Search results for "Hamiltonian"

showing 10 items of 662 documents

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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Probing the chiral weak Hamiltonian at finite volumes

2006

Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose couplings ("low-energy constants") encode all non-perturbative QCD physics. It has recently been suggested that these low-energy constants could be determined at finite volumes by matching the non-perturbatively measured three-point correlation functions between the weak Hamiltonian and two left-handed flavour currents, to analytic predictions following from chiral perturbation theory. Here we complete the analytic side in two respects: by inspecting how small ("epsilon-regime") and intermediate or large ("p-regime") quark masses connect to each other, and by including in the discussion the two …

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsChiral perturbation theoryHigh Energy Physics - Lattice (hep-lat)FlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableweak decaysPseudoscalarsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Latticelattice QCDkaon physicssymbolschiral lagrangiansHamiltonian (quantum mechanics)Mathematical physics
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Kaon mixing beyond the SM from N-f=2 tmQCD and model independent constraints from the UTA

2013

We present the first unquenched, continuum limit, lattice QCD results for the matrix elements of the operators describing neutral kaon oscillations in extensions of the Standard Model. Owing to the accuracy of our calculation on Delta S = 2 weak Hamiltonian matrix elements, we are able to provide a refined Unitarity Triangle analysis improving the bounds coming from model independent constraints on New Physics. In our non-perturbative computation we use a combination of N-f = 2 maximally twisted sea quarks and Osterwalder-Seiler valence quarks in order to achieve both O(a)-improvement and continuum-like renormalization properties for the relevant four-fermion operators. The calculation of t…

QuarkStrange quarkParticle physicsNuclear and High Energy PhysicsPhysics beyond the Standard ModelComputationHigh Energy Physics::LatticeFOS: Physical sciencesLattice QCD01 natural sciencesRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciences010306 general physicsPhysicsHamiltonian matrixUnitarity010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]Computer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)FísicaLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelBeyond the Standard Model Physics
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Scattering and gluon emission in a color field : a light-front Hamiltonian approach

2021

We develop a numerical method to nonperturbatively study scattering and gluon emission of a quark from a colored target using a light-front Hamiltonian approach. The target is described as a classical color field, as in the color glass condensate effective theory. The Fock space of the scattering system is restricted to the |q⟩+|qg⟩ sectors, but the time evolution of this truncated system is solved exactly. This method allows us to study the interplay between coherence and multiple scattering in gluon emission. It could be applied both to studying subeikonal effects in high-energy scattering and to understanding jet quenching in a hot plasma.

Quarkelectron-ion collisionsNuclear TheoryField (physics)High Energy Physics::LatticeFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesquantum chromodynamicsEffective field theory010306 general physicsquantum field theoryPhysics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyTime evolutionGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicssymbolskvanttiväridynamiikkakvanttikenttäteoriaHamiltonian (quantum mechanics)relativistic heavy-ion collisions
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