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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="ru"><front><journal-meta><journal-id journal-id-type="publisher-id">bsuir</journal-id><journal-title-group><journal-title xml:lang="ru">Доклады БГУИР</journal-title><trans-title-group xml:lang="en"><trans-title>Doklady BGUIR</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">1729-7648</issn><issn pub-type="epub">2708-0382</issn><publisher><publisher-name>БГУИР</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.35596/1729-7648-2020-18-3-28-35</article-id><article-id custom-type="elpub" pub-id-type="custom">bsuir-2665</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>ЭЛЕКТРОНИКА, РАДИОФИЗИКА, РАДИОТЕХНИКА, ИНФОРМАТИКА</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>ELECTRONICS, RADIOPHYSICS, RADIOENGINEERING, INFORMATICS</subject></subj-group></article-categories><title-group><article-title>Делокализация электронных состояний В n-Si при низких температурах</article-title><trans-title-group xml:lang="en"><trans-title>Delocalization of electron states in n-Si at low temperatures</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>Данилюк</surname><given-names>А. Л.</given-names></name><name name-style="western" xml:lang="en"><surname>Danilyuk</surname><given-names>A. L.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Кандидат физико-математических наук, доцент, доцент кафедры микро- и наноэлектроники.</p><p>220013, Минск, ул. П. Бровки, 6.</p><p>тел. +375-17-293-23-17</p></bio><bio xml:lang="en"><p>Alexander L. Danilyuk - PhD, Associate Professor, Associate Professor of Micro- and Nanoelectronics Department of Belarusian State University of Informatics and Radioelectronics.</p><p>220013, Minsk, P. Brovka str., 6.</p><p>tel. +375-17-293-23-17</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>Трафименко</surname><given-names>А. Г.</given-names></name><name name-style="western" xml:lang="en"><surname>Trafimenko</surname><given-names>A. G.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Младший научный сотрудник Центра наноэлектроники и новых материалов.</p><p>220013, Минск, ул. П. Бровки, 6.</p><p>тел. +375-17-293-23-17</p></bio><bio xml:lang="en"><p>Anton G. Trafimenko - Junior Researcher of Center of Nanoelectronics and Novel Materials of Belarusian State University of Informatics and Radioelectronics.</p><p>220013, Minsk, P. Brovka str., 6.</p><p>tel. +375-17-293-23-17</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>Федотов</surname><given-names>А. К.</given-names></name><name name-style="western" xml:lang="en"><surname>Fedotov</surname><given-names>A. K.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Доктор физико-математических наук, профессор, главный научный сотрудник лаборатории физики перспективных материалов.</p><p>220013, Минск, ул. П. Бровки, 6.</p><p>тел. +375-17-293-23-17</p></bio><bio xml:lang="en"><p>Alexander K. Fedotov - D.Sci., Professor, Chief Researcher of the Laboratory of Physics of Prospective Materials, Research Institute for Nuclear Problems of Belarusian State University.</p><p>220013, Minsk, P. Brovka str., 6.</p><p>tel. +375-17-293-23-17</p></bio><xref ref-type="aff" rid="aff-2"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Прищепа</surname><given-names>С. Л.</given-names></name><name name-style="western" xml:lang="en"><surname>Prischepa</surname><given-names>S. L.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Прищепа Сергей Леонидович - доктор физико-математических наук, профессор, профессор кафедры защиты информации.</p><p>220013, Минск, ул. П. Бровки, 6.</p><p>тел. +375-17-293-23-17</p></bio><bio xml:lang="en"><p>Serghej L. Prischepa - D.Sci., Professor, Professor of Information Security Department of Belarusian State University of Informatics and Radioelectronics.</p><p>220013, Minsk, P. Brovka str., 6.</p><p>tel. +375-17-293-23-17</p></bio><email xlink:type="simple">prischepa@bsuir.by</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Белорусский государственный университет информатики и радиоэлектроники</institution><country>Беларусь</country></aff><aff xml:lang="en"><institution>Belarusian State University of Informatics and Radioelectronics</institution><country>Belarus</country></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>Научно-исследовательское учреждение «Институт ядерных проблем» Белорусского государственного университета</institution><country>Беларусь</country></aff><aff xml:lang="en"><institution>Research Institute for Nuclear Problems of Belarusian State University</institution><country>Belarus</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2020</year></pub-date><pub-date pub-type="epub"><day>16</day><month>05</month><year>2020</year></pub-date><volume>18</volume><issue>3</issue><fpage>28</fpage><lpage>35</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Данилюк А.Л., Трафименко А.Г., Федотов А.К., Прищепа С.Л., 2020</copyright-statement><copyright-year>2020</copyright-year><copyright-holder xml:lang="ru">Данилюк А.Л., Трафименко А.Г., Федотов А.К., Прищепа С.Л.</copyright-holder><copyright-holder xml:lang="en">Danilyuk A.L., Trafimenko A.G., Fedotov A.K., Prischepa S.L.</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://doklady.bsuir.by/jour/article/view/2665">https://doklady.bsuir.by/jour/article/view/2665</self-uri><abstract><p>Приводятся данные измерений транспортных свойств Si, легированного Sb, в температурном диапазоне 1,9 - 3,0 К и при плотностях токов J&lt; 0,2 А/см2. На основе анализа вольт-амперных характеристик получены значения сопротивления при разных плотностях токов. Обнаружено, что с увеличением тока изменяется знак температурного коэффициента сопротивления. При значениях J &lt; 0,045 А/см2 температурный коэффициент сопротивления положительный, а с превышением плотности тока значения 0,045 А/см2 он становится отрицательным. Для объяснения этого токового кроссовера в знаке температурного коэффициента сопротивления были проведены холловские измерения при температуре 2 К, позволившие определить значения концентрации носителей заряда и их подвижность. На основе этих измерений и с учетом модели концентрационной нестабильности были получены токовые зависимости таких параметров, описывающих электрический транспорт в полупроводниках, как энергия активации, неравновесная концентрация носителей заряда, подвижность и время рассеяния электронов проводимости. В результате проведенного анализа было установлено, что изменение знака температурного коэффициента сопротивления с ростом тока можно объяснить обменом электронами между верхней зоной Хаббарда, формирующейся за счет захвата инжектируемых электронов нейтральными атомами примеси, и краем зоны проводимости. При этом происходит делокализация электронных состояний с ростом тока. Полученные данные хорошо согласуются с выдвинутой гипотезой. Проведено рассмотрение возможных механизмов делокализации путем анализа времени рассеяния электронов. В результате установлено, что электрон-электронные взаимодействия, вызванные кулоновским потенциалом, являются доминирующими.</p></abstract><trans-abstract xml:lang="en"><p>We report on the electric transport properties of Si heavily doped with Sb in the temperature range of 1.9 - 3.0 K and at current density of J &lt; 0.2 A/cm2. Based on the analysis of the current - voltage characteristics, the resistance values at different current densities are obtained. It was found that an increase in current changes the sign of the temperature coefficient of resistance. At J &lt; 0,045 А/cm2, the temperature coefficient of resistance is positive, whereas when the current density exceeds the value of 0,045 А/cm2 it becomes negative. To explain this current crossover in the sign of the temperature coefficient of resistance, we performed Hall measurements at a temperature of 2 K, which allowed us to determine the values of the concentration of charge carriers and their mobility. Based on these measurements and taking into account the concentration instability model, we obtained current dependences of the parameters describing the electric transport in semiconductors, such as activation energy, non-equilibrium concentration of charge carriers, mobility, and scattering time of conduction electrons. As a result of the analysis, it was found that the change in the sign of the temperature coefficient of resistance with an increase in current can be explained by the exchange of electrons between the upper Hubbard band, formed by the capture of injected electrons by neutral impurity atoms, and the edge of the conduction band. In this case, delocalization of electronic states occurs with an increase in current. The data obtained are in good agreement with the proposed hypothesis. Possible delocalization mechanisms are considered by analyzing the electron scattering time. As a result, it was found that electron-electron interactions caused by the Coulomb potential are dominant.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>токовая нестабильность</kwd><kwd>делокализация</kwd><kwd>верхняя зона Хаббарда</kwd><kwd>температурный коэффициент сопротивления</kwd></kwd-group><kwd-group xml:lang="en"><kwd>current instability</kwd><kwd>delocalization</kwd><kwd>upper Hubbard band</kwd><kwd>temperature coefficient of resistance</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">Dobrosavlievic V., Trivedi N., Valles J.M.Jr. Conductor-Insulator Quantum Phase Transitions. Oxford University Press; 2012.</mixed-citation><mixed-citation xml:lang="en">Dobrosavlievic V., Trivedi N., Valles J.M.Jr. Conductor-Insulator Quantum Phase Transitions. 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