Abstract
One key component of any active interrogation (AI) system that is not present in passive measurements is the source of probing radiation. This chapter introduces the physical principles of operation of linear accelerators, cyclotrons, and novel laser-driven sources, along with the review of radioisotope sources and the use of natural radiation for AI. Some of the critical parts of these technologies are discussed in more detail. In addition, the common characteristics of various probe technologies are provided.
Section 5.4 was prepared by Cameron Geddes (Lawrence Berkeley National Laboratory, 1 Cyclotron Rd, Berkeley, CA 94720, USA), e-mail: CGRGeddes@lbl.gov
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Acknowledgements
The Sect. 5.4 was supported by the U.S. Dept. of Energy National Nuclear Security administration Defense Nuclear Nonproliferation R and D (NA-22), and by the Office of Science Office of High Energy Physics, under Contract No. DE-AC02-05CH11231 to Lawrence Berkeley National Laboratory. The simulations used the computational facilities at the National Energy Research Scientific Computing Center, a DOE Office of Science User Facility supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231. We would like to acknowledge contributions by Markus Roth, Hai-En Tsai, Jeroen van Tilborg, Sven Steinke, Csaba Toth, Jean-Luc Vay, Carl Schroeder, Eric Esarey, Kei Nakamura, Bernhard Ludewigt, Brian Quiter, John Valentine, Marie-Anne Descalle, Matt Kinalw, David Chichester, Glen Warren, Cameron Miller, Sara Pozzi, and Wim Leemans.
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Garnett, R. (2018). Active Interrogation Probe Technologies. In: Jovanovic, I., Erickson, A. (eds) Active Interrogation in Nuclear Security. Advanced Sciences and Technologies for Security Applications. Springer, Cham. https://doi.org/10.1007/978-3-319-74467-4_5
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