On Finite-Dimensional Hopf Algebras and Their Classifications Michael John Hilgemann Iowa State University
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Hopf Rings in Algebraic Topology
HOPF RINGS IN ALGEBRAIC TOPOLOGY W. STEPHEN WILSON Abstract. These are colloquium style lecture notes about Hopf rings in al- gebraic topology. They were designed for use by non-topologists and graduate students but have been found helpful for those who want to start learning about Hopf rings. They are not “up to date,” nor are then intended to be, but instead they are intended to be introductory in nature. Although these are “old” notes, Hopf rings are thriving and these notes give a relatively painless introduction which should prepare the reader to approach the current litera- ture. This is a brief survey about Hopf rings: what they are, how they arise, examples, and how to compute them. There are very few proofs. The bulk of the technical details can be found in either [RW77] or [Wil82], but a “soft” introduction to the material is difficult to find. Historically, Hopf algebras go back to the early days of our subject matter, homotopy theory and algebraic topology. They arise naturally from the homology of spaces with multiplications on them, i.e. H-spaces, or “Hopf” spaces. In our language, this homology is a group object in the category of coalgebras. Hopf algebras have become objects of study in their own right, e.g. [MM65] and [Swe69]. They were also able to give great insight into complicated structures such as with Milnor’s work on the Steenrod algebra [Mil58]. However, when spaces have more structure than just a multiplication, their homology produces even richer algebraic stuctures. In particular, with the development of generalized cohomology theories, we have seen that the spaces which classify them have a structure mimicking that of a graded ring. -
Algebra & Number Theory
Algebra & Number Theory Volume 7 2013 No. 7 Hopf monoids from class functions on unitriangular matrices Marcelo Aguiar, Nantel Bergeron and Nathaniel Thiem msp ALGEBRA AND NUMBER THEORY 7:7 (2013) msp dx.doi.org/10.2140/ant.2013.7.1743 Hopf monoids from class functions on unitriangular matrices Marcelo Aguiar, Nantel Bergeron and Nathaniel Thiem We build, from the collection of all groups of unitriangular matrices, Hopf monoids in Joyal’s category of species. Such structure is carried by the collection of class function spaces on those groups and also by the collection of superclass function spaces in the sense of Diaconis and Isaacs. Superclasses of unitriangular matrices admit a simple description from which we deduce a combinatorial model for the Hopf monoid of superclass functions in terms of the Hadamard product of the Hopf monoids of linear orders and of set partitions. This implies a recent result relating the Hopf algebra of superclass functions on unitriangular matrices to symmetric functions in noncommuting variables. We determine the algebraic structure of the Hopf monoid: it is a free monoid in species with the canonical Hopf structure. As an application, we derive certain estimates on the number of conjugacy classes of unitriangular matrices. Introduction A Hopf monoid (in Joyal’s category of species) is an algebraic structure akin to that of a Hopf algebra. Combinatorial structures that compose and decompose give rise to Hopf monoids. These objects are the subject of[Aguiar and Mahajan 2010, Part II]. The few basic notions and examples needed for our purposes are reviewed in Section 1, including the Hopf monoids of linear orders, set partitions, and simple graphs and the Hadamard product of Hopf monoids. -
Arxiv:1906.03655V2 [Math.AT] 1 Jul 2020
RATIONAL HOMOTOPY EQUIVALENCES AND SINGULAR CHAINS MANUEL RIVERA, FELIX WIERSTRA, MAHMOUD ZEINALIAN Abstract. Bousfield and Kan’s Q-completion and fiberwise Q-completion of spaces lead to two different approaches to the rational homotopy theory of non-simply connected spaces. In the first approach, a map is a weak equivalence if it induces an isomorphism on rational homology. In the second, a map of path-connected pointed spaces is a weak equivalence if it induces an isomorphism between fun- damental groups and higher rationalized homotopy groups; we call these maps π1-rational homotopy equivalences. In this paper, we compare these two notions and show that π1-rational homotopy equivalences correspond to maps that induce Ω-quasi-isomorphisms on the rational singular chains, i.e. maps that induce a quasi-isomorphism after applying the cobar functor to the dg coassociative coalge- bra of rational singular chains. This implies that both notions of rational homotopy equivalence can be deduced from the rational singular chains by using different alge- braic notions of weak equivalences: quasi-isomorphism and Ω-quasi-isomorphisms. We further show that, in the second approach, there are no dg coalgebra models of the chains that are both strictly cocommutative and coassociative. 1. Introduction One of the questions that gave birth to rational homotopy theory is the commuta- tive cochains problem which, given a commutative ring k, asks whether there exists a commutative differential graded (dg) associative k-algebra functorially associated to any topological space that is weakly equivalent to the dg associative algebra of singu- lar k-cochains on the space with the cup product [S77], [Q69]. -
Map Composition Generalized to Coherent Collections of Maps
Front. Math. China 2015, 10(3): 547–565 DOI 10.1007/s11464-015-0435-5 Map composition generalized to coherent collections of maps Herng Yi CHENG1, Kang Hao CHEONG1,2 1 National University of Singapore High School of Mathematics and Science, Singapore 129957, Singapore 2 Tanglin Secondary School, Singapore 127391, Singapore c Higher Education Press and Springer-Verlag Berlin Heidelberg 2015 Abstract Relation algebras give rise to partial algebras on maps, which are generalized to partial algebras on polymaps while preserving the properties of relation union and composition. A polymap is defined as a map with every point in the domain associated with a special set of maps. Polymaps can be represented as small subcategories of Set∗, the category of pointed sets. Map composition and the counterpart of relation union for maps are generalized to polymap composition and sum. Algebraic structures and categories of polymaps are investigated. Polymaps present the unique perspective of an algebra that can retain many of its properties when its elements (maps) are augmented with collections of other elements. Keywords Relation algebra, partial algebra, composition MSC 08A02 1 Introduction This paper considers partial algebras on maps (similar to those defined in [15]), constructed in analogy to relation algebras [5,12,16]. The sum of two maps f0 : X0 → Y0 and f1 : X1 → Y1 is defined if the union of their graphs is a functional binary relation R ⊆ (X0 ∪ X1) × (Y0 ∪ Y1), in which case the sum is the map (f0 + f1): X0 ∪ X1 → Y0 ∪ Y1 with graph R. This is defined similarly to the union operation + from [10]. -
LOW-DIMENSIONAL UNITARY REPRESENTATIONS of B3 1. Introduction Unitary Braid Representations Have Been Constructed in Several
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 129, Number 9, Pages 2597{2606 S 0002-9939(01)05903-2 Article electronically published on March 15, 2001 LOW-DIMENSIONAL UNITARY REPRESENTATIONS OF B3 IMRE TUBA (Communicated by Stephen D. Smith) Abstract. We characterize all simple unitarizable representations of the braid group B3 on complex vector spaces of dimension d ≤ 5. In particular, we prove that if σ1 and σ2 denote the two generating twists of B3,thenasimple representation ρ : B3 ! GL(V )(fordimV ≤ 5) is unitarizable if and only if the eigenvalues λ1,λ2;::: ;λd of ρ(σ1) are distinct, satisfy jλij =1and (d) ≤ ≤ (d) µ1i > 0for2 i d,wheretheµ1i are functions of the eigenvalues, explicitly described in this paper. 1. Introduction Unitary braid representations have been constructed in several ways using the representation theory of Kac-Moody algebras and quantum groups (see e.g. [1], [2], and [4]), and specializations of the reduced Burau and Gassner representations in [5]. Such representations easily lead to representations of PSL(2; Z)=B3=Z ,where Z is the center of B3,andPSL(2; Z)=SL(2; Z)={1g,where{1g is the center of SL(2; Z). We give a complete classification of simple unitary representations of B3 of dimension d ≤ 5 in this paper. In particular, the unitarizability of a braid rep- resentation depends only on the the eigenvalues λ1,λ2;::: ,λd of the images of the two generating twists of B3. The condition for unitarizability is a set of linear in- equalities in the logarithms of these eigenvalues. In other words, the representation is unitarizable if and only if the (arg λ1; arg λ2;::: ;arg λd) is a point inside a poly- hedron in (R=2π)d, where we give the equations of the hyperplanes that bound this polyhedron. -
Rational Homotopy Theory: a Brief Introduction
Contemporary Mathematics Rational Homotopy Theory: A Brief Introduction Kathryn Hess Abstract. These notes contain a brief introduction to rational homotopy theory: its model category foundations, the Sullivan model and interactions with the theory of local commutative rings. Introduction This overview of rational homotopy theory consists of an extended version of lecture notes from a minicourse based primarily on the encyclopedic text [18] of F´elix, Halperin and Thomas. With only three hours to devote to such a broad and rich subject, it was difficult to choose among the numerous possible topics to present. Based on the subjects covered in the first week of this summer school, I decided that the goal of this course should be to establish carefully the founda- tions of rational homotopy theory, then to treat more superficially one of its most important tools, the Sullivan model. Finally, I provided a brief summary of the ex- tremely fruitful interactions between rational homotopy theory and local algebra, in the spirit of the summer school theme “Interactions between Homotopy Theory and Algebra.” I hoped to motivate the students to delve more deeply into the subject themselves, while providing them with a solid enough background to do so with relative ease. As these lecture notes do not constitute a history of rational homotopy theory, I have chosen to refer the reader to [18], instead of to the original papers, for the proofs of almost all of the results cited, at least in Sections 1 and 2. The reader interested in proper attributions will find them in [18] or [24]. The author would like to thank Luchezar Avramov and Srikanth Iyengar, as well as the anonymous referee, for their helpful comments on an earlier version of this article. -
The Continuum As a Final Coalgebra
Theoretical Computer Science 280 (2002) 105–122 www.elsevier.com/locate/tcs The continuum as a ÿnal coalgebra D. PavloviÃca, V. Prattb; ∗ aKestrel Institute, Palo Alto, CA, USA bDepartment of Computer Science, Stanford University, Stanford, CA 94305-9045, USA Abstract We deÿne the continuum up to order isomorphism, and hence up to homeomorphism via the order topology, in terms of the ÿnal coalgebra of either the functor N ×X , product with the set of natural numbers, or the functor 1+N ×X . This makes an attractive analogy with the deÿnition of N itself as the initial algebra of the functor 1 + X , disjoint union with a singleton. We similarly specify Baire space and Cantor space in terms of these ÿnal coalgebras. We identify two variants of this approach, a coinductive deÿnition based on ÿnal coalgebraic structure in the category of sets, and a direct deÿnition as a ÿnal coalgebra in the category of posets. We conclude with some paradoxical discrepancies between continuity and constructiveness in this setting. c 2002 Elsevier Science B.V. All rights reserved. 1. Introduction The algebra (N; 0;s) of non-negative integers under successor s with constant 0, the basic number system of mathematics, occupies a distinguished position in the category of algebras having a unary operation and a constant, namely as its initial object. In this paper we show that the continuum, the basic environment of physics, occu- pies an equally distinguished position in the category of coalgebras having one “dual operation” of arity N, namely as its ÿnal object. Here a dual operation is understood as a function X → X + X + ··· dual to an operation as a function X × X ×···X , with arity being the number of copies of X in each case. -
Arxiv:1907.08255V2 [Math.RA] 26 Aug 2020 Olers Eso Htte R Pitn of Splitting Are They That Show We Coalgebras
COHOMOLOGY AND DEFORMATIONS OF DENDRIFORM COALGEBRAS APURBA DAS Abstract. Dendriform coalgebras are the dual notion of dendriform algebras and are splitting of as- sociative coalgebras. In this paper, we define a cohomology theory for dendriform coalgebras based on some combinatorial maps. We show that the cohomology with self coefficients governs the formal defor- mation of the structure. We also relate this cohomology with the cohomology of dendriform algebras, coHochschild (Cartier) cohomology of associative coalgebras and cohomology of Rota-Baxter coalgebras which we introduce in this paper. Finally, using those combinatorial maps, we introduce homotopy analogue of dendriform coalgebras and study some of their properties. 1. Introduction Dendriform algebras were first introduced by Jean-Louis Loday in his study on periodicity phe- nomenons in algebraic K-theory [13]. These algebras are Koszul dual to diassociative algebras (also called associative dialgebras). More precisely, a dendriform algebra is a vector space equipped with two binary operations satisfying three new identities. The sum of the two operations turns out to be associa- tive. Thus, a dendriform algebra can be thought of like a splitting of associative algebras. Dendriform algebras are closely related to Rota-Baxter algebras [1,8]. Recently, the present author defines a coho- mology and deformation theory for dendriform algebras [3]. See [6–8,17] and references therein for more literature about dendriform algebras. The dual picture of dendriform algebras is given by dendriform coalgebras. It is given by two coproducts on a vector space satisfying three identities (dual to dendriform algebra identities), and the sum of the two coproducts makes the underlying vector space into an associative coalgebra. -
The Method of Coalgebra: Exercises in Coinduction
The Method of Coalgebra: exercises in coinduction Jan Rutten CWI & RU [email protected] Draft d.d. 8 July 2018 (comments are welcome) 2 Draft d.d. 8 July 2018 Contents 1 Introduction 7 1.1 The method of coalgebra . .7 1.2 History, roughly and briefly . .7 1.3 Exercises in coinduction . .8 1.4 Enhanced coinduction: algebra and coalgebra combined . .8 1.5 Universal coalgebra . .8 1.6 How to read this book . .8 1.7 Acknowledgements . .9 2 Categories { where coalgebra comes from 11 2.1 The basic definitions . 11 2.2 Category theory in slogans . 12 2.3 Discussion . 16 3 Algebras and coalgebras 19 3.1 Algebras . 19 3.2 Coalgebras . 21 3.3 Discussion . 23 4 Induction and coinduction 25 4.1 Inductive and coinductive definitions . 25 4.2 Proofs by induction and coinduction . 28 4.3 Discussion . 32 5 The method of coalgebra 33 5.1 Basic types of coalgebras . 34 5.2 Coalgebras, systems, automata ::: ....................... 34 6 Dynamical systems 37 6.1 Homomorphisms of dynamical systems . 38 6.2 On the behaviour of dynamical systems . 41 6.3 Discussion . 44 3 4 Draft d.d. 8 July 2018 7 Stream systems 45 7.1 Homomorphisms and bisimulations of stream systems . 46 7.2 The final system of streams . 52 7.3 Defining streams by coinduction . 54 7.4 Coinduction: the bisimulation proof method . 59 7.5 Moessner's Theorem . 66 7.6 The heart of the matter: circularity . 72 7.7 Discussion . 76 8 Deterministic automata 77 8.1 Basic definitions . 78 8.2 Homomorphisms and bisimulations of automata . -
Long Dimodules and Quasitriangular Weak Hopf Monoids
mathematics Article Long Dimodules and Quasitriangular Weak Hopf Monoids José Nicanor Alonso Álvarez 1 , José Manuel Fernández Vilaboa 2 and Ramón González Rodríguez 3,* 1 Departamento de Matemáticas, Universidade de Vigo, Campus Universitario Lagoas-Marcosende, E-36280 Vigo, Spain; [email protected] 2 Departamento de Álxebra, Universidade de Santiago de Compostela, E-15771 Santiago de Compostela, Spain; [email protected] 3 Departamento de Matemática Aplicada II, Universidade de Vigo, Campus Universitario Lagoas Marcosende, E-36310 Vigo, Spain * Correspondence: [email protected] Abstract: In this paper, we prove that for any pair of weak Hopf monoids H and B in a symmetric monoidal category where every idempotent morphism splits, the category of H-B-Long dimodules B HLong is monoidal. Moreover, if H is quasitriangular and B coquasitriangular, we also prove that B HLong is braided. As a consequence of this result, we obtain that if H is triangular and B cotriangular, B HLong is an example of a symmetric monoidal category. Keywords: Braided (symmetric) monoidal category; Long dimodule; (co)quasitriangular weak Hopf monoid Citation: Alonso Álvarez, J.N.; 1. Introduction Fernández Vilaboa, J.M.; González Let R be a commutative fixed ring with unit and let C be the non-strict symmetric Rodríguez, R. Long Dimodules and monoidal category of R-Mod where ⊗ denotes the tensor product over R. The notion Quasitriangular Weak Hopf Monoids. of Long H-dimodule for a commutative and cocommutative Hopf algebra H in C was Mathematics 2021, 9, 424. https:// introduced by Long [1] to study the Brauer group of H-dimodule algebras. -
Coalgebras from Formulas
Coalgebras from Formulas Serban Raianu California State University Dominguez Hills Department of Mathematics 1000 E Victoria St Carson, CA 90747 e-mail:[email protected] Abstract Nichols and Sweedler showed in [5] that generic formulas for sums may be used for producing examples of coalgebras. We adopt a slightly different point of view, and show that the reason why all these constructions work is the presence of certain representative functions on some (semi)group. In particular, the indeterminate in a polynomial ring is a primitive element because the identity function is representative. Introduction The title of this note is borrowed from the title of the second section of [5]. There it is explained how each generic addition formula naturally gives a formula for the action of the comultiplication in a coalgebra. Among the examples chosen in [5], this situation is probably best illus- trated by the following two: Let C be a k-space with basis {s, c}. We define ∆ : C −→ C ⊗ C and ε : C −→ k by ∆(s) = s ⊗ c + c ⊗ s ∆(c) = c ⊗ c − s ⊗ s ε(s) = 0 ε(c) = 1. 1 Then (C, ∆, ε) is a coalgebra called the trigonometric coalgebra. Now let H be a k-vector space with basis {cm | m ∈ N}. Then H is a coalgebra with comultiplication ∆ and counit ε defined by X ∆(cm) = ci ⊗ cm−i, ε(cm) = δ0,m. i=0,m This coalgebra is called the divided power coalgebra. Identifying the “formulas” in the above examples is not hard: the for- mulas for sin and cos applied to a sum in the first example, and the binomial formula in the second one. -
LOCAL-GLOBAL PRINCIPLE for TRANSVECTION GROUPS 1. Introduction in 1956, J-P. Serre Asked If a Finitely Generated Projective Modu
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 138, Number 4, April 2010, Pages 1191–1204 S 0002-9939(09)10198-3 Article electronically published on November 20, 2009 LOCAL-GLOBAL PRINCIPLE FOR TRANSVECTION GROUPS A. BAK, RABEYA BASU, AND RAVI A. RAO (Communicated by Martin Lorenz) Abstract. In this article we extend the validity of Suslin’s Local-Global Prin- ciple for the elementary transvection subgroup of the general linear group GLn(R), the symplectic group Sp2n(R), and the orthogonal group O2n(R), where n>2, to a Local-Global Principle for the elementary transvection sub- group of the automorphism group Aut(P ) of either a projective module P of global rank > 0 and constant local rank > 2, or of a nonsingular symplec- tic or orthogonal module P of global hyperbolic rank > 0 and constant local hyperbolic rank > 2. In Suslin’s results, the local and global ranks are the same, because he is concerned only with free modules. Our assumption that the global (hyperbolic) rank > 0 is used to define the elementary transvec- tion subgroups. We show further that the elementary transvection subgroup ET(P )isnormalinAut(P ), that ET(P )=T(P ), where the latter denotes the full transvection subgroup of Aut(P ), and that the unstable K1-group K1(Aut(P )) = Aut(P )/ET(P )=Aut(P )/T(P ) is nilpotent by abelian, pro- vided R has finite stable dimension. The last result extends previous ones of Bak and Hazrat for GLn(R), Sp2n(R), and O2n(R). An important application to the results in the current paper can be found in a preprint of Basu and Rao in which the last two named authors studied the decrease in the injective stabilization of classical modules over a nonsingular affine algebra over perfect C1-fields.