lor series expansion does not appear to converge rapidly. For nonbackbending CHFB spectra, the expansion seems well behaved at all spins.In conclusion, a simple expression is derived which uses the angular momentum fluctuations in CHFB wave functions to obtain high-spin spectra which are approximately angular momentum projected. Although the fluctuations in J x are most important, those in J y and J z should not be omitted. The projected spectra are less compressed than the CHFB spectra and are closer to the experimental excitation energies.New differential cross section and analyzing--power data for 800-MeV j> p oi+ 12 C, 116,124 Sn inelastic scattering to the first 2 + states are presented. A distorted-wave Born-approximation analysis which utilizes collective form factors and includes deformation of the spin-orbit potential is shown to provide a reasonable description of the analyzing-power data.
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