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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.
J. W. T. Dabbs, C. H. Johnson, C. E. Bemis, Jr.
Nuclear Science and Engineering | Volume 83 | Number 1 | January 1983 | Pages 22-36
Technical Paper | doi.org/10.13182/NSE83-A17986
Articles are hosted by Taylor and Francis Online.
The fission cross section of 241Am has been measured from 0.02 eV to 20 MeV using time-of-flight techniques at the Oak Ridge Electron Linear Accelerator. A “honeycomb” fission ionization chamber that contained six deposits totaling 14.3 mg of 241Am, six deposits totaling 116 mg of 235U, and a single deposit of 252Cf, which served as a monitor for the chamber performance, was used. The 235U fission served as the cross-section standard for energies above 101 keV while 6Li(n, α), normalized to 235U fission in the 7.8- to 11.0-eV interval, served as a shape standard below 101 keV. Approximately 700 h of data were obtained at a flight path distance of 9.1 m, primarily with 40-ns bursts. Because the fission cross section of 241Am is very small in the midrange of neutron energies, particular attention was paid to correction of backgrounds, particularly inscattered neutron-induced events. The fission resonance integral was found to be 14.1 ± 0.9 b.