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High order entropies in zero external field

Substituting for the various quantities with R=0 in the expression for tex2html_wrap_inline14531 and simplifying we find
equation2383
where tex2html_wrap_inline14533 and tex2html_wrap_inline14535 are defined as
 eqnarray2392
In terms of the R=0 value of tex2html_wrap_inline14539 (see equation 6.23) we have
 equation2403
From equation 6.30 we see that the entropy per spin decreases as the order increases, consistent with the reduced entropy per degree of freedom theorem of chapter 2. From the form of equation 6.30 it is implied that the change in entropy with changes in the average energy (or any parameter) decreases in magnitude as the order increases. Thus it is important to observe the high-order structure indicated by the high order entropy in order to understand the creation of that structure as the average energy changes. In fact, since tex2html_wrap_inline14541 (see chapter 10, equation 10.22), note that
equation2733
Note the extremely simple k-dependence of the kth order entropy tex2html_wrap_inline14531. Note that the quantities tex2html_wrap_inline14533 and tex2html_wrap_inline14535 obey
equation2420
so that they may be interpreted as probabilities, and referring to equation 6.5 we see that tex2html_wrap_inline14533 and tex2html_wrap_inline14535 are the probabilities that any two neighboring spins are the same and different respectively. Note that tex2html_wrap_inline14557.

Note that all derivatives of tex2html_wrap_inline14531 with respect to system parameters or variables have the same functional dependence on system parameters up to the factor 1-1/k.



David Wolf
Tue Mar 25 08:11:49 CST 1997