Search results for " Monte Carlo"

showing 10 items of 400 documents

Structure of metastable 2D liquid helium

2007

We present diffusion Monte Carlo (DMC) results on a novel, superfluid phase in two-dimensional 4He at densities higher than 0.065 A-2, which is very close to the freezing density. The new phase has anisotropic, hexatic orbital order, but the single-particle density remains constant. By increasing density the hexatic superfluid forms a metastable state, which lies above the crystal ground state in energy. This implies that the liquid-solid phase transition takes place in two stages: a second-order phase transition from the isotropic superfluid to the hexatic superfluid, followed by a first-order transition that localizes atoms into the triangular crystal order.

Condensed Matter::Quantum GasesPhase transitionMaterials scienceCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Liquid heliumCondensed Matter::OtherGeneral Physics and AstronomyFOS: Physical scienceslaw.inventionCondensed Matter - Other Condensed MatterSuperfluidityCrystalCondensed Matter::Soft Condensed MatterlawPhase (matter)MetastabilityDiffusion Monte CarloGround stateCondensed Matter - Statistical MechanicsOther Condensed Matter (cond-mat.other)
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Magnetic phase diagram of the anisotropic multi-band Hubbard model

2007

Using quantum Monte Carlo (QMC) simulations we determine the magnetic phase diagram of the anisotropic two-band Hubbard model within the dynamical mean-field theory (DMFT) in the important intermediate-coupling regime. We compare the QMC predictions with exact results from second-order weak-and strong-coupling perturbation theory. We find that the orbital-selective Mott transition (OSMT), which occurs in the fully frustrated case, is completely hidden in the antiferromagnetic (AF) ground state of the model. On the basis of our results, we discuss possible mechanisms of frustration. We also demonstrate the close relationship of the physics of the two-band Hubbard model in the orbital-selecti…

Condensed Matter::Quantum GasesPhysicsHubbard modelCondensed matter physicsQuantum Monte Carlomedia_common.quotation_subjectPhase (waves)FrustrationCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMott transitionAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsPerturbation theoryGround statemedia_commonphysica status solidi (b)
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Néel Transition of Lattice Fermions in a Harmonic Trap: A Real-Space Dynamic Mean-Field Study

2010

We study the magnetic ordering transition for a system of harmonically trapped ultracold fermions with repulsive interactions in a cubic optical lattice, within a real-space extension of dynamical mean-field theory. Using a quantum Monte Carlo impurity solver, we establish that antiferromagnetic correlations are signaled, at strong coupling, by an enhanced double occupancy. This signature is directly accessible experimentally and should be observable well above the critical temperature for long-range order. Dimensional aspects appear less relevant than naively expected.

Condensed Matter::Quantum GasesPhysicsOptical latticeCondensed matter physicsMean field theoryQuantum mechanicsQuantum Monte CarloMonte Carlo methodGeneral Physics and AstronomyAntiferromagnetismObservableFermionNéel temperaturePhysical Review Letters
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Mott transitions in ternary flavor mixtures of ultracold fermions on optical lattices

2009

Ternary flavor mixtures of ultracold fermionic atoms in an optical lattice are studied in the case of equal, repulsive on-site interactions U>0. The corresponding SU(3) invariant Hubbard model is solved numerically exactly within dynamical mean-field theory using multigrid Hirsch-Fye quantum Monte Carlo simulations. We establish Mott transitions close to integer filling at low temperatures and show that the associated signatures in the compressibility and pair occupancy persist to high temperatures, i.e., should be accessible to experiments. In addition, we present spectral functions and discuss the properties of a ``semi-compressible'' state observed for large U near half filling.

Condensed Matter::Quantum GasesPhysicsOptical latticeStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsQuantum Monte CarloFOS: Physical sciencesFermionAtomic and Molecular Physics and OpticsCondensed Matter - Strongly Correlated ElectronsMultigrid methodQuantum Gases (cond-mat.quant-gas)Quantum mechanicsCompressibilityInvariant (mathematics)Condensed Matter - Quantum GasesTernary operationPhysical Review A
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Orbital-selective Mott transitions in two-band Hubbard models

2006

The anisotropic two-orbital Hubbard model is investigated at low temperatures using high-precision quantum Monte Carlo (QMC) simulations within dynamical mean-field theory (DMFT). We demonstrate that two distinct orbital-selective Mott transitions (OSMTs) occur for a bandwidth ratio of 2 even without spin-flip contributions to the Hund exchange, and we quantify numerical errors in earlier QMC data which had obscured the second transition. The limit of small inter-orbital coupling is introduced via a new generalized Hamiltonian and studied using QMC and Potthoff's self-energy functional method, yielding insight into the nature of the OSMTs and the non-Fermi-liquid OSM phase and opening the p…

Condensed Matter::Quantum GasesPhysicsQuantum phase transitionStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsHubbard modelQuantum Monte CarloMonte Carlo methodFOS: Physical sciencesCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMott transitionCondensed Matter - Strongly Correlated Electronssymbols.namesakeSelf-energysymbolsCondensed Matter::Strongly Correlated ElectronsSpin-flipHamiltonian (quantum mechanics)Journal of Magnetism and Magnetic Materials
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Momentum-dependent pseudogaps in the half-filled two-dimensional Hubbard model

2012

We compute unbiased spectral functions of the two-dimensional Hubbard model by extrapolating Green functions, obtained from determinantal quantum Monte Carlo simulations, to the thermodynamic and continuous time limits. Our results clearly resolve the pseudogap at weak to intermediate coupling, originating from a momentum selective opening of the charge gap. A characteristic pseudogap temperature T*, determined consistently from the spectra and from the momentum dependence of the imaginary-time Green functions, is found to match the dynamical mean-field critical temperature, below which antiferromagnetic fluctuations become dominant. Our results identify a regime where pseudogap physics is …

Condensed Matter::Quantum GasesPhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsHubbard modelCondensed Matter - SuperconductivityQuantum Monte CarloFOS: Physical sciencesCharge (physics)FermionCondensed Matter PhysicsCoupling (probability)Electronic Optical and Magnetic MaterialsSuperconductivity (cond-mat.supr-con)MomentumCondensed Matter - Strongly Correlated ElectronsQuantum Gases (cond-mat.quant-gas)Condensed Matter::Strongly Correlated ElectronsStrongly correlated materialCondensed Matter - Quantum GasesPseudogapPhysical Review B
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Efficiency of quantum Monte Carlo impurity solvers for dynamical mean-field theory

2007

Since the inception of the dynamical mean-field theory, numerous numerical studies have relied on the Hirsch-Fye quantum Monte Carlo (HF-QMC) method for solving the associated impurity problem. Recently developed continuous-time algorithms (CT-QMC) avoid the Trotter discretization error and allow for faster configuration updates, which makes them candidates for replacing HF-QMC. We demonstrate, however, that a state-of-the-art implementation of HF-QMC (with extrapolation of discretization delta_tau -> 0) is competitive with CT-QMC. A quantitative analysis of Trotter errors in HF-QMC estimates and of appropriate delta_tau values is included.

Condensed Matter::Quantum GasesPhysicsStrongly Correlated Electrons (cond-mat.str-el)DiscretizationQuantum Monte CarloExtrapolationFOS: Physical sciencesCondensed Matter PhysicsDiscretization errorElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsDynamical mean field theoryImpurityDynamic Monte Carlo methodCondensed Matter::Strongly Correlated ElectronsStrongly correlated materialStatistical physics
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Quantum critical point in a periodic Anderson model

2000

We investigate the symmetric Periodic Anderson Model (PAM) on a three-dimensional cubic lattice with nearest-neighbor hopping and hybridization matrix elements. Using Gutzwiller's variational method and the Hubbard-III approximation (which corresponds to the exact solution of an appropriate Falicov-Kimball model in infinite dimensions) we demonstrate the existence of a quantum critical point at zero temperature. Below a critical value $V_c$ of the hybridization (or above a critical interaction $U_c$) the system is an {\em insulator} in Gutzwiller's and a {\em semi-metal} in Hubbard's approach, whereas above $V_c$ (below $U_c$) it behaves like a metal in both approximations. These prediction…

Condensed Matter::Quantum GasesPhysicsStrongly Correlated Electrons (cond-mat.str-el)Quantum Monte CarloFOS: Physical sciencesCritical value01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityVariational methodQuantum critical pointQuantum mechanics0103 physical sciencesDensity of statesCondensed Matter::Strongly Correlated ElectronsStrongly correlated material010306 general physicsAnderson impurity modelPhysical Review B
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Simulation of Transport in Partially Miscible Binary Fluids: Combination of Semigrandcanonical Monte Carlo and Molecular Dynamics Methods

2004

Binary Fluids that exhibit a miscibility gap are ubiquitous in nature (glass melts, polymer solutions and blends, mixtures of molten metals, etc.) and exhibit a delicate interplay between static and dynamic properties. This is exemplified for a simple model system, the symmetrical AB Lennard-Jones mixture. It is shown how semigrandcanonical Monte Carlo methods, that include A→B (B→A) identity switches as Monte Carlo moves, can yield the phase diagram, the interfacial tension between coexisting phases, and various pair correlation functions and structure factors. In addition to the build-up of long-ranged concentration correlations near the critical point, unmixing is also accompanied by the…

Condensed Matter::Soft Condensed MatterBinodalMolecular dynamicsMaterials scienceCritical point (thermodynamics)Spinodal decompositionMonte Carlo methodDynamic Monte Carlo methodThermodynamicsStatistical physicsPhase diagramMonte Carlo molecular modeling
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Phase transitions in nonadditive hard disc systems: a Gibbs ensemble Monte Carlo Study

2007

we study the properties of a model fluid in two dimensions with Gibbs ensemble Monte Carlo (GEMC) techniques, in particular we analyze the entropy-driven phase separation in case of a nonadditive symmetric hard disc fluid. By a combination of GEMC with finite size scaling techniques we locate the critical line of nonadditivities as a function of the system density, which separates the mixing/demixing regions and compare with a simple analytical approximation.

Condensed Matter::Soft Condensed MatterCanonical ensemblePhysicsPhase transitionCritical lineMonte Carlo methodDynamic Monte Carlo methodStatistical physicsFunction (mathematics)ScalingMixing (physics)
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