Abstract
The change in an observable due to collisions is written, using near classical collision theory, as a simple average over the initial internal state. For most observables of physical interest this average assumes the usual form of a classical phase average. The most valid means of characterizing the distribution of final states is in terms of its moments.
Original language | English |
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Pages (from-to) | 1633-1637 |
Number of pages | 5 |
Journal | The Journal of Chemical Physics |
Volume | 56 |
Issue number | 4 |
DOIs | |
State | Published - 1972 |
Externally published | Yes |