Investigation of the dynamics of hadron nucleus interactions at 40-GeV by using the features of neutral strange particles.

Akhobadze, K.G. ; Chikovani, L.D. ; Ioramashvili, E.Sh. ; et al.
Phys.Atom.Nucl. 61 (1998) 196-202, 1998.
Inspire Record 442181 DOI 10.17182/hepdata.17088

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5 data tables

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Nuclear dependence of charm production by a 340-GeV pi- beam

The WA82 collaboration Adamovich, M. ; Alexandrov, Yu. ; Antinori, F. ; et al.
Phys.Lett.B 284 (1992) 453-456, 1992.
Inspire Record 334932 DOI 10.17182/hepdata.48417

Charmed mesons, produced on silicon, copper and tungsten by 340 GeV π - , have been identified as peaks in invariant mass distributions. The comparison of the yields of charmed particles originating from interactions in Si, Cu and W allows the mass number dependence of the charm hadroproduction cross section to be measured. Assuming the usual parametrization σ c = σ 0 A α , we find α =0.92±0.06 for charmed mesons with 〈 x F 〉=0.24. We do not find any decrease of α with increasing x F in contrast to the case of the production of particles containing only light quarks.

1 data table

SI, CU, and WT are used. The cross section is parametrized as : SIG = CONST*A**POWER.


Forward Inclusive Production Spectrum of $K(s$), $\Lambda^0$, $\bar{\Lambda}$0, and $n$ in the Collision of 200-{GeV}/$c \pi^-$, $K^-$, $\bar{p}$ and $p$ on Be

Edwards, R.T. ; Devlin, T. ; Edelman, B. ; et al.
Phys.Rev.D 18 (1978) 76, 1978.
Inspire Record 6216 DOI 10.17182/hepdata.24325

We have measured the forward production spectra of various neutral particles produced by π−, K−, p¯, and p at 200 GeV/c, and by π− at 290 GeV/c incident on a Be target. The salient features of these measurements are (1) copious production of KSo at large Feynman xL for incident π− and K−, (2) production of roughly equal fluxes of Λ0 and Λ¯0 for incident π−, and (3) close similarity of the following spectra: π−→n and K−→Λ0; π−→Λ0, π−→Λ¯0, and p→KS0; π−→KS0 and p→Λ0. The overall features of the various distributions seem to agree with the ideas of dimensional counting presented in the constituent-interchange model of quark collisions. Results are presented in terms of the invariant cross section Ed3σ(xL, PT=0)dp3 per Be nucleus for each inclusive reaction.

5 data tables

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