Search results for "Boltzmann constant"

showing 10 items of 34 documents

On the CP asymmetries in Majorana neutrino decays

1997

We study the CP asymmetries in lepton number violating two body scattering processes and show explicitly how they vanish, in agreement with unitarity constraints. We relate these cross section asymmetries to the CP decay rate asymmetries of the intermediate massive neutrinos and show how the inclusion of the Universe expansion via Boltzmann equations is the key ingredient to allow the production of a non-vanishing asymmetry in spite of the unitarity constraint on the cross sections. We then show that the absorptive parts of both the one loop vertex and self energy corrections do contribute to the CP decay asymmetries.

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityScatteringmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyFOS: Physical sciencesLepton numberAsymmetryHigh Energy Physics - Phenomenologysymbols.namesakeMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Self-energyBoltzmann constantsymbolsHigh Energy Physics::ExperimentNeutrinomedia_common
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Trajectory Statistics of Confined L\'evy Flights and Boltzmann-type Equilibria

2013

We analyze a specific class of random systems that are driven by a symmetric L\'{e}vy stable noise, where Langevin representation is absent. In view of the L\'{e}vy noise sensitivity to environmental inhomogeneities, the pertinent random motion asymptotically sets down at the Boltzmann-type equilibrium, represented by a probability density function (pdf) $\rho_*(x) \sim \exp [-\Phi (x)]$. Here, we infer pdf $\rho (x,t)$ based on numerical path-wise simulation of the underlying jump-type process. A priori given data are jump transition rates entering the master equation for $\rho (x,t)$ and its target pdf $\rho_*(x)$. To simulate the above processes, we construct a suitable modification of t…

PhysicsPhysical systemGeneral Physics and AstronomyContext (language use)Probability density functionGillespie algorithmsymbols.namesakeLévy flightBoltzmann constantMaster equationsymbolsStatistical physicsCondensed Matter - Statistical MechanicsBrownian motionActa Physica Polonica B
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Analytical Expressions for Radiative Losses in Solar Cells

2019

Analytical expressions for the fundamental losses in single junction solar cells are revised and improved. The losses are, as far as possible, described using parameters with clear physical interpretations. One important improvement compared to earlier work is the use of Lambert’s W function, which allows for analytical expressions for the voltage and current at the maximum power point. Other improvements include the use of Stefan Boltzmann’s law to describe the incoming energy flux as well as taking into account the fermionic nature of the electrons when calculating the thermalization loss. A new expression, which combines emission, Boltzmann and Carnot losses, is presented. Finally, an ex…

PhysicsWork (thermodynamics)Stefan–Boltzmann lawMaximum power principleEnergy flux02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesExpression (mathematics)Computational physicssymbols.namesake0103 physical sciencesBoltzmann constantsymbolsRadiative transfer010306 general physics0210 nano-technologyCarnot cycle2019 IEEE 46th Photovoltaic Specialists Conference (PVSC)
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On the full Boltzmann equations for leptogenesis

2009

We consider the full Boltzmann equations for standard and soft leptogenesis, instead of the usual integrated Boltzmann equations which assume kinetic equilibrium for all species. Decays and inverse decays may be inefficient for thermalising the heavy-(s)neutrino distribution function, leading to significant deviations from kinetic equilibrium. We analyse the impact of using the full kinetic equations in the case of a previously generated lepton asymmetry, and find that the washout of this initial asymmetry due to the interactions of the right-handed neutrino is larger than when calculated via the integrated equations. We also solve the full Boltzmann equations for soft leptogenesis, where t…

PhysicsleptogenesisParticle physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyFOS: Physical sciencesInverseFísicaAstronomy and AstrophysicsKinetic energyAsymmetrysymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution functionneutrino theoryLeptogenesisBoltzmann constantsymbolsphysics of the early universeHigh Energy Physics::ExperimentNeutrinomedia_commonLepton
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Exact results for the homogeneous cooling state of an inelastic hard-sphere gas

1998

The infinite set of moments of the two-particle distribution function is found exactly for the uniform cooling state of a hard-sphere gas with inelastic collisions. Their form shows that velocity correlations cannot be neglected, and consequently the 'molecular chaos' hypothesis leading to the inelastic Boltzmann and Enskog kinetic equations must be questioned. © 1998 Cambridge University Press.

Physicssymbols.namesakeInfinite setClassical mechanicsDistribution functionBoltzmann constantsymbolsInelastic collisionMolecular chaosHard spheresInelastic scatteringCondensed Matter PhysicsBoltzmann equationJournal of Plasma Physics
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Iterative integral equation methods for structural coarse-graining

2021

In this paper, new Newton and Gauss-Newton methods for iterative coarse-graining based on integral equation theory are evaluated and extended. In these methods, the potential update is calculated from the current and target radial distribution function, similar to iterative Boltzmann inversion, but gives a potential update of quality comparable with inverse Monte Carlo. This works well for the coarse-graining of molecules to single beads, which we demonstrate for water. We also extend the methods to systems that include coarse-grained bonded interactions and examine their convergence behavior. Finally, using the Gauss-Newton method with constraints, we derive a model for single bead methano…

Quantitative Biology::BiomoleculesMonte Carlo methodGeneral Physics and AstronomyInverseRadial distribution functionIntegral equationInversion (discrete mathematics)symbols.namesakeBoltzmann constantConvergence (routing)symbolsApplied mathematicsGranularityPhysical and Theoretical ChemistryMathematicsThe Journal of Chemical Physics
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2019

Abstract Heavy quarkonium related observables are very useful to obtain information about the medium created in relativistic heavy ion collisions. In recent years the theoretical description of quarkonium in a medium has moved towards a more dynamical picture in which decay and recombination processes are very important. In this talk we will discuss the equations that describe the evolution of the heavy quark reduced density matrix in different approximations, highlighting the color dynamics that is absent in the Abelian case, and we will study their semi-classical limit. This will allow us to obtain stochastic equations (similar to Langevin or Boltzmann equations) that can be useful to obt…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyObservableQuarkonium7. Clean energy01 natural sciencesBoltzmann equationsymbols.namesake0103 physical sciencesBoltzmann constantQuark–gluon plasmasymbols010306 general physicsQuantumNuclear Physics A
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Fractional Viscoelasticity Under Combined Stress and Temperature Variations

2020

Nowadays polymeric materials or composites with polymeric matrices are widely used in a very wide range of applications such as aerospace, automotive, biomedical and also civil engineering. From a mechanical point of view, polymers are characterized by high viscoelastic properties and high sensitiveness of mechanical parameters from temperature. Analytical predictions in real-life conditions of mechanical behaviour of such a kind of materials is not trivial for the intrinsic hereditariness that imply the knowledge of all the history of the material at hand in order to predict the response to applied external loads. If temperature variations are also present in the materials, a reliable eval…

Stress (mechanics)symbols.namesakeWork (thermodynamics)Superposition principleMaterials scienceDiscretizationStochastic processMonte Carlo methodBoltzmann constantsymbolsMechanicsViscoelasticity
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Transition probabilities for some infrared O I spectral lines—Application for determining excitation temperatures in low temperature plasmas

2008

Intensities of selected spectral transitions of neutral oxygen emitted from a wall-stabilized arc have been measured. Applying reliable transition probability data taken from literature, Boltzmann plots have been constructed and the temperatures of the plasma have been obtained. At arc plasma conditions ensuring partial local thermal equilibrium, transition probabilities for 4 O I spectral lines from the near infrared spectral range have been obtained. These new results, together with data for two other studied O I spectral lines taken from the National Institute of Standards and Technology data base, are proposed as a suitable set of transition probabilities applicable for diagnostics of l…

Thermal equilibriumRange (particle radiation)ChemistryInfraredNear-infrared spectroscopyPlasmaAtomic and Molecular Physics and OpticsSpectral lineAnalytical Chemistrysymbols.namesakeBoltzmann constantsymbolsAtomic physicsInstrumentationSpectroscopyExcitationSpectrochimica Acta Part B: Atomic Spectroscopy
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Intrinsic viscosities of polyelectrolytes in the absence and in the presence of extra salt: Consequences of the stepwise conversion of dextran into a…

2011

Abstract Viscosities of dilute polymer solutions were measured in capillary viscometers for samples varying in their fraction f of charged units from 0.00 to 0.90. The dependence of the logarithm of the relative viscosity on polymer concentration c is in all cases reproduced quantitatively by three characteristic parameters: [ η ], the intrinsic viscosity; B , a viscometric interaction parameter (related to the Huggins constant); [ η ] , a parameter required only for polyelectrolytes at low concentrations of extra salt. In pure water [ η ] increases more than 80 times as the fraction f rises from zero to 0.90 and [ η ] starts from zero and goes up to ≈71 mL/g. Upon the addition of NaCl [ η …

chemistry.chemical_classificationPolymers and PlasticsChemistryIntrinsic viscosityRelative viscosityOrganic ChemistryViscometerThermodynamicsPolymerFlory–Huggins solution theoryPolyelectrolytesymbols.namesakeBoltzmann constantPolymer chemistryMaterials ChemistrysymbolsOrder of magnitudeCarbohydrate polymers
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