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Ivanov, V. A.

Publications and source records attributed to Ivanov, V. A..

Thermodynamic characteristics of praseodymium in the gallium–aluminum eutectic melt

The Ga–Al eutectic melt saturated with praseodymium was studied in the temperature range 572–1076 K by electromotive force (emf) method relative to the reference electrode (In{sub L} + PrIn{sub 3}, where L is the liquid phase) in a LiCl–KCl–CsCl eutectic electrolyte. The partial molar thermodynamic functions (enthalpy, entropy, and Gibbs energy) of praseo dymium in a Ga–Al eutectic melt were calculated. According to the emf measurements of the two-phase Pr–Ga–Al{sub L} + intermetallic compound alloys equilibrated with the Ga–Al eutectic melt saturated with praseodymium, there are intermetallic compounds PrGa{sub 6}, PrGa{sub 4}, and Pr{sub 0.22}Ga{sub 0.78}(PrGa{sub 2}) in the temperature ranges 572–741, 741–883, and 883–1076 K, respectively.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Growth and Elemental Analysis of a Series of KTi{sub 1–x}Zr{sub x}OPO{sub 4} Crystals

Crystals of the KTi{sub 1–x}Zr{sub x}OPO{sub 4} concentration series with a zirconium content y (in atomic fractions) in the melt ranging from 0 to 0.13 have been grown by the flux method. The Zr impurity distribution coefficient in potassium titanyl phosphate crystals at y ≤ 0.07 has been determined by two methods to be 1.64 ± 0.11. Saturation is found to occur at y > 0.07; the zirconium concentration in the samples is about x = 0.12 atomic fractions.

36 MATERIALS SCIENCE↗

MAGO-IX Experiment

The results of the last (in the thermonuclear program “Magnetic compression”) MAGO-IX experiment with a plasma chamber including a third compartment designed to compress plasma with a converging liner are presented. An X-ray pulse consisting of an intense peak of 1-μs duration, followed by a low-intensity tail with a duration of more than 10 μs, was recorded. In the MAGO-IX experiment, the neutrons were generated mainly in the third compartment. A neutron yield of 2 × 10{sup 12} was obtained. The results demonstrate that the expected compression of preheated plasma in chambers similar to MAGO-IX is promising for achieving thermonuclear ignition.

70 PLASMA PHYSICS AND FUSION TECHNOLOGY↗

Specific Features of Vapor–Liquid–Solid Nanostructure Growth on the Surface of SnS Films during Plasma Treatment

The formation of nanostructure arrays on the surface of nanocrystalline tin sulfide (SnS) films during inductively coupled argon plasma treatment is investigated. The parameters of the nanostructures are studied by electron microscopy and energy-dispersive X-ray microanalysis and the main regularities of nanostructure growth are established. It is shown that the SnS nanostructure growth during plasma treatment is complex and involves the vapor–liquid–solid mechanism with self-assembled tin seeds.

36 MATERIALS SCIENCE↗

Spectroscopy of He–Ne afterglow plasma

The afterglow of pulsed low-current discharge in a He–Ne mixture is spectroscopically studied under conditions of competition between the processes of Ne{sub 2}{sup +} and HeNe{sup +} dissociative recombination with electrons, which are the sources of population of excited levels of neon atoms. The behavior of neon spectral lines in the wavelength range of 350–850 nm corresponding to the transitions from the levels of neon atoms of the 2p{sup 5}3p, 2p{sup 5}3d, 2p{sup 5}4p, 2p{sup 5}4d, 2p5{sup 5}s, 2p{sup 5}5d, 2p5{sup 6}s configurations are studied by the multichannel photoncounting method at electron density n{sub e} < 10{sup 11} cm{sup –3} and helium and neon pressures P{sub He} = 38 Torr and P{sub Ne} ≈ 10{sup -5}p{sub He} Distributions of recombination fluxes and population over excited states of the neon atom formed in the afterglow by homo- and heteronuclear ions are found. The data obtained show that vibrationally excited molecular ions make no noticeable contribution to the spectrum of decaying He–Ne plasma.

70 PLASMA PHYSICS AND FUSION TECHNOLOGY↗

Microwave capillary torch as a means for modifying the electrophysical characteristics of metal surfaces

An experiment layout based on a pulsed capillary microwave torch and making it possible to excite an explosive emission microplasma on a metal surface in open air is implemented for the first time. It is shown that a microrelief in the form of micron-size microcraters forms on the initially smooth surface under the action of microsparks. As a result, the maximum secondary electron emission yield σ{sub max} decreases from ∼2 for the untreated surface to ∼0.4 for the rough treated surface and remains low for a long time when exposed to atmospheric air.

70 PLASMA PHYSICS AND FUSION TECHNOLOGY↗

Particle-in-cell simulation of multipactor discharge on a dielectric in a parallel-plate waveguide

An original 2D3V (two-dimensional in coordinate space and three-dimensional in velocity space) particle-in-cell code has been developed for simulation of multipactor discharge on a dielectric in a parallelplate metal waveguide with allowance for secondary electron emission (SEE) from the dielectric surface and waveguide walls, finite temperature of secondary electrons, electron space charge, and elastic and inelastic scattering of electrons from the dielectric and metal surfaces. The code allows one to simulate all stages of the multipactor discharge, from the onset of the electron avalanche to saturation. It is shown that the threshold for the excitation of a single-surface multipactor on a dielectric placed in a low-profile waveguide with absorbing walls increases as compared to that in the case of an unbounded dielectric surface due to escape of electrons onto the waveguide walls. It is found that, depending on the microwave field amplitude and the SEE characteristics of the waveguide walls, the multipactor may operate in two modes. In the first mode, which takes place at relatively low microwave amplitudes, a single-surface multipactor develops only on the dielectric, the surface of which acquires a positively potential with respect to the waveguide walls. In the second mode, which occurs at sufficiently high microwave intensities, a single-surface multipactor on the dielectric and a two-surface multipactor between the waveguide walls operate simultaneously. In this case, both the dielectric surface and the interwall space acquire a negative potential. It is shown that electron scattering from the dielectric surface and waveguide walls results in the appearance of high-energy tails in the electron distribution function.

70 PLASMA PHYSICS AND FUSION TECHNOLOGY↗

Study of the Electron Distribution in GaN and GaAs after γ-Neutron Irradiation

The results of experimental studies of the parameters of GaN and GaAs structures before and after γ-neutron irradiation are reported. A special set of test diodes making it possible to reduce the error in the results of measuring the parameters of the structures, which is important in the design and optimization of the structure of semiconductor devices, is suggested.

36 MATERIALS SCIENCE↗