English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Plus monthly

Global: Zendy Tools annual

Global: Zendy Tools monthly

Global: Zendy Free Plan

A new interpretation for the wobbling bands in $^{163}$Lu is given within aparticle-triaxial rotor semi-classical formalism. While in the previous papersthe bands TSD1, TSD2, TSD3 and TSD4 are viewed as the ground, one, two andthree phonon wobbling bands, here the corresponding experimental results aredescribed as the ground band with spin equal to I=R+j, for R=0,2,4,...(TSD1),the ground band with I=R+j and R=1,3,5,...(TSD2), the one phonon excitations ofTSD2 (TSD3), with the odd proton moving in the orbit $j=i_{13/2}$, and theground band of I=R+j, with R=1,3,5,... and $j=h_{9/2}$ (TSD4). The moments ofinertia (MoI) of the core for the first three bands are the same, andconsidered to be free parameters. Due to the core polarization effect caused bythe particle-core coupling, the MoI's for TSD4 are different. The energies andthe e.m. transitions are quantitatively well described. Also, the phase diagramof the odd system is drawn. In the parameter space one indicates where thepoint associated with the fitted parameters is located and also which is theregion of transversal wobbling mode as well as where the wobbling motion isforbidden.

Towards a new semi-classical interpretation of the wobbling motion in $^{163}$Lu