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Canonical strangeness and distillation effects in hadron production

V D Toneev1,2 and A S Parvan2,3

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The strangeness canonical ensemble for Maxwell–Boltzmann statistics is reconsidered for excited nuclear systems with non-vanishing net strangeness. A new recurrence relation method is applied to find the partition function. The method is first generalized to the case of quantum strangeness canonical ensemble. Uncertainties in the calculation of the K++ excitation function are discussed. A new scenario based on the strangeness distillation effect is put forward for a possible explanation of anomalous strangeness production observed at the bombarding energy ~30 GeV. The peaked maximum in the K++ ratio is considered as a sign of the critical endpoint reached in evolution of the system rather than a latent heat jump emerging from the onset of the first-order deconfinement phase transition.


PACS

25.75.Nq Quark deconfinement, quark–gluon plasma production, and phase transitions

23.20.Lv gamma transitions and level energies

24.10.Pa Thermal and statistical models

25.75.Dw Particle and resonance production

Subjects

Nuclear physics

Dates

Issue 7 (July 2005)

Received 1 December 2004

Published 21 April 2005



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