Spectrum of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>γ</mml:mi></mml:math>Rays Connecting Superdeformed and Normal States in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Hg</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>192</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>
R.G. HenryT. LauritsenT. L. KhooI. AhmadM. P. CarpenterB. CrowellT. DøssingR. V. F. JanssensF. HannachiA. KorichiCarsten SchuckF. AzaiezC. W. BeausangR. BéraudC. BourgeoisR. M. ClarkI. DeloncleJ. DupratB. GallH. HübelMalcolm J. JoyceM. KaciY LecozM. MeyerE. S. PaulN. PerrinN. PofféM.-G. PorquetN. RedonH. SergolleJ.F. Sharpey-SchaferJ. SimpsonA. G. SmithNuclear PhysicsR. WadsworthP. Willsau
ABI
Abstract
The complete spectrum of $\ensuremath{\gamma}$ rays following the decay of superdeformed (SD) states in $^{192}\mathrm{Hg}$ has been extracted. The spectrum, which comprises a quasicontinuous component and sharp lines, reveals the decay mechanism and defines the excitation energies of the SD band. The decay of SD states results from the coupling between a cold, ordered SD system with a hot, chaotic one with normal deformation.
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