6 research outputs found
High-spin states in the nucleus
High-spin states in the Tc nucleus have been studied with the reactions
Se(F,5n) at 68 MeV and Zn(S,pn)
at 130 MeV. Two -ray cascades (irregular bandlike
structures) have been observed up to an excitation energy of about 10 MeV and
spin 21-22
Band structures in doubly-odd Rh
High spin states of Rh have been populated using the
reaction Zn+S at 130 MeV. -rays were detected
with the EUROGAM2 array. The level structure of Rh has been extended up to
14.41 MeV excitation energy. Several band structures are observed.
A band based on a I=8 state is developed up to
the I=24 level. It is assigned as the
configuration
Level structure of
The decay of 123Ba to 123Cs has been studied with mass-separated sources. Singles spectra of γ-rays, X-rays and conversion electrons as well as γ - γ - t, γ - e
− - t, and X - e
− - t coincidences were recorded. A level scheme of 123Cs has been constructed including 26 new excited states and 82 transitions. The existence of a I
π
= 11/2−, T
1/2 = 1.7 s isomer, bandhead of the h
11/2 band, is confirmed. Its excitation energy equals 156.3 keV. A new T
1/2 = 114 ns isomer has been established at 232 keV using the in-beam recoil catcher technique. It is assigned to the I
π
= 9/2+ bandhead of the gpg
9/2 band. Collective bands based on the 1/2+ ground state and first 3/2+ excited state are proposed. The level structure is described in the frame of the interacting boson-fermion and core-quasiparticle coupling models
Low-spin excitations in
The low-spin excitations of the nucleus 146Sm which is just two neutrons and two protons away from the N = 82 shell and Z = 64 subshell closures have been investigated by means of the 143Nd (α, n) and 144Nd (α, 2n) fusion-evaporation reactions. We established 47 hitherto unknown energy levels up to 4.7MeV and 75 new transitions. In addition, 7 spin assignments were possible from the γ-γ angular correlation analysis. The structure of the possible candidates for a 2+ ⊗ 3− quadrupole-octupole multiplet are first discussed in terms of the harmonic vibrational model. A comparison of these states with the corresponding ones in the neighboring N = 84 isotones is also presented. Finally, the structure of the 146Sm nucleus is interpreted in terms of the IBA-spdf model. It is shown that the model is able to reproduce the experimental relative transition strengths of the 2+ ⊗ 3− quadrupole-octupole multiplet and also a series of collective properties such as the proposed double-octupole excitations