Ya. E. Krasik

Plasma‐assisted electron emission from (Pb,La)(Zr,Ti)O3 ceramic cathodes

Strong pulsed electron emission has been observed from 12/65/35 lead lanthanum zirconate titanate ceramic composition in two different nonswitched phases at room temperature and at the temperature 100u2009°C. The electron emission parameters of this composition appear to be independent of phase for the two phases investigated. Fast photography and direct observation show that the strong electron emission occurs from the surface discharge plasma. The new experimental data make it possible to demonstrate the validity of the Child–Langmuir law for this electron emitter. A pulsed plasma lead lanthanum zirconate titanate ceramic cathode with burst frequency up to 100 kHz and collector current density up to 10 A/cm2 is developed.

Surface discharge plasma induced by spontaneous polarization switching

A flashover plasma has been induced by spontaneous polarization switching on a polar surface of the ferroelectric crystal triglycine sulphate (TGS). The effect has not been observed in the paraelectric phase. The threshold switching voltage for a surface flashover ignition was as low as 100 V for pulsed and ac voltage. A mechanism of plasma initiation on a ferroelectric surface is proposed. It is assumed that the plasma is ignited by electron emission initiated by polarization switching. Subsequent electron avalanching occurs as a result of the high potential gradient along the ferroelectric surface caused by inhomogeneous polarization switching. Electrons and ions with energies up to several hundreds of eV were been recorded due to a high surface potential of the switched ferroelectric.

Copious electron emission from triglycine sulfate ferroelectric crystals

It is shown experimentally that the electron charge emitted from triglycine sulfate pulse ferroelectric cathodes can be as large as 129 μC/cm2. This charge considerably exceeds the measured value of spontaneous polarization, Ps=2.8 μC/cm2. A bipolar voltage is found to facilitate the appearance of the electron emission. It is proposed that the source of the emission current is the plasma of uncompleted surface discharges. This plasma is initiated at the metal‐vacuum‐dielectric triple points both by the field electron emission and the electron emission stimulated by polarization switching.

Observations of two-dimensional magnetic field evolution in a plasma opening switch

The time dependent magnetic field distribution was studied in a coaxial 100-ns positive-polarity Plasma Opening Switch (POS) by observing the Zeeman effect in ionic line emission. Measurements local in three dimensions are obtained by doping the plasma using laser evaporation techniques. Fast magnetic field penetration with a relatively sharp magnetic field front (⩽1 cm) is observed at the early stages of the pulse (t≲25). Later in the pulse, the magnetic field is observed at the load-side edge of the plasma, leaving “islands” of low magnetic field at the plasma center that last for about 10 ns. The two-dimensional (2-D) structure of the magnetic field in the r,z plane is compared to the results of an analytical model based on electron-magneto-hydrodynamics, that utilizes the measured 2-D plasma density distribution and assumes fast magnetic field penetration along both POS electrodes. The model results provide quantitative explanation for the magnetic field evolution observed.

Spectroscopic investigation of fast (ns) magnetic field penetration in a plasma

The time‐dependent magnetic field spatial distribution in a coaxial positive‐polarity plasma opening switch (POS) carrying a current ≂135 kA during ≂100 ns, was investigated by two methods. In the first, ionic line emission was observed simultaneously for two polarizations to yield the Doppler and Zeeman contributions to the line profiles. In the second method, the axial velocity distribution of ions was determined, giving the magnetic field through the ion equation of motion. This method requires knowledge of the electron density, here obtained from the observed particle ionization times. To this end, a lower bound for the electron kinetic energy was determined using various line intensities and time‐dependent collisional‐radiative calculations. An important necessity for POS studies is the locality of all measurements in r, z, and θ. This was achieved by using laser evaporation to seed the plasma nonperturbingly with the species desired for the various measurements. The Zeeman splitting and the ion moti...

Spectroscopic investigations of the plasma behavior in a plasma opening switch experiment

The electron density, the electron kinetic energy, the particle motion, and electric fields in a coaxial positive‐polarity plasma opening switch (POS) were studied using spectroscopic diagnostics. A gaseous source that injects the plasma radially outward from inside the inner POS electrode was developed. The plasma was locally seeded with various species, desired for the various measurements allowing for axial, radial, and azimuthal resolutions both prior to and during the 180 ns long current pulse. The electron density was determined from particle ionization times and the electron energy from line intensities and time dependent collisional‐radiative calculations. Fluctuating electric fields were studied from Stark broadening. The ion velocity distributions were obtained from emission‐line Doppler broadenings and shifts. The early ion motion, the relatively low ion velocities and the nearly linear velocity dependence on the ion charge‐to‐mass ratio, leads to the conclusion that the magnetic field penetrat...

Visible-light spectroscopy of pulsed-power plasmas (invited)

We describe the investigations of the plasma behavior in three pulsed‐power systems: a magnetically insulated ion diode, and plasma opening switch, and a gas‐puffed Z pinch. Recently developed spectroscopic diagnostic techniques allow for measurements with relatively high spectral, temporal, and spatial resolutions. The particle velocity and density distributions within a few tens of microns from the dielectric‐anode surface are observed using laser spectroscopy. Fluctuating electric fields in the plasma are inferred from anisotropic Stark broadening. For the plasma opening switch experiment, a novel gaseous plasma source was developed which is mounted inside the high‐voltage inner conductor. The properties of this source, together with spectroscopic observations of the electron density and particle velocities of the injected plasma, are described. Emission line intensities during the switch operation are discussed. In the Z‐pinch experiment, spectral emission‐line profiles of various charge‐state ions ar...

Spectroscopic Investigations Of The Plasma Behavior In A Plasma Opening Switch Experiment

Abstracts IEEE hztemational Conference on Plasma Science, Tampa, Florida, 1992 (The Institute of Electrical and Electronics Engineers, New York, 1992), p. 166. 32M. Sarfaty, Ya. E. Krasik, R. Arad, A. Weingarten, S. Shkolnikov, and Y Maron, in Ref. 27, p. 633; A. Weingxten, M.Sc. thesis, Feinberg Graduate School, Weizmann Institute of Science, Israel, 1993. 33M. Sarfaty, R. Arad, Ya. E. Krasik, Y. Maron. B. Peryaslovetz, S. Shkolni- kov, R. Shpitalnik, and A. Weingarten, Bull. Am. Phys. Sot. 38, 1895 (1993). 34Yu. Ralchenko (private communication, 1993). 35H. J. Kunze and H. R. Griem, Phys. Rev. Lett. 21, 1048 (1968). 36G. V. Sholin and E. A. Oks, Sov. Phys. Dokl. 18, 254 (1973). 37H G. Griem, Spectral Line Broadening by Plasmas (Academic, New York 1674). “G Bekefi C. Deutch, and B. Yakobi, in Principles of Laser Plasmas, edited by b. Beketi (Wiley, New York 1976). “E. Sarid. Y. Maron, and L. Troyansky, Phys. Rev. E 48, 1364 (1993). ‘ @H. Tawara, T. Kato, and M. Ohnishi, At. Data Nucl. TabIes 36, 167 (1987);

Novel diagnostic for nonthermal electric fields in plasmas

Two new methods are proposed and illustrated for spectroscopic diagnostics of nonthermal electric fields in plasmas. These methods were used to analyse Hα and Hβ profiles from a Plasma Opening Switch experiment.

Spectroscopic determination of the time dependent magnetic field distribution in pulsed-power plasmas

Summary form only given. Observation of the magnetic field distribution in short-duration plasmas is of major importance since it allows for investigating the field penetration mechanisms and for determining the energy dissipation in the plasma. The current density obtained allows the electron drift velocity to be known, using independent measurement of the electron density. In the case of field diffusion, the penetration depth gives the plasma conductivity yielding the plasma Ohmic heating. Here, we report on the determination of the magnetic field distribution in a coaxial Plasma Opening Switch (POS) and a gas-puffed Z-pinch plasma using two methods: 1) Observation of the Zeeman splitting of emission lines where emissions with two different polarizations were observed in a single discharge in order to discriminate the Zeeman splitting against the inevitable Doppler line broadening of ions moving under the field gradients. 2) Observation of the ion acceleration due to the field gradients from the line Doppler shifts. Together with the electron density determined from particle ionization times and Stark broadening, this yields the magnetic field gradient. For these methods, lines from heavy ions (such as Ba II) and light ions (Li II, C II-C V, Mg II, Ca II), respectively, were used in order to minimize or maximize the Doppler contribution to the line profiles.