Search results for "Ham"

showing 10 items of 2612 documents

Exact Solution of Quantum Optical Models by Algebraic Bethe Ansatz Methods

1996

From long standing interests in solitons and integrable systems, e.g. SIT (1968– 74)1,2, “optical solitons” CQ04 (1977)3, we solve exactly, by algebraic Bettie ansatz (= quantum inverse) methods4, models of importance to quantum optics including the quantum Maxwell-Bloch envelope equations for plane-wave quantum self-induced transparency (SIT) in one space variable (x) and one time (t)2; and in the one tinte (t)5 a family of models surrounding and extending the Tavis-Cummings model6 of N 2-level atoms coupled to one cavity mode for ideal cavity (Q = ∞) QED. Additional Kerr type nonlinearities or Stark shifted levels can he incorporated into the Hamiltonian H of one of the most general model…

Quantum opticsPhysicssymbols.namesakeThirring modelPhotonQuantum mechanicssymbolsGround stateHamiltonian (quantum mechanics)Nonlinear Schrödinger equationAnsatzBethe ansatz
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Incommensurate phases of a bosonic two-leg ladder under a flux

2016

A boson two--leg ladder in the presence of a synthetic magnetic flux is investigated by means of bosonization techniques and Density Matrix Renormalization Group (DMRG). We follow the quantum phase transition from the commensurate Meissner to the incommensurate vortex phase with increasing flux at different fillings. When the applied flux is $\rho \pi$ and close to it, where $\rho$ is the filling per rung, we find a second incommensuration in the vortex state that affects physical observables such as the momentum distribution, the rung-rung correlation function and the spin-spin and charge-charge static structure factors.

Quantum phase transitionBosonizationBosonisation[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]IncommensurationsFOS: Physical sciencesGeneral Physics and Astronomychamps de jauge artificiels01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)Condensed Matter - Strongly Correlated ElectronsCorrelation functionGauge fieldsCondensed Matter::Superconductivity0103 physical sciencesBosonizationtranstion commensurable-incommensurable010306 general physicsCommensurate-Incommensurate transitions[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsartificial gauge fieldsDensity matrix renormalization groupGauge fields; Incommensurations; Meissner to vortex transition; Physics and Astronomy (all)Vortex stateMagnetic fluxVortexQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality.Quantum Gases (cond-mat.quant-gas)Meissner to vortex transitionCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality
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Geometry of quantum phase transitions

2020

In this article we provide a review of geometrical methods employed in the analysis of quantum phase transitions and non-equilibrium dissipative phase transitions. After a pedagogical introduction to geometric phases and geometric information in the characterisation of quantum phase transitions, we describe recent developments of geometrical approaches based on mixed-state generalisation of the Berry-phase, i.e. the Uhlmann geometric phase, for the investigation of non-equilibrium steady-state quantum phase transitions (NESS-QPTs ). Equilibrium phase transitions fall invariably into two markedly non-overlapping categories: classical phase transitions and quantum phase transitions, whereas i…

Quantum phase transitionPhysicsPhase transitionQuantum PhysicsDissipative phase transitions Geometric phase Quantum geometric information Quantum metrology Quantum phase transitionsStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsCritical phenomenaGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesTheoretical physicssymbols.namesakeGeometric phase0103 physical sciencesQuantum metrologyDissipative systemsymbols010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)QuantumCondensed Matter - Statistical Mechanics
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Shortcut to Adiabaticity in the Lipkin-Meshkov-Glick Model

2015

We study transitionless quantum driving in an infinite-range many-body system described by the Lipkin-Meshkov-Glick model. Despite the correlation length being always infinite the closing of the gap at the critical point makes the driving Hamiltonian of increasing complexity also in this case. To this aim we develop a hybrid strategy combining shortcut to adiabaticity and optimal control that allows us to achieve remarkably good performance in suppressing the defect production across the phase transition.

Quantum phase transitionPhysicsPhase transitionQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)General Physics and AstronomyFOS: Physical sciencesNanotechnologyOptimal controlSettore FIS/03 - Fisica Della Materiashortcut to adiabaticity Lipkin-Meshkov-Glick Model many body hamiltoniansymbols.namesakesymbolsStatistical physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)QuantumShortcut to adiabaticity in the Lipkin-Meshkov-Glick modelCondensed Matter - Statistical Mechanics
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Parton distribution functions of heavy mesons on the light front

2019

The parton distribution functions (PDFs) of heavy mesons are evaluated from their light-front wave functions, which are obtained from a basis light-front quantization in the leading Fock sector representation. We consider the mass eigenstates from an effective Hamiltonian consisting of the confining potential adopted from light-front holography in the transverse direction, a longitudinal confinement, and a one-gluon exchange interaction with running coupling. We present the gluon and the sea quark PDFs which we generate dynamically from the QCD evolution of the valence quark distributions.

QuarkParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciencesFock spaceNuclear Theory (nucl-th)Quantization (physics)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessironta010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicskvarkitHigh Energy Physics::PhenomenologyGluonHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentkvanttikenttäteoriaHamiltonian (quantum mechanics)ydinfysiikka
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Ultrarelativistic quark-nucleus scattering in a light-front Hamiltonian approach

2020

We investigate the scattering of a quark on a heavy nucleus at high energies using the time-dependent basis light-front quantization (tBLFQ) formalism, which is the first application of the tBLFQ formalism in QCD. We present the real-time evolution of the quark wave function in a strong classical color field of the relativistic nucleus, described as the color glass condensate. The quark and the nucleus color field are simulated in the QCD SU(3) color space. We calculate the total and the differential cross sections, and the quark distribution in coordinate and color spaces using the tBLFQ approach. We recover the eikonal cross sections in the eikonal limit. We find that the differential cro…

QuarkParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceshiukkasfysiikka01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)Quantization (physics)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessironta010306 general physicsWave functionPhysicsQuantum chromodynamics010308 nuclear & particles physicsEikonal equationkvarkitHigh Energy Physics::PhenomenologyDeep inelastic scatteringHigh Energy Physics - PhenomenologysymbolskvanttikenttäteoriaHamiltonian (quantum mechanics)ydinfysiikkaPhysical Review D
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Spectrum of fully-heavy tetraquarks from a diquark+antidiquark perspective

2019

Using a relativized diquark model Hamiltonian, we calculate the masses of $J^{PC}=0^{++}$ ground-state tetraquarks in the following systems: $b s \bar b \bar s$, $bb \bar n \bar n$ ($n=u, d$), $bb \bar s \bar s$, $cc\bar c \bar c$, $b b \bar b \bar b$, $b c\bar b \bar c$ and $b b \bar c \bar c$. We also compute extensive spectra for the fully-heavy quark flavour combinations. Finally, as a test of the diquark model approach, we compute the masses of fully-heavy baryons in the diquark model. Our results may be compared soon to the forthcoming experimental data for fully-heavy three-quark systems.

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceslcsh:AstrophysicshiukkasfysiikkaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)lcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)Engineering (miscellaneous)Nuclear theoryNuclear ExperimentPhysicstheoretical physicskvarkitHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)DiquarkBaryonHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentHamiltonian (quantum mechanics)European Physical Journal
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New method for determining the quark-gluon vertex

2014

We present a novel nonperturbative approach for calculating the form factors of the quark-gluon vertex, in a general covariant gauge. The key ingredient of this method is the exact all-order relation connecting the conventional quark-gluon vertex with the corresponding vertex of the background field method, which is Abelian-like. When this latter relation is combined with the standard gauge technique, supplemented by a crucial set of transverse Ward identities, it allows the approximate determination of the nonperturbative behavior of all twelve form factors comprising the quark-gluon vertex, for arbitrary values of the momenta. The actual implementation of this procedure is carried out in …

QuarkPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyForm factor (quantum field theory)FOS: Physical sciencesFísicaGauge (firearms)Theoretical physicsLattice (module)High Energy Physics - PhenomenologyHamiltonian lattice gauge theoryHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)Vertex (curve)
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New physics effects in tree-level decays and the precision in the determination of the quark mixing angle γ.

2015

We critically review the assumption that no new physics is acting in tree-level B-meson decays and study the consequences for the ultimate precision in the direct determination of the Cabibbo-Kobayashi-Maskawa (CKM) angle γ. In our exploratory study we find that sizeable universal new physics contributions, ΔC1,2, to the tree-level Wilson coefficients C1,2 of the effective Hamiltonian describing weak decays of the b quark are currently not excluded by experimental data. In particular, we find that ImΔC1 and ImΔC2 can easily be of order ±10% without violating any constraints from data. Such a size of new physics effects in C1 and C2 corresponds to an intrinsic uncertainty in the CKM angle γ …

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyObservableBottom quarksymbols.namesakesymbolsHeavy quark effective theoryHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)
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T-odd and CP-odd triple momentum correlations in the exclusive semi-leptonic bottom meson decay

1990

Abstract We study T-odd triple momentum correlations in exclusive semi-leptonic (S l ) bottom meson decays B → D ∗ (→ D π)+ l +ν l . We define asymmetry ratios that measure these T-odd triple momentum correlation effects. We provide a careful discussion of possible unitarity contributions to the asymmetry ratios. The conclusion is that strong interaction unitarity contributions are small or, in the case of one particular T-odd observable, absent. CP-violating contributions to the asymmetry ratios would have to come from new non-standard sources as there are no standard model contributions. Possible new CP-violating contributions are parametrized in terms of an effective four-fermion hamilto…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMesonUnitaritymedia_common.quotation_subjectHigh Energy Physics::PhenomenologyStrong interactionObservableAsymmetryNuclear physicssymbols.namesakesymbolsHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)media_commonPhysics Letters B
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