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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="en"><front><journal-meta><journal-id journal-id-type="publisher-id">najo</journal-id><journal-title-group><journal-title xml:lang="en">Nanosystems: Physics, Chemistry, Mathematics</journal-title><trans-title-group xml:lang="ru"><trans-title>Наносистемы: физика, химия, математика</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2220-8054</issn><issn pub-type="epub">2305-7971</issn><publisher><publisher-name>Университет ИТМО</publisher-name></publisher></journal-meta><article-meta><article-id custom-type="elpub" pub-id-type="custom">najo-1102</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>Статьи</subject></subj-group></article-categories><title-group><article-title>Stability of 2D triangular lattice under finite biaxial strain</article-title><trans-title-group xml:lang="ru"><trans-title>Устойчивость 2D треугольной решетки при конечном двухосном натяжении</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Подольская</surname><given-names>Е. А.</given-names></name><name name-style="western" xml:lang="en"><surname>Podolskaya</surname><given-names>E. A.</given-names></name></name-alternatives><bio xml:lang="en"><p>Saint-Petersburg</p></bio><email xlink:type="simple">katepodolskaya@gmail.com</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Панченко</surname><given-names>А. Ю.</given-names></name><name name-style="western" xml:lang="en"><surname>Panchenko</surname><given-names>A. Yu.</given-names></name></name-alternatives><bio xml:lang="en"><p>Saint-Petersburg</p></bio><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Кривцов</surname><given-names>А. М.</given-names></name><name name-style="western" xml:lang="en"><surname>Krivtsov</surname><given-names>A. M.</given-names></name></name-alternatives><bio xml:lang="en"><p>Saint-Petersburg</p></bio><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Institute for Problems in Mechanical Engineering (IPME RAS)</institution><country>Russian Federation</country></aff><pub-date pub-type="collection"><year>2011</year></pub-date><pub-date pub-type="epub"><day>17</day><month>08</month><year>2025</year></pub-date><volume>2</volume><issue>2</issue><fpage>84</fpage><lpage>90</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Podolskaya E.A., Panchenko A.y., Krivtsov A.M., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Подольская Е.А., Панченко А.Ю., Кривцов А.М.</copyright-holder><copyright-holder xml:lang="en">Podolskaya E.A., Panchenko A.y., Krivtsov A.M.</copyright-holder><license xml:lang="ru" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>Данная работа распространяется под лицензией Creative Commons Attribution 4.0.</license-p></license><license xml:lang="en" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://nanojournal.ifmo.ru/jour/article/view/1102">https://nanojournal.ifmo.ru/jour/article/view/1102</self-uri><abstract><p>Stability of 2D triangular lattice under finite biaxial strain is investigated. In this work only diagonal strain tensor is regarded. The lattice is considered infinite and consisting of particles which interact by pair force central potential. Dynamic stability criterion is used: frequency of elastic waves is required to be real for any real wave vector. Two stability regions corresponding to horizontal and vertical orientations of the lattice are obtained. It means that a structural transition, which is equal to the change of lattice orientation, is possible. The regions’ boundaries are explained: wave equation coefficients change their signs at the border, as well as Young modulae and shear modulae. The results are proved by direct numerical simulation.</p></abstract><trans-abstract xml:lang="ru"><p>.</p></trans-abstract><kwd-group xml:lang="en"><kwd>stability</kwd><kwd>triangular lattice</kwd><kwd>finite strain</kwd><kwd>biaxial strain</kwd><kwd>pair potential</kwd><kwd>elastic wave</kwd><kwd>structural transition</kwd></kwd-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Tkachev P.V., Krivtsov A.M. Stability criterion of internal structure of the material // XXXIII Science week, St. Petersburg State Polytechnical University, Part V, 2004. P. 4–6.</mixed-citation><mixed-citation xml:lang="en">Tkachev P.V., Krivtsov A.M. Stability criterion of internal structure of the material // XXXIII Science week, St. Petersburg State Polytechnical University, Part V, 2004. 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