Search results for "REPRESENTATION"

showing 10 items of 1710 documents

Examples of pseudo-bosons in quantum mechanics

2010

We discuss two physical examples of the so-called {\em pseudo-bosons}, recently introduced in connection with pseudo-hermitian quantum mechanics. In particular, we show that the so-called {\em extended harmonic oscillator} and the {\em Swanson model} satisfy all the assumptions of the pseudo-bosonic framework introduced by the author. We also prove that the biorthogonal bases they produce are not Riesz bases.

PhysicsQuantum PhysicsRiesz representation theoremquantum mechanicsFOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)pseudo-bosonConnection (mathematics)Quantum mechanicsBiorthogonal systemSupersymmetric quantum mechanicsQuantum Physics (quant-ph)Quantum statistical mechanicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsHarmonic oscillatorBosonPhysics Letters A
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Solution of the Lindblad equation in Kraus representation

2006

The so-called Lindblad equation, a typical master equation describing the dissipative quantum dynamics, is shown to be solvable for finite-level systems in a compact form without resort to writing it down as a set of equations among matrix elements. The solution is then naturally given in an operator form, known as the Kraus representation. Following a few simple examples, the general applicability of the method is clarified.

PhysicsQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciLindblad equationFOS: Physical sciencesAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaThe so-called Lindblad equation a typical master equation describing the dissipative quantum dynamics is shown to be solvable for finite-level systems in a compact form without resort to writing it down as a set of equations among matrix elements. The solution is then naturally given in an operator form known as the Kraus representation. Following a few simple examples the general applicability of the method is clarified.Open quantum systemQuantum processMaster equationDissipative systemQuantum operationMethod of quantum characteristicsQuantum Physics (quant-ph)Quantum statistical mechanicsMathematical physics
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Systematic construction of spin liquids on the square lattice from tensor networks with SU(2) symmetry

2016

We elaborate a simple classification scheme of all rank-5 SU(2)-spin rotational symmetric tensors according to i) the on-site physical spin-$S$, (ii) the local Hilbert space $V^{\otimes 4}$ of the four virtual (composite) spins attached to each site and (iii) the irreducible representations of the $C_{4v}$ point group of the square lattice. We apply our scheme to draw a complete list of all SU(2)-symmetric translationally and rotationally-invariant Projected Entangled Pair States (PEPS) with bond dimension $D\leqslant 6$. All known SU(2)-symmetric PEPS on the square lattice are recovered and simple generalizations are provided in some cases. More generally, to each of our symmetry class can…

PhysicsQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)High Energy Physics - Lattice (hep-lat)FOS: Physical sciences01 natural sciencesSquare lattice010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsHigh Energy Physics - LatticeT-symmetryLattice (order)Irreducible representationQuantum mechanics0103 physical sciencesHomogeneous spaceTensor[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]Quantum spin liquidQuantum Physics (quant-ph)010306 general physicsComputingMilieux_MISCELLANEOUSSpecial unitary groupPhysical Review B
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The strong coupling from ALEPH tau decays

2017

The strong coupling from ALEPH tau decays. We use the publically available non-strange spectral function from ALEPH tau decays to critically analyze the different determinations of αs(mτ2) that can be found in the literature and the numerical impact of their possible weaknesses. We also introduce some novel approaches. We find that perturbative uncertainties dominate. Our results with different approaches are very stable. Our final value is αs(mτ2)=0.328±0.013.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsAlephParticle physicsSpectral representation010308 nuclear & particles physics01 natural sciencesStability (probability)0103 physical sciencesStrong couplingHigh Energy Physics::ExperimentSpectral function010306 general physicsNuclear and Particle Physics Proceedings
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Identifying spin and parity of charmonia in flight with lattice QCD

2019

The spectrum of charmonium resonances contains a number of unanticipated states along with several conventional quark-model excitations. The hadrons of different quantum numbers $J^P$ appear in a fairly narrow energy band, where $J^P$ refers to the spin-parity of a hadron at rest. This poses a challenge for Lattice QCD studies of (coupled-channel) meson-meson scattering aimed at the determination of scattering amplitudes and resonance pole positions. A wealth of information for this purpose can be obtained from the lattice spectra in frames with nonzero total momentum. These are particularly dense since hadrons with different $J^P$ contribute to any given lattice irreducible representation.…

PhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)ddc:530High Energy Physics::PhenomenologyQuark modelLattice field theoryFOS: Physical sciencesLattice QCD530 PhysikQuantum number01 natural sciencesGood quantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Irreducible representationHadron spectroscopy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Nonperturbative Determination of the QCD Potential atO(1/m)

2006

The relativistic correction to the QCD static interquark potential at O(1/m) is investigated nonperturbatively for the first time by using lattice Monte Carlo QCD simulations. The correction is found to be comparable with the Coulombic term of the static potential when applied to charmonium, and amounts to one-fourth of the Coulombic term for bottomonium.

PhysicsQuantum chromodynamicsParticle physicsSpectral representationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyMonte Carlo methodLattice field theoryGeneral Physics and AstronomyLattice monte carloQuantum electrodynamicsLattice gauge theoryHigh Energy Physics::ExperimentNuclear theoryPhysical Review Letters
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Noncompact Topological Quantum Groups

1995

A star-product construction of quantum semisimple real Lie groups is performed for the noncompact case.

PhysicsQuantum groupLie groupTopological entropy in physicsSymmetry protected topological orderTheoretical physicsMathematics::Quantum AlgebraInverse scattering problemAstrophysics::Solar and Stellar AstrophysicsMathematics::Differential GeometryMathematics::Representation TheoryQuantumAstrophysics::Galaxy AstrophysicsTopological quantum number
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Quarkonium spectral functions with complex potential

2011

Abstract We study quarkonium spectral functions at high temperatures using a potential model with complex potential. The real part of the potential is constrained by the lattice QCD data on static quark anti-quark correlation functions, while the imaginary part of the potential is taken from perturbative calculations. We find that the imaginary part of the potential has significant effect on quarkonium spectral functions, in particular, it leads to the dissolution of the 1S charmonium and excited bottomonium states at temperatures about 250 MeV and melting of the ground state bottomonium at temperatures slightly above 450 MeV.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsSpectral representationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryLattice QCDQuarkoniumCorrelation function (statistical mechanics)Excited stateHigh Energy Physics::ExperimentGround stateNuclear Physics A
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FITTING LAW FOR THE DENSITY SHIFT OF Q(J) TRANSITIONS OF H2 IN H2–X (X: H2, He, N2) MIXTURES

1998

Abstract A variety of fitting laws have been developed for the purpose of modelling broadening effects in collisional processes, but only a few have been proposed for modelling collision-induced lineshifts in molecules. We analysed accurate stimulated Raman data obtained in several H2–X mixtures (X: H2, He and N2). For the first time, we show that an empirical law provides a very good representation of collisional lineshift coefficients in the range 300–1200 K and for J quantum number up to 9.

PhysicsRange (particle radiation)RadiationLawMoleculeStimulated ramanQuantum numberRepresentation (mathematics)SpectroscopyAtomic and Molecular Physics and OpticsJournal of Quantitative Spectroscopy and Radiative Transfer
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Classical anomalies of supersymmetric extended objects

1991

Abstract The hamiltonian form of the action for a p-extended supersymmetric object is presented, and used to deduce both the algebra generated by the constraints, in agreement with previous results for p=1,2, and the algebra of the supersymmetry charges. The “anomalous” contributions in each algebra (for given p) are shown to be related, and the origin of their different properties is exhibited. In particular, it is shown why only in the charge algebra are the “anomalous” contributions always topological and the commutators of the translations always zero.

PhysicsSymmetric algebraNuclear and High Energy PhysicsConstraint algebraCurrent algebraSupersymmetrySuper-Poincaré algebraTheoretical physicssymbols.namesakeQuantum mechanicssymbolsAlgebra representationComposition algebraHamiltonian (quantum mechanics)Physics Letters B
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