Search results for "Ising Model"

showing 10 items of 241 documents

Universal scaling for the quantum Ising chain with a classical impurity

2017

We study finite size scaling for the magnetic observables of an impurity residing at the endpoint of an open quantum Ising chain in a transverse magnetic field, realized by locally rescaling the magnetic field by a factor $\mu \neq 1$. In the homogeneous chain limit at $\mu = 1$, we find the expected finite size scaling for the longitudinal impurity magnetization, with no specific scaling for the transverse magnetization. At variance, in the classical impurity limit, $\mu = 0$, we recover finite scaling for the longitudinal magnetization, while the transverse one basically does not scale. For this case, we provide both analytic approximate expressions for the magnetization and the susceptib…

PhysicsLength scaleElectronic Optical and Magnetic Materials; Condensed Matter PhysicsElectronic Optical and Magnetic MaterialObservable--Condensed Matter Physics01 natural sciencesSquare latticeSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasMagnetic fieldMagnetizationQuantum mechanics0103 physical sciencesIsing model010306 general physicsQuantumScaling
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Determination of the origin and magnitude of logarithmic finite-size effects on interfacial tension: Role of interfacial fluctuations and domain brea…

2014

The ensemble-switch method for computing wall excess free energies of condensed matter is extended to estimate the interface free energies between coexisting phases very accurately. By this method, system geometries with linear dimensions $L$ parallel and $L_z$ perpendicular to the interface with various boundary conditions in the canonical or grandcanonical ensemble can be studied. Using two- and three-dimensional Ising models, the nature of the occurring logarithmic finite size corrections is studied. It is found crucial to include interfacial fluctuations due to "domain breathing".

PhysicsLogarithmCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)General Physics and AstronomyMagnitude (mathematics)ThermodynamicsFOS: Physical sciencesDomain (mathematical analysis)Surface tensionGrand canonical ensemblePerpendicularIsing modelBoundary value problemCondensed Matter - Statistical Mechanics
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Noise enhanced stability in magnetic systems

2009

In this paper noise enhanced stability in magnetic systems is studied by both an Ising-type model and a Preisach–Arrhenius model as well as a dynamic Preisach model. It is shown that in one nonequilibrium Ising system noise enhanced stability occurs and that dynamic Preisach model has the capability to predict the occurrence of noise enhanced stability in magnetic systems. On the contrary, in a Preisach–Arrhenius model of a single quadrant magnetic material, noise enhanced stability is not detected.

PhysicsMagnetic noiseCondensed matter physicsIsing systemGeneral Physics and AstronomyNon-equilibrium thermodynamicsSettore ING-IND/32 - Convertitori Macchine E Azionamenti ElettriciCondensed Matter::Disordered Systems and Neural NetworksElectric Machines Power Systems Electric TechnologyMagnetizationMagnetCondensed Matter::Statistical MechanicsIsing modelStatistical physics
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Properties of small antiferromagnetic Ising clusters

1997

Magnetic properties of small antiferromagnetic clusters have been studied by using the Ising model with nearest-neighbour interactions. The number of atoms in the clusters varied between 6 and 30. Several cluster geometries were analysed in detail with the result that there is no generic phase diagram. In an external magnetic field magnetisation can increase with increasing temperature in a considerable temperature range. Magnetisation was found to strongly depend on both the overall geometry of the cluster and on the symmetry of the underlaying lattice structure.

PhysicsMagnetizationCondensed matter physicsCluster (physics)AntiferromagnetismIsing modelAtmospheric temperature rangeAtomic and Molecular Physics and OpticsSymmetry (physics)Phase diagramMagnetic field
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Wetting transitions near the bulk critical point: Monte Carlo simulations for the Ising model

1989

Critical, tricritical, and first-order wetting transitions are studied near the bulk critical point of a simple cubic nearest-neighbor Ising model by extensive Monte Carlo simulations. The model applies an exchange J in the bulk and exchange ${J}_{s}$ in the surface planes, where surface fields ${H}_{1}$ also act in addition to a possible bulk field H. Lattices in a thin-film geometry L\ifmmode\times\else\texttimes\fi{}L\ifmmode\times\else\texttimes\fi{}D are used, with two free L\ifmmode\times\else\texttimes\fi{}L surfaces (with L up to 256) and film thickness D up to 160, applying a very fast fully vectorizing multispin coding program. Our results present the first quantitative evidence f…

PhysicsMagnetizationCondensed matter physicsCritical point (thermodynamics)Monte Carlo methodIsing modelMulticritical pointWettingCubic crystal systemCritical fieldPhysical Review B
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Corner wetting in the two-dimensional Ising model: Monte Carlo results

2003

Square L ? L (L = 24?128) Ising lattices with nearest neighbour ferromagnetic exchange are considered using free boundary conditions at which boundary magnetic fields ? h are applied, i.e., at the two boundary rows ending at the lower left corner a field +h acts, while at the two boundary rows ending at the upper right corner a field ?h acts. For temperatures T less than the critical temperature Tc of the bulk, this boundary condition leads to the formation of two domains with opposite orientations of the magnetization direction, separated by an interface which for T larger than the filling transition temperature Tf (h) runs from the upper left corner to the lower right corner, while for T …

PhysicsMagnetizationCondensed matter physicsFerromagnetismTransition temperatureMonte Carlo methodBoundary (topology)General Materials ScienceIsing modelBoundary value problemCondensed Matter PhysicsScalingJournal of Physics: Condensed Matter
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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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Ferromagnetism in small clusters.

1991

Magnetization of small ferromagnetic clusters at finite temperatures has been studied using the Ising model and Monte Carlo techniques. The magnetization of finite clusters is reduced from the bulk value, and increases with the external magnetic field and with the cluster size. The results explain qualitatively the recent observations by de Heer, Milani, and Chatelain of the reduction with decreasing cluster size of the average magnetic moment in small iron clusters.

PhysicsMagnetizationFerromagnetismCondensed matter physicsMagnetic momentMonte Carlo methodCluster sizeGeneral Physics and AstronomyCurie temperatureIsing modelMagnetic fieldPhysical review letters
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Ising systems with pairwise competing surface fields

2005

The magnetization distribution and phase behaviour of large but finite Ising simple cubic L × L × L lattices in d = 3 dimensions and square L × L lattices in d = 2 dimensions are studied for the case where four free boundaries are present, at which surface fields +Hs act on one pair of opposite boundaries while surface fields −Hs act on the other pair (in d = 3, periodic boundary conditions are used for the remaining pair). Both the distribution PL(m) of the global magnetization and also the distribution of the local magnetization m(x,z) are obtained by Monte Carlo simulations, where x and z denote the coordinates when the boundaries are oriented along the x-axis and z-axis (in d = 2); or a…

PhysicsMagnetizationPhase transitionCondensed matter physicsPhenomenological modelPeriodic boundary conditionsGeneral Materials ScienceIsing modelBoundary value problemCubic crystal systemCondensed Matter PhysicsScalingJournal of Physics: Condensed Matter
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Phase transitions in nanosystems caused by interface motion: the Ising bipyramid with competing surface fields.

2005

The phase behavior of a large but finite Ising ferromagnet in the presence of competing surface magnetic fields +/- H_s is studied by Monte Carlo simulations and by phenomenological theory. Specifically, the geometry of a double pyramid of height 2L is considered, such that the surface field is positive on the four upper triangular surfaces of the bi-pyramid and negative on the lower ones. It is shown that the total spontaneous magnetization vanishes (for L -> infinity) at the temperature T_f(H), related to the "filling transition" of a semi-infinite pyramid, which can be well below the critical temperature of the bulk. The discontinuous vanishing of the magnetization is accompanied by a…

PhysicsMagnetizationPhase transitionStatistical Mechanics (cond-mat.stat-mech)Condensed matter physicsFOS: Physical sciencesIsing modelCritical exponentPower lawSpontaneous magnetizationCondensed Matter - Statistical MechanicsLandau theoryPyramid (geometry)Physical review. E, Statistical, nonlinear, and soft matter physics
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