Computer Simulation Studies in Condensed Matter Physics III: by D. P. Landau, K. K. Mon, H.-B. Schüttler (auth.), Professor

By D. P. Landau, K. K. Mon, H.-B. Schüttler (auth.), Professor David P. Landau Ph.D, Professor K. K. Mon Ph.D, Professor Heinz-Bernd Schüttler Ph.D (eds.)

The contribution of laptop simulation reviews to our knowing of the prop­ erties of a variety of condensed subject platforms is now weIl validated. the heart for Simulational Physics of the collage of Georgia has been internet hosting a chain of annual workshops with the reason of bringing jointly skilled prac­ titioners within the box, as weIl as relative novices, to supply a discussion board for the alternate of rules and up to date effects. This year's workshop, the 3rd within the sequence, used to be held February 12-16, 1990. those complaints are arecord of the workshop and are released with the objective of well timed dissemination of the papers to a much wider viewers. The complaints are divided into 4 components. the 1st includes invited pa­ pers facing simulational experiences of classical platforms and likewise contains an advent to a couple new simulation suggestions. Aseparate part is dedicated to invited papers on quantum structures, together with new effects for strongly correlated electron and quantum spin types believed to be very important for the outline of high-Tc superconductors. The 3rd half includes a unmarried invited paper, which offers a accomplished therapy of matters linked to excessive perfor­ mance computing, together with transformations in architectures and a dialogue of entry recommendations. The contributed papers represent the ultimate part.

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Extra resources for Computer Simulation Studies in Condensed Matter Physics III: Proceedings of the Third Workshop Athens, GA, USA, February 12–16, 1990

Example text

Writing the spinodal value of tP obtained from eq. p (9) Inserting eq. 9 into eq. h = h. - h where h. is the value of the magnetic field at the spinodal. h < < 1.

Although this system is quite simple, and has been solved exactly [25], we chose to simulate it [26] because it possesses some of the important properties of more realistic dimer and polymer models. The most important property is the presence of "hard" (excluded volume) interactions in this model. Unlike spin systems, where the energy cost for flipping a spin is of the order of kB T c near the phase transition, dense polymer systems contain interactions, arising when two particles attempt to occupy the same volume, that are very large compared to kBTc' In this dimer model, we assign an infinite energy to configurations in which two dimers attempt to occupy the same lattice site.

Conclusions We have presented an overview of the use of histogram techniques in the study of critical phenomena. Although these methods have been known for more than thirty years, they have only recently been applied with success to the study of critical phenomena. It is hoped that the current interest in these methods will lead to further refinements and the development of even more efficient uses of simulation data. The author wishes to acknowledge fruitful collaboration with C. G. F. Nagle, P.

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