Measure Theoretic Foundations of Statistical Mechanics

Cover Measure Theoretic Foundations of Statistical Mechanics
Measure Theoretic Foundations of Statistical Mechanics
Robert M Lewis
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Then T. Will no longer be given by (i*^l), nor, in general, will T be measure-preserving with respect to (P, (^, m), nor will all the y', y" be invariants of T. .
J J t However, if the magnitvide of the physical interaction is small, we may suppose that some of the above features are preserved. Oliis leads to the definition of "weak interaction" given in the previous section. We assume that ( P, ^, m, T^, y) is a complete space where (1, 2) y = {yr"-yk] =y' + y" • Some of the requirements of th
...e definition of weak interaction, in particular (^2), may be met only in an approximate sense* .
One further physical condition must be met before we can apply our theory: P must be "large" compared to P . By this we mean that the behavior of the system P is not appreciably affected by its interaction with P . In particular, the value of y «= y" + y" is not appreciably affected by fluctuations Urns, e. G. , there may be some " interaction parameter", £, and (^2) may be an asymptotic relation valid for € ■> 0.


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