By D. P. Landau, S. P. Lewis, H.-B. Schüttler
This quantity is a standing record according to the displays and discussions that came about throughout the twelfth Annual Workshop on laptop Simulation stories in Condensed topic Physics on the middle for Simulation Physics on the college of Georgia in March 1999. It presents a wide evaluation of the latest advancements within the box, spanning a variety of topical parts in simulational condensed subject physics. those parts contain contemporary advancements in simulations of classical statistical mechanics types, digital constitution calculations, quantum Monte Carlo simulations and simulations of polymers. New actual effects and novel simulation and information research tools are presented.
Read or Download Computer Simulation Studies in Condensed-Matter Physics XII: Proceedings of the Twelfth Workshop, Athens, GA, USA, March 8–12, 1999 PDF
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Extra resources for Computer Simulation Studies in Condensed-Matter Physics XII: Proceedings of the Twelfth Workshop, Athens, GA, USA, March 8–12, 1999
The method retains many of the advaritages of the standard formalism. ations. With the second-quantization representation, it also automatically accounts for particle permutations. Both diagonal and off-diagonal expectations are easily computed, as well as imaginary-time correlation functions. Below we first recapitulate the formalism of Blankenbecler, Scalapino, and Sugar (BSS) [4,6]' in a way that will facilitate our introduction of the new method. We then discuss the new method and present some benchmark data.
As a specific application we discuss the implications of the efficient screening for the superconductivity in the doped Fullerenes. In the Monte Carlo calculations we use trial functions with two Gutzwiller-type parameters. To deal with such trial functions, we introduce a method for efficiently optimizing the Gutzwiller parameters, both in variational and in fixed-node diffusion Monte Carlo. 1 Introduction The random phase approximation (RPA) is widely used throughout solid state physics. It properly describes the screening when the kinetic energy is much larger than the Coulomb energy.
The New Finite-T Method The implicit nature of the formalism above poses difficulties in understanding how to control the sign problem. Paths in the grand-canonical formulation, contrary to ground-state projector QMC, do not originate or end at a single explicit point in Slater determinant space. Instead they involve many points, due to the trace over states with varying number of particles. " A straightforward application of the ideas from ground-state CPMC[8,9] would require separate constraining conditions for paths with different end points.