Structure of $^{\bf 136}$Te and the problem of mass of $^{\bf 134}$Te

A. Nowak; W. Urban; M. Rejmund; J.L. Durell; M.J. Leddy; M.A. Jones; W.R. Phillips; A.G. Smith; B.J. Varley; I. Ahmad; L.R. Morss; M. Bentaleb; E. Lubkiewicz; N. Schulz

doi:doi:10.1007/s100500050156

2022 Impact factor 2.7

Hadrons and Nuclei

Eur. Phys. J. A 3, 111-113

Short note

Structure of $^{\bf 136}$ Te and the problem of mass of $^{\bf 134}$ Te

A. Nowak¹ - W. Urban¹ - M. Rejmund¹ - J.L. Durell² - M.J. Leddy² - M.A. Jones² - W.R. Phillips² - A.G. Smith² - B.J. Varley² - I. Ahmad³ - L.R. Morss³ - M. Bentaleb⁴ - E. Lubkiewicz⁴ - N. Schulz⁴

¹ Institue of Experimental Physics, Warsaw University, ul.Hoza 69, 00-681 Warszawa, Poland
² Schuster Laboratory, Department of Physics and Astronomy, University of Manchester, Manchester M13 9PL, UK
³ Argonne National Laboratory, Argonne, IL 60439, USA
⁴ Centre de Recherches Nucléaires, IN2P3-CNRS/Université Louis Pasteur, 67037 Strasbourg, France

Received: 3 August 1998 Communicated by B. Povh

Abstract
Neutron-rich, N=84 nuclei from the ¹³²Sn region, populated in spontaneous fission of ²⁴⁸Cm, have been studied with EUROGAM 2. Excited states and their spins and parities in the ¹³⁶Te nucleus were established up to 17 $\hbar$ . OXBASH code calculations support the experimental identification of maximum aligned configurations in ¹³⁶Te. Empirical shell model calculations for the I $^{\pi}$ = 14⁺ level in ¹³⁶Te indicate that the adopted mass of the ¹³⁴Te nucleus should be lowered by 200(80) keV.

PACS
21.60.Cs Shell model - 23.20.Lv Gamma transitions and level energies - 27.80.+w $190 \le A \le 219$ - 25.70.-z Low and intermediate energy heavy ion reactions