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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">mateltech</journal-id><journal-title-group><journal-title xml:lang="ru">Известия высших учебных заведений. Материалы электронной техники</journal-title><trans-title-group xml:lang="en"><trans-title>Izvestiya Vysshikh Uchebnykh Zavedenii. Materialy Elektronnoi Tekhniki = Materials of Electronics Engineering</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">1609-3577</issn><issn pub-type="epub">2413-6387</issn><publisher><publisher-name>MISIS</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.17073/1609-3577-2017-4-239-255</article-id><article-id custom-type="elpub" pub-id-type="custom">mateltech-214</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><subj-group subj-group-type="section-heading" xml:lang="en"><subject>ARTICLES</subject></subj-group></article-categories><title-group><article-title>Использование Оже-электронной спектроскопии  и спектроскопии характерных потерь энергии электронов  для комплексного анализа двумерных покрытий  и процесса их роста</article-title><trans-title-group xml:lang="en"><trans-title>The use of AES and EELS for complex analysis of two-dimensional coatings and their growth process</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>Плюснин</surname><given-names>Н. И.</given-names></name><name name-style="western" xml:lang="en"><surname>Plyusnin</surname><given-names>N. I.</given-names></name></name-alternatives><bio xml:lang="ru"><p>ул. Радио, д. 5, Владивосток, 690041</p><p>Плюснин Николай Инокентьевич — доктор физ.-мат. наук, доцент, главный научный сотрудник</p></bio><bio xml:lang="en"><p>5 Radio Str., Vladivostok 690041</p><p>Nikolay I. Plyusnin: Dr. Sci. (Phys.-Math.), Chief Researcher, Department of Physics of Nanostructures</p></bio><email xlink:type="simple">plusnin@iacp.dvo.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт автоматики и процессов управления ДВО РАН</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Institute of Automation and Control Processes of the Far Eastern Branch of the Russian Academy of Sciences</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2017</year></pub-date><pub-date pub-type="epub"><day>14</day><month>11</month><year>2017</year></pub-date><volume>20</volume><issue>4</issue><fpage>239</fpage><lpage>255</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Плюснин Н.И., 2019</copyright-statement><copyright-year>2019</copyright-year><copyright-holder xml:lang="ru">Плюснин Н.И.</copyright-holder><copyright-holder xml:lang="en">Plyusnin N.I.</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://met.misis.ru/jour/article/view/214">https://met.misis.ru/jour/article/view/214</self-uri><abstract><p>Выявлены дополнительные возможности для комплексного анализа двумерных покрытий (толщиной &lt;1 нм или &lt;10 ML), выращенных физическим осаждением в паровой фазе на подложке монокристаллического кремния. Рост покрытий проводили при двух режимах осаждения: низкотемпературном (при пониженной температуре пучка); и обычном (при повышенной температуре пучка). Покрытия, в том числе в виде чистого металла и силицидной смеси, и их границу раздела с подложкой анализировали методами Оже-электронной спектроскопии (ЭОС) и спектроскопии характерных потерь энергии электронов (СХПЭ). Для обеспечения обоих режимов осаждения, была разработана технология осаждения из ленточного источника. Традиционное использование ЭОС ограничено определением состава элементов, энергетической электронной структуры и толщины покрытия. А применение СХПЭ — определением типа фаз (по плотности валентных электронов) и стадий их образования. Одновременное использование обоих методов и выбор равной (и минимальной) глубины зондирования, ~2,5 нм (за счет установки энергии первичных электронов 300 эВ) обеспечили новые возможности для исследования субнанометровых и двумерных покрытий. В частности, стало возможным сопоставление состава покрытий и их плотности. Выбранная глубина зондирования позволила охватить также их границу раздела. При этом одинаковая глубина зондирования дала возможность использовать толщину покрытия, полученную из данных ЭОС, для анализа данных СХПЭ. Рассмотрены зависимости: а) энергии плазмонного сателлита Оже-пика в зависимости от толщины покрытия для анализа изменений электронной плотности в приграничном слое кремния; б) затухания Оже-сигнала, генерируемого маркерными атомами на границе раздела между покрытием и подложкой, для локализации мест адсорбции осажденных атомов; в) интенсивности и энергии пиков потерь в спектрах СХПЭ от энергии первичных электронов для профилирования состава покрытий по глубине. Использование двух функций затухания по глубине для двух глубин зондирования сделало возможным количественный Оже-анализ неоднородных по толщине покрытий. Все это позволило более полно охарактеризовать как сами двумерные покрытия, так и приграничный слой подложки, а также процессы их образования. В частности, впервые идентифицирован смачивающий нанофазный слой металла на кремниевой подложке, исследован процесс его образования и показано, как его состав зависит от режимов парофазного физического осаждения.</p></abstract><trans-abstract xml:lang="en"><p>Additional possibilities for complex analysis of two-dimensional coatings (thickness &lt;1 nm or &lt;10 ML) grown by physical vapor deposition (PVD) on a single-crystal silicon substrate under two deposition regimes are revealed: 1) low-temperature (at low beam temperature) and 2) high-temperature (at an elevated temperature of the beam), respectively. Coatings, including in the form of pure metal and a silicide mixture, and their interface with the substrate were analyzed by Auger electron spectroscopy (AES) and characteristic electron energy loss spectroscopy (EELS). To ensure both deposition regimes, a technology of the deposition from the ribboned source was developed. The traditional use of AES is limited to determining the composition of the elements, the energy electronic structure, and the thickness of the coating. And EELS — the types of phases (the density of valence electrons) and the stages of their formation. The simultaneous use of both methods and the choice of equal (and minimal) probing depths, ~ 2.5 nm (primary electron energy 300 eV), provided new possibilities for studying subnanometric two-dimensional coatings, in particular, — for comparison of the composition of coatings and their density. The chosen probing depth made it possible to characterize also interface between coating and substrate. At the same time, the same probing depth made it possible to use the thickness of the coating obtained from the AES data to analyze the data of the EELS. In addition, other possibilities are considered. This is the use of dependencies: a) the energy of the plasmon satellite of Auger peak, depending on the thickness of the coating, for analyzing changes in the electron density in the near-interface layer of silicon; B) attenuation of the Auger signal generated by marker atoms at the interface between the coating and the substrate to localize the places of adsorption of deposited atoms; and c) the intensity and energy of the loss peaks in the EELS in dependence on the primary-electron energy for profiling the composition of coatings over the depth. The use of two attenuation functions for two depths of probing provided a quantitative Auger analysis of binary coatings. All this made it possible to characterize more fully both the two-dimensional coatings themselves and the interface layer of the substrate, as well as the processes of their formation. And, in particular, this made it possible to identify for the first time the wetting nanophase layer of metal on a silicon substrate, to investigate the process of its formation and to show how its composition depends on the modes of vapor-phase physical deposition.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>Оже-электронная спектроскопия</kwd><kwd>спектроскопия характерных потерь энергии электронов</kwd><kwd>двумерные покрытия</kwd><kwd>смачивающий нанофазный слой</kwd><kwd>количественный Оже-анализ</kwd><kwd>локализация мест адсорбции</kwd><kwd>металл</kwd><kwd>силицид</kwd><kwd>кремний</kwd></kwd-group><kwd-group xml:lang="en"><kwd>PVD</kwd><kwd>AES</kwd><kwd>EELS</kwd><kwd>two-dimensional coatings</kwd><kwd>wetting nanophase layer</kwd><kwd>sub-nanometer thickness</kwd><kwd>quantitative Auger analysis</kwd><kwd>plasmon satellite of Auger peak</kwd><kwd>localization of places of adsorption</kwd><kwd>EELS depth profiling</kwd><kwd>metal</kwd><kwd>silicide</kwd><kwd>silicon</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">Fiori G., Bonaccorso F., Iannaccone G., Palacios T., Neumaier D., Seabaugh A., Banerjee S. 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