• https://doi.org/10.1007/978-94-015-7744-1_4Copy DOI Icon

The relation with statistical physics

  • Jan 1, 1987
  • Peter J. M. Van Laarhoven +1 more
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Abstract

As pointed out in the introduction (chapter 1) there exists a clear analogy between the annealing of solids and the problem of solving large combinatorial optimization problems. The physical annealing process can be successfully modelled by using computer simulation methods from condensed matter physics [BAR76], [WOOD68]. These methods in turn are based on the theory of statistical mechanics which can be viewed as the central discipline of condensed matter physics [BIN78], [TOD83]. Starting off with the first paper on simulated annealing by Kirkpatrick et al. [KIR82], a number of authors elaborate on the relation between combinatorial optimization and statistical mechanics, either because of a phenomenological interest in the analogy (Bernasconi [BER87], Bonomi and Lutton [BON84], Kirkpatrick et al. [KIR82], [KIR83], [KIR85] and Mezard and Parisi [MEZ85], [MEZ86]) or because of a possible framework to model the convergence and the corresponding control of the simulated annealing algorithm (Aarts and Van Laarhoven [AAR85a], [AAR88a], Grest et al. [GRES86], Kirkpatrick et al. [KIR82], [KIR83], Otten and Van Ginneken [OTT84], Randelman and Grest [RAN86] and White [WHI84]). In this chapter a number of quantities are discussed that are defined in the theory of statistical mechanics for the description of a physical many-particle system at equilibrium and it will be elucidated how these quantities are related to the problem of solving large combinatorial optimization problems.

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