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Neutron hole states in sup 89 Zr via the ( rvec p , d ) reaction at 58 MeV

Differential cross-section and vector analyzing-power angular distributions were measured at {ital E}{sub {ital {rvec p}}} =58 MeV for the {sup 90}Zr({ital {rvec p}},{ital d}){sup 89}Zr reaction in the angular range from 6{degree} to 50{degree} and up to 10 MeV excitation energy, with 80 keV energy...

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Bibliographic Details
Published in:Physical review. C, Nuclear physics Nuclear physics, 1991-03, Vol.43:3
Main Authors: Duhamel-Chretien, G., Perrin, G., Perrin, C., Comparat, V., Gerlic, E., Gales, S., Massolo, C.P.
Format: Article
Language:English
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Summary:Differential cross-section and vector analyzing-power angular distributions were measured at {ital E}{sub {ital {rvec p}}} =58 MeV for the {sup 90}Zr({ital {rvec p}},{ital d}){sup 89}Zr reaction in the angular range from 6{degree} to 50{degree} and up to 10 MeV excitation energy, with 80 keV energy resolution. In addition to the transitions to low-lying states, the spectra display strong clusters of states from {ital E}{sub {ital x}}=3.5 to 7 MeV. The observed fine structure was used to define energy bins for which cross sections and analyzing powers were obtained. The latter allowed spin and parity assignments for deep-lying hole states. Spectroscopic factors were deduced from standard distorted-wave Born approximation calculations. From the vector analyzing-power measurements, it was shown that most of the strength observed above 3.5 MeV belongs to the 1{ital f}{sub 7/2} inner neutron hole orbital.
ISSN:0556-2813
1089-490X
DOI:10.1103/PhysRevC.43.1116