Phys.Rev. C 104, 064605 (2021)

W.Liu, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, S.M.Wang, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, B.L.Xia

s- and d-wave intruder strengths in ¹³B_g.s. via the ¹H(¹³B, d)¹²B reaction

NUCLEAR REACTIONS ¹H(¹³B, p), (¹³B, d)¹²B, E=23 MeV/nucleon, [¹³B secondary beam from ⁹Be(¹⁸O, X), E=58 MeV/nucleon]; measured reaction products, E(d), I(d), E(p), I(p), σ(θ), (particle)(particle)-coin using four sets of charged-particle telescopes of double-sided silicon strip (DSSD) detectors at RCNP-Osaka accelerator facility. ^12,13B; analyzed optical potential parameters for low energy elastic scattering and single-neutron transfer reaction. ¹³B; deduced levels, J, π, L-transfers from σ(θ) distributions relative spectroscopic factors, s- and d-wave intruder strengths in the ground state; calculated p-, s-, and d-wave intensities from the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach. Comparison with systematics of p-, s-, and d-wave intensities in the ground state of ¹²Be, ¹³B and ¹⁴C.

doi: 10.1103/PhysRevC.104.064605