Shell model isomers near Z = 64, N = 82: g-factors of Yrast states in 146Gd and 147Gd

Böhn, H.; Feilitzsch, F. von; Sunyar, A.W.; Broda, R.; Kleinheinz, P.; Ogawa, Masahiro

doi:10.1016/0370-2693(79)90195-3

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1994

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Cited by 13 publications

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“…43 (2) 4o (2) 91(4) 32(2) 41(2) 37(2) 6o (4) 96(6)' 32 (2) 43(s)' 341 (30) 16o(io)' si{v)' 24(v)' iis(s) 57(3) csv (22) 72 (3) is2 ( (21) io2 (6) 1S2 (9) 624 (28) svs (25) 511 (23) 180{8)…”

Section: Experimental Techniques and Data Analysisunclassified

Evidence for single particle structure of high spin states inPm144andPm<

et al. 1993

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Excited states of the Z = 61 isotopes Pm83 and Pm84 have been studied in the F + Te reaction at a beam energy of 85 MeV. Gamma-ray and conversion electron spectroscopy were used to establish the high spin states of Pm up to spin 20h and to extend the level spectrum of Pm up to a tentative spin of 2 h. Empirical shell model calculations in a configuration space truncated to the vr 1hiiy2, vr 1g~&'2, and vr 2d5&~p rotons and the v 2f7y2 neutron outside the ' Gd core reproduce the observed energy levels in good agreement with the experimental results. (nhiig2) configurations are suggested in an N = 83 isotone for Z (64.PACS number(s): 23.20.En, 23.20.Lv, 23.20.Nx, 27.60. +j

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“…43 (2) 4o (2) 91(4) 32(2) 41(2) 37(2) 6o (4) 96(6)' 32 (2) 43(s)' 341 (30) 16o(io)' si{v)' 24(v)' iis(s) 57(3) csv (22) 72 (3) is2 ( (21) io2 (6) 1S2 (9) 624 (28) svs (25) 511 (23) 180{8)…”

Section: Experimental Techniques and Data Analysisunclassified