Europium-doped strontium and barium iodide are found to be readily growable by the Bridgman method and to produce high scintillation light yields. Sr12(Eu) emits into the Eu2+ band, centered at 435 nm, with a decay time of 1.2 ps and a light yield of -90 000 photons/MeV. It offers energy resolution better than 4% full width at half maximum at 662 keV, and exhibits excellent light yield proportionality. BaIz(Eu) produces >30 000 photons/MeV into the Eu2+ band at 420 nm (< 1 ps decay). An additional broad impurity-mediated recombination band is present at 550 nm (>3 ps decay), unless high-purity feedstock is used.
is the most promising. SrI 2 (Eu) emits into the Eu 2+ band, centered at 435 nm, with a decay time of 1.2 µs and a light yield of up to 115,000 photons/MeV. It offers energy resolution better than 3% FWHM at 662 keV, and exhibits excellent light yield proportionality. Transparent ceramics fabrication allows production of Gadolinium-and Terbium-based garnets which are not growable by melt techniques due to phase instabilities. While scintillation light yields of Cerium-doped ceramic garnets are high, light yield non-proportionality and slow decay components appear to limit their prospects for high energy resolution.We are developing an understanding of the mechanisms underlying energy dependent scintillation light yield non-proportionality and how it affects energy resolution. We have also identified aspects of optical design that can be optimized to enhance energy resolution.
Transmission nuclear resonance fluorescence measurements were made on targets consisting of Pb and depleted U with total areal densities near 86 g/cm 2 . The 238 U content in the targets varied from 0 to 8.5% (atom fraction). The experiment demonstrates the capability of using transmission measurements as a non-destructive technique to identify and quantify the presence of an isotope in samples with thicknesses comparable to the average thickness of a nuclear fuel assembly. The experimental data also appear to demonstrate the process of notch refilling with a predictable intensity. Comparison of measured spectra to previous backscatter 238 U measurements indicates general agreement in observed excited states. Evidence of two new 238 U excited states and possibly a third state have also been observed.
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