By R. Balescu, J. L. Lebowitz, I. Prigogine, P. Resibois, Z. Salsburg, W. C. Schieve, M. G. Velarde, A. P. Grecos
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Shall present x = {pN,qN} be a point distribution functions properly = e B o. 20) space. and g(x) due Then both to Isihara consider of w h i c h [33]. zz) , distribution functions. Next and normalized fS(x)dx which ' as o Then using we start with the 60 - $S(x) I n g ( x ) d x J = fS(x) i n S ( x ) d x = $g{ ! ins g = This proves Sg{i in/ g To c o n v e r t - ! 22). 26) o where A is the free energy for the h a m i l t o n i a n o H . 27) Then >
20) space. and g(x) due Then both to Isihara consider of w h i c h [33]. zz) , distribution functions. Next and normalized fS(x)dx which '
44 (b) A model of two-dimensional polymer crystalization. was solved exactly by Zwanzig and Lauritzen 5. Rigorous Results [29]. of a General Nature In the last decade the theory of Phase Transitions characterized analysis more and more by careful of a general recent developments Lebowitz sort. has been and rigorous mathematical Particularly pertinent (see for other details are two fairly the lectures by Professor and also ref. 8). (a) Some general proofs transitions. lattice This The results systems.