Inclusive ∑±(1385) production inK − p interactions at 110 GeV/c

Inclusive ∑±(1385) production inK − p interactions at 110 GeV/c

S. Banerjee,S. N. Ganguli,A. Gurtu,R. Raghavan,K. Shankar,Y. Goldschmidt-Clermont,R. T. Ross,S. Squarcia,K. Dziunikowska,T. Haupt,P. Girtler,D. Kuhn,G. Koul,Devanand,P. V. K. S. Baba,Gian Singh,K. W. J. Barnham,J. Wells,P. R. S. Wright,F. Mandl,M. Markytan,M. Bardadin-Otwinowska,M. Szczekowski;S. Banerjee;S. N. Ganguli;A. Gurtu;R. Raghavan;K. Shankar;Y. Goldschmidt-Clermont;R. T. Ross;S. Squarcia;K. Dziunikowska;T. Haupt;P. Girtler;D. Kuhn;G. Koul;Devanand;P. V. K. S. Baba;Gian Singh;K. W. J. Barnham;J. Wells;P. R. S. Wright;F. Mandl;M. Markytan;M. Bardadin-Otwinowska;M. Szczekowski;
the european physical journal c 1986 Vol. 31 pp. 409-416
184
szczekowski1986theinclusive

Abstract

Results are presented on inclusive production of ∑+(1385) and ∑−(1385) inK−p interactions at 110 GeV/c. The inclusive and topological cross sections have been estimated and compared with published results at lower energies. The inclusive cross section of ∑+(1385) seems to decrease with c.m. energy, while that of the ∑−(1385) is nearly constant. The mean charged multiplicity associate to Σ(1385) increases with c.m. energy. The ∑+(1385) is produced both in the target fragmentation region and in the central region where ∑−(1385) is predominantly produced in the central region. Approximately 16% of the Λ's stem from the decay of ∑±(1385) and the kinematic distributions of these Λ's are not very different from the inclusive Λ's.

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