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25 pages, 506 KiB  
Article
Discrete Pseudo-Quasi Overlap Functions and Their Applications in Fuzzy Multi-Attribute Group Decision-Making
by Mei Jing, Jingqian Wang, Mei Wang and Xiaohong Zhang
Mathematics 2024, 12(22), 3569; https://doi.org/10.3390/math12223569 - 15 Nov 2024
Viewed by 302
Abstract
The overlap function, a continuous aggregation function, is widely used in classification, decision-making, image processing, etc. Compared to applications, overlap functions have also achieved fruitful results in theory, such as studies on the fundamental properties of overlap functions, various generalizations of the concept, [...] Read more.
The overlap function, a continuous aggregation function, is widely used in classification, decision-making, image processing, etc. Compared to applications, overlap functions have also achieved fruitful results in theory, such as studies on the fundamental properties of overlap functions, various generalizations of the concept, and the construction of additive and multiplicative generators based on overlap functions. However, most of the research studies on the overlap functions mentioned above assume commutativity and continuity, which can limit their practical applications. In this paper, we remove the symmetry and continuity from overlap functions and define discrete pseudo-quasi-overlap functions on finite chains. Meanwhile, we also discuss their related properties. Then, we introduce pseudo-quasi-overlap functions on sub-chains and construct discrete pseudo-quasi-overlap functions on finite chains using these sub-chain functions. Unlike quasi-overlap functions on finite chains generated by the ordinal sum, discrete pseudo-quasi-overlap functions on finite chains constructed through pseudo-quasi-overlap functions on different sub-chains are dissimilar. Eventually, we remove the continuity from pseudo-automorphisms and propose the concept of pseudo-quasi-automorphisms. Based on this, we utilize pseudo-overlap functions, pseudo-quasi-automorphisms, and integral functions to obtain discrete pseudo-quasi-overlap functions on finite chains; moreover, we apply them to fuzzy multi-attribute group decision-making. The results indicate that—compared to overlap functions and pseudo-overlap functions—discrete pseudo-quasi-overlap functions on finite chains have stronger flexibility and a wider range of practical applications. Full article
(This article belongs to the Special Issue Fuzzy Sets and Fuzzy Systems)
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<p>Framework diagram of the paper.</p>
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<p>A discrete pseudo-quasi-overlap function <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>Q</mi> <msub> <mi>O</mi> <mi mathvariant="script">L</mi> </msub> </mrow> </semantics></math>.</p>
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<p>A discrete pseudo-quasi-overlap function <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>Q</mi> <msub> <mi>O</mi> <mi>L</mi> </msub> </mrow> </semantics></math>.</p>
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<p>A discrete pseudo-quasi-overlap function <math display="inline"><semantics> <msub> <mrow> <mi>P</mi> <mi>Q</mi> <mi>O</mi> </mrow> <msub> <mi>L</mi> <mi>N</mi> </msub> </msub> </semantics></math>.</p>
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<p>A discrete pseudo-quasi-overlap function <math display="inline"><semantics> <msub> <mrow> <mi>P</mi> <mi>Q</mi> <mi>O</mi> </mrow> <msub> <mi>L</mi> <msup> <mi>N</mi> <mo>+</mo> </msup> </msub> </msub> </semantics></math>.</p>
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20 pages, 492 KiB  
Article
Spin(8,C)-Higgs Bundles and the Hitchin Integrable System
by Álvaro Antón-Sancho
Mathematics 2024, 12(21), 3436; https://doi.org/10.3390/math12213436 - 3 Nov 2024
Viewed by 370
Abstract
Let M(Spin(8,C)) be the moduli space of Spin(8,C)-Higgs bundles over a compact Riemann surface X of genus g2. This admits a system called the Hitchin integrable [...] Read more.
Let M(Spin(8,C)) be the moduli space of Spin(8,C)-Higgs bundles over a compact Riemann surface X of genus g2. This admits a system called the Hitchin integrable system, induced by the Hitchin map, the fibers of which are Prym varieties. Moreover, the triality automorphism of Spin(8,C) acts on M(Spin(8,C)), and those Higgs bundles that admit a reduction in the structure group to G2 are fixed points of this action. This defines a map of moduli spaces of Higgs bundles M(G2)M(Spin(8,C)). In this work, the action of triality automorphism is extended to an action on the Hitchin integrable system associated with M(Spin(8,C)). In particular, it is checked that the map M(G2)M(Spin(8,C)) is restricted to a map at the level of the Prym varieties induced by the Hitchin map. Necessary and sufficient conditions are also provided for the Prym varieties associated with the moduli spaces of G2 and Spin(8,C)-Higgs bundles to be disconnected. Finally, some consequences are drawn from the above results in relation to the geometry of the Prym varieties involved. Full article
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<p>Dynkin diagram of the simple Lie group <math display="inline"><semantics> <mrow> <mo>Spin</mo> <mo>(</mo> <mn>8</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo>)</mo> </mrow> </semantics></math>, where the nodes of the diagram correspond to the vectorial representation <math display="inline"><semantics> <msub> <mi>V</mi> <mn>8</mn> </msub> </semantics></math> and the spinor representations <math display="inline"><semantics> <msub> <mi>S</mi> <mo>+</mo> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>S</mi> <mo>−</mo> </msub> </semantics></math> of <math display="inline"><semantics> <mrow> <mo>Spin</mo> <mo>(</mo> <mn>8</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo>)</mo> </mrow> </semantics></math>, corresponding to the two types of spinors in dimension 8, known as Weyl spinors (which are 8-dimensional and interchanged by the action of the triality automorphism) and the adjoint representation Ad (which is 28-dimensional and fixed by the action of triality) [<a href="#B30-mathematics-12-03436" class="html-bibr">30</a>]. The figure is original and was made using Microsoft Word<sup>®</sup> v. 2409.</p>
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<p>Action of triality on a fiber of the Hitchin map of <math display="inline"><semantics> <mrow> <mi mathvariant="script">M</mi> <mo>(</mo> <mo>Spin</mo> <mo>(</mo> <mn>8</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo>)</mo> <mo>)</mo> </mrow> </semantics></math>. In blue is an orbit corresponding to the irreducible vectorial representation of <math display="inline"><semantics> <mrow> <mo>Spin</mo> <mo>(</mo> <mn>8</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo>)</mo> </mrow> </semantics></math>, and in red and green are orbits corresponding to the two spinor representations. These three orbits are interchanged by the action of triality. The figure is original and was made using Microsoft Word<sup>®</sup> v. 2409.</p>
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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
18 pages, 2622 KiB  
Review
Automorphism Groups in Polyhedral Graphs
by Modjtaba Ghorbani, Razie Alidehi-Ravandi and Matthias Dehmer
Symmetry 2024, 16(9), 1157; https://doi.org/10.3390/sym16091157 - 5 Sep 2024
Viewed by 523
Abstract
The study delves into the relationship between symmetry groups and automorphism groups in polyhedral graphs, emphasizing their interconnected nature and their significance in understanding the symmetries and structural properties of fullerenes. It highlights the visual importance of symmetry and its applications in architecture, [...] Read more.
The study delves into the relationship between symmetry groups and automorphism groups in polyhedral graphs, emphasizing their interconnected nature and their significance in understanding the symmetries and structural properties of fullerenes. It highlights the visual importance of symmetry and its applications in architecture, as well as the mathematical structure of the automorphism group, which captures all of the symmetries of a graph. The paper also discusses the significance of groups in Abstract Algebra and their relevance to understanding the behavior of mathematical systems. Overall, the findings offer an inclusive understanding of the relationship between symmetry groups and automorphism groups, paving the way for further research in this area. Full article
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<p>All elements of Aut(<span class="html-italic">C</span><sub>3</sub>).</p>
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<p>The smallest asymmetric graph which is not a tree.</p>
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<p>Three different labelings of path <span class="html-italic">P</span><sub>3</sub>.</p>
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<p>Two connected graphs of order 3.</p>
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<p>Graph <span class="html-italic">G</span>.</p>
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<p><span class="html-italic">K</span><sub>8</sub> with one edge removed.</p>
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<p>Some polyhedral graphs.</p>
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<p>Some polyhedral graphs.</p>
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<p>A labeling of the vertices of fullerene <span class="html-italic">F</span><sub>96</sub>.</p>
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<p>Labeling of the vertices of polyhedral graph <span class="html-italic">F</span><sub>48</sub>.</p>
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14 pages, 485 KiB  
Article
Group Theoretic Approach towards the Balaban Index of Catacondensed Benzenoid Systems and Linear Chain of Anthracene
by Muhammad Yaseen, Badr S. Alkahtani, Hong Min and Mohd Anjum
Symmetry 2024, 16(8), 996; https://doi.org/10.3390/sym16080996 - 6 Aug 2024
Viewed by 1133
Abstract
In this work, we present the analytical closed forms of the Balaban index for anthracene and catacondensed benzenoid systems using group theoretic techniques. The Balaban index is a distance-based topological index that provides valuable information about the properties of chemical structures. We emphasize [...] Read more.
In this work, we present the analytical closed forms of the Balaban index for anthracene and catacondensed benzenoid systems using group theoretic techniques. The Balaban index is a distance-based topological index that provides valuable information about the properties of chemical structures. We emphasize the importance of determining analytical closed forms of the Balaban index for catacondensed benzenoid systems and linear chains of anthracene, as it enables a deeper understanding of these systems and their behavior. Our analysis utilizes the group action of the automorphism group of these chains on the set of vertices, which refer to the points where the chains intersect. In future work, we plan to determine the Balaban index of other polymeric linear chains using group theoretic techniques and extend the applications of this index to other fields, such as materials science and biology. It is clear that the Balaban index remains a valuable tool in theoretical and computational chemistry, and its applications are constantly evolving. Full article
(This article belongs to the Section Mathematics)
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<p><math display="inline"><semantics> <msub> <mi>A</mi> <mn>3</mn> </msub> </semantics></math> with 48 vertices and 52 edges.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mn>0</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>A</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., identity automorphism.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>A</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., where axis of symmetry is horizontal.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>A</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., where symmetry axis is vertical.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">Φ</mi> <mn>4</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>A</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., composition of above automorphisms <math display="inline"><semantics> <msub> <mi mathvariant="normal">Φ</mi> <mn>2</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi mathvariant="normal">Φ</mi> <mn>1</mn> </msub> </semantics></math>.</p>
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<p>Structural graph of Linear chain of anthracene.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ψ</mi> <mn>0</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., identity automorphism, possessing 30 vertices and 34 edges.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ψ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., symmetry axis is horizontal.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ψ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., axis of symmetry is slightly tilt.</p>
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<p><math display="inline"><semantics> <mrow> <mspace width="3.33333pt"/> <msub> <mi>ψ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., symmetry axis is slightly tilt.</p>
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<p><math display="inline"><semantics> <mrow> <mspace width="3.33333pt"/> <msub> <mi>ψ</mi> <mn>4</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., composition of automorphisms <math display="inline"><semantics> <msub> <mi>ψ</mi> <mn>2</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>ψ</mi> <mn>1</mn> </msub> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>ψ</mi> <mn>5</mn> </msub> <mrow> <mo>(</mo> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> i.e., composition of automorphisms <math display="inline"><semantics> <msub> <mi>ψ</mi> <mn>3</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>ψ</mi> <mn>1</mn> </msub> </semantics></math>.</p>
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<p>Structural graph of CB system.</p>
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13 pages, 297 KiB  
Article
On Centralizers of Idempotents with Restricted Range
by Dilawar J. Mir and Amal S. Alali
Symmetry 2024, 16(6), 769; https://doi.org/10.3390/sym16060769 - 19 Jun 2024
Viewed by 867
Abstract
This study delves into the structure and properties of left inverse zero divisor bands within semigroups, identifying their maximal forms and broadening the theoretical landscape of semigroup analysis. A significant focus is placed on the automorphisms of a semigroup S of centralizers of [...] Read more.
This study delves into the structure and properties of left inverse zero divisor bands within semigroups, identifying their maximal forms and broadening the theoretical landscape of semigroup analysis. A significant focus is placed on the automorphisms of a semigroup S of centralizers of idempotent transformations with restricted range, revealing that these automorphisms are inner ones and induced by the units of S. Additionally, we establish that the automorphism group Aut(S) is isomorphic to US, the group of units of S. These findings extend previous results on semigroups of transformations, enhancing their applicability and providing a more unified theory. The practical implications of this work span multiple fields, including automata theory, coding theory, cryptography, and graph theory, offering tools for more efficient algorithms and models. By simplifying complex concepts and providing a solid foundation for future research, this study makes significant contributions to both theoretical and applied mathematics. Full article
(This article belongs to the Special Issue Algebraic Systems, Models and Applications)
15 pages, 294 KiB  
Article
The Hopf Automorphism Group of Two Classes of Drinfeld Doubles
by Hua Sun, Mi Hu and Jiawei Hu
Symmetry 2024, 16(6), 735; https://doi.org/10.3390/sym16060735 - 12 Jun 2024
Viewed by 632
Abstract
Let D(Rm,n(q)) be the Drinfeld double of Radford Hopf algebra Rm,n(q) and D(Hs,t) be the Drinfeld double of generalized Taft algebra [...] Read more.
Let D(Rm,n(q)) be the Drinfeld double of Radford Hopf algebra Rm,n(q) and D(Hs,t) be the Drinfeld double of generalized Taft algebra Hs,t. Both D(Rm,n(q)) and D(Hs,t) have very symmetric structures. We calculate all Hopf automorphisms of D(Rm,n(q)) and D(Hs,t), respectively. Furthermore, we prove that the Hopf automorphism group AutHopf(D(Rm,n(q))) is isomorphic to the direct sum ZnZm of cyclic groups Zm and Zn, the Hopf automorphism group AutHopf(D(Hs,t)) is isomorphic to the semi-direct products k*Zd of multiplicative group k* and cyclic group Zd, where s=td,k*=k\{0}, and k is an algebraically closed field with char (k)t. Full article
(This article belongs to the Section Mathematics)
8 pages, 280 KiB  
Article
The Three Faces of U(3)
by John LaChapelle
Symmetry 2024, 16(4), 504; https://doi.org/10.3390/sym16040504 - 22 Apr 2024
Viewed by 1330
Abstract
U(n) is a semi-direct product group characterized by nontrivial homomorphisms mapping U(1) into the automorphism group of SU(n). For U(3), there are three nontrivial homomorphisms that induce three [...] Read more.
U(n) is a semi-direct product group characterized by nontrivial homomorphisms mapping U(1) into the automorphism group of SU(n). For U(3), there are three nontrivial homomorphisms that induce three separate defining representations. In a toy model of U(3) Yang–Mills (endowed with a suitable inner product) coupled to massive fermions, this renders three distinct covariant derivatives acting on a single matter field. Employing a mod3 permutation induced by a large gauge transformation acting on the defining representation vector space, the three covariant derivatives and one matter field can alternatively be expressed as a single covariant derivative acting on three distinct species of matter fields possessing the same U(3) quantum numbers. One can interpret this as three species of matter fields in the defining representation. Full article
(This article belongs to the Section Physics)
15 pages, 267 KiB  
Article
Hyperstability for a Generalized Class of Pexiderized Functional Equations on Monoids via Páles’ Approach
by Rashad M. Asharabi and Muaadh Almahalebi
Mathematics 2024, 12(6), 838; https://doi.org/10.3390/math12060838 - 13 Mar 2024
Viewed by 770
Abstract
In this paper, we deduce some hyperstability results for a generalized class of homogeneous Pexiderized functional equations, expressed as ρΓfxρ.y=f(x)+g(y), [...] Read more.
In this paper, we deduce some hyperstability results for a generalized class of homogeneous Pexiderized functional equations, expressed as ρΓfxρ.y=f(x)+g(y), x,yM, which is inspired by the concept of Ulam stability. Indeed, we prove that function f that approximately satisfies an equation can, under certain conditions, be considered an exact solution. Domain M is a monoid (semigroup with a neutral element), Γ is a finite subgroup of the automorphisms group of M, is the cardinality of Γ, and f,g:MG such that (G,+) denotes an -cancellative commutative group. We also examine the hyperstability of the given equation in its inhomogeneous version ρΓfxρ.y=f(x)+g(y)+ψ(x,y),x,yM, where ψ:M×MG. Additionally, we apply the main results to elucidate the hyperstability of various functional equations with involutions. Full article
10 pages, 340 KiB  
Article
Classifying Seven-Valent Symmetric Graphs of Order 8pq
by Yingbi Jiang, Bo Ling, Jinlong Yang and Yun Zhao
Mathematics 2024, 12(6), 787; https://doi.org/10.3390/math12060787 - 7 Mar 2024
Viewed by 832
Abstract
A graph is symmetric if its automorphism group is transitive on the arcs of the graph. Guo et al. determined all of the connected seven-valent symmetric graphs of order 8p for each prime p. We shall generalize this result by determining [...] Read more.
A graph is symmetric if its automorphism group is transitive on the arcs of the graph. Guo et al. determined all of the connected seven-valent symmetric graphs of order 8p for each prime p. We shall generalize this result by determining all of the connected seven-valent symmetric graphs of order 8pq with p and q to be distinct primes. As a result, we show that for each such graph of Γ, it is isomorphic to one of seven graphs. Full article
(This article belongs to the Special Issue Algebraic Structures and Graph Theory, 2nd Edition)
10 pages, 216 KiB  
Article
Frobenius Modules Associated to Algebra Automorphisms
by Ji-Wei He and Chenglong Rong
Mathematics 2024, 12(4), 531; https://doi.org/10.3390/math12040531 - 8 Feb 2024
Viewed by 762
Abstract
Here, we study Frobenius bimodules associated with a pair of automorphisms of an algebra and discuss their basic properties. In particular, some equivalent conditions for a finite-dimensional bimodule are proved to be Frobenius and some isomorphisms between Ext-groups and Tor-groups of Frobenius modules [...] Read more.
Here, we study Frobenius bimodules associated with a pair of automorphisms of an algebra and discuss their basic properties. In particular, some equivalent conditions for a finite-dimensional bimodule are proved to be Frobenius and some isomorphisms between Ext-groups and Tor-groups of Frobenius modules over finite dimensional algebras are established. Full article
13 pages, 1588 KiB  
Article
Dynamics of Fricke–Painlevé VI Surfaces
by Michel Planat, David Chester and Klee Irwin
Dynamics 2024, 4(1), 1-13; https://doi.org/10.3390/dynamics4010001 - 2 Jan 2024
Cited by 1 | Viewed by 1509
Abstract
The symmetries of a Riemann surface Σ{ai} with n punctures ai are encoded in its fundamental group π1(Σ). Further structure may be described through representations (homomorphisms) of π1 over a Lie [...] Read more.
The symmetries of a Riemann surface Σ{ai} with n punctures ai are encoded in its fundamental group π1(Σ). Further structure may be described through representations (homomorphisms) of π1 over a Lie group G as globalized by the character variety C=Hom(π1,G)/G. Guided by our previous work in the context of topological quantum computing (TQC) and genetics, we specialize on the four-punctured Riemann sphere Σ=S2(4) and the ‘space-time-spin’ group G=SL2(C). In such a situation, C possesses remarkable properties: (i) a representation is described by a three-dimensional cubic surface Va,b,c,d(x,y,z) with three variables and four parameters; (ii) the automorphisms of the surface satisfy the dynamical (non-linear and transcendental) Painlevé VI equation (or PVI); and (iii) there exists a finite set of 1 (Cayley–Picard)+3 (continuous platonic)+45 (icosahedral) solutions of PVI. In this paper, we feature the parametric representation of some solutions of PVI: (a) solutions corresponding to algebraic surfaces such as the Klein quartic and (b) icosahedral solutions. Applications to the character variety of finitely generated groups fp encountered in TQC or DNA/RNA sequences are proposed. Full article
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<p>(<b>Left</b>): Parametric plot for the modulus of Klein solution of <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mi>V</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (solution 8 of ([<a href="#B18-dynamics-04-00001" class="html-bibr">18</a>], p. 157)); the discontinuities of the plot correspond to the four poles. (<b>Right</b>): the corresponding cubic surface <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> <mi>z</mi> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>−</mo> <mi>x</mi> <mo>−</mo> <mi>y</mi> <mo>−</mo> <mi>z</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>.</p>
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<p>Solutions related to the algebraic surface <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> <mi>z</mi> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>−</mo> <mi>x</mi> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math> are indexed in [<a href="#B18-dynamics-04-00001" class="html-bibr">18</a>]. (<b>Upper left</b>): the tetrahedral solution 3. (<b>Upper right</b>): solution 21. (<b>Middle</b>): modulus of solution 42. (<b>Lower</b>): the corresponding algebraic surface. It is a degree 3 del Pezzo surface of the <math display="inline"><semantics> <msub> <mi>A</mi> <mn>1</mn> </msub> </semantics></math> type.</p>
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<p>Solutions related to the algebraic surface <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> <mi>z</mi> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>−</mo> <mn>3</mn> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> are indexed in [<a href="#B18-dynamics-04-00001" class="html-bibr">18</a>]. (<b>Upper left</b>): the modulus of the octahedral solution 20. (<b>Upper right</b>): the modulus of solution 45. (<b>Lower</b>): the corresponding algebraic surface.</p>
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<p>(<b>Left</b>): Parametric plot for the modulus of the great dodecahedron solution of <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mi>V</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (solution 31 of ([<a href="#B18-dynamics-04-00001" class="html-bibr">18</a>], p. 157)); the three poles are identified. (<b>Right</b>): the corresponding cubic surface is a degree 3 del Pezzo surface of type <math display="inline"><semantics> <mrow> <mn>3</mn> <msub> <mi>A</mi> <mn>1</mn> </msub> </mrow> </semantics></math> that is with three isolated singularities).</p>
Full article ">Figure 5
<p>Parametric plots for the modulus of solutions 1 (with 5 branches: Fricke–Painlevé form <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> <mi>z</mi> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>−</mo> <mi>y</mi> <mo>−</mo> <mi>z</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>), 30 (an octahedral solution with 16 branches: Fricke–Painlevé form <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> <mi>z</mi> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>−</mo> <mn>2</mn> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>) and 39 (a Valentiner solution with 24 branches: Fricke–Painlevé form <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> <mi>z</mi> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>−</mo> <mi>x</mi> <mo>−</mo> <mi>y</mi> <mo>−</mo> <mi>z</mi> <mo>−</mo> <mn>1</mn> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>.)</p>
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<p>(<b>Left</b>): Parametric plot of an icosahedral solution of <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mi>V</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (solution 7 of ([<a href="#B18-dynamics-04-00001" class="html-bibr">18</a>], p. 157)); the discontinuities of the plot correspond to the poles. (<b>Right</b>): the corresponding cubic surface.</p>
Full article ">Figure 7
<p>Parametric plots for the modulus of solutions III (the tetrahedral solution), IV (the dihedral solution), solutions 16 and 17 (icosahedral solutions) as first described in [<a href="#B26-dynamics-04-00001" class="html-bibr">26</a>]. For the later two solutions, we find poles located at irrational values <math display="inline"><semantics> <mrow> <mi>s</mi> <mo>=</mo> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>/</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>2</mn> <mo>±</mo> <msqrt> <mn>5</mn> </msqrt> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>±</mo> <mn>1</mn> <mo>/</mo> <msqrt> <mn>3</mn> </msqrt> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>Parametric plots for the modulus of solutions 26 and 27 that are related to the Valentiner group.</p>
Full article ">Figure 9
<p>Parametric plots for the modulus of solutions 33 and 34.</p>
Full article ">
53 pages, 649 KiB  
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Viewed by 1158
Abstract
Let (kμ)μ=14 be a quartet of cyclic cubic number fields sharing a common conductor c=pqr divisible by exactly three prime(power)s, p,q,r. For those components of the quartet [...] Read more.
Let (kμ)μ=14 be a quartet of cyclic cubic number fields sharing a common conductor c=pqr divisible by exactly three prime(power)s, p,q,r. For those components of the quartet whose 3-class group Cl3(kμ)(Z/3Z)2 is elementary bicyclic, the automorphism group M=Gal(F32(kμ)/kμ) of the maximal metabelian unramified 3-extension of kμ is determined by conditions for cubic residue symbols between p,q,r and for ambiguous principal ideals in subfields of the common absolute 3-genus field k* of all kμ. With the aid of the relation rank d2(M), it is decided whether M coincides with the Galois group G=Gal(F3(kμ)/kμ) of the maximal unramified pro-3-extension of kμ. Full article
(This article belongs to the Section Algebra, Geometry and Topology)
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Viewed by 884
Abstract
This paper contributes to the classification of flag-transitive symmetric 2-(v,k,λ) designs with λ prime. We investigate the structure of flag-transitive, point-quasiprimitive automorphism groups (G) of such 2-designs by applying the classification of quasiprimitive permutation [...] Read more.
This paper contributes to the classification of flag-transitive symmetric 2-(v,k,λ) designs with λ prime. We investigate the structure of flag-transitive, point-quasiprimitive automorphism groups (G) of such 2-designs by applying the classification of quasiprimitive permutation groups. It is shown that the automorphism groups (G) have either an abelian socle or a non-abelian simple socle. Moreover, according to the classification of finite simple groups, we demonstrate that point-quasiprimitivity implies point-primitivity of G, except when the socle of G is PSLn(q). Full article
(This article belongs to the Special Issue Algebra and Discrete Mathematics 2023)
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Abstract
Consider G to be a finite group and p to be a prime divisor of the order |G| in the group G. The main aim of this paper is to prove that the outcome in a recent paper of A. [...] Read more.
Consider G to be a finite group and p to be a prime divisor of the order |G| in the group G. The main aim of this paper is to prove that the outcome in a recent paper of A. Laradji is true in the case of a p-constrained group. We observe that the generalization of the concept of Navarro’s vertex for an irreducible character in a p-constrained group G is generally undefined. We illustrate this with a suitable example. Let ϕIrr(G) have a positive height, and let there be an anchor group Aϕ. We prove that if the normalizer NG(Aϕ) is p-constrained, then Op´(NG(Aϕ)){1G}, where Op´(NG(Aϕ)) is the maximal normal p´ subgroup of NG(Aϕ). We use character theoretic methods. In particular, Clifford theory is the main tool used to accomplish the results. Full article
(This article belongs to the Section Mathematics)
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