2002
DOI: 10.1016/s0375-9474(02)00658-9
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Asymmetries between strange and antistrange particle production in pion–proton interactions

Abstract: Recent measurements of the asymmetries between Feynman x distributions of strange and antistrange hadrons in π − A interactions show a strong effect as a function of x F . We calculate strange hadron production in the context of the intrinsic model and make predictions for particle/antiparticle asymmetries in these interactions.

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Cited by 3 publications
(14 citation statements)
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“…The apparent difficulties with uncorrelated fragmentation seen in Ref. [28] are confirmed here. Thus coalescence production is the most effective mechanism for strange hadron production in the intrinsic model.…”
Section: Discussionsupporting
confidence: 81%
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“…The apparent difficulties with uncorrelated fragmentation seen in Ref. [28] are confirmed here. Thus coalescence production is the most effective mechanism for strange hadron production in the intrinsic model.…”
Section: Discussionsupporting
confidence: 81%
“…We treat the strange quark as heavy, as in Ref. [28], rather than as a massless parton in jet-like processes. Treating the strange quark as a jet means selecting a minimum p T to keep the cross section finite.…”
Section: Leading-twist Productionmentioning
confidence: 99%
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“…In spite of this uncertainty, the existing experience in the literature is encouraging. In [27] the authors used (15) to compute the cross section of strange particle production and calculated the asymmetries in the production of K + /K − , Λ/Λ, .…”
Section: A T 4cmentioning
confidence: 99%
“…In spite of this uncertainty, the existing experience in the literature is encouraging. In [24] the authors used (16) to compute the cross section of strange particle production and calculated the asymmetries in the production of K + /K − , Λ/Λ, ...etc. They have used the convolution formula of the parton model and have taken the strange quark mass to be m s 500 MeV.…”
Section: The Production Cross Sectionmentioning
confidence: 99%