TY - JOUR
T1 - Electroexcitation of isoscalar states in sup16O
AU - Buti, T. N.
AU - Kelly, J.
AU - Bertozzi, W.
AU - Finn, J. M.
AU - Hersman, F. W.
AU - Hyde-Wright, C.
AU - Hynes, M. V.
AU - Kovash, M. A.
AU - Kowalski, S.
AU - Lourie, R. W.
AU - Murdock, B.
AU - Norum, B. E.
AU - Pugh, B.
AU - Sargent, C. P.
AU - Turchinetz, W.
AU - Berman, B. L.
PY - 1986
Y1 - 1986
N2 - We report high resolution measurements of inelastic electron scattering to all narrow normal-parity states of O16 up to 12.05 MeV, which include states with Jn(Ex MeV): 02+(6.049), 03+(12.049), 11-(7.117), 21+(6.917), 22+(9.845), 23+(11.52), 31-(6.130), 41+(10.356), and 42+(11.097). The measurements were performed primarily at 90°and 160°and span momentum transfers between 0.6 and 2.6 fm-1. Improved line shape fitting techniques have been developed. These are the first electron scattering measurements for the 42+ state and of second form-factor maxima for several states. The form factor for excitation of the 22+ state is strikingly different from that of the other 2+ states and indicates a transition density peaked in the interior. Transition charge densities were extracted from a combined data set that includes earlier electron scattering data renormalized to a recent analysis of elastic scattering from O16. Comparisons have been made with several structure models, including the Brown-Green model, the weak-coupling model, a 2Latin small letter h with stroke shell model, and the tetrahedral alpha-cluster model.
AB - We report high resolution measurements of inelastic electron scattering to all narrow normal-parity states of O16 up to 12.05 MeV, which include states with Jn(Ex MeV): 02+(6.049), 03+(12.049), 11-(7.117), 21+(6.917), 22+(9.845), 23+(11.52), 31-(6.130), 41+(10.356), and 42+(11.097). The measurements were performed primarily at 90°and 160°and span momentum transfers between 0.6 and 2.6 fm-1. Improved line shape fitting techniques have been developed. These are the first electron scattering measurements for the 42+ state and of second form-factor maxima for several states. The form factor for excitation of the 22+ state is strikingly different from that of the other 2+ states and indicates a transition density peaked in the interior. Transition charge densities were extracted from a combined data set that includes earlier electron scattering data renormalized to a recent analysis of elastic scattering from O16. Comparisons have been made with several structure models, including the Brown-Green model, the weak-coupling model, a 2Latin small letter h with stroke shell model, and the tetrahedral alpha-cluster model.
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U2 - 10.1103/PhysRevC.33.755
DO - 10.1103/PhysRevC.33.755
M3 - Article
AN - SCOPUS:0000797187
SN - 0556-2813
VL - 33
SP - 755
EP - 775
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 3
ER -