<SUP>3</SUP>He<SUP>3</SUP>He核融合反応プラズマからの中性子発生の概算
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概要
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A qualitative estimation is presented for the yields of neutron and <SUP>7</SUP>Be frrara <SUP>3</SUP>He <SUP>3</SUP>He fusion plasma by the following reactions: <SUP>3</SUP>He (<SUP>3</SUP>He, n) <SUP>5</SUP>Be, (γ, n) reaction of the structure material (SUS316) by 10MeV γ-ray of <SUP>3</SUP>He (<SUP>3</SUP>He, γ) He (p, n) 3p by reaction product of protons, and, <SUP>3</SUP>He (α, n) <SUP>6</SUP>Be and <SUP>3</SUP>He (α γ) <SUP>7</SUP>Be by the same product of α Since both reactions of <SUP>3</SUP>He (<SUP>3</SUP>He, n) <SUP>5</SUP>Be and <SUP>3</SUP>He (p, n) <SUP>3</SUP>p have threshold energy of-20 MeV and 10.27 MeV, respectively, neutron yield rapidly increases as ion temperature in plasma increases: i. e. the values of the fraction of the total energy released in the reaction that is carried by neutrons, “Neutronicism” are 3×10<SUP>-5</SUP> and 0.005 at ion temperature of 300 find 800 keV in the plasma with the same electron temperature, respectively. The yields by the (γ, n) reaction and <SUP>3</SUP>He (αn) <SUP>6</SUP>Be are less than the others. The yield of 7Be is 9×10<SUP>-5</SUP> one <SUP>3</SUP>He <SUP>3</SUP>He fusion reaction and <SUP>4</SUP>He impurity concentration in the plasma.
- 社団法人 プラズマ・核融合学会の論文