Abstract:The contribution of the electrode material to the formation of the plasma of a low inductive high current vacuum spark and its influence on the process of discharge micropinching were studied using X ray spectroscopy and laser diagnostics. Electrode system configurations are determined in which the contribu tions of the materials of both electrodes to the plasma emitting X rays are comparable and in which the con tribution of one electrode is dominating. It is found that discharge pinching occurs primarily in … Show more
“…We believe that the low energy of electrons in the axial beam was related to the inverse polarity of the voltage applied to electrodes. It has been previously shown [8] that this leads to decrease in the efficiency of pinching in high current low inductance vacuum spark and, hence, in the mag nitude of axial electric field.…”
54Among X ray sources of various types for techno logical and diagnostic applications, a special place belongs to pinched discharges. A characteristic feature of these is that the radiation spectrum contains pho tons with energies significantly exceeding the potential difference between electrodes [1,2]. The origin of this radiation is related to the interaction of discharge plasma and electrode surfaces with high energy elec tron beams formed during local pinching of the plasma column to micron dimensions (micropinch). Information concerning the directional and energy characteristics of such nonthermal electron beams is important for understanding the mechanism of their formation and controlling the radiation parameters.This Letter presents the results of our investigation of nonthermal electron beams formed in plasma of a high current low inductance vacuum spark, which was based on an analysis of the polarization of X ray emission from the discharge plasma.The experiments were performed on a Zona 2 micropinch setup (National Research Nuclear Uni versity MEPhI, Moscow) [3] using an electrode con figuration with inner point anode and outer plane cathode. Both electrodes were made of iron. At an ini tial charging voltage of 15 kV, the maximum discharge current reached 150 kA at a discharge period duration of 8.5 μs. The X ray emission spectrum was measured by two identical FSSR 1D focusing spectrographs with a spatial resolution of ~100 μm in the direction perpendicular to the dispersion plane. The spectro graphs were oriented at an angle of 90° relative to the discharge system axis and arranged so that the disper sion plane of one spectrograph was perpendicular, while that of the other spectrograph was parallel to the discharge axis. The spectra were recorded on an X ray sensitive photographic film. For the adopted adjust ment, the system monitored a spectral interval of 1.83-1.88 Å that contained the lines of helium like FeXXV and lithium like FeXXIV iron ions.Measured radiation intensity I 0 can be treated as a superposition of components with the electric field vectors directed parallel (I || ) and perpendicular (I ⊥ ) to the discharge system axis. Accordingly, one spec trograph separated predominantly the component with the electric field vector parallel to the discharge axis, while the other spectrograph measured the com ponent with perpendicular orientation of the electric field vector. Integral densitograms of the emission spectra over the entire discharge gap are presented in the figure. As can be seen, the characteristic lines of multiply charged ions are observed on the background of a rather intense continuum. The intensity of the continuum with a predominantly perpendicular com ponent I ⊥ is higher than that of the parallel component I || . The spatial region of continuous emission occurs between the point of micropinch localization and the anode.The electron temperature in the micropinch reaches T e > 1 keV. When electrons with these energies interact with atoms and ions in the surrounding plasma, th...
“…We believe that the low energy of electrons in the axial beam was related to the inverse polarity of the voltage applied to electrodes. It has been previously shown [8] that this leads to decrease in the efficiency of pinching in high current low inductance vacuum spark and, hence, in the mag nitude of axial electric field.…”
54Among X ray sources of various types for techno logical and diagnostic applications, a special place belongs to pinched discharges. A characteristic feature of these is that the radiation spectrum contains pho tons with energies significantly exceeding the potential difference between electrodes [1,2]. The origin of this radiation is related to the interaction of discharge plasma and electrode surfaces with high energy elec tron beams formed during local pinching of the plasma column to micron dimensions (micropinch). Information concerning the directional and energy characteristics of such nonthermal electron beams is important for understanding the mechanism of their formation and controlling the radiation parameters.This Letter presents the results of our investigation of nonthermal electron beams formed in plasma of a high current low inductance vacuum spark, which was based on an analysis of the polarization of X ray emission from the discharge plasma.The experiments were performed on a Zona 2 micropinch setup (National Research Nuclear Uni versity MEPhI, Moscow) [3] using an electrode con figuration with inner point anode and outer plane cathode. Both electrodes were made of iron. At an ini tial charging voltage of 15 kV, the maximum discharge current reached 150 kA at a discharge period duration of 8.5 μs. The X ray emission spectrum was measured by two identical FSSR 1D focusing spectrographs with a spatial resolution of ~100 μm in the direction perpendicular to the dispersion plane. The spectro graphs were oriented at an angle of 90° relative to the discharge system axis and arranged so that the disper sion plane of one spectrograph was perpendicular, while that of the other spectrograph was parallel to the discharge axis. The spectra were recorded on an X ray sensitive photographic film. For the adopted adjust ment, the system monitored a spectral interval of 1.83-1.88 Å that contained the lines of helium like FeXXV and lithium like FeXXIV iron ions.Measured radiation intensity I 0 can be treated as a superposition of components with the electric field vectors directed parallel (I || ) and perpendicular (I ⊥ ) to the discharge system axis. Accordingly, one spec trograph separated predominantly the component with the electric field vector parallel to the discharge axis, while the other spectrograph measured the com ponent with perpendicular orientation of the electric field vector. Integral densitograms of the emission spectra over the entire discharge gap are presented in the figure. As can be seen, the characteristic lines of multiply charged ions are observed on the background of a rather intense continuum. The intensity of the continuum with a predominantly perpendicular com ponent I ⊥ is higher than that of the parallel component I || . The spatial region of continuous emission occurs between the point of micropinch localization and the anode.The electron temperature in the micropinch reaches T e > 1 keV. When electrons with these energies interact with atoms and ions in the surrounding plasma, th...
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