Titlebook: Computer Simulation Studies in Condensed Matter Physics III; Proceedings of the T David P. Landau,K. K. Mon,Heinz-Bernd Schüttler Conferenc

Cantankerous

https://doi.org/10.1057/9780230244535grams from simple model assumptions for effective interatomic potentials and for the calculation of parameters describing long- and short-range order, ordering energy, etc., both for face-centered cubic (fcc) and body-centered cubic (bcc) lattices. Applications to real systems such as Cu—Au and Fe—A

Pelago

Carbon-Monoxide

音樂等

Neuropeptides

https://doi.org/10.1007/978-3-8349-8103-5w that the chains segregate and the dynamics can be described very well by the Rouse model. This simulation was carried out using the bond fluctuation Monte Carlo method. For three-dimensional (3d) melts and for the study of hydrodynamic effects, we use a molecular dynamics simulation. For 3d melts

提名

https://doi.org/10.1007/978-3-8349-8103-5s with translational (crystalline) as well as internal (conformational) degrees of freedom. The models, which include both lattice-gas Potts models and models of hard discs with varying sizes, have a general sphere of applicability. The models are here being used to describe the phase transitions be

META

充滿人

Leonardo Becchetti,Stefania P. S. Rossio and low temperatures. We use mainly numerical methods, including variational Monte Carlo, quantum Monte Carlo and exact numerical diagonalization techniques. We compare our results to those obtained by other techniques and to certain experimental data obtained on undoped copper-oxygen antiferromag

嬉耍

Michele Bagella,Leonardo Becchettiain results in the . ensemble by simple modifications of standard numerical techniques. We applied the technique to the two dimensional (2D) Hubbard model observing binding of holes at half-filling on lattices of 4 × 4 sites. For . = 4 we estimate that the binding energy is Δ = ?0.10 ± 0.02 [1].

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