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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 pub-id-type="doi">10.47612/0514-7506-2023-90-2-324-328</article-id><article-id custom-type="elpub" pub-id-type="custom">zhps-1278</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>НЕЛИНЕЙНАЯ СПЕКТРОСКОПИЯ</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>NONLINEAR SPECTROSCOPY</subject></subj-group></article-categories><title-group><article-title>Оптическая анизотропия нанопористых пленок оксида алюминия как основа для создания ахроматических фазовых пластин с переменной разностью фаз ортогонально поляризованных компонент излучения, прошедшего пленку</article-title><trans-title-group xml:lang="en"><trans-title>Nanoporous  Alumina  Films  Optical  Anisotropy as the Basis for Creation of Achromatic Phase Plates with a Variable Phase Difference of the Orthogonal Polarized</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>Длугунович</surname><given-names>В. А.</given-names></name><name name-style="western" xml:lang="en"><surname>Dlugunovich</surname><given-names>V. A.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Минск</p></bio><bio xml:lang="en"><p>Minsk</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>Жумарь</surname><given-names>А. Ю.</given-names></name><name name-style="western" xml:lang="en"><surname>Zhumar</surname><given-names>A. Yu.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Минск</p></bio><bio xml:lang="en"><p>Minsk</p></bio><email xlink:type="simple">a.zhumar@ifanbel.bas-net.by</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Мухуров</surname><given-names>Н. И.</given-names></name><name name-style="western" xml:lang="en"><surname>Mukhurov</surname><given-names>N. I.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Минск</p></bio><bio xml:lang="en"><p>Minsk,</p></bio><email xlink:type="simple">mukhurov@oelt.basnet.by</email><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт физики НАН Беларуси</institution></aff><aff xml:lang="en"><institution>B. I. Stepanov Institute of Physics of the National Academy of Sciences of Belarus</institution></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>ГНПО “Оптика, оптоэлектроника и лазерная техника”</institution></aff><aff xml:lang="en"><institution>SSPA “Optics, Optoelectronics, and Laser Technology”</institution></aff></aff-alternatives><pub-date pub-type="collection"><year>2023</year></pub-date><pub-date pub-type="epub"><day>25</day><month>03</month><year>2023</year></pub-date><volume>90</volume><issue>2</issue><fpage>324</fpage><lpage>328</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Длугунович В.А., Жумарь А.Ю., Мухуров Н.И., 2023</copyright-statement><copyright-year>2023</copyright-year><copyright-holder xml:lang="ru">Длугунович В.А., Жумарь А.Ю., Мухуров Н.И.</copyright-holder><copyright-holder xml:lang="en">Dlugunovich V.A., Zhumar A.Y., Mukhurov 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://zhps.ejournal.by/jour/article/view/1278">https://zhps.ejournal.by/jour/article/view/1278</self-uri><abstract><p>Методом стокс-поляриметрии определены значения двулучепреломления нанопористых пленок оксида алюминия. Измерены коэффициенты пропускания пленки и степень поляризации прошедшего излучения для углов падения, при которых разность фаз ортогонально поляризованных компонент излучения, прошедшего пленку, составляет λ/4 или λ/2. С использованием модели Максвелла— Гарнета проведены оценки пористости и радиусов пор пленок. Показана возможность создания на основе нанопористой пленки оксида алюминия ахроматических фазовых пластин с переменной разностью фаз ортогонально поляризованных компонент излучения, прошедшего пленку, которые могут функционировать как четвертьволновая и полуволновая пластины.</p></abstract><trans-abstract xml:lang="en"><p>Stokes polarimetry was used to evaluate the birefringence of nanoporous alumina films. The transmittance of the film and the degree of polarization of the transmitted radiation were measured for the angles of incidence at which the phase difference of the orthogonal polarized components of the transmitted radiation reach to λ/4 or λ/2. Using the Maxwell—Garnet model, the porosity and pore radii of the films were estimated. The possibility of creating achromatic phase plates with a variable phase difference of the orthogonal polarized components of the transmitted radiation, which can function as a quarter-wave and half-wave plates, based on a nanoporous alumina film, is shown.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>нанопористая пленка</kwd><kwd>оксид алюминия</kwd><kwd>параметры Стокса</kwd><kwd>двулучепреломление</kwd><kwd>фазовая пластина</kwd><kwd>теория эффективной среды</kwd><kwd>коэффициент пропускания</kwd></kwd-group><kwd-group xml:lang="en"><kwd>nanoporous film</kwd><kwd>alumina</kwd><kwd>Stokes parameters</kwd><kwd>birefringence</kwd><kwd>phase plate</kwd><kwd>effective medium theory</kwd><kwd>transmittance</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">М. Борн, Э. Вольф. 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