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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-144</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>Spin response in HTSC cuprates: generalized RPA approach with projection operators method</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>Eremin</surname><given-names>E. V.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya, 18, Kazan 420008</p></bio><email xlink:type="simple">meremin@kpfu.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>Shigapov</surname><given-names>I. M.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya, 18, Kazan 420008</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>Eremin</surname><given-names>I. M.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya, 18, Kazan 420008; D-44801 Bochum, Germany</p></bio><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Kazan Federal University</institution><country>Russian Federation</country></aff><aff xml:lang="en" id="aff-2"><institution>Kazan Federal University; Institut fur Theoretische Physik III, Ruhr-Universit at Bochum</institution><country>Russian Federation</country></aff><pub-date pub-type="collection"><year>2014</year></pub-date><pub-date pub-type="epub"><day>19</day><month>04</month><year>2014</year></pub-date><volume>16</volume><issue>2</issue><issue-title>SPECIAL ISSUE dedicated to Boris I. Kochelaev's 80th birthday</issue-title><elocation-id>14206 (21 pp.)</elocation-id><permissions><copyright-statement>Copyright &amp;#x00A9; Eremin E.V., Shigapov I.M., Eremin I.M., 2024</copyright-statement><copyright-year>2024</copyright-year><copyright-holder xml:lang="ru">Eremin E.V., Shigapov I.M., Eremin I.M.</copyright-holder><copyright-holder xml:lang="en">Eremin E.V., Shigapov I.M., Eremin I.M.</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/144">https://www.mrsej.ru/jour/article/view/144</self-uri><abstract><p>We derive the dynamical spin susceptibility in the t-J-G model combining the random phase approximation (RPA) and projection operator method, which allows describing the mutual interplay between the local and the itinerant components of susceptibility. Near the antiferromagnetic wave vector the calculated dispersion of the spin excitations reproduces well the so-called hour-glass dispersion, characteristic for several layered cuprates. It is formed as a result of competition between the original spin-gap in magnon-like excitations spectrum and the superconducting gap, which affects the itinerant component of the susceptibility. Furthermore, the calculated collective spin excitations along (0,0)-(0,π) are in agreement with the positions of the absorption peaks in the inelastic X-ray scattering spectra. They refer to the paramagnon-like modes, characteristic to the itinerant spin system, rather than magnon-like excitations that originate from short range order effect in the system of local spins at Cu sites.</p></abstract><kwd-group xml:lang="en"><kwd>HTSC</kwd><kwd>cuprates</kwd><kwd>dynamical spin susceptibility</kwd><kwd>collective spin excitations</kwd></kwd-group><funding-group><funding-statement xml:lang="en">This work is supported by RFBR Grant 13-02-00492 a</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">Eremin M.V., Aleev A.A., Eremin I.M. JETP 106, 752 (2008) [Zh. Eksp. Teor. Fiz. 133, 862 (2008), in Russian]</mixed-citation><mixed-citation xml:lang="en">Eremin M.V., Aleev A.A., Eremin I.M. JETP 106, 752 (2008) [Zh. Eksp. Teor. 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