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On pomonoid of partial transformations of a poset 论正集部分变换的 "π"(pomonoid)
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-16 DOI: 10.1515/math-2023-0161
Bana Al Subaiei
The main objective of this article is to study the ordered partial transformations <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0161_eq_001.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mi mathvariant="script">PO</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>X</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> <jats:tex-math>{mathcal{PO}}left(X)</jats:tex-math> </jats:alternatives> </jats:inline-formula> of a poset <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0161_eq_002.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mi>X</m:mi> </m:math> <jats:tex-math>X</jats:tex-math> </jats:alternatives> </jats:inline-formula>. The findings show that the set of all partial transformations of a poset with a pointwise order is not necessarily a pomonoid. Some conditions are implemented to guarantee that <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0161_eq_003.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mi mathvariant="script">PO</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>X</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> <jats:tex-math>{mathcal{PO}}left(X)</jats:tex-math> </jats:alternatives> </jats:inline-formula> is a pomonoid and this pomonoid is denoted by <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0161_eq_004.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msup> <m:mrow> <m:mi mathvariant="script">PO</m:mi> </m:mrow> <m:mrow> <m:mi>↑</m:mi> </m:mrow> </m:msup> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>X</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> <jats:tex-math>{{mathcal{PO}}}^{uparrow }left(X)</jats:tex-math> </jats:alternatives> </jats:inline-formula>. Moreover, we determine the necessary conditions in order that the partial order-embedding transformations define the ordered version of the symmetric inverse monoid. The findings show that this set is an inverse pomonoid and we will denote it by <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0161_eq_005.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msup> <m:mrow> <m:mi mathvariant="script">ℐPO</m:mi> </m:mrow> <m:mrow> <m:mi>↑</m:mi> </m:mrow> </m:msup> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>X</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> <jats:tex-math>{{mathcal{ {mathcal I} PO}}}^{uparrow }left(X)</jats:tex-math> </jats:alternatives> </jats:inline-formula>. In case the order on the poset <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0161_eq_006.png
本文的主要目的是研究正集 X X 的有序部分变换 PO ( X ) {mathcal{PO}}left(X) 。研究结果表明,poset 的所有有序部分变换的集合并不一定是一个 pomonoid。我们提出了一些条件来保证 PO ( X ) {mathcal{PO}}left(X) 是一个 pomonoid,这个 pomonoid 用 PO ↑ ( X ) {{mathcal{PO}}^{uparrow }left(X) 表示。此外,我们还确定了一些必要条件,以使部分有序嵌入变换定义对称逆单元的有序版本。研究结果表明,这个集合是一个逆单元集,我们将用ℐPO ↑ ( X ) {{mathcal{ {mathcal I} PO}}^{uparrow }left(X) 来表示它。如果集合 X X 上的阶是全阶,我们将探讨 PO ↑ ( X ) {{mathcal{PO}}^{uparrow }/left(X)和ℐPO ↑ ( X ) {{mathcal{ {mathcal I} PO}}^{uparrow }/left(X)的一些性质,包括回归性、单一性和可逆性。
{"title":"On pomonoid of partial transformations of a poset","authors":"Bana Al Subaiei","doi":"10.1515/math-2023-0161","DOIUrl":"https://doi.org/10.1515/math-2023-0161","url":null,"abstract":"The main objective of this article is to study the ordered partial transformations &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0161_eq_001.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mi mathvariant=\"script\"&gt;PO&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;X&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{mathcal{PO}}left(X)&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; of a poset &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0161_eq_002.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mi&gt;X&lt;/m:mi&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;X&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;. The findings show that the set of all partial transformations of a poset with a pointwise order is not necessarily a pomonoid. Some conditions are implemented to guarantee that &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0161_eq_003.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mi mathvariant=\"script\"&gt;PO&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;X&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{mathcal{PO}}left(X)&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; is a pomonoid and this pomonoid is denoted by &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0161_eq_004.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msup&gt; &lt;m:mrow&gt; &lt;m:mi mathvariant=\"script\"&gt;PO&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;↑&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msup&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;X&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{{mathcal{PO}}}^{uparrow }left(X)&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;. Moreover, we determine the necessary conditions in order that the partial order-embedding transformations define the ordered version of the symmetric inverse monoid. The findings show that this set is an inverse pomonoid and we will denote it by &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0161_eq_005.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msup&gt; &lt;m:mrow&gt; &lt;m:mi mathvariant=\"script\"&gt;ℐPO&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;↑&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msup&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;X&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{{mathcal{ {mathcal I} PO}}}^{uparrow }left(X)&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;. In case the order on the poset &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0161_eq_006.png","PeriodicalId":48713,"journal":{"name":"Open Mathematics","volume":"25 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-12-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138687900","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Global well-posedness of initial-boundary value problem of fifth-order KdV equation posed on finite interval 有限区间上五阶 KdV 方程初始边界值问题的全局好求解性
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-16 DOI: 10.1515/math-2023-0158
Xiangqing Zhao, Chengqiang Wang, Jifeng Bao
We have established the existence and uniqueness of the local solution for <jats:disp-formula> <jats:label>(0.1)</jats:label> <jats:alternatives> <jats:graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0158_eq_001.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="block"> <m:mfenced open="{" close=""> <m:mrow> <m:mtable displaystyle="true"> <m:mtr> <m:mtd columnalign="left"> <m:msub> <m:mrow> <m:mo>∂</m:mo> </m:mrow> <m:mrow> <m:mi>t</m:mi> </m:mrow> </m:msub> <m:mi>u</m:mi> <m:mo>+</m:mo> <m:msubsup> <m:mrow> <m:mo>∂</m:mo> </m:mrow> <m:mrow> <m:mi>x</m:mi> </m:mrow> <m:mrow> <m:mn>5</m:mn> </m:mrow> </m:msubsup> <m:mi>u</m:mi> <m:mo>−</m:mo> <m:mi>u</m:mi> <m:msub> <m:mrow> <m:mo>∂</m:mo> </m:mrow> <m:mrow> <m:mi>x</m:mi> </m:mrow> </m:msub> <m:mi>u</m:mi> <m:mo>=</m:mo> <m:mn>0</m:mn> <m:mo>,</m:mo> </m:mtd> <m:mtd columnalign="left"> <m:mn>0</m:mn> <m:mo><</m:mo> <m:mi>x</m:mi> <m:mo><</m:mo> <m:mn>1</m:mn> <m:mo>,</m:mo> <m:mspace width="1.0em" /> <m:mi>t</m:mi> <m:mo>></m:mo> <m:mn>0</m:mn> <m:mo>,</m:mo> </m:mtd> </m:mtr> <m:mtr> <m:mtd columnalign="left"> <m:mi>u</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>x</m:mi> <m:mo>,</m:mo> <m:mn>0</m:mn> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>=</m:mo> <m:mi>φ</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>x</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>,</m:mo> </m:mtd> <m:mtd columnalign="left"> <m:mn>0</m:mn> <m:mo><</m:mo> <m:mi>x</m:mi> <m:mo><</m:mo> <m:mn>1</m:mn> <m:mo>,</m:mo> </m:mtd> </m:mtr> <m:mtr> <m:mtd columnalign="left"> <m:mi>u</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>=</m:mo> <m:msub> <m:mrow> <m:mi>h</m:mi> </m:mrow> <m:mrow> <m:mn>1</m:mn> </m:mrow> </m:msub> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>,</m:mo> <m:mi>u</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>1</m:mn> <m:mo>,</m:mo> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>=</m:mo> <m:msub> <m:mrow> <m:mi>h</m:mi> </m:mrow> <m:mrow> <m:mn>2</m:mn> </m:mrow> </m:msub> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>,</m:mo> <m:mspace width="0.33em" /> <m:msub> <m:mrow> <m:mo>∂</m:mo> </m:mrow> <m:mrow> <m:mi>x</m:mi> </m:mrow> </m:msub> <m:mi>u</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>1</m:mn> <m:mo>,</m:mo> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>=</m:mo> <m:msub> <m:mrow> <m:mi>h</m:mi> </m:mrow> <m:mrow> <m:mn>3</m:mn> </m:mrow> </m:msub> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>,</m:mo> </m:mtd> <m:mtd columnalign="left" /> </m:mtr> <m:mtr> <m:mtd columnalign="left"> <m:msub> <m:mrow> <m:mo>∂</m:mo> </m:mrow> <m:mrow> <m:mi>x</m:mi> </m:mrow> </m:msub> <m:mi>u</m:mi> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:mi>t</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> <m:mo>=</m:mo> <m:msub
我们已经确定了 (0) 的局部解的存在性和唯一性。1) ∂ t u + ∂ x 5 u - u ∂ x u = 0 , 0 < x < 1 , t > 0 , u ( x , 0 ) = φ ( x ) , 0 < x <;1 , u ( 0 , t ) = h 1 ( t ) , u ( 1 , t ) = h 2 ( t ) , ∂ x u ( 1 , t ) = h 3 ( t ) , ∂ x u ( 0 , t ) = h 4 ( t ) , ∂ x 2 u ( 1 , t ) = h 5 ( t ) , t >;0 ,left{begin{array}{ll}{partial }_{t}u+{partial }_{x}^{5}u-u{partial }_{x}u=0,& 0lt xlt 1,hspace{1.0lt xlt 1,uleft(0,t)={h}_{1}left(t),uleft(1,t)={h}_{2}left(t),hspace{0.33em} {partial }_{x}uleft(1,t)={h}_{3}left(t),& {partial }_{x}uleft(0,t)={h}_{4}left(t),hspace{0.33em}{partial }_{x}^{2}uleft(1,t)={h}_{5}left(t),& tgt 0,end{array}right. in the study of Zhao and Zhang [Non-homogeneous boundary value problem of the fifth-order KdV equations posed on a bounded interval, J. Math.Anal.Appl. 470 (2019),251-278]。一个问题自然而然地产生了:局部解能否扩展为全局解?本文将探讨这个问题。首先,通过一系列逻辑推导,建立一个全局先验估计,然后将局部解自然扩展为全局解。
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&lt;m:mrow&gt; &lt;m:mo&gt;∂&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mn&gt;5&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;/m:msubsup&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mo&gt;−&lt;/m:mo&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;∂&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;/m:mtd&gt; &lt;m:mtd columnalign=\"left\"&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;m:mo&gt;&lt;&lt;/m:mo&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;m:mo&gt;&lt;&lt;/m:mo&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mspace width=\"1.0em\" /&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;m:mo&gt;&gt;&lt;/m:mo&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;/m:mtd&gt; &lt;/m:mtr&gt; &lt;m:mtr&gt; &lt;m:mtd columnalign=\"left\"&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:mi&gt;φ&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;/m:mtd&gt; &lt;m:mtd columnalign=\"left\"&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;m:mo&gt;&lt;&lt;/m:mo&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;m:mo&gt;&lt;&lt;/m:mo&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;/m:mtd&gt; &lt;/m:mtr&gt; &lt;m:mtr&gt; &lt;m:mtd columnalign=\"left\"&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;h&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;h&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mn&gt;2&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mspace width=\"0.33em\" /&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;∂&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;h&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mn&gt;3&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;/m:mtd&gt; &lt;m:mtd columnalign=\"left\" /&gt; &lt;/m:mtr&gt; &lt;m:mtr&gt; &lt;m:mtd columnalign=\"left\"&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;∂&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;x&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mn&gt;0&lt;/m:mn&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:mi&gt;t&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:msub","PeriodicalId":48713,"journal":{"name":"Open Mathematics","volume":"131 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-12-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138687816","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Approximate solvability method for nonlocal impulsive evolution equation 非局部脉冲演化方程的近似可解法
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-14 DOI: 10.1515/math-2023-0155
Weifeng Ma, Yongxiang Li
In this article, without assuming the compactness of semigroup, we deal with the existence and uniqueness of a mild solution for semilinear impulsive evolution equation with nonlocal condition in a reflexive Banach space by applying the approximate solvability method and Yosida approximations of the infinitesimal generator of C 0-semigroup.
在本文中,我们在不假设半群紧凑性的情况下,通过应用近似可解性方法和 C 0 半群无穷小生成器的 Yosida 近似,处理了在反身巴纳赫空间中具有非局部条件的半线性脉冲演化方程的温和解的存在性和唯一性问题。
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引用次数: 0
Construction of a functional by a given second-order Ito stochastic equation 通过给定的二阶伊托随机方程构建函数
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-11 DOI: 10.1515/math-2023-0148
Marat Tleubergenov, Gulmira Vassilina, Shakhmira Ismailova
In this article, we consider the problem of extending Hamilton’s principle to the class of natural mechanical systems with random perturbing forces of white noise type. By the method of moment functions, we construct the functionals taking a stationary value on the solutions of a given stochastic equation of Lagrangian structure.
在本文中,我们考虑了将汉密尔顿原理扩展到具有白噪声类型随机扰动力的自然机械系统的问题。通过矩函数方法,我们构建了在给定的拉格朗日结构随机方程的解上取静止值的函数。
{"title":"Construction of a functional by a given second-order Ito stochastic equation","authors":"Marat Tleubergenov, Gulmira Vassilina, Shakhmira Ismailova","doi":"10.1515/math-2023-0148","DOIUrl":"https://doi.org/10.1515/math-2023-0148","url":null,"abstract":"In this article, we consider the problem of extending Hamilton’s principle to the class of natural mechanical systems with random perturbing forces of white noise type. By the method of moment functions, we construct the functionals taking a stationary value on the solutions of a given stochastic equation of Lagrangian structure.","PeriodicalId":48713,"journal":{"name":"Open Mathematics","volume":"81 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-12-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138575883","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
The 𝔪-WG° inverse in the Minkowski space 闵科夫斯基空间中的ᵒ-WG°反演
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-08 DOI: 10.1515/math-2023-0145
Xiaoji Liu, Kaiyue Zhang, Hongwei Jin
In this article, we study the m {mathfrak{m}} -WG {}^{circ } inverse which presents a generalization of the m {mathfrak{m}} -WG inverse in the Minkowski space. We first show the existence and the uniqueness of the generalized inverse. Then, we discuss several properties and characterizations of the m {mathfrak{m}} -WG {}^{circ } inverse by using the core-EP decomposition. Applying the generalized inverse, we obtain the solutions of some matrix equations in Minkowski space.
在本文中,我们研究了 m {mathfrak{m}} -WG ∘ {}^{circ } 逆,它是 m {mathfrak{m}} 的广义化。 -WG 在闵科夫斯基空间中的逆。我们首先证明了广义逆的存在性和唯一性。然后,我们讨论了 m {mathfrak{m}} -WG ˲Sm_2F2} 的几个性质和特征。 -WG ∘ {}^{circ }逆的几个性质和特征。应用广义逆,我们得到了闵科夫斯基空间中一些矩阵方程的解。
{"title":"The 𝔪-WG° inverse in the Minkowski space","authors":"Xiaoji Liu, Kaiyue Zhang, Hongwei Jin","doi":"10.1515/math-2023-0145","DOIUrl":"https://doi.org/10.1515/math-2023-0145","url":null,"abstract":"In this article, we study the <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0145_eq_001.png\" /> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi mathvariant=\"fraktur\">m</m:mi> </m:math> <jats:tex-math>{mathfrak{m}}</jats:tex-math> </jats:alternatives> </jats:inline-formula>-WG<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0145_eq_002.png\" /> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:msup> <m:mrow /> <m:mrow> <m:mrow> <m:mo>∘</m:mo> </m:mrow> </m:mrow> </m:msup> </m:math> <jats:tex-math>{}^{circ }</jats:tex-math> </jats:alternatives> </jats:inline-formula> inverse which presents a generalization of the <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0145_eq_999.png\" /> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi mathvariant=\"fraktur\">m</m:mi> </m:math> <jats:tex-math>{mathfrak{m}}</jats:tex-math> </jats:alternatives> </jats:inline-formula>-WG inverse in the Minkowski space. We first show the existence and the uniqueness of the generalized inverse. Then, we discuss several properties and characterizations of the <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0145_eq_003.png\" /> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi mathvariant=\"fraktur\">m</m:mi> </m:math> <jats:tex-math>{mathfrak{m}}</jats:tex-math> </jats:alternatives> </jats:inline-formula>-WG<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0145_eq_004.png\" /> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:msup> <m:mrow /> <m:mrow> <m:mrow> <m:mo>∘</m:mo> </m:mrow> </m:mrow> </m:msup> </m:math> <jats:tex-math>{}^{circ }</jats:tex-math> </jats:alternatives> </jats:inline-formula> inverse by using the core-EP decomposition. Applying the generalized inverse, we obtain the solutions of some matrix equations in Minkowski space.","PeriodicalId":48713,"journal":{"name":"Open Mathematics","volume":"18 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138560953","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
A series expansion of a logarithmic expression and a decreasing property of the ratio of two logarithmic expressions containing cosine 一个对数表达式的级数展开和两个包含余弦的对数表达式之比递减的性质
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-08 DOI: 10.1515/math-2023-0159
Yan-Fang Li, Feng Qi
In this study, by virtue of a derivative formula for the ratio of two differentiable functions and with aid of a monotonicity rule, the authors expand a logarithmic expression involving the cosine function into the Maclaurin power series in terms of specific determinants and prove a decreasing property of the ratio of two logarithmic expressions containing the cosine function.
在这项研究中,作者根据两个可微分函数之比的导数公式,并借助单调性规则,将涉及余弦函数的对数表达式扩展为特定行列式的麦克劳林幂级数,并证明了包含余弦函数的两个对数表达式之比的递减性质。
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引用次数: 0
Stability result for Lord Shulman swelling porous thermo-elastic soils with distributed delay term 带有分布式延迟项的 Lord Shulman 膨胀多孔热弹性土的稳定性结果
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-08 DOI: 10.1515/math-2023-0165
Abdelbaki Choucha, Salah Mahmoud Boulaaras, Rashid Jan
The Lord Shulman swelling porous thermo-elastic soil system with the presence of a distributed delay term is studied in this work. We will establish the well-posedness of the system and the exponential stability of the system is derived.
本文研究了存在分布式延迟项的 Lord Shulman 膨胀多孔热弹性土壤系统。我们将建立系统的良好拟合性,并推导出系统的指数稳定性。
{"title":"Stability result for Lord Shulman swelling porous thermo-elastic soils with distributed delay term","authors":"Abdelbaki Choucha, Salah Mahmoud Boulaaras, Rashid Jan","doi":"10.1515/math-2023-0165","DOIUrl":"https://doi.org/10.1515/math-2023-0165","url":null,"abstract":"The Lord Shulman swelling porous thermo-elastic soil system with the presence of a distributed delay term is studied in this work. We will establish the well-posedness of the system and the exponential stability of the system is derived.","PeriodicalId":48713,"journal":{"name":"Open Mathematics","volume":"195 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138560947","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
A double-phase eigenvalue problem with large exponents 大指数双相特征值问题
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-06 DOI: 10.1515/math-2023-0138
Lujuan Yu
In the present article, we consider a double-phase eigenvalue problem with large exponents. Let <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0138_eq_001.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msubsup> <m:mrow> <m:mi>λ</m:mi> </m:mrow> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:msub> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> <m:mo>,</m:mo> <m:msub> <m:mrow> <m:mi>q</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mn>1</m:mn> </m:mrow> </m:msubsup> </m:math> <jats:tex-math>{lambda }_{left({p}_{n},{q}_{n})}^{1}</jats:tex-math> </jats:alternatives> </jats:inline-formula> be the first eigenvalues and <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0138_eq_002.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msub> <m:mrow> <m:mi>u</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> </m:math> <jats:tex-math>{u}_{n}</jats:tex-math> </jats:alternatives> </jats:inline-formula> be the first eigenfunctions, normalized by <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0138_eq_003.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msub> <m:mrow> <m:mo>‖</m:mo> <m:msub> <m:mrow> <m:mi>u</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> <m:mo>‖</m:mo> </m:mrow> <m:mrow> <m:msub> <m:mrow> <m:mi mathvariant="script">ℋ</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> </m:mrow> </m:msub> <m:mo>=</m:mo> <m:mn>1</m:mn> </m:math> <jats:tex-math>Vert {u}_{n}{Vert }_{{{mathcal{ {mathcal H} }}}_{n}}=1</jats:tex-math> </jats:alternatives> </jats:inline-formula>. Under some assumptions on the exponents <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0138_eq_004.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msub> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> </m:math> <jats:tex-math>{p}_{n}</jats:tex-math> </jats:alternatives> </jats:inline-formula> and <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0138_eq_005.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msub> <m:mrow> <m:mi>q</m:mi> </m:mrow> <m:mrow> <m:mi>n</m:mi> </m:mrow> </m:msub> </m:math> <jats:tex-math>{q}_{n}</jats:tex-math> </jats:alternatives> </jats:inline-formula>, we show that <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_math-2023-0138_eq_006.png" /> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msubsup> <m:mr
在本文中,我们考虑一个具有大指数的双相特征值问题。设 λ ( p n , q n ) 1 {lambda }_{left({p}_{n},{q}_{n})}^{1} 为第一特征值,u n {u}_{n} 为第一特征函数,归一化为 ‖ u n ‖ ℋ n = 1 Vert {u}_{n} {}Vert }_{{mathcal{ {mathcal H} }}_{n}}=1 .}}}_{n}}=1 .在对指数 p n {p}_{n} 和 q n {q}_{n} 有一些假设的情况下 我们证明 λ ( p n , q n ) 1 {lambda }_{left({p}_{n}、{q}_{n})}^{1} 收敛到 Λ ∞ {Lambda }_{infty },并且 u n {u}_{n} 收敛到 u ∞ {u}_{infty },在空间 C α ( Ω ) {C}^{alpha }left(Omega ) 中均匀分布、且 u ∞ {u}_{infty } 是一个 Dirichlet ∞ infty -Laplacian 问题的非微观粘性解。
{"title":"A double-phase eigenvalue problem with large exponents","authors":"Lujuan Yu","doi":"10.1515/math-2023-0138","DOIUrl":"https://doi.org/10.1515/math-2023-0138","url":null,"abstract":"In the present article, we consider a double-phase eigenvalue problem with large exponents. Let &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0138_eq_001.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msubsup&gt; &lt;m:mrow&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mrow&gt; &lt;m:mo&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;p&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;q&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;/m:msubsup&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{lambda }_{left({p}_{n},{q}_{n})}^{1}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; be the first eigenvalues and &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0138_eq_002.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{u}_{n}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; be the first eigenfunctions, normalized by &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0138_eq_003.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mo&gt;‖&lt;/m:mo&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;u&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mo&gt;‖&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi mathvariant=\"script\"&gt;ℋ&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;Vert {u}_{n}{Vert }_{{{mathcal{ {mathcal H} }}}_{n}}=1&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;. Under some assumptions on the exponents &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0138_eq_004.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;p&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{p}_{n}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; and &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0138_eq_005.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msub&gt; &lt;m:mrow&gt; &lt;m:mi&gt;q&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;m:mrow&gt; &lt;m:mi&gt;n&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:msub&gt; &lt;/m:math&gt; &lt;jats:tex-math&gt;{q}_{n}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;, we show that &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_math-2023-0138_eq_006.png\" /&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:msubsup&gt; &lt;m:mr","PeriodicalId":48713,"journal":{"name":"Open Mathematics","volume":"108 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-12-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138547194","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Evolutoids and pedaloids of frontals on timelike surfaces 类时间曲面上正面的演化和踏板
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-06 DOI: 10.1515/math-2023-0149
Yongqiao Wang, Lin Yang, Yuan Chang, Haiming Liu
In this article, we define evolutoids and pedaloids of frontals on timelike surfaces in Minkowski 3-space. The evolutoids of frontals on timelike surfaces are not only the generalization of evolutoids of curves in the Minkowski plane but also the generalization of caustics in Minkowski 3-space. As an application of the singularity theory, we classify the singularities of evolutoids and reveal the relationships between the singularities and geometric invariants of frontals. Furthermore, we find that there exists a close connection between the pedaloids of frontals and the pedal surfaces of evolutoids. Finally, we give some examples to demonstrate the results.
在这篇文章中,我们定义了闵科夫斯基三维空间中类时间曲面上正面的 evolutoids 和 pedaloids。类时间曲面上正面的 evolutoids 不仅是闵科夫斯基平面上曲线 evolutoids 的一般化,也是闵科夫斯基 3 空间中凹凸的一般化。作为奇点理论的应用,我们对 evolutoids 的奇点进行了分类,并揭示了奇点与正面几何不变式之间的关系。此外,我们还发现正面的踏板面与 evolutoids 的踏板面之间存在着密切联系。最后,我们举例说明了这些结果。
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引用次数: 0
On the number of perfect matchings in random polygonal chains 论随机多边形链中完全匹配的数量
IF 1.7 4区 数学 Q1 MATHEMATICS Pub Date : 2023-12-06 DOI: 10.1515/math-2023-0146
Shouliu Wei, Yongde Feng, Xiaoling Ke, Jianwu Huang
Let G G be a graph. A perfect matching of G G is a regular spanning subgraph of degree one. Enumeration of perfect matchings of a (molecule) graph is interest in chemistry, physics, and mathematics. But the enumeration problem of perfect matchings for general graphs (even in bipartite graphs) is non-deterministic polynomial (NP)-hard. Xiao et al. [C. Xiao, H. Chen, L. Liu, Perfect matchings in random pentagonal chains, J. Math. Chem. 55 (2017), 1878–1886] have studied the problem of perfect matchings for random odd-polygonal chain (i.e., with odd polygons). In this article, we further present simple counting formulae for the expected value of the number of perfect matchings in random even-polygonal chains (i.e., with even polygons). Based on these formulae, we obtain the average values of the number for perfect matchings with respect to the set of all even-polygonal chains with n n polygons.
设 G G 是一个图。G G 的完美匹配是阶数为 1 的正则遍历子图。枚举(分子)图的完全匹配是化学、物理和数学领域的兴趣所在。但对于一般图(即使是二方图)来说,完美匹配的枚举问题是非确定性多项式(NP)困难的。Xiao et al.Xiao, H. Chen, L. Liu, Perfect matchings in random pentagonal chains, J. Math.Chem.55 (2017), 1878-1886] 研究了随机奇多边形链(即奇多边形)的完全匹配问题。在本文中,我们进一步提出了随机偶多边形链(即偶数多边形)中完全匹配次数期望值的简单计数公式。根据这些计算公式,我们可以得到具有 n n 个多边形的所有偶多边形链的完全匹配数的平均值。
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引用次数: 0
期刊
Open Mathematics
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