Search results for "renormalization"

showing 10 items of 470 documents

The classical statistical mechanics of Frenkel-Kontorova models

1995

The scaling properties of the free energy, specific heat, and mean spacing are calculated for classical Frenkel-Kontorova models at low temperature, in three regimes: near the integrable limit, the anti-integrable limit, and the sliding-pinned transition (“transition by breaking of analyticity”). In particular, the renormalization scheme given in previous work for ground states of Frenkel-Kontorova models is extended to nonzero-temperature Gibbs states, and the hierarchical melting phenomenon of Vallet, Schilling, and Aubry is put on a rigorous footing.

PhysicsRenormalizationWork (thermodynamics)Integrable systemSpecific heatQuantum mechanicsScheme (mathematics)Statistical and Nonlinear PhysicsStatistical physicsStatistical mechanicsLimit (mathematics)ScalingMathematical PhysicsJournal of Statistical Physics
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Note on the pragmatic mode-sum regularization method: Translational-splitting in a cosmological background

2021

The point-splitting renormalization method offers a prescription to calculate finite expectation values of quadratic operators constructed from quantum fields in a general curved spacetime. It has been recently shown by Levi and Ori that when the background metric possesses an isometry, like stationary or spherically symmetric black holes, the method can be upgraded into a pragmatic procedure of renormalization that produces efficient numerical calculations. In this note we show that when the background enjoys three-dimensional spatial symmetries, like homogeneous expanding universes, the above pragmatic regularization technique reduces to the well established adiabatic regularization metho…

PhysicsSpacetime010308 nuclear & particles physicsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)16. Peace & justiceIsometry (Riemannian geometry)01 natural sciencesGeneral Relativity and Quantum CosmologyRenormalizationTheoretical physicsQuadratic equationRegularization (physics)0103 physical sciencesMetric (mathematics)Homogeneous space010306 general physicsAdiabatic process
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First Glimpse of the N=82 Shell Closure below Z=50 from Masses of Neutron-Rich Cadmium Isotopes and Isomers

2020

We probe the $N=82$ nuclear shell closure by mass measurements of neutron-rich cadmium isotopes with the ISOLTRAP spectrometer at ISOLDE-CERN. The new mass of $^{132}\mathrm{Cd}$ offers the first value of the $N=82$, two-neutron shell gap below $Z=50$ and confirms the phenomenon of mutually enhanced magicity at $^{132}\mathrm{Sn}$. Using the recently implemented phase-imaging ion-cyclotron-resonance method, the ordering of the low-lying isomers in $^{129}\mathrm{Cd}$ and their energies are determined. The new experimental findings are used to test large-scale shell-model, mean-field, and beyond-mean-field calculations, as well as the ab initio valence-space in-medium similarity renormalizat…

PhysicsSpectrometerAb initioShell (structure)Closure (topology)General Physics and AstronomyRenormalization group7. Clean energy01 natural sciencesISOLTRAPIsotopes of cadmium0103 physical sciencesPhysics::Atomic and Molecular ClustersNeutronAtomic physicsNuclear Experiment010306 general physicsPhysical Review Letters
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Monte Carlo study of the order-parameter distribution in the four-dimensional Ising spin glass

1990

We investigate the order-parameter distribution P(q) of the Ising spin glass with nearest-neighbor interactions in four dimensions using Monte Carlo simulations on lattices of linear dimension up to L=6. We find that, below the transition temperature ${\mathit{T}}_{\mathit{c}}$, the weight at small q seems to saturate to a nonzero value as the size increases, similar to the infinite-range Sherrington-Kirkpatrick model. We discuss our results in the light of recent theoretical predictions for the nature of the spin-glass phase.

PhysicsSpin glassCondensed matter physicsTransition temperatureMonte Carlo methodGeneral Physics and AstronomyRenormalization groupCondensed Matter::Disordered Systems and Neural Networkssymbols.namesakeDistribution functionsymbolsIsing spinIsing modelHamiltonian (quantum mechanics)Physical Review Letters
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Transient Reversible Growth and Percolation During Phase Separation

1988

Binary mixtures when quenched into the two-phase region exhibit transient percolation phenomena. These transient percolation phenomena and the underlying mechanism of transient reversible growth are investigated. In particular, one of the possible dynamical percolation lines between the dynamical spinodal and the line of macroscopic percolation is traced out. Analyzing the finite size effects with the usual scaling theory one finds exponents which seem to be inconsistent with the universality class of percolation. However, at zero temperature, where the growth is non-reversible and the transition of a sol-gel type, the exponents are consistent with those of random percolation.

PhysicsSpinodalMathematics::ProbabilityCondensed matter physicsPercolationCondensed Matter::Statistical MechanicsTransient (oscillation)Type (model theory)Renormalization groupZero temperatureScaling theoryCondensed Matter::Disordered Systems and Neural NetworksLine (formation)
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Low-energy fixed points of random Heisenberg models

2002

The effect of quenched disorder on the low-energy and low-temperature properties of various two- and three-dimensional Heisenberg models is studied by a numerical strong disorder renormalization group method. For strong enough disorder we have identified two relevant fixed points, in which the gap exponent, omega, describing the low-energy tail of the gap distribution, P(Delta) ~ Delta^omega is independent of disorder, the strength of couplings and the value of the spin. The dynamical behavior of non-frustrated random antiferromagnetic models is controlled by a singlet-like fixed point, whereas for frustrated models the fixed point corresponds to a large spin formation and the gap exponent …

PhysicsStatistical Mechanics (cond-mat.stat-mech)Condensed matter physicsInfrared fixed pointFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Type (model theory)Fixed pointRenormalization groupCondensed Matter - Disordered Systems and Neural NetworksOmegaExponentCondensed Matter::Strongly Correlated ElectronsRandomnessCondensed Matter - Statistical MechanicsSpin-½Mathematical physics
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Universality in disordered systems: The case of the three-dimensional random-bond Ising model

2010

We study the critical behavior of the $d=3$ Ising model with bond randomness through extensive Monte Carlo simulations and finite-size scaling techniques. Our results indicate that the critical behavior of the random-bond model is governed by the same universality class as the site- and bond-diluted models, clearly distinct from that of the pure model, thus providing a complete set of universality in disordered systems.

PhysicsStatistical Mechanics (cond-mat.stat-mech)Critical phenomenaMonte Carlo methodFOS: Physical sciencesIsing modelSquare-lattice Ising modelStatistical physicsRenormalization groupScalingRandomnessCondensed Matter - Statistical MechanicsUniversality (dynamical systems)
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Kinetic Roughening in Slow Combustion of Paper

2001

Results of experiments on the dynamics and kinetic roughening of one-dimensional slow-combustion fronts in three grades of paper are reported. Extensive averaging of the data allows a detailed analysis of the spatial and temporal development of the interface fluctuations. The asymptotic scaling properties, on long length and time scales, are well described by the Kardar-Parisi-Zhang (KPZ) equation with short-range, uncorrelated noise. To obtain a more detailed picture of the strong-coupling fixed point, characteristic of the KPZ universality class, universal amplitude ratios, and the universal coupling constant are computed from the data and found to be in good agreement with theory. Below …

PhysicsStatistical Mechanics (cond-mat.stat-mech)PhysicspaperCrossoverFOS: Physical sciencesGeneral Physics and AstronomyDisordered Systems and Neural Networks (cond-mat.dis-nn)Fixed pointRenormalization groupCondensed Matter - Disordered Systems and Neural NetworksKinetic energyNoise (electronics)AmplitudeCondensed Matter::Statistical MechanicsStatistical physicsinterface dynamicsslow combustionkinetic rougheningConstant (mathematics)ScalingCondensed Matter - Statistical MechanicsPhysical Review Letters
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Renormalization group analysis of thermal transport in the disordered Fermi liquid

2014

We present a detailed study of thermal transport in the disordered Fermi liquid with short-range interactions. At temperatures smaller than the impurity scattering rate, i.e., in the diffusive regime, thermal conductivity acquires non-analytic quantum corrections. When these quantum corrections become large at low temperatures, the calculation of thermal conductivity demands a theoretical approach that treats disorder and interactions on an equal footing. In this paper, we develop such an approach by merging Luttinger's idea of using gravitational potentials for the analysis of thermal phenomena with a renormalization group calculation based on the Keldysh nonlinear sigma model. The gravita…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - Mesoscale and Nanoscale PhysicsSigma modelFOS: Physical sciencesPartition function (mathematics)Renormalization groupCondensed Matter Physics5307. Clean energy3. Good healthElectronic Optical and Magnetic MaterialsGravitationCondensed Matter - Strongly Correlated ElectronsThermal conductivityCorrelation functionQuantum mechanicsQuantum electrodynamicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)Fermi liquid theoryQuantumPhysical Review B
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Dynamical Density-Matrix Renormalization Group for the Mott--Hubbard insulator in high dimensions

2004

We study the Hubbard model at half band-filling on a Bethe lattice with infinite coordination number in the paramagnetic insulating phase 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 (FE) approach to the DMFT. In FE-DMFT the onset and the width of the Hubbard bands are adjusted self-consistently but the energies of the bath levels are kept fixed relatively to both band edges during the calculation of self-consistent hybridization strengths between impurity …

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsBethe latticeHubbard modelDensity matrix renormalization groupCoordination numberFOS: Physical sciencesRenormalization groupCondensed Matter PhysicsParamagnetismCondensed Matter - Strongly Correlated ElectronsDensity of statesGeneral Materials ScienceCondensed Matter::Strongly Correlated ElectronsAnderson impurity model
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