Alexey V Sobolev

Dr. Alexey V Sobolev

orcid

Research Focus & Metrics

Academic Career Length

25Years (2002-Present)

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

Representative Publications

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4 May 2023 in Chemistry of Materials
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Journal Article
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VSVitalii Shevchenko
Vitalii Shevchenko
IGIana S. Glazkova
Iana S. Glazkova
DNDaniil A. Novichkov
Daniil A. Novichkov
ISIrina Skvortsova
Irina Skvortsova
ASAlexey V Sobolev
Alexey V Sobolev
EAEvgeny Antipov
Evgeny Antipov

23 October 2012 in Dalton Transactions
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Journal Article
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EZE. A. Zvereva
E. A. Zvereva
OSO. A. Savelieva
O. A. Savelieva
YTYa. D. Titov
Ya. D. Titov
MEMaria Evstigneeva
Maria Evstigneeva
VNVladimir B. Nalbandyan
Vladimir B. Nalbandyan
Alexander VasilievAlexander Vasiliev
Alexander Vasiliev
Structure, electrochemical, magnetic and resonance properties of new layered antimonate Li4FeSbO6 were comprehensively studied using powder X-ray diffraction, cyclic voltammetry, magnetic susceptibility, heat capacity, electron spin resonance and Mössbauer spectroscopy. In the crystal structure the iron ions form the triangular network within (LiFeSbO6)3− layers alternating with nonmagnetic lithium layers. The electrochemical activity studied implies an Fe3+/Fe4+ redox couple at 4.3 V (ox.) and 3.9 V (red.) thereby revealing that Li can be reversibly extracted. The long-range antiferromagnetic order was found to occur at the Néel temperature, TN ≈ 3.6 K, confirmed both by the magnetic susceptibility data and specific heat ones. The effective magnetic moment is estimated to be 5.93 μB/f.u. and satisfactorily agrees with theoretical estimations assuming high-spin configuration of Fe3+ (S = 5/2). In the magnetically ordered state, though, the magnetization demonstrates rather peculiar behavior. An additional anomaly on the M(T) curves appears at T2 < TN in moderate magnetic field. The positions of transitions at TN and T2 separate increasingly with increasing external field. Multiple measurements consistently demonstrated field-sensitive moving of magnetic phase boundaries constituting a unique phase diagram for the compound under study. The complex low-dimensional (2D) nature of magnetic coupling was confirmed by the dynamic magnetic properties study. Electron spin resonance from Fe3+ ions in paramagnetic phase is characterized by a temperature independent effective g-factor of 1.99 ± 0.01. However, the distortion and broadening of the ESR line were found to take place upon approaching the magnetically ordered state from above. The divergence of the temperature-dependent linewidth is analyzed in terms of both critical behavior close to long-range magnetic order and the Berezinskii–Kosterlitz–Thouless (BKT)-type transition. Heat capacity measurements even at zero field manifested an appearance of the additional anomaly at temperatures below the Néel temperature. The temperature dependence of ESR intensity, linewidth and shift of the resonant field imply an extended region of short-range order correlations in the compound studied. The rich variety of the anomalies in magnetic and resonance properties makes this new antimonate a very interesting system to investigate the multiple phase transitions and competing exchange interaction due to the critical role of the layered structure organization accompanied by the frustration effects in triangular antiferromagnets.

22 October 2008 in Journal of Materials Chemistry
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AKAndreas Kaltzoglou
Andreas Kaltzoglou
TFThomas Fässler
Thomas Fässler
MCMogens Christensen
Mogens Christensen
SJSimon Johnsen
Simon Johnsen
BIBo Iversen
Bo Iversen
ASAndrei Shevelkov
Andrei Shevelkov
Multi-temperature synchrotron powder diffraction and differential thermal analysis have revealed an enantiotropic order–disorder phase transition in Rb8Sn44□2 and Cs8Sn44□2 at 353 and 363 K, respectively. The low-temperature phases crystallize with a 2 × 2 × 2 superstructure of the conventional type-I clathrate. At higher temperatures both compounds show a phase transition with less ordering of the framework vacancies (□). Rb8Sn44 has a Debye temperature of 152(1) K whereas the Rb atoms in the large cages have Einstein temperatures of 81(1) and 54(1) K for the displacement perpendicular and parallel to the host-structure hexagons. Thermoelectric properties of Rb8Sn44 have been measured from 2 to 400 K. The Seebeck coefficient decreases rapidly above the transition temperature. This is explained by changes in the band structure following the phase transition. The 119Sn Mössbauer spectra for both compounds have also been investigated and their analysis suggests that the transformation occurs without altering the local environment of the tin atoms, but with a variation of the vacancy concentration in the domains of the crystal.

7 March 2008 in Chemistry of Materials
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Journal Article
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JZJulia Zaikina
Julia Zaikina
KKKirill A. Kovnir
Kirill A. Kovnir
ASAlexey V Sobolev
Alexey V Sobolev
IPIgor A. Presniakov
Igor A. Presniakov
VKVladimir G. Kytin
Vladimir G. Kytin
ASAndrei V. Shevelkov
Andrei V. Shevelkov

23 February 2018 in Journal of the American Chemical Society
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Journal Article
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ITIvan V. Tereshchenko
Ivan V. Tereshchenko
DADmitry A. Aksyonov
Dmitry A. Aksyonov
ODOleg Drozhzhin
Oleg Drozhzhin
IPIgor A. Presniakov
Igor A. Presniakov
ASAlexey V Sobolev
Alexey V Sobolev
AAArtem Abakumov
Artem Abakumov

1 June 2007 in Chemistry – A European Journal
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JZJulia Zaikina
Julia Zaikina
KKKirill A. Kovnir
Kirill A. Kovnir
ASAlexey V Sobolev
Alexey V Sobolev
IPIgor A. Presniakov
Igor A. Presniakov
YPYuri Prots
Yuri Prots
Andrei V ShevelkovAndrei V Shevelkov
Andrei V Shevelkov