“…In this nucleus, the high-spin 21 + isomer has a high excitation energy of 6.7 (5) MeV with a notably long half-life of 0.39(4) s, and is open to β, one-proton, and two-proton decays [12,13]. Although the shell model calculations with the empirical effective interaction in the restricted (1p 1/2 , 0g 9/2 ) model space could reproduce the energy levels and high-spin isomers in 95 Ag, 95 Pd, and 94 Pd, it failed to predict the isomerism of 21 + state in 94 Ag [9,10]. On the other hand, it has been shown that the large-scale shell model calculations with the extended model space (0g 9/2 , 1d 5/2 , 0g 7/2 , 1d 3/2 , 2s 1/2 ) can obtain a 21 + -19 + level inversion, which suggests that the core excitations across the 100 Sn shell-closure play a crucial role in generating the 21 + isomer with such a long halflife [9].…”