By Landau D.P., Binder K.

Facing all features of Monte Carlo simulation of advanced actual platforms encountered in condensed-matter physics and statistical mechanics, this e-book presents an advent to desktop simulations in physics. This variation now includes fabric describing robust new algorithms that experience seemed because the earlier version was once released, and highlights contemporary technical advances and key purposes that those algorithms now make attainable. Updates additionally contain a number of new sections and a bankruptcy at the use of Monte Carlo simulations of organic molecules. in the course of the publication there are numerous purposes, examples, recipes, case stories, and workouts to aid the reader comprehend the fabric. it really is perfect for graduate scholars and researchers, either in academia and undefined, who are looking to examine strategies that experience develop into a 3rd device of actual technology, complementing test and analytical conception

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**Additional info for A Guide to Monte Carlo Simulations in Statistical Physics**

**Example text**

In Fig. 3 we show characteristic behavior for both kinds of phase transitions. At a first order phase transition the free energy curves for ordered and disordered states cross with a finite difference in slope and both stable and metastable states exist for some region of temperature. In contrast, at a second order transition the two free energy curves meet tangentially. 4 Phase diagrams Phase transitions occur as one of several different thermodynamic fields is varied. Thus, the loci of all points at which phase transitions occur form phase boundaries in a multidimensional space of thermodynamic fields.

More sophisticated, high quality generators, such as RANLUX (James, 1994; Lu¨scher, 1994) which is based upon an algorithm by Marsaglia and Zaman (1991), are finding their way into use, but they are slow and must still be carefully tested with new algorithms as they are devised. (RANLUX includes two lags, plus a carry, plus it discards portions of the sequence of generated numbers. 5 Suppose we have a computer with 4 bit words. Produce a sequence of random numbers using a congruential generator.

Most notable are two-dimensional XY-models with Hamiltonian X H ¼ ÀJ ðSix Sjx þ Siy Sjy Þ; ð2:26Þ nn where Si is a unit vector which may have either two components (plane rotator model) or three components (XY-model). These models develop no long range order at low temperature but have topological excitations, termed vortex–antivortex pairs, which unbind at the transition temperature TKT (Kosterlitz and Thouless, 1973). g. $ / expða"À# Þ; ð2:27Þ and every temperature below TKT is a critical point.