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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">zhps</journal-id><journal-title-group><journal-title xml:lang="ru">Журнал прикладной спектроскопии</journal-title><trans-title-group xml:lang="en"><trans-title>Zhurnal Prikladnoii Spektroskopii</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">0514-7506</issn><publisher><publisher-name>B. I. Stepanov Institute of Physics of the National Academy of Sciences</publisher-name></publisher></journal-meta><article-meta><article-id custom-type="elpub" pub-id-type="custom">zhps-1490</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>АННОТАЦИИ АНГЛОЯЗЫЧНЫХ СТАТЕЙ</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>ABSTRACTS ENGLISH-LANGUAGE ARTICLES</subject></subj-group></article-categories><title-group><article-title>Стабильность частоты диодного лазера, полученная методами частотной и зеемановской модуляции</article-title><trans-title-group xml:lang="en"><trans-title>Diode Laser Frequency Stabilities Obtained by Frequency and Zeeman Modulation Methods</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>Şahin</surname><given-names>E.</given-names></name><name name-style="western" xml:lang="en"><surname>Şahin</surname><given-names>E.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Гебзе, Коджаэли</p></bio><bio xml:lang="en"><p>Gebze, Kocaeli</p></bio><email xlink:type="simple">ersoy.sahin@tubitak.gov.tr</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Национальный метрологический институт Тубитака</institution></aff><aff xml:lang="en"><institution>Tübitak National Metrology Institute (Tubitak UME)</institution></aff></aff-alternatives><pub-date pub-type="collection"><year>2024</year></pub-date><pub-date pub-type="epub"><day>14</day><month>02</month><year>2024</year></pub-date><volume>91</volume><issue>1</issue><fpage>162</fpage><lpage>162</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Şahin E., 2024</copyright-statement><copyright-year>2024</copyright-year><copyright-holder xml:lang="ru">Şahin E.</copyright-holder><copyright-holder xml:lang="en">Şahin E.</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://zhps.ejournal.by/jour/article/view/1490">https://zhps.ejournal.by/jour/article/view/1490</self-uri><abstract><p>Для стабилизации диодных лазеров с расширенным резонатором использованы первая и третья производные, полученные методом частотной модуляции по сверхтонким резонансам D2-линии перехода 87Rb. С использованием первых производных по резонансам F=1→F¢=1 и F=1→F¢=2 получена стабильность частоты 3.1´10–12, 5.6´10–13 и 1.9´10–12 для времен интегрирования 1, 102 и 104 с соответственно, при использовании третьих производных перекрестных резонансов F=2→F¢=1,3 и F=2→F¢=2,3, соответственно, 4.0´10–12, 5.7´10–13 и 9.3´10–13 для времен 1, 102 и 104 с. Эти значения сравниваются с результатами, полученными методом зеемановской модуляции.</p></abstract><trans-abstract xml:lang="en"><p>The extended cavity diode lasers were stabilized using the first and third derivatives obtained by the frequency modulation method from the hyperfine resonances of the 87Rb D2 transition line. The frequency stability values were measured as 3.1´10–12, 5.6´10–13, and 1.9´10–12 for integration times of 1, 102, and 104 s, respectively, using the first derivatives of F=1→F¢=1 and F=1→F¢=2 resonances. By use of the third derivatives of F=2→F¢=1,3 and F=2→F¢=2,3 cross-over resonances, 4.0´10–12 − 1 s, 5.7´10–13 − 102 s, 9.3´10–13 − 104 s frequency stability values were obtained. These values compared with the results of the previous study obtained by the Zeeman modulation method.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>стабилизация частоты лазера</kwd><kwd>частотная модуляция</kwd><kwd>зеемановская модуляция</kwd></kwd-group><kwd-group xml:lang="en"><kwd>laser frequency stabilization</kwd><kwd>frequency modulation</kwd><kwd>Zeeman modulation</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">T. J. Quinn, Metrologia, 40, 103 (2003), https://doi.org/10.1088/0026-1394/40/2/316.</mixed-citation><mixed-citation xml:lang="en">T. J. 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