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Featured researches published by S.G. Buga.


Carbon | 1998

Structures and physical properties of superhard and ultrahard 3D polymerized fullerites created from solid C60 by high pressure high temperature treatment

V.D. Blank; S.G. Buga; Nadejda R. Serebryanaya; Gennadii A. Dubitsky; B.N. Mavrin; M.Yu. Popov; R.H. Bagramov; V. M. Prokhorov; S.N. Sulyanov; B.A. Kulnitskiy; Ye.V. Tatyanin

Abstract Superhard and ultrahard phases of C60 were synthesized by quenching at high pressures up to 13 GPa and high temperatures in the 300–2100 K range. The structures of the samples are discussed on the basis of X-ray and Raman spectra and electron microscopy data. The following physical properties of hard samples were studied: specific gravity; specific heat in the range 400–600 K; sound velocities; elastic moduli; electrical properties; resistance to uniaxial stress; stability against oxidation. These properties are different from those of diamond and other carbon forms. The hardness of ultrahard fullerites exceeds the hardness of diamond.


Journal of Experimental and Theoretical Physics | 2007

Electronic properties of single-crystal diamonds heavily doped with boron

S.G. Buga; V. D. Blank; S. A. Terent’ev; M. S. Kuznetsov; S. A. Nosukhin; V.A. Kulbachinskii; A. V. Krechetov; V. G. Kytin; G. A. Kytin

Single-crystal diamonds with characteristic sizes of 2–7 mm doped with boron in the concentration range 1019–1020 cm−3 have been grown by the temperature gradient method at high static pressures. The temperature dependence of the resistance R of the synthesized single crystals has been measured in the range 0.5 K < T < 297 K. An activated dependence R(T) with an activation energy of about 50 meV is observed in the range from room temperature to T ≈ 200 K. At temperatures below approximately 50 K, the temperature dependence of the conductivity for heavily doped crystals is proportional to T1/2, which is characteristic of degenerate semiconductors with a high number of defects.


Semiconductors | 2011

Thermoelectric properties of bismuth telluride nanocomposites with fullerene

V.A. Kulbachinskii; V. G. Kytin; V.D. Blank; S.G. Buga; M.Yu. Popov

A nanocomposite material consisting of Bi2Te3 nanocrystals 30 nm in size coated with a C60 molecule layer is obtained. The Hall effect and thermoelectric properties of the composite are studied. The acceptor effect of fullerene in both p- and n-type Bi2Te3 is detected. Nanocomposite material properties are modified due to the formation of layers of fullerene charged molecules: the nanocomposite thermopower increases, while the thermal conductivity decreases.


Instruments and Experimental Techniques | 2009

Fast-response thermistors made of synthetic single-crystal diamonds

V. S. Bormashov; S.G. Buga; V. D. Blank; M. S. Kuznetsov; S. A. Nosukhin; S. A. Terent’ev; E. G. Pel

Miniature thermistors are produced from boron-doped synthetic single-crystal diamonds grown under pressure using the thermal gradient method. It is shown that heavily doped diamonds with a boron concentration of 1019 cm−3 or higher are most suitable for this purpose. In the temperature range of 300–700 K, coefficient β = ln(R1/R2)/(1/T1 − 1/T2) is 2500 K. The characteristic response time of temperature-sensitive elements based on crystals with dimensions of 1 × 1 × 0.3 mm is ∼100 µs; i.e., they can be used in monitoring systems with a response speed of up to 10 kHz.


Journal of Superhard Materials | 2016

Heat capacity of bulk boron-doped single-crystal HPHT diamonds in the temperature range from 2 to 400 K

S.A. Tarelkin; V.S. Bormashov; M. Kuznetsov; S.G. Buga; S. Terentiev; D.D. Prikhodko; Anton Golovanov; V.D. Blank

The heat capacity, Cp, of boron-doped single-crystal diamonds grown by the temperature gradient method was studied. The boron contents were < 1016, ~ 1018, and ~ 1020 cm–3. The heat capacity data for all tested crystals match well (within the measurement accuracy 1%) in the temperature range of 150–400 K and obey the Debye law. At low temperatures the heat capacity follows linear law possibly due to metallic inclusions in diamond bulk. Using this data the amount of metal can be calculated for each sample.


9TH EUROPEAN CONFERENCE ON THERMOELECTRICS: ECT2011 | 2012

Thermoelectric properties of nanostructured Bi-Sb-Te doped with C60

V.A. Kulbachinskii; V. G. Kytin; M. Popov; S.G. Buga; V.D. Blank; P.B. Stepanov

New nanocomposite thermoelectric material composed from nanocrystallites of Bi-Sb-Te alloys covered by C60 molecules has been synthesized and studied. The fullerene molecules provide additional thermal phonons blocking. The observed effects give opportunities for optimizations of transport properties of thermoelectric materials. The figure of merit ZT has increased in relation to starting material by 30% and equals to 1.16 for the optimized thermoelectric nanocomposite of p-type.


Diamond and Related Materials | 2013

Electrical properties of the high quality boron-doped synthetic single-crystal diamonds grown by the temperature gradient method

V.S. Bormashov; S.A. Tarelkin; S.G. Buga; M.S. Kuznetsov; S.A. Terentiev; A.N. Semenov; V.D. Blank


Diamond and Related Materials | 2015

Power high-voltage and fast response Schottky barrier diamond diodes

Vladimir Blank; V.S. Bormashov; S.A. Tarelkin; S.G. Buga; M. S. Kuznetsov; D.V. Teteruk; N.V. Kornilov; S.A. Terentiev; A.P. Volkov


Journal of Solid State Chemistry | 2012

Composites of Bi2–xSbxTe3 nanocrystals and fullerene molecules for thermoelectricity

V.A. Kulbachinskii; V. G. Kytin; M.Yu. Popov; S.G. Buga; P.B. Stepanov; V.D. Blank


Physica Status Solidi (a) | 2015

Development of nuclear microbattery prototype based on Schottky barrier diamond diodes

V.S. Bormashov; Sergey Troschiev; Alexander Volkov; S.A. Tarelkin; Eugeniy Korostylev; Anton Golovanov; Mikhail Kuznetsov; Dmitry Teteruk; Nikolay Kornilov; Sergey Terentiev; S.G. Buga; Vladimir Blank

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V.D. Blank

Russian Academy of Sciences

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V. G. Kytin

Moscow State University

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V.S. Bormashov

Moscow Institute of Physics and Technology

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Vladimir Blank

Moscow Institute of Physics and Technology

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S.A. Tarelkin

National University of Science and Technology

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Nadezhda Serebryanaya

Moscow Institute of Physics and Technology

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G. A. Kytin

Moscow State University

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N.A. Lvova

Moscow Institute of Physics and Technology

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