TY - JOUR
T1 - In-beam [Formula Presented] spectroscopy of [Formula Presented] with deuteron inelastic scattering using reverse kinematics
AU - Iwasa, N.
AU - Motobayashi, T.
AU - Sakurai, H.
AU - Akiyoshi, H.
AU - Ando, Y.
AU - Aoi, N.
AU - Baba, H.
AU - Fukuda, N.
AU - Fülöp, Z.
AU - Futakami, U.
AU - Gomi, T.
AU - Higurashi, Y.
AU - Ieki, K.
AU - Iwasaki, H.
AU - Kubo, T.
AU - Kubono, S.
AU - Kinugawa, H.
AU - Kumagai, H.
AU - Kunibu, M.
AU - Michimasa, S.
AU - Minemura, T.
AU - Murakami, H.
AU - Sagara, K.
AU - Saito, A.
AU - Shimoura, S.
AU - Takeuchi, S.
AU - Yanagisawa, Y.
AU - Yoneda, K.
AU - Ishihara, M.
PY - 2003
Y1 - 2003
N2 - Excited states of [Formula Presented] were studied in the [Formula Presented] reaction using a radioactive [Formula Presented] beam at [Formula Presented] and a liquid deuterium target. Deexcitation [Formula Presented] rays were measured using a NaI(Tl)-scintillator array in coincidence with scattered [Formula Presented] particles. From [Formula Presented] coincidence analyses, the [Formula Presented] lines at 1.193, 1.715, and 2.696 MeV, which were reported previously but unplaced in the level diagram, were found to be associated with the 3.326-MeV [Formula Presented] line corresponding to the transition from the first [Formula Presented] state to the ground state. This excludes the 1.193-MeV line as a candidate for the transition from the [Formula Presented] state to the second [Formula Presented] state, as suggested by Nummela et al. [Phys. Rev. C 63, 044316 (2001)].
AB - Excited states of [Formula Presented] were studied in the [Formula Presented] reaction using a radioactive [Formula Presented] beam at [Formula Presented] and a liquid deuterium target. Deexcitation [Formula Presented] rays were measured using a NaI(Tl)-scintillator array in coincidence with scattered [Formula Presented] particles. From [Formula Presented] coincidence analyses, the [Formula Presented] lines at 1.193, 1.715, and 2.696 MeV, which were reported previously but unplaced in the level diagram, were found to be associated with the 3.326-MeV [Formula Presented] line corresponding to the transition from the first [Formula Presented] state to the ground state. This excludes the 1.193-MeV line as a candidate for the transition from the [Formula Presented] state to the second [Formula Presented] state, as suggested by Nummela et al. [Phys. Rev. C 63, 044316 (2001)].
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U2 - 10.1103/PhysRevC.67.064315
DO - 10.1103/PhysRevC.67.064315
M3 - Article
AN - SCOPUS:85038974218
VL - 67
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
SN - 0556-2813
IS - 6
ER -