Search results for "Nearest neighbor"

showing 10 items of 63 documents

Spin and charge orderings in the atomic limit of the U-V-J model

2011

In this paper we study a generalization of the 1D Hubbard model by considering density-density and Ising-type spin-spin nearest neighbor (NN) interactions, parameterized by $V$ and $J$, respectively. We present the T=0 phase diagram for both ferro ($J>0$) and anti-ferro ($J<0$) coupling obtained in the narrow-band limit by means of an extension to zero-temperature of the transfer-matrix method. Based on the values of the Hamiltonian parameters, we identify a number of phases that involve orderings of the double occupancy, NN density and spin correlations, being these latter very fragile.

PhysicsHistoryHubbard modelStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - SuperconductivityParameterized complexityFOS: Physical sciencesComputer Science ApplicationsEducationk-nearest neighbors algorithmSuperconductivity (cond-mat.supr-con)symbols.namesakeCondensed Matter - Strongly Correlated ElectronssymbolsCondensed Matter::Strongly Correlated ElectronsHamiltonian (quantum mechanics)Mathematical physicsPhase diagram
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Green functions for nearest- and next-nearest-neighbor hopping on the Bethe lattice

2005

We calculate the local Green function for a quantum-mechanical particle with hopping between nearest and next-nearest neighbors on the Bethe lattice, where the on-site energies may alternate on sublattices. For infinite connectivity the renormalized perturbation expansion is carried out by counting all non-self-intersecting paths, leading to an implicit equation for the local Green function. By integrating out branches of the Bethe lattice the same equation is obtained from a path integral approach for the partition function. This also provides the local Green function for finite connectivity. Finally, a recently developed topological approach is extended to derive an operator identity whic…

PhysicsImplicit functionBethe latticeStrongly Correlated Electrons (cond-mat.str-el)Operator (physics)Spectrum (functional analysis)General Physics and AstronomyFOS: Physical sciencesPartition function (mathematics)01 natural sciences010305 fluids & plasmask-nearest neighbors algorithmCondensed Matter - Strongly Correlated Electrons0103 physical sciencesPath integral formulationGravitational singularityddc:530Condensed Matter::Strongly Correlated ElectronsStatistical physics010306 general physics
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Wetting and layering in the nearest-neighbor simple-cubic Ising lattice: A Monte Carlo investigation.

1988

Critical, tricritical, and first-order wetting transitions are studied in a simple-cubic nearest-neighbor Ising model, with exchange J in the bulk and exchange ${J}_{s}$ in the surface planes, by applying suitable bulk and surface fields H and ${H}_{1}$. Monte Carlo calculations are presented for systems of size L\ifmmode\times\else\texttimes\fi{}L\ifmmode\times\else\texttimes\fi{}D, in a thin film geometry with D=40 layers and two free L\ifmmode\times\else\texttimes\fi{}L surfaces, with L ranging from L=10 to L=50. In addition, evidence for prewetting transitions and for layering transitions (the latter occur for temperatures T less than the roughening temperature ${T}_{R}$) is presented. …

PhysicsMagnetizationCondensed matter physicsMonte Carlo methodDiagramIsing modelCubic crystal systemSurface (topology)Energy (signal processing)k-nearest neighbors algorithmPhysical review. B, Condensed matter
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Classical Heisenberg antiferromagnets with nearest and next-nearest neighbor interactions on the face-centered cubic lattice: a model for EuTe?

1989

Magnetic properties of the Heisenberg antiferromagnet with spin quantum numberS→∞ on the face-centered cubic lattice are studied as function of temperature and magnetic field, using molecular field approximation and Monte Carlo methods. In order to model Europiumtelluride, we use isotropic exchange interactions between nearest- and nextnearest neighbors; the values of these exchange constants are taken from experiments. In addition, a pseudo-dipolar anisotropy (truncated after the next-nearest neighbor distance) is included; the molecular field calculations also are performed with the full dipolar of real EuTe in two respects: the structure in zero magnetic field involves 8 sublattices in t…

PhysicsMagnetizationDipoleCondensed matter physicsHeisenberg modelExchange interactionAntiferromagnetismGeneral Materials ScienceCubic crystal systemCondensed Matter PhysicsElectronic Optical and Magnetic Materialsk-nearest neighbors algorithmMagnetic fieldZeitschrift f�r Physik B Condensed Matter
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Modulational stability brought by cubic–quartic interactions of the nearest-neighbor in FK model subjected in a parametrized on-site potential

2022

Abstract This work extends to higher-order interactions the results of Ref. Nguetcho (2021), in which we discussed only on modulational instability in one-dimensional chain made of atoms, harmonically coupled to their nearest neighbors and subjected to an external on-site potential. Here we investigate the competition between cubic-quartic nonlinearities interactions of the nearest-neighbor and substrate’s deformability, and mainly discuss its impact on the modulational instability of the system. This makes it possible to adapt the theoretical model to a real physical system such as atomic chains or DNA lattices. The governing equation, derived from the modified Frenkel-Kontorova model, is …

PhysicsNumerical AnalysisGeneric propertyApplied MathematicsPhysical systemInstabilityk-nearest neighbors algorithmsymbols.namesakeModulational instabilityNonlinear systemModeling and SimulationQuartic functionsymbolsStatistical physicsNonlinear Schrödinger equationCommunications in Nonlinear Science and Numerical Simulation
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Phase Transitions in Multicomponent Widom-Rowlinson Models

1995

We use Monte Carlo techniques to study the phase diagram of multicomponent Widom-Rowlinson models on a square lattice: there are M species all with the same fugacity z and a nearest neighbor hard core exclusion between unlike particles. For M between two and six there is a direct transition from the gas phase at z z d (M). For M ≥ 7 there is an intermediate ordered phase in which the even (or odd) sublattice is occupied preferentially by particles chosen at random from any of the species. The existence of such an intermediate phase was proven earlier for M ≥ M 0, M 0 very large. Exact calculations on the Bethe lattice give M0 = 4.

PhysicsPhase transitionCondensed matter physicsBethe latticePhase (matter)Monte Carlo methodFugacitySquare latticek-nearest neighbors algorithmPhase diagram
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The Ising square lattice in aL�M geometry: A model for the effect of surface steps on phase transitions in adsorbed monolayers

1989

Critical phenomena in adsorbed monolayers on surfaces are influenced by limited substrate homogeneity, such as surface steps. We consider the resulting finite-size and boundary effects in the framework of a lattice gas system with nearest neighbor attraction in aL×M geometry, with two free boundaries of lengthM≫L, and periodic boundary conditions in the other direction (along the direction of the steps). This geometry thus models a “terrace” of the stepped surface, and adatoms adsorbed on neighboring terraces are assumed to be non-interacting. Also the effect of boundary “fields” is considered (describing the effects of missing neighbors and changed binding energy to the substrate near the …

PhysicsPhase transitionCondensed matter physicsCritical phenomenaGeometryCondensed Matter PhysicsSquare latticeElectronic Optical and Magnetic Materialsk-nearest neighbors algorithmHomogeneity (physics)Periodic boundary conditionsGeneral Materials ScienceIsing modelScalingZeitschrift f�r Physik B Condensed Matter
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Monte Carlo simulation of phase separation and clustering in the ABV model

1991

As a model for a binary alloy undergoing an unmixing phase transition, we consider a square lattice where each site can be either taken by an A atom, a B atom, or a vacancy (V), and there exists a repulsive interaction between AB nearest neighbor pairs. Starting from a random initial configuration, unmixing proceeds via random jumps of A atoms or B atoms to nearest neighbor vacant sites. In the absence of any interaction, these jumps occur at jump ratesΓ A andΓ B, respectively. For a small concentration of vacancies (c v=0.04) the dynamics of the structure factorS(k,t) and its first two momentsk 1(t),k 2 2 (t) is studied during the early stages of phase separation, for several choices of co…

PhysicsPhase transitionCondensed matter physicsVacancy defectMonte Carlo methodAtomCluster (physics)Time evolutionStatistical and Nonlinear PhysicsSquare latticeMolecular physicsMathematical Physicsk-nearest neighbors algorithmJournal of Statistical Physics
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Finite-Size Scaling Study of the Simple Cubic Three-State Potts Glass

1991

During the last few years the Potts glass model has attracted more and more attention. It is considered as a first step towards modelling the phase transition of structural and orientational glasses. A mean-field approach /1/ predicts a low temperature behavior completely different from what is known from Ising spin glasses /2/. But short range models differ markedly from mean-field-predictions. So it is natural to ask, how the short range Potts glass behaves. Especially the question of the lower critical dimension d l is important, below which a finite temperature transition ceases to occur. We tried to answer this by combining Monte-Carlo simulations with a finite-size scaling analysis. T…

PhysicsPhase transitionsymbols.namesakeSpin glassCondensed matter physicssymbolsCubic crystal systemHamiltonian (quantum mechanics)Orientational glassScalingk-nearest neighbors algorithmPotts model
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Multiparticle breathers for a chain with double-quadratic on-site potential

1999

We investigate the existence and properties of multiparticle breathers for a one-dimensional model with harmonic nearest neighbor interactions where a group of r particles $(r=1,2,3,\dots{})$ perform interwell oscillations between both wells of a double-quadratic on-site potiential. We find two types of such breathers. For the first type the breather frequency $\ensuremath{\Omega}$ is within the single-particle oscillator spectrum, and the ``residence'' time of each breather particle in the left and right well is about the same. For the second breather $\ensuremath{\Omega}$ is below that spectrum, and the ratio ${\ensuremath{\tau}}_{L}/{\ensuremath{\tau}}_{R}$ of the residence time in the l…

PhysicsQuadratic equationGroup (mathematics)BreatherQuantum mechanicsSpectrum (functional analysis)Zero (complex analysis)Type (model theory)Nonlinear Sciences::Pattern Formation and SolitonsOmegak-nearest neighbors algorithmPhysical Review E
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