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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="en"><front><journal-meta><journal-id journal-id-type="publisher-id">mrisel</journal-id><journal-title-group><journal-title xml:lang="en">Magnetic Resonance in Solids</journal-title><trans-title-group xml:lang="ru"><trans-title>Magnetic Resonance in Solids</trans-title></trans-title-group></journal-title-group><issn pub-type="epub">2072-5981</issn><publisher><publisher-name>Kazan Federal University</publisher-name></publisher></journal-meta><article-meta><article-id custom-type="elpub" pub-id-type="custom">mrisel-149</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></article-categories><title-group><article-title>Alternative theoretical approach of the exact ferromagnetic resonance frequency for common sample shapes by considering the phenomenological damping parameter - A tribute to C. Kittel and T.L. Gilbert</article-title><trans-title-group xml:lang="ru"><trans-title></trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Seemann</surname><given-names>K.</given-names></name></name-alternatives><bio xml:lang="en"><p>Hermann von Helmholtz Platz 1, 76344 Eggenstein-Leopoldshafen</p></bio><email xlink:type="simple">klaus.seemann@kit.edu</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Leiste</surname><given-names>H.</given-names></name></name-alternatives><bio xml:lang="en"><p>Hermann von Helmholtz Platz 1, 76344 Eggenstein-Leopoldshafen</p></bio><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Krüger</surname><given-names>K.</given-names></name></name-alternatives><bio xml:lang="en"><p>Hermann von Helmholtz Platz 1, 76344 Eggenstein-Leopoldshafen</p></bio><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Karlsruhe Institute of Technology KIT (Campus North), Institute for Applied Materials</institution><country>Germany</country></aff><pub-date pub-type="collection"><year>2014</year></pub-date><pub-date pub-type="epub"><day>25</day><month>07</month><year>2014</year></pub-date><volume>16</volume><issue>3</issue><elocation-id>14301 (5 pp.)</elocation-id><permissions><copyright-statement>Copyright &amp;#x00A9; Seemann K., Leiste H., Krüger K., 2024</copyright-statement><copyright-year>2024</copyright-year><copyright-holder xml:lang="ru">Seemann K., Leiste H., Krüger K.</copyright-holder><copyright-holder xml:lang="en">Seemann K., Leiste H., Krüger K.</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://www.mrsej.ru/jour/article/view/149">https://www.mrsej.ru/jour/article/view/149</self-uri><abstract><p>In order to establish an expression for the ferromagnetic resonance frequency of specimen with general shape, the Landau-Lifschitz-Gilbert differential equation was solved by considering demagnetisation effects and damping. By beginning the approach of calculation in a three dimensional space the sample was regarded as a uniformly magnetised ferro- or ferrimagnetic conventional ellipsoid. The condition for calculation must be a one-domain state which can be obtained by introducing a marked uniaxial anisotropy field and/or by applying an external magnetic saturation field. This can now be put on the level with a macro-spin precessing about its preferred direction. As a result, a more exact solution for the ferromagnetic resonance frequency was achieved which takes the phenomenological damping parameter as well as the demagnetisation factors into account. Applying it to certain sample shapes (plane, spherical or cylindrical) the uniaxial anisotropy field, the saturation magnetisation and especially the damping parameter show a different impact on the resonance frequency value. It could be shown that a plane sample (film) is more influenced by the damping parameter.</p></abstract><kwd-group xml:lang="en"><kwd>Landau-Lifschitz-Gilbert differential equation</kwd><kwd>FMR</kwd><kwd>damping parameter</kwd><kwd>demagnetisation factors</kwd></kwd-group><funding-group><funding-statement xml:lang="en">This work was partially supported by the Karlsruhe Nano Micro Facility (KNMF, www.knmf.kit.edu), a Helmholtz research infrastructure at the Karlsruhe Institute of Technology (KIT, www.kit.edu).</funding-statement></funding-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Griffiths J.H.E. Nature 158, 670 (1946)</mixed-citation><mixed-citation xml:lang="en">Griffiths J.H.E. Nature 158, 670 (1946)</mixed-citation></citation-alternatives></ref><ref id="cit2"><label>2</label><citation-alternatives><mixed-citation xml:lang="ru">Kittel C. Phys. 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