New isomeric transition in Mg36: Bridging the N=20 and N=28 islands of inversion

M. Madurga, J. M. Christie, Z. Xu, R. Grzywacz, A. Poves, T. King, J. M. Allmond, A. Chester, I. Cox, J. Farr, I. Fletcher, J. Heideman, D. Hoskins, A. Laminack, S. Liddick, S. Neupane, A. L. Richard, N. Shimizu, P. Shuai, K. SieglY. Utsuno, P. Wagenknecht, R. Yokoyama

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Abstract

We observed a new isomeric γ transition at 168 keV in Mg36, with a half-life of T1/2=90(-50+410) ns. We propose that the observed transition deexcites a new 0+ isomeric state at 833 keV and populates the previously known first 2+ state. The existence of this isomer is consistent with the predictions of the large-scale shell-model calculations of Mg36 using the sdpf-u-mix interaction. The observed excitation energy of the second 0+ state is caused by the small energy separation between two prolate-deformed configurations where the intruder configuration corresponds to two-neutron excitations from the sd to the pf shell. Within this interpretation, Mg36 becomes the crossing point between nuclei in which ground state deformed/superdeformed configurations are caused by the dominance of N=20 intruders (Mg32,34) and nuclei where deformed configurations are associated with the breaking of the N=28 closure and a large occupancy of the 1p3/2 neutron orbit (Mg38 and beyond). We found the lack of three-body monopole corrections in other effective interactions results in a predominance of N=20 intruder configurations past Mg38 incompatible with our observation. We conclude that Mg36 bridges the N=20 and N=28 islands of inversion, forming the so-called big island of deformation.

Original languageEnglish
Article numberL061301
JournalPhysical Review C
Volume109
Issue number6
DOIs
StatePublished - Jun 2024

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