Phys.Rev. C 87, 044328 (2013)

Y.Zheng, G.de France, E.Clement, A.Dijon, B.Cederwall, R.Wadsworth, T.Back, F.Ghazi Moradi, G.Jaworski, B.M.Nyako, J.Nyberg, M.Palacz, H.Al-Azri, G.de Angelis, A.Atac, O.Aktas, S.Bhattacharyya, T.Brock, P.J.Davies, A.Di Nitto, Zs.Dombradi, A.Gadea, J.Gal, P.Joshi, K.Juhasz, R.Julin, A.Jungclaus, G.Kalinka, J.Kownacki, G.La Rana, S.M.Lenzi, J.Molnar, R.Moro, D.R.Napoli, B.S.Nara Singh, A.Persson, F.Recchia, M.Sandzelius, J.-N.Scheurer, G.Sletten, D.Sohler, P.-A.Soderstrom, M.J.Taylor, J.Timar, J.J.Valiente-Dobon, E.Vardaci

γ-ray linear polarization measurements and (g_9/2)^-3 neutron alignment in ⁹¹Ru

NUCLEAR REACTIONS ⁵⁸Ni(³⁶Ar, n2p), E=111 MeV; measured Eγ, Iγ, nγ-, pγ-, αγ-, γγ-coin, γγ(θ)(DCO), γ(θ, lin pol) using the EXOGAM array, Neutron Wall array and the DIAMANT detector system at GANIL facility. ⁹¹Ru; deduced high-spin levels, J, π, multipolarity, configuration. Comparison with semiempirical shell model predictions. ⁵⁸Ni(³⁶Ar, 2pα), (³⁶Ar, 4p), (³⁶Ar, 3p), E=111 MeV; measured γ(θ), γ(lin pol) for selected transitions in ^88,90Mo, ⁹¹Tc.

doi: 10.1103/PhysRevC.87.044328