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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">najo</journal-id><journal-title-group><journal-title xml:lang="en">Nanosystems: Physics, Chemistry, Mathematics</journal-title><trans-title-group xml:lang="ru"><trans-title>Наносистемы: физика, химия, математика</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2220-8054</issn><issn pub-type="epub">2305-7971</issn><publisher><publisher-name>Университет ИТМО</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.17586/2220-8054-2023-14-5-505-510</article-id><article-id custom-type="elpub" pub-id-type="custom">najo-286</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="en"><subject>MATHEMATICS</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>МАТЕМАТИКА</subject></subj-group></article-categories><title-group><article-title>On the spectrum of the two-particle Schrödinger operator with point potential: one dimensional case</article-title><trans-title-group xml:lang="ru"><trans-title>О спектре двухчастичного оператора Шредингера с точечным потенциалом в одномерном случае</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>Кулжанов</surname><given-names>У. Н.</given-names></name><name name-style="western" xml:lang="en"><surname>Kuljanov</surname><given-names>U. N.</given-names></name></name-alternatives><bio xml:lang="en"><p>Utkir Nematovich Kuljanov</p><p>140104, University boulvare. 15, Samarkand</p><p>Professorlar street 51, Samarkand</p></bio><email xlink:type="simple">uquljonov@bk.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Samarkand State University; Samarkand branch of Tashkent State University of Economics</institution><country>Uzbekistan</country></aff><pub-date pub-type="collection"><year>2023</year></pub-date><pub-date pub-type="epub"><day>08</day><month>06</month><year>2025</year></pub-date><volume>14</volume><issue>5</issue><fpage>505</fpage><lpage>510</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Kuljanov U.N., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Кулжанов У.Н.</copyright-holder><copyright-holder xml:lang="en">Kuljanov U.N.</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://nanojournal.ifmo.ru/jour/article/view/286">https://nanojournal.ifmo.ru/jour/article/view/286</self-uri><abstract><p>In the paper, a one-dimensional two-particle quantum system interacted by two identical point interactions is considered. The corresponding Schrödinger operator (energy operator) h" depending on " is constructed as a self-adjoint extension of the symmetric Laplace operator. The main results of the work are based on the study of the operator h". First, the essential spectrum is described. The existence of unique negative eigenvalue of the Schr¨odinger operator is proved. Further, this eigenvalue and the corresponding eigenfunction are found.</p></abstract><trans-abstract xml:lang="ru"><p>В работе рассматривается точечно-взаимодействующая одномерная двухчастичная квантовая система. Соответствующий оператор Шредингера (оператор энергии)  $h_\varepsilon$, зависящего от параметра расширения  строится как самосопряженное расширение $\varepsilon$ симметрического оператора Лапласа. Основные результаты работы основываются на изучение спектра оператора $h_\varepsilon$. Описан существенный спектр и доказано существование одного отрицательного собственного значения оператора Шредингера при положительных значениях параметра расширения. Более того, найдены отрицательные собственные значение и соответствующая собственная функция.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>двухчастичная квантовая система</kwd><kwd>симметричный оператор Лапласа</kwd><kwd>собственное значение</kwd><kwd>собственная функция</kwd><kwd>оператор энергии</kwd></kwd-group><kwd-group xml:lang="en"><kwd>two-particle quantum system</kwd><kwd>symmetric Laplace operator</kwd><kwd>eigenvalue</kwd><kwd>eigenfunction</kwd><kwd>energy operator</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">Berezin F. A., Faddeev L. D. Remark on the Schr¨odinger equation with singular potential. Dokl. Akad. 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