Search results for "EXPA"

showing 10 items of 820 documents

The Fokker-Planck Equation

2009

PhysicsStochastic differential equationSystem size expansionStochastic processFokker–Planck equationStatistical physics
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Quantum order by disorder in the Kitaev model on a triangular lattice

2015

We identify and discuss the ground state of a quantum magnet on a triangular lattice with bond-dependent Ising-type spin couplings, that is, a triangular analog of the Kitaev honeycomb model. The classical ground-state manifold of the model is spanned by decoupled Ising-type chains, and its accidental degeneracy is due to the frustrated nature of the anisotropic spin couplings. We show how this subextensive degeneracy is lifted by a quantum order-by-disorder mechanism and study the quantum selection of the ground state by treating short-wavelength fluctuations within the linked cluster expansion and by using the complementary spin-wave theory. We find that quantum fluctuations couple next-n…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Topological degeneracyFOS: Physical sciencesCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter Physics; Electronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsQuantum mechanicsElectronicHexagonal latticeOptical and Magnetic MaterialsGround stateDegeneracy (mathematics)QuantumQuantum fluctuationCluster expansionSpin-½Physical Review B
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Relative velocities for radial motion in expanding Robertson-Walker spacetimes

2011

The expansion of space, and other geometric properties of cosmological models, can be studied using geometrically defined notions of relative velocity. In this paper, we consider test particles undergoing radial motion relative to comoving (geodesic) observers in Robertson-Walker cosmologies, whose scale factors are increasing functions of cosmological time. Analytical and numerical comparisons of the Fermi, kinematic, astrometric, and the spectroscopic relative velocities of test particles are given under general circumstances. Examples include recessional comoving test particles in the de Sitter universe, the radiation-dominated universe, and the matter-dominated universe. Three distinct …

PhysicsSuperluminal motionPhysics and Astronomy (miscellaneous)SpacetimeGeodesicmedia_common.quotation_subjectFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)83F05 83C99General Relativity and Quantum CosmologyUniverseMetric expansion of spaceGeneral Relativity and Quantum CosmologyClassical mechanicsDe Sitter universeFermi coordinatesTest particleMathematical Physicsmedia_commonGeneral Relativity and Gravitation
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Heavy Elements and Age Determinations

2002

The age of the universe, measured from the Big Bang to the present, is at the focus of cosmology. Its determination relies, however, on the use of stellar objects or their products. Stellar explosions, like type Ia supernovae serve as standard(izable) candles to measure the expansion of the universe. Hertzsprung—Russell diagrams of globular clusters can determine the age of such clusters and thus are lower limits of the age of the galaxy and therefore also the universe. Some nuclear isotopes with half-lives comparable to the age of galaxies (and the universe) can serve as clocks (chronometers) for the duration of nucleosynthesis. The isotopes 238U and 232Th with half-lives of 4.5 × l09 and …

PhysicsSupernovaAge of the universeNucleosynthesisGlobular clusterAstronomyAstrophysicsGalaxyCosmologyNucleocosmochronologyMetric expansion of space
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Dust Envelope in Young Supernova Remnants

1974

As stated by Hoyle and Wickramasinghe (1970), hereafter referred to as HW, a significant fraction of the mass ejected by exploding supernovae may condense into solid particles during the expansion phase following explosion. Hence, observable effects on supernova light curves are to be expected.

PhysicsSupernovaCrab NebulaAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Solar and Stellar AstrophysicsAstronomyObservableAstrophysicsExpansion phaseNear-Earth supernovaLight curveEnvelope (waves)Luminosity
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Memory expansion for diffusion coefficients

1998

We present a memory expansion for macroscopic transport coefficients such as the collective and tracer diffusion coefficients ${D}_{C}$ and ${D}_{T},$ respectively. The successive terms in this expansion for ${D}_{C}$ describe rapidly decaying memory effects of the center-of-mass motion, leading to fast convergence when evaluated numerically. For ${D}_{T},$ one obtains an expansion of similar form that contains terms describing memory effects in single-particle motion. As an example we evaluate ${D}_{C}$ and ${D}_{T}$ for three strongly interacting surface systems through Monte Carlo simulations, and for a simple model diffusion system via molecular dynamics calculations. We show that the n…

PhysicsSurface (mathematics)SpeedupNumerical analysisPhysicsMonte Carlo methodmacroscopic transport coefficients02 engineering and technology021001 nanoscience & nanotechnologysurface systems01 natural sciencesMonte Carlo simulationsMolecular dynamics0103 physical sciencesConvergence (routing)numerical methodsDiffusion (business)010306 general physics0210 nano-technologyOrder of magnitudeMathematical physicsmemory expansions
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Multipole response of $^3$He clusters

1991

Ground state properties of normal 3He drops have been studied using either a correlated wave function in conjunction with a realistic potential of Aziz type1) or a mean-field description based on an effective potential 2,3). In general, an overall good agreement between both methods has been found. The second one has the advantage of being rather easily applicable to both static and dynamic calculations, although being less fundamental than the first one. In this work we are concerned with the description of the collective modes of normal 3He drops within the self-consistent Random-Phase Approximation (RPA), in which the same effective interaction is used to generate both the mean-field and…

PhysicsSurface (mathematics)[PHYS.NUCL] Physics [physics]/Nuclear Theory [nucl-th]Work (thermodynamics)[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Field (physics)Magnetic monopoleResidual01 natural sciences010305 fluids & plasmasQuantum electrodynamics0103 physical sciences010306 general physicsMultipole expansionGround stateWave function
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Elementary theory and brief history

1991

In the history of the theory of deuteron photodisintegration one may distinguish roughly three periods: (i) the primitive period of the elementary theory using very simple wave functions and forces and considering lowest multipoles (E1, M1) only, (ii) the classical period still in the framework f conventional nuclear physics, but using realstic forces with correspondingly elaborate wave functions and considering also higher multipole transitions, (ii) the post-classic period with explicit treatment of subnuclear degrees of freedom like meson and isobar degrees of freedom and very recently quark-gluon degrees of freedom.

PhysicsTheoretical physicsMesonPhotodisintegrationSimple (abstract algebra)Nuclear TheoryDegrees of freedomIsobarElementary theoryNuclear ExperimentMultipole expansionWave function
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Methods of calculation for the T-matrix

1991

In the preceding section we have shown how the observables can be expressed in terms of the T-matrix elements or in terms of the multipole amplitudes OLλ(μjls) which contain all the relevant information on the dynamical properties of the system. For the calculation of these amplitudes a variety of different methods have been developed utilizing various kinds of approximations.

PhysicsTheoretical physicsT matrixAmplitudeSection (archaeology)ObservableVariety (universal algebra)Multipole expansionRelevant information
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Isovector spin-multipole strength distributions in double- β -decay triplets

2017

In this work the energetics and strength distributions of isovector spin-dipole and spin-quadrupole transitions from the ground states of the pairs ($^{76}\mathrm{Ge}, ^{76}\mathrm{Se}$), ($^{82}\mathrm{Se}, ^{82}\mathrm{Kr}$), ($^{96}\mathrm{Zr}, ^{96}\mathrm{Mo}$), ($^{100}\mathrm{Mo}, ^{100}\mathrm{Ru}$), ($^{116}\mathrm{Cd}, ^{116}\mathrm{Sn}$), ($^{128}\mathrm{Te}, ^{128}\mathrm{Xe}$), ($^{130}\mathrm{Te}, ^{130}\mathrm{Xe}$), and ($^{136}\mathrm{Xe}, ^{136}\mathrm{Ba}$), of double-$\ensuremath{\beta}$-decay initial and final nuclei, to the ${J}^{\ensuremath{\pi}}={0}^{\ensuremath{-}},{1}^{\ensuremath{-}},{2}^{\ensuremath{-}},{1}^{+},{2}^{+}$, and ${3}^{+}$ excited states of the interm…

PhysicsValence (chemistry)ta114Isovector010308 nuclear & particles physicsdouble beta decaycollective models01 natural sciencesExcited state0103 physical sciencesQuasiparticlecharge-exchange reactionsAtomic physics010306 general physicsMultipole expansionSpin (physics)Physical Review C
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