id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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706.2914 | Comment on "Infrared freezing of Euclidean QCD observables" | Recently, P. M. Brooks and C.J. Maxwell [Phys. Rev. D{\bf 74} 065012 (2006)]
claimed that the Landau pole of the one-loop coupling at $Q^2=\Lambda^2$ is
absent from the leading one-chain term in a skeleton expansion of the Euclidean
Adler ${\cal D}$ function. Moreover, in this approximation one has continuity
along t... | hep-ph | recently p m brooks and cj maxwell phys rev dbf 74 065012 2006 claimed that the landau pole of the oneloop coupling at q2lambda2 is absent from the leading onechain term in a skeleton expansion of the euclidean adler cal d function moreover in this approximation one has continuity along the euclidean axis and a smooth ... | [['recently', 'p', 'm', 'brooks', 'and', 'cj', 'maxwell', 'phys', 'rev', 'dbf', '74', '065012', '2006', 'claimed', 'that', 'the', 'landau', 'pole', 'of', 'the', 'oneloop', 'coupling', 'at', 'q2lambda2', 'is', 'absent', 'from', 'the', 'leading', 'onechain', 'term', 'in', 'a', 'skeleton', 'expansion', 'of', 'the', 'eucli... | [-0.1301923331704789, 0.0807922155862408, -0.12304426702626405, 0.05494976200362933, -0.09959080131458385, -0.07406538153466369, 0.06268757344001816, 0.27625439662841106, -0.2388934421098037, -0.24002670374632415, 0.025541279752117892, -0.25313688699776926, -0.184330679582698, 0.1128222039191141, -0.05943268116208769, ... |
706.2915 | Interplay between structure and density anomaly for an isotropic
core-softened ramp-like potential | Using molecular dynamics simulations and integral equations we investigate
the structure, the thermodynamics and the dynamics of a system of particles
interacting through a continuous core- softened ramp-like interparticle
potential. We found density, dynamic and structural anomalies similar to that
found in water. A... | cond-mat.stat-mech cond-mat.soft | using molecular dynamics simulations and integral equations we investigate the structure the thermodynamics and the dynamics of a system of particles interacting through a continuous core softened ramplike interparticle potential we found density dynamic and structural anomalies similar to that found in water analysis ... | [['using', 'molecular', 'dynamics', 'simulations', 'and', 'integral', 'equations', 'we', 'investigate', 'the', 'structure', 'the', 'thermodynamics', 'and', 'the', 'dynamics', 'of', 'a', 'system', 'of', 'particles', 'interacting', 'through', 'a', 'continuous', 'core', 'softened', 'ramplike', 'interparticle', 'potential'... | [-0.151950552018688, 0.1280111718977637, -0.1561154312281253, 0.07161880495464977, 0.005140068060855436, -0.05400925264556838, 0.02923545617993702, 0.3464746050098363, -0.2840814126299365, -0.28854503345620985, 0.06783226386281005, -0.279542216045015, -0.1705186615958262, 0.1059446844874936, 0.08143490047522765, 0.0526... |
706.2916 | Factor Two Discrepancy of Hawking Radiation Temperature | The possibility of an alternative way to formulate the Hawking radiation in a
static Schwarzschild spacetime has been explored. To calculate the Hawking
radiation, there can be two possible choices of the spacetime wedge pairs in
the Krucal-Szekeres coordinates. One is the wedge pair consists of exterior
spacetime of... | hep-th | the possibility of an alternative way to formulate the hawking radiation in a static schwarzschild spacetime has been explored to calculate the hawking radiation there can be two possible choices of the spacetime wedge pairs in the krucalszekeres coordinates one is the wedge pair consists of exterior spacetime of a bla... | [['the', 'possibility', 'of', 'an', 'alternative', 'way', 'to', 'formulate', 'the', 'hawking', 'radiation', 'in', 'a', 'static', 'schwarzschild', 'spacetime', 'has', 'been', 'explored', 'to', 'calculate', 'the', 'hawking', 'radiation', 'there', 'can', 'be', 'two', 'possible', 'choices', 'of', 'the', 'spacetime', 'wedge... | [-0.1228362659477971, 0.10968905474712504, -0.12689555812085795, 0.10820466025660817, -0.09834687606208663, -0.11551242474164082, -0.04370687517604162, 0.2960601138890299, -0.20334039381745025, -0.2680018142852773, 0.11108675659395373, -0.32049653644108367, -0.07579571820206495, 0.1864274919558412, -0.07101928778231525... |
706.2917 | A variational theory for point defects in patterns | We derive a rigorous scaling law for minimizers in a natural version of the
regularized Cross-Newell model for pattern formation far from threshold. These
energy-minimizing solutions support defects having the same character as what
is seen in experimental studies of the corresponding physical systems and in
numerica... | math.AP nlin.PS | we derive a rigorous scaling law for minimizers in a natural version of the regularized crossnewell model for pattern formation far from threshold these energyminimizing solutions support defects having the same character as what is seen in experimental studies of the corresponding physical systems and in numerical sim... | [['we', 'derive', 'a', 'rigorous', 'scaling', 'law', 'for', 'minimizers', 'in', 'a', 'natural', 'version', 'of', 'the', 'regularized', 'crossnewell', 'model', 'for', 'pattern', 'formation', 'far', 'from', 'threshold', 'these', 'energyminimizing', 'solutions', 'support', 'defects', 'having', 'the', 'same', 'character', ... | [-0.11340493122115732, 0.042400810873897916, -0.12199511775238947, 0.11692534858064557, -0.01367374500259757, -0.1015505475923419, 0.04703454989939928, 0.30853882797739723, -0.26325938281264494, -0.2767094748264009, 0.11354683204342357, -0.29251895851709625, -0.1817327584055337, 0.18575878519226205, -0.0154892602935433... |
706.2918 | Enumerative properties of Ferrers graphs | We define a class of bipartite graphs that correspond naturally with Ferrers
diagrams. We give expressions for the number of spanning trees, the number of
Hamiltonian paths when applicable, the chromatic polynomial, and the chromatic
symmetric function. We show that the linear coefficient of the chromatic
polynomial ... | math.CO | we define a class of bipartite graphs that correspond naturally with ferrers diagrams we give expressions for the number of spanning trees the number of hamiltonian paths when applicable the chromatic polynomial and the chromatic symmetric function we show that the linear coefficient of the chromatic polynomial is give... | [['we', 'define', 'a', 'class', 'of', 'bipartite', 'graphs', 'that', 'correspond', 'naturally', 'with', 'ferrers', 'diagrams', 'we', 'give', 'expressions', 'for', 'the', 'number', 'of', 'spanning', 'trees', 'the', 'number', 'of', 'hamiltonian', 'paths', 'when', 'applicable', 'the', 'chromatic', 'polynomial', 'and', 'th... | [-0.1905091859193312, 0.15208824649798097, -0.05320461729058513, 0.06479420631270234, -0.11622972200038256, -0.096951488017415, 0.01906546274269069, 0.32699634864736626, -0.2719999037820984, -0.33245504542288407, 0.043033482562923046, -0.24758863766436223, -0.23203080564875295, 0.18289483131633866, -0.07256185403093696... |
706.2919 | The statistics of LCDM Halo Concentrations | We use the Millennium Simulation (MS) to study the statistics of LCDM halo
concentrations at z = 0. Our results confirm that the average halo
concentration declines monotonically with mass; a power-law fits well the
concentration-mass relation for over 3 decades in mass, up to the most massive
objects to form in a LC... | astro-ph | we use the millennium simulation ms to study the statistics of lcdm halo concentrations at z 0 our results confirm that the average halo concentration declines monotonically with mass a powerlaw fits well the concentrationmass relation for over 3 decades in mass up to the most massive objects to form in a lcdm universe... | [['we', 'use', 'the', 'millennium', 'simulation', 'ms', 'to', 'study', 'the', 'statistics', 'of', 'lcdm', 'halo', 'concentrations', 'at', 'z', '0', 'our', 'results', 'confirm', 'that', 'the', 'average', 'halo', 'concentration', 'declines', 'monotonically', 'with', 'mass', 'a', 'powerlaw', 'fits', 'well', 'the', 'concen... | [-0.041060580953065806, 0.11193669828199093, -0.0882052332162857, 0.12273856865898197, -0.06256738689639474, -0.05245518022563746, 0.024727298817804708, 0.3841417677745766, -0.1203371675618828, -0.43243026504149806, 0.040274830622719186, -0.31804146725676863, -0.0008556726513532281, 0.18017884660540487, -0.031125028874... |
706.292 | Tropical hyperplane arrangements and oriented matroids | We study the combinatorial properties of a tropical hyperplane arrangement.
We define tropical oriented matroids, and prove that they share many of the
properties of ordinary oriented matroids. We show that a tropical oriented
matroid determines a subdivision of a product of two simplices, and conjecture
that this co... | math.CO | we study the combinatorial properties of a tropical hyperplane arrangement we define tropical oriented matroids and prove that they share many of the properties of ordinary oriented matroids we show that a tropical oriented matroid determines a subdivision of a product of two simplices and conjecture that this correspo... | [['we', 'study', 'the', 'combinatorial', 'properties', 'of', 'a', 'tropical', 'hyperplane', 'arrangement', 'we', 'define', 'tropical', 'oriented', 'matroids', 'and', 'prove', 'that', 'they', 'share', 'many', 'of', 'the', 'properties', 'of', 'ordinary', 'oriented', 'matroids', 'we', 'show', 'that', 'a', 'tropical', 'ori... | [-0.2658635178007759, 0.08913689015361552, -0.12164778509535469, 0.08528377285424191, -0.10033761383965611, -0.08473607796566704, 0.009215889820972314, 0.36570531939371276, -0.41400396093153036, -0.21074434237268108, 0.07750471447462377, -0.2443259573281886, -0.2625166801019357, 0.11631506326823281, -0.1973565394202104... |
706.2921 | Herwig++ | We describe the recent development of the Herwig++ event generator.
| hep-ph | we describe the recent development of the herwig event generator | [['we', 'describe', 'the', 'recent', 'development', 'of', 'the', 'herwig', 'event', 'generator']] | [-0.08065405562520027, 0.05637899274006486, -0.05513874813914299, 0.1173476368188858, -0.10554763916879892, 0.04081140123307705, -0.19563838839530945, 0.4471614882349968, -0.1824308312498033, -0.29168557599186895, 0.08510464834980666, -0.3022811532020569, -0.09025022089481353, 0.15735853761434554, -0.0381288155913353, ... |
706.2922 | Mackey functors on compact closed categories | We develop and extend the theory of Mackey functors as an application of
enriched category theory. We define Mackey functors on a lextensive category
$\E$ and investigate the properties of the category of Mackey functors on $\E$.
We show that it is a monoidal category and the monoids are Green functors.
Mackey functo... | math.CT | we develop and extend the theory of mackey functors as an application of enriched category theory we define mackey functors on a lextensive category e and investigate the properties of the category of mackey functors on e we show that it is a monoidal category and the monoids are green functors mackey functors are seen... | [['we', 'develop', 'and', 'extend', 'the', 'theory', 'of', 'mackey', 'functors', 'as', 'an', 'application', 'of', 'enriched', 'category', 'theory', 'we', 'define', 'mackey', 'functors', 'on', 'a', 'lextensive', 'category', 'e', 'and', 'investigate', 'the', 'properties', 'of', 'the', 'category', 'of', 'mackey', 'functor... | [-0.1412622423538256, -0.025788145648986377, -0.13845889059605426, 0.131653815636983, -0.08654430860395332, -0.05982361545574178, -0.0015430670948514697, 0.39881957405348223, -0.42199968647599073, -0.19818506701987718, 0.07006079530905895, -0.1642473596200061, -0.15794312388700718, 0.12092839791854419, -0.2239153793100... |
706.2923 | Representations of Truncated Current Lie Algebras | Let g denote a Lie algebra, and let T(g) denote the tensor product of g with
a ring of truncated polynomials. The Lie algebra T(g) is called a truncated
current Lie algebra. The highest-weight representation theory of T(g) is
developed, and a reducibility criterion for the Verma modules is described.
| math.RT math-ph math.MP | let g denote a lie algebra and let tg denote the tensor product of g with a ring of truncated polynomials the lie algebra tg is called a truncated current lie algebra the highestweight representation theory of tg is developed and a reducibility criterion for the verma modules is described | [['let', 'g', 'denote', 'a', 'lie', 'algebra', 'and', 'let', 'tg', 'denote', 'the', 'tensor', 'product', 'of', 'g', 'with', 'a', 'ring', 'of', 'truncated', 'polynomials', 'the', 'lie', 'algebra', 'tg', 'is', 'called', 'a', 'truncated', 'current', 'lie', 'algebra', 'the', 'highestweight', 'representation', 'theory', 'of... | [-0.2648057864513248, 0.12298359550535679, -0.1299738928489387, -0.0719318009656854, -0.21193720111623407, -0.14659386221319437, -0.08271161682205275, 0.29755047684535385, -0.38469559647142887, -0.1238904783129692, 0.10353869641199707, -0.20511964045464992, -0.13404689052928007, 0.12747688012197614, -0.0950354583561420... |
706.2924 | A scaling relation of anomalous Hall effect in ferromagnetic
semiconductors and metals | A scaling relation of the anomalous Hall effect recently found in a
ferromagnetic semiconductor (Ti,Co)O_2_ is compared with those of various
ferromagnetic semiconductors and metals. Many of these compounds with
relatively low conductivity sigma_xx_ < 10^4 ohm^-1 cm^-1 are also found to
exhibit similar relation: anom... | cond-mat.mtrl-sci cond-mat.str-el | a scaling relation of the anomalous hall effect recently found in a ferromagnetic semiconductor ticoo_2_ is compared with those of various ferromagnetic semiconductors and metals many of these compounds with relatively low conductivity sigma_xx_ 104 ohm1 cm1 are also found to exhibit similar relation anomalous hall con... | [['a', 'scaling', 'relation', 'of', 'the', 'anomalous', 'hall', 'effect', 'recently', 'found', 'in', 'a', 'ferromagnetic', 'semiconductor', 'ticoo_2_', 'is', 'compared', 'with', 'those', 'of', 'various', 'ferromagnetic', 'semiconductors', 'and', 'metals', 'many', 'of', 'these', 'compounds', 'with', 'relatively', 'low',... | [-0.1437265615242953, 0.23741347042345246, -0.019760420099950174, 0.023797266226274972, -0.03680179100221311, -0.20715589488161282, 0.019118898461284246, 0.3701911831773083, -0.22370621265554932, -0.32171576066126284, 0.03337228611524833, -0.3677209288563947, -0.1577617983878131, 0.2371314215296748, 0.02662123564768477... |
706.2925 | Non-Markovian dynamics in the theory of full counting statistics | We consider the theoretical description of real-time counting of electrons
tunneling through a Coulomb-blockade quantum dot using a detector with finite
bandwidth. By tracing out the quantum dot we find that the dynamics of the
detector effectively is non-Markovian. We calculate the cumulant generating
function corre... | cond-mat.mes-hall | we consider the theoretical description of realtime counting of electrons tunneling through a coulombblockade quantum dot using a detector with finite bandwidth by tracing out the quantum dot we find that the dynamics of the detector effectively is nonmarkovian we calculate the cumulant generating function correspondin... | [['we', 'consider', 'the', 'theoretical', 'description', 'of', 'realtime', 'counting', 'of', 'electrons', 'tunneling', 'through', 'a', 'coulombblockade', 'quantum', 'dot', 'using', 'a', 'detector', 'with', 'finite', 'bandwidth', 'by', 'tracing', 'out', 'the', 'quantum', 'dot', 'we', 'find', 'that', 'the', 'dynamics', '... | [-0.14364612564882812, 0.13385597167618793, -0.10715013819144052, 0.06464015076646105, 0.024216472231509054, -0.14014223701704073, 0.056090363186291035, 0.3221115392906701, -0.2561207384802401, -0.2843351458363673, -0.014649213501252234, -0.31687994949957904, -0.12135638875119827, 0.2301459795137977, -0.004036873732419... |
706.2926 | Reducing the Error Floor | We discuss how the loop calculus approach of [Chertkov, Chernyak '06],
enhanced by the pseudo-codeword search algorithm of [Chertkov, Stepanov '06]
and the facet-guessing idea from [Dimakis, Wainwright '06], improves decoding
of graph based codes in the error-floor domain. The utility of the new, Linear
Programming b... | cs.IT math.IT | we discuss how the loop calculus approach of chertkov chernyak 06 enhanced by the pseudocodeword search algorithm of chertkov stepanov 06 and the facetguessing idea from dimakis wainwright 06 improves decoding of graph based codes in the errorfloor domain the utility of the new linear programming based decoding is demo... | [['we', 'discuss', 'how', 'the', 'loop', 'calculus', 'approach', 'of', 'chertkov', 'chernyak', '06', 'enhanced', 'by', 'the', 'pseudocodeword', 'search', 'algorithm', 'of', 'chertkov', 'stepanov', '06', 'and', 'the', 'facetguessing', 'idea', 'from', 'dimakis', 'wainwright', '06', 'improves', 'decoding', 'of', 'graph', ... | [-0.10084557500586175, 0.00406890453182553, -0.10882860178683411, 0.06335685997098488, -0.06500591782509889, -0.1875651697709895, 0.10466679679883416, 0.3318752074581489, -0.2678030777657241, -0.35435881557171806, 0.11262620013133672, -0.2247199516318608, -0.22927047906999, 0.18761485045481668, -0.10259429816352694, 0.... |
706.2927 | Green's function approach to transport through a gate-all-around Si
nanowire under impurity scattering | We investigate transport properties of gate-all-around Si nanowires using
non-equilibrium Green's function technique. By taking into account of the
ionized impurity scattering we calculate Green's functions self-consistently
and examine the effects of ionized impurity scattering on electron densities
and currents. Fo... | cond-mat.mes-hall | we investigate transport properties of gateallaround si nanowires using nonequilibrium greens function technique by taking into account of the ionized impurity scattering we calculate greens functions selfconsistently and examine the effects of ionized impurity scattering on electron densities and currents for nanoscal... | [['we', 'investigate', 'transport', 'properties', 'of', 'gateallaround', 'si', 'nanowires', 'using', 'nonequilibrium', 'greens', 'function', 'technique', 'by', 'taking', 'into', 'account', 'of', 'the', 'ionized', 'impurity', 'scattering', 'we', 'calculate', 'greens', 'functions', 'selfconsistently', 'and', 'examine', '... | [-0.09469986032003287, 0.18225851891197495, -0.04569818483684788, 0.11186752657732475, 0.01788399487580221, -0.14639534260933623, 0.05610363921102559, 0.39484602270513464, -0.23970787932846657, -0.2802644151541376, -0.02616547535956098, -0.33450334712373303, -0.08894614556554667, 0.14845435354455383, 0.0860123471404934... |
706.2928 | Strong effect of weak diffusion on scalar turbulence at large scales | Passive scalar turbulence forced steadily is characterized by the velocity
correlation scale, $L$, injection scale, $l$, and diffusive scale, $r_d$. The
scales are well separated if the diffusivity is small, $r_d\ll l,L$, and one
normally says that effects of diffusion are confined to smaller scales, $r\ll
r_d$. Howe... | nlin.CD | passive scalar turbulence forced steadily is characterized by the velocity correlation scale l injection scale l and diffusive scale r_d the scales are well separated if the diffusivity is small r_dll ll and one normally says that effects of diffusion are confined to smaller scales rll r_d however if the velocity is si... | [['passive', 'scalar', 'turbulence', 'forced', 'steadily', 'is', 'characterized', 'by', 'the', 'velocity', 'correlation', 'scale', 'l', 'injection', 'scale', 'l', 'and', 'diffusive', 'scale', 'r_d', 'the', 'scales', 'are', 'well', 'separated', 'if', 'the', 'diffusivity', 'is', 'small', 'r_dll', 'll', 'and', 'one', 'nor... | [-0.21531919326201732, 0.27758438440056843, -0.043182981360720796, 0.09886804541440493, -0.0346607298316827, -0.1914916082516039, -0.06685037388671361, 0.283267707538304, -0.2964373979580785, -0.2849478412402469, 0.05183138769256686, -0.2713228050499744, -0.06170051423576447, 0.16576767408656418, 0.05801357116994508, 0... |
706.2929 | Noncompact sigma-models: Large N expansion and thermodynamic limit | Noncompact SO(1,N) sigma-models are studied in terms of their large N
expansion in a lattice formulation in dimensions d \geq 2. Explicit results for
the spin and current two-point functions as well as for the Binder cumulant are
presented to next to leading order on a finite lattice. The dynamically
generated gap is... | hep-th hep-lat | noncompact so1n sigmamodels are studied in terms of their large n expansion in a lattice formulation in dimensions d geq 2 explicit results for the spin and current twopoint functions as well as for the binder cumulant are presented to next to leading order on a finite lattice the dynamically generated gap is negative ... | [['noncompact', 'so1n', 'sigmamodels', 'are', 'studied', 'in', 'terms', 'of', 'their', 'large', 'n', 'expansion', 'in', 'a', 'lattice', 'formulation', 'in', 'dimensions', 'd', 'geq', '2', 'explicit', 'results', 'for', 'the', 'spin', 'and', 'current', 'twopoint', 'functions', 'as', 'well', 'as', 'for', 'the', 'binder', ... | [-0.16522362341605862, 0.19143674550266465, -0.05329474558870138, 0.10737174624104945, 0.004008106060955726, -0.08463149124585932, 0.008774500566495346, 0.3306861379196946, -0.2006661741613922, -0.23389269195129753, 0.1389901577388461, -0.3095572285459075, -0.1331753934467946, 0.14982423370763082, 0.00878265422041705, ... |
706.293 | Strong magnetic field enhancement of spin triplet pairing arising from
coexisting $2k_F$ spin and $2k_F$ charge fluctuations | We study the effect of the magnetic field (Zeeman splitting) on the triplet
pairing. We show generally that the enhancement of spin triplet pairing
mediated by coexisting $2k_F$ spin and $2k_F$ charge fluctuations can be much
larger than in the case of triplet pairing mediated by ferromagnetic spin
fluctuations. We p... | cond-mat.supr-con | we study the effect of the magnetic field zeeman splitting on the triplet pairing we show generally that the enhancement of spin triplet pairing mediated by coexisting 2k_f spin and 2k_f charge fluctuations can be much larger than in the case of triplet pairing mediated by ferromagnetic spin fluctuations we propose tha... | [['we', 'study', 'the', 'effect', 'of', 'the', 'magnetic', 'field', 'zeeman', 'splitting', 'on', 'the', 'triplet', 'pairing', 'we', 'show', 'generally', 'that', 'the', 'enhancement', 'of', 'spin', 'triplet', 'pairing', 'mediated', 'by', 'coexisting', '2k_f', 'spin', 'and', '2k_f', 'charge', 'fluctuations', 'can', 'be',... | [-0.21477772988379001, 0.29946898405750594, -0.023815865491827327, 0.13435778853017838, -0.05517889351894458, -0.13795947816843787, -0.001461924562851588, 0.37096909537911416, -0.2300631689094007, -0.2731218099097411, -0.05740842853672803, -0.2757273764908314, -0.10808603507466615, 0.11849565923213959, 0.07976836580783... |
706.2931 | Markov Process of Muscle Motors | We study a Markov random process describing a muscle molecular motor
behavior. Every motor is either bound up with a thin filament or unbound. In
the bound state the motor creates a force proportional to its displacement from
the neutral position. In both states the motor spend an exponential time
depending on the st... | math-ph math.MP | we study a markov random process describing a muscle molecular motor behavior every motor is either bound up with a thin filament or unbound in the bound state the motor creates a force proportional to its displacement from the neutral position in both states the motor spend an exponential time depending on the state t... | [['we', 'study', 'a', 'markov', 'random', 'process', 'describing', 'a', 'muscle', 'molecular', 'motor', 'behavior', 'every', 'motor', 'is', 'either', 'bound', 'up', 'with', 'a', 'thin', 'filament', 'or', 'unbound', 'in', 'the', 'bound', 'state', 'the', 'motor', 'creates', 'a', 'force', 'proportional', 'to', 'its', 'dis... | [-0.16463812403804198, 0.20756457416917493, -0.08780139980583705, -0.040440798853970505, -0.0524754710749469, -0.13630526795221323, 0.0781502744521607, 0.35365733456882564, -0.2804304845207794, -0.25984465533190154, 0.06531930032546039, -0.2698423920537938, -0.11195515270175582, 0.1643746877406639, -0.01364769433117048... |
706.2932 | The formation of the [alpha/Fe] radial gradients in the stars of
elliptical galaxies | The scope of this paper is two-fold: i) to test and improve our previous
models of an outside-in formation for the majority of ellipticals in the
context of the SN-driven wind scenario, by means of a careful study of gas
inflows/outflows; ii) to explain the observed slopes, either positive or
negative, in the radial ... | astro-ph | the scope of this paper is twofold i to test and improve our previous models of an outsidein formation for the majority of ellipticals in the context of the sndriven wind scenario by means of a careful study of gas inflowsoutflows ii to explain the observed slopes either positive or negative in the radial gradient of t... | [['the', 'scope', 'of', 'this', 'paper', 'is', 'twofold', 'i', 'to', 'test', 'and', 'improve', 'our', 'previous', 'models', 'of', 'an', 'outsidein', 'formation', 'for', 'the', 'majority', 'of', 'ellipticals', 'in', 'the', 'context', 'of', 'the', 'sndriven', 'wind', 'scenario', 'by', 'means', 'of', 'a', 'careful', 'stud... | [-0.05337385298085839, 0.10127493645061526, -0.06051568236421945, 0.0805435618785179, -0.031456051434723596, -0.037619950280720675, 0.016209722523632498, 0.40782809364042377, -0.19473435496052252, -0.3568904814533752, 0.03817722781791568, -0.24937360900766956, -0.05212053040049393, 0.1689423167755023, -0.04766508869094... |
706.2933 | Electromagnetic quasinormal modes of D-dimensional black holes II | By using the sixth order WKB approximation we calculate for an
electromagnetic field propagating in D-dimensional Schwarzschild and
Schwarzschild de Sitter black holes its quasinormal frequencies for the
fundamental mode and first overtones. We study the dependence of these QN
frequencies on the value of the cosmolog... | gr-qc | by using the sixth order wkb approximation we calculate for an electromagnetic field propagating in ddimensional schwarzschild and schwarzschild de sitter black holes its quasinormal frequencies for the fundamental mode and first overtones we study the dependence of these qn frequencies on the value of the cosmological... | [['by', 'using', 'the', 'sixth', 'order', 'wkb', 'approximation', 'we', 'calculate', 'for', 'an', 'electromagnetic', 'field', 'propagating', 'in', 'ddimensional', 'schwarzschild', 'and', 'schwarzschild', 'de', 'sitter', 'black', 'holes', 'its', 'quasinormal', 'frequencies', 'for', 'the', 'fundamental', 'mode', 'and', '... | [-0.1949438889799196, 0.16599904204000873, -0.03552930165259611, 0.10034792995346443, -0.09978318998944902, -0.07986286996109855, -0.0519999896663995, 0.2839994767015534, -0.15008202591644867, -0.22342553864277545, 0.05331393001889367, -0.31126531976319494, -0.1313049841938274, 0.1746150282799222, 0.042904392097677505,... |
706.2934 | Recent heavy flavor results from STAR | We report on recent heavy flavor measurements from the STAR experiment at
RHIC. The measured charm cross section in heavy-ion collisions scales with the
number of binary collisions, which is an indication for exclusive charm
production in the initial state of the collision. The observed strong
suppression of non-phot... | nucl-ex | we report on recent heavy flavor measurements from the star experiment at rhic the measured charm cross section in heavyion collisions scales with the number of binary collisions which is an indication for exclusive charm production in the initial state of the collision the observed strong suppression of nonphotonic el... | [['we', 'report', 'on', 'recent', 'heavy', 'flavor', 'measurements', 'from', 'the', 'star', 'experiment', 'at', 'rhic', 'the', 'measured', 'charm', 'cross', 'section', 'in', 'heavyion', 'collisions', 'scales', 'with', 'the', 'number', 'of', 'binary', 'collisions', 'which', 'is', 'an', 'indication', 'for', 'exclusive', ... | [-0.09931934797793798, 0.2533088294515218, -0.19139041398362866, 0.08913308170747183, 0.08621490466269269, -0.05273546338423915, -0.08338399333397634, 0.3021293550076755, -0.1989536335070928, -0.2733798124880969, -0.13606547761505106, -0.4398857281896575, 0.1648193278574738, 0.1203962789912676, 0.11068343665536451, 0.1... |
706.2935 | Preferential attachment during the evolution of a potential energy
landscape | It has previously been shown that the network of connected minima on a
potential energy landscape is scale-free, and that this reflects a power-law
distribution for the areas of the basins of attraction surrounding the minima.
Here, we set out to understand more about the physical origins of these
puzzling properties... | cond-mat.stat-mech | it has previously been shown that the network of connected minima on a potential energy landscape is scalefree and that this reflects a powerlaw distribution for the areas of the basins of attraction surrounding the minima here we set out to understand more about the physical origins of these puzzling properties by exa... | [['it', 'has', 'previously', 'been', 'shown', 'that', 'the', 'network', 'of', 'connected', 'minima', 'on', 'a', 'potential', 'energy', 'landscape', 'is', 'scalefree', 'and', 'that', 'this', 'reflects', 'a', 'powerlaw', 'distribution', 'for', 'the', 'areas', 'of', 'the', 'basins', 'of', 'attraction', 'surrounding', 'the... | [-0.12362234292221189, 0.13825066738586494, -0.12124283490522544, 0.09500388824839635, -0.022170825562201405, -0.09511335149344399, 0.06801037587099461, 0.3455138389315852, -0.2780635261948666, -0.32077765470181685, 0.057774518556883876, -0.3003874949723986, -0.19025660950492546, 0.1661303788828461, -0.0249800849413490... |
706.2936 | High-Resolution Spectra Observed for SPY. II. DB and DBA Stars | We present a detailed spectroscopic analysis of the stars with
helium-dominated spectra in the ESO Supernova Ia Progenitor Survey (SPY).
Atmospheric parameters, masses, and abundances of trace hydrogen are determined
and discussed in the context of spectral evolution of white dwarfs. Our final
sample contains 71 obje... | astro-ph | we present a detailed spectroscopic analysis of the stars with heliumdominated spectra in the eso supernova ia progenitor survey spy atmospheric parameters masses and abundances of trace hydrogen are determined and discussed in the context of spectral evolution of white dwarfs our final sample contains 71 objects of wh... | [['we', 'present', 'a', 'detailed', 'spectroscopic', 'analysis', 'of', 'the', 'stars', 'with', 'heliumdominated', 'spectra', 'in', 'the', 'eso', 'supernova', 'ia', 'progenitor', 'survey', 'spy', 'atmospheric', 'parameters', 'masses', 'and', 'abundances', 'of', 'trace', 'hydrogen', 'are', 'determined', 'and', 'discussed... | [-0.06885728069003029, 0.17684976039005598, 0.010347459442326295, 0.04086219699963872, -0.03102534298963955, -0.09439134755369111, 0.12731228733384808, 0.38005700834288164, -0.1963249719799198, -0.37912594533887845, 0.10725683051108709, -0.296508841558355, -0.0063466026683984865, 0.1808722599242066, -0.0331109726659292... |
706.2937 | On the dependence of the wave function of a bound nucleon on its
momentum and the EMC effect | It is widely discussed in the literature that the wave function of the
nucleon bound in a nucleus is modified due to the interaction with the
surrounding medium. We argue that the modification should strongly depend on
the momentum of the nucleon. We study such an effect in the case of the
point-like configuration co... | nucl-th hep-ph nucl-ex | it is widely discussed in the literature that the wave function of the nucleon bound in a nucleus is modified due to the interaction with the surrounding medium we argue that the modification should strongly depend on the momentum of the nucleon we study such an effect in the case of the pointlike configuration compone... | [['it', 'is', 'widely', 'discussed', 'in', 'the', 'literature', 'that', 'the', 'wave', 'function', 'of', 'the', 'nucleon', 'bound', 'in', 'a', 'nucleus', 'is', 'modified', 'due', 'to', 'the', 'interaction', 'with', 'the', 'surrounding', 'medium', 'we', 'argue', 'that', 'the', 'modification', 'should', 'strongly', 'depe... | [-0.10735524989704186, 0.18346883934259012, -0.11954795781701327, 0.09584200182071266, -0.043123688595864844, -0.013858158012574657, 0.048163796353966316, 0.32554825482533334, -0.20016369971872724, -0.26637891166706623, -0.014325201515098439, -0.2795433204712723, -0.0809556114452673, 0.1320201243618206, 0.0626398037717... |
706.2938 | New Heavy Quark Baryons | During the past year many interesting results were published in heavy quark
baryon spectroscopy. In addition to several refined measurements, new states
were directly observed both in the charm and the bottom sector. In this paper
we review recent results on heavy quark baryons from B-factories and Tevatron
experimen... | hep-ex | during the past year many interesting results were published in heavy quark baryon spectroscopy in addition to several refined measurements new states were directly observed both in the charm and the bottom sector in this paper we review recent results on heavy quark baryons from bfactories and tevatron experiments | [['during', 'the', 'past', 'year', 'many', 'interesting', 'results', 'were', 'published', 'in', 'heavy', 'quark', 'baryon', 'spectroscopy', 'in', 'addition', 'to', 'several', 'refined', 'measurements', 'new', 'states', 'were', 'directly', 'observed', 'both', 'in', 'the', 'charm', 'and', 'the', 'bottom', 'sector', 'in',... | [0.00901614891707289, 0.2550905101305368, -0.09843655394352212, 0.10354103295046989, -0.07598521142285697, -0.0915876781301839, 0.11165688814338753, 0.3263269842659332, -0.17299415441039873, -0.3059243767389229, 0.03932212971683059, -0.41385627583581575, -0.0015632965582974103, 0.19032558157317797, -0.00680257226055374... |
706.2939 | On the stabilization of the elasticity system by the boundary | We obtain free of resonances regions for the elasticity system in the
exterior of a strictly convex body with dissipative boundary conditions under
some natural assumptions on the behaviour of the geodesics on the boundary.
| math.AP | we obtain free of resonances regions for the elasticity system in the exterior of a strictly convex body with dissipative boundary conditions under some natural assumptions on the behaviour of the geodesics on the boundary | [['we', 'obtain', 'free', 'of', 'resonances', 'regions', 'for', 'the', 'elasticity', 'system', 'in', 'the', 'exterior', 'of', 'a', 'strictly', 'convex', 'body', 'with', 'dissipative', 'boundary', 'conditions', 'under', 'some', 'natural', 'assumptions', 'on', 'the', 'behaviour', 'of', 'the', 'geodesics', 'on', 'the', 'b... | [-0.18972652591764927, 0.0864149264193007, -0.11239011198548333, 0.009324703964271716, -0.0632793731388769, -0.08703125559591822, -0.013979672374469893, 0.31404928235071045, -0.25139492473431996, -0.18534629291721752, 0.17043904252017716, -0.26765288550938876, -0.12032674221055849, 0.1923495008477143, -0.11265438877578... |
706.294 | Early Electroweak and Top Quark Physics with CMS | The Large Hadron Collider is an ideal place for precision measurements of the
properties of the electroweak gauge bosons W^\pm, Z^0, as well as of the top
quark. In this article, a few highlights of the prospects for performing such
measurements with the CMS detector are summarized, with an emphasis on the
first few ... | hep-ex | the large hadron collider is an ideal place for precision measurements of the properties of the electroweak gauge bosons wpm z0 as well as of the top quark in this article a few highlights of the prospects for performing such measurements with the cms detector are summarized with an emphasis on the first few 1fb of dat... | [['the', 'large', 'hadron', 'collider', 'is', 'an', 'ideal', 'place', 'for', 'precision', 'measurements', 'of', 'the', 'properties', 'of', 'the', 'electroweak', 'gauge', 'bosons', 'wpm', 'z0', 'as', 'well', 'as', 'of', 'the', 'top', 'quark', 'in', 'this', 'article', 'a', 'few', 'highlights', 'of', 'the', 'prospects', '... | [-0.05439508843578791, 0.21151345194237747, -0.041325252915716225, 0.06447493397679768, -0.054526412369389286, -0.10682322982731357, -0.004412028240039945, 0.3237410098510353, -0.20461160022961467, -0.30540937427104564, 0.10113135504479144, -0.3524160023386541, 0.03538763818837572, 0.21303020037400225, 0.07844932420636... |
706.2941 | A Common Origin for Quasar Extended Emission-Line Regions and Their
Broad-Line Regions | We present a correlation between the presence of luminous extended
emission-line regions (EELRs) and the metallicity of the broad-line regions
(BLRs) of low-redshift quasars. The result is based on ground-based [O III]
5007 narrow-band imaging and Hubble Space Telescope UV spectra of 12 quasars at
0.20 < z < 0.45. Qu... | astro-ph | we present a correlation between the presence of luminous extended emissionline regions eelrs and the metallicity of the broadline regions blrs of lowredshift quasars the result is based on groundbased o iii 5007 narrowband imaging and hubble space telescope uv spectra of 12 quasars at 020 z 045 quasars showing luminou... | [['we', 'present', 'a', 'correlation', 'between', 'the', 'presence', 'of', 'luminous', 'extended', 'emissionline', 'regions', 'eelrs', 'and', 'the', 'metallicity', 'of', 'the', 'broadline', 'regions', 'blrs', 'of', 'lowredshift', 'quasars', 'the', 'result', 'is', 'based', 'on', 'groundbased', 'o', 'iii', '5007', 'narro... | [-0.04442662933569712, 0.08699377610037724, -0.02547419728090366, 0.14438164062875633, -0.06982700987253337, -0.09047329727870723, 0.08684807192378988, 0.4660036328807473, -0.06702138086780905, -0.3037277479516342, 0.014876632824695358, -0.32323300338660677, 0.011993156935398777, 0.19429920084109956, 0.0004372599907219... |
706.2942 | Astrometric effects of solar-like magnetic activity in late-type stars
and their relevance for the detection of extrasolar planets | Using a simple model based on the characteristics of sunspots and faculae in
solar active regions, the effects of surface brightness inhomogeneities on the
position of the photocentre of the disk of a solar-like, magnetically active
star, are studied. A general law is introduced, giving the maximum amplitude of
the p... | astro-ph | using a simple model based on the characteristics of sunspots and faculae in solar active regions the effects of surface brightness inhomogeneities on the position of the photocentre of the disk of a solarlike magnetically active star are studied a general law is introduced giving the maximum amplitude of the photocent... | [['using', 'a', 'simple', 'model', 'based', 'on', 'the', 'characteristics', 'of', 'sunspots', 'and', 'faculae', 'in', 'solar', 'active', 'regions', 'the', 'effects', 'of', 'surface', 'brightness', 'inhomogeneities', 'on', 'the', 'position', 'of', 'the', 'photocentre', 'of', 'the', 'disk', 'of', 'a', 'solarlike', 'magne... | [-0.12129897043427852, 0.17783081919558652, -0.048800262019143135, 0.06042131880039192, -0.08279365281128442, -0.029079786406725015, 0.08323806030741356, 0.33612753443594556, -0.18839709224297443, -0.37468517225393105, 0.10968838694987451, -0.2685752847546738, -0.10523867488733794, 0.24174626327191912, -0.0833036074116... |
706.2943 | Kondo physics in the algebraic spin liquid | We study Kondo physics in the algebraic spin liquid, recently proposed to
describe $ZnCu_{3}(OH)_{6}Cl_{2}$ [Phys. Rev. Lett. {\bf 98}, 117205 (2007)].
Although spin dynamics of the algebraic spin liquid is described by massless
Dirac fermions, this problem differs from the Pseudogap Kondo model, because
the bulk phy... | cond-mat.str-el | we study kondo physics in the algebraic spin liquid recently proposed to describe zncu_3oh_6cl_2 phys rev lett bf 98 117205 2007 although spin dynamics of the algebraic spin liquid is described by massless dirac fermions this problem differs from the pseudogap kondo model because the bulk physics in the algebraic spin ... | [['we', 'study', 'kondo', 'physics', 'in', 'the', 'algebraic', 'spin', 'liquid', 'recently', 'proposed', 'to', 'describe', 'zncu_3oh_6cl_2', 'phys', 'rev', 'lett', 'bf', '98', '117205', '2007', 'although', 'spin', 'dynamics', 'of', 'the', 'algebraic', 'spin', 'liquid', 'is', 'described', 'by', 'massless', 'dirac', 'fer... | [-0.15559363020183417, 0.24326898000224667, -0.0808895862616238, 0.03024736701846323, -0.0495494939508893, -0.1881777406244549, 0.08681881555821747, 0.2816734261565431, -0.24457317762332217, -0.27849091609479276, -0.00796410378809738, -0.32592261344775236, -0.14335151300490184, 0.14722483237499312, 0.012075799692582379... |
706.2944 | Summing Pomeron loops in the dipole approach | In this paper we argue that in the kinematic range given by $ 1 \ll
\ln(1/\as^2) \ll \as Y \ll \frac{1}{\as}$, we can reduce the Pomeron calculus
to the exchange of non-interacting Pomerons with the renormalized amplitude of
their interaction with the target. Therefore, the summation of the Pomeron
loops can be perfo... | hep-ph | in this paper we argue that in the kinematic range given by 1 ll ln1as2 ll as y ll frac1as we can reduce the pomeron calculus to the exchange of noninteracting pomerons with the renormalized amplitude of their interaction with the target therefore the summation of the pomeron loops can be performed using the improved m... | [['in', 'this', 'paper', 'we', 'argue', 'that', 'in', 'the', 'kinematic', 'range', 'given', 'by', '1', 'll', 'ln1as2', 'll', 'as', 'y', 'll', 'frac1as', 'we', 'can', 'reduce', 'the', 'pomeron', 'calculus', 'to', 'the', 'exchange', 'of', 'noninteracting', 'pomerons', 'with', 'the', 'renormalized', 'amplitude', 'of', 'th... | [-0.12128867961618366, 0.09729643736500293, -0.12380651867359269, 0.10717425967462132, -0.05978965046530475, -0.12153390588295855, 0.033680951294052054, 0.3540138177839773, -0.22314856211863915, -0.28719413588393705, 0.025793323433501835, -0.29436504091041127, -0.13711490339995422, 0.11830410058134977, -0.0354932494442... |
706.2945 | Atom capture by nanotube and scaling anomaly | The existence of bound state of the polarizable neutral atom in the inverse
square potential created by the electric field of single walled charged carbon
nanotube (SWNT) is shown to be theoretically possible. The consideration of
inequivalent boundary conditions due to self-adjoint extensions lead to this
nontrivial... | cond-mat.mtrl-sci hep-th | the existence of bound state of the polarizable neutral atom in the inverse square potential created by the electric field of single walled charged carbon nanotube swnt is shown to be theoretically possible the consideration of inequivalent boundary conditions due to selfadjoint extensions lead to this nontrivial bound... | [['the', 'existence', 'of', 'bound', 'state', 'of', 'the', 'polarizable', 'neutral', 'atom', 'in', 'the', 'inverse', 'square', 'potential', 'created', 'by', 'the', 'electric', 'field', 'of', 'single', 'walled', 'charged', 'carbon', 'nanotube', 'swnt', 'is', 'shown', 'to', 'be', 'theoretically', 'possible', 'the', 'cons... | [-0.14942362378680646, 0.1965731718586852, -0.03532408858882263, 0.01721591838503802, -0.027203773070747655, -0.17916264416734604, 0.036478810299263156, 0.37428577850111805, -0.2532208470364261, -0.27864658864534864, 0.039975582193959545, -0.25214052717454233, -0.11160666470161894, 0.12905190749601883, 0.00809686755375... |
706.2946 | An Obstruction to Quantization of the Sphere | In the standard example of strict deformation quantization of the symplectic
sphere $S^2$, the set of allowed values of the quantization parameter $\hbar$
is not connected; indeed, it is almost discrete. Li recently constructed a
class of examples (including $S^2$) in which $\hbar$ can take any value in an
interval, ... | math-ph math.MP math.OA math.QA | in the standard example of strict deformation quantization of the symplectic sphere s2 the set of allowed values of the quantization parameter hbar is not connected indeed it is almost discrete li recently constructed a class of examples including s2 in which hbar can take any value in an interval but these examples ar... | [['in', 'the', 'standard', 'example', 'of', 'strict', 'deformation', 'quantization', 'of', 'the', 'symplectic', 'sphere', 's2', 'the', 'set', 'of', 'allowed', 'values', 'of', 'the', 'quantization', 'parameter', 'hbar', 'is', 'not', 'connected', 'indeed', 'it', 'is', 'almost', 'discrete', 'li', 'recently', 'constructed'... | [-0.16758645640220493, 0.12925798021893659, -0.033461615091144314, 0.06535713237897697, -0.0976022036643926, -0.1680031604837717, 0.0343186964235473, 0.3426945303544039, -0.2772950738350429, -0.23870330721866795, 0.09932728489809783, -0.2210485234532914, -0.14913364349887137, 0.193801090155342, -0.13321440695875847, -0... |
706.2947 | Quantum Coherence Engines | In a report published in Science, Scully et al propose to generate
"phaseonium", and "extract work from a single heat bath via vanishing
coherence" [1]. On the basis of the laws of physics, such a proposal is futile
for at least two reasons.
| quant-ph | in a report published in science scully et al propose to generate phaseonium and extract work from a single heat bath via vanishing coherence 1 on the basis of the laws of physics such a proposal is futile for at least two reasons | [['in', 'a', 'report', 'published', 'in', 'science', 'scully', 'et', 'al', 'propose', 'to', 'generate', 'phaseonium', 'and', 'extract', 'work', 'from', 'a', 'single', 'heat', 'bath', 'via', 'vanishing', 'coherence', '1', 'on', 'the', 'basis', 'of', 'the', 'laws', 'of', 'physics', 'such', 'a', 'proposal', 'is', 'futile'... | [-0.04985875360191215, 0.13408237004782572, -0.08848040627835449, -0.010632806157065166, -0.05914982144049434, -0.15796720909041373, 0.07350295080348503, 0.29212786417541114, -0.22549190975422428, -0.360717796839687, 0.054548192850509006, -0.29863612916927007, -0.12919396147954948, 0.2091847560382015, -0.06657347383064... |
706.2948 | Do local analogs of Lyman Break Galaxies exist? | The optical properties of a number of supercompact ultraviolet luminous
galaxies (UVLG), recently discovered in the local Universe matching GALEX and
Sloan Digital Sky Survey (SDSS) data, are discussed. Detailed re-analysis of
the SDSS data for these and other similar but nearer galaxies shows that their
surface brig... | astro-ph | the optical properties of a number of supercompact ultraviolet luminous galaxies uvlg recently discovered in the local universe matching galex and sloan digital sky survey sdss data are discussed detailed reanalysis of the sdss data for these and other similar but nearer galaxies shows that their surface brightness rad... | [['the', 'optical', 'properties', 'of', 'a', 'number', 'of', 'supercompact', 'ultraviolet', 'luminous', 'galaxies', 'uvlg', 'recently', 'discovered', 'in', 'the', 'local', 'universe', 'matching', 'galex', 'and', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'data', 'are', 'discussed', 'detailed', 'reanalysis', 'of', 'th... | [-0.047104907048866156, 0.03926701718394179, -0.0747032186165452, 0.12255723919160665, -0.13733020404726268, -0.05682619491778314, 0.049647733638063074, 0.4166284783780575, -0.14205861058365554, -0.3355107838511467, 0.10072173611912877, -0.3341555525176227, -0.008446400051936507, 0.21816058487139525, -0.081052094459533... |
706.2949 | AGN effect on cooling flow dynamics | We analyzed the feedback of AGN jets on cooling flow clusters using
three-dimensional AMR hydrodynamic simulations. We studied the interaction of
the jet with the intracluster medium and creation of low X-ray emission
cavities (Bubbles) in cluster plasma. The distribution of energy input by the
jet into the system wa... | astro-ph | we analyzed the feedback of agn jets on cooling flow clusters using threedimensional amr hydrodynamic simulations we studied the interaction of the jet with the intracluster medium and creation of low xray emission cavities bubbles in cluster plasma the distribution of energy input by the jet into the system was quanti... | [['we', 'analyzed', 'the', 'feedback', 'of', 'agn', 'jets', 'on', 'cooling', 'flow', 'clusters', 'using', 'threedimensional', 'amr', 'hydrodynamic', 'simulations', 'we', 'studied', 'the', 'interaction', 'of', 'the', 'jet', 'with', 'the', 'intracluster', 'medium', 'and', 'creation', 'of', 'low', 'xray', 'emission', 'cav... | [-0.1134048123056368, 0.15793049127369382, -0.05086739414463533, 0.10812105810453679, -0.021725754012112266, -0.042683655171896574, 0.008023667965590217, 0.4159182051518633, -0.22421879452411775, -0.3510557202461325, 0.01404490857385099, -0.28939376559890345, 0.033015916871343864, 0.191420582289819, 0.07961280248559045... |
706.295 | Electron Bunching in Stacks of Coupled Quantum Dots | We study the transport properties of two double quantum dots in a parallel
arrangement at temperatures of a few Kelvin. Thereby, we show that decoherence
entailed by the substrate phonons affects the shot noise. For asymmetric
coupling between the dots and the respective lead, the current noise is
sub-Poissonian for ... | cond-mat.mes-hall cond-mat.mtrl-sci | we study the transport properties of two double quantum dots in a parallel arrangement at temperatures of a few kelvin thereby we show that decoherence entailed by the substrate phonons affects the shot noise for asymmetric coupling between the dots and the respective lead the current noise is subpoissonian for resonan... | [['we', 'study', 'the', 'transport', 'properties', 'of', 'two', 'double', 'quantum', 'dots', 'in', 'a', 'parallel', 'arrangement', 'at', 'temperatures', 'of', 'a', 'few', 'kelvin', 'thereby', 'we', 'show', 'that', 'decoherence', 'entailed', 'by', 'the', 'substrate', 'phonons', 'affects', 'the', 'shot', 'noise', 'for', ... | [-0.1405528144545811, 0.20996189768828283, -0.03321450390979986, 0.057911179814254865, 0.036783298432551834, -0.14273296952755612, 0.07465748514567333, 0.3928627979476005, -0.27528198361820116, -0.2702045415909114, -0.0294342671695631, -0.34823835031552747, -0.10737244127614592, 0.22407166159246117, 0.00917114892085506... |
706.2951 | Collinear versus non-collinear magnetic order in Pd atomic clusters:
ab-initio calculations | We present a thorough theoretical assessment of the stability of
non-collinear spin arrangements in small palladium clusters. We generally find
that ferromagnetic order is always preferred, but that antiferromagnetic and
non-collinear configurations of different sorts exist and compete for the first
excited isomers. ... | cond-mat.mtrl-sci | we present a thorough theoretical assessment of the stability of noncollinear spin arrangements in small palladium clusters we generally find that ferromagnetic order is always preferred but that antiferromagnetic and noncollinear configurations of different sorts exist and compete for the first excited isomers we also... | [['we', 'present', 'a', 'thorough', 'theoretical', 'assessment', 'of', 'the', 'stability', 'of', 'noncollinear', 'spin', 'arrangements', 'in', 'small', 'palladium', 'clusters', 'we', 'generally', 'find', 'that', 'ferromagnetic', 'order', 'is', 'always', 'preferred', 'but', 'that', 'antiferromagnetic', 'and', 'noncollin... | [-0.12485976232223459, 0.13527540273748892, -0.04782079159828626, 0.10197713374822162, 0.010770484718517208, -0.0879019030508362, 0.07773010841809398, 0.39886442053108667, -0.21384820531792015, -0.2883139682148606, 0.02021800417911015, -0.2981991811909459, -0.09697709712276835, 0.14512970317001186, 0.09623549766992488,... |
706.2952 | Mass distributions for nuclear disintegration from fission to
evaporation | By a proper choice of the excitation energy per nucleon we analyze the mass
distributions of the nuclear fragmentation at various excitation energies.
Starting from low energies (between 0.1 and 1 MeV/nucleon) up to higher
energies about 12 MeV/n, we classified the mass yield characteristics for heavy
nuclei (A>200) ... | nucl-th | by a proper choice of the excitation energy per nucleon we analyze the mass distributions of the nuclear fragmentation at various excitation energies starting from low energies between 01 and 1 mevnucleon up to higher energies about 12 mevn we classified the mass yield characteristics for heavy nuclei a200 on the basis... | [['by', 'a', 'proper', 'choice', 'of', 'the', 'excitation', 'energy', 'per', 'nucleon', 'we', 'analyze', 'the', 'mass', 'distributions', 'of', 'the', 'nuclear', 'fragmentation', 'at', 'various', 'excitation', 'energies', 'starting', 'from', 'low', 'energies', 'between', '01', 'and', '1', 'mevnucleon', 'up', 'to', 'high... | [-0.026680553958822902, 0.17651603021658957, -0.10417369267759988, 0.14088827221152875, 0.07095067043943952, -0.04975824814456969, 0.051487160730175674, 0.3987535236355586, -0.1885902025223447, -0.37727810537967926, -0.03572612446852219, -0.3013465947543199, 0.06818204701472169, 0.15578329638064575, 0.09173052685144238... |
706.2953 | Running of $\alpha_s$ and $m_b$ in the MSSM | A consistent evolution of the strong coupling constant $\alpha_s$ from $M_Z$
to the GUT scale is presented, involving three-loop running and two-loop
decoupling. The two-loop transition from the MS- to the DR-scheme is properly
taken into account. In the second part of the paper, the bottom quark mass in
the DR-schem... | hep-ph | a consistent evolution of the strong coupling constant alpha_s from m_z to the gut scale is presented involving threeloop running and twoloop decoupling the twoloop transition from the ms to the drscheme is properly taken into account in the second part of the paper the bottom quark mass in the drscheme at the electrow... | [['a', 'consistent', 'evolution', 'of', 'the', 'strong', 'coupling', 'constant', 'alpha_s', 'from', 'm_z', 'to', 'the', 'gut', 'scale', 'is', 'presented', 'involving', 'threeloop', 'running', 'and', 'twoloop', 'decoupling', 'the', 'twoloop', 'transition', 'from', 'the', 'ms', 'to', 'the', 'drscheme', 'is', 'properly', ... | [-0.10140355377665695, 0.18856598636940927, -0.056998794111800755, 0.13251769960373389, -0.05922185341399666, -0.03820508892169675, 0.04143964703276602, 0.3257985076162259, -0.16393016500247493, -0.3106547005575251, 0.08296697057871702, -0.30935876723378897, -0.001243559316404768, 0.14959641274637417, 0.055478884146322... |
706.2954 | Ergodicity properties of quantum expectation values in entangled states | Using a model Hamiltonian for a single-mode electromagnetic field interacting
with a nonlinear medium, we show that quantum expectation values of subsystem
observables can exhibit remarkably diverse ergodic properties even when the
dynamics of the total system is regular. The time series of the mean photon
number is ... | quant-ph | using a model hamiltonian for a singlemode electromagnetic field interacting with a nonlinear medium we show that quantum expectation values of subsystem observables can exhibit remarkably diverse ergodic properties even when the dynamics of the total system is regular the time series of the mean photon number is studi... | [['using', 'a', 'model', 'hamiltonian', 'for', 'a', 'singlemode', 'electromagnetic', 'field', 'interacting', 'with', 'a', 'nonlinear', 'medium', 'we', 'show', 'that', 'quantum', 'expectation', 'values', 'of', 'subsystem', 'observables', 'can', 'exhibit', 'remarkably', 'diverse', 'ergodic', 'properties', 'even', 'when',... | [-0.1796984330322298, 0.19765989874149598, -0.07292954489913961, 0.06740317410985304, 0.012916698631006368, -0.1137476533047101, 0.011737109867796774, 0.3196741304995995, -0.28607346781341003, -0.294497080782931, 0.042925313758176, -0.2825907726646475, -0.09850914314960219, 0.20259231833984986, 0.03559026990588459, 0.0... |
706.2955 | Thue equations and torsion groups of elliptic curves | A new characterization of rational torsion subgroups of elliptic curves is
found, for points of order greater than 4, through the existence of solution
for systems of Thue equations.
| math.NT | a new characterization of rational torsion subgroups of elliptic curves is found for points of order greater than 4 through the existence of solution for systems of thue equations | [['a', 'new', 'characterization', 'of', 'rational', 'torsion', 'subgroups', 'of', 'elliptic', 'curves', 'is', 'found', 'for', 'points', 'of', 'order', 'greater', 'than', '4', 'through', 'the', 'existence', 'of', 'solution', 'for', 'systems', 'of', 'thue', 'equations']] | [-0.26732043754951706, 0.03391067216429731, -0.11197147871656664, 0.035095312588462796, -0.09093965644594924, -0.13037424057657862, 0.01763864068699808, 0.21155221663929266, -0.23151666109032673, -0.3028638682745654, 0.11076842248439789, -0.3484406119276737, -0.11191073907860394, 0.31098651411493533, -0.071384262582608... |
706.2956 | Density-dependent interactions and structure of charged colloidal
dispersions in the weak screening regime | We determine the structure of charge-stabilized colloidal suspensions at low
ionic strength over an extended range of particle volume fractions using a
combination of light and small angle neutron scattering experiments. The
variation of the structure factor with concentration is analyzed within a
one-component model... | cond-mat.soft | we determine the structure of chargestabilized colloidal suspensions at low ionic strength over an extended range of particle volume fractions using a combination of light and small angle neutron scattering experiments the variation of the structure factor with concentration is analyzed within a onecomponent model of a... | [['we', 'determine', 'the', 'structure', 'of', 'chargestabilized', 'colloidal', 'suspensions', 'at', 'low', 'ionic', 'strength', 'over', 'an', 'extended', 'range', 'of', 'particle', 'volume', 'fractions', 'using', 'a', 'combination', 'of', 'light', 'and', 'small', 'angle', 'neutron', 'scattering', 'experiments', 'the',... | [-0.10389825757239747, 0.2199117938081768, -0.11579227972817555, 0.0074348707403464435, 0.02124963568659562, -0.07917755712974775, 0.020647379899334708, 0.372574018042409, -0.25995849094908224, -0.32571924726865936, -0.011058093710499031, -0.29570811247097306, -0.1633186914508095, 0.1597356535402765, 0.0345590319039739... |
706.2957 | Reply to Comment on "A local realist model for correlations of the
singlet state" | The general conclusion of Seevinck and Larsson is that our model exploits the
so-called coincidence-time loophole and produces sinusoidal (quantum-like)
correlations but does not model the singlet state because it does not violate
the relevant Bell inequality derived by Larsson and Gill, since in order to
obtain the ... | quant-ph | the general conclusion of seevinck and larsson is that our model exploits the socalled coincidencetime loophole and produces sinusoidal quantumlike correlations but does not model the singlet state because it does not violate the relevant bell inequality derived by larsson and gill since in order to obtain the sinusoid... | [['the', 'general', 'conclusion', 'of', 'seevinck', 'and', 'larsson', 'is', 'that', 'our', 'model', 'exploits', 'the', 'socalled', 'coincidencetime', 'loophole', 'and', 'produces', 'sinusoidal', 'quantumlike', 'correlations', 'but', 'does', 'not', 'model', 'the', 'singlet', 'state', 'because', 'it', 'does', 'not', 'vio... | [-0.07014473337684902, 0.11874223670912619, -0.12928302964368432, 0.08709738129322638, -0.08182742838392552, -0.18913249688741474, 0.07396290258302823, 0.3448219846972485, -0.187130102328101, -0.3309209513737215, 0.047880680732352215, -0.2830178012937, -0.15691389065194147, 0.17745548362853295, -0.11299735657179479, 0.... |
706.2958 | On the shadow boundary of a centrally symmetric convex body | We discuss the concept of the shadow boundary of a centrally symmetric convex
ball $K$ (actually being the unit ball of a Minkowski normed space) with
respect to a direction ${\bf x}$ of the Euclidean n-space $R^n$. We introduce
the concept of general parameter spheres of $K$ corresponding to this direction
and prove... | math.MG math.GT | we discuss the concept of the shadow boundary of a centrally symmetric convex ball k actually being the unit ball of a minkowski normed space with respect to a direction bf x of the euclidean nspace rn we introduce the concept of general parameter spheres of k corresponding to this direction and prove that the shadow b... | [['we', 'discuss', 'the', 'concept', 'of', 'the', 'shadow', 'boundary', 'of', 'a', 'centrally', 'symmetric', 'convex', 'ball', 'k', 'actually', 'being', 'the', 'unit', 'ball', 'of', 'a', 'minkowski', 'normed', 'space', 'with', 'respect', 'to', 'a', 'direction', 'bf', 'x', 'of', 'the', 'euclidean', 'nspace', 'rn', 'we',... | [-0.16612647916027506, 0.1130735123134381, -0.0697214953353876, 0.0384318404619328, -0.08617596161206598, -0.0999212657342424, 0.003434606078829799, 0.3936187790094556, -0.29581829830613376, -0.13258861978839548, 0.12749869139194228, -0.30855067898161137, -0.13067480476273524, 0.13684390852605546, -0.13970153073461114,... |
706.2959 | The variability plane of accreting compact objects | Recently, it has been shown that soft-state black hole X-ray binaries and
active galactic nuclei populate a plane in the space defined by the black hole
mass, accretion rate and characteristic frequency. We show that this plane can
be extended to hard-state objects if one allows a constant offset for the
frequencies ... | astro-ph | recently it has been shown that softstate black hole xray binaries and active galactic nuclei populate a plane in the space defined by the black hole mass accretion rate and characteristic frequency we show that this plane can be extended to hardstate objects if one allows a constant offset for the frequencies in the s... | [['recently', 'it', 'has', 'been', 'shown', 'that', 'softstate', 'black', 'hole', 'xray', 'binaries', 'and', 'active', 'galactic', 'nuclei', 'populate', 'a', 'plane', 'in', 'the', 'space', 'defined', 'by', 'the', 'black', 'hole', 'mass', 'accretion', 'rate', 'and', 'characteristic', 'frequency', 'we', 'show', 'that', '... | [-0.08400913053460848, 0.20330333811725723, -0.05886367183321944, 0.13882643208892728, -0.13014886257453606, -0.09377412115796828, 0.10147842499069297, 0.374512022246535, -0.2062430525198579, -0.3198298809190209, 0.09755288923624902, -0.2813391223139031, -0.05483699183409604, 0.2590485038379064, -0.028837077878415586, ... |
706.296 | Constraints on top-down models for the origin of UHECRs from the Pierre
Auger Observatory data | Taking into account the Pierre Auger Observatory limits on the photon
fraction among the highest energy cosmic rays, we show that the models based on
the decay of super-heavy dark matter in the halo of our Galaxy are essentially
excluded from being the sources of UHECRs unless their contribution becomes
significant o... | astro-ph | taking into account the pierre auger observatory limits on the photon fraction among the highest energy cosmic rays we show that the models based on the decay of superheavy dark matter in the halo of our galaxy are essentially excluded from being the sources of uhecrs unless their contribution becomes significant only ... | [['taking', 'into', 'account', 'the', 'pierre', 'auger', 'observatory', 'limits', 'on', 'the', 'photon', 'fraction', 'among', 'the', 'highest', 'energy', 'cosmic', 'rays', 'we', 'show', 'that', 'the', 'models', 'based', 'on', 'the', 'decay', 'of', 'superheavy', 'dark', 'matter', 'in', 'the', 'halo', 'of', 'our', 'galax... | [-0.04735921745199755, 0.22867123191301003, -0.02605990797887186, 0.170753128288022, -0.07374471057969403, -0.024012339492160154, 0.04460220524749483, 0.384322418775185, -0.18962815087513032, -0.36371069781325127, 0.027154393870024437, -0.3460014456636216, 0.011743060840540621, 0.2558559606143509, 0.04815284442717591, ... |
706.2961 | Structure of glassy lithium sulfate films sputtered in nitrogen (LISON):
Insight from Raman spectroscopy and ab initio calculations | Raman spectra of thin solid electrolyte films obtained by sputtering a
lithium sulfate target in nitrogen plasma are measured and compared to ab
initio electronic structure calculations for clusters composed of 28 atoms.
Agreement between measured and calculated spectra is obtained when oxygen atoms
are replaced by n... | cond-mat.mtrl-sci | raman spectra of thin solid electrolyte films obtained by sputtering a lithium sulfate target in nitrogen plasma are measured and compared to ab initio electronic structure calculations for clusters composed of 28 atoms agreement between measured and calculated spectra is obtained when oxygen atoms are replaced by nitr... | [['raman', 'spectra', 'of', 'thin', 'solid', 'electrolyte', 'films', 'obtained', 'by', 'sputtering', 'a', 'lithium', 'sulfate', 'target', 'in', 'nitrogen', 'plasma', 'are', 'measured', 'and', 'compared', 'to', 'ab', 'initio', 'electronic', 'structure', 'calculations', 'for', 'clusters', 'composed', 'of', '28', 'atoms',... | [-0.007814597045345342, 0.22582911757533164, 0.01901760520961355, -0.06833477979446745, 0.1125678155817749, -0.1526850619353354, 0.10245229647741379, 0.4902628940256203, -0.2454981685780427, -0.3140172262840411, -0.037708716086276316, -0.37877673401552087, 0.003961540605215465, 0.14070887333056067, 0.03467109149650616,... |
706.2962 | Variable stars in the open cluster NGC 6791 and its surrounding field | Aims: This work presents a high--precision variability survey in the field of
the old, super metal-rich open cluster NGC 6791.
Methods: The data sample consists of more than 75,000 high-precision CCD time
series measurements in the V band obtained mainly at the Canada-France-Hawaii
Telescope, with additional data f... | astro-ph | aims this work presents a highprecision variability survey in the field of the old super metalrich open cluster ngc 6791 methods the data sample consists of more than 75000 highprecision ccd time series measurements in the v band obtained mainly at the canadafrancehawaii telescope with additional data from s pedro mart... | [['aims', 'this', 'work', 'presents', 'a', 'highprecision', 'variability', 'survey', 'in', 'the', 'field', 'of', 'the', 'old', 'super', 'metalrich', 'open', 'cluster', 'ngc', '6791', 'methods', 'the', 'data', 'sample', 'consists', 'of', 'more', 'than', '75000', 'highprecision', 'ccd', 'time', 'series', 'measurements', ... | [-0.10789942941990624, 0.10159043923764499, -0.10264731109688367, 0.05169064382873408, -0.12404857011237215, -0.08129011805122383, 0.1372411576268873, 0.40852869714764384, -0.16526166500235578, -0.37486270062307986, 0.1047330651379512, -0.29895976409322345, -0.03408392448323316, 0.236958791828453, -0.09090983971665285,... |
706.2963 | Outage Behavior of Discrete Memoryless Channels Under Channel Estimation
Errors | Classically, communication systems are designed assuming perfect channel
state information at the receiver and/or transmitter. However, in many
practical situations, only an estimate of the channel is available that differs
from the true channel. We address this channel mismatch scenario by using the
notion of estima... | cs.IT math.IT | classically communication systems are designed assuming perfect channel state information at the receiver andor transmitter however in many practical situations only an estimate of the channel is available that differs from the true channel we address this channel mismatch scenario by using the notion of estimationindu... | [['classically', 'communication', 'systems', 'are', 'designed', 'assuming', 'perfect', 'channel', 'state', 'information', 'at', 'the', 'receiver', 'andor', 'transmitter', 'however', 'in', 'many', 'practical', 'situations', 'only', 'an', 'estimate', 'of', 'the', 'channel', 'is', 'available', 'that', 'differs', 'from', '... | [-0.25192232385836544, 0.006018608400830999, -0.06989229090139269, 0.06759172708448023, -0.05110344524681568, -0.28623275185003877, 0.1589186328658834, 0.4009220997095108, -0.28584813755750654, -0.2505805585980415, 0.1385472969384864, -0.22303375071659684, -0.12534439706336706, 0.1654562829080969, -0.1401594649888575, ... |
706.2964 | Local models and EPR quantum correlations | A model for two entangled systems in an EPR setting is shown to reproduce the
quantum-mechanical outcomes and expectation values. Each system is represented
by a small sphere containing a point-like particle embedded in a field. A
quantum state appears as an equivalence class of several possible
particle-field config... | quant-ph | a model for two entangled systems in an epr setting is shown to reproduce the quantummechanical outcomes and expectation values each system is represented by a small sphere containing a pointlike particle embedded in a field a quantum state appears as an equivalence class of several possible particlefield configuration... | [['a', 'model', 'for', 'two', 'entangled', 'systems', 'in', 'an', 'epr', 'setting', 'is', 'shown', 'to', 'reproduce', 'the', 'quantummechanical', 'outcomes', 'and', 'expectation', 'values', 'each', 'system', 'is', 'represented', 'by', 'a', 'small', 'sphere', 'containing', 'a', 'pointlike', 'particle', 'embedded', 'in',... | [-0.1394020223370136, 0.14326432219696658, -0.07707741615609322, 0.13072547571542842, -0.027890367155715107, -0.19528176536200098, 0.03744424138700657, 0.317355909799955, -0.2373896277781733, -0.29283874962164697, 0.048596599200987314, -0.2697493363934827, -0.06497019072070631, 0.14384649947134173, -0.06273004572546806... |
706.2965 | The two Josephson junction flux qubit with large tunneling amplitude | In this paper we discuss solid-state nanoelectronic realizations of Josephson
flux qubits with large tunneling amplitude between the two macroscopic states.
The latter can be controlled via the height and wells form of the potential
barrier, which is determined by quantum-state engineering of the flux qubit
circuit. ... | cond-mat.supr-con cond-mat.mes-hall | in this paper we discuss solidstate nanoelectronic realizations of josephson flux qubits with large tunneling amplitude between the two macroscopic states the latter can be controlled via the height and wells form of the potential barrier which is determined by quantumstate engineering of the flux qubit circuit the sim... | [['in', 'this', 'paper', 'we', 'discuss', 'solidstate', 'nanoelectronic', 'realizations', 'of', 'josephson', 'flux', 'qubits', 'with', 'large', 'tunneling', 'amplitude', 'between', 'the', 'two', 'macroscopic', 'states', 'the', 'latter', 'can', 'be', 'controlled', 'via', 'the', 'height', 'and', 'wells', 'form', 'of', 't... | [-0.23906420774355128, 0.20609880337567144, 0.01321879520861281, 0.03252269911416177, 0.02357441376315782, -0.2307069428441291, 0.07646435380699365, 0.3724073971445496, -0.21216230108528525, -0.3304728473763208, -0.026994074728792988, -0.2643572846411828, -0.10765216186944697, 0.2794033875135151, 0.018365291436832097, ... |
706.2966 | Surface melting of nanoscopic epitaxial films | By introducing finite size surface and interfacial excess quantities,
interactions between interfaces are shown to modify the usual surface
premelting phenomenon. It is the case of surface melting of a thin solid film s
deposited on a planar solid substrate S. More precisely to the usual wetting
condition of the soli... | cond-mat.mtrl-sci | by introducing finite size surface and interfacial excess quantities interactions between interfaces are shown to modify the usual surface premelting phenomenon it is the case of surface melting of a thin solid film s deposited on a planar solid substrate s more precisely to the usual wetting condition of the solid s b... | [['by', 'introducing', 'finite', 'size', 'surface', 'and', 'interfacial', 'excess', 'quantities', 'interactions', 'between', 'interfaces', 'are', 'shown', 'to', 'modify', 'the', 'usual', 'surface', 'premelting', 'phenomenon', 'it', 'is', 'the', 'case', 'of', 'surface', 'melting', 'of', 'a', 'thin', 'solid', 'film', 's'... | [-0.13686571036378153, 0.25375136428419864, -0.10744054248862085, -0.009032870298688067, -0.06284471948165446, -0.1675061811954947, 0.04541190597083187, 0.36455289557925424, -0.30928477678389754, -0.2672795205657167, 0.04515462744166143, -0.3026748288189992, -0.11390294155426091, 0.12794595114246476, -0.007580282766139... |
706.2967 | Terahertz Parametric Gain in Semiconductor Superlattices | We consider a high-frequency response of electrons in a single miniband of
superlattice subject to dc and ac electric fields. Action of ac electric field
causes oscillations of electron's effective mass in miniband, which result in a
parametric resonance. We have established a theoretical feasibility of
phase-sensiti... | cond-mat.mes-hall cond-mat.stat-mech | we consider a highfrequency response of electrons in a single miniband of superlattice subject to dc and ac electric fields action of ac electric field causes oscillations of electrons effective mass in miniband which result in a parametric resonance we have established a theoretical feasibility of phasesensitive param... | [['we', 'consider', 'a', 'highfrequency', 'response', 'of', 'electrons', 'in', 'a', 'single', 'miniband', 'of', 'superlattice', 'subject', 'to', 'dc', 'and', 'ac', 'electric', 'fields', 'action', 'of', 'ac', 'electric', 'field', 'causes', 'oscillations', 'of', 'electrons', 'effective', 'mass', 'in', 'miniband', 'which'... | [-0.20706804389927055, 0.1709321942433973, -0.01518140620284594, -0.0045875783958979465, -0.10768620015841236, -0.11407825617709814, 0.10565121805682631, 0.4256923285377498, -0.24212248758920055, -0.2893120029775223, 0.012961443243917115, -0.21784459121783475, -0.08307703023794855, 0.25305985780156187, -0.0199274091697... |
706.2968 | Random resistor network model of minimal conductivity in graphene | Transport in undoped graphene is related to percolating current patterns in
the networks of {\em N-} and {\em P}-type regions reflecting the strong bipolar
charge density fluctuations. Transmissions of the {\em P-N} junctions, though
small, are vital in establishing the macroscopic conductivity. We propose a
random r... | cond-mat.mes-hall cond-mat.dis-nn | transport in undoped graphene is related to percolating current patterns in the networks of em n and em ptype regions reflecting the strong bipolar charge density fluctuations transmissions of the em pn junctions though small are vital in establishing the macroscopic conductivity we propose a random resistor network mo... | [['transport', 'in', 'undoped', 'graphene', 'is', 'related', 'to', 'percolating', 'current', 'patterns', 'in', 'the', 'networks', 'of', 'em', 'n', 'and', 'em', 'ptype', 'regions', 'reflecting', 'the', 'strong', 'bipolar', 'charge', 'density', 'fluctuations', 'transmissions', 'of', 'the', 'em', 'pn', 'junctions', 'thoug... | [-0.25688842981648835, 0.15994987570161026, 0.006483668474939423, 0.02064678257338001, 0.023927178955974356, -0.1651023282210572, 0.0923025741012416, 0.3519329543130985, -0.2654376578908684, -0.2572377568272793, -0.042389499919448535, -0.33891276564395084, -0.18268136148664937, 0.11819295611138037, -0.02105375141769215... |
706.2969 | Optical spectroscopy of RU Cam, a pulsating carbon star | We analysed the high resolution spectra of a RU Cam, classified as W Vir type
star. The atmospheric parameters of RU Cam were estimated Teff=5250K and log
g=1.0. The hydrogen deficiency of RU Cam was not confirmed. The iron abundance,
[Fe/H]=-0.37, is close to the solar one. Abundances of most other elements are
also... | astro-ph | we analysed the high resolution spectra of a ru cam classified as w vir type star the atmospheric parameters of ru cam were estimated teff5250k and log g10 the hydrogen deficiency of ru cam was not confirmed the iron abundance feh037 is close to the solar one abundances of most other elements are also close to normal w... | [['we', 'analysed', 'the', 'high', 'resolution', 'spectra', 'of', 'a', 'ru', 'cam', 'classified', 'as', 'w', 'vir', 'type', 'star', 'the', 'atmospheric', 'parameters', 'of', 'ru', 'cam', 'were', 'estimated', 'teff5250k', 'and', 'log', 'g10', 'the', 'hydrogen', 'deficiency', 'of', 'ru', 'cam', 'was', 'not', 'confirmed',... | [-0.0683374595410865, 0.12925010643636503, 0.01725925362251442, 0.03856288428851885, -0.014319660410220767, -0.1359813028400571, 0.05718269167018348, 0.44343752213593185, -0.192053924378104, -0.33112456398405904, 0.0002706762098161311, -0.3428402964154194, 0.013984292960757838, 0.13291863376949112, -0.02062173178098325... |
706.297 | On Scattering for CMV Matrices | Adamjan-Arov (Lax--Phillips) model space is considered as a scattering
representation space for a CMV matrix in context of an extended
Marchenko--Faddeev scattering theory. That is, there exists a basis in which
the multiplication by independent variable is a CMV matrix. This basis as well
as Verblunski coefficients ... | math.SP math.FA | adamjanarov laxphillips model space is considered as a scattering representation space for a cmv matrix in context of an extended marchenkofaddeev scattering theory that is there exists a basis in which the multiplication by independent variable is a cmv matrix this basis as well as verblunski coefficients are computed... | [['adamjanarov', 'laxphillips', 'model', 'space', 'is', 'considered', 'as', 'a', 'scattering', 'representation', 'space', 'for', 'a', 'cmv', 'matrix', 'in', 'context', 'of', 'an', 'extended', 'marchenkofaddeev', 'scattering', 'theory', 'that', 'is', 'there', 'exists', 'a', 'basis', 'in', 'which', 'the', 'multiplication... | [-0.09007436040087373, 0.13219329563151688, -0.10866651560675789, 0.1019148820294551, -0.0677769234428158, -0.09547955044484757, 0.015038984581259648, 0.3670984621026686, -0.33092756017849045, -0.18579547583766573, 0.14164331566403293, -0.2712760276624906, -0.22477935693625892, 0.1578025491515102, -0.033020313345379644... |
706.2971 | Entropy profiles in X-ray luminous galaxy clusters at z>0.1 | [Abridged] The entropy distribution of the intracluster gas reflects both
accretion history of the gas and processes of feedback which provide a further
non-gravitational energy besides the potential one. In this work, we study the
profiles and the scaling properties of the gas entropy in 24 hot (kT_{gas} > 6
keV) ga... | astro-ph | abridged the entropy distribution of the intracluster gas reflects both accretion history of the gas and processes of feedback which provide a further nongravitational energy besides the potential one in this work we study the profiles and the scaling properties of the gas entropy in 24 hot kt_gas 6 kev galaxy clusters... | [['abridged', 'the', 'entropy', 'distribution', 'of', 'the', 'intracluster', 'gas', 'reflects', 'both', 'accretion', 'history', 'of', 'the', 'gas', 'and', 'processes', 'of', 'feedback', 'which', 'provide', 'a', 'further', 'nongravitational', 'energy', 'besides', 'the', 'potential', 'one', 'in', 'this', 'work', 'we', 's... | [-0.0758771464954147, 0.13608124672448738, -0.08989343583234585, 0.08523614797075944, 0.011020526820461132, -0.05673644545687628, 0.07311145611373442, 0.37113941676382506, -0.2219948090363427, -0.3583470197959936, 0.05438752291083802, -0.3202423631795682, 0.0187473730865999, 0.17244820862210222, 0.008173393335268234, -... |
706.2972 | Electron-positron annihilation into phi f_{0}(980) and clues for a new
1^{--} resonance | We study the e^{+}e^{-} to phi pi pi reaction for pions in an isoscalar
s-wave which is dominated by loop mechanisms. For kaon loops we start from the
conventional RCHPT, but use the unitarized amplitude for KbarK-pipi scattering
and the full kaon form factor instead of the lowest order terms. We study also
effects o... | hep-ph | we study the ee to phi pi pi reaction for pions in an isoscalar swave which is dominated by loop mechanisms for kaon loops we start from the conventional rchpt but use the unitarized amplitude for kbarkpipi scattering and the full kaon form factor instead of the lowest order terms we study also effects of vector mesons... | [['we', 'study', 'the', 'ee', 'to', 'phi', 'pi', 'pi', 'reaction', 'for', 'pions', 'in', 'an', 'isoscalar', 'swave', 'which', 'is', 'dominated', 'by', 'loop', 'mechanisms', 'for', 'kaon', 'loops', 'we', 'start', 'from', 'the', 'conventional', 'rchpt', 'but', 'use', 'the', 'unitarized', 'amplitude', 'for', 'kbarkpipi', ... | [-0.11163261632113416, 0.2153529404603295, -0.0867398792562467, 0.13443331232817052, -0.05473577559476705, -0.09376057721808445, 0.07461853634914477, 0.3023257739171922, -0.20698880826344165, -0.22518194846058492, -0.04601587334366368, -0.3270669388417289, -0.07370941294341476, 0.11373996343329656, 0.12757780303066368,... |
706.2973 | Nontrivial critical crossover between directed percolation models:
Effect of infinitely many absorbing states | At non-equilibrium phase transitions into absorbing (trapped) states, it is
well known that the directed percolation (DP) critical scaling is shared by two
classes of models with a single (S) absorbing state and with infinitely many
(IM) absorbing states. We study the crossover behavior in one dimension,
arising from... | cond-mat.stat-mech | at nonequilibrium phase transitions into absorbing trapped states it is well known that the directed percolation dp critical scaling is shared by two classes of models with a single s absorbing state and with infinitely many im absorbing states we study the crossover behavior in one dimension arising from a considerabl... | [['at', 'nonequilibrium', 'phase', 'transitions', 'into', 'absorbing', 'trapped', 'states', 'it', 'is', 'well', 'known', 'that', 'the', 'directed', 'percolation', 'dp', 'critical', 'scaling', 'is', 'shared', 'by', 'two', 'classes', 'of', 'models', 'with', 'a', 'single', 's', 'absorbing', 'state', 'and', 'with', 'infini... | [-0.130272738077261, 0.22318718020655653, -0.061110205081991276, 0.04754755160583502, -0.030762262936316183, -0.23598564675499722, 0.0944323804903549, 0.3360573098125214, -0.2919048042916461, -0.23562532449295506, 0.050073862074519304, -0.309886398672471, -0.1468384808395058, 0.12958455640174324, 0.03149413230291244, 0... |
706.2974 | Remote laboratories: new technology and standard based architecture | E-Laboratories are important components of e- learning environments,
especially in scientific and technical disciplines. First widespread E-Labs
consisted in proposing simulations of real systems (virtual labs), as building
remote labs (remote control of real systems) was difficult by lack of
industrial standards and... | cs.OH | elaboratories are important components of e learning environments especially in scientific and technical disciplines first widespread elabs consisted in proposing simulations of real systems virtual labs as building remote labs remote control of real systems was difficult by lack of industrial standards and common prot... | [['elaboratories', 'are', 'important', 'components', 'of', 'e', 'learning', 'environments', 'especially', 'in', 'scientific', 'and', 'technical', 'disciplines', 'first', 'widespread', 'elabs', 'consisted', 'in', 'proposing', 'simulations', 'of', 'real', 'systems', 'virtual', 'labs', 'as', 'building', 'remote', 'labs', ... | [-0.11815052443361353, 0.06827815891731354, -0.0066195245050559084, 0.005700717449543022, -0.07999876393670483, -0.16684849729672785, 0.029515512581426828, 0.40774938194524674, -0.25026089598735174, -0.38457788436540535, 0.13369383859847273, -0.2457227991095611, -0.1501221173886387, 0.2890128384033839, -0.1179236587403... |
706.2975 | U_{PMNS} = U_ell^dagger U_nu | We consider corrections to vanishing U_{e3} and maximal atmospheric neutrino
mixing originating from the relation U = U_ell^dagger U_nu, where U is the PMNS
mixing matrix and U_ell (U_nu) is associated with the diagonalization of the
charged lepton (neutrino) mass matrix. We assume that in the limit of U_ell or
U_nu ... | hep-ph | we consider corrections to vanishing u_e3 and maximal atmospheric neutrino mixing originating from the relation u u_elldagger u_nu where u is the pmns mixing matrix and u_ell u_nu is associated with the diagonalization of the charged lepton neutrino mass matrix we assume that in the limit of u_ell or u_nu being the uni... | [['we', 'consider', 'corrections', 'to', 'vanishing', 'u_e3', 'and', 'maximal', 'atmospheric', 'neutrino', 'mixing', 'originating', 'from', 'the', 'relation', 'u', 'u_elldagger', 'u_nu', 'where', 'u', 'is', 'the', 'pmns', 'mixing', 'matrix', 'and', 'u_ell', 'u_nu', 'is', 'associated', 'with', 'the', 'diagonalization', ... | [-0.15650638843413872, 0.31967042497916137, 0.0686662201055948, 0.1500900212971344, -0.051257113261550816, -0.17743366920557715, 0.0918110856363999, 0.2849059229828979, -0.2782161178291967, -0.26488765206506204, 0.07565560896328684, -0.3366596049327291, -0.07129317952961141, 0.15380867538697568, 0.02074029099608037, 0.... |
706.2976 | The Interaction Of Multiple Convection Zones In A-type Stars | A-type stars have a complex internal structure with the possibility of
multiple convection zones. If not sufficiently separated, such zones will
interact through the convectively stable regions that lie between them. It is
therefore of interest to ask whether the typical conditions that exist within
such stars are su... | astro-ph | atype stars have a complex internal structure with the possibility of multiple convection zones if not sufficiently separated such zones will interact through the convectively stable regions that lie between them it is therefore of interest to ask whether the typical conditions that exist within such stars are such tha... | [['atype', 'stars', 'have', 'a', 'complex', 'internal', 'structure', 'with', 'the', 'possibility', 'of', 'multiple', 'convection', 'zones', 'if', 'not', 'sufficiently', 'separated', 'such', 'zones', 'will', 'interact', 'through', 'the', 'convectively', 'stable', 'regions', 'that', 'lie', 'between', 'them', 'it', 'is', ... | [-0.11628088928325084, 0.23476165761375456, -0.06487368040003823, 0.07615642283830647, -0.08295399479305787, -0.08360011681679239, 0.06259029277134687, 0.41254625256055766, -0.2889124870535384, -0.28657221318520965, 0.10189845386973935, -0.26885985875574564, -0.1553516806944192, 0.20227266430348448, -0.0183646077387943... |
706.2977 | Rational formality of function spaces | Let $X$ be a nilpotent space such that there exists $N\geq 1$ with
$H^N(X,\mathbb Q) \ne 0$ and $H^n(X,\mathbb Q)=0$ if $n>N$. Let $Y$ be a
m-connected space with $m\geq N+1$ and $H^*(Y,\mathbb Q)$ is finitely generated
as algebra. We assume that the odd part of the rational Hurewicz homomorphism:
$\pi_{odd}(X)\otime... | math.AT | let x be a nilpotent space such that there exists ngeq 1 with hnxmathbb q ne 0 and hnxmathbb q0 if nn let y be a mconnected space with mgeq n1 and hymathbb q is finitely generated as algebra we assume that the odd part of the rational hurewicz homomorphism pi_oddxotimes mathbb qto h_oddxmathbb q is nonzero we prove tha... | [['let', 'x', 'be', 'a', 'nilpotent', 'space', 'such', 'that', 'there', 'exists', 'ngeq', '1', 'with', 'hnxmathbb', 'q', 'ne', '0', 'and', 'hnxmathbb', 'q0', 'if', 'nn', 'let', 'y', 'be', 'a', 'mconnected', 'space', 'with', 'mgeq', 'n1', 'and', 'hymathbb', 'q', 'is', 'finitely', 'generated', 'as', 'algebra', 'we', 'ass... | [-0.21226625703275204, 0.11434021977559906, -0.08828704668192473, 0.0005991277037666435, -0.052523478301060675, -0.2437863926304323, -0.025571815504700737, 0.4037886108642658, -0.38879287305527027, -0.09596496272782705, 0.0598269623489968, -0.2714189817156412, -0.09793619202878491, 0.12217959486343692, -0.1631389218712... |
706.2978 | Quantum and semiclassical phase functions for the quantization of
symmetric oscillators | We investigate symmetric oscillators, and in particular their quantization,
by employing semiclassical and quantum phase functions introduced in the
context of Liouville-Green transformations of the Schr\"{o}dinger equation. For
anharmonic oscillators, first order semiclassical quantization is seldom
accurate and the... | quant-ph hep-th math-ph math.MP | we investigate symmetric oscillators and in particular their quantization by employing semiclassical and quantum phase functions introduced in the context of liouvillegreen transformations of the schrodinger equation for anharmonic oscillators first order semiclassical quantization is seldom accurate and the higher ord... | [['we', 'investigate', 'symmetric', 'oscillators', 'and', 'in', 'particular', 'their', 'quantization', 'by', 'employing', 'semiclassical', 'and', 'quantum', 'phase', 'functions', 'introduced', 'in', 'the', 'context', 'of', 'liouvillegreen', 'transformations', 'of', 'the', 'schrodinger', 'equation', 'for', 'anharmonic',... | [-0.14779116333212092, 0.17465373238215462, -0.06279538496077727, 0.050520472682025565, -0.09356465914682832, -0.14221866076826048, 0.04989549230763327, 0.3248278524504224, -0.24656835328196802, -0.24455089424476167, 0.07686946202337103, -0.2614299225894154, -0.17738943654043016, 0.16234383158344054, -0.027329955517606... |
706.2979 | Security problems with a SC-CNN-based Chaotic Masking Secure
Communication System | This paper studies the security of a chaotic cryptosystem based on the Chua
circuit and implemented with State Controlled Cellular Neural Networks. It is
shown that the plaintext can be retrieved by ciphertext band-pass filtering
after an imperfect decoding with wrong receiver parameters. It is also shown
that the ke... | nlin.CD | this paper studies the security of a chaotic cryptosystem based on the chua circuit and implemented with state controlled cellular neural networks it is shown that the plaintext can be retrieved by ciphertext bandpass filtering after an imperfect decoding with wrong receiver parameters it is also shown that the key spa... | [['this', 'paper', 'studies', 'the', 'security', 'of', 'a', 'chaotic', 'cryptosystem', 'based', 'on', 'the', 'chua', 'circuit', 'and', 'implemented', 'with', 'state', 'controlled', 'cellular', 'neural', 'networks', 'it', 'is', 'shown', 'that', 'the', 'plaintext', 'can', 'be', 'retrieved', 'by', 'ciphertext', 'bandpass'... | [-0.16392854666176798, 0.07730233399669142, -0.0796264632439091, 0.019751146945556432, -0.02114195311334969, -0.28749672508124136, 0.0741565881267554, 0.36960280280902813, -0.300466304366616, -0.31800731252236614, 0.13289058225593348, -0.2202356266360944, -0.19054807197093834, 0.21716683150279795, -0.1261270452911655, ... |
706.298 | Kinetics of cell division in epidermal maintenance | The rules governing cell division and differentiation are central to
understanding the mechanisms of development, aging and cancer. By utilising
inducible genetic labelling, recent studies have shown that the clonal
population in transgenic mouse epidermis can be tracked in vivo. Drawing on
these results, we explain ... | physics.bio-ph cond-mat.stat-mech q-bio.CB | the rules governing cell division and differentiation are central to understanding the mechanisms of development aging and cancer by utilising inducible genetic labelling recent studies have shown that the clonal population in transgenic mouse epidermis can be tracked in vivo drawing on these results we explain how clo... | [['the', 'rules', 'governing', 'cell', 'division', 'and', 'differentiation', 'are', 'central', 'to', 'understanding', 'the', 'mechanisms', 'of', 'development', 'aging', 'and', 'cancer', 'by', 'utilising', 'inducible', 'genetic', 'labelling', 'recent', 'studies', 'have', 'shown', 'that', 'the', 'clonal', 'population', '... | [-0.0489736498514768, 0.1376774372957364, -0.06699160922786937, 0.06330514777101034, -0.05965090450636241, -0.11841448883067734, 0.10055063472312133, 0.3527006869516748, -0.24890714656868124, -0.2023323698004684, 0.12163339886015659, -0.20842954323662422, -0.2528285916034085, 0.18697836504559492, -0.1357265181627266, -... |
706.2981 | Moduli space of Brody curves, energy and mean dimension | We study the mean dimension of the moduli space of Brody curves. We introduce
the notion of "mean energy" and show that this can be used to estimate the mean
dimension.
| math.DG math.CV | we study the mean dimension of the moduli space of brody curves we introduce the notion of mean energy and show that this can be used to estimate the mean dimension | [['we', 'study', 'the', 'mean', 'dimension', 'of', 'the', 'moduli', 'space', 'of', 'brody', 'curves', 'we', 'introduce', 'the', 'notion', 'of', 'mean', 'energy', 'and', 'show', 'that', 'this', 'can', 'be', 'used', 'to', 'estimate', 'the', 'mean', 'dimension']] | [-0.10693291772998148, 0.13374761110472103, -0.1646420309590476, 0.1374318958823419, -0.022822856106945583, -0.011195686495592517, 0.011968403934471069, 0.3498482535923681, -0.3120140176446688, -0.27831255524389203, 0.06359564251596889, -0.20620170593141549, -0.19575051911693486, 0.1798050496126375, -0.1670748322841621... |
706.2982 | Dimensional Reduction applied to QCD at higher orders | Recent developments in higher order calculations within the framework of
Dimensional Reduction, the preferred regularization scheme for supersymmetric
theories, are reported on. Special emphasis is put on the treatment of
evanescent couplings, the equivalence to Dimensional Regularization, and the
evaluation of $\alp... | hep-ph | recent developments in higher order calculations within the framework of dimensional reduction the preferred regularization scheme for supersymmetric theories are reported on special emphasis is put on the treatment of evanescent couplings the equivalence to dimensional regularization and the evaluation of alpha_sm_gut... | [['recent', 'developments', 'in', 'higher', 'order', 'calculations', 'within', 'the', 'framework', 'of', 'dimensional', 'reduction', 'the', 'preferred', 'regularization', 'scheme', 'for', 'supersymmetric', 'theories', 'are', 'reported', 'on', 'special', 'emphasis', 'is', 'put', 'on', 'the', 'treatment', 'of', 'evanesce... | [-0.09307550911813281, 0.07739817275297503, -0.030512852854160374, 0.05706430848438813, -0.0796369836600714, -0.14673452191921169, 0.035304522401718205, 0.36782824594614116, -0.12473947203956372, -0.27165108572605046, 0.0847369680143243, -0.26498975930194, -0.09750512909404067, 0.1865645469177168, -0.028132192081187005... |
706.2983 | Real Forms of Complex Higher Spin Field Equations and New Exact
Solutions | We formulate four dimensional higher spin gauge theories in spacetimes with
signature (4-p,p) and nonvanishing cosmological constant. Among them are chiral
models in Euclidean (4,0) and Kleinian (2,2) signature involving half-flat
gauge fields. Apart from the maximally symmetric solutions, including de Sitter
spaceti... | hep-th | we formulate four dimensional higher spin gauge theories in spacetimes with signature 4pp and nonvanishing cosmological constant among them are chiral models in euclidean 40 and kleinian 22 signature involving halfflat gauge fields apart from the maximally symmetric solutions including de sitter spacetime we find a so4... | [['we', 'formulate', 'four', 'dimensional', 'higher', 'spin', 'gauge', 'theories', 'in', 'spacetimes', 'with', 'signature', '4pp', 'and', 'nonvanishing', 'cosmological', 'constant', 'among', 'them', 'are', 'chiral', 'models', 'in', 'euclidean', '40', 'and', 'kleinian', '22', 'signature', 'involving', 'halfflat', 'gauge... | [-0.20707967918780115, 0.23500413365103737, -0.024270454714833585, 0.07256989207256723, -0.10967226501347291, -0.2071100468100566, -0.08454159021170603, 0.298213188584756, -0.16293473098840977, -0.22713787079685263, 0.10362827293229876, -0.2892432801425457, -0.15172104174443693, 0.11236894201590783, 0.01935269424898757... |
706.2984 | QED collinear radiation factors in the next-to-leading logarithmic
approximation | The effect of the collinear photon radiation by charged particles is
considered in the second order of the perturbation theory. Double and single
photon radiation is evaluated. The corresponding radiation factors are
obtained. The QED renormalization group approach is exploited in the
next-to-leading order. The resul... | hep-ph | the effect of the collinear photon radiation by charged particles is considered in the second order of the perturbation theory double and single photon radiation is evaluated the corresponding radiation factors are obtained the qed renormalization group approach is exploited in the nexttoleading order the results are s... | [['the', 'effect', 'of', 'the', 'collinear', 'photon', 'radiation', 'by', 'charged', 'particles', 'is', 'considered', 'in', 'the', 'second', 'order', 'of', 'the', 'perturbation', 'theory', 'double', 'and', 'single', 'photon', 'radiation', 'is', 'evaluated', 'the', 'corresponding', 'radiation', 'factors', 'are', 'obtain... | [-0.10214732276782502, 0.1619843079636613, -0.08160195816034342, 0.12346753892865416, -0.028063548002939892, -0.05891811366275172, -0.008915261988209643, 0.35841566381756873, -0.19377719934153206, -0.2963100860669168, 0.022058564440265077, -0.34614545636063937, -0.047221850210061186, 0.14307800975888418, 0.064504470552... |
706.2985 | Characterization of an asynchronous source of heralded single photons
generated at a wavelength of 1550 nm | We make a thorough analysis of heralded single photon sources regarding how
factors such as the detector gate-period, the photon rates, the fiber coupling
efficiencies, and the system losses affect the performance of the source. In
the course of this we give a detailed description of how to determine fiber
coupling e... | quant-ph | we make a thorough analysis of heralded single photon sources regarding how factors such as the detector gateperiod the photon rates the fiber coupling efficiencies and the system losses affect the performance of the source in the course of this we give a detailed description of how to determine fiber coupling efficien... | [['we', 'make', 'a', 'thorough', 'analysis', 'of', 'heralded', 'single', 'photon', 'sources', 'regarding', 'how', 'factors', 'such', 'as', 'the', 'detector', 'gateperiod', 'the', 'photon', 'rates', 'the', 'fiber', 'coupling', 'efficiencies', 'and', 'the', 'system', 'losses', 'affect', 'the', 'performance', 'of', 'the',... | [-0.10893631816756541, 0.18701316678956945, -0.046040164537086925, -0.0017211746063924606, 0.002031065549911751, -0.1923318334394485, 0.09790298716798525, 0.47605971834792565, -0.19527972109117595, -0.2930830690264326, 0.026142416565093182, -0.3050278930434136, -0.008015841725082087, 0.26370902412686176, -0.05001261477... |
706.2986 | Dark Matter and Dark Energy | This is a short review, aimed at a general audience, of several current
subjects of research in cosmology. The topics discussed include the cosmic
microwave background (CMB), with particular emphasis on its relevance for
testing inflation; dark matter, with a brief review of astrophysical evidence
and more emphasis o... | astro-ph | this is a short review aimed at a general audience of several current subjects of research in cosmology the topics discussed include the cosmic microwave background cmb with particular emphasis on its relevance for testing inflation dark matter with a brief review of astrophysical evidence and more emphasis on particle... | [['this', 'is', 'a', 'short', 'review', 'aimed', 'at', 'a', 'general', 'audience', 'of', 'several', 'current', 'subjects', 'of', 'research', 'in', 'cosmology', 'the', 'topics', 'discussed', 'include', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'with', 'particular', 'emphasis', 'on', 'its', 'relevance', 'for', '... | [-0.07828510963315095, 0.12351625246044837, -0.09145904618535976, 0.14618562993526116, -0.15337874692570613, -0.12434998004525703, -0.024078846198359604, 0.33956378355230155, -0.14550139395961245, -0.30992745340948824, 0.12493746918105324, -0.2791334476787597, -0.0849204478099158, 0.26547404093894567, -0.03174261707126... |
706.2987 | Explicit birational geometry of threefolds of general type | Let $V$ be a complex nonsingular projective 3-fold of general type. We prove
$P_{12}(V)>0$ and $P_{24}(V)>1$ (which answers an open problem of J. Kollar and
S. Mori). We also prove that the canonical volume has an universal lower bound
$\text{Vol}(V) \geq 1/2660$ and that the pluri-canonical map $\Phi_m$ is
birationa... | math.AG | let v be a complex nonsingular projective 3fold of general type we prove p_12v0 and p_24v1 which answers an open problem of j kollar and s mori we also prove that the canonical volume has an universal lower bound textvolv geq 12660 and that the pluricanonical map phi_m is birational onto its image for all mgeq 77 as an... | [['let', 'v', 'be', 'a', 'complex', 'nonsingular', 'projective', '3fold', 'of', 'general', 'type', 'we', 'prove', 'p_12v0', 'and', 'p_24v1', 'which', 'answers', 'an', 'open', 'problem', 'of', 'j', 'kollar', 'and', 's', 'mori', 'we', 'also', 'prove', 'that', 'the', 'canonical', 'volume', 'has', 'an', 'universal', 'lower... | [-0.16970656940506565, 0.02365736055831399, -0.06311056644966205, 0.05603178153073208, -0.0482021799000601, -0.23836717950180172, -0.008048432338465418, 0.30778449123932256, -0.2867108613045679, -0.21829917997690954, 0.06381619229602317, -0.28755747713924695, -0.14089574198523122, 0.2318482349264539, -0.179466732943223... |
706.2988 | Parton distribution functions and quark orbital motion | Covariant version of the quark-parton model is studied. Dependence of the
structure functions and parton distributions on the 3D quark intrinsic motion
is discussed. The important role of the quark orbital momentum, which is a
particular case of intrinsic motion, appears as a direct consequence of the
covariant descr... | hep-ph | covariant version of the quarkparton model is studied dependence of the structure functions and parton distributions on the 3d quark intrinsic motion is discussed the important role of the quark orbital momentum which is a particular case of intrinsic motion appears as a direct consequence of the covariant description ... | [['covariant', 'version', 'of', 'the', 'quarkparton', 'model', 'is', 'studied', 'dependence', 'of', 'the', 'structure', 'functions', 'and', 'parton', 'distributions', 'on', 'the', '3d', 'quark', 'intrinsic', 'motion', 'is', 'discussed', 'the', 'important', 'role', 'of', 'the', 'quark', 'orbital', 'momentum', 'which', '... | [-0.11108057259996205, 0.1771852993135622, -0.15506690628501738, 0.1356138589339829, -0.07864020163529055, -0.01033057838808312, -0.004630527794794287, 0.38182681543362695, -0.2446473005043646, -0.24666301352729977, -0.013650914356329067, -0.23576934703863983, -0.044138526619780204, 0.13612853715921816, 0.0501729511157... |
706.2989 | Low-energy Dipole Excitations in Nuclei at the N=50,82 and Z=50 Shell
Closures as Signatures for a Neutron Skin | Low-energy dipole excitations have been investigated theoretically in N=50,
several N=82 isotones and the Z=50 Sn isotopes. For this purpose a method
incorporating both HFB and multi-phonon QPM theory is applied. A concentration
of one-phonon dipole strength located below the neutron emission threshold has
been calcu... | nucl-th | lowenergy dipole excitations have been investigated theoretically in n50 several n82 isotones and the z50 sn isotopes for this purpose a method incorporating both hfb and multiphonon qpm theory is applied a concentration of onephonon dipole strength located below the neutron emission threshold has been calculated in th... | [['lowenergy', 'dipole', 'excitations', 'have', 'been', 'investigated', 'theoretically', 'in', 'n50', 'several', 'n82', 'isotones', 'and', 'the', 'z50', 'sn', 'isotopes', 'for', 'this', 'purpose', 'a', 'method', 'incorporating', 'both', 'hfb', 'and', 'multiphonon', 'qpm', 'theory', 'is', 'applied', 'a', 'concentration'... | [-0.03740222061917718, 0.18545034251719555, -0.06306619128389727, 0.16872504380317258, -0.009257726881298282, -0.08774041760452314, 0.05527751416333818, 0.4051186252119286, -0.14858861065780124, -0.2513703397005826, -0.07084165723709804, -0.3469556992567959, -0.029494705211300966, 0.14154786947700712, 0.126539099776733... |
706.299 | QCD dynamics at low x in ep collisions at HERA | Forward jet and multijet production has been measured at low Bjorken x at
HERA. The measured cross sections and correlations were compared to predictions
from DGLAP-based fixed-order calculations. Further comparisons were made to
DGLAP-based and CCFM-based leading-order Monte Carlo predictions, as well as to
Colour-D... | hep-ex | forward jet and multijet production has been measured at low bjorken x at hera the measured cross sections and correlations were compared to predictions from dglapbased fixedorder calculations further comparisons were made to dglapbased and ccfmbased leadingorder monte carlo predictions as well as to colourdipole model... | [['forward', 'jet', 'and', 'multijet', 'production', 'has', 'been', 'measured', 'at', 'low', 'bjorken', 'x', 'at', 'hera', 'the', 'measured', 'cross', 'sections', 'and', 'correlations', 'were', 'compared', 'to', 'predictions', 'from', 'dglapbased', 'fixedorder', 'calculations', 'further', 'comparisons', 'were', 'made',... | [0.012576668132096529, 0.07584249179364026, -0.1237949416662256, 0.16388515040278434, 0.00033282662431399025, -0.06229635163831214, -0.006502068725725015, 0.4113151728113492, -0.16413408456370235, -0.31264627354840435, 0.04418077561228226, -0.4047454388315479, 0.06597970990464092, 0.1566552175115794, 0.0726643264134569... |
706.2991 | Wave propagation in axion electrodynamics | In this paper, the axion contribution to the electromagnetic wave propagation
is studied. First we show how the axion electrodynamics model can be embedded
into a premetric formalism of Maxwell electrodynamics. In this formalism, the
axion field is not an arbitrary added Chern-Simon term of the Lagrangian, but
emerge... | hep-th | in this paper the axion contribution to the electromagnetic wave propagation is studied first we show how the axion electrodynamics model can be embedded into a premetric formalism of maxwell electrodynamics in this formalism the axion field is not an arbitrary added chernsimon term of the lagrangian but emerges in a n... | [['in', 'this', 'paper', 'the', 'axion', 'contribution', 'to', 'the', 'electromagnetic', 'wave', 'propagation', 'is', 'studied', 'first', 'we', 'show', 'how', 'the', 'axion', 'electrodynamics', 'model', 'can', 'be', 'embedded', 'into', 'a', 'premetric', 'formalism', 'of', 'maxwell', 'electrodynamics', 'in', 'this', 'fo... | [-0.1731397567983075, 0.16640392355541486, -0.10754265525861773, 0.11075588757212332, -0.15020045433104323, -0.08441264567112453, -0.04345187992269717, 0.3288644061660011, -0.2678856931784988, -0.28814485169608484, 0.02491435591848879, -0.23191448852740693, -0.1983449552854318, 0.16256079930059042, -0.03806342630041095... |
706.2992 | Strong Lensing Analysis of the Cluster RCS0224-0002 at $z=0.77$ | We present a detailed mass reconstruction of the cluster RCS0224-0002 at
$z=0.773$ from the strong lensing features observed with HST/WFPC2. The mass
profile is reconstructed using a parametric approach. We introduce a novel
method to fit extended multiple images based on the Modified Hausdorff Distance
between obser... | astro-ph | we present a detailed mass reconstruction of the cluster rcs02240002 at z0773 from the strong lensing features observed with hstwfpc2 the mass profile is reconstructed using a parametric approach we introduce a novel method to fit extended multiple images based on the modified hausdorff distance between observed arcs a... | [['we', 'present', 'a', 'detailed', 'mass', 'reconstruction', 'of', 'the', 'cluster', 'rcs02240002', 'at', 'z0773', 'from', 'the', 'strong', 'lensing', 'features', 'observed', 'with', 'hstwfpc2', 'the', 'mass', 'profile', 'is', 'reconstructed', 'using', 'a', 'parametric', 'approach', 'we', 'introduce', 'a', 'novel', 'm... | [-0.05117261299535897, 0.0386599342593542, -0.1299010554776389, 0.10820932809877501, -0.049967696125546066, -0.11048642617842074, 0.014167203502866495, 0.37480956349777533, -0.21116289252006704, -0.36174296465355393, 0.03917860372309281, -0.3074794354318988, -0.05470874289269833, 0.21990215036643634, 0.0041324427721145... |
706.2993 | Sensitivity of the NEMO detector to galactic microquasars | We present the results of Monte Carlo simulation studies of the capability of
the proposed NEMO km$^3$ telescope to detect TeV muon neutrinos from Galactic
microquasars. In particular we determined the detector sensitivity to each
known microquasar, optimizing the event selection in order to reject the
atmospheric ba... | astro-ph | we present the results of monte carlo simulation studies of the capability of the proposed nemo km3 telescope to detect tev muon neutrinos from galactic microquasars in particular we determined the detector sensitivity to each known microquasar optimizing the event selection in order to reject the atmospheric backgroun... | [['we', 'present', 'the', 'results', 'of', 'monte', 'carlo', 'simulation', 'studies', 'of', 'the', 'capability', 'of', 'the', 'proposed', 'nemo', 'km3', 'telescope', 'to', 'detect', 'tev', 'muon', 'neutrinos', 'from', 'galactic', 'microquasars', 'in', 'particular', 'we', 'determined', 'the', 'detector', 'sensitivity', ... | [-0.062274351096881043, 0.1279339464005804, -0.000867787207807264, 0.17266357086238363, -0.11351243831637886, -0.06609309783896371, 0.05557280001906498, 0.3649906184704554, -0.17608167432368763, -0.39979801282137367, 0.048477882718397, -0.34493238022250516, -0.033918439230370905, 0.20992809559984674, 0.0037070751911209... |
706.2994 | The cluster galaxy luminosity function at $z=0.3$: a recent origin for
the faint-end upturn ? | We derive deep luminosity functions (to $M_z=-15$) for galaxies in Abell 1835
($z=0.25$) and AC 114 ($z=0.31$) and compare these with the local $z'$
luminosity function for 69 clusters. The data show that the faint-end upturn,
the excess of galaxies above a single Schechter function at $M_z < -17$, does
not exist in ... | astro-ph | we derive deep luminosity functions to m_z15 for galaxies in abell 1835 z025 and ac 114 z031 and compare these with the local z luminosity function for 69 clusters the data show that the faintend upturn the excess of galaxies above a single schechter function at m_z 17 does not exist in the higher redshift clusters thi... | [['we', 'derive', 'deep', 'luminosity', 'functions', 'to', 'm_z15', 'for', 'galaxies', 'in', 'abell', '1835', 'z025', 'and', 'ac', '114', 'z031', 'and', 'compare', 'these', 'with', 'the', 'local', 'z', 'luminosity', 'function', 'for', '69', 'clusters', 'the', 'data', 'show', 'that', 'the', 'faintend', 'upturn', 'the', ... | [-0.021597646038841317, 0.07922398587861271, -0.10744671275793219, 0.14373964233824085, -0.10667121753292043, -0.02165024417716964, 0.060823120901154146, 0.4767195415901549, -0.05543093320936608, -0.38906656999003003, -0.03944666680511961, -0.3193101863273316, -0.027806627193327854, 0.17327301391618855, 0.0184073208566... |
706.2995 | Injectivity and Projectivity in Analysis and Topology | We give new proofs for many injectivity results in analysis that make more
careful use of the duality between unital abelian C*-algebras and compact
Hausdorff spaces. We then extend many of these results to incorporate group
actions. Our approach uses only elementary topological constructions and
eliminates the need ... | math.OA | we give new proofs for many injectivity results in analysis that make more careful use of the duality between unital abelian calgebras and compact hausdorff spaces we then extend many of these results to incorporate group actions our approach uses only elementary topological constructions and eliminates the need for re... | [['we', 'give', 'new', 'proofs', 'for', 'many', 'injectivity', 'results', 'in', 'analysis', 'that', 'make', 'more', 'careful', 'use', 'of', 'the', 'duality', 'between', 'unital', 'abelian', 'calgebras', 'and', 'compact', 'hausdorff', 'spaces', 'we', 'then', 'extend', 'many', 'of', 'these', 'results', 'to', 'incorporate... | [-0.04998947675994714, 0.08093235725391423, -0.14366405695909634, 0.12118693823140347, -0.14333333374815993, -0.16373046925582457, 0.04749508245186007, 0.413496430759551, -0.24220855688326992, -0.23132788739167154, 0.11665257286222186, -0.2587416436872445, -0.1766617252260403, 0.2795397877052892, -0.1647402452508686, 0... |
706.2996 | The forgotten monoid | We study properties of the forgotten monoid which appeared in work of Lascoux
and Schutzenberger and recently resurfaced in the construction of dual
equivalence graphs by Assaf. In particular, we provide an explicit
characterization of the forgotten classes in terms of inversion numbers and
show that there are n^2-3n... | math.CO | we study properties of the forgotten monoid which appeared in work of lascoux and schutzenberger and recently resurfaced in the construction of dual equivalence graphs by assaf in particular we provide an explicit characterization of the forgotten classes in terms of inversion numbers and show that there are n23n4 forg... | [['we', 'study', 'properties', 'of', 'the', 'forgotten', 'monoid', 'which', 'appeared', 'in', 'work', 'of', 'lascoux', 'and', 'schutzenberger', 'and', 'recently', 'resurfaced', 'in', 'the', 'construction', 'of', 'dual', 'equivalence', 'graphs', 'by', 'assaf', 'in', 'particular', 'we', 'provide', 'an', 'explicit', 'char... | [-0.13536341874493976, 0.11998696225316635, -0.07255436066705524, 0.06432834786253071, -0.07571550887705905, -0.058899210844440074, 0.017653281766439925, 0.38842793968453837, -0.3105533123748858, -0.2342504666218262, 0.09187367852918511, -0.2362602955342553, -0.2147351001295146, 0.20571580261326908, -0.1302634894303726... |
706.2997 | Constraining the Two-Higgs-Doublet-Model parameter space | We confront the Two-Higgs-Doublet Model with a variety of experimental
constraints as well as theoretical consistency conditions. The most
constraining data are the \bar B\to X_s\gamma decay rate (at low values of
M_{H^\pm}), and \Delta\rho (at both low and high M_{H^\pm}). We also take into
account the B\bar B oscil... | hep-ph | we confront the twohiggsdoublet model with a variety of experimental constraints as well as theoretical consistency conditions the most constraining data are the bar bto x_sgamma decay rate at low values of m_hpm and deltarho at both low and high m_hpm we also take into account the bbar b oscillation rate and r_b or th... | [['we', 'confront', 'the', 'twohiggsdoublet', 'model', 'with', 'a', 'variety', 'of', 'experimental', 'constraints', 'as', 'well', 'as', 'theoretical', 'consistency', 'conditions', 'the', 'most', 'constraining', 'data', 'are', 'the', 'bar', 'bto', 'x_sgamma', 'decay', 'rate', 'at', 'low', 'values', 'of', 'm_hpm', 'and',... | [-0.09113829592617866, 0.23428727146988146, 0.023314346306200995, 0.15367510532038348, -0.07202653994239967, -0.1937348242636595, 0.1111245052814765, 0.2861938110612108, -0.21529000187558342, -0.28922535900351587, 0.08280214971015792, -0.26665380387566984, 0.05366583858404134, 0.16853211491818745, 0.050537212658048475,... |
706.2998 | Conformal oxide coating of Carbon Nanotubes | The International Roadmap for Ferroelectric Memories requires
three-dimensional integration of high-dielectric materials onto metal
interconnects or bottom electrodes by 2010. We report the first integration of
high-dielectric oxide films onto carbon nanotube electrodes with an aim of
ultra-high integration density o... | cond-mat.mtrl-sci | the international roadmap for ferroelectric memories requires threedimensional integration of highdielectric materials onto metal interconnects or bottom electrodes by 2010 we report the first integration of highdielectric oxide films onto carbon nanotube electrodes with an aim of ultrahigh integration density of feram... | [['the', 'international', 'roadmap', 'for', 'ferroelectric', 'memories', 'requires', 'threedimensional', 'integration', 'of', 'highdielectric', 'materials', 'onto', 'metal', 'interconnects', 'or', 'bottom', 'electrodes', 'by', '2010', 'we', 'report', 'the', 'first', 'integration', 'of', 'highdielectric', 'oxide', 'film... | [-0.148466412324545, 0.1425509293550804, 0.08469702994320975, -0.16909193589222118, -0.003437835463257723, -0.12784639323606742, 0.11942508607712943, 0.48841963855679643, -0.1954719073593963, -0.3138671686742888, 0.06374794377967022, -0.31734225613086725, -0.09452399014776876, 0.19279191555823524, -0.002629049750434797... |
706.2999 | Searches in Photon and Jet States | We present recent results from the Collider Detector at Fermilab (CDF) and D0
experiments using data from proton-antiproton collisions with sqrt(s) = 1.96
TeV at Run II of the Fermilab Tevatron. New physics may appear in events with
high transverse momentum objects, including photons and quark or gluon jets.
The resu... | hep-ex | we present recent results from the collider detector at fermilab cdf and d0 experiments using data from protonantiproton collisions with sqrts 196 tev at run ii of the fermilab tevatron new physics may appear in events with high transverse momentum objects including photons and quark or gluon jets the results described... | [['we', 'present', 'recent', 'results', 'from', 'the', 'collider', 'detector', 'at', 'fermilab', 'cdf', 'and', 'd0', 'experiments', 'using', 'data', 'from', 'protonantiproton', 'collisions', 'with', 'sqrts', '196', 'tev', 'at', 'run', 'ii', 'of', 'the', 'fermilab', 'tevatron', 'new', 'physics', 'may', 'appear', 'in', '... | [-0.0013060707976852639, 0.2988716376931879, -0.09712793290669071, 0.1287498335097579, -0.09178435164031343, -0.17413488969854687, -0.03700765867825544, 0.3166265044415343, -0.12906965086965458, -0.36113813778628473, -0.006157946842047723, -0.4273584753922794, 0.12474521824860595, 0.1433873384570082, 0.1038882989314911... |
706.3 | Discovery of diffuse radio emission at the center of the most
X-ray-luminous cluster RX J1347.5-1145 | We report on new VLA radio observations of the distant cluster RX
J1347.5-1145, which is the most luminous in X-rays. We aim at investigating the
possible presence of diffuse and extended radio emission in this very peculiar
system which shows both a massive cooling flow and merging signatures. New low
resolution (~1... | astro-ph | we report on new vla radio observations of the distant cluster rx j134751145 which is the most luminous in xrays we aim at investigating the possible presence of diffuse and extended radio emission in this very peculiar system which shows both a massive cooling flow and merging signatures new low resolution 18 arcsec v... | [['we', 'report', 'on', 'new', 'vla', 'radio', 'observations', 'of', 'the', 'distant', 'cluster', 'rx', 'j134751145', 'which', 'is', 'the', 'most', 'luminous', 'in', 'xrays', 'we', 'aim', 'at', 'investigating', 'the', 'possible', 'presence', 'of', 'diffuse', 'and', 'extended', 'radio', 'emission', 'in', 'this', 'very',... | [-0.10387170053190656, 0.08720232314177943, -0.04629148630321854, 0.060664989491407244, -0.12152478519516687, -0.08154276384661595, 0.053950149377601016, 0.45027166649699213, -0.20704431619909075, -0.3112540133049091, 0.09632342407945543, -0.283561427049701, -0.01800475623458624, 0.18795111352304553, 0.0273072303261142... |
706.3001 | Mass distribution in the most X-ray-luminous galaxy cluster RX
J1347.5-1145 studied with XMM-Newton | We report on the analysis of XMM-Newton observations of RX J1347.5-1145
(z=0.451), the most X-ray-luminous galaxy cluster. We present a detailed total
and gas mass determination up to large distances (~1.7 Mpc), study the scaling
properties of the cluster, and explore the role of AGN heating in the cluster
cool core.... | astro-ph | we report on the analysis of xmmnewton observations of rx j134751145 z0451 the most xrayluminous galaxy cluster we present a detailed total and gas mass determination up to large distances 17 mpc study the scaling properties of the cluster and explore the role of agn heating in the cluster cool core by means of spatial... | [['we', 'report', 'on', 'the', 'analysis', 'of', 'xmmnewton', 'observations', 'of', 'rx', 'j134751145', 'z0451', 'the', 'most', 'xrayluminous', 'galaxy', 'cluster', 'we', 'present', 'a', 'detailed', 'total', 'and', 'gas', 'mass', 'determination', 'up', 'to', 'large', 'distances', '17', 'mpc', 'study', 'the', 'scaling',... | [-0.08282850883590852, 0.07431656386428845, -0.07316207244730322, 0.09818305511570154, -0.06007001666148426, -0.035165449486937304, 0.09068757413998745, 0.4034173201237406, -0.19419605723305722, -0.3560023672013943, 0.059360233231667996, -0.3140592180965801, -0.004121042790627273, 0.19005136689130658, 0.046690571376400... |
706.3002 | Potential energy curves and transition moments for the excimer states
0u+ (3P1) and 1u (3P2) of Ar2 | Exactly solvable rererence potentials of several smoothly joined Morse-type
components were constructed for the lowest two excimer states of Ar2 molecule.
The parameters of the potentials have been ascertained by fitting to the
experimental data, and they are reliable in a wide range of nuclear
separations. A large n... | physics.chem-ph | exactly solvable rererence potentials of several smoothly joined morsetype components were constructed for the lowest two excimer states of ar2 molecule the parameters of the potentials have been ascertained by fitting to the experimental data and they are reliable in a wide range of nuclear separations a large number ... | [['exactly', 'solvable', 'rererence', 'potentials', 'of', 'several', 'smoothly', 'joined', 'morsetype', 'components', 'were', 'constructed', 'for', 'the', 'lowest', 'two', 'excimer', 'states', 'of', 'ar2', 'molecule', 'the', 'parameters', 'of', 'the', 'potentials', 'have', 'been', 'ascertained', 'by', 'fitting', 'to', ... | [-0.0570546083946106, 0.11770285473005133, -0.042963866530386294, 0.035665915578903765, -0.00974707002595267, -0.14075319812751858, 0.0420649762456024, 0.3747088162215964, -0.19396860067476362, -0.35880641702987603, 0.0019026534552154626, -0.2903542195903075, -0.06225993242350152, 0.15892835718035797, 0.029871359622010... |
706.3003 | Connections between real polynomial solutions of hypergeometric-type
differential equations with Rodrigues formula | Starting from the Rodrigues representation of polynomial solutions of the
general hypergeometric-type differential equation complementary polynomials are
constructed using a natural method. Among the key results is a generating
function in closed form leading to short and transparent derivations of
recursion relation... | math.CA | starting from the rodrigues representation of polynomial solutions of the general hypergeometrictype differential equation complementary polynomials are constructed using a natural method among the key results is a generating function in closed form leading to short and transparent derivations of recursion relations an... | [['starting', 'from', 'the', 'rodrigues', 'representation', 'of', 'polynomial', 'solutions', 'of', 'the', 'general', 'hypergeometrictype', 'differential', 'equation', 'complementary', 'polynomials', 'are', 'constructed', 'using', 'a', 'natural', 'method', 'among', 'the', 'key', 'results', 'is', 'a', 'generating', 'func... | [-0.15593120642006397, 0.0345502581543163, -0.15106942522753444, 0.12067399007274718, -0.18129840361264846, -0.16270232505889404, -0.012851157678394683, 0.25568211576642674, -0.33803641410647994, -0.2350005376760641, 0.05176457868785494, -0.31535870067050886, -0.2056726796953525, 0.2618695544661023, -0.0506275420830206... |
706.3004 | Strong extinction of a far-field laser beam by a single quantum dot | Through the utilization of index-matched GaAs immersion lens techniques we
demonstrate a record extinction (12%) of a far-field focused laser by a single
InAs/GaAs quantum dot. This contrast level enables us to report for the first
time resonant laser transmission spectroscopy on a single InAs/GaAs quantum dot
withou... | cond-mat.other cond-mat.mes-hall quant-ph | through the utilization of indexmatched gaas immersion lens techniques we demonstrate a record extinction 12 of a farfield focused laser by a single inasgaas quantum dot this contrast level enables us to report for the first time resonant laser transmission spectroscopy on a single inasgaas quantum dot without the need... | [['through', 'the', 'utilization', 'of', 'indexmatched', 'gaas', 'immersion', 'lens', 'techniques', 'we', 'demonstrate', 'a', 'record', 'extinction', '12', 'of', 'a', 'farfield', 'focused', 'laser', 'by', 'a', 'single', 'inasgaas', 'quantum', 'dot', 'this', 'contrast', 'level', 'enables', 'us', 'to', 'report', 'for', '... | [-0.1401802100137704, 0.09198212395077227, -0.05122082192381775, -0.05234080869747602, 0.005573756009754207, -0.2290522346135091, 0.13760054659063894, 0.4721190024305273, -0.21426804207644803, -0.30033664377751174, 0.0007189755690180593, -0.27157644653278923, -0.09148650099005964, 0.29291250504967237, -0.03313848316772... |
706.3005 | Two Stellar Components in the Halo of the Milky Way | The halo of the Milky Way provides unique elemental abundance and kinematic
information on the first objects to form in the Universe, which can be used to
tightly constrain models of galaxy formation and evolution. Although the halo
was once considered a single component, evidence for its dichotomy has slowly
emerged... | astro-ph | the halo of the milky way provides unique elemental abundance and kinematic information on the first objects to form in the universe which can be used to tightly constrain models of galaxy formation and evolution although the halo was once considered a single component evidence for its dichotomy has slowly emerged in r... | [['the', 'halo', 'of', 'the', 'milky', 'way', 'provides', 'unique', 'elemental', 'abundance', 'and', 'kinematic', 'information', 'on', 'the', 'first', 'objects', 'to', 'form', 'in', 'the', 'universe', 'which', 'can', 'be', 'used', 'to', 'tightly', 'constrain', 'models', 'of', 'galaxy', 'formation', 'and', 'evolution', ... | [-0.09049719817058485, 0.141469032582078, -0.13990851434742568, 0.09629268989717339, -0.1102954196234999, -0.0075941931391075536, -0.021737182569233286, 0.4065220023314083, -0.19315559479888458, -0.3687851136004564, -0.01994397666025017, -0.24353526902806227, -0.030258352298787823, 0.18538556818310528, -0.0164427975530... |
706.3006 | Recollement of Deformed Preprojective Algebras and the Calogero-Moser
Correspondence | The aim of this paper is to clarify the relation between the following
objects: $ (a) $ rank 1 projective modules (ideals) over the first Weyl algebra
$ A_1(\C)$; $ (b) $ simple modules over deformed preprojective algebras $
\Pi_{\lambda}(Q) $ introduced by Crawley-Boevey and Holland; and $ (c) $ simple
modules over ... | math.RT math.QA | the aim of this paper is to clarify the relation between the following objects a rank 1 projective modules ideals over the first weyl algebra a_1c b simple modules over deformed preprojective algebras pi_lambdaq introduced by crawleyboevey and holland and c simple modules over the rational cherednik algebras h_0cs_n as... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'clarify', 'the', 'relation', 'between', 'the', 'following', 'objects', 'a', 'rank', '1', 'projective', 'modules', 'ideals', 'over', 'the', 'first', 'weyl', 'algebra', 'a_1c', 'b', 'simple', 'modules', 'over', 'deformed', 'preprojective', 'algebras', 'pi_lambdaq', 'int... | [-0.14790917771328663, 0.05007588320718655, -0.07534692123193633, 0.06331535353004283, -0.11619431325446138, -0.16036102377851916, -0.0353464506590006, 0.34508493596292805, -0.3899003195604592, -0.17896732622863387, 0.07866237270134276, -0.21124369665190126, -0.13427763043507707, 0.1909932630016666, -0.1839877709457086... |
706.3007 | Relations among Supersymmetric Lattice Gauge Theories via Orbifolding | We show how to derive Catterall's supersymmetric lattice gauge theories
directly from the general principle of orbifolding followed by a variant of the
usual deconstruction. These theories are forced to be complexified due to a
clash between charge assignments under U(1)-symmetries and lattice assignments
in terms of... | hep-lat hep-th | we show how to derive catteralls supersymmetric lattice gauge theories directly from the general principle of orbifolding followed by a variant of the usual deconstruction these theories are forced to be complexified due to a clash between charge assignments under u1symmetries and lattice assignments in terms of scalar... | [['we', 'show', 'how', 'to', 'derive', 'catteralls', 'supersymmetric', 'lattice', 'gauge', 'theories', 'directly', 'from', 'the', 'general', 'principle', 'of', 'orbifolding', 'followed', 'by', 'a', 'variant', 'of', 'the', 'usual', 'deconstruction', 'these', 'theories', 'are', 'forced', 'to', 'be', 'complexified', 'due'... | [-0.0633351230271495, 0.18989222358924543, -0.08779974105140681, 0.09317783674655053, -0.10339375544124497, -0.15989736539090815, 0.028794566014906965, 0.346811658798311, -0.20661328852069205, -0.2639850395752523, 0.08509125687907307, -0.23311763734389573, -0.20547959994441137, 0.09564894568085527, -0.08999898730932425... |
706.3008 | A Generic Deployment Framework for Grid Computing and Distributed
Applications | Deployment of distributed applications on large systems, and especially on
grid infrastructures, becomes a more and more complex task. Grid users spend a
lot of time to prepare, install and configure middleware and application
binaries on nodes, and eventually start their applications. The problem is that
the deploym... | cs.DC | deployment of distributed applications on large systems and especially on grid infrastructures becomes a more and more complex task grid users spend a lot of time to prepare install and configure middleware and application binaries on nodes and eventually start their applications the problem is that the deployment proc... | [['deployment', 'of', 'distributed', 'applications', 'on', 'large', 'systems', 'and', 'especially', 'on', 'grid', 'infrastructures', 'becomes', 'a', 'more', 'and', 'more', 'complex', 'task', 'grid', 'users', 'spend', 'a', 'lot', 'of', 'time', 'to', 'prepare', 'install', 'and', 'configure', 'middleware', 'and', 'applica... | [-0.14445602929021564, 0.019569550287620776, -0.028170903764622307, 0.03748955069486642, -0.14523683130692946, -0.1618944343511315, 0.08628842648421146, 0.3957937262342151, -0.24581647499721368, -0.34085987213445057, 0.1481769621136716, -0.22426409964535343, -0.13975914925786442, 0.2129095166452609, -0.1146111921567855... |
706.3009 | Application of a design space exploration tool to enhance interleaver
generation | This paper presents a methodology to efficiently explore the design space of
communication adapters. In most digital signal processing (DSP) applications,
the overall performance of the system is significantly affected by
communication architectures, as a consequence the designers need specifically
optimized adapters... | cs.AR cs.IT math.IT | this paper presents a methodology to efficiently explore the design space of communication adapters in most digital signal processing dsp applications the overall performance of the system is significantly affected by communication architectures as a consequence the designers need specifically optimized adapters by exp... | [['this', 'paper', 'presents', 'a', 'methodology', 'to', 'efficiently', 'explore', 'the', 'design', 'space', 'of', 'communication', 'adapters', 'in', 'most', 'digital', 'signal', 'processing', 'dsp', 'applications', 'the', 'overall', 'performance', 'of', 'the', 'system', 'is', 'significantly', 'affected', 'by', 'commun... | [-0.18443352879867667, -0.007877631062578912, -0.07184295510015791, 0.018565918696815117, -0.14359608127935125, -0.21005689622169094, 0.06828273543145597, 0.4098759609023257, -0.2932517982230315, -0.3783949477494591, 0.10516235096258156, -0.19724983281441152, -0.21098541818366992, 0.1949888167233901, -0.123124761287019... |
706.301 | Quasi-invariance properties of a class of subordinators | We study absolute-continuity properties of a class of stochastic processes,
including the gamma and the Dirichlet processes. We prove that the laws of a
general class of non-linear transformations of such processes are locally
equivalent to the law of the original process and we compute explicitly the
associated Rado... | math.PR | we study absolutecontinuity properties of a class of stochastic processes including the gamma and the dirichlet processes we prove that the laws of a general class of nonlinear transformations of such processes are locally equivalent to the law of the original process and we compute explicitly the associated radonnikod... | [['we', 'study', 'absolutecontinuity', 'properties', 'of', 'a', 'class', 'of', 'stochastic', 'processes', 'including', 'the', 'gamma', 'and', 'the', 'dirichlet', 'processes', 'we', 'prove', 'that', 'the', 'laws', 'of', 'a', 'general', 'class', 'of', 'nonlinear', 'transformations', 'of', 'such', 'processes', 'are', 'loc... | [-0.07811648919638517, 0.10190228280354885, -0.07950648758560419, 0.06599099453858903, -0.09887322926542898, -0.060142497127146824, 0.033302263262263244, 0.3586040578134682, -0.3314049336384388, -0.19415358160419957, 0.08993611286353806, -0.26994936303168104, -0.17528589258807292, 0.2068069760242234, -0.064506229492363... |
706.3011 | Axial Nucleon and Nucleon to Delta form fractors and the
Goldberger-Treiman Relations from Lattice QCD | We evaluate the nucleon axial form factor, $G_A(q^2)$, and induced
pseudoscalar form factor, $G_p(q^2)$, as well as the pion-nucleon form factor,
$G_{\pi N N}(q^2)$, in lattice QCD. We also evaluate the corresponding nucleon
to $\Delta$ transition form factors, $C_5^A(q^2)$ and $C_6^A(q^2)$, and the
pion-nucleon-$\De... | hep-lat | we evaluate the nucleon axial form factor g_aq2 and induced pseudoscalar form factor g_pq2 as well as the pionnucleon form factor g_pi n nq2 in lattice qcd we also evaluate the corresponding nucleon to delta transition form factors c_5aq2 and c_6aq2 and the pionnucleondelta form factor g_pi ndeltaq2 the nucleon form fa... | [['we', 'evaluate', 'the', 'nucleon', 'axial', 'form', 'factor', 'g_aq2', 'and', 'induced', 'pseudoscalar', 'form', 'factor', 'g_pq2', 'as', 'well', 'as', 'the', 'pionnucleon', 'form', 'factor', 'g_pi', 'n', 'nq2', 'in', 'lattice', 'qcd', 'we', 'also', 'evaluate', 'the', 'corresponding', 'nucleon', 'to', 'delta', 'tran... | [-0.11924034042312996, 0.26237106655617026, -0.028190414709388278, 0.11200975646497682, -0.029596700415459053, -0.06327415039777406, 0.0970688109540788, 0.3681576655304525, -0.13703868624579627, -0.26761777815627286, -0.012102815824619029, -0.33061901706969365, -0.06671919558866649, 0.08938824964570813, 0.1137441007653... |
706.3012 | Unbound exotic nuclei studied by projectile fragmentation | We call "projectile fragmentation" of neutron halo nuclei the elastic breakup
(diffraction) reaction, when the observable studied is the neutron-core
relative energy spectrum. This observable has been measured in relation to the
Coulomb breakup on heavy target and recently also on light targets. Such data
enlighten t... | nucl-th | we call projectile fragmentation of neutron halo nuclei the elastic breakup diffraction reaction when the observable studied is the neutroncore relative energy spectrum this observable has been measured in relation to the coulomb breakup on heavy target and recently also on light targets such data enlighten the effect ... | [['we', 'call', 'projectile', 'fragmentation', 'of', 'neutron', 'halo', 'nuclei', 'the', 'elastic', 'breakup', 'diffraction', 'reaction', 'when', 'the', 'observable', 'studied', 'is', 'the', 'neutroncore', 'relative', 'energy', 'spectrum', 'this', 'observable', 'has', 'been', 'measured', 'in', 'relation', 'to', 'the', ... | [-0.08426085628812487, 0.2221507644312235, -0.14533807046318908, 0.11698762120049559, -0.00754177261228163, -0.08565175752319283, 0.038886169048292965, 0.3588183542442082, -0.24798078917144756, -0.29173586525060424, 0.024015865410940168, -0.2971636059333631, -0.03978594007841007, 0.14394746501298256, 0.0606963202291771... |
706.3013 | Oscillation regimes of a solid-state ring laser with active beat note
stabilization : from a chaotic device to a ring laser gyroscope | We report experimental and theoretical study of a rotating diode-pumped
Nd-YAG ring laser with active beat note stabilization. Our experimental setup
is described in the usual Maxwell-Bloch formalism. We analytically derive a
stability condition and some frequency response characteristics for the
solid-state ring las... | physics.optics | we report experimental and theoretical study of a rotating diodepumped ndyag ring laser with active beat note stabilization our experimental setup is described in the usual maxwellbloch formalism we analytically derive a stability condition and some frequency response characteristics for the solidstate ring laser gyros... | [['we', 'report', 'experimental', 'and', 'theoretical', 'study', 'of', 'a', 'rotating', 'diodepumped', 'ndyag', 'ring', 'laser', 'with', 'active', 'beat', 'note', 'stabilization', 'our', 'experimental', 'setup', 'is', 'described', 'in', 'the', 'usual', 'maxwellbloch', 'formalism', 'we', 'analytically', 'derive', 'a', '... | [-0.1607678466484197, 0.11154256787820727, -0.10598830693239762, 0.021508680953844336, -0.03384790346526718, -0.16626672126537512, 0.02649230703476755, 0.377941251670834, -0.239181484932788, -0.2710724389180541, 0.08106867694642303, -0.23715437497955186, -0.1564622966203192, 0.2956598300644589, -0.042957402973566663, 0... |
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