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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.
O. Kaneko, Y. Takeiri, K. Tsumori, M. Osakabe, K. Ikeda, K. Nagaoka, H. Nakano, LHD Experiment Group
Fusion Science and Technology | Volume 58 | Number 1 | July-August 2010 | Pages 497-503
Chapter 9. Neutral Beam Interaction | Special Issue on Large Helical Device (LHD) | doi.org/10.13182/FST10-A10836
Articles are hosted by Taylor and Francis Online.
A unique and reliable method of plasma initiation has been established in the Large Helical Device (LHD) by using neutral beam (NB) injection into vacuum. Since LHD is a superconducting machine, the confining magnetic field exists unrelated to plasma. Under these circumstances it is demonstrated that the NB can initiate plasma by itself. A small fraction of injected NB is ionized by collision with the background neutral gas and is confined by the magnetic field. Although these high-energy ions are lost quickly by charge exchange, they work as the energy source for ionizing the background neutral particles and heating the produced plasma. As a result, very thin but hot "seed" plasma is generated, which ionizes puffed gas and makes dense target plasma that is sufficient for NB absorption. This process is simulated numerically and the results agree well with the experimental observations for both absolute values and temporal behavior of plasma parameters. The method does not depend on magnetic field strength strongly, and plasma can be initiated at the magnetic field strength as low as 0.4 T, although standard field strength of LHD is 2.75 T. The progress of high-beta studies in LHD owes this plasma production method much.