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Optical soliton solutions of time-space nonlinear fractional Schrödinger's equation via two different techniques
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-18 DOI: 10.1016/j.jmaa.2025.129387
Waseem Razzaq , Asim Zafar , M. Raheel , Jian-Guo Liu
This paper contains the optical soliton solutions of the nonlinear Schrödinger equation in the different cases i.e. Kerr law, Power law of nonlinearity, Parabolic law of nonlinearity, dual-power law and log law based on two different techniques named, modified (G/G2)-expansion method and modified simplest equation method. As a result, a consequence of traveling wave solutions are obtained and are verified through MATHEMATICA. These solutions show that the suggested methods are effective, reliable and simple as compared to many other methods.
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引用次数: 0
Explicit values of Bernoulli polynomials at rational numbers
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-17 DOI: 10.1016/j.jmaa.2025.129381
Florian Münkel , Lerna Pehlivan , Kenneth S. Williams
We give an explicit formula for the value of the Bernoulli polynomial B2k(t) when t is a rational number in the interval (0,1). When t=12,13,23,14,34,16,56 the value of B2k(t) is known explicitly. In 1938 Emma Lehmer asked for the value of B2k(t) when the denominator of t is 5, 8, 10, or 12. We apply our formula to determine B2k(t) when the denominator of t is 5, 8, 10, and 12 thereby answering Lehmer's 87 year old question.
{"title":"Explicit values of Bernoulli polynomials at rational numbers","authors":"Florian Münkel ,&nbsp;Lerna Pehlivan ,&nbsp;Kenneth S. Williams","doi":"10.1016/j.jmaa.2025.129381","DOIUrl":"10.1016/j.jmaa.2025.129381","url":null,"abstract":"<div><div>We give an explicit formula for the value of the Bernoulli polynomial <span><math><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn><mi>k</mi></mrow></msub><mo>(</mo><mi>t</mi><mo>)</mo></math></span> when <em>t</em> is a rational number in the interval <span><math><mo>(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>)</mo></math></span>. When <span><math><mi>t</mi><mo>=</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mn>2</mn></mrow></mfrac><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mo>,</mo><mfrac><mrow><mn>2</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mn>4</mn></mrow></mfrac><mo>,</mo><mfrac><mrow><mn>3</mn></mrow><mrow><mn>4</mn></mrow></mfrac><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mn>6</mn></mrow></mfrac><mo>,</mo><mfrac><mrow><mn>5</mn></mrow><mrow><mn>6</mn></mrow></mfrac></math></span> the value of <span><math><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn><mi>k</mi></mrow></msub><mo>(</mo><mi>t</mi><mo>)</mo></math></span> is known explicitly. In 1938 Emma Lehmer asked for the value of <span><math><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn><mi>k</mi></mrow></msub><mo>(</mo><mi>t</mi><mo>)</mo></math></span> when the denominator of <em>t</em> is 5, 8, 10, or 12. We apply our formula to determine <span><math><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn><mi>k</mi></mrow></msub><mo>(</mo><mi>t</mi><mo>)</mo></math></span> when the denominator of <em>t</em> is 5, 8, 10, and 12 thereby answering Lehmer's 87 year old question.</div></div>","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"548 2","pages":"Article 129381"},"PeriodicalIF":1.2,"publicationDate":"2025-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143465026","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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
Asymptotic behavior of the coupled Allen-Cahn/Cahn-Hilliard system with proliferation term
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-17 DOI: 10.1016/j.jmaa.2025.129382
Ahmad Makki , Rim Mheich , Madalina Petcu , Raafat Talhouk
In this article, we investigate the coupled Allen-Cahn/Cahn-Hilliard equations with a proliferation term, which can model the growth of cancerous tumors and other biological entities. We focus on establishing the existence, uniqueness, and regularity of solutions, as well as analyzing their asymptotic behavior, with particular attention to the existence of finite-dimensional attractors. The system is considered under Dirichlet boundary conditions, and we introduce assumptions on the proliferation term to ensure dissipativity.
在本文中,我们研究了带有增殖项的 Allen-Cahn/Cahn-Hilliard 耦合方程,它可以模拟癌症肿瘤和其他生物实体的生长。我们的重点是建立解的存在性、唯一性和正则性,并分析其渐近行为,尤其关注有限维吸引子的存在。该系统是在 Dirichlet 边界条件下考虑的,我们引入了增殖项的假设,以确保分散性。
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引用次数: 0
On some renormings of l2
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-17 DOI: 10.1016/j.jmaa.2025.129383
Bozena Piatek
Inspired by Melado and Llorens-Fustera (2013) [9] and Dutta and Veeramani (2021) [5], we analyse some renormings of l2. In this class of spaces, we consider the existence of fixed points for two types of mappings: nonexpansive ones and mappings of asymptotically nonexpansive type.
{"title":"On some renormings of l2","authors":"Bozena Piatek","doi":"10.1016/j.jmaa.2025.129383","DOIUrl":"10.1016/j.jmaa.2025.129383","url":null,"abstract":"<div><div>Inspired by Melado and Llorens-Fustera (2013) <span><span>[9]</span></span> and Dutta and Veeramani (2021) <span><span>[5]</span></span>, we analyse some renormings of <span><math><msub><mrow><mi>l</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>. In this class of spaces, we consider the existence of fixed points for two types of mappings: nonexpansive ones and mappings of asymptotically nonexpansive type.</div></div>","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"547 2","pages":"Article 129383"},"PeriodicalIF":1.2,"publicationDate":"2025-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143453246","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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
Study of a new nonlinear Kaup-Newell equations by using nonlocal symmetry method
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-17 DOI: 10.1016/j.jmaa.2025.129379
Weiao Yang, Chen Wang, Yue Shi, Xiangpeng Xin
An important research topic in mathematical physics is the construction of high-dimensional integrable systems. First, based on the method of constructing a high-dimensional integrable system proposed by Lou et al. in this paper, a new (2+1)-dimensional Kaup-Newell (KN) equations are derived through the conservation laws of the (1+1)-dimensional KN equations. Subsequently, we study for the first time the new (1+1)-dimensional KN equations using nonlocal symmetric methods and with the help of constructed closed systems. We then obtained exact solutions of the KN equations, both explicit and special function solution.
{"title":"Study of a new nonlinear Kaup-Newell equations by using nonlocal symmetry method","authors":"Weiao Yang,&nbsp;Chen Wang,&nbsp;Yue Shi,&nbsp;Xiangpeng Xin","doi":"10.1016/j.jmaa.2025.129379","DOIUrl":"10.1016/j.jmaa.2025.129379","url":null,"abstract":"<div><div>An important research topic in mathematical physics is the construction of high-dimensional integrable systems. First, based on the method of constructing a high-dimensional integrable system proposed by Lou et al. in this paper, a new (2+1)-dimensional Kaup-Newell (KN) equations are derived through the conservation laws of the (1+1)-dimensional KN equations. Subsequently, we study for the first time the new (1+1)-dimensional KN equations using nonlocal symmetric methods and with the help of constructed closed systems. We then obtained exact solutions of the KN equations, both explicit and special function solution.</div></div>","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"548 1","pages":"Article 129379"},"PeriodicalIF":1.2,"publicationDate":"2025-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143445257","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 log-majorization version of Audenaert's inequality
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-14 DOI: 10.1016/j.jmaa.2025.129372
Saja Hayajneh , Fuad Kittaneh
For i=1,,k, let Ai and Bi be positive definite matrices. It is shown thats(i=1mAitBi)rlogs((i=1mBi)tpr2(i=1mAi)(1t)pr(i=1mBi)tpr2)1pfor all r>0, p>0 and t[0,1]. This is stronger than the inequalitywhere Ai commutes with Bi for each i and for all unitarily invariant norms, which has been proved by Audenaert. Applications of these inequalities shed some light on the solution of a question of Bourin.
{"title":"A log-majorization version of Audenaert's inequality","authors":"Saja Hayajneh ,&nbsp;Fuad Kittaneh","doi":"10.1016/j.jmaa.2025.129372","DOIUrl":"10.1016/j.jmaa.2025.129372","url":null,"abstract":"<div><div>For <span><math><mi>i</mi><mo>=</mo><mn>1</mn><mo>,</mo><mo>…</mo><mo>,</mo><mi>k</mi></math></span>, let <span><math><msub><mrow><mi>A</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> and <span><math><msub><mrow><mi>B</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> be positive definite matrices. It is shown that<span><span><span><math><mrow><mi>s</mi><msup><mrow><mo>(</mo><munderover><mo>∑</mo><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>m</mi></mrow></munderover><msub><mrow><mi>A</mi></mrow><mrow><mi>i</mi></mrow></msub><msub><mrow><mo>♯</mo></mrow><mrow><mi>t</mi></mrow></msub><msub><mrow><mi>B</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mrow><mi>r</mi></mrow></msup><msub><mrow><mo>≺</mo></mrow><mrow><mi>log</mi></mrow></msub><mi>s</mi><msup><mrow><mo>(</mo><msup><mrow><mo>(</mo><munderover><mo>∑</mo><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>m</mi></mrow></munderover><msub><mrow><mi>B</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mrow><mfrac><mrow><mi>t</mi><mi>p</mi><mi>r</mi></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup><msup><mrow><mo>(</mo><munderover><mo>∑</mo><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>m</mi></mrow></munderover><msub><mrow><mi>A</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mrow><mo>(</mo><mn>1</mn><mo>−</mo><mi>t</mi><mo>)</mo><mi>p</mi><mi>r</mi></mrow></msup><msup><mrow><mo>(</mo><munderover><mo>∑</mo><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>m</mi></mrow></munderover><msub><mrow><mi>B</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mrow><mfrac><mrow><mi>t</mi><mi>p</mi><mi>r</mi></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup><mo>)</mo></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>p</mi></mrow></mfrac></mrow></msup></mrow></math></span></span></span>for all <span><math><mi>r</mi><mo>&gt;</mo><mn>0</mn></math></span>, <span><math><mi>p</mi><mo>&gt;</mo><mn>0</mn></math></span> and <span><math><mi>t</mi><mo>∈</mo><mo>[</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>]</mo></math></span>. This is stronger than the inequality<span><span><img></span></span>where <span><math><msub><mrow><mi>A</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> commutes with <span><math><msub><mrow><mi>B</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> for each <em>i</em> and for all unitarily invariant norms, which has been proved by Audenaert. Applications of these inequalities shed some light on the solution of a question of Bourin.</div></div>","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"548 1","pages":"Article 129372"},"PeriodicalIF":1.2,"publicationDate":"2025-02-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143429037","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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
Quasilinear Schrödinger equation involving critical Hardy potential and Choquard type exponential nonlinearity
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-13 DOI: 10.1016/j.jmaa.2025.129361
Shammi Malhotra , Sarika Goyal , K. Sreenadh
<div><div>In this article, we study the following quasilinear Schrödinger equation involving Hardy potential and Choquard type exponential nonlinearity with a parameter <em>α</em><span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><mo>−</mo><msub><mrow><mi>Δ</mi></mrow><mrow><mi>N</mi></mrow></msub><mi>w</mi><mo>−</mo><msub><mrow><mi>Δ</mi></mrow><mrow><mi>N</mi></mrow></msub><mo>(</mo><mo>|</mo><mi>w</mi><msup><mrow><mo>|</mo></mrow><mrow><mn>2</mn><mi>α</mi></mrow></msup><mo>)</mo><mo>|</mo><mi>w</mi><msup><mrow><mo>|</mo></mrow><mrow><mn>2</mn><mi>α</mi><mo>−</mo><mn>2</mn></mrow></msup><mi>w</mi><mo>−</mo><mi>λ</mi><mfrac><mrow><mo>|</mo><mi>w</mi><msup><mrow><mo>|</mo></mrow><mrow><mn>2</mn><mi>α</mi><mi>N</mi><mo>−</mo><mn>2</mn></mrow></msup><mi>w</mi></mrow><mrow><msup><mrow><mo>(</mo><mo>|</mo><mi>x</mi><mo>|</mo><mi>log</mi><mo>⁡</mo><mrow><mo>(</mo><mfrac><mrow><mi>R</mi></mrow><mrow><mo>|</mo><mi>x</mi><mo>|</mo></mrow></mfrac><mo>)</mo></mrow><mo>)</mo></mrow><mrow><mi>N</mi></mrow></msup></mrow></mfrac></mtd></mtr><mtr><mtd><mspace></mspace><mo>=</mo><mrow><mo>(</mo><msub><mrow><mo>∫</mo></mrow><mrow><mi>Ω</mi></mrow></msub><mfrac><mrow><mi>H</mi><mo>(</mo><mi>y</mi><mo>,</mo><mi>w</mi><mo>(</mo><mi>y</mi><mo>)</mo><mo>)</mo></mrow><mrow><mo>|</mo><mi>x</mi><mo>−</mo><mi>y</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>μ</mi></mrow></msup></mrow></mfrac><mi>d</mi><mi>y</mi><mo>)</mo></mrow><mi>h</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>w</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>)</mo><mspace></mspace><mtext>in </mtext><mspace></mspace><mi>Ω</mi><mo>,</mo></mtd></mtr><mtr><mtd><mi>w</mi><mo>></mo><mn>0</mn><mtext> in </mtext><mi>Ω</mi><mo>∖</mo><mo>{</mo><mn>0</mn><mo>}</mo><mo>,</mo><mspace></mspace><mspace></mspace><mi>w</mi><mo>=</mo><mn>0</mn><mtext> on </mtext><mo>∂</mo><mi>Ω</mi><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> where <span><math><mi>N</mi><mo>≥</mo><mn>2</mn></math></span>, <span><math><mi>α</mi><mo>></mo><mfrac><mrow><mn>1</mn></mrow><mrow><mn>2</mn></mrow></mfrac></math></span>, <span><math><mn>0</mn><mo>≤</mo><mi>λ</mi><mo><</mo><msup><mrow><mo>(</mo><mfrac><mrow><mi>N</mi><mo>−</mo><mn>1</mn></mrow><mrow><mi>N</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mi>N</mi></mrow></msup></math></span>, <span><math><mn>0</mn><mo><</mo><mi>μ</mi><mo><</mo><mi>N</mi></math></span>, <span><math><mi>h</mi><mo>:</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup><mo>×</mo><mi>R</mi><mo>→</mo><mi>R</mi></math></span> is a continuous function with critical exponential growth in the sense of the Trudinger-Moser inequality and <span><math><mi>H</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>=</mo><msubsup><mrow><mo>∫</mo></mrow><mrow><mn>0</mn></mrow><mrow><mi>t</mi></mrow></msubsup><mi>h</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>s</mi><mo>)</mo><mi>d</mi><mi>s</mi></math></span> is the primitive of <em>h</em>. With the help of the Mountain Pass Theorem and critical level, which is
{"title":"Quasilinear Schrödinger equation involving critical Hardy potential and Choquard type exponential nonlinearity","authors":"Shammi Malhotra ,&nbsp;Sarika Goyal ,&nbsp;K. Sreenadh","doi":"10.1016/j.jmaa.2025.129361","DOIUrl":"10.1016/j.jmaa.2025.129361","url":null,"abstract":"&lt;div&gt;&lt;div&gt;In this article, we study the following quasilinear Schrödinger equation involving Hardy potential and Choquard type exponential nonlinearity with a parameter &lt;em&gt;α&lt;/em&gt;&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;λ&lt;/mi&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;log&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;in &lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mtext&gt; in &lt;/mtext&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;∖&lt;/mo&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;}&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mtext&gt; on &lt;/mtext&gt;&lt;mo&gt;∂&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; where &lt;span&gt;&lt;math&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mi&gt;λ&lt;/mi&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mo&gt;→&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is a continuous function with critical exponential growth in the sense of the Trudinger-Moser inequality and &lt;span&gt;&lt;math&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is the primitive of &lt;em&gt;h&lt;/em&gt;. With the help of the Mountain Pass Theorem and critical level, which is ","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"548 1","pages":"Article 129361"},"PeriodicalIF":1.2,"publicationDate":"2025-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143445219","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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
Nonformal deformations of the algebras of holomorphic functions on the polydisk and on the ball in Cn
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-13 DOI: 10.1016/j.jmaa.2025.129371
Alexei Yu. Pirkovskii
<div><div>We construct Fréchet <span><math><mi>O</mi><mo>(</mo><msup><mrow><mi>C</mi></mrow><mrow><mo>×</mo></mrow></msup><mo>)</mo></math></span>-algebras <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>def</mi></mrow></msub><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> and <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>def</mi></mrow></msub><mo>(</mo><msup><mrow><mi>B</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> which may be interpreted as nonformal (or, more exactly, holomorphic) deformations of the algebras <span><math><mi>O</mi><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> and <span><math><mi>O</mi><mo>(</mo><msup><mrow><mi>B</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> of holomorphic functions on the polydisk <span><math><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>⊂</mo><msup><mrow><mi>C</mi></mrow><mrow><mi>n</mi></mrow></msup></math></span> and on the ball <span><math><msup><mrow><mi>B</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>⊂</mo><msup><mrow><mi>C</mi></mrow><mrow><mi>n</mi></mrow></msup></math></span>, respectively. The fibers of our algebras over <span><math><mi>q</mi><mo>∈</mo><msup><mrow><mi>C</mi></mrow><mrow><mo>×</mo></mrow></msup></math></span> are isomorphic to the previously introduced “quantum polydisk” and “quantum ball” algebras, <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> and <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub><mo>(</mo><msup><mrow><mi>B</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span>. We show that the algebras <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>def</mi></mrow></msub><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> and <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>def</mi></mrow></msub><mo>(</mo><msup><mrow><mi>B</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> yield continuous Fréchet algebra bundles over <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>×</mo></mrow></msup></math></span> which are strict deformation quantizations (in Rieffel's sense) of <span><math><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup></math></span> and <span><math><msup><mrow><mi>B</mi></mrow><mrow><mi>n</mi></mrow></msup></math></span>. We also give a noncommutative power series interpretation of <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>def</mi></mrow></msub><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> and apply it to showing that <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>def</mi></mrow></msub><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> is not topologically projective (and a fortiori is not topol
{"title":"Nonformal deformations of the algebras of holomorphic functions on the polydisk and on the ball in Cn","authors":"Alexei Yu. Pirkovskii","doi":"10.1016/j.jmaa.2025.129371","DOIUrl":"10.1016/j.jmaa.2025.129371","url":null,"abstract":"&lt;div&gt;&lt;div&gt;We construct Fréchet &lt;span&gt;&lt;math&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;-algebras &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;def&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;def&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; which may be interpreted as nonformal (or, more exactly, holomorphic) deformations of the algebras &lt;span&gt;&lt;math&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; of holomorphic functions on the polydisk &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; and on the ball &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;, respectively. The fibers of our algebras over &lt;span&gt;&lt;math&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; are isomorphic to the previously introduced “quantum polydisk” and “quantum ball” algebras, &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;. We show that the algebras &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;def&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;def&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; yield continuous Fréchet algebra bundles over &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; which are strict deformation quantizations (in Rieffel's sense) of &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;. We also give a noncommutative power series interpretation of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;def&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and apply it to showing that &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;def&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is not topologically projective (and a fortiori is not topol","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"547 2","pages":"Article 129371"},"PeriodicalIF":1.2,"publicationDate":"2025-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143427892","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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
Subordination and related inequalities on a C⁎−algebra
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-12 DOI: 10.1016/j.jmaa.2025.129365
A.K. Mishra , P. Gochhayat
Let X be a C-algebra, xX and x<1. For a complex valued function f, which is analytic in U={λC:|λ|<1} let f(x) be defined by the following integral: f(x)=Γf(λ)(λex)1dλ, where Γ is a positively oriented rectifiable simple closed contour in U that surrounds σ(x), the spectrum of x. In this paper Schwarz's lemma, Harnack's inequalities and results related to subordination are obtained for f(x).
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引用次数: 0
Multi-dimensional fractional Brownian motion in the G-setting
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2025-02-12 DOI: 10.1016/j.jmaa.2025.129364
Francesca Biagini , Andrea Mazzon , Katharina Oberpriller
In this paper we introduce a definition of a multi-dimensional fractional Brownian motion of Hurst index H(0,1) under volatility uncertainty (in short G-fBm). We study the properties of such a process and provide first results about stochastic calculus with respect to a multi-dimensional G-fBm for a Hurst index H(12,1).
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引用次数: 0
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Journal of Mathematical Analysis and Applications
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