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    Energy averages and fluctuations in the decay out of superdeformed bands

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    We derive analytic formulae for the energy average (including the energy average of the fluctuation contribution) and variance of the intraband decay intensity of a superdeformed band. Our results may be expressed in terms of three dimensionless variables: Γ↓/ΓS\Gamma^{\downarrow}/\Gamma_S, ΓN/d\Gamma_N/d, and ΓN/(ΓS+Γ↓)\Gamma_N/(\Gamma_S+\Gamma^{\downarrow}). Here Γ↓\Gamma^{\downarrow} is the spreading width for the mixing of a superdeformed (SD) state ∣0>|0> with the normally deformed (ND) states ∣Q>|Q> whose spin is the same as ∣0>|0>'s. The ∣Q>|Q> have mean level spacing dd and mean electromagnetic decay width ΓN\Gamma_N whilst ∣0>|0> has electromagnetic decay width ΓS\Gamma_S. The average decay intensity may be expressed solely in terms of the variables Γ↓/ΓS\Gamma^{\downarrow}/\Gamma_S and ΓN/d\Gamma_N/d or, analogously to statistical nuclear reaction theory, in terms of the transmission coefficients T0(E)T_0(E) and TNT_N describing transmission from the ∣Q>|Q> to the SD band via ∣0∠|0\angle and to lower ND states. The variance of the decay intensity, in analogy with Ericson's theory of cross section fluctuations depends on an additional variable, the correlation length \Gamma_N/(\Gamma_S+\Gamma^{\downarrow})=\frac{d}{2\pi}T_N/(\Gamma_S+\Gamma^{\d ownarrow}). This suggests that analysis of an experimentally obtained variance could yield the mean level spacing dd as does analysis of the cross section autocorrelation function in compound nuclear reactions. We compare our results with those of Gu and Weidenm\"uller.Comment: revtex4, 14 pages, 4 figures, to appear in Physical Review
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