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15 pages, 309 KiB  
Article
Existence of Solutions for a Perturbed N-Laplacian Boundary Value Problem with Critical Growth
by Sheng Shi and Yang Yang
Axioms 2024, 13(11), 733; https://doi.org/10.3390/axioms13110733 - 23 Oct 2024
Viewed by 414
Abstract
In this paper, we investigate a perturbed elliptic boundary value problem that exhibits critical growth characterized by a Trudinger–Moser-type inequality. Our primary focus is to establish the existence of two nontrivial solutions. This is achieved by employing a combination of the Trudinger–Moser-type inequality [...] Read more.
In this paper, we investigate a perturbed elliptic boundary value problem that exhibits critical growth characterized by a Trudinger–Moser-type inequality. Our primary focus is to establish the existence of two nontrivial solutions. This is achieved by employing a combination of the Trudinger–Moser-type inequality and a linking theorem based on the Z2-cohomological index. The main feature and novelty of this paper lies in extending the equation to N-Laplacian boundary value problems utilizing the aforementioned methods. This extension not only broadens the applicability of these techniques but also enriches the research outcomes in the field of nonlinear analysis. Full article
(This article belongs to the Special Issue Differential Equations and Related Topics, 2nd Edition)
28 pages, 407 KiB  
Article
Continuity Equation of Transverse Kähler Metrics on Sasakian Manifolds
by Yushuang Fan and Tao Zheng
Mathematics 2024, 12(19), 3132; https://doi.org/10.3390/math12193132 - 7 Oct 2024
Viewed by 538
Abstract
We introduce the continuity equation of transverse Kähler metrics on Sasakian manifolds and establish its interval of maximal existence. When the first basic Chern class is null (resp. negative), we prove that the solution of the (resp. normalized) continuity equation converges smoothly to [...] Read more.
We introduce the continuity equation of transverse Kähler metrics on Sasakian manifolds and establish its interval of maximal existence. When the first basic Chern class is null (resp. negative), we prove that the solution of the (resp. normalized) continuity equation converges smoothly to the unique η-Einstein metric in the basic Bott–Chern cohomological class of the initial transverse Kähler metric (resp. first basic Chern class). These results are the transverse version of the continuity equation of the Kähler metrics studied by La Nave and Tian, and also counterparts of the Sasaki–Ricci flow studied by Smoczyk, Wang, and Zhang. Full article
(This article belongs to the Special Issue Complex Analysis and Geometric Function Theory, 2nd Edition)
17 pages, 296 KiB  
Article
Crossed Modules and Non-Abelian Extensions of Differential Leibniz Conformal Algebras
by Hui Wu, Shuangjian Guo and Xiaohui Zhang
Axioms 2024, 13(10), 685; https://doi.org/10.3390/axioms13100685 - 2 Oct 2024
Viewed by 380
Abstract
In this paper, we introduce two-term differential Leib-conformal algebras and give characterizations of some particular classes of such two-term differential Leib-conformal algebras. Furthermore, we discuss the classification of the non-Abelian extensions in terms [...] Read more.
In this paper, we introduce two-term differential Leib-conformal algebras and give characterizations of some particular classes of such two-term differential Leib-conformal algebras. Furthermore, we discuss the classification of the non-Abelian extensions in terms of non-Abelian cohomology groups. Finally, we explore the inducibility of pairs of automorphisms and derive the analog Wells exact sequences under the circumstance of differential Leibniz conformal algebras. Full article
32 pages, 437 KiB  
Article
The Dirac-Dolbeault Operator Approach to the Hodge Conjecture
by Simone Farinelli
Symmetry 2024, 16(10), 1291; https://doi.org/10.3390/sym16101291 - 1 Oct 2024
Viewed by 1726
Abstract
The Dirac-Dolbeault operator for a compact Kähler manifold is a special case of Dirac operator. The Green function for the Dirac Laplacian over a Riemannian manifold with boundary allows the expression of the values of the sections of the Dirac bundle in terms [...] Read more.
The Dirac-Dolbeault operator for a compact Kähler manifold is a special case of Dirac operator. The Green function for the Dirac Laplacian over a Riemannian manifold with boundary allows the expression of the values of the sections of the Dirac bundle in terms of the values on the boundary, extending the mean value theorem of harmonic analysis. Utilizing this representation and the Nash–Moser generalized inverse function theorem, we prove the existence of complex submanifolds of a complex projective manifold satisfying globally a certain partial differential equation under a certain injectivity assumption. Thereby, internal symmetries of Dolbeault and rational Hodge cohomologies play a crucial role. Next, we show the existence of complex submanifolds whose fundamental classes span the rational Hodge classes, proving the Hodge conjecture for complex projective manifolds. Full article
(This article belongs to the Section Mathematics)
4 pages, 210 KiB  
Correction
Correction: Bychkov et al. The σ Cohomology Analysis for Symmetric Higher-Spin Fields. Symmetry 2021, 13, 1498
by Alexey S. Bychkov, Kirill A. Ushakov and Mikhail A. Vasiliev
Symmetry 2024, 16(9), 1115; https://doi.org/10.3390/sym16091115 - 28 Aug 2024
Viewed by 330
Abstract
There was an error in the original publication [...] Full article
(This article belongs to the Section Physics)
7 pages, 241 KiB  
Article
Geometry of Torsion Gerbes and Flat Twisted Vector Bundles
by Byungdo Park
Axioms 2024, 13(8), 504; https://doi.org/10.3390/axioms13080504 - 26 Jul 2024
Viewed by 449
Abstract
Gerbes and higher gerbes are geometric cocycles representing higher degree cohomology classes, and are attracting considerable interest in differential geometry and mathematical physics. We prove that a 2-gerbe has a torsion Dixmier–Douady class if and only if the gerbe has locally constant cocycle [...] Read more.
Gerbes and higher gerbes are geometric cocycles representing higher degree cohomology classes, and are attracting considerable interest in differential geometry and mathematical physics. We prove that a 2-gerbe has a torsion Dixmier–Douady class if and only if the gerbe has locally constant cocycle data. As an application, we give an alternative description of flat twisted vector bundles in terms of locally constant transition maps. These results generalize to n-gerbes for n=1 and n3, providing insights into the structure of higher gerbes and their applications to the geometry of twisted vector bundles. Full article
(This article belongs to the Special Issue Differential Geometry and Its Application, 2nd Edition)
17 pages, 310 KiB  
Article
Cohomology and Crossed Modules of Modified Rota–Baxter Pre-Lie Algebras
by Fuyang Zhu and Wen Teng
Mathematics 2024, 12(14), 2260; https://doi.org/10.3390/math12142260 - 19 Jul 2024
Viewed by 749
Abstract
The goal of the present paper is to provide a cohomology theory and crossed modules of modified Rota–Baxter pre-Lie algebras. We introduce the notion of a modified Rota–Baxter pre-Lie algebra and its bimodule. We define a cohomology of modified Rota–Baxter pre-Lie algebras with [...] Read more.
The goal of the present paper is to provide a cohomology theory and crossed modules of modified Rota–Baxter pre-Lie algebras. We introduce the notion of a modified Rota–Baxter pre-Lie algebra and its bimodule. We define a cohomology of modified Rota–Baxter pre-Lie algebras with coefficients in a suitable bimodule. Furthermore, we study the infinitesimal deformations and abelian extensions of modified Rota–Baxter pre-Lie algebras and relate them with the second cohomology groups. Finally, we investigate skeletal and strict modified Rota–Baxter pre-Lie 2-algebras. We show that skeletal modified Rota–Baxter pre-Lie 2-algebras can be classified into the third cohomology group, and strict modified Rota–Baxter pre-Lie 2-algebras are equivalent to the crossed modules of modified Rota–Baxter pre-Lie algebras. Full article
(This article belongs to the Special Issue Advanced Research in Pure and Applied Algebra)
28 pages, 999 KiB  
Article
Applications of Differential Geometry Linking Topological Bifurcations to Chaotic Flow Fields
by Peter D. Neilson and Megan D. Neilson
AppliedMath 2024, 4(2), 763-790; https://doi.org/10.3390/appliedmath4020041 - 15 Jun 2024
Viewed by 835
Abstract
At every point p on a smooth n-manifold M there exist n+1 skew-symmetric tensor spaces spanning differential r-forms ω with r=0,1,,n. Because dd is always zero where d [...] Read more.
At every point p on a smooth n-manifold M there exist n+1 skew-symmetric tensor spaces spanning differential r-forms ω with r=0,1,,n. Because dd is always zero where d is the exterior differential, it follows that every exact r-form (i.e., ω=dλ where λ is an r1-form) is closed (i.e., dω=0) but not every closed r-form is exact. This implies the existence of a third type of differential r-form that is closed but not exact. Such forms are called harmonic forms. Every smooth n-manifold has an underlying topological structure. Many different possible topological structures exist. What distinguishes one topological structure from another is the number of holes of various dimensions it possesses. De Rham’s theory of differential forms relates the presence of r-dimensional holes in the underlying topology of a smooth n-manifold M to the presence of harmonic r-form fields on the smooth manifold. A large amount of theory is required to understand de Rham’s theorem. In this paper we summarize the differential geometry that links holes in the underlying topology of a smooth manifold with harmonic fields on the manifold. We explore the application of de Rham’s theory to (i) visual, (ii) mechanical, (iii) electrical and (iv) fluid flow systems. In particular, we consider harmonic flow fields in the intracellular aqueous solution of biological cells and we propose, on mathematical grounds, a possible role of harmonic flow fields in the folding of protein polypeptide chains. Full article
Show Figures

Figure 1

Figure 1
<p>A diagram illustrating homotopy. The 2-torus (surface of a donut) in the topological space <math display="inline"><semantics> <mi>Y</mi> </semantics></math> and the coffee mug with handle in the topological space <math display="inline"><semantics> <mi>Y</mi> </semantics></math> are equivalent topological structures. These are not only homeomorphically related (i.e., continuous, one-to-one, onto and invertible) but there are continuous homotopic maps <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> <mo>,</mo> <msub> <mi>f</mi> <mn>1</mn> </msub> <mo>:</mo> <mi>X</mi> <mo>→</mo> <mi>Y</mi> </mrow> </semantics></math> that map the topological space <math display="inline"><semantics> <mi>X</mi> </semantics></math> to both the 2-torus and the mug. The fact that the donut can be continuously transformed into the mug implies the existence of all the intermediate shapes in the transformation. The hole in the donut morphs into the hole between the mug and its handle. This is illustrated in the diagram by the special case in which <math display="inline"><semantics> <mrow> <mi>Y</mi> <mo>=</mo> <mi>X</mi> <mo>×</mo> <mi>I</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> <mo>=</mo> <msub> <mi>i</mi> <mn>0</mn> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>i</mi> <mn>1</mn> </msub> </mrow> </semantics></math>, where the interval <math display="inline"><semantics> <mi>I</mi> </semantics></math> varies from <math display="inline"><semantics> <mn>0</mn> </semantics></math> to <math display="inline"><semantics> <mn>1</mn> </semantics></math>. For each point <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>∈</mo> <mi>X</mi> </mrow> </semantics></math>, the map <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> <mfenced> <mi>x</mi> </mfenced> <mo>=</mo> <msub> <mi>i</mi> <mn>0</mn> </msub> <mfenced> <mi>x</mi> </mfenced> <mo>=</mo> <mfenced> <mrow> <mi>x</mi> <mo>,</mo> <mn>0</mn> </mrow> </mfenced> </mrow> </semantics></math> corresponds to the 2-torus, the map <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>1</mn> </msub> <mfenced> <mi>x</mi> </mfenced> <mo>=</mo> <msub> <mi>i</mi> <mn>1</mn> </msub> <mfenced> <mi>x</mi> </mfenced> <mo>=</mo> <mfenced> <mrow> <mi>x</mi> <mo>,</mo> <mn>1</mn> </mrow> </mfenced> </mrow> </semantics></math> corresponds to the mug and all the other points along the interval <math display="inline"><semantics> <mi>I</mi> </semantics></math> correspond to the intermediate shapes. This is represented in the diagram by the homotopy <math display="inline"><semantics> <mi>H</mi> </semantics></math>. More generally, while the topological spaces <math display="inline"><semantics> <mi>X</mi> </semantics></math> and <math display="inline"><semantics> <mi>Y</mi> </semantics></math> can include holes of various dimensions, they must have the same topological structure in order for the homotopy <math display="inline"><semantics> <mi>H</mi> </semantics></math> to exist. In other words, for <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> <mo>,</mo> <msub> <mi>f</mi> <mn>1</mn> </msub> <mo>:</mo> <mi>X</mi> <mo>→</mo> <mi>Y</mi> </mrow> </semantics></math> to be homotopic maps, the induced homomorphisms <math display="inline"><semantics> <mrow> <msub> <mrow> <mfenced> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> </mrow> </mfenced> </mrow> <mo>*</mo> </msub> <mo>,</mo> <msub> <mrow> <mfenced> <mrow> <msub> <mi>f</mi> <mn>1</mn> </msub> </mrow> </mfenced> </mrow> <mo>*</mo> </msub> <mo>:</mo> <msub> <mi>H</mi> <mi>r</mi> </msub> <mfenced> <mi>X</mi> </mfenced> <mo>→</mo> <msub> <mi>H</mi> <mi>r</mi> </msub> <mfenced> <mi>Y</mi> </mfenced> </mrow> </semantics></math> for all <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>≥</mo> <mn>0</mn> </mrow> </semantics></math> between the homology groups for <math display="inline"><semantics> <mi>X</mi> </semantics></math> and <math display="inline"><semantics> <mi>Y</mi> </semantics></math> must be equal, i.e., <math display="inline"><semantics> <mrow> <msub> <mrow> <mfenced> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> </mrow> </mfenced> </mrow> <mo>*</mo> </msub> <mo>=</mo> <msub> <mrow> <mfenced> <mrow> <msub> <mi>f</mi> <mn>1</mn> </msub> </mrow> </mfenced> </mrow> <mo>*</mo> </msub> <mo>.</mo> </mrow> </semantics></math></p>
Full article ">Figure 2
<p>A diagram illustrating the fact that if <math display="inline"><semantics> <mrow> <mi>F</mi> <mo>,</mo> <mi>G</mi> <mo>:</mo> <mi>M</mi> <mo>→</mo> <mi>N</mi> </mrow> </semantics></math> are diffeomorphic maps between smooth manifolds <math display="inline"><semantics> <mi>M</mi> </semantics></math> and <math display="inline"><semantics> <mi>N</mi> </semantics></math>, then the pull-back maps <math display="inline"><semantics> <mrow> <msup> <mi>F</mi> <mo>*</mo> </msup> <mo>,</mo> <msup> <mi>G</mi> <mo>*</mo> </msup> <mo>:</mo> <msubsup> <mi>H</mi> <mrow> <mi>d</mi> <mi>R</mi> </mrow> <mi>r</mi> </msubsup> <mfenced> <mi>N</mi> </mfenced> <mo>→</mo> <msubsup> <mi>H</mi> <mrow> <mi>d</mi> <mi>R</mi> </mrow> <mi>r</mi> </msubsup> <mfenced> <mi>M</mi> </mfenced> </mrow> </semantics></math> between the de Rham cohomology groups <math display="inline"><semantics> <mrow> <msubsup> <mi>H</mi> <mrow> <mi>d</mi> <mi>R</mi> </mrow> <mi>r</mi> </msubsup> <mfenced> <mi>N</mi> </mfenced> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msubsup> <mi>H</mi> <mrow> <mi>d</mi> <mi>R</mi> </mrow> <mi>r</mi> </msubsup> <mfenced> <mi>M</mi> </mfenced> </mrow> </semantics></math> for all values of <math display="inline"><semantics> <mi>r</mi> </semantics></math> are equal, i.e., <math display="inline"><semantics> <mrow> <msup> <mi>F</mi> <mo>*</mo> </msup> <mo>=</mo> <msup> <mi>G</mi> <mo>*</mo> </msup> </mrow> </semantics></math>. In other words, if the maps <math display="inline"><semantics> <mi>F</mi> </semantics></math> and <math display="inline"><semantics> <mi>G</mi> </semantics></math> are diffeomorphic, they have the same homeomorphic topological structure and so they are homotopy-invariant. This means that homotopy-equivalent manifolds have isomorphic de Rham groups. The labels <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="sans-serif">Ω</mi> <mrow> <mi>r</mi> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mfenced> <mi>M</mi> </mfenced> <mo>,</mo> <msup> <mrow> <mrow> <mo> </mo> <mi mathvariant="sans-serif">Ω</mi> </mrow> </mrow> <mi>r</mi> </msup> <mfenced> <mi>M</mi> </mfenced> </mrow> </semantics></math> represent the skew-symmetric tensor spaces of degree <math display="inline"><semantics> <mrow> <mfenced> <mrow> <mi>r</mi> <mo>−</mo> <mn>1</mn> </mrow> </mfenced> </mrow> </semantics></math> and degree <math display="inline"><semantics> <mrow> <mfenced> <mi>r</mi> </mfenced> </mrow> </semantics></math> for differential forms at each point on the smooth manifold <math display="inline"><semantics> <mi>M</mi> </semantics></math>. The labels <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="sans-serif">Ω</mi> <mrow> <mi>r</mi> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mfenced> <mi>N</mi> </mfenced> <mo>,</mo> <msup> <mrow> <mrow> <mo> </mo> <mi mathvariant="sans-serif">Ω</mi> </mrow> </mrow> <mi>r</mi> </msup> <mfenced> <mi>N</mi> </mfenced> <mo>,</mo> <msup> <mrow> <mrow> <mo> </mo> <mi mathvariant="sans-serif">Ω</mi> </mrow> </mrow> <mrow> <mi>r</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> <mfenced> <mrow> <mo> </mo> <mi>N</mi> </mrow> </mfenced> </mrow> </semantics></math> represent the skew-symmetric tensor spaces of degree <math display="inline"><semantics> <mrow> <mfenced> <mrow> <mi>r</mi> <mo>−</mo> <mn>1</mn> </mrow> </mfenced> </mrow> </semantics></math>, degree <math display="inline"><semantics> <mrow> <mfenced> <mi>r</mi> </mfenced> </mrow> </semantics></math> and degree <math display="inline"><semantics> <mrow> <mfenced> <mrow> <mi>r</mi> <mo>+</mo> <mn>1</mn> </mrow> </mfenced> </mrow> </semantics></math> for differential forms at each point on the smooth manifold <math display="inline"><semantics> <mi>N</mi> </semantics></math>. The maps <math display="inline"><semantics> <mrow> <mi>h</mi> <mo>:</mo> <msup> <mrow> <mrow> <mo> </mo> <mi mathvariant="sans-serif">Ω</mi> </mrow> </mrow> <mrow> <mi>r</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> <mfenced> <mrow> <mo> </mo> <mi>N</mi> </mrow> </mfenced> <mo>→</mo> <msup> <mi mathvariant="sans-serif">Ω</mi> <mi>r</mi> </msup> <mfenced> <mi>M</mi> </mfenced> </mrow> </semantics></math> for all values of <math display="inline"><semantics> <mi>r</mi> </semantics></math> are called homotopy operators. Examination of the diagram shows that if the <math display="inline"><semantics> <mi>r</mi> </semantics></math>-form <math display="inline"><semantics> <mi>ω</mi> </semantics></math> is closed, i.e., <math display="inline"><semantics> <mrow> <mi>d</mi> <mi>ω</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>, then <math display="inline"><semantics> <mrow> <mi>d</mi> <mfenced> <mrow> <mi>h</mi> <mo> </mo> <mi>ω</mi> </mrow> </mfenced> <mo>=</mo> <msup> <mi>G</mi> <mo>*</mo> </msup> <mi>ω</mi> <mo>−</mo> <msup> <mi>F</mi> <mo>*</mo> </msup> <mi>ω</mi> </mrow> </semantics></math>. In other words, <math display="inline"><semantics> <mrow> <msup> <mi>G</mi> <mo>*</mo> </msup> <mi>ω</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msup> <mi>F</mi> <mo>*</mo> </msup> <mi>ω</mi> </mrow> </semantics></math> differ by an exact differential <math display="inline"><semantics> <mrow> <mi>d</mi> <mfenced> <mrow> <mi>h</mi> <mo> </mo> <mi>ω</mi> </mrow> </mfenced> </mrow> </semantics></math>. The maps <math display="inline"><semantics> <mrow> <msup> <mi>F</mi> <mo>*</mo> </msup> <mo>,</mo> <msup> <mi>G</mi> <mo>*</mo> </msup> <mo>:</mo> <msubsup> <mi>H</mi> <mrow> <mi>d</mi> <mi>R</mi> </mrow> <mi>r</mi> </msubsup> <mfenced> <mi>N</mi> </mfenced> <mo>→</mo> <msubsup> <mi>H</mi> <mrow> <mi>d</mi> <mi>R</mi> </mrow> <mi>r</mi> </msubsup> <mfenced> <mi>M</mi> </mfenced> </mrow> </semantics></math> are said to be cohomologous. This is exactly how equal cohomology groups are defined. Therefore, cohomologous groups have isomorphic de Rham cohomology groups.</p>
Full article ">
14 pages, 289 KiB  
Article
Abelian Extensions of Modified λ-Differential Left-Symmetric Algebras and Crossed Modules
by Fuyang Zhu, Taijie You and Wen Teng
Axioms 2024, 13(6), 380; https://doi.org/10.3390/axioms13060380 - 4 Jun 2024
Viewed by 664
Abstract
In this paper, we define a cohomology theory of a modified λ-differential left-symmetric algebra. Moreover, we introduce the notion of modified λ-differential left-symmetric 2-algebras, which is the categorization of a modified λ-differential left-symmetric algebra. As applications of cohomology, we classify [...] Read more.
In this paper, we define a cohomology theory of a modified λ-differential left-symmetric algebra. Moreover, we introduce the notion of modified λ-differential left-symmetric 2-algebras, which is the categorization of a modified λ-differential left-symmetric algebra. As applications of cohomology, we classify linear deformations and abelian extensions of modified λ-differential left-symmetric algebras using the second cohomology group and classify skeletal modified λ-differential left-symmetric 2-algebra using the third cohomology group. Finally, we show that strict modified λ-differential left-symmetric 2-algebras are equivalent to crossed modules of modified λ-differential left-symmetric algebras. Full article
(This article belongs to the Section Algebra and Number Theory)
9 pages, 253 KiB  
Article
The de Rham Cohomology Classes of Hemi-Slant Submanifolds in Locally Product Riemannian Manifolds
by Mustafa Gök and Erol Kılıç
Mathematics 2024, 12(11), 1730; https://doi.org/10.3390/math12111730 - 2 Jun 2024
Viewed by 469
Abstract
This paper aims to discuss the de Rham cohomology of hemi-slant submanifolds in locally product Riemannian manifolds. The integrability and geodesical invariance conditions of the distributions derived from the definition of a hemi-slant submanifold are given. The existence and non-triviality of de Rham [...] Read more.
This paper aims to discuss the de Rham cohomology of hemi-slant submanifolds in locally product Riemannian manifolds. The integrability and geodesical invariance conditions of the distributions derived from the definition of a hemi-slant submanifold are given. The existence and non-triviality of de Rham cohomology classes of hemi-slant submanifolds are investigated. Finally, an example is presented. Full article
(This article belongs to the Special Issue Differentiable Manifolds and Geometric Structures)
12 pages, 244 KiB  
Article
A Classification of Compact Cohomogeneity One Locally Conformal Kähler Manifolds
by Daniel Guan
Mathematics 2024, 12(11), 1710; https://doi.org/10.3390/math12111710 - 30 May 2024
Viewed by 746
Abstract
In this paper, we apply a result of the classification of a compact cohomogeneity one Riemannian manifold with a compact Lie group G to obtain a classification of compact cohomogeneity one locally conformal Kähler manifolds. In particular, we prove that the compact complex [...] Read more.
In this paper, we apply a result of the classification of a compact cohomogeneity one Riemannian manifold with a compact Lie group G to obtain a classification of compact cohomogeneity one locally conformal Kähler manifolds. In particular, we prove that the compact complex manifold is a complex one-dimensional torus bundle over a projective rational homogeneous, or cohomogeneity one manifold except of a class of manifolds with a generalized Hopf surface bundle over a projective rational homogeneous space. Additionally, it is a homogeneous compact complex manifold under the complexification GC of the given compact Lie group G under an extra condition that the related closed one form is cohomologous to zero on the generic G orbit. Moreover, the semi-simple part S of the Lie group action has hypersurface orbits, i.e., it is of cohomogeneity one with respect to the semi-simple Lie group S in that special case. Full article
15 pages, 347 KiB  
Article
In Pursuit of BRST Symmetry and Observables in 4D Topological Gauge-Affine Gravity
by Oussama Abdelghafour Belarbi and Ahmed Meziane
Symmetry 2024, 16(5), 528; https://doi.org/10.3390/sym16050528 - 28 Apr 2024
Viewed by 823
Abstract
The realization of a BRST cohomology of the 4D topological gauge-affine gravity is established in terms of a superconnection formalism. The identification of fields in the quantized theory occurs directly as is usual in terms of superconnection and its supercurvature components with the [...] Read more.
The realization of a BRST cohomology of the 4D topological gauge-affine gravity is established in terms of a superconnection formalism. The identification of fields in the quantized theory occurs directly as is usual in terms of superconnection and its supercurvature components with the double covering of the general affine group GA¯(4,R). Then, by means of an appropriate decomposition of the metalinear double-covering group SL¯(5,R) with respect to the general linear double-covering group GL¯(4,R), one can easily obtain the enlargements of the fields while remaining consistent with the BRST algebra. This leads to the descent equations, allowing us to build the observables of the theory by means of the BRST algebra constructed using a sa¯(5,R) algebra-valued superconnection. In particular, we discuss the construction of topological invariants with torsion. Full article
(This article belongs to the Special Issue Symmetries in Gravity Research: Classical and Quantum)
19 pages, 310 KiB  
Article
The Gauge Equation in Statistical Manifolds: An Approach through Spectral Sequences
by Michel Nguiffo Boyom and Stephane Puechmorel
Mathematics 2024, 12(8), 1177; https://doi.org/10.3390/math12081177 - 14 Apr 2024
Viewed by 1060
Abstract
The gauge equation is a generalization of the conjugacy relation for the Koszul connection to bundle morphisms that are not isomorphisms. The existence of nontrivial solution to this equation, especially when duality is imposed upon related connections, provides important information about the geometry [...] Read more.
The gauge equation is a generalization of the conjugacy relation for the Koszul connection to bundle morphisms that are not isomorphisms. The existence of nontrivial solution to this equation, especially when duality is imposed upon related connections, provides important information about the geometry of the manifolds under consideration. In this article, we use the gauge equation to introduce spectral sequences that are further specialized to Hessian structures. Full article
(This article belongs to the Special Issue Advances in Differential Geometry and Its Applications)
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17 pages, 282 KiB  
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Maps on the Mirror Heisenberg–Virasoro Algebra
by Xuelian Guo, Ivan Kaygorodov and Liming Tang
Mathematics 2024, 12(6), 802; https://doi.org/10.3390/math12060802 - 8 Mar 2024
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Abstract
Using the first cohomology from the mirror Heisenberg–Virasoro algebra to the twisted Heisenberg algebra (as the mirror Heisenberg–Virasoro algebra module), in this paper, we determined the derivations on the mirror Heisenberg–Virasoro algebra. Based on this result, we proved that any two-local derivation on [...] Read more.
Using the first cohomology from the mirror Heisenberg–Virasoro algebra to the twisted Heisenberg algebra (as the mirror Heisenberg–Virasoro algebra module), in this paper, we determined the derivations on the mirror Heisenberg–Virasoro algebra. Based on this result, we proved that any two-local derivation on the mirror Heisenberg–Virasoro algebra is a derivation. All half-derivations are described, and as corollaries, we have descriptions of transposed Poisson structures and local (two-local) half-derivations on the mirror Heisenberg–Virasoro algebra. Full article
(This article belongs to the Section Algebra, Geometry and Topology)
16 pages, 303 KiB  
Article
Generalized Reynolds Operators on Hom-Lie Triple Systems
by Yunpeng Xiao, Wen Teng and Fengshan Long
Symmetry 2024, 16(3), 262; https://doi.org/10.3390/sym16030262 - 21 Feb 2024
Viewed by 1467
Abstract
In this paper, we first introduce the notion of generalized Reynolds operators on Hom-Lie triple systems associated to a representation and a 3-cocycle. Then, we develop a cohomology of generalized Reynolds operators on Hom-Lie triple systems. As applications, we use the first cohomology [...] Read more.
In this paper, we first introduce the notion of generalized Reynolds operators on Hom-Lie triple systems associated to a representation and a 3-cocycle. Then, we develop a cohomology of generalized Reynolds operators on Hom-Lie triple systems. As applications, we use the first cohomology group to classify linear deformations and we study the obstruction class of an extendable order n deformation. Finally, we introduce and investigate Hom-NS-Lie triple system as the underlying structure of generalized Reynolds operators on Hom-Lie triple systems. Full article
(This article belongs to the Section Mathematics)
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