THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS

CLEYMANS J, Satz H (1993)
ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS 57(1): 135-147.

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We provide a method to test if hadrons produced in high energy heavy ion collisions were emitted at freeze-out from an equilibrium hadron gas. Our considerations are based on an ideal gas at fixed temperature T(f), baryon number density n(B), and vanishing total strangeness. The constituents of this gas are all hadron resonances up to a mass of 2 GeV; they are taken to decay according to the experimentally observed branching ratios. The ratios of the various resulting hadron production rates are tabulated as functions of T(f) and n(B). These tables can be used for the equilibration analysis of any heavy ion data; we illustrate this for some specific cases.
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CLEYMANS J, Satz H. THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS. 1993;57(1):135-147.
CLEYMANS, J., & Satz, H. (1993). THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS, 57(1), 135-147.
CLEYMANS, J., and Satz, H. (1993). THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS 57, 135-147.
CLEYMANS, J., & Satz, H., 1993. THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS, 57(1), p 135-147.
J. CLEYMANS and H. Satz, “THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS”, ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS, vol. 57, 1993, pp. 135-147.
CLEYMANS, J., Satz, H.: THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS. 57, 135-147 (1993).
CLEYMANS, J, and Satz, Helmut. “THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS”. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS 57.1 (1993): 135-147.
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