Search results for "transfer matrix"

showing 10 items of 30 documents

Low-temperature spectrum of correlation lengths of the XXZ chain in the antiferromagnetic massive regime

2015

We consider the spectrum of correlation lengths of the spin-$\frac{1}{2}$ XXZ chain in the antiferromagnetic massive regime. These are given as ratios of eigenvalues of the quantum transfer matrix of the model. The eigenvalues are determined by integrals over certain auxiliary functions and by their zeros. The auxiliary functions satisfy nonlinear integral equations. We analyse these nonlinear integral equations in the low-temperature limit. In this limit we can determine the auxiliary functions and the expressions for the eigenvalues as functions of a finite number of parameters which satisfy finite sets of algebraic equations, the so-called higher-level Bethe Ansatz equations. The behavio…

High Energy Physics - TheoryStatistics and ProbabilityPhysicsStatistical Mechanics (cond-mat.stat-mech)Strongly Correlated Electrons (cond-mat.str-el)Zero (complex analysis)FOS: Physical sciencesGeneral Physics and AstronomyStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Auxiliary functionTransfer matrixBethe ansatzCondensed Matter - Strongly Correlated ElectronsAlgebraic equationHigh Energy Physics - Theory (hep-th)Modeling and SimulationComplex planeCondensed Matter - Statistical MechanicsMathematical PhysicsEigenvalues and eigenvectorsMathematical physicsSpin-½Journal of Physics A: Mathematical and Theoretical
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FINITE-SIZE CORRECTIONS TO CORRELATION FUNCTION AND SUSCEPTIBILITY IN 2D ISING MODEL

2006

Transfer matrix calculations of the critical two-point correlation function in 2D Ising model on a finite-size [Formula: see text] lattice with periodic boundaries along 〈11〉 direction are extended to L = 21. A refined analysis of the correlation function in 〈10〉 crystallographic direction at the distance r = L indicates the existence of a nontrivial finite-size correction of a very small amplitude with correction-to-scaling exponent ω < 2 in agreement with our foregoing study for L ≤ 20. Here we provide an additional evidence and show that amplitude a of the multiplicative correction term 1 + aL-ωis about -3.5·10-8if ω = 1/4 (the expected value). We calculate also the susceptibility for…

Multiplicative functionGeneral Physics and AstronomyStatistical and Nonlinear PhysicsExpected valueTransfer matrixComputer Science ApplicationsAmplitudeComputational Theory and MathematicsQuantum electrodynamicsLattice (order)ExponentIsing modelScalingMathematical PhysicsMathematical physicsMathematicsInternational Journal of Modern Physics C
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Spatial fluctuations of the chemical potential in case of nearly coherent transport along an ordered chain

1991

The Landauer-Buttiker approach is used to describe electron transport along a chain of scatterers which allow elastic as well as inelastic processes. The inelastic scattering takes place via side branches coupling the chain to electron reservoirs which serve as a heat bath. For small inelastic coupling of the scatterers to the heat bath strong interference effects lead to spatial fluctuations of the charge density. The corresponding oscillations of the chemical potential are discussed in view of phase-sensitive experiments measuring the four-probe resistance.

PhysicsCouplingElastic scatteringCondensed matter physicsOscillationCharge densityGeneral Materials ScienceElectronInelastic scatteringCondensed Matter PhysicsElectron transport chainTransfer matrixElectronic Optical and Magnetic MaterialsZeitschrift f�r Physik B Condensed Matter
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Numerical studies of Minimally Doubled Fermions

2013

We have performed the first numerical study of minimally doubled fermions of the Karsten-Wilczek class in the quenched approximation. This requires fixing the counterterms, which arise due to hypercubic symmetry breaking induced by the Karsten-Wilczek term. Non-perturbative renormalisation criteria are formulated after a detailed study of the parameter dependence of mesonic observables. Minimisation of the mass anisotropy of the pseudoscalar ground state fixes non-perturbative renormalisation conditions for the counterterm coefficients. These anisotropies are mapped out by probing different euclidean components of the transfer matrix through calculations of the pseudoscalar ground state mas…

PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Lattice (group)FOS: Physical sciencesObservableQuenched approximationFermionTransfer matrixPseudoscalarHigh Energy Physics - LatticeSymmetry breakingGround stateMathematical physics
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Measurement of the top quark mass in thelepton+jetsfinal state with the matrix element method

2006

We present a measurement of the top quark mass with the Matrix Element method in the lepton+jets final state. As the energy scale for calorimeter jets represents the dominant source of systematic uncertainty, the Matrix Element likelihood is extended by an additional parameter, which is defined as a global multiplicative factor applied to the standard energy scale. The top quark mass is obtained from a fit that yields the combined statistical and systematic jet energy scale uncertainty.

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkScale (ratio)010308 nuclear & particles physicsTop quark condensateJet (particle physics)01 natural sciencesTransfer matrixParticle identificationNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant mass010306 general physicsLeptonPhysical Review D
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Bloch analysis of finite periodic microring chains

2005

We apply Bloch analysis to the study of finite periodic cascading of microring resonators. Diagonalization of the standard transfer matrix approach not only allows to find an exact analytic expression for transmission and reflection, but also to derive a closed form solution for the field in every point of the structure. To give more physical insight we analyze the main features of the transmission resonances in a finite chain and we give some hints for their experimental verification

PhysicsPhysics and Astronomy (miscellaneous)Field (physics)Mathematical analysisGeneral EngineeringFOS: Physical sciencesGeneral Physics and AstronomyTransfer matrixResonatorReflection (mathematics)Chain (algebraic topology)Transmission (telecommunications)Point (geometry)Closed-form expressionOptics (physics.optics)Physics - OpticsApplied Physics B
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Infinite projected entangled-pair state algorithm for ruby and triangle-honeycomb lattices

2018

The infinite Projected Entangled-Pair State (iPEPS) algorithm is one of the most efficient techniques for studying the ground-state properties of two-dimensional quantum lattice Hamiltonians in the thermodynamic limit. Here, we show how the algorithm can be adapted to explore nearest-neighbor local Hamiltonians on the ruby and triangle-honeycomb lattices, using the Corner Transfer Matrix (CTM) renormalization group for 2D tensor network contraction. Additionally, we show how the CTM method can be used to calculate the ground state fidelity per lattice site and the boundary density operator and entanglement entropy (EE) on an infinite cylinder. As a benchmark, we apply the iPEPS method to th…

PhysicsQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciences02 engineering and technologyQuantum entanglementRenormalization group021001 nanoscience & nanotechnology01 natural sciencesTransfer matrixCondensed Matter - Strongly Correlated ElectronsLattice (order)0103 physical sciencesThermodynamic limitQuantum Physics (quant-ph)010306 general physics0210 nano-technologyAnisotropyAlgorithmQuantumPhase diagramPhysical Review B
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Teaching stable two-mirror resonators through the fractional Fourier transform

2009

We analyse two-mirror resonators in terms of their fractional Fourier transform (FRFT) properties. We use the basic ABCD ray transfer matrix method to show how the resonator can be regarded as the cascade of two propagation–lens–propagation FRFT systems. Then, we present a connection between the geometric properties of the resonator (the g parameters) and those of the equivalent FRFT systems (the FRFT order and scaling parameters). Expressions connecting Gaussian beam q-transformation with FRFT parameters are derived. In particular, we show that the beam waist of the resonator's mode is located at the plane leading to two FRFT subsystems with equal scaling parameter which, moreover, coincid…

PhysicsRay transfer matrix analysisbusiness.industryFourier opticsMathematical analysisTransfer-matrix method (optics)General Physics and AstronomyFractional Fourier transformResonatorOpticsRayleigh lengthPhotonicsbusinessGaussian beamEuropean Journal of Physics
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One-dimensional Ising-like systems: an analytical investigation of the static and dynamic properties, applied to spin-crossover relaxation

2000

We investigate the dynamical properties of the 1-D Ising-like Hamiltonian taking into account short and long range interactions, in order to predict the static and dynamic behavior of spin crossover systems. The stochastic treatment is carried out within the frame of the local equilibrium method [1]. The calculations yield, at thermodynamic equilibrium, the exact analytic expression previously obtained by the transfer matrix technique [2]. We mainly discuss the shape of the relaxation curves: (i) for large (positive) values of the short range interaction parameter, a saturation of the relaxation curves is observed, reminiscent of the behavior of the width of the static hysteresis loop [3]; …

PhysicsSolid-state physicsCondensed matter physicsThermodynamic equilibriumComplex systemCondensed Matter PhysicsTransfer matrixElectronic Optical and Magnetic Materialssymbols.namesakeSpin crossoversymbolsIsing modelStatistical physicsHamiltonian (quantum mechanics)Phase diagramThe European Physical Journal B
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Exact solution of the 1D Hubbard model with NN and NNN interactions in the narrow-band limit

2013

We present the exact solution, obtained by means of the Transfer Matrix (TM) method, of the 1D Hubbard model with nearest-neighbor (NN) and next-nearest-neighbor (NNN) Coulomb interactions in the atomic limit (t=0). The competition among the interactions ($U$, $V_1$, and $V_2$) generates a plethora of T=0 phases in the whole range of fillings. $U$, $V_1$, and $V_2$ are the intensities of the local, NN and NNN interactions, respectively. We report the T=0 phase diagram, in which the phases are classified according to the behavior of the principal correlation functions, and reconstruct a representative electronic configuration for each phase. In order to do that, we make an analytic limit $T\…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Statistical Mechanics (cond-mat.stat-mech)Hubbard modelFOS: Physical sciencesCondensed Matter PhysicsTransfer matrixElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityQuantum mechanicsCoulombLimit (mathematics)Electron configurationGround stateCondensed Matter - Statistical MechanicsPhase diagramThe European Physical Journal B
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