Decomposition Spaces, Incidence Algebras and Mobius Inversion II
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Nonablian Cocycles and Their Σ-Model Qfts
Nonablian cocycles and their σ-model QFTs December 31, 2008 Abstract Nonabelian cohomology can be regarded as a generalization of group cohomology to the case where both the group itself as well as the coefficient object are allowed to be generalized to 1-groupoids or even to general 1-categories. Cocycles in nonabelian cohomology in particular represent higher principal bundles (gerbes) { possibly equivariant, possibly with connection { as well as the corresponding associated higher vector bundles. We propose, expanding on considerations in [13, 34, 5], a systematic 1-functorial formalization of the σ-model quantum field theory associated with a given nonabelian cocycle regarded as the background field for a brane coupled to it. We define propagation in these σ-model QFTs and recover central aspects of groupoidification [1, 2] of linear algebra. In a series of examples we show how this formalization reproduces familiar structures in σ-models with finite target spaces such as Dijkgraaf-Witten theory and the Yetter model. The generalization to σ-models with smooth target spaces is developed elsewhere [24]. 1 Contents 1 Introduction 3 2 1-Categories and Homotopy Theory 4 2.1 Shapes for 1-cells . 5 2.2 !-Categories . 5 2.3 !-Groupoids . 7 2.4 Cosimplicial !-categories . 7 2.5 Monoidal biclosed structure on !Categories ............................ 7 2.6 Model structure on !Categories ................................... 9 3 Nonabelian cohomology and higher vector bundles 9 3.1 Principal !-bundles . 10 3.2 Associated !-bundles . 11 3.3 Sections and homotopies . 12 4 Quantization of !-bundles to σ-models 15 4.1 σ-Models . 16 4.2 Branes and bibranes . -
Decomposition Spaces, Incidence Algebras and M\" Obius Inversion I
DECOMPOSITION SPACES, INCIDENCE ALGEBRAS AND MOBIUS¨ INVERSION I: BASIC THEORY IMMA GALVEZ-CARRILLO,´ JOACHIM KOCK, AND ANDREW TONKS Abstract. This is the first in a series of papers devoted to the theory of decomposition spaces, a general framework for incidence algebras and M¨obius inversion, where algebraic identities are realised by taking homotopy cardinality of equivalences of ∞-groupoids. A decomposition space is a simplicial ∞-groupoid satisfying an exactness condition, weaker than the Segal condition, expressed in terms of active and inert maps in ∆. Just as the Segal condition expresses composition, the new exactness condition expresses decomposition, and there is an abundance of examples in combinatorics. After establishing some basic properties of decomposition spaces, the main result of this first paper shows that to any decomposition space there is an associated incidence coalgebra, spanned by the space of 1-simplices, and with coefficients in ∞-groupoids. We take a functorial viewpoint throughout, emphasising conservative ULF functors; these induce coalgebra homomorphisms. Reduction procedures in the classical theory of incidence coalgebras are examples of this notion, and many are examples of decalage of decomposition spaces. An interesting class of examples of decomposition spaces beyond Segal spaces is provided by Hall algebras: the Waldhausen S•-construction of an abelian (or stable infinity) category is shown to be a decomposition space. In the second paper in this series we impose further conditions on decomposition spaces, to obtain a general M¨obius inversion principle, and to ensure that the various constructions and results admit a homotopy cardinality. In the third paper we show that the Lawvere–Menni Hopf algebra of M¨obius intervals is the homotopy cardinality of a certain universal decomposition space. -
THE MCM-APPROXIMATION of the TRIVIAL MODULE OVER a CATEGORY ALGEBRA3 Unfactorizable Morphism
THE MCM-APPROXIMATION OF THE TRIVIAL MODULE OVER A CATEGORY ALGEBRA REN WANG Abstract. For a finite free EI category, we construct an explicit module over its category algebra. If in addition the category is projective over the ground field, the constructed module is Gorenstein-projective and is a maximal Cohen- Macaulay approximation of the trivial module. We give conditions on when the trivial module is Gorenstein-projective. 1. Introduction Let k be a field and C be a finite EI category. Here, the EI condition means that all endomorphisms in C are isomorphisms. In particular, HomC (x, x) = AutC (x) is a finite group for each object x. Denote by kAutC (x) the group algebra. Recall that a finite EI category C is projective over k if each kAutC (y)-kAutC (x)-bimodule kHomC (x, y) is projective on both sides; see [9, Definition 4.2]. The concept of a finite free EI category is introduced in [6, 7]. Let C be a finite α free EI category. For any morphism x → y in C , set V (α) to be the set of objects ′ ′′ α α w such that there are factorizations x → w → y of α with α′′ a non-isomorphism. ′′ For any w ∈ V (α), we set tw(α) = α ◦ ( g), which is an element in g∈AutPC (w) kHomC (w,y). The freeness of C implies that the element tw(α) is independent of the choice of α′′. Denote by k-mod the category of finite dimensional k-vector spaces. We identify covariant functors from C to k-mod with left modules over the category algebra. -
Pathlike Co/Bialgebras and Their Antipodes with Applications to Bi- and Hopf Algebras Appearing in Topology, Number Theory and Physics
PATHLIKE CO/BIALGEBRAS AND THEIR ANTIPODES WITH APPLICATIONS TO BI- AND HOPF ALGEBRAS APPEARING IN TOPOLOGY, NUMBER THEORY AND PHYSICS. RALPH M. KAUFMANN AND YANG MO Dedicated to Professor Dirk Kreimer on the occasion of his 60th birthday Abstract. We develop an algebraic theory of flavored and pathlike co-, bi- and Hopf algebras. This is the right framework in which to discuss antipodes for bialgebras naturally appearing in topology, number theory and physics. In particular, we can precisely give conditions the invert- ibility of characters needed for renormalization in the formulation of Connes and Kreimer and in the canonical examples these conditions are met. To construct the antipodes directly, we discuss formal localization constructions and quantum deformations. These allow to construct and naturally explain the appearance Brown style coactions. Using previous results, we can tie all the relevant coalgebras to categorical constructions and the bialgebra structures to Feynman categories. Introduction Although the use of Hopf algebras has a long history, the seminal pa- per [CK98] led to a turbocharged development for their use which has pene- trated deeply into mathematical physics, number theory and also topology, their original realm|see [AFS08] for the early beginnings. The important realization in [CK98, CK00, CK01] was that the renormalization procedure for quantum field theory can be based on a character theory for Hopf al- gebras via a so-called Birkhoff factorization and convolution inverses. The relevant Hopf algebras are those of trees with a coproduct given by a sum over so{called admissible cuts |with the factors of the coproduct being the arXiv:2104.08895v1 [math.QA] 18 Apr 2021 left over stump and the collection of cut off branches| and Hopf algebras of graphs in which the factors of the summands of the coproduct are given by a subgraph and the quotient graph. -
Combinatorics
09.10.74 Combinatorics Lectures of Mark Dukes Typing and layout by Líney Halla Kristinsdóttir University of Iceland Spring Term 2008 Contents 1 Enumeration1 1.1 Counting Arguments...............................2 1.2 Elementary Counting Coecients........................3 1.3 Compositions & Partitions of an Integer....................7 1.4 The Reection Principle.............................9 1.5 Stirling Numbers................................. 10 1.5.1 Stirling Numbers of the 2nd Kind: S(n; k) ............... 10 1.5.2 Signless Stirling Numbers of the 1st Kind............... 12 1.6 Multinomial Coecients............................. 14 1.7 Generating Functions I.............................. 15 1.8 Generating Functions II............................. 22 2 Permutations & Permutation Statistics 27 2.1 Descents & the Eulerian Polynomial...................... 27 2.2 Cycle structure & left-to-right maxima..................... 32 2.3 Excedances & weak excedances......................... 33 2.4 Inversions & the Major index.......................... 35 2.5 Multisets, Permutations & q-series....................... 39 2.6 Subspaces of a Vector Space.......................... 43 2.7 Permutations as Increasing Binary Trees.................... 45 2.8 Standard Young Tableaux............................ 46 2.9 Robinson-Schensted-Knuth (RSK) correspondence............... 48 i 3 Partially Ordered Sets (Posets) 53 3.1 Posets...................................... 53 3.2 Lattices..................................... 60 3.3 Modular Lattices................................ -
Quiver Generalized Weyl Algebras, Skew Category Algebras and Diskew Polynomial Rings
Math.Comput.Sci. (2017) 11:253–268 DOI 10.1007/s11786-017-0313-5 Mathematics in Computer Science Quiver Generalized Weyl Algebras, Skew Category Algebras and Diskew Polynomial Rings V. V. B av u l a Received: 7 December 2016 / Revised: 3 March 2017 / Accepted: 11 March 2017 / Published online: 28 April 2017 © The Author(s) 2017. This article is an open access publication Abstract The aim of the paper is to introduce new large classes of algebras—quiver generalized Weyl algebras, skew category algebras, diskew polynomial rings and skew semi-Laurent polynomial rings. Keywords Skew category algebra · Quiver generalized Weyl algebra · Diskew polynomial ring · Generalized Weyl algebra · Skew double quiver algebra · Double quiver groupoid Mathematics Subject Classification 16D30 · 16P40 · 16D25 · 16P50 · 16S85 1 Introduction In this paper, K is a commutative ring with 1, algebra means a K -algebra. In general, it is not assumed that a K -algebra has an identity element. Module means a left module. Missing definitions can be found in [11]. The aim of the paper is to introduce new large classes of algebras—quiver generalized Weyl algebras, skew category algebras, diskew polynomial rings, skew semi-Laurent polynomial rings and the simplex generalized Weyl algebras. 2 Skew Category Algebras The aim of this section is to introduce skew category algebras; to consider new interesting examples (skew tree rings, skew semi-Laurent polynomial rings, etc); to give criteria for a skew category algebra to be a left/right Noetherian algebra (Theorem 2.2, Proposition 2.3). In Sect. 3, skew category algebras are used to define the quiver generalized Weyl algebras. -
Monoids in Representation Theory, Markov Chains, Combinatorics and Operator Algebras
Monoids in Representation Theory, Markov Chains, Combinatorics and Operator Algebras Benjamin Steinberg, City College of New York Australian Mathematical Society Meeting December 2019 Group representation theory and Markov chains • Group representation theory is sometimes a valuable tool for analyzing Markov chains. Group representation theory and Markov chains • Group representation theory is sometimes a valuable tool for analyzing Markov chains. • The method (at least for nonabelian groups) was perhaps first popularized in a paper of Diaconis and Shahshahani from 1981. Group representation theory and Markov chains • Group representation theory is sometimes a valuable tool for analyzing Markov chains. • The method (at least for nonabelian groups) was perhaps first popularized in a paper of Diaconis and Shahshahani from 1981. • They analyzed shuffling a deck of cards by randomly transposing cards. Group representation theory and Markov chains • Group representation theory is sometimes a valuable tool for analyzing Markov chains. • The method (at least for nonabelian groups) was perhaps first popularized in a paper of Diaconis and Shahshahani from 1981. • They analyzed shuffling a deck of cards by randomly transposing cards. • Because the transpositions form a conjugacy class, the eigenvalues and convergence time of the walk can be understood via characters of the symmetric group. Group representation theory and Markov chains • Group representation theory is sometimes a valuable tool for analyzing Markov chains. • The method (at least for nonabelian groups) was perhaps first popularized in a paper of Diaconis and Shahshahani from 1981. • They analyzed shuffling a deck of cards by randomly transposing cards. • Because the transpositions form a conjugacy class, the eigenvalues and convergence time of the walk can be understood via characters of the symmetric group. -
LTCC Enumerative Combinatorics 5 Posets and M¨Obius Inversion
LTCC Enumerative Combinatorics Notes 5 Alex Fink Fall 2015 5 Posets and Mobius¨ inversion Mobius¨ inversion can be viewed as a generalisation of the inclusion-exclusion principle with an apparatus to keep track of how the conditions intersect, as an apparatus to reduce the number of terms. The apparatus, that of partial orders, turns out to be of great combinatorial utility in its own right. 5.1 The inclusion-exclusion principle Often we are in the situation where we have a number of conditions on a set of combinatorial objects, and we have information about the number of objects which satisfy various combinations of these conditions (inclusion), while we want to count the objects satisfying none of the conditions (exclusion), or perhaps satis- fying some but not others. What is known as the sieve method is of general use in this situation: overcount the objects satisfying the conditions, and then make cor- rections and subtract off elements that have been multiply counted, and so forth. The sieve of Eratosthenes gave its name to the class (although, alone, it’s not es- pecially helpful for the enumeration of primes): the primes are the integers which satify none of the conditions of having the forms 2n;3n;5n;7n;::: for n ≥ 2. Let A1;:::;An be subsets of a finite set X. For any non-empty subset J of the index set [n], we put \ AJ = A j; j2J and take A/0 = X by convention. Theorem 5.1 (Inclusion-Exclusion Principle) The number of elements of X ly- ing in none of the sets Ai is equal to jJj ∑ (−1) jAJj: J⊆[n] Proof The expression in the theorem is a linear combination of the cardinalities of the sets AJ, and so we can calculate it by working out, for each x 2 X, the contribution of x to the sum. -
Adjoint Associativity: an Invitation to Algebra in -Categories 1 JOSEPHLIPMAN
Commutative Algebra and Noncommutative Algebraic Geometry, II MSRI Publications Volume 68, 2015 Adjoint associativity: an invitation to algebra in -categories 1 JOSEPH LIPMAN There appeared not long ago a reduction formula for derived Hochschild cohomology, that has been useful, for example, in the study of Gorenstein maps and of rigidity with respect to semidualizing complexes. The formula involves the relative dualizing complex of a ring homomorphism, so brings out a connection between Hochschild homology and Grothendieck duality. The proof, somewhat ad hoc, uses homotopical considerations via a number of noncanonical projective and injective resolutions of differential graded objects. Recent efforts aim at more intrinsic approaches, hopefully upgradable to “higher” contexts — like bimodules over algebras in -categories. This 1 would lead to wider applicability, for example to ring spectra; and the methods might be globalizable, revealing some homotopical generalizations of aspects of Grothendieck duality. (The original formula has a geometric version, proved by completely different methods coming from duality theory.) A first step is to extend Hom-Tensor adjunction — adjoint associativity — to the -category 1 setting. Introduction 266 1. Motivation: reduction of Hochschild (co)homology 266 2. Enter homotopy 268 3. Adjoint associativity 269 4. -categories 270 1 5. The homotopy category of an -category 273 1 6. Mapping spaces; equivalences 276 7. Colimits 279 8. Adjoint functors 280 9. Algebra objects in monoidal -categories 282 1 This expository article is an elaboration of a colloquium talk given April 17, 2013 at the Mathemat- ical Sciences Research Institute in Berkeley, under the Commutative Algebra program supported by the National Science Foundation. -
Operator Algebras in Rigid C*-Tensor Categories Arxiv:1611.04620V2
Operator algebras in rigid C*-tensor categories Corey Jones and David Penneys December 5, 2016 Abstract In this article, we define operator algebras internal to a rigid C*-tensor category C. A C*/W*-algebra object in C is an algebra object A in ind-C whose category of free modules FreeModC(A) is a C-module C*/W*-category respectively. When C = Hilbf:d:, the category of finite dimensional Hilbert spaces, we recover the usual notions of operator algebras. We generalize basic representation theoretic results, such as the Gelfand-Naimark and von Neumann bicommutant theorems, along with the GNS construction. We define the notion of completely positive maps between C*-algebra objects in C and prove the analog of the Stinespring dilation theorem. As an application, we discuss approximation and rigidity properties, including amenability, the Haagerup property, and property (T) for a connected W*-algebra M in C. Our definitions simultaneously unify the definitions of analytic properties for discrete quantum groups and rigid C*-tensor categories. Contents 1 Introduction2 2 Background7 2.1 Linear, dagger, and C*-categories . .8 2.2 Involutions on tensor categories . .9 2.3 Rigid C*-tensor categories . 10 arXiv:1611.04620v2 [math.OA] 1 Dec 2016 2.4 The category Vec(C)............................... 13 2.5 Graphical calculus for the Yoneda embedding . 15 2.6 The category Hilb(C)............................... 17 3 ∗-Algebras in Vec(C) 20 3.1 Algebras and module categories . 20 3.2 Equivalence between algebras and cyclic module categories . 22 3.3 ∗-Algebra objects and dagger module categories . 25 3.4 C* and W*-algebra objects . -
Elementary Proof of a Theorem of Hawkes, Isaacs And¨Ozaydin
Elementary Proof of a Theorem of Hawkes, Isaacs and Ozaydin¨ Matth´evan der Lee Abstract We present an elementary proof of the theorem of Hawkes, Isaacs and Ozaydin,¨ which states that Σ µG(H, K) ≡ 0 mod d, where µG denotes the M¨obius function for the subgroup lattice of a finite group G, H ranges over the conjugates of a given subgroup F of G with [G : F ] divisible by d, and K over the supergroups of the H for which [K : H] divides d. We apply the theorem to obtain a result on the number of solutions of |hH,gi| | n, for said H and a natural number n. The present version of the article includes an additional result on a quantity studied by K.S. Brown. Keywords: M¨obius function, arithmetic functions, subgroup lattice 2010 MSC: 05E15, 11A25, 20D30 1 Introduction The purpose of this note is to present a simple proof for the theorem of Hawkes, Isaacs and Ozaydin,¨ an important tool in the area of counting problems in finite groups. We refer to [3], where the result has appeared as Theorem 5.1, for background information regarding the subject. The exposition uses minimal group theory. The ingredients for the proof are Burnside’s Lemma, the incidence algebra of a finite partially ordered set (of which we use only the basic properties), and a feature of arithmetic functions: Corollary 3.4. Next, we derive a result on the number of solutions g of |hH,gi| | n, for a finite group G, a subgroup H ≤ G, and n | |G| (Theorem 6.1), and some results on a quantity studied by K.S. -
The Incidence Algebra and the Möbius Function
Monday 2/25 The Incidence Algebra Many enumerative properties of posets P can be expressed in terms of a ring called its incidence algebra. Definition 1. Let P be a locally finite poset and let Int(P ) denote the set of intervals of P . The incidence algebra I(P ) is the set of functions f : Int(P ) ! C. I'll abbreviate f([x; y]) by f(x; y). (For convenience, we set f(x; y) = 0 if x 6≤ y.) This is a C-vector space with pointwise addition, subtraction and scalar multiplication. It can be made into an associative algebra by the convolution product: (f ∗ g)(x; y) = f(x; z)g(z; y): z2X[x;y] Proposition 1. Convolution is associative. Proof. [(f ∗ g) ∗ h](x; y) = (f ∗ g)(x; z) · h(z; y) z2X[x;y] = f(x; w)g(w; z) h(z; y) 0 1 z2X[x;y] w2X[x;z] @ A = f(x; w) g(w; z)h(z; y) 0 1 w2X[x;y] z2X[w;y] = f(x; w) @· (g ∗ h)(w; y) A w2X[x;y] = [f ∗ (g ∗ h)](x; y): Proposition 2. f 2 I(P ) is invertible if and only if f(x; x) 6= 0 for all x. Proof. If f is invertible with inverse g, then (f ∗g)(x; x) = f(x; x)g(x; x) for all x, so in particular f(x; x) 6= 0. OTOH, if f(x; x) 6= 0, then we can define a left inverse g inductively: g(x; x) = 1=f(x; x), and for x < y, we want to have (g ∗ f)(x; y) = 0 = g(x; z)f(z; y) x z y ≤X≤ = g(x; y)f(x; x) + f(x; z)g(z; y) x z<y ≤X so define 1 g(x; y) = − g(x; z)f(z; y): f(x; x) x≤zy X The identity element of I(P ) is the Kronecker delta function: 1 if x = y; δ(x; y) = (0 if x 6= y: The zeta function is defined as 1 if x ≤ y; ζ(x; y) = (0 if x 6≤ y and the eta function is 1 if x < y; η(x; y) = (0 if x 6< y; i.e., η = ζ − δ.