Search results for "quantity"

showing 10 items of 151 documents

Spectral energy distribution and generalized Wien's law for photons and cosmic string loops

2014

Physical objects with energy $u_w(l) \sim l^{-3w}$ with $l$ characteristic length and $w$ a dimensionless constant, lead to an equation of state $p=w\rho$, with $p$ the pressure and $\rho$ the energy density. Special entities with thisbproperty are, for instance, photons ($u = hc/l$, with $l$ the wavelength) with $w = 1/3$, and some models of cosmic string loops ($u =(c^4/aG)l$, with $l$ the length of the loop and $a$ a numerical constant), with $w = -1/3$. Here, we discuss some features of the spectral energy distribution of these systems and the corresponding generalization of Wien's law, which in terms of $l$ has the form $Tl_{mp}^{3w}=constant$, being $l_{mp}$ the most probable size of …

PhysicsPhotons cosmic string loops statistical mechanics Wien's law dark energy.PhotonCharacteristic lengthEquation of state (cosmology)Condensed Matter PhysicsAtomic and Molecular Physics and OpticsLoop (topology)Cosmic stringLawSpectral energy distributionConstant (mathematics)Settore MAT/07 - Fisica MatematicaMathematical PhysicsDimensionless quantityPhysica Scripta
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Nonstationary oscillations in gyrotrons

2001

The onset of stochastic oscillations in gyrotrons is studied by means of the self-consistent theory describing nonstationary processes. Complicated alternating sequences of regions of stationary, automodulation, and chaotic oscillations are found in the plane of the generalized gyrotron variables: cyclotron resonance mismatch and dimensionless current. The results of the investigations are important in connection with attempts to increase the output power of gyrotrons by raising the current.

PhysicsPlane (geometry)Cyclotron resonanceCondensed Matter PhysicsMicrowave oscillatorslaw.inventionPower (physics)Nuclear magnetic resonancePhysics::Plasma PhysicslawGyrotronQuantum electrodynamicsCurrent (fluid)Chaotic oscillationsDimensionless quantityPhysics of Plasmas
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Anomalous Spreading of Power-Law Quantum Wave Packets

1999

We introduce power-law tail quantum wave packets. We show that they can be seen as eigenfunctions of a Hamiltonian with a physical potential. We prove that the free evolution of these packets presents an asymptotic decay of the maximum of the wave packets which is anomalous for an interval of the characterizing power-law exponent. We also prove that the number of finite moments of the wave packets is a conserved quantity during the evolution of the wave packet in the free space.

PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Network packetWave packetFOS: Physical sciencesGeneral Physics and AstronomyEigenfunctionPower lawConserved quantityComputer Science::Performancesymbols.namesakeQuantum mechanicsComputer Science::Networking and Internet ArchitecturesymbolsExponentQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)QuantumCondensed Matter - Statistical MechanicsPhysical Review Letters
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Measurement of theB0→π−l+νForm-Factor Shape and Branching Fraction, and Determination of|Vub|with a Loose Neutrino Reconstruction Technique

2007

We report the results of a study of the exclusive charmless semileptonic decay, B-0 ->pi(-)center dot(+)nu, undertaken with approximately 227x10(6) BB pairs collected at the Upsilon(4S) resonance with the BABAR detector. The analysis uses events in which the signal B decays are reconstructed with an innovative loose neutrino reconstruction technique. We obtain partial branching fractions in 12 bins of q(2), the momentum transfer squared, from which we extract the f(+)(q(2)) form-factor shape and the total branching fraction B(B-0 ->pi(-)l(+)nu)=(1.46 +/- 0.07(stat)+/- 0.08(syst))x10(-4). Based on a recent unquenched lattice QCD calculation of the form factor in the range q(2)> 16 GeV2, we f…

PhysicsSemileptonic decayParticle physicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationGeneral Physics and AstronomyAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentB mesonNeutrino010306 general physicsDimensionless quantityLeptonPhysical Review Letters
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Magnetic properties of a strongly correlated system on the Bethe lattice

2010

We study the influence of an external magnetic field h on the phase diagram of a system of Fermi particles living on the sites of a Bethe lattice with coordination number z and interacting through on-site U and nearest-neighbor V interactions. This is a physical realization of the extended Hubbard model in the narrow-band limit. Our results establish that the magnetic field may dramatically affect the critical temperature below which a long-range charge ordered phase is observed, as well as the behavior of physical quantities, inducing, for instance, magnetization plateaus in the magnetization curves. Relevant thermodynamic quantities - such as the specific heat and the susceptibility - are…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelBethe latticeCondensed matter physicsFOS: Physical sciencesGeneral Physics and AstronomyCharge (physics)Magnetic fieldCondensed Matter - Strongly Correlated ElectronsMagnetizationPhase (matter)Phase diagramPhysical quantityJournal of Physical Studies
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Self-consistent calculation of the flux-flow conductivity in diffusive superconductors

2017

In the framework of Keldysh-Usadel kinetic theory, we study the temperature dependence of flux-flow conductivity (FFC) in diffusive superconductors. By using self-consistent vortex solutions we find the exact values of dimensionless parameters that determine the diffusion-controlled FFC both in the limit of the low temperatures and close to the critical one. Taking into account the electron-phonon scattering we study the transition between flux-flow regimes controlled either by the diffusion or the inelastic relaxation of non-equilibrium quasiparticles. We demonstrate that the inelastic electron-phonon relaxation leads to the strong suppression of FFC as compared to the previous estimates m…

PhysicsSuperconductivityCondensed matter physicsta114ScatteringCondensed Matter - SuperconductivitysuperconductivityNon-equilibrium thermodynamicsFOS: Physical sciencesconductivit01 natural sciences010305 fluids & plasmasVortexSuperconductivity (cond-mat.supr-con)Condensed Matter::SuperconductivityKeldysh-Usadel kinetic theory0103 physical sciencesQuasiparticleRelaxation (physics)Diffusion (business)010306 general physicsDimensionless quantityPhysical Review B
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To the theory of high-power gyrotrons with uptapered resonators

2010

In high-power gyrotrons it is desirable to combine an optimal resonator length with the optimal value of the resonator quality factor. In resonators with the constant radius of the central part, the possibilities of this combination are limited because the quality factor of the resonator sharply increases with its length. Therefore the attempts to increase the length for maximizing the efficiency leads to such increase in the quality factor which makes the optimal current too small. Resonators with slightly uptapered profiles offer more flexibility in this regard. In such resonators, one can separate optimization of the interaction length from optimization of the quality factor because the …

PhysicsTerahertz radiationbusiness.industryElectromagnetic spectrumRadiusCondensed Matter Physicslaw.inventionPower (physics)ResonatorElectricity generationNuclear magnetic resonanceOpticsQuality (physics)ModulationlawQ factorGyrotronOptoelectronicsPower modulationbusinessDimensionless quantityPhysics of Plasmas
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Beyond the Minimal Standard Model

2011

The GSW theory is a great step forward in our understanding of electroweak interactions because it allows the well-known extremely successful theory of quantized electrodynamics and the theory of the weak CC and NC interactions to be cast into one unified, renormalizable local gauge theory. Renormalizability, in particular, is a very desirable property of the theory because it makes covariant perturbation theory a reasonable and well-defined approximation method for calculating physical quantities beyond the lowest order diagrams. Nevertheless, this model, very likely, is not the corner stone of a final theory of weak and electromagnetic interactions. It contains very many parameters which …

PhysicsTheoretical physicsElectroweak interactionAxial currentCovariant transformationParity (physics)Gauge theoryHeavy neutrinoNeutrinoPhysical quantity
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Connection between the pinch technique and the background field method

1995

The connection between the pinch technique and the background field method is further explored. We show by explicit calculations that the application of the pinch technique in the framework of the background field method gives rise to exactly the same results as in the linear renormalizable gauges. The general method for extending the pinch technique to the case of Green's functions with off-shell fermions as incoming particles is presented. As an example, the one-loop gauge independent quark self-energy is constructed. We briefly discuss the possibility that the gluonic Green's functions, obtained by either method, correspond to physical quantities.

PhysicsWilson loop010308 nuclear & particles physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPropagator01 natural sciencesHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Self-energyQuantum electrodynamics0103 physical sciencesPinchsymbolsFeynman diagram010306 general physicsS-matrixPhysical quantityPhysical Review D
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Transition cancellations of 87Rb and 85Rb atoms in a magnetic field

2020

We have analyzed the magnetic field dependencies of the intensities of all the optical transitions between magnetic sublevels of hyperfine levels, excited with σ + , π , and σ − polarized light, for the D 1 and D 2 lines of 87 R b and 85 R b atoms. Depending on the type of transition and the quantum numbers of the involved levels, the Hamiltonian matrices are of 1 × 1 , 2 × 2 , 3 × 3 , or 4 × 4 dimension. As an example, analytical expressions are presented for the case of 2 × 2 dimension matrices for the D 1 line of both isotopes. Eigenvalues and eigenkets are given, and the expression for the transition intensity as a function of B has been determined. It is found that some π transitions o…

Physics[PHYS]Physics [physics]Statistical and Nonlinear PhysicsQuantum number01 natural sciencesAtomic and Molecular Physics and OpticsMagnetic field010309 opticssymbols.namesakeExcited state0103 physical sciencessymbolsAtomic physicsHamiltonian (quantum mechanics)SpectroscopyHyperfine structureEigenvalues and eigenvectorsComputingMilieux_MISCELLANEOUSPhysical quantity
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