Search results for "Hamiltonian"

showing 10 items of 662 documents

A new lattice action for studying topological charge

1996

We propose a new lattice action for non-abelian gauge theories, which will reduce short-range lattice artifacts in the computation of the topological susceptibility. The standard Wilson action is replaced by the Wilson action of a gauge covariant interpolation of the original fields to a finer lattice. If the latter is fine enough, the action of all configurations with non-zero topological charge will satisfy the continuum bound. As a simpler example we consider the $O(3)$ $\sigma$-model in two dimensions, where a numerical analysis of discretized continuum instantons indicates that a finer lattice with half the lattice spacing of the original is enough to satisfy the continuum bound.

InstantonNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice field theoryFOS: Physical sciencesTheoretical physicsLattice constantHigh Energy Physics - LatticeHamiltonian lattice gauge theoryLattice (order)Lattice gauge theoryCovariant transformationGauge theoryScalingTopological quantum numberMathematicsPhysicsQuantum gauge theoryNumerical analysisHigh Energy Physics - Lattice (hep-lat)FísicaLattice QCDMap of latticesAtomic and Molecular Physics and OpticsReciprocal latticeQuantum electrodynamicsLattice model (physics)Nuclear Physics B - Proceedings Supplements
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A family of complex potentials with real spectrum

1999

We consider a two-parameter non-Hermitian quantum mechanical Hamiltonian operator that is invariant under the combined effects of parity and time reversal transformations. Numerical investigation shows that for some values of the potential parameters the Hamiltonian operator supports real eigenvalues and localized eigenfunctions. In contrast with other parity times time reversal symmetric models which require special integration paths in the complex plane, our model is integrable along a line parallel to the real axis.

Integrable systemFOS: Physical sciencesGeneral Physics and AstronomyComplex planeQuantum mechanicsMathematical analysisQuantumsymbols.namesakeHamiltonian (quantum mechanics)EigenfunctionEigenvalues and eigenvectorsEigenvalues and eigenvectorsPhysicsIntegrable systemQuantum PhysicsPhysicsMathematical analysisFísicaStatistical and Nonlinear PhysicsParity (physics)EigenfunctionInvariant (physics)Invariant (physics)Parity (physics)Mathematical physicssymbolsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Complex planeMathematics
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Three-dimensional singletons

1990

The three-dimensional analog of singleton gauge theory turns out to be related to the topological gauge theory of Schwartz and Witten. It is a fully-fledged gauge theory, though it involves only a single scalar field. Real, physical degrees of freedom propagate in 3-space, but they are ‘confined’ in the sense that they cannot be detected locally. The physical Hamiltonian density is not zero, but it is concentrated on the boundary at spatial infinity. This boundary surface, a torus, supports a two-dimensional conformal field theory.

Introduction to gauge theoryHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice field theoryStatistical and Nonlinear PhysicsGeometryMathematical PhysicsGauge anomalyBRST quantizationGauge symmetryMathematicsGauge fixingMathematical physicsLetters in Mathematical Physics
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Searches for B0 decays to combinations of charmless isoscalar mesons

2004

We search for B meson decays into two-body combinations of eta, eta', omega, and phi mesons from 89 million B B-bar pairs collected with the BaBar detector at the PEP-II asymmetric-energy e+e- collider at SLAC. We find the branching fraction BF(B0 -> eta omega) = (4.0^{+1.3}_{-1.2} +- 0.4) x 10^-6 with a significance of 4.3 sigma. For all the other decay modes we set the following 90% confidence level upper limits on the branching fractions, in units of 10^-6 : BF(B0 -> eta eta)<2.8, BF(B0 -> eta eta')<4.6, BF(B0 -> eta' eta')<10, BF(B0 -> eta'omega)<2.8, BF(B0 -> eta phi)<1.0, BF(B0 -> eta' phi)<4.5, BF(B0 -> phi phi)<1.5.

IsoscalarElectron–positron annihilationBABARGeneral Physics and AstronomyQCD FACTORIZATION01 natural sciencesOmega13.25.Hw 11.30.Er 12.15.HhHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Mathematical modelProbability density function[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PEP2B mesonNuclear ExperimentQCD FACTORIZATION; STANDARD MODEL; BABAR; SLACPhysicsQuantum chromodynamicsSigmaHamiltonianMonte Carlo methodSensitivity analysiPARTICLE PHYSICSBranching fractionSLACParticle physicsMesonSTANDARD MODELQCD FACTORIZATION STANDARD MODELFOS: Physical sciencesLikelihood distributionPARTICLE PHYSICS; PEP2; BABARSolenoidHigh energy physicNuclear physicsPhysics and Astronomy (all)ElectromagnetismElectromagnetic calorimeterPseudoscalar meson0103 physical sciencesPerturbation technique010306 general physicsCalorimeterError analysi010308 nuclear & particles physicsBranching fractionHEPMagnetic fieldHigh Energy Physics::Experiment
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High-resolution FTIR spectra analysis of sulfur dioxide isotopologues

2019

In this thesis we considered the spectral properties of the sulfur dioxide. The experimental FTIR spectra of numerous sulfur dioxide isotopologues, 32S16O2, 34S16O2, 32S18O2 and 32S16O18O, were first recorded in the regions of fundamental, «hot», combination and overtone bands. The wide variability of the experimental conditions gave possibility to observe and identify for the first time transitions be¬ longing to the following of ro-vibrational bands: 3v2, 3v2 - v2, 2v2 - v2 bands of 32S16O2; 2v2 - v2 band of 34S16O2; v1 + v2, v2 + v3, v1 + v3, 2v1, 2v3 bands of 32S18O2; v1, v3, 2v1, v1 + v3, 2v3 bands of 32S16O18O. The inverse spectroscopic problems were solved for the studied states with…

IsotopologuesConstantes spectroscopiquesSpectres rovibrationnelsPotentiel intramoléculaireDioxyde de soufre[PHYS.PHYS]Physics [physics]/Physics [physics]Effective HamiltonianIntramolec¬ular potentialSotopologuesSpectroscopic constantsRo-Vibrational spectraSulfur dioxideHamiltonien effectif[PHYS.PHYS] Physics [physics]/Physics [physics]
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Cavity-aided quantum parameter estimation in a bosonic double-well Josephson junction

2014

We describe an apparatus designed to make non-demolition measurements on a Bose-Einstein condensate (BEC) trapped in a double-well optical cavity. This apparatus contains, as well as the bosonic gas and the trap, an optical cavity. We show how the interaction between the light and the atoms, under appropriate conditions, can allow for a weakly disturbing yet highly precise measurement of the population imbalance between the two wells and its variance. We show that the setting is well suited for the implementation of quantum-limited estimation strategies for the inference of the key parameters defining the evolution of the atomic system and based on measurements performed on the cavity field…

Josephson effectDe factoAtomic systemPopulationFOS: Physical sciences-01 natural sciencesSettore FIS/03 - Fisica Della Materia010305 fluids & plasmaslaw.inventionsymbols.namesakequant-phlawQuantum mechanics0103 physical sciences:Science::Physics::Atomic physics::Quantum theory [DRNTU]010306 general physicseducationQuantumCondensed Matter::Quantum GasesPhysicsQuantum Physicseducation.field_of_studyCondensed Matter::OtherEstimation theoryAtomic and Molecular Physics and OpticsQuantum Gases (cond-mat.quant-gas)Optical cavitysymbolsCondensed Matter - Quantum GasesQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)cond-mat.quant-gasPhysical Review A
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Approximate renormalization-group transformation for Hamiltonian systems with three degrees of freedom

1999

We construct an approximate renormalization transformation that combines Kolmogorov-Arnold-Moser (KAM)and renormalization-group techniques, to analyze instabilities in Hamiltonian systems with three degrees of freedom. This scheme is implemented both for isoenergetically nondegenerate and for degenerate Hamiltonians. For the spiral mean frequency vector, we find numerically that the iterations of the transformation on nondegenerate Hamiltonians tend to degenerate ones on the critical surface. As a consequence, isoenergetically degenerate and nondegenerate Hamiltonians belong to the same universality class, and thus the corresponding critical invariant tori have the same type of scaling prop…

KAM TORI; RENORMALIZATION GROUP; STRANGE ATTRACTORSDegenerate energy levelsFOS: Physical sciencesKAM TORIRenormalization groupNonlinear Sciences - Chaotic DynamicsStrange nonchaotic attractorSTRANGE ATTRACTORSHamiltonian systemNonlinear Sciences::Chaotic DynamicsRenormalizationTransformation (function)RENORMALIZATION GROUPQuantum mechanicsChaotic Dynamics (nlin.CD)Invariant (mathematics)Settore MAT/07 - Fisica MatematicaMathematics::Symplectic GeometryScalingMathematicsMathematical physicsPhysical Review E
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Invariant rotational curves in Sitnikov's Problem

1993

The Sitnikov's Problem is a Restricted Three-Body Problem of Celestial Mechanics depending on a parameter, the eccentricity,e. The Hamiltonian,H(z, v, t, e), does not depend ont ife=0 and we have an integrable system; ife is small the KAM Theory proves the existence of invariant rotational curves, IRC. For larger eccentricities, we show that there exist two complementary sequences of intervals of values ofe that accumulate to the maximum admissible value of the eccentricity, 1, and such that, for one of the sequences IRC around a fixed point persist. Moreover, they shrink to the planez=0 ase tends to 1.

Kolmogorov–Arnold–Moser theoremApplied MathematicsMathematical analysisKepler's laws of planetary motionAstronomy and AstrophysicsGeometryInvariant (physics)Fixed pointThree-body problemSitnikov problemCelestial mechanicsComputational Mathematicssymbols.namesakeSpace and Planetary ScienceModeling and SimulationsymbolsAstrophysics::Earth and Planetary AstrophysicsHamiltonian (quantum mechanics)Mathematical PhysicsMathematicsCelestial Mechanics & Dynamical Astronomy
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Spin dynamics in the single-ion magnet [Er(W5O18)2]9−

2018

In this work we present a detailed NMR and ${\ensuremath{\mu}}^{+}\mathrm{SR}$ investigation of the spin dynamics in the new hydrated sodium salt containing the single-ion magnet ${[\mathrm{Er}{({\mathrm{W}}_{5}{\mathrm{O}}_{18})}_{2}]}^{9\ensuremath{-}}$. The $^{1}\mathrm{H}\phantom{\rule{0.16em}{0ex}}\mathrm{NMR}$ absorption spectra at various applied magnetic fields present a line broadening on decreasing temperature which indicates a progressive spin freezing of the single-molecule magnetic moments. The onset of quasistatic local magnetic fields, due to spin freezing, is observed also in the muon relaxation curves at low temperature. Both techniques yield a local field distribution of t…

Larmor precessionPhysicsMuonMagnetic momentMagnetism02 engineering and technologyMuon spin spectroscopy021001 nanoscience & nanotechnology01 natural sciencesDipolesymbols.namesake0103 physical sciencessymbolsAtomic physics010306 general physics0210 nano-technologyHamiltonian (quantum mechanics)Local fieldPhysical Review B
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Role of Orbital Degeneracy in the Single Molecule Magnet Behavior of a Mononuclear High-Spin Fe(II) Complex

2010

To explain the single-molecule magnet behavior of the mononuclear complex [(tpaMes)Fe](-) we have developed a model that takes into account the trigonal ligand field splitting of the atomic (5)D term of the Fe(II) ion, and the spin-orbital splitting and mixing of the ligand field terms. The ground ligand field term is shown to be the orbital doublet (5)E possessing an unquenched orbital angular momentum. We demonstrate that the splitting of this term cannot be described by the conventional zero-field splitting Hamiltonian proving thus the irrelevance of the spin-Hamiltonian formalism in the present case. The first-order orbital angular momentum is shown to lead to the strong magnetic anisot…

Ligand field theoryAngular momentumCondensed matter physicsChemistryIonInorganic ChemistryMagnetizationsymbols.namesakeMagnetic anisotropyMagnetsymbolsSingle-molecule magnetPhysical and Theoretical ChemistryHamiltonian (quantum mechanics)Inorganic Chemistry
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