Search results for " glass"

showing 10 items of 409 documents

Two-dimensional isotropic orientational glasses: a computer-simulation study

1989

The analogue of the Edwards-Anderson model for isotropic vector spin glasses, but taking three-component quadrupoles instead of spins at each lattice site, is studied on the square lattice with extensive Monte Carlo calculations, using a nearest-neighbor symmetric gaussian interaction. It is shown that at low temperaturesT the model develops a short range order both with respect to glass like correlations and with respect to “ferromagnetic” correlations among the quadrupoles. The associated correlation lengths and susceptibilities diverge asT→0, and the critical exponents for this zero-temperature phase transition are estimated. Dynamic correlation functions are analyzed as well and it is s…

PhysicsPhase transitionSpin glassSpinsCondensed matter physicsLattice (order)Monte Carlo methodIsotropyGeneral Materials ScienceCondensed Matter PhysicsSquare latticeCritical exponentElectronic Optical and Magnetic MaterialsZeitschrift f�r Physik B Condensed Matter
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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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Domain-wall excitations in the two-dimensional Ising spin glass

2018

The Ising spin glass in two dimensions exhibits rich behavior with subtle differences in the scaling for different coupling distributions. We use recently developed mappings to graph-theoretic problems together with highly efficient implementations of combinatorial optimization algorithms to determine exact ground states for systems on square lattices with up to $10\,000\times 10\,000$ spins. While these mappings only work for planar graphs, for example for systems with periodic boundary conditions in at most one direction, we suggest here an iterative windowing technique that allows one to determine ground states for fully periodic samples up to sizes similar to those for the open-periodic…

PhysicsQuantum PhysicsSpin glassStatistical Mechanics (cond-mat.stat-mech)SpinsPhase (waves)FOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksComputational Physics (physics.comp-ph)01 natural sciences010305 fluids & plasmasTheoretical physicsDomain wall (magnetism)Spin wave0103 physical sciencesCombinatorial optimizationIsing spinQuantum Physics (quant-ph)010306 general physicsPhysics - Computational PhysicsCritical exponentCondensed Matter - Statistical MechanicsPhysical Review B
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Forward J / ψ and D meson nuclear suppression at the LHC

2017

Abstract Using the color glass condensate formalism, we study the nuclear modification of forward J/ψ and D meson production in high energy proton-nucleus collisions at the LHC. We show that relying on the optical Glauber model to obtain the dipole cross section of the nucleus from the one of the proton fitted to HERA DIS data leads to a smaller nuclear suppression than in the first study of these processes in this formalism and a better agreement with experimental data.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Colliderta114010308 nuclear & particles physicsNuclear TheoryquarkoniaHERABalitsky-Kovchegov equationDeep inelastic scattering01 natural sciencesColor-glass condensateNuclear physicsDipole0103 physical sciencesD mesoncolor glass condensateHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsGlauberNuclear and Particle Physics Proceedings
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Ising Spin-Glass on a Lattice with Small Loops

1991

We consider the Ising spin-glass on a special lattice containing small loops with finite coordination number c. We derive the equation for the effective field distribution. With zero external field, we calculate the spin-glass transition temperature and obtain the lower critical dimension of the system. We investigate the system near and below the spin-glass transition and find that the replica symmetric solution is unstable in the low-temperature phase. Our results indicate that the replica symmetry breaking (RSB) effects are stronger than that of the Bethe lattice and furthermore, RSB is enhanced as the dimension (c/2) is decreased. Comparison with recent results of the 1/d expansion is a…

PhysicsSpin glassBethe latticeCondensed matter physicsTransition temperatureGeneral Physics and AstronomyCondensed Matter::Disordered Systems and Neural Networkssymbols.namesakeLattice (order)symbolsIsing modelSymmetry breakingHamiltonian (quantum mechanics)Critical dimensionEurophysics Letters (EPL)
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Multioverlap Simulations of the 3D Edwards-Anderson Ising Spin Glass

1997

We introduce a novel method for numerical spin glass investigations: Simulations of two replica at fixed temperature, weighted such that a broad distribution of the Parisi overlap parameter $q$ is achieved. Canonical expectation values for the entire $q$-range (multi-overlap) follow by re-weighting. We demonstrate the feasibility of the approach by studying the $3d$ Edwards-Anderson Ising ($J_{ik}=\pm 1$) spin glass in the broken phase ($\beta=1$). For the first time it becomes possible to obtain reliable results about spin glass tunneling barriers. In addition, as do some earlier numerical studies, our results support that Parisi mean field theory is valid down to $3d$.

PhysicsSpin glassCondensed matter physicsCondensed Matter (cond-mat)High Energy Physics - Lattice (hep-lat)FOS: Physical sciencesGeneral Physics and AstronomyCondensed MatterCondensed Matter::Disordered Systems and Neural NetworksFreezing pointHigh Energy Physics - LatticeDistribution (mathematics)Phase (matter)Ising spinIsing modelScalingQuantum tunnellingPhysical Review Letters
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Superspin glass phase and hierarchy of interactions in multiferroic PbFe1/2Sb1/2O3: an analog of ferroelectric relaxors?

2014

We have fabricated new perovskite multiferroic PbFeSbO3 with a high degree (up to 0.9) of chemical ordering and unexpectedly high-temperature magnetic relaxor properties, which can barely be described within concepts of conventional spin glass physics. Notably, we found that the field-temperature phase diagram of this material, in the extremely wide temperature interval, contains the de Almeida–Thouless-type critical line, which has been the subject of long debates regarding its possible experimental realization. We explain our findings by the creation, at high temperatures of not less than 250 K, of giant superspins (SSs), owing, curiously enough, to the antiferromagnetic superexchange int…

PhysicsSpin glassCondensed matter physicsCritical lineSuperexchangePhase (matter)General Physics and AstronomyAntiferromagnetismMultiferroicsFerroelectricityPhase diagramNew Journal of Physics
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Griffiths phase manifestation in disordered dielectrics

2000

We predict the existence of Griffith phase in the dielectrics with concentrational crossover between dipole glass (electric analog of spin glass) and ferroelectricity. The peculiar representatives of above substances are $KTaO_3:Li$, $Nb$, $Na$ or relaxor ferroelectrics like $Pb_{1-x}La_xZr_{0.65}Ti_{0.35}O_3$. Since this phase exists above ferroelectric phase transition temperature (but below that temperature for ordered substance), we call it "para-glass phase". We assert that the difference between paraelectric and para-glass phase of above substances is the existence of clusters (inherent to "ordinary" Griffiths phase in Ising magnets) of correlated dipoles. We show that randomness play…

PhysicsSpin glassCondensed matter physicsFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)DielectricCondensed Matter - Disordered Systems and Neural NetworksCondensed Matter PhysicsFerroelectricityCondensed Matter::Disordered Systems and Neural NetworksElectronic Optical and Magnetic MaterialsDipoleCondensed Matter::Materials ScienceMean field theoryPhase (matter)Ising modelRandomness
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Spin stiffness of vector spin glasses

2011

Abstract We study domain-wall excitations for O ( m ) vector spin glasses in the limit m → ∞ , where the energy landscape is simplified considerably compared to XY or Heisenberg models due to the complete disappearance of metastability. Using numerical ground-state calculations and appropriate pairs of complementary boundary conditions, domain-wall defects are inserted into the systems and their excitation energies are measured. This allows us to determine the stiffness exponents for lattices of a range of spatial dimensions d = 2 , … , 7 . Compiling these results, we can finally determine the lower critical dimension of the model. The outcome is compared to estimates resulting from field-t…

PhysicsSpin glassCondensed matter physicsGeneral Physics and AstronomyEnergy landscapeStiffnessHardware and ArchitectureQuantum mechanicsMetastabilitymedicineBoundary value problemmedicine.symptomCritical dimensionExcitationSpin-½Computer Physics Communications
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Monte Carlo investigation of a model for a three-dimensional orientational glass with short-range gaussian interaction

1987

The analogue of the Edwards-Anderson model for isotropic vector spin glasses, but taking quadrupoles instead of unit vectors at each lattice site of the considered simple cubic lattice, is studied as a model for an orientational glass. We study both the case where the quadrupole moment can orient in a three-dimensional space (m=3) and the case where the orientation is restricted to a plane (m=2), but otherwise the Hamiltonian is fully isotropic. ℋ= $$ - \sum\limits_{\left\langle {i,j} \right\rangle } {J_{ij} } \left[ {\left( {\sum\limits_{\mu = 1}^m {S_i^\mu S_j^\mu } } \right)^2 - \frac{1}{m}} \right]$$ , whereJ ij is a random gaussian interaction between nearest neighbors, andS i μ the μ'…

PhysicsSpin glassCondensed matter physicsIsotropyCondensed Matter PhysicsElectronic Optical and Magnetic Materialssymbols.namesakeNull vectorUnit vectorLattice (order)QuadrupolesymbolsGeneral Materials ScienceHamiltonian (quantum mechanics)Orientational glassMathematical physicsZeitschrift f�r Physik B Condensed Matter
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