<?xml version="1.0" encoding="utf-8"?>
<journal>
  <titleid>https://www.elibrary.ru/title_about_new.asp?i</titleid>
  <issn>1605-8119</issn>
  <journalInfo lang="ENG">
    <title>Materials physics and mechanics</title>
  </journalInfo>
  <issue>
    <volume>39</volume>
    <number>1</number>
    <altNumber> </altNumber>
    <dateUni>2018</dateUni>
    <pages>1-134</pages>
    <articles>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>1-7</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Tver State University</orgName>
              <surname>Alekseev</surname>
              <address>Tver, Russia </address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Krivosheeva</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Shaposhnikov</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="004">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Borisenko</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Lattice thermal conductivity of transition metal dichalcogenides</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Ab initio simulation of phonon spectra and lattice thermal conductivity of monomolecular layers of transition metal dichalcogenides is performed. Size and temperature dependence of lattice thermal conductivity are analyzed and the difference between transition metal dichalcogenides is explained.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_1</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>dichalcogenide</keyword>
            <keyword>phonon</keyword>
            <keyword>thermal conductivity</keyword>
            <keyword>transition metal</keyword>
            <keyword>monolayer</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.1/</furl>
          <file>MPM139_01_alexeev.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>8-14</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Lobachevsky State University of Nizhni Novgorod</orgName>
              <surname>Baranova</surname>
              <address>Nizhni Novgorod, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Hvazdouski</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Stempitsky</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="004">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Vauchok</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="005">
            <individInfo lang="ENG">
              <orgName>University of Bialystok</orgName>
              <surname>Najbuk</surname>
              <address>Bialystok, Poland</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Electronic and optic properties of transition metal dichalcogenides (MoS2, WSe2) and graphene heterostructures</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Double-layer heterostructures were studied. The energetic influence of the quasi-twodimensional materials (MoS2 and WSe2) on the electrical properties of graphene was simulated. Electron density functional (DFT) implemented into VASP program was chosen to take into account van der Waals forces. Interlayer distances were determined for the systems studied by suitable electron density functional (DFT-D2). The distance is 3.50 Å for WSe2/G and 3.45 Å for MoS2/G respectively. Energy band structures were calculated; the influence of electric field on band structure being taken into account. A quantum-mechanical simulation was performed for determining dielectric permittivity, absorption coefficient, reflected index, Brewster angle and the critical angle.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_2</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>ab initio simulation</keyword>
            <keyword>dichalcogenide</keyword>
            <keyword>graphene</keyword>
            <keyword>heterostructure</keyword>
            <keyword>transition metal</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.2/</furl>
          <file>MPM139_02_baranava.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>15-20</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Lobachevsky State University of Nizhni Novgorod</orgName>
              <surname>Baranova</surname>
              <address>Nizhni Novgorod, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Danilyuk</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Stempitsky</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Direct exchange interaction of cobalt chains in zinc oxide: model approach</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Magnetic properties of ZnO with intrinsic point defects, such as Co impurity, were calculated in the framework of quantum-mechanical Heisenberg model. Direct exchange in the chain model of magnetic ion impurities was studied, the magnetic chain was being created in (001) and (100) planes. In both cases the ground states of systems have antiferromagnetic order. Exchange interaction integrals were obtained (-1.5 and 0.5 meV). We have also calculated microscopic magnetic parameters: Curie temperature (Tc_in = 34.04 and Tc_out=10.7 K), stiffness constant (Din=82.4, Dout=25.8 meV Å2), saturation magnetization (Msat_in=2.88×105, Msat_out=2.89×105A/m), exchange constant (Ain=4.46× 10-13 and Aout=1.42×10-12 J/m), and Bloch constant (Bin=6.53×10-5Bout= 3.7×10-4 K3/2). For the energy of magnetic anisotropy of ZnO:Co structure it was found that the easy magnetization axis lies in (100) plane. The value of magnetic anisotropy for the whole cell is 0.06 meV. The anisotropy energy density is 5.54 × 104 J / m3.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_3</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>cobalt impurity</keyword>
            <keyword>density functional theory calculation</keyword>
            <keyword>zinc oxide</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.3/</furl>
          <file>MPM139_03_baranava.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>21-26</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Institute of Theoretical Physics and Astronomy of Vilnius University</orgName>
              <surname>Tamuliene</surname>
              <address>Vilnius, Lithuania</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Ab initio studies of silver precursor for febid: Ag(PMe3)n n=2,3,4</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">The detailed structure, thermal and chemical stability of the Ag(PMe3)n compounds were studied by applying quantum chemical method. The results obtained showed that Ag(PMe3)2 and Ag(PMe3)4 could be used as precursors for FEBID. The appearance energy of Ag was evaluated to find the most promising dissociation ways.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_4</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>Ag compound</keyword>
            <keyword>DFT calculation</keyword>
            <keyword>dissociation</keyword>
            <keyword>precursor</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.4/</furl>
          <file>MPM139_04_tamuliene.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>27-34</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Hvazdouski</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Stempitsky</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Ab initio simulation of graphene interaction with SiO2 substrate for nanoelectronics application</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">First-principles calculations were carried out by the Vienna Ab initio Simulation Package (VASP). Preliminary calculations showed that DFT-D3 method with Becke-Jonson damping present good agreement of lattice constant with experiment data. Ground state of graphene position on the SiO2 surfaces obtained has been determined. Interlayer distances between graphene and different types of quartz substrate have been calculated; the interlayer distances being 3.31 Å and 4.32 Å for models with open oxygen dangling bonds and with open silicon dangling bonds, respectively. The adsorption energy of graphene on the amorphous SiO2 surface with open oxygen dangling bonds is larger than the adsorption energy on the second type of surface. We observed the 0.12 eV band gap in the case with open oxygen dangling bonds. This kind of quartz surface can be source of a charge puddle.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_5</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>ab initio calculation</keyword>
            <keyword>adsorption</keyword>
            <keyword>amorphous SiO2</keyword>
            <keyword>graphene</keyword>
            <keyword>surface</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.5/</furl>
          <file>MPM139_05_hvazdouski.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>35-42</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Skachkova</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Electronic properties of phosphorene with vacancies: ab initio study</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Vacancy influences on phosphorene electronic properties were investigated using Density Functional Theory for structures with one, two and three vacancies. It's shown that divacancy has the minimal formation energy. One and three vacancies lead to magnetic moment emergence on dangling bonds.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_6</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>density functional theory</keyword>
            <keyword>electronic property</keyword>
            <keyword>phosphorene</keyword>
            <keyword>vacancy</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.6/</furl>
          <file>MPM139_06_skachkova.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>43-48</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Melker</surname>
              <initials>A.I.</initials>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Vorobyeva</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Zarafutdinov</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Fullerenes of the Δn=4 series</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Fusion reactions of cages and fullerenes C4, C6 C8, C10, C12 and C14 with each other are modeled on the basis of Arrhenius's postulate. It means that at first there forms an intermediate compound and afterwards a chemical reaction is going on. During the reactions new covalent bonds between the reacting atoms of different fullerenes are formed and old covalent bonds are destroyed. The process is similar to fusion of bubbles in a soap solution. The graphs describing the process are suggested. We have obtained fullerenes C8, C12 C16, C20, C24 and C28 that can be incorporated in the fullerene periodic system as the Δn=4 series.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_7</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>cage</keyword>
            <keyword>energy</keyword>
            <keyword>fullerene</keyword>
            <keyword>fusion reaction</keyword>
            <keyword>graph</keyword>
            <keyword>modeling</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.7/</furl>
          <file>MPM139_07_melker.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>49-55</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Melker</surname>
              <initials>A.I.</initials>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Krupina</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Zarafutdinov</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Fullerenes of the Δn=2 series</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Fusion reactions of triangle C3 and square C4 carbon molecule with each other create elementary fullerenes C6 and C8. In its turn surface reactions of the fullerenes formed with square C4 carbon molecule produce other prism fullerenes C10, C12 and C14. The surface reactions C6 + C4 → (C6 C4) → C10,   C10 + C4 → (C10 C4) → C14,   C8 + C4 → (C8 C4) → C12   are modeled on the basis of Arrhenius's postulate. All the fullerenes obtained constitute the Δn= 2 series fullerenes of the periodic system of basic perfect fullerenes. Together with the Δn= 4 series this series finishes designing the periodic system from above.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_8</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>carbon molecule</keyword>
            <keyword>energy</keyword>
            <keyword>fullerene</keyword>
            <keyword>fusion reaction</keyword>
            <keyword>modeling</keyword>
            <keyword>periodic system</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.8/</furl>
          <file>MPM139_08_melker.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>56-60</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Gerasimov</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Zarafutdinov</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>St.Petersburg State Technological Institute</orgName>
              <surname>Proskurina</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">C60 copper fullerite: synthesis and properties</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Chemical method for copper fullerite synthesis is presented. In order to complete reaction, chemical reagents fullerenol C60OH42 and copper sulphate II CuSO4 were used. The data obtained allow conclude that chemical method for metal fullerites synthesis is perspective for further study.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_9</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>chemical synthesis</keyword>
            <keyword>copper</keyword>
            <keyword>fullerene</keyword>
            <keyword>fullerite</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.9/</furl>
          <file>MPM139_09_gerasimov.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>61-67</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Sanin</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Smirnovsky </surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Stochastic resonances of quantum quartic oscillator</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Quantum oscillator with spatial quartic potential and parametric complement has been investigated in context of the Schrödinger-Langevin-Kostin equation. The properties and stochastic resonances are numerically studied by means of the time realizations for mean coordinate and its Fourier spectra. Analogous effects take place in an empty well.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_10</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>friction</keyword>
            <keyword>quantum quartic oscillator</keyword>
            <keyword>stochastic resonance</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.10/</furl>
          <file>MPM139_10_sanin.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>68-74</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Podryabinkin</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Danilyuk</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Breakdown and conductivity switching in nanosized hafnium dioxide</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Atomic migration and electronic switching of bi-stable centers in conducting filaments formed in nanooxide based resistive random access memory (RRAM) cells are modeled and analyzed as competitive mechanisms determining their operation frequency. They are mediated by the filament growth dynamics. Atomic migration is responsible for a slow change of the filament resistivity with typical switching times in the millisecond range. Fast switching with the shortest nanosecond delay can be achieved using bi-stable electronic centers in the filaments. Possible configurations of such centers are discussed.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_11</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>conductivity switching</keyword>
            <keyword>memory cell</keyword>
            <keyword>nanooxide</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.11/</furl>
          <file>MPM139_11_podryabinkin.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>75-80</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Trafimenko</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Danilyuk</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Emission properties of an array of silicon nanocones</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">In this paper we investigate the emission properties of an array of silicon nanocones containing cobalt nanoparticles at their vertices. Nanocones are formed on a silicon substrate by deposition a cobalt film, processing it to obtain an array of nanoparticles with a diameter of 20-30 nm and subsequent etching of silicon. Nanocones of silicon are separated from the conductive substrate by a layer of silicon oxynitride with the thickness of 8 nm. The results of modeling the current transfer in Si(Sb)/SiOxNy/Co nanocones and an estimation of their emission properties are presented.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_12</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>electron transport</keyword>
            <keyword>emission</keyword>
            <keyword>nanocone</keyword>
            <keyword>oxynitride</keyword>
            <keyword>silicon</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.12/</furl>
          <file>MPM139_12_trafimenko.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>81-86</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Bezrukova</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Vlasova</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Optical characterization of 3D disperse systems with nano- and micro- particles: unique vectors</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Three classes of parameters can be obtained from the different optical methods for nondestructive testing of 3D disperse systems with nano- and microparticles. These optical methods are refractometry, absorbance, fluorescence, light scattering (integral and differential, static and dynamic, unpolarized and polarized). Each of 3D disperse system can be characterized by unique vector in the N-dimensional space of the second-class optical parameters. The phenomenon can be used for elaboration of on-line control of systems with nano- and / or microparticles in the water or air medium.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_13</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>absorbance</keyword>
            <keyword>disperse system</keyword>
            <keyword>fluorescence</keyword>
            <keyword>light scattering</keyword>
            <keyword>nanoparticle</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.13/</furl>
          <file>MPM139_13_bezrukova.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>87-91</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Pechen</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Prudnik</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Interaction of optical waves with a screening thin-film aluminum coating having nickel nanoparticles</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Simulation of interaction of the optical waves (200...1000 nm) with nanostructure aluminum-nickel thin-film shields in the program CST Studio Suit is presented. Relationships between optical properties, substrate temperature and film composition are found.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_14</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>absorption</keyword>
            <keyword>nanoparticle</keyword>
            <keyword>reflection</keyword>
            <keyword>thin film</keyword>
            <keyword>ultraviolet region</keyword>
            <keyword>wavelength</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.14/</furl>
          <file>MPM139_14_pechen.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>92-101</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Lovshenko</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Khanko</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Belarusian State University of Informatics and Radioelectronics</orgName>
              <surname>Stempitsky</surname>
              <address>Minsk, Belarus</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Radiation influence on electrical characteristics of complementary junction field-effect transistors exploited at low temperatures</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Computer simulations of fabrication processing p-and n-channel junction field-effect transistor with design norms of 1.5 µm is presented. Corrections to parameters of Klassen mobility model are proposed. They ensure the correspondence between calculated current-voltage characteristics and experimental data. For the investigated device structures of JFET, an analysis of the influence of various types of penetrating radiation on electrical characteristics is carried out. Optimization calculations gave the modes of processing procedure, which reduce the effect of the neutron flux with energy 1.5 MeV on the electrical characteristics of n-JFET device structure by 1.45 times.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_15</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>computer simulation</keyword>
            <keyword>current-voltage characteristic</keyword>
            <keyword>field-effect transistor</keyword>
            <keyword>neutron</keyword>
            <keyword>radiation</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.15/</furl>
          <file>MPM139_15_lovshenko.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>102-110</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Serikbayev East Kazakhstan State Technical University</orgName>
              <surname>Alontseva</surname>
              <address>Ust-Kamenogorsk, Kazakhstan</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Paton Electric Welding Institute</orgName>
              <surname>Borisov</surname>
              <address>Kiev, Ukraine</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Paton Electric Welding Institute</orgName>
              <surname>Voinarovych</surname>
              <address>Kiev, Ukraine</address>
            </individInfo>
          </author>
          <author num="004">
            <individInfo lang="ENG">
              <orgName>Paton Electric Welding Institute</orgName>
              <surname>Kyslytsia</surname>
              <address>Kiev, Ukraine</address>
            </individInfo>
          </author>
          <author num="005">
            <individInfo lang="ENG">
              <orgName>Serikbayev East Kazakhstan State Technical University</orgName>
              <surname>Prokhorenkova</surname>
              <address>Ust-Kamenogorsk, Kazakhstan</address>
            </individInfo>
          </author>
          <author num="006">
            <individInfo lang="ENG">
              <orgName>Serikbayev East Kazakhstan State Technical University</orgName>
              <surname>Russakova</surname>
              <address>Ust-Kamenogorsk, Kazakhstan</address>
            </individInfo>
          </author>
          <author num="007">
            <individInfo lang="ENG">
              <orgName>Serikbayev East Kazakhstan State Technical University</orgName>
              <surname>Krasavin</surname>
              <address>Ust-Kamenogorsk, Kazakhstan</address>
            </individInfo>
          </author>
          <author num="008">
            <individInfo lang="ENG">
              <orgName>East-Kazakhstan State University</orgName>
              <surname>Bektasova</surname>
              <address>Ust-Kamenogorsk, Kazakhstan</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Development of microplasma spraying technology for applying biocompatible coatings</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">This paper describes the equipment and technology of microplasma spraying from powder and wire materials for applying biocompatible coatings for medical imlants and instruments. The authors observe the challenges and prospects of the implementation of the technology for manufacturing medical products and point out the successful application of microplasma spraying technology for applying biocompatible coatings for hip implants.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_16</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>biocompatible coating</keyword>
            <keyword>hydroxyapatite</keyword>
            <keyword>medical implant</keyword>
            <keyword>microplasma spraying</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.16/</furl>
          <file>MPM139_16_alontseva.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>111-119</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Vasilyev</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Golikov</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Carbon diffusion coefficient in alloyed ferrite</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">A novel expression of carbon diffusivity in pure ferrite has been derived with parameters fitted to known empirical equations and additional experimental data obtained by the tracer atoms method. The expression is then refined by allowance for the alloying effect on the activation energy revealed with available experimental data on Fe-X binary alloys (X = Cr, Mo, Ni, Si) and our investigation of strain aging kinetics in low-carbon automotive BH.steels with various contents of Mn and P.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_17</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>alloy</keyword>
            <keyword>carbon</keyword>
            <keyword>diffusion</keyword>
            <keyword>ferrite</keyword>
            <keyword>steel</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.17/</furl>
          <file>MPM139_17_vasilyev.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>120-127</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Bauman Moscow State Technical University</orgName>
              <surname>Savel'eva</surname>
              <address>Moscow, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Bauman Moscow State Technical University</orgName>
              <surname>Zhuravskii</surname>
              <address>Moscow, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Modeling heat transfer in built-up curvilinear plate</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">A mathematical model of material deposition on a curvilinear surface is constructed. The model considers convective heat transfer, heat transfer by radiation, heat and mass transfer during the material attachment to the surface. The possibility of model modification is shown by considering diffusive transfer of a material and the linear change of curvature through the plate thickness. The numerical algorithm developed allows finding the temperature profile in a curvilinear plate.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_18</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>chemical vapor deposition</keyword>
            <keyword>curvilinear surface</keyword>
            <keyword>numerical modeling</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.18/</furl>
          <file>MPM139_18_saveleva.pdf</file>
        </files>
      </article>
      <article>
        <artType>RAR</artType>
        <langPubl>RUS</langPubl>
        <pages>128-134</pages>
        <authors>
          <author num="001">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Krylov</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="002">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Skotnikova</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="003">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Tsvetkova</surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
          <author num="004">
            <individInfo lang="ENG">
              <orgName>Peter the Great St. Petersburg Polytechnic University</orgName>
              <surname>Ivanova </surname>
              <address>St.Petersburg, Russia</address>
            </individInfo>
          </author>
        </authors>
        <artTitles>
          <artTitle lang="ENG">Resistance to erosive destruction of steam turbine blades from titanium alloys, their structure and phase composition</artTitle>
        </artTitles>
        <abstracts>
          <abstract lang="ENG">Using optical metallography, electron microscopy, X-ray analysis and X-ray microspectral analysis, we have developed a procedure for studying structural and phase transformations in the material of steam turbine blades from titanium alloy VT6 after technological treatments. An attempt was made establish a link between resistance to erosion destruction and structural and phase composition of titanium alloys.</abstract>
        </abstracts>
        <codes>
          <doi>10.18720/MPM.3912018_19</doi>
        </codes>
        <keywords>
          <kwdGroup lang="ENG">
            <keyword>microhardness</keyword>
            <keyword>phase composition</keyword>
            <keyword>steam turbine blade</keyword>
            <keyword>titanium alloy</keyword>
          </kwdGroup>
        </keywords>
        <files>
          <furl>https://mpm.spbstu.ru/article/2018.64.19/</furl>
          <file>MPM139_19_krylov.pdf</file>
        </files>
      </article>
    </articles>
  </issue>
</journal>
