Search results for "singular"

showing 10 items of 589 documents

Electrodynamic Characteristics of a Strip Antenna Located on a Plane Interface of a Resonant Magnetoplasma and an Isotropic Medium

2015

We study the electrodynamic characteristics of an antenna having the form of an infinitesimally thin, perfectly conducting narrow strip located on a plane interface of a resonant magnetoplasma and an isotropic medium. The antenna is perpendicular to an external magnetic field and is excited by a given voltage. Singular integral equations for the antenna current, on the basis of which the current distribution is found in the case of an infinitely long radiator, are obtained. The limits of applicability of an approximate method based on the transmission line theory for determining the current distribution and input impedance of the antenna are established. Within the framework of this method,…

PhysicsNuclear and High Energy PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciPlane (geometry)business.industryIsotropyAstronomy and AstrophysicsStatistical and Nonlinear PhysicsInput impedanceSingular integralresonant magnetoplasmaElectronic Optical and Magnetic MaterialsMagnetic fieldElectrodynamic characteristicElectrodynamic characteristics; metal antennas; resonant magnetoplasmaOpticsTransmission linePerpendicularmetal antennaElectrical and Electronic EngineeringAntenna (radio)businessComputer Science::Information Theory
researchProduct

Regular black hole metrics and the weak energy condition

2014

In this work we construct a family of spherically symmetric, static, charged regular black hole metrics in the context of Einstein-nonlinear electrodynamics theory. The construction of the charged regular black hole metrics is based on three requirements: (a) the weak energy condition should be satisfied, (b) the energy-momentum tensor should have the symmetry $T^{0}_{0}=T^{1}_{1}$, and (c) these metrics have to asymptotically behave as the Reissner-Nordstr\"{o}m black hole metric. In addition, these charged regular black hole metrics depend on two parameters which for specific values yield regular black hole metrics that already exist in the literature. Furthermore, by relaxing the third r…

PhysicsNuclear and High Energy PhysicsWhite holeAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyBlack hole electronBlack holeTheoretical physicsGeneral Relativity and Quantum CosmologyClassical mechanicsde Sitter–Schwarzschild metricNonsingular black hole modelsExtremal black holeBlack braneEnergy conditionPhysics Letters B
researchProduct

Quantum-mechanical model of the Kerr-Newman black hole

2000

We consider a Hamiltonian quantum theory of stationary spacetimes containing a Kerr-Newman black hole. The physical phase space of such spacetimes is just six-dimensional, and it is spanned by the mass $M$, the electric charge $Q$ and angular momentum $J$ of the hole, together with the corresponding canonical momenta. In this six-dimensional phase space we perform a canonical transformation such that the resulting configuration variables describe the dynamical properties of Kerr-Newman black holes in a natural manner. The classical Hamiltonian written in terms of these variables and their conjugate momenta is replaced by the corresponding self-adjoint Hamiltonian operator and an eigenvalue …

PhysicsNuclear and High Energy PhysicsWhite holeFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)FuzzballGeneral Relativity and Quantum CosmologyBlack holeGeneral Relativity and Quantum CosmologyRotating black holeNonsingular black hole modelsQuantum mechanicsExtremal black holeBlack hole thermodynamicsHawking radiation
researchProduct

Bouncing Cosmologies in Palatini $f(R)$ Gravity

2009

7 pages, 4 figures.-- PACS nrs.: 04.50.Kd; 98.80.-k; 98.80.Qc.-- ArXiv pre-print available at: http://arxiv.org/abs/0907.0318

PhysicsNuclear and High Energy Physicsmedia_common.quotation_subjectFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)UniverseCosmologyGeneral Relativity and Quantum CosmologyTheoretical physicsGeneral Relativity and Quantum CosmologyClassical mechanicsQuantum cosmologyGravitational collapsef(R) gravityGravitational singularityBig Bouncemedia_commonLoop quantum cosmology
researchProduct

Triangle amplitude with off-shell CoulombTmatrix for exchange reactions in atomic and nuclear physics

1996

The lowest-order rescattering contribution (triangle amplitude) in three-body models of exchange reactions with charged particles contains the off-shell two-body T matrix describing the intermediate-state Coulomb scattering of charged subsystems. General properties of the exact exchange triangle amplitude, when the incoming and outgoing particles are on the energy shell, are derived. This includes the analytic behavior, i.e., the positions and characters of its leading singularities, in the cos\ensuremath{\vartheta} plane, where \ensuremath{\vartheta} is the scattering angle, in the vicinity of the forward- and backward-scattering directions. Since for computational reasons the Coulomb T ma…

PhysicsNuclear reactionAmplitudeScatteringQuantum mechanicsQuantum electrodynamicsCoulombGravitational singularityElectric potentialThree-body problemAtomic and Molecular Physics and OpticsCharged particlePhysical Review A
researchProduct

Non-existence of dark solitons in a nonlinear Schrödinger-Maxwell-Bloch fibre system

2000

We consider the coupled system of nonlinear Schrodinger and Maxwell-Bloch (NLS-MB) equations, which govern the nonlinear pulse propagation in erbium doped optical fibres. With the help of the Painleve singularity structure analysis, we prove the non-existence of optical solitons in the NLS-MB fibre system in the normal dispersion regime.

PhysicsOptical fiberbusiness.industryPhysics::OpticsGeneral Physics and Astronomychemistry.chemical_elementStatistical and Nonlinear Physicslaw.inventionErbiumNonlinear systemsymbols.namesakeNonlinear Sciences::Exactly Solvable and Integrable SystemsSingularityOpticschemistrylawNonlinear pulse propagationQuantum mechanicsDispersion (optics)symbolsSolitonbusinessNonlinear Sciences::Pattern Formation and SolitonsMathematical PhysicsSchrödinger's catJournal of Physics A: Mathematical and General
researchProduct

Triangle singularity enhancing isospin violation in $D_s^ + \to {\pi ^ + }{\pi ^0}{f_0}(980)$ and $\overline B _s^0 \to J/\psi {\pi ^0}{f_0}(980)$ de…

2019

We investigate isospin violation in the and reactions, which proceed via a triangle mechanism. We show that the mechanism develops a singularity around the π 0 f 0 (980) or π 0 a0 (980) invariant mass of 1420 MeV where the π 0 f 0 and π 0 a0 decay modes are magnified and also the ratio of π 0 f0 to π 0 a0 production, stressing the role of the triangle singularities as a factor to enhance isospin violation. The measurement of these reactions would bring further information into the role of triangle singularities in isospin violation and the a 0 – f 0 mixing in particular and shed further light into the nature of the low lying scalar mesons.

PhysicsParticle physicsMeson010308 nuclear & particles physicsScalar (mathematics)01 natural sciencesSingularityIsospin0103 physical sciencesGravitational singularityInvariant mass010306 general physicsScalar mesonMixing (physics)EPJ Web of Conferences
researchProduct

Triangle mechanisms in the build up and decay of the N*(1875)

2017

We have studied the $N^*(1875) (3/2^-)$ resonance with a multichannel unitary scheme, considering the $\Delta \pi$ and $\Sigma^* K$, with their interaction extracted from chiral Lagrangians, and then have added two more channels, the $N^*(1535) \pi$ and $N \sigma$, which proceed via triangle diagrams involving the $\Sigma^* K$ and $\Delta \pi$ respectively in the intermediate states. The triangle diagram in the $N^*(1535) \pi$ case develops a singularity at the same energy as the resonance mass. We determine the couplings of the resonance to the different channels and the partial decay widths. We find a very large decay width to $\Sigma^* K$, and also see that, due to interference with othe…

PhysicsParticle physicsNuclear TheoryUnitarity010308 nuclear & particles physicsFOS: Physical sciencesSigma01 natural sciencesResonance (particle physics)Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Singularity0103 physical sciencesMass spectrumIntermediate stateInvariant (mathematics)010306 general physicsEnergy (signal processing)Physical Review C
researchProduct

Calculation of theO(? s 2 ) parity-violating structure functions in $$e^ + e^ - \to q\bar qg$$

1986

We calculate the two nonvanishingO(αs2) parity-violating structure functions that contribute to\(e^ + e^ - \xrightarrow{{\gamma ,Z}}q\bar qg\). We discuss how these can be measured. We work with massless quarks and gluons and use dimensional regularization to regularize ultra-violet and infrared singularities. We carefully discuss how to deal withγ5 in the dimensional regularization scheme when infrared singularities are present.

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeElectron–positron annihilationHigh Energy Physics::PhenomenologyElementary particleParity (physics)Massless particleDimensional regularizationQuark–gluon plasmaHigh Energy Physics::ExperimentGravitational singularityQuantum field theoryEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
researchProduct

Study of the possible role of triangle singularities in ${B^ - }\, \to {D^{*0}}{\pi ^ - }{\pi ^0}\eta $ and ${B^ - }\, \to {D^{*0}}{\pi ^ - }{\pi ^ +…

2019

Studying the effects of triangle singularities in hadronic processes is of the utmost importance since they can originate peaks that may wrongfully be associated with resonances. In this work, the role of the triangle mechanism in the decays and is explored. Here, the singularity appears when B- decays into , K *0 decays into K + through pion emission, and K - K + fuse together forming either the a 0 (980) or f 0 (980) which then decays into π 0 η or π+ π – , respectively. As a result, the K * K + K - loop generates a peak in the invariant mass of π - a 0 or π - f 0 around 1420 MeV. The branching ratios that come from this peak are and , which are well within the measurable range. Thus, thi…

PhysicsParticle physicsPionSingularity010308 nuclear & particles physicsBranching fraction0103 physical sciencesHadronPiInvariant massGravitational singularity010306 general physics01 natural sciencesEPJ Web of Conferences
researchProduct