Elongated shape isomers in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Ar</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>36</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>nucleus
J. CsehInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryJ. DaraiInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryW. ScianiInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryYul OtaniInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryA. Lépine‐SzilyInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryE. A. BenjamimInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryL. C. ChamonInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, HungaryR. LichtenthälerInstitute of Nuclear Research of the Hungarian Academy of Sciences, HU-4001, Debrecen Pf 51, Hungary
2009lv
ABI
Abstract
A recent analysis of the $^{12}\mathrm{C}$$+$$^{24}\mathrm{Mg}$ scattering [W. Sciani et al., Phys. Rev. C 80, 034319 (2009)] suggests the existence of a hyperdeformed band in the $^{36}\mathrm{Ar}$ nucleus, completely in line with the predictions of $\ensuremath{\alpha}$ [W. D. M. Rae and A. C. Merchant, Phys. Lett. B279, 207 (1992)] and binary cluster calculations [J. Cseh et al., Phys. Rev. C 70, 034311 (2004)]. Here we review the structural understanding of the superdeformed and the hyperdeformed states of $^{36}\mathrm{Ar}$ and present new results on the shape isomers as well. Special attention is paid to the clusterization of these states, which indicates the appropriate reaction channels for their formation.
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Cited by 20 references