High-spin spectroscopy of 159,160Er

James Ollier and John Simpson

 

We have continued our experimental programme to study the highest possible angular momentum states by discrete line gamma-ray spectroscopy [1, 2, 3].

Our recent work in the mass 160 region has unearthed a series of collective structures in a range of Er [2], Yb [4] and Tm [5] nuclei.

These studies heralded entry to the regime of ultra-high-spin spectroscopy.

Our most spectacular work was the discovery of rotational bands that bypass the classic band-terminating states [2] and herald a return to collectivity in 157,158Er.

These rotational structures have characteristics of triaxially strongly-deformed (TSD) bands.

In order to confirm this interpretation and gather an understanding of the nature of highly collective structures in the wider region

(from superdeformation near 152Dy, TSD structures in the Lu's and enhanced deformation or triaxial deformation in the mass~170 Hf's)

we recently performed and experiment to study high spin states in 159,160Er.

This experiment was performed using the Gammasphere spectrometer at Argonne National Laboratory (ANL) in the USA.

This work is a collaboration with the University of Liverpool, Florida State University, ANL, the U.S naval Academy, the University of Tennessee and Lund University.

Background subtracted g-ray spectra showing 3 new bands associated with the decays of 159,160Er and their Dynamic moments-of-inertia (J(2)) with bands found in other Er isotopes.

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

The analysis of this experiment has so far revealed three new bands, one in 159Er and two in 160Er.

These bands show similar characteristics in their moments-of-inertia to those observed previously in 157,158Er [2] which suggest a common underlying structure.

Cranked Nilsson-Strutinsky calculations indicate that they may arise from well-deformed triaxial configurations, extending discrete-line spectroscopy to 60ћ.

[1] J Simpson et al., Phys. Lett. B327, 187 (1994)

[2] E. S. Paul et al., Phys. Rev. Lett. 98, 012501 (2007).

[3] A. O. Evans et al., Phys. Rev. Lett. 92, 252502 (2004).

[4] A. Aguilar et al., Phys. Rev C 77, 021302 (2008)

[5] C. Teal et al., Phys. Rev. C 78, 017305 (2008)