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Going Nuclear: Notes from the officially unofficial book tour
I work in the analytical labs at one of Europe’s oldest and largest nuclear sites: Sellafield, in northwestern England. I spend my days at the fume hood front, pipette in one hand and radiation probe in the other (and dosimeter pinned to my chest, of course). Outside the lab, I have a second job: I moonlight as a writer and public speaker. My new popular science book—Going Nuclear: How the Atom Will Save the World—came out last summer, and it feels like my life has been running at full power ever since.
G. J. Kirouac, H. M. Eiland, C. A. Conrad, R. E. Slovacek, K. W. Seemann
Nuclear Science and Engineering | Volume 52 | Number 3 | November 1973 | Pages 310-320
Technical Paper | doi.org/10.13182/NSE73-A19478
Articles are hosted by Taylor and Francis Online.
Resonance parameters for 147Pm and 148mPm have been determined and the resonances 147Pm have been analyzed up to 317 eV. Only one resonance was observed for 148mPm; its location at 0.17 eV is important for thermal reactor calculations Transmission measurements were initially made on four samples of 147Pm2O3 containing 1.6% of the decay product 147Sm. Later measurements, made on a mixed sample of (148mPm + 147Pm)2O3 and on 147Sm, provided resonance parameters for 147Pm and an opportunity for a complete reevaluation of the previous 147Pm results. Corrections for the samarium content could also be made. Both shape and area analyses were performed. The measured total cross section for 147Pm at 0.025 eV was 198 ± 8 b and a capture resonance integral of 2280 ± 200 b was calculated. Using the parameters of the 148mPm resonance at 0.17 eV, a corresponding total thermal-neutron cross section of 10 600 b was ob-tained. Integral measurements with cadmium-covered samples gave a value of (3.6 ± 2.4) × 103 b for the resonance integral of 148mPm, thereby setting an upper limit of 6000 b.