Search results for "electrodynamics"

showing 10 items of 820 documents

Analyse statistique de la phase des solitons optiques

2005

On analyse numeriquement la statistique de la phase des solitons optiques et on arrive a determiner la fonction de densite de probabilite. Nos resultats sont en accord avec les theories existantes, qui sont basees sur les proprietes des solitons.

Physicsoptical fibersnonlinear opticsoptical fibers; nonlinear optics; optical solitons; Kerr effectGeneral Physics and AstronomyNonlinear optics01 natural sciences010305 fluids & plasmasPulse propagationoptical solitonsKerr effectQuantum electrodynamics0103 physical sciences010306 general physics
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Small-$x$ Physics in the Dipole Picture at NLO Accuracy

2018

International audience; We review recent progress in NLO calculations for dilute-dense processes in the CGC picture. In particular, we focus here on recent steps in understanding high energy renormalization group evolution (BK/JIMWLK), the total DIS cross section at small x and forward particle production in proton-nucleus collisions at next-to-leading order.

Physicssmall-xenergy: highhigher-order: 1hiukkasfysiikkaBalitsky-Kovchegov equationDipoleforward productionQuantum electrodynamicsdeep inelastic scattering[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]color glass condensatesirontarenormalization groupNuclear Experimentp nucleus: scatteringtalkdipole
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Experimental Setup with Chaotic and Periodic Excitations for Cell Growth Studies

2020

The paper presents circuits used for excitation living cells to increase their growth rate. The main novelty is the proposal of using chaotic oscillations for the electromagnetic excitation. The research is in a preliminary phase and no conclusions have been yet derived for applications in biotechnology.

Physicsstimulace buněčného růstuchaotic generators020208 electrical & electronic engineering010401 analytical chemistryPhase (waves)ChaoticNovelty02 engineering and technologybiotechnologie01 natural sciences0104 chemical sciencesharmonic oscillatorscell growth stimulationQuantum electrodynamics0202 electrical engineering electronic engineering information engineeringchaotické generátoryGrowth rateharmonické oscilátoryExcitationChaotic oscillationsHarmonic oscillatorElectronic circuitbiotechnology
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Path Integral Formulation of Quantum Electrodynamics

2020

Let us consider a pure Abelian gauge theory given by the Lagrangian $$\displaystyle\begin{array}{rcl} \mathcal{L}_{\text{photon}}& =& -\frac{1} {4}F_{\mu \nu }F^{\mu \nu } \\ & =& -\frac{1} {4}\left (\partial _{\mu }A_{\nu } - \partial _{\nu }A_{\mu }\right )\left (\partial ^{\mu }A^{\nu } - \partial ^{\nu }A^{\mu }\right ){}\end{array}$$ (36.1) or, after integration by parts, $$\displaystyle\begin{array}{rcl} \mathcal{L}_{\text{photon}}& =& -\frac{1} {2}\left [-\left (\partial _{\mu }\partial ^{\mu }A_{\nu }\right )A^{\nu } + \left (\partial ^{\mu }\partial ^{\nu }A_{\mu }\right )A_{\nu }\right ] \\ & =& \frac{1} {2}A_{\mu }\left [g^{\mu \nu }\square - \partial ^{\mu }\partial ^{\nu }\righ…

Physicssymbols.namesakeQuantum electrodynamicsPath integral formulationZero (complex analysis)symbolsInverseAbelian groupLagrangian
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Rotational Three-Body Resonances: A New Adiabatic Approach

2001

In the standard adiabatic approach the motion of the fast, light particle (electron) is treated so as to produce an effective potential that governs the motion of the heavy particles (nuclei). The rotational degrees of freedom are then taken into account by adding the centrifugal J(J + 1)-term to the channel potentials and introducing rotational (Coriolis) couplings into conventional close-coupling calculations. Of course, a perturbative treatment of the rotational motion is justified only provided the rotational energy is sufficiently small. If, however, the rotation is as energetic as the motion of the fast particle, both motions should be treated on the same footing in order to produce s…

Physicssymbols.namesakeTotal angular momentum quantum numberQuantum electrodynamicsRotation around a fixed axissymbolsElectronRotational partition functionMagnetic quantum numberAdiabatic processSchrödinger equationRotational energy
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Multidimensional Skyrme-density-functional Study of the Spontaneous Fission of 238U

2015

We determined the spontaneous fission lifetime of 238U by a minimization of the action integral in a three-dimensional space of collective variables. Apart from the mass-distribution multipole moments Q20 (elongation) and Q30 (left–right asymmetry), we also considered the pairing- fluctuation parameter λ2 as a collective coordinate. The collective potential was obtained self-consistently using the Skyrme energy density functional SkM∗ . The inertia tensor was obtained within the nonperturbative cranking approximation to the adiabatic time-dependent Hartree–Fock– Bogoliubov approach. The pairing-fluctuation parameter λ2 allowed us to control the pairing gap along the fission path, which sign…

Physicsta114Fissionmedia_common.quotation_subjectNuclear TheoryGeneral Physics and AstronomyMoment of inertiaAsymmetryAction (physics)uraniumuraanispontaneous fissionQuantum electrodynamicsPairingStatistical physicsMultipole expansionAdiabatic processSpontaneous fissionmedia_commonActa Physica Polonica B
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Mean-Field Calculation Based on Proton-Neutron Mixed Energy Density Functionals

2015

We have performed calculations based on the Skyrme energy density functional (EDF) that includes arbitrary mixing between protons and neutrons. In this framework, single-particle states are generalized as mixtures of proton and neutron components. The model assumes that the Skyrme EDF is invariant under the rotation in isospin space and the Coulomb force is the only source of the isospin symmetry breaking. To control the isospin of the system, we employ the isocranking method, which is analogous to the standard cranking approach used for describing high-spin states. Here, we present results of the isocranking calculations performed for the isobaric analog states in A = 40 and A = 54 nuclei.

Physicsta114Proton010308 nuclear & particles physicsNuclear TheoryInvariant (physics)01 natural sciencesenergy density functionalsCoulomb's lawNuclear physicssymbols.namesakeMean field theoryproton-neutron mixingisobaric analog statesQuantum electrodynamicsIsospin0103 physical sciencessymbolsIsobaric processNeutronSymmetry breakingNuclear Experiment010306 general physicsProceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014)
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Detuning-induced robustness of a three-state Landau-Zener model against dissipation

2019

A three-state system subjected to a time-dependent Hamiltonian whose bare energies undergo one or more crossings, depending on the relevant parameters, is considered, also taking into account the role of dissipation in the adiabatic following of the Hamiltonian eigenstates. Depending on the fact that the bare energies are equidistant or not, the relevant population transfer turns out to be very sensitive to the environmental interaction or relatively robust. The physical mechanisms on the basis of this behavior are discussed in detail.

Physicstime-dependent hamiltonianQuantum Physicsquantum noiseFOS: Physical sciencesDissipation01 natural sciencesSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasLandau-Zenersymbols.namesakeQuantum electrodynamics0103 physical sciencessymbolsEquidistantStandard linear solid modelQuantum Physics (quant-ph)010306 general physicsAdiabatic processHamiltonian (quantum mechanics)Eigenvalues and eigenvectorsPhysical Review A
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Particle in Harmonic E-Field E ( t ) = E sin ω 0 t $$E(t)= E \sin \omega _0 t$$ ; Schwinger–Fock Proper-Time Method

2020

Since the Green’s function of a Dirac particle in an external field, which is described by a potential Aμ(x), is given by

Physics::Computational PhysicsPhysicsElectric fieldQuantum electrodynamicsDirac (software)Proper timeParticleHarmonic (mathematics)Function (mathematics)Computer Science::Numerical AnalysisOmegaFock space
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Analytic behavior of the QED polarizability function at finite temperature

2012

We revisit the analytical properties of the static quasi-photon polarizability function for an electron gas at finite temperature, in connection with the existence of Friedel oscillations in the potential created by an impurity. In contrast with the zero temperature case, where the polarizability is an analytical function, except for the two branch cuts which are responsible for Friedel oscillations, at finite temperature the corresponding function is not analytical, in spite of becoming continuous everywhere on the complex plane. This effect produces, as a result, the survival of the oscillatory behavior of the potential. We calculate the potential at large distances, and relate the calcul…

Polarització (Física nuclear)OscillationsFOS: Physical sciencesGeneral Physics and AstronomyPolarizabilityImpurityQuantum mechanicsOscil·lacionsGas d'electronsMathematical PhysicsPhysicsFriedel oscillationsQuantum electrodynamicsPolarization (Nuclear physics)FísicaMathematical Physics (math-ph)Function (mathematics)Electrodinàmica quànticalcsh:QC1-999Connection (mathematics)Electron gasQuantum electrodynamicsFermi gasComplex planelcsh:PhysicsAnalytic function
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