Abstract
Multiplicity distributions Ψn(k) in the generalized Feynman gas model of order k (defined by saying that all integrated correlation functions fn except f1,...,fk are zero) are derived and expressed in terms of Poisson distributions with different "average multiplicities", which are related to the integrated correlation functions. The relations between Ψn(k) and Ψn(j) for arbitrary positive integers k,j are found. An intuitive picture to gain a better feeling for these relations is developed. On the basis of our formulae we show that the experimentally observed multiplicity distributions (between 50 GeV/c and 303 GeV/c incoming momentum) can be well reproduced by those of a Feynman gas model of order two. Other applications of our formulae are suggested.
| Original language | English |
|---|---|
| Pages (from-to) | 275-286 |
| Number of pages | 12 |
| Journal | Nuclear Physics, Section B |
| Volume | 56 |
| Issue number | 1 |
| DOIs | |
| State | Published - 21 May 1973 |
| Externally published | Yes |
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