Search results for "Mathematical physics"

showing 10 items of 2687 documents

Fundamental Principles of Quantum Mechanics

2001

There are two alternative methods of quantizing a system: a) quantization via the Feynman Path Integral (equivalent to Schwinger’s Action Principle); b) canonical quantization.

PhysicsOpen quantum systemmedicine.medical_specialtyCanonical quantizationQuantization (signal processing)Quantum dynamicsStochastic interpretationPath integral formulationQuantum nanosciencemedicinePropagatorMathematical physics
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Two-dimensional quantum scattering by non-isotropic interactions localized on a circle, applications to open billiards

2018

Two-dimensional quantum scattering by isotropic and non-isotropic interactions localized on a circle is considered. The expansion of the interaction on the circle in a Fourier series allows us to express basic objects of scattering theory (resolvent, T operator, differential cross length, cross length, and cross length averaged over all orientations of the incident particle), in terms of operations on matrices. For numerical applications, these matrices are truncated to a given order. If the interaction is isotropic, this general formulation reduces to the usual one, and the resonances in the isotropic cases are studied because they allow us to interpret resonances in some non-isotropic cas…

PhysicsOperator (physics)IsotropyMathematical analysisStatistical and Nonlinear Physics01 natural sciences010305 fluids & plasmas0103 physical sciencesLimit (mathematics)Scattering theoryDynamical billiards010306 general physics[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]QuantumFourier seriesMathematical PhysicsComputingMilieux_MISCELLANEOUSResolvent
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An exact soliton solution for an averaged dispersion-managed fibre system equation

2001

We consider the nonlinear wave propagation in an averaged dispersion-managed (DM) fibre system. We present the explicit Lax pair with a variable spectral parameter and derive the exact soliton solution using the Backlund transformation. A similar study is also carried out for simultaneous propagation of N nonlinear pulses in the averaged DM fibre system.

PhysicsOptical fiberMathematical analysisGeneral Physics and AstronomyStatistical and Nonlinear Physicslaw.inventionNonlinear systemNonlinear Sciences::Exactly Solvable and Integrable SystemsTransformation (function)lawLax pairDispersion managedSolitonReduction (mathematics)Mathematical PhysicsVariable (mathematics)Journal of Physics A: Mathematical and General
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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
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Exact dark soliton solutions for a family ofNcoupled nonlinear Schrödinger equations in optical fiber media

2001

We consider a family of N coupled nonlinear Schr\"odinger equations which govern the simultaneous propagation of N fields in the normal dispersion regime of an optical fiber with various important physical effects. The linear eigenvalue problem associated with the integrable form of all the equations is constructed with the help of the Ablowitz-Kaup-Newell-Segur method. Using the Hirota bilinear method, exact dark soliton solutions are explicitly derived.

PhysicsPartial differential equationMathematical analysisSchrödinger equationNonlinear systemDissipative solitonsymbols.namesakeNonlinear Sciences::Exactly Solvable and Integrable SystemsDispersion (optics)symbolsPeregrine solitonSolitonNonlinear Sciences::Pattern Formation and SolitonsEigenvalues and eigenvectorsMathematical physicsPhysical Review E
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Glueball masses from ratios of path integrals

2011

By generalizing our previous work on the parity symmetry, the partition function of a Yang-Mills theory is decomposed into a sum of path integrals each giving the contribution from multiplets of states with fixed quantum numbers associated to parity, charge conjugation, translations, rotations and central conjugations. Ratios of path integrals and correlation functions can then be computed with a multi-level Monte Carlo integration scheme whose numerical cost, at a fixed statistical precision and at asymptotically large times, increases power-like with the time extent of the lattice. The strategy is implemented for the SU(3) Yang-Mills theory, and a full-fledged computation of the mass and …

PhysicsParticle Physics QCD lattice gauge theoryGlueballHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesParity (physics)Charge (physics)Partition function (mathematics)Quantum numberFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeCorrelation functionQuantum mechanicsPath integral formulationMonte Carlo integrationMathematical physics
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Observation of ψ(3686)→e+e−χcJ and χcJ→e+e−J/ψ

2018

Using 4.479 x 10(8) psi(3686) events collected with the BESIII detector, we search for the decays psi(3686) -> e(+)e(-)chi(cJ) and chi(cJ) -> e(+)e(-)J/psi, where J = 0, 1, 2. The decays psi(3686) -> e(+)e(-)chi(cJ) and chi(cJ) -> e(+)e(-)J/psi are observed for the first time. The measured branching fractions are B(psi(3686) -> e(+)e(-)chi(cJ)) = (11.7 +/- 2.5 +/- 1.0) x 10(-4), (8.6 +/- 0.3 +/- 0.6) x 10(-4), (6.9 +/- 0.5 +/- 0.6) x 10(-4) for J = 0, 1, 2, and B(chi(cJ) -> e(+)e(-)J/psi) = (1.51 +/- 0.30 +/- 0.13)x10(-4), (3.73 +/- 0.09 +/- 0.25)x10(-3), (2.48 +/- 0.08 +/- 0.16)x10(-3) for J = 0, 1, 2, respectively. The ratios of the branching fractions B(psi(3686) -> e(+)e(-)chi(cJ))/B(ps…

PhysicsParticle physics010308 nuclear & particles physicsElectron–positron annihilation0103 physical sciencesAnalytical chemistryGeneral Physics and AstronomyHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary Astrophysics010306 general physics01 natural sciencesMathematical physicsPhysical Review Letters
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Lattice QCD and the timelike pion form factor.

2011

We present a formula that allows one to calculate the pion form factor in the timelike region 2mpi <= sqrt{s} <= 4mpi in lattice QCD. The form factor quantifies the contribution of two-pion states to the vacuum polarization. It must be known very accurately in order to reduce the theoretical uncertainty on the anomalous magnetic moment of the muon. At the same time, the formula constitutes a rare example where, in a restricted kinematic regime, the spectral function of a conserved current can be determined from Euclidean observables without an explicit analytic continuation.

PhysicsParticle physicsAnomalous magnetic dipole momentAnalytic continuationHigh Energy Physics - Lattice (hep-lat)Form factor (quantum field theory)FOS: Physical sciencesGeneral Physics and AstronomyOrder (ring theory)Mathematical Physics (math-ph)Lattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticePionVacuum polarizationConserved currentMathematical PhysicsPhysical review letters
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The MuPix high voltage monolithic active pixel sensor for the Mu3e experiment

2015

Mu3e is a novel experiment searching for charged lepton flavor violation in the rare decay μ → eee. In order to reduce background by up to 16 orders of magnitude, decay vertex position, decay time and particle momenta have to be measured precisely. A pixel tracker based on 50 μm thin high voltage monolithic active pixel sensors (HV-MAPS) in a magnetic field will deliver precise vertex and momentum information. Test beam results like an excellent efficiency of >99.5% and a time resolution of better than 16.6 ns obtained with the MuPix HV-MAPS chip developed for the Mu3e pixel tracker are presented.

PhysicsParticle physicsCMOS sensorElectronic detector readout concepts (solid-state)PixelPhysics::Instrumentation and Detectorsbusiness.industryHigh voltageChipElectronic detector readout concepts (solid-state); Particle tracking detectors (solidstate detectors)Magnetic fieldVertex (geometry)OpticsHigh Energy Physics::Experimentddc:610Electric potentialDetectors and Experimental TechniquesParticle tracking detectors (solidstate detectors)ddc:620businessInstrumentationParticle Physics - ExperimentMathematical PhysicsEngineering & allied operationsLepton
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Leading SU(3)-breaking corrections to the baryon magnetic moments in Chiral Perturbation Theory

2008

We calculate the baryon magnetic moments using covariant Chiral Perturbation Theory ($\chi$PT) within the Extended-on-mass-shell (EOMS) renormalization scheme. By fitting the two available low-energy constants (LECs), we improve the Coleman-Glashow description of the data when we include the leading SU(3) breaking effects coming from the lowest-order loops. This success is in dramatic contrast with previous attempts at the same order using Heavy Baryon (HB) $\chi$PT and covariant Infrared (IR) $\chi$PT. We also analyze the source of this improvement with particular attention on the comparison between the covariant results.

PhysicsParticle physicsChiral perturbation theoryMagnetic momentHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesGeneral Physics and AstronomyOrder (ring theory)FísicaRenormalizationBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsCovariant transformationPerturbation theory (quantum mechanics)Symmetry breakingMathematical physics
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