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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709.3335 | The quest for three-color entanglement: experimental investigation of
new multipartite quantum correlations | We experimentally investigate quadrature correlations between pump, signal,
and idler fields in an above-threshold optical parametric oscillator. We
observe new quantum correlations among the pump and signal or idler beams, as
well as among the pump and a combined quadrature of signal and idler beams. A
further inves... | quant-ph physics.optics | we experimentally investigate quadrature correlations between pump signal and idler fields in an abovethreshold optical parametric oscillator we observe new quantum correlations among the pump and signal or idler beams as well as among the pump and a combined quadrature of signal and idler beams a further investigation... | [['we', 'experimentally', 'investigate', 'quadrature', 'correlations', 'between', 'pump', 'signal', 'and', 'idler', 'fields', 'in', 'an', 'abovethreshold', 'optical', 'parametric', 'oscillator', 'we', 'observe', 'new', 'quantum', 'correlations', 'among', 'the', 'pump', 'and', 'signal', 'or', 'idler', 'beams', 'as', 'we... | [-0.15208334506051727, 0.18140399640202326, -0.07141109315835568, 0.051059978720956446, 0.005858879424182765, -0.16362658683883857, 0.08322981432506657, 0.43306772980883895, -0.24136275457532472, -0.28786950298102504, 0.005665346383992358, -0.27152131881609737, -0.14260076120192836, 0.2246607058732041, -0.0287894993762... |
709.3336 | The Variable Warm Absorber in Circinus X-1 | We observed Circinus X-1 twice during a newly reached low-flux phase near
zero orbital phase using the High-Energy Transmission Grating Spectrometer
(HETGS) onboard Chandra. In both observations the source did not show the P
Cygni lines we observed during the high-flux phases of the source in 2000 and
2001. During pr... | astro-ph | we observed circinus x1 twice during a newly reached lowflux phase near zero orbital phase using the highenergy transmission grating spectrometer hetgs onboard chandra in both observations the source did not show the p cygni lines we observed during the highflux phases of the source in 2000 and 2001 during prezero phas... | [['we', 'observed', 'circinus', 'x1', 'twice', 'during', 'a', 'newly', 'reached', 'lowflux', 'phase', 'near', 'zero', 'orbital', 'phase', 'using', 'the', 'highenergy', 'transmission', 'grating', 'spectrometer', 'hetgs', 'onboard', 'chandra', 'in', 'both', 'observations', 'the', 'source', 'did', 'not', 'show', 'the', 'p... | [-0.05117291248783748, 0.13210655731065762, -0.021339700803481288, 0.08747215683812459, -0.061317991474872366, -0.16087590428985288, 0.050447962492070786, 0.49516851296953734, -0.18976379956403122, -0.3448651408601064, 0.06962532386494816, -0.32849378643374216, -0.005374059946558698, 0.17860982090150784, -0.03825956578... |
709.3337 | Polynomial Fusion Rings of Logarithmic Minimal Models | We identify quotient polynomial rings isomorphic to the recently found
fundamental fusion algebras of logarithmic minimal models.
| hep-th math-ph math.MP | we identify quotient polynomial rings isomorphic to the recently found fundamental fusion algebras of logarithmic minimal models | [['we', 'identify', 'quotient', 'polynomial', 'rings', 'isomorphic', 'to', 'the', 'recently', 'found', 'fundamental', 'fusion', 'algebras', 'of', 'logarithmic', 'minimal', 'models']] | [-0.14656303603859508, -0.017227352268117314, -0.06630046950543628, 0.13098152057500556, -0.09884619203341358, -0.22798391990363598, -0.11575781498344012, 0.31388463049798326, -0.501188084264012, -0.16102938373189637, 0.054379964986925614, -0.2188800836858504, -0.17680621344377012, 0.12614788816255681, -0.1916922362630... |
709.3338 | The Classification of Higher Order Modular Forms and their Cohomology | We construct bases for the spaces of higher order modular forms of all orders
and weights. We also provide a cohomological interpretation of these forms.
| math.NT | we construct bases for the spaces of higher order modular forms of all orders and weights we also provide a cohomological interpretation of these forms | [['we', 'construct', 'bases', 'for', 'the', 'spaces', 'of', 'higher', 'order', 'modular', 'forms', 'of', 'all', 'orders', 'and', 'weights', 'we', 'also', 'provide', 'a', 'cohomological', 'interpretation', 'of', 'these', 'forms']] | [-0.18629178181290626, 0.07038515707477927, -0.10445279188454151, 0.11317009594291448, -0.10034691693261266, -0.017574180234223604, 0.0053505093231797215, 0.3507057291269302, -0.274338546693325, -0.2428248219192028, 0.1142131520807743, -0.22095008585602044, -0.21039947643876075, 0.22955812618136406, -0.0119570961222052... |
709.3339 | On posterior distribution of Bayesian wavelet thresholding | We investigate the posterior rate of convergence for wavelet shrinkage using
a Bayesian approach in general Besov spaces. Instead of studying the Bayesian
estimator related to a particular loss function, we focus on the posterior
distribution itself from a nonparametric Bayesian asymptotics point of view and
study it... | math.ST stat.TH | we investigate the posterior rate of convergence for wavelet shrinkage using a bayesian approach in general besov spaces instead of studying the bayesian estimator related to a particular loss function we focus on the posterior distribution itself from a nonparametric bayesian asymptotics point of view and study its ra... | [['we', 'investigate', 'the', 'posterior', 'rate', 'of', 'convergence', 'for', 'wavelet', 'shrinkage', 'using', 'a', 'bayesian', 'approach', 'in', 'general', 'besov', 'spaces', 'instead', 'of', 'studying', 'the', 'bayesian', 'estimator', 'related', 'to', 'a', 'particular', 'loss', 'function', 'we', 'focus', 'on', 'the'... | [-0.031173170092241728, -0.053799975601791894, -0.16112508409766152, 0.15210711136323346, -0.04055619762306485, -0.06091477832866504, 0.10933049795601298, 0.38519107333987074, -0.3132309489061727, -0.20966200705836802, 0.16280360132633873, -0.21295428287018747, -0.14796161825549514, 0.18075895683346865, -0.107586544972... |
709.334 | Flow Field Evolution of a Decaying Sunspot | We study the evolution of the flows and horizontal proper motions in and
around a decaying follower sunspot based on time sequences of two-dimensional
spectroscopic observations in the visible and white light imaging data obtained
over six days from June~7 to~12, 2005. During this time period the sunspot
decayed grad... | astro-ph | we study the evolution of the flows and horizontal proper motions in and around a decaying follower sunspot based on time sequences of twodimensional spectroscopic observations in the visible and white light imaging data obtained over six days from june7 to12 2005 during this time period the sunspot decayed gradually t... | [['we', 'study', 'the', 'evolution', 'of', 'the', 'flows', 'and', 'horizontal', 'proper', 'motions', 'in', 'and', 'around', 'a', 'decaying', 'follower', 'sunspot', 'based', 'on', 'time', 'sequences', 'of', 'twodimensional', 'spectroscopic', 'observations', 'in', 'the', 'visible', 'and', 'white', 'light', 'imaging', 'da... | [-0.10888341996062811, 0.16845730832918202, -0.0388064089632558, 0.0429966196858141, -0.06553506140086356, -0.07590783210705078, 0.020142817644136432, 0.4545872616406265, -0.23669948782693892, -0.3367237175803117, 0.10135140023866443, -0.27153237694757504, -0.08142838022714505, 0.18379915460445392, -0.05966264394084654... |
709.3341 | The QCD potential | After reviewing the definition of the heavy quark-antiquark potential in
pNRQCD, we discuss recent advances in the calculation.
| hep-ph | after reviewing the definition of the heavy quarkantiquark potential in pnrqcd we discuss recent advances in the calculation | [['after', 'reviewing', 'the', 'definition', 'of', 'the', 'heavy', 'quarkantiquark', 'potential', 'in', 'pnrqcd', 'we', 'discuss', 'recent', 'advances', 'in', 'the', 'calculation']] | [-0.07704067685537869, 0.1733526050940984, -0.07570926213843955, 0.0355299238063809, 0.020040254419048626, -0.0329421724503239, 0.05976189380615122, 0.335611822290553, -0.15411378849401242, -0.227631331110994, -0.013518124598906271, -0.32397980196401477, -0.12448010469476382, 0.10858354200091627, -0.05973887557370795, ... |
709.3342 | Microscopic formulation of the S-matrix in AdS/CFT | We develop the derivation we proposed in hep-th/0703177 of the dressing phase
of the S-matrix in the AdS/CFT correspondence in the framework of the
underlying bare integrable model. We elaborate the configuration of the Bethe
roots describing the physical vacuum, which consists of a long Bethe string
stretched along ... | hep-th | we develop the derivation we proposed in hepth0703177 of the dressing phase of the smatrix in the adscft correspondence in the framework of the underlying bare integrable model we elaborate the configuration of the bethe roots describing the physical vacuum which consists of a long bethe string stretched along the imag... | [['we', 'develop', 'the', 'derivation', 'we', 'proposed', 'in', 'hepth0703177', 'of', 'the', 'dressing', 'phase', 'of', 'the', 'smatrix', 'in', 'the', 'adscft', 'correspondence', 'in', 'the', 'framework', 'of', 'the', 'underlying', 'bare', 'integrable', 'model', 'we', 'elaborate', 'the', 'configuration', 'of', 'the', '... | [-0.1879219438466761, 0.12309322504119741, -0.10956985636924704, 0.05735082750519117, -0.05750453388835821, -0.045949307477308646, 0.02302299273950565, 0.33688319424788155, -0.2522556546506368, -0.19429838008557757, 0.051093261192242306, -0.24887051085631054, -0.13217212425831046, 0.11228225281617293, 0.046705187220747... |
709.3343 | On the Schwartz space isomorphism theorem for rank one symmetric space | In this paper we give a simpler proof of the $L^p$-Schwartz space isomorphism
$(0< p\leq 2)$ under the Fourier transform for the class of functions of left
$\delta$-type on a Riemannian symmetric space of rank one. Our treatment rests
on Anker's \cite{A} proof of the corresponding result in the case of left
$K$-invar... | math.RT | in this paper we give a simpler proof of the lpschwartz space isomorphism 0 pleq 2 under the fourier transform for the class of functions of left deltatype on a riemannian symmetric space of rank one our treatment rests on ankers citea proof of the corresponding result in the case of left kinvariant functions on x thus... | [['in', 'this', 'paper', 'we', 'give', 'a', 'simpler', 'proof', 'of', 'the', 'lpschwartz', 'space', 'isomorphism', '0', 'pleq', '2', 'under', 'the', 'fourier', 'transform', 'for', 'the', 'class', 'of', 'functions', 'of', 'left', 'deltatype', 'on', 'a', 'riemannian', 'symmetric', 'space', 'of', 'rank', 'one', 'our', 'tr... | [-0.12748043572724754, 0.03912016356523747, -0.11385311569962929, 0.05655391213185251, -0.08745224580669136, -0.11954611675716492, 0.034138520458476866, 0.3031720161549191, -0.24311797076196812, -0.17561975021415682, 0.13469871979401404, -0.2194438626739516, -0.13937863084807325, 0.2473720456334526, -0.1061767306067605... |
709.3344 | On the cohomology of orbit space of free \pmb{${\ZZ}_{p}$}-actions on
lens spaces | Let $G = \ZZ_p$, $p$ an odd prime, act freely on a finite-dimensional
CW-complex $X$ with mod $p$ cohomology isomorphic to that of a lens space
$L^{2m-1} (p;q_1,...,q_m)$. In this paper, we determine the mod $p$ cohomology
ring of the orbit space $X/G$, when $p^2\nmid m$.
| math.AT | let g zz_p p an odd prime act freely on a finitedimensional cwcomplex x with mod p cohomology isomorphic to that of a lens space l2m1 pq_1q_m in this paper we determine the mod p cohomology ring of the orbit space xg when p2nmid m | [['let', 'g', 'zz_p', 'p', 'an', 'odd', 'prime', 'act', 'freely', 'on', 'a', 'finitedimensional', 'cwcomplex', 'x', 'with', 'mod', 'p', 'cohomology', 'isomorphic', 'to', 'that', 'of', 'a', 'lens', 'space', 'l2m1', 'pq_1q_m', 'in', 'this', 'paper', 'we', 'determine', 'the', 'mod', 'p', 'cohomology', 'ring', 'of', 'the',... | [-0.33206065536238427, 0.09189246260584061, -0.13327068014633517, -0.04581179133708437, -0.09736663601252922, -0.21669666116060907, -0.02088790250194887, 0.3200481274749997, -0.3742397296740565, -0.21284827732935893, -0.019689425915414685, -0.2174651761820843, -0.0977559561223918, 0.16256449158779931, -0.19671305307988... |
709.3345 | Approximation of functions of two variables by certain linear positive
operators | We introduce certain linear positive operators and study some approximation
properties of these operators in the space of functions, continuous on a
compact set, of two variables. We also find the order of this approximation by
using modulus of continuity. Moreover we define an $r$th order generalization
of these ope... | math.CA | we introduce certain linear positive operators and study some approximation properties of these operators in the space of functions continuous on a compact set of two variables we also find the order of this approximation by using modulus of continuity moreover we define an rth order generalization of these operators a... | [['we', 'introduce', 'certain', 'linear', 'positive', 'operators', 'and', 'study', 'some', 'approximation', 'properties', 'of', 'these', 'operators', 'in', 'the', 'space', 'of', 'functions', 'continuous', 'on', 'a', 'compact', 'set', 'of', 'two', 'variables', 'we', 'also', 'find', 'the', 'order', 'of', 'this', 'approxi... | [-0.14369172221699425, 0.07274423236028037, -0.09032776663188151, 0.06703529477411838, -0.029257137512484956, 0.0005272274003039266, 0.07510500752399567, 0.355682709909499, -0.3309675593708837, -0.2141346324365153, 0.12626924045481394, -0.2729623257290832, -0.1862863849761874, 0.1655391011560379, -0.022992676210611365,... |
709.3346 | On an inequality concerning the polar derivative of a polynomial | In this paper, we present a correct proof of an $L_p$-inequality concerning
the polar derivative of a polynomial with restricted zeros. We also extend
Zygmund's inequality to the polar derivative of a polynomial.
| math.CV | in this paper we present a correct proof of an l_pinequality concerning the polar derivative of a polynomial with restricted zeros we also extend zygmunds inequality to the polar derivative of a polynomial | [['in', 'this', 'paper', 'we', 'present', 'a', 'correct', 'proof', 'of', 'an', 'l_pinequality', 'concerning', 'the', 'polar', 'derivative', 'of', 'a', 'polynomial', 'with', 'restricted', 'zeros', 'we', 'also', 'extend', 'zygmunds', 'inequality', 'to', 'the', 'polar', 'derivative', 'of', 'a', 'polynomial']] | [-0.19194987925584428, 0.00037638446201526676, -0.11314181531633949, 0.04382895498929429, -0.1419127708650194, -0.07037684008537326, 0.055689724100375315, 0.2760953465185594, -0.29063658381346613, -0.18027758135576732, 0.12016926482829149, -0.19113436015322804, -0.20711044443305582, 0.17080600163899362, -0.126056352717... |
709.3347 | Weighted composition operators from Bergman-type spaces into Bloch
spaces | Let $\phi$ be an analytic self-map and $u$ be a fixed analytic function on
the open unit disk $D$ in the complex plane $\CC.$ The weighted composition
operator is defined\break by \begin{equation*} uC_\phi f =u \cdot (f\circ
\phi), f \in H(D). \end{equation*} Weighted composition operators from
Bergman-type spaces in... | math.CV | let phi be an analytic selfmap and u be a fixed analytic function on the open unit disk d in the complex plane cc the weighted composition operator is definedbreak by beginequation uc_phi f u cdot fcirc phi f in hd endequation weighted composition operators from bergmantype spaces into bloch spaces and little bloch spa... | [['let', 'phi', 'be', 'an', 'analytic', 'selfmap', 'and', 'u', 'be', 'a', 'fixed', 'analytic', 'function', 'on', 'the', 'open', 'unit', 'disk', 'd', 'in', 'the', 'complex', 'plane', 'cc', 'the', 'weighted', 'composition', 'operator', 'is', 'definedbreak', 'by', 'beginequation', 'uc_phi', 'f', 'u', 'cdot', 'fcirc', 'phi... | [-0.21017359416296202, 0.1184958322770572, -0.04864068622405212, 0.05868068665066468, -0.0639488164793759, -0.10217361985188392, 0.00973204128252017, 0.3920379884481903, -0.39521447261647574, -0.1433502928287323, 0.05507232489374777, -0.3282467918322673, -0.10517020683203425, 0.2037203156736694, -0.06563286957818837, 0... |
709.3348 | A generalization of d'Alembert formula | In this paper we find a closed form of the solution for the factored
inhomogeneous linear equation \begin{equation*}
\prod_{j=1}^{n}(\frac{\hbox{d}}{\hbox{d}t}-A_{j}) u(t) =f(t). \end{equation*}
Under the hypothesis $A_{1},A_{2}, ..., A_{n}$ are infinitesimal generators of
mutually commuting strongly continuous semig... | math.AP | in this paper we find a closed form of the solution for the factored inhomogeneous linear equation beginequation prod_j1nfrachboxdhboxdta_j ut ft endequation under the hypothesis a_1a_2 a_n are infinitesimal generators of mutually commuting strongly continuous semigroups of bounded linear operators on a banach space x ... | [['in', 'this', 'paper', 'we', 'find', 'a', 'closed', 'form', 'of', 'the', 'solution', 'for', 'the', 'factored', 'inhomogeneous', 'linear', 'equation', 'beginequation', 'prod_j1nfrachboxdhboxdta_j', 'ut', 'ft', 'endequation', 'under', 'the', 'hypothesis', 'a_1a_2', 'a_n', 'are', 'infinitesimal', 'generators', 'of', 'mu... | [-0.19611378798863904, 0.10366675837020226, -0.043868214282316756, 0.04115588717018802, -0.1022218759479823, -0.14430983897353358, -0.02598099715781727, 0.3677056597764878, -0.3384485989809036, -0.1277606504804948, 0.10098727887516896, -0.3335130695075564, -0.13130102938671104, 0.1691666158097659, -0.06530052787103854,... |
709.3349 | A sharp upper bound for the first eigenvalue of the Laplacian of compact
hypersurfaces in rank-1 symmetric spaces | Let $M$ be a closed hypersurface in a simply connected rank-1 symmetric space
$\olm$. In this paper, we give an upper bound for the first eigenvalue of the
Laplacian of $M$ in terms of the Ricci curvature of $\olm$ and the square of
the length of the second fundamental form of the geodesic spheres with center
at the ... | math.DG math.MG | let m be a closed hypersurface in a simply connected rank1 symmetric space olm in this paper we give an upper bound for the first eigenvalue of the laplacian of m in terms of the ricci curvature of olm and the square of the length of the second fundamental form of the geodesic spheres with center at the centerofmass of... | [['let', 'm', 'be', 'a', 'closed', 'hypersurface', 'in', 'a', 'simply', 'connected', 'rank1', 'symmetric', 'space', 'olm', 'in', 'this', 'paper', 'we', 'give', 'an', 'upper', 'bound', 'for', 'the', 'first', 'eigenvalue', 'of', 'the', 'laplacian', 'of', 'm', 'in', 'terms', 'of', 'the', 'ricci', 'curvature', 'of', 'olm',... | [-0.20692869230005584, 0.11325646919550443, -0.0548748320854101, -0.03915231346084019, -0.05298648528815782, -0.07985700118798213, -0.030036468972971082, 0.27590512505686676, -0.2434154527383994, -0.25368105110208516, 0.0952555529456433, -0.263108376001359, -0.11911907577581826, 0.147971347298809, -0.0621223441767888, ... |
709.335 | Equivariant embeddings of Hermitian symmetric spaces | We prove that equivariant, holomorphic embeddings of Hermitian symmetric
spaces are totally geodesic (when the image is not of exceptional type).
| math.MG | we prove that equivariant holomorphic embeddings of hermitian symmetric spaces are totally geodesic when the image is not of exceptional type | [['we', 'prove', 'that', 'equivariant', 'holomorphic', 'embeddings', 'of', 'hermitian', 'symmetric', 'spaces', 'are', 'totally', 'geodesic', 'when', 'the', 'image', 'is', 'not', 'of', 'exceptional', 'type']] | [-0.1895318819830815, 0.07286569799873091, -0.06449056940064543, 0.15588164083947914, -0.1770313633162351, -0.17374473921067657, -0.11482044335986887, 0.4596141179402669, -0.323866104973214, -0.07443993494269394, 0.145028095936314, -0.28403001048025633, -0.22854042585406983, 0.17950320128528846, -0.20903406771165983, -... |
709.3351 | A succession of relaxor ferroelectric transitions coexisting with
ferroelectric states in Ba_0.55Sr_0.45TiO_3 | We present here the results of frequency dependent dielectric, polarization
and powder X-ray powder diffraction studies in the 300 to 100K temperature
range for Ba_0.55Sr_0.45TiO_3. The dielectric results indicate a succession of
three relaxor ferroelectric transitions accompanying the cubic to tetragonal to
orthorho... | cond-mat.mtrl-sci | we present here the results of frequency dependent dielectric polarization and powder xray powder diffraction studies in the 300 to 100k temperature range for ba_055sr_045tio_3 the dielectric results indicate a succession of three relaxor ferroelectric transitions accompanying the cubic to tetragonal to orthorhombic to... | [['we', 'present', 'here', 'the', 'results', 'of', 'frequency', 'dependent', 'dielectric', 'polarization', 'and', 'powder', 'xray', 'powder', 'diffraction', 'studies', 'in', 'the', '300', 'to', '100k', 'temperature', 'range', 'for', 'ba_055sr_045tio_3', 'the', 'dielectric', 'results', 'indicate', 'a', 'succession', 'of... | [-0.12659142675599264, 0.23445965668877528, -0.04583093983631942, -0.08978789822468834, -0.1405486029032017, -0.04212191967564004, 0.1846630302700965, 0.5302125997841358, -0.2229823237285018, -0.23936246221344318, 0.03331568096050872, -0.3622899811729909, -0.13706802920768818, 0.18895207075101714, 0.09330540902221636, ... |
709.3352 | Relation between fundamental estimation limit and stability in linear
quantum systems with imperfect measurement | From the noncommutative nature of quantum mechanics, estimation of canonical
observables $\hat{q}$ and $\hat{p}$ is essentially restricted in its
performance by the Heisenberg uncertainty relation, $\mean{\Delta
\hat{q}^2}\mean{\Delta \hat{p}^2}\geq \hbar^2/4$. This fundamental lower-bound
may become bigger when taki... | quant-ph | from the noncommutative nature of quantum mechanics estimation of canonical observables hatq and hatp is essentially restricted in its performance by the heisenberg uncertainty relation meandelta hatq2meandelta hatp2geq hbar24 this fundamental lowerbound may become bigger when taking the structure and quality of a spec... | [['from', 'the', 'noncommutative', 'nature', 'of', 'quantum', 'mechanics', 'estimation', 'of', 'canonical', 'observables', 'hatq', 'and', 'hatp', 'is', 'essentially', 'restricted', 'in', 'its', 'performance', 'by', 'the', 'heisenberg', 'uncertainty', 'relation', 'meandelta', 'hatq2meandelta', 'hatp2geq', 'hbar24', 'thi... | [-0.12130515684839338, 0.19592447993151532, -0.10373668514754779, 0.061578879577912936, -0.03172706779635822, -0.17721299523933945, 0.040200321410035635, 0.3371769120567478, -0.2866827206259283, -0.2399878909539742, 0.10203647298233894, -0.2536941603757441, -0.08688596369271788, 0.21731655978389122, -0.0610432671383023... |
709.3353 | A trivial observation on time reversal in random matrix theory | It is commonly thought that a state-dependent quantity, after being averaged
over a classical ensemble of random Hamiltonians, will always become
independent of the state. We point out that this is in general incorrect: if
the ensemble of Hamiltonians is time reversal invariant, and the quantity
involves the state in... | quant-ph | it is commonly thought that a statedependent quantity after being averaged over a classical ensemble of random hamiltonians will always become independent of the state we point out that this is in general incorrect if the ensemble of hamiltonians is time reversal invariant and the quantity involves the state in higher ... | [['it', 'is', 'commonly', 'thought', 'that', 'a', 'statedependent', 'quantity', 'after', 'being', 'averaged', 'over', 'a', 'classical', 'ensemble', 'of', 'random', 'hamiltonians', 'will', 'always', 'become', 'independent', 'of', 'the', 'state', 'we', 'point', 'out', 'that', 'this', 'is', 'in', 'general', 'incorrect', '... | [-0.1530842180083315, 0.18773137966552414, -0.11355544213789055, 0.08574948395765106, -0.004816285098190363, -0.10532197909968266, 0.035308530206332005, 0.37245787935982266, -0.2647350003426693, -0.22044796425938964, 0.1159443409428988, -0.25962934650884695, -0.13695493789883442, 0.21026063316602664, -0.066059229110019... |
709.3354 | Some notes on the equivalence of first-order rigidity in various
geometries | These pages serve two purposes. First, they are notes to accompany the talk
"Hyperbolic and projective geometry in constraint programming for CAD" by
Walter Whiteley at the "Janos Bolyai Conference on Hyperbolic Geometry", 8--12
July 2002, in Budapest, Hungary. Second, they sketch results that will be
included in a f... | math.MG math.CO | these pages serve two purposes first they are notes to accompany the talk hyperbolic and projective geometry in constraint programming for cad by walter whiteley at the janos bolyai conference on hyperbolic geometry 812 july 2002 in budapest hungary second they sketch results that will be included in a forthcoming pape... | [['these', 'pages', 'serve', 'two', 'purposes', 'first', 'they', 'are', 'notes', 'to', 'accompany', 'the', 'talk', 'hyperbolic', 'and', 'projective', 'geometry', 'in', 'constraint', 'programming', 'for', 'cad', 'by', 'walter', 'whiteley', 'at', 'the', 'janos', 'bolyai', 'conference', 'on', 'hyperbolic', 'geometry', '81... | [-0.09946191495246424, 0.11496616633281073, -0.0985892746616535, 0.07558702423394069, -0.11912522677389183, -0.140033456729725, -0.037407334491239896, 0.3324649157501491, -0.19938771822252216, -0.31306116744799883, 0.17257801530293512, -0.30417488698790573, -0.19256482380965, 0.21752751925580052, -0.16306812877883203, ... |
709.3355 | On the Gauss Map with Vanishing Biharmonic stress-energy tensor | We study the biharmonic stress-energy tensor $S_2$ of Gauss map. Adding few
assumptions, the Gauss map with vanishing $S_2$ would be harmonic.
| math.DG | we study the biharmonic stressenergy tensor s_2 of gauss map adding few assumptions the gauss map with vanishing s_2 would be harmonic | [['we', 'study', 'the', 'biharmonic', 'stressenergy', 'tensor', 's_2', 'of', 'gauss', 'map', 'adding', 'few', 'assumptions', 'the', 'gauss', 'map', 'with', 'vanishing', 's_2', 'would', 'be', 'harmonic']] | [-0.24225047658282248, 0.13518805027177389, 0.007879435084760189, 0.03373184783214873, -0.1241684067486362, -0.15490249078720808, -0.12430670637298714, 0.3864994225176898, -0.31143802738833154, -0.19277812862260776, 0.10984919886951419, -0.30849359641698276, -0.10812989618121223, 0.13479626991532065, -0.039370870979672... |
709.3356 | Discovery of Par 1802 as a Low-Mass, Pre-Main-Sequence Eclipsing Binary
in the Orion Star-Forming Region | We report the discovery of a pre-main-sequence, low-mass, double-lined,
spectroscopic, eclipsing binary in the Orion star-forming region. We present
our observations including radial velocities derived from optical
high-resolution spectroscopy, and present an orbit solution that permits the
determination of precise e... | astro-ph | we report the discovery of a premainsequence lowmass doublelined spectroscopic eclipsing binary in the orion starforming region we present our observations including radial velocities derived from optical highresolution spectroscopy and present an orbit solution that permits the determination of precise empirical masse... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'premainsequence', 'lowmass', 'doublelined', 'spectroscopic', 'eclipsing', 'binary', 'in', 'the', 'orion', 'starforming', 'region', 'we', 'present', 'our', 'observations', 'including', 'radial', 'velocities', 'derived', 'from', 'optical', 'highresolution', 'spectroscopy'... | [-0.12565116418235694, 0.09859827834762408, -0.07479045426300326, 0.026446954640929915, -0.08653750973414408, -0.07825054624272103, 0.08723334022658871, 0.4159012672472869, -0.13986415909726593, -0.3395361544329994, 0.05427437038345891, -0.2826941952460896, -0.027351524534370036, 0.2223371953074358, -0.0486465448159755... |
709.3357 | Spectrum of the non-commutative spherical well | We give precise meaning to piecewise constant potentials in non-commutative
quantum mechanics. In particular we discuss the infinite and finite
non-commutative spherical well in two dimensions. Using this, bound-states and
scattering can be discussed unambiguously. Here we focus on the infinite well
and solve for the... | hep-th | we give precise meaning to piecewise constant potentials in noncommutative quantum mechanics in particular we discuss the infinite and finite noncommutative spherical well in two dimensions using this boundstates and scattering can be discussed unambiguously here we focus on the infinite well and solve for the eigenval... | [['we', 'give', 'precise', 'meaning', 'to', 'piecewise', 'constant', 'potentials', 'in', 'noncommutative', 'quantum', 'mechanics', 'in', 'particular', 'we', 'discuss', 'the', 'infinite', 'and', 'finite', 'noncommutative', 'spherical', 'well', 'in', 'two', 'dimensions', 'using', 'this', 'boundstates', 'and', 'scattering... | [-0.1285480199446685, 0.20191019861742335, -0.06891042019543779, 0.12382998682022485, -0.06116209742288257, -0.13291100304313871, -0.01096657123470809, 0.3908626247240707, -0.2887499922789027, -0.22547413959969267, 0.11081314954343577, -0.2468758400009815, -0.14714878214371585, 0.1280982023711468, -0.054919769122471034... |
709.3358 | Polarization-independent CP-odd Observable in e^+e^- Chargino Production
at One Loop | We discuss CP violation in the process e^+e^- \to
\tilde\chi^+_i\tilde\chi^-_j with unpolarized beams. When the scalars are
heavy, the box-diagram results constitute a major part of the full result.
However, there are situations when the vertex and self-energy corrections
dominate over the box diagrams. We also comme... | hep-ph | we discuss cp violation in the process ee to tildechi_itildechi_j with unpolarized beams when the scalars are heavy the boxdiagram results constitute a major part of the full result however there are situations when the vertex and selfenergy corrections dominate over the box diagrams we also comment on cp violation in ... | [['we', 'discuss', 'cp', 'violation', 'in', 'the', 'process', 'ee', 'to', 'tildechi_itildechi_j', 'with', 'unpolarized', 'beams', 'when', 'the', 'scalars', 'are', 'heavy', 'the', 'boxdiagram', 'results', 'constitute', 'a', 'major', 'part', 'of', 'the', 'full', 'result', 'however', 'there', 'are', 'situations', 'when', ... | [-0.10715391241352666, 0.2008338700725951, -0.018496280832385473, 0.13459704148028157, -0.040406838702884584, -0.13566097132014956, 0.06909519259563901, 0.3182958324524489, -0.2025255768305876, -0.2163977835835381, 0.04384446978907693, -0.35801577229391446, -0.0339733844792301, 0.1682813700627197, 0.03692894650792534, ... |
709.3359 | Transition states in protein folding kinetics: Modeling Phi-values of
small beta-sheet proteins | Small single-domain proteins often exhibit only a single free-energy barrier,
or transition state, between the denatured and the native state. The folding
kinetics of these proteins is usually explored via mutational analysis. A
central question is which structural information on the transition state can be
derived f... | q-bio.BM | small singledomain proteins often exhibit only a single freeenergy barrier or transition state between the denatured and the native state the folding kinetics of these proteins is usually explored via mutational analysis a central question is which structural information on the transition state can be derived from the ... | [['small', 'singledomain', 'proteins', 'often', 'exhibit', 'only', 'a', 'single', 'freeenergy', 'barrier', 'or', 'transition', 'state', 'between', 'the', 'denatured', 'and', 'the', 'native', 'state', 'the', 'folding', 'kinetics', 'of', 'these', 'proteins', 'is', 'usually', 'explored', 'via', 'mutational', 'analysis', '... | [-0.09156673882440057, 0.154208660616139, -0.06945492341048151, 0.08577460259230636, -0.007803722295419714, -0.1513386405194583, 0.053176371806980545, 0.386296220285737, -0.2918423352862038, -0.2824876125506013, 0.02474263036603351, -0.2682260782390401, -0.1629194593662171, 0.10876172343898871, 0.023859318667473855, 0.... |
709.336 | A non-monotone conservation law for dune morphodynamics | We investigate a non-local non linear conservation law, first introduced by
A.C. Fowler to describe morphodynamics of dunes, see \cite{Fow01, Fow02}. A
remarkable feature is the violation of the maximum principle, which allows for
erosion phenomenon. We prove well-posedness for initial data in $L^2$ and give
explicit... | math.AP | we investigate a nonlocal non linear conservation law first introduced by ac fowler to describe morphodynamics of dunes see citefow01 fow02 a remarkable feature is the violation of the maximum principle which allows for erosion phenomenon we prove wellposedness for initial data in l2 and give explicit counterexample fo... | [['we', 'investigate', 'a', 'nonlocal', 'non', 'linear', 'conservation', 'law', 'first', 'introduced', 'by', 'ac', 'fowler', 'to', 'describe', 'morphodynamics', 'of', 'dunes', 'see', 'citefow01', 'fow02', 'a', 'remarkable', 'feature', 'is', 'the', 'violation', 'of', 'the', 'maximum', 'principle', 'which', 'allows', 'fo... | [-0.1268310162664975, 0.053890478256616296, -0.13606501028131127, 0.12106835336416517, -0.09234046018919197, -0.11896097489585311, 0.04973354350017794, 0.2696294553451619, -0.24591882009122332, -0.27723992082400845, 0.08270120034901962, -0.25004308558314825, -0.1730757306203625, 0.20162980443150816, -0.0962118186940581... |
709.3361 | On a property of the number 977731833235239280 | We solve a theoretical arithmetics problem stated by Wac{\l}aw Sierpi\'nski.
The problem has remained open for a couple of decades.
| math.NT | we solve a theoretical arithmetics problem stated by waclaw sierpinski the problem has remained open for a couple of decades | [['we', 'solve', 'a', 'theoretical', 'arithmetics', 'problem', 'stated', 'by', 'waclaw', 'sierpinski', 'the', 'problem', 'has', 'remained', 'open', 'for', 'a', 'couple', 'of', 'decades']] | [-0.11118867218886551, 0.05541239159279748, -0.08550653268436068, 0.08923133854803286, -0.09524571856385783, -0.1772119055355066, 0.035717233427261054, 0.3851537833872594, -0.34180480280989095, -0.30405972388229874, 0.19185461385763788, -0.2607462243422082, -0.1129173455563815, 0.24341865452496628, -0.12634205935817017... |
709.3362 | Standard-smooth hybrid inflation | We consider the extended supersymmetric Pati-Salam model which, for mu>0 and
universal boundary conditions, succeeds to yield experimentally acceptable
b-quark masses by moderately violating Yukawa unification. It is known that
this model can lead to new shifted or new smooth hybrid inflation. We show that
a successf... | hep-ph astro-ph | we consider the extended supersymmetric patisalam model which for mu0 and universal boundary conditions succeeds to yield experimentally acceptable bquark masses by moderately violating yukawa unification it is known that this model can lead to new shifted or new smooth hybrid inflation we show that a successful twosta... | [['we', 'consider', 'the', 'extended', 'supersymmetric', 'patisalam', 'model', 'which', 'for', 'mu0', 'and', 'universal', 'boundary', 'conditions', 'succeeds', 'to', 'yield', 'experimentally', 'acceptable', 'bquark', 'masses', 'by', 'moderately', 'violating', 'yukawa', 'unification', 'it', 'is', 'known', 'that', 'this'... | [-0.14004538936447775, 0.19089412250676155, -0.06425274045620645, 0.09050172345375124, -0.08903372942941996, -0.18426081909043757, -0.005967691857831308, 0.31890638088449264, -0.23036547291737336, -0.28969735897786714, 0.12504149244716856, -0.18363948991707615, -0.08186120166321079, 0.14066903902258834, -0.049709373955... |
709.3363 | Can a resonance theory be a renormalizable theory? | In this talk we make an exhaustive analysis of the possible chiral invariant
operators that may described the resonance decay S->pi pi. These provide at the
same time the only available chiral invariant structures for the loop
ultraviolet divergences in this amplitude. Independently of the order in
perturbation theor... | hep-ph | in this talk we make an exhaustive analysis of the possible chiral invariant operators that may described the resonance decay spi pi these provide at the same time the only available chiral invariant structures for the loop ultraviolet divergences in this amplitude independently of the order in perturbation theory we f... | [['in', 'this', 'talk', 'we', 'make', 'an', 'exhaustive', 'analysis', 'of', 'the', 'possible', 'chiral', 'invariant', 'operators', 'that', 'may', 'described', 'the', 'resonance', 'decay', 'spi', 'pi', 'these', 'provide', 'at', 'the', 'same', 'time', 'the', 'only', 'available', 'chiral', 'invariant', 'structures', 'for'... | [-0.16720687466509201, 0.223301104922404, -0.11277938396532965, 0.10484009511042934, -0.0747583193005994, -0.12146915910382043, 0.012789650327142547, 0.34683306915137696, -0.24708765936905847, -0.22960742649978355, 0.09145560775547945, -0.30755478779182716, -0.1413826560601592, 0.06688339389203225, 0.01909089307574665,... |
709.3364 | Baryon Modes of B Meson Decays | The baryon decay modes of B,bar{B}-> N_{1}bar{N}_{2}(f),
bar{N}_{1}N_{2}(bar{f}) provide a frame work to test CP-invariance in baryon
sector. It is shown that in the rest frame of B, N_{1} and bar{N}_{2} come out
with longitudnal polarization lambda_{1}=lambda_{2}=\pm 1 with decay width
Gamma_{f}=Gamma_{f}^{++}+Gamma... | hep-ph | the baryon decay modes of bbarb n_1barn_2f barn_1n_2barf provide a frame work to test cpinvariance in baryon sector it is shown that in the rest frame of b n_1 and barn_2 come out with longitudnal polarization lambda_1lambda_2pm 1 with decay width gamma_fgamma_fgamma_f and the asymmetry parameter alpha _fdelta gamma_fg... | [['the', 'baryon', 'decay', 'modes', 'of', 'bbarb', 'n_1barn_2f', 'barn_1n_2barf', 'provide', 'a', 'frame', 'work', 'to', 'test', 'cpinvariance', 'in', 'baryon', 'sector', 'it', 'is', 'shown', 'that', 'in', 'the', 'rest', 'frame', 'of', 'b', 'n_1', 'and', 'barn_2', 'come', 'out', 'with', 'longitudnal', 'polarization', ... | [-0.06863278256067516, 0.2626001369673759, -0.09669431488973236, 0.10424844006713675, -0.06803805143817475, -0.18946200940561922, 0.036238794414767704, 0.3119991122499893, -0.23728746626232017, -0.20336357792042883, 0.001149150458360581, -0.2972616346994121, 0.002675130853037301, 0.1195726950481338, 0.09445319669811349... |
709.3365 | A deep Large Binocular Telescope view of the Canes Venatici I dwarf
galaxy | We present the first deep color-magnitude diagram of the Canes Venatici I
(CVnI) dwarf galaxy from observations with the wide field Large Binocular
Camera on the Large Binocular Telescope. Reaching down to the main-sequence
turnoff of the oldest stars, it reveals a dichotomy in the stellar populations
of CVnI: it har... | astro-ph | we present the first deep colormagnitude diagram of the canes venatici i cvni dwarf galaxy from observations with the wide field large binocular camera on the large binocular telescope reaching down to the mainsequence turnoff of the oldest stars it reveals a dichotomy in the stellar populations of cvni it harbors an o... | [['we', 'present', 'the', 'first', 'deep', 'colormagnitude', 'diagram', 'of', 'the', 'canes', 'venatici', 'i', 'cvni', 'dwarf', 'galaxy', 'from', 'observations', 'with', 'the', 'wide', 'field', 'large', 'binocular', 'camera', 'on', 'the', 'large', 'binocular', 'telescope', 'reaching', 'down', 'to', 'the', 'mainsequence... | [-0.027207713916141074, 0.14368499556667302, -0.10537750959629193, 0.11390673728310503, -0.14951175955065993, -0.06700594968278892, 0.06237175555870635, 0.4314489312469959, -0.13003617219874286, -0.4165434158872813, 0.0009739807981532067, -0.26554948485354546, -0.012035239183751401, 0.18008573814513512, -0.117306007268... |
709.3366 | Jozso's Legacy: Chemical and Kinetic Freeze-out in Heavy-Ion Collisions | We review J. Zimanyi's key contributions to the theoretical understanding of
dynamical freeze-out in nuclear collisions and their subsequent applications to
ultra-relativistic heavy-ion collisions, leading to the discovery of a
freeze-out hierarchy where chemical freeze-out of hadron yields precedes the
thermal decou... | nucl-th | we review j zimanyis key contributions to the theoretical understanding of dynamical freezeout in nuclear collisions and their subsequent applications to ultrarelativistic heavyion collisions leading to the discovery of a freezeout hierarchy where chemical freezeout of hadron yields precedes the thermal decoupling of t... | [['we', 'review', 'j', 'zimanyis', 'key', 'contributions', 'to', 'the', 'theoretical', 'understanding', 'of', 'dynamical', 'freezeout', 'in', 'nuclear', 'collisions', 'and', 'their', 'subsequent', 'applications', 'to', 'ultrarelativistic', 'heavyion', 'collisions', 'leading', 'to', 'the', 'discovery', 'of', 'a', 'freez... | [-0.08446006379028978, 0.2240760660209497, -0.23341504461989787, 0.08366714399623897, -0.005228276745612292, -0.0856421723453279, -0.00961286436312979, 0.3287797560572232, -0.25385214917753873, -0.28776643818342373, -0.04548428586659659, -0.31463849427619656, 0.03746514961772176, 0.102439754511847, 0.06068514775803411,... |
709.3367 | Implementing Few-Body Algorithmic Regularization with Post-Newtonian
Terms | We discuss the implementation of a new regular algorithm for simulation of
the gravitational few-body problem. The algorithm uses components from earlier
methods, including the chain structure, the logarithmic Hamiltonian, and the
time-transformed leapfrog. This algorithmic regularization code, AR-CHAIN, can
be used ... | astro-ph | we discuss the implementation of a new regular algorithm for simulation of the gravitational fewbody problem the algorithm uses components from earlier methods including the chain structure the logarithmic hamiltonian and the timetransformed leapfrog this algorithmic regularization code archain can be used for the norm... | [['we', 'discuss', 'the', 'implementation', 'of', 'a', 'new', 'regular', 'algorithm', 'for', 'simulation', 'of', 'the', 'gravitational', 'fewbody', 'problem', 'the', 'algorithm', 'uses', 'components', 'from', 'earlier', 'methods', 'including', 'the', 'chain', 'structure', 'the', 'logarithmic', 'hamiltonian', 'and', 'th... | [-0.0944596131323088, 0.05893899162437461, -0.07374262435854796, 0.08987042105953008, -0.09076735817863807, -0.13999423085182322, 0.01760816683164711, 0.3677591190344709, -0.2260929552984296, -0.33435746260340027, 0.09135767838326465, -0.2793375574488606, -0.09286897018318996, 0.2564285096641648, -0.03685805769711413, ... |
709.3368 | Track Based Alignment in CMS | The strategy for track based alignment of the CMS tracking and muon detectors
is presented. After an overview over the used data samples, the general
alignment strategy is presented, with a focus of the procedures envisaged at
the start of data taking in 2008. The three currently used alignment algorithms
are discuss... | physics.ins-det | the strategy for track based alignment of the cms tracking and muon detectors is presented after an overview over the used data samples the general alignment strategy is presented with a focus of the procedures envisaged at the start of data taking in 2008 the three currently used alignment algorithms are discussed and... | [['the', 'strategy', 'for', 'track', 'based', 'alignment', 'of', 'the', 'cms', 'tracking', 'and', 'muon', 'detectors', 'is', 'presented', 'after', 'an', 'overview', 'over', 'the', 'used', 'data', 'samples', 'the', 'general', 'alignment', 'strategy', 'is', 'presented', 'with', 'a', 'focus', 'of', 'the', 'procedures', 'e... | [-0.04813509334072277, 0.072303478716602, -0.06600544004785744, 0.059012913825474196, -0.021613918843546083, -0.09924977186268993, -0.0393782446959189, 0.38780180626101307, -0.18412949841517906, -0.37754773511853695, 0.15103668481710233, -0.2991359762532951, -0.054377678564036046, 0.23732868506113527, -0.04592229895801... |
709.3369 | On the magnetically driven ferroelectric phase in GdMnO3 | At room temperature, GdMnO3 is a paraelectric and paramagnetic with a
distorted perovskite structure of orthorhombic symmetry (space group Pnma). On
cooling, it undergoes a phase transition sequence to a magnetic incommensurate
phase (k=delta a*; Tc1=42K) and a A-type antiferromagnetic phase (Tc2=27K). At
low tempera... | cond-mat.mtrl-sci | at room temperature gdmno3 is a paraelectric and paramagnetic with a distorted perovskite structure of orthorhombic symmetry space group pnma on cooling it undergoes a phase transition sequence to a magnetic incommensurate phase kdelta a tc142k and a atype antiferromagnetic phase tc227k at low temperatures t12k a magne... | [['at', 'room', 'temperature', 'gdmno3', 'is', 'a', 'paraelectric', 'and', 'paramagnetic', 'with', 'a', 'distorted', 'perovskite', 'structure', 'of', 'orthorhombic', 'symmetry', 'space', 'group', 'pnma', 'on', 'cooling', 'it', 'undergoes', 'a', 'phase', 'transition', 'sequence', 'to', 'a', 'magnetic', 'incommensurate',... | [-0.24124661049015983, 0.3166252645137517, -0.07549027551684286, -0.038845129650207644, -0.0865848906991153, -0.09714362322373073, 0.16268588396538372, 0.43877378292381763, -0.28177529458543693, -0.21925256512654218, 0.04911080044289322, -0.2982109017649908, -0.1538588497079099, 0.07014642203727778, 0.09291164356830489... |
709.337 | Nucleon form factors on the lattice with light dynamical fermions | The electromagnetic form factors provide important insight into the internal
structure of the nucleon and continue to be of major interest for experiment
and phenomenology. For an intermediate range of momenta the form factors can be
calculated on the lattice. However, the reliability of the results is limited
by sys... | hep-lat | the electromagnetic form factors provide important insight into the internal structure of the nucleon and continue to be of major interest for experiment and phenomenology for an intermediate range of momenta the form factors can be calculated on the lattice however the reliability of the results is limited by systemat... | [['the', 'electromagnetic', 'form', 'factors', 'provide', 'important', 'insight', 'into', 'the', 'internal', 'structure', 'of', 'the', 'nucleon', 'and', 'continue', 'to', 'be', 'of', 'major', 'interest', 'for', 'experiment', 'and', 'phenomenology', 'for', 'an', 'intermediate', 'range', 'of', 'momenta', 'the', 'form', '... | [-0.08133884907389681, 0.26209493907119213, -0.08708300440874253, 0.10240120333850149, -0.07032396601274954, -0.05385995944563367, 0.09004076045879104, 0.3755484333446434, -0.14909614493382406, -0.3298242894202672, 0.05523141175886062, -0.25294239280392994, -0.04304634412616357, 0.1625505457674195, 0.051087504026253484... |
709.3371 | Search for the C-parity violating process J/psi->gamma gamma via
psi(2S)->pi+pi- J/psi | Using 14.0\times 10^6 \psi(2S) events collected with the BES-II detector, the
C-parity violating process J/psi->gamma gamma via psi(2S)->pi+pi- J/psi is
studied. We determine a new upper limit for the J/psi->gamma gamma branching
ratio of B(J/psi->gamma gamma)<2.2\times 10^{-5} at the 90% C.L., which is
about 20 time... | hep-ex | using 140times 106 psi2s events collected with the besii detector the cparity violating process jpsigamma gamma via psi2spipi jpsi is studied we determine a new upper limit for the jpsigamma gamma branching ratio of bjpsigamma gamma22times 105 at the 90 cl which is about 20 times lower than the previous measurement | [['using', '140times', '106', 'psi2s', 'events', 'collected', 'with', 'the', 'besii', 'detector', 'the', 'cparity', 'violating', 'process', 'jpsigamma', 'gamma', 'via', 'psi2spipi', 'jpsi', 'is', 'studied', 'we', 'determine', 'a', 'new', 'upper', 'limit', 'for', 'the', 'jpsigamma', 'gamma', 'branching', 'ratio', 'of', ... | [-0.06594929303997671, 0.24269812192995938, -0.02328374548530092, 0.11929585116729645, -0.0012730524438072223, -0.09092105312120853, 0.18044157972445293, 0.2366636166044948, -0.07644931259279956, -0.321590890461693, 0.025923592390074413, -0.4162415973842144, 0.12434877311734825, 0.1967905676039886, 0.10949001424204634,... |
709.3372 | Two-dimensional Radiation-hydrodynamic Model for Supercritical Disk
Accretion Flows onto Neutron Stars | We performed two-dimensional radiation hydrodynamic simulations of
supercritical accretion flows around neutron stars (NSs). In contrast with the
accretion flows onto black holes (BHs), we find that the shell-shaped
high-density regions form around the NSs, since the radiation force is enhanced
in the innermost regio... | astro-ph | we performed twodimensional radiation hydrodynamic simulations of supercritical accretion flows around neutron stars nss in contrast with the accretion flows onto black holes bhs we find that the shellshaped highdensity regions form around the nss since the radiation force is enhanced in the innermost regions the enhan... | [['we', 'performed', 'twodimensional', 'radiation', 'hydrodynamic', 'simulations', 'of', 'supercritical', 'accretion', 'flows', 'around', 'neutron', 'stars', 'nss', 'in', 'contrast', 'with', 'the', 'accretion', 'flows', 'onto', 'black', 'holes', 'bhs', 'we', 'find', 'that', 'the', 'shellshaped', 'highdensity', 'regions... | [-0.15031175362156932, 0.1819494788817286, 0.01636374066899872, 0.10308430519648216, -0.024626415519452573, -0.039092036463505675, 0.020007907077922944, 0.3599936327859085, -0.203972284745307, -0.2918389479785618, 0.10325773453394718, -0.29097071896429383, 0.07002196403228725, 0.26605579268231533, 0.003542849584377257,... |
709.3373 | Hyperbolicity of general deformations: proofs | We modify the deformation method explored previously in a joint work of B.
Shiffman and the author, in order to construct further examples of Kobayashi
hyperbolic surfaces in the projective 3-space of any even degree starting with
degree 8.
| math.AG math.CV | we modify the deformation method explored previously in a joint work of b shiffman and the author in order to construct further examples of kobayashi hyperbolic surfaces in the projective 3space of any even degree starting with degree 8 | [['we', 'modify', 'the', 'deformation', 'method', 'explored', 'previously', 'in', 'a', 'joint', 'work', 'of', 'b', 'shiffman', 'and', 'the', 'author', 'in', 'order', 'to', 'construct', 'further', 'examples', 'of', 'kobayashi', 'hyperbolic', 'surfaces', 'in', 'the', 'projective', '3space', 'of', 'any', 'even', 'degree',... | [-0.14355073577891558, 0.0649893645149393, -0.0668740247686704, 0.013790400173419561, -0.07416751966453515, -0.1428100195570061, 0.02677846283245927, 0.3434078239668638, -0.23869376728693262, -0.3058995202374764, 0.04175579874143482, -0.2350492598488927, -0.2057263262760945, 0.16382799135186735, -0.14612895171516216, 0... |
709.3374 | Local equivalence of symmetric hypersurfaces in $\mathbb C^2$ | The Chern-Moser normal form and its analog on finite type hypersurfaces in
general do not respect symmetries. Extending the work of N. K. Stanton, we
consider the local equivalence problem for symmetric Levi degenerate
hypersurfaces of finite type in $\mathbb C^2$. The results give for all such
hypersurfaces a comple... | math.CV | the chernmoser normal form and its analog on finite type hypersurfaces in general do not respect symmetries extending the work of n k stanton we consider the local equivalence problem for symmetric levi degenerate hypersurfaces of finite type in mathbb c2 the results give for all such hypersurfaces a complete normaliza... | [['the', 'chernmoser', 'normal', 'form', 'and', 'its', 'analog', 'on', 'finite', 'type', 'hypersurfaces', 'in', 'general', 'do', 'not', 'respect', 'symmetries', 'extending', 'the', 'work', 'of', 'n', 'k', 'stanton', 'we', 'consider', 'the', 'local', 'equivalence', 'problem', 'for', 'symmetric', 'levi', 'degenerate', 'h... | [-0.14917818288143614, 0.05643048010435702, -0.022671173133029795, 0.07256237868943463, -0.08249439502891043, -0.15268220740490326, -0.030047065689053278, 0.3181222512520444, -0.23484910584266971, -0.2123875321277491, 0.09444598392191536, -0.2468342916754139, -0.12211306275578566, 0.18262852417503364, -0.13022179559961... |
709.3375 | Compatible Geometric Matchings | This paper studies non-crossing geometric perfect matchings. Two such perfect
matchings are \emph{compatible} if they have the same vertex set and their
union is also non-crossing. Our first result states that for any two perfect
matchings $M$ and $M'$ of the same set of $n$ points, for some $k\in\Oh{\log
n}$, there ... | math.CO | this paper studies noncrossing geometric perfect matchings two such perfect matchings are emphcompatible if they have the same vertex set and their union is also noncrossing our first result states that for any two perfect matchings m and m of the same set of n points for some kinohlog n there is a sequence of perfect ... | [['this', 'paper', 'studies', 'noncrossing', 'geometric', 'perfect', 'matchings', 'two', 'such', 'perfect', 'matchings', 'are', 'emphcompatible', 'if', 'they', 'have', 'the', 'same', 'vertex', 'set', 'and', 'their', 'union', 'is', 'also', 'noncrossing', 'our', 'first', 'result', 'states', 'that', 'for', 'any', 'two', '... | [-0.21798002273633985, 0.12753324464589955, -0.026366273963732735, -0.0003613887934365889, -0.06501947401964164, -0.14594176533742698, 0.040888397603530205, 0.38656357912854716, -0.2376023448248218, -0.3212584401643672, 0.03956954734696245, -0.33254040718417277, -0.12989050761301565, 0.08162929379166318, -0.11983711620... |
709.3376 | Bar formation and galaxy interactions in MOND | The LCDM model is the most commonly admitted to describe our Universe. In
spite of a great success with regard to the large scale structure formation,
some problems are still unresolved at galactic scales. Alternative scenarios
have to be explored such as modified gravity. We have developed an N-body code
able to sol... | astro-ph | the lcdm model is the most commonly admitted to describe our universe in spite of a great success with regard to the large scale structure formation some problems are still unresolved at galactic scales alternative scenarios have to be explored such as modified gravity we have developed an nbody code able to solve in a... | [['the', 'lcdm', 'model', 'is', 'the', 'most', 'commonly', 'admitted', 'to', 'describe', 'our', 'universe', 'in', 'spite', 'of', 'a', 'great', 'success', 'with', 'regard', 'to', 'the', 'large', 'scale', 'structure', 'formation', 'some', 'problems', 'are', 'still', 'unresolved', 'at', 'galactic', 'scales', 'alternative'... | [-0.1086464380630948, 0.09315193871349002, -0.12250179602659028, 0.1407917348898516, -0.07059703772919702, -0.12861100300226655, -0.1032635724961097, 0.3701955785084828, -0.20706919453444023, -0.3396884483856429, 0.035066343616267544, -0.24111848957653115, -0.0742499164335448, 0.19550452301974908, -0.003743638373966434... |
709.3377 | Algebraic causality: Bayes nets and beyond | The relationship between algebraic geometry and the inferential framework of
the Bayesian Networks with hidden variables has now been fruitfully explored
and exploited by a number of authors. More recently the algebraic formulation
of Causal Bayesian Networks has also been investigated in this context. After
reviewin... | stat.ME | the relationship between algebraic geometry and the inferential framework of the bayesian networks with hidden variables has now been fruitfully explored and exploited by a number of authors more recently the algebraic formulation of causal bayesian networks has also been investigated in this context after reviewing th... | [['the', 'relationship', 'between', 'algebraic', 'geometry', 'and', 'the', 'inferential', 'framework', 'of', 'the', 'bayesian', 'networks', 'with', 'hidden', 'variables', 'has', 'now', 'been', 'fruitfully', 'explored', 'and', 'exploited', 'by', 'a', 'number', 'of', 'authors', 'more', 'recently', 'the', 'algebraic', 'fo... | [-0.07051557148439123, 0.05375958906339579, -0.12603167328787476, 0.12103995325313391, -0.12201004704754603, -0.13187492929497047, 0.02833278848771251, 0.36759324446320535, -0.3102231713060878, -0.31803475448273516, 0.10736263483199046, -0.20921182591762197, -0.22918653784221724, 0.1989546510219378, -0.0769808687367721... |
709.3378 | Intersection numbers of Riemann surfaces from Gaussian matrix models | We consider a Gaussian random matrix theory in the presence of an external
matrix source. This matrix model, after duality (a simple version of the
closed/open string duality), yields a generalized Kontsevich model through an
appropriate tuning of the external source. The n-point correlation functions of
this theory ... | hep-th | we consider a gaussian random matrix theory in the presence of an external matrix source this matrix model after duality a simple version of the closedopen string duality yields a generalized kontsevich model through an appropriate tuning of the external source the npoint correlation functions of this theory are shown ... | [['we', 'consider', 'a', 'gaussian', 'random', 'matrix', 'theory', 'in', 'the', 'presence', 'of', 'an', 'external', 'matrix', 'source', 'this', 'matrix', 'model', 'after', 'duality', 'a', 'simple', 'version', 'of', 'the', 'closedopen', 'string', 'duality', 'yields', 'a', 'generalized', 'kontsevich', 'model', 'through',... | [-0.1801660990164451, 0.13640275665264412, -0.12936896964469377, 0.10605521743487129, -0.05743130396175034, -0.13265011472737087, 0.0632199148674879, 0.3181994769064819, -0.29176593118292443, -0.256957081157495, 0.04624789806548506, -0.2572368188350297, -0.21945504151996884, 0.14248505912392456, -0.058009178826914115, ... |
709.3379 | Luescher-Weisz algorithm for excited states of the QCD flux-tube | We present a version of the Luescher-Weisz multilevel algorithm ideally
suited for studying excited states of the QCD flux tube. While the original
version achieved error reduction only in the temporal direction, the new
algorithm reduces fluctuations in the sources as well. We report on the
implementation of this al... | hep-lat | we present a version of the luescherweisz multilevel algorithm ideally suited for studying excited states of the qcd flux tube while the original version achieved error reduction only in the temporal direction the new algorithm reduces fluctuations in the sources as well we report on the implementation of this algorith... | [['we', 'present', 'a', 'version', 'of', 'the', 'luescherweisz', 'multilevel', 'algorithm', 'ideally', 'suited', 'for', 'studying', 'excited', 'states', 'of', 'the', 'qcd', 'flux', 'tube', 'while', 'the', 'original', 'version', 'achieved', 'error', 'reduction', 'only', 'in', 'the', 'temporal', 'direction', 'the', 'new'... | [-0.06377632873083808, 0.05139595770742744, -0.07108902584418263, 0.09917382400109138, -0.008074950604503485, -0.11180487011657342, 0.0860556092689206, 0.4004378359470713, -0.1874141563832956, -0.34326531779707264, 0.0890568586305323, -0.22330236165343145, -0.1412826537362937, 0.226468935216728, -0.057447068577044104, ... |
709.338 | The causal manipulation of chain event graphs | Discrete Bayesian Networks have been very successful as a framework both for
inference and for expressing certain causal hypotheses. In this paper we
present a class of graphical models called the chain event graph (CEG) models,
that generalises the class of discrete BN models. It provides a flexible and
expressive f... | stat.ME | discrete bayesian networks have been very successful as a framework both for inference and for expressing certain causal hypotheses in this paper we present a class of graphical models called the chain event graph ceg models that generalises the class of discrete bn models it provides a flexible and expressive framewor... | [['discrete', 'bayesian', 'networks', 'have', 'been', 'very', 'successful', 'as', 'a', 'framework', 'both', 'for', 'inference', 'and', 'for', 'expressing', 'certain', 'causal', 'hypotheses', 'in', 'this', 'paper', 'we', 'present', 'a', 'class', 'of', 'graphical', 'models', 'called', 'the', 'chain', 'event', 'graph', 'c... | [-0.10133219750908513, 0.017985511798609945, -0.09397924021403822, 0.12962512079846217, -0.09783299248320637, -0.13761732444011918, 0.05415274827693658, 0.36149372034533706, -0.27000980575879413, -0.2888180607352061, 0.09902357295612563, -0.1942086373973224, -0.18329727615195293, 0.18795524234021152, -0.042198902164171... |
709.3381 | Generalized ABCD propagation for interacting atomic clouds | We present a treatment of the nonlinear matter wave propagation inspired from
optical methods, which includes interaction effects within the atom optics
equivalent of the aberrationless approximation. The atom-optical ABCD matrix
formalism, considered so far for non-interacting clouds, is extended
perturbatively beyo... | cond-mat.quant-gas cond-mat.other physics.atom-ph physics.optics quant-ph | we present a treatment of the nonlinear matter wave propagation inspired from optical methods which includes interaction effects within the atom optics equivalent of the aberrationless approximation the atomoptical abcd matrix formalism considered so far for noninteracting clouds is extended perturbatively beyond the l... | [['we', 'present', 'a', 'treatment', 'of', 'the', 'nonlinear', 'matter', 'wave', 'propagation', 'inspired', 'from', 'optical', 'methods', 'which', 'includes', 'interaction', 'effects', 'within', 'the', 'atom', 'optics', 'equivalent', 'of', 'the', 'aberrationless', 'approximation', 'the', 'atomoptical', 'abcd', 'matrix'... | [-0.11201446363702416, 0.11289673908605145, -0.09286954224977678, 0.08575518558692477, -0.08054487239026907, -0.1241248300145335, -0.00912657806432797, 0.35920052295460286, -0.22358240648308425, -0.2206221961131482, 0.021071212244156784, -0.24689296387967843, -0.12615141478249603, 0.19217704888433218, 0.053104292688375... |
709.3382 | Spin-Peierls transition in carbynoid conductors: infrared absorption
study | The results of IR-studies in quasi-1D carbynoid films produced by
dehydrohalogenation of poly(vinilidene fluoride) are in good agreement with the
assumption that carbynoid films studied are generalized spin -Peierls
conductors, the metal to insulator transition in which can be described in the
frame of t-J model. Res... | cond-mat.str-el | the results of irstudies in quasi1d carbynoid films produced by dehydrohalogenation of polyvinilidene fluoride are in good agreement with the assumption that carbynoid films studied are generalized spin peierls conductors the metal to insulator transition in which can be described in the frame of tj model residual atom... | [['the', 'results', 'of', 'irstudies', 'in', 'quasi1d', 'carbynoid', 'films', 'produced', 'by', 'dehydrohalogenation', 'of', 'polyvinilidene', 'fluoride', 'are', 'in', 'good', 'agreement', 'with', 'the', 'assumption', 'that', 'carbynoid', 'films', 'studied', 'are', 'generalized', 'spin', 'peierls', 'conductors', 'the',... | [-0.14969779242388903, 0.24205447761155666, -0.004509156351676211, 0.029400865783914924, -0.04054952719062567, -0.146165076572448, 0.0009358542659319937, 0.4282758005037904, -0.22340289265103638, -0.26676645410154015, 0.008580917591694742, -0.30307470524683594, -0.07956203507911414, 0.14472181419748814, 0.0761886051092... |
709.3383 | n-Dimensional geometric-shifted global bilinear correspondences of
Langlands on mixed motives III | This third paper,devoted to global correspondences of Langlands,bears more
particularly on geometric-shifted bilinear correspondences on mixed (bi)motives
generated under the action of the products,right by left,of differential
elliptic operators.The mathematical frame,underlying these
correspondences,deals with the ... | math.RT math.AC | this third paperdevoted to global correspondences of langlandsbears more particularly on geometricshifted bilinear correspondences on mixed bimotives generated under the action of the productsright by leftof differential elliptic operatorsthe mathematical frameunderlying these correspondencesdeals with the categories o... | [['this', 'third', 'paperdevoted', 'to', 'global', 'correspondences', 'of', 'langlandsbears', 'more', 'particularly', 'on', 'geometricshifted', 'bilinear', 'correspondences', 'on', 'mixed', 'bimotives', 'generated', 'under', 'the', 'action', 'of', 'the', 'productsright', 'by', 'leftof', 'differential', 'elliptic', 'ope... | [-0.14329281016556628, 0.03440046179099042, -0.13201280262159265, 0.07828514427756486, -0.09983938630076422, -0.10133483437686294, -0.05265681255284859, 0.3049209884678324, -0.36116522188851796, -0.21122350402014411, 0.10436618050553606, -0.23357953636002712, -0.15616961121829093, 0.17883325895915428, -0.14925565409298... |
709.3384 | Weighted Matching in the Semi-Streaming Model | We reduce the best known approximation ratio for finding a weighted matching
of a graph using a one-pass semi-streaming algorithm from 5.828 to 5.585. The
semi-streaming model forbids random access to the input and restricts the
memory to O(n*polylog(n)) bits. It was introduced by Muthukrishnan in 2003 and
is appropr... | cs.DM cs.DS | we reduce the best known approximation ratio for finding a weighted matching of a graph using a onepass semistreaming algorithm from 5828 to 5585 the semistreaming model forbids random access to the input and restricts the memory to onpolylogn bits it was introduced by muthukrishnan in 2003 and is appropriate when deal... | [['we', 'reduce', 'the', 'best', 'known', 'approximation', 'ratio', 'for', 'finding', 'a', 'weighted', 'matching', 'of', 'a', 'graph', 'using', 'a', 'onepass', 'semistreaming', 'algorithm', 'from', '5828', 'to', '5585', 'the', 'semistreaming', 'model', 'forbids', 'random', 'access', 'to', 'the', 'input', 'and', 'restri... | [-0.09476156029160376, 0.06241027132987424, -0.028354620716224115, 0.09013166665681638, -0.12494892133744778, -0.1680861863143811, 0.1485904008495035, 0.35783904920228654, -0.23736593429068173, -0.3832270316089745, 0.09694454785979663, -0.2604839098467319, -0.13455549102380043, 0.13080151281233324, -0.14552789500535088... |
709.3385 | Mass generation of elementary particles and origin of the fundamental
forces in algebraic quantum theory | The main thesis of this paper deals with the interactions of a set of
fermions which are described by one basic type of bilinear interactions,two
symmetric semiobjects,three embedded shells and four fundamental (strong)
gravito-electro-magnetic forces between left and right semiobjects,i.e
semifermions.
| physics.gen-ph | the main thesis of this paper deals with the interactions of a set of fermions which are described by one basic type of bilinear interactionstwo symmetric semiobjectsthree embedded shells and four fundamental strong gravitoelectromagnetic forces between left and right semiobjectsie semifermions | [['the', 'main', 'thesis', 'of', 'this', 'paper', 'deals', 'with', 'the', 'interactions', 'of', 'a', 'set', 'of', 'fermions', 'which', 'are', 'described', 'by', 'one', 'basic', 'type', 'of', 'bilinear', 'interactionstwo', 'symmetric', 'semiobjectsthree', 'embedded', 'shells', 'and', 'four', 'fundamental', 'strong', 'gr... | [-0.17170177880875967, 0.1336723794606892, 0.023312057108882612, 0.027104752625942835, -0.04677546286099666, -0.15049863132220265, -0.05481591233920709, 0.28534252095866847, -0.2721996307373047, -0.2582799690599377, 0.07778103648357697, -0.2732287517975311, -0.14239469778447136, 0.1265246802437547, -0.02718365622835384... |
709.3386 | Exploring the transition into the Chiral Regime of QCD using the
Interacting Instanton Liquid Model | The non-perturbative quark-gluon interaction depends significantly on the
value of the quark mass. In particular, in the light quark mass regime,
correlations are strongly influenced by dynamics associated to chiral symmetry
breaking. We use the Interacting Instanton Liquid Model (IILM) as a tool to
investigate the m... | hep-lat hep-ph | the nonperturbative quarkgluon interaction depends significantly on the value of the quark mass in particular in the light quark mass regime correlations are strongly influenced by dynamics associated to chiral symmetry breaking we use the interacting instanton liquid model iilm as a tool to investigate the microscopic... | [['the', 'nonperturbative', 'quarkgluon', 'interaction', 'depends', 'significantly', 'on', 'the', 'value', 'of', 'the', 'quark', 'mass', 'in', 'particular', 'in', 'the', 'light', 'quark', 'mass', 'regime', 'correlations', 'are', 'strongly', 'influenced', 'by', 'dynamics', 'associated', 'to', 'chiral', 'symmetry', 'brea... | [-0.09260466993307798, 0.2522881353700844, -0.10184153324613969, 0.10313230288981383, -0.03517367956232596, -0.06374881021959784, 0.035179734322203636, 0.30200026417959536, -0.20757486257611568, -0.2633292561513372, 0.02532920619786536, -0.295125079861868, -0.09217712567058495, 0.11104551025750374, 0.07072370099033126,... |
709.3387 | Finite-Dimensional Calculus | We discuss topics related to finite-dimensional calculus in the context of
finite-dimensional quantum mechanics. The truncated Heisenberg-Weyl algebra is
called a TAA algebra after Tekin, Aydin, and Arik who formulated it in terms of
orthofermions. It is shown how to use a matrix approach to implement analytic
repres... | math-ph math.MP | we discuss topics related to finitedimensional calculus in the context of finitedimensional quantum mechanics the truncated heisenbergweyl algebra is called a taa algebra after tekin aydin and arik who formulated it in terms of orthofermions it is shown how to use a matrix approach to implement analytic representations... | [['we', 'discuss', 'topics', 'related', 'to', 'finitedimensional', 'calculus', 'in', 'the', 'context', 'of', 'finitedimensional', 'quantum', 'mechanics', 'the', 'truncated', 'heisenbergweyl', 'algebra', 'is', 'called', 'a', 'taa', 'algebra', 'after', 'tekin', 'aydin', 'and', 'arik', 'who', 'formulated', 'it', 'in', 'te... | [-0.06098676612288857, 0.03213302231194705, -0.12098276952747256, 0.11619644721213263, -0.1433167893992504, -0.1502648715229173, -0.011303168802572015, 0.360179779128105, -0.32101861647762625, -0.1994268314447254, 0.13626701677172345, -0.2254460337447069, -0.24670072081166186, 0.22246645281224378, -0.15867985078200167,... |
709.3388 | Loop-closure principles in protein folding | Simple theoretical concepts and models have been helpful to understand the
folding rates and routes of single-domain proteins. As reviewed in this
article, a physical principle that appears to underly these models is loop
closure.
| q-bio.BM | simple theoretical concepts and models have been helpful to understand the folding rates and routes of singledomain proteins as reviewed in this article a physical principle that appears to underly these models is loop closure | [['simple', 'theoretical', 'concepts', 'and', 'models', 'have', 'been', 'helpful', 'to', 'understand', 'the', 'folding', 'rates', 'and', 'routes', 'of', 'singledomain', 'proteins', 'as', 'reviewed', 'in', 'this', 'article', 'a', 'physical', 'principle', 'that', 'appears', 'to', 'underly', 'these', 'models', 'is', 'loop... | [-0.07901656718126365, 0.15227991810866764, -0.12115139145004962, 0.1491516907300268, -0.10617648112986769, -0.14109167782589793, 0.0475226284137794, 0.40097425345863613, -0.2971332405294691, -0.2676082730293274, 0.05964992067310959, -0.2005670698891793, -0.23427388330123255, 0.21119757448988302, -0.06435226989643915, ... |
709.3389 | Gauge Variant Symmetries for the Schr\"odinger Equation | The last multiplier of Jacobi provides a route for the determination of
families of Lagrangians for a given system. We show that the members of a
family are equivalent in that they differ by a total time derivative. We derive
the Schr\"odinger equation for a one-degree-of-freedom system with a constant
multiplier. In... | nlin.SI | the last multiplier of jacobi provides a route for the determination of families of lagrangians for a given system we show that the members of a family are equivalent in that they differ by a total time derivative we derive the schrodinger equation for a onedegreeoffreedom system with a constant multiplier in the seque... | [['the', 'last', 'multiplier', 'of', 'jacobi', 'provides', 'a', 'route', 'for', 'the', 'determination', 'of', 'families', 'of', 'lagrangians', 'for', 'a', 'given', 'system', 'we', 'show', 'that', 'the', 'members', 'of', 'a', 'family', 'are', 'equivalent', 'in', 'that', 'they', 'differ', 'by', 'a', 'total', 'time', 'der... | [-0.1572436531551364, 0.0926311744924311, -0.06865571887796457, 0.02093201422897296, -0.05867577332726914, -0.1307980716872082, -0.0065042168750026365, 0.3247208627682876, -0.2541891453935333, -0.2457021012394954, 0.07890266975543152, -0.2783282188683506, -0.1642007948717148, 0.19772477727572668, -0.015602378946978872,... |
709.339 | Composition of UHECR and the Pierre Auger Observatory Spectrum | We fit the recently published Pierre Auger ultra-high energy cosmic ray
spectrum assuming that either nucleons or nuclei are emitted at the sources. We
consider the simplified cases of pure proton, or pure oxygen, or pure iron
injection. We perform an exhaustive scan in the source evolution factor, the
spectral index... | astro-ph | we fit the recently published pierre auger ultrahigh energy cosmic ray spectrum assuming that either nucleons or nuclei are emitted at the sources we consider the simplified cases of pure proton or pure oxygen or pure iron injection we perform an exhaustive scan in the source evolution factor the spectral index the max... | [['we', 'fit', 'the', 'recently', 'published', 'pierre', 'auger', 'ultrahigh', 'energy', 'cosmic', 'ray', 'spectrum', 'assuming', 'that', 'either', 'nucleons', 'or', 'nuclei', 'are', 'emitted', 'at', 'the', 'sources', 'we', 'consider', 'the', 'simplified', 'cases', 'of', 'pure', 'proton', 'or', 'pure', 'oxygen', 'or', ... | [-0.07304648746320475, 0.21955183375668536, 0.0037845622619274277, 0.10644434985346687, 0.00141160575374258, -0.07939896810984344, 0.03547633256479137, 0.40336926850056826, -0.22393712252612757, -0.37746663350588494, 0.03761619432542309, -0.38924285665787056, 0.033499135928661945, 0.17065599747002125, 0.053023035480251... |
709.3391 | General relativity, Lauricella's hypergeometric function $F_D$ and the
theory of braids | The exact (closed form) solutions of the equations of motion in the theory of
general relativity that describe motion of test particle and photon in Kerr and
Kerr-(anti) de Sitter spacetimes all involve the multivariable hypergeometric
function of Lauricella $F_D$: Kraniotis [Class. Quantum Grav. {\bf 21} 2004,
4743;... | gr-qc | the exact closed form solutions of the equations of motion in the theory of general relativity that describe motion of test particle and photon in kerr and kerranti de sitter spacetimes all involve the multivariable hypergeometric function of lauricella f_d kraniotis class quantum grav bf 21 2004 4743 class quantum gra... | [['the', 'exact', 'closed', 'form', 'solutions', 'of', 'the', 'equations', 'of', 'motion', 'in', 'the', 'theory', 'of', 'general', 'relativity', 'that', 'describe', 'motion', 'of', 'test', 'particle', 'and', 'photon', 'in', 'kerr', 'and', 'kerranti', 'de', 'sitter', 'spacetimes', 'all', 'involve', 'the', 'multivariable... | [-0.16315468261353402, 0.12136736077354073, -0.04324012295604288, 0.041331657439657894, -0.08873277532754184, -0.11919866616522773, -0.021138704546037123, 0.2613586478082718, -0.19548431459291699, -0.2857018264023949, 0.06145710251696086, -0.2418315902472936, -0.1678508636390911, 0.17620172739956902, -0.096556840060369... |
709.3392 | Optimally localized Wannier functions for quasi one-dimensional
nonperiodic insulators | It is proved that for general, not necessarily periodic quasi one dimensional
systems, the band position operator corresponding to an isolated part of the
energy spectrum has discrete spectrum and its eigenfunctions have the same
spatial localization as the corresponding spectral projection.
As a consequence, an ei... | cond-mat.other math-ph math.MP | it is proved that for general not necessarily periodic quasi one dimensional systems the band position operator corresponding to an isolated part of the energy spectrum has discrete spectrum and its eigenfunctions have the same spatial localization as the corresponding spectral projection as a consequence an eigenbasis... | [['it', 'is', 'proved', 'that', 'for', 'general', 'not', 'necessarily', 'periodic', 'quasi', 'one', 'dimensional', 'systems', 'the', 'band', 'position', 'operator', 'corresponding', 'to', 'an', 'isolated', 'part', 'of', 'the', 'energy', 'spectrum', 'has', 'discrete', 'spectrum', 'and', 'its', 'eigenfunctions', 'have', ... | [-0.1341347963093443, 0.09865125235042564, -0.09041922576626406, 0.08336676668222161, -0.035707093388872575, -0.1387389527802217, -0.014664707170518244, 0.3712518895639384, -0.3062023066301295, -0.20006717053895934, 0.11609644592898165, -0.2705967688729907, -0.11179430712202683, 0.151691909374154, -0.03487076398302266,... |
709.3393 | Pulsation of EE Cam | EE Cam is a previously little studied Delta Scuti pulsator with amplitudes
between those of the HADS (High-Amplitude Delta Scuti stars) group and the
average low-amplitude pulsators. Since the size of stellar rotation determines
both which pulsation modes are selected by the star as well as their
amplitudes, the star... | astro-ph | ee cam is a previously little studied delta scuti pulsator with amplitudes between those of the hads highamplitude delta scuti stars group and the average lowamplitude pulsators since the size of stellar rotation determines both which pulsation modes are selected by the star as well as their amplitudes the star offers ... | [['ee', 'cam', 'is', 'a', 'previously', 'little', 'studied', 'delta', 'scuti', 'pulsator', 'with', 'amplitudes', 'between', 'those', 'of', 'the', 'hads', 'highamplitude', 'delta', 'scuti', 'stars', 'group', 'and', 'the', 'average', 'lowamplitude', 'pulsators', 'since', 'the', 'size', 'of', 'stellar', 'rotation', 'deter... | [-0.1253488234523684, 0.19511949885636568, -0.06822475678101182, 0.06443793620169162, -0.1346047845967114, -0.13699342705029993, 0.14290780726075172, 0.3751622599065304, -0.16268987064808607, -0.32527066429704427, 0.041926797459833326, -0.32923319675028323, -0.05516474569588899, 0.2169621392264962, -0.01442399440368171... |
709.3394 | Cluster and nebular properties of the central star-forming region of NGC
1140 | We present new high spatial resolution HST/ACS imaging of NGC 1140 and high
spectral resolution VLT/UVES spectroscopy of its central star-forming region.
The central region contains several clusters, the two brightest of which are
clusters 1 and 6 from Hunter, O'Connell & Gallagher, located within
star-forming knots ... | astro-ph | we present new high spatial resolution hstacs imaging of ngc 1140 and high spectral resolution vltuves spectroscopy of its central starforming region the central region contains several clusters the two brightest of which are clusters 1 and 6 from hunter oconnell gallagher located within starforming knots a and b respe... | [['we', 'present', 'new', 'high', 'spatial', 'resolution', 'hstacs', 'imaging', 'of', 'ngc', '1140', 'and', 'high', 'spectral', 'resolution', 'vltuves', 'spectroscopy', 'of', 'its', 'central', 'starforming', 'region', 'the', 'central', 'region', 'contains', 'several', 'clusters', 'the', 'two', 'brightest', 'of', 'which... | [-0.0621136742148308, 0.12262962420681102, -0.05084371676595087, 0.07310092807446997, -0.024960752431383376, -0.10743693839366411, 0.0719094741997713, 0.424902613134554, -0.1383422582930181, -0.3949332604832333, 0.05008310575361988, -0.3073254764133457, 0.03800840081820618, 0.15079554816954985, -0.04224697071629139, -0... |
709.3395 | A note on scaling asymptotics for Bohr-Sommerfeld Lagrangian
submanifolds | An important problem in geometric quantization is that of quantizing certain
classes of Lagrangian submanifolds, so-called Bohr-Sommerfeld Lagrangian
submanifolds, equipped with a smooth half-density. A procedure for this in the
complex projective setting is, roughly speaking, to apply the Szego kernel of
the quantiz... | math.SG math-ph math.MP | an important problem in geometric quantization is that of quantizing certain classes of lagrangian submanifolds socalled bohrsommerfeld lagrangian submanifolds equipped with a smooth halfdensity a procedure for this in the complex projective setting is roughly speaking to apply the szego kernel of the quantizing line b... | [['an', 'important', 'problem', 'in', 'geometric', 'quantization', 'is', 'that', 'of', 'quantizing', 'certain', 'classes', 'of', 'lagrangian', 'submanifolds', 'socalled', 'bohrsommerfeld', 'lagrangian', 'submanifolds', 'equipped', 'with', 'a', 'smooth', 'halfdensity', 'a', 'procedure', 'for', 'this', 'in', 'the', 'comp... | [-0.22584697262144984, 0.06736230461219989, -0.07318261386084873, 0.07739500027763929, -0.10626111495662975, -0.13607681352661644, 0.005069746172253405, 0.326560058548585, -0.27208575477774166, -0.16212672106839254, 0.09299495644595442, -0.2750283643042883, -0.1663732353218757, 0.13412096188197623, -0.1326345538028178,... |
709.3396 | Cooling of Particle Beams in Storage Rings | Methods of particle beam cooling are reviewed.
| physics.acc-ph physics.class-ph | methods of particle beam cooling are reviewed | [['methods', 'of', 'particle', 'beam', 'cooling', 'are', 'reviewed']] | [-0.00519726744719914, 0.33952089133007185, -0.048330681365249414, 0.09590271354785987, 0.025860076637140343, -0.25764825620821546, -0.11780590058437415, 0.5521288248045104, -0.18040728462593897, -0.2929860789860998, 0.08811825939587184, -0.29718402134520666, 0.17589488359434263, 0.34220227580850143, 0.0113984891878707... |
709.3397 | Aharonov-Bohm effect for a valley-polarized current in graphene | This is a numerical study of the conductance of an Aharonov-Bohm
interferometer in a tight-binding model of graphene. Two single-mode ballistic
point contacts with zigzag edges are connected by two arms of a hexagonal ring
enclosing a magnetic flux $\Phi$. The point contacts function as valley
filters, transmitting e... | cond-mat.mes-hall | this is a numerical study of the conductance of an aharonovbohm interferometer in a tightbinding model of graphene two singlemode ballistic point contacts with zigzag edges are connected by two arms of a hexagonal ring enclosing a magnetic flux phi the point contacts function as valley filters transmitting electrons fr... | [['this', 'is', 'a', 'numerical', 'study', 'of', 'the', 'conductance', 'of', 'an', 'aharonovbohm', 'interferometer', 'in', 'a', 'tightbinding', 'model', 'of', 'graphene', 'two', 'singlemode', 'ballistic', 'point', 'contacts', 'with', 'zigzag', 'edges', 'are', 'connected', 'by', 'two', 'arms', 'of', 'a', 'hexagonal', 'r... | [-0.2332879743603228, 0.1746941751922384, -0.03277903245308044, 0.025823936248549593, -0.004592914176363873, -0.1761524688171328, 0.02537834944654514, 0.4128247581879204, -0.2833533552387413, -0.2551783357553606, 0.026638117478281823, -0.3011062095094027, -0.14055218869591798, 0.19620608894810457, -0.001696996279529430... |
709.3398 | Spatial image of reaction area from scattering.II: On connection between
the differential cross-sections in transverse momentum and in nearest
approach parameter | We develop general formalism of how to relate cross-section for exclusive
processes to spatial image of reaction area. More precisely we show how to
determine the spatial distribution of outgoing particles in the space of
so-called nearest approach parameter. This parameter characterizes the position
in the coordinat... | hep-ph | we develop general formalism of how to relate crosssection for exclusive processes to spatial image of reaction area more precisely we show how to determine the spatial distribution of outgoing particles in the space of socalled nearest approach parameter this parameter characterizes the position in the coordinate spac... | [['we', 'develop', 'general', 'formalism', 'of', 'how', 'to', 'relate', 'crosssection', 'for', 'exclusive', 'processes', 'to', 'spatial', 'image', 'of', 'reaction', 'area', 'more', 'precisely', 'we', 'show', 'how', 'to', 'determine', 'the', 'spatial', 'distribution', 'of', 'outgoing', 'particles', 'in', 'the', 'space',... | [-0.06688596523391814, 0.14155954174098692, -0.1174060157713289, 0.09945519064785913, -0.06450249499591466, -0.07391337056677523, 0.024699102604894767, 0.353588622296229, -0.2777993320986362, -0.26787111864957425, -0.00922122476705616, -0.22818166599608958, -0.09819096982079957, 0.12595186895798957, -0.0256964487821928... |
709.3399 | Two-dimensional discrete solitons in rotating lattices | We introduce a two-dimensional (2D) discrete nonlinear Schr\"{o}dinger (DNLS)
equation with self-attractive cubic nonlinearity in a rotating reference frame.
The model applies to a Bose-Einstein condensate stirred by a rotating strong
optical lattice, or light propagation in a twisted bundle of nonlinear fibers.
Two ... | nlin.PS | we introduce a twodimensional 2d discrete nonlinear schrodinger dnls equation with selfattractive cubic nonlinearity in a rotating reference frame the model applies to a boseeinstein condensate stirred by a rotating strong optical lattice or light propagation in a twisted bundle of nonlinear fibers two species of local... | [['we', 'introduce', 'a', 'twodimensional', '2d', 'discrete', 'nonlinear', 'schrodinger', 'dnls', 'equation', 'with', 'selfattractive', 'cubic', 'nonlinearity', 'in', 'a', 'rotating', 'reference', 'frame', 'the', 'model', 'applies', 'to', 'a', 'boseeinstein', 'condensate', 'stirred', 'by', 'a', 'rotating', 'strong', 'o... | [-0.20705623373870258, 0.18339249759830617, -0.03559517169180633, 0.010493404180793971, -0.045250270034667556, -0.2002488419229349, 0.007167025008699396, 0.39820980010052076, -0.22435237359828675, -0.20796221678892335, 0.11320526954068055, -0.2818541818574726, -0.04123390133999247, 0.16149483441316348, 0.00153505504703... |
709.34 | First order formalism for spin one fields | We study two general approaches how to describe spin one particles, using
vector and antisymmetric tensor fields within RChT. In this paper we focus on
the question of an equivalence of both ways. The appearing problems lead us to
the introduction of a new type of the description - the first order formalism
which nat... | hep-ph | we study two general approaches how to describe spin one particles using vector and antisymmetric tensor fields within rcht in this paper we focus on the question of an equivalence of both ways the appearing problems lead us to the introduction of a new type of the description the first order formalism which naturally ... | [['we', 'study', 'two', 'general', 'approaches', 'how', 'to', 'describe', 'spin', 'one', 'particles', 'using', 'vector', 'and', 'antisymmetric', 'tensor', 'fields', 'within', 'rcht', 'in', 'this', 'paper', 'we', 'focus', 'on', 'the', 'question', 'of', 'an', 'equivalence', 'of', 'both', 'ways', 'the', 'appearing', 'prob... | [-0.10749614146008188, 0.14161101440332385, -0.0818613837205473, 0.06967077801812269, -0.10554824591261046, -0.0957955907837584, -0.035576437668200456, 0.3007112497961598, -0.2267909843806477, -0.2722037227345288, 0.02973827369907207, -0.2397986040504157, -0.22577744148585988, 0.13641572013582992, -0.012069655997121984... |
709.3401 | Large Deviations in the Superstable Weakly Imperfect Bose Gas | The superstable Weakly Imperfect Bose Gas {(WIBG)} was originally derived to
solve the inconsistency of the Bogoliubov theory of superfluidity. Its
grand-canonical thermodynamics was recently solved but not at {point of} the
{(first order)} phase transition. This paper proposes to close this gap by
using the large de... | math-ph math.MP | the superstable weakly imperfect bose gas wibg was originally derived to solve the inconsistency of the bogoliubov theory of superfluidity its grandcanonical thermodynamics was recently solved but not at point of the first order phase transition this paper proposes to close this gap by using the large deviations formal... | [['the', 'superstable', 'weakly', 'imperfect', 'bose', 'gas', 'wibg', 'was', 'originally', 'derived', 'to', 'solve', 'the', 'inconsistency', 'of', 'the', 'bogoliubov', 'theory', 'of', 'superfluidity', 'its', 'grandcanonical', 'thermodynamics', 'was', 'recently', 'solved', 'but', 'not', 'at', 'point', 'of', 'the', 'firs... | [-0.09165021876491236, 0.2258359865663806, -0.11655788926017362, 0.05096232509223388, 0.03110304075936951, -0.1235589446287657, 0.08246792443712954, 0.27474247845684124, -0.23629590199904188, -0.29351837782408385, 0.027350307996076642, -0.3142968658734496, -0.08545741174620002, 0.04574211650983403, 0.04171621729619801,... |
709.3402 | Amplified signal response in scale-free networks by collaborative
signaling | Many natural and artificial two-states signaling devices are connected
forming networks. The information-processing potential of these systems is
usually related to the response to weak external signals. Here, using a network
of overdamped bistable elements, we study the effect of a heterogeneous complex
topology on ... | physics.comp-ph | many natural and artificial twostates signaling devices are connected forming networks the informationprocessing potential of these systems is usually related to the response to weak external signals here using a network of overdamped bistable elements we study the effect of a heterogeneous complex topology on the sign... | [['many', 'natural', 'and', 'artificial', 'twostates', 'signaling', 'devices', 'are', 'connected', 'forming', 'networks', 'the', 'informationprocessing', 'potential', 'of', 'these', 'systems', 'is', 'usually', 'related', 'to', 'the', 'response', 'to', 'weak', 'external', 'signals', 'here', 'using', 'a', 'network', 'of'... | [-0.23364579524326173, 0.11089519057363932, -0.03872076349474395, 0.05814516797950609, -0.053266372813849085, -0.13398424629416741, 0.03567703839544725, 0.39886572940534426, -0.26356601946739644, -0.2680140136021979, 0.05913251815098515, -0.2853858649636371, -0.3119175302312721, 0.18187212494579202, -0.0077059727244644... |
709.3403 | Enhanced Optical Cooling of Particle Beams in Storage Rings | A method of enhanced optical cooling (EOC) based on nonlinear selective
interaction between particles and theirs amplified undulator radiation wavelets
(URW) in storage rings is discussed. It leads to non-exponential fast damping.
The selectivity is arranged by a moving screen located on the image plane of
the optica... | physics.acc-ph physics.class-ph | a method of enhanced optical cooling eoc based on nonlinear selective interaction between particles and theirs amplified undulator radiation wavelets urw in storage rings is discussed it leads to nonexponential fast damping the selectivity is arranged by a moving screen located on the image plane of the optical system ... | [['a', 'method', 'of', 'enhanced', 'optical', 'cooling', 'eoc', 'based', 'on', 'nonlinear', 'selective', 'interaction', 'between', 'particles', 'and', 'theirs', 'amplified', 'undulator', 'radiation', 'wavelets', 'urw', 'in', 'storage', 'rings', 'is', 'discussed', 'it', 'leads', 'to', 'nonexponential', 'fast', 'damping'... | [-0.18122390940785407, 0.17773574804421513, -0.07470611493568867, 0.023364873575046657, -0.04150039158761501, -0.21645532744005322, -0.003315551919513382, 0.45702363952994346, -0.27264856463298204, -0.22100857203826307, 0.05599952360498719, -0.2671518311463296, -0.09832557454705239, 0.2401543678715825, -0.0209910991881... |
709.3404 | Optimization of the Asymptotic Property of Mutual Learning Involving an
Integration Mechanism of Ensemble Learning | We propose an optimization method of mutual learning which converges into the
identical state of optimum ensemble learning within the framework of on-line
learning, and have analyzed its asymptotic property through the statistical
mechanics method.The proposed model consists of two learning steps: two
students indepe... | cond-mat.dis-nn cond-mat.stat-mech | we propose an optimization method of mutual learning which converges into the identical state of optimum ensemble learning within the framework of online learning and have analyzed its asymptotic property through the statistical mechanics methodthe proposed model consists of two learning steps two students independentl... | [['we', 'propose', 'an', 'optimization', 'method', 'of', 'mutual', 'learning', 'which', 'converges', 'into', 'the', 'identical', 'state', 'of', 'optimum', 'ensemble', 'learning', 'within', 'the', 'framework', 'of', 'online', 'learning', 'and', 'have', 'analyzed', 'its', 'asymptotic', 'property', 'through', 'the', 'stat... | [0.002468261981700012, 0.05419877595015853, -0.1371848926076943, 0.06862609125574694, -0.08608052249443024, -0.18648723698657085, 0.06488069551352887, 0.4005726454482275, -0.2990215685555434, -0.33333598631632294, 0.014640213182305005, -0.26074943219143104, -0.1792666011501074, 0.14768005274062818, -0.12300605194499478... |
709.3405 | Identifying pulsation modes from two-passband photometry | I discuss a prospect for mode identification from two-passband photometry of
forthcoming BRITE space mission. Examples of photometric diagnostic diagrams
are shown for three types of main sequence pulsating variables: $\beta$ Cephei,
Slowly Pulsating B-type and $\delta$ Scuti stars. I consider also taking into
accoun... | astro-ph | i discuss a prospect for mode identification from twopassband photometry of forthcoming brite space mission examples of photometric diagnostic diagrams are shown for three types of main sequence pulsating variables beta cephei slowly pulsating btype and delta scuti stars i consider also taking into account the radial v... | [['i', 'discuss', 'a', 'prospect', 'for', 'mode', 'identification', 'from', 'twopassband', 'photometry', 'of', 'forthcoming', 'brite', 'space', 'mission', 'examples', 'of', 'photometric', 'diagnostic', 'diagrams', 'are', 'shown', 'for', 'three', 'types', 'of', 'main', 'sequence', 'pulsating', 'variables', 'beta', 'ceph... | [-0.04956783160708065, 0.17743789993746337, -0.09014967698495575, 0.06885279901325703, -0.15182928058730308, -0.16832153689181215, 0.07417710343521998, 0.3668409818133643, -0.2307550344334612, -0.3277758352978285, 0.07887948372639543, -0.2775984391959947, -0.06724534109830423, 0.2793346667164114, -0.04669093197755797, ... |
709.3406 | Equal Superposition Transformations and Quantum Random Walks | The largest ensemble of qubits which satisfy the general transformation of
equal superposition is obtained by different methods, namely, linearity,
no-superluminal signalling and non-increase of entanglement under LOCC. We also
consider the associated quantum random walk and show that all unitary balanced
coins give ... | quant-ph | the largest ensemble of qubits which satisfy the general transformation of equal superposition is obtained by different methods namely linearity nosuperluminal signalling and nonincrease of entanglement under locc we also consider the associated quantum random walk and show that all unitary balanced coins give the same... | [['the', 'largest', 'ensemble', 'of', 'qubits', 'which', 'satisfy', 'the', 'general', 'transformation', 'of', 'equal', 'superposition', 'is', 'obtained', 'by', 'different', 'methods', 'namely', 'linearity', 'nosuperluminal', 'signalling', 'and', 'nonincrease', 'of', 'entanglement', 'under', 'locc', 'we', 'also', 'consi... | [-0.11082127592290171, 0.2222507845448411, -0.09348879406309646, 0.09846010971881881, 0.012080652241095684, -0.27266106234215526, 0.050589135291216815, 0.361759804027236, -0.22504161633011224, -0.22066143572168506, 0.07517578614963408, -0.2301010391202526, -0.168907321949044, 0.16897165607930958, -0.08434246628936651, ... |
709.3407 | Non-commutative residue of projections in Boutet de Monvel's calculus | Using results by Melo, Nest, Schick, and Schrohe on the K-theory of Boutet de
Monvel's calculus of boundary value problems, we show that the non-commutative
residue introduced by Fedosov, Golse, Leichtnam, and Schrohe vanishes on
projections in the calculus. This partially answers a question raised in a
recent collab... | math.AP math.KT | using results by melo nest schick and schrohe on the ktheory of boutet de monvels calculus of boundary value problems we show that the noncommutative residue introduced by fedosov golse leichtnam and schrohe vanishes on projections in the calculus this partially answers a question raised in a recent collaboration with ... | [['using', 'results', 'by', 'melo', 'nest', 'schick', 'and', 'schrohe', 'on', 'the', 'ktheory', 'of', 'boutet', 'de', 'monvels', 'calculus', 'of', 'boundary', 'value', 'problems', 'we', 'show', 'that', 'the', 'noncommutative', 'residue', 'introduced', 'by', 'fedosov', 'golse', 'leichtnam', 'and', 'schrohe', 'vanishes',... | [-0.10566739109042403, 0.07062964819299129, -0.10490674639193269, 0.09027296895094748, -0.0909571706910025, -0.12118284233736915, -0.010056607032122163, 0.2751035827224131, -0.31439332872048603, -0.21222119678005383, 0.16700587657358884, -0.272388341934148, -0.16111709727821025, 0.18289181946885663, -0.2201684643937782... |
709.3408 | Discrete Koenigs nets and discrete isothermic surfaces | We discuss discretization of Koenigs nets (conjugate nets with equal Laplace
invariants) and of isothermic surfaces. Our discretization is based on the
notion of dual quadrilaterals: two planar quadrilaterals are called dual, if
their corresponding sides are parallel, and their non-corresponding diagonals
are paralle... | math.DG | we discuss discretization of koenigs nets conjugate nets with equal laplace invariants and of isothermic surfaces our discretization is based on the notion of dual quadrilaterals two planar quadrilaterals are called dual if their corresponding sides are parallel and their noncorresponding diagonals are parallel discret... | [['we', 'discuss', 'discretization', 'of', 'koenigs', 'nets', 'conjugate', 'nets', 'with', 'equal', 'laplace', 'invariants', 'and', 'of', 'isothermic', 'surfaces', 'our', 'discretization', 'is', 'based', 'on', 'the', 'notion', 'of', 'dual', 'quadrilaterals', 'two', 'planar', 'quadrilaterals', 'are', 'called', 'dual', '... | [-0.15583988241704666, 0.10348683955994853, -0.042769667047156595, 0.09372365864188095, -0.13004041480369807, -0.181895978723132, -0.05185573876058081, 0.4315072618659556, -0.3462361613449853, -0.20476734900606913, 0.1330729861565917, -0.2981211951398474, -0.16456781819464608, 0.12642728133259093, -0.19411259798670377,... |
709.3409 | The transition from highly to fully stretched polymer brushes in good
solvent | The stretching of brushes of long polymers grafted to a planar surface is
investigated byMonte Carlo simulations in the limit of very high grafting
densities, as achieved in recent experiments. The monomer density profiles are
shown to deviate considerably from the parabolic limiting form predicted by
self-consistent... | cond-mat.soft cond-mat.stat-mech | the stretching of brushes of long polymers grafted to a planar surface is investigated bymonte carlo simulations in the limit of very high grafting densities as achieved in recent experiments the monomer density profiles are shown to deviate considerably from the parabolic limiting form predicted by selfconsistent fiel... | [['the', 'stretching', 'of', 'brushes', 'of', 'long', 'polymers', 'grafted', 'to', 'a', 'planar', 'surface', 'is', 'investigated', 'bymonte', 'carlo', 'simulations', 'in', 'the', 'limit', 'of', 'very', 'high', 'grafting', 'densities', 'as', 'achieved', 'in', 'recent', 'experiments', 'the', 'monomer', 'density', 'profil... | [-0.08996046058806208, 0.20441358484985198, -0.11801636414876317, 0.030685254189131015, 0.04734966135857736, -0.1278654521879028, 0.02244318051071947, 0.3995837130748174, -0.26890812629306526, -0.2903632076785845, 0.017065566608353573, -0.26593842629124137, -0.10595430022872546, 0.15599560531623224, -0.0123959345989586... |
709.341 | Quantum Knizhnik-Zamolodchikov equation: reflecting boundary conditions
and combinatorics | We consider the level 1 solution of quantum Knizhnik-Zamolodchikov equation
with reflecting boundary conditions which is relevant to the Temperley--Lieb
model of loops on a strip. By use of integral formulae we prove conjectures
relating it to the weighted enumeration of Cyclically Symmetric Transpose
Complement Plan... | math-ph math.CO math.MP nlin.SI | we consider the level 1 solution of quantum knizhnikzamolodchikov equation with reflecting boundary conditions which is relevant to the temperleylieb model of loops on a strip by use of integral formulae we prove conjectures relating it to the weighted enumeration of cyclically symmetric transpose complement plane part... | [['we', 'consider', 'the', 'level', '1', 'solution', 'of', 'quantum', 'knizhnikzamolodchikov', 'equation', 'with', 'reflecting', 'boundary', 'conditions', 'which', 'is', 'relevant', 'to', 'the', 'temperleylieb', 'model', 'of', 'loops', 'on', 'a', 'strip', 'by', 'use', 'of', 'integral', 'formulae', 'we', 'prove', 'conje... | [-0.16111756371808986, 0.07166772436504093, -0.050907126865258404, 0.06011599139082154, -0.13118895767347924, -0.16558102678105818, 0.030286763487703296, 0.3051699575986348, -0.30106934517914175, -0.2427224095764698, 0.1553488078563675, -0.2790577521949422, -0.16990064495407484, 0.17710449606381065, -0.1034946142348880... |
709.3411 | Sure Wins, Separating Probabilities and the Representation of Linear
Functionals | We discuss conditions under which a convex cone $\K\subset \R^{\Omega}$
admits a probability $m$ such that $\sup_{k\in \K} m(k)\leq0$. Based on these,
we also characterize linear functionals that admit the representation as
finitely additive expectations. A version of Riesz decomposition based on this
property is obt... | math.FA math.PR | we discuss conditions under which a convex cone ksubset romega admits a probability m such that sup_kin k mkleq0 based on these we also characterize linear functionals that admit the representation as finitely additive expectations a version of riesz decomposition based on this property is obtained as well as a charact... | [['we', 'discuss', 'conditions', 'under', 'which', 'a', 'convex', 'cone', 'ksubset', 'romega', 'admits', 'a', 'probability', 'm', 'such', 'that', 'sup_kin', 'k', 'mkleq0', 'based', 'on', 'these', 'we', 'also', 'characterize', 'linear', 'functionals', 'that', 'admit', 'the', 'representation', 'as', 'finitely', 'additive... | [-0.11897136158598907, 0.0693153023462871, -0.1415778193301682, 0.0818654288084182, -0.07392227268729616, -0.10041431375329607, 0.02102513193827251, 0.37572121369684564, -0.28267562773945776, -0.14491106317667612, 0.13297271662680754, -0.2518610303964594, -0.19910115655511618, 0.22662248404230922, -0.09201049294065812,... |
709.3412 | Characterization of quasi-coherent modules that are module schemes | The R-module functors that are essential for the development of the theory of
the linear representations of an affine R-group are the quasi-coherent
R-modules and the R-module schemes. The aim of this paper is to study when a
quasi-coherent R-module is an R-module scheme. We will prove that it is
equivalent to giving... | math.AC | the rmodule functors that are essential for the development of the theory of the linear representations of an affine rgroup are the quasicoherent rmodules and the rmodule schemes the aim of this paper is to study when a quasicoherent rmodule is an rmodule scheme we will prove that it is equivalent to giving a character... | [['the', 'rmodule', 'functors', 'that', 'are', 'essential', 'for', 'the', 'development', 'of', 'the', 'theory', 'of', 'the', 'linear', 'representations', 'of', 'an', 'affine', 'rgroup', 'are', 'the', 'quasicoherent', 'rmodules', 'and', 'the', 'rmodule', 'schemes', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'study... | [-0.20284137871024793, 0.04651495654443202, -0.09385267431374456, 0.053954566985399265, -0.04789991817269169, -0.18546129053183755, -0.11400713766237995, 0.39547267925666, -0.43122523264257145, -0.10474778599579071, 0.1277207096076769, -0.2121438751241467, -0.10833954244668854, 0.1618847233075343, -0.23722060980489018,... |
709.3413 | Deconvolution for an atomic distribution | Let $X_1,...,X_n$ be i.i.d. observations, where $X_i=Y_i+\sigma Z_i$ and
$Y_i$ and $Z_i$ are independent. Assume that unobservable $Y$'s are distributed
as a random variable $UV,$ where $U$ and $V$ are independent, $U$ has a
Bernoulli distribution with probability of zero equal to $p$ and $V$ has a
distribution funct... | math.ST stat.TH | let x_1x_n be iid observations where x_iy_isigma z_i and y_i and z_i are independent assume that unobservable ys are distributed as a random variable uv where u and v are independent u has a bernoulli distribution with probability of zero equal to p and v has a distribution function f with density f furthermore let the... | [['let', 'x_1x_n', 'be', 'iid', 'observations', 'where', 'x_iy_isigma', 'z_i', 'and', 'y_i', 'and', 'z_i', 'are', 'independent', 'assume', 'that', 'unobservable', 'ys', 'are', 'distributed', 'as', 'a', 'random', 'variable', 'uv', 'where', 'u', 'and', 'v', 'are', 'independent', 'u', 'has', 'a', 'bernoulli', 'distributio... | [-0.10285433925884335, 0.10464680605546985, -0.1251712873669103, 0.008175723226670931, -0.021444892092376835, -0.22317227693904834, 0.05669837633736039, 0.37378989697847154, -0.28689433650911916, -0.20022098511401423, 0.09956105150758549, -0.3260369223255412, -0.09959816953948089, 0.12246994676481568, -0.08565047295077... |
709.3414 | A normal distribution for the disturbance term in regression theory | In regression theory, it is stated that the disturbance term follows the
normal distribution when the sample size is large. In Professor J.Johnston's
words: "In view of the many factors involved, an appeal to the Central Limit
Theorem would further suggest a normal distribution for u." This paper includes
an elementa... | math.PR | in regression theory it is stated that the disturbance term follows the normal distribution when the sample size is large in professor jjohnstons words in view of the many factors involved an appeal to the central limit theorem would further suggest a normal distribution for u this paper includes an elementary proof th... | [['in', 'regression', 'theory', 'it', 'is', 'stated', 'that', 'the', 'disturbance', 'term', 'follows', 'the', 'normal', 'distribution', 'when', 'the', 'sample', 'size', 'is', 'large', 'in', 'professor', 'jjohnstons', 'words', 'in', 'view', 'of', 'the', 'many', 'factors', 'involved', 'an', 'appeal', 'to', 'the', 'centra... | [-0.0969385836820399, 0.13489990009203745, -0.11967432652304452, 0.09964196687372076, -0.06573663184064485, -0.09919199503455607, 0.02704416566513597, 0.27469361623719574, -0.32167246999839944, -0.2634521267406406, 0.07003670336774713, -0.290478895699221, -0.13555538841053874, 0.1707249452177036, -0.15402590095375976, ... |
709.3415 | Towards a good definition of algebraically overtwisted | Symplectic field theory (SFT) is a collection of homology theories that
provide invariants for contact manifolds. We give a proof that vanishing of any
one of either contact homology, rational SFT or (full) SFT are equivalent. We
call a manifold for which these theories vanish "algebraically overtwisted".
| math.SG | symplectic field theory sft is a collection of homology theories that provide invariants for contact manifolds we give a proof that vanishing of any one of either contact homology rational sft or full sft are equivalent we call a manifold for which these theories vanish algebraically overtwisted | [['symplectic', 'field', 'theory', 'sft', 'is', 'a', 'collection', 'of', 'homology', 'theories', 'that', 'provide', 'invariants', 'for', 'contact', 'manifolds', 'we', 'give', 'a', 'proof', 'that', 'vanishing', 'of', 'any', 'one', 'of', 'either', 'contact', 'homology', 'rational', 'sft', 'or', 'full', 'sft', 'are', 'equ... | [-0.2915361437926743, 0.12666597134096824, -0.15646219689478266, 0.14428847783710808, -0.12274921586380359, -0.29697703283795335, -0.044978139478653825, 0.3165537076506843, -0.24813932025844745, -0.19322978817124634, 0.10759060234425867, -0.25583572718413905, -0.23425792289917616, 0.15870615034958624, -0.12184638234766... |
709.3416 | G\'eom\'etrie, points entiers et courbes enti\`eres | Let $X$ be a projective variety over a number field $K$ (resp. over
$\mathbb{C}$). Let $H$ be the sum of ``sufficiently many positive divisors'' on
$X$. We show that any set of quasi-integral points (resp. any integral curve)
in $X-H$ is not Zariski dense.
| math.AG | let x be a projective variety over a number field k resp over mathbbc let h be the sum of sufficiently many positive divisors on x we show that any set of quasiintegral points resp any integral curve in xh is not zariski dense | [['let', 'x', 'be', 'a', 'projective', 'variety', 'over', 'a', 'number', 'field', 'k', 'resp', 'over', 'mathbbc', 'let', 'h', 'be', 'the', 'sum', 'of', 'sufficiently', 'many', 'positive', 'divisors', 'on', 'x', 'we', 'show', 'that', 'any', 'set', 'of', 'quasiintegral', 'points', 'resp', 'any', 'integral', 'curve', 'in'... | [-0.2722317768599499, 0.07565099460242147, -0.0935365641489625, -0.07454869886384007, -0.0422571569850499, -0.15793334941157477, 0.035028433993416416, 0.3752672157504342, -0.3353514497761022, -0.14070291952653366, 0.04833304356824639, -0.27117158491587773, -0.05642702054782686, 0.25182336734988814, -0.127475361043418, ... |
709.3417 | The innermost region of the water megamaser radio galaxy 3C403 | The standard unified scheme of active galactic nuclei requires the presence
of high column densities of gas and dust potentially obscuring the central
engine. So far, few direct subarcsecond resolution studies of this material
have been performed toward radio galaxies. The goal of this paper is to
elucidate the nucle... | astro-ph | the standard unified scheme of active galactic nuclei requires the presence of high column densities of gas and dust potentially obscuring the central engine so far few direct subarcsecond resolution studies of this material have been performed toward radio galaxies the goal of this paper is to elucidate the nuclear en... | [['the', 'standard', 'unified', 'scheme', 'of', 'active', 'galactic', 'nuclei', 'requires', 'the', 'presence', 'of', 'high', 'column', 'densities', 'of', 'gas', 'and', 'dust', 'potentially', 'obscuring', 'the', 'central', 'engine', 'so', 'far', 'few', 'direct', 'subarcsecond', 'resolution', 'studies', 'of', 'this', 'ma... | [-0.05799288396036474, 0.048480088723224256, 0.00033794696462321116, 0.07768606328180751, -0.09938085410203394, -0.12539297136172026, 0.02353402176445311, 0.4702400542287664, -0.14299802954302177, -0.3413589880834301, 0.12469377837606244, -0.25195781602621914, 0.005826475921777318, 0.13272962209091269, 0.07177650358957... |
709.3418 | Spartan Random Processes in Time Series Modeling | A Spartan random process (SRP) is used to estimate the correlation structure
of time series and to predict (extrapolate) the data values. SRP's are
motivated from statistical physics, and they can be viewed as Ginzburg-Landau
models. The temporal correlations of the SRP are modeled in terms of
`interactions' between ... | physics.soc-ph physics.data-an | a spartan random process srp is used to estimate the correlation structure of time series and to predict extrapolate the data values srps are motivated from statistical physics and they can be viewed as ginzburglandau models the temporal correlations of the srp are modeled in terms of interactions between the field val... | [['a', 'spartan', 'random', 'process', 'srp', 'is', 'used', 'to', 'estimate', 'the', 'correlation', 'structure', 'of', 'time', 'series', 'and', 'to', 'predict', 'extrapolate', 'the', 'data', 'values', 'srps', 'are', 'motivated', 'from', 'statistical', 'physics', 'and', 'they', 'can', 'be', 'viewed', 'as', 'ginzburgland... | [-0.05412798630455476, 0.05906031827908009, -0.09476817578404581, 0.12098810453034485, -0.03990245818883389, -0.11097726711215308, 0.031332267743007805, 0.3806354183234743, -0.2638085718312255, -0.36137727777623424, 0.12878293396458942, -0.2757795929967367, -0.10547499918628002, 0.21809717588015942, 0.00301569578452752... |
709.3419 | Density modulo 1 of sublacunary sequences: application of Peres-Schlag's
arguments | Let the sequence
$\{t_n\}_{n=1}^{\infty}$ of reals satisfy the condition $ \frac{t_{n+1}}{t_n}
\ge 1+ \frac{\gamma}{n^\beta},0\le \beta <1, \gamma >0. $ Then the set $
\{\alpha \in [0,1]: \exists \varkappa > 0 \forall n \in \mathbb{N}
||t_n \alpha || > \frac{\varkappa}{n^\beta \log (n+1)} \} $ is uncountable.
Mor... | math.NT | let the sequence t_n_n1infty of reals satisfy the condition fract_n1t_n ge 1 fracgammanbeta0le beta 1 gamma 0 then the set alpha in 01 exists varkappa 0 forall n in mathbbn t_n alpha fracvarkappanbeta log n1 is uncountable moreover its hausdorff dimension is equal to 1 consider the set of naturals of the form 2n3m and ... | [['let', 'the', 'sequence', 't_n_n1infty', 'of', 'reals', 'satisfy', 'the', 'condition', 'fract_n1t_n', 'ge', '1', 'fracgammanbeta0le', 'beta', '1', 'gamma', '0', 'then', 'the', 'set', 'alpha', 'in', '01', 'exists', 'varkappa', '0', 'forall', 'n', 'in', 'mathbbn', 't_n', 'alpha', 'fracvarkappanbeta', 'log', 'n1', 'is',... | [-0.16651895602495925, 0.20859991083429105, 0.020996132666624867, 0.04550170641758669, 0.014863841814323537, -0.2164034588235313, 0.02223722101754319, 0.3301972987229746, -0.30467041425443103, -0.1903049261987354, 0.033304868957696895, -0.3985482826105599, -0.05543655361437682, 0.11951149322852059, -0.05692812521010637... |
709.342 | Co-Betweenness: A Pairwise Notion of Centrality | Betweenness centrality is a metric that seeks to quantify a sense of the
importance of a vertex in a network graph in terms of its "control" on the
distribution of information along geodesic paths throughout that network. This
quantity however does not capture how different vertices participate together
in such contr... | cs.NI physics.soc-ph | betweenness centrality is a metric that seeks to quantify a sense of the importance of a vertex in a network graph in terms of its control on the distribution of information along geodesic paths throughout that network this quantity however does not capture how different vertices participate together in such control in... | [['betweenness', 'centrality', 'is', 'a', 'metric', 'that', 'seeks', 'to', 'quantify', 'a', 'sense', 'of', 'the', 'importance', 'of', 'a', 'vertex', 'in', 'a', 'network', 'graph', 'in', 'terms', 'of', 'its', 'control', 'on', 'the', 'distribution', 'of', 'information', 'along', 'geodesic', 'paths', 'throughout', 'that',... | [-0.14247875734806506, 0.06069346676915963, -0.09067489072913304, 0.06077199613289188, -0.10149557920257476, -0.11073769315044046, 0.06651248003816529, 0.3929008399983021, -0.27229079389904987, -0.2970665206667036, 0.04466169221665372, -0.2741317722764672, -0.19915150512348523, 0.14831355546431785, -0.10935684208958595... |
709.3421 | Elaborations on the String Dual to N=1 SQCD | In this paper we make further refinements to the duality proposed between N=1
SQCD and certain string (supergravity plus branes) backgrounds, working in the
regime of comparable large number of colors and flavors. Using the string
theory solutions, we predict different field theory observables and phenomena
like Seib... | hep-th | in this paper we make further refinements to the duality proposed between n1 sqcd and certain string supergravity plus branes backgrounds working in the regime of comparable large number of colors and flavors using the string theory solutions we predict different field theory observables and phenomena like seiberg dual... | [['in', 'this', 'paper', 'we', 'make', 'further', 'refinements', 'to', 'the', 'duality', 'proposed', 'between', 'n1', 'sqcd', 'and', 'certain', 'string', 'supergravity', 'plus', 'branes', 'backgrounds', 'working', 'in', 'the', 'regime', 'of', 'comparable', 'large', 'number', 'of', 'colors', 'and', 'flavors', 'using', '... | [-0.1635623433111796, 0.2114887008425391, -0.09111887694831522, 0.14459326550323806, -0.09583984416439334, -0.19787225176272824, 0.06934288666850336, 0.3307438321361879, -0.16005901809673287, -0.32479777852597747, 0.060143837146913105, -0.27719049469242324, -0.18191346821818247, 0.056212243479360074, -0.045792049719291... |
709.3422 | Constraining Newtonian stellar configurations in f(R) theories of
gravity | We consider general metric $f(R)$ theories of gravity by solving the field
equations in the presence of a spherical static mass distribution by analytical
perturbative means. Expanding the field equations systematically in $\cO(G)$,
we solve the resulting set of equations and show that $f(R)$ theories which
attempt t... | astro-ph gr-qc | we consider general metric fr theories of gravity by solving the field equations in the presence of a spherical static mass distribution by analytical perturbative means expanding the field equations systematically in cog we solve the resulting set of equations and show that fr theories which attempt to solve the dark ... | [['we', 'consider', 'general', 'metric', 'fr', 'theories', 'of', 'gravity', 'by', 'solving', 'the', 'field', 'equations', 'in', 'the', 'presence', 'of', 'a', 'spherical', 'static', 'mass', 'distribution', 'by', 'analytical', 'perturbative', 'means', 'expanding', 'the', 'field', 'equations', 'systematically', 'in', 'cog... | [-0.12084502948013695, 0.07662479569184123, -0.09371119819741736, 0.11651712835651211, -0.08778722081533684, -0.10761045562904528, -0.01661411791248748, 0.29682422396276265, -0.22116774403720454, -0.37073545554472553, 0.046948558459388876, -0.21852992214663056, -0.15325669735489833, 0.14391101372017656, -0.037063066943... |
709.3423 | Molecular properties of (U)LIRGs: CO, HCN, HNC and HCO+ | The observed molecular properties of a sample of FIR-luminous and OH
megamaser (OH-MM) galaxies have been investigated. The ratio of high and
low-density tracer lines is found to be determined by the progression of the
star formation in the system. The HCO+/HCN and HCO+/HNC line ratios are good
proxies for the densit... | astro-ph | the observed molecular properties of a sample of firluminous and oh megamaser ohmm galaxies have been investigated the ratio of high and lowdensity tracer lines is found to be determined by the progression of the star formation in the system the hcohcn and hcohnc line ratios are good proxies for the density of the gas ... | [['the', 'observed', 'molecular', 'properties', 'of', 'a', 'sample', 'of', 'firluminous', 'and', 'oh', 'megamaser', 'ohmm', 'galaxies', 'have', 'been', 'investigated', 'the', 'ratio', 'of', 'high', 'and', 'lowdensity', 'tracer', 'lines', 'is', 'found', 'to', 'be', 'determined', 'by', 'the', 'progression', 'of', 'the', ... | [-0.06542272828813209, 0.08203125427685028, -0.016127533311006224, 0.04644428554908779, 0.052490298398906024, -0.07942379353278615, 0.056963727633170425, 0.42237351769671855, -0.13232810141572965, -0.3619834316614111, 0.06338343327046707, -0.2590838298201561, 0.0013788096896074351, 0.15474850388506012, 0.00455846645625... |
709.3424 | Lattice exciton-polaron problem by quantum Monte Carlo simulations | Exciton-polaron formation in one-dimensional lattice models with short or
long-range carrier-phonon interaction is studied by quantum Monte Carlo
simulations. Depending on the relative sign of electron and hole-phonon
coupling, the exciton-polaron size increases or decreases with increasing
interaction strength. Quan... | cond-mat.str-el | excitonpolaron formation in onedimensional lattice models with short or longrange carrierphonon interaction is studied by quantum monte carlo simulations depending on the relative sign of electron and holephonon coupling the excitonpolaron size increases or decreases with increasing interaction strength quantum phonon ... | [['excitonpolaron', 'formation', 'in', 'onedimensional', 'lattice', 'models', 'with', 'short', 'or', 'longrange', 'carrierphonon', 'interaction', 'is', 'studied', 'by', 'quantum', 'monte', 'carlo', 'simulations', 'depending', 'on', 'the', 'relative', 'sign', 'of', 'electron', 'and', 'holephonon', 'coupling', 'the', 'ex... | [-0.16328291615678203, 0.34752994453258534, 0.014070508510081304, 0.07281757064413762, 0.019926821666390256, -0.19246345449721924, 0.012070560163852793, 0.3900241937350344, -0.26759454759734647, -0.2674567000595508, -0.028081224776407773, -0.35724748195045525, -0.03419907449710148, 0.11653112779647389, 0.14654756154589... |
709.3425 | The complexity of the envelope of line and plane arrangements | A facet of an hyperplane arrangement is called external if it belongs to
exactly one bounded cell. The set of all external facets forms the envelope of
the arrangement. The number of external facets of a simple arrangement defined
by $n$ hyperplanes in dimension $d$ is hypothesized to be at least $d{n-2
\choose d-1}$... | math.MG | a facet of an hyperplane arrangement is called external if it belongs to exactly one bounded cell the set of all external facets forms the envelope of the arrangement the number of external facets of a simple arrangement defined by n hyperplanes in dimension d is hypothesized to be at least dn2 choose d1 in this note w... | [['a', 'facet', 'of', 'an', 'hyperplane', 'arrangement', 'is', 'called', 'external', 'if', 'it', 'belongs', 'to', 'exactly', 'one', 'bounded', 'cell', 'the', 'set', 'of', 'all', 'external', 'facets', 'forms', 'the', 'envelope', 'of', 'the', 'arrangement', 'the', 'number', 'of', 'external', 'facets', 'of', 'a', 'simple'... | [-0.19734447107718248, 0.1401149376823317, 0.014946770495347058, -0.010043143633083673, -0.0662058246283171, -0.16973062801601677, 0.029663266381248832, 0.37246348112724564, -0.26679510761944886, -0.29169054989082116, 0.0514184328179302, -0.30261380872495164, -0.13540036764122002, 0.1355258231027013, -0.063285037831519... |
709.3426 | Raman imaging and electronic properties of graphene | Graphite is a well-studied material with known electronic and optical
properties. Graphene, on the other hand, which is just one layer of carbon
atoms arranged in a hexagonal lattice, has been studied theoretically for quite
some time but has only recently become accessible for experiments. Here we
demonstrate how si... | cond-mat.mes-hall | graphite is a wellstudied material with known electronic and optical properties graphene on the other hand which is just one layer of carbon atoms arranged in a hexagonal lattice has been studied theoretically for quite some time but has only recently become accessible for experiments here we demonstrate how single and... | [['graphite', 'is', 'a', 'wellstudied', 'material', 'with', 'known', 'electronic', 'and', 'optical', 'properties', 'graphene', 'on', 'the', 'other', 'hand', 'which', 'is', 'just', 'one', 'layer', 'of', 'carbon', 'atoms', 'arranged', 'in', 'a', 'hexagonal', 'lattice', 'has', 'been', 'studied', 'theoretically', 'for', 'q... | [-0.12568057579740596, 0.14461376843257592, -0.05466978839025474, -0.025837510908380722, 0.01254596313318381, -0.19783699239532535, 0.11200431154037897, 0.49637886537955356, -0.2774043896665367, -0.2715821684123232, 0.039891300369233176, -0.3294786768750502, -0.15981732058840303, 0.2204575716285035, 0.03764761201679133... |
709.3427 | Mutual information for the selection of relevant variables in
spectrometric nonlinear modelling | Data from spectrophotometers form vectors of a large number of exploitable
variables. Building quantitative models using these variables most often
requires using a smaller set of variables than the initial one. Indeed, a too
large number of input variables to a model results in a too large number of
parameters, lead... | cs.LG cs.NE stat.AP | data from spectrophotometers form vectors of a large number of exploitable variables building quantitative models using these variables most often requires using a smaller set of variables than the initial one indeed a too large number of input variables to a model results in a too large number of parameters leading to... | [['data', 'from', 'spectrophotometers', 'form', 'vectors', 'of', 'a', 'large', 'number', 'of', 'exploitable', 'variables', 'building', 'quantitative', 'models', 'using', 'these', 'variables', 'most', 'often', 'requires', 'using', 'a', 'smaller', 'set', 'of', 'variables', 'than', 'the', 'initial', 'one', 'indeed', 'a', ... | [-0.06854725681784514, 0.0646430146083922, -0.09189894498252359, 0.07778825038449692, -0.11490991923308588, -0.1324844455724049, 0.093908979414999, 0.34254394813538774, -0.2812135232846853, -0.34713549594476045, 0.12179041970950111, -0.2777439023899014, -0.11276685520792135, 0.20363406722562535, -0.09234188778301407, 0... |
709.3428 | Bulk antisymmetric tensor fields in a Randall-Sundrum model | We consider bulk antisymmetric tensor fields of various ranks in a
Randall-Sundrum scenario. We show that, rank-2 onwards, the zero-modes of the
projections of these fields on the (3+1) dimensional visible brane become
increasingly weaker as the rank of the tensor increases. All such tensor fields
of rank 4 or more a... | hep-th hep-ph | we consider bulk antisymmetric tensor fields of various ranks in a randallsundrum scenario we show that rank2 onwards the zeromodes of the projections of these fields on the 31 dimensional visible brane become increasingly weaker as the rank of the tensor increases all such tensor fields of rank 4 or more are absent fr... | [['we', 'consider', 'bulk', 'antisymmetric', 'tensor', 'fields', 'of', 'various', 'ranks', 'in', 'a', 'randallsundrum', 'scenario', 'we', 'show', 'that', 'rank2', 'onwards', 'the', 'zeromodes', 'of', 'the', 'projections', 'of', 'these', 'fields', 'on', 'the', '31', 'dimensional', 'visible', 'brane', 'become', 'increasi... | [-0.16087057803304414, 0.23976031073310353, -0.023857435521980126, 0.10683795949234418, -0.05242160599057873, -0.13719018458531382, -0.07391106538256412, 0.3402763391920441, -0.1921547581399749, -0.28466115625961136, 0.11380453111062683, -0.2735280267373021, -0.1454745090801504, 0.1480390762968979, 0.022769162796337058... |
709.3429 | Weak and strong coupling limits of the two-dimensional Fr\"ohlich
polaron with spin-orbit Rashba interaction | The continuous progress in fabricating low-dimensional systems with large
spin-orbit couplings has reached a point in which nowadays materials may
display spin-orbit splitting energies ranging from a few to hundreds of meV.
This situation calls for a better understanding of the interplay between the
spin-orbit coupli... | cond-mat.str-el | the continuous progress in fabricating lowdimensional systems with large spinorbit couplings has reached a point in which nowadays materials may display spinorbit splitting energies ranging from a few to hundreds of mev this situation calls for a better understanding of the interplay between the spinorbit coupling and ... | [['the', 'continuous', 'progress', 'in', 'fabricating', 'lowdimensional', 'systems', 'with', 'large', 'spinorbit', 'couplings', 'has', 'reached', 'a', 'point', 'in', 'which', 'nowadays', 'materials', 'may', 'display', 'spinorbit', 'splitting', 'energies', 'ranging', 'from', 'a', 'few', 'to', 'hundreds', 'of', 'mev', 't... | [-0.1977660050665181, 0.19851189172011316, -0.015944641050872975, 0.08485070366172807, -0.035738657929676614, -0.14144215885843478, 0.043673090349314776, 0.35086050509336053, -0.28770451733858915, -0.29191840962696186, -0.02743273448871441, -0.2775234750750247, -0.10479653978148375, 0.1798164857999727, 0.08554237960934... |
709.343 | The irradiated ISM of ULIRGs | The nuclei of ULIRGs harbor massive young stars, an accreting central black
hole, or both. Results are presented for molecular gas that is exposed to
X-rays (1-100 keV, XDRs) and far-ultraviolet radiation (6-13.6 eV, PDRs).
Attention is paid to species like HCO+, HCN, HNC, OH, H2O and CO. Line ratios
of HCN/HCO+ and ... | astro-ph | the nuclei of ulirgs harbor massive young stars an accreting central black hole or both results are presented for molecular gas that is exposed to xrays 1100 kev xdrs and farultraviolet radiation 6136 ev pdrs attention is paid to species like hco hcn hnc oh h2o and co line ratios of hcnhco and hnchcn discriminate betwe... | [['the', 'nuclei', 'of', 'ulirgs', 'harbor', 'massive', 'young', 'stars', 'an', 'accreting', 'central', 'black', 'hole', 'or', 'both', 'results', 'are', 'presented', 'for', 'molecular', 'gas', 'that', 'is', 'exposed', 'to', 'xrays', '1100', 'kev', 'xdrs', 'and', 'farultraviolet', 'radiation', '6136', 'ev', 'pdrs', 'att... | [0.021895505589485283, 0.12091472130449969, 0.10188321633340448, 0.14867407111159991, -0.009605187352518646, -0.1467737493114736, 0.03470027402318938, 0.5251460442395539, -0.0975577070767402, -0.33374391699551925, -0.054204854722210795, -0.31157962981687515, 0.06787396850164182, 0.09430666422062763, 0.00124275573168178... |
709.3431 | K-Scaffold subgraphs of Complex networks | Complex networks with high numbers of nodes or links are often difficult to
analyse. However, not all elements contribute equally to their structural
patterns. A small number of elements (the hubs) seem to play a particularly
relevant role in organizing the overall structure around them. But other parts
of the archit... | physics.soc-ph | complex networks with high numbers of nodes or links are often difficult to analyse however not all elements contribute equally to their structural patterns a small number of elements the hubs seem to play a particularly relevant role in organizing the overall structure around them but other parts of the architecture s... | [['complex', 'networks', 'with', 'high', 'numbers', 'of', 'nodes', 'or', 'links', 'are', 'often', 'difficult', 'to', 'analyse', 'however', 'not', 'all', 'elements', 'contribute', 'equally', 'to', 'their', 'structural', 'patterns', 'a', 'small', 'number', 'of', 'elements', 'the', 'hubs', 'seem', 'to', 'play', 'a', 'part... | [-0.14859744351347315, 0.1049885851271609, -0.031088406804632, 0.1003509001407594, -0.10224930618077199, -0.12011600561697591, 0.03840497441520478, 0.3971423167893861, -0.29878476692086203, -0.33292472673619683, 0.08262529346269575, -0.27397160435050844, -0.237861097390278, 0.14355914462902683, -0.04792975182545946, 0.... |
709.3432 | Bifurcation From Networks of Unstable Attractors to Heteroclinic
Switching | We present a dynamical system that naturally exhibits two unstable attractors
that are completely enclosed by each others basin volume. This
counter-intuitive phenomenon occurs in networks of pulse-coupled oscillators
with delayed interactions. We analytically and numerically investigate this
phenomenon and clarify t... | nlin.CD cond-mat.dis-nn nlin.AO q-bio.NC | we present a dynamical system that naturally exhibits two unstable attractors that are completely enclosed by each others basin volume this counterintuitive phenomenon occurs in networks of pulsecoupled oscillators with delayed interactions we analytically and numerically investigate this phenomenon and clarify the mec... | [['we', 'present', 'a', 'dynamical', 'system', 'that', 'naturally', 'exhibits', 'two', 'unstable', 'attractors', 'that', 'are', 'completely', 'enclosed', 'by', 'each', 'others', 'basin', 'volume', 'this', 'counterintuitive', 'phenomenon', 'occurs', 'in', 'networks', 'of', 'pulsecoupled', 'oscillators', 'with', 'delayed... | [-0.2838393531323589, 0.18783532616068074, -0.1015236074819497, 0.07464402637251237, -0.00030670580553247574, -0.17603901535658997, 0.09280628953475822, 0.29405833636360995, -0.29238851885608536, -0.19616112809509356, 0.10404128851022254, -0.28443912815357103, -0.26737504801217543, 0.1484908239440398, -0.05121816002189... |
709.3433 | Attempted density blowup in a freely cooling dilute granular gas:
hydrodynamics versus molecular dynamics | It has been recently shown (Fouxon et al. 2007) that, in the framework of
ideal granular hydrodynamics (IGHD), an initially smooth hydrodynamic flow of a
granular gas can produce an infinite gas density in a finite time. Exact
solutions that exhibit this property have been derived. Close to the
singularity, the granu... | cond-mat.soft physics.flu-dyn | it has been recently shown fouxon et al 2007 that in the framework of ideal granular hydrodynamics ighd an initially smooth hydrodynamic flow of a granular gas can produce an infinite gas density in a finite time exact solutions that exhibit this property have been derived close to the singularity the granular gas pres... | [['it', 'has', 'been', 'recently', 'shown', 'fouxon', 'et', 'al', '2007', 'that', 'in', 'the', 'framework', 'of', 'ideal', 'granular', 'hydrodynamics', 'ighd', 'an', 'initially', 'smooth', 'hydrodynamic', 'flow', 'of', 'a', 'granular', 'gas', 'can', 'produce', 'an', 'infinite', 'gas', 'density', 'in', 'a', 'finite', 't... | [-0.12389613854324896, 0.09323181148177198, -0.1623948360264132, 0.04804302422292154, 0.006423729520074722, -0.09828913831293132, -0.019109997756642787, 0.3197212200235538, -0.2658730768104733, -0.2602541545556501, 0.06706237860701302, -0.28721611576173645, -0.0926172170515238, 0.1567895152780105, 0.01848764746271149, ... |
709.3434 | Phase Transitions and the Perfectness of Fluids | We calculate the ratio eta/s, the shear viscosity (eta) to entropy density
(s), which characterizes how perfect a fluid is, in weakly coupled real scalar
field theories with different types of phase transitions. The mean-field
results of the eta/s behaviors agree with the empirical observations in atomic
and molecula... | hep-ph cond-mat.other cond-mat.soft hep-lat nucl-ex nucl-th | we calculate the ratio etas the shear viscosity eta to entropy density s which characterizes how perfect a fluid is in weakly coupled real scalar field theories with different types of phase transitions the meanfield results of the etas behaviors agree with the empirical observations in atomic and molecular systems suc... | [['we', 'calculate', 'the', 'ratio', 'etas', 'the', 'shear', 'viscosity', 'eta', 'to', 'entropy', 'density', 's', 'which', 'characterizes', 'how', 'perfect', 'a', 'fluid', 'is', 'in', 'weakly', 'coupled', 'real', 'scalar', 'field', 'theories', 'with', 'different', 'types', 'of', 'phase', 'transitions', 'the', 'meanfiel... | [-0.15193910769742439, 0.21142993609151872, -0.10793522259081599, 0.055038275349305193, -0.005806477764915479, -0.1501343096238806, 0.005919099572980613, 0.30284637414539856, -0.2183853662572801, -0.3010615843201154, 0.03316123310063982, -0.34035713455982897, -0.1020004034569291, 0.12494954437001102, -0.001680562041879... |
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