Final states with three charged particles and a visible lambda from k- d interactions at 4.5 gev/c

Amman, A.C. ; Carmony, D.D. ; Garfinkel, A.F. ; et al.
Phys.Rev.D 7 (1973) 1345-1361, 1973.
Inspire Record 82333 DOI 10.17182/hepdata.22153

This report concerns itself with the study of four- or five-body final states produced by the interaction of 4.48-GeV/c K− mesons on neutrons. The data result from a 372 000-picture exposure in the Argonne National Laboratory 30-in. deuterium-filled bubble chamber. The reactions studied include (1) K−n→Λπ+π−π−, (2) K−n→Σ0π+π−π−, (3) K−n→Λπ+π−π−π0, (4) K−n→Λπ+π−π−MM, (5) K−n→Λπ−K+K−, and (6) K−n→Λπ−KL0KS0, where all the Λ particles decayed visibly. Evidence is presented for the existence of the Σ(1640) whose mass and width are 1642 ± 12 MeV/c2 and 55 ± 24 MeV/c2, respectively. The branching ratios are found to be consistent with an octet assignment. The A2 data are presented and are compatible with JPC=2++. In addition, the productions of ρ0, ω, and φ0 are discussed in conjunction with simultaneous Σ−(1385) production and the results are compared with quark-model predictions.

2 data tables

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Measurement of the proton-antiproton total annihilation cross section at low energy

Cline, D. ; English, J. ; Reeder, D.D. ;
Phys.Rev.Lett. 27 (1971) 71-74, 1971.
Inspire Record 68958 DOI 10.17182/hepdata.21462

The p¯p total inelastic cross section has been measured in a hydrogen bubble chamber for p¯ momenta from 100 to 550 MeV/c. Below 200 MeV/c the cross section increases rapidly to several barns. From this behavior it is inferred that high partial waves, perhaps to L=3, are important in the annihilation at the lowest momenta studied. An abrupt change in the momentum dependence of the total absorption cross section occurs at about 350 MeV/c in the vicinity of previously observed structure in backward elastic scattering.

5 data tables

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