Abstract
In scattering experiments, where the energy resolution is much greater than widths and spacings of the finestructure resonances, the energy averaged cross section is a sum of the direct (DI) and compound nucleus (CN) cross section. The polarization dependent part of the cross section 〈σA〉, which is independent of the CN-scattering, can be used to determine the direct part of the cross section and from that σCN = 6exp − σDI 1). We have investigated the proton induced CN-reactions on the target nuclei 88Sr and 89Y near the lowest isobaric analog resonances (IAR). In this energy region around 5 MeV direct inelastic reactions are strongly reduced due to the Coulomb barrier and the (p,n)-reactions proceed to 3 levels in the residual nuclei 88Y and 89Zr, respectively. Most partial waves have weak or medium absorption, the absorption is strong for the resonant d5/2 partial wave at resonance energy and for the neutron p-waves. The simultaneous description of compound-elastic and (p,n)-cross sections allows a critical test of the various Hauser-Feshbach formulas2, 3) for a situation, where only few channels are open and furthermore weak and strong absorption is present. Recently a similar test of CN-formulas has been made by Genz et al.4) in a many channel case (Ep ≈ 6.1MeV near the S1/2 IAR observed in the (p,po) and (p,n) reactions on88Sr), where the compoundelastic cross section has been extracted from a fluctuation analysis.
Supported by the Deutsche Forschungsgemeinschaft
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Reference
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Kretschmer, W., Graw, G. (1976). Investigation of Compound Nucleus Reactions on the Target Nuclei 88Sr and 89Y with Polarized Protons. In: Grüebler, W., König, V. (eds) Proceedings of the Fourth International Symposium on Polarization Phenomena in Nuclear Reactions. Experientia Supplementum, vol 25. Birkhäuser, Basel. https://doi.org/10.1007/978-3-0348-5506-8_193
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DOI: https://doi.org/10.1007/978-3-0348-5506-8_193
Publisher Name: Birkhäuser, Basel
Print ISBN: 978-3-0348-5507-5
Online ISBN: 978-3-0348-5506-8
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