TY - JOUR
T1 - High resolution study of isovector negative parity states in the O16(He3,t)F16 reaction at 140 MeV/nucleon
AU - Fujita, H.
AU - Berg, G. P.A.
AU - Fujita, Y.
AU - Rapaport, J.
AU - Adachi, T.
AU - Botha, N. T.
AU - Fujimura, H.
AU - Fujita, K.
AU - Hara, K.
AU - Hatanaka, K.
AU - Kamiya, J.
AU - Kawabata, T.
AU - Nakanishi, K.
AU - Neveling, R.
AU - Sakamoto, N.
AU - Sakemi, Y.
AU - Shimbara, Y.
AU - Shimizu, Y.
AU - Smit, F. D.
AU - Uchida, M.
AU - Wakasa, T.
AU - Yoshifuku, M.
AU - Yosoi, M.
AU - Zegers, R. G.T.
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2009/2/2
Y1 - 2009/2/2
N2 - The isovector transitions from the ground state (g.s.) of O16 to the negative parity states in F16, i.e., the Jπ=0- g.s., the 0.193 MeV, 1- state, the 0.424 MeV, 2- state, the 0.721 MeV, 3- state, and the 4- "stretched" state at 6.372 MeV, were studied by using a high resolution O16(He3,t)F16 reaction at 140 MeV/nucleon. With the help of high energy resolution, these states were, for the first time, clearly resolved in a charge exchange reaction at an intermediate energy, which favorably excites spin-flip states. Angular distributions of the reaction cross sections were measured in the laboratory frame from 0° to 14°. Parameters of phenomenological effective interactions were derived so as to reproduce these angular distributions in distorted wave Born approximation (DWBA) calculations. The angular distribution of the 0- state could be reproduced well at θc.m.<10°. The empirical values, however, are larger by a factor of 2-2.5 in the larger angle region, where the contribution of the so-called "condensed pion field" is expected. The high resolution also enabled the decay widths of these states to be measured.
AB - The isovector transitions from the ground state (g.s.) of O16 to the negative parity states in F16, i.e., the Jπ=0- g.s., the 0.193 MeV, 1- state, the 0.424 MeV, 2- state, the 0.721 MeV, 3- state, and the 4- "stretched" state at 6.372 MeV, were studied by using a high resolution O16(He3,t)F16 reaction at 140 MeV/nucleon. With the help of high energy resolution, these states were, for the first time, clearly resolved in a charge exchange reaction at an intermediate energy, which favorably excites spin-flip states. Angular distributions of the reaction cross sections were measured in the laboratory frame from 0° to 14°. Parameters of phenomenological effective interactions were derived so as to reproduce these angular distributions in distorted wave Born approximation (DWBA) calculations. The angular distribution of the 0- state could be reproduced well at θc.m.<10°. The empirical values, however, are larger by a factor of 2-2.5 in the larger angle region, where the contribution of the so-called "condensed pion field" is expected. The high resolution also enabled the decay widths of these states to be measured.
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U2 - 10.1103/PhysRevC.79.024314
DO - 10.1103/PhysRevC.79.024314
M3 - Article
AN - SCOPUS:61549118457
SN - 0556-2813
VL - 79
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 2
M1 - 024314
ER -