1958
DOI: 10.1007/bf02828860
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About high energy interactions in nuclear emulsions

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1963
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Cited by 113 publications
(16 citation statements)
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“…• their 'thermal behaviour' and thus their accessibility to statistical thermodynamical descriptions, 14 • the existence of clusters (fireballs), • the production rates of particles and their typical multiplicity distributions, • large-angle elastic scattering,…”
Section: Resultsmentioning
confidence: 99%
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“…• their 'thermal behaviour' and thus their accessibility to statistical thermodynamical descriptions, 14 • the existence of clusters (fireballs), • the production rates of particles and their typical multiplicity distributions, • large-angle elastic scattering,…”
Section: Resultsmentioning
confidence: 99%
“…Cerulus [32] had used a very elegant group theoretical method to solve the problem of charge distribution, and then employed the same method to implement angular momentum conservation in phase space [33], in the hope of reproducing the known anisotropy. It failed (because it required more computing than was then possible and also) because the process was not so statistical as we had hoped: angular momentum conservation could not produce the pronounced anisotropy found in cosmic ray events and well accounted for by two-centre models [11,14]-a fact strongly suggesting that phase relations between partial waves survived the statistical mixing assumed in the Fermi model. In principle we had the tools to build and correctly evaluate a two-centre model, but it would have required at least ten times more computing (summing over impact parameters with varying fireball energies), which was impossible (we had already spent several years to do all the computing for single fireballs).…”
Section: The Cern Statistical Model (1958-1962)mentioning
confidence: 98%
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