Serge A. Beznosyuk

Dr. Serge A. Beznosyuk

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Research Focus & Metrics

Academic Career Length

21Years (2006-Present)

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

Representative Publications

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22 April 2023 in Crystals
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Anastasiya Alexandrovna EliseevaAnastasiya Alexandrovna Eliseeva
Anastasiya Alexandrovna Eliseeva
MKMarina A. Khazanova
Marina A. Khazanova
ACAnna Cheranyova
Anna Cheranyova
IAIrina S. Aliyarova
Irina S. Aliyarova
RKRoman I. Kravchuk
Roman I. Kravchuk
SBSerge A. Beznosyuk
Serge A. Beznosyuk
The cocrystallization of trans-[PtI2(NCN(CH2)5)2] and iodoform (CHI3) yields crystalline adduct trans-[PtI2(NCN(CH2)5)2]∙2CHI3, the structure of which was studied via single-crystal X-ray diffractometry (XRD). In the XRD structure of trans-[PtI2(NCN(CH2)5)2]∙2CHI3, apart from rather predictable C–H∙∙∙I hydrogen bonds (HBs) and C−I∙∙∙I halogen bonds (XBs) with the iodide ligands, we identified C–I∙∙∙Pt metal-involving XBs, where the platinum center functions as an XB acceptor (that includes a metal dz2-orbital) toward the σ-holes of I atoms of CHI3. DFT calculations (PBE-D3/jorge-TZP-DKH with plane waves in the GAPW method) were carried out in the CP2K program for isolated molecules, complex–iodoform clusters, and crystal models with periodic boundary conditions, where the noncovalent nature and the existence of the interactions were confirmed using charge analysis, Wiberg bond indexes, and QTAIM topology analysis of electron density, whereas the philicities of the noncovalent partners were proved using charge analysis, electron localization function, electron density deformation, and one-electron potential projections, as well as electron density/electrostatic potential profiles for cluster models and electrostatic potential surfaces (ρ = 0.001 a.u.) for isolated molecules.

1 January 2017 in Physical Mesomechanics
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SBSerge A. Beznosyuk
Serge A. Beznosyuk
MZM. S. Zhukovsky
M. S. Zhukovsky
The fundamental supra-atomic scale of nanometer attosecond processes in condensed matter creates a multiscale hierarchy of electromechanical interfaces through two-electron dissipation of energy of quantum nanoelectromechanical systems. The space-time scales of electromechanical interfaces are specified, beginning with the subatomic scale of electron Compton length λe, by a sequence of degrees n = 1, 2, 3,... of the fine structure constant α -n. The third scale, with n = 3, corresponds to quantum mesoelectromechanical 2D interfaces which form functional matrices of electromechanical energy stores and converters as active nucleation centers of fractal topological defects in adjacent crystal structure regions. The hierarchy of electromechanical interfaces creates a hierarchy of dissipative structures in mesomechanics of solids and biomimetics of soft materials.

13 September 2013 in Russian Physics Journal
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SBSerge A. Beznosyuk
Serge A. Beznosyuk
MZM. S. Zhukovskii
M. S. Zhukovskii
APA. I. Potekaev
A. I. Potekaev

1 May 2016 in International Journal of Hydrogen Energy
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Journal Article
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SBSerge A. Beznosyuk
Serge A. Beznosyuk
OMO.A. Maslova
O.A. Maslova
MZM.S. Zhukovsky
M.S. Zhukovsky

1 July 2006 in Russian Physics Journal
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AFA. S. Fomin
A. S. Fomin
MZM. S. Zhukovskii
M. S. Zhukovskii
SBSerge A. Beznosyuk
Serge A. Beznosyuk

1 September 2019 in Physical Mesomechanics
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SBSerge A. Beznosyuk
Serge A. Beznosyuk
OMO. A. Maslova
O. A. Maslova
MZM. S. Zhukovsky
M. S. Zhukovsky
The advances in new smart materials are linked with attosecond subatomic technologies which can create entangled subatomic electron pairs by attosecond hard ultraviolet and soft X rays in addition to...