Pub Date : 2025-09-10DOI: 10.1007/s13324-025-01127-w
Hidemasa Suzuki
Fukaya and Oh studied the correspondence between pseudoholomorphic disks in (T^{*}M) which are bounded by Lagrangian sections ({L_{i}^{epsilon }}) and gradient trees in M which consist of gradient curves of ({f_{i}-f_{j}}). Here, (L_{i}^{epsilon }) is defined by (L_{i}^{epsilon }=) graph((epsilon df_{i})). They constructed approximate pseudoholomorphic disks in the case (epsilon >0) is sufficiently small. When (M=mathbb {R}) and Lagrangian sections are affine, pseudoholomorphic disks (w_{epsilon }) can be constructed explicitly. In this paper, we show that pseudoholomorphic disks (w_{epsilon }) converges to the gradient tree in the limit (epsilon rightarrow +0) when the number of Lagrangian sections is three and four.
{"title":"Explicit correspondences between gradient trees in (mathbb {R}) and holomorphic disks in (T^{*}mathbb {R})","authors":"Hidemasa Suzuki","doi":"10.1007/s13324-025-01127-w","DOIUrl":"10.1007/s13324-025-01127-w","url":null,"abstract":"<div><p>Fukaya and Oh studied the correspondence between pseudoholomorphic disks in <span>(T^{*}M)</span> which are bounded by Lagrangian sections <span>({L_{i}^{epsilon }})</span> and gradient trees in <i>M</i> which consist of gradient curves of <span>({f_{i}-f_{j}})</span>. Here, <span>(L_{i}^{epsilon })</span> is defined by <span>(L_{i}^{epsilon }=)</span> graph<span>((epsilon df_{i}))</span>. They constructed approximate pseudoholomorphic disks in the case <span>(epsilon >0)</span> is sufficiently small. When <span>(M=mathbb {R})</span> and Lagrangian sections are affine, pseudoholomorphic disks <span>(w_{epsilon })</span> can be constructed explicitly. In this paper, we show that pseudoholomorphic disks <span>(w_{epsilon })</span> converges to the gradient tree in the limit <span>(epsilon rightarrow +0)</span> when the number of Lagrangian sections is three and four.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145021706","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}
Pub Date : 2025-09-03DOI: 10.1007/s13324-025-01123-0
Sultana Ben Aadi, Khalid Akhlil, Daniela Inoan
In this paper, we define generalized monotonicity concepts related to equilibrium problems generated by trifunctions. We then study the existence of solutions to mixed equilibrium problems described as the sum of a maximal monotone trifunction and a pseudomonotone trifunction in Brézis sense. The main tools for this study are a Thikonov regularization procedure with respect to the generalized duality mapping and recession analysis adapted to trifunctions. An application consists in an existence result for a noncoercive hemivariational inequality.
{"title":"Equilibrium problems with trifunctions and applications to hemivariational inequalities","authors":"Sultana Ben Aadi, Khalid Akhlil, Daniela Inoan","doi":"10.1007/s13324-025-01123-0","DOIUrl":"10.1007/s13324-025-01123-0","url":null,"abstract":"<div><p>In this paper, we define generalized monotonicity concepts related to equilibrium problems generated by trifunctions. We then study the existence of solutions to mixed equilibrium problems described as the sum of a maximal monotone trifunction and a pseudomonotone trifunction in Brézis sense. The main tools for this study are a Thikonov regularization procedure with respect to the generalized duality mapping and recession analysis adapted to trifunctions. An application consists in an existence result for a noncoercive hemivariational inequality.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144934500","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}
Pub Date : 2025-09-03DOI: 10.1007/s13324-025-01125-y
Khaled Hleili, Youssef El Haoui
The aim of this paper is to investigate the right-sided quaternionic free metaplectic transformation (QFMT) and its associated uncertainty principles (UPs) for (mathbb {R}^{2d})-dimensional quaternionic-valued signals. First, we establish the fundamental mathematical properties of the QFMT, including partial derivatives, the inversion formula, Parseval’s theorem, and the Hausdorff–Young inequality. Next, we establish various UPs within this framework, such as the Rènyi and Shannon entropy UPs and Donoho–Stark’s UP in terms of concentration. Finally, we derive (L^a)-bandlimited variant of the Donoho–Stark UP in the QFMT domain.
{"title":"The right-sided quaternionic free metaplectic transformation and associated uncertainty principles","authors":"Khaled Hleili, Youssef El Haoui","doi":"10.1007/s13324-025-01125-y","DOIUrl":"10.1007/s13324-025-01125-y","url":null,"abstract":"<div><p>The aim of this paper is to investigate the right-sided quaternionic free metaplectic transformation (QFMT) and its associated uncertainty principles (UPs) for <span>(mathbb {R}^{2d})</span>-dimensional quaternionic-valued signals. First, we establish the fundamental mathematical properties of the QFMT, including partial derivatives, the inversion formula, Parseval’s theorem, and the Hausdorff–Young inequality. Next, we establish various UPs within this framework, such as the Rènyi and Shannon entropy UPs and Donoho–Stark’s UP in terms of concentration. Finally, we derive <span>(L^a)</span>-bandlimited variant of the Donoho–Stark UP in the QFMT domain.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144934578","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}
Pub Date : 2025-09-02DOI: 10.1007/s13324-025-01124-z
Boris Kruglikov, Vladimir S. Matveev, Wijnand Steneker
Conformal geodesics form an invariantly defined family of unparametrized curves in a conformal manifold generalizing unparametrized geodesics/paths of projective connections. The equation describing them is of third order, and it was an open problem whether they are given by an Euler–Lagrange equation. In dimension 3 (the simplest, but most important from the viewpoint of physical applications) we demonstrate that the equation for unparametrized conformal geodesics is variational.
{"title":"Variationality of Conformal Geodesics in dimension 3","authors":"Boris Kruglikov, Vladimir S. Matveev, Wijnand Steneker","doi":"10.1007/s13324-025-01124-z","DOIUrl":"10.1007/s13324-025-01124-z","url":null,"abstract":"<div><p>Conformal geodesics form an invariantly defined family of unparametrized curves in a conformal manifold generalizing unparametrized geodesics/paths of projective connections. The equation describing them is of third order, and it was an open problem whether they are given by an Euler–Lagrange equation. In dimension 3 (the simplest, but most important from the viewpoint of physical applications) we demonstrate that the equation for unparametrized conformal geodesics is variational.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s13324-025-01124-z.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144929265","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-29DOI: 10.1007/s13324-025-01122-1
Oleg Safronov
We consider the Schrödinger operator on the quantum graph whose edges connect the points of ({{mathbb {Z}}}). The numbers of the edges connecting two consecutive points n and (n+1) are read along the orbits of a shift of finite type. We prove that the Lyapunov exponent is potitive for energies E that do not belong to a discrete subset of ([0,infty )). The number of points E of this subset in ([(pi (j-1))^2, (pi j)^2]) is the same for all (jin {{mathbb {N}}}).
{"title":"Lyapunov exponent for quantum graphs coded as elements of a subshift of finite type","authors":"Oleg Safronov","doi":"10.1007/s13324-025-01122-1","DOIUrl":"10.1007/s13324-025-01122-1","url":null,"abstract":"<div><p>We consider the Schrödinger operator on the quantum graph whose edges connect the points of <span>({{mathbb {Z}}})</span>. The numbers of the edges connecting two consecutive points <i>n</i> and <span>(n+1)</span> are read along the orbits of a shift of finite type. We prove that the Lyapunov exponent is potitive for energies <i>E</i> that do not belong to a discrete subset of <span>([0,infty ))</span>. The number of points <i>E</i> of this subset in <span>([(pi (j-1))^2, (pi j)^2])</span> is the same for all <span>(jin {{mathbb {N}}})</span>.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s13324-025-01122-1.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144918340","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-29DOI: 10.1007/s13324-025-01120-3
Ahmed Ahmed, Mohamed Saad Bouh Elemine Vall, Taghi Ahmedatt
In this paper, we investigate the existence of multiple weak solutions for a Schrödinger-Kirchhoff type elliptic system involving nonlocal ((alpha _1(cdot ), ldots , alpha _N(cdot )))-Laplacian operator. The system is modeled as follows:
$$begin{aligned} {left{ begin{array}{ll} mathfrak {M}_ileft( int _{mathbb {R}^N}frac{1}{alpha _{i}(y)}|nabla u_{i}|^{alpha _{i}(y)} dy+int _{mathbb {R}^N}frac{mathcal {V}_{i}(y)}{alpha _{i}(y)}| u_{i}|^{alpha _{i}(y)} dyright) Big (-Delta _{alpha _{i}(cdot )} u_{i} +mathcal {V}_{i}(y)|u_{i}|^{alpha _{i}(y)-2}u_{i}Big ) quad = mu mathcal {F}_{u_i}(y, u_{1}, ldots , u_{N}) + nu mathcal {G}_{u_i}(y, u_{1}, ldots , u_{N}), quad text {in } mathbb {R}^N, text { for all } i = 1, dots , N, (u_{1}, ldots , u_{N}) in mathbb {H}. end{array}right. } end{aligned}$$
We apply the three critical points theorem to establish sufficient conditions for the existence of at least three weak solutions under appropriate assumptions on the system’s parameters and nonlinearity terms. This work extends the analysis of elliptic systems involving variable exponent spaces and nonlocal operators, offering novel insights into their mathematical structure and solution properties.
本文研究了一类涉及非局部的Schrödinger-Kirchhoff型椭圆系统的多个弱解的存在性 ((alpha _1(cdot ), ldots , alpha _N(cdot )))-拉普拉斯算子。系统建模如下: $$begin{aligned} {left{ begin{array}{ll} mathfrak {M}_ileft( int _{mathbb {R}^N}frac{1}{alpha _{i}(y)}|nabla u_{i}|^{alpha _{i}(y)} dy+int _{mathbb {R}^N}frac{mathcal {V}_{i}(y)}{alpha _{i}(y)}| u_{i}|^{alpha _{i}(y)} dyright) Big (-Delta _{alpha _{i}(cdot )} u_{i} +mathcal {V}_{i}(y)|u_{i}|^{alpha _{i}(y)-2}u_{i}Big ) quad = mu mathcal {F}_{u_i}(y, u_{1}, ldots , u_{N}) + nu mathcal {G}_{u_i}(y, u_{1}, ldots , u_{N}), quad text {in } mathbb {R}^N, text { for all } i = 1, dots , N, (u_{1}, ldots , u_{N}) in mathbb {H}. end{array}right. } end{aligned}$$应用三个临界点定理,在系统参数和非线性项的适当假设下,建立了系统存在至少三个弱解的充分条件。这项工作扩展了涉及变指数空间和非局部算子的椭圆系统的分析,提供了对其数学结构和解性质的新见解。
{"title":"Three Weak Solutions of ((alpha _1(cdot ), ldots , alpha _N(cdot )))-Laplacian-Schrödinger-Kirchhoff Systems","authors":"Ahmed Ahmed, Mohamed Saad Bouh Elemine Vall, Taghi Ahmedatt","doi":"10.1007/s13324-025-01120-3","DOIUrl":"10.1007/s13324-025-01120-3","url":null,"abstract":"<div><p>In this paper, we investigate the existence of multiple weak solutions for a Schrödinger-Kirchhoff type elliptic system involving nonlocal <span>((alpha _1(cdot ), ldots , alpha _N(cdot )))</span>-Laplacian operator. The system is modeled as follows: </p><div><div><span>$$begin{aligned} {left{ begin{array}{ll} mathfrak {M}_ileft( int _{mathbb {R}^N}frac{1}{alpha _{i}(y)}|nabla u_{i}|^{alpha _{i}(y)} dy+int _{mathbb {R}^N}frac{mathcal {V}_{i}(y)}{alpha _{i}(y)}| u_{i}|^{alpha _{i}(y)} dyright) Big (-Delta _{alpha _{i}(cdot )} u_{i} +mathcal {V}_{i}(y)|u_{i}|^{alpha _{i}(y)-2}u_{i}Big ) quad = mu mathcal {F}_{u_i}(y, u_{1}, ldots , u_{N}) + nu mathcal {G}_{u_i}(y, u_{1}, ldots , u_{N}), quad text {in } mathbb {R}^N, text { for all } i = 1, dots , N, (u_{1}, ldots , u_{N}) in mathbb {H}. end{array}right. } end{aligned}$$</span></div></div><p>We apply the three critical points theorem to establish sufficient conditions for the existence of at least three weak solutions under appropriate assumptions on the system’s parameters and nonlinearity terms. This work extends the analysis of elliptic systems involving variable exponent spaces and nonlocal operators, offering novel insights into their mathematical structure and solution properties.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144918341","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}
Pub Date : 2025-08-28DOI: 10.1007/s13324-025-01119-w
Oleg I. Morozov
We find two Lax representations for the reduced magnetohydrodynamics equations (rmhd) and construct a local variational Poisson structure (a Hamiltonian operator) for them. Its inverse defines a nonlocal symplectic structure for the same equations. We describe the action of both operators on the second-order cosymmetries and on the infinitesimal contact symmetries of rmhd, respectively. The reduction of rmhd by the symmetry of shifts along the z-axis coincides with the equations of two-dimensional ideal magnetohydrodynamics (imhd). Applied to the Lax representations and the variational Poisson structure of rmhd, the reduction provides analogous constructions for imhd.
{"title":"Lax representations and variational Poisson structures for magnetohydrodynamics equations","authors":"Oleg I. Morozov","doi":"10.1007/s13324-025-01119-w","DOIUrl":"10.1007/s13324-025-01119-w","url":null,"abstract":"<div><p>We find two Lax representations for the reduced magnetohydrodynamics equations (<span>rmhd</span>) and construct a local variational Poisson structure (a Hamiltonian operator) for them. Its inverse defines a nonlocal symplectic structure for the same equations. We describe the action of both operators on the second-order cosymmetries and on the infinitesimal contact symmetries of <span>rmhd</span>, respectively. The reduction of <span>rmhd</span> by the symmetry of shifts along the <i>z</i>-axis coincides with the equations of two-dimensional ideal magnetohydrodynamics (<span>imhd</span>). Applied to the Lax representations and the variational Poisson structure of <span>rmhd</span>, the reduction provides analogous constructions for <span>imhd</span>.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144914569","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}
Pub Date : 2025-08-27DOI: 10.1007/s13324-025-01121-2
Jørgen Olsen Lye, Boris Vertman, Mannaim Gennaro Vitti
In this work we introduce a family of conformal flows generalizing the classical Yamabe flow. We prove that for a large class of such flows long-time existence holds, and the arguments are in fact simpler than in the classical case. Moreover, we establish convergence for the case of negative scalar curvature and expect a similar statement for the positive and the flat cases as well.
{"title":"Generalized Yamabe Flows","authors":"Jørgen Olsen Lye, Boris Vertman, Mannaim Gennaro Vitti","doi":"10.1007/s13324-025-01121-2","DOIUrl":"10.1007/s13324-025-01121-2","url":null,"abstract":"<div><p>In this work we introduce a family of conformal flows generalizing the classical Yamabe flow. We prove that for a large class of such flows long-time existence holds, and the arguments are in fact simpler than in the classical case. Moreover, we establish convergence for the case of negative scalar curvature and expect a similar statement for the positive and the flat cases as well.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-08-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s13324-025-01121-2.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144905081","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-14DOI: 10.1007/s13324-025-01117-y
Aiting Wang, Wenhua Wang, Mingquan Wei, Baode Li
Let X be a ball quasi-Banach function space, (alpha in mathbb {R}) and (qin (0,infty )). In this article, the authors first introduce the Herz-type Hardy space (mathcal {Hdot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n)), which is defined via the non-tangential grand maximal function. Under some mild assumptions on X, the authors establish the atomic decompositions of (mathcal {Hdot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n)). As an application, the authors obtain the boundedness of certain sublinear operators from (mathcal {Hdot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n)) to (mathcal {dot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n)), where (mathcal {dot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n)) denotes the Herz-type space associated with ball quasi-Banach function space X. Finally, the authors apply these results to three concrete function spaces: Herz-type Hardy spaces with variable exponent, mixed Herz-Hardy spaces and Orlicz-Herz Hardy spaces, which belong to the family of Herz-type Hardy spaces associated with ball quasi-Banach function spaces.
{"title":"Herz-type Hardy spaces associated with ball quasi-Banach function spaces","authors":"Aiting Wang, Wenhua Wang, Mingquan Wei, Baode Li","doi":"10.1007/s13324-025-01117-y","DOIUrl":"10.1007/s13324-025-01117-y","url":null,"abstract":"<div><p>Let <i>X</i> be a ball quasi-Banach function space, <span>(alpha in mathbb {R})</span> and <span>(qin (0,infty ))</span>. In this article, the authors first introduce the Herz-type Hardy space <span>(mathcal {Hdot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n))</span>, which is defined via the non-tangential grand maximal function. Under some mild assumptions on <i>X</i>, the authors establish the atomic decompositions of <span>(mathcal {Hdot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n))</span>. As an application, the authors obtain the boundedness of certain sublinear operators from <span>(mathcal {Hdot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n))</span> to <span>(mathcal {dot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n))</span>, where <span>(mathcal {dot{K}}_{X}^{alpha ,,q}({mathbb {R}}^n))</span> denotes the Herz-type space associated with ball quasi-Banach function space <i>X</i>. Finally, the authors apply these results to three concrete function spaces: Herz-type Hardy spaces with variable exponent, mixed Herz-Hardy spaces and Orlicz-Herz Hardy spaces, which belong to the family of Herz-type Hardy spaces associated with ball quasi-Banach function spaces.</p></div>","PeriodicalId":48860,"journal":{"name":"Analysis and Mathematical Physics","volume":"15 5","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144832305","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}