In nuclear physics, hyperdeformation is theoretically predicted states of an atomic nucleus with extremely elongated shape and very high angular momentum. Less elongated states, superdeformation, have been well observed, but the experimental evidence for hyperdeformation is more limited. Hyperdeformed states correspond to an axis ratio of 3:1. They would be caused by a third minimum in the potential energy surface, the second causing superdeformation and the first minimum being normal deformation.[1][2][3] Hyperdeformation is predicted to be found in 107Cd.
References
^Adamian, G. G.; N. V. Antonenko; Z. Gagyi-Palffy; S.P. Ivanova; R. V. Jolos; Yu. V. Palchikov; W. Scheid; T.M. Shneidman; A.S. Zubov (2007). "Nuclear Molecular Structure". Collective Motion and Phase Transitions in Nuclear Systems: Proceedings of the Predeal International Summer School in Nuclear Physics (illustrated ed.). World Scientific. p. 483. ISBN981-270-083-8.
^Schunck, N.; Dudek, J.; Herskind, B. (May 2007). "Nuclear hyperdeformation and the Jacobi shape transition". Physical Review C. 75 (5): id. 054304. Bibcode:2007PhRvC..75e4304S. doi:10.1103/PhysRevC.75.054304.
^Abusara, H.; Afanasjev, A. V. (2009). "Hyperdeformation in the Cd isotopes: A microscopic analysis". Physical Review C. American Physical Society. 79 (2): eid 024317. arXiv:0902.0095. Bibcode:2009PhRvC..79b4317A. doi:10.1103/PhysRevC.79.024317. arXiv: 0902.0095v1
hyperdeformation, nuclear, physics, hyperdeformation, theoretically, predicted, states, atomic, nucleus, with, extremely, elongated, shape, very, high, angular, momentum, less, elongated, states, superdeformation, have, been, well, observed, experimental, evid. In nuclear physics hyperdeformation is theoretically predicted states of an atomic nucleus with extremely elongated shape and very high angular momentum Less elongated states superdeformation have been well observed but the experimental evidence for hyperdeformation is more limited Hyperdeformed states correspond to an axis ratio of 3 1 They would be caused by a third minimum in the potential energy surface the second causing superdeformation and the first minimum being normal deformation 1 2 3 Hyperdeformation is predicted to be found in 107Cd References Edit Adamian G G N V Antonenko Z Gagyi Palffy S P Ivanova R V Jolos Yu V Palchikov W Scheid T M Shneidman A S Zubov 2007 Nuclear Molecular Structure Collective Motion and Phase Transitions in Nuclear Systems Proceedings of the Predeal International Summer School in Nuclear Physics illustrated ed World Scientific p 483 ISBN 981 270 083 8 Schunck N Dudek J Herskind B May 2007 Nuclear hyperdeformation and the Jacobi shape transition Physical Review C 75 5 id 054304 Bibcode 2007PhRvC 75e4304S doi 10 1103 PhysRevC 75 054304 Abusara H Afanasjev A V 2009 Hyperdeformation in the Cd isotopes A microscopic analysis Physical Review C American Physical Society 79 2 eid 024317 arXiv 0902 0095 Bibcode 2009PhRvC 79b4317A doi 10 1103 PhysRevC 79 024317 arXiv 0902 0095v1 This nuclear physics or atomic physics related article is a stub You can help Wikipedia by expanding it vte Retrieved from https en wikipedia org w index php title Hyperdeformation amp oldid 1000106439, wikipedia, wiki, book, books, library,
