Mechanisms of cumulative-proton production in pion-nucleus interactions at 5 GeV/c. Phenomenological analysis
O.B. Abdinov, A.A. Bairamov, Yu.A. Budagov, А.М. Дворник, Yu.F. Lomakin, A.A. Mailov, V.B. Flyagin, Y. N. Kharzheev
Abstract
O.B. Abdinov, A.A. Bairamov, Yu.A. Budagov, А.М. Дворник, Yu.F. Lomakin, A.A. Mailov, V.B. Flyagin, Y. N. Kharzheev
Abstract
We have obtained the contributions of individual mechanisms to the production of cumulative protons in C interactions at 5 GeV/c in the framework of the cascade-evaporative model. Independently we have evaluated from experiment the contribution of the reaction ''d'' parrow-down/sub back/ p to the production of cumulative protons sigma = 1.5 +- 0.4 mb. We have obtained the separation angle of the two protons (one of which is emitted into the backward hemisphere in the lab) as a function of the sum of their kinetic energies T/sub 2p/ in pion-carbon and pion-Freon (A-barroughly-equal24) interactions. In the region 0.19 < T/sub 2p/ < 0.26 GeV we observe a characteristic maximum due to the absorption of slow pions.
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We have obtained the contributions of individual mechanisms to the production of cumulative protons in C interactions at 5 GeV/c in the framework of the cascade-evaporative model. Independently we have evaluated from experiment the contribution of the reaction ''d'' parrow-down/sub back/ p to the production of cumulative protons sigma = 1.5 +- 0.4 mb. We have obtained the separation angle of the two protons (one of which is emitted into the backward hemisphere in the lab) as a function of the sum of their kinetic energies T/sub 2p/ in pion-carbon and pion-Freon (A-barroughly-equal24) interactions. In the region 0.19 < T/sub 2p/ < 0.26 GeV we observe a characteristic maximum due to the absorption of slow pions.
Key concepts: Pion, Physics, Nuclear physics, Freon, Proton, Cascade, Production (economics), Particle physics