Formation of tight plasma pinches and generation of high-power soft x-ray radiation pulses in fast Z-pinch implosions / A. V. Shishlov [et al.]

Уровень набора: Laser Physics = 2006-Альтернативный автор-лицо: Shishlov, A. V., physicist, Associate Professor of Tomsk Polytechnic University, Candidate of physical and mathematical sciences, 1968-, Aleksandr Viktorovich;Baksht, R. V.;Chaikovsky, S. A.;Fedunin, A. V.;Fursov, F. I.;Kokshenev, V. A.;Kurmaev, N. E.;Labetsky, A. Yu.;Oreshkin, V. I., specialist in the field of non-destructive testing, Senior researcher of Tomsk Polytechnic University, Doctor of physical and mathematical sciences, 1960-, Vladimir Ivanovich;Ratakhin, N. A., physicist, Head of the Department of Tomsk Polytechnic University, Doctor of physical and mathematical sciences, 1950-, Nikolay Aleksandrovich;Russkikh, A. G.;Shlykhtun, S. V.Язык: английский.Резюме или реферат: Argon K-shell plasma radiation source experiments were carried out on the GIT-12 generator [Bugaev, S.P. et al., 1997, Russian Phys. Journal, 40, 38] for a long (300 ns) implosion regime. The performance of a shell-on-solid-fill double gas puff was characterized in the experiments with and without an external axial magnetic field. The maximum Ar K-shell radiation yield registered in the experiments without an axial magnetic field was at the level of 1100 J/cm. This yield is consistent with the theoretically predicted yield for a short (100 ns) implosion regime. The experiments showed that the initial magnetic field which provides stabilization of the shell-on-solid-fill double gas puff was lower than that required for stabilization of a single annular gas puff. Satisfactory stabilization of the double gas puff was observed at an initial axial magnetic field of 1.4 kG. The maximum Ar K-shell radiation yield registered in the experiments with the axial magnetic field did not exceed 400 J/cm. A sharp reduction of the K-shell yield cannot be explained only by taking into account the energy losses associated with the compression of the axial magnetic field..Примечания о наличии в документе библиографии/указателя: [References: p. 193 (24 tit.].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ | генерация импульсов | рентгеновские излучения Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: p. 193 (24 tit.]

Argon K-shell plasma radiation source experiments were carried out on the GIT-12 generator [Bugaev, S.P. et al., 1997, Russian Phys. Journal, 40, 38] for a long (300 ns) implosion regime. The performance of a shell-on-solid-fill double gas puff was characterized in the experiments with and without an external axial magnetic field. The maximum Ar K-shell radiation yield registered in the experiments without an axial magnetic field was at the level of 1100 J/cm. This yield is consistent with the theoretically predicted yield for a short (100 ns) implosion regime. The experiments showed that the initial magnetic field which provides stabilization of the shell-on-solid-fill double gas puff was lower than that required for stabilization of a single annular gas puff. Satisfactory stabilization of the double gas puff was observed at an initial axial magnetic field of 1.4 kG. The maximum Ar K-shell radiation yield registered in the experiments with the axial magnetic field did not exceed 400 J/cm. A sharp reduction of the K-shell yield cannot be explained only by taking into account the energy losses associated with the compression of the axial magnetic field.

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