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Dive into the research topics where A. A. Zenin is active.

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Featured researches published by A. A. Zenin.


Technical Physics Letters | 2013

Generating stationary electron beams by a forevacuum plasma source at pressures up to 100 Pa

A. A. Zenin; A. S. Klimov; V. A. Burdovitsin; E. M. Oks

It is shown that, as the gas pressure in a forevacuum plasma electron source increases, electric breakdown in the accelerating gap is caused by the reverse flow of ions from plasma that is generated by both the electron beam and high-voltage glow discharge (HGD). By modifying the electrode system geometry in the accelerating gap of the electron source, it is possible to provide for a two-to threefold decrease in the HGD current. This allows the upper pressure in the electron source to be increased up to about 100 Pa when air is used as the working gas and up to 160 Pa in the source filled with helium.


Technical Physics | 2012

Expansion of the working range of forevacuum plasma electron sources toward higher pressures

V. A. Burdovitsin; A. K. Goreev; A. S. Klimov; A. A. Zenin; E. M. Oks

It is shown that the pressure in forevacuum plasma electron sources is limited from above by a current component that arises in the accelerating gap from a high-voltage glow discharge and dominates in the electron beam. The working pressure range of such electron sources can be expanded toward higher pressures by limiting the current of the high-voltage glow discharge in the accelerating gap.


Technical Physics Letters | 2016

Electron beam focusing features in a plasma electron source under forevacuum pressures

A. A. Zenin; I. Yu. Bakeev; Yu. A. Burachevskii; A. S. Klimov; E. M. Oks

Features of focusing electron beams generated by a forevacuum plasma source under pressures of 10–30 Pa are investigated and the principle possibility of obtaining submillimeter beams is demonstrated. A beam power density of 105 W/cm2 is reached at an electron beam diameter of 0.6 mm. The obtained beam parameters offer opportunities for precision electron beam processing of dielectric materials, including hightemperature alumina ceramics.


Technical Physics Letters | 2015

Specific features of the charge neutralization of silicon carbide in sintering by electron beam in the forevacuum range of pressures

A. S. Klimov; V. A. Burdovitsin; A. A. Zenin; E. M. Oks; Oleg L. Khasanov; Edgar S. Dvilis; A. O. Khasanov

It is shown that a noticeable role in the electron beam charge neutralization in the course of electron-beam sintering of compacted silicon carbide samples is played, as the sample temperature increases, by the electrical conductivity of a sample being sintered, as well as by thermionic emission from its surface. Experimental results obtained for compacted silicon carbide are used to determine its energy gap width and the electron work function.


Advanced Materials Research | 2013

Electron Beam Sintering of Zirconia Ceramics

Victor Burdovitsin; Edgar S. Dvilis; A. A. Zenin; A. S. Klimov; E. M. Oks; Vitaliy Sokolov; Artem Kachaev; Oleg L. Khasanov

The work demonstrated the sintering of zirconium dioxide ceramics by means of an electron beam produced by a plasma-cathode e-beam source operating at fore-vacuum pressure. The sintered ceramics consist of tetragonal-modified zirconium dioxide with grain size from 0.7 to 10 micrometers, depending on the sintering conditions. At constant sintering temperature, the density of the material and its grain size depend on the integrated energy injected into the sintered material by the electron beam.


PROSPECTS OF FUNDAMENTAL SCIENCES DEVELOPMENT (PFSD-2017): Proceedings of the XIV International Conference of Students and Young Scientists | 2017

Plasma density distribution in a plasma source of a ribbon electron beam with an extended hollow cathode

A. S. Klimov; A. A. Zenin; E. M. Oks

The paper presents a study of the influence of the hollow cathode geometry in a plasma electron source on the plasma density distribution near the emission boundary and of the features of discharge ignition with an extended hollow cathode at forevacuum pressures. It is shown that the plasma density distribution is mostly influenced by the cathode cavity depth. Decreasing the cavity depth results in distribution maxima at the cavity edges. Decreasing the cavity width gives rise to a maximum in the middle of the cavity. The conditions that provide plasma inhomogeneity no more than 10 % lengthwise the cavity are determined.


PROSPECTS OF FUNDAMENTAL SCIENCES DEVELOPMENT (PFSD-2016): Proceedings of the XIII International Conference of Students and Young Scientists | 2016

Electron beam evaporation of alumina ceramics at forevacuum pressure range

Alexandr Klimov; A. A. Zenin; Yury Yushkov; E. M. Oks

We describe the electron beam evaporation of aluminum oxide ceramic in the pressure range of 5-15 Pa using the forevacuum plasma electron source. In the irradiation of an ceramic target by an electron beam in the fore-vacuum pressure range, the target potential is much lower than the electron beam energy, offering the possibility of direct electron evaporation of insulating ceramic materials. The speed of ceramic evaporation was 4 g/h, while the electron beam power density of 10 kW/cm2. These results open the possibility of effective application of ceramic coatings on the basis of electron-beam technologies in the forevacuum pressure range.


Russian Physics Journal | 2018

Generation of Ribbon Electron Beams by Fore-Vacuum Plasma Sources Based on the Discharge with an Extended Hollow Cathode

A. S. Klimov; E. M. Oks; A. A. Zenin


Plasma Sources Science and Technology | 2018

Generation of high-power-density electron beams by a forevacuum-pressure plasma-cathode electron source

I Yu Bakeev; A. S. Klimov; E. M. Oks; A. A. Zenin


MATEC Web of Conferences | 2018

Surface treatment by the ion flow from electron beam generated plasma in the forevacuum pressure range

A. S. Klimov; A. A. Zenin

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E. M. Oks

Tomsk State University of Control Systems and Radio-electronics

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Edgar S. Dvilis

Tomsk Polytechnic University

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Oleg L. Khasanov

Tomsk Polytechnic University

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A. K. Goreev

Tomsk State University of Control Systems and Radio-electronics

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A. O. Khasanov

Tomsk Polytechnic University

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A.V. Kazakov

Tomsk State University of Control Systems and Radio-electronics

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A.V. Medovnik

Tomsk State University of Control Systems and Radio-electronics

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Artem Kachaev

Tomsk Polytechnic University

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