The binding energies of 29 Si, 33 S, and 36 Cl have been measured with a relative uncertainty of <0.59 × 10 −6 using a flat-crystal spectrometer. The unique features of these measurements are (1) nearly perfect crystals whose lattice spacing is known in meters, (2) a highly precise angle scale that is derived from first principles, and (3) a γ -ray measurement facility that is coupled to a high-flux reactor with near-core source capability. The binding energy is obtained by measuring all γ -rays in a cascade scheme connecting the capture and ground states. The measurements require the extension of precision flat-crystal diffraction techniques to the 5-to 6-MeV energy region, a significant precision measurement challenge. The binding energies determined from these γ -ray measurements are consistent with recent highly accurate atomic-mass measurements within a relative uncertainty of 4.3 × 10 −7 . The γ -ray measurement uncertainties are the dominant contributors to the uncertainty of this consistency test. The measured γ -ray energies are in agreement with earlier precision γ -ray measurements.
The lifetimes of the 2 ϩ states of the first excited K ϭ0 ϩ band in 168 Er and 164 Dy have been measured using the ␥-ray induced Doppler broadening technique. Although the deduced uncertainties for the lifetimes are rather large the data indicate that in 168 Er the decay to the ␥ band is moderately collective. In 164 Dy, however, a less collective decay pattern is observed. The transition rates are compared to the available theoretical descriptions. ͓S0556-2813͑98͒00902-9͔
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.