id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.0553 | Zooming in on light relic neutralinos by direct detection and
measurements of galactic antimatter | The DAMA Collaboration has recently analyzed its data of the extensive WIMP
direct search (DAMA/NaI) which detected an annual modulation, by taking into
account the channelling effect which occurs when an ion traverses a detector
with a crystalline structure. Among possible implications, this Collaboration
has consid... | hep-ph astro-ph hep-ex | the dama collaboration has recently analyzed its data of the extensive wimp direct search damanai which detected an annual modulation by taking into account the channelling effect which occurs when an ion traverses a detector with a crystalline structure among possible implications this collaboration has considered the... | [['the', 'dama', 'collaboration', 'has', 'recently', 'analyzed', 'its', 'data', 'of', 'the', 'extensive', 'wimp', 'direct', 'search', 'damanai', 'which', 'detected', 'an', 'annual', 'modulation', 'by', 'taking', 'into', 'account', 'the', 'channelling', 'effect', 'which', 'occurs', 'when', 'an', 'ion', 'traverses', 'a',... | [-0.10023695984924796, 0.1601334034862861, -0.09993852883929488, 0.10756638390996692, -0.08694124221917594, -0.08108653989968015, 0.06698613589692082, 0.3649922794667049, -0.22678082298941502, -0.3128886661603491, 0.044564322589905885, -0.3017224536986271, -0.08143634615299195, 0.22399263034704425, 0.020707499907428484... |
710.0554 | CP Violation and Neutrino Oscillations | We review the basic mechanisms of neutrino mass generation and the
corresponding structure of the lepton mixing matrix. We summarize the status of
three-neutrino oscillation parameters as determined from current observations,
using state-of-the-art solar and atmospheric neutrino fluxes, as well as latest
experimental... | hep-ph | we review the basic mechanisms of neutrino mass generation and the corresponding structure of the lepton mixing matrix we summarize the status of threeneutrino oscillation parameters as determined from current observations using stateoftheart solar and atmospheric neutrino fluxes as well as latest experimental data as ... | [['we', 'review', 'the', 'basic', 'mechanisms', 'of', 'neutrino', 'mass', 'generation', 'and', 'the', 'corresponding', 'structure', 'of', 'the', 'lepton', 'mixing', 'matrix', 'we', 'summarize', 'the', 'status', 'of', 'threeneutrino', 'oscillation', 'parameters', 'as', 'determined', 'from', 'current', 'observations', 'u... | [-0.06687284435043339, 0.20795349749415637, 0.03095815351577873, 0.15574622194129384, -0.09336362225173904, -0.12810229017433325, 0.0935944572443188, 0.3015866523052043, -0.23634001580223146, -0.3323192755434742, 0.13105577411252164, -0.2971170264148585, -0.12008257475170511, 0.22365697809756258, 0.03884162614547943, 0... |
710.0555 | Investigation of one boundary-value problem for elliptic type equation | The goal of the paper is to study a spectral problem corresponding to the
mixed problem for a sixth order weak parabolic equation.
| math.CA | the goal of the paper is to study a spectral problem corresponding to the mixed problem for a sixth order weak parabolic equation | [['the', 'goal', 'of', 'the', 'paper', 'is', 'to', 'study', 'a', 'spectral', 'problem', 'corresponding', 'to', 'the', 'mixed', 'problem', 'for', 'a', 'sixth', 'order', 'weak', 'parabolic', 'equation']] | [-0.12167862073882767, -0.03388301050796619, -0.06978227991772734, 0.08051579156586819, -0.15762810528521304, -0.05176529798494733, -0.014618443279608113, 0.2631403304960417, -0.3721155475663102, -0.2943388937527071, 0.15587850384738133, -0.2803045720995768, -0.11128211264377055, 0.1561335296896489, -0.0632948614656925... |
710.0556 | A Game Theoretic Approach to Quantum Information | This work is an application of game theory to quantum information. In a state
estimate, we are given observations distributed according to an unknown
distribution $P_{\theta}$ (associated with award $Q$), which Nature chooses at
random from the set $\{P_{\theta}: \theta \in \Theta \}$ according to a known
prior distr... | quant-ph cs.GT cs.IT math.IT | this work is an application of game theory to quantum information in a state estimate we are given observations distributed according to an unknown distribution p_theta associated with award q which nature chooses at random from the set p_theta theta in theta according to a known prior distribution mu on theta we produ... | [['this', 'work', 'is', 'an', 'application', 'of', 'game', 'theory', 'to', 'quantum', 'information', 'in', 'a', 'state', 'estimate', 'we', 'are', 'given', 'observations', 'distributed', 'according', 'to', 'an', 'unknown', 'distribution', 'p_theta', 'associated', 'with', 'award', 'q', 'which', 'nature', 'chooses', 'at',... | [-0.11530745635867458, 0.10889690967222013, -0.11316138559521995, 0.06375270943496038, -0.05899481691532966, -0.16145941794031496, 0.08247564141074139, 0.3374967153325225, -0.29237208678810434, -0.26603044590940983, 0.07185420838509207, -0.2864579148759896, -0.09860287590770785, 0.13848332713329883, -0.1587260419178302... |
710.0557 | Trace ideals for pseudo-differential operators and their commutators
with symbols in $\alpha$-modulation spaces | In this paper, we consider the trace property of pseudo-differential
operators with symbols in $\alpha$-modulation spaces.
| math.FA math.AP | in this paper we consider the trace property of pseudodifferential operators with symbols in alphamodulation spaces | [['in', 'this', 'paper', 'we', 'consider', 'the', 'trace', 'property', 'of', 'pseudodifferential', 'operators', 'with', 'symbols', 'in', 'alphamodulation', 'spaces']] | [-0.18470320908818394, 0.10111362970201299, -0.008550582802854478, 0.10896581011911621, -0.07166219411010388, -0.03382358720409684, -0.04696226718806429, 0.3747922512702644, -0.33289153035730124, -0.1137325381860137, 0.14739336191269103, -0.30681691667996347, -0.1916489431168884, 0.102431672567036, -0.224010371719487, ... |
710.0558 | The Stellar Mass Distribution in the Giant Star Forming Region NGC 346 | Deep F555W and F814W Hubble Space Telescope ACS images are the basis for a
study of the present day mass function (PDMF) of NGC346, the largest active
star forming region in the Small Magellanic Cloud (SMC). We find a PDMF slope
of Gamma=-1.43+/-0.18 in the mass range 0.8-60 Mo, in excellent agreement with
the Salpet... | astro-ph | deep f555w and f814w hubble space telescope acs images are the basis for a study of the present day mass function pdmf of ngc346 the largest active star forming region in the small magellanic cloud smc we find a pdmf slope of gamma143018 in the mass range 0860 mo in excellent agreement with the salpeter initial mass fu... | [['deep', 'f555w', 'and', 'f814w', 'hubble', 'space', 'telescope', 'acs', 'images', 'are', 'the', 'basis', 'for', 'a', 'study', 'of', 'the', 'present', 'day', 'mass', 'function', 'pdmf', 'of', 'ngc346', 'the', 'largest', 'active', 'star', 'forming', 'region', 'in', 'the', 'small', 'magellanic', 'cloud', 'smc', 'we', 'f... | [-0.06629149872749884, 0.09057709708047862, -0.10491686952823305, 0.12017145061298819, -0.09035674596384646, -0.009133447716162008, 0.06184965963251291, 0.4238229038363153, -0.16950080974368667, -0.36796978513466166, 0.023732992534695022, -0.22263750734235993, -0.032031710399065744, 0.18368275580120916, -0.066595349534... |
710.0559 | Panel and Pseudo-Panel Estimation of Cross-Sectional and Time Series
Elasticities of Food Consumption: The Case of American and Polish Data | The problem addressed in this article is the bias to income and expenditure
elasticities estimated on pseudo-panel data caused by measurement error and
unobserved heterogeneity. We gauge empirically these biases by comparing
cross-sectional, pseudo-panel and true panel data from both Polish and American
expenditure s... | stat.AP | the problem addressed in this article is the bias to income and expenditure elasticities estimated on pseudopanel data caused by measurement error and unobserved heterogeneity we gauge empirically these biases by comparing crosssectional pseudopanel and true panel data from both polish and american expenditure surveys ... | [['the', 'problem', 'addressed', 'in', 'this', 'article', 'is', 'the', 'bias', 'to', 'income', 'and', 'expenditure', 'elasticities', 'estimated', 'on', 'pseudopanel', 'data', 'caused', 'by', 'measurement', 'error', 'and', 'unobserved', 'heterogeneity', 'we', 'gauge', 'empirically', 'these', 'biases', 'by', 'comparing',... | [-0.030090910342179845, 0.11308365532957916, -0.046982459498246254, 0.16880975048086244, -0.09248040699012748, -0.11841292402051314, 0.156432070187293, 0.4054178913332978, -0.24102878674617684, -0.3589662107810074, 0.13009122025806039, -0.33211785320154563, -0.06975903004236823, 0.2000734569048699, -0.19872662920875436... |
710.056 | The lattice gluon propagator in stochastic perturbation theory | We calculate loop contributions up to four loops to the Landau gauge gluon
propagator in numerical stochastic perturbation theory. For different lattice
volumes we carefully extrapolate the Euler time step to zero for the Langevin
dynamics derived from the Wilson action. The one-loop result for the gluon
propagator i... | hep-lat | we calculate loop contributions up to four loops to the landau gauge gluon propagator in numerical stochastic perturbation theory for different lattice volumes we carefully extrapolate the euler time step to zero for the langevin dynamics derived from the wilson action the oneloop result for the gluon propagator is com... | [['we', 'calculate', 'loop', 'contributions', 'up', 'to', 'four', 'loops', 'to', 'the', 'landau', 'gauge', 'gluon', 'propagator', 'in', 'numerical', 'stochastic', 'perturbation', 'theory', 'for', 'different', 'lattice', 'volumes', 'we', 'carefully', 'extrapolate', 'the', 'euler', 'time', 'step', 'to', 'zero', 'for', 't... | [-0.09439565339901795, 0.21803847902143994, -0.153392446336026, 0.15288410675129854, -0.03402545644591252, -0.05562780583277345, 0.0624836008491305, 0.3361460034114619, -0.2241857507576545, -0.19662131828566393, 0.04946815148578025, -0.2957881833387849, -0.08794814383533472, 0.10263776439242064, 0.03469921081171681, 0.... |
710.0561 | Extragalactic Surveys: AGN physics and evolution | We review the most important findings on AGN physics and cosmological
evolution as obtained by extragalactic X-ray surveys and associated
multiwavelength observations. We briefly discuss the perspectives for future
enterprises and in particular the scientific case for an extremely deep (2-3
Ms) XMM survey.
| astro-ph | we review the most important findings on agn physics and cosmological evolution as obtained by extragalactic xray surveys and associated multiwavelength observations we briefly discuss the perspectives for future enterprises and in particular the scientific case for an extremely deep 23 ms xmm survey | [['we', 'review', 'the', 'most', 'important', 'findings', 'on', 'agn', 'physics', 'and', 'cosmological', 'evolution', 'as', 'obtained', 'by', 'extragalactic', 'xray', 'surveys', 'and', 'associated', 'multiwavelength', 'observations', 'we', 'briefly', 'discuss', 'the', 'perspectives', 'for', 'future', 'enterprises', 'an... | [-0.03860991475680335, 0.08607342755931313, -0.015051493209532717, 0.1631886167240075, -0.1525690007362176, -0.040536001144739035, 0.03107303158718754, 0.4450456547466191, -0.16667903149870902, -0.32420442885168915, 0.1777684721878772, -0.3572920464106243, -0.11355541752312671, 0.2998152262192558, 0.006975543981587345,... |
710.0562 | On the Origin of Strong-Field Polarity Inversion Lines | Several studies have correlated observations of impulsive solar activity --
flares and coronal mass ejections (CMEs) -- with the amount of magnetic flux
near strong-field polarity inversion lines (PILs) in active regions'
photospheric magnetic fields, as measured in line-of-sight (LOS) magnetograms.
Practically, this... | astro-ph | several studies have correlated observations of impulsive solar activity flares and coronal mass ejections cmes with the amount of magnetic flux near strongfield polarity inversion lines pils in active regions photospheric magnetic fields as measured in lineofsight los magnetograms practically this empirical correlatio... | [['several', 'studies', 'have', 'correlated', 'observations', 'of', 'impulsive', 'solar', 'activity', 'flares', 'and', 'coronal', 'mass', 'ejections', 'cmes', 'with', 'the', 'amount', 'of', 'magnetic', 'flux', 'near', 'strongfield', 'polarity', 'inversion', 'lines', 'pils', 'in', 'active', 'regions', 'photospheric', 'm... | [-0.17763232626271264, 0.2561906654868395, 0.054883190961454505, 0.17059328978047555, -0.055005817253503106, -0.06454221894764291, 0.01209634564934619, 0.47007013787265106, -0.1866267369959944, -0.4104448829437055, 0.04344114789899479, -0.23936845191756903, -0.1250632821259299, 0.20583237620616351, -0.05194171148625212... |
710.0563 | Newly observed charmed states: the case of X(3872) | I briefly review the properties of the hidden charm meson X(3872), discussing
some puzzling aspects concerning its theoretical interpretation.
| hep-ph | i briefly review the properties of the hidden charm meson x3872 discussing some puzzling aspects concerning its theoretical interpretation | [['i', 'briefly', 'review', 'the', 'properties', 'of', 'the', 'hidden', 'charm', 'meson', 'x3872', 'discussing', 'some', 'puzzling', 'aspects', 'concerning', 'its', 'theoretical', 'interpretation']] | [-0.07827328968989222, 0.1877256365198838, -0.10926874491729234, 0.2456224919541886, -0.19703262711041852, -0.15525760195267044, 0.1524196864154778, 0.2858538635467228, -0.24483787346827357, -0.15599569972408445, 0.03381979578223668, -0.32303861175712784, -0.13304187254490038, 0.033930365682432524, -0.01812392835946459... |
710.0564 | TP Decoding | `Tree pruning' (TP) is an algorithm for probabilistic inference on binary
Markov random fields. It has been recently derived by Dror Weitz and used to
construct the first fully polynomial approximation scheme for counting
independent sets up to the `tree uniqueness threshold.' It can be regarded as a
clever method fo... | cs.IT math.IT | tree pruning tp is an algorithm for probabilistic inference on binary markov random fields it has been recently derived by dror weitz and used to construct the first fully polynomial approximation scheme for counting independent sets up to the tree uniqueness threshold it can be regarded as a clever method for pruning ... | [['tree', 'pruning', 'tp', 'is', 'an', 'algorithm', 'for', 'probabilistic', 'inference', 'on', 'binary', 'markov', 'random', 'fields', 'it', 'has', 'been', 'recently', 'derived', 'by', 'dror', 'weitz', 'and', 'used', 'to', 'construct', 'the', 'first', 'fully', 'polynomial', 'approximation', 'scheme', 'for', 'counting',... | [-0.083438181581388, 0.08068219620393649, -0.11005326140430251, 0.1130254590734555, -0.10805987091806099, -0.15576791304398244, 0.1360977250711196, 0.4292345445972818, -0.3214725411234011, -0.2751365522036457, 0.09962896473229443, -0.18204390304707407, -0.20920608082893064, 0.19725636840719757, -0.04364710489691427, 0.... |
710.0565 | Quantum key distribution using a triggered quantum dot source emitting
near 1.3 microns | We report the distribution of a cryptographic key, secure from photon number
splitting attacks, over 35 km of optical fiber using single photons from an
InAs quantum dot emitting ~1.3 microns in a pillar microcavity. Using below
GaAs-bandgap optical excitation, we demonstrate suppression of multiphoton
emission to 10... | quant-ph | we report the distribution of a cryptographic key secure from photon number splitting attacks over 35 km of optical fiber using single photons from an inas quantum dot emitting 13 microns in a pillar microcavity using below gaasbandgap optical excitation we demonstrate suppression of multiphoton emission to 10 of the p... | [['we', 'report', 'the', 'distribution', 'of', 'a', 'cryptographic', 'key', 'secure', 'from', 'photon', 'number', 'splitting', 'attacks', 'over', '35', 'km', 'of', 'optical', 'fiber', 'using', 'single', 'photons', 'from', 'an', 'inas', 'quantum', 'dot', 'emitting', '13', 'microns', 'in', 'a', 'pillar', 'microcavity', '... | [-0.1559854768589139, 0.12435558586046681, -0.0758033027255442, -0.00485056183184497, 0.06592168361879885, -0.2223471589293331, 0.07035680332919583, 0.4755784438597038, -0.23919229693710803, -0.29335521078901367, -0.00015489531913772224, -0.25978770735673606, -0.004377813306637108, 0.27479478634195403, -0.0375872229784... |
710.0566 | Post-Outburst Observations of V1647 Ori: Detection of a Brief Warm,
Molecular Outflow | We present new observations of the fundamental ro-vibrational CO spectrum of
V1647 Ori, the young star whose recent outburst illuminated McNeil's Nebula.
Previous spectra, acquired during outburst in 2004 February and July, had shown
the CO emission lines to be broad and centrally peaked-similar to the CO
spectrum of... | astro-ph | we present new observations of the fundamental rovibrational co spectrum of v1647 ori the young star whose recent outburst illuminated mcneils nebula previous spectra acquired during outburst in 2004 february and july had shown the co emission lines to be broad and centrally peakedsimilar to the co spectrum of a typica... | [['we', 'present', 'new', 'observations', 'of', 'the', 'fundamental', 'rovibrational', 'co', 'spectrum', 'of', 'v1647', 'ori', 'the', 'young', 'star', 'whose', 'recent', 'outburst', 'illuminated', 'mcneils', 'nebula', 'previous', 'spectra', 'acquired', 'during', 'outburst', 'in', '2004', 'february', 'and', 'july', 'had... | [-0.03784479568074233, 0.08247008379997618, -0.04349267311641071, 0.009529005425437971, -0.07375536114959248, -0.10256205184710582, 0.0633496384498248, 0.4695376112428774, -0.1611098074213972, -0.393784846844017, 0.0857274886865887, -0.2932483574700912, -0.03378872393422861, 0.1248061624650159, -0.06045591024996107, -0... |
710.0567 | Dynamical Wave Function Collapse: Could It Have Cosmological
Consequences? | This talk was in response to the conference injunction to present "one bold
but half-baked idea that you have been thinking about recently.. .". After a
brief introduction to the ideas and formalism of the CSL theory of dynamical
wave function collapse, some possible cosmological effects associated with
applying it t... | quant-ph | this talk was in response to the conference injunction to present one bold but halfbaked idea that you have been thinking about recently after a brief introduction to the ideas and formalism of the csl theory of dynamical wave function collapse some possible cosmological effects associated with applying it to the creat... | [['this', 'talk', 'was', 'in', 'response', 'to', 'the', 'conference', 'injunction', 'to', 'present', 'one', 'bold', 'but', 'halfbaked', 'idea', 'that', 'you', 'have', 'been', 'thinking', 'about', 'recently', 'after', 'a', 'brief', 'introduction', 'to', 'the', 'ideas', 'and', 'formalism', 'of', 'the', 'csl', 'theory', '... | [-0.057207272951067846, 0.149466341056607, -0.16379315124993973, 0.09529744304335591, -0.15131793337112123, -0.09477898040998049, -0.01121204893147065, 0.3385266971520402, -0.20989410652017051, -0.3039882531897588, 0.12414335291621022, -0.2675771862437779, -0.2138923485509374, 0.12972556456754153, -0.03149805957959457,... |
710.0568 | Sparticle masses from hadronic decays | We present our work on reconstructing sparticle masses in purely hadronic
decay chains, using the $k_T$ jet-algorithm on Monte Carlo simulated events at
LHC energies.
| hep-ph | we present our work on reconstructing sparticle masses in purely hadronic decay chains using the k_t jetalgorithm on monte carlo simulated events at lhc energies | [['we', 'present', 'our', 'work', 'on', 'reconstructing', 'sparticle', 'masses', 'in', 'purely', 'hadronic', 'decay', 'chains', 'using', 'the', 'k_t', 'jetalgorithm', 'on', 'monte', 'carlo', 'simulated', 'events', 'at', 'lhc', 'energies']] | [-0.012631206540390849, 0.26329922148336965, -0.11959333091120546, 0.21279074612539262, -0.006886744988150895, -0.03178015002049506, 0.0358652296611884, 0.4611237586165468, -0.15934070312262824, -0.29525278011957806, 0.0006045287445886061, -0.3643582076765597, 0.12427176379909118, 0.18327947768072286, 0.177436995708073... |
710.0569 | Twisted mass QCD at finite temperature | We discuss the use of Wilson fermions with twisted mass for simulations of
QCD thermodynamics. As a prerequisite for a future analysis of the
finite-temperature transition making use of automatic O(a) improvement, we
investigate the phase structure in the space spanned by the hopping parameter
kappa, the coupling bet... | hep-lat | we discuss the use of wilson fermions with twisted mass for simulations of qcd thermodynamics as a prerequisite for a future analysis of the finitetemperature transition making use of automatic oa improvement we investigate the phase structure in the space spanned by the hopping parameter kappa the coupling beta and th... | [['we', 'discuss', 'the', 'use', 'of', 'wilson', 'fermions', 'with', 'twisted', 'mass', 'for', 'simulations', 'of', 'qcd', 'thermodynamics', 'as', 'a', 'prerequisite', 'for', 'a', 'future', 'analysis', 'of', 'the', 'finitetemperature', 'transition', 'making', 'use', 'of', 'automatic', 'oa', 'improvement', 'we', 'invest... | [-0.16949527217651306, 0.24504210300801788, -0.014739466773480484, 0.059173891858495385, -0.033789907150047344, -0.09543590418533567, 0.13677247241859505, 0.3696549328562525, -0.1818416208489654, -0.2438391803034111, 0.0933554168807381, -0.2580087180297399, -0.0911206571702106, 0.1204520593752566, 0.06813773075982775, ... |
710.057 | Dirac phase leptogenesis | I present here a concise summary of the preprint arXiv:0707.3024, written in
collaboration with A. Anisimov and P. Di Bari. There we discuss leptogenesis
when {\em CP} violation stems exlusively from the Dirac phase in the PMNS
mixing matrix. Under this assumption it turns out that the situation is very
constrained w... | hep-ph | i present here a concise summary of the preprint arxiv07073024 written in collaboration with a anisimov and p di bari there we discuss leptogenesis when em cp violation stems exlusively from the dirac phase in the pmns mixing matrix under this assumption it turns out that the situation is very constrained when a hierar... | [['i', 'present', 'here', 'a', 'concise', 'summary', 'of', 'the', 'preprint', 'arxiv07073024', 'written', 'in', 'collaboration', 'with', 'a', 'anisimov', 'and', 'p', 'di', 'bari', 'there', 'we', 'discuss', 'leptogenesis', 'when', 'em', 'cp', 'violation', 'stems', 'exlusively', 'from', 'the', 'dirac', 'phase', 'in', 'th... | [-0.1495361605417981, 0.2411731025935816, -0.051233433093875645, 0.14416705636457275, -0.07841803960618562, -0.1596551666535171, 0.07342746367711307, 0.30182753577329485, -0.20552276268468372, -0.2941281960262651, 0.07802286922066871, -0.27851421664069803, -0.06978434773793976, 0.14283091041392515, 0.007195123507907348... |
710.0571 | Analytic Expressions for Geometric Measure of Three Qubit States | A new method is developed to derive an algebraic equations for the geometric
measure of entanglement of three qubit pure states. The equations are derived
explicitly and solved in cases of most interest. These equations allow oneself
to derive the analytic expressions of the geometric entanglement measure in the
wide... | quant-ph | a new method is developed to derive an algebraic equations for the geometric measure of entanglement of three qubit pure states the equations are derived explicitly and solved in cases of most interest these equations allow oneself to derive the analytic expressions of the geometric entanglement measure in the wide ran... | [['a', 'new', 'method', 'is', 'developed', 'to', 'derive', 'an', 'algebraic', 'equations', 'for', 'the', 'geometric', 'measure', 'of', 'entanglement', 'of', 'three', 'qubit', 'pure', 'states', 'the', 'equations', 'are', 'derived', 'explicitly', 'and', 'solved', 'in', 'cases', 'of', 'most', 'interest', 'these', 'equatio... | [-0.14214655000346998, 0.17130743365550571, -0.06499899779100063, 0.05101711218522415, 0.012517826467144402, -0.21682599257708582, 0.01601128731777291, 0.322358982160318, -0.2491274547449521, -0.27096396164337466, 0.08591172254157507, -0.2578110806105181, -0.08150865959892557, 0.22718633685553494, -0.023504378770531947... |
710.0572 | The diagonal of the Stasheff polytope | We construct an A-infinity structure on the tensor product of two A-infinity
algebras by using the simplicial decomposition of the Stasheff polytope. The
key point is the construction of an operad AA-infinity based on the simplicial
Stasheff polytope. The operad AA-infinity admits a coassociative diagonal and
the ope... | math.AT math.QA | we construct an ainfinity structure on the tensor product of two ainfinity algebras by using the simplicial decomposition of the stasheff polytope the key point is the construction of an operad aainfinity based on the simplicial stasheff polytope the operad aainfinity admits a coassociative diagonal and the operad ainf... | [['we', 'construct', 'an', 'ainfinity', 'structure', 'on', 'the', 'tensor', 'product', 'of', 'two', 'ainfinity', 'algebras', 'by', 'using', 'the', 'simplicial', 'decomposition', 'of', 'the', 'stasheff', 'polytope', 'the', 'key', 'point', 'is', 'the', 'construction', 'of', 'an', 'operad', 'aainfinity', 'based', 'on', 't... | [-0.14127207376264236, 0.007094080878085004, -0.10601430742472813, 0.05038328837867625, -0.14604328784185486, -0.0722692117623582, -0.06519031760635206, 0.35573761492363504, -0.4356595156966029, -0.16928446394819263, 0.13089836424065604, -0.2145318629069103, -0.24975941919193073, 0.1018795949985852, -0.2507274847578358... |
710.0573 | Nonlinear Brownian Motion and Higgs Mechanism | An extension of the stochastic quantization scheme is proposed by adding
nonlinear terms to the field equations. Our modification is motivated by the
recently established theory of active Brownian motion. We discuss a way of
promoting this theory to the case of infinite degrees of freedom. Equilibrium
distributions c... | hep-th | an extension of the stochastic quantization scheme is proposed by adding nonlinear terms to the field equations our modification is motivated by the recently established theory of active brownian motion we discuss a way of promoting this theory to the case of infinite degrees of freedom equilibrium distributions can be... | [['an', 'extension', 'of', 'the', 'stochastic', 'quantization', 'scheme', 'is', 'proposed', 'by', 'adding', 'nonlinear', 'terms', 'to', 'the', 'field', 'equations', 'our', 'modification', 'is', 'motivated', 'by', 'the', 'recently', 'established', 'theory', 'of', 'active', 'brownian', 'motion', 'we', 'discuss', 'a', 'wa... | [-0.1443253036655755, 0.1562388536693172, -0.10875096062130957, 0.04692390820162977, -0.07420610364930458, -0.11011445136875453, 0.006041833118210177, 0.302733036610915, -0.2925448707102921, -0.31014224541575525, 0.06044441738715732, -0.23346719200756536, -0.1819458951702319, 0.1182600115369781, -0.03623102844064405, 0... |
710.0574 | Combinatorial Aspects of Elliptic Curves II: Relationship between
Elliptic Curves and Chip-Firing Games on Graphs | Let q be a power of a prime and E be an elliptic curve defined over F_q. In
"Combinatorial aspects of elliptic curves" [17], the present author examined a
sequence of polynomials which express the N_k's, the number of points on E over
the field extensions F_{q^k}, in terms of the parameters q and N_1 = #E(F_q).
These... | math.CO math.NT | let q be a power of a prime and e be an elliptic curve defined over f_q in combinatorial aspects of elliptic curves 17 the present author examined a sequence of polynomials which express the n_ks the number of points on e over the field extensions f_qk in terms of the parameters q and n_1 ef_q these polynomials have in... | [['let', 'q', 'be', 'a', 'power', 'of', 'a', 'prime', 'and', 'e', 'be', 'an', 'elliptic', 'curve', 'defined', 'over', 'f_q', 'in', 'combinatorial', 'aspects', 'of', 'elliptic', 'curves', '17', 'the', 'present', 'author', 'examined', 'a', 'sequence', 'of', 'polynomials', 'which', 'express', 'the', 'n_ks', 'the', 'number... | [-0.21634196193190292, 0.06805292148806075, -0.13049471190151962, 0.04035713180110179, -0.08146859219414182, -0.10214957515927381, 0.02184148919513973, 0.33165348388138227, -0.31149751994234975, -0.28063555311564414, 0.07702813202013203, -0.2540308441821253, -0.16395936357002938, 0.2328780449461192, -0.1283558284922037... |
710.0575 | Hadronic photon-photon scattering at LEP | Hadronic interactions of two quasi-real photons have been studied extensively
both during the LEP1 and the LEP2 data taking periods. The higher energies
available at LEP2 in particular opened regions of phase space where hadronic
processes can be predicted reliably by perturbative QCD calculations, usually
available ... | hep-ex | hadronic interactions of two quasireal photons have been studied extensively both during the lep1 and the lep2 data taking periods the higher energies available at lep2 in particular opened regions of phase space where hadronic processes can be predicted reliably by perturbative qcd calculations usually available to ne... | [['hadronic', 'interactions', 'of', 'two', 'quasireal', 'photons', 'have', 'been', 'studied', 'extensively', 'both', 'during', 'the', 'lep1', 'and', 'the', 'lep2', 'data', 'taking', 'periods', 'the', 'higher', 'energies', 'available', 'at', 'lep2', 'in', 'particular', 'opened', 'regions', 'of', 'phase', 'space', 'where... | [-0.059693889435509156, 0.23757237334061285, -0.06495147836755898, 0.12068927771907856, -0.031029884057954468, -0.11595286939550063, 0.033669578666188596, 0.391369963347398, -0.20238563060953185, -0.34902120037325496, 0.06748697722716064, -0.3617623867284394, 0.038415353608735166, 0.1900104657803052, 0.0808364197097975... |
710.0576 | Shrinkage and spectral filtering of correlation matrices: a comparison
via the Kullback-Leibler distance | The problem of filtering information from large correlation matrices is of
great importance in many applications. We have recently proposed the use of the
Kullback-Leibler distance to measure the performance of filtering algorithms in
recovering the underlying correlation matrix when the variables are described
by a ... | physics.data-an physics.soc-ph q-fin.ST | the problem of filtering information from large correlation matrices is of great importance in many applications we have recently proposed the use of the kullbackleibler distance to measure the performance of filtering algorithms in recovering the underlying correlation matrix when the variables are described by a mult... | [['the', 'problem', 'of', 'filtering', 'information', 'from', 'large', 'correlation', 'matrices', 'is', 'of', 'great', 'importance', 'in', 'many', 'applications', 'we', 'have', 'recently', 'proposed', 'the', 'use', 'of', 'the', 'kullbackleibler', 'distance', 'to', 'measure', 'the', 'performance', 'of', 'filtering', 'al... | [-0.03718601888470838, 0.004404906773150129, -0.1317031189961278, 0.10541787420262826, -0.044470494858535894, -0.08986123161815593, 0.027434579138492194, 0.43092233539842395, -0.3140482210918613, -0.27050148629401205, 0.13377168715511367, -0.3146513556332692, -0.20853198564651867, 0.1751867817492103, -0.100650774593384... |
710.0577 | Multi-Orbital Lattice Model for (Ga,Mn)As and Other Lightly Magnetically
Doped Zinc-Blende-Type Semiconductors | We present a Hamiltonian in real space which is well suited to study
numerically the behavior of holes introduced in III-V semiconductors by Mn
doping when the III$^{3+}$ ion is replaced by Mn$^{2+}$. We consider the actual
lattice with the diamond structure. Since the focus is on light doping by
acceptors, a bonding... | cond-mat.mtrl-sci | we present a hamiltonian in real space which is well suited to study numerically the behavior of holes introduced in iiiv semiconductors by mn doping when the iii3 ion is replaced by mn2 we consider the actual lattice with the diamond structure since the focus is on light doping by acceptors a bonding combination of ii... | [['we', 'present', 'a', 'hamiltonian', 'in', 'real', 'space', 'which', 'is', 'well', 'suited', 'to', 'study', 'numerically', 'the', 'behavior', 'of', 'holes', 'introduced', 'in', 'iiiv', 'semiconductors', 'by', 'mn', 'doping', 'when', 'the', 'iii3', 'ion', 'is', 'replaced', 'by', 'mn2', 'we', 'consider', 'the', 'actual... | [-0.11884640152146189, 0.16680283078109978, 0.02263934187246614, 0.06899856622426528, 0.03246706961462759, -0.14786452759423008, 0.061307761494971844, 0.4192786477676265, -0.24309556839188143, -0.29220369522838285, 0.020040170020598186, -0.3596644984591714, -0.1157824183159325, 0.17499536796277346, 0.05095762373522332,... |
710.0578 | The B-meson mass splitting from non-perturbative quenched lattice QCD | We perform the non-perturbative (quenched) renormalization of the
chromo-magnetic operator in Heavy Quark Effective Theory and its three-loop
matching to QCD. At order 1/m of the expansion, the operator is responsible for
the mass splitting between the pseudoscalar and vector B-mesons. These new
computed factors are ... | hep-lat hep-ph | we perform the nonperturbative quenched renormalization of the chromomagnetic operator in heavy quark effective theory and its threeloop matching to qcd at order 1m of the expansion the operator is responsible for the mass splitting between the pseudoscalar and vector bmesons these new computed factors are affected by ... | [['we', 'perform', 'the', 'nonperturbative', 'quenched', 'renormalization', 'of', 'the', 'chromomagnetic', 'operator', 'in', 'heavy', 'quark', 'effective', 'theory', 'and', 'its', 'threeloop', 'matching', 'to', 'qcd', 'at', 'order', '1m', 'of', 'the', 'expansion', 'the', 'operator', 'is', 'responsible', 'for', 'the', '... | [-0.08986321375206378, 0.23018043044651545, -0.06466638230319534, 0.1300176049252124, -0.042855005873466974, -0.08256993173355502, 0.06663508385307589, 0.3585051475924307, -0.21196856811210246, -0.25914773639358046, 0.04854329768360393, -0.30742974472897394, -0.05175314386100841, 0.12342457483412415, 0.0577246866139051... |
710.0579 | Late stages of the evolution of A-type stars on the main sequence:
comparison between observed chemical abundances and diffusion models for 8 Am
stars of the Praesepe cluster | Aims. We aim to provide observational constraints on diffusion models that
predict peculiar chemical abundances in the atmospheres of Am stars. We also
intend to check if chemical peculiarities and slow rotation can be explained by
the presence of a weak magnetic field.
Methods. We have obtained high resolution, hi... | astro-ph | aims we aim to provide observational constraints on diffusion models that predict peculiar chemical abundances in the atmospheres of am stars we also intend to check if chemical peculiarities and slow rotation can be explained by the presence of a weak magnetic field methods we have obtained high resolution high signal... | [['aims', 'we', 'aim', 'to', 'provide', 'observational', 'constraints', 'on', 'diffusion', 'models', 'that', 'predict', 'peculiar', 'chemical', 'abundances', 'in', 'the', 'atmospheres', 'of', 'am', 'stars', 'we', 'also', 'intend', 'to', 'check', 'if', 'chemical', 'peculiarities', 'and', 'slow', 'rotation', 'can', 'be',... | [-0.05510386205414723, 0.13326992726623943, -0.04518544431931678, 0.06798603124507395, -0.0737463425319821, -0.11706583704565608, 0.09054165799706536, 0.43590617391853653, -0.1447868883886441, -0.3565002447189023, 0.014885159751505563, -0.28410930780374355, -0.03672047923260591, 0.2018256111286783, -0.07774741139855221... |
710.058 | Primordial magnetic fields at preheating | Using lattice techniques we investigate the generation of long range
cosmological magnetic fields during a cold electroweak transition. We will show
how magnetic fields arise, during bubble collisions, in the form of magnetic
strings. We conjecture that these magnetic strings originate from the alignment
of magnetic ... | hep-lat astro-ph hep-ph | using lattice techniques we investigate the generation of long range cosmological magnetic fields during a cold electroweak transition we will show how magnetic fields arise during bubble collisions in the form of magnetic strings we conjecture that these magnetic strings originate from the alignment of magnetic dipole... | [['using', 'lattice', 'techniques', 'we', 'investigate', 'the', 'generation', 'of', 'long', 'range', 'cosmological', 'magnetic', 'fields', 'during', 'a', 'cold', 'electroweak', 'transition', 'we', 'will', 'show', 'how', 'magnetic', 'fields', 'arise', 'during', 'bubble', 'collisions', 'in', 'the', 'form', 'of', 'magneti... | [-0.20650696450136077, 0.3133747116728148, -0.041063630786186585, 0.12483875341319912, -0.03826200274724356, -0.03360809214596807, -0.03581693411712915, 0.3965147052379981, -0.26446884362892786, -0.320957730825938, 0.034155689329105676, -0.2113372158401803, -0.0704887671081323, 0.14497646943889034, 0.08474273590082435,... |
710.0581 | Quark and lepton masses and mixing in SO(10) with a GUT-scale vector
matter | We explore in detail the effective matter fermion mass sum-rules in a class
of renormalizable SUSY SO(10) grand unified models where the quark and lepton
mass and mixing patterns originate from non-decoupling effects of an extra
vector matter multiplet living around the unification scale. If the
renormalizable type-I... | hep-ph | we explore in detail the effective matter fermion mass sumrules in a class of renormalizable susy so10 grand unified models where the quark and lepton mass and mixing patterns originate from nondecoupling effects of an extra vector matter multiplet living around the unification scale if the renormalizable typeii contri... | [['we', 'explore', 'in', 'detail', 'the', 'effective', 'matter', 'fermion', 'mass', 'sumrules', 'in', 'a', 'class', 'of', 'renormalizable', 'susy', 'so10', 'grand', 'unified', 'models', 'where', 'the', 'quark', 'and', 'lepton', 'mass', 'and', 'mixing', 'patterns', 'originate', 'from', 'nondecoupling', 'effects', 'of', ... | [-0.09895981104743508, 0.30560834396086783, -0.016288461856453156, 0.23743879967709866, -0.07293623805659391, -0.15096070244624393, 0.054421595428366124, 0.2601180538171675, -0.21554431795119877, -0.2913825478086748, -0.011353581879719547, -0.2623155101588586, -0.08349512150602006, 0.04653967474019382, 0.03616923351897... |
710.0582 | Quantum Spin Hall Insulator State in HgTe Quantum Wells | Recent theory predicted that the Quantum Spin Hall Effect, a fundamentally
novel quantum state of matter that exists at zero external magnetic field, may
be realized in HgTe/(Hg,Cd)Te quantum wells. We have fabricated such sample
structures with low density and high mobility in which we can tune, through an
external ... | cond-mat.mes-hall | recent theory predicted that the quantum spin hall effect a fundamentally novel quantum state of matter that exists at zero external magnetic field may be realized in hgtehgcdte quantum wells we have fabricated such sample structures with low density and high mobility in which we can tune through an external gate volta... | [['recent', 'theory', 'predicted', 'that', 'the', 'quantum', 'spin', 'hall', 'effect', 'a', 'fundamentally', 'novel', 'quantum', 'state', 'of', 'matter', 'that', 'exists', 'at', 'zero', 'external', 'magnetic', 'field', 'may', 'be', 'realized', 'in', 'hgtehgcdte', 'quantum', 'wells', 'we', 'have', 'fabricated', 'such', ... | [-0.18097573298768238, 0.2717414441769046, -0.03625656929584327, -0.0274481732965629, 0.028713095459508998, -0.23142386630081155, 0.09494153011373468, 0.38341278785133154, -0.27893726516183165, -0.34232496181181793, -0.018491089762852197, -0.30078034688472405, -0.12357708612649605, 0.18980411840495706, 0.00923009646184... |
710.0583 | The SF running coupling with four flavours of staggered quarks | In order to study the running coupling in four-flavour QCD, we review the
set-up of the Schr\"odinger functional (SF) with staggered quarks. Staggered
quarks require lattices which, in the usual counting, have even spatial lattice
extent $L/a$ while the time extent $T/a$ must be odd. Setting $T=L$ is
therefore only p... | hep-lat | in order to study the running coupling in fourflavour qcd we review the setup of the schrodinger functional sf with staggered quarks staggered quarks require lattices which in the usual counting have even spatial lattice extent la while the time extent ta must be odd setting tl is therefore only possible up to rm oa wh... | [['in', 'order', 'to', 'study', 'the', 'running', 'coupling', 'in', 'fourflavour', 'qcd', 'we', 'review', 'the', 'setup', 'of', 'the', 'schrodinger', 'functional', 'sf', 'with', 'staggered', 'quarks', 'staggered', 'quarks', 'require', 'lattices', 'which', 'in', 'the', 'usual', 'counting', 'have', 'even', 'spatial', 'la... | [-0.10422586025854591, 0.20848604794568612, -0.06732084284914602, 0.0799922882579267, -0.07812027125573247, -0.11538508274859868, 0.03375071613924891, 0.3898715388841263, -0.20391689158865425, -0.2798071551035241, 0.05480012614487458, -0.2661591691730341, -0.04750650491344162, 0.049119763334493825, -0.00453779608066571... |
710.0584 | Exotic physics with ultrahigh energy cosmic rays | Ultrahigh energy cosmic rays provide a unique ground for probing new physics.
In this talk we review the possibility of testing TeV gravity in interactions
of cosmogenic neutrinos and the potential to discover long-lived exotic
particles in nucleon-produced air showers, such as gluinos of split-SUSY models
or staus o... | hep-ph | ultrahigh energy cosmic rays provide a unique ground for probing new physics in this talk we review the possibility of testing tev gravity in interactions of cosmogenic neutrinos and the potential to discover longlived exotic particles in nucleonproduced air showers such as gluinos of splitsusy models or staus of super... | [['ultrahigh', 'energy', 'cosmic', 'rays', 'provide', 'a', 'unique', 'ground', 'for', 'probing', 'new', 'physics', 'in', 'this', 'talk', 'we', 'review', 'the', 'possibility', 'of', 'testing', 'tev', 'gravity', 'in', 'interactions', 'of', 'cosmogenic', 'neutrinos', 'and', 'the', 'potential', 'to', 'discover', 'longlived... | [-0.08960561526732312, 0.36294360153584015, -0.055724822619662585, 0.2686655484032127, -0.06512293868042805, -0.13457022326205065, -0.011008074144936271, 0.3188344854861498, -0.2047485445401873, -0.4063785201007569, -0.0024841615307162066, -0.31091062628008703, 0.024146430207312934, 0.12707638433116866, 0.0436456384982... |
710.0585 | Dancing with black holes | We describe efforts over the last six years to implement regularization
methods suitable for studying one or more interacting black holes by direct
N-body simulations. Three different methods have been adapted to large-N
systems: (i) Time-Transformed Leapfrog, (ii) Wheel-Spoke, and (iii) Algorithmic
Regularization. T... | astro-ph | we describe efforts over the last six years to implement regularization methods suitable for studying one or more interacting black holes by direct nbody simulations three different methods have been adapted to largen systems i timetransformed leapfrog ii wheelspoke and iii algorithmic regularization these methods have... | [['we', 'describe', 'efforts', 'over', 'the', 'last', 'six', 'years', 'to', 'implement', 'regularization', 'methods', 'suitable', 'for', 'studying', 'one', 'or', 'more', 'interacting', 'black', 'holes', 'by', 'direct', 'nbody', 'simulations', 'three', 'different', 'methods', 'have', 'been', 'adapted', 'to', 'largen', '... | [-0.0598623465308226, 0.01202987759631682, -0.06817237798996428, 0.10500794705597961, -0.0971685760689186, -0.15778568508896104, -0.03084099624167256, 0.41782555346714056, -0.1436159243569412, -0.3260493350433225, 0.1386204204024212, -0.27956576712994263, -0.1341931227659014, 0.25750520356009376, -0.05138298855262234, ... |
710.0586 | Strict essential extensions of C*-algebras and Hilbert C*-modules | In the present paper we develop both ideas of D. Baki\'c and B. Gulja{\v{s}}
and the categorical approach to multipliers from E.C. Lance's book and
publications of the second author, for the introduction and study of left
multipliers of Hilbert $C^*$-modules. Some properties and, in particular, the
property of maxima... | math.OA | in the present paper we develop both ideas of d bakic and b guljavs and the categorical approach to multipliers from ec lances book and publications of the second author for the introduction and study of left multipliers of hilbert cmodules some properties and in particular the property of maximality among all strictly... | [['in', 'the', 'present', 'paper', 'we', 'develop', 'both', 'ideas', 'of', 'd', 'bakic', 'and', 'b', 'guljavs', 'and', 'the', 'categorical', 'approach', 'to', 'multipliers', 'from', 'ec', 'lances', 'book', 'and', 'publications', 'of', 'the', 'second', 'author', 'for', 'the', 'introduction', 'and', 'study', 'of', 'left'... | [-0.09074106962092358, 0.09627049512885234, -0.04297282082390868, 0.0888355005051751, -0.04947828712519603, -0.1756012736155686, -0.04510719104695858, 0.3406157934503561, -0.33111383546902623, -0.16992318623319821, 0.12620223276058418, -0.2860718328667173, -0.13967279168018312, 0.18560413128041006, -0.1035823499939094,... |
710.0587 | Single top-quark production by strong and electroweak supersymmetric
flavor-changing interactions at the LHC | (Abridged) We report on a complete study of the single top-quark production
by direct supersymmetric flavor-changing neutral-current (FCNC) processes at
the LHC. The total cross section for pp(gg)->t\bar{c}+\bar{t}c is computed at
the 1-loop order within the unconstrained Minimal Supersymmetric Standard Model
(MSSM).... | hep-ph | abridged we report on a complete study of the single topquark production by direct supersymmetric flavorchanging neutralcurrent fcnc processes at the lhc the total cross section for ppggtbarcbartc is computed at the 1loop order within the unconstrained minimal supersymmetric standard model mssm the present study extend... | [['abridged', 'we', 'report', 'on', 'a', 'complete', 'study', 'of', 'the', 'single', 'topquark', 'production', 'by', 'direct', 'supersymmetric', 'flavorchanging', 'neutralcurrent', 'fcnc', 'processes', 'at', 'the', 'lhc', 'the', 'total', 'cross', 'section', 'for', 'ppggtbarcbartc', 'is', 'computed', 'at', 'the', '1loop... | [-0.09011231694302264, 0.16482908831275037, -0.020376379902731497, 0.14556406663855184, -0.04062322295343118, -0.0960961541146891, 0.08074995158300415, 0.2931687765150604, -0.16971366018596795, -0.32336988582291865, 0.04001427905389172, -0.3168716909893756, -0.027646520145434148, 0.1765553013246972, 0.01199418527452006... |
710.0588 | On the Fraction of Quasars with Outflows | Outflows from active galactic nuclei (AGNs) seem to be common and are thought
to be important from a variety of perspectives: as an agent of chemical
enhancement of the interstellar and intergalactic media, as an agent of angular
momentum removal from the accreting central engine, and as an agent limiting
star format... | astro-ph | outflows from active galactic nuclei agns seem to be common and are thought to be important from a variety of perspectives as an agent of chemical enhancement of the interstellar and intergalactic media as an agent of angular momentum removal from the accreting central engine and as an agent limiting star formation in ... | [['outflows', 'from', 'active', 'galactic', 'nuclei', 'agns', 'seem', 'to', 'be', 'common', 'and', 'are', 'thought', 'to', 'be', 'important', 'from', 'a', 'variety', 'of', 'perspectives', 'as', 'an', 'agent', 'of', 'chemical', 'enhancement', 'of', 'the', 'interstellar', 'and', 'intergalactic', 'media', 'as', 'an', 'age... | [-0.05262588203917656, 0.06957932003550568, -0.04678787003186616, 0.0951021467839781, -0.12653783750863506, -0.07851233954894989, 0.05436868025836619, 0.4329614934118036, -0.2144342153532341, -0.33036223937443554, 0.07035511946069067, -0.31072908260530846, -0.04714546416622193, 0.2224167861806398, -0.024018492410208453... |
710.0589 | The Lopsidedness of Present-Day Galaxies: Results from the Sloan Digital
Sky Survey | Large-scale asymmetries in the stellar mass distribution in galaxies are
believed to trace non-equilibrium situations in the luminous and/or dark matter
component. These may arise in the aftermath of events like mergers, accretion,
and tidal interactions. These events are key in the evolution of galaxies. In
this pap... | astro-ph | largescale asymmetries in the stellar mass distribution in galaxies are believed to trace nonequilibrium situations in the luminous andor dark matter component these may arise in the aftermath of events like mergers accretion and tidal interactions these events are key in the evolution of galaxies in this paper we quan... | [['largescale', 'asymmetries', 'in', 'the', 'stellar', 'mass', 'distribution', 'in', 'galaxies', 'are', 'believed', 'to', 'trace', 'nonequilibrium', 'situations', 'in', 'the', 'luminous', 'andor', 'dark', 'matter', 'component', 'these', 'may', 'arise', 'in', 'the', 'aftermath', 'of', 'events', 'like', 'mergers', 'accre... | [-0.09695647732234043, 0.15573348979105578, -0.08021866680553695, 0.15139874586739355, -0.07978575308392435, -0.017389822725361204, -0.02652447057302536, 0.411212471513613, -0.18686556386495545, -0.35978794215164084, 0.052691339150821484, -0.2898101257438383, -0.0942909629140728, 0.18399940141079782, -0.057582844486120... |
710.059 | Speed of Meridional Flows and Magnetic Flux Transport on the Sun | We use the magnetic butterfly diagram to determine the speed of the magnetic
flux transport on the solar surface towards the poles. The manifestation of the
flux transport is clearly visible as elongated structures extended from the
sunspot belt to the polar regions. The slopes of these structures are measured
and in... | astro-ph | we use the magnetic butterfly diagram to determine the speed of the magnetic flux transport on the solar surface towards the poles the manifestation of the flux transport is clearly visible as elongated structures extended from the sunspot belt to the polar regions the slopes of these structures are measured and interp... | [['we', 'use', 'the', 'magnetic', 'butterfly', 'diagram', 'to', 'determine', 'the', 'speed', 'of', 'the', 'magnetic', 'flux', 'transport', 'on', 'the', 'solar', 'surface', 'towards', 'the', 'poles', 'the', 'manifestation', 'of', 'the', 'flux', 'transport', 'is', 'clearly', 'visible', 'as', 'elongated', 'structures', 'e... | [-0.15999689777716172, 0.18763532062338983, -0.055939240417139637, 0.09491452493818055, -0.0315274012735556, -0.019110017000743863, -0.007817925284590922, 0.37647685430203026, -0.2842904160529869, -0.33665112845434997, 0.07613581513904147, -0.23852771413975615, -0.09250944349091521, 0.2417772103529372, -0.0295763466894... |
710.0591 | Fully Sampled Maps of Ices and Silicates in Front of Cepheus A East with
Spitzer | We report the first fully sampled maps of the distribution of interstellar
CO2 ices, H2O ices and total hydrogen nuclei, as inferred from the 9.7 micron
silicate feature, toward the star-forming region Cepheus A East with the IRS
instrument onboard the Spitzer Space Telescope. We find that the column density
distribu... | astro-ph | we report the first fully sampled maps of the distribution of interstellar co2 ices h2o ices and total hydrogen nuclei as inferred from the 97 micron silicate feature toward the starforming region cepheus a east with the irs instrument onboard the spitzer space telescope we find that the column density distributions fo... | [['we', 'report', 'the', 'first', 'fully', 'sampled', 'maps', 'of', 'the', 'distribution', 'of', 'interstellar', 'co2', 'ices', 'h2o', 'ices', 'and', 'total', 'hydrogen', 'nuclei', 'as', 'inferred', 'from', 'the', '97', 'micron', 'silicate', 'feature', 'toward', 'the', 'starforming', 'region', 'cepheus', 'a', 'east', '... | [-0.04467886508454453, 0.15614401441354248, -0.01772706223004238, 0.020802729026126662, 0.03739724589048089, -0.03698023514374451, 0.07540465718387054, 0.43398321389576394, -0.22928272527412716, -0.3143638100893768, 0.081809371758788, -0.2908327103514512, -0.03491744429848353, 0.08911603877556715, 0.03345289632471682, ... |
710.0592 | Accuracy of approximation of subharmonic functions by logarithms of
moduli of analytic ones in Chebyshev metrics | It is known that a subharmonic function of finite order $\rho$ can be
approximated by the logarithm of the modulus of an entire function at the point
$z$ outside an exceptional set up to $C\log|z|$. In this article we prove that
if such an approximation is made more precise, i. e. a constant
$C$ decreases, then, be... | math.CV | it is known that a subharmonic function of finite order rho can be approximated by the logarithm of the modulus of an entire function at the point z outside an exceptional set up to clogz in this article we prove that if such an approximation is made more precise i e a constant c decreases then beginning with crho4 the... | [['it', 'is', 'known', 'that', 'a', 'subharmonic', 'function', 'of', 'finite', 'order', 'rho', 'can', 'be', 'approximated', 'by', 'the', 'logarithm', 'of', 'the', 'modulus', 'of', 'an', 'entire', 'function', 'at', 'the', 'point', 'z', 'outside', 'an', 'exceptional', 'set', 'up', 'to', 'clogz', 'in', 'this', 'article', ... | [-0.11927094518150724, 0.11383369769616396, -0.06962061054738504, 0.04054568722910647, -0.04825378515358482, -0.0917743132986988, 0.06818643967099078, 0.33678171087752334, -0.29493523126590876, -0.22257591513814506, 0.0960471956136094, -0.26805234196401395, -0.13769226128511786, 0.23325880329319082, -0.0498587646787720... |
710.0593 | Novel Precursors for Boron Nanotubes: The Competition of Two-Center and
Three-Center Bonding in Boron Sheets | We present a new class of boron sheets, composed of triangular and hexagonal
motifs, that are more stable than structures considered to date and thus are
likely to be the precursors of boron nanotubes. We describe a simple and clear
picture of electronic bonding in boron sheets and highlight the importance of
three-c... | cond-mat.mtrl-sci | we present a new class of boron sheets composed of triangular and hexagonal motifs that are more stable than structures considered to date and thus are likely to be the precursors of boron nanotubes we describe a simple and clear picture of electronic bonding in boron sheets and highlight the importance of threecenter ... | [['we', 'present', 'a', 'new', 'class', 'of', 'boron', 'sheets', 'composed', 'of', 'triangular', 'and', 'hexagonal', 'motifs', 'that', 'are', 'more', 'stable', 'than', 'structures', 'considered', 'to', 'date', 'and', 'thus', 'are', 'likely', 'to', 'be', 'the', 'precursors', 'of', 'boron', 'nanotubes', 'we', 'describe',... | [-0.11408759318703018, 0.10553281819995712, -0.011987137553446433, 0.02429825574543108, -0.019707585605518784, -0.1178292835733908, 0.11612276096061311, 0.456362043014344, -0.24395703510347042, -0.2604363128561732, -0.016646184058695595, -0.3305300402948085, -0.22262361860176658, 0.1546768798985902, 0.02557916952406658... |
710.0594 | Absence of Quantum States Corresponding to Unstable Classical Channels | We consider Hamiltonian systems of a certain class with unstable orbits
moving to infinity. We prove a theorem showing that analogous quantum states do
not exist. This theorem is applied to Schrodinger operators with potentials of
degree zero which are Morse when restricted to the unit sphere.
| math-ph math.MP | we consider hamiltonian systems of a certain class with unstable orbits moving to infinity we prove a theorem showing that analogous quantum states do not exist this theorem is applied to schrodinger operators with potentials of degree zero which are morse when restricted to the unit sphere | [['we', 'consider', 'hamiltonian', 'systems', 'of', 'a', 'certain', 'class', 'with', 'unstable', 'orbits', 'moving', 'to', 'infinity', 'we', 'prove', 'a', 'theorem', 'showing', 'that', 'analogous', 'quantum', 'states', 'do', 'not', 'exist', 'this', 'theorem', 'is', 'applied', 'to', 'schrodinger', 'operators', 'with', '... | [-0.18717843547780463, 0.16268554745994984, -0.1106093390349378, 0.07655884999227017, -0.06099136786515567, -0.23490327479753723, 0.02056852040225343, 0.3488669334811733, -0.25890840534517107, -0.1821931426988003, 0.0760250817241266, -0.27039775038336183, -0.15689246118702788, 0.18306362383473823, -0.10502625375669053,... |
710.0595 | Ratio of charm to bottom R_AA as a test of pQCD vs. AdS/CFT energy loss | LHC predictions for the charm and bottom nuclear modification factors using
pQCD and AdS/CFT drag energy loss models are given. We show that a new
observable, the double ratio of charm to bottom nuclear modification factors,
allows for easy experimental distinction between the two classes of energy loss
models.
| hep-ph | lhc predictions for the charm and bottom nuclear modification factors using pqcd and adscft drag energy loss models are given we show that a new observable the double ratio of charm to bottom nuclear modification factors allows for easy experimental distinction between the two classes of energy loss models | [['lhc', 'predictions', 'for', 'the', 'charm', 'and', 'bottom', 'nuclear', 'modification', 'factors', 'using', 'pqcd', 'and', 'adscft', 'drag', 'energy', 'loss', 'models', 'are', 'given', 'we', 'show', 'that', 'a', 'new', 'observable', 'the', 'double', 'ratio', 'of', 'charm', 'to', 'bottom', 'nuclear', 'modification', ... | [-0.02098209579114099, 0.19303931931166776, -0.13443783147982796, 0.19235701779169695, -0.06485894307190058, -0.14972279926914037, 0.06501124822059456, 0.373051898439928, -0.2647798059850323, -0.309957940853676, -0.059730410623383155, -0.31168462093283983, -0.01256200334779462, 0.1798768189488625, 0.028050188640398637,... |
710.0596 | Commuting Families in Temperley-Lieb Algebras | We define analogs of the Jucys-Murphy elements for the affine Temperley-Lieb
algebra and give their explicit expansion in terms of the basis of planar
Brauer diagrams. These Jucys-Murphy elements are a family of commuting elements
in the affine Temperley-Lieb algebra, and we compute their eigenvalues on the
generic i... | math.RT math.QA | we define analogs of the jucysmurphy elements for the affine temperleylieb algebra and give their explicit expansion in terms of the basis of planar brauer diagrams these jucysmurphy elements are a family of commuting elements in the affine temperleylieb algebra and we compute their eigenvalues on the generic irreducib... | [['we', 'define', 'analogs', 'of', 'the', 'jucysmurphy', 'elements', 'for', 'the', 'affine', 'temperleylieb', 'algebra', 'and', 'give', 'their', 'explicit', 'expansion', 'in', 'terms', 'of', 'the', 'basis', 'of', 'planar', 'brauer', 'diagrams', 'these', 'jucysmurphy', 'elements', 'are', 'a', 'family', 'of', 'commuting'... | [-0.1344751811120659, 0.11291342481221679, -0.07734335827357743, 0.012289899694935782, -0.10391690549643143, -0.06030093008935775, -0.02264757510325264, 0.3488522738714338, -0.37177210896397417, -0.16439554083120564, 0.09223296144552043, -0.27536796948761155, -0.18191698815106697, 0.1865325817413142, -0.122415932442021... |
710.0597 | Highly Collimated Jets and Wide-Angle Outflows in HH46/47: New Evidence
from Spitzer IR Images | We present new details of the structure and morphology of the jets and
outflows in HH46/47 as seen in Spitzer infrared images from IRAC and MIPS,
reprocessed using the ``HiRes'' deconvolution technique. HiRes improves the
visualization of spatial morphology by enhancing resolution (to sub-arcsec
levels in IRAC bands)... | astro-ph | we present new details of the structure and morphology of the jets and outflows in hh4647 as seen in spitzer infrared images from irac and mips reprocessed using the hires deconvolution technique hires improves the visualization of spatial morphology by enhancing resolution to subarcsec levels in irac bands and removin... | [['we', 'present', 'new', 'details', 'of', 'the', 'structure', 'and', 'morphology', 'of', 'the', 'jets', 'and', 'outflows', 'in', 'hh4647', 'as', 'seen', 'in', 'spitzer', 'infrared', 'images', 'from', 'irac', 'and', 'mips', 'reprocessed', 'using', 'the', 'hires', 'deconvolution', 'technique', 'hires', 'improves', 'the'... | [-0.017120917262161136, 0.05285604164741317, -0.061028212096219454, 0.0647789249563311, -0.10418536458311119, -0.09103653167959258, 0.02235628373271925, 0.5243627066159342, -0.22091956865571816, -0.3312838192457172, 0.044587464480638855, -0.3057410213656313, 0.010567211337006234, 0.13400536706381455, -0.018273491652106... |
710.0598 | Cosmic gamma-ray burst 060428C detected in the fields of view of the
IBIS and SPI telescopes of the INTEGRAL observatory and its early afterglow | Analyzing archival data of the INTEGRAL observatory we discovered and
localized a cosmic gamma-ray burst detected within fields of view of the
IBIS/ISGRI and SPI telescopes on April 28, 2006. The burst has not been
revealed by the INTEGRAL Burst Alert System (IBAS), so the information on its
coordinates has not been ... | astro-ph | analyzing archival data of the integral observatory we discovered and localized a cosmic gammaray burst detected within fields of view of the ibisisgri and spi telescopes on april 28 2006 the burst has not been revealed by the integral burst alert system ibas so the information on its coordinates has not been distribut... | [['analyzing', 'archival', 'data', 'of', 'the', 'integral', 'observatory', 'we', 'discovered', 'and', 'localized', 'a', 'cosmic', 'gammaray', 'burst', 'detected', 'within', 'fields', 'of', 'view', 'of', 'the', 'ibisisgri', 'and', 'spi', 'telescopes', 'on', 'april', '28', '2006', 'the', 'burst', 'has', 'not', 'been', 'r... | [-0.07394448663792846, 0.15411868037293008, -0.08275126528597491, 0.1306384270243785, -0.06780708115547895, -0.10869922801742658, 0.07641305061372217, 0.4662486201888361, -0.16582528348149295, -0.422156539197792, 0.09778798414832529, -0.3577801016104572, 0.003491106388323447, 0.22442243511939203, 0.002932676288080128, ... |
710.0599 | Nonlinear Optical Spectroscopy of Photonic Metamaterials | We have obtained spectra of second-harmonic generation, third harmonic
generation, and four-wave mixing from a fishnet metamaterial around its
magnetic resonance. The resonant behaviors are distinctly different from those
for ordinary materials. They result from the fact that the resonance is
plasmonic, and its enhan... | cond-mat.mtrl-sci cond-mat.other | we have obtained spectra of secondharmonic generation third harmonic generation and fourwave mixing from a fishnet metamaterial around its magnetic resonance the resonant behaviors are distinctly different from those for ordinary materials they result from the fact that the resonance is plasmonic and its enhancement ap... | [['we', 'have', 'obtained', 'spectra', 'of', 'secondharmonic', 'generation', 'third', 'harmonic', 'generation', 'and', 'fourwave', 'mixing', 'from', 'a', 'fishnet', 'metamaterial', 'around', 'its', 'magnetic', 'resonance', 'the', 'resonant', 'behaviors', 'are', 'distinctly', 'different', 'from', 'those', 'for', 'ordina... | [-0.13733386617364748, 0.19149500201016945, -0.052743464620467626, 0.005761909010855235, -0.058108844214452886, -0.0955679185319481, -0.01799427774154915, 0.4378366006432839, -0.2754076892896643, -0.3080374881765752, 0.023014898207653664, -0.33573357985829405, -0.21150813685765243, 0.2591887967625879, 0.058194001318386... |
710.06 | A Search for EHB Pulsators in the Globular Cluster NGC 6752 | We describe the status of a project whose main goal is to detect variability
along the extreme horizontal branch of the globular cluster NGC 6752. Based on
Magellan 6.5m data, preliminary light curves are presented for some candidate
variables. By combining our time-series data, we also produce a deep CMD of
unpreced... | astro-ph | we describe the status of a project whose main goal is to detect variability along the extreme horizontal branch of the globular cluster ngc 6752 based on magellan 65m data preliminary light curves are presented for some candidate variables by combining our timeseries data we also produce a deep cmd of unprecedented qu... | [['we', 'describe', 'the', 'status', 'of', 'a', 'project', 'whose', 'main', 'goal', 'is', 'to', 'detect', 'variability', 'along', 'the', 'extreme', 'horizontal', 'branch', 'of', 'the', 'globular', 'cluster', 'ngc', '6752', 'based', 'on', 'magellan', '65m', 'data', 'preliminary', 'light', 'curves', 'are', 'presented', '... | [-0.10747657242041297, 0.04813659603209936, -0.1540000044536611, 0.07204613686150119, -0.15320083712329705, -0.0632013022797565, 0.09444448555666596, 0.42828527485875234, -0.16703435199650973, -0.3510367548833155, 0.09783861293674331, -0.29799273222276607, -0.10117466476098443, 0.24676486812787105, -0.13894626466327742... |
710.0601 | Long time limit of equilibrium glassy dynamics and replica calculation | It is shown that the limit $t-t'\to\infty$ of the equilibrium dynamic
self-energy can be computed from the $n\to 1$ limit of the static self-energy
of a $n$-times replicated system with one step replica symmetry breaking
structure. It is also shown that the Dyson equation of the replicated system
leads in the $n\to 1... | cond-mat.stat-mech cond-mat.dis-nn | it is shown that the limit tttoinfty of the equilibrium dynamic selfenergy can be computed from the nto 1 limit of the static selfenergy of a ntimes replicated system with one step replica symmetry breaking structure it is also shown that the dyson equation of the replicated system leads in the nto 1 limit to the bifur... | [['it', 'is', 'shown', 'that', 'the', 'limit', 'tttoinfty', 'of', 'the', 'equilibrium', 'dynamic', 'selfenergy', 'can', 'be', 'computed', 'from', 'the', 'nto', '1', 'limit', 'of', 'the', 'static', 'selfenergy', 'of', 'a', 'ntimes', 'replicated', 'system', 'with', 'one', 'step', 'replica', 'symmetry', 'breaking', 'struc... | [-0.15456017234202435, 0.13719196049796958, -0.14977193723923415, 0.08016260201486969, 0.023110204969622915, -0.10947278044837457, 0.03667485622829327, 0.28403862203241037, -0.3067565243591064, -0.2248230099838267, 0.1055276137651495, -0.29555348779565543, -0.1309294143456325, 0.0778712913874657, 0.0691010540912068, 0.... |
710.0602 | HAT-P-4b: A metal-rich low-density transiting hot Jupiter | We describe the discovery of HAT-P-4b, a low-density extrasolar planet
transiting BD+36 2593, a V = 11.2 mag slightly evolved metal-rich late F star.
The planet's orbital period is 3.056536+/-0.000057 d with a mid-transit epoch
of 2,454,245.8154 +/- 0.0003 (HJD). Based on high-precision photometric and
spectroscopic ... | astro-ph | we describe the discovery of hatp4b a lowdensity extrasolar planet transiting bd36 2593 a v 112 mag slightly evolved metalrich late f star the planets orbital period is 30565360000057 d with a midtransit epoch of 24542458154 00003 hjd based on highprecision photometric and spectroscopic data and by using transit light ... | [['we', 'describe', 'the', 'discovery', 'of', 'hatp4b', 'a', 'lowdensity', 'extrasolar', 'planet', 'transiting', 'bd36', '2593', 'a', 'v', '112', 'mag', 'slightly', 'evolved', 'metalrich', 'late', 'f', 'star', 'the', 'planets', 'orbital', 'period', 'is', '30565360000057', 'd', 'with', 'a', 'midtransit', 'epoch', 'of', ... | [-0.12647605423650174, 0.1693474980110355, -0.13107775928992255, 0.00876094337343891, -0.13600351564394675, -0.14096406758893457, 0.14522137342099206, 0.330278916789271, -0.12189595734865935, -0.38582906121753646, 0.07205410074729855, -0.3182027833275149, -0.044272231653976805, 0.14908518940950177, -0.14921984342840788... |
710.0603 | An Initial Assessment of the GOES Microburst Windspeed Potential Index | A suite of products has been developed and evaluated to assess hazards
presented by convective downbursts to aircraft in flight derived from the
current generation of Geostationary Operational Environmental Satellite. The
existing suite of GOES microburst products employs the GOES sounder to
calculate risk based on c... | physics.ao-ph | a suite of products has been developed and evaluated to assess hazards presented by convective downbursts to aircraft in flight derived from the current generation of geostationary operational environmental satellite the existing suite of goes microburst products employs the goes sounder to calculate risk based on conc... | [['a', 'suite', 'of', 'products', 'has', 'been', 'developed', 'and', 'evaluated', 'to', 'assess', 'hazards', 'presented', 'by', 'convective', 'downbursts', 'to', 'aircraft', 'in', 'flight', 'derived', 'from', 'the', 'current', 'generation', 'of', 'geostationary', 'operational', 'environmental', 'satellite', 'the', 'exi... | [-0.07693304376002273, 0.07263189811221372, -0.05072689210867574, 0.0673466549343269, -0.032241498577761755, -0.07754373091818957, 0.04881557903718203, 0.3533216363397138, -0.18166065717613775, -0.3497608055970792, 0.13130752831970438, -0.23800870668271493, -0.12235237554614914, 0.24506547221078956, -0.1118744896853278... |
710.0604 | Control landscapes for two-level open quantum systems | A quantum control landscape is defined as the physical objective as a
function of the control variables. In this paper the control landscapes for
two-level open quantum systems, whose evolution is described by general
completely positive trace preserving maps (i.e., Kraus maps), are investigated
in details. The objec... | quant-ph math-ph math.MP | a quantum control landscape is defined as the physical objective as a function of the control variables in this paper the control landscapes for twolevel open quantum systems whose evolution is described by general completely positive trace preserving maps ie kraus maps are investigated in details the objective functio... | [['a', 'quantum', 'control', 'landscape', 'is', 'defined', 'as', 'the', 'physical', 'objective', 'as', 'a', 'function', 'of', 'the', 'control', 'variables', 'in', 'this', 'paper', 'the', 'control', 'landscapes', 'for', 'twolevel', 'open', 'quantum', 'systems', 'whose', 'evolution', 'is', 'described', 'by', 'general', '... | [-0.18925801044793628, 0.10517689414163767, -0.05991480633714053, 0.10052334984884431, 0.016335150868505826, -0.14266233808766668, 0.053104526446176505, 0.31882756950809543, -0.25966615411686794, -0.2883191621053037, 0.14185906982600413, -0.27958469428569405, -0.1383766892333576, 0.1625518302970025, -0.0428674927369719... |
710.0605 | Radiative and Collisional Jet Energy Loss in the Quark-Gluon Plasma at
RHIC | We calculate and compare bremsstrahlung and collisional energy loss of hard
partons traversing a quark-gluon plasma. Our treatment of both processes is
complete at leading order in the coupling and accounts for the probabilistic
nature of the jet energy loss. We find that the nuclear modification factor
$R_{AA}$ for ... | hep-ph nucl-th | we calculate and compare bremsstrahlung and collisional energy loss of hard partons traversing a quarkgluon plasma our treatment of both processes is complete at leading order in the coupling and accounts for the probabilistic nature of the jet energy loss we find that the nuclear modification factor r_aa for neutral p... | [['we', 'calculate', 'and', 'compare', 'bremsstrahlung', 'and', 'collisional', 'energy', 'loss', 'of', 'hard', 'partons', 'traversing', 'a', 'quarkgluon', 'plasma', 'our', 'treatment', 'of', 'both', 'processes', 'is', 'complete', 'at', 'leading', 'order', 'in', 'the', 'coupling', 'and', 'accounts', 'for', 'the', 'proba... | [-0.046324351454111, 0.22688175716885287, -0.1220586272063203, 0.15819904072395036, 0.01356595743959414, -0.06961025391129479, -0.06285536631351721, 0.38006606976366564, -0.20876809349639042, -0.2995107233638072, -0.08212306378818053, -0.3567575137486383, 0.11617803181173238, 0.12832154863947676, 0.08742969021741442, 0... |
710.0606 | Extended Einstein-Maxwell model | A self-consistent extended Einstein-Maxwell model for relativistic
non-stationary polarizable-magnetizable anisotropic media is presented. Based
on the analogy with relativistic extended irreversible (transient)
thermodynamics, the extended constitutive equations for the electrodynamics of
continua are formulated phe... | gr-qc astro-ph hep-th | a selfconsistent extended einsteinmaxwell model for relativistic nonstationary polarizablemagnetizable anisotropic media is presented based on the analogy with relativistic extended irreversible transient thermodynamics the extended constitutive equations for the electrodynamics of continua are formulated phenomenologi... | [['a', 'selfconsistent', 'extended', 'einsteinmaxwell', 'model', 'for', 'relativistic', 'nonstationary', 'polarizablemagnetizable', 'anisotropic', 'media', 'is', 'presented', 'based', 'on', 'the', 'analogy', 'with', 'relativistic', 'extended', 'irreversible', 'transient', 'thermodynamics', 'the', 'extended', 'constitut... | [-0.1413591548085346, 0.12608152693636449, -0.06318960744621498, 0.10893605150548476, -0.1379138405734141, -0.1332221200531681, -0.06143974859566827, 0.30458123236063067, -0.21233847341500223, -0.27814634530347704, 0.05603716287026016, -0.2403145866368764, -0.12730599577272578, 0.13003940357469088, 0.06172101464056011,... |
710.0607 | Localized modes of binary mixtures of Bose-Einstein condensates in
nonlinear optical lattices | The properties of the localized states of a two component Bose-Einstein
condensate confined in a nonlinear periodic potential [nonlinear optical
lattice] are investigated. We reveal the existence of new types of solitons and
study their stability by means of analytical and numerical approaches. The
symmetry propertie... | cond-mat.other | the properties of the localized states of a two component boseeinstein condensate confined in a nonlinear periodic potential nonlinear optical lattice are investigated we reveal the existence of new types of solitons and study their stability by means of analytical and numerical approaches the symmetry properties of th... | [['the', 'properties', 'of', 'the', 'localized', 'states', 'of', 'a', 'two', 'component', 'boseeinstein', 'condensate', 'confined', 'in', 'a', 'nonlinear', 'periodic', 'potential', 'nonlinear', 'optical', 'lattice', 'are', 'investigated', 'we', 'reveal', 'the', 'existence', 'of', 'new', 'types', 'of', 'solitons', 'and'... | [-0.1825991182300449, 0.20909099248906146, -0.05343467533269799, 0.03270438504420638, -0.020893653848600622, -0.13605445287631532, 0.004078320886229018, 0.3654766662083076, -0.2331127927663099, -0.2141228284978608, 0.10194590431331706, -0.29298858048002185, -0.13205013126379958, 0.1450588457871498, 0.054315441919147577... |
710.0608 | Fermi pockets and quantum oscillations of the Hall coefficient in high
temperature superconductors | Recent quantum oscillation measurements in high temperature superconductors
in high magnetic fields and low temperatures have ushered in a new era. These
experiments explore the normal state from which superconductivity arises and
provide evidence of a reconstructed Fermi surface consisting of electron and
hole pocke... | cond-mat.supr-con cond-mat.str-el | recent quantum oscillation measurements in high temperature superconductors in high magnetic fields and low temperatures have ushered in a new era these experiments explore the normal state from which superconductivity arises and provide evidence of a reconstructed fermi surface consisting of electron and hole pockets ... | [['recent', 'quantum', 'oscillation', 'measurements', 'in', 'high', 'temperature', 'superconductors', 'in', 'high', 'magnetic', 'fields', 'and', 'low', 'temperatures', 'have', 'ushered', 'in', 'a', 'new', 'era', 'these', 'experiments', 'explore', 'the', 'normal', 'state', 'from', 'which', 'superconductivity', 'arises',... | [-0.17981408586255984, 0.23655644234057005, -0.06218799582539004, 0.03779680217849091, -0.06634750754386975, -0.11933652182717382, 0.07419559857941241, 0.33560784740405064, -0.24629533597094527, -0.28924590800454747, 0.08911786095132672, -0.29632444841929284, -0.13050448079001536, 0.1664046926376552, 0.0126029756926473... |
710.0609 | Numerical investigation of the quantum fluctuations of optical fields
transmitted through an atomic medium | We have numerically solved the Heisenberg-Langevin equations describing the
propagation of quantized fields through an optically thick sample of atoms. Two
orthogonal polarization components are considered for the field and the
complete Zeeman sublevel structure of the atomic transition is taken into
account. Quantum... | quant-ph | we have numerically solved the heisenberglangevin equations describing the propagation of quantized fields through an optically thick sample of atoms two orthogonal polarization components are considered for the field and the complete zeeman sublevel structure of the atomic transition is taken into account quantum fluc... | [['we', 'have', 'numerically', 'solved', 'the', 'heisenberglangevin', 'equations', 'describing', 'the', 'propagation', 'of', 'quantized', 'fields', 'through', 'an', 'optically', 'thick', 'sample', 'of', 'atoms', 'two', 'orthogonal', 'polarization', 'components', 'are', 'considered', 'for', 'the', 'field', 'and', 'the',... | [-0.21288821414393716, 0.24095108524329278, -0.047192920492132744, 0.047228185448808316, 0.0024504814351181663, -0.09371620015088111, -0.021029596805432173, 0.43867686387049415, -0.25174828359780654, -0.24549756654895433, 0.010132716367442212, -0.22983764383737762, -0.027758593406298594, 0.17375527556398757, 0.07718444... |
710.061 | de Sitter Relativity and Quantum Physics | In the presence of a cosmological constant, interpreted as a purely geometric
entity, absence of matter is represented by a de Sitter spacetime. As a
consequence, ordinary Poincare' special relativity is no longer valid and must
be replaced by a de Sitter special relativity. By considering the kinematics of
a spinles... | gr-qc hep-th | in the presence of a cosmological constant interpreted as a purely geometric entity absence of matter is represented by a de sitter spacetime as a consequence ordinary poincare special relativity is no longer valid and must be replaced by a de sitter special relativity by considering the kinematics of a spinless partic... | [['in', 'the', 'presence', 'of', 'a', 'cosmological', 'constant', 'interpreted', 'as', 'a', 'purely', 'geometric', 'entity', 'absence', 'of', 'matter', 'is', 'represented', 'by', 'a', 'de', 'sitter', 'spacetime', 'as', 'a', 'consequence', 'ordinary', 'poincare', 'special', 'relativity', 'is', 'no', 'longer', 'valid', '... | [-0.1943701265936161, 0.17269768671120528, -0.15013872348255924, 0.16502138012687542, -0.10559462673067078, -0.13603497530611885, -0.058341650065494244, 0.2401607365698203, -0.166608716034657, -0.2627570525102027, 0.05234929560320815, -0.1906215446009361, -0.1149578605379377, 0.15133242958146692, -0.07236158997183303, ... |
710.0611 | Complex Network Analysis of State Spaces for Random Boolean Networks | We apply complex network analysis to the state spaces of random Boolean
networks (RBNs). An RBN contains $N$ Boolean elements each with $K$ inputs. A
directed state space network (SSN) is constructed by linking each dynamical
state, represented as a node, to its temporal successor. We study the
heterogeneity of an SS... | cond-mat.stat-mech cond-mat.dis-nn | we apply complex network analysis to the state spaces of random boolean networks rbns an rbn contains n boolean elements each with k inputs a directed state space network ssn is constructed by linking each dynamical state represented as a node to its temporal successor we study the heterogeneity of an ssn at both local... | [['we', 'apply', 'complex', 'network', 'analysis', 'to', 'the', 'state', 'spaces', 'of', 'random', 'boolean', 'networks', 'rbns', 'an', 'rbn', 'contains', 'n', 'boolean', 'elements', 'each', 'with', 'k', 'inputs', 'a', 'directed', 'state', 'space', 'network', 'ssn', 'is', 'constructed', 'by', 'linking', 'each', 'dynami... | [-0.18489995350440344, 0.1472069636856085, -0.03025797274081953, 0.04332820369083454, -0.0061597430058533235, -0.13284427108841815, 0.054039565570376535, 0.341065647223442, -0.2722212273686651, -0.30843843257291215, 0.042774819989476805, -0.3338901834986197, -0.17328140078846702, 0.09236076868893135, -0.024816705622321... |
710.0612 | Fermions Tunnelling from Black Holes | We investigate the tunnelling of spin 1/2 particles through event horizons.
We first apply the tunnelling method to Rindler spacetime and obtain the Unruh
temperature. We then apply fermion tunnelling to a general non-rotating black
hole metric and show that the Hawking temperature is recovered.
| hep-th | we investigate the tunnelling of spin 12 particles through event horizons we first apply the tunnelling method to rindler spacetime and obtain the unruh temperature we then apply fermion tunnelling to a general nonrotating black hole metric and show that the hawking temperature is recovered | [['we', 'investigate', 'the', 'tunnelling', 'of', 'spin', '12', 'particles', 'through', 'event', 'horizons', 'we', 'first', 'apply', 'the', 'tunnelling', 'method', 'to', 'rindler', 'spacetime', 'and', 'obtain', 'the', 'unruh', 'temperature', 'we', 'then', 'apply', 'fermion', 'tunnelling', 'to', 'a', 'general', 'nonrota... | [-0.10935939611453149, 0.1910374162459953, -0.12572639893947377, 0.18120214729311152, -0.06935838229126401, -0.1821295100471212, 0.026267975692947705, 0.3442640153484212, -0.15482124756607746, -0.24544415084852111, 0.005361577764981322, -0.3369193452099959, -0.11304739059673416, 0.16282689111928145, -0.0767619036758939... |
710.0613 | Back-door fine-tuning in supersymmetric low scale inflation | Low scale inflation has many virtues and it has been claimed that its natural
realisation in supersymmetric standard model can be achieved rather easily. In
this letter we have demonstrated that also in this case the dynamics of the
hidden sector responsible for supersymmetry breakdown and the structure of the
soft t... | hep-th | low scale inflation has many virtues and it has been claimed that its natural realisation in supersymmetric standard model can be achieved rather easily in this letter we have demonstrated that also in this case the dynamics of the hidden sector responsible for supersymmetry breakdown and the structure of the soft term... | [['low', 'scale', 'inflation', 'has', 'many', 'virtues', 'and', 'it', 'has', 'been', 'claimed', 'that', 'its', 'natural', 'realisation', 'in', 'supersymmetric', 'standard', 'model', 'can', 'be', 'achieved', 'rather', 'easily', 'in', 'this', 'letter', 'we', 'have', 'demonstrated', 'that', 'also', 'in', 'this', 'case', '... | [-0.11064949341011981, 0.1696608590579593, -0.10779351762346463, 0.12056483205387737, -0.06060407985933125, -0.12855657201501422, 0.0044493040825918685, 0.3256912179187768, -0.2644085260970449, -0.28787093525637447, 0.11741917306646406, -0.23017463944191227, -0.19134635490905724, 0.15701431444742614, -0.039322592703234... |
710.0614 | Using Full Information When Computing Modes of Post-Newtonian Waveforms
From Inspiralling Compact Binaries in Circular Orbit | The increasing sophistication and accuracy of numerical simulations of
compact binaries (especially binary black holes) presents the opportunity to
test the regime in which post-Newtonian (PN) predictions for the emitted
gravitational waves are accurate. In order to confront numerical results with
those of post-Newto... | gr-qc | the increasing sophistication and accuracy of numerical simulations of compact binaries especially binary black holes presents the opportunity to test the regime in which postnewtonian pn predictions for the emitted gravitational waves are accurate in order to confront numerical results with those of postnewtonian theo... | [['the', 'increasing', 'sophistication', 'and', 'accuracy', 'of', 'numerical', 'simulations', 'of', 'compact', 'binaries', 'especially', 'binary', 'black', 'holes', 'presents', 'the', 'opportunity', 'to', 'test', 'the', 'regime', 'in', 'which', 'postnewtonian', 'pn', 'predictions', 'for', 'the', 'emitted', 'gravitation... | [-0.16892804755286003, 0.10585881296234827, -0.042359260159234205, 0.08508623730619244, -0.09267400198344451, -0.06586988923372701, -0.016240549530872766, 0.3337970590296512, -0.17794383252039553, -0.3421138648254176, 0.03759714042632065, -0.3038257593599459, -0.08834785348153673, 0.23194934602943248, 0.036566697705226... |
710.0615 | Magnetic relaxation in the Bianchi-I universe | Extended Einstein-Maxwell model and its application to the problem of
evolution of magnetized Bianchi-I Universe are considered. The evolution of
medium magnetization is governed by a relaxation type extended constitutive
equation. The series of exact solutions to the extended master equations is
obtained and discuss... | gr-qc astro-ph hep-th | extended einsteinmaxwell model and its application to the problem of evolution of magnetized bianchii universe are considered the evolution of medium magnetization is governed by a relaxation type extended constitutive equation the series of exact solutions to the extended master equations is obtained and discussed the... | [['extended', 'einsteinmaxwell', 'model', 'and', 'its', 'application', 'to', 'the', 'problem', 'of', 'evolution', 'of', 'magnetized', 'bianchii', 'universe', 'are', 'considered', 'the', 'evolution', 'of', 'medium', 'magnetization', 'is', 'governed', 'by', 'a', 'relaxation', 'type', 'extended', 'constitutive', 'equation... | [-0.1724979312297924, 0.1277826730735027, -0.08096800897664462, 0.07796854502969207, -0.12329025152408016, -0.09517712668569472, -0.08288712557763435, 0.31976278179969925, -0.2851827889501762, -0.25834073953760356, 0.10872478370639818, -0.23272626070628086, -0.1038489455375104, 0.17489830459817313, 0.05977787970019003,... |
710.0616 | Nanofilters for Optical Nanocircuits | We theoretically and numerically study the design of optical 'lumped'
nanofiltering devices in the framework of our recently proposed paradigm for
optical nanocircuits. In particular, we present the design of basic filtering
elements, such as low-pass, band-pass, stop-band and high-pass 'lumped'
nanofilters, for use ... | cond-mat.mtrl-sci | we theoretically and numerically study the design of optical lumped nanofiltering devices in the framework of our recently proposed paradigm for optical nanocircuits in particular we present the design of basic filtering elements such as lowpass bandpass stopband and highpass lumped nanofilters for use in optical nanoc... | [['we', 'theoretically', 'and', 'numerically', 'study', 'the', 'design', 'of', 'optical', 'lumped', 'nanofiltering', 'devices', 'in', 'the', 'framework', 'of', 'our', 'recently', 'proposed', 'paradigm', 'for', 'optical', 'nanocircuits', 'in', 'particular', 'we', 'present', 'the', 'design', 'of', 'basic', 'filtering', '... | [-0.0928427950946708, 0.08264538665701236, -0.016001993551568575, -0.06152916487067656, -0.10681096458917155, -0.18619369517839632, 0.029587194371475455, 0.5235632857260835, -0.22043704520519666, -0.2704102277223553, 0.08369387316756233, -0.2255652765469516, -0.244289516215017, 0.279201839577031, -0.05996289108527683, ... |
710.0617 | Numerical evidence of regularized correlations in spin foam gravity | We report on the numerical analysis of the area correlations in spin foam
gravity on a single 4-simplex considered by Rovelli in PRL 97 (2006) 151301. We
compare the asymptotics and confirm the inverse squared distance leading
behaviour at large scales. This supports the recent advances on testing the
semiclassical l... | gr-qc hep-th | we report on the numerical analysis of the area correlations in spin foam gravity on a single 4simplex considered by rovelli in prl 97 2006 151301 we compare the asymptotics and confirm the inverse squared distance leading behaviour at large scales this supports the recent advances on testing the semiclassical limit of... | [['we', 'report', 'on', 'the', 'numerical', 'analysis', 'of', 'the', 'area', 'correlations', 'in', 'spin', 'foam', 'gravity', 'on', 'a', 'single', '4simplex', 'considered', 'by', 'rovelli', 'in', 'prl', '97', '2006', '151301', 'we', 'compare', 'the', 'asymptotics', 'and', 'confirm', 'the', 'inverse', 'squared', 'distan... | [-0.12900381366728664, 0.13314679643611282, -0.10001868780141007, 0.08414143995439302, 0.003672948030576314, -0.035880671893820576, 0.031850852324206334, 0.27942014541732124, -0.22576414207666348, -0.29222693705089287, 0.06584784738107087, -0.3305852583048176, -0.1563954947592869, 0.16139322253939223, -0.03859033149169... |
710.0618 | Anosov AdS representations are quasi-Fuchsian | Let Gamma be a cocompact lattice in SO(1,n). A representation rho: Gamma \to
SO(2,n) is quasi-Fuchsian if it is faithfull, discrete, and preserves an
acausal subset in the boundary of anti-de Sitter space - a particular case is
the case of Fuchsian representations, ie. composition of the inclusions of
Gamma in SO(1,n... | math.DG math.RT | let gamma be a cocompact lattice in so1n a representation rho gamma to so2n is quasifuchsian if it is faithfull discrete and preserves an acausal subset in the boundary of antide sitter space a particular case is the case of fuchsian representations ie composition of the inclusions of gamma in so1n and of so1n in so2n ... | [['let', 'gamma', 'be', 'a', 'cocompact', 'lattice', 'in', 'so1n', 'a', 'representation', 'rho', 'gamma', 'to', 'so2n', 'is', 'quasifuchsian', 'if', 'it', 'is', 'faithfull', 'discrete', 'and', 'preserves', 'an', 'acausal', 'subset', 'in', 'the', 'boundary', 'of', 'antide', 'sitter', 'space', 'a', 'particular', 'case', ... | [-0.17085855034060946, 0.2025684312212892, -0.13563145174035676, 0.06565601675669641, -0.1251473059576649, -0.10102831213419936, -0.08955594087089587, 0.39354714296786186, -0.2683847293089655, -0.11242378226488381, 0.13163886557305163, -0.29142404896648305, -0.1825619802960804, 0.17518171881976768, -0.16221409199209674... |
710.0619 | Unresolved Unidentified Source Contribution to the Gamma-ray Background | The large majority of EGRET point sources remain without an identified
low-energy counterpart, and a large fraction of these sources are most likely
extragalactic. Whatever the nature of the extragalactic EGRET unidentified
sources, faint unresolved objects of the same class must have a contribution to
the diffuse ex... | astro-ph | the large majority of egret point sources remain without an identified lowenergy counterpart and a large fraction of these sources are most likely extragalactic whatever the nature of the extragalactic egret unidentified sources faint unresolved objects of the same class must have a contribution to the diffuse extragal... | [['the', 'large', 'majority', 'of', 'egret', 'point', 'sources', 'remain', 'without', 'an', 'identified', 'lowenergy', 'counterpart', 'and', 'a', 'large', 'fraction', 'of', 'these', 'sources', 'are', 'most', 'likely', 'extragalactic', 'whatever', 'the', 'nature', 'of', 'the', 'extragalactic', 'egret', 'unidentified', '... | [-0.05229649423210887, 0.14072590386831224, -0.057575486678491286, 0.20199733499440464, -0.18535737372553035, -0.0667659766763819, 0.08051322365573012, 0.44744426224912914, -0.20057121956191656, -0.3858316706273682, 0.03717553302477929, -0.40271037819749034, -0.03437149642586349, 0.22523041742836467, -0.036610017947112... |
710.062 | Deforming, revolving and resolving - New paths in the string theory
landscape | In this paper we investigate the properties of series of vacua in the string
theory landscape. In particular, we study minima to the flux potential in type
IIB compactifications on the mirror quintic. Using geometric transitions, we
embed its one dimensional complex structure moduli space in that of another
Calabi-Ya... | hep-th math.AG math.DG | in this paper we investigate the properties of series of vacua in the string theory landscape in particular we study minima to the flux potential in type iib compactifications on the mirror quintic using geometric transitions we embed its one dimensional complex structure moduli space in that of another calabiyau with ... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'properties', 'of', 'series', 'of', 'vacua', 'in', 'the', 'string', 'theory', 'landscape', 'in', 'particular', 'we', 'study', 'minima', 'to', 'the', 'flux', 'potential', 'in', 'type', 'iib', 'compactifications', 'on', 'the', 'mirror', 'quintic', 'using', 'geometric',... | [-0.1279402437752911, 0.08850185596517748, -0.09809247001872531, 0.114852963915874, -0.07333664616750439, -0.09333457632408458, 0.05093494974782367, 0.3530205358389993, -0.2975371505266854, -0.2500667138956487, 0.11947523227926078, -0.24881943810389054, -0.23135462625674447, 0.1677960022257603, -0.11420988912542103, -0... |
710.0621 | X-ray Fluorescent Fe Kalpha Lines from Stellar Photospheres | X-ray spectra from stellar coronae are reprocessed by the underlying
photosphere through scattering and photoionization events. While reprocessed
X-ray spectra reaching a distant observer are at a flux level of only a few
percent of that of the corona itself, characteristic lines formed by inner
shell photoionization... | astro-ph | xray spectra from stellar coronae are reprocessed by the underlying photosphere through scattering and photoionization events while reprocessed xray spectra reaching a distant observer are at a flux level of only a few percent of that of the corona itself characteristic lines formed by inner shell photoionization of so... | [['xray', 'spectra', 'from', 'stellar', 'coronae', 'are', 'reprocessed', 'by', 'the', 'underlying', 'photosphere', 'through', 'scattering', 'and', 'photoionization', 'events', 'while', 'reprocessed', 'xray', 'spectra', 'reaching', 'a', 'distant', 'observer', 'are', 'at', 'a', 'flux', 'level', 'of', 'only', 'a', 'few', ... | [-0.008308539170756996, 0.1617978405433733, 0.02170284261251707, 0.12700301406263148, -0.0694593265847455, -0.11799168511872658, 0.042904336690954656, 0.5138014188681941, -0.17167085466861903, -0.3638315577620262, 0.03583236167993975, -0.3177495342234068, -0.00275106836793076, 0.19855448141122659, 0.003547240293536528,... |
710.0622 | Charge response function and a novel plasmon mode in graphene | Polarizability of non-interacting 2D Dirac electrons has a 1/\sqrt{qv-\omega}
singularity at the boundary of electron-hole excitations. The screening of this
singularity by long-range electron-electron interactions is usually treated
within the random phase approximation. The latter is exact only in the limit of
N ->... | cond-mat.mes-hall | polarizability of noninteracting 2d dirac electrons has a 1sqrtqvomega singularity at the boundary of electronhole excitations the screening of this singularity by longrange electronelectron interactions is usually treated within the random phase approximation the latter is exact only in the limit of n infinity where n... | [['polarizability', 'of', 'noninteracting', '2d', 'dirac', 'electrons', 'has', 'a', '1sqrtqvomega', 'singularity', 'at', 'the', 'boundary', 'of', 'electronhole', 'excitations', 'the', 'screening', 'of', 'this', 'singularity', 'by', 'longrange', 'electronelectron', 'interactions', 'is', 'usually', 'treated', 'within', '... | [-0.1646169531746071, 0.1518680217887173, -0.06717297588864908, 0.10274920700618825, -0.041346144099414596, -0.11459442793916003, 0.03730529318211459, 0.31304974049454976, -0.2361980599249486, -0.24233316914608874, -0.0007268099570177307, -0.35019628421849563, -0.1221667650476599, 0.06414342046316181, 0.077122701091316... |
710.0623 | Electroweak Symmetry Breaking from a Holographic Fourth Generation | We consider a model with four generations of standard model fermions
propagating in an extra dimension with an AdS background metric. We show that
if the zero modes of the fourth generation are highly localized towards the
infrared brane, it is possible to break the electroweak symmetry via their
condensation, partly... | hep-ph hep-ex hep-th | we consider a model with four generations of standard model fermions propagating in an extra dimension with an ads background metric we show that if the zero modes of the fourth generation are highly localized towards the infrared brane it is possible to break the electroweak symmetry via their condensation partly driv... | [['we', 'consider', 'a', 'model', 'with', 'four', 'generations', 'of', 'standard', 'model', 'fermions', 'propagating', 'in', 'an', 'extra', 'dimension', 'with', 'an', 'ads', 'background', 'metric', 'we', 'show', 'that', 'if', 'the', 'zero', 'modes', 'of', 'the', 'fourth', 'generation', 'are', 'highly', 'localized', 'to... | [-0.11115503682410471, 0.26493883585539, -0.03087689062741534, 0.09912974854105165, -0.05401281167893377, -0.13969908743277065, -0.0010622002412437473, 0.2921664833732281, -0.24617905502386186, -0.28915240775717244, 0.09310468805679567, -0.28899885833977834, -0.10569316276495842, 0.11317925253876625, 0.0363829979256379... |
710.0624 | Reflexive Ideals in Iwasawa Algebras | Let $G$ be a torsionfree compact $p$-adic analytic group. We give sufficient
conditions on $p$ and $G$ which ensure that the Iwasawa algebra $\Omega_G$ of
$G$ has no non-trivial two-sided reflexive ideals. Consequently, these
conditions imply that every nonzero normal element in $\Omega_G$ is a unit. We
show that the... | math.RA math.NT | let g be a torsionfree compact padic analytic group we give sufficient conditions on p and g which ensure that the iwasawa algebra omega_g of g has no nontrivial twosided reflexive ideals consequently these conditions imply that every nonzero normal element in omega_g is a unit we show that these conditions hold in the... | [['let', 'g', 'be', 'a', 'torsionfree', 'compact', 'padic', 'analytic', 'group', 'we', 'give', 'sufficient', 'conditions', 'on', 'p', 'and', 'g', 'which', 'ensure', 'that', 'the', 'iwasawa', 'algebra', 'omega_g', 'of', 'g', 'has', 'no', 'nontrivial', 'twosided', 'reflexive', 'ideals', 'consequently', 'these', 'conditio... | [-0.20583903517129015, 0.11001820430951297, -0.11551203128708674, 0.04153026576541298, -0.13094200108373388, -0.1618720701425872, -0.0038701482570474652, 0.3692470461097175, -0.2914253549765697, -0.2193454655909301, 0.1307923059989863, -0.24306773173054103, -0.10800581456335114, 0.21195561721492395, -0.1315586989564178... |
710.0625 | Oscillating Starless Cores: The Nonlinear Regime | In a previous paper, we modeled the oscillations of a thermally-supported
(Bonnor-Ebert) sphere as non-radial, linear perturbations following a standard
analysis developed for stellar pulsations. The predicted column density
variations and molecular spectral line profiles are similar to those observed
in the Bok glob... | astro-ph | in a previous paper we modeled the oscillations of a thermallysupported bonnorebert sphere as nonradial linear perturbations following a standard analysis developed for stellar pulsations the predicted column density variations and molecular spectral line profiles are similar to those observed in the bok globule b68 su... | [['in', 'a', 'previous', 'paper', 'we', 'modeled', 'the', 'oscillations', 'of', 'a', 'thermallysupported', 'bonnorebert', 'sphere', 'as', 'nonradial', 'linear', 'perturbations', 'following', 'a', 'standard', 'analysis', 'developed', 'for', 'stellar', 'pulsations', 'the', 'predicted', 'column', 'density', 'variations', ... | [-0.14647035387366317, 0.14792303549930771, -0.07079904912718275, 0.09406508968749568, -0.04734991970219354, -0.06294564088597143, 0.01762808662073961, 0.3582537285333803, -0.2477519509090154, -0.29744102592154065, 0.1337555860762138, -0.26603662434991543, -0.11067686593629304, 0.1882406461175329, 0.002887659401149135,... |
710.0626 | Valence bond solid order near impurities in two-dimensional quantum
antiferromagnets | Recent scanning tunnelling microscopy (STM) experiments on underdoped
cuprates have displayed modulations in the local electronic density of states
which are centered on a Cu-O-Cu bond (Kohsaka et. al., cond-mat/0703309). As a
paradigm of the pinning of such bond-centered ordering in strongly correlated
systems, we p... | cond-mat.str-el cond-mat.supr-con | recent scanning tunnelling microscopy stm experiments on underdoped cuprates have displayed modulations in the local electronic density of states which are centered on a cuocu bond kohsaka et al condmat0703309 as a paradigm of the pinning of such bondcentered ordering in strongly correlated systems we present the theor... | [['recent', 'scanning', 'tunnelling', 'microscopy', 'stm', 'experiments', 'on', 'underdoped', 'cuprates', 'have', 'displayed', 'modulations', 'in', 'the', 'local', 'electronic', 'density', 'of', 'states', 'which', 'are', 'centered', 'on', 'a', 'cuocu', 'bond', 'kohsaka', 'et', 'al', 'condmat0703309', 'as', 'a', 'paradi... | [-0.1882921347483814, 0.23755267170241484, -0.03832320739727044, 0.05000339851025938, -0.009355097378933145, -0.1411187842175989, 0.10928852630682948, 0.3725964520126581, -0.2614870309316648, -0.24107449109147408, 0.039045384794356534, -0.38422264970705183, -0.14605048206958274, 0.10659120948901567, 0.06068330086923823... |
710.0627 | Kinetic theory of non-Abelian plasma: a non-minimal model | The self-consistent system of master equations describing the kinetics of a
relativistic non-Abelian plasma, influenced by curvature interactions, is
formulated. Non-minimal (curvature induced) coupling is shown to modify all the
subsystems of the model: the gauge field equations, the gravity field equations
and the ... | gr-qc astro-ph hep-ph hep-th | the selfconsistent system of master equations describing the kinetics of a relativistic nonabelian plasma influenced by curvature interactions is formulated nonminimal curvature induced coupling is shown to modify all the subsystems of the model the gauge field equations the gravity field equations and the kinetic equa... | [['the', 'selfconsistent', 'system', 'of', 'master', 'equations', 'describing', 'the', 'kinetics', 'of', 'a', 'relativistic', 'nonabelian', 'plasma', 'influenced', 'by', 'curvature', 'interactions', 'is', 'formulated', 'nonminimal', 'curvature', 'induced', 'coupling', 'is', 'shown', 'to', 'modify', 'all', 'the', 'subsy... | [-0.24097767411683668, 0.24184641880648478, -0.07581911432409506, 0.09695985665715927, -0.08194250148740045, -0.16550447285289363, -0.12284943981248202, 0.2103643799200654, -0.24755286545093572, -0.30343539742942977, -0.05603279169572859, -0.24952393344470433, -0.12379202330294921, 0.08848725912655342, 0.03927891662496... |
710.0628 | New explicit spike solution -- non-local component of the generalized
Mixmaster attractor | By applying a standard solution-generating transformation to an arbitrary
vacuum Bianchi type II solution, one generates a new solution with spikes
commonly observed in numerical simulations. It is conjectured that the spike
solution is part of the generalized Mixmaster attractor.
| gr-qc | by applying a standard solutiongenerating transformation to an arbitrary vacuum bianchi type ii solution one generates a new solution with spikes commonly observed in numerical simulations it is conjectured that the spike solution is part of the generalized mixmaster attractor | [['by', 'applying', 'a', 'standard', 'solutiongenerating', 'transformation', 'to', 'an', 'arbitrary', 'vacuum', 'bianchi', 'type', 'ii', 'solution', 'one', 'generates', 'a', 'new', 'solution', 'with', 'spikes', 'commonly', 'observed', 'in', 'numerical', 'simulations', 'it', 'is', 'conjectured', 'that', 'the', 'spike', ... | [-0.10610316530801356, 0.03913826184907521, -0.10003128123935312, 0.0852746416174341, -0.1178336882032454, -0.19509410883765668, -0.045054493565112354, 0.2567437572404742, -0.26293746517039834, -0.2300828795414418, 0.14189333395042922, -0.2827975083841011, -0.20693330437643453, 0.14003960588015615, -0.04535079378983937... |
710.0629 | Three Disk Oscillation Modes of Rotating Magnetized Neutron Stars | We discuss three specific modes of accretion disks around rotating magnetized
neutron stars which may explain the separations of the kilo Hertz quasi
periodic oscillations (QPO) seen in low mass X-ray binaries. The existence of
these modes requires that there be a maximum in the angular velocity of the
accreting mate... | astro-ph | we discuss three specific modes of accretion disks around rotating magnetized neutron stars which may explain the separations of the kilo hertz quasi periodic oscillations qpo seen in low mass xray binaries the existence of these modes requires that there be a maximum in the angular velocity of the accreting material a... | [['we', 'discuss', 'three', 'specific', 'modes', 'of', 'accretion', 'disks', 'around', 'rotating', 'magnetized', 'neutron', 'stars', 'which', 'may', 'explain', 'the', 'separations', 'of', 'the', 'kilo', 'hertz', 'quasi', 'periodic', 'oscillations', 'qpo', 'seen', 'in', 'low', 'mass', 'xray', 'binaries', 'the', 'existen... | [-0.18451769763952075, 0.20251346847050758, -0.03295684605445556, 0.042160095153435155, -0.10629049216655373, -0.08428491845515658, 0.03116246132205041, 0.3342244717362924, -0.21506842192919814, -0.2600820541319226, 0.11604923962521516, -0.27122757173957257, -0.023679246283684147, 0.2333535778976022, -0.022431126048524... |
710.063 | Disk-Halo Interplay in Galaxy Evolution | Some aspects of disk-halo interactions for models of in and out of
equilibrium disk galaxies are reviewed. Specifically, we focus on disk-halo
resonant interaction without and in the presence of a gas component. Another
issue is the disk growth within an assembling triaxial dark matter halo. We
argue that while the t... | astro-ph | some aspects of diskhalo interactions for models of in and out of equilibrium disk galaxies are reviewed specifically we focus on diskhalo resonant interaction without and in the presence of a gas component another issue is the disk growth within an assembling triaxial dark matter halo we argue that while the triaxiali... | [['some', 'aspects', 'of', 'diskhalo', 'interactions', 'for', 'models', 'of', 'in', 'and', 'out', 'of', 'equilibrium', 'disk', 'galaxies', 'are', 'reviewed', 'specifically', 'we', 'focus', 'on', 'diskhalo', 'resonant', 'interaction', 'without', 'and', 'in', 'the', 'presence', 'of', 'a', 'gas', 'component', 'another', '... | [-0.18530680280598752, 0.14609433573392702, -0.10579825368183274, 0.09024558229561012, -0.04761087575875153, -0.0345203608761881, -0.019962725760502235, 0.3349621767291329, -0.2236641843620444, -0.27188502212934124, 0.06367245562500799, -0.26044036741324955, -0.10188292145128493, 0.17173390017352372, 0.0499993386584830... |
710.0631 | Gauge Theory And Wild Ramification | The gauge theory approach to the geometric Langlands program is extended to
the case of wild ramification. The new ingredients that are required, relative
to the tamely ramified case, are differential operators with irregular
singularities, Stokes phenomena, isomonodromic deformation, and, from a
physical point of vi... | hep-th | the gauge theory approach to the geometric langlands program is extended to the case of wild ramification the new ingredients that are required relative to the tamely ramified case are differential operators with irregular singularities stokes phenomena isomonodromic deformation and from a physical point of view new su... | [['the', 'gauge', 'theory', 'approach', 'to', 'the', 'geometric', 'langlands', 'program', 'is', 'extended', 'to', 'the', 'case', 'of', 'wild', 'ramification', 'the', 'new', 'ingredients', 'that', 'are', 'required', 'relative', 'to', 'the', 'tamely', 'ramified', 'case', 'are', 'differential', 'operators', 'with', 'irreg... | [-0.16443766083533842, 0.05106992481483354, -0.15344513987225514, 0.11806167946930078, -0.1658164658497467, -0.19105805497168116, -0.04148178293447321, 0.24744569799966282, -0.3205551186369525, -0.24162235666342355, 0.09227828318210042, -0.25192069400239875, -0.2182212755670426, 0.17685912959967498, -0.1810110041319772... |
710.0632 | Dependence of the Build-up of the Colour-Magnitude Relation on Cluster
Richness at z ~ 0.8 | We present environmental dependence of the build-up of the colour-magnitude
relation (CMR) at z ~ 0.8. It is well established that massive early-type
galaxies exhibit a tight CMR in clusters up to at least z ~ 1. The faint end of
the relation, however, has been much less explored especially at high redshifts
primaril... | astro-ph | we present environmental dependence of the buildup of the colourmagnitude relation cmr at z 08 it is well established that massive earlytype galaxies exhibit a tight cmr in clusters up to at least z 1 the faint end of the relation however has been much less explored especially at high redshifts primarily due to limited... | [['we', 'present', 'environmental', 'dependence', 'of', 'the', 'buildup', 'of', 'the', 'colourmagnitude', 'relation', 'cmr', 'at', 'z', '08', 'it', 'is', 'well', 'established', 'that', 'massive', 'earlytype', 'galaxies', 'exhibit', 'a', 'tight', 'cmr', 'in', 'clusters', 'up', 'to', 'at', 'least', 'z', '1', 'the', 'fain... | [-0.06864021402064034, 0.08843278592850601, -0.09736891653473405, 0.10255772209017198, -0.08360722914803773, -0.07781686223620041, 0.07374992682572074, 0.4372929236004976, -0.12536254437978972, -0.3558761112518947, 0.059250645971835846, -0.32905062182848765, -0.09130982057170266, 0.19433625091531379, -0.075975333533080... |
710.0633 | The Effect of Pure State Structure on Nonequilibrium Dynamics | Motivated by short-range Ising spin glasses, we review some rigorous results
and their consequences for the relation between the number/nature of
equilibrium pure states and nonequilibrium dynamics. Two of the consequences
for spin glass dynamics following a deep quench to a temperature with broken
spin flip symmetry... | cond-mat.dis-nn cond-mat.stat-mech | motivated by shortrange ising spin glasses we review some rigorous results and their consequences for the relation between the numbernature of equilibrium pure states and nonequilibrium dynamics two of the consequences for spin glass dynamics following a deep quench to a temperature with broken spin flip symmetry are 1... | [['motivated', 'by', 'shortrange', 'ising', 'spin', 'glasses', 'we', 'review', 'some', 'rigorous', 'results', 'and', 'their', 'consequences', 'for', 'the', 'relation', 'between', 'the', 'numbernature', 'of', 'equilibrium', 'pure', 'states', 'and', 'nonequilibrium', 'dynamics', 'two', 'of', 'the', 'consequences', 'for',... | [-0.14947421559477922, 0.2367195773800062, -0.10158818619496816, 0.07317325411139525, 0.0015618036988945235, -0.13449958334898665, 0.030069807514256867, 0.37327325465094274, -0.24476170318429263, -0.2636187370093603, 0.11022293605353861, -0.29442028746287635, -0.11368996612284155, 0.13635910708349527, 0.033426387305213... |
710.0634 | Collective stimulated Brillouin backscatter | We develop the statistical theory of the stimulated Brillouin backscatter
(BSBS) instability of a spatially and temporally partially incoherent laser
beam for laser fusion relevant plasma. We find a new regime of BSBS which has a
much larger threshold than the classical threshold of a coherent beam in
long-scale-leng... | physics.plasm-ph | we develop the statistical theory of the stimulated brillouin backscatter bsbs instability of a spatially and temporally partially incoherent laser beam for laser fusion relevant plasma we find a new regime of bsbs which has a much larger threshold than the classical threshold of a coherent beam in longscalelength lase... | [['we', 'develop', 'the', 'statistical', 'theory', 'of', 'the', 'stimulated', 'brillouin', 'backscatter', 'bsbs', 'instability', 'of', 'a', 'spatially', 'and', 'temporally', 'partially', 'incoherent', 'laser', 'beam', 'for', 'laser', 'fusion', 'relevant', 'plasma', 'we', 'find', 'a', 'new', 'regime', 'of', 'bsbs', 'whi... | [-0.1456631919933208, 0.24313630270709177, -0.08259579423665, 0.09747318282173384, -0.0471673614795526, -0.12909907540743984, 0.08143294437229008, 0.3706844900359693, -0.2571691708614262, -0.23154240196583256, 0.07214632055537788, -0.22229034004845474, -0.0614967103020113, 0.22514106791416472, -0.056417266821259034, 0.... |
710.0635 | Nonexistence of reflexive ideals in Iwasawa algebras of Chevalley type | Let $\Phi$ be a root system and let $\Phi(\Zp)$ be the standard Chevalley
$\Zp$-Lie algebra associated to $\Phi$. For any integer $t\geq 1$, let $G$ be
the uniform pro-$p$ group corresponding to the powerful Lie algebra $p^t
\Phi(\Zp)$ and suppose that $p\geq 5$. Then the Iwasawa algebra $\Omega_G$ has
no nontrivial ... | math.RA math.NT | let phi be a root system and let phizp be the standard chevalley zplie algebra associated to phi for any integer tgeq 1 let g be the uniform prop group corresponding to the powerful lie algebra pt phizp and suppose that pgeq 5 then the iwasawa algebra omega_g has no nontrivial reflexive twosided ideals this was previou... | [['let', 'phi', 'be', 'a', 'root', 'system', 'and', 'let', 'phizp', 'be', 'the', 'standard', 'chevalley', 'zplie', 'algebra', 'associated', 'to', 'phi', 'for', 'any', 'integer', 'tgeq', '1', 'let', 'g', 'be', 'the', 'uniform', 'prop', 'group', 'corresponding', 'to', 'the', 'powerful', 'lie', 'algebra', 'pt', 'phizp', '... | [-0.18102261735341296, 0.11849991085115247, -0.10806431909306691, 0.013717767329385074, -0.14932676968522943, -0.23546694717011774, -0.09828760275760522, 0.30978536227574716, -0.3878230290630689, -0.1886071148292663, 0.12936008697590576, -0.26384397567464757, -0.05245853674669678, 0.19088849949722106, -0.12827275803742... |
710.0636 | Extended cavity diode lasers with tracked resonances | We present a painless, almost-free upgrade to present extended cavity diode
lasers (ECDLs), which improves the long term mode-hop free performance by
stabilizing the resonance of the internal cavity to the external cavity. This
stabilization is based on the observation that the frequency or amplitude noise
of the ECD... | physics.optics physics.atom-ph | we present a painless almostfree upgrade to present extended cavity diode lasers ecdls which improves the long term modehop free performance by stabilizing the resonance of the internal cavity to the external cavity this stabilization is based on the observation that the frequency or amplitude noise of the ecdl is lowe... | [['we', 'present', 'a', 'painless', 'almostfree', 'upgrade', 'to', 'present', 'extended', 'cavity', 'diode', 'lasers', 'ecdls', 'which', 'improves', 'the', 'long', 'term', 'modehop', 'free', 'performance', 'by', 'stabilizing', 'the', 'resonance', 'of', 'the', 'internal', 'cavity', 'to', 'the', 'external', 'cavity', 'th... | [-0.1477073227467903, 0.17360273211807303, -0.03649579937376032, -0.03226137879357717, -0.01729645888671129, -0.19862607644320834, 0.07017609821601252, 0.4403655593027204, -0.25446536770753014, -0.30647384095311964, 0.09699713298972797, -0.21886169132245267, -0.03578349775103415, 0.21727448425899515, -0.082885556524594... |
710.0637 | Super-resolving distant galaxies with gravitational telescopes:
Keck-LGSAO and Hubble imaging of the lens system SDSSJ0737+3216 | We combine high-resolution images in four optical/infra-red bands, obtained
with the laser guide star adaptive optics system on the Keck Telescope and with
the Hubble Space Telescope, to study the gravitational lens system
SDSSJ0737+3216 (lens redshift 0.3223, source redshift 0.5812). We show that
(under favorable ob... | astro-ph | we combine highresolution images in four opticalinfrared bands obtained with the laser guide star adaptive optics system on the keck telescope and with the hubble space telescope to study the gravitational lens system sdssj07373216 lens redshift 03223 source redshift 05812 we show that under favorable observing conditi... | [['we', 'combine', 'highresolution', 'images', 'in', 'four', 'opticalinfrared', 'bands', 'obtained', 'with', 'the', 'laser', 'guide', 'star', 'adaptive', 'optics', 'system', 'on', 'the', 'keck', 'telescope', 'and', 'with', 'the', 'hubble', 'space', 'telescope', 'to', 'study', 'the', 'gravitational', 'lens', 'system', '... | [-0.04037676888864906, 0.05307053754905628, -0.09628191328968624, 0.08619367538750729, -0.1333950694336803, -0.07751761244571939, 0.005513291872505631, 0.45052034094625587, -0.15081737817179564, -0.38636915431338914, 0.07388911592508, -0.2881799745734553, -0.04575848710362096, 0.22747817853636734, -0.04696723890623876,... |
710.0638 | Sheaves on abelian surfaces and Strange Duality | We formulate three versions of a strange duality conjecture for sections of
the Theta bundles on the moduli spaces of sheaves on abelian surfaces. As
supporting evidence, we check the equality of dimensions on dual moduli spaces,
answering a question raised by Gottsche-Nakajima-Yoshioka.
| math.AG | we formulate three versions of a strange duality conjecture for sections of the theta bundles on the moduli spaces of sheaves on abelian surfaces as supporting evidence we check the equality of dimensions on dual moduli spaces answering a question raised by gottschenakajimayoshioka | [['we', 'formulate', 'three', 'versions', 'of', 'a', 'strange', 'duality', 'conjecture', 'for', 'sections', 'of', 'the', 'theta', 'bundles', 'on', 'the', 'moduli', 'spaces', 'of', 'sheaves', 'on', 'abelian', 'surfaces', 'as', 'supporting', 'evidence', 'we', 'check', 'the', 'equality', 'of', 'dimensions', 'on', 'dual', ... | [-0.2031814420895119, 0.11025376795719023, -0.08634732104837894, 0.18639924931561663, -0.06347686451460634, -0.13254230972822933, 0.062404532162916096, 0.3185962669196583, -0.24539603820691505, -0.21230909485547317, 0.12991884896819966, -0.22484084750370434, -0.14349116923819696, 0.22014723526358249, -0.155686412893590... |
710.0639 | Dirac geometry, quasi-Poisson actions and D/G-valued moment maps | We study Dirac structures associated with Manin pairs (\d,\g) and give a
Dirac geometric approach to Hamiltonian spaces with D/G-valued moment maps,
originally introduced by Alekseev and Kosmann-Schwarzbach in terms of
quasi-Poisson structures. We explain how these two distinct frameworks are
related to each other, p... | math.DG math.SG | we study dirac structures associated with manin pairs dg and give a dirac geometric approach to hamiltonian spaces with dgvalued moment maps originally introduced by alekseev and kosmannschwarzbach in terms of quasipoisson structures we explain how these two distinct frameworks are related to each other proving that th... | [['we', 'study', 'dirac', 'structures', 'associated', 'with', 'manin', 'pairs', 'dg', 'and', 'give', 'a', 'dirac', 'geometric', 'approach', 'to', 'hamiltonian', 'spaces', 'with', 'dgvalued', 'moment', 'maps', 'originally', 'introduced', 'by', 'alekseev', 'and', 'kosmannschwarzbach', 'in', 'terms', 'of', 'quasipoisson',... | [-0.15206545111673173, 0.0871360531397244, -0.06190126018738875, 0.13783748595417047, -0.1317015483234358, -0.1295782137231561, -0.04451204578064242, 0.3846428514087713, -0.35023450490928465, -0.2938766306947156, 0.050125550213319964, -0.2534967659101371, -0.26468508604974034, 0.1634167962337053, -0.17561427265485768, ... |
710.064 | The Toda system and multiple-end solutions of autonomous planar elliptic
problems | We construct a new class of positive solutions for a classical semilinear
elliptic problem in the plane which arise for instance as the standing-wave
problem for the standard nonlinear Schr\"odinger equation or in nonlinear
models in Turing's theory biological theory of pattern formation such as the
Gray-Scott or Gie... | math.AP | we construct a new class of positive solutions for a classical semilinear elliptic problem in the plane which arise for instance as the standingwave problem for the standard nonlinear schrodinger equation or in nonlinear models in turings theory biological theory of pattern formation such as the grayscott or gierermein... | [['we', 'construct', 'a', 'new', 'class', 'of', 'positive', 'solutions', 'for', 'a', 'classical', 'semilinear', 'elliptic', 'problem', 'in', 'the', 'plane', 'which', 'arise', 'for', 'instance', 'as', 'the', 'standingwave', 'problem', 'for', 'the', 'standard', 'nonlinear', 'schrodinger', 'equation', 'or', 'in', 'nonline... | [-0.13464302114938953, 0.061551406851102566, -0.04742550924313308, 0.05886578815186332, -0.071365629499457, -0.17336041104562325, -0.05991235359614694, 0.26817079909659663, -0.34286801234401504, -0.22756191594097977, 0.14472247002614214, -0.3316837745162005, -0.16656940324959912, 0.20502771849840365, -0.029483476359311... |
710.0641 | Random Diffusion Model | We study here the random diffusion model. This is a continuum model for a
conserved scalar density field $\phi$ driven by diffusive dynamics. The
interesting feature of the dynamics is that the {\it bare} diffusion
coefficient $D$ is density dependent. In the simplest case
$D=\bar{D}+D_{1}\delta \phi $ where $\bar{D}... | cond-mat.soft | we study here the random diffusion model this is a continuum model for a conserved scalar density field phi driven by diffusive dynamics the interesting feature of the dynamics is that the it bare diffusion coefficient d is density dependent in the simplest case dbardd_1delta phi where bard is the constant average diff... | [['we', 'study', 'here', 'the', 'random', 'diffusion', 'model', 'this', 'is', 'a', 'continuum', 'model', 'for', 'a', 'conserved', 'scalar', 'density', 'field', 'phi', 'driven', 'by', 'diffusive', 'dynamics', 'the', 'interesting', 'feature', 'of', 'the', 'dynamics', 'is', 'that', 'the', 'it', 'bare', 'diffusion', 'coeff... | [-0.1598794196933868, 0.19585128551573558, -0.07631660722579588, 0.05875649873828594, -0.038438042768613755, -0.14842842266887052, 0.0031211297653865916, 0.3084164912335011, -0.2915136930317532, -0.24892503524173692, 0.062012719044250535, -0.30282661119405524, -0.14082012823665468, 0.12661156428199136, 0.06872488293961... |
710.0642 | Appendix to 'Roth's theorem on progressions revisited' by J Bourgain | We show two results. First, a refinement of Freiman's theorem: if A is a
finite set of integers and |A+A| < K|A|, then A is contained in a
multidimensional progression of dimension at most O(K^{7/4} log^3K) and size at
most exp(O(K^{7/4} log^3K))|A|. Secondly, an improvement of a result of
Konyagin and Laba: if A is ... | math.CA math.NT | we show two results first a refinement of freimans theorem if a is a finite set of integers and aa ka then a is contained in a multidimensional progression of dimension at most ok74 log3k and size at most expok74 log3ka secondly an improvement of a result of konyagin and laba if a is a finite set of reals and a is a tr... | [['we', 'show', 'two', 'results', 'first', 'a', 'refinement', 'of', 'freimans', 'theorem', 'if', 'a', 'is', 'a', 'finite', 'set', 'of', 'integers', 'and', 'aa', 'ka', 'then', 'a', 'is', 'contained', 'in', 'a', 'multidimensional', 'progression', 'of', 'dimension', 'at', 'most', 'ok74', 'log3k', 'and', 'size', 'at', 'mos... | [-0.1441557017634764, 0.09593957415486468, -0.09831262690325578, 0.03470294475978748, -0.026684334882619707, -0.0960337704499111, 0.06151108459259073, 0.30699407445464394, -0.2752478733891621, -0.1599671635000656, 0.12779639637147105, -0.31399756622020947, -0.11259704197150175, 0.2333073111138109, -0.06201722591438077,... |
710.0643 | Chern character for twisted complexes | We construct a Chern character of a perfect complex of twisted modules over
an algebroid stack.
| math.KT | we construct a chern character of a perfect complex of twisted modules over an algebroid stack | [['we', 'construct', 'a', 'chern', 'character', 'of', 'a', 'perfect', 'complex', 'of', 'twisted', 'modules', 'over', 'an', 'algebroid', 'stack']] | [-0.3665453948196955, 0.014918346693775675, -0.07353638974018395, 0.039719678374240175, -0.16441000811755657, -0.13120178080862388, -0.023582065827213228, 0.43530779844149947, -0.39099133817944676, -0.1616085934219882, -0.005061806965386495, -0.13981296005658805, -0.22019072745752055, 0.20440678391605616, -0.1566840591... |
710.0644 | Difference sets and the primes | Suppose that A is a subset of {1,...,N} such that the difference between any
two elements of A is never one less than a prime. We show that |A| = O(N
exp(-c(log N)^{1/4})) for some absolute c>0.
| math.CA math.NT | suppose that a is a subset of 1n such that the difference between any two elements of a is never one less than a prime we show that a on expclog n14 for some absolute c0 | [['suppose', 'that', 'a', 'is', 'a', 'subset', 'of', '1n', 'such', 'that', 'the', 'difference', 'between', 'any', 'two', 'elements', 'of', 'a', 'is', 'never', 'one', 'less', 'than', 'a', 'prime', 'we', 'show', 'that', 'a', 'on', 'expclog', 'n14', 'for', 'some', 'absolute', 'c0']] | [-0.1594048242485668, 0.14218721717285612, -0.10255074785608384, 0.06728218819221689, -0.006776685554844637, -0.1291021132815836, 0.056104558183708124, 0.3789582600713604, -0.21785283738022876, -0.1963130271113995, 0.10185545133168085, -0.3686827054868142, -0.1281907255243924, 0.2339437250047922, -0.03737566481706583, ... |
710.0645 | Statistical analysis of Ni nanowires breaking processes: a numerical
simulation study | A statistical analysis of the breaking behavior of Ni nanowires is presented.
Using molecular dynamic simulations, we have determined the time evolution of
both the nanowire atomic structure and its minimum cross section (Sm(t)).
Accumulating thousands of independent breaking events, Sm histograms are built
and used ... | cond-mat.mes-hall cond-mat.mtrl-sci | a statistical analysis of the breaking behavior of ni nanowires is presented using molecular dynamic simulations we have determined the time evolution of both the nanowire atomic structure and its minimum cross section smt accumulating thousands of independent breaking events sm histograms are built and used to study t... | [['a', 'statistical', 'analysis', 'of', 'the', 'breaking', 'behavior', 'of', 'ni', 'nanowires', 'is', 'presented', 'using', 'molecular', 'dynamic', 'simulations', 'we', 'have', 'determined', 'the', 'time', 'evolution', 'of', 'both', 'the', 'nanowire', 'atomic', 'structure', 'and', 'its', 'minimum', 'cross', 'section', ... | [-0.1634932145773616, 0.19044446519209096, -0.019756472599900526, 0.019888208721779068, -0.015828487459917336, -0.12429876267456816, 0.03123948397114873, 0.44425269722185995, -0.2654171067240116, -0.3235154169087764, 0.04431599890228556, -0.2935420034918934, -0.06172563095917992, 0.1200889420875423, 0.07545065251516851... |
710.0646 | B_s and B_d mixing in full lattice QCD using NRQCD b quarks | We give a progress report on studies of B_s and B_d mixing with valence NRQCD
b quarks and asqtad light quarks on the MILC configurations including the
effect of 2+1 flavours of sea quarks. We explore methods for reducing
statistical and systematic errors in the ratio \xi =
f_{B_s}\sqrt{B_{B_s}}/f_{B_d}\sqrt{B_{B_d}}... | hep-lat | we give a progress report on studies of b_s and b_d mixing with valence nrqcd b quarks and asqtad light quarks on the milc configurations including the effect of 21 flavours of sea quarks we explore methods for reducing statistical and systematic errors in the ratio xi f_b_ssqrtb_b_sf_b_dsqrtb_b_d | [['we', 'give', 'a', 'progress', 'report', 'on', 'studies', 'of', 'b_s', 'and', 'b_d', 'mixing', 'with', 'valence', 'nrqcd', 'b', 'quarks', 'and', 'asqtad', 'light', 'quarks', 'on', 'the', 'milc', 'configurations', 'including', 'the', 'effect', 'of', '21', 'flavours', 'of', 'sea', 'quarks', 'we', 'explore', 'methods', ... | [-0.0676926461722147, 0.3749378610877915, -0.06650624261733065, 0.07399606712638064, 0.032607868908250584, -0.0799920286368975, 0.20987780075123968, 0.3827642050591555, -0.08432801133219867, -0.2456984411370247, -0.0019873510971863536, -0.35479135335759915, 0.016891545883597845, 0.0779390866927644, 0.004453889371708352... |
710.0647 | Absorption spectrum of the quasar HS1603+3820 I. Observations and data
analysis | We present the analysis of multi-wavelength observations of bright quasar
HS1603+3820: the optical data taken with the MMT and Keck telescopes, and X-ray
data obtained with the Chandra X-ray Observatory. The optical spectra contain a
very large number of absorption lines from numerous heavy elements. We derived
X-ray... | astro-ph | we present the analysis of multiwavelength observations of bright quasar hs16033820 the optical data taken with the mmt and keck telescopes and xray data obtained with the chandra xray observatory the optical spectra contain a very large number of absorption lines from numerous heavy elements we derived xray properties... | [['we', 'present', 'the', 'analysis', 'of', 'multiwavelength', 'observations', 'of', 'bright', 'quasar', 'hs16033820', 'the', 'optical', 'data', 'taken', 'with', 'the', 'mmt', 'and', 'keck', 'telescopes', 'and', 'xray', 'data', 'obtained', 'with', 'the', 'chandra', 'xray', 'observatory', 'the', 'optical', 'spectra', 'c... | [-0.06069940182792603, 0.09886507940722904, -0.02780977729326267, 0.050645276745704966, -0.08360885621094313, -0.10088522590651008, 0.04164768720893037, 0.49754614789099966, -0.14945013838682752, -0.35679672066061224, 0.07324278095859241, -0.3748957791029796, 0.003044036518568631, 0.18110322401921844, 0.019163702782548... |
710.0648 | Fragmenting D4 branes and coupled q-deformed Yang Mills | We compute the index of BPS states for two stacks of D4-branes wrapped on
ample divisors and overlapping over a compact Riemann surface inside
non-compact Calabi-Yau 3-fold. This index is given in terms of U(N) x U(M)
q-deformed Yang Mills theory with bifundamental matter. From the factorization
in the limit of large... | hep-th | we compute the index of bps states for two stacks of d4branes wrapped on ample divisors and overlapping over a compact riemann surface inside noncompact calabiyau 3fold this index is given in terms of un x um qdeformed yang mills theory with bifundamental matter from the factorization in the limit of large d4 charge we... | [['we', 'compute', 'the', 'index', 'of', 'bps', 'states', 'for', 'two', 'stacks', 'of', 'd4branes', 'wrapped', 'on', 'ample', 'divisors', 'and', 'overlapping', 'over', 'a', 'compact', 'riemann', 'surface', 'inside', 'noncompact', 'calabiyau', '3fold', 'this', 'index', 'is', 'given', 'in', 'terms', 'of', 'un', 'x', 'um'... | [-0.16102891063524616, 0.13394229443122943, -0.09049717168220216, 0.07628109039117893, -0.012784442991121775, -0.11709435061137709, 0.013621267336162014, 0.2888526788291832, -0.16127403467479678, -0.249776487911327, 0.06392470637543334, -0.2767227929085493, -0.10789161415563689, 0.0973608285913037, -0.10769786107767787... |
710.0649 | Exploring Partially Confined Phases | Phases of SU(N) gauge theories in which the global Z(N) symmetry breaks
spontaneously to a subgroup Z(L) can be realized by adding appropriate Wilson
line terms to the gauge action. These phases are partially confining, in the
sense that quarks are confined but bound states of L quarks are not. At
temperatures large ... | hep-lat | phases of sun gauge theories in which the global zn symmetry breaks spontaneously to a subgroup zl can be realized by adding appropriate wilson line terms to the gauge action these phases are partially confining in the sense that quarks are confined but bound states of l quarks are not at temperatures large compared to... | [['phases', 'of', 'sun', 'gauge', 'theories', 'in', 'which', 'the', 'global', 'zn', 'symmetry', 'breaks', 'spontaneously', 'to', 'a', 'subgroup', 'zl', 'can', 'be', 'realized', 'by', 'adding', 'appropriate', 'wilson', 'line', 'terms', 'to', 'the', 'gauge', 'action', 'these', 'phases', 'are', 'partially', 'confining', '... | [-0.1612825947519306, 0.35606074778512975, -0.08140334211261113, 0.1126158931774312, -0.05471183374609755, -0.19784491695998901, 0.09051354645066306, 0.3728339338444987, -0.23631038928896875, -0.29753715449665813, 0.07574383434090207, -0.2609420750737083, -0.06270661590428188, 0.05390119137263846, -0.019021725442645878... |
710.065 | Off-center impurity in alkali halides: reorientation, electric
polarization and pairing to F center. II. In-plane rotation and
polarizability | Because of its inherent 2-D character, the eigenvalue equation for the
hindered rotation around a normal cation site of an off-center impurity
nearest-neighboring an F center is the well-known Mathieu equation. We present
an overview of literature data on Mathieu's periodic functions providing exact
solutions to the ... | physics.chem-ph | because of its inherent 2d character the eigenvalue equation for the hindered rotation around a normal cation site of an offcenter impurity nearestneighboring an f center is the wellknown mathieu equation we present an overview of literature data on mathieus periodic functions providing exact solutions to the li reorie... | [['because', 'of', 'its', 'inherent', '2d', 'character', 'the', 'eigenvalue', 'equation', 'for', 'the', 'hindered', 'rotation', 'around', 'a', 'normal', 'cation', 'site', 'of', 'an', 'offcenter', 'impurity', 'nearestneighboring', 'an', 'f', 'center', 'is', 'the', 'wellknown', 'mathieu', 'equation', 'we', 'present', 'an... | [-0.16959530178849636, 0.07925006299429745, 0.0026220623354770633, 0.042181106726638974, -0.07746516783770761, -0.1283525649164068, 0.04144647619441936, 0.3863865846866055, -0.283634371496737, -0.23863921920756662, 0.020244101591800387, -0.3245219760721451, -0.10435147834941745, 0.1368399211058491, 0.037603072211832594... |
710.0651 | Quantum Margulis expanders | We present a simple way to quantize the well-known Margulis expander map. The
result is a quantum expander which acts on discrete Wigner functions in the
same way the classical Margulis expander acts on probability distributions. The
quantum version shares all essential properties of the classical counterpart,
e.g., ... | quant-ph math-ph math.MP | we present a simple way to quantize the wellknown margulis expander map the result is a quantum expander which acts on discrete wigner functions in the same way the classical margulis expander acts on probability distributions the quantum version shares all essential properties of the classical counterpart eg it has th... | [['we', 'present', 'a', 'simple', 'way', 'to', 'quantize', 'the', 'wellknown', 'margulis', 'expander', 'map', 'the', 'result', 'is', 'a', 'quantum', 'expander', 'which', 'acts', 'on', 'discrete', 'wigner', 'functions', 'in', 'the', 'same', 'way', 'the', 'classical', 'margulis', 'expander', 'acts', 'on', 'probability', ... | [-0.09772243513611566, 0.1009850976166918, -0.1436214073488087, 0.08176473265755739, -0.1205278494676082, -0.15146257415158199, 0.01884266307951846, 0.37520462458989784, -0.25837030564891356, -0.24302697914889923, 0.10913704585411824, -0.2506752816741081, -0.1854190691328589, 0.24956516057764197, -0.13950672469503594, ... |
710.0652 | Matrix pairs over discrete valuation rings determine
Littlewood-Richardson fillings | Let M and N be two r x r matrices over a discrete valuation ring of
characteristic zero. The orders (with respect to a uniformizing parameter) of
the invariant factors of M form a partition of non-negative integers, called
the invariant partition of M. Let the invariant partition of M be mu, of N be
nu, and of the pr... | math.CO math.AC | let m and n be two r x r matrices over a discrete valuation ring of characteristic zero the orders with respect to a uniformizing parameter of the invariant factors of m form a partition of nonnegative integers called the invariant partition of m let the invariant partition of m be mu of n be nu and of the product mn b... | [['let', 'm', 'and', 'n', 'be', 'two', 'r', 'x', 'r', 'matrices', 'over', 'a', 'discrete', 'valuation', 'ring', 'of', 'characteristic', 'zero', 'the', 'orders', 'with', 'respect', 'to', 'a', 'uniformizing', 'parameter', 'of', 'the', 'invariant', 'factors', 'of', 'm', 'form', 'a', 'partition', 'of', 'nonnegative', 'inte... | [-0.21906801438091128, 0.12386730379599178, -0.10043783857375939, 0.01612936941222218, -0.05347553165907513, -0.16605448535879824, 0.029974271537242598, 0.3076893380189787, -0.33647361805023096, -0.22947634716340995, 0.05275543809889246, -0.2538714673345797, -0.1190209594214641, 0.1195895043757758, -0.06028795617618667... |
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