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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">npe</journal-id><journal-title-group><journal-title xml:lang="ru">Ядерная физика и инжиниринг</journal-title><trans-title-group xml:lang="en"><trans-title>Nuclear Physics and Engineering</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2079-5629</issn><issn pub-type="epub">2079-5637</issn><publisher><publisher-name>МИФИ</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.56304/S2079562924050373</article-id><article-id custom-type="edn" pub-id-type="custom">NQOHQO</article-id><article-id custom-type="elpub" pub-id-type="custom">npe-439</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>Ускорители заряженных частиц для ядерных технологий</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>Charged Particles Accelerators for Nuclear Technologies</subject></subj-group></article-categories><title-group><article-title>ДИСПЕРСИОННЫЕ СВОЙСТВА УСКОРЯЮЩЕЙ СТРУКТУРЫ SDTL</article-title><trans-title-group xml:lang="en"><trans-title>DISPERSION PROPERTIES OF THE SDTL ACCELERATING STRUCTURE</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>Парамонов</surname><given-names>В. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Paramonov</surname><given-names>V. V.</given-names></name></name-alternatives><email xlink:type="simple">paramono@inr.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт ядерных исследований РАН</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Institute for Nuclear Research, Russian Academy of Sciences</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2025</year></pub-date><pub-date pub-type="epub"><day>16</day><month>01</month><year>2025</year></pub-date><volume>16</volume><issue>2</issue><fpage>183</fpage><lpage>186</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Парамонов В.В., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Парамонов В.В.</copyright-holder><copyright-holder xml:lang="en">Paramonov V.V.</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://npe.elpub.ru/jour/article/view/439">https://npe.elpub.ru/jour/article/view/439</self-uri><abstract><p>В коротких резонаторах структуры SDTL, работающей на колебании ТМ010, не предусматривается элементов для стабилизации распределения ускоряющего поля и смещения нерабочих колебания. Рассмотрены дисперсионные свойства резонаторов SDTL оптимизированных для максимального эффективного шунтового сопротивления. Дополнительными ограничениями при разработке резонаторов SDTL является нежелательная близость частот мод ТМ011 и ТЕ111 к рабочей</p></abstract><trans-abstract xml:lang="en"><p>In short SDTL cavities, operating in TM010 mode, there are no elements for accelerating field distribution stabilization and parasitic modes removal. Dispersion properties of cavities, optimized for maximal shunt impedance, are considered. An additional limitation in cavities development is undesirable proximity of TM011 and TE111 modes to the operating one.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>ускоряющая структура</kwd><kwd>резонатор</kwd><kwd>взаимодействие колебаний</kwd></kwd-group><kwd-group xml:lang="en"><kwd>accelerating structure</kwd><kwd>cavity</kwd><kwd>mode interaction</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">Kaтo T. // KEK Report No. 92-10. 1992.</mixed-citation><mixed-citation xml:lang="en">Kaтo T. // KEK Report No. 92-10. 1992.</mixed-citation></citation-alternatives></ref><ref id="cit2"><label>2</label><citation-alternatives><mixed-citation xml:lang="ru">Ito T. et al. // Proc. Conf. LINAC-2006. Knoxville, USA. 2006. P. 740.</mixed-citation><mixed-citation xml:lang="en">Ito T. et al. // Proc. Conf. LINAC-2006. Knoxville, USA. 2006. 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