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 |
|---|---|---|---|---|---|---|
707.283 | Characterization of thermalized Fermi-Pasta-Ulam chains | The Fermi-Pasta-Ulam (FPU) chains of particles in \textit{thermal
equilibrium} are studied from both wave-interaction and particle-interaction
points of view. It is shown that, even in a strongly nonlinear regime, the
chain in thermal equilibrium can be effectively described by a system of weakly
interacting \textit{... | math-ph math.DS math.MP | the fermipastaulam fpu chains of particles in textitthermal equilibrium are studied from both waveinteraction and particleinteraction points of view it is shown that even in a strongly nonlinear regime the chain in thermal equilibrium can be effectively described by a system of weakly interacting textitrenormalized non... | [['the', 'fermipastaulam', 'fpu', 'chains', 'of', 'particles', 'in', 'textitthermal', 'equilibrium', 'are', 'studied', 'from', 'both', 'waveinteraction', 'and', 'particleinteraction', 'points', 'of', 'view', 'it', 'is', 'shown', 'that', 'even', 'in', 'a', 'strongly', 'nonlinear', 'regime', 'the', 'chain', 'in', 'therma... | [-0.1898261323850602, 0.20139558650346265, -0.1254329933420134, 0.09835030651547842, -0.033808407791786725, -0.13849654145849247, 0.025637932598797812, 0.36741564890576733, -0.2688414780588614, -0.23400074704653687, 0.05376456544889758, -0.30732936777174474, -0.12105793577308456, 0.17779046737899382, 0.0732067547495373... |
707.2831 | Estimating Jones polynomials is a complete problem for one clean qubit | It is known that evaluating a certain approximation to the Jones polynomial
for the plat closure of a braid is a BQP-complete problem. That is, this
problem exactly captures the power of the quantum circuit model. The one clean
qubit model is a model of quantum computation in which all but one qubit starts
in the max... | quant-ph math.GT | it is known that evaluating a certain approximation to the jones polynomial for the plat closure of a braid is a bqpcomplete problem that is this problem exactly captures the power of the quantum circuit model the one clean qubit model is a model of quantum computation in which all but one qubit starts in the maximally... | [['it', 'is', 'known', 'that', 'evaluating', 'a', 'certain', 'approximation', 'to', 'the', 'jones', 'polynomial', 'for', 'the', 'plat', 'closure', 'of', 'a', 'braid', 'is', 'a', 'bqpcomplete', 'problem', 'that', 'is', 'this', 'problem', 'exactly', 'captures', 'the', 'power', 'of', 'the', 'quantum', 'circuit', 'model', ... | [-0.16122942243027918, 0.12527501367277907, -0.06874722021235945, 0.08093894480638385, -0.05460591318398089, -0.22586223143180775, 0.006406598709960061, 0.2897079768981004, -0.3346250911806515, -0.2700325023315981, 0.07938613974444657, -0.2399851605909581, -0.1325103775570225, 0.26096235041250054, -0.05277328872979998,... |
707.2832 | Relative States and the Environment: Einselection, Envariance, Quantum
Darwinism, and the Existential Interpretation | Starting with basic axioms of quantum theory I revisit "Relative State
Interpretation'' set out 50 years ago by Hugh Everett.
| quant-ph | starting with basic axioms of quantum theory i revisit relative state interpretation set out 50 years ago by hugh everett | [['starting', 'with', 'basic', 'axioms', 'of', 'quantum', 'theory', 'i', 'revisit', 'relative', 'state', 'interpretation', 'set', 'out', '50', 'years', 'ago', 'by', 'hugh', 'everett']] | [-0.03162622700911015, 0.1379627471906133, -0.09305228907614946, 0.05943784755654633, -0.045144188962876794, -0.2012518578674644, 0.12125102277495899, 0.2200058669783175, -0.2479760733898729, -0.34668050752952695, 0.028953068441478536, -0.28239064533263447, -0.07961728535592556, 0.11840531546622515, -0.1354277524165809... |
707.2833 | A Comparative Study between Two Three-DOF Parallel Kinematic Machines
using Kinetostatic Criteria and Interval Analysis | This paper addresses the workspace analysis of two 3-DOF translational
parallel mechanisms designed for machining applications. The two machines
features three fixed linear joints. The joint axes of the first machine are
orthogonal whereas these of the second are parallel. In both cases, the mobile
platform moves in ... | cs.RO | this paper addresses the workspace analysis of two 3dof translational parallel mechanisms designed for machining applications the two machines features three fixed linear joints the joint axes of the first machine are orthogonal whereas these of the second are parallel in both cases the mobile platform moves in the car... | [['this', 'paper', 'addresses', 'the', 'workspace', 'analysis', 'of', 'two', '3dof', 'translational', 'parallel', 'mechanisms', 'designed', 'for', 'machining', 'applications', 'the', 'two', 'machines', 'features', 'three', 'fixed', 'linear', 'joints', 'the', 'joint', 'axes', 'of', 'the', 'first', 'machine', 'are', 'ort... | [-0.20084669828945553, 0.03662837179767531, -0.03129953037687512, -0.0373230449825547, -0.09628629759712101, -0.13422359840749482, -0.030117112524580037, 0.4276970453711963, -0.2513383412571234, -0.2996086358352629, 0.12899334164103493, -0.24799338484529493, -0.08329783678921156, 0.17054037245391154, -0.049825306267066... |
707.2834 | Poincar\'e inequality for non euclidean metrics and transportation cost
inequalities on $\mathbb{R}^d$ | In this paper, we consider Poincar\'e inequalities for non euclidean metrics
on $\mathbb{R}^d$. These inequalities enable us to derive precise dimension
free concentration inequalities for product measures. This technique is
appropriate for a large scope of concentration rate: between exponential and
gaussian and bey... | math.PR | in this paper we consider poincare inequalities for non euclidean metrics on mathbbrd these inequalities enable us to derive precise dimension free concentration inequalities for product measures this technique is appropriate for a large scope of concentration rate between exponential and gaussian and beyond we give di... | [['in', 'this', 'paper', 'we', 'consider', 'poincare', 'inequalities', 'for', 'non', 'euclidean', 'metrics', 'on', 'mathbbrd', 'these', 'inequalities', 'enable', 'us', 'to', 'derive', 'precise', 'dimension', 'free', 'concentration', 'inequalities', 'for', 'product', 'measures', 'this', 'technique', 'is', 'appropriate',... | [-0.0647361579822836, 0.0632519737617778, -0.0638665659836941, 0.14815544356386384, -0.05347473216968794, -0.21668123002708345, 0.042703415323109305, 0.31274645780394605, -0.26180197469370026, -0.25162064197606276, 0.13440784515341284, -0.26191199676121596, -0.13854234996433187, 0.24883762382079738, -0.1239972665131866... |
707.2835 | Optical Aharonov-Bohm effect: an inverse hyperbolic problems approach | We describe the general setting for the optical Aharonov-Bohm effect based on
the inverse problem of the identification of the coefficients of the governing
hyperbolic equation by the boundary measurements. We interpret the inverse
problem result as a possibility in principle to detect the optical
Aharonov-Bohm effec... | math-ph math.AP math.MP | we describe the general setting for the optical aharonovbohm effect based on the inverse problem of the identification of the coefficients of the governing hyperbolic equation by the boundary measurements we interpret the inverse problem result as a possibility in principle to detect the optical aharonovbohm effect by ... | [['we', 'describe', 'the', 'general', 'setting', 'for', 'the', 'optical', 'aharonovbohm', 'effect', 'based', 'on', 'the', 'inverse', 'problem', 'of', 'the', 'identification', 'of', 'the', 'coefficients', 'of', 'the', 'governing', 'hyperbolic', 'equation', 'by', 'the', 'boundary', 'measurements', 'we', 'interpret', 'the... | [-0.13192996648927768, 0.08440866967772737, -0.08135439773254535, 0.06293697991207534, -0.11834106923026197, -0.07516843463093334, 0.03150991313889915, 0.3035110848791459, -0.31991200674982634, -0.2987896182811728, 0.12854916480707698, -0.261968792872686, -0.19413227244627243, 0.22446788358045558, -0.02784081796805064,... |
707.2836 | Multimedia Capacity Analysis of the IEEE 802.11e Contention-based
Infrastructure Basic Service Set | We first propose a simple mathematical analysis framework for the Enhanced
Distributed Channel Access (EDCA) function of the recently ratified IEEE
802.11e standard. Our analysis considers the fact that the distributed random
access systems exhibit cyclic behavior. The proposed model is valid for
arbitrary assignment... | cs.IT cs.MM math.IT | we first propose a simple mathematical analysis framework for the enhanced distributed channel access edca function of the recently ratified ieee 80211e standard our analysis considers the fact that the distributed random access systems exhibit cyclic behavior the proposed model is valid for arbitrary assignments of ac... | [['we', 'first', 'propose', 'a', 'simple', 'mathematical', 'analysis', 'framework', 'for', 'the', 'enhanced', 'distributed', 'channel', 'access', 'edca', 'function', 'of', 'the', 'recently', 'ratified', 'ieee', '80211e', 'standard', 'our', 'analysis', 'considers', 'the', 'fact', 'that', 'the', 'distributed', 'random', ... | [-0.2004338902751765, 0.025270750804573312, -0.07371267100786089, 0.029818510778138154, -0.049300806108681906, -0.18168446029816823, 0.13754220278457968, 0.39936324798311756, -0.22793059394524623, -0.3042027636140745, 0.06297248436428446, -0.2159609543694739, -0.15519489550221993, 0.16671271711933397, -0.10962431056434... |
707.2837 | Solutions for certain classes of Riccati differential equation | We derive some analytic closed-form solutions for a class of Riccati equation
y'(x)-\lambda_0(x)y(x)\pm y^2(x)=\pm s_0(x), where \lambda_0(x), s_0(x) are
C^{\infty}-functions. We show that if \delta_n=\lambda_n
s_{n-1}-\lambda_{n-1}s_n=0, where \lambda_{n}=
\lambda_{n-1}^\prime+s_{n-1}+\lambda_0\lambda_{n-1} and
s_{n... | math-ph math.MP | we derive some analytic closedform solutions for a class of riccati equation yxlambda_0xyxpm y2xpm s_0x where lambda_0x s_0x are cinftyfunctions we show that if delta_nlambda_n s_n1lambda_n1s_n0 where lambda_n lambda_n1primes_n1lambda_0lambda_n1 and s_ns_n1primes_0lambda_k1 n12 then the riccati equation has a solution ... | [['we', 'derive', 'some', 'analytic', 'closedform', 'solutions', 'for', 'a', 'class', 'of', 'riccati', 'equation', 'yxlambda_0xyxpm', 'y2xpm', 's_0x', 'where', 'lambda_0x', 's_0x', 'are', 'cinftyfunctions', 'we', 'show', 'that', 'if', 'delta_nlambda_n', 's_n1lambda_n1s_n0', 'where', 'lambda_n', 'lambda_n1primes_n1lambd... | [-0.14516302934566208, -0.0034440690868122632, -0.07386083194856034, 0.05274782974413748, -0.14178509176383877, -0.22461182465993387, -0.020531456755084353, 0.295112194103557, -0.3085041623941601, -0.16639506004664095, 0.16636620301125182, -0.30276192289365583, -0.23576028103571992, 0.18725166595974113, -0.018823633874... |
707.2838 | A solution to B --> pi pi puzzle and B --> K K | The large ratio of color-suppressed tree amplitude to color-allowed one in $B
\to \pi \pi$ decays is difficult to understand within the Standard Model, which
is known as the "$B \to \pi\pi$ puzzle". The two tree diagrams contain the up-
and charm-quark component of penguin amplitude, $P_{uc}$, which cannot be
separat... | hep-ph | the large ratio of colorsuppressed tree amplitude to colorallowed one in b to pi pi decays is difficult to understand within the standard model which is known as the b to pipi puzzle the two tree diagrams contain the up and charmquark component of penguin amplitude p_uc which cannot be separated by measuring b to pi pi... | [['the', 'large', 'ratio', 'of', 'colorsuppressed', 'tree', 'amplitude', 'to', 'colorallowed', 'one', 'in', 'b', 'to', 'pi', 'pi', 'decays', 'is', 'difficult', 'to', 'understand', 'within', 'the', 'standard', 'model', 'which', 'is', 'known', 'as', 'the', 'b', 'to', 'pipi', 'puzzle', 'the', 'two', 'tree', 'diagrams', 'c... | [-0.12314775078481659, 0.20365532418814924, -0.09976774964415462, 0.07050516458501015, -0.08699190258682216, -0.16889580647659505, 0.10245260990503073, 0.2840041102422677, -0.3315156144138216, -0.2765474211226201, 0.02333246679706554, -0.32262479948408945, -0.05169655550161057, 0.10779538743760018, 0.03925110295431457,... |
707.2839 | Critical percolation on random regular graphs | We describe the component sizes in critical independent p-bond percolation on
a random d-regular graph on n vertices, where d \geq 3 is fixed and n grows. We
prove mean-field behavior around the critical probability p_c=1/(d-1).
In particular, we show that there is a scaling window of width n^{-1/3}
around p_c in w... | math.PR math.CO | we describe the component sizes in critical independent pbond percolation on a random dregular graph on n vertices where d geq 3 is fixed and n grows we prove meanfield behavior around the critical probability p_c1d1 in particular we show that there is a scaling window of width n13 around p_c in which the sizes of the ... | [['we', 'describe', 'the', 'component', 'sizes', 'in', 'critical', 'independent', 'pbond', 'percolation', 'on', 'a', 'random', 'dregular', 'graph', 'on', 'n', 'vertices', 'where', 'd', 'geq', '3', 'is', 'fixed', 'and', 'n', 'grows', 'we', 'prove', 'meanfield', 'behavior', 'around', 'the', 'critical', 'probability', 'p_... | [-0.15888689331643815, 0.19384824240374396, -0.054548200372872606, 0.022935411360646998, 0.0004999906706091549, -0.13140241176089537, 0.04119412761314639, 0.33004262171951787, -0.23589848240704409, -0.24236969401660774, 0.10538166265219583, -0.33296228684152346, -0.09456680554264624, 0.12044480172917246, -0.00848256245... |
707.284 | On the extraction of weak transition strengths via the (3He,t) reaction
at 420 MeV | Differential cross sections for transitions of known weak strength were
measured with the (3He,t) reaction at 420 MeV on targets of 12C, 13C, 18O,
26Mg, 58Ni, 60Ni, 90Zr, 118Sn, 120Sn and 208Pb. Using this data, it is shown
the proportionalities between strengths and cross sections for this probe
follow simple trends... | nucl-ex | differential cross sections for transitions of known weak strength were measured with the 3het reaction at 420 mev on targets of 12c 13c 18o 26mg 58ni 60ni 90zr 118sn 120sn and 208pb using this data it is shown the proportionalities between strengths and cross sections for this probe follow simple trends as a function ... | [['differential', 'cross', 'sections', 'for', 'transitions', 'of', 'known', 'weak', 'strength', 'were', 'measured', 'with', 'the', '3het', 'reaction', 'at', '420', 'mev', 'on', 'targets', 'of', '12c', '13c', '18o', '26mg', '58ni', '60ni', '90zr', '118sn', '120sn', 'and', '208pb', 'using', 'this', 'data', 'it', 'is', 's... | [0.026801391693624554, 0.14507132349535823, -0.06134381292111101, 0.18609287718355885, 0.019059524941615547, -0.11281810835894328, 0.0660810090086766, 0.40038096672740947, -0.18527264811564237, -0.33359419431112575, -0.076593534505248, -0.3359883744759779, -0.01027674502039557, 0.1858464923029635, 0.06865186431330808, ... |
707.2841 | The Virtual Manufacturing concept: Scope, Socio-Economic Aspects and
Future Trends | The research area "Virtual Manufacturing (VM)'' is the use of information
technology and computer simulation to model real world manufacturing processes
for the purpose of analysing and understanding them. As automation technologies
such as CAD/CAM have substantially shortened the time required to design
products, Vi... | cs.RO | the research area virtual manufacturing vm is the use of information technology and computer simulation to model real world manufacturing processes for the purpose of analysing and understanding them as automation technologies such as cadcam have substantially shortened the time required to design products virtual manu... | [['the', 'research', 'area', 'virtual', 'manufacturing', 'vm', 'is', 'the', 'use', 'of', 'information', 'technology', 'and', 'computer', 'simulation', 'to', 'model', 'real', 'world', 'manufacturing', 'processes', 'for', 'the', 'purpose', 'of', 'analysing', 'and', 'understanding', 'them', 'as', 'automation', 'technologi... | [-0.08933765465887833, 0.10517413987141407, -0.048501740779955775, 0.0135045240749605, -0.05887260153528531, -0.09056302998690124, 0.04256235297272761, 0.3810153002945744, -0.26614808298324294, -0.34369638150234766, 0.15783644142342085, -0.2312636598944664, -0.15405711121096902, 0.26517575349877304, -0.1000869521034919... |
707.2842 | A Classification of 3R Orthogonal Manipulators by the Topology of their
Workspace | A classification of a family of 3-revolute (3R) positining manipulators is
established. This classification is based on the topology of their workspace.
The workspace is characterized in a half-cross section by the singular curves.
The workspace topology is defined by the number of cusps and nodes that appear
on thes... | cs.RO | a classification of a family of 3revolute 3r positining manipulators is established this classification is based on the topology of their workspace the workspace is characterized in a halfcross section by the singular curves the workspace topology is defined by the number of cusps and nodes that appear on these singula... | [['a', 'classification', 'of', 'a', 'family', 'of', '3revolute', '3r', 'positining', 'manipulators', 'is', 'established', 'this', 'classification', 'is', 'based', 'on', 'the', 'topology', 'of', 'their', 'workspace', 'the', 'workspace', 'is', 'characterized', 'in', 'a', 'halfcross', 'section', 'by', 'the', 'singular', '... | [-0.22289776943233292, 0.04699736215517423, -0.09840681935906753, -0.0072713870777288215, -0.08421220146012547, -0.10624769814687128, -0.011852100293483886, 0.3631748790991889, -0.2484112061645793, -0.2951131749298723, 0.10744043345557762, -0.24184670628465968, -0.15693706431393994, 0.20676801250391136, -0.099698837022... |
707.2843 | A study of B-meson decays to eta_c K* and eta_c gamma K(*) | We present preliminary results of a study of the two-body B-meson decays to a
charmonium state (ccbar) and a K+ or K*0(892) meson using a sample of about 349
fb-1 of data collected with the BABAR detector at the PEP-II asymmetric-energy
B Factory at SLAC. Here ccbar indicates either the eta_c state, reconstructed
in ... | hep-ex | we present preliminary results of a study of the twobody bmeson decays to a charmonium state ccbar and a k or k0892 meson using a sample of about 349 fb1 of data collected with the babar detector at the pepii asymmetricenergy b factory at slac here ccbar indicates either the eta_c state reconstructed in the k_s k pi an... | [['we', 'present', 'preliminary', 'results', 'of', 'a', 'study', 'of', 'the', 'twobody', 'bmeson', 'decays', 'to', 'a', 'charmonium', 'state', 'ccbar', 'and', 'a', 'k', 'or', 'k0892', 'meson', 'using', 'a', 'sample', 'of', 'about', '349', 'fb1', 'of', 'data', 'collected', 'with', 'the', 'babar', 'detector', 'at', 'the'... | [-0.10332990240583077, 0.27109247947884524, -0.08741967924474243, 0.07568686361365179, -0.011014244915481577, -0.1488383666889623, 0.21804810292954419, 0.2776409331461454, -0.11779125569824209, -0.18312647966469855, -0.07703311850088945, -0.5154654457768861, 0.13523034780642929, 0.1050192020967246, 0.18232629673823, 0.... |
707.2844 | Heavy-light quark pseudoscalar and vector mesons at finite temperature | The temperature dependence of the mass, leptonic decay constant, and width of
heavy-light quark peseudoscalar and vector mesons is obtained in the framework
of thermal Hilbert moment QCD sum rules. The leptonic decay constants of both
pseudoscalar and vector mesons decrease with increasing $T$, and vanish at a
critic... | hep-ph | the temperature dependence of the mass leptonic decay constant and width of heavylight quark peseudoscalar and vector mesons is obtained in the framework of thermal hilbert moment qcd sum rules the leptonic decay constants of both pseudoscalar and vector mesons decrease with increasing t and vanish at a critical temper... | [['the', 'temperature', 'dependence', 'of', 'the', 'mass', 'leptonic', 'decay', 'constant', 'and', 'width', 'of', 'heavylight', 'quark', 'peseudoscalar', 'and', 'vector', 'mesons', 'is', 'obtained', 'in', 'the', 'framework', 'of', 'thermal', 'hilbert', 'moment', 'qcd', 'sum', 'rules', 'the', 'leptonic', 'decay', 'const... | [-0.07689185616900839, 0.3407695717664797, -0.04065398783631512, 0.08396494254615824, -0.03992229443192899, -0.1320778000821818, 0.11589319314659963, 0.3286568596264097, -0.2119210922843846, -0.2240975212458688, 0.00551693231204469, -0.3265437918372883, 0.014722375042819933, 0.09772453338964217, 0.09776222723911503, 0.... |
707.2845 | Quantum engineering of squeezed states for quantum communication and
metrology | We report the experimental realization of squeezed quantum states of light,
tailored for new applications in quantum communication and metrology. Squeezed
states in a broad Fourier frequency band down to 1 Hz has been observed for the
first time. Nonclassical properties of light in such a low frequency band is
requir... | quant-ph | we report the experimental realization of squeezed quantum states of light tailored for new applications in quantum communication and metrology squeezed states in a broad fourier frequency band down to 1 hz has been observed for the first time nonclassical properties of light in such a low frequency band is required fo... | [['we', 'report', 'the', 'experimental', 'realization', 'of', 'squeezed', 'quantum', 'states', 'of', 'light', 'tailored', 'for', 'new', 'applications', 'in', 'quantum', 'communication', 'and', 'metrology', 'squeezed', 'states', 'in', 'a', 'broad', 'fourier', 'frequency', 'band', 'down', 'to', '1', 'hz', 'has', 'been', ... | [-0.15038532154379874, 0.2321970141639547, -0.08109782262044585, 0.03371572548734486, -0.04980698079228974, -0.1320678887443028, 0.08754716269695798, 0.42190938455681515, -0.25645974174571723, -0.2969236491630093, 0.06495743822584996, -0.24565798588670218, -0.07785952789310971, 0.27156963196989053, -0.04985925344288604... |
707.2846 | Disentanglement of two qubits coupled to an XY spin chain: Role of
quantum phase transition | We study the disentanglement of two spin qubits which interact with a general
XY spin-chain environment. The dynamical process of the disentanglement is
numerically and analytically investigated in the vicinity of quantum phase
transition (QPT) of the spin chain in both weak and strong coupling cases. We
find that th... | quant-ph | we study the disentanglement of two spin qubits which interact with a general xy spinchain environment the dynamical process of the disentanglement is numerically and analytically investigated in the vicinity of quantum phase transition qpt of the spin chain in both weak and strong coupling cases we find that the disen... | [['we', 'study', 'the', 'disentanglement', 'of', 'two', 'spin', 'qubits', 'which', 'interact', 'with', 'a', 'general', 'xy', 'spinchain', 'environment', 'the', 'dynamical', 'process', 'of', 'the', 'disentanglement', 'is', 'numerically', 'and', 'analytically', 'investigated', 'in', 'the', 'vicinity', 'of', 'quantum', 'p... | [-0.18130185362421955, 0.18976139772984416, -0.048790184545772844, 0.0745726746168069, 0.01804641414095055, -0.15967576158811536, 0.03212697962251953, 0.3834704577386605, -0.24665112157982558, -0.2284084927253049, 0.06360248161122353, -0.2857190898297392, -0.13680098410883937, 0.15090141101091198, 0.07844409709702237, ... |
707.2847 | The massive star binary fraction in young open clusters I. NGC 6231
revisited | We present the results of a long-term high-resolution spectroscopy campaign
on the O-type stars in NGC 6231. We revise the spectral classification and
multiplicity of these objects and we constrain the fundamental properties of
the O-star population. Almost three quarters of the O-type stars in the cluster
are member... | astro-ph | we present the results of a longterm highresolution spectroscopy campaign on the otype stars in ngc 6231 we revise the spectral classification and multiplicity of these objects and we constrain the fundamental properties of the ostar population almost three quarters of the otype stars in the cluster are members of a bi... | [['we', 'present', 'the', 'results', 'of', 'a', 'longterm', 'highresolution', 'spectroscopy', 'campaign', 'on', 'the', 'otype', 'stars', 'in', 'ngc', '6231', 'we', 'revise', 'the', 'spectral', 'classification', 'and', 'multiplicity', 'of', 'these', 'objects', 'and', 'we', 'constrain', 'the', 'fundamental', 'properties'... | [-0.11420473597012461, 0.09795075734320563, -0.11464153566087286, 0.0787052492160971, -0.1249451442901045, -0.04068739297178885, 0.12436734517260144, 0.38130569798716657, -0.13561842781181135, -0.33429958126197257, 0.044573853485441454, -0.32092573973660665, -0.013483771948764722, 0.21099403937657674, -0.07922143635650... |
707.2848 | Prospects of inflation in delicate D-brane cosmology | We study D-brane inflation in a warped conifold background that includes
brane-position dependent corrections for the nonperturbative superpotential.
Instead of stabilizing the volume modulus chi at instantaneous minima of the
potential and studying the inflation dynamics with an effective single field
(radial distan... | hep-th astro-ph gr-qc hep-ph | we study dbrane inflation in a warped conifold background that includes braneposition dependent corrections for the nonperturbative superpotential instead of stabilizing the volume modulus chi at instantaneous minima of the potential and studying the inflation dynamics with an effective single field radial distance bet... | [['we', 'study', 'dbrane', 'inflation', 'in', 'a', 'warped', 'conifold', 'background', 'that', 'includes', 'braneposition', 'dependent', 'corrections', 'for', 'the', 'nonperturbative', 'superpotential', 'instead', 'of', 'stabilizing', 'the', 'volume', 'modulus', 'chi', 'at', 'instantaneous', 'minima', 'of', 'the', 'pot... | [-0.1617223211576999, 0.14760965693643863, -0.10275388069124677, 0.0966919186317967, -0.06392922019800558, -0.12444988104690742, -0.029266055709841202, 0.3017015201275662, -0.2217764346409709, -0.32841242261634374, 0.05671108399532856, -0.2309601765709676, -0.1190013774310685, 0.14709194997338415, -0.044176116431226375... |
707.2849 | Complete sums of products of (h,q)-extension of Euler numbers and
polynomials | In this paper we investigate some interesting of the (h,q)-extension of Euler
numbers and polynomials. Finally, we will give some relations between these
numbers anf polynomials
| math.NT | in this paper we investigate some interesting of the hqextension of euler numbers and polynomials finally we will give some relations between these numbers anf polynomials | [['in', 'this', 'paper', 'we', 'investigate', 'some', 'interesting', 'of', 'the', 'hqextension', 'of', 'euler', 'numbers', 'and', 'polynomials', 'finally', 'we', 'will', 'give', 'some', 'relations', 'between', 'these', 'numbers', 'anf', 'polynomials']] | [-0.29840127045575243, 0.12936002367104477, -0.1175892550784808, 0.1374136183115367, -0.09660737932874607, -0.08074500146680154, 0.030488373250521433, 0.31450642537898743, -0.32914828681028807, -0.2624761178516425, 0.09244443108596337, -0.23820681711479735, -0.27189115427721006, 0.2252079970561541, -0.10216627159836487... |
707.285 | Nuclear Georeactor Generation of Earth's Geomagnetic Field | The purpose of this communication is to suggest that the mechanism for
generating the geomagnetic field and the energy source for powering it are one
and the same, a nuclear georeactor at the center of the Earth. Toward this end,
I: i) Present evidence that the nuclear georeactor fission-product sub-shell is
fluid; i... | physics.geo-ph physics.gen-ph physics.space-ph | the purpose of this communication is to suggest that the mechanism for generating the geomagnetic field and the energy source for powering it are one and the same a nuclear georeactor at the center of the earth toward this end i i present evidence that the nuclear georeactor fissionproduct subshell is fluid iisuggest t... | [['the', 'purpose', 'of', 'this', 'communication', 'is', 'to', 'suggest', 'that', 'the', 'mechanism', 'for', 'generating', 'the', 'geomagnetic', 'field', 'and', 'the', 'energy', 'source', 'for', 'powering', 'it', 'are', 'one', 'and', 'the', 'same', 'a', 'nuclear', 'georeactor', 'at', 'the', 'center', 'of', 'the', 'eart... | [-0.0964481273000096, 0.19133543926519114, -0.05243308521103817, 0.13000930998298516, -0.06421594631734427, -0.07392166458864834, 0.019143177064500385, 0.3335068076327964, -0.22680961687143866, -0.29451212844440156, 0.06028096121898689, -0.23041071817018352, -0.07170716142347017, 0.19206612283637473, -0.010139381916789... |
707.2851 | Geometrical relations and plethysms in the Homfly skein of the annulus | The oriented framed Homfly skein C of the annulus provides the natural
parameter space for the Homfly satellite invariants of a knot. It contains a
submodule C+ isomorphic to the algebra of the symmetric functions.
We collect and expand formulae relating elements expressed in terms of
symmetric functions to Turaev'... | math.GT | the oriented framed homfly skein c of the annulus provides the natural parameter space for the homfly satellite invariants of a knot it contains a submodule c isomorphic to the algebra of the symmetric functions we collect and expand formulae relating elements expressed in terms of symmetric functions to turaevs geomet... | [['the', 'oriented', 'framed', 'homfly', 'skein', 'c', 'of', 'the', 'annulus', 'provides', 'the', 'natural', 'parameter', 'space', 'for', 'the', 'homfly', 'satellite', 'invariants', 'of', 'a', 'knot', 'it', 'contains', 'a', 'submodule', 'c', 'isomorphic', 'to', 'the', 'algebra', 'of', 'the', 'symmetric', 'functions', '... | [-0.20493100289625268, 0.06938204511191781, -0.08413127980175171, 0.03766960764414439, -0.09666696652202002, -0.14093039989973424, 0.016846138448537003, 0.30168677406742217, -0.3020957831148032, -0.26216208562915416, 0.05316054169171166, -0.2352133330101385, -0.17702149723306404, 0.19712180139642235, -0.091510624116194... |
707.2852 | Electron fishbones: Theory and experimental evidence | We discuss the processes underlying the excitation of fishbone-like internal
kink instabilities driven by supra-thermal electrons generated experimentally
by different means: Electron Cyclotron Resonance Heating (ECRH) and by Lower
Hybrid (LH) power injection. The peculiarity and interest of exciting these
electron f... | physics.plasm-ph | we discuss the processes underlying the excitation of fishbonelike internal kink instabilities driven by suprathermal electrons generated experimentally by different means electron cyclotron resonance heating ecrh and by lower hybrid lh power injection the peculiarity and interest of exciting these electron fishbones b... | [['we', 'discuss', 'the', 'processes', 'underlying', 'the', 'excitation', 'of', 'fishbonelike', 'internal', 'kink', 'instabilities', 'driven', 'by', 'suprathermal', 'electrons', 'generated', 'experimentally', 'by', 'different', 'means', 'electron', 'cyclotron', 'resonance', 'heating', 'ecrh', 'and', 'by', 'lower', 'hyb... | [-0.1290713284373958, 0.3051080706303337, 0.016414285303172245, 0.0986689057388182, -0.016252076237887034, -0.15964835084399537, 0.01595289161452777, 0.33599962442017656, -0.24416918238378404, -0.2938373038846561, 0.04490607672264827, -0.2492770392255967, -0.062014150544521675, 0.23798246543019025, 0.013896067371687797... |
707.2853 | Phase transition in the maximum clique problem: the case of Erdos-Renyi
graphs | A phase transition, like the one already found on Boolean satisfiability
problem by Kirkpatrick and Selman, is found on max clique problem on ER graphs.
Although number of the datapoints is limited, the transition seems to obey
finite size scaling. The transition also shows concentration of the graph
instances which ... | cond-mat.stat-mech | a phase transition like the one already found on boolean satisfiability problem by kirkpatrick and selman is found on max clique problem on er graphs although number of the datapoints is limited the transition seems to obey finite size scaling the transition also shows concentration of the graph instances which need pa... | [['a', 'phase', 'transition', 'like', 'the', 'one', 'already', 'found', 'on', 'boolean', 'satisfiability', 'problem', 'by', 'kirkpatrick', 'and', 'selman', 'is', 'found', 'on', 'max', 'clique', 'problem', 'on', 'er', 'graphs', 'although', 'number', 'of', 'the', 'datapoints', 'is', 'limited', 'the', 'transition', 'seems... | [-0.09068753766386133, 0.1143328937652864, -0.021465085218088667, 0.07990977310640901, -0.12332181116206604, -0.1731397661119046, 0.10588295656468785, 0.3324724772062741, -0.26090378931870584, -0.37285822401182694, 0.11621199837444644, -0.2959991282816127, -0.09919770271925811, 0.14482028850991474, -0.06282740339571447... |
707.2854 | Boost invariance of the gravitational field dynamics: quantization
without time gauge | We perform a canonical quantization of gravity in a second-order formulation,
taking as configuration variables those describing a 4-bein, not adapted to the
space-time splitting. We outline how, neither if we fix the Lorentz frame
before quantizing, nor if we perform no gauge fixing at all, is invariance
under boost... | gr-qc | we perform a canonical quantization of gravity in a secondorder formulation taking as configuration variables those describing a 4bein not adapted to the spacetime splitting we outline how neither if we fix the lorentz frame before quantizing nor if we perform no gauge fixing at all is invariance under boost transforma... | [['we', 'perform', 'a', 'canonical', 'quantization', 'of', 'gravity', 'in', 'a', 'secondorder', 'formulation', 'taking', 'as', 'configuration', 'variables', 'those', 'describing', 'a', '4bein', 'not', 'adapted', 'to', 'the', 'spacetime', 'splitting', 'we', 'outline', 'how', 'neither', 'if', 'we', 'fix', 'the', 'lorentz... | [-0.1465609581802379, 0.15511297713965178, -0.12391067974756217, 0.09725838379130106, -0.12445526623421095, -0.17406206958165224, 0.04072873797691004, 0.4009258748794144, -0.21630810704928907, -0.26036440655589105, 0.06459958238146184, -0.17350969013165343, -0.16205841000615195, 0.08736580495129932, -0.0929248975928534... |
707.2855 | Non-planar structure of analytical QCD predictions for the Gottfried sum
rule | It is stressed that within large N_c-expansion {\bf analytical calculations}
of the $(\alpha_s/\pi)^2$ QCD contributions to the valence part of the
Gottfried sum rule for F_2 structure function of charged leptons-nucleon
deep-inelastic scattering reveals the existence of the $O(1/N_c^2)$ {\bf
non-planar} corrections ... | hep-ph hep-ex hep-th | it is stressed that within large n_cexpansion bf analytical calculations of the alpha_spi2 qcd contributions to the valence part of the gottfried sum rule for f_2 structure function of charged leptonsnucleon deepinelastic scattering reveals the existence of the o1n_c2 bf nonplanar corrections only and the disappearance... | [['it', 'is', 'stressed', 'that', 'within', 'large', 'n_cexpansion', 'bf', 'analytical', 'calculations', 'of', 'the', 'alpha_spi2', 'qcd', 'contributions', 'to', 'the', 'valence', 'part', 'of', 'the', 'gottfried', 'sum', 'rule', 'for', 'f_2', 'structure', 'function', 'of', 'charged', 'leptonsnucleon', 'deepinelastic', ... | [-0.12827448488427526, 0.1647628211247125, -0.058760887599824896, 0.11819713408036975, -0.06367401854074795, -0.028848057240080223, 0.06481805019308444, 0.3079577967283323, -0.21497407363955495, -0.21035857943536565, -0.011191140373719842, -0.309485839545834, -0.08366412311191872, 0.09477463141318224, 0.072222109360573... |
707.2856 | The Oxygen Abundance of Nearby Galaxies from Sloan Digital Sky Survey
Spectra | We have derived the oxygen abundance for a sample of nearby galaxies in the
Data Release 5 of the Sloan Digital Sky Survey (SDSS) which possess at least
two independent spectra of one or several HII regions with a detected
[OIII]4363 auroral line. Since, for nearby galaxies, the [OII]3727 nebular line
is out of the o... | astro-ph | we have derived the oxygen abundance for a sample of nearby galaxies in the data release 5 of the sloan digital sky survey sdss which possess at least two independent spectra of one or several hii regions with a detected oiii4363 auroral line since for nearby galaxies the oii3727 nebular line is out of the observed wav... | [['we', 'have', 'derived', 'the', 'oxygen', 'abundance', 'for', 'a', 'sample', 'of', 'nearby', 'galaxies', 'in', 'the', 'data', 'release', '5', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'which', 'possess', 'at', 'least', 'two', 'independent', 'spectra', 'of', 'one', 'or', 'several', 'hii', 'regions', 'w... | [-0.027782711593394793, 0.044971566726133304, -0.01329535847312953, 0.03578797938479554, -0.029173232872462856, -0.06299890180625928, 0.059480243364950176, 0.4494013501153815, -0.12448444972395288, -0.34013452699220686, 0.027837278483381307, -0.30549271654081406, 0.006493378717639537, 0.21366466834116235, 0.00783086269... |
707.2857 | Coronal abundances of X-ray bright pre-main sequence stars in the Taurus
Molecular Cloud | We studied the thermal properties and chemical composition of the X-ray
emitting plasma of a sample of bright members of the Taurus Molecular Cloud to
investigate possible differences among classical and weak-lined T Tauri stars
and possible dependences of the abundances on the stellar activity level and/or
on the pr... | astro-ph | we studied the thermal properties and chemical composition of the xray emitting plasma of a sample of bright members of the taurus molecular cloud to investigate possible differences among classical and weaklined t tauri stars and possible dependences of the abundances on the stellar activity level andor on the presenc... | [['we', 'studied', 'the', 'thermal', 'properties', 'and', 'chemical', 'composition', 'of', 'the', 'xray', 'emitting', 'plasma', 'of', 'a', 'sample', 'of', 'bright', 'members', 'of', 'the', 'taurus', 'molecular', 'cloud', 'to', 'investigate', 'possible', 'differences', 'among', 'classical', 'and', 'weaklined', 't', 'tau... | [-0.012361324257149368, 0.1537558296309248, -0.027810567993344398, 0.07767670754093446, -0.052810737273883565, -0.07875116403472956, 0.08417073343845423, 0.44634894589404067, -0.1482848772561572, -0.40586657659596775, 0.018952389206077877, -0.345190298478425, 0.01786015682979521, 0.18710677534508363, -0.037605711575903... |
707.2858 | Spheroidal and elliptical galaxy radial velocity dispersion determined
from Cosmological General Relativity | Radial velocity dispersion in spheroidal and elliptical galaxies, as a
function of radial distance from the center of the galaxy, has been derived
from Cosmological Special Relativity. For velocity dispersions in the outer
regions of spherical galaxies, the dynamical mass calculated for a galaxy using
Carmelian theor... | physics.gen-ph | radial velocity dispersion in spheroidal and elliptical galaxies as a function of radial distance from the center of the galaxy has been derived from cosmological special relativity for velocity dispersions in the outer regions of spherical galaxies the dynamical mass calculated for a galaxy using carmelian theory may ... | [['radial', 'velocity', 'dispersion', 'in', 'spheroidal', 'and', 'elliptical', 'galaxies', 'as', 'a', 'function', 'of', 'radial', 'distance', 'from', 'the', 'center', 'of', 'the', 'galaxy', 'has', 'been', 'derived', 'from', 'cosmological', 'special', 'relativity', 'for', 'velocity', 'dispersions', 'in', 'the', 'outer',... | [-0.039066475893368306, 0.09738039597509034, -0.14663872630986316, 0.0823201580055719, -0.08900031957134444, -0.04788928459553669, -0.05682671656556708, 0.3960161568967485, -0.1932542363622336, -0.3441397570754572, 0.015525685370429069, -0.2573655826935885, 0.01123226020405049, 0.2478117620352135, 0.011872096532349906,... |
707.2859 | A Clifford analysis approach to superspace | A new framework for studying superspace is given, based on methods from
Clifford analysis. This leads to the introduction of both orthogonal and
symplectic Clifford algebra generators, allowing for an easy and canonical
introduction of a super-Dirac operator, a super-Laplace operator and the like.
This framework is t... | hep-th math-ph math.MP | a new framework for studying superspace is given based on methods from clifford analysis this leads to the introduction of both orthogonal and symplectic clifford algebra generators allowing for an easy and canonical introduction of a superdirac operator a superlaplace operator and the like this framework is then used ... | [['a', 'new', 'framework', 'for', 'studying', 'superspace', 'is', 'given', 'based', 'on', 'methods', 'from', 'clifford', 'analysis', 'this', 'leads', 'to', 'the', 'introduction', 'of', 'both', 'orthogonal', 'and', 'symplectic', 'clifford', 'algebra', 'generators', 'allowing', 'for', 'an', 'easy', 'and', 'canonical', 'i... | [-0.10109947551516633, 0.02860888872451409, -0.15027120098352945, 0.08176569905766633, -0.1565261519167061, -0.10873261130159247, -0.0130124385948019, 0.30583651243325544, -0.28686400871796935, -0.23690733434997646, 0.12752746931601353, -0.23024775739759207, -0.1928370722076472, 0.17381572746215204, -0.1153449790995093... |
707.286 | Dimensional Reduction and the Yang-Mills Vacuum State in 2+1 Dimensions | We propose an approximation to the ground state of Yang-Mills theory,
quantized in temporal gauge and 2+1 dimensions, which satisfies the Yang-Mills
Schrodinger equation in both the free-field limit, and in a strong-field zero
mode limit. Our proposal contains a single parameter with dimensions of mass;
confinement v... | hep-lat hep-th | we propose an approximation to the ground state of yangmills theory quantized in temporal gauge and 21 dimensions which satisfies the yangmills schrodinger equation in both the freefield limit and in a strongfield zero mode limit our proposal contains a single parameter with dimensions of mass confinement via dimension... | [['we', 'propose', 'an', 'approximation', 'to', 'the', 'ground', 'state', 'of', 'yangmills', 'theory', 'quantized', 'in', 'temporal', 'gauge', 'and', '21', 'dimensions', 'which', 'satisfies', 'the', 'yangmills', 'schrodinger', 'equation', 'in', 'both', 'the', 'freefield', 'limit', 'and', 'in', 'a', 'strongfield', 'zero... | [-0.09802761257366999, 0.17734858692652308, -0.06576971738268772, 0.04166973191369776, -0.022894904687775358, -0.1288906478646001, 0.044280811771562685, 0.3220881087341226, -0.19825169259603437, -0.29016070794915, 0.07709078573726959, -0.24905073321274213, -0.08262681445827888, 0.15588807308250258, -0.01003480361091093... |
707.2861 | Soliton oscillations in collisionally inhomogeneous attractive
Bose-Einstein condensates | We investigate bright matter-wave solitons in the presence of a spatially
varying nonlinearity. It is demonstrated that a translation mode is excited due
to the spatial inhomogeneity and its frequency is derived analytically and also
studied numerically. Both cases of purely one-dimensional and ``cigar-shaped''
conde... | cond-mat.other | we investigate bright matterwave solitons in the presence of a spatially varying nonlinearity it is demonstrated that a translation mode is excited due to the spatial inhomogeneity and its frequency is derived analytically and also studied numerically both cases of purely onedimensional and cigarshaped condensates are ... | [['we', 'investigate', 'bright', 'matterwave', 'solitons', 'in', 'the', 'presence', 'of', 'a', 'spatially', 'varying', 'nonlinearity', 'it', 'is', 'demonstrated', 'that', 'a', 'translation', 'mode', 'is', 'excited', 'due', 'to', 'the', 'spatial', 'inhomogeneity', 'and', 'its', 'frequency', 'is', 'derived', 'analyticall... | [-0.13055416348359505, 0.12896219090071517, -0.05374211769807955, 0.09116717018909624, 0.0031326189262514143, -0.14891512646478997, -0.02292761066393263, 0.41159364463354664, -0.20301010540483155, -0.26188713523034735, 0.1016770979073755, -0.2585749745237823, -0.1436131341307927, 0.2232499472721983, 0.02092234047408076... |
707.2862 | Fundamental solutions for the super Laplace and Dirac operators and all
their natural powers | The fundamental solutions of the super Dirac and Laplace operators and their
natural powers are determined within the framework of Clifford analysis.
| math.AP hep-th | the fundamental solutions of the super dirac and laplace operators and their natural powers are determined within the framework of clifford analysis | [['the', 'fundamental', 'solutions', 'of', 'the', 'super', 'dirac', 'and', 'laplace', 'operators', 'and', 'their', 'natural', 'powers', 'are', 'determined', 'within', 'the', 'framework', 'of', 'clifford', 'analysis']] | [-0.10306659036061981, 0.1101481814614751, -0.02450180561705069, 0.09947447817433965, -0.05552110110875219, -0.06956792140210216, 0.03472022686830976, 0.2939789594913071, -0.2858173765919425, -0.28023945447057486, 0.14982228192754768, -0.2824463028968735, -0.19117429725487123, 0.19986435275694187, -0.015207417277534578... |
707.2863 | Hermite and Gegenbauer polynomials in superspace using Clifford analysis | The Clifford-Hermite and the Clifford-Gegenbauer polynomials of standard
Clifford analysis are generalized to the new framework of Clifford analysis in
superspace in a merely symbolic way. This means that one does not a priori need
an integration theory in superspace. Furthermore a lot of basic properties,
such as or... | hep-th math.CA | the cliffordhermite and the cliffordgegenbauer polynomials of standard clifford analysis are generalized to the new framework of clifford analysis in superspace in a merely symbolic way this means that one does not a priori need an integration theory in superspace furthermore a lot of basic properties such as orthogona... | [['the', 'cliffordhermite', 'and', 'the', 'cliffordgegenbauer', 'polynomials', 'of', 'standard', 'clifford', 'analysis', 'are', 'generalized', 'to', 'the', 'new', 'framework', 'of', 'clifford', 'analysis', 'in', 'superspace', 'in', 'a', 'merely', 'symbolic', 'way', 'this', 'means', 'that', 'one', 'does', 'not', 'a', 'p... | [-0.11392130734480145, 0.05689604397919443, -0.10465194411134641, 0.10479504778662599, -0.15763945409439897, -0.12132940216504626, 0.0005427251775185333, 0.30645549527712557, -0.29339836709397404, -0.25202864832489896, 0.12091306378409315, -0.22277557602348297, -0.23542808148225672, 0.22419168057508373, -0.127869625781... |
707.2864 | Search for the lightest scalar top quark in events with two leptons in
p-pbar collisions at sqrt(s) = 1.96 TeV | Data collected by the D0 detector at a p-pbar center-of-mass energy of 1.96
TeV at the Fermilab Tevatron Collider have been used to search for pair
production of the lightest supersymmetric partner of the top quark decaying
into $b \ell \tilde{\nu}$. The search is performed in the $\ell\ell' = e\mu$
and $\mu \mu$ fin... | hep-ex | data collected by the d0 detector at a ppbar centerofmass energy of 196 tev at the fermilab tevatron collider have been used to search for pair production of the lightest supersymmetric partner of the top quark decaying into b ell tildenu the search is performed in the ellell emu and mu mu final states no evidence for ... | [['data', 'collected', 'by', 'the', 'd0', 'detector', 'at', 'a', 'ppbar', 'centerofmass', 'energy', 'of', '196', 'tev', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'have', 'been', 'used', 'to', 'search', 'for', 'pair', 'production', 'of', 'the', 'lightest', 'supersymmetric', 'partner', 'of', 'the', 'top', 'quark',... | [-0.043389767042005103, 0.2164757223909392, -0.07852126115604359, 0.1277628221639187, -0.022166775345035337, -0.14313473722842687, 0.07138485568027725, 0.29711308545323417, -0.1656666661229204, -0.349702947455294, 0.014791411143618033, -0.39694991178043626, 0.16372977762537844, 0.127661197287414, 0.162839286686743, 0.1... |
707.2865 | A Chandra study of particle acceleration in the multiple hotspots of
nearby radio galaxies | We present Chandra observations of a small sample of nearby classical double
radio galaxies which have more than one radio hotspot in at least one of their
lobes. The X-ray emission from the hotspots of these comparatively low-power
objects is expected to be synchrotron in origin, and therefore to provide
information... | astro-ph | we present chandra observations of a small sample of nearby classical double radio galaxies which have more than one radio hotspot in at least one of their lobes the xray emission from the hotspots of these comparatively lowpower objects is expected to be synchrotron in origin and therefore to provide information about... | [['we', 'present', 'chandra', 'observations', 'of', 'a', 'small', 'sample', 'of', 'nearby', 'classical', 'double', 'radio', 'galaxies', 'which', 'have', 'more', 'than', 'one', 'radio', 'hotspot', 'in', 'at', 'least', 'one', 'of', 'their', 'lobes', 'the', 'xray', 'emission', 'from', 'the', 'hotspots', 'of', 'these', 'co... | [-0.061208831624588296, 0.15375128361020787, -0.08482162517347289, 0.13921826860843628, -0.10475815316154198, -0.11334090150987984, 0.0437095543139466, 0.46580798335542734, -0.22509895101591776, -0.3091348976489495, 0.06699405270178845, -0.2865994968134063, -0.02086013671545185, 0.22195256913520015, 0.00445624577431854... |
707.2866 | Magnetic-glassy multicritical behavior of the three-dimensional +- J
Ising model | We consider the three-dimensional $\pm J$ model defined on a simple cubic
lattice and study its behavior close to the multicritical Nishimori point where
the paramagnetic-ferromagnetic, the paramagnetic-glassy, and the
ferromagnetic-glassy transition lines meet in the T-p phase diagram (p
characterizes the disorder d... | cond-mat.dis-nn | we consider the threedimensional pm j model defined on a simple cubic lattice and study its behavior close to the multicritical nishimori point where the paramagneticferromagnetic the paramagneticglassy and the ferromagneticglassy transition lines meet in the tp phase diagram p characterizes the disorder distribution a... | [['we', 'consider', 'the', 'threedimensional', 'pm', 'j', 'model', 'defined', 'on', 'a', 'simple', 'cubic', 'lattice', 'and', 'study', 'its', 'behavior', 'close', 'to', 'the', 'multicritical', 'nishimori', 'point', 'where', 'the', 'paramagneticferromagnetic', 'the', 'paramagneticglassy', 'and', 'the', 'ferromagneticgla... | [-0.1786998961915207, 0.14112462870338383, -0.08081638036288924, 0.02948771555469755, 0.00959272108722122, -0.1740811650935725, 0.128048680120093, 0.3556715025787365, -0.21528081709573813, -0.20681204355787486, 0.06294634868990055, -0.3617405220215647, -0.12998361174092732, 0.14077293570667013, 0.07583968657640713, 0.0... |
707.2867 | Quadratic Deformations of Lie-Poisson Structures | In this letter, first we give a decomposition for any Lie-Poisson structure
$\pi_g$ associated to the modular vector. In particular, $\pi_g$ splits into
two compatible Lie-Poisson structures if $dim{g} \leq 3$. As an application, we
classified quadratic deformations of Lie-Poisson structures on $\mathbb R^3$ up
to li... | math.DG math-ph math.MP | in this letter first we give a decomposition for any liepoisson structure pi_g associated to the modular vector in particular pi_g splits into two compatible liepoisson structures if dimg leq 3 as an application we classified quadratic deformations of liepoisson structures on mathbb r3 up to linear diffeomorphisms | [['in', 'this', 'letter', 'first', 'we', 'give', 'a', 'decomposition', 'for', 'any', 'liepoisson', 'structure', 'pi_g', 'associated', 'to', 'the', 'modular', 'vector', 'in', 'particular', 'pi_g', 'splits', 'into', 'two', 'compatible', 'liepoisson', 'structures', 'if', 'dimg', 'leq', '3', 'as', 'an', 'application', 'we'... | [-0.21503526521458602, 0.09803427323428575, -0.026782571687363088, 0.027248840686903957, -0.12700345161526153, -0.11760189268776837, -0.08628630209326123, 0.3799021258018911, -0.3768788605229929, -0.1675702814827673, 0.06274951817370795, -0.2342839456978254, -0.19775841039760658, 0.14778173952557458, -0.077487960108555... |
707.2868 | Constructing quantum games from non-factorizable joint probabilities | A probabilistic framework is developed that gives a unifying perspective on
both the classical and the quantum games. We suggest exploiting peculiar
probabilities involved in Einstein-Podolsky-Rosen (EPR) experiments to
construct quantum games. In our framework a game attains classical
interpretation when joint proba... | quant-ph | a probabilistic framework is developed that gives a unifying perspective on both the classical and the quantum games we suggest exploiting peculiar probabilities involved in einsteinpodolskyrosen epr experiments to construct quantum games in our framework a game attains classical interpretation when joint probabilities... | [['a', 'probabilistic', 'framework', 'is', 'developed', 'that', 'gives', 'a', 'unifying', 'perspective', 'on', 'both', 'the', 'classical', 'and', 'the', 'quantum', 'games', 'we', 'suggest', 'exploiting', 'peculiar', 'probabilities', 'involved', 'in', 'einsteinpodolskyrosen', 'epr', 'experiments', 'to', 'construct', 'qu... | [-0.06744549807048805, 0.08082929067974183, -0.18259571593069862, 0.1879324920422642, -0.014331502671492226, -0.23232203306207524, 0.11852490635430242, 0.3724444342169462, -0.23865959154613686, -0.2446486250404929, 0.0050097351979649235, -0.24366483813587655, -0.21548371598230187, 0.0634414114723484, -0.166316699705595... |
707.2869 | Clifford Algebras and Possible Kinematics | We review Bacry and Levy-Leblond's work on possible kinematics as applied to
2-dimensional spacetimes, as well as the nine types of 2-dimensional
Cayley-Klein geometries, illustrating how the Cayley-Klein geometries give
homogeneous spacetimes for all but one of the kinematical groups. We then
construct a two-paramet... | math-ph math.MP math.RT | we review bacry and levyleblonds work on possible kinematics as applied to 2dimensional spacetimes as well as the nine types of 2dimensional cayleyklein geometries illustrating how the cayleyklein geometries give homogeneous spacetimes for all but one of the kinematical groups we then construct a twoparameter family of... | [['we', 'review', 'bacry', 'and', 'levyleblonds', 'work', 'on', 'possible', 'kinematics', 'as', 'applied', 'to', '2dimensional', 'spacetimes', 'as', 'well', 'as', 'the', 'nine', 'types', 'of', '2dimensional', 'cayleyklein', 'geometries', 'illustrating', 'how', 'the', 'cayleyklein', 'geometries', 'give', 'homogeneous', ... | [-0.08720689216707216, 0.06910434278872717, -0.07013249315366328, 0.12765543721616268, -0.09948157957553055, -0.1491085956187313, -0.05525593344312924, 0.40973860985902416, -0.20835909051596221, -0.2638687644580222, 0.1266161816023537, -0.1946942750364542, -0.1685683310301189, 0.24187274009595255, -0.08206157972026303,... |
707.287 | Linear Poisson structures on R^4 | We classify all of the 4-dimensional linear Poisson structures of which the
corresponding Lie algebras can be considered as the extension by a derivation
of 3-dimensional unimodular Lie algebras. The affine Poisson structures on R^3
are totally classified.
| math.DG math-ph math.MP | we classify all of the 4dimensional linear poisson structures of which the corresponding lie algebras can be considered as the extension by a derivation of 3dimensional unimodular lie algebras the affine poisson structures on r3 are totally classified | [['we', 'classify', 'all', 'of', 'the', '4dimensional', 'linear', 'poisson', 'structures', 'of', 'which', 'the', 'corresponding', 'lie', 'algebras', 'can', 'be', 'considered', 'as', 'the', 'extension', 'by', 'a', 'derivation', 'of', '3dimensional', 'unimodular', 'lie', 'algebras', 'the', 'affine', 'poisson', 'structure... | [-0.17456468126099361, 0.06611024108899169, -0.024993995302601865, 0.07989340498553295, -0.1785077014692912, -0.12125712242222537, -0.10922915021901165, 0.3642187727811305, -0.3595993911945506, -0.18043761825385063, 0.1661408264557586, -0.19633309699987112, -0.20430538764125422, 0.17688755865061753, -0.0948968554393535... |
707.2871 | Theory of Weiss oscillations in the magnetoplasmon spectrum of Dirac
electrons in graphene | We present the collective excitations spectrum (magnetoplasmon spectrum) of
Dirac electrons in a weakly modulated single graphene layer in the presence
of a uniform magnetic field. We consider electric modulation in one-dimension
and the magnetic field applied perpendicular to graphene.We derive analytical
results ... | cond-mat.mes-hall | we present the collective excitations spectrum magnetoplasmon spectrum of dirac electrons in a weakly modulated single graphene layer in the presence of a uniform magnetic field we consider electric modulation in onedimension and the magnetic field applied perpendicular to graphenewe derive analytical results for the i... | [['we', 'present', 'the', 'collective', 'excitations', 'spectrum', 'magnetoplasmon', 'spectrum', 'of', 'dirac', 'electrons', 'in', 'a', 'weakly', 'modulated', 'single', 'graphene', 'layer', 'in', 'the', 'presence', 'of', 'a', 'uniform', 'magnetic', 'field', 'we', 'consider', 'electric', 'modulation', 'in', 'onedimensio... | [-0.20350377252768903, 0.18825824080877715, -0.029870649389479132, 0.05942762626468071, -0.029395566329300876, -0.09880727872119419, 0.017718671715729647, 0.3993029977889761, -0.22481938782018712, -0.2911775279402112, -0.01980978291433689, -0.28262262721915565, -0.15485919949909052, 0.2215174208487576, 0.02295153680634... |
707.2872 | Cluster simulation of relativistic fermions in two space-time dimensions | For Majorana-Wilson lattice fermions in two dimensions we derive a dimer
representation. This is equivalent to Gattringer's loop representation, but is
made exact here on the torus. A subsequent dual mapping leads to yet another
representation in which a highly efficient Swendsen-Wang type cluster algorithm
is constr... | hep-lat cond-mat.stat-mech hep-th | for majoranawilson lattice fermions in two dimensions we derive a dimer representation this is equivalent to gattringers loop representation but is made exact here on the torus a subsequent dual mapping leads to yet another representation in which a highly efficient swendsenwang type cluster algorithm is constructed it... | [['for', 'majoranawilson', 'lattice', 'fermions', 'in', 'two', 'dimensions', 'we', 'derive', 'a', 'dimer', 'representation', 'this', 'is', 'equivalent', 'to', 'gattringers', 'loop', 'representation', 'but', 'is', 'made', 'exact', 'here', 'on', 'the', 'torus', 'a', 'subsequent', 'dual', 'mapping', 'leads', 'to', 'yet', ... | [-0.11352880264166743, 0.15659758633023074, -0.10214767694978559, 0.11288168394512081, -0.11490518211862667, -0.19232194249003015, 0.03262225144785492, 0.4248248400919615, -0.20238251740142624, -0.2690582617156287, 0.10079613143325526, -0.2313371315337482, -0.16217385219568584, 0.19756969947496705, -0.02171862566784183... |
707.2873 | On the Orbits of Solvable Linear Groups | Let $G$ be a solvable linear group acting on the finite vectorpace $V$ and
assume that $(|G|,|V|)=1$. In this paper we find $x,y\in V$ such that
$C_G(x)\cap C_G(y)=1$. In particular, this answers a question of I. M. Isaacs.
We complete some results of S. Dolphi, A. Seress and T. R. Wolf.
| math.GR | let g be a solvable linear group acting on the finite vectorpace v and assume that gv1 in this paper we find xyin v such that c_gxcap c_gy1 in particular this answers a question of i m isaacs we complete some results of s dolphi a seress and t r wolf | [['let', 'g', 'be', 'a', 'solvable', 'linear', 'group', 'acting', 'on', 'the', 'finite', 'vectorpace', 'v', 'and', 'assume', 'that', 'gv1', 'in', 'this', 'paper', 'we', 'find', 'xyin', 'v', 'such', 'that', 'c_gxcap', 'c_gy1', 'in', 'particular', 'this', 'answers', 'a', 'question', 'of', 'i', 'm', 'isaacs', 'we', 'compl... | [-0.1839431906118989, 0.11240426545112353, -0.06267596873373765, -0.040832745503512735, -0.10239128452857309, -0.18500415718628335, 0.06808962558811206, 0.3563911792538736, -0.28162510061393614, -0.22003018507814925, 0.04756599000108469, -0.2867632751231608, -0.15391911597639, 0.15348649296767847, -0.1142444621629851, ... |
707.2874 | Giant fluctuations of topological charge in a disordered wave guide | We study the fluctuations of the total topological charge of a scalar wave
propagating in a hollow conducting wave guide filled with scatterers inside. We
investigate the dependence of the screening on the scattering mean free path
and on the presence of boundaries. Near the cut-off frequencies of the wave
guide, scr... | cond-mat.other | we study the fluctuations of the total topological charge of a scalar wave propagating in a hollow conducting wave guide filled with scatterers inside we investigate the dependence of the screening on the scattering mean free path and on the presence of boundaries near the cutoff frequencies of the wave guide screening... | [['we', 'study', 'the', 'fluctuations', 'of', 'the', 'total', 'topological', 'charge', 'of', 'a', 'scalar', 'wave', 'propagating', 'in', 'a', 'hollow', 'conducting', 'wave', 'guide', 'filled', 'with', 'scatterers', 'inside', 'we', 'investigate', 'the', 'dependence', 'of', 'the', 'screening', 'on', 'the', 'scattering', ... | [-0.21231971089154072, 0.2513852697120954, -0.03896791326545485, 0.06758909318628019, -0.04156967776840272, -0.039142451287336545, 0.04021419533400809, 0.33533112462354847, -0.23096741217966765, -0.2631398177106086, 0.057485745471825646, -0.3480012647246253, -0.11613545703306181, 0.10702462627054894, 0.0466521543272043... |
707.2875 | Quantum transport in noncentrosymmetric superconductors and
thermodynamics of ferromagnetic superconductors | We consider a general Hamiltonian describing coexistence of itinerant
ferromagnetism, spin-orbit coupling and mixed spin-singlet/triplet
superconducting pairing in the context of mean-field theory. The Hamiltonian is
diagonalized and exact eigenvalues are obtained, thus allowing us to write down
the coupled gap equat... | cond-mat.supr-con | we consider a general hamiltonian describing coexistence of itinerant ferromagnetism spinorbit coupling and mixed spinsinglettriplet superconducting pairing in the context of meanfield theory the hamiltonian is diagonalized and exact eigenvalues are obtained thus allowing us to write down the coupled gap equations for ... | [['we', 'consider', 'a', 'general', 'hamiltonian', 'describing', 'coexistence', 'of', 'itinerant', 'ferromagnetism', 'spinorbit', 'coupling', 'and', 'mixed', 'spinsinglettriplet', 'superconducting', 'pairing', 'in', 'the', 'context', 'of', 'meanfield', 'theory', 'the', 'hamiltonian', 'is', 'diagonalized', 'and', 'exact... | [-0.18461132953187104, 0.15013751451225227, -0.03166157661309076, 0.08100633562845719, -0.08108622976578772, -0.18092586708060185, 0.09350017052804402, 0.32774205253903516, -0.2428016969999082, -0.29352432903725395, 0.027147029717127943, -0.3007285213661055, -0.10528225638946995, 0.1496944477045259, 0.03516399361366449... |
707.2876 | Shack-Hartmann sensor improvement using optical binning | We present a design improvement for a recently proposed type of
Shack-Hartmann wavefront sensor that uses a cylindrical (lenticular) lenslet
array. The improved sensor design uses optical binning and requires
significantly fewer detector pixels than the corresponding conventional or
cylindrical Shack-Hartmann sensor,... | physics.optics physics.ins-det | we present a design improvement for a recently proposed type of shackhartmann wavefront sensor that uses a cylindrical lenticular lenslet array the improved sensor design uses optical binning and requires significantly fewer detector pixels than the corresponding conventional or cylindrical shackhartmann sensor and so ... | [['we', 'present', 'a', 'design', 'improvement', 'for', 'a', 'recently', 'proposed', 'type', 'of', 'shackhartmann', 'wavefront', 'sensor', 'that', 'uses', 'a', 'cylindrical', 'lenticular', 'lenslet', 'array', 'the', 'improved', 'sensor', 'design', 'uses', 'optical', 'binning', 'and', 'requires', 'significantly', 'fewer... | [-0.10150471277302131, 0.03800278019688059, -0.057831838760258894, 0.00905060932771968, -0.10049742402458962, -0.2326609087550813, -0.010136618031538092, 0.46533444044845446, -0.16579840595555392, -0.3573313925215708, 0.1312878709400788, -0.2744685650478849, -0.1720892613209019, 0.2620830193918664, -0.14662662832831433... |
707.2877 | Voronoi Tessellations and the Cosmic Web: Spatial Patterns and
Clustering across the Universe | The spatial cosmic matter distribution on scales of a few up to more than a
hundred Megaparsec displays a salient and pervasive foamlike pattern. Voronoi
tessellations are a versatile and flexible mathematical model for such weblike
spatial patterns. They would be the natural asymptotic result of an evolution
in whic... | astro-ph | the spatial cosmic matter distribution on scales of a few up to more than a hundred megaparsec displays a salient and pervasive foamlike pattern voronoi tessellations are a versatile and flexible mathematical model for such weblike spatial patterns they would be the natural asymptotic result of an evolution in which lo... | [['the', 'spatial', 'cosmic', 'matter', 'distribution', 'on', 'scales', 'of', 'a', 'few', 'up', 'to', 'more', 'than', 'a', 'hundred', 'megaparsec', 'displays', 'a', 'salient', 'and', 'pervasive', 'foamlike', 'pattern', 'voronoi', 'tessellations', 'are', 'a', 'versatile', 'and', 'flexible', 'mathematical', 'model', 'for... | [-0.1089104699682616, 0.11679600634144005, -0.13656530420276078, 0.11797102009431716, -0.06531556227561483, -0.043075331206043774, -0.009640185492681273, 0.37712762040475795, -0.2586594243659407, -0.3217540623765465, 0.03325201979019276, -0.2582201900816001, -0.12080001536135872, 0.13696044048538814, 0.0047673618186476... |
707.2878 | Determining the CP properties of the Higgs boson | The search and the probe of the fundamental properties of Higgs boson(s) and,
in particular, the determination of their charge conjugation and parity (CP)
quantum numbers, is one of the main tasks of future high-energy colliders. We
demonstrate that the CP properties of a Standard Model-like Higgs particle can
be una... | hep-ph | the search and the probe of the fundamental properties of higgs bosons and in particular the determination of their charge conjugation and parity cp quantum numbers is one of the main tasks of future highenergy colliders we demonstrate that the cp properties of a standard modellike higgs particle can be unambiguously a... | [['the', 'search', 'and', 'the', 'probe', 'of', 'the', 'fundamental', 'properties', 'of', 'higgs', 'bosons', 'and', 'in', 'particular', 'the', 'determination', 'of', 'their', 'charge', 'conjugation', 'and', 'parity', 'cp', 'quantum', 'numbers', 'is', 'one', 'of', 'the', 'main', 'tasks', 'of', 'future', 'highenergy', 'c... | [-0.10954787201764113, 0.24171962806753614, -0.0660086241204644, 0.1194792139498089, -0.04199137532378774, -0.14801805808108198, 0.049416479311656915, 0.29498704809796167, -0.265162674137517, -0.28258289067653586, -0.003071777313330991, -0.2976961545772045, 0.007266240420977812, 0.16083974745344823, 0.09030177583917975... |
707.2879 | Spin injection and relaxation in a mesoscopic superconductor | We study spin accumulation and spin relaxation in a superconducting nanowire.
Spins are injected and detected by using a set of magnetic tunnel contact
electrodes, closely spaced along the nanowire. We observe a giant enhancement
of the spin accumulation of up to five orders of magnitude on transition into
the superc... | cond-mat.mes-hall cond-mat.supr-con | we study spin accumulation and spin relaxation in a superconducting nanowire spins are injected and detected by using a set of magnetic tunnel contact electrodes closely spaced along the nanowire we observe a giant enhancement of the spin accumulation of up to five orders of magnitude on transition into the superconduc... | [['we', 'study', 'spin', 'accumulation', 'and', 'spin', 'relaxation', 'in', 'a', 'superconducting', 'nanowire', 'spins', 'are', 'injected', 'and', 'detected', 'by', 'using', 'a', 'set', 'of', 'magnetic', 'tunnel', 'contact', 'electrodes', 'closely', 'spaced', 'along', 'the', 'nanowire', 'we', 'observe', 'a', 'giant', '... | [-0.18732627626641804, 0.2229799723709609, -0.016227097482232448, 0.007470285855273469, -0.0025168278445609105, -0.10659618055623056, 0.0592658936073924, 0.37796636588043636, -0.24166329125037941, -0.3298201253796872, -0.003228959775704922, -0.3413636450074677, -0.042661729499570325, 0.1887868637453892, 0.0788530433693... |
707.288 | Manipulating biphotonic qutrits | Quantum information carriers with higher dimension than the canonical qubit
offer significant advantages. However, manipulating such systems is extremely
difficult. We show how measurement induced non-linearities can be employed to
dramatically extend the range of possible transforms on biphotonic qutrits; the
three ... | quant-ph | quantum information carriers with higher dimension than the canonical qubit offer significant advantages however manipulating such systems is extremely difficult we show how measurement induced nonlinearities can be employed to dramatically extend the range of possible transforms on biphotonic qutrits the three level q... | [['quantum', 'information', 'carriers', 'with', 'higher', 'dimension', 'than', 'the', 'canonical', 'qubit', 'offer', 'significant', 'advantages', 'however', 'manipulating', 'such', 'systems', 'is', 'extremely', 'difficult', 'we', 'show', 'how', 'measurement', 'induced', 'nonlinearities', 'can', 'be', 'employed', 'to', ... | [-0.12066627285155923, 0.195644440750023, -0.07565051816562389, 0.06516767255194049, -0.029332693970881084, -0.19275255979811576, 0.02052595770789033, 0.36116186549213336, -0.26084619806088666, -0.26782149407378536, 0.037265994426289056, -0.26020868833330363, -0.14218274850715348, 0.240638524120515, -0.0341398632339637... |
707.2881 | VLT spectroscopy of blue supergiants in IC 1613 | We present multi-object spectroscopy of young, massive stars in the Local
Group galaxy IC 1613. We provide the spectral classification and a detailed
spectral catalog for 54 OBA stars in this galaxy. The majority of the
photometrically selected sample is composed of B- and A-type supergiants. The
remaining stars incl... | astro-ph | we present multiobject spectroscopy of young massive stars in the local group galaxy ic 1613 we provide the spectral classification and a detailed spectral catalog for 54 oba stars in this galaxy the majority of the photometrically selected sample is composed of b and atype supergiants the remaining stars include early... | [['we', 'present', 'multiobject', 'spectroscopy', 'of', 'young', 'massive', 'stars', 'in', 'the', 'local', 'group', 'galaxy', 'ic', '1613', 'we', 'provide', 'the', 'spectral', 'classification', 'and', 'a', 'detailed', 'spectral', 'catalog', 'for', '54', 'oba', 'stars', 'in', 'this', 'galaxy', 'the', 'majority', 'of', '... | [-0.04201504993386426, 0.06497001436553777, -0.03634405994255628, 0.07946237771668369, -0.11660315706634834, -0.03426397282866731, 0.1424316475592879, 0.4310922779379383, -0.07671162490511224, -0.36966693630471587, 0.005840078969153443, -0.3221735450187846, -0.010871329477855138, 0.1610190509485879, -0.0783651698498971... |
707.2882 | Structure formation in the presence of dark energy perturbations | We study non-linear structure formation in the presence of dark energy. The
influence of dark energy on the growth of large-scale cosmological structures
is exerted both through its background effect on the expansion rate, and
through its perturbations as well. In order to compute the rate of formation of
massive obj... | astro-ph hep-ph | we study nonlinear structure formation in the presence of dark energy the influence of dark energy on the growth of largescale cosmological structures is exerted both through its background effect on the expansion rate and through its perturbations as well in order to compute the rate of formation of massive objects we... | [['we', 'study', 'nonlinear', 'structure', 'formation', 'in', 'the', 'presence', 'of', 'dark', 'energy', 'the', 'influence', 'of', 'dark', 'energy', 'on', 'the', 'growth', 'of', 'largescale', 'cosmological', 'structures', 'is', 'exerted', 'both', 'through', 'its', 'background', 'effect', 'on', 'the', 'expansion', 'rate... | [-0.1311889465280295, 0.10543416384842833, -0.10926177436659966, 0.0866105129080607, -0.08289920658560766, -0.017065344380528154, -0.04915802427959219, 0.3075568473802131, -0.2612855999391073, -0.35046892610996544, 0.04923085211509638, -0.24275731823758537, -0.10849491462424815, 0.1537874482189105, 0.043933734874117024... |
707.2883 | Construction and purpose of effective field theories for frustrated
magnetic order | This article reviews recent years' progress in the low temperature analysis
of standard models of spin glass order such as the Sherrington-Kirkpatrick (SK)
model. Applications to CdTe/CdMnTe layered systems and explanation of glassy
antiferromagnetic order at lowest temperatures stimulated us to study in detail
the b... | cond-mat.dis-nn | this article reviews recent years progress in the low temperature analysis of standard models of spin glass order such as the sherringtonkirkpatrick sk model applications to cdtecdmnte layered systems and explanation of glassy antiferromagnetic order at lowest temperatures stimulated us to study in detail the beautiful... | [['this', 'article', 'reviews', 'recent', 'years', 'progress', 'in', 'the', 'low', 'temperature', 'analysis', 'of', 'standard', 'models', 'of', 'spin', 'glass', 'order', 'such', 'as', 'the', 'sherringtonkirkpatrick', 'sk', 'model', 'applications', 'to', 'cdtecdmnte', 'layered', 'systems', 'and', 'explanation', 'of', 'g... | [-0.1290653883246705, 0.13943123205099256, -0.07328226225716727, 0.08455381145301674, -0.0876443713703858, -0.10273991115391254, 0.06724923793309634, 0.31027965805094154, -0.21880456036888063, -0.31758829786309173, 0.10799998594447971, -0.2664597250188568, -0.18968339732715062, 0.15134442729010647, 0.008114826739100474... |
707.2884 | On multidimensional item response theory -- a coordinate free approach | A coordinate system free definition of complex structure multidimensional
item response theory (MIRT) for dichotomously scored items is presented. The
point of view taken emphasizes the possibilities and subtleties of
understanding MIRT as a multidimensional extension of the ``classical''
unidimensional item response... | math.ST stat.TH | a coordinate system free definition of complex structure multidimensional item response theory mirt for dichotomously scored items is presented the point of view taken emphasizes the possibilities and subtleties of understanding mirt as a multidimensional extension of the classical unidimensional item response theory m... | [['a', 'coordinate', 'system', 'free', 'definition', 'of', 'complex', 'structure', 'multidimensional', 'item', 'response', 'theory', 'mirt', 'for', 'dichotomously', 'scored', 'items', 'is', 'presented', 'the', 'point', 'of', 'view', 'taken', 'emphasizes', 'the', 'possibilities', 'and', 'subtleties', 'of', 'understandin... | [-0.08994972560743707, 0.07747565909032372, -0.10887940154424396, 0.10366946631921051, -0.1215099052499062, -0.2001354247196645, 0.037741206886678716, 0.31335919185717037, -0.29899594603457313, -0.22487106884870192, 0.046919863881065386, -0.31443321955241804, -0.1951159155941096, 0.11781462322097218, -0.082722262597467... |
707.2885 | Sylvester's Minorant Criterion, Lagrange-Beltrami Identity, and
Nonnegative Definiteness | We consider the characterizations of positive definite as well as nonnegative
definite quadratic forms in terms of the principal minors of the associated
symmetric matrix. We briefly review some of the known proofs, including a
classical approach via the Lagrange-Beltrami identity. For quadratic forms in
up to 3 vari... | math.HO math.GM | we consider the characterizations of positive definite as well as nonnegative definite quadratic forms in terms of the principal minors of the associated symmetric matrix we briefly review some of the known proofs including a classical approach via the lagrangebeltrami identity for quadratic forms in up to 3 variables ... | [['we', 'consider', 'the', 'characterizations', 'of', 'positive', 'definite', 'as', 'well', 'as', 'nonnegative', 'definite', 'quadratic', 'forms', 'in', 'terms', 'of', 'the', 'principal', 'minors', 'of', 'the', 'associated', 'symmetric', 'matrix', 'we', 'briefly', 'review', 'some', 'of', 'the', 'known', 'proofs', 'incl... | [-0.12068202243873527, 0.041935243693045285, -0.03337757564207286, 0.08857230576309738, -0.09996738592967574, -0.15801987110027743, -0.00516590285172433, 0.2918486123283704, -0.3010095057112199, -0.23108993247611287, 0.16135015859222615, -0.26726503719081296, -0.21911755372140626, 0.1868696910340661, -0.038732875736407... |
707.2886 | OA@MPS - a colourful view | The open access agenda of the Max Planck Society, initiator of the Berlin
Declaration, envisions the support of both the green way and the golden way to
open access. For the implementation of the green way the Max Planck Society
through its newly established unit (Max Planck Digital Library) follows the
idea of provi... | cs.DL | the open access agenda of the max planck society initiator of the berlin declaration envisions the support of both the green way and the golden way to open access for the implementation of the green way the max planck society through its newly established unit max planck digital library follows the idea of providing a ... | [['the', 'open', 'access', 'agenda', 'of', 'the', 'max', 'planck', 'society', 'initiator', 'of', 'the', 'berlin', 'declaration', 'envisions', 'the', 'support', 'of', 'both', 'the', 'green', 'way', 'and', 'the', 'golden', 'way', 'to', 'open', 'access', 'for', 'the', 'implementation', 'of', 'the', 'green', 'way', 'the', ... | [-0.11117580829335279, 0.05941333531549103, -0.07292383682767027, 0.06789459043035381, -0.14475679672568253, -0.1252194277402994, 0.14321235758497528, 0.2854100157947917, -0.2687929183244705, -0.30768408143990916, 0.12244985190152778, -0.299609475210309, -0.12542489954319438, 0.21576375624066904, -0.06699820143219672, ... |
707.2887 | Kelvin-Helmholtz modes revealed by the transversal structure of the jet
in 0836+710 | Studying transversal structure in extragalactic jets is crucial for
understanding their physics. The Japanese led space VLBI project VSOP has
offered arguably the best opportunity for such studies, by reaching baseline
lengths of up to 36,000 km and resolving structures down to an angular size of
0.3 mas at 5 GHz. VS... | astro-ph | studying transversal structure in extragalactic jets is crucial for understanding their physics the japanese led space vlbi project vsop has offered arguably the best opportunity for such studies by reaching baseline lengths of up to 36000 km and resolving structures down to an angular size of 03 mas at 5 ghz vsop obse... | [['studying', 'transversal', 'structure', 'in', 'extragalactic', 'jets', 'is', 'crucial', 'for', 'understanding', 'their', 'physics', 'the', 'japanese', 'led', 'space', 'vlbi', 'project', 'vsop', 'has', 'offered', 'arguably', 'the', 'best', 'opportunity', 'for', 'such', 'studies', 'by', 'reaching', 'baseline', 'lengths... | [-0.11807641496369303, 0.1443330806207526, -0.0702127013167979, 0.041723863510008674, -0.058445897484635745, -0.06228885836211727, -0.00258161407276588, 0.3903433622154813, -0.2349672262625606, -0.32741704645047853, 0.09213110253030447, -0.2493984959113268, -0.009183403459649483, 0.21827182007465987, 0.0481795615633384... |
707.2888 | Quantum Hall effect in carbon nanotubes and curved graphene strips | We develop a long wavelength approximation in order to describe the
low-energy states of carbon nanotubes in a transverse magnetic field. We show
that, in the limit where the square of the magnetic length $l = \sqrt{\hbar c
/e B}$ is much larger than the $C$-$C$ distance times the nanotube radius $R$,
the low-energy ... | cond-mat.mes-hall | we develop a long wavelength approximation in order to describe the lowenergy states of carbon nanotubes in a transverse magnetic field we show that in the limit where the square of the magnetic length l sqrthbar c e b is much larger than the cc distance times the nanotube radius r the lowenergy theory is given by the ... | [['we', 'develop', 'a', 'long', 'wavelength', 'approximation', 'in', 'order', 'to', 'describe', 'the', 'lowenergy', 'states', 'of', 'carbon', 'nanotubes', 'in', 'a', 'transverse', 'magnetic', 'field', 'we', 'show', 'that', 'in', 'the', 'limit', 'where', 'the', 'square', 'of', 'the', 'magnetic', 'length', 'l', 'sqrthbar... | [-0.18250852375607587, 0.2020031738612265, -0.009175061243849824, 0.01696171762557911, -0.005940814643937936, -0.1346054787479587, 0.04557633467616057, 0.4010753951843758, -0.24983107151130307, -0.2819692445921663, 0.013208320881086314, -0.2648666683487805, -0.09555052213847444, 0.12504928061554102, 0.01690297725961603... |
707.2889 | Geography of local configurations | A $d$-dimensional binary Markov random field on a lattice torus is
considered. As the size $n$ of the lattice tends to infinity, potentials
$a=a(n)$ and $b=b(n)$ depend on $n$. Precise bounds for the probability for
local configurations to occur in a large ball are given. Under some conditions
bearing on $a(n)$ and $... | math.PR math-ph math.MP | a ddimensional binary markov random field on a lattice torus is considered as the size n of the lattice tends to infinity potentials aan and bbn depend on n precise bounds for the probability for local configurations to occur in a large ball are given under some conditions bearing on an and bn the distance between copi... | [['a', 'ddimensional', 'binary', 'markov', 'random', 'field', 'on', 'a', 'lattice', 'torus', 'is', 'considered', 'as', 'the', 'size', 'n', 'of', 'the', 'lattice', 'tends', 'to', 'infinity', 'potentials', 'aan', 'and', 'bbn', 'depend', 'on', 'n', 'precise', 'bounds', 'for', 'the', 'probability', 'for', 'local', 'configu... | [-0.16317468068917237, 0.177414410250224, -0.05020912969484925, 0.03502755828196227, -0.030953428594373344, -0.14245671221786843, 0.08046120671012129, 0.38245341593089205, -0.2353326705107022, -0.2122301353762547, 0.11996027220794488, -0.23710312764714694, -0.08160577087463546, 0.13699244151523868, -0.05981518812976511... |
707.289 | Constructing level-2 phylogenetic networks from triplets | Jansson and Sung showed that, given a dense set of input triplets T
(representing hypotheses about the local evolutionary relationships of triplets
of species), it is possible to determine in polynomial time whether there
exists a level-1 network consistent with T, and if so to construct such a
network. They also sho... | q-bio.PE | jansson and sung showed that given a dense set of input triplets t representing hypotheses about the local evolutionary relationships of triplets of species it is possible to determine in polynomial time whether there exists a level1 network consistent with t and if so to construct such a network they also showed that ... | [['jansson', 'and', 'sung', 'showed', 'that', 'given', 'a', 'dense', 'set', 'of', 'input', 'triplets', 't', 'representing', 'hypotheses', 'about', 'the', 'local', 'evolutionary', 'relationships', 'of', 'triplets', 'of', 'species', 'it', 'is', 'possible', 'to', 'determine', 'in', 'polynomial', 'time', 'whether', 'there'... | [-0.09728347786774787, 0.09519217818878688, -0.039464908216584035, 0.10803529599155359, -0.04385223220308106, -0.14487497662435975, 0.06090650835521247, 0.39447607327397766, -0.29383682972727365, -0.28689551426932314, 0.08952212178219388, -0.23148880285730997, -0.20655528201975606, 0.15782934615566915, -0.0766346398642... |
707.2891 | Transport, magnetic and superconducting properties of RuSr2RCu2O8 (R=
Eu, Gd) doped with Sn | Ru{1-x}Sn{x}Sr2EuCu2O8 and Ru{1-x}Sn{x}Sr2GdCu2O8 have been comprehensively
studied by microwave and dc resistivity and magnetoresistivity and by the dc
Hall measurements. The magnetic ordering temperature T_m is considerably
reduced with increasing Sn content. However, doping with Sn leads to only
slight reduction o... | cond-mat.supr-con cond-mat.str-el | ru1xsnxsr2eucu2o8 and ru1xsnxsr2gdcu2o8 have been comprehensively studied by microwave and dc resistivity and magnetoresistivity and by the dc hall measurements the magnetic ordering temperature t_m is considerably reduced with increasing sn content however doping with sn leads to only slight reduction of the supercond... | [['ru1xsnxsr2eucu2o8', 'and', 'ru1xsnxsr2gdcu2o8', 'have', 'been', 'comprehensively', 'studied', 'by', 'microwave', 'and', 'dc', 'resistivity', 'and', 'magnetoresistivity', 'and', 'by', 'the', 'dc', 'hall', 'measurements', 'the', 'magnetic', 'ordering', 'temperature', 't_m', 'is', 'considerably', 'reduced', 'with', 'in... | [-0.19242126342512414, 0.24358288623030108, 0.042986146927291115, -0.02971616626774602, -0.015313345361380027, -0.15938037648409992, 0.10918426173572827, 0.33023524985273744, -0.25014404323354195, -0.3155872092099237, -0.0021232283634871436, -0.37080592506069254, -0.10466721822362539, 0.1968411704368115, 0.005355970596... |
707.2892 | Electron Pair Resonance in the Coulomb Blockade | We study many-body corrections to the cotunneling current via a localized
state with energy $\epsilon_d$ at large bias voltages $V$. We show that the
transfer of {\em electron pairs}, enabled by the Coulomb repulsion in the
localized level, results in ionization resonance peaks in the third derivative
of the current ... | cond-mat.mes-hall cond-mat.str-el | we study manybody corrections to the cotunneling current via a localized state with energy epsilon_d at large bias voltages v we show that the transfer of em electron pairs enabled by the coulomb repulsion in the localized level results in ionization resonance peaks in the third derivative of the current with respect t... | [['we', 'study', 'manybody', 'corrections', 'to', 'the', 'cotunneling', 'current', 'via', 'a', 'localized', 'state', 'with', 'energy', 'epsilon_d', 'at', 'large', 'bias', 'voltages', 'v', 'we', 'show', 'that', 'the', 'transfer', 'of', 'em', 'electron', 'pairs', 'enabled', 'by', 'the', 'coulomb', 'repulsion', 'in', 'the... | [-0.13317046922919176, 0.12005514526219271, -0.02335266609203673, 0.06062592231832883, 0.025769156431231427, -0.11109417522846557, 0.09209323373130139, 0.3572474503615761, -0.26382241317290156, -0.29639372996290847, -0.037581630610956755, -0.3387490618042648, -0.07748279830112177, 0.13287160399041192, 0.043846239880247... |
707.2893 | Excitons in long molecular chains near the reflecting interface | We discuss coherent exciton-polariton states in long molecular chains that
are formed due to the interaction of molecular excitations with both vacuum
photons and surface excitations of the neighboring reflecting substrate. The
resonance coupling with surface plasmons (or surface polaritons) of the
substrate can subs... | cond-mat.other | we discuss coherent excitonpolariton states in long molecular chains that are formed due to the interaction of molecular excitations with both vacuum photons and surface excitations of the neighboring reflecting substrate the resonance coupling with surface plasmons or surface polaritons of the substrate can substantia... | [['we', 'discuss', 'coherent', 'excitonpolariton', 'states', 'in', 'long', 'molecular', 'chains', 'that', 'are', 'formed', 'due', 'to', 'the', 'interaction', 'of', 'molecular', 'excitations', 'with', 'both', 'vacuum', 'photons', 'and', 'surface', 'excitations', 'of', 'the', 'neighboring', 'reflecting', 'substrate', 'th... | [-0.16725355713660348, 0.2703129771633218, -0.05175756181566173, 0.05945998962480848, -0.0372934540059289, -0.11874403660346208, 0.041562807158534894, 0.42364379924176065, -0.24872064555770365, -0.2704547216605941, -0.045295614448921946, -0.296362603112156, -0.0411043845614868, 0.1632415437155628, 0.08637563354046694, ... |
707.2894 | CMB temperature anisotropies from third order gravitational
perturbations | In this paper we present a complete computation of the Cosmic Microwave
Background (CMB) anisotropies up to third order from gravitational
perturbations accounting for scalar, vector and tensor perturbations. We then
specify our results to the large scale limit, providing the evolution of the
gravitational potentials... | astro-ph | in this paper we present a complete computation of the cosmic microwave background cmb anisotropies up to third order from gravitational perturbations accounting for scalar vector and tensor perturbations we then specify our results to the large scale limit providing the evolution of the gravitational potentials in a f... | [['in', 'this', 'paper', 'we', 'present', 'a', 'complete', 'computation', 'of', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'anisotropies', 'up', 'to', 'third', 'order', 'from', 'gravitational', 'perturbations', 'accounting', 'for', 'scalar', 'vector', 'and', 'tensor', 'perturbations', 'we', 'then', 'specify', '... | [-0.1332687937275127, 0.11330602870633205, -0.08619968930638774, 0.11183451236639586, -0.10584435237882038, -0.054263495436559124, -0.06346977517370962, 0.29770057967829483, -0.2208857776424675, -0.28297743178748835, 0.06617655086641511, -0.27293605654396946, -0.12074222486914583, 0.19091921722930338, 0.047076023547021... |
707.2895 | Mass-Radius Relationships for Solid Exoplanets | We use new interior models of cold planets to investigate the mass-radius
relationships of solid exoplanets, considering planets made primarily of iron,
silicates, water, and carbon compounds. We find that the mass-radius
relationships for cold terrestrial-mass planets of all compositions we
considered follow a gener... | astro-ph | we use new interior models of cold planets to investigate the massradius relationships of solid exoplanets considering planets made primarily of iron silicates water and carbon compounds we find that the massradius relationships for cold terrestrialmass planets of all compositions we considered follow a generic functio... | [['we', 'use', 'new', 'interior', 'models', 'of', 'cold', 'planets', 'to', 'investigate', 'the', 'massradius', 'relationships', 'of', 'solid', 'exoplanets', 'considering', 'planets', 'made', 'primarily', 'of', 'iron', 'silicates', 'water', 'and', 'carbon', 'compounds', 'we', 'find', 'that', 'the', 'massradius', 'relati... | [-0.08973133235259576, 0.19672804051005524, -0.03548401334931649, 0.06406607757428823, -0.08787181348297891, -0.08425585002689732, 0.0896027111986883, 0.34640965535576773, -0.1663357153222997, -0.36224874219028497, 0.06516596596911696, -0.29853565270066496, -0.08127333487725018, 0.15441744351909883, -0.0508469344798739... |
707.2896 | The GALEX UV emission in shell galaxies: tracing galaxy "rejuvenation"
episodes | We present the GALEX far FUV and near NUV ultraviolet imaging of three nearby
shell galaxies, namely NGC 2865, NGC 5018 and NGC 7135. The system of shells
and fine structures visible in the optical is detected in the NUV image of NGC
2865 and in both NUV and FUV images of NGC 7135. The NUV image of NGC 5018 does
not ... | astro-ph | we present the galex far fuv and near nuv ultraviolet imaging of three nearby shell galaxies namely ngc 2865 ngc 5018 and ngc 7135 the system of shells and fine structures visible in the optical is detected in the nuv image of ngc 2865 and in both nuv and fuv images of ngc 7135 the nuv image of ngc 5018 does not presen... | [['we', 'present', 'the', 'galex', 'far', 'fuv', 'and', 'near', 'nuv', 'ultraviolet', 'imaging', 'of', 'three', 'nearby', 'shell', 'galaxies', 'namely', 'ngc', '2865', 'ngc', '5018', 'and', 'ngc', '7135', 'the', 'system', 'of', 'shells', 'and', 'fine', 'structures', 'visible', 'in', 'the', 'optical', 'is', 'detected', ... | [0.018928143961311174, 0.046859730616314633, -0.09564383624820039, 0.10135286112665613, -0.057092240782872214, -0.04245582778749199, 0.00982100759124138, 0.5581264588252718, -0.10075371637832692, -0.3432614750529596, 0.0164964504907027, -0.30668389472407803, -0.05913892724083942, 0.15820434141706913, -0.105731336129071... |
707.2897 | Electroweak structure of the nucleon, meson cloud and light-cone
wavefunctions | The meson-cloud model of the nucleon consisting of a system of three valence
quarks surrounded by a meson cloud is applied to study the electroweak
structure of the proton and neutron. Light-cone wavefunctions are derived for
the dressed nucleon as pictured to be part of the time a bare nucleon and part
of the time a... | hep-ph | the mesoncloud model of the nucleon consisting of a system of three valence quarks surrounded by a meson cloud is applied to study the electroweak structure of the proton and neutron lightcone wavefunctions are derived for the dressed nucleon as pictured to be part of the time a bare nucleon and part of the time a bary... | [['the', 'mesoncloud', 'model', 'of', 'the', 'nucleon', 'consisting', 'of', 'a', 'system', 'of', 'three', 'valence', 'quarks', 'surrounded', 'by', 'a', 'meson', 'cloud', 'is', 'applied', 'to', 'study', 'the', 'electroweak', 'structure', 'of', 'the', 'proton', 'and', 'neutron', 'lightcone', 'wavefunctions', 'are', 'deri... | [-0.09949474345829168, 0.2285970659790275, -0.07212907865601169, 0.09548450601604683, -0.038020955687600444, -0.05939531082192182, 0.041006124797488816, 0.33254869815639476, -0.21241583730231717, -0.2549000266635134, 0.0011929830313998867, -0.30291555850681934, -0.013081593012380339, 0.12558616832247935, 0.074318675288... |
707.2898 | Meromorphic solutions of higher order Briot-Bouquet differential
equations | For differential equations $P(y^{(k)},y)=0,$ where $P$ is a polynomial, we
prove that all meromorphic solutions having at least one pole are elliptic
functions, possibly degenerate.
| math.CA math.CV | for differential equations pyky0 where p is a polynomial we prove that all meromorphic solutions having at least one pole are elliptic functions possibly degenerate | [['for', 'differential', 'equations', 'pyky0', 'where', 'p', 'is', 'a', 'polynomial', 'we', 'prove', 'that', 'all', 'meromorphic', 'solutions', 'having', 'at', 'least', 'one', 'pole', 'are', 'elliptic', 'functions', 'possibly', 'degenerate']] | [-0.2609017393551767, 0.04511361138429493, -0.12029348145006225, 0.09587716771541939, -0.13671111082658172, -0.23695048889688528, -0.12672150216531008, 0.24877079095070562, -0.3260901435278356, -0.17045728511099392, 0.14778224578670537, -0.40300696219007176, -0.10315589203188817, 0.1983994534239173, 0.02593679512695719... |
707.2899 | Thermodynamics of low dimensional spin-1/2 Heisenberg ferromagnets in an
external magnetic field within Green function formalism | The thermodynamics of low dimensional spin-1/2 Heisenberg ferromagnets (HFM)
in an external magnetic field is investigated within a second-order two-time
Green function formalism in the wide temperature and field range. A crucial
point of the proposed scheme is a proper account of the analytical properties
for the ap... | cond-mat.str-el cond-mat.dis-nn | the thermodynamics of low dimensional spin12 heisenberg ferromagnets hfm in an external magnetic field is investigated within a secondorder twotime green function formalism in the wide temperature and field range a crucial point of the proposed scheme is a proper account of the analytical properties for the approximate... | [['the', 'thermodynamics', 'of', 'low', 'dimensional', 'spin12', 'heisenberg', 'ferromagnets', 'hfm', 'in', 'an', 'external', 'magnetic', 'field', 'is', 'investigated', 'within', 'a', 'secondorder', 'twotime', 'green', 'function', 'formalism', 'in', 'the', 'wide', 'temperature', 'and', 'field', 'range', 'a', 'crucial',... | [-0.15607778599055913, 0.1144593614405424, -0.06626022986064736, 0.09298232045078364, -0.014560961538854127, -0.08393131444015756, 0.0385748543866122, 0.37453474072882764, -0.2195586595379819, -0.25300508455122606, 0.07458308580188223, -0.27642340533292065, -0.08720452224728294, 0.22929754611104727, 0.09686401038466451... |
707.29 | Zeptosecond $\gamma$-ray pulses | High-order harmonic generation (HHG) in the relativistic regime is employed
to obtain zeptosecond pulses of $\gamma$-rays. The harmonics are generated from
atomic systems in counterpropagating strong attosecond laser pulse trains of
linear polarization. In this setup recollisions of the ionized electrons can be
achie... | physics.atom-ph physics.optics | highorder harmonic generation hhg in the relativistic regime is employed to obtain zeptosecond pulses of gammarays the harmonics are generated from atomic systems in counterpropagating strong attosecond laser pulse trains of linear polarization in this setup recollisions of the ionized electrons can be achieved in the ... | [['highorder', 'harmonic', 'generation', 'hhg', 'in', 'the', 'relativistic', 'regime', 'is', 'employed', 'to', 'obtain', 'zeptosecond', 'pulses', 'of', 'gammarays', 'the', 'harmonics', 'are', 'generated', 'from', 'atomic', 'systems', 'in', 'counterpropagating', 'strong', 'attosecond', 'laser', 'pulse', 'trains', 'of', ... | [-0.09483719334471971, 0.28843775650952014, -0.053930479185655716, 0.13478850647807122, 0.013838904457516036, -0.1036413950752467, -0.009322364814579487, 0.48035546861588957, -0.2827164710871875, -0.291433288436383, -0.03882824236294255, -0.25758966434979813, 0.028314361427910627, 0.30356087306514384, 0.058520269128493... |
707.2901 | Effect of in-plane line defects on field-tuned superconductor-insulator
transition behavior in homogeneous thin film | Field-tuned superconductor-insulator transition (FSIT) behavior in 2D
isotropic and homogeneous thin films is usually accompanied by a nonvanishing
critical resistance at low $T$. It is shown that, in a 2D film including line
defects paralle to each other but with random positions perpendicular to them,
the (apparent... | cond-mat.supr-con | fieldtuned superconductorinsulator transition fsit behavior in 2d isotropic and homogeneous thin films is usually accompanied by a nonvanishing critical resistance at low t it is shown that in a 2d film including line defects paralle to each other but with random positions perpendicular to them the apparent critical re... | [['fieldtuned', 'superconductorinsulator', 'transition', 'fsit', 'behavior', 'in', '2d', 'isotropic', 'and', 'homogeneous', 'thin', 'films', 'is', 'usually', 'accompanied', 'by', 'a', 'nonvanishing', 'critical', 'resistance', 'at', 'low', 't', 'it', 'is', 'shown', 'that', 'in', 'a', '2d', 'film', 'including', 'line', '... | [-0.1696727891640666, 0.20758167514129758, -0.062403141834343284, 0.03540468010275314, -0.022815094038378447, -0.2129638776099548, 0.06075411235603193, 0.38460336902584785, -0.23645085681420872, -0.23596701880272192, 0.04801605747138055, -0.32752087842434263, -0.1314842799155229, 0.15757877842182866, 0.0158185209117782... |
707.2902 | Fabrication, Dynamics, and Electrical Properties of Insulated SPM Probes
for Electrical and Electromechanical Imaging in Liquids | Insulated cantilever probes with a high aspect ratio conducting apex have
been fabricated and their dynamic and electrical properties analyzed. The
cantilevers were coated with silicon dioxide and a via was fabricated through
the oxide at the tip apex and backfilled with tungsten to create an insulated
probe with a c... | cond-mat.mtrl-sci | insulated cantilever probes with a high aspect ratio conducting apex have been fabricated and their dynamic and electrical properties analyzed the cantilevers were coated with silicon dioxide and a via was fabricated through the oxide at the tip apex and backfilled with tungsten to create an insulated probe with a cond... | [['insulated', 'cantilever', 'probes', 'with', 'a', 'high', 'aspect', 'ratio', 'conducting', 'apex', 'have', 'been', 'fabricated', 'and', 'their', 'dynamic', 'and', 'electrical', 'properties', 'analyzed', 'the', 'cantilevers', 'were', 'coated', 'with', 'silicon', 'dioxide', 'and', 'a', 'via', 'was', 'fabricated', 'thro... | [-0.09665299909189344, 0.1654707836000307, -0.0029217314114794134, -0.10496176519014626, -0.04112960675731301, -0.21261971786618233, 0.055672145560383794, 0.4721583800017834, -0.23934516113251447, -0.3421738824993372, 0.10633732890710235, -0.33072351752780377, -0.09008183915633708, 0.2190706563554704, 0.004096859218552... |
707.2903 | Speckle Interferometry of Metal-Poor Stars in the Solar Neighborhood. I | We report the results of speckle-interferometric observations of 109 high
proper-motion metal-poor stars made with the 6-m telescope of the Special
Astrophysical Observatory of the Russian Academy of Sciences. We resolve eight
objects -- G102-20, G191-55, BD+19$^\circ$~1185A, G89-14, G87-45, G87-47,
G111-38, and G114... | astro-ph | we report the results of speckleinterferometric observations of 109 high propermotion metalpoor stars made with the 6m telescope of the special astrophysical observatory of the russian academy of sciences we resolve eight objects g10220 g19155 bd19circ1185a g8914 g8745 g8747 g11138 and g11425 into individual components... | [['we', 'report', 'the', 'results', 'of', 'speckleinterferometric', 'observations', 'of', '109', 'high', 'propermotion', 'metalpoor', 'stars', 'made', 'with', 'the', '6m', 'telescope', 'of', 'the', 'special', 'astrophysical', 'observatory', 'of', 'the', 'russian', 'academy', 'of', 'sciences', 'we', 'resolve', 'eight', ... | [-0.13308770306829415, 0.08761111462539801, -0.025745915606209677, 0.0406790360846646, -0.12611375273243614, -0.062405820859417524, 0.07438050815197703, 0.357578008397393, -0.1237551708233683, -0.4137371518738466, 0.06527341423198989, -0.342350625780679, -0.04901591722202832, 0.23659740717306554, -0.04367226748791051, ... |
707.2904 | The 10^5Lsun High-Mass Protostellar Object IRAS23151+5912 | While most sources above 10^5Lsun have already formed an Ultracompact HII
region (UCHII), this is not necessarily the case for sources of lower
luminosity. Characterizing sources in the transition phase, i.e., very luminous
objects without any detectable free-free emission, is important for a general
understanding of... | astro-ph | while most sources above 105lsun have already formed an ultracompact hii region uchii this is not necessarily the case for sources of lower luminosity characterizing sources in the transition phase ie very luminous objects without any detectable freefree emission is important for a general understanding of massive star... | [['while', 'most', 'sources', 'above', '105lsun', 'have', 'already', 'formed', 'an', 'ultracompact', 'hii', 'region', 'uchii', 'this', 'is', 'not', 'necessarily', 'the', 'case', 'for', 'sources', 'of', 'lower', 'luminosity', 'characterizing', 'sources', 'in', 'the', 'transition', 'phase', 'ie', 'very', 'luminous', 'obj... | [-0.08168944097053248, 0.09441491126186143, -0.018088727584318468, 0.06929544634542319, -0.07592403789696929, -0.10763390557756564, 0.004558720659498159, 0.48572101769549353, -0.13493097706767102, -0.2916654237873248, 0.08231042993993305, -0.28010571769256193, 0.015627045867133985, 0.1607289358989956, 0.018658374968327... |
707.2905 | Molecular line radiative transfer in protoplanetary disks: Monte Carlo
simulations versus approximate methods | We analyze the line radiative transfer in protoplanetary disks using several
approximate methods and a well-tested Accelerated Monte Carlo code. A low-mass
flaring disk model with uniform as well as stratified molecular abundances is
adopted. Radiative transfer in low and high rotational lines of CO, C18O, HCO+,
DCO+... | astro-ph | we analyze the line radiative transfer in protoplanetary disks using several approximate methods and a welltested accelerated monte carlo code a lowmass flaring disk model with uniform as well as stratified molecular abundances is adopted radiative transfer in low and high rotational lines of co c18o hco dco hcn cs and... | [['we', 'analyze', 'the', 'line', 'radiative', 'transfer', 'in', 'protoplanetary', 'disks', 'using', 'several', 'approximate', 'methods', 'and', 'a', 'welltested', 'accelerated', 'monte', 'carlo', 'code', 'a', 'lowmass', 'flaring', 'disk', 'model', 'with', 'uniform', 'as', 'well', 'as', 'stratified', 'molecular', 'abun... | [-0.04691638569680175, 0.10000191129354993, -0.005040593041123185, 0.1258703288843944, 0.0054773294167327026, -0.12501184037559993, 0.068454298412516, 0.46776016266186, -0.2001750951582965, -0.3177741563957572, 0.048385619440869915, -0.21439838667855762, -0.04323362132929491, 0.16953620174294942, 0.04664999432055465, 0... |
707.2906 | Two-loop renormalization of scalar and pseudoscalar fermion bilinears on
the lattice | We compute the two-loop renormalization functions, in the RI $^\prime$
scheme, of local bilinear quark operators $\bar{\psi}\Gamma\psi$, where
$\Gamma$ denotes the Scalar and Pseudoscalar Dirac matrices, in the lattice
formulation of QCD. We consider both the flavor non-singlet and singlet
operators; the latter, in t... | hep-lat | we compute the twoloop renormalization functions in the ri prime scheme of local bilinear quark operators barpsigammapsi where gamma denotes the scalar and pseudoscalar dirac matrices in the lattice formulation of qcd we consider both the flavor nonsinglet and singlet operators the latter in the scalar case leads direc... | [['we', 'compute', 'the', 'twoloop', 'renormalization', 'functions', 'in', 'the', 'ri', 'prime', 'scheme', 'of', 'local', 'bilinear', 'quark', 'operators', 'barpsigammapsi', 'where', 'gamma', 'denotes', 'the', 'scalar', 'and', 'pseudoscalar', 'dirac', 'matrices', 'in', 'the', 'lattice', 'formulation', 'of', 'qcd', 'we'... | [-0.12364438106305897, 0.23386196815504504, -0.05901032726978883, 0.11264431287877653, -0.032027890207245946, -0.08877516409235173, 0.044713104636206195, 0.3664479680592194, -0.15820483796874454, -0.2216818577757007, 0.01149897143630752, -0.2855526587656258, -0.12415747323661651, 0.1275628982096494, 0.04162025244410248... |
707.2907 | Group theoretical approach to quantum fields in de Sitter space II. The
complementary and discrete series | We use an algebraic approach based on representations of de Sitter group to
construct covariant quantum fields in arbitrary dimensions. We study the
complementary and the discrete series which correspond to light and massless
fields and which lead new feature with respect to the massive principal series
we previously... | hep-th | we use an algebraic approach based on representations of de sitter group to construct covariant quantum fields in arbitrary dimensions we study the complementary and the discrete series which correspond to light and massless fields and which lead new feature with respect to the massive principal series we previously st... | [['we', 'use', 'an', 'algebraic', 'approach', 'based', 'on', 'representations', 'of', 'de', 'sitter', 'group', 'to', 'construct', 'covariant', 'quantum', 'fields', 'in', 'arbitrary', 'dimensions', 'we', 'study', 'the', 'complementary', 'and', 'the', 'discrete', 'series', 'which', 'correspond', 'to', 'light', 'and', 'ma... | [-0.1424449698044219, 0.1507051060413527, -0.13801559867287883, 0.08491905927937878, -0.0967376665581945, -0.11348992911299347, -0.004298256572646732, 0.3096551004829197, -0.21899935747436827, -0.22731726470852046, 0.0564565783033803, -0.2579877201363828, -0.1579662789510715, 0.1213310425491532, -0.04590591340617561, 0... |
707.2908 | Some particular self-interacting diffusions: Ergodic behaviour and
almost sure convergence | This paper deals with some self-interacting diffusions $(X_t,t\geq 0)$ living
on $\mathbb{R}^d$. These diffusions are solutions to stochastic differential
equations: \[\mathrm{d}X_t=\mathrm{d}B_t-g(t)\nabla
V(X_t-\bar{\mu}_t)\,\mathrm{d}t,\] where $\bar{\mu}_t$ is the empirical mean of
the process $X$, $V$ is an asym... | math.PR math.ST stat.TH | this paper deals with some selfinteracting diffusions x_ttgeq 0 living on mathbbrd these diffusions are solutions to stochastic differential equations mathrmdx_tmathrmdb_tgtnabla vx_tbarmu_tmathrmdt where barmu_t is the empirical mean of the process x v is an asymptotically strictly convex potential and g is a given fu... | [['this', 'paper', 'deals', 'with', 'some', 'selfinteracting', 'diffusions', 'x_ttgeq', '0', 'living', 'on', 'mathbbrd', 'these', 'diffusions', 'are', 'solutions', 'to', 'stochastic', 'differential', 'equations', 'mathrmdx_tmathrmdb_tgtnabla', 'vx_tbarmu_tmathrmdt', 'where', 'barmu_t', 'is', 'the', 'empirical', 'mean',... | [-0.1523388835658478, 0.1067107094396364, -0.08925982074257224, 0.040647144031317244, -0.042630767467075045, -0.14330830159993407, 0.01973151148698154, 0.40490904521751914, -0.29616864754798566, -0.1498568690520652, 0.12613647343823686, -0.33956775881667084, -0.17678858900561611, 0.1620350293815136, -0.1322762011302674... |
707.2909 | Evolutionary dynamics and diversity in populations | The dynamics of populations is rich, taking into account that both, the
individual's actions and the population's fitness are coupled. The way in which
an individual chooses a strategy depends off course on the interaction with
other individuals and the relation between selection and mutation within the
population. T... | physics.bio-ph physics.soc-ph | the dynamics of populations is rich taking into account that both the individuals actions and the populations fitness are coupled the way in which an individual chooses a strategy depends off course on the interaction with other individuals and the relation between selection and mutation within the population the prese... | [['the', 'dynamics', 'of', 'populations', 'is', 'rich', 'taking', 'into', 'account', 'that', 'both', 'the', 'individuals', 'actions', 'and', 'the', 'populations', 'fitness', 'are', 'coupled', 'the', 'way', 'in', 'which', 'an', 'individual', 'chooses', 'a', 'strategy', 'depends', 'off', 'course', 'on', 'the', 'interacti... | [-0.09992748458835735, 0.13881082097077732, -0.09077268121891642, 0.07302668194906344, -0.08248097544587026, -0.16444918170537307, 0.08350568260363894, 0.3993070738041374, -0.28682011041841277, -0.3244502035046175, 0.0830137429893927, -0.2538216838360786, -0.13814867376328605, 0.1495984374188295, -0.08823513640324716, ... |
707.291 | Convergence in distribution of some particular self-interacting
diffusions: the simulated annealing method | The present paper is concerned with some self-interacting diffusions
$(X_t,t\geq 0)$ living on $\mathbb{R}^d$. These diffusions are solutions to
stochastic differential equations: $$\mathrm{d}X_t = \mathrm{d}B_t - g(t)\nabla
V(X_t - \bar{\mu}_t) \mathrm{d}t$$ where $\bar{\mu}_t$ is the empirical mean of
the process $... | math.PR | the present paper is concerned with some selfinteracting diffusions x_ttgeq 0 living on mathbbrd these diffusions are solutions to stochastic differential equations mathrmdx_t mathrmdb_t gtnabla vx_t barmu_t mathrmdt where barmu_t is the empirical mean of the process x v is an asymptotically strictly convex potential a... | [['the', 'present', 'paper', 'is', 'concerned', 'with', 'some', 'selfinteracting', 'diffusions', 'x_ttgeq', '0', 'living', 'on', 'mathbbrd', 'these', 'diffusions', 'are', 'solutions', 'to', 'stochastic', 'differential', 'equations', 'mathrmdx_t', 'mathrmdb_t', 'gtnabla', 'vx_t', 'barmu_t', 'mathrmdt', 'where', 'barmu_t... | [-0.14678694098856607, 0.1061388286871454, -0.07168937410160746, 0.05733589575570524, -0.04328524943239526, -0.15369111503541624, 0.0137475131706037, 0.36882913016627744, -0.2720124338916743, -0.19160832801699332, 0.11710121210414878, -0.3195988392822214, -0.16286565226109065, 0.13396291845698946, -0.11085427491973664,... |
707.2911 | Half or full core-hole in density functional theory X-ray absorption
spectrum calculations of water? | We analyze the performance of two different core-hole potentials in the
theoretical modeling of XAS of ice, liquid and gas phase water; the use of a
full core-hole (FCH) in the calculations, as suggested by Hetenyi et al. [J.
Chem. Phys. 120 (18), 8632 (2004)], gives poor agreement with experiment in
terms of intensi... | cond-mat.soft cond-mat.mtrl-sci | we analyze the performance of two different corehole potentials in the theoretical modeling of xas of ice liquid and gas phase water the use of a full corehole fch in the calculations as suggested by hetenyi et al j chem phys 120 18 8632 2004 gives poor agreement with experiment in terms of intensity distribution as we... | [['we', 'analyze', 'the', 'performance', 'of', 'two', 'different', 'corehole', 'potentials', 'in', 'the', 'theoretical', 'modeling', 'of', 'xas', 'of', 'ice', 'liquid', 'and', 'gas', 'phase', 'water', 'the', 'use', 'of', 'a', 'full', 'corehole', 'fch', 'in', 'the', 'calculations', 'as', 'suggested', 'by', 'hetenyi', 'e... | [-0.04604037237429489, 0.0662967785774322, -0.041296778390644474, 0.027673709551604947, 0.01758555977950605, -0.08900790825862898, 0.10464357813883028, 0.3533638378898247, -0.1296016568516831, -0.3958311962445131, 0.005666260649397802, -0.32866972209781076, -0.08095754548028279, 0.1372691688593477, -0.0195329862207258,... |
707.2912 | Frictional quantum decoherence | The dynamics associated with a measurement-based master equation for quantum
Brownian motion are investigated. A scheme for obtaining time evolution from
general initial conditions is derived. This is applied to analyze dissipation
and decoherence in the evolution of both a Gaussian and a Schr\"{o}dinger cat
initial ... | quant-ph | the dynamics associated with a measurementbased master equation for quantum brownian motion are investigated a scheme for obtaining time evolution from general initial conditions is derived this is applied to analyze dissipation and decoherence in the evolution of both a gaussian and a schrodinger cat initial state dep... | [['the', 'dynamics', 'associated', 'with', 'a', 'measurementbased', 'master', 'equation', 'for', 'quantum', 'brownian', 'motion', 'are', 'investigated', 'a', 'scheme', 'for', 'obtaining', 'time', 'evolution', 'from', 'general', 'initial', 'conditions', 'is', 'derived', 'this', 'is', 'applied', 'to', 'analyze', 'dissipa... | [-0.12629328553071795, 0.11770814898259499, -0.13450833716813257, 0.06487667448613245, -0.027628395333201352, -0.12652525004437742, -0.030911549706669414, 0.34537874359418363, -0.2759728550582248, -0.23845460706883492, 0.09360000520246103, -0.2242165831164183, -0.09770290783661253, 0.20722116423798176, -0.0139347340035... |
707.2913 | Possible vortex splitting in the cuprate superconductors | We propose that the observed splitting of the vortices in the cuprates into
fractional vortices (partons) may be of static rather than of dynamic origin.
This interpretation is backed by a study of a model with a dominant d-wave and
subdominant s-wave pairing interaction. We find that the vortex may split into
two pa... | cond-mat.supr-con | we propose that the observed splitting of the vortices in the cuprates into fractional vortices partons may be of static rather than of dynamic origin this interpretation is backed by a study of a model with a dominant dwave and subdominant swave pairing interaction we find that the vortex may split into two partons bo... | [['we', 'propose', 'that', 'the', 'observed', 'splitting', 'of', 'the', 'vortices', 'in', 'the', 'cuprates', 'into', 'fractional', 'vortices', 'partons', 'may', 'be', 'of', 'static', 'rather', 'than', 'of', 'dynamic', 'origin', 'this', 'interpretation', 'is', 'backed', 'by', 'a', 'study', 'of', 'a', 'model', 'with', 'a... | [-0.20849264489704553, 0.2801619540184253, -0.12328386768112304, 0.11103499933853056, -0.0395436824032071, -0.13125583729534238, 0.06576231065749501, 0.33363307326281855, -0.23706130356165683, -0.25753256149969445, 0.0008506926447066858, -0.31781263804684085, -0.03998489813723912, 0.09980563441489788, 0.066878953827889... |
707.2914 | Pretty clean monomial ideals and linear quotients | We study basic properties of monomial ideals with linear quotients. It is
shown that if the monomial ideal $I$ has linear quotients, then the squarefree
part of $I$ and each component of $I$ as well as $\mm I$ have linear quotients,
where $\mm$ is the graded maximal ideal of the polynomial ring. As an analogy
to the ... | math.AC | we study basic properties of monomial ideals with linear quotients it is shown that if the monomial ideal i has linear quotients then the squarefree part of i and each component of i as well as mm i have linear quotients where mm is the graded maximal ideal of the polynomial ring as an analogy to the rearrangement lemm... | [['we', 'study', 'basic', 'properties', 'of', 'monomial', 'ideals', 'with', 'linear', 'quotients', 'it', 'is', 'shown', 'that', 'if', 'the', 'monomial', 'ideal', 'i', 'has', 'linear', 'quotients', 'then', 'the', 'squarefree', 'part', 'of', 'i', 'and', 'each', 'component', 'of', 'i', 'as', 'well', 'as', 'mm', 'i', 'have... | [-0.09116566799514528, 0.08012669837842362, -0.06400871298675026, 0.010276930748618076, -0.0898940825848175, -0.15796889297930258, -0.049635101343904225, 0.3472385837882757, -0.37972532853484153, -0.1638437996033047, 0.12156396646318691, -0.2764592316028263, -0.17423734136990138, 0.15952551499142179, -0.119074034672230... |
707.2915 | Gamma-ray background: a review | The gamma-ray background is still a subject under great debate.
All phenomena in the universe emitting gamma-rays can contribute directly as
diffuse emission or as an isotropic component from unresolved point sources.
The question of the origin of the extragalactic component cannot be answered
without determining t... | astro-ph | the gammaray background is still a subject under great debate all phenomena in the universe emitting gammarays can contribute directly as diffuse emission or as an isotropic component from unresolved point sources the question of the origin of the extragalactic component cannot be answered without determining the galac... | [['the', 'gammaray', 'background', 'is', 'still', 'a', 'subject', 'under', 'great', 'debate', 'all', 'phenomena', 'in', 'the', 'universe', 'emitting', 'gammarays', 'can', 'contribute', 'directly', 'as', 'diffuse', 'emission', 'or', 'as', 'an', 'isotropic', 'component', 'from', 'unresolved', 'point', 'sources', 'the', '... | [-0.035397499710781856, 0.15581917972189474, -0.021935237545436352, 0.1584760432322562, -0.12383556264888212, -0.017429678931078885, 0.019201557959032275, 0.40662231474193966, -0.23580983245556944, -0.3197018661002597, 0.053597618129857805, -0.3390703483411435, -0.010806137729917517, 0.23065599397065514, -0.02227676495... |
707.2916 | Effect of connecting wires on the decoherence due to electron-electron
interaction in a metallic ring | We consider the weak localization in a ring connected to reservoirs through
leads of finite length and submitted to a magnetic field. The effect of
decoherence due to electron-electron interaction on the harmonics of AAS
oscillations is studied, and more specifically the effect of the leads. Two
results are obtained ... | cond-mat.dis-nn cond-mat.mes-hall | we consider the weak localization in a ring connected to reservoirs through leads of finite length and submitted to a magnetic field the effect of decoherence due to electronelectron interaction on the harmonics of aas oscillations is studied and more specifically the effect of the leads two results are obtained for sh... | [['we', 'consider', 'the', 'weak', 'localization', 'in', 'a', 'ring', 'connected', 'to', 'reservoirs', 'through', 'leads', 'of', 'finite', 'length', 'and', 'submitted', 'to', 'a', 'magnetic', 'field', 'the', 'effect', 'of', 'decoherence', 'due', 'to', 'electronelectron', 'interaction', 'on', 'the', 'harmonics', 'of', '... | [-0.20684468842534298, 0.20901065422099477, -0.0751893790775763, 0.07952976692927462, -0.019077660577175647, -0.13683317995348357, -0.024341695396670776, 0.3529699368794498, -0.26271870648978574, -0.24265123887820855, 0.05244626092424273, -0.2617162778654969, -0.11845435395126085, 0.23159988992847502, 0.007330796975446... |
707.2917 | Renormalization Group and Asymptotic Spin--Charge separation for Chiral
Luttinger liquids | The phenomenon of Spin-Charge separation in non-Fermi liquids is well
understood only in certain solvable d=1 fermionic systems. In this paper we
furnish the first example of asymptotic Spin-Charge separation in a d=1 non
solvable model. This goal is achieved using Renormalization Group approach
combined with Ward-Id... | cond-mat.str-el math-ph math.MP | the phenomenon of spincharge separation in nonfermi liquids is well understood only in certain solvable d1 fermionic systems in this paper we furnish the first example of asymptotic spincharge separation in a d1 non solvable model this goal is achieved using renormalization group approach combined with wardidentities a... | [['the', 'phenomenon', 'of', 'spincharge', 'separation', 'in', 'nonfermi', 'liquids', 'is', 'well', 'understood', 'only', 'in', 'certain', 'solvable', 'd1', 'fermionic', 'systems', 'in', 'this', 'paper', 'we', 'furnish', 'the', 'first', 'example', 'of', 'asymptotic', 'spincharge', 'separation', 'in', 'a', 'd1', 'non', ... | [-0.15382625358800092, 0.13821823986557621, -0.11031159620732069, 0.09957355979209145, -0.04835288624589642, -0.20596822579701743, 0.04436213688459247, 0.3695636202643315, -0.22596706597755353, -0.24915698312222959, 0.07194037896736215, -0.2303046137839556, -0.17386522754716377, 0.1588617919005143, -0.0446954006018738,... |
707.2918 | Anderson Localization of Bogolyubov Quasiparticles in Interacting
Bose-Einstein Condensates | We study the Anderson localization of Bogolyubov quasiparticles in an
interacting Bose-Einstein condensate (with healing length \xi) subjected to a
random potential (with finite correlation length \sigma_R). We derive
analytically the Lyapunov exponent as a function of the quasiparticle momentum
k and we study the lo... | cond-mat.other | we study the anderson localization of bogolyubov quasiparticles in an interacting boseeinstein condensate with healing length xi subjected to a random potential with finite correlation length sigma_r we derive analytically the lyapunov exponent as a function of the quasiparticle momentum k and we study the localization... | [['we', 'study', 'the', 'anderson', 'localization', 'of', 'bogolyubov', 'quasiparticles', 'in', 'an', 'interacting', 'boseeinstein', 'condensate', 'with', 'healing', 'length', 'xi', 'subjected', 'to', 'a', 'random', 'potential', 'with', 'finite', 'correlation', 'length', 'sigma_r', 'we', 'derive', 'analytically', 'the'... | [-0.1542354511638355, 0.24341126222227616, -0.07862502184465654, 0.08239744250905405, -0.0051333881127568455, -0.17512589598345196, 0.004791441743668073, 0.34978690654294103, -0.19368933510377556, -0.20154898748215702, -0.006686889393350635, -0.3573515082014979, -0.11404460971840681, 0.1817108978692474, 0.0344765806713... |
707.2919 | Spectroscopic analysis of two peculiar emission line stars: RJHA 49 and
SS73 21 | Aims: To investigate the spectra and the evolutionary stages of two peculiar
emission-line stars: RJHA 49 and SS73 21. Methods: We used low and high
resolution optical data. Line identifications and measurements were performed
for several features in their spectra. Results: For each object, we have
derived the extinc... | astro-ph | aims to investigate the spectra and the evolutionary stages of two peculiar emissionline stars rjha 49 and ss73 21 methods we used low and high resolution optical data line identifications and measurements were performed for several features in their spectra results for each object we have derived the extinction and th... | [['aims', 'to', 'investigate', 'the', 'spectra', 'and', 'the', 'evolutionary', 'stages', 'of', 'two', 'peculiar', 'emissionline', 'stars', 'rjha', '49', 'and', 'ss73', '21', 'methods', 'we', 'used', 'low', 'and', 'high', 'resolution', 'optical', 'data', 'line', 'identifications', 'and', 'measurements', 'were', 'perform... | [-0.04851394398047992, 0.03922073423758533, -0.05201393045692868, 0.06548097918045911, -0.06822956385202866, -0.14820018641514776, 0.062097608077823475, 0.4402665730102124, -0.16126163548161876, -0.34808231120761246, 0.09433901059998863, -0.29984158438594427, -0.07288136514195524, 0.16662888113677085, -0.05014760938149... |
707.292 | A non-homogeneous orbit of a diagonal subgroup | Let G=SL(n,R) with n>5. We construct examples of lattices Gamma of G,
subgroup A of the diagonal group and points x in G/Gamma such that the closure
of the orbit Ax is not homogeneous but does not factors through the action of a
one-parameter non-unipotent group. This contradicts a conjecture of Margulis.
| math.DS | let gslnr with n5 we construct examples of lattices gamma of g subgroup a of the diagonal group and points x in ggamma such that the closure of the orbit ax is not homogeneous but does not factors through the action of a oneparameter nonunipotent group this contradicts a conjecture of margulis | [['let', 'gslnr', 'with', 'n5', 'we', 'construct', 'examples', 'of', 'lattices', 'gamma', 'of', 'g', 'subgroup', 'a', 'of', 'the', 'diagonal', 'group', 'and', 'points', 'x', 'in', 'ggamma', 'such', 'that', 'the', 'closure', 'of', 'the', 'orbit', 'ax', 'is', 'not', 'homogeneous', 'but', 'does', 'not', 'factors', 'throug... | [-0.23554438978488393, 0.11590601038187742, -0.1178847667761147, -0.03467779179268023, -0.11611553368286467, -0.11391565931376581, 0.08678961400965265, 0.3663626484134618, -0.27047861484335917, -0.18148931904750712, 0.0942672463293717, -0.26634866353033076, -0.1279541536362148, 0.19440821074314563, -0.1401086371921587,... |
707.2921 | Covering a line segment with variable radius discs | The paper addresses the problem of locating sensors with a circular field of
view so that a given line segment is under full surveillance, which is termed
as the Disc Covering Problem on a Line. The cost of each sensor includes a
fixed component, and a variable component that is proportional to the
field-of-view area... | cs.DM cs.NA | the paper addresses the problem of locating sensors with a circular field of view so that a given line segment is under full surveillance which is termed as the disc covering problem on a line the cost of each sensor includes a fixed component and a variable component that is proportional to the fieldofview area when o... | [['the', 'paper', 'addresses', 'the', 'problem', 'of', 'locating', 'sensors', 'with', 'a', 'circular', 'field', 'of', 'view', 'so', 'that', 'a', 'given', 'line', 'segment', 'is', 'under', 'full', 'surveillance', 'which', 'is', 'termed', 'as', 'the', 'disc', 'covering', 'problem', 'on', 'a', 'line', 'the', 'cost', 'of',... | [-0.12552272377454884, 0.029126056078518356, -0.032420726292882084, 0.023714732028513163, -0.10304619255668122, -0.18857712149697026, 0.04511396381484483, 0.381135458588477, -0.2819381979378787, -0.3074486284008758, 0.16529409141060397, -0.26523328711825217, -0.14672751973521672, 0.20535804431746937, -0.114249574128261... |
707.2922 | Measurement of the tau- --> K- pi0 nu_tau Branching Fraction | A measurement of the tau- --> K- pi0 nu_tau branching fraction has been made
using 230.2 fb-1 of data recorded by the BABAR detector at the PEP-II e+ e-
collider, located at the Stanford Linear Accelerator Center (SLAC), at a center
of mass energy sqrt{s} close to 10.58 GeV. We measure BF(tau- --> K- pi0
nu_tau) = (0... | hep-ex | a measurement of the tau k pi0 nu_tau branching fraction has been made using 2302 fb1 of data recorded by the babar detector at the pepii e e collider located at the stanford linear accelerator center slac at a center of mass energy sqrts close to 1058 gev we measure bftau k pi0 nu_tau 0416 0003 stat 0018 syst | [['a', 'measurement', 'of', 'the', 'tau', 'k', 'pi0', 'nu_tau', 'branching', 'fraction', 'has', 'been', 'made', 'using', '2302', 'fb1', 'of', 'data', 'recorded', 'by', 'the', 'babar', 'detector', 'at', 'the', 'pepii', 'e', 'e', 'collider', 'located', 'at', 'the', 'stanford', 'linear', 'accelerator', 'center', 'slac', '... | [-0.09238516404152976, 0.19367036411281804, -0.10279032584793608, 0.04818680694985107, -0.028063493403445543, -0.15145070425331078, 0.0699303901858692, 0.2734676505085723, -0.12880986344454617, -0.3007733405664049, -0.1028341090322697, -0.5348023414483358, 0.2416362818812245, 0.16811434343730197, 0.09891493295736868, 0... |
707.2923 | The Odderon at RHIC and LHC | The Odderon remains an elusive object, 33 years after its invention. The
Odderon is now a fundamental object in QCD and CGC and it has to be found
experimentally if QCD and CGC are right. In the present talk, we show how to
find it at RHIC and LHC. The most spectacular signature of the Odderon is the
predicted differ... | hep-ph | the odderon remains an elusive object 33 years after its invention the odderon is now a fundamental object in qcd and cgc and it has to be found experimentally if qcd and cgc are right in the present talk we show how to find it at rhic and lhc the most spectacular signature of the odderon is the predicted difference be... | [['the', 'odderon', 'remains', 'an', 'elusive', 'object', '33', 'years', 'after', 'its', 'invention', 'the', 'odderon', 'is', 'now', 'a', 'fundamental', 'object', 'in', 'qcd', 'and', 'cgc', 'and', 'it', 'has', 'to', 'be', 'found', 'experimentally', 'if', 'qcd', 'and', 'cgc', 'are', 'right', 'in', 'the', 'present', 'tal... | [-0.05483339105304035, 0.19185625786612656, -0.16021010944885866, 0.08608249844595169, -0.04363480977536667, -0.11071726868653463, -0.018920080314966895, 0.36704065477741615, -0.2319612747533173, -0.29685254039109815, 0.07337646328821956, -0.34513806986312073, -0.03263699310639548, 0.1755957970532426, 0.041802849243616... |
707.2924 | On the Quantum Kolmogorov Complexity of Classical Strings | We show that classical and quantum Kolmogorov complexity of binary strings
agree up to an additive constant. Both complexities are defined as the minimal
length of any (classical resp. quantum) computer program that outputs the
corresponding string.
It follows that quantum complexity is an extension of classical co... | quant-ph | we show that classical and quantum kolmogorov complexity of binary strings agree up to an additive constant both complexities are defined as the minimal length of any classical resp quantum computer program that outputs the corresponding string it follows that quantum complexity is an extension of classical complexity ... | [['we', 'show', 'that', 'classical', 'and', 'quantum', 'kolmogorov', 'complexity', 'of', 'binary', 'strings', 'agree', 'up', 'to', 'an', 'additive', 'constant', 'both', 'complexities', 'are', 'defined', 'as', 'the', 'minimal', 'length', 'of', 'any', 'classical', 'resp', 'quantum', 'computer', 'program', 'that', 'output... | [-0.11909867669314597, 0.12946516325543847, -0.10599748304847514, 0.11137423536392173, -0.05943980944258245, -0.17947693121139752, 0.052434980067320995, 0.2777982228059284, -0.32656450671228493, -0.2631327857761973, 0.08569725285251295, -0.22495865506223506, -0.16773432604215963, 0.2794854003051766, -0.1249198607813491... |
707.2925 | Swift observations of high-redshift radio-loud quasars | We report on Swift observations of four z>2 radio-loud quasars (0212+735,
0537-286, 0836+710, and 2149-307), classified as blazars. The sources,
well-known emitters at soft-medium X-rays, were detected at >5sigma with the
BAT experiment in 15-150 keV. No flux variability was detected within the XRT
and BAT exposures,... | astro-ph | we report on swift observations of four z2 radioloud quasars 0212735 0537286 0836710 and 2149307 classified as blazars the sources wellknown emitters at softmedium xrays were detected at 5sigma with the bat experiment in 15150 kev no flux variability was detected within the xrt and bat exposures with the exception of 0... | [['we', 'report', 'on', 'swift', 'observations', 'of', 'four', 'z2', 'radioloud', 'quasars', '0212735', '0537286', '0836710', 'and', '2149307', 'classified', 'as', 'blazars', 'the', 'sources', 'wellknown', 'emitters', 'at', 'softmedium', 'xrays', 'were', 'detected', 'at', '5sigma', 'with', 'the', 'bat', 'experiment', '... | [-0.031118167861332667, 0.13343111313072326, -0.030503735476141346, 0.12327937091748904, -0.056034944098204226, -0.13992784287908983, 0.020447501364471436, 0.49120303371856955, -0.1367769727364109, -0.40110555480651816, 0.051949400689310664, -0.39471121782005714, 0.06382420794290532, 0.22492437161134757, -0.01971726080... |
707.2926 | Robust Hypothesis Testing with a Relative Entropy Tolerance | This paper considers the design of a minimax test for two hypotheses where
the actual probability densities of the observations are located in
neighborhoods obtained by placing a bound on the relative entropy between
actual and nominal densities. The minimax problem admits a saddle point which
is characterized. The r... | cs.IT math.IT | this paper considers the design of a minimax test for two hypotheses where the actual probability densities of the observations are located in neighborhoods obtained by placing a bound on the relative entropy between actual and nominal densities the minimax problem admits a saddle point which is characterized the robus... | [['this', 'paper', 'considers', 'the', 'design', 'of', 'a', 'minimax', 'test', 'for', 'two', 'hypotheses', 'where', 'the', 'actual', 'probability', 'densities', 'of', 'the', 'observations', 'are', 'located', 'in', 'neighborhoods', 'obtained', 'by', 'placing', 'a', 'bound', 'on', 'the', 'relative', 'entropy', 'between',... | [-0.13902060815314876, 0.06634472768254034, -0.0735075158498636, 0.07150405147623998, 0.01297862937378629, -0.15563878086509136, 0.10241676302393898, 0.29537879420080926, -0.23760608481470405, -0.304941521446425, 0.12243233255547949, -0.2691116014995226, -0.12363551869965726, 0.17765063649361454, -0.09993381287175708, ... |
707.2927 | Constructing simply laced Lie algebras from extremal elements | For any finite graph Gamma and any field K of characteristic unequal to 2 we
construct an algebraic variety X over K whose K-points parameterise K-Lie
algebras generated by extremal elements, corresponding to the vertices of the
graph, with prescribed commutation relations, corresponding to the non-edges.
After that,... | math.RA math.AG | for any finite graph gamma and any field k of characteristic unequal to 2 we construct an algebraic variety x over k whose kpoints parameterise klie algebras generated by extremal elements corresponding to the vertices of the graph with prescribed commutation relations corresponding to the nonedges after that we study ... | [['for', 'any', 'finite', 'graph', 'gamma', 'and', 'any', 'field', 'k', 'of', 'characteristic', 'unequal', 'to', '2', 'we', 'construct', 'an', 'algebraic', 'variety', 'x', 'over', 'k', 'whose', 'kpoints', 'parameterise', 'klie', 'algebras', 'generated', 'by', 'extremal', 'elements', 'corresponding', 'to', 'the', 'verti... | [-0.1702740162384147, 0.1117417423097672, -0.05953191922535785, 0.03240724486479452, -0.18205147564041022, -0.16340652495348015, 0.03543282580003739, 0.39408605825155973, -0.37462648185781944, -0.18281336377064386, 0.10385126324492888, -0.23496785697240669, -0.1217634286925507, 0.17914078610155207, -0.13356324540785489... |
707.2928 | Formation of Protoplanets from Massive Planetesimals in Binary Systems | More than half of stars reside in binary or multiple star systems and many
planets have been found in binary systems. From theoretical point of view,
however, whether or not the planetary formation proceeds in a binary system is
a very complex problem, because secular perturbation from the companion star
can easily s... | astro-ph | more than half of stars reside in binary or multiple star systems and many planets have been found in binary systems from theoretical point of view however whether or not the planetary formation proceeds in a binary system is a very complex problem because secular perturbation from the companion star can easily stir up... | [['more', 'than', 'half', 'of', 'stars', 'reside', 'in', 'binary', 'or', 'multiple', 'star', 'systems', 'and', 'many', 'planets', 'have', 'been', 'found', 'in', 'binary', 'systems', 'from', 'theoretical', 'point', 'of', 'view', 'however', 'whether', 'or', 'not', 'the', 'planetary', 'formation', 'proceeds', 'in', 'a', '... | [-0.14802180362364523, 0.17130862351788104, -0.09185512392553237, 0.07084708209131006, -0.05463316412642598, -0.06610051390016451, -0.009440599983329622, 0.30365114047912495, -0.263822378499328, -0.3098084549191144, 0.09075346930778393, -0.2513576539514481, -0.08487587928385386, 0.1683797690253002, -0.03698560070984487... |
707.2929 | Superbosonization of invariant random matrix ensembles | Superbosonization is a new variant of the method of commuting and
anti-commuting variables as used in studying random matrix models of disordered
and chaotic quantum systems. We here give a concise mathematical exposition of
the key formulas of superbosonization. Conceived by analogy with the
bosonization technique f... | math-ph math.MP | superbosonization is a new variant of the method of commuting and anticommuting variables as used in studying random matrix models of disordered and chaotic quantum systems we here give a concise mathematical exposition of the key formulas of superbosonization conceived by analogy with the bosonization technique for di... | [['superbosonization', 'is', 'a', 'new', 'variant', 'of', 'the', 'method', 'of', 'commuting', 'and', 'anticommuting', 'variables', 'as', 'used', 'in', 'studying', 'random', 'matrix', 'models', 'of', 'disordered', 'and', 'chaotic', 'quantum', 'systems', 'we', 'here', 'give', 'a', 'concise', 'mathematical', 'exposition',... | [-0.09674196424316335, 0.14087745706862384, -0.1070825523824634, 0.0880673354048688, -0.062667005742669, -0.18882756311922594, 0.011379177838780995, 0.30473295505389686, -0.22602538995206692, -0.2429481412711224, 0.07484167554727371, -0.23923424786811037, -0.19389528813911952, 0.19165921301924085, -0.044324978709346055... |
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