Acceleration of protons and deuterons up to 35 MeV and generation of 1013 neutrons in a megaampere deuterium gas-puff z-pinch

Xehetasun bibliografikoak
Parent link:Plasma Physics and Controlled Fusion
Vol. 61, iss. 1 : Special Issue Featuring the Invited Talks.— 2019.— [014018, 11 p.]
Egile korporatiboa: Национальный исследовательский Томский политехнический университет Инженерная школа новых производственных технологий Отделение материаловедения, Национальный исследовательский Томский политехнический университет (ТПУ) Физико-технический институт (ФТИ) Лаборатория № 33 ядерного реактора
Beste egile batzuk: Klir D. Daniel, Shishlov A. V. Aleksandr Viktorovich, Kokshenev V. A. Vladimir Alekseevich, Kubes P. Pavel, Rezac K. Karel, Dudkin G. N. Gennadiy Nikolaevich, Padalko V. N. Vladimir Nikolaevich, Ratakhin N. A. Nikolay Aleksandrovich, Varlachev V. A. Valery Aleksandrovich
Gaia:Title screen
The acceleration of hydrogen ions up to 35 MeV is observed in the z-pinch experiments on the GIT-12 generator at a 3 MA current and 0.6 MV driving voltage. High ion energies are obtained with a novel configuration of a deuterium gas-puff z-pinch. In this configuration, a hollow cylindrical plasma shell is injected around an inner deuterium gas puff to form a homogeneous, uniformly conducting layer between electrodes at the initial phase of z-pinch implosion. The stable implosion at the velocity up to 650 km s-1 is important to deliver more current onto the z-pinch axis. Magnetohydrodynamic instabilities become apparent first at stagnation. After the disruptive development of m = 0 instabilities, ~20 ns pulses of high-energy photons, neutrons, electrons, and ions are observed. The average neutron yield is 2 Ч 1012. The ion emission is characterized by various diagnostic techniques including those based on the usage of neutron-producing samples. When a large neutron-producing sample is placed onto the axis below a cathode mesh, the neutron yield is increased up to (1.1 ± 0.3) Ч 1013. Considering a ~130 kJ energy input into z-pinch plasmas and magnetic field, this implies the neutron production efficiency of ~108 neutrons per one Joule of the z-pinch energy.
Режим доступа: по договору с организацией-держателем ресурса
Hizkuntza:ingelesa
Argitaratua: 2019
Gaiak:
Sarrera elektronikoa:https://doi.org/10.1088/1361-6587/aadc99
Formatua: Baliabide elektronikoa Liburu kapitulua
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=659682

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200 1 |a Acceleration of protons and deuterons up to 35 MeV and generation of 1013 neutrons in a megaampere deuterium gas-puff z-pinch  |f D. Klir [et al.] 
203 |a Text  |c electronic 
300 |a Title screen 
320 |a [References: 51 tit.] 
330 |a The acceleration of hydrogen ions up to 35 MeV is observed in the z-pinch experiments on the GIT-12 generator at a 3 MA current and 0.6 MV driving voltage. High ion energies are obtained with a novel configuration of a deuterium gas-puff z-pinch. In this configuration, a hollow cylindrical plasma shell is injected around an inner deuterium gas puff to form a homogeneous, uniformly conducting layer between electrodes at the initial phase of z-pinch implosion. The stable implosion at the velocity up to 650 km s-1 is important to deliver more current onto the z-pinch axis. Magnetohydrodynamic instabilities become apparent first at stagnation. After the disruptive development of m = 0 instabilities, ~20 ns pulses of high-energy photons, neutrons, electrons, and ions are observed. The average neutron yield is 2 Ч 1012. The ion emission is characterized by various diagnostic techniques including those based on the usage of neutron-producing samples. When a large neutron-producing sample is placed onto the axis below a cathode mesh, the neutron yield is increased up to (1.1 ± 0.3) Ч 1013. Considering a ~130 kJ energy input into z-pinch plasmas and magnetic field, this implies the neutron production efficiency of ~108 neutrons per one Joule of the z-pinch energy. 
333 |a Режим доступа: по договору с организацией-держателем ресурса 
461 |t Plasma Physics and Controlled Fusion 
463 |t Vol. 61, iss. 1 : Special Issue Featuring the Invited Talks  |o proceeding of the 45th EPS Conference on Plasma Physics, Prague, 2-6 July 2018  |v [014018, 11 p.]  |d 2019 
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610 1 |a нейтроны 
610 1 |a дейтроны 
610 1 |a генерация 
701 1 |a Klir  |b D.  |g Daniel 
701 1 |a Shishlov  |b A. V.  |c physicist  |c Associate Professor of Tomsk Polytechnic University, Candidate of physical and mathematical sciences  |f 1968-  |g Aleksandr Viktorovich  |3 (RuTPU)RU\TPU\pers\36689 
701 1 |a Kokshenev  |b V. A.  |g Vladimir Alekseevich 
701 1 |a Kubes  |b P.  |g Pavel 
701 1 |a Rezac  |b K.  |g Karel 
701 1 |a Dudkin  |b G. N.  |c specialist in the field of nuclear physics  |c Senior researcher of Tomsk Polytechnic University, Candidate of physical and mathematical sciences  |f 1944-  |g Gennadiy Nikolaevich  |3 (RuTPU)RU\TPU\pers\34190  |9 17724 
701 1 |a Padalko  |b V. N.  |c physicist  |c Leading engineer of Tomsk Polytechnic University  |f 1949-  |g Vladimir Nikolaevich  |3 (RuTPU)RU\TPU\pers\32978 
701 1 |a Ratakhin  |b N. A.  |c physicist  |c Head of the Department of Tomsk Polytechnic University, Doctor of physical and mathematical sciences  |f 1950-  |g Nikolay Aleksandrovich  |3 (RuTPU)RU\TPU\pers\36686 
701 1 |a Varlachev  |b V. A.  |c physicist, specialist in the field of nuclear physics  |c Professor-consultant of Tomsk Polytechnic University, Doctor of Technical Sciences  |f 1948-  |g Valery Aleksandrovich  |y Tomsk  |3 (RuTPU)RU\TPU\pers\33722  |9 17353 
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712 0 2 |a Национальный исследовательский Томский политехнический университет (ТПУ)  |b Физико-технический институт (ФТИ)  |b Лаборатория № 33 ядерного реактора  |3 (RuTPU)RU\TPU\col\19896 
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