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Direct observation of the giant dipole resonance of sup 16 O via electromagnetic dissociation

We have measured the invariant-mass spectrum of the final-state {sup 15}N+{ital p} system in the reaction {ital T}({sup 16}O,{sup 15}N+{ital p}){ital X} at 2.1{ital A} GeV with Be, Cu, and U targets ({ital T}). Electromagnetic dissociation of the {sup 16}O projectile nucleus in the Coulomb field of...

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Bibliographic Details
Published in:Physical review. C, Nuclear physics Nuclear physics, 1991-11, Vol.44:5
Main Authors: Olson, D.L., Baumgartner, M., Greiner, D.E., Lindstrom, P.J., Symons, T.J.M., Wada, R., Webb, M.L., Berman, B.L., Crawford, H.J., Engelage, J.M.
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Language:English
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Summary:We have measured the invariant-mass spectrum of the final-state {sup 15}N+{ital p} system in the reaction {ital T}({sup 16}O,{sup 15}N+{ital p}){ital X} at 2.1{ital A} GeV with Be, Cu, and U targets ({ital T}). Electromagnetic dissociation of the {sup 16}O projectile nucleus in the Coulomb field of the target nucleus produces two prominent peaks in the proton-energy spectrum, one at 9 MeV, from transitions to the ground state of the residual {sup 15}N nucleus, and the other at 4 MeV, from transitions to excited states. This is corroborated by {gamma} rays corresponding to the deexcitation of the {sup 15}N nucleus which are in coincidence with the 4-MeV peak and are suppressed for the 9-MeV peak. Nucleon-nucleus diffractive dissociation makes a significant contribution to the cross section and results in a peak at 1.5 MeV. Nucleon-nucleon quasielastic scattering results in a featureless high-energy tail above 20 MeV.
ISSN:0556-2813
1089-490X
DOI:10.1103/PhysRevC.44.1862