O. Sila
Czech Technical University in Prague
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Featured researches published by O. Sila.
Plasma Physics and Controlled Fusion | 2013
D. Klir; A V Shishlov; V. A. Kokshenev; Pavel Kubes; A Yu Labetsky; K. Rezac; J. Cikhardt; F. I. Fursov; B.M. Kovalchuk; J. Kravarik; N. E. Kurmaev; Nicolai Ratakhin; O. Sila; J Stodulka
Experiments with deuterium (D2) triple shell gas puffs were carried out on the GIT-12 generator at a 3 MA current level and microsecond implosion times. The outer, middle and inner nozzle diameters were 160 mm, 80 mm and 30 mm, respectively. The influence of the mass of deuterium shells on neutron emission times, neutron yields and neutron energy spectra was studied. The injected linear mass of deuterium varied between 50 and 255 µg cm−1. Gas puffs imploded onto the axis before the peak of generator current at 700–1100 ns. Most of the neutrons were emitted during the second neutron pulse after the development of instabilities. Despite higher currents, heavier gas puffs produced lower neutron yields. Optimal mass and a short time delay between the valve opening and the generator triggering were more important than the better coincidence of stagnation with peak current. The peak neutron yield from D(d, n)3He reactions reached 3 × 1011 at 2.8 MA current, 90 µg cm−1 injected linear mass and 37 mm anode–cathode gap. In the case of lower mass shots, a large number of 10 MeV neutrons were produced either by secondary DT reactions or by DD reactions of deuterons with energies above 7 MeV. The average neutron yield ratio Y>10 MeV/Y2.5 MeV reached (6 ± 3) × 10−4. Such a result can be explained by a power law distribution for deuterons as . The optimization of a D2 gas puff Z-pinch and similarities to a plasma focus and its drive parameter are described.
Physics of Plasmas | 2016
D. Klir; A V Shishlov; V. A. Kokshenev; P. Kubes; A Yu Labetsky; K. Rezac; R. K. Cherdizov; J. Cikhardt; B. Cikhardtova; G. N. Dudkin; F. I. Fursov; A A Garapatsky; B.M. Kovalchuk; J. Krása; J. Kravarik; N. E. Kurmaev; H. Orcikova; V. N. Padalko; Nicolai Ratakhin; O. Sila; K. Turek; V. A. Varlachev; A. Velyhan; R. Wagner
A novel configuration of a deuterium z-pinch has been used to generate a nanosecond pulse of fast ions and neutrons. At a 3 MA current, the peak neutron yield of (3.6 ± 0.5) × 1012 was emitted within 20 ns implying the production rate of 1020 neutrons/s. High neutron yields resulted from the magnetization of MeV deuterons inside plasmas. Whereas deuterons were trapped in the radial direction, a lot of fast ions escaped the z-pinch along the z-axis. A large number of >25 MeV ions were emitted into a 250 mrad cone. The cut-off energy of broad energy spectra of hydrogen ions approached 40 MeV. The total number of >1 MeV and >25 MeV deuterons were 1016 and 1013, respectively. Utilizing these ions offers a real possibility of various applications, including the increase of neutron yields or the production of short-lived isotopes in samples placed in ion paths. On the basis of our experiments with various samples, we concluded that a single shot would have been sufficient to obtain GBq positron activity of 13N ...
Acta Polytechnica | 2013
O. Sila; Pavel Kubes; J. Kravarik; K. Rezac; D. Klir; J. Cikhardt
Our work is dedicated to pinch effect occurring during current discharge in deuterium plasma, and our results are connected with two devices – plasma focus PFZ, situated in the Faculty of Electrical Engineering, CTU, Prague, and Z-pinch GIT-12, which is situated in the Institute of High Current Electronics, Tomsk. During fusion reactions that proceed in plasma during discharge, neutrons are produced. We use neutrons as instrument for plasma diagnostics. Despite of the advantage that neutrons do not interact with electric and magnetic fields inside device, they are inevitably scattered by materials that are placed between their source and probe, and information about plasma from which they come from is distorted. For estimation of rate of neutron scattering we use MCNP code.
IEEE Transactions on Plasma Science | 2017
J. Cikhardt; D. Klir; K. Rezac; A. V. Shishlov; R. K. Cherdizov; B. Cikhardtova; G. N. Dudkin; F. I. Fursov; V. A. Kokshenev; J. Kravarik; P. Kubes; N. E. Kurmaev; A. Yu. Labetsky; V. N. Padalko; N. A. Ratakhin; O. Sila; K. Turek; V. A. Varlachev
A set of neutron diagnostics including scintillation time-of-flight detectors, bubble detectors, and several kinds of threshold nuclear activation samples is used to obtain information about the yield and spectrum of the neutrons produced by a deuterium gas-puff z-pinch. The experiments are performed at a current of about 3 MA on the GIT-12 generator at the Institute of High Current Electronics of the Siberian Branch of Russian Academy of Sciences in Tomsk. The average neutron yield in the experiments in 2016 was
Acta Polytechnica | 2013
J. Cikhardt; D. Klir; Pavel Kubes; J. Kravarik; K. Rezac; O. Sila; A. V. Shishlov; Alexey Yu. Labetsky
2.3 \times 10^{12}
Physical Review Letters | 2014
D. Klir; P. Kubes; K. Rezac; J. Cikhardt; J. Kravarik; O. Sila; A. V. Shishlov; B.M. Kovalchuk; N. A. Ratakhin; V. A. Kokshenev; A Yu Labetsky; R. K. Cherdizov; F. I. Fursov; N. E. Kurmaev; G. N. Dudkin; B. A. Nechaev; V. N. Padalko; H. Orcikova; K. Turek
neutrons per single shot. Using the data obtained with the help of neutron activation diagnostics, the time-of-flight detectors have been absolutely calibrated and the broad energy spectrum of the produced neutrons was evaluated. By the calculations presented in this paper, due to the multi-MeV energies of deuterons generated in the pinch, up to 15% of the total neutron yield could be produced by nuclear reactions of deuterons with a stainless steel vacuum chamber and aluminum components of the diagnostic apparatus inside the chamber.
Plasma Physics and Controlled Fusion | 2015
D. Klir; A V Shishlov; V. A. Kokshenev; P. Kubes; A Yu Labetsky; K. Rezac; R. K. Cherdizov; J. Cikhardt; B. Cikhardtova; G. N. Dudkin; F. I. Fursov; A A Garapatsky; B.M. Kovalchuk; J. Kravarik; N. E. Kurmaev; H. Orcikova; V. N. Padalko; Nicolai Ratakhin; O. Sila; K. Turek; V. A. Varlachev
A lot of kinds of instruments are used for the SXR measurement at pulsed power facilities, but most of them are difficult to calibrate absolutely. For the determination of the energy of SXR radiated by the discharge on Z-pinches, it is possible to use the bolometer which can be calibrated analytically. The bolometer can be constructed with the sufficient sensitivity and, at the same time, with the time resolution in the order of nanoseconds. This bolometer was designed and constructed for the measurement on the 5MA facility GIT-12 at the Institute of High Current Electronics (IHCE) of the Siberian Branch Russian Academy of Sciences in Tomsk. The experiments on GIT-12 with the neon and deuterium gas-puff load were diagnosed by the copper bolometer with the time resolution of 4 ns and the sensitivity of 12 V cm2 J-1.
New Journal of Physics | 2018
D. Klir; A. V. Shishlov; V. A. Kokshenev; P. Kubes; K. Rezac; R. K. Cherdizov; J. Cikhardt; B. Cikhardtova; G. N. Dudkin; F. I. Fursov; T Hyhlik; J Kaufman; B.M. Kovalchuk; J. Krása; J. Kravarik; N. E. Kurmaev; A Yu Labetsky; V Munzar; H. Orcikova; V. N. Padalko; N. A. Ratakhin; O. Sila; J Stodulka; K. Turek; V. A. Varlachev; R. Wagner
Plasma Physics and Controlled Fusion | 2018
D. Klir; A. V. Shishlov; V. A. Kokshenev; P. Kubes; K. Rezac; Simona Buryskova; Rustam K Cherdizov; J. Cikhardt; B. Cikhardtova; G. N. Dudkin; Joseph T Engelbrecht; F. I. Fursov; Stuart L. Jackson; J. Krása; Jozef Kravarik; N. E. Kurmaev; Vojtech Munzar; V. N. Padalko; Nikolai A. Ratakhin; O. Sila; Karel Turek; V. A. Varlachev; Richard Wagner
Bulletin of the American Physical Society | 2016
K. Rezac; D. Klir; J. Cikhardt; P. Kubes; O. Sila; J. Kravarik; A. V. Shishlov; A.Yu. Labetsky; R. K. Cherdizov; N. A. Ratakhin; H. Orcikova; K. Turek; N. Dudkin; V. N. Padalko