Astrophysical S-factor of T(4He, γ)7Li reaction at Ecm = 15.7 keV / V. M. Bystritsky [et al.]

Уровень набора: Physics of Particles and Nuclei Letters, Scientific JournalАльтернативный автор-лицо: Bystritsky, V. M., Vyacheslav Mikhaylovich;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;Emets, E. G., physicist, specialist in the field of nuclear physics, Engineer-designer of Tomsk Polytechnic University, 1984-, Evgeny Gennadievich;Filipovich, M., Marius;Krylov, A. R., Aleksandr Romanovich;Nechaev, B. A., physicist, leading engineer of Tomsk Polytechnic University, 1945-, Boris Aleksandrovich;Nurkin, А., physicist, engineer of Tomsk Polytechnic University, 1991-, Azamat;Padalko, V. N., physicist, Leading engineer of Tomsk Polytechnic University, 1949-, Vladimir Nikolaevich;Filippov, A. V., Aleksandr Viktorovich;Sadovsky, A. B., Andrey BorisovichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет (ТПУ), Физико-технический институт (ФТИ), Лаборатория № 33 ядерного реактораЯзык: английский.Страна: Россия.Резюме или реферат: The astrophysical S-factor of the reaction T(4He, γ)7Li is measured for the first time at the center of mass energy Ecm = 15.7 keV, lower than the energy range of the Standard Big Bang Nucleosynthesis (SBBN) model. The experiment is performed on a Hall pulsed accelerator (TPU, Tomsk). An acceleration pulse length of 10 μs allows one to suppress the background of cosmic radiation and the ambient medium by five orders of magnitude. A beam intensity of ~ 5 × 10144He+ ions per pulse allows one to measure an extremely low reaction yield. The yield of γ-quanta with the energies Eγ0= 2483.7 keV and Eγ1= 2006.1 keV is registered by NaI(Tl) detectors with the efficiency ε = 0.331 ± 0.026. A method for direct measurement of the background from the chain of reactions T(4He, 4He)T→T(T, 2n)X→(n, γ) and/or (n, n′γ) which ends by neutron activation of materials surrounding the target is proposed and implemented in this study. The value of the astrophysical S-factor of the reaction T(4He, γ)7Li Sαt(Ecm = 15.7 keV) = 0.091 ± 0.032 keV b provides the choice from the set of experimental data for the astrophysical Sαt-factor in favor of experimental data [4] with Sαt(Ecm = 0) = 0.1067 ± 0.0064 keV b..Примечания о наличии в документе библиографии/указателя: [References: p. 570 (32 tit.)].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: p. 570 (32 tit.)]

The astrophysical S-factor of the reaction T(4He, γ)7Li is measured for the first time at the center of mass energy Ecm = 15.7 keV, lower than the energy range of the Standard Big Bang Nucleosynthesis (SBBN) model. The experiment is performed on a Hall pulsed accelerator (TPU, Tomsk). An acceleration pulse length of 10 μs allows one to suppress the background of cosmic radiation and the ambient medium by five orders of magnitude. A beam intensity of ~ 5 × 10144He+ ions per pulse allows one to measure an extremely low reaction yield. The yield of γ-quanta with the energies Eγ0= 2483.7 keV and Eγ1= 2006.1 keV is registered by NaI(Tl) detectors with the efficiency ε = 0.331 ± 0.026. A method for direct measurement of the background from the chain of reactions T(4He, 4He)T→T(T, 2n)X→(n, γ) and/or (n, n′γ) which ends by neutron activation of materials surrounding the target is proposed and implemented in this study. The value of the astrophysical S-factor of the reaction T(4He, γ)7Li Sαt(Ecm = 15.7 keV) = 0.091 ± 0.032 keV b provides the choice from the set of experimental data for the astrophysical Sαt-factor in favor of experimental data [4] with Sαt(Ecm = 0) = 0.1067 ± 0.0064 keV b.

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