In-beam gamma-ray spectroscopy of odd-neutron Mo and Ru isotopes

High-spin level structure inMo94,95

“…[6,7]. However, the strong dipole transition of 152 keV had been placed to feed directly the (17/2 + ) level at 2580 keV [4,6,7]; this is not consistent with our work considering the γ -γ coincidence relationships. From the double-gated spectra shown in the upper and middle panels of transition.…”

“…Most of the γ rays reported in the literature [4][5][6][7]9] have been observed in this experiment. The γ -ray coincidence relationships and their ADO ratios have been analyzed with care, leading to the establishment of the revised level schemes for 94,94 Mo that significantly differ from the previous work.…”

“…From the double-gated spectra shown in the upper and middle panels of transition. In fact, the 386-keV line was reported as a doublet [6], and the authors of Refs. [6,7] had assigned one of them in the low-lying level scheme corresponding to the 11/2 − → (9/2 + ) transition, leaving one 386-keV γ ray unassigned.…”

“…In fact, the 386-keV line was reported as a doublet [6], and the authors of Refs. [6,7] had assigned one of them in the low-lying level scheme corresponding to the 11/2 − → (9/2 + ) transition, leaving one 386-keV γ ray unassigned. The ADO ratio analysis shows that the second 386-keV transition has a quadrupole multipolarity (see Table II + ) → (17/2 + ) transition may be highly converted and the low-energy γ ray of 38 keV could be out of the detection limit of GASP.…”

“…The high-spin states of 94,95 Mo were investigated a long time ago by Lederer et al [5,6] and Mesko et al [7] via (α, xnγ ) reactions. The level schemes have been extended up to I ∼19 at 12 MeV excitation energy by Kharraja and coworkers [4] using heavy-ion-induced fusion-evaporation reactions and the early implementation phase of the Gammasphere array.…”