Search results for "Mathematical physics"

showing 10 items of 2687 documents

B-parameters for ΔS=2 supersymmetric operators

1998

We present a calculation of the matrix elements of the most general set of DeltaS=2 dimension-six four-fermion operators. The values of the matrix elements are given in terms of the corresponding B-parameters. Our results can be used in many phenomenological applications, since the operators considered here give important contributions to K^0--K^0bar mixing in several extensions of the Standard Model (supersymmetry, left-right symmetric models, multi-Higgs models etc.). The determination of the matrix elements improves the accuracy of the phenomenological analyses intended to put bounds on basic parameters of the different models, as for example the pattern of the sfermion mass matrices. Th…

DeltaNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesQuenched approximationRenormalizationMatrix (mathematics)Theoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Mixing (physics)Mathematical physicskaon decays lattice supersymmetryPhysicsHigh Energy Physics - Lattice (hep-lat)FísicaSupersymmetryAtomic and Molecular Physics and Opticskaone decays lattice supersymmetryFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)SfermionNon-perturbative
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2019

The in-medium dynamics of heavy particles are governed by transport coefficients. The heavy quark momentum diffusion coefficient, $\ensuremath{\kappa}$, is an object of special interest in the literature, but one which has proven notoriously difficult to estimate, despite the fact that it has been computed by weak-coupling methods at next-to-leading order accuracy, and by lattice simulations of the pure SU(3) gauge theory. Another coefficient, $\ensuremath{\gamma}$, has been recently identified. It can be understood as the dispersive counterpart of $\ensuremath{\kappa}$. Little is known about $\ensuremath{\gamma}$. Both $\ensuremath{\kappa}$ and $\ensuremath{\gamma}$ are, however, of foremo…

Density matrixQuarkPhysics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice QCDQuarkonium01 natural sciencesMomentum diffusionLattice (order)0103 physical sciencesGauge theory010306 general physicsBrownian motionMathematical physicsPhysical Review D
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Entanglement dynamics of two independent cavity-embedded quantum dots

2010

We investigate the dynamical behavior of entanglement in a system made by two solid-state emitters, as two quantum dots, embedded in two separated micro-cavities. In these solid-state systems, in addition to the coupling with the cavity mode, the emitter is coupled to a continuum of leaky modes providing additional losses and it is also subject to a phonon-induced pure dephasing mechanism. We model this physical configuration as a multipartite system composed by two independent parts each containing a qubit embedded in a single-mode cavity, exposed to cavity losses, spontaneous emission and pure dephasing. We study the time evolution of entanglement of this multipartite open system finally …

DephasingFOS: Physical sciencesQuantum entanglementOpen system (systems theory)Settore FIS/03 - Fisica Della MateriaOpen quantum systemsAtomic and Molecular PhysicsQuantum mechanicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)Spontaneous emissionMathematical PhysicsPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsTime evolutionCondensed Matter PhysicsAtomic and Molecular Physics and Optics; Mathematical Physics; Condensed Matter PhysicsAtomic and Molecular Physics and OpticsMultipartite68.65.Hb Quantum dots (patterned in quantum wells)Quantum dotQubitPhysics::Accelerator Physicsand OpticsQuantum Physics (quant-ph)68.65.Hb Quantum dots (patterned in quantum wells); Open quantum systems
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On the time function of the Dulac map for families of meromorphic vector fields

2003

Given an analytic family of vector fields in Bbb R2 having a saddle point, we study the asymptotic development of the time function along the union of the two separatrices. We obtain a result (depending uniformly on the parameters) which we apply to investigate the bifurcation of critical periods of quadratic centres.

Differential equationApplied MathematicsMathematical analysisGeneral Physics and AstronomyStatistical and Nonlinear PhysicsQuadratic equationSaddle pointtime-map; quadratic centresDevelopment (differential geometry)Vector fieldAsymptotic expansionMathematical PhysicsBifurcationMathematicsMeromorphic functionNonlinearity
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An abstract doubly nonlinear equation with a measure as initial value

2007

Abstract The solvability of the abstract implicit nonlinear nonautonomous differential equation ( A ( t ) u ( t ) ) ′ + B ( t ) u ( t ) + C ( t ) u ( t ) ∋ f ( t ) will be investigated in the case of a measure as an initial value. It will be shown that this problem has a solution if the inner product of A ( t ) x and B ( t ) x + C ( t ) x is bounded below.

Differential equationApplied MathematicsMathematical analysisMonotonic functionNonlinear evolution equationMeasure (mathematics)Nonlinear systemMaximal monotone operatorProduct (mathematics)Bounded functionEvolution equationInitial value problemAnalysisMathematical physicsMathematicsJournal of Mathematical Analysis and Applications
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On critical behaviour in generalized Kadomtsev-Petviashvili equations

2016

International audience; An asymptotic description of the formation of dispersive shock waves in solutions to the generalized Kadomtsev–Petviashvili (KP) equation is conjectured. The asymptotic description based on a multiscales expansion is given in terms of a special solution to an ordinary differential equation of the Painlevé I hierarchy. Several examples are discussed numerically to provide strong evidence for the validity of the conjecture. The numerical study of the long time behaviour of these examples indicates persistence of dispersive shock waves in solutions to the (subcritical) KP equations, while in the supercritical KP equations a blow-up occurs after the formation of the disp…

Differential equationsShock waveSpecial solutionBlow-upKadomtsev–Petviashvili equations[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]Mathematics::Analysis of PDEsFOS: Physical sciencesPainlevé equationsKadomtsev-Petviashvili equationsKadomtsev–Petviashvili equation01 natural sciences010305 fluids & plasmasShock wavesDispersive partial differential equationMathematics - Analysis of PDEs0103 physical sciencesFOS: MathematicsCritical behaviourLong-time behaviourSupercriticalDispersion (waves)0101 mathematicsKP equationSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsMathematical physicsKadomtsev-Petviashvili equationPainleve equationsConjectureNonlinear Sciences - Exactly Solvable and Integrable Systems010102 general mathematicsMathematical analysisDispersive shocks Kadomtsev–Petviashvili equations Painlevé equations Differential equations Dispersion (waves) Ordinary differential equations Shock waves Blow-up Critical behaviour Dispersive shocks Kadomtsev-Petviashvili equation KP equation Long-time behaviour Special solutions Supercritical Partial differential equationsStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Condensed Matter PhysicsDispersive shocksPartial differential equationsNonlinear Sciences::Exactly Solvable and Integrable SystemsOrdinary differential equationSpecial solutions[ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]Exactly Solvable and Integrable Systems (nlin.SI)Ordinary differential equationsAnalysis of PDEs (math.AP)
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Character Tables and Sylow Subgroups Revisited

2018

Suppose that G is a finite group. A classical and difficult problem is to determine how much the character table knows about the local structure of G and vice versa.

Difficult problemPure mathematicsFinite group010102 general mathematicsSylow theorems01 natural sciencesLocal structureConjugacy classCharacter table0103 physical sciences010307 mathematical physics0101 mathematicsVersaMathematics
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Analytical solution for multisingular vortex Gaussian beams: The mathematical theory of scattering modes

2016

We present a novel procedure to solve the Schr\"odinger equation, which in optics is the paraxial wave equation, with an initial multisingular vortex Gaussian beam. This initial condition has a number of singularities in a plane transversal to propagation embedded in a Gaussian beam. We use the scattering modes, which are solutions of the paraxial wave equation that can be combined straightforwardly to express the initial condition and therefore permit to solve the problem. To construct the scattering modes one needs to obtain a particular set of polynomials, which play an analogous role than Laguerre polynomials for Laguerre-Gaussian modes. We demonstrate here the recurrence relations need…

DiffractionGaussianFOS: Physical sciences01 natural sciencesSchrödinger equation010309 opticssymbols.namesakeOptics0103 physical sciencesInitial value problem010306 general physicsMathematical PhysicsPhysicsQuantum Physicsbusiness.industryMathematical analysisMathematical Physics (math-ph)Atomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsVortexQuantum Gases (cond-mat.quant-gas)symbolsLaguerre polynomialsCondensed Matter - Quantum GasesbusinessQuantum Physics (quant-ph)Fresnel diffractionPhysics - OpticsGaussian beamOptics (physics.optics)
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Electric and dielectric properties of nanostructured stoichiometric and excess-iron Ni–Zn ferrites

2013

In this paper, we report a study of the effect of excess iron on structural, microstructural, electric and dielectric properties of the nanostructured Ni–Zn ferrites Ni1−xZnxFe2+zO4−δ of different compositions with x = 0, 0.3, 0.5, 0.7, 1 and z = 0, 0.1. The structural and microstructural properties are estimated from x-ray diffraction and atomic force microscopy (AFM) data. The average grain size, evaluated from AFM topographical analysis, is found to be below 70 nm. The samples exhibit low values of dielectric constant and dielectric loss and a high resistivity. Contrary to earlier conclusions regarding microstructured Ni–Zn ferrites, in nanostructured Ni–Zn ferrites sintered at relativel…

DiffractionMaterials scienceElectrical resistivity and conductivityAtomic force microscopyAnalytical chemistryDissipation factorDielectric lossDielectricCondensed Matter PhysicsMathematical PhysicsAtomic and Molecular Physics and OpticsStoichiometryGrain sizePhysica Scripta
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Atomistic simulations of the FeK-edge EXAFS in FeF3using molecular dynamics and reverse Monte Carlo methods

2016

Atomistic simulations of the experimental Fe K-edge extended x-ray absorption fine structure (EXAFS) of rhombohedral (space group ) FeF3 at T = 300 K were performed using classical molecular dynamics and reverse Monte Carlo (RMC) methods. The use of two complementary theoretical approaches allowed us to account accurately for thermal disorder effects in EXAFS and to validate the developed force-field model, which was constructed as a sum of two-body Buckingham-type (Fe–F and F–F), three-body harmonic (Fe–F–Fe) and Coulomb potentials. We found that the shape of the Fe K-edge EXAFS spectrum of FeF3 is a more sensitive probe for the determination of potential parameters than the values of stru…

DiffractionMaterials scienceExtended X-ray absorption fine structureAb initio02 engineering and technologyReverse Monte Carlo010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesAtomic and Molecular Physics and OpticsSpectral lineEffective nuclear charge0104 chemical sciencesCondensed Matter::Materials ScienceMolecular dynamicsK-edgeAtomic physics0210 nano-technologyMathematical PhysicsPhysica Scripta
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