1. New isomeric transition in $^{36}$Mg: Bridging the N=20 and N=28 islands of inversion
- Author
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Madurga, M., Christie, J. M., Xu, Z., Grzywacz, R., Poves, A., King, T., Allmond, J. M., Chester, A., Cox, I., Farr, J., Fletcher, I., Heideman, J., Hoskins, D., Laminack, A., Liddick, S., Neupane, S., Richard, A. L., Shimizu, N., Shuai, P., Siegl, K., Utsuno, Y., Wagenknecht, P., and Yokoyama, R.
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Nuclear Experiment ,Nuclear Theory - Abstract
We observed a new isomeric gamma transition at 168 keV in $^{36}$Mg, with a half-life of T$_{1/2}$=[130-500]$(\pm40)(^{+800}_{-20})_{sys}$ ns. We propose that the observed transition de-excites a new 0$^+$ isomeric state 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 $^{36}$Mg 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 {\it sd} to the {\it pf} shell. Within this interpretation, $^{36}$Mg becomes the crossing point between nuclei in which ground state deformed/superdeformed configurations are caused by the dominance of N=20 intruders ($^{32,34}$Mg) and nuclei where deformed configurations are associated with N=28 intruders ($^{38}$Mg 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 $^{38}$Mg incompatible with our observation. We conclude that $^{36}$Mg bridges the N=20 and N=28 islands of inversion, forming the so-called Big Island of Deformation., Comment: 7 pages, 4 figures
- Published
- 2023
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