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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 pub-id-type="doi">10.26907/mrsej-25101</article-id><article-id custom-type="elpub" pub-id-type="custom">mrisel-276</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>DFT study of magnetic order in Fe-Al-based ternary alloys</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>Abdullin</surname><given-names>A. F.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kazan 420008</p></bio><email xlink:type="simple">ayazik@bk.ru</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>Voronina</surname><given-names>E. V.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kazan 420008</p></bio><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="en">Kazan Federal University<country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2025</year></pub-date><pub-date pub-type="epub"><day>21</day><month>01</month><year>2025</year></pub-date><volume>27</volume><issue>1</issue><elocation-id>25101 (14 pp.)</elocation-id><permissions><copyright-statement>Copyright &amp;#x00A9; Abdullin A.F., Voronina E.V., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Abdullin A.F., Voronina E.V.</copyright-holder><copyright-holder xml:lang="en">Abdullin A.F., Voronina E.V.</copyright-holder><license 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://mrsej.elpub.ru/jour/article/view/276">https://mrsej.elpub.ru/jour/article/view/276</self-uri><abstract><p>In this study, we utilized quantum-mechanical calculations to explore the electronic structure of binary and ternary Fe-Al-based systems with noncollinear magnetic configurations. Our findings indicate that the ground state of systems, such as Fe9Al7, Fe9Al6B, Fe9Al6Ga, and Fe9Ga6, is not ferromagnetic, but rather exhibits a spin spiral structure in the [<xref ref-type="bibr" rid="cit111">111</xref>] direction. We analyzed the effects of different types of exchange-correlation potentials, aluminum concentration, relaxation of interatomic distances, substituting atom positions, and spin wave orientations on magnetic properties. Various exchange-correlation potentials consistently demonstrated the dependency of the total energy on the spin spiral q-vector, with the generalized gradient approximation closely matching experimental observations. In the Fe9Al7 unit cell, a spin spiral structure prevails at 43.75% atomic Al, while other compositions favor ferromagnetism. The system can support spin spiral vectors in the [<xref ref-type="bibr" rid="cit001">001</xref>], [<xref ref-type="bibr" rid="cit110">110</xref>], and [<xref ref-type="bibr" rid="cit111">111</xref>] directions, with [<xref ref-type="bibr" rid="cit111">111</xref>] being the most energetically favorable. The equilibrium state is highly sensitive to the position and type of sp-elements within the unit cell. Overall, our results show that spin spiral structures with the [<xref ref-type="bibr" rid="cit111">111</xref>] q-vector are energetically favored when the average magnetic moment is approximately 1 μB per Fe atom, which is consistent with Mössbauer data</p></abstract><kwd-group xml:lang="en"><kwd>DFT</kwd><kwd>Fe-Al</kwd><kwd>Fe-Al-B</kwd><kwd>Fe-Al-Ga</kwd><kwd>noncollinear magnetism</kwd><kwd>ternary alloys</kwd><kwd>nuclear resonance</kwd><kwd>SDW</kwd><kwd>spin spiral wave</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">Arrott A., Sato H., Physical Review 114, 1420 (1959).</mixed-citation><mixed-citation xml:lang="en">Arrott A., Sato H., Physical Review 114, 1420 (1959).</mixed-citation></citation-alternatives></ref><ref id="cit2"><label>2</label><citation-alternatives><mixed-citation xml:lang="ru">Danan H., Gengnagel H., Journal of Applied Physics 39, 678 (1968).</mixed-citation><mixed-citation xml:lang="en">Danan H., Gengnagel H., Journal of Applied Physics 39, 678 (1968).</mixed-citation></citation-alternatives></ref><ref id="cit3"><label>3</label><citation-alternatives><mixed-citation xml:lang="ru">Cable J. 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