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Microscopic investigation of $γ~$ vibrational band structures in odd-mass nuclei

Uzma Jahangir, S. P. Rouoof, S. Jehangir, G. H. Bhat, J. A. Sheikh, N. A. Rather

Abstract

A systematic investigation of the high-spin band structures observed in $^{103,105,107,109}$Nb and $^{103,105,107,109}$Tc nuclides is performed using the triaxial projected shell model (TPSM) approach. For $^{103,105}$Nb isotopes, four bands have been populated with the lowest three bands corresponding to yrast, $γ$ and 2$γ$ bands. The nature of the fourth observed band has remained unresolved as it has been shown from the transition intensity ratios that this band cannot correspond to the expected 3$γ$ band. It is demonstrated in the present work that this fourth band is the second $γ$ band, resulting from the combination, $K=K_0-2$ with $K_0$ being the "$K$" value of the parent configuration. The excitation energy and other properties of this band structure are predicted for all the studied nuclides.

Microscopic investigation of $γ~$ vibrational band structures in odd-mass nuclei

Abstract

A systematic investigation of the high-spin band structures observed in Nb and Tc nuclides is performed using the triaxial projected shell model (TPSM) approach. For Nb isotopes, four bands have been populated with the lowest three bands corresponding to yrast, and 2 bands. The nature of the fourth observed band has remained unresolved as it has been shown from the transition intensity ratios that this band cannot correspond to the expected 3 band. It is demonstrated in the present work that this fourth band is the second band, resulting from the combination, with being the "" value of the parent configuration. The excitation energy and other properties of this band structure are predicted for all the studied nuclides.
Paper Structure (4 sections, 10 equations, 9 figures, 1 table)

This paper contains 4 sections, 10 equations, 9 figures, 1 table.

Figures (9)

  • Figure 1: (Color online) Projected energies are shown before diagonalization of the shell model Hamiltonian for $^{105}$Nb. The bands are labelled by three quantities : $K$-quantum number, energy and group structure of the quasiparticle state. For instance, $(1/2, 0.98, 1\pi)$ designates one-quasiproton state having intrinsic energy of 0.98 MeV and K$=1/2$.
  • Figure 2: (Color online) TPSM energies for the lowest five bands after configuration mixing are plotted along with the available experimental data for $^{105}$Nb isotope. Data are taken from Li054311.
  • Figure 3: (Color online) Probabilities of various projected $K$ configurations in the orthonormal basis of $^{105}$Nb. The curves are labelled by three quantities: $K$ quantum number, energy of the quasiparticle state and quasiparticle character. For instance, [1/2, 0.98, 1$\pi$] designates one quasiproton state with $K$= 1/2 having intrinsic energy of 0.98 MeV.
  • Figure 4: (Color online) TPSM and experimental energies of the Yrast, $\gamma_1$, $2\gamma$, $\gamma_2$ and $3\gamma$ bands of $^{103,105,107,109}$Nb isotopes. The scaling factor, $\kappa=32.32A^{-5/3}$.
  • Figure 5: (Color online) TPSM and experimental energies of the Yrast, $\gamma_1$, $2\gamma$, $\gamma_2$ and $3\gamma$ bands of $^{103,105,107,109}$Tc isotopes. The scaling factor, $\kappa=32.32A^{-5/3}$.
  • ...and 4 more figures