Search results for "Crete"

showing 10 items of 2495 documents

Comment on "Highly nonlinear, sign-varying shift of hydrogen spectral lines in dense plasmas".

2004

The shift of hydrogen and hydrogenlike spectral lines in dense plasmas, calculated with the full computer simulation method, in nonquenching, classical path, dipole approximation for plasma-emitter interaction, is equal to zero. In the paper commented on, Escarguel et al., Phys. Rev. E 62, 2667 (2000) the electron concentrations ${N}_{e}$ and the corresponding temperature values T are shown to have been determined incorrectly.

PhysicsNonlinear systemHydrogenchemistrychemistry.chemical_elementPhysics::Atomic PhysicsElectronPlasmaDiscrete dipole approximationAtomic physicsHydrogen spectral seriesSpectral lineSign (mathematics)Physical review. E, Statistical, nonlinear, and soft matter physics
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Polarizability effects in electronic and muonic atoms

1983

TheS state polarizability shifts are derived from the virtual forward Compton scattering in the unretarded dipole approximation. In the non-relativistic limit ω N /2m≪1, the shift is proportional to the photonuclear sum rule σ−3/2, while in the relativistic limit ω N /2m≫1 it is proportional to a logarithmically weighted σ−2 sum rule. In both cases, the characteristic momentum transfer is (2mω N )1/2. The non-locality from the intermediate lepton propagation removes the divergence typical of the static limit. Explicit formulas for the shifts are given for both the relativistic and non-relativistic limits.

PhysicsNuclear and High Energy PhysicsMomentum transferCompton scatteringFísicaElementary particleDiscrete dipole approximationPolarizabilityQuantum electrodynamicsQuantum mechanicsSum rule in quantum mechanicsLimit (mathematics)Nuclear PhysicsLeptonZeitschrift f�r Physik A Atoms and Nuclei
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The minimal adjoint-SU (5) x Z(4) GUT model

2013

An extension of the adjoint SU (5) model with a flavour symmetry based on the Z(4) group is investigated. The Z(4) symmetry is introduced with the aim of leading the up-and down-quark mass matrices to the Nearest-Neighbour-Interaction form. As a consequence of the discrete symmetry embedded in the SU (5) gauge group, the charged lepton mass matrix also gets the same form. Within this model, light neutrinos get their masses through type-I, type-III and one-loop radiative seesaw mechanisms, implemented, respectively, via a singlet, a triplet and an octet from the adjoint fermionic 24 fields. It is demonstrated that the neutrino phenomenology forces the introduction of at least three 24 fermio…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsProton decayHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciencesSymmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryGauge group0103 physical sciencesHiggs bosonDiscrete and Finite SymmetriesHigh Energy Physics::ExperimentNeutrino PhysicsGUTNeutrino010306 general physicsLeptonDiscrete symmetry
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Probing CPT in transitions with entangled neutral kaons

2015

In this paper we present a novel CPT symmetry test in the neutral kaon system based, for the first time, on the direct comparison of the probabilities of a transition and its CPT reverse. The required interchange of in ↔ out states for a given process is obtained exploiting the Einstein-Podolsky-Rosen correlations of neutral kaon pairs produced at a ϕ-factory. The observable quantities have been constructed by selecting the two semileptonic decays for flavour tag, the ππ and 3π 0 decays for CP tag and the time orderings of the decay pairs. The interpretation in terms of the standard Weisskopf-Wigner approach to this system, directly connects CPT violation in these observables to the violati…

PhysicsNuclear and High Energy PhysicsParticle physicsCPT symmetryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableQuantum entanglementDiscrete and finite symmetries; Kaon Physics; CP violationMass matrixHigh Energy Physics - PhenomenologyKaon Physicssymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)CP violationsymbolsCP violationDiscrete and finite symmetriesHigh Energy Physics::ExperimentEPR paradoxSensitivity (control systems)Spurious relationshipJournal of High Energy Physics
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Direct test of time reversal symmetry in the entangled neutral kaon system at a phi-factory

2013

We present a novel method to perform a direct T (time reversal) symmetry test in the neutral kaon system, independent of any CP and/or CPT symmetry tests. This is based on the comparison of suitable transition probabilities, where the required interchange of in out states for a given process is obtained exploiting the Einstein-Podolski-Rosen correlations of neutral kaon pairs produced at a phi-factory. In the time distribution between the two decays, we compare a reference transition like the one defined by the time-ordered decays (l(-), pi pi) with the T-conjugated one defined by (3 pi(0), l(+)). With the use of this and other T-conjugated comparisons, the KLOE-2 experiment at DA Phi NE co…

PhysicsNuclear and High Energy PhysicsParticle physicsphi-FactoryTime reversal violationCPT symmetryDiscrete symmetriesTime distributionQuantum entanglementdiscrete symmetries; time reversal violation; neutral kaons; phi-factory; φ-factoryNuclear physicsSymmetry testHigh Energy Physics - PhenomenologyT-symmetryViolació CP (Física nuclear)φ-factoryDirect testFactory (object-oriented programming)CP violationFísica nuclearHigh Energy Physics::ExperimentNeutral kaonsParticle Physics - Phenomenology
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Photon Scattering with the Lorentz Integral Transform Method

2011

The application of the Lorentz integral transform (LIT) method to photon scattering off nuclei is presented in general. As an example, elastic photon scattering off the deuteron in the unretarded dipole approximation is considered using the LIT method. The inversion of the integral transform is discussed in detail paying particular attention to the high-energy contributions in the resonance term. The obtained E1-polarizabilities are compared to results from the literature. The corresponding theoretical cross section is confronted with experimental results confirming, as already known from previous studies, that the E1-contribution is the most important one at lower energies.

PhysicsNuclear and High Energy PhysicsPhotonNuclear TheoryLorentz transformationFOS: Physical sciencesElementary particleDiscrete dipole approximationIntegral transformMassless particleNuclear Theory (nucl-th)symbols.namesakeDipolePolarizabilityQuantum mechanicsQuantum electrodynamicssymbols
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Soliton topology versus discrete symmetry in optical lattices

2005

We address the existence of vortex solitons supported by azimuthally modulated lattices and reveal how the global lattice discrete symmetry has fundamental implications on the possible topological charges of solitons. We set a general ``charge rule'' using group-theory techniques, which holds for all lattices belonging to a given symmetry group. Focusing in the case of Bessel lattices allows us to derive also a overall stability rule for the allowed vortex solitons.

PhysicsOptical communicationsHigh Energy Physics::LatticeFotònicaGeneral Physics and AstronomyFOS: Physical sciencesPattern Formation and Solitons (nlin.PS)Symmetry groupTopologyNonlinear Sciences - Pattern Formation and SolitonsVortexsymbols.namesake:Enginyeria de la telecomunicació::Telecomunicació òptica [Àrees temàtiques de la UPC]PhotonicsLattice (order)Bessel beamsymbolsComunicacions òptiquesSoliton:Enginyeria de la telecomunicació::Telecomunicació òptica::Fotònica [Àrees temàtiques de la UPC]Optical vortexBessel functionDiscrete symmetry
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Introduction: Signals and Transforms

2015

In this chapter we outline some well known facts about periodic signals and transforms, which are needed throughout the book. For details we refer to the classical textbook Oppenheim and Schafer [2].

PhysicsPeriodic functionDiscrete Fourier transform (general)Fast Fourier transformMathematical analysisFinite differenceFourier series
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Electric quantum walks in two dimensions

2015

We study electric quantum walks in two dimensions considering Grover, Alternate, Hadamard, and DFT quantum walks. In the Grover walk the behaviour under an electric field is easy to summarize: when the field direction coincides with the x or y axes, it produces a transient trapping of the probability distribution along the direction of the field, while when it is directed along the diagonals, a perfect 2D trapping is frustrated. The analysis of the alternate walk helps to understand the behaviour of the Grover walk as both walks are partially equivalent; in particular, it helps to understand the role played by the existence of conical intersections in the dispersion relations, as we show th…

PhysicsQuantum PhysicsField (physics)DiagonalFOS: Physical sciences01 natural sciences010305 fluids & plasmasDiscrete Fourier transform (general)Hadamard transformQuantum mechanicsDispersion relationElectric field0103 physical sciencesProbability distributionQuantum walkStatistical physics010306 general physicsQuantum Physics (quant-ph)
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Initial correlations effects on decoherence at zero temperature

2004

We consider a free charged particle interacting with an electromagnetic bath at zero temperature. The dipole approximation is used to treat the bath wavelengths larger than the width of the particle wave packet. The effect of these wavelengths is described then by a linear Hamiltonian whose form is analogous to phenomenological Hamiltonians previously adopted to describe the free particle-bath interaction. We study how the time dependence of decoherence evolution is related with initial particle-bath correlations. We show that decoherence is related to the time dependent dressing of the particle. Moreover because decoherence induced by the T=0 bath is very rapid, we make some considerations…

PhysicsQuantum PhysicsQuantum decoherenceFOS: Physical sciencesGeneral Physics and AstronomyStatistical and Nonlinear PhysicsDiscrete dipole approximationharmonic oscillators.Charged particlesymbols.namesakeWavelengthWave–particle dualityQuantum mechanicsoscillatorsymbolsZero temperatureQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)bathMathematical Physics
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