, -0.1130291336116248, -0.097004482963322, 0.21514425526506134, -0.311093413404056, -0.24001022641147887, 0.03915612535950329, -0.38967406869466814, -0.13810038156641116, 0.14053107877511398, 0.09395381631994885, 0.... |
710.2805 | Nouvelle analyse des ph\'enom\`enes vibratoires en tournage | In the cutting process, machine-tools vibrations are generally a real problem
when the amplitude crosses the limits of dimensional or surface quality
workpiece precision required. It is necessary to develop models taking into
account the three-dimensional vibratory approach to control the vibrations
phenomena. An exp... | physics.class-ph | in the cutting process machinetools vibrations are generally a real problem when the amplitude crosses the limits of dimensional or surface quality workpiece precision required it is necessary to develop models taking into account the threedimensional vibratory approach to control the vibrations phenomena an experiment... | [['in', 'the', 'cutting', 'process', 'machinetools', 'vibrations', 'are', 'generally', 'a', 'real', 'problem', 'when', 'the', 'amplitude', 'crosses', 'the', 'limits', 'of', 'dimensional', 'or', 'surface', 'quality', 'workpiece', 'precision', 'required', 'it', 'is', 'necessary', 'to', 'develop', 'models', 'taking', 'int... | [-0.08470821677631624, 0.09177286237982198, -0.11216939327953097, 0.01717603189809689, -0.04841004932081109, -0.09164961170812079, 0.02954396305119132, 0.36362724336753555, -0.2696760960326001, -0.28896246113822804, 0.09641101883791454, -0.254233002253763, -0.15822541832017736, 0.21987528645282461, -0.04524978872824897... |
710.2806 | Direct measurement of the coherence length of edge states in the Integer
Quantum Hall Regime | We have determined the finite temperature coherence length of edge states in
the Integer Quantum Hall Effect (IQHE) regime. This was realized by measuring
the visibility of electronic Mach-Zehnder interferometers of different sizes,
at filling factor 2. The visibility shows an exponential decay with the
temperature. ... | cond-mat.mes-hall | we have determined the finite temperature coherence length of edge states in the integer quantum hall effect iqhe regime this was realized by measuring the visibility of electronic machzehnder interferometers of different sizes at filling factor 2 the visibility shows an exponential decay with the temperature the chara... | [['we', 'have', 'determined', 'the', 'finite', 'temperature', 'coherence', 'length', 'of', 'edge', 'states', 'in', 'the', 'integer', 'quantum', 'hall', 'effect', 'iqhe', 'regime', 'this', 'was', 'realized', 'by', 'measuring', 'the', 'visibility', 'of', 'electronic', 'machzehnder', 'interferometers', 'of', 'different', ... | [-0.20528061101558032, 0.2688339036056412, -0.09440843106023278, 0.010602652315153845, 0.020865934387849713, -0.14033021937184795, 0.015445030893682054, 0.33978819190007115, -0.2827599291793174, -0.2890979095482854, 0.041102865396101994, -0.25873087551789703, -0.07814732337094567, 0.20847270905937035, 0.009033416111142... |
710.2807 | Metal-rich debris discs around white dwarfs | We have identified two moderately hot (~18000-22000K) white dwarfs,
SDSSJ1228+1040 and SDSSJ1043+0855, which exhibit double-peaked emission lines
in the CaII 8600A triplet. These line profiles are unambiguous signatures of
gaseous discs with outer radii of ~1Rsun orbiting the two white dwarfs. Both
stars accrete from... | astro-ph | we have identified two moderately hot 1800022000k white dwarfs sdssj12281040 and sdssj10430855 which exhibit doublepeaked emission lines in the caii 8600a triplet these line profiles are unambiguous signatures of gaseous discs with outer radii of 1rsun orbiting the two white dwarfs both stars accrete from the circumste... | [['we', 'have', 'identified', 'two', 'moderately', 'hot', '1800022000k', 'white', 'dwarfs', 'sdssj12281040', 'and', 'sdssj10430855', 'which', 'exhibit', 'doublepeaked', 'emission', 'lines', 'in', 'the', 'caii', '8600a', 'triplet', 'these', 'line', 'profiles', 'are', 'unambiguous', 'signatures', 'of', 'gaseous', 'discs'... | [-0.07092954856221025, 0.19472963451162764, -0.01848800850443934, 0.07775424820015599, -0.10171487424195859, -0.07102131663837977, 0.02316391129524594, 0.4245537531913438, -0.13248341919123113, -0.32010214146341015, 0.020478070015087724, -0.3340596185114823, -0.021121272596677666, 0.14723128505386085, -0.09926831018865... |
710.2808 | Identification of specificity determining residues in enzymes using
environment specific substitution tables | Environment specific substitution tables have been used effectively for
distinguishing structural and functional constraints on proteins and thereby
identify their active sites (Chelliah et al. (2004)). This work explores
whether a similar approach can be used to identify specificity determining
residues (SDRs) respo... | q-bio.QM | environment specific substitution tables have been used effectively for distinguishing structural and functional constraints on proteins and thereby identify their active sites chelliah et al 2004 this work explores whether a similar approach can be used to identify specificity determining residues sdrs responsible for... | [['environment', 'specific', 'substitution', 'tables', 'have', 'been', 'used', 'effectively', 'for', 'distinguishing', 'structural', 'and', 'functional', 'constraints', 'on', 'proteins', 'and', 'thereby', 'identify', 'their', 'active', 'sites', 'chelliah', 'et', 'al', '2004', 'this', 'work', 'explores', 'whether', 'a',... | [-0.04109973675741624, 0.03247255434392281, -0.04157998405837564, 0.14397217658528638, -0.12311870979285368, -0.16399787152085893, 0.1658562988203059, 0.42597103120899327, -0.25231882664362487, -0.4138087894647352, 0.014422628512826337, -0.2797028970133553, -0.19444313400014435, 0.1190859520161945, -0.08346031646254243... |
710.2809 | Rescuing H -> bb in VBF at the LHC by requiring a central photon | The LHC potential for a measurement of the Higgs boson coupling to the b
quark in the standard model is not well established yet. We show that requiring
a large transverse momentum photon in the light Higgs boson production via
vector-boson fusion (with subsequent H->bb decay) could provide a further
handle on the Hb... | hep-ph | the lhc potential for a measurement of the higgs boson coupling to the b quark in the standard model is not well established yet we show that requiring a large transverse momentum photon in the light higgs boson production via vectorboson fusion with subsequent hbb decay could provide a further handle on the hbb coupli... | [['the', 'lhc', 'potential', 'for', 'a', 'measurement', 'of', 'the', 'higgs', 'boson', 'coupling', 'to', 'the', 'b', 'quark', 'in', 'the', 'standard', 'model', 'is', 'not', 'well', 'established', 'yet', 'we', 'show', 'that', 'requiring', 'a', 'large', 'transverse', 'momentum', 'photon', 'in', 'the', 'light', 'higgs', '... | [-0.07349727526800989, 0.2535951589798611, -0.060700158602699186, 0.10545356168983165, -0.07134985247499902, -0.19481686540089097, 0.0896268264164753, 0.32273395113632874, -0.21536361929875883, -0.26304751657175296, 0.031857635085047645, -0.24563492090921057, 0.032222549177028915, 0.1630274758102711, 0.0415351669529848... |
710.281 | A note on the mass splitting of K*(892) | Belle Collaboration reported a new observed value of K*-(892) mass by
studying tau --> K_S pi nu_tau decay, which is significantly different from the
current world average value given by Particle Data Group 2006. Motivated by
this new data, we revisit the issue on the K*0(892)-K*+(892) mass splitting.
Our theoretical... | hep-ph hep-ex | belle collaboration reported a new observed value of k892 mass by studying tau k_s pi nu_tau decay which is significantly different from the current world average value given by particle data group 2006 motivated by this new data we revisit the issue on the k0892k892 mass splitting our theoretical estimation favors the... | [['belle', 'collaboration', 'reported', 'a', 'new', 'observed', 'value', 'of', 'k892', 'mass', 'by', 'studying', 'tau', 'k_s', 'pi', 'nu_tau', 'decay', 'which', 'is', 'significantly', 'different', 'from', 'the', 'current', 'world', 'average', 'value', 'given', 'by', 'particle', 'data', 'group', '2006', 'motivated', 'by... | [-0.07340799530169793, 0.17667865172095065, -0.050987624882587367, 0.07366141846370218, -0.13698540292680264, -0.10250118090771139, 0.12711425188130565, 0.28130590729415417, -0.17059400454995088, -0.3712186642523323, 0.031528719860528194, -0.29691164694460376, -0.06157537286968103, 0.1820708960111785, -0.03080175530963... |
710.2811 | Charge disproportionation and collinear magnetic order in the frustrated
triangular antiferromagnet AgNiO2 | We report a high-resolution neutron diffraction study of the crystal and
magnetic structure of the orbitally-degenerate frustrated metallic magnet
AgNiO2. At high temperatures the structure is hexagonal with a single
crystallographic Ni site, low-spin Ni3+ with spin-1/2 and two-fold orbital
degeneracy, arranged in an... | cond-mat.str-el | we report a highresolution neutron diffraction study of the crystal and magnetic structure of the orbitallydegenerate frustrated metallic magnet agnio2 at high temperatures the structure is hexagonal with a single crystallographic ni site lowspin ni3 with spin12 and twofold orbital degeneracy arranged in an antiferroma... | [['we', 'report', 'a', 'highresolution', 'neutron', 'diffraction', 'study', 'of', 'the', 'crystal', 'and', 'magnetic', 'structure', 'of', 'the', 'orbitallydegenerate', 'frustrated', 'metallic', 'magnet', 'agnio2', 'at', 'high', 'temperatures', 'the', 'structure', 'is', 'hexagonal', 'with', 'a', 'single', 'crystallograp... | [-0.20469815453532808, 0.273018759705288, 0.08791456604519804, 0.009788363761374076, -0.03408419296461997, -0.13661402231254363, 0.0998365683733426, 0.4304792936398129, -0.29280194768617895, -0.2701136723809917, 0.002703295515969469, -0.38059867238121226, -0.045101836241157774, 0.0319061488064529, 0.11206503068853922, ... |
710.2812 | Ultra-Broadband Radial Polarization Conversion based on Goos-Hanchen
Shift | We demonstrate, for the first time, a scheme that generates
radially-polarized light using Goos-Hanchen shift of a cylindrically symmetric
Total Internal Reflection. It allows ultra-broadband radial polarization
conversion for wavelengths differing >1 micron.
| physics.optics | we demonstrate for the first time a scheme that generates radiallypolarized light using gooshanchen shift of a cylindrically symmetric total internal reflection it allows ultrabroadband radial polarization conversion for wavelengths differing 1 micron | [['we', 'demonstrate', 'for', 'the', 'first', 'time', 'a', 'scheme', 'that', 'generates', 'radiallypolarized', 'light', 'using', 'gooshanchen', 'shift', 'of', 'a', 'cylindrically', 'symmetric', 'total', 'internal', 'reflection', 'it', 'allows', 'ultrabroadband', 'radial', 'polarization', 'conversion', 'for', 'wavelengt... | [-0.13561793931788116, 0.2035358799057025, -0.0972436844992141, -0.027971378307098126, -0.11340226221716765, -0.1369678576505094, 0.00889670645648783, 0.561991302352963, -0.23216673449584932, -0.2520962383485202, -0.0188764988049639, -0.2024815840665145, -0.08868892853515166, 0.22618016578031308, 0.023701580812815915, ... |
710.2813 | A Search for Mid-Infrared Molecular Hydrogen Emission from
Protoplanetary Disks | We observed the Herbig Ae/Be stars UX Ori, HD 34282, HD 100453, HD 101412, HD
104237 and HD 142666, and the T Tauri star HD 319139 and searched for H2 0-0
S(2) emission at 12.278 micron and H2 0-0 S(1) emission at 17.035 micron with
VISIR, ESO-VLT's high-resolution MIR spectrograph. None of the sources present
eviden... | astro-ph | we observed the herbig aebe stars ux ori hd 34282 hd 100453 hd 101412 hd 104237 and hd 142666 and the t tauri star hd 319139 and searched for h2 00 s2 emission at 12278 micron and h2 00 s1 emission at 17035 micron with visir esovlts highresolution mir spectrograph none of the sources present evidence for h2 emission st... | [['we', 'observed', 'the', 'herbig', 'aebe', 'stars', 'ux', 'ori', 'hd', '34282', 'hd', '100453', 'hd', '101412', 'hd', '104237', 'and', 'hd', '142666', 'and', 'the', 't', 'tauri', 'star', 'hd', '319139', 'and', 'searched', 'for', 'h2', '00', 's2', 'emission', 'at', '12278', 'micron', 'and', 'h2', '00', 's1', 'emission... | [-0.04189021239782978, 0.11355241777220626, 0.02859955029380098, 0.0564270768294123, -0.0340520739324045, -0.07712708514165557, 0.06876606651785076, 0.4341042783378293, -0.15192052036757409, -0.3431610261569412, 0.07488941436016125, -0.3174220250960415, 0.07289199844300019, 0.1780717277907727, -0.004905745012424765, -0... |
710.2814 | CO abundances in a protostellar cloud: freeze-out and desorption in the
envelope and outflow of L483 | CO isotopes are able to probe the different components in protostellar
clouds. These components, core, envelope and outflow have distinct physical
conditions and sometimes more than one component contributes to the observed
line profile. In this study we determine how CO isotope abundances are altered
by the physical... | astro-ph | co isotopes are able to probe the different components in protostellar clouds these components core envelope and outflow have distinct physical conditions and sometimes more than one component contributes to the observed line profile in this study we determine how co isotope abundances are altered by the physical condi... | [['co', 'isotopes', 'are', 'able', 'to', 'probe', 'the', 'different', 'components', 'in', 'protostellar', 'clouds', 'these', 'components', 'core', 'envelope', 'and', 'outflow', 'have', 'distinct', 'physical', 'conditions', 'and', 'sometimes', 'more', 'than', 'one', 'component', 'contributes', 'to', 'the', 'observed', '... | [-0.03784588530765004, 0.07078882823796968, 0.002360008280014708, 0.04336912403826838, -0.0882216610036613, -0.10257436814884256, -0.022930775774598476, 0.4949559914835152, -0.16001393531682662, -0.2820215346291661, 0.045213829045505485, -0.2501845216722272, -0.01927710722971131, 0.08840982172391489, 0.0391701177209359... |
710.2815 | Optical emission from massive donors in ULX binary systems | We present evolutionary tracks of binary systems with high mass companion
stars and stellar-through-intermediate mass BHs. Using Eggleton's stellar
evolution code, we compute the luminosity produced by accretion from the donor
during its entire evolution. We compute also the evolution of the optical
spectrum of the b... | astro-ph | we present evolutionary tracks of binary systems with high mass companion stars and stellarthroughintermediate mass bhs using eggletons stellar evolution code we compute the luminosity produced by accretion from the donor during its entire evolution we compute also the evolution of the optical spectrum of the binary sy... | [['we', 'present', 'evolutionary', 'tracks', 'of', 'binary', 'systems', 'with', 'high', 'mass', 'companion', 'stars', 'and', 'stellarthroughintermediate', 'mass', 'bhs', 'using', 'eggletons', 'stellar', 'evolution', 'code', 'we', 'compute', 'the', 'luminosity', 'produced', 'by', 'accretion', 'from', 'the', 'donor', 'du... | [-0.06661681470629081, 0.10287545209585809, -0.11461180309308883, 0.13981275918630592, -0.09357399148169626, -0.0575600053202741, 0.09299425156882071, 0.4093104365224741, -0.1883191817636494, -0.3625450515422691, 0.1004241524497047, -0.26015558101388875, -0.05485163403035072, 0.22662224927853766, -0.03432302130386233, ... |
710.2816 | A classification of some Finsler connections and their applications | Some general Finsler connections are defined. Emphasis is being made on the
Cartan tensor and its derivatives. Vanishing of the hv-curvature tensors of
these connections characterizes Landsbergian, Berwaldian as well as Riemannian
structures. This view point makes it possible to give a smart representation of
connect... | math.DG | some general finsler connections are defined emphasis is being made on the cartan tensor and its derivatives vanishing of the hvcurvature tensors of these connections characterizes landsbergian berwaldian as well as riemannian structures this view point makes it possible to give a smart representation of connection the... | [['some', 'general', 'finsler', 'connections', 'are', 'defined', 'emphasis', 'is', 'being', 'made', 'on', 'the', 'cartan', 'tensor', 'and', 'its', 'derivatives', 'vanishing', 'of', 'the', 'hvcurvature', 'tensors', 'of', 'these', 'connections', 'characterizes', 'landsbergian', 'berwaldian', 'as', 'well', 'as', 'riemanni... | [-0.1984307645382642, 0.059116249974591265, -0.054924148600548506, 0.1322068852005583, -0.20710126282365032, -0.17707892313289145, -0.035843120035927066, 0.39915110506681784, -0.2922895857782075, -0.23353075679165847, 0.14931082582122393, -0.27788620899346744, -0.2812589870652918, 0.16652734552961634, -0.13151942848608... |
710.2817 | Progress in the evaluation of the anti-B -> X_s gamma decay rate at NNLO | The theoretical status of NNLO QCD corrections to the inclusive radiative
anti-B -> X_s gamma decay in the standard model is briefly overviewed. Emphasis
is put on recent results for three-loop fermionic corrections to matrix
elements of the most relevant four-quark operators.
| hep-ph | the theoretical status of nnlo qcd corrections to the inclusive radiative antib x_s gamma decay in the standard model is briefly overviewed emphasis is put on recent results for threeloop fermionic corrections to matrix elements of the most relevant fourquark operators | [['the', 'theoretical', 'status', 'of', 'nnlo', 'qcd', 'corrections', 'to', 'the', 'inclusive', 'radiative', 'antib', 'x_s', 'gamma', 'decay', 'in', 'the', 'standard', 'model', 'is', 'briefly', 'overviewed', 'emphasis', 'is', 'put', 'on', 'recent', 'results', 'for', 'threeloop', 'fermionic', 'corrections', 'to', 'matri... | [-0.020608602364252254, 0.21126435804975832, -0.04424510153419361, 0.16093304374527823, -0.08633964434379666, -0.11788491832046974, 0.054092823595898905, 0.3006119727179771, -0.12990365165183548, -0.12097469887628061, 0.011983640665165716, -0.42198789128806535, -0.010737979353019378, 0.13525383147019213, 0.058785407463... |
710.2818 | Track finding in gamma conversions in CMS | A track finding algorithm has been developed for reconstruction of e+e-
pairs. It combines the information of the electromagnetic calorimeter with the
information provided by the Tracker. Results on reconstruction efficiency of
converted photons, as well as on fake rate are shown for single isolated
photons and for p... | physics.data-an hep-ex | a track finding algorithm has been developed for reconstruction of ee pairs it combines the information of the electromagnetic calorimeter with the information provided by the tracker results on reconstruction efficiency of converted photons as well as on fake rate are shown for single isolated photons and for photons ... | [['a', 'track', 'finding', 'algorithm', 'has', 'been', 'developed', 'for', 'reconstruction', 'of', 'ee', 'pairs', 'it', 'combines', 'the', 'information', 'of', 'the', 'electromagnetic', 'calorimeter', 'with', 'the', 'information', 'provided', 'by', 'the', 'tracker', 'results', 'on', 'reconstruction', 'efficiency', 'of'... | [-0.021776854599480547, 0.10493826006178654, -0.035578469242600184, 0.09210569047999959, -0.0040147262775609574, -0.12331940578446994, -0.029275098425005714, 0.42350989447966697, -0.15547620862602227, -0.4288785520400251, 0.050688251928095854, -0.420327533697409, 0.0502784498817017, 0.2560961926205745, 0.01627440425387... |
710.2819 | Fractional diffusion equation for aging and equilibrated random walks | We consider continuous time random walks (CTRW) and discuss situations
pertinent to aging. These correspond to the case when the initial state of the
system is known not at preparation (at $t=0$) but at the later instant of time
$t_1>0$ (intermediate-time initial condition). We derive the generalized aging
diffusion ... | cond-mat.stat-mech | we consider continuous time random walks ctrw and discuss situations pertinent to aging these correspond to the case when the initial state of the system is known not at preparation at t0 but at the later instant of time t_10 intermediatetime initial condition we derive the generalized aging diffusion equation for this... | [['we', 'consider', 'continuous', 'time', 'random', 'walks', 'ctrw', 'and', 'discuss', 'situations', 'pertinent', 'to', 'aging', 'these', 'correspond', 'to', 'the', 'case', 'when', 'the', 'initial', 'state', 'of', 'the', 'system', 'is', 'known', 'not', 'at', 'preparation', 'at', 't0', 'but', 'at', 'the', 'later', 'inst... | [-0.10240765015997395, 0.17094810742796776, -0.12235962244763819, 0.0646046727016329, -0.006711096704207562, -0.15666400201027156, 0.029863375511234375, 0.3534503990180186, -0.2710195092839894, -0.2513183716344773, 0.12878990415530908, -0.2412888562948619, -0.11984409835988756, 0.17285574219154975, -0.03533055354853639... |
710.282 | Resonant mode flopping in modulated waveguiding structures | We put forward the concept of resonant, Rabi-like flopping and adiabatic
transitions between confined light modes in properly modulated multimode
waveguides. The phenomenon is shown to take place in both, the linear and the
nonlinear regimes. In addition, we find that the mode transitions occur not
only in simple geo... | physics.optics nlin.PS | we put forward the concept of resonant rabilike flopping and adiabatic transitions between confined light modes in properly modulated multimode waveguides the phenomenon is shown to take place in both the linear and the nonlinear regimes in addition we find that the mode transitions occur not only in simple geometries ... | [['we', 'put', 'forward', 'the', 'concept', 'of', 'resonant', 'rabilike', 'flopping', 'and', 'adiabatic', 'transitions', 'between', 'confined', 'light', 'modes', 'in', 'properly', 'modulated', 'multimode', 'waveguides', 'the', 'phenomenon', 'is', 'shown', 'to', 'take', 'place', 'in', 'both', 'the', 'linear', 'and', 'th... | [-0.16224920285438277, 0.24214270968653567, -0.0821493117087712, 0.09960447433595992, -0.033351317191598555, -0.19953000383477096, 0.062441136621015324, 0.4194055667580807, -0.26121034579070873, -0.18745285979382795, 0.01968630911361375, -0.21587361935972657, -0.21151655157134958, 0.20544593728287783, -0.01803167510063... |
710.2821 | First Stiefel-Whitney class of real moduli spaces of stable maps to a
convex surface | Let $(X,c_X)$ be a convex projective surface equipped with a real structure.
The space of stable maps $\bar{\mathcal{M}}_{0,k}(X,d)$ carries different real
structures induced by $c_X$ and any order two element $\tau$ of permutation
group $S_k$ acting on marked points. Each corresponding real part
$\R_{\tau}\bar{\math... | math.AG math.AT | let xc_x be a convex projective surface equipped with a real structure the space of stable maps barmathcalm_0kxd carries different real structures induced by c_x and any order two element tau of permutation group s_k acting on marked points each corresponding real part r_taubarmathcalm_0kxd is a real normal projective ... | [['let', 'xc_x', 'be', 'a', 'convex', 'projective', 'surface', 'equipped', 'with', 'a', 'real', 'structure', 'the', 'space', 'of', 'stable', 'maps', 'barmathcalm_0kxd', 'carries', 'different', 'real', 'structures', 'induced', 'by', 'c_x', 'and', 'any', 'order', 'two', 'element', 'tau', 'of', 'permutation', 'group', 's_... | [-0.20463673296932863, 0.10962667436639248, -0.06088785941616815, 0.030871022443687456, -0.0703373480692645, -0.1271412388604378, -0.023962999261027882, 0.32888305030554255, -0.3027633058525204, -0.18553309155645492, 0.10861604795007854, -0.26274364429447694, -0.1596183542501634, 0.22535964461896463, -0.070351002589368... |
710.2822 | SFitter: Reconstructing the MSSM Lagrangian from LHC data | Once supersymmetry is found at the LHC, the question arises what are the
fundamental parameters of the Lagrangian. The answer to this question should
thereby not be biased by assumptions on high-scale models. SFitter is a tool
designed for this task. Taking LHC (and possibly ILC) data as input it scans
the TeV-scale ... | hep-ph | once supersymmetry is found at the lhc the question arises what are the fundamental parameters of the lagrangian the answer to this question should thereby not be biased by assumptions on highscale models sfitter is a tool designed for this task taking lhc and possibly ilc data as input it scans the tevscale mssm param... | [['once', 'supersymmetry', 'is', 'found', 'at', 'the', 'lhc', 'the', 'question', 'arises', 'what', 'are', 'the', 'fundamental', 'parameters', 'of', 'the', 'lagrangian', 'the', 'answer', 'to', 'this', 'question', 'should', 'thereby', 'not', 'be', 'biased', 'by', 'assumptions', 'on', 'highscale', 'models', 'sfitter', 'is... | [-0.04098974300550938, 0.12309642507624562, -0.09254449504297427, 0.17286691479184615, -0.1528528835424172, -0.20297757436030656, 0.05808238241501072, 0.3694892846528561, -0.2912779022659105, -0.32523427179624, 0.10800074354334864, -0.2241977108742601, -0.07025081727163045, 0.16256112020753163, -0.05022397899739845, 0.... |
710.2823 | On the Whitehead spectrum of the circle | The seminal work of Waldhausen, Farrell and Jones, Igusa, and Weiss and
Williams shows that the homotopy groups in low degrees of the space of
homeomorphisms of a closed Riemannian manifold of negative sectional curvature
can be expressed as a functor of the fundamental group of the manifold. To
determine this functo... | math.AT math.KT | the seminal work of waldhausen farrell and jones igusa and weiss and williams shows that the homotopy groups in low degrees of the space of homeomorphisms of a closed riemannian manifold of negative sectional curvature can be expressed as a functor of the fundamental group of the manifold to determine this functor howe... | [['the', 'seminal', 'work', 'of', 'waldhausen', 'farrell', 'and', 'jones', 'igusa', 'and', 'weiss', 'and', 'williams', 'shows', 'that', 'the', 'homotopy', 'groups', 'in', 'low', 'degrees', 'of', 'the', 'space', 'of', 'homeomorphisms', 'of', 'a', 'closed', 'riemannian', 'manifold', 'of', 'negative', 'sectional', 'curvat... | [-0.20119793201419747, 0.05934957695033171, -0.11939188910626053, 0.05267993446059769, -0.07189553530631765, -0.10048691321363938, 0.03863187036975952, 0.2933572096351002, -0.3302462746675398, -0.25833319457403076, 0.06819356983760372, -0.219332905205582, -0.16977250804137883, 0.1798397718812339, -0.19461611263076997, ... |
710.2824 | Polarization Retarder with Cylindrical-Symmetry for Radially Polarized
Light | We demonstrate a cylindrically-symmetric polarization retarder for generating
exact radially polarized light. It involves an uni-axial crystal whose
crystallographic optics axis is aligned to its optical axis. This method offers
high power-handling capability
| physics.optics | we demonstrate a cylindricallysymmetric polarization retarder for generating exact radially polarized light it involves an uniaxial crystal whose crystallographic optics axis is aligned to its optical axis this method offers high powerhandling capability | [['we', 'demonstrate', 'a', 'cylindricallysymmetric', 'polarization', 'retarder', 'for', 'generating', 'exact', 'radially', 'polarized', 'light', 'it', 'involves', 'an', 'uniaxial', 'crystal', 'whose', 'crystallographic', 'optics', 'axis', 'is', 'aligned', 'to', 'its', 'optical', 'axis', 'this', 'method', 'offers', 'hi... | [-0.20335488384025116, 0.15143986488383784, -0.08672273945888843, -0.0861204636254997, -0.17221248931618352, -0.17894102586433291, -0.05397454193073579, 0.6268474838950417, -0.29898490621285007, -0.20672265993374767, 0.016535121453643747, -0.22335991760094961, -0.08068299692857897, 0.23176425119692629, 0.03839956080033... |
710.2825 | Spatially extended PAHs in circumstellar disks around T Tauri and Herbig
Ae stars | Our aim is to determine the presence and location of the emission from
polycyclic aromatic hydrocarbons (PAHs) towards low and intermediate mass young
stars with disks using large aperture telescopes.
VLT-VISIR N-band spectra and VLT-ISAAC and VLT-NACO L-band spectra of 29
sources are presented, spectrally resolvin... | astro-ph | our aim is to determine the presence and location of the emission from polycyclic aromatic hydrocarbons pahs towards low and intermediate mass young stars with disks using large aperture telescopes vltvisir nband spectra and vltisaac and vltnaco lband spectra of 29 sources are presented spectrally resolving the 33 86 1... | [['our', 'aim', 'is', 'to', 'determine', 'the', 'presence', 'and', 'location', 'of', 'the', 'emission', 'from', 'polycyclic', 'aromatic', 'hydrocarbons', 'pahs', 'towards', 'low', 'and', 'intermediate', 'mass', 'young', 'stars', 'with', 'disks', 'using', 'large', 'aperture', 'telescopes', 'vltvisir', 'nband', 'spectra'... | [-0.01901647256801386, 0.09397606432186563, 0.017372374944018804, 0.04886638806070454, -0.01681437385684829, -0.12020965405610322, 0.0315750810689299, 0.4498730256370213, -0.1539258422836544, -0.36337383700086, 0.04977991134398586, -0.33295892811818234, 0.026643841779507106, 0.12424836010153294, -0.02163447927822871, -... |
710.2826 | Ferromagnetic resonance study of polycrystalline Fe_{1-x}V_x alloy thin
films | Ferromagnetic resonance has been used to study the magnetic properties and
magnetization dynamics of polycrystalline Fe$_{1-x}$V$_{x}$ alloy films with
$0\leq x < 0.7$. Films were produced by co-sputtering from separate Fe and V
targets, leading to a composition gradient across a Si substrate. FMR studies
were conduc... | cond-mat.mes-hall cond-mat.mtrl-sci | ferromagnetic resonance has been used to study the magnetic properties and magnetization dynamics of polycrystalline fe_1xv_x alloy films with 0leq x 07 films were produced by cosputtering from separate fe and v targets leading to a composition gradient across a si substrate fmr studies were conducted at room temperatu... | [['ferromagnetic', 'resonance', 'has', 'been', 'used', 'to', 'study', 'the', 'magnetic', 'properties', 'and', 'magnetization', 'dynamics', 'of', 'polycrystalline', 'fe_1xv_x', 'alloy', 'films', 'with', '0leq', 'x', '07', 'films', 'were', 'produced', 'by', 'cosputtering', 'from', 'separate', 'fe', 'and', 'v', 'targets',... | [-0.08678514058456609, 0.18357648360788037, -0.015033469672657942, -0.08241368730209375, -0.029383434002336704, -0.14838837714081532, 0.05325650856094925, 0.5009816063273894, -0.22145754577297913, -0.34152679762950067, 0.0265829291176296, -0.33161084951930925, -0.018168278773756402, 0.23528850194507916, 0.0909474881267... |
710.2827 | A high fidelity approximation of radial polarization conversion | We report a high fidelity (>90%) approximation of radial polarization
conversion using a birefringent lens. It offers the advantages of low-cost,
easy fabrication, alignment robustness and high laser power handling
capability.
| physics.optics | we report a high fidelity 90 approximation of radial polarization conversion using a birefringent lens it offers the advantages of lowcost easy fabrication alignment robustness and high laser power handling capability | [['we', 'report', 'a', 'high', 'fidelity', '90', 'approximation', 'of', 'radial', 'polarization', 'conversion', 'using', 'a', 'birefringent', 'lens', 'it', 'offers', 'the', 'advantages', 'of', 'lowcost', 'easy', 'fabrication', 'alignment', 'robustness', 'and', 'high', 'laser', 'power', 'handling', 'capability']] | [-0.19014353545442705, 0.05374316589516257, -0.04514161590486765, -0.05075894755822036, -0.14251786794873975, -0.18525364036641775, 0.09190650061974602, 0.5090263628911588, -0.19822126038132176, -0.34309760433050895, 0.023420239933916637, -0.21287467317175, -0.078884566983869, 0.22656629198501188, -0.06399234228076474,... |
710.2828 | Fermionic representation for the ferromagnetic Kondo lattice model --
diagrammatic study of spin-charge coupling effects on magnon excitations | A purely fermionic representation is introduced for the ferromagnetic Kondo
lattice model which allows conventional diagrammatic tools to be employed to
study correlation effects. Quantum 1/S corrections to magnon excitations are
investigated using a systematic inverse-degeneracy expansion scheme which
incorporates c... | cond-mat.str-el | a purely fermionic representation is introduced for the ferromagnetic kondo lattice model which allows conventional diagrammatic tools to be employed to study correlation effects quantum 1s corrections to magnon excitations are investigated using a systematic inversedegeneracy expansion scheme which incorporates correl... | [['a', 'purely', 'fermionic', 'representation', 'is', 'introduced', 'for', 'the', 'ferromagnetic', 'kondo', 'lattice', 'model', 'which', 'allows', 'conventional', 'diagrammatic', 'tools', 'to', 'be', 'employed', 'to', 'study', 'correlation', 'effects', 'quantum', '1s', 'corrections', 'to', 'magnon', 'excitations', 'are... | [-0.16930869966625361, 0.18607248598949733, -0.07343394975129937, 0.09647998226489679, -0.11767787391982358, -0.13201416549800904, 0.04572168508419748, 0.34931876538465395, -0.24234369489335522, -0.225004678342453, -0.031240799931746898, -0.34764991373501203, -0.11945960122537463, 0.13336954357765002, 0.090152573435730... |
710.2829 | Nonequilibrium critical dynamics of the two-dimensional Ising model
quenched from a correlated initial state | The universality class, even the order of the transition, of the
two-dimensional Ising model depends on the range and the symmetry of the
interactions (Onsager model, Baxter-Wu model, Turban model, etc.), but the
critical temperature is generally the same due to self-duality. Here we
consider a sudden change in the f... | cond-mat.stat-mech | the universality class even the order of the transition of the twodimensional ising model depends on the range and the symmetry of the interactions onsager model baxterwu model turban model etc but the critical temperature is generally the same due to selfduality here we consider a sudden change in the form of the inte... | [['the', 'universality', 'class', 'even', 'the', 'order', 'of', 'the', 'transition', 'of', 'the', 'twodimensional', 'ising', 'model', 'depends', 'on', 'the', 'range', 'and', 'the', 'symmetry', 'of', 'the', 'interactions', 'onsager', 'model', 'baxterwu', 'model', 'turban', 'model', 'etc', 'but', 'the', 'critical', 'temp... | [-0.1406373688543081, 0.18054863863346196, -0.07630346722711243, 0.05271016793522369, -0.021382049570993048, -0.13941014752622463, 0.025172932515132057, 0.28897858596978154, -0.2729800486578318, -0.277859439967757, 0.07464253552589259, -0.28472152119022365, -0.15091022973899373, 0.14519096216542127, 0.08844581586125753... |
710.283 | Precision extraction of a_nn from pi- d --> n n gamma using chiral
perturbation theory | The neutron-neutron scattering length a_nn provides a sensitive probe of
charge-symmetry breaking in the strong interaction. Here we summarize our
recent efforts to use chiral perturbation theory in order to systematically
relate a_nn to the shape of the neutron spectrum in the reaction pi- d --> n n
gamma. In partic... | nucl-th hep-ph | the neutronneutron scattering length a_nn provides a sensitive probe of chargesymmetry breaking in the strong interaction here we summarize our recent efforts to use chiral perturbation theory in order to systematically relate a_nn to the shape of the neutron spectrum in the reaction pi d n n gamma in particular we sho... | [['the', 'neutronneutron', 'scattering', 'length', 'a_nn', 'provides', 'a', 'sensitive', 'probe', 'of', 'chargesymmetry', 'breaking', 'in', 'the', 'strong', 'interaction', 'here', 'we', 'summarize', 'our', 'recent', 'efforts', 'to', 'use', 'chiral', 'perturbation', 'theory', 'in', 'order', 'to', 'systematically', 'rela... | [-0.12661787610790715, 0.208767042176314, -0.10878550019468122, 0.06376344154781204, -0.05130456795725297, -0.08394718649393813, 0.05816571229397811, 0.3099066631531152, -0.2483038745131197, -0.2632603856760598, -0.053094666291717586, -0.3338088180493301, -0.09988777310492133, 0.11063525401877136, 0.05267952118567595, ... |
710.2831 | Quantum dynamics in phase space: From coherent states to the Gaussian
representation | We give an outlook on the future of coherence theory and many-body quantum
dynamics as experiments develop in the arena of ultra-cold atoms. Novel results
on quantum heating of center-of-mass temperature in evaporative cooling and
simulation methods for long-range interactions are obtained, using positive-P
phase-spa... | cond-mat.other cond-mat.stat-mech | we give an outlook on the future of coherence theory and manybody quantum dynamics as experiments develop in the arena of ultracold atoms novel results on quantum heating of centerofmass temperature in evaporative cooling and simulation methods for longrange interactions are obtained using positivep phasespace techniqu... | [['we', 'give', 'an', 'outlook', 'on', 'the', 'future', 'of', 'coherence', 'theory', 'and', 'manybody', 'quantum', 'dynamics', 'as', 'experiments', 'develop', 'in', 'the', 'arena', 'of', 'ultracold', 'atoms', 'novel', 'results', 'on', 'quantum', 'heating', 'of', 'centerofmass', 'temperature', 'in', 'evaporative', 'cool... | [-0.10362718105518623, 0.22937815748034907, -0.10930449922655142, 0.04703055014428885, 0.05092831964240126, -0.12425270413412996, 0.004894045158795527, 0.3970867250033695, -0.20249852938982454, -0.2605455309031126, -0.0007109926638962781, -0.30159895907601586, -0.08827163347893435, 0.2906602603261885, 0.048567535639133... |
710.2832 | Schr\"odinger operator with periodic plus compactly supported potentials
on the half-line | We consider the Schr\"odinger operator $H$ with a periodic potential $p$ plus
a compactly supported potential $q$ on the half-line. We prove the following
results: 1) a forbidden domain for the resonances is specified, 2) asymptotics
of the resonance-counting function is determined, 3) in each nondegenerate gap
$\g_n... | math-ph math.MP | we consider the schrodinger operator h with a periodic potential p plus a compactly supported potential q on the halfline we prove the following results 1 a forbidden domain for the resonances is specified 2 asymptotics of the resonancecounting function is determined 3 in each nondegenerate gap g_n for n large enough t... | [['we', 'consider', 'the', 'schrodinger', 'operator', 'h', 'with', 'a', 'periodic', 'potential', 'p', 'plus', 'a', 'compactly', 'supported', 'potential', 'q', 'on', 'the', 'halfline', 'we', 'prove', 'the', 'following', 'results', '1', 'a', 'forbidden', 'domain', 'for', 'the', 'resonances', 'is', 'specified', '2', 'asym... | [-0.20464059947254626, 0.2118173447684967, -0.026180812533895828, 0.06853000972677316, 0.046421263862009114, -0.2217888320355039, 0.019315921056304912, 0.3436219040696558, -0.2389383108061003, -0.26732085096698843, 0.05969379954775305, -0.3718914719200448, -0.06829712070818794, 0.09494634386348097, 0.03299641473659951,... |
710.2833 | Marchenko-Ostrovski mappings for periodic Jacobi matrices | We consider the 1D periodic Jacobi matrices. The spectrum of this operator is
purely absolutely continuous and consists of intervals separated by gaps. We
solve the inverse problem (including characterization) in terms of vertical
slits on the quasimomentum domain . Furthermore, we obtain a priori two-sided
estimates... | math-ph math.MP math.SP | we consider the 1d periodic jacobi matrices the spectrum of this operator is purely absolutely continuous and consists of intervals separated by gaps we solve the inverse problem including characterization in terms of vertical slits on the quasimomentum domain furthermore we obtain a priori twosided estimates for verti... | [['we', 'consider', 'the', '1d', 'periodic', 'jacobi', 'matrices', 'the', 'spectrum', 'of', 'this', 'operator', 'is', 'purely', 'absolutely', 'continuous', 'and', 'consists', 'of', 'intervals', 'separated', 'by', 'gaps', 'we', 'solve', 'the', 'inverse', 'problem', 'including', 'characterization', 'in', 'terms', 'of', '... | [-0.17185179629639066, 0.08665018816720005, -0.029845023501871362, 0.06015685576669596, -0.0421168802788964, -0.08108962267956317, 0.023526815236201166, 0.41297298214501804, -0.29428342622877274, -0.2148053734563291, 0.1255100684249084, -0.25758186517352305, -0.09232406580337772, 0.2006588068411306, -0.0641736332499594... |
710.2834 | Fermion masses and neutrino mixing in an U(1)_H flavor symmetry model
with hierarchical radiative generation for light charged fermion masses | I report the analysis performed on fermion masses and mixing, including
neutrino mixing, within the context of a model with hierarchical radiative mass
generation mechanism for light charged fermions, mediated by exotic scalar
particles at one and two loops, respectively, meanwhile the neutrinos get
Majorana mass ter... | hep-ph | i report the analysis performed on fermion masses and mixing including neutrino mixing within the context of a model with hierarchical radiative mass generation mechanism for light charged fermions mediated by exotic scalar particles at one and two loops respectively meanwhile the neutrinos get majorana mass terms at t... | [['i', 'report', 'the', 'analysis', 'performed', 'on', 'fermion', 'masses', 'and', 'mixing', 'including', 'neutrino', 'mixing', 'within', 'the', 'context', 'of', 'a', 'model', 'with', 'hierarchical', 'radiative', 'mass', 'generation', 'mechanism', 'for', 'light', 'charged', 'fermions', 'mediated', 'by', 'exotic', 'scal... | [-0.10931979982450189, 0.3424416349720122, 0.09082917414621607, 0.14996445093547742, 0.0015166517039321267, -0.17929736857578285, 0.0850285752648635, 0.3023940116854568, -0.16274269875148992, -0.38532123219845377, 0.03737957534268339, -0.3255292242352927, 0.019800288906488807, 0.1373464844335478, 0.0807018006418316, 0.... |
710.2835 | Folksonomies and clustering in the collaborative system CiteULike | We analyze CiteULike, an online collaborative tagging system where users
bookmark and annotate scientific papers. Such a system can be naturally
represented as a tripartite graph whose nodes represent papers, users and tags
connected by individual tag assignments. The semantics of tags is studied here,
in order to un... | physics.soc-ph physics.data-an | we analyze citeulike an online collaborative tagging system where users bookmark and annotate scientific papers such a system can be naturally represented as a tripartite graph whose nodes represent papers users and tags connected by individual tag assignments the semantics of tags is studied here in order to uncover t... | [['we', 'analyze', 'citeulike', 'an', 'online', 'collaborative', 'tagging', 'system', 'where', 'users', 'bookmark', 'and', 'annotate', 'scientific', 'papers', 'such', 'a', 'system', 'can', 'be', 'naturally', 'represented', 'as', 'a', 'tripartite', 'graph', 'whose', 'nodes', 'represent', 'papers', 'users', 'and', 'tags'... | [-0.11114510251407898, 0.0432153398629985, -0.043434065005673865, 0.11106620158392527, -0.19068783650560894, -0.19838941191527537, 0.10262072468659182, 0.40771420735286595, -0.281689085276434, -0.39035034122899537, -0.010400474504510895, -0.38624845190746027, -0.17373338741500202, 0.11177784413462732, -0.07974316116149... |
710.2836 | Topological entropies of equivalent smooth flows | Two flows defined on a smooth manifold are equivalent if there exists a
homeomorphism of the manifold that sends each orbit of one flow onto an orbit
of the other flow while preserving the time orientation. The topological
entropy of a flow is defined as the entropy of its time-1 map. While
topological entropy is an ... | math.DS | two flows defined on a smooth manifold are equivalent if there exists a homeomorphism of the manifold that sends each orbit of one flow onto an orbit of the other flow while preserving the time orientation the topological entropy of a flow is defined as the entropy of its time1 map while topological entropy is an invar... | [['two', 'flows', 'defined', 'on', 'a', 'smooth', 'manifold', 'are', 'equivalent', 'if', 'there', 'exists', 'a', 'homeomorphism', 'of', 'the', 'manifold', 'that', 'sends', 'each', 'orbit', 'of', 'one', 'flow', 'onto', 'an', 'orbit', 'of', 'the', 'other', 'flow', 'while', 'preserving', 'the', 'time', 'orientation', 'the... | [-0.1939063108655397, 0.1674110209015109, -0.10746343746228794, 0.06948672456201166, -0.04008890212286246, -0.2125421174195858, -0.01288969435062901, 0.33925700035730477, -0.30918483551074727, -0.16373186993844915, 0.11497052100489281, -0.318855533471585, -0.11708826488819704, 0.18123067474286808, -0.15279447950387115,... |
710.2837 | Overhauser effect in individual InP/GaInP dots | Sizable nuclear spin polarization is pumped in individual InP/GaInP dots in a
wide range of external magnetic fields B_ext=0-5T by circularly polarized
optical excitation. We observe nuclear polarization of up to ~40% at Bext=1.5T
and corresponding to an Overhauser field of ~1.2T. We find a strong feedback of
the nuc... | cond-mat.mes-hall cond-mat.mtrl-sci | sizable nuclear spin polarization is pumped in individual inpgainp dots in a wide range of external magnetic fields b_ext05t by circularly polarized optical excitation we observe nuclear polarization of up to 40 at bext15t and corresponding to an overhauser field of 12t we find a strong feedback of the nuclear spin on ... | [['sizable', 'nuclear', 'spin', 'polarization', 'is', 'pumped', 'in', 'individual', 'inpgainp', 'dots', 'in', 'a', 'wide', 'range', 'of', 'external', 'magnetic', 'fields', 'b_ext05t', 'by', 'circularly', 'polarized', 'optical', 'excitation', 'we', 'observe', 'nuclear', 'polarization', 'of', 'up', 'to', '40', 'at', 'bex... | [-0.18462223562840205, 0.25269993476116986, 0.0043294100489999566, 0.06003920274088159, -0.005444197688900333, -0.09104529938797766, 0.012918834581796546, 0.43777100232961985, -0.28298122356084476, -0.34967151907871347, -0.07787780790386023, -0.2334824582877835, -0.004306607817332926, 0.2180194540165498, 0.056189480137... |
710.2838 | Experimental Precision Tests for the Electroweak Standard Model | This paper contains a review of recent precision measurements of electroweak
observables and resulting tests of the electroweak Standard Model.
| hep-ex | this paper contains a review of recent precision measurements of electroweak observables and resulting tests of the electroweak standard model | [['this', 'paper', 'contains', 'a', 'review', 'of', 'recent', 'precision', 'measurements', 'of', 'electroweak', 'observables', 'and', 'resulting', 'tests', 'of', 'the', 'electroweak', 'standard', 'model']] | [-0.06960717719048262, 0.1841369532601675, -0.07051394702866673, 0.005949176632566377, -0.02999122077599168, -0.1087121065473184, 0.03565199697040953, 0.24300193525850772, -0.19975716918706893, -0.3187972826883197, 0.08389039393514394, -0.29512891490012405, -0.0509537685662508, 0.14234589551342652, -0.01279188492335379... |
710.2839 | Magnetic field evolution in neutron stars | Neutron stars contain persistent, ordered magnetic fields that are the
strongest known in the Universe. However, their magnetic fluxes are similar to
those in magnetic A and B stars and white dwarfs, suggesting that flux
conservation during gravitational collapse may play an important role in
establishing the field, ... | astro-ph | neutron stars contain persistent ordered magnetic fields that are the strongest known in the universe however their magnetic fluxes are similar to those in magnetic a and b stars and white dwarfs suggesting that flux conservation during gravitational collapse may play an important role in establishing the field althoug... | [['neutron', 'stars', 'contain', 'persistent', 'ordered', 'magnetic', 'fields', 'that', 'are', 'the', 'strongest', 'known', 'in', 'the', 'universe', 'however', 'their', 'magnetic', 'fluxes', 'are', 'similar', 'to', 'those', 'in', 'magnetic', 'a', 'and', 'b', 'stars', 'and', 'white', 'dwarfs', 'suggesting', 'that', 'flu... | [-0.1420058344008625, 0.2562215127124193, -0.04268432983427558, 0.1586558419887913, -0.08821221112618427, -0.04819342492484167, -0.014122776324540133, 0.34701086919311985, -0.2469909210527784, -0.35312408803678447, 0.044430023794001364, -0.20406580536214056, -0.04208773503314114, 0.2046799533415199, -0.0036263067639163... |
710.284 | Effective Action, Conformal Anomaly and the Issue of Quadratic
Divergences | For massless $\phi^4$ theory, we explicitly compute the lowest order
non-local contributions to the one-loop effective action required for the
determination of the trace anomaly. Imposing exact conformal invariance of the
local part of the effective action, we argue that the issue of quadratic
divergences does not ar... | hep-th | for massless phi4 theory we explicitly compute the lowest order nonlocal contributions to the oneloop effective action required for the determination of the trace anomaly imposing exact conformal invariance of the local part of the effective action we argue that the issue of quadratic divergences does not arise in a th... | [['for', 'massless', 'phi4', 'theory', 'we', 'explicitly', 'compute', 'the', 'lowest', 'order', 'nonlocal', 'contributions', 'to', 'the', 'oneloop', 'effective', 'action', 'required', 'for', 'the', 'determination', 'of', 'the', 'trace', 'anomaly', 'imposing', 'exact', 'conformal', 'invariance', 'of', 'the', 'local', 'p... | [-0.16656411820212785, 0.19542659029526555, -0.05945503836568526, 0.1489548608539221, -0.12018921064901288, -0.14004711294749184, 0.007394339852844892, 0.3013215505963434, -0.25604516863418014, -0.30395977144008096, 0.09040038692530841, -0.24032758475969668, -0.13963659055045116, 0.07230815970865281, 0.0479453333618553... |
710.2841 | Interplay of causticity and vorticality within the complex quantum
Hamilton-Jacobi formalism | Interference dynamics is analyzed in the light of the complex quantum
Hamilton-Jacobi formalism, using as a working model the collision of two
Gaussian wave packets. Though simple, this model nicely shows that interference
in quantum scattering processes gives rise to rich dynamics and trajectory
topologies in the co... | quant-ph | interference dynamics is analyzed in the light of the complex quantum hamiltonjacobi formalism using as a working model the collision of two gaussian wave packets though simple this model nicely shows that interference in quantum scattering processes gives rise to rich dynamics and trajectory topologies in the complex ... | [['interference', 'dynamics', 'is', 'analyzed', 'in', 'the', 'light', 'of', 'the', 'complex', 'quantum', 'hamiltonjacobi', 'formalism', 'using', 'as', 'a', 'working', 'model', 'the', 'collision', 'of', 'two', 'gaussian', 'wave', 'packets', 'though', 'simple', 'this', 'model', 'nicely', 'shows', 'that', 'interference', ... | [-0.1794438336609288, 0.13672756415217782, -0.12378557031835488, 0.10367667076046386, -0.036377047391687616, -0.14537836728924688, 0.0054868959692960725, 0.35840650307054217, -0.27595636702360626, -0.2417345150730553, 0.02322665437625008, -0.26960438811666076, -0.2054058958558326, 0.18817098904896448, 0.019366259741141... |
710.2842 | Coherence and Correlations in Atom Lasers | We review and characterize the quantum coherence measures that are most
useful for quantum gases, including Bose-Einstein condensates (BEC) and
ultra-cold fermions, and outline how to calculate these in the typically
dynamical environment of an interacting multi-mode quantum gas.
| cond-mat.other cond-mat.stat-mech | we review and characterize the quantum coherence measures that are most useful for quantum gases including boseeinstein condensates bec and ultracold fermions and outline how to calculate these in the typically dynamical environment of an interacting multimode quantum gas | [['we', 'review', 'and', 'characterize', 'the', 'quantum', 'coherence', 'measures', 'that', 'are', 'most', 'useful', 'for', 'quantum', 'gases', 'including', 'boseeinstein', 'condensates', 'bec', 'and', 'ultracold', 'fermions', 'and', 'outline', 'how', 'to', 'calculate', 'these', 'in', 'the', 'typically', 'dynamical', '... | [-0.12553301378517437, 0.31510259991083356, -0.06845653687532131, 0.10105604625557764, 0.0720713907518448, -0.20655520763307905, -0.019117983577486414, 0.3648316258421311, -0.1852159800921352, -0.18726310421688816, 0.03147217474627094, -0.29008188967903453, -0.1246530699949616, 0.2358287580144138, 0.02215593074185726, ... |
710.2843 | Relativistic time dilatation and the spectrum of electrons emitted by 33
TeV lead ions penetrating thin foils | We study the energy distribution of ultrarelativistic electrons produced when
a beam of 33 TeV Pb$^{81+}$(1s) ions penetrates a thin Al foil. We show that,
because of a prominent role of the excitations of the ions inside the foil
which becomes possible due to the relativistic time dilatation, the width of
this distr... | physics.atom-ph physics.acc-ph | we study the energy distribution of ultrarelativistic electrons produced when a beam of 33 tev pb811s ions penetrates a thin al foil we show that because of a prominent role of the excitations of the ions inside the foil which becomes possible due to the relativistic time dilatation the width of this distribution can b... | [['we', 'study', 'the', 'energy', 'distribution', 'of', 'ultrarelativistic', 'electrons', 'produced', 'when', 'a', 'beam', 'of', '33', 'tev', 'pb811s', 'ions', 'penetrates', 'a', 'thin', 'al', 'foil', 'we', 'show', 'that', 'because', 'of', 'a', 'prominent', 'role', 'of', 'the', 'excitations', 'of', 'the', 'ions', 'insi... | [-0.05842879959031841, 0.22329158777272148, -0.06647122318370152, 0.11581532837950781, -0.008377712642345412, -0.12169829688850889, 0.0069291195296476375, 0.4127307834219089, -0.2500995004186984, -0.3261165432183822, -0.009946743138670196, -0.3248821214846937, 0.016614062433435984, 0.17769395859119538, 0.01763794615666... |
710.2844 | Does a particle swept by a turbulent liquid diffuse? | Since the famous 1926 paper by Richardson, the relative diffusion of two
particles in a turbulent liquid has attracted a lot of interest. The motion of
a single particle on the other hand is usually considered not to be especially
interesting. The widely accepted picture is that the velocity of the particle
has short... | cond-mat.stat-mech | since the famous 1926 paper by richardson the relative diffusion of two particles in a turbulent liquid has attracted a lot of interest the motion of a single particle on the other hand is usually considered not to be especially interesting the widely accepted picture is that the velocity of the particle has shortrange... | [['since', 'the', 'famous', '1926', 'paper', 'by', 'richardson', 'the', 'relative', 'diffusion', 'of', 'two', 'particles', 'in', 'a', 'turbulent', 'liquid', 'has', 'attracted', 'a', 'lot', 'of', 'interest', 'the', 'motion', 'of', 'a', 'single', 'particle', 'on', 'the', 'other', 'hand', 'is', 'usually', 'considered', 'n... | [-0.1278451997970574, 0.20888609228974306, -0.11719973464578129, 0.04824278671028942, -0.0647449926820404, -0.12798809660435245, -0.04384961135158511, 0.3382837863214183, -0.2901650480762647, -0.2783313715797767, 0.09341275765920025, -0.2748365920167743, -0.0932152032558071, 0.1867206606446161, -0.037987470749373496, 0... |
710.2845 | Current saturation and Coulomb interactions in organic single-crystal
transistors | Electronic transport through rubrene single-crystal field effect transistors
(FETs) is investigated experimentally in the high carrier density regime (n ~
0.1 carrier/molecule). In this regime, we find that the current does not
increase linearly with the density of charge carriers, and tends to saturate.
At the same ... | cond-mat.str-el cond-mat.mtrl-sci | electronic transport through rubrene singlecrystal field effect transistors fets is investigated experimentally in the high carrier density regime n 01 carriermolecule in this regime we find that the current does not increase linearly with the density of charge carriers and tends to saturate at the same time the activa... | [['electronic', 'transport', 'through', 'rubrene', 'singlecrystal', 'field', 'effect', 'transistors', 'fets', 'is', 'investigated', 'experimentally', 'in', 'the', 'high', 'carrier', 'density', 'regime', 'n', '01', 'carriermolecule', 'in', 'this', 'regime', 'we', 'find', 'that', 'the', 'current', 'does', 'not', 'increas... | [-0.14879117805450673, 0.19933232953471522, -0.039963376698314505, 0.0008659907566603794, 0.021651018656269515, -0.13764191668240294, 0.10085313765692615, 0.3849069748514442, -0.2211301108391615, -0.3101156686072148, -0.029261897404437825, -0.3294706871052102, -0.13751166895712896, 0.1923987344145194, 0.016630469651151... |
710.2846 | Two-photon decay of heavy quarkonium from heavy-quark spin symmetry | With the recent measurements on $\eta_{c}$ and $\eta_{c}^{\prime}$ at CLEO,
Babar and Belle, and with the prospect of finding the $\eta_{b}$ at the
Tevatron, it seems appropriate to have another look at the two-photon decay of
heavy quarkonium from the standpoint of an effective Lagrangian based on local
operator exp... | hep-ph | with the recent measurements on eta_c and eta_cprime at cleo babar and belle and with the prospect of finding the eta_b at the tevatron it seems appropriate to have another look at the twophoton decay of heavy quarkonium from the standpoint of an effective lagrangian based on local operator expansion and heavyquark spi... | [['with', 'the', 'recent', 'measurements', 'on', 'eta_c', 'and', 'eta_cprime', 'at', 'cleo', 'babar', 'and', 'belle', 'and', 'with', 'the', 'prospect', 'of', 'finding', 'the', 'eta_b', 'at', 'the', 'tevatron', 'it', 'seems', 'appropriate', 'to', 'have', 'another', 'look', 'at', 'the', 'twophoton', 'decay', 'of', 'heavy... | [-0.04360127928455106, 0.21399867089320498, -0.09523533326089866, 0.09657027090025776, -0.05596360078613673, -0.13463851371356708, 0.09749854770912365, 0.34289277941230445, -0.1826405798405554, -0.22711476396055674, -0.011210488395118337, -0.3529500556299342, 0.01734329032252071, 0.14361332450062037, 0.1040196069637192... |
710.2847 | A synchrotron self-Compton scenario for the very high energy gamma-ray
emission of the radiogalaxy M87 | M87 is the first extragalactic source detected in the TeV range that is not a
blazar. With the increasing performances of ground-based Cherenkov telescopes,
we can now probe the variability in the gamma-ray flux at small timescales,
thus putting strong constraints on the size of the emitting zone. A
modification of s... | astro-ph | m87 is the first extragalactic source detected in the tev range that is not a blazar with the increasing performances of groundbased cherenkov telescopes we can now probe the variability in the gammaray flux at small timescales thus putting strong constraints on the size of the emitting zone a modification of standard ... | [['m87', 'is', 'the', 'first', 'extragalactic', 'source', 'detected', 'in', 'the', 'tev', 'range', 'that', 'is', 'not', 'a', 'blazar', 'with', 'the', 'increasing', 'performances', 'of', 'groundbased', 'cherenkov', 'telescopes', 'we', 'can', 'now', 'probe', 'the', 'variability', 'in', 'the', 'gammaray', 'flux', 'at', 's... | [-0.07651185010712193, 0.15000322097649524, -0.025995067879903827, 0.14950626803913455, -0.13524161697777343, -0.1317189364697521, -0.013628590262263882, 0.44356124461749674, -0.17415255162913393, -0.37482897899213996, 0.04480277915003962, -0.2809315907542133, 0.04547104184501925, 0.23890596046285587, -0.00793374114415... |
710.2848 | Consistency of trace norm minimization | Regularization by the sum of singular values, also referred to as the trace
norm, is a popular technique for estimating low rank rectangular matrices. In
this paper, we extend some of the consistency results of the Lasso to provide
necessary and sufficient conditions for rank consistency of trace norm
minimization wi... | cs.LG | regularization by the sum of singular values also referred to as the trace norm is a popular technique for estimating low rank rectangular matrices in this paper we extend some of the consistency results of the lasso to provide necessary and sufficient conditions for rank consistency of trace norm minimization with the... | [['regularization', 'by', 'the', 'sum', 'of', 'singular', 'values', 'also', 'referred', 'to', 'as', 'the', 'trace', 'norm', 'is', 'a', 'popular', 'technique', 'for', 'estimating', 'low', 'rank', 'rectangular', 'matrices', 'in', 'this', 'paper', 'we', 'extend', 'some', 'of', 'the', 'consistency', 'results', 'of', 'the',... | [-0.06651078592743967, 0.03954753510570063, -0.06982767909187702, 0.1256681005682119, -0.07033542095526278, -0.16327859227267372, -0.007224707929236064, 0.38263804194602097, -0.25577029656292266, -0.22837570813399824, 0.2156123892606732, -0.19456654975747134, -0.17126018013321348, 0.13690467827118835, -0.14724492695327... |
710.2849 | NA57 main results | The CERN NA57 experiment was designed to study the production of strange and
multi-strange particles in heavy ion collisions at SPS energies; its physics
programme is essentially completed. A review of the main results is presented.
| nucl-ex | the cern na57 experiment was designed to study the production of strange and multistrange particles in heavy ion collisions at sps energies its physics programme is essentially completed a review of the main results is presented | [['the', 'cern', 'na57', 'experiment', 'was', 'designed', 'to', 'study', 'the', 'production', 'of', 'strange', 'and', 'multistrange', 'particles', 'in', 'heavy', 'ion', 'collisions', 'at', 'sps', 'energies', 'its', 'physics', 'programme', 'is', 'essentially', 'completed', 'a', 'review', 'of', 'the', 'main', 'results', ... | [-0.04125608100245396, 0.27535593637730926, -0.18974773770767367, 0.11762898873874089, 0.02487140754237771, -0.1084829886806094, -0.0731621687559204, 0.2659314652490947, -0.15494637932473174, -0.30153069909041125, -0.009980125446519297, -0.3847599686123431, 0.09257277039190133, 0.15432831747198683, 0.03654101467691362,... |
710.285 | Local SU(5) Unification in 6D from the Heterotic String | We present a six-dimensional T^2/Z_2 orbifold model which arises as an
intermediate step in the compactification of the heterotic string to the MSSM.
The orbifold contains two pairs of inequivalent fixed points, with unbroken
local gauge groups SU(5) and SU(2)xSU(4), respectively, the intersection of
which gives the ... | hep-ph | we present a sixdimensional t2z_2 orbifold model which arises as an intermediate step in the compactification of the heterotic string to the mssm the orbifold contains two pairs of inequivalent fixed points with unbroken local gauge groups su5 and su2xsu4 respectively the intersection of which gives the standard model ... | [['we', 'present', 'a', 'sixdimensional', 't2z_2', 'orbifold', 'model', 'which', 'arises', 'as', 'an', 'intermediate', 'step', 'in', 'the', 'compactification', 'of', 'the', 'heterotic', 'string', 'to', 'the', 'mssm', 'the', 'orbifold', 'contains', 'two', 'pairs', 'of', 'inequivalent', 'fixed', 'points', 'with', 'unbrok... | [-0.1781657585227976, 0.19186369159418676, -0.02963713583137308, 0.11514053692950924, -0.08555089379423203, -0.19640866287850908, 0.04913142183082825, 0.311068707031711, -0.2058504461738452, -0.268373013851803, 0.06416946141481665, -0.26473138959869286, -0.0663147966914373, 0.04354515288984973, -0.046443997673234164, -... |
710.2851 | CP asymmetries at D0 | Using two independent measurements of the semileptonic CP asymmetry in the
$B_s$ system, we constrain the CP violating phase of the $B_s$ system to be
$\phi_s = -0.70^{+0.47}_{-0.39}$. The data sample corresponds to an integrated
luminosity of 1.1 fb$^{-1}$ accumulated with D0 detector at the Fermilab
Tevatron collid... | hep-ex | using two independent measurements of the semileptonic cp asymmetry in the b_s system we constrain the cp violating phase of the b_s system to be phi_s 070047_039 the data sample corresponds to an integrated luminosity of 11 fb1 accumulated with d0 detector at the fermilab tevatron collider we also measure the direct c... | [['using', 'two', 'independent', 'measurements', 'of', 'the', 'semileptonic', 'cp', 'asymmetry', 'in', 'the', 'b_s', 'system', 'we', 'constrain', 'the', 'cp', 'violating', 'phase', 'of', 'the', 'b_s', 'system', 'to', 'be', 'phi_s', '070047_039', 'the', 'data', 'sample', 'corresponds', 'to', 'an', 'integrated', 'luminos... | [-0.07941442320146892, 0.19683873268246616, -0.08338570432690313, 0.07210295201762568, -0.08634766582635385, -0.12171464913253542, 0.08758285971759242, 0.28005160174415084, -0.21689476058641566, -0.30012586241281486, -0.013700447563977935, -0.43493396156361397, 0.15529103465142508, 0.12568401999453294, 0.09069819402987... |
710.2852 | Generating models for temporal representations | We discuss the use of model building for temporal representations. We chose
Polish to illustrate our discussion because it has an interesting aspectual
system, but the points we wish to make are not language specific. Rather, our
goal is to develop theoretical and computational tools for temporal model
building tasks... | cs.CL | we discuss the use of model building for temporal representations we chose polish to illustrate our discussion because it has an interesting aspectual system but the points we wish to make are not language specific rather our goal is to develop theoretical and computational tools for temporal model building tasks in co... | [['we', 'discuss', 'the', 'use', 'of', 'model', 'building', 'for', 'temporal', 'representations', 'we', 'chose', 'polish', 'to', 'illustrate', 'our', 'discussion', 'because', 'it', 'has', 'an', 'interesting', 'aspectual', 'system', 'but', 'the', 'points', 'we', 'wish', 'to', 'make', 'are', 'not', 'language', 'specific'... | [-0.06180206651451311, 0.04082570237259268, -0.12886732402775022, 0.13703700338109312, -0.1722266141118275, -0.16892760073427449, 0.06054181028086918, 0.43722357928771716, -0.268788732550662, -0.3285910454249442, 0.05266880141829865, -0.25956340009026757, -0.16994526813916785, 0.15055989191368824, -0.12428204761818051,... |
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