Search results for "Computer program"

showing 10 items of 807 documents

Use of Prandtl-Ishlinskii hysteresis operators for Coulomb friction modeling with presliding

2017

Prandtl-Ishlinskii stop-type hysteresis operators allow for modeling elasto-plasticity in the relative stress-strain coordinates including the saturation level of the residual constant-tension flow. This lies in direct equivalence to the force-displacement characteristics of nonlinear Coulomb friction, whose constant average value at unidirectional motion depends on the motion sign only, after the transient presliding phase at each motion reversal. In this work, we analyze and demonstrate the use of Prandtl-Ishlinskii operators for modeling the Coulomb friction with presliding phase. No viscous i.e. velocity-dependent component is considered at this stage, and the constant damping rate of t…

Physics0209 industrial biotechnologyHistoryWork (thermodynamics)020208 electrical & electronic engineeringPrandtl number02 engineering and technologyMechanicsFinite element methodPhysics::GeophysicsComputer Science ApplicationsEducationHysteresissymbols.namesakeNonlinear system020901 industrial engineering & automationOperator (computer programming)Classical mechanicsDistribution function0202 electrical engineering electronic engineering information engineeringsymbolsConstant (mathematics)Journal of Physics: Conference Series
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Simultaneously recovering potentials and embedded obstacles for anisotropic fractional Schrödinger operators

2017

Let \begin{document}$A∈{\rm{Sym}}(n× n)$\end{document} be an elliptic 2-tensor. Consider the anisotropic fractional Schrodinger operator \begin{document}$\mathscr{L}_A^s+q$\end{document} , where \begin{document}$\mathscr{L}_A^s: = (-\nabla·(A(x)\nabla))^s$\end{document} , \begin{document}$s∈ (0, 1)$\end{document} and \begin{document}$q∈ L^∞$\end{document} . We are concerned with the simultaneous recovery of \begin{document}$q$\end{document} and possibly embedded soft or hard obstacles inside \begin{document}$q$\end{document} by the exterior Dirichlet-to-Neumann (DtN) map outside a bounded domain \begin{document}$Ω$\end{document} associated with \begin{document}$\mathscr{L}_A^s+q$\end{docume…

PhysicsControl and OptimizationApproximation property02 engineering and technology01 natural sciences010101 applied mathematicsCombinatoricssymbols.namesakeMathematics - Analysis of PDEsOperator (computer programming)Modeling and SimulationBounded functionDomain (ring theory)0202 electrical engineering electronic engineering information engineeringsymbolsDiscrete Mathematics and Combinatorics020201 artificial intelligence & image processingPharmacology (medical)Nabla symbolUniqueness0101 mathematicsAnisotropyAnalysisSchrödinger's catInverse Problems & Imaging
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A non self-adjoint model on a two dimensional noncommutative space with unbound metric

2013

We demonstrate that a non self-adjoint Hamiltonian of harmonic oscillator type defined on a two-dimensional noncommutative space can be diagonalized exactly by making use of pseudo-bosonic operators. The model admits an antilinear symmetry and is of the type studied in the context of PT-symmetric quantum mechanics. Its eigenvalues are computed to be real for the entire range of the coupling constants and the biorthogonal sets of eigenstates for the Hamiltonian and its adjoint are explicitly constructed. We show that despite the fact that these sets are complete and biorthogonal, they involve an unbounded metric operator and therefore do not constitute (Riesz) bases for the Hilbert space $\L…

PhysicsCoupling constantPure mathematicsQuantum PhysicsHilbert spacepseudo-bosoniFOS: Physical sciencesMathematical Physics (math-ph)Noncommutative geometryAtomic and Molecular Physics and Opticssymbols.namesakeOperator (computer programming)Biorthogonal systemQuantum mechanicssymbolsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)QASettore MAT/07 - Fisica MatematicaSelf-adjoint operatorEigenvalues and eigenvectorsMathematical Physics
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Dissipation evidence for the quantum damped harmonic oscillator via pseudo-bosons

2011

It is known that a self-adjoint, time-independent hamiltonian can be defined for the quantum damped harmonic oscillator. We show here that the two vacua naturally associated to this operator, when expressed in terms of pseudo-bosonic lowering and raising operators, appear to be non square-integrable. This fact is interpreted as the evidence of the dissipation effect of the classical oscillator at a purely quantum level.

PhysicsFOS: Physical sciencesQuantum levelStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Dissipationsymbols.namesakeOperator (computer programming)Quantum mechanicssymbolspseudo-bosonsHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaQuantumMathematical PhysicsHarmonic oscillatorBosonTheoretical and Mathematical Physics
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Geometrical foundations of fractional supersymmetry

1997

A deformed $q$-calculus is developed on the basis of an algebraic structure involving graded brackets. A number operator and left and right shift operators are constructed for this algebra, and the whole structure is related to the algebra of a $q$-deformed boson. The limit of this algebra when $q$ is a $n$-th root of unity is also studied in detail. By means of a chain rule expansion, the left and right derivatives are identified with the charge $Q$ and covariant derivative $D$ encountered in ordinary/fractional supersymmetry and this leads to new results for these operators. A generalized Berezin integral and fractional superspace measure arise as a natural part of our formalism. When $q$…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsBerezin integralRoot of unityAlgebraic structureFOS: Physical sciencesAstronomy and AstrophysicsSuperspaceAtomic and Molecular Physics and OpticsCovariant derivativeFractional supersymmetryOperator (computer programming)High Energy Physics - Theory (hep-th)Mathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)nth rootMathematical physics
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Right-handed neutrino magnetic moments

2009

PACS numbers: 14.60.St, 13.15.+g, 13.35.Hb, 13.66.Hk

PhysicsHistoryNuclear and High Energy PhysicsParticle physicsMagnetic momentElectron–positron annihilationElectroweak interactionHigh Energy Physics::PhenomenologyVertex functionFOS: Physical sciencesPartícules (Física nuclear)Computer Science ApplicationsEducationHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)BibliographyCP violationHigh Energy Physics::ExperimentNeutrino
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Sub-Barrier Coulomb Excitation ofSn110and Its Implications for theSn100Shell Closure

2007

The first excited 2(+) state of the unstable isotope Sn-110 has been studied in safe Coulomb excitation at 2.82 MeV/u using the MINIBALL array at the REX-ISOLDE post accelerator at CERN. This is the first measurement of the reduced transition probability of this state using this method for a neutron deficient Sn isotope. The strength of the approach lies in the excellent peak-to-background ratio that is achieved. The extracted reduced transition probability, B(E2 : 0(+) -> 2(+)) 0.220 +/- 0.022e(2) b(2), strengthens the observation of the evolution of the B(E2) values of neutron deficient Sn isotopes that was observed recently in intermediate-energy Coulomb excitation of Sn-108. It implies …

PhysicsMass numberIsotope010308 nuclear & particles physicsShell (structure)Nuclear shell modelGeneral Physics and AstronomyCoulomb excitation7. Clean energy01 natural sciencesClosure (computer programming)Excited state0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsPhysical Review Letters
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Self-referenced phase reconstruction proposal of Ghz bandwidth non-periodical optical pulses by in-fiber semi-differintegration

2011

Abstract We propose two new techniques able to retrieve the phase profile of a given temporal optical pulse based on the use of in-fiber semi-differintegral operators, where by semi-differintegration we mean either a 0.5th-order differentiation or integration. In both cases, the signal's temporal phase can be obtained by simple dividing two temporal intensity profiles, namely the intensities of the input and output pulses of a spectrally shifted semi-differintegral operator. In both cases, we obtained simple analytical expressions for the phase profile. The techniques are self-referenced and well-suited for real-time applications. We numerically prove the viability of these proposals.

PhysicsMode volumePhase reconstructionMulti-mode optical fiberbusiness.industryFiber optics systemsBandwidth (signal processing)Fractional calculusPolarization-maintaining optical fiberLong-period fiber gratingAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsOpticsOperator (computer programming)Fiber Bragg gratingFiber optic sensorFiber Bragg gratingsElectrical and Electronic EngineeringPhysical and Theoretical Chemistrybusiness
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Correlators of left charges and weak operators in finite volume chiral perturbation theory

2002

We compute the two-point correlator between left-handed flavour charges, and the three-point correlator between two left-handed charges and one strangeness violating \Delta I=3/2 weak operator, at next-to-leading order in finite volume SU(3)_L x SU(3)_R chiral perturbation theory, in the so-called epsilon-regime. Matching these results with the corresponding lattice measurements would in principle allow to extract the pion decay constant F, and the effective chiral theory parameter g_27, which determines the \Delta I = 3/2 amplitude of the weak decays K to \pi\pi as well as the kaon mixing parameter B_K in the chiral limit. We repeat the calculations in the replica formulation of quenched c…

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeFlavourHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFísicaParticle Physics - LatticeStrangenessweak decaysOperator (computer programming)AmplitudeHigh Energy Physics - Latticechiral Lagrangianslattice QCDLattice (order)kaon physicsPion decay constantMathematical physics
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Non-perturbative renormalization of lattice operators in coordinate space

2004

We present the first numerical implementation of a non-perturbative renormalization method for lattice operators, based on the study of correlation functions in coordinate space at short Euclidean distance. The method is applied to compute the renormalization constants of bilinear quark operators for the non-perturbative O(a)-improved Wilson action in the quenched approximation. The matching with perturbative schemes, such as MS-bar, is computed at the next-to-leading order in continuum perturbation theory. A feasibility study of this technique with Neuberger fermions is also presented.

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::Latticefield theory gauge theory lattice renormalizationHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesQuenched approximationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIRenormalizationEuclidean distanceHigh Energy Physics - LatticeOperator (computer programming)Quantum mechanicsFunctional renormalization groupPerturbation theory (quantum mechanics)Coordinate spaceNon-perturbativeMathematical physics
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