Partial-wave analysis in the Q region of (ππ)- systems produced in K-p reactions at 4.2 GeV/c
Nuclear Physics, Section B 158:2-3 (1979) 265-279
Abstract:
A partial-wave analysis and an isospin analysis are presented of the (Kππ)- systems produced in the reactions K-p→K-π-π+ and K-p→K0π-π-p u sing the high-statistics bubble-chamber data at 4.2 GeV/c. The energy dependence of JP = 1+ waves is investigated in a comparison with results at higher energy. The dominant 1+0+ (K*π) with its maximum in the Q2 (1.4 GeV) region is an almost pure I = 1 2 state. The energy dependence of 1+0+ (K*π) at low masses is consistent with pomeron exchange while at higher masses (including the Q2 region) other natural exchanges are involved. The 1*1+ (Kρ{variant}) has its maximum at about 1.3 GeV. The relative phase between these two 1+ states is consistent with Q1-Q2 contribution to the 1+ state. Properties of the Q resonances are obtained in a fit of a two-resonance model to the 1+ date. There is no clear evidence for the 0- resonance seen at SLAC. © 1979.Production and decay properties of the D(1285) meson in K-p interactions at 4.2 GeV/c
Nuclear Physics, Section B 151:C (1979) 181-192
Abstract:
We have studied the production and decay of the D(1285) meson in the reaction K-p→ ΛD at an incident K- momentum of 4.2 GeV/c. The cross section for this reaction is 11 ± 3 μb and the branching ratios D→ KKπ/D → ηππ and D → 4π/D → ηππ are found to be 0.42 ± 0.15 and 0.7 ± 0.5, respectively. The proportion of D → ηπ+π- going through the intermediate δ±π∓ states is 0.72 ± 0.15. Forward and backward exchange mechanisms are found to contribute in the ratio 3 : 2. © 1979.Test of an additive diquark spectator model for meson-baryon quasi-two-body reactions
Physical Review D 19:3 (1979) 820-837
Abstract:
An additive diquark model is proposed to relate the forward cross sections of meson-baryon quasi-two-body reactions. The model consists of a quark-diquark structure for baryons combined with additivity of quark-(di)quark amplitudes. Good agreement is found between this model, which contains only one free parameter, and a large body of experimental data for charge-exchange and strangeness-exchange meson-baryon two-body reactions. This is in contrast to the SU(6)-symmetric additive quark model which disagrees violently with the data. © 1979 The American Physical Society.KBAR-K AND PBAR-P OFF-SHELL ANNIHILATIONS FROM K-+P-]LAMBDAL+PIONS AT 4.2 GEV-C
ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS 1:1 (1979) 3-17
PRODUCTION AND DECAY PROPERTIES OF THE D(1285) MESON IN K-P INTERACTIONS AT 4.2 GEV-C
NUCLEAR PHYSICS B 151:2 (1979) 181-192