Abstract:Nuclear elastic scattering is included in the analysis of ignition condition and thermal instability in pure and catalysed D-D fusion reactor plasmas. Nuclear-elastic-scattering events take place, to some extent, during the slowing-down of energetic fusion products and enhance the heating of the background ions. The inclusion of this effect relaxes the minimum of the confinement requirement for self-sustained D-D plasmas by about 15%. It enhances, however, the thermal instability of the plasma, leading to an i… Show more
“…In this manner, the previously proposed method [3,8,9] can prove the presence of a knock-on tail by capturing the quantitative changes of these reaction rates. Although the change in neutron generation rate from the D(d, n) 3 He reaction is smaller than that change in γ-ray generation rate from the 6 Li(d, pγ) 7 Li and 6 Li(d, nγ) 7 Be reactions due to a knock-on tail formation, the higher emission rate from the D(d, n) 3 He reaction can still be expected than that γ-ray generation rate from the 6 Li(d, pγ) 7 Li and 6 Li(d, nγ) 7 Be reactions. The experiment using the proposed method for observing a knock-on tail has been projected on the Large Helical Device (LHD) at National Institute for Fusion Science.…”
Section: Introductionmentioning
confidence: 89%
“…The nonMaxwellian components in the velocity distribution functions via NES are referred to as a "knock-on tail." A knock-on tail has various effects on plasmas, e.g., reaction rate variations [3], spectrum modification of emission particles due to nuclear reactions [4], and ion-heating enhancement [5,6]. It is expected that a knock-on tail would be utilized for diagnosing fusion reactors [7].…”
Section: Introductionmentioning
confidence: 99%
“…This method employed the γ-raygenerating and neutron-generating nuclear reactions, such as 6 Li(d, pγ) 7 Li, 6 Li(d, nγ) 7 Be, and D(d, n) 3 He, occurring in a proton-beam-injected deuterium plasma admixed with a small amount of 6 Li. By injecting a high-energy proton beam into a deuterium plasma, the NES between protons and deuterons causes the formation of a knock-on tail in the high-energy region of the deuteron distribution function.…”
Section: Introductionmentioning
confidence: 99%
“…The following reactions are written as 6 Li(d, nγ) 7 Be, 6 Li(d, pγ) 7 Li, 6 Li(t, dγ) 7 Li, 6 Li(t, pγ) 8 Li, D(d, n) 3 He, D(d, p)T, and T(d, n) 4 He respectively. The cross sections of reactions (1), (2), (5), and (6) are shown in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…The cross sections of reactions (1), (2), and (5) are employed for observing a knock-on tail. Because the 6 Li(d, nγ) 7 Be reaction, whose γ-ray energy is 0.429 MeV, and the 6 Li(d, pγ) 7 Li reaction, whose γ-ray energy is 0.478 MeV, have a reaction threshold, a rapid increase in the reaction rates can be expected by a knockon tail formation in the deuteron distribution function. In this manner, the previously proposed method [3,8,9] can prove the presence of a knock-on tail by capturing the quantitative changes of these reaction rates.…”
It is important to understand the phenomena occurring in nuclear burning plasmas in order to operate fusion reactors. Although multiple studies have been conducted on nuclear elastic scattering (NES), only few experiments have focused on the observation of a knock-on tail via NES in nuclear burning plasmas. NES is an important phenomenon because it occurs in various plasmas and affects their energy balance. As for the observation of a knock-on tail, a method using γ-rays/neutrons generated fromHe + n reactions in a proton-beam-injected deuterium plasma has been proposed. However, there is a possibility to be unable to distinguish whether the main factor affecting the reaction rates is the plasma temperature or the formation of a knock-on tail. To avoid this confusion, herein, we proposed a method based on 6 Li + t → 8 Li * + p or D + t → 4 He + n reactions. These reactions can reveal the plasma temperature without the influence of a knock-on tail because the triton distribution function in deuterium plasmas is remarkably distorted from Maxwellian. The procedure and utilization possibility of the proposed method are discussed.
“…In this manner, the previously proposed method [3,8,9] can prove the presence of a knock-on tail by capturing the quantitative changes of these reaction rates. Although the change in neutron generation rate from the D(d, n) 3 He reaction is smaller than that change in γ-ray generation rate from the 6 Li(d, pγ) 7 Li and 6 Li(d, nγ) 7 Be reactions due to a knock-on tail formation, the higher emission rate from the D(d, n) 3 He reaction can still be expected than that γ-ray generation rate from the 6 Li(d, pγ) 7 Li and 6 Li(d, nγ) 7 Be reactions. The experiment using the proposed method for observing a knock-on tail has been projected on the Large Helical Device (LHD) at National Institute for Fusion Science.…”
Section: Introductionmentioning
confidence: 89%
“…The nonMaxwellian components in the velocity distribution functions via NES are referred to as a "knock-on tail." A knock-on tail has various effects on plasmas, e.g., reaction rate variations [3], spectrum modification of emission particles due to nuclear reactions [4], and ion-heating enhancement [5,6]. It is expected that a knock-on tail would be utilized for diagnosing fusion reactors [7].…”
Section: Introductionmentioning
confidence: 99%
“…This method employed the γ-raygenerating and neutron-generating nuclear reactions, such as 6 Li(d, pγ) 7 Li, 6 Li(d, nγ) 7 Be, and D(d, n) 3 He, occurring in a proton-beam-injected deuterium plasma admixed with a small amount of 6 Li. By injecting a high-energy proton beam into a deuterium plasma, the NES between protons and deuterons causes the formation of a knock-on tail in the high-energy region of the deuteron distribution function.…”
Section: Introductionmentioning
confidence: 99%
“…The following reactions are written as 6 Li(d, nγ) 7 Be, 6 Li(d, pγ) 7 Li, 6 Li(t, dγ) 7 Li, 6 Li(t, pγ) 8 Li, D(d, n) 3 He, D(d, p)T, and T(d, n) 4 He respectively. The cross sections of reactions (1), (2), (5), and (6) are shown in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…The cross sections of reactions (1), (2), and (5) are employed for observing a knock-on tail. Because the 6 Li(d, nγ) 7 Be reaction, whose γ-ray energy is 0.429 MeV, and the 6 Li(d, pγ) 7 Li reaction, whose γ-ray energy is 0.478 MeV, have a reaction threshold, a rapid increase in the reaction rates can be expected by a knockon tail formation in the deuteron distribution function. In this manner, the previously proposed method [3,8,9] can prove the presence of a knock-on tail by capturing the quantitative changes of these reaction rates.…”
It is important to understand the phenomena occurring in nuclear burning plasmas in order to operate fusion reactors. Although multiple studies have been conducted on nuclear elastic scattering (NES), only few experiments have focused on the observation of a knock-on tail via NES in nuclear burning plasmas. NES is an important phenomenon because it occurs in various plasmas and affects their energy balance. As for the observation of a knock-on tail, a method using γ-rays/neutrons generated fromHe + n reactions in a proton-beam-injected deuterium plasma has been proposed. However, there is a possibility to be unable to distinguish whether the main factor affecting the reaction rates is the plasma temperature or the formation of a knock-on tail. To avoid this confusion, herein, we proposed a method based on 6 Li + t → 8 Li * + p or D + t → 4 He + n reactions. These reactions can reveal the plasma temperature without the influence of a knock-on tail because the triton distribution function in deuterium plasmas is remarkably distorted from Maxwellian. The procedure and utilization possibility of the proposed method are discussed.
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