Study of background processes with the formation of neutrons in nuclear reactions in the energy range of 26–32 kev

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...

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Veröffentlicht in:Journal of experimental and theoretical physics 2017-11, Vol.125 (5), p.741-751
Hauptverfasser: Bystritsky, V. M., Varlachev, V. A., Dudkin, G. N., Nurkin, A. S., Nechaev, B. A., Padalko, V. N., Pen’kov, F. M., Tuleushev, Yu. Zh, Filipowicz, M., Philippov, A. V.
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container_issue 5
container_start_page 741
container_title Journal of experimental and theoretical physics
container_volume 125
creator Bystritsky, V. M.
Varlachev, V. A.
Dudkin, G. N.
Nurkin, A. S.
Nechaev, B. A.
Padalko, V. N.
Pen’kov, F. M.
Tuleushev, Yu. Zh
Filipowicz, M.
Philippov, A. V.
description 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(4He, γ)6Li 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.
doi_str_mv 10.1134/S1063776117100041
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M. ; Varlachev, V. A. ; Dudkin, G. N. ; Nurkin, A. S. ; Nechaev, B. A. ; Padalko, V. N. ; Pen’kov, F. M. ; Tuleushev, Yu. Zh ; Filipowicz, M. ; Philippov, A. V.</creator><creatorcontrib>Bystritsky, V. M. ; Varlachev, V. A. ; Dudkin, G. N. ; Nurkin, A. S. ; Nechaev, B. A. ; Padalko, V. N. ; Pen’kov, F. M. ; Tuleushev, Yu. Zh ; Filipowicz, M. ; Philippov, A. V.</creatorcontrib><description>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. 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The main contribution to the yields of background neutrons and γ-quanta comes from doubly charged neon ions. 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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(4He, γ)6Li 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. 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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(4He, γ)6Li 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.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S1063776117100041</doi><tpages>11</tpages></addata></record>
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source SpringerLink Journals
subjects Astrophysics
Chains
Classical and Quantum Gravitation
CROSS SECTIONS
Deuteration
Deuterium
DEUTERONS
ELASTIC SCATTERING
Elementary Particles
Fields
Gravitation
Helium
HELIUM 3
HELIUM 4
Hydrogen
HYDROGEN 1
Inelastic scattering
INTERACTIONS
KEV RANGE 10-100
MEV RANGE 01-10
Neon
NEON IONS
NEUTRONS
NUCLEAR PHYSICS AND RADIATION PHYSICS
NUCLEAR REACTIONS
Nuclei
Particle and Nuclear Physics
Particles
Photons
Physics
Physics and Astronomy
Quantum Field Theory
Relativity Theory
Solid State Physics
title Study of background processes with the formation of neutrons in nuclear reactions in the energy range of 26–32 kev
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