Proton propagation in nuclei studied in the (e,e'p) reaction

Proton propagation in nuclei was studied using the ({ital e},{ital e}{prime}{ital p}) reaction in the quasifree region. The coincidence ({ital e},{ital e}{prime}{ital p}) cross sections were measured at an electron angle of 50.4{degree} and proton angles of 50.1{degree}, 58.2{degree}, 67.9{degree},...

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Veröffentlicht in:Physical review. C, Nuclear physics Nuclear physics, 1992-02, Vol.45 (2), p.780-790
Hauptverfasser: Garino, G, Saber, M, Segel, RE, Geesaman, DF, Gilman, R, Green, MC, Holt, RJ, Schiffer, JP, Zeidman, B, Beise, EJ, Dodson, GW, Hoibråten, S, Pham, LD, Redwine, RP, Sapp, WW, Williamson, CF, Wood, SA, Chant, NS, Roos, PG, Silk, JD, Deady, M, Maruyama, XK
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Sprache:eng
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Zusammenfassung:Proton propagation in nuclei was studied using the ({ital e},{ital e}{prime}{ital p}) reaction in the quasifree region. The coincidence ({ital e},{ital e}{prime}{ital p}) cross sections were measured at an electron angle of 50.4{degree} and proton angles of 50.1{degree}, 58.2{degree}, 67.9{degree}, and 72.9{degree} for {sup 12}C, {sup 27}Al, {sup 58}Ni, and {sup 181}Ta targets at a beam energy of 779.5 MeV. The average outgoing proton energy was 180 MeV. The ratio of the ({ital e},{ital e}{prime}{ital p}) yield to the simultaneously measured ({ital e},{ital e}{prime}) yield was compared to that calculated in the plane-wave impulse approximation and an experimental transmission defined. These experimental transmissions are considerably larger (a factor of {similar to}2 for {sup 181}Ta) than those one would calculate from the free {ital N}-{ital N} cross sections folded into the nuclear density distribution. A new calculation that includes medium effects ({ital N}-{ital N} correlations, density dependence of the {ital N}-{ital N} cross sections and Pauli suppression) accounts for this increase.
ISSN:0556-2813
1089-490X
DOI:10.1103/PhysRevC.45.780