Search results for "BEC"

showing 10 items of 947 documents

First-order and tricritical wetting transitions in the two-dimensional Ising model caused by interfacial pinning at a defect line

2014

We present a study of the critical behavior of the Blume-Capel model with three spin states (S=±1,0) confined between parallel walls separated by a distance L where competitive surface magnetic fields act. By properly choosing the crystal field (D), which regulates the density of nonmagnetic species (S=0), such that those impurities are excluded from the bulk (where D=) except in the middle of the sample [where DM(L/2)≠], we are able to control the presence of a defect line in the middle of the sample and study its influence on the interface between domains of different spin orientations. So essentially we study an Ising model with a defect line but, unlike previous work where defect lines …

Spin statesCiencias FísicasMateriales confinadosInterfacesPhase Transition//purl.org/becyt/ford/1 [https]ImpurityComputer SimulationSimulaciones computacionalesPhase diagramPhysicsCondensed matter physics//purl.org/becyt/ford/1.3 [https]Models TheoreticalFirst orderMagnetic fieldHysteresisMagnetic FieldsWettabilityThermodynamicsTransiciones de mojadoIsing modelWettingMonte Carlo MethodCIENCIAS NATURALES Y EXACTASFísica de los Materiales CondensadosPhysical Review E
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Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC

2013

We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portu…

Standard Modeldilepton: mass spectrumCiencias Físicas01 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHiggs particle: hadroproduction//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)vector boson: fusion[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCBosonPhysicsHIGGS BOSONLarge Hadron Collidervector boson: pair productiontransverse energy: missing-energy4. EducationATLAS experimentSettore FIS/01 - Fisica SperimentaleATLAS3. Good healthMassless particleCERN LHC CollHiggs particle: massPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs boson7000: 8000 GeV-cmsFísica nuclearAtlasLhcNeutrinoHiggs particle: decay modesParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASp p: scatteringNuclear and High Energy PhysicsParticle physicsmass spectrum: (4lepton)530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2ATLASdetector; LHC; Higgsbosonproduction; diboson530Massless ParticlesNnlo QCDNuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsTransverse-MomentumCondensed Matter::Quantum GasesHiggs particle: couplingScience & Technologyhep-ex010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQCD CorrectionsFermion//purl.org/becyt/ford/1.3 [https]Hadron CollidersDiboson ProductionAstronomíavector boson: leptonic decayHADRON-HADRON COLLISIONSProton-Proton CollisionsRoot-S=7 TevHiggs particle: hadroproduction ; Higgs particle: coupling ; vector boson: fusion ; p p: scattering ; CERN LHC Coll ; ATLAS ; Higgs particle: decay modes ; vector boson: pair production ; vector boson: leptonic decay ; mass spectrum: two-photon ; mass spectrum: (4lepton) ; dilepton: mass spectrum ; transverse energy: missing-energy ; Higgs particle: mass ; experimental results ; 7000: 8000 GeV-cmsExperimental High Energy PhysicsHigh Energy Physics::ExperimentCross-Sectionsmass spectrum: two-photonexperimental resultsLeptonBroken Symmetries
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Cross-Commodity Spot Price Modeling with Stochastic Volatility and Leverage For Energy Markets

2013

Spot prices in energy markets exhibit special features, such as price spikes, mean reversion, stochastic volatility, inverse leverage effect, and dependencies between the commodities. In this paper a multivariate stochastic volatility model is introduced which captures these features. The second-order structure and stationarity of the model are analyzed in detail. A simulation method for Monte Carlo generation of price paths is introduced and a numerical example is presented.

Statistics and Probability15A04Spot contractSABR volatility model01 natural sciences010104 statistics & probabilityEnergy marketVolatility swap0502 economics and businessEconometricsForward volatilityMean reversionstochastic volatilityleverage0101 mathematicsMathematics050208 financeStochastic volatilityApplied Mathematics05 social sciences91G60subordinator91G20Constant elasticity of variance modelVolatility smileOrnstein-Uhlenbeck process60H3060G1060G51Advances in Applied Probability
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Dynamic-Interactive Graphics for Statistics (26 years later)

2014

This paper briefly reviews the history of dynamic-interactive graphicsfor statistics, introduces an example of such graphics, and provides a fewglimpses as to the current state of things and the future trends we envision.The general conclusion is that dynamic-interactive graphics for statistics arethriving more than ever as they shift from the desktop to the internet. Thus,dynamic-interactive graphics are becoming increasingly important as they: 1) provide non-experts in statistics with the means to carry out analyses on their own; and 2) teach the basic concepts of statistics to students and practitioners with low to moderate  mathematics skills. Their increasingpopularity makes the lesson…

Statistics and ProbabilityDYNAMIC-GRAPHICS31 Colecciones de estadística general / StatisticsInteractive graphics//purl.org/becyt/ford/1 [https]Data visualizationStatisticsGraphicsGráficas dinámicasStatistical graphicslcsh:Statisticslcsh:HA1-4737business.industryData VisualizationSubject (documents)Dynamic Graphics//purl.org/becyt/ford/1.2 [https]PopularitySTATISTICSStatistical Graphicsgráficas dinámicas51 Matemáticas / MathematicsVisualizaciónvisualizaciónCiencias de la Computación e InformaciónThrivingThe InternetDATA-VISUALIZATIONbusinessgráficas estadísticasGráficas estadísticasCiencias de la Información y BioinformáticaCIENCIAS NATURALES Y EXACTAS
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Ergodicity for a stochastic Hodgkin–Huxley model driven by Ornstein–Uhlenbeck type input

2013

We consider a model describing a neuron and the input it receives from its dendritic tree when this input is a random perturbation of a periodic deterministic signal, driven by an Ornstein-Uhlenbeck process. The neuron itself is modeled by a variant of the classical Hodgkin-Huxley model. Using the existence of an accessible point where the weak Hoermander condition holds and the fact that the coefficients of the system are analytic, we show that the system is non-degenerate. The existence of a Lyapunov function allows to deduce the existence of (at most a finite number of) extremal invariant measures for the process. As a consequence, the complexity of the system is drastically reduced in c…

Statistics and ProbabilityDegenerate diffusion processesWeak Hörmander conditionType (model theory)01 natural sciencesPeriodic ergodicity010104 statistics & probability60H0760J25FOS: Mathematics0101 mathematicsComputingMilieux_MISCELLANEOUSMathematical physicsMathematics60J60Quantitative Biology::Neurons and CognitionProbability (math.PR)010102 general mathematicsErgodicityOrnstein–Uhlenbeck processHodgkin–Huxley model[MATH.MATH-PR]Mathematics [math]/Probability [math.PR]Hodgkin–Huxley model60J60 60J25 60H07Statistics Probability and UncertaintyTime inhomogeneous diffusion processesMathematics - Probability
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Tucumanin, a β-hydroxy-γ-lactone bistetrahydrofuranic acetogenin from Annona cherimolia, is a potent inhibitor of mitochondrial complex I

2004

A new β-hydroxy-γ-methyl-γ-lactone bistetrahydrofuranic acetogenin, tucumanin, with the infrequent symmetrical threo/trans/threo/trans/ threo relative configuration at the tetrahydrofuran rings was isolated from Annona cherimolia (Annonaceae) seeds. The inhibitory potency on the mitochondrial complex I of acetogenins with this relative configuration (tucumanin and asimicin) was compared with that shown by the corresponding pairs with an asymmetrical threo/trans/threo/trans/erythro relative configuration (laherradurin/rolliniastatin-2, and itrabin/molvizarin). All these compounds act as selective inhibitors of mitochondrial complex 1 in the 0.18 - 1.55 nM range. Fil: Barrachina, Isabel. Univ…

StereochemistryChemical structurePharmaceutical Scienceinhibitory potencyBiologyAnnonaMitochondria HeartAnalytical Chemistry//purl.org/becyt/ford/1 [https]chemistry.chemical_compoundInhibitory Concentration 50LactonesDrug Discovery//purl.org/becyt/ford/1.4 [https]HumansEnzyme InhibitorsAnnona cherimoliaFuransTetrahydrofuranPharmacologychemistry.chemical_classificationElectron Transport Complex IPlant ExtractsOtras Ciencias QuímicasOrganic ChemistryDiastereomerCiencias Químicasbiology.organism_classificationβ-hydroxy-γ-methyl-γ-lactoneComplementary and alternative medicinechemistryAnnonaceaeAnnona cherimolia (Annonaceae)AcetogeninSeedsMolecular MedicineMitochondrial Complex ILactonemitochondrial complex ICIENCIAS NATURALES Y EXACTASPhytotherapy
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BROWNIAN DYNAMICS SIMULATIONS WITHOUT GAUSSIAN RANDOM NUMBERS

1991

We point out that in a Brownian dynamics simulation it is justified to use arbitrary distribution functions of random numbers if the moments exhibit the correct limiting behavior prescribed by the Fokker-Planck equation. Our argument is supported by a simple analytical consideration and some numerical examples: We simulate the Wiener process, the Ornstein-Uhlenbeck process and the diffusion in a Φ4 potential, using both Gaussian and uniform random numbers. In these examples, the rate of convergence of the mean first exit time is found to be nearly identical for both types of random numbers.

Stochastic processMathematical analysisGeneral Physics and AstronomyStatistical and Nonlinear PhysicsOrnstein–Uhlenbeck processBrownian excursionBrownian bridgeComputer Science Applicationssymbols.namesakeComputational Theory and MathematicsWiener processReflected Brownian motionStochastic simulationsymbolsStatistical physicsGaussian processMathematical PhysicsMathematicsInternational Journal of Modern Physics C
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L'Analogie chez Aristote

2021

Revue de philosophie dont l’objet est de montrer, d’interroger ou d’évaluer les comparaisons effectives dans les différents champs disciplinaires, Analogia est une publication scientifique annuelle de l’IPC.Chaque numéro réunit un conseil scientifique nouveau chargé de sélectionner les contributions en double aveugle.L’Analogie chez Aristote.Sous la direction d’Emmanuel Brochier.Conseil scientifique :- Katerina Ierodiakonou (Genève – Athènes)- André Laks (Paris)- Benjamin C. Morison (Princeton)- Jean-Luc Solère (Boston)Sommaire :- Présentation, par Emmanuel Brochier, p. 5 ;- Christof Rapp : "Spotting similarities between disparate items" Observations on the use of analogy in Aristotle’s met…

StoïcismeThomas d'AquinAnalogieLightAlbert le GrandMetaphysicsPrime unmoved moverPuissanceAlbert the GreatPrincipesPlatonActeScala naturaeRhétorique[SHS.PHIL] Humanities and Social Sciences/PhilosophyThomas AquinasConcept formationÉtiologieMétaphysiqueMétaphoreMeteorologiaPoétiqueDiaphaneCouleursColorsUnityAristotle's Theory of CausesBienCausesTopiquesEthical naturalismActualizationNaturalisme éthiqueAnalogia entisMetaphorPremier moteur immobileComparaisonBiologieBecomingStoicismCauses chez AristoteÉquivocité (homonymie)AnalogyScienceMétaphysique LambdaAgent intellectEpicurianismLumièreSpontaneous generationBeingÊtreComparisonAristotle's PhysicsFormation de conceptsÉpicurismeAristotleUnitéGoodPoeticsGodSubstancePhysique d'AristoteBiologyMétéorologiePlatoMetaphysics LambdaRègles de comparaisonDevenirHomonymyDiaphanousCommensuratePotencyNon homonymyAristoteDieuActSimilitudeGénération spontanéeNon-équivocitéCommensurableTopicsPowerPrénotion (prolepsis)Rules of comparisonAnticipation (prolepsis)ActualisationRhetoricsÆtiologyIntellect AgentPrinciplesNotion
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Structure finding in cosmological simulations: the state of affairs

2013

The ever increasing size and complexity of data coming from simulations of cosmic structure formation demands equally sophisticated tools for their analysis. During the past decade, the art of object finding in these simulations has hence developed into an important discipline itself. A multitude of codes based upon a huge variety of methods and techniques have been spawned yet the question remained as to whether or not they will provide the same (physical) information about the structures of interest. Here we summarize and extent previous work of the "halo finder comparison project": we investigate in detail the (possible) origin of any deviations across finders. To this extent we decipher…

Structure formationCosmology and Nongalactic Astrophysics (astro-ph.CO)Ciencias FísicasDark matterFOS: Physical sciencesAstrophysicsGALAXIES HALOESAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciences//purl.org/becyt/ford/1 [https]0103 physical sciencesGalaxy formation and evolutionStatistical physics010303 astronomy & astrophysicsGalaxy rotation curveComputingMilieux_MISCELLANEOUSPhysics[PHYS]Physics [physics]COSMIC cancer database010308 nuclear & particles physicsAstronomy and AstrophysicsObservable//purl.org/becyt/ford/1.3 [https]AstronomíaGravitational lensSpace and Planetary ScienceLUMINOSITY FUNCTIONHaloGALAXIES EVOLUTION[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]CIENCIAS NATURALES Y EXACTASAstrophysics - Cosmology and Nongalactic AstrophysicsGALAXIES STATISTICS
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Observable Variables in Thermoelectric Phenomena

2002

New transport equations for the thermoelectric phenomena have been deduced. All of the variables in this formulation are observable quantities. The limitations of the usual formulations, which work with nonobservable quantities, have been overcome. The electric potential can be measured by using auxiliary probes which connect the electronic conductor to a potentiometer. This observable electric potential depends on the nature of the probes but not on the room temperature where the potentiometer is placed. Also, we emphasize that absolute values for the thermoelectric power are in contradiction with the thermodynamic limitation of measuring electric potential differences in these systems. Th…

SuperconductivityWork (thermodynamics)ChemistryThermodynamicsObservableSurfaces Coatings and FilmsConductorQuantum electrodynamicsSeebeck coefficientThermoelectric effectMaterials ChemistryPotentiometerElectric potentialPhysical and Theoretical ChemistryThe Journal of Physical Chemistry B
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