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Pi-minus + p ---> k-neutral + lambda/sigma-neutral associated production in the forward direction at 6,8,10 and 11.2 gev/c

Bertolucci, E. ; Mannelli, I. ; Pierazzini, G. ; et al.

Lett.Nuovo Cim. 2S1 (1969) 149-155, 1969.

Inspire Record 58290 DOI 10.17182/hepdata.37419

None

2 data tables

Table 1

Only statistical errors are given.

Table 2

Only statistical errors are given.

P-P Interactions at 10 GEV/C

Almeida, S.P. ; Rushbrooke, John G. ; Scharenguivel, J.H. ; et al.

Phys.Rev. 174 (1968) 1638-1661, 1968.

Inspire Record 55886 DOI 10.17182/hepdata.5529

About 3700 two-prong and 5600 four-prong events of 10-GeV/c pp interactions in the Saclay 81-cm hydrogen bubble chamber have been measured and analyzed. The reliability of the identification of the different final states has been checked using Monte Carlo-generated events. For the channels accessible to analysis, cross sections and invariant-mass distributions are given. The c.m. angular distributions and the mean values of the transverse momentum for all final-state particles are shown and discussed. Production of Δ++(1236) accounts for about 30% of the cross section σ(pp→pnπ+)=4.1±0.4 mb. About 50% of the cross section σ(pp→ppπ+π−)=2.4±0.2 mb can be accounted for by Δ++ production. Production of nucleon isobars at 1450, 1520, and 1730 MeV and their subsequent decay into pπ+π− are investigated. Their cross sections, t dependences, and branching ratios are determined, using a one-pion-exchange model (OPEM) for calculating the background distributions. The production of resonances decaying into pπ− at 1236, 1500, and 1690 MeV is seen, and cross sections are given. Resonance production in the ppπ+π−π0 and pnπ+π+π− reactions is studied using background curves calculated with a model based on simple parametrizations of the c.m. momentum distributions. The production of nucleon isobars accounts for nearly 100% of these reactions. For the reactions pp→ppω, ppη, and ppf0, the cross sections found are 0.16±0.03, 0.16±0.07, and 0.10±0.04 mb, respectively, corrected for unobserved decay modes. It is shown that most of the gross features of the pion-production reactions can be explained by the OPEM with the form factors of Ferrari and Selleri.

2 data tables

Table 1

No description provided.

Table 2

No description provided.

Differential Pion Charge-Exchange Scattering and $\eta$ Production: $\pi^-+p\to \pi^0 + n$ from 2.4 to 3.8 GeV/c, at 6 GeV/c and at 10 GeV/c, $\pi^-+p\to \eta^0 + n$ at 10 GeV/c

Wahlig, M.A. ; Mannelli, I. ;

Phys.Rev. 168 (1968) 1515-1526, 1968.

Inspire Record 1186784 DOI 10.17182/hepdata.749

Small-angle differential cross sections are presented here for π−+p→π0+n charge-exchange scattering between 2.4 and 3.8 GeV/c. The differential cross section near t=0 displays two minima and one maximum in this momentum interval, reflecting the presence of the N32*(2420), N32*(2850), and N12*(2650) resonances; at larger t values, the cross sections fall off exponentially as a function of t, just as has been previously observed for charge-exchange scattering above 6 GeV/c. The pion-charge-exchange data reported here at 6 and 10 GeV/c extend out to large angles, showing a maximum near t=0, followed by an exponential falloff as e10t, a minimum near −t=0.6 (GeV/c)2, and then a second maximum near −t=1.0 (GeV/c)2. The π−+p→η0+n differential cross section shows a maximum near t=0, followed by an exponential falloff as e4t, much less steep than the π0 slope. These data are compared to our previously published data and to those of the Saclay-Orsay group.

15 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.