Strangeness production in anti-proton annihilation at rest on He-3, He-4 and Ne-20

Balestra, F. ; Batusov, Yu.A. ; Bendiscioli, G. ; et al.
Nucl.Phys.A 526 (1991) 415-452, 1991.
Inspire Record 320088 DOI 10.17182/hepdata.36782

New data are reported on antiproton annihilations at rest with production of Λ and K s 0 , using a streamer chamber with 3 He, 4 He and 20 Ne as gas targets. The data include Λ, K s 0 , ΛK s 0 and K s 0 K S 0 production rates and momentum distributions, π − momentum spectra, mean numbers of charged particles generally and of negatively charged particles separately for different reaction channels. The yields are compared to simple combinatorial calculations based on the extreme assumptions of Λ production via B = 1 or via B = 0 ( K ̄ rescattering) annihilations. Λ and K s 0 momentum spectra are compared to simple model calculations where B = 0 and B = 1 annihilations with and without final-state interactions are considered. A review of existing data on Λ and K s 0 production is presented, showing the dependence on the p ̄ momentum and on the mass number of the target.

6 data tables

No description provided.

No description provided.

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PRODUCTION OF BACKWARD PROTONS IN LAB SYSTEM WITH 0.2-GeV/c - 0.5-GeV/c MOMENTA IN anti-p A INTERACTIONS AT 40-GeV/c

Gabunia, L.L. ; Dzhavrishvili, A.K. ; Ivanova, A.B. ; et al.
Yad.Fiz. 46 (1987) 540-548, 1987.
Inspire Record 236228 DOI 10.17182/hepdata.39002

None

14 data tables

NUCLEUS IS C6J.

NUCLEUS IS C6J.

NUCLEUS IS C6J.

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CHARGED PARTICLE MULTIPLICITIES IN PI-, K- AND ANTI-P INTERACTIONS WITH NUCLEI AT 40-GEV/C

The RISK collaboration Boos, E.G. ; Mosienko, A.M. ; Pokrovsky, N.A. ; et al.
Z.Phys.C 26 (1984) 43-52, 1984.
Inspire Record 214970 DOI 10.17182/hepdata.22350

Interactions of 40 GeV/c πp-,K− and\(\bar p\) on Li, C, S, Cu, CsI and Pb were studied with the RISK-streamer chamber spectrometer. We present multiplicities of negatively charged particles, as well as of protons, and the correlations between them. The normalized mean multiplicity of negative particles,R−, depends on\(\bar v\), the average number of inelastic collisions as\(R^ -= (0.73 \pm 0.04) + (0.34 \pm 0.02)\bar v\). The dependence of the normalized dispersion of negative particles,D−/<N−>, on the number of protons favours independent collision models and contradicts the coherent tube picture. The excess of fast positive particles behaves asA0.4 and shows, for the heavier nuclei, a clear correlation with identified protons.

2 data tables

AVERAGE MULTIPLICITIES OF ALL CHARGED PARTICLES.

AVERAGE MULTIPLICITIES OF ALL NEGATIVELY CHARGED PARTICLES.


CESIUM-IODINE DESIGNATED NUCLEUS.

CESIUM-IODINE DESIGNATED NUCLEUS.

CESIUM-IODINE DESIGNATED NUCLEUS.