2016
DOI: 10.1585/pfr.11.1403105
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Knock-on Tail Formation Due to Nuclear Elastic Scattering and Its Observation Method Using <i>γ</i>-Ray-Generating <sup>6</sup>Li+d Reaction in Tokamak Deuterium Plasmas

Abstract: A knock-on tail formation in deuteron velocity distribution function due to nuclear elastic scattering (NES) by energetic protons and its observation method using γ-ray-generating 6 Li(d,pγ) 7 Li reaction are examined for proton-beam-injected deuterium plasmas. The proton velocity distribution function is obtained by means of the ion trajectory analysis in a Tokamak magnetic configuration. The knock-on tail in two-dimensional (2D) deuteron velocity distribution function due to NES by energetic protons is evalu… Show more

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Cited by 7 publications
(10 citation statements)
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(61 reference statements)
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“…For detailed evaluation, more sophisticated simulations considering the anisotropy of the plasma would be necessary. Currently the analysis using the particle simulation code considering the NES phenomena is developing 20 . The discussion including anisotropic effects will be made in the subsequent analysis.…”
Section: Discussionmentioning
confidence: 99%
“…For detailed evaluation, more sophisticated simulations considering the anisotropy of the plasma would be necessary. Currently the analysis using the particle simulation code considering the NES phenomena is developing 20 . The discussion including anisotropic effects will be made in the subsequent analysis.…”
Section: Discussionmentioning
confidence: 99%
“…According to the treatment developed by our research group, [34][35][36][37][38][39][40] the new velocity of the scattered ion is calculated using Equation ( 1) and is shown in Figure 3.…”
Section: Treatment Of Elastic Scattering In the Orbital Calculationmentioning
confidence: 99%
“…Figure 4 shows the change of the ion and neutral particle velocities before and after the elastic scattering. The scattered ion velocity is expressed by the probability distribution function [13,14]. P represents the probability that an ion velocity changes from − → v ı to − → v ı as a result of a collision with a neutral particle that has velocity − → v n in the laboratory system.…”
Section: Large-angle Elastic Scattering Transport Model: the El Modelmentioning
confidence: 99%
“…In this work, the probability distribution function [13,14] (described in section 2.4) was applied to fluid equations forthe plasma, and the transport driven by largeangle elastic scattering between ions and neutral particles was studied including the radial direction. Furthermore, Fig.…”
Section: Introductionmentioning
confidence: 99%