Study of Background Processes with the Formation of Neutrons in Nuclear Reactions in the Energy Range of 26-32 keV / V. M. Bystritsky [et al.]

Уровень набора: Journal of Experimental and Theoretical Physics, Scientific JournalАльтернативный автор-лицо: Bystritsky, V. M., Vyacheslav Mikhaylovich;Varlachev, V. A., physicist, specialist in the field of nuclear physics, Head of the laboratory of Tomsk Polytechnic University, Candidate of technical sciences, 1948-, Valery Aleksandrovich;Dudkin, G. N., specialist in the field of nuclear physics, Senior researcher of Tomsk Polytechnic University, Candidate of physical and mathematical sciences, 1944-, Gennadiy Nikolaevich;Nurkin, А., physicist, engineer of Tomsk Polytechnic University, 1991-, Azamat;Nechaev, B. A., physicist, leading engineer of Tomsk Polytechnic University, 1945-, Boris Aleksandrovich;Padalko, V. N., physicist, Leading engineer of Tomsk Polytechnic University, 1949-, Vladimir Nikolaevich;Penkov, F. M., Fedor Mikhaylovich;Tuleushev, Y. Z., Yury Zhianshakhovich;Filipowiczd, M., Marius;Filippov, A. V., Aleksandr ViktorovichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет (ТПУ), Физико-технический институт (ФТИ), Лаборатория № 33 ядерного реактораЯзык: английский.Страна: .Серия: Nuclei, particles, fields, gravitation, and astrophysicsРезюме или реферат: The nature of background processes accompanying astrophysical nuclear reactions induced by hydrogen, helium, and neon ions in deuterated targets with small cross sections has been studied in calculations and experiments. The experiments have been performed at a Hall pulsed plasma accelerator in the ion energy range of 26-32 keV. The yield of background neutrons and γ-quanta with energies below 4 MeV in the proton-induced D(p, γ)3 He reaction is primarily due to the presence of a natural impurity of gaseous deuterium in gaseous hydrogen and the chain of D(D, 3 He)n → (n, γ) or (n, n'γ) reactions. A small contribution comes from the chain of D(1 H, 1 H)D → D(D, 3 He)n → (n, γ) or (n, n'γ) reactions. It has been shown that background neutrons and γ-quanta from the D(4 He, γ)6 Li reaction are entirely due to the chain of D(4 He, 4 He)D → D(D, 3 He)n → (n, γ) or (n, n'γ) reactions. It has been shown that the yield of neutrons and γ-ray photons detected at the interaction of neon ions with deuterated targets is also entirely due to the chain of elastic-scattering reactions of neon ions on deuterons in the target and to subsequent inelastic processes of interaction of deuterons accelerated at elastic scattering with other deuterons of the target. The main contribution to the yields of background neutrons and γ-quanta comes from doubly charged neon ions. The main conclusion is that the explanation of the yield of neutrons and γ-quanta at the interaction of hydrogen, helium, and neon ions with deuterated targets does not require “exotic” theoretical models..Примечания о наличии в документе библиографии/указателя: [References: p. 751 (31 tit.)].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ | нейтроны | ядерные реакции | ионы водорода | гелий Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: p. 751 (31 tit.)]

The nature of background processes accompanying astrophysical nuclear reactions induced by hydrogen, helium, and neon ions in deuterated targets with small cross sections has been studied in calculations and experiments. The experiments have been performed at a Hall pulsed plasma accelerator in the ion energy range of 26-32 keV. The yield of background neutrons and γ-quanta with energies below 4 MeV in the proton-induced D(p, γ)3 He reaction is primarily due to the presence of a natural impurity of gaseous deuterium in gaseous hydrogen and the chain of D(D, 3 He)n → (n, γ) or (n, n'γ) reactions. A small contribution comes from the chain of D(1 H, 1 H)D → D(D, 3 He)n → (n, γ) or (n, n'γ) reactions. It has been shown that background neutrons and γ-quanta from the D(4 He, γ)6 Li reaction are entirely due to the chain of D(4 He, 4 He)D → D(D, 3 He)n → (n, γ) or (n, n'γ) reactions. It has been shown that the yield of neutrons and γ-ray photons detected at the interaction of neon ions with deuterated targets is also entirely due to the chain of elastic-scattering reactions of neon ions on deuterons in the target and to subsequent inelastic processes of interaction of deuterons accelerated at elastic scattering with other deuterons of the target. The main contribution to the yields of background neutrons and γ-quanta comes from doubly charged neon ions. The main conclusion is that the explanation of the yield of neutrons and γ-quanta at the interaction of hydrogen, helium, and neon ions with deuterated targets does not require “exotic” theoretical models.

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