Antiproton Production in \(p+A\) Collisions at AGS Energies

Inclusive and semi-inclusive measurements are presented for antiproton (\(\bar{p}\)) production in proton-nucleus collisions at the AGS. The inclusive yields per event increase strongly with increasing beam energy and decrease slightly with increasing target mass. The \(\bar{p}\) yield in 17.5 GeV/c...

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Veröffentlicht in:arXiv.org 2001-07
Hauptverfasser: Chemakin, I, Cianciolo, V, Cole, B A, Fernow, R, Frawley, A, Gilkes, M, Gushue, S, Hartouni, E, Hiejima, H, Justice, M, Kang, J H, Keane, D, Kirk, H, Kreisler, M, Maeda, N, McGrath, R L, Mioduszewski, S, Morrison, D, Moulson, M, Namboodiri, N, Rai, G, Read, K, Remsberg, L, Rosati, M, Shin, Y, Soltz, R, Sorensen, S, Thomas, J, Torun, Y, Winter, D, Yang, X, Zajc, W A, Zhang, Y
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Sprache:eng
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Zusammenfassung:Inclusive and semi-inclusive measurements are presented for antiproton (\(\bar{p}\)) production in proton-nucleus collisions at the AGS. The inclusive yields per event increase strongly with increasing beam energy and decrease slightly with increasing target mass. The \(\bar{p}\) yield in 17.5 GeV/c p+Au collisions decreases with grey track multiplicity, \(N_g\), for \(N_g>0\), consistent with annihilation within the target nucleus. The relationship between \(N_g\) and the number of scatterings of the proton in the nucleus is used to estimate the \(\bar{p}\) annihilation cross section in the nuclear medium. The resulting cross section is at least a factor of five smaller than the free \(\bar{p}-p\) annihilation cross section when assuming a small or negligible formation time. Only with a long formation time can the data be described with the free \(\bar{p}-p\) annihilation cross section.
ISSN:2331-8422
DOI:10.48550/arxiv.0107013