Band structures in⁹⁹Rh

Abstract

Excited states in the 99 Rh nucleus were populated using the fusion-evaporation reaction 75 As( 28 Si,2p2n) at = E 120 MeV lab 9 2 15 2 5 configuration with one anti-aligned g 9 2 proton, respectively.

Band structures in Pd101

“…The efficiency of the array for energies up to ∼ 3 MeV were deduced from the measured γ ray spectra of the 133 Ba and 152 Eu standard radioactive sources and the intensity balance along the transition sequence in higherlying transition gated coincidence spectra in the 38 Ar, 39 K, and 96 Ru nuclei populated in the present experiment. The details are given elsewhere [27,28].…”

Level structures of 96Tc and their microscopic description

“…Level structures in the 96 Tc nucleus were populated in the 75 As( 28 Si, 4p3n) fusion-evaporation reaction at E lab = 120 MeV. Various reaction channels populated in the present reaction were discussed in earlier reported work [27][28][29]. The 15UD Pelletron accelerator facility at inter university accelerator centre (IUAC), New Delhi [30,31] delivered the required 28 Si beam.…”

“…Various reaction channels populated in the present reaction were discussed in earlier reported work [27][28][29]. The 15UD Pelletron accelerator facility at inter university accelerator centre (IUAC), New Delhi [30,31] delivered the required 28 Si beam. The 75 As target of thickness 3 mg cm −2 was fabricated by vacuum evaporation and rolled onto a 10 mg cm −2 thick Pb backing [32].…”

“…Efficiency values at the higher energies up to ∼3 MeV were deduced from the intensity balance along the transition sequences observed in the coincidence spectra with gate on the higher-lying transitions following de-excitations in the 38 Ar [34], 39 K [35], 93 Tc [36], and 96 Ru [37] nuclei. The 38 Ar and 39 K were produced as fission products in the reaction of 28 Si ion beam with the light nuclei present in the target, viz., the 27 Al frame of the target and 16 O in the oxide form.…”