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<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD with OASIS Tables with MathML3 v1.4 20241031//EN" "https://jats.nlm.nih.gov/archiving/1.4/JATS-archive-oasis-article1-4-mathml3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:ali="http://www.niso.org/schemas/ali/1.0/" dtd-version="1.4" article-type="research-article" xml:lang="en"><front><journal-meta><journal-title-group><journal-title xml:lang="ru">Математическая физика и компьютерное моделирование</journal-title></journal-title-group><issn publication-format="print">2587-6325</issn><issn publication-format="electronic">2587-6902</issn></journal-meta><article-meta><article-id pub-id-type="doi">10.15688/mpcm.jvolsu.2024.4.2</article-id><article-categories><subj-group><subject>Other</subject></subj-group></article-categories><title-group><article-title xml:lang="ru">ПРИНЦИП НЕОПРЕДЕЛЕННОСТИ ДЛЯ РАЗНЫХ СИСТЕМ КООРДИНАТ</article-title><trans-title-group xml:lang="en"><trans-title>THE UNCERTAINTY PRINCIPLE FOR DIFFERENT SYSTEMS OF COORDINATE</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author"><name-alternatives><name xml:lang="ru"><surname>Павлов</surname><given-names>Андрей Валерианович</given-names></name><name xml:lang="en"><surname>Pavlov</surname><given-names>Andrey</given-names></name></name-alternatives><xref ref-type="aff" rid="aff1"/><email>avpavlovmgu@my-post.ru</email><contrib-id contrib-id-type="orcid">0000-0002-1082-2222</contrib-id></contrib><aff-alternatives id="aff1"><aff xml:lang="en"><institution>Moscow Institute of Radiotechnics, Electronics and Automatics — RTU (Moscow, Russian Federation)</institution></aff><aff xml:lang="ru"><institution>Московский институт радиотехники, электроники и автоматики — РТУ (Москва, Российская Федерация)</institution></aff></aff-alternatives></contrib-group><pub-date pub-type="epub" iso-8601-date="2024-12-27"><day>27</day><month>12</month><year>2024</year></pub-date><volume>27</volume><issue>4</issue><fpage>17</fpage><lpage>22</lpage><history><date date-type="received" iso-8601-date="2024-07-15"><day>15</day><month>07</month><year>2024</year></date><date date-type="accepted" iso-8601-date="2024-10-10"><day>10</day><month>10</month><year>2024</year></date></history><permissions><license xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:title="CC BY 4.0"><ali:license_ref>https://creativecommons.org/licenses/by/4.0/</ali:license_ref><license-p xml:lang="ru">CC BY 4.0</license-p></license></permissions><abstract xml:lang="ru"><p>Рассматриваются комплексные аналитические функции в разных системах координат. Доказаны факты, приводящие к периодичности аналитических функций как следствие совпадения данных функций с некоторыми комплексными функциями, совпадающими с симметричным отражением относительно одной из осей системы координат (полями сдвигов). Доказаны теоремы о возникновении второго уравнения одного многообразия решений уравнения 𝑧 = 𝑓(𝑝) (графика) с точки зрения рассмотрения новых систем координат на комплексной плоскости. Доказательство этих теорем опирается только на известные факты математического анализа.</p></abstract><abstract xml:lang="en" abstract-type="summary"><p>We consider the analytical 𝑧 = 𝑓(𝑝) functions in different coordinate systems. The centers of coordinates of the new systems are located in the (𝐴, 0) points, with the r variable. With point of view of the new coordinate system we obtain some new 𝑦 = 𝑓(𝑥 + 𝐴) equations for the same 𝑦 = 𝑓(𝑥) graph for the only function, (the new equation of the same (𝑧, 𝑓(𝑝)) set of points for the 𝑝 = 𝑥, 𝑧 = 𝑦 complex variables). To prove the fact we can consider the 𝑦 = 𝑓(𝑝) equation for the new 𝑝 = 𝑟 + 𝐴 variable with 𝑟 = 𝑥; by definition of the 𝑝 and 𝑟 variables 𝑝 = 𝑟 + 𝐴, (the 𝑝 variable we consider in the primary coordinate system, the 𝑟 variable we consider in the new coordinate system with the (𝐴, 0) center of coordinate); for all the 𝑟, 𝑥 variables 𝑟 = 𝑥 by definition of the radius-vectors in both coordinate systems, (𝑟 is other designation of 𝑥). The consideration of the equations results in periodicity of the 𝑓(𝑝) function. The same result we obtain for the complex 𝐹(𝑝) field, where 𝐹(𝑥+𝑖𝑦) = 𝑓(−𝑥+𝑖𝑦) by definition for the 𝑝 = 𝑥 + 𝑖𝑦 complex variable. In the new coordinate system the i constant is located on the OX axis instead of the 𝑂𝑌 axis. In the system of coordinates the new equation of the (𝑧, 𝑓(𝑝)) set of points (graph) is the same as in the initial system of coordinates. It is proved, that the 𝑓(𝑖𝑥 + 𝑦) field in relation to the 𝑥 = 𝑦 diagonal is equal to the 𝑓(−𝑖(−𝑥 + 𝑖𝑦)) field in relation to the 𝑖𝑂𝑋 axis.</p></abstract><kwd-group xml:lang="ru"><kwd>периодичность функций</kwd><kwd>аналитические функции</kwd><kwd>комплексные поля сдвигов</kwd><kwd>разные системы координат</kwd><kwd>неоднозначность представления функций</kwd></kwd-group><kwd-group xml:lang="en"><kwd>different coordinate systems</kwd><kwd>double representation of functions</kwd><kwd>function periodicity</kwd><kwd>analytical functions</kwd><kwd>complex fields of movements</kwd></kwd-group></article-meta></front><back><ref-list><ref id="ref1"><mixed-citation publication-type="other" xml:lang="ru">Лаврентьев, М. А. Методы теории функций комплексного переменного / М. А. Лаврентьев, Б. В. Шабат. — М. : Наука, 1987. — 688 c.</mixed-citation></ref><ref id="ref2"><mixed-citation publication-type="other" xml:lang="ru">Павлов, А. В. Отраженные функции и периодичность / А. В. 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