Comparable analysis of shielding layer parameters for different target materials under the plasma stream exposure

Numerous experiments on the plasma-wall interaction problem have been performed with the powerful quasistationary plasma accelerator (QSPA) K-50 device during last decades. These investigations were performed with different target materials (carbon, tungsten, steel etc.) at the different plasma stre...

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Збережено в:
Бібліографічні деталі
Дата:2005
Автори: Tsarenko, A.V., Trubchaninov, S.A., Marchenko, A.K., Chebotarev, V.V., Staltsov, V.V., Tereshin, V.I., Garkusha, I.E., Makhlaj, V.A., Solyakov, D.G., Landman, I.S.
Формат: Стаття
Мова:English
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2005
Назва видання:Вопросы атомной науки и техники
Теми:
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/78888
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Comparable analysis of shielding layer parameters for different target materials under the plasma stream exposure / A.V. Tsarenko, S.A. Trubchaninov, A.K. Marchenko, V.V. Chebotarev, V.V. Staltsov, V.I. Tereshin, I.E. Garkusha, V.A. Makhlaj, D.G. Solyakov, I.S. Landman // Вопросы атомной науки и техники. — 2005. — № 1. — С. 107-109. — Бібліогр.: 4 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Резюме:Numerous experiments on the plasma-wall interaction problem have been performed with the powerful quasistationary plasma accelerator (QSPA) K-50 device during last decades. These investigations were performed with different target materials (carbon, tungsten, steel etc.) at the different plasma stream parameters. But such problems as, for example, impact of target material on the basic plasma characteristics at the same plasma stream parameters were unsolved. So this paper is summarizing data of researches of plasma shielding layer using different materials of targets. The plasma parameters (peak values) obtained at the longitudinal magnetic field B=0.54 T were as follows: Ne~10¹⁷ cm⁻³ (measured from Hβ linear Stark-effect), Te~2.7 eV, plasma pressure ~16 Bar. Working gas was hydrogen with a small diagnostics dope of nitrogen.