Inesh Kenzhina

Dr. Inesh Kenzhina


Research Focus & Metrics

Academic Career Length

11Years (2016-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 November 2021 in Fusion Engineering and Design
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Journal Article
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TKTimur Kulsartov
Timur Kulsartov
ASAsset Shaimerdenov
Asset Shaimerdenov
ZZZhanna Zaurbekova
Zhanna Zaurbekova
IKInesh Kenzhina
Inesh Kenzhina
YCYevgen Chikhray
Yevgen Chikhray
YPYuriy Ponkratov
Yuriy Ponkratov

21 September 2020 in Journal of Nanostructure in Chemistry
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Journal Article
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Artem KozlovskiyArtem Kozlovskiy
Artem Kozlovskiy
MZMaxim Zdorovets
Maxim Zdorovets
IKInesh Kenzhina
Inesh Kenzhina
ABA. Berguzinov
A. Berguzinov
Daria TishkevichDaria Tishkevich
Daria Tishkevich
ATA. Trukhanov
A. Trukhanov

17 May 2019 in Nanomaterials
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Journal Article
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KKKayrat Kadyrzhanov
Kayrat Kadyrzhanov
VRVyacheslav Serafimovich Rusakov
Vyacheslav Serafimovich Rusakov
MFMaxim S. Fadeev
Maxim S. Fadeev
TKTatiana Yu Kiseleva
Tatiana Yu Kiseleva
Artem KozlovskiyArtem Kozlovskiy
Artem Kozlovskiy
MZMaxim Zdorovets
Maxim Zdorovets
Hyperfine interactions of 57Fe nuclei in Fe100-xNix nanostructures synthesized in polymer ion-track membranes were studied by Mössbauer spectroscopy. The main part of obtained nanostructures was Fe100-xNix nanotubes with bcc structure for 0 ≤ x ≤ 40, and with fcc structure for 50 ≤ x ≤ 90. The length, outside diameter and wall thickness of nanotubes were 12 μm, 400 ± 10 nm and 120 ± 5 nm respectively. For the studied nanotubes a magnetic texture is observedalong their axis. The average value of the angle between the direction of the Fe atom magnetic moment and the nanotubes axis decreases with increasing of Ni concentration for nanotubes with bcc structure from ~50° to ~40°, and with fcc structure from ~55° to ~46°. The concentration dependences of the hyperfine parameters of nanotubes Mössbauer spectra are qualitatively consistent with the data for bulk polycrystalline samples. With Ni concentration increasing the average value of the hyperfine magnetic field increases from ~328 kOe to ~335 kOe for the bcc structure and drops to ~303 kOe in the transition to the fcc structure and then decreases to ~290 kOe at x = 90. Replacing the Fe atom with the Ni atom in the nearest environment of Fe atom within nanotubes with bcc structure lead to an increase in the hyperfine magnetic field by “6–9 kOe”, and in tubes with fcc structure—to a decrease in the hyperfine magnetic field by “11–16 kOe”. The changes of the quadrupole shift and hyperfine magnetic field are linearly correlated with the coefficient −(15 ± 5)·10−4 mm/s/kOe.

29 June 2022 in Nanomaterials
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MZMaxim Zdorovets
Maxim Zdorovets
DBDaryn B. Borgekov
Daryn B. Borgekov
IZInesh Z. Zhumatayeva
Inesh Z. Zhumatayeva
IKInesh Kenzhina
Inesh Kenzhina
Artem KozlovskiyArtem Kozlovskiy
Artem Kozlovskiy
The aim of this work is to study the effect of lanthanum doping on the phase formation processes in ceramics based on CaTiO3, as well as to evaluate the effectiveness of the ceramics as photocatalysts for the decomposition of the organic dye Rhodamine B. The methods used were scanning electron microscopy to evaluate the morphological features of the synthesized ceramics, X-ray diffraction to determine the phase composition and structural parameters, and UV-Vis spectroscopy to determine the optical properties of the ceramics. During the experiments it was found that an increase in the lanthanum dopant concentration from 0.05 to 0.25 mol leads to the formation of the orthorhombic phase La0.3Ca0.7TiO3 and the displacement from the ceramic structure of the impurity phase TiO2, which presence is typical for the synthesized ceramics by solid-phase synthesis. On the basis of the data of the X-ray phase analysis the dynamics of phase transformations depending on concentration of lanthanum was established: CaTiO3/TiO2 → CaTiO3/La2TiO5 → CaTiO3/La0.3Ca0.7TiO3 → La0.3Ca0.7TiO3. During the determination of photocatalytic activity it was found that the formation of La0.3Ca0.7TiO3 phase leads to an increase in the decomposition rate as well as the degree of mineralization.

1 September 2021 in Fusion Engineering and Design
Verified
Journal Article
Closed access
TKT. Kulsartov
T. Kulsartov
IKInesh Kenzhina
Inesh Kenzhina
ATA. Tolenova
A. Tolenova
YKYe. Kenzhin
Ye. Kenzhin
ASAsset Shaimerdenov
Asset Shaimerdenov
AGA. Gluchshenko
A. Gluchshenko

2 September 2020 in Science and Technology of Nuclear Installations
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Journal Article
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KSKuanysh Samarkhanov
Kuanysh Samarkhanov
MKMendykhan Khasenov
Mendykhan Khasenov
EBErlan Batyrbekov
Erlan Batyrbekov
IKInesh Kenzhina
Inesh Kenzhina
YSYerzhan Sapatayev
Yerzhan Sapatayev
BBBochkov Bochkov
Bochkov Bochkov
The luminescence of Kr-Xe, Ar-Kr, and Ar-Xe mixtures was studied in the spectral range 300–970 nm when excited by 6Li (n, α)3 H nuclear reaction products in the core of a nuclear reactor. Lithium was deposited on walls of experimental cell in the form of a capillary-porous structure, which made it possible to measure up to a temperature of 730 K. The temperature dependence of the radiation intensity of noble gas atoms, alkali metals, and heteronuclear ionic noble gas molecules was studied. Also, as in the case of single-component gases, the appearance of lithium lines and impurities of sodium and potassium is associated with vaporization during the release of nuclear reaction products from the lithium layer. The excitation of lithium atoms occurs mainly as a result of the Penning process of lithium atoms on noble gas atoms in the 1s states and subsequent ion-molecular reactions. Simultaneous radiation at transitions of atoms of noble gases and lithium, heteronuclear ion molecules of noble gases allows us to increase the efficiency of direct conversion of nuclear energy into light.