Search results for "Bethe"

showing 10 items of 82 documents

Gluon mass generation in the massless bound-state formalism

2013

We present a detailed, all-order study of gluon mass generation within the massless bound-state formalism, which constitutes the general framework for the systematic implementation of the Schwinger mechanism in non-Abelian gauge theories. The main ingredient of this formalism is the dynamical formation of bound states with vanishing mass, which give rise to effective vertices containing massless poles; these latter vertices, in turn, trigger the Schwinger mechanism, and allow for the gauge-invariant generation of an effective gluon mass. This particular approach has the conceptual advantage of relating the gluon mass directly to quantities that are intrinsic to the bound-state formation its…

Nuclear and High Energy PhysicsRenormalizationBethe–Salpeter equationHigh Energy Physics::LatticeBackground field methodFOS: Physical sciencesPinch techniqueRenormalizationTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeGauge symmetriesQuantum mechanicsGauge theory3-gluon vertexPhysicsBackground field methodDynamical symmetry breakingGlueballsPhysicsHigh Energy Physics - Lattice (hep-lat)Mass generationInvarianceHigh Energy Physics::PhenomenologyPropagatorQCDGluonMassless particleHigh Energy Physics - PhenomenologyFísica nuclear
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Exotic states in the S=1 N-pi-K system and low-lying 1/2+ S=-1 resonances

2010

In this manuscript we discuss about our study of the $N \pi \bar{K}$ and the NπK systems made by solving the Faddeev equations with the two-body t-matrices obtained by solving the Bethe-Salpeter equations with the potentials obtained from chiral dynamics. In the strangeness = -1 case, we found that all the Λ and Σ resonances listed by the particle data group, with spin-parity 1/2+ , in the 1550-1800 MeV region get generated due to the involved three-body dynamics. This motivated us to study the strangeness =1 three-body system, i.e., NπK , where we did not find any evidence for the Θ + (1542) but found a broad bump around 1700 MeV which has a κ (800)N structure.

Nuclear physicsPhysicsFaddeev equationsParticle physicsBethe–Salpeter equationPhysicsQC1-999Structure (category theory)Particle Data GroupStrangenessThree-body problemBar (unit)S-matrixEPJ Web of Conferences
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Thermodynamics of Toda lattice models: application to DNA

1993

Abstract Our generalised Bethe ansatz method is used to formulate the statistical mechanics of the classical Toda lattice in terms of a set of coupled integral equations expressed in terms of appropriate action-angle variables. The phase space as coordinatised by these action-angle variables is constrained; and both the soliton number density and the soliton contribution to the free energy density can be shown to decouple from the phonon degrees of freedom and to depend only on soliton-soliton interactions. This makes it possible to evaluate the temperature dependence of the soliton number density which, to leading order, is found to be proportional to T 1 3 .

Number densityDegrees of freedom (physics and chemistry)Statistical and Nonlinear PhysicsStatistical mechanicsCondensed Matter PhysicsBethe ansatzNonlinear Sciences::Exactly Solvable and Integrable SystemsPhase spaceSolitonPerturbation theory (quantum mechanics)Toda latticeNonlinear Sciences::Pattern Formation and SolitonsMathematicsMathematical physicsPhysica D: Nonlinear Phenomena
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Mott insulator: Tenth-order perturbation theory extended to infinite order using a quantum Monte Carlo scheme

2005

We present a method based on the combination of analytical and numerical techniques within the framework of the dynamical mean-field theory. Building upon numerically exact results obtained in an improved quantum Monte Carlo scheme, tenth-order strong-coupling perturbation theory for the Hubbard model on the Bethe lattice is extrapolated to infinite order. We obtain continuous estimates of energy $E$ and double occupancy $D$ with unprecedented precision $\mathcal{O}({10}^{\ensuremath{-}5})$ for the Mott insulator above its stability edge ${U}_{c1}\ensuremath{\approx}4.78$ as well as critical exponents. The relevance for recent experiments on Cr-doped ${\mathrm{V}}_{2}{\mathrm{O}}_{3}$ is po…

PhysicsBethe latticeHubbard modelMean field theoryQuantum mechanicsQuantum Monte CarloMott insulatorOrder (ring theory)Condensed Matter PhysicsCritical exponentEnergy (signal processing)Electronic Optical and Magnetic MaterialsPhysical Review B
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The band structure of double excited states for a linear chain

2000

Abstract The energy band structure in the case of double excited states of finite spin systems (s= 1 2 ) has been investigated. A geometrical construction based on the Bethe Ansatz method for determining eigenstates has been proposed. The formula for energy spectrum in the center and at the border of Brillouin zone has been obtained. Classification of energy bands has been elaborated on and approximated dispersion law for bounded states given. Some problems with application of the Bethe Ansatz in the case of finite system has been pointed out.

PhysicsCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsBethe ansatzBrillouin zoneQuantum mechanicsBounded functionExcited stateQuantum electrodynamicsDispersion relationElectrical and Electronic EngineeringElectronic band structureEigenvalues and eigenvectorsSpin-½Physica B: Condensed Matter
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Ground state of the frustrated Hubbard model within DMFT: energetics of Mott insulator and metal from ePT and QMC

2004

We present a new method, ePT, for extrapolating few known coefficients of a perturbative expansion. Controlled by comparisons with numerically exact quantum Monte Carlo (QMC) results, 10th order strong-coupling perturbation theory (PT) for the Hubbard model on the Bethe lattice is reliably extrapolated to infinite order. Within dynamical mean-field theory (DMFT), we obtain continuous estimates of energy E and double occupancy D with unprecedented precision O(10^{-5}) for the Mott insulator above its stability edge U_{c1}=4.78 as well as critical exponents. In addition, we derive corresponding precise estimates for E and D in the metallic ground state from extensive low-temperature QMC simul…

PhysicsCondensed Matter::Quantum GasesHubbard modelBethe latticeCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Quantum Monte CarloMott insulatorFOS: Physical sciencesCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMott transitionCondensed Matter - Strongly Correlated ElectronsCondensed Matter::Strongly Correlated ElectronsElectrical and Electronic EngineeringGround stateCritical exponentLattice model (physics)
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Dynamical mean-field theory calculation with the dynamical density-matrix renormalization group

2006

Abstract We study the Hubbard model at half band-filling on a Bethe lattice with infinite coordination number at zero temperature. We use the dynamical mean-field theory (DMFT) mapping to a single-impurity Anderson model with a bath whose properties have to be determined self-consistently. For a controlled and systematic implementation of the self-consistency scheme we use the fixed-energy approach to the DMFT. Using the dynamical density–matrix renormalization group method (DDMRG) we calculate the density of states (DOS) with a resolution ranging from 3% of the bare bandwidth W = 4 t at high energies to 0.01% for the quasi-particle peak. The DDMRG resolution and accuracy for the DOS is sup…

PhysicsDensity matrixHubbard modelBethe latticeDensity matrix renormalization groupNumerical analysisRenormalization groupCondensed Matter Physics01 natural sciences010305 fluids & plasmasElectronic Optical and Magnetic MaterialsQuantum electrodynamics0103 physical sciencesDensity of statesCondensed Matter::Strongly Correlated ElectronsElectrical and Electronic Engineering010306 general physicsAnderson impurity modelMathematical physicsPhysica B: Condensed Matter
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Spectral Function of the One-Dimensional Hubbard Model away from Half Filling

2004

We calculate the photoemission spectral function of the one-dimensional Hubbard model away from half filling using the dynamical density matrix renormalization group method. An approach for calculating momentum-dependent quantities in finite open chains is presented. Comparison with exact Bethe Ansatz results demonstrates the unprecedented accuracy of our method. Our results show that the photoemission spectrum of the quasi-one-dimensional conductor TTF-TCNQ provides evidence for spin-charge separation on the scale of the conduction band width.

PhysicsDensity matrixStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelFOS: Physical sciencesGeneral Physics and AstronomyRenormalization groupThermal conductionSpinonBethe ansatzConductorCondensed Matter - Strongly Correlated ElectronsLuttinger liquidQuantum electrodynamicsQuantum mechanicsCondensed Matter::Strongly Correlated ElectronsPhysical Review Letters
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Dynamical behaviour of an XX central spin model through Bethe ansatz techniques

2009

Following the Bethe ansazt procedure the exact dynamics of an XX central spin model is revealed. Particular initial conditions are analyzed and the consequent time evolution is compared with the exact solution obtained by solving the time-dependent Schrudinger equation. The interest towards spin systems and in particular central spin systems, is motivated by the recent developments in more applicative contexts.

PhysicsExact solutions in general relativityQuantum mechanicsSpin modelTime evolutionCondensed Matter::Strongly Correlated ElectronsStatistical and Nonlinear PhysicsMathematical PhysicsBethe ansatzMathematical physicsSpin-½Reports on Mathematical Physics
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Relativistic, model-independent, multichannel $2\to2$ transition amplitudes in a finite volume

2016

We derive formalism for determining $\textbf{2} + \mathcal J \to \textbf{2}$ infinite-volume transition amplitudes from finite-volume matrix elements. Specifically, we present a relativistic, model-independent relation between finite-volume matrix elements of external currents and the physically observable infinite-volume matrix elements involving two-particle asymptotic states. The result presented holds for states composed of two scalar bosons. These can be identical or non-identical and, in the latter case, can be either degenerate or non-degenerate. We further accommodate any number of strongly-coupled two-scalar channels. This formalism will, for example, allow future lattice QCD calcu…

PhysicsFinite volume methodBethe–Salpeter equationNuclear Theory010308 nuclear & particles physicsDegenerate energy levelsHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesObservableParity (physics)Lattice QCD01 natural sciencesScattering amplitudeNuclear Theory (nucl-th)High Energy Physics - LatticeQuantum mechanics0103 physical sciences010306 general physicsBosonMathematical physics
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