Search results for "Hamiltonian"

showing 10 items of 662 documents

CP, T and CPT versus temporal asymmetries for entangled states of the B-system

1999

The observables used in the K-system to characterize T and CPT violation are no longer useful for the Bd-system, since the width difference between the physical states is vanishingly small. We show that only Im(epsilon) and Re(delta) can survive if Delta Gamma=0, and build alternative CP-odd, CPT-odd, T-odd and temporal asymmetries for the (B_CP -> B0, B0bar) transitions. These quantities enable us to test T and CPT invariances of the effective Hamiltonian for the B-system. The method needs the CP eigenstates B_CP, which can be tagged unambiguously to order lambda^3 from the entangled states of a B-factory.

PhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesFísicaObservableHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)Eigenvalues and eigenvectorsParticle Physics - PhenomenologyPhysics Letters B
researchProduct

Indirect CP violation in the B-system

1997

We show that, contrary to the flavour mixing amplitude q/p, both Re(epsilon) and Im(epsilon) are observable quantities, where epsilon is the phase- convention-independent CP mixing. We consider semileptonic B_d decays from a CP tag and build appropriate time-dependent asymmetries to separate out Re(epsilon) and Im(epsilon). "Indirect" CP violation would have in Im(epsilon)/(1+|epsilon|^2) its most prominent manifestation in the B-system, with expected values in the standard model ranging from -0.37 to -0.18. This quantity is controlled by a new observable phase: the relative one between the CP-violating and CP-conserving parts of the effective hamiltonian. For time-integrated rates we point…

PhysicsNuclear and High Energy PhysicsParticle physicsFlavourFOS: Physical sciencesFísicaObservableExpected valueStandard Modelsymbols.namesakeHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)symbolsCP violationHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)Mixing (physics)Particle Physics - Phenomenology
researchProduct

Running soft parameters in SUSY models with multiple U(1) gauge factors

2012

Abstract We generalize the two-loop renormalization group equations for the parameters of the softly broken SUSY gauge theories given in the literature to the most general case when the gauge group contains more than a single Abelian gauge factor. The complete method is illustrated at two-loop within a specific example and compared to some of the previously proposed partial treatments.

PhysicsNuclear and High Energy PhysicsParticle physicsIntroduction to gauge theoryQuantum gauge theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology01 natural sciencesBRST quantizationHigh Energy Physics::TheoryTheoretical physicsHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theory0103 physical sciences010306 general physicsGauge anomalyGauge fixingNuclear Physics B
researchProduct

Systematic study of neutrinoless double beta decay to excited 0+ states

2003

Abstract A systematic study of neutrinoless double beta (0 νββ ) decay to excited 0 + states, described as monopole-vibrational states or as composed of two collective quadrupole-phonon states, has been performed. Both double β − and double β + /EC decays have been analyzed within the framework of the multiple commutator model (MCM) by using a realistic nuclear many-body Hamiltonian and realistic mean-field single-particle bases. It is found that the associated 0 νββ -decay transitions are suppressed relative to the decay to the final ground state both by the available phase space and especially by the smallness of the involved transition matrix elements. For completeness, also the double β…

PhysicsNuclear and High Energy PhysicsParticle physicsMany-body problemNuclear physicssymbols.namesakeMean field theoryDouble beta decayExcited statePhase spacesymbolsRandom phase approximationHamiltonian (quantum mechanics)Ground stateNuclear Physics A
researchProduct

A consistent study of the the low energy baryon spectrum and the nucleon-nucleon interaction within the chiral quark model

1995

By solving the Schr\"{o}dinger equation for the three-quark system in the hyperspherical harmonic approach, we have studied the low energy part of the nucleon and $\Delta$ spectra using a quark-quark interaction which reproduces the nucleon-nucleon phenomenology. The quark-quark hamiltonian considered includes, besides the usual one-gluon exchange, pion and sigma exchanges generated by the chiral symmetry breaking. The baryonic spectrum obtained is reasonable and the resulting wave function gives consistency to the ansatz used in the two baryon system.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuark modelFOS: Physical sciencesFísicaNuclear Theory (nucl-th)Baryonsymbols.namesakePionsymbolsHigh Energy Physics::ExperimentNuclear ExperimentHamiltonian (quantum mechanics)Chiral symmetry breakingNucleonWave functionAnsatzPhysics Letters B
researchProduct

Spin-dependent potentials from lattice QCD

2006

The spin-dependent corrections to the static inter-quark potential are phenomenologically relevant to describing the fine and hyperfine spin splitting of the heavy quarkonium spectra. We investigate these corrections, which are represented as the field strength correlators on the quark-antiquark source, in SU(3) lattice gauge theory. We use the Polyakov loop correlation function as the quark-antiquark source, and by employing the multi-level algorithm, we obtain remarkably clean signals for these corrections up to intermediate distances of around 0.6 fm. Our observation suggests several new features of the corrections.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesField strengthLattice QCDQuarkoniumNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - LatticeHamiltonian lattice gauge theoryHigh Energy Physics - Phenomenology (hep-ph)Lattice gauge theoryQuantum electrodynamicsHyperfine structureLattice model (physics)
researchProduct

Relations between the Hepp-Lieb and the Alli-Sewell Laser Models

2009

In this paper we show that the dissipative version of the laser model proposed by Alli and Sewell can be obtained by considering the stochastic limit of the (open system) hamiltonian introduced by Hepp and Lieb in their seminal work. We also prove that the Dicke-Haken-Lax hamiltonian produces, after the stochastic limit is considered, the generator of a semigroup with equations of motion very similar to those of Alli-Sewell, and coinciding with these under suitable conditions.

PhysicsNuclear and High Energy PhysicsSemigroupFOS: Physical sciencesEquations of motionStatistical and Nonlinear PhysicsMathematical Physics (math-ph)LaserQuantum mechanicslaw.inventionsymbols.namesakelawsymbolsDissipative systemHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaMathematical PhysicsMathematical physicsAnnales Henri Poincaré
researchProduct

SEMICLASSICAL DESCRIPTION OF SPIN EXCITATIONS OF THE PARTICLE-CORE INTERACTION SYSTEM

1993

A model Hamiltonian describing a nucleon moving in a shifted oscillator well and inter-acting with a harmonic core through a quadrupole-quadrupole term is semiclassically treated. The solutions of the linearised equations of motion are quantised by the Bohr-Sommerfeld procedure. Among the four RPA modes, there is one which corresponds to the harmonic vibration of the spin degree of freedom. This mode is analogous to the spin wave mode describing a system of interacting spins placed in a magnetic field. The state describes a harmonic wobbling motion around a stationary state belonging to the ground rotational band.

PhysicsNuclear and High Energy PhysicsSpinsNuclear TheoryComplex harmonic motionGeneral Physics and AstronomySemiclassical physicsEquations of motionsymbols.namesakeSpin waveQuantum mechanicssymbolsNucleonHamiltonian (quantum mechanics)Stationary stateInternational Journal of Modern Physics E
researchProduct

On the hamiltonian approach to commutator anomalies in (3+1) dimensions

1990

Abstract The quantization of Weyl fermions in the presence of an external nonabelian vector potential is discussed in the case of spacetime dimension (3+1). The hamiltonian approach is used, in the temporal gauge A 0 = 0. In particular, it is explicitly shown how one can lift the action of (an extension of) the group of gauge transformations to the bundle of Fock spaces parametrized by smooth vector potentials.

PhysicsNuclear and High Energy PhysicsWeyl groupSpacetimeHigh Energy Physics::LatticeBRST quantizationFock spacesymbols.namesakeHamiltonian lattice gauge theoryQuantum mechanicsLie algebrasymbolsHamiltonian (quantum mechanics)Mathematical physicsVector potentialPhysics Letters B
researchProduct

Determination of the ΔS=1 weak Hamiltonian of the SU(4) chiral limit through topological zero-mode wave functions

2008

38 pages, 9 figures.-- Published in: JHEP05(2008)043, available at: http://dx.doi.org/10.1088/1126-6708/2008/05/043 (open-acess).

PhysicsNuclear and High Energy PhysicsZero modeChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaObservableLattice QCDTopologyweak decaysCharm quarkPseudoscalarsymbols.namesakeHigh Energy Physics - Phenomenologylattice QCDHigh Energy Physics - Latticekaon physicssymbolsHamiltonian (quantum mechanics)Wave function
researchProduct