- Lubna, RS;
- Liddick, SN;
- Ogunbeku, TH;
- Chester, A;
- Allmond, JM;
- Bhattacharya, Soumik;
- Campbell, CM;
- Carpenter, MP;
- Childers, KL;
- Chowdhury, P;
- Christie, J;
- Clark, BR;
- Clark, RM;
- Cox, I;
- Crawford, HL;
- Crider, BP;
- Doetsch, AA;
- Fallon, P;
- Frotscher, A;
- Gaballah, T;
- Gray, TJ;
- Grzywacz, R;
- Harke, JT;
- Hartley, AC;
- Jain, R;
- King, TT;
- Kitamura, N;
- Kolos, K;
- Kondev, FG;
- Lamere, E;
- Lewis, R;
- Longfellow, B;
- Lyons, S;
- Luitel, S;
- Madurga, M;
- Mahajan, R;
- Mogannam, MJ;
- Morse, C;
- Neupane, SK;
- Ong, W-J;
- Perez-Loureiro, D;
- Porzio, C;
- Prokop, CJ;
- Richard, AL;
- Ronning, EK;
- Rubino, E;
- Rykaczewski, K;
- Seweryniak, D;
- Siegl, K;
- Silwal, U;
- Singh, M;
- Siwakoti, DP;
- Smith, DC;
- Smith, MK;
- Tabor, SL;
- Tang, TL;
- Tripathi, Vandana;
- Volya, A;
- Wheeler, T;
- Xiao, Y;
- Xu, Z
The level structure of Al36 has been studied via β decay of Mg36 at the Facility for Rare Isotope Beams (FRIB) and the National Superconducting Cyclotron Laboratory (NSCL). A long-lived isomer in Al36 was identified which decays by β to an excited state of Si36. The ground state and the isomeric state of Al36 were found to populate different energy levels of Si36. The results from the two data sets in the present work complement each other. Configuration interaction calculations performed with the FSU shell-model Hamiltonians provide reasonable descriptions to the experimental observations and offer insight into future improvements of the theoretical interpretation.