Plasma and Fusion Research
Volume 11, 2403049 (2016)
Regular Articles
- Department of Applied Quantum Physics and Nuclear Engineering, Kyushu University, 744 Motooka, Fukuoka 819-0395, Japan
- 1)
- National Institute for Fusion Science, 322-6 Oroshi-cho, Toki 509-5292, Japan
Abstract
Assuming a deuterium-beam-injected deuterium plasma confined in the Large Helical Device (LHD), the incident angle distribution and energy spectra of neutrons at various wall positions are evaluated by considering the complex shape of the vacuum vessel and the deuteron velocity distribution function. The effect of anisotropy of this function on the incident flux, the energy spectra, and the incident angle distribution of the neutrons to the vacuum vessel, are examined. In this paper, the neutron spectra are shown to depend on the wall position and the incident direction because of the formation of anisotropic high-energy tail in the deuteron velocity distribution function and the characteristic shape of the vacuum vessel of the LHD.
Keywords
fast-ion velocity distribution function, neutron emission spectrum, beam-injected deuterium plasma, neutron incident angle distribution, neutron incident energy spectrum, Large Helical Device
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References
- [1] P.P.H. Wilson et al., Fusion Eng. Des. 83, 824 (2008).
- [2] J.C. Rivas et al., Fusion Sci. Technol. 64, 687 (2013).
- [3] Y. Nakano et al., Rev. Sci. Instrum. 85, 11E116 (2014).
- [4] M. Homma et al., Plasma Fusion Res. 10, 3403050 (2015).
- [5] S. Sugiyama et al., Plasma Fusion Res. 10, 3403055 (2015).
- [6] H. Matsuura and Y. Nakao, Phys. Plasmas 16, 042507 (2009).
- [7] H. Matsuura et al., Plasma Phys. Control. Fusion 53, 035023 (2011).
- [8] H.-S. Bosch and G.M. Hale, Nucl. Fusion 32, 611 (1992).
- [9] M. Drosg and O. Schwerer, Production of monoenergetic neutrons between 0.1 and 23 MeV: neutron energies and cross-sections, Handbook of Nuclear Activation Data (Vienna: IAEA) STI/DOC/10/273, ISBN 92-0-135087-2 (1987).
- [10] H. Brysk, Plasma Phys. 15, 611 (1973).