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This study explores transitions in the A80 superdeformed region using experimental and theoretical methods. Detailed analysis of 84Zr spectra and comparison with calculated results provide insights into the structure and properties of superdeformed nuclei. The depopulation of the superdeformed well in 84Zr is examined, along with comparisons to neighboring nuclei. Theoretical models are employed to understand the weak decay-out processes in superdeformed states. Potential energy surfaces for fixed spins are calculated for 84Zr and 152Dy, unveiling barriers along the least-action paths. The study presents a comprehensive characterization of superdeformed bands, highlighting the unique properties of 84Zr. Results support theoretical calculations and reveal similarities with other nuclei in different mass regions.
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Linking Transitions (and Search for Superintruders) in the A80 Region of Superdeformation C. J. Chiara, D. G. Sarantites, M. Montero, J. O’Brien, O. L. Pechenaya, and W. Reviol, Washington University R. M. Clark, P. Fallon, A. Görgen, A. O. Macchiavelli, and D. Ward, Lawrence Berkeley National Laboratory W. Satuła, University of Warsaw Y. R. Shimizu, KyushuUniversity Nilsson Conf. Lund, Sweden 17 June 2005
TSD (linked) A190 (linked) A150 A130 A80 (linked) (linked) (not linked!) 84Zr A60 (linked) A40 (linked) SD regions F. Lerma et al., PRC 67, 044310 (2003) B. Singh, R. Zywina, R.B. Firestone, Nucl. Data Sheets 97, 241 (2002)
Experimental details • 140-MeV 32S + 0.5-mg/cm258Ni 84Zr + a2p • Gammasphere [102 Ge detectors] • Microball [95 CsI(Tl) detectors] for charged particle detection; ep80%, ea70% • Total of 2.2109 events of fold 5 or higher over 6 days.
spectra Double-gated spectra of 84Zr links
84Zr lev.sch. E1 M1/E2 E1 I0p = 25-
CSLN Compare with calculations using Cranked Strutinsky + Lipkin-Nogami pairing n52p51 configuration previously assigned to SD1 based on Qt—now compare Ex, Ip as well: • Ex (near ND-SD crossing) • spin (except at alignments) • parity
84Zr 152Dy* 192Pb† B(E1) ~10-6 W.u. ~10-6 W.u. ~10-7-10-8 W.u. Depopulation of the SD well SD1 in 84Zr has weak decays to ND states, similar to the A=150,190 SD bands. *T.Lauritsen, PRL88, 042501 (2002) †A.N.Wilson, PRL90, 142501 (2003)
stat’l • Weak decay-out explored with several statistical models, e.g.: • E.Vigezzi et al., PLB249,163 (1990) • J.-z.Gu and H.A.Weidenmüller, NPA660, 197 (1999) • D.M.Cardamone et al., PRL91, 102502 (2003) • Each relates GS, GN, d, FS with spreading width G. • Compare 84Zr with results inA.N.Wilson, Prog. Theor. Phys. (Kyoto), Suppl. 154, 138 (2004):
Tunneling paths and barriers • Calculate potential energy surfaces for fixed spins. • Determine least-action path from SD min to ND well. • Get barrier height in direction of path. • [K.Yoshida et al., NPA696, 85 (2001) and refs. therein.] Compare 152Dy and 84Zr surfaces….
barriers Barrier heights calculated along least-action paths from fixed-spin potential surfaces, as in K.Yoshida et al., NPA696, 85 (2001).
Summary • “Full” characterization of an A80 SD band: Ex, Ip, Qt, B(sl) [several neighbors studied too, but no luck linking!] • Results are consistent with CS-LN calculations for n52p51 configuration [esp. Ex(I) in crossing region] • 84Zr SD1 has eclectic properties; similar to: • 152Dy [spin, energy, B(E1)] • 192Pb [strength of SD-ND coupling] • A60,130 regions [potential barriers] • HF+SLy4 calcs at I=25 reveal many configs at different deformations with similar energies supports PES picture
The End C. J. Chiara, D. G. Sarantites, M. Montero, J. O’Brien, O. L. Pechenaya, and W. Reviol, Washington U. R. M. Clark, P. Fallon, A. Görgen, A. O. Macchiavelli, and D. Ward, LBNL Theoretical support from W.Satuła, U. of Warsaw and Y.R.Shimizu, Kyushu U.