Abstract

The results of the microscopic transport calculations of -nucleus interactions within a GiBUU model are presented. The dominating mechanism of hyperon production is the strangeness exchange processes → γπ and → ΞK. The calculated rapidity spectra of Ξ hyperons are significantly shifted to forward rapidities with respect to the spectra of S = −1 hyperons. We argue that this shift should be a sensitive test for the possible exotic mechanisms of -nucleus annihilation. The production of the double Λ-hypernuclei by Ξ− interaction with a secondary target is calculated.

Highlights

  • The interest to strangeness production in p-nucleus interactions was originally related to the mechanism of strangeness enhancement in a quark-gluon plasma (QGP) proposed by Rafelski and Muller in early 80’s for relativistic heavy-ion collisions [1]

  • The following-up theoretical analyses within the intranuclear cascade (INC) models [6,7] seem to support the usual mechanism of strangeness production in terms of binary hadron-hadron collisions, the collected experimental data constitute a very useful base for testing newly developing theoretical models needed in view of forthcoming experiments with antiproton beams at FAIR

  • In this talk we discuss our recent results of the microscopic transport calculations of the KS0, Λ- and Ξ−-hyperon and double-Λ hypernuclei production based on the Giessen BoltzmannUehling-Uhlenbeck (GiBUU) transport model

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Summary

Introduction

The interest to strangeness production in p-nucleus interactions was originally related to the mechanism of strangeness enhancement in a quark-gluon plasma (QGP) proposed by Rafelski and Muller in early 80’s for relativistic heavy-ion collisions [1]. The following-up theoretical analyses within the intranuclear cascade (INC) models [6,7] seem to support the usual mechanism of strangeness production in terms of binary hadron-hadron collisions, the collected experimental data constitute a very useful base for testing newly developing theoretical models needed in view of forthcoming experiments with antiproton beams at FAIR.

Results
Conclusion

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