2019 Impact factor 2.176
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

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.

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

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