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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">radioelectronics</journal-id><journal-title-group><journal-title xml:lang="ru">Известия высших учебных заведений России. Радиоэлектроника</journal-title><trans-title-group xml:lang="en"><trans-title>Journal of the Russian Universities. Radioelectronics</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">1993-8985</issn><issn pub-type="epub">2658-4794</issn><publisher><publisher-name>Saint Petersburg Electrotechnical University</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.32603/1993-8985-2025-28-2-69-79</article-id><article-id custom-type="elpub" pub-id-type="custom">radioelectronics-996</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>МИКРО- И НАНОЭЛЕКТРОНИКА</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>MICRO- AND NANOELECTRONICS</subject></subj-group></article-categories><title-group><article-title>Модель асимметричного сдвига порогового напряжения МОП-структур при термополевых обработках</article-title><trans-title-group xml:lang="en"><trans-title>Modeling Asymmetric Shift in the Threshold Voltage of MOS Structures under Thermal Field Treatment</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0009-0008-1016-1031</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Александров</surname><given-names>О. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Aleksandrov</surname><given-names>O. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Александров Олег Викторович – доктор физико-математических наук (2003), профессор (2008) кафедры электронного приборостроения</p><p>ул. Профессора Попова, д. 5 Ф, Санкт-Петербург, 197022</p></bio><bio xml:lang="en"><p>Oleg V. Aleksandrov, Dr Sci. (Phys.-Math.) (2003), Professor (2008) of the Department of Electronic Instrumentation</p><p>5 F, Professor Popov St., St Petersburg 197022</p></bio><email xlink:type="simple">Aleksandr_ov@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0009-0001-3655-4860</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Морозов</surname><given-names>Н. Н.</given-names></name><name name-style="western" xml:lang="en"><surname>Morozov</surname><given-names>N. N.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Морозов Никита Николаевич – магистр по направлению "Электроника и наноэлектроника" (2022), аспирант и ассистент кафедры электронного приборостроения</p><p>ул. Профессора Попова, д. 5 Ф, Санкт-Петербург, 197022</p></bio><bio xml:lang="en"><p>Nikita N. Morozov, Master's degree in Electronics and Nanoelectronics (2022), Postgraduate student and assistant of the Department of Electronic Instrumentation</p><p>5 F, Professor Popov St., St Petersburg 197022</p></bio><email xlink:type="simple">laughter-maiden@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Санкт-Петербургский государственный электротехнический университет "ЛЭТИ" им. В. И. Ульянова (Ленина)</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Saint Petersburg Electrotechnical University</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2025</year></pub-date><pub-date pub-type="epub"><day>03</day><month>05</month><year>2025</year></pub-date><volume>28</volume><issue>2</issue><fpage>69</fpage><lpage>79</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Александров О.В., Морозов Н.Н., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Александров О.В., Морозов Н.Н.</copyright-holder><copyright-holder xml:lang="en">Aleksandrov O.V., Morozov N.N.</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://re.eltech.ru/jour/article/view/996">https://re.eltech.ru/jour/article/view/996</self-uri><abstract><p>Введение. При термополевых обработках (ТПО) МОП-структур наблюдается нестабильность порогового напряжения, связанная с транспортом подвижных ионов примесей щелочноземельных металлов (в основном Na+) в электрическом поле подзатворного диэлектрика. Экспериментальные кинетики накопления и восстановления подвижного заряда при ТПО отклоняются от известных моделей: диффузионной модели Сноу и модели пограничного захвата Хофстейна.Цель работы. Разработка количественной модели поведения МОП-структур при термополевых обработках в режимах накопления и восстановления подвижного заряда ионной примеси.Материалы и методы. Модель базируется на анализе кинетики захвата подвижных ионов примеси на полиэнергетические ловушки в объеме аморфного подзатворного диэлектрика. На основе анализа физических процессов составлена система дифференциальных уравнений, которая решается методом конечных разностей по явной и неявной разностным схемам.Результаты. Из сопоставления расчетов по модели с литературными экспериментальными данными для временных зависимостей смещения порогового напряжения МОП-структур при положительном и последующем отрицательном смещении затвора определены: диапазон энергий связи, характеристическая энергия дисперсии, концентрации ионов примеси и ловушек вблизи затвора и кремниевой подложки, а также ширина области их локализации. Обнаружено уменьшение диапазона энергий связи вблизи межфазной границы SiO2–Si по сравнению с межфазной границей SiO2–металлический затвор, что может свидетельствовать о наличии упорядоченного тонкого слоя SiO2 вблизи кремния.Заключение. Показано, что процесс восстановления заряда происходит с бóльшей скоростью, чем процесс накопления, вследствие различия в распределениях ловушек вблизи межфазных границ SiO2 с кремниевой подложкой и с затвором. Предложенная модель позволяет описать экспериментальное асимметричное поведение МОП-структур, загрязненных ионами щелочноземельных металлов при ТПО.</p></abstract><trans-abstract xml:lang="en"><p>Introduction. Thermal field treatment (TFT) of MOS structures causes instability of the threshold voltage associated with the transport of mobile ions of alkaline earth metal impurities (mainly Na+) in the electric field of the gate dielectric. Experimental kinetics of accumulation and restoration of the mobile charge during TFT deviate from the known descriptions by Snow’s diffusion and Hofstein’s boundary capture models.Aim. Development of a quantitative model for the behavior of MOS structures during thermal field treatment in the modes of accumulation and restoration of the mobile charge of an ionic impurity.Materials and methods. The model is based on the analysis of the capture kinetics of mobile impurity ions on polyenergetic traps in the volume of an amorphous gate dielectric. Following the analysis of physical processes, a system of differential equations is compiled and solved by the finite difference method using explicit and implicit difference schemes.Results. The conducted comparison of the data calculated by the developed model and the experimental data reported in literature for the time dependencies of the threshold voltage shift of MOS structures with positive and subsequent negative gate bias determined the range of binding energies, the characteristic dispersion energy, the concentrations of impurity ions and traps near the gate and the silicon substrate, and the width of the region of their localization. A decrease in the range of binding energies in the vicinity of the SiO2–Si interface compared to the SiO2–metal gate interface was found, which may indicate the presence of an ordered thin SiO2 layer in the vicinity of silicon.Conclusion. It was shown that the charge recovery process occurs at a higher rate than the accumulation process due to the difference in the distribution of traps in the vicinity of the interphase boundaries of SiO2 with the silicon substrate and with the gate. The proposed model can be used to describe the experimental asymmetric behavior of MOS structures contaminated with alkaline earth metal ions during TFT.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>МОП-структура</kwd><kwd>подзатворный диэлектрик</kwd><kwd>подвижный заряд</kwd><kwd>термополевая обработка</kwd><kwd>дисперсионный транспорт</kwd></kwd-group><kwd-group xml:lang="en"><kwd>MOS structure</kwd><kwd>gate dielectric</kwd><kwd>mobile charge</kwd><kwd>thermal field treatment</kwd><kwd>dispersion transport</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">Bias temperature instability for devices and circuits / Ed. by T. Grasser. New York: Springer, 2013. 810 p. doi: 10.1007/978-1-4614-7909-3</mixed-citation><mixed-citation xml:lang="en">Bias Temperature Instability for Devices and Circuits. Ed. by T. Grasser. 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