CLIFFORD MODULES and INVARIANTS of QUADRATIC FORMS Since the Source and the Target Are Different Groups
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THE DIRAC OPERATOR 1. First Properties 1.1. Definition. Let X Be A
THE DIRAC OPERATOR AKHIL MATHEW 1. First properties 1.1. Definition. Let X be a Riemannian manifold. Then the tangent bundle TX is a bundle of real inner product spaces, and we can form the corresponding Clifford bundle Cliff(TX). By definition, the bundle Cliff(TX) is a vector bundle of Z=2-graded R-algebras such that the fiber Cliff(TX)x is just the Clifford algebra Cliff(TxX) (for the inner product structure on TxX). Definition 1. A Clifford module on X is a vector bundle V over X together with an action Cliff(TX) ⊗ V ! V which makes each fiber Vx into a module over the Clifford algebra Cliff(TxX). Suppose now that V is given a connection r. Definition 2. The Dirac operator D on V is defined in local coordinates by sending a section s of V to X Ds = ei:rei s; for feig a local orthonormal frame for TX and the multiplication being Clifford multiplication. It is easy to check that this definition is independent of the coordinate system. A more invariant way of defining it is to consider the composite of differential operators (1) V !r T ∗X ⊗ V ' TX ⊗ V,! Cliff(TX) ⊗ V ! V; where the first map is the connection, the second map is the isomorphism T ∗X ' TX determined by the Riemannian structure, the third map is the natural inclusion, and the fourth map is Clifford multiplication. The Dirac operator is clearly a first-order differential operator. We can work out its symbol fairly easily. The symbol1 of the connection r is ∗ Sym(r)(v; t) = iv ⊗ t; v 2 Vx; t 2 Tx X: All the other differential operators in (1) are just morphisms of vector bundles. -
Adams Operations and Symmetries of Representation Categories Arxiv
Adams operations and symmetries of representation categories Ehud Meir and Markus Szymik May 2019 Abstract: Adams operations are the natural transformations of the representation ring func- tor on the category of finite groups, and they are one way to describe the usual λ–ring structure on these rings. From the representation-theoretical point of view, they codify some of the symmetric monoidal structure of the representation category. We show that the monoidal structure on the category alone, regardless of the particular symmetry, deter- mines all the odd Adams operations. On the other hand, we give examples to show that monoidal equivalences do not have to preserve the second Adams operations and to show that monoidal equivalences that preserve the second Adams operations do not have to be symmetric. Along the way, we classify all possible symmetries and all monoidal auto- equivalences of representation categories of finite groups. MSC: 18D10, 19A22, 20C15 Keywords: Representation rings, Adams operations, λ–rings, symmetric monoidal cate- gories 1 Introduction Every finite group G can be reconstructed from the category Rep(G) of its finite-dimensional representations if one considers this category as a symmetric monoidal category. This follows from more general results of Deligne [DM82, Prop. 2.8], [Del90]. If one considers the repre- sentation category Rep(G) as a monoidal category alone, without its canonical symmetry, then it does not determine the group G. See Davydov [Dav01] and Etingof–Gelaki [EG01] for such arXiv:1704.03389v3 [math.RT] 3 Jun 2019 isocategorical groups. Examples go back to Fischer [Fis88]. The representation ring R(G) of a finite group G is a λ–ring. -
Differential Forms As Spinors Annales De L’I
ANNALES DE L’I. H. P., SECTION A WOLFGANG GRAF Differential forms as spinors Annales de l’I. H. P., section A, tome 29, no 1 (1978), p. 85-109 <http://www.numdam.org/item?id=AIHPA_1978__29_1_85_0> © Gauthier-Villars, 1978, tous droits réservés. L’accès aux archives de la revue « Annales de l’I. H. P., section A » implique l’accord avec les conditions générales d’utilisation (http://www.numdam. org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Henri Poincare, Section A : Vol. XXIX. n° L 1978. p. 85 Physique’ théorique.’ Differential forms as spinors Wolfgang GRAF Fachbereich Physik der Universitat, D-7750Konstanz. Germany ABSTRACT. 2014 An alternative notion of spinor fields for spin 1/2 on a pseudoriemannian manifold is proposed. Use is made of an algebra which allows the interpretation of spinors as elements of a global minimal Clifford- ideal of differential forms. The minimal coupling to an electromagnetic field is introduced by means of an « U(1 )-gauging ». Although local Lorentz transformations play only a secondary role and the usual two-valuedness is completely absent, all results of Dirac’s equation in flat space-time with electromagnetic coupling can be regained. 1. INTRODUCTION It is well known that in a riemannian manifold the laplacian D := - (d~ + ~d) operating on differential forms admits as « square root » the first-order operator ~ 2014 ~ ~ being the exterior derivative and e) the generalized divergence. -
Principal Bundles, Vector Bundles and Connections
Appendix A Principal Bundles, Vector Bundles and Connections Abstract The appendix defines fiber bundles, principal bundles and their associate vector bundles, recall the definitions of frame bundles, the orthonormal frame bun- dle, jet bundles, product bundles and the Whitney sums of bundles. Next, equivalent definitions of connections in principal bundles and in their associate vector bundles are presented and it is shown how these concepts are related to the concept of a covariant derivative in the base manifold of the bundle. Also, the concept of exterior covariant derivatives (crucial for the formulation of gauge theories) and the meaning of a curvature and torsion of a linear connection in a manifold is recalled. The concept of covariant derivative in vector bundles is also analyzed in details in a way which, in particular, is necessary for the presentation of the theory in Chap. 12. Propositions are in general presented without proofs, which can be found, e.g., in Choquet-Bruhat et al. (Analysis, Manifolds and Physics. North-Holland, Amsterdam, 1982), Frankel (The Geometry of Physics. Cambridge University Press, Cambridge, 1997), Kobayashi and Nomizu (Foundations of Differential Geometry. Interscience Publishers, New York, 1963), Naber (Topology, Geometry and Gauge Fields. Interactions. Applied Mathematical Sciences. Springer, New York, 2000), Nash and Sen (Topology and Geometry for Physicists. Academic, London, 1983), Nicolescu (Notes on Seiberg-Witten Theory. Graduate Studies in Mathematics. American Mathematical Society, Providence, RI, 2000), Osborn (Vector Bundles. Academic, New York, 1982), and Palais (The Geometrization of Physics. Lecture Notes from a Course at the National Tsing Hua University, Hsinchu, 1981). A.1 Fiber Bundles Definition A.1 A fiber bundle over M with Lie group G will be denoted by E D .E; M;;G; F/. -
ADAMS OPERATIONS on HIGHER K-THEORY Daniel R. Grayson
February 6, 1995 ADAMS OPERATIONS ON HIGHER K-THEORY Daniel R. Grayson University of Illinois at Urbana-Champaign Abstract. We construct Adams operations on higher algebraic K-groups induced by oper- ations such as symmetric powers on any suitable exact category, by constructing an explicit map of spaces, combinatorially defined. The map uses the S-construction of Waldhausen, and deloops (once) earlier constructions of the map. 1. Introduction. Let P be an exact category with a suitable notion of tensor product M ⊗ N, symmetric power SkM,andexteriorpowerΛkM. For example, we may take P to be the category P(X) of vector bundles on some scheme X.OrwemaytakeP to be the category P(R)of finitely generated projective R-modules, where R is a commutative ring. Or we may fix a group Γ and a commutative ring R and take P to be the category P(R, Γ) of representations of Γ on projective finitely generated R-modules. We impose certain exactness requirements on these functors, so that in particular the tensor product is required to be bi-exact, and this prevents us from taking for P a category such as the category M(R) of finitely generated R-modules. In a previous paper [5] I showed how to use the exterior power operations on modules to construct the lambda operations λk on the higher K-groups as a map of spaces λk : |GP| → |GkP| in a combinatorial fashion. Here the simplicial set GP, due to Gillet and me [3], provides an alternate definition for the K-groups of any exact category, KiP = πiGP, which has the advantage that the Grothendieck group appears as π0 and is not divorced from the higher K-groups. -
Local SU-Bordism
On K(1)-local SU-bordism Dissertation zur Erlangung des Doktorgrades (Dr. rer. nat.) der Fakult¨at f¨urMathematik der Ruhr-Universit¨at Bochum vorgelegt von Dipl.-Math. Holger Reeker Mai 2009 Contents Chapter 1. Introduction and statement of results 5 Chapter 2. Some homotopical algebra 9 1. Generalized cohomology theories and spectra 9 2. Symmetric spectra over topological spaces 11 3. Complex oriented theories and computational methods 14 4. Bousfield localization of spectra 15 5. Algebraic manipulations of spectra 18 6. A resolution of the K(1)-local sphere 20 7. Thom isomorphism 21 Chapter 3. The algebraic structure of K(1)-local E∞ ring spectra 23 1. Operads 23 2. Dyer-Lashof operations for K(1)-local E∞ spectra 25 3. The θ-algebra structure of π0K ∧ MU 26 4. The θ-algebra structure of π0K ∧ MSU 29 Chapter 4. Splitting off an E∞ summand Tζ 31 1. The image of MSU∗ → MU∗ 32 2. Formal group laws and Miscenkos formula 34 3. Construction of an SU-manifold with Aˆ = 1 38 4. Construction of an Artin-Schreier class 41 5. Construction of an E∞ map Tζ → MSU 41 6. Split map - direct summand argument 42 0 Chapter 5. Detecting free E∞ summands TS 45 1. Introduction to Adams operations in K-theory 45 ∞ 2. Calculating operations on K∗CP 47 3. Bott’s formula and cannibalistic classes 52 4. Spherical classes in K∗MSU 55 5. Umbral calculus 57 Chapter 6. Open questions and concluding remarks 61 Bibliography 63 3 CHAPTER 1 Introduction and statement of results One of the highlights in algebraic topology was the invention of generalized homology and cohomology theories by Whitehead and Brown in the 1960s. -
Adams Operations in Differential Algebraic K-Theory
Adams Operations in Differential Algebraic K-theory Dissertation zur Erlangung des Doktorgrades der Naturwissenschaften (Dr. rer. nat.) der Fakult¨atf¨urMathematik der Universit¨atRegensburg vorgelegt von Christoph Schrade aus Leipzig im Jahr 2018 Promotionsgesuch eingereicht am: 29.05.2018 Die Arbeit wurde angeleitet von: • Prof. Dr. Ulrich Bunke • Dr. Georg Tamme 1 Contents 1. Introduction 3 2. 1-categorical background 7 2.1. General theory 7 2.2. Higher commutative algebra 25 2.3. Additive and stable 1-categories 41 3. Multiplicative Adams operations on algebraic K-theory 50 3.1. The Snaith model for the motivic K-theory spectrum 51 3.2. Construction of the Adams operations 61 4. Adams operations on differential algebraic K-theory 66 4.1. The Beilinson regulator as a map of ring spectra 67 4.2. Construction of the differential refinement of the Adams operations 79 Appendix A. Segre embeddings and commutative algebra structure on P1 95 References 101 3 1. Introduction Adams operations first appeared in the context of K-theory of topo- logical spaces. For a finite CW-complex X there is the zeroth topolog- ical K-group K0(X) constructed by group completion of the monoid Vect(X) of isomorphism classes of finite rank vector bundles over X with the direct sum operation. In fact there is even a ring structure on K0(X) which is induced by the tensor product operation of vector bundles. For a natural number k, the k-th Adams operation is then a ring homomorphism k : K0(X) ! K0(X) which is characterized by the property that it sends the class of a line bundle to the class of its k-th tensor power. -
A-RINGS and ALGEBRAIC K-THEORY Howard L. HILLER* We
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Journal of Pure and Applied Algebra 20 (1981) 241-266 North-Holland Publishing Company A-RINGS AND ALGEBRAIC K-THEORY Howard L. HILLER* Mathematical Institute, Oxford University, Oxford OX1 3LB, England Communicated by H. Bass Received 6 December 1979 Let A be a commutative ring with identity. Loday [14] and others have described the mutliplicative structure (both graded and ungraded) on the higher algebraic K-theory of A. In [ 191 and [24], Quillen has indicated the existence of a A-ring structure on the “K-cohomology” groups K(X, A) = [X, K,(A) x BGL(A)+]. The purpose of this paper is to develop some of this structure and show how it can be useful in obtaining information about the K-groups themselves. In particular, standard techniques will then allow one to construct Adams operations Gk in algebraic K-theory. These operations enjoy some of the attractive properties of their counterparts in the K-theory of complex vector bundles over a finite complex. Indeed, with this machinery and the itale Chern classes of Soul6 [27], one can hope to lift other results from the topological to the algebraic setting. We now give a more detailed description of the contents of this paper. In Section 1 we rapidly review the fundamentals of the Quillen K-theory and construct a natural transformation q connecting representations and K-theory using certain cohomological input from [24]. In Section 2 we demonstrate an important universal property that q enjoys and indicate its usefulness in producing maps between algebraic K-groups. -
Arxiv:Math/9802033V1 [Math.DG] 6 Feb 1998
Cartan Spinor Bundles on Manifolds. ∗ Thomas Friedrich, Berlin July 26, 2021 1 Introduction. Spinor fields and Dirac operators on Riemannian manifolds M n can be introduced by means of a reduction of the frame bundle from the structure group O(n) to one of the groups Spin(n), P in(n) or SpinC(n). In any case the existence of a corre- sponding reduction imposes topological restrictions on the manifold M n. The aim of the present paper is the construction of spinor bundles of Cartan type over certain non-orientable manifolds. The bundles under consideration do not split into sub- bundles invariant under the action of the Clifford algebra and therefore they are not induced from P inC structure of the manifold. Moreover, we study the case of the real projective space RPn and its spinor bundle in more detail. These bundles over RPn admit a suitable metric connection ∇S and the corresponding Dirac operator. In particular it turns out that there are Killing spinors in the constructed twisted spinor bundle over RPn for all dimensions. C ∼ Let us fix some notations. In case n ≡ 0 mod 2 we denote by γ : Cliff (n) → End(∆n) the isomorphism between the Clifford algebra and the algebra of endomorphisms of the space ∆n of all Dirac spinor. In this way we obtain the so called Dirac representation γ of the Clifford algebra. In case n ≡ 1 mod 2 we have the Pauli C C C representation γ : Cliff (n) → End(∆n). Denote by α : Cliff (n) → Cliff (n) the canonical involution. -
Klassen Theorie, December 26, 2016 to January 7, 2017
Klassen Theorie B.Sury School on K-theory and its applications December 26, 2016 - January 7, 2017 I.S.I. Bangalore . "The way I first visualized a K-group was as a group of classes of objects of an abelian (or more generally, additive) category, such as coherent sheaves on an algebraic variety, or vector bundles, etc. I would presumably have called this group C(X) (X being a variety or any other kind of space), C the initial letter of class, but my past in functional analysis may have prevented this, as C(X) designates also the space of continuous functions on X (when X is a topological space). Thus, I reverted to K instead of C, since my mother tongue is German, Class = Klasse (in German), and the sounds corresponding to C and K are the same" .......................Alexander Grothendieck. 1 Introduction In 1957, Grothendieck (handwritten notes) formulated the "Grothendieck- Riemann-Roch theorem". In 1958, there was an exposition of this by Borel & Serre. In 1959, Bott proved his periodicity theorems on stable homotopy groups. His proof involved Riemannian geometry and Morse theory. In 1961, Atiyah & Hirzebruch realized that Bott periodicity is related to a new K- theory (topologial version) analogous to Grothendieck's algebraic K-theory. They developed the topological theory which followed a similar pattern. A new feature was that they could define derived functors K−n and Bott peri- odicity simplified to the statements −n ∼ −n−2 −n ∼ −n−8 KC = KC ;KR = KR : This K-theory is an extraordinary cohomology theory (satisfies all the axioms of cohomology theories save the dimension axiom). -
Journal of Pure and Applied Algebra Adams Operations and Λ-Operations
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Journal of Pure and Applied Algebra 213 (2009) 409–420 Contents lists available at ScienceDirect Journal of Pure and Applied Algebra journal homepage: www.elsevier.com/locate/jpaa Adams operations and λ-operations on classifying oriented cohomology theories José Malagón-López Department of Mathematics, University of Western Ontario, London, Ontario N6A 5B7, Canada article info a b s t r a c t Article history: Adams operations on algebraic cobordism with rational coefficients are defined and shown Received 19 October 2007 to descend to the oriented cohomology theories with rational coefficients which are Received in revised form 21 June 2008 universal with respect to their group law. With the induced structure of special λ-ring Available online 30 August 2008 ∗ we show that we can regard the γ -filtration on CH as a deformation of the classical γ - Communicated by C.A. Weibel Q filtration on K0 . Q MSC: ' 2008 Elsevier B.V. All rights reserved. 14F43 14C15 19A99 1. Introduction In [6] Levine and Morel introduced the notion of an oriented cohomology theory (OCT) on the category of smooth quasi- projective varieties over a field k. An important feature of these theories is the existence of a formal group law describing the behaviour of the first Chern class with respect to the tensor product of line bundles. When char.k/ D 0, in [6] the theory X 7! Ω∗.X/, called algebraic cobordism, is constructed as the universal OCT in the sense that for any such theory A∗, there is a unique map Ω∗ ! A∗ of OCTs so that the induced map on the coefficient rings is precisely the map classifying the ∗ ∗ formal group law of A . -
Something on Spin Structures Sven-S. Porst
something on spin structures sven-s. porst∗ spring abstract This will give a brief introduction to spin structures on vector bundles to pave the way for the definition and introduction of Dirac operators. The presentation is mainly a brief summary of that given in [1]. principal G-bundles definition Let M be a manifold, π : P → M be a bundle over M and G be a Lie group. If there is a right action of G on P preserving fibres and acting freely on each fibre, π : P → M is called a principal G-bundle. In particular, a principal G-bundle is locally of the form U × G → U. equivalence Given two principal G-bundles π : P → M and π0 : P 0 → M over the same base space M, we say that these ϕ P / P 0 bundles are called equivalent if there exists a diffeo- AA | 0 0 AA || morphism ϕ : P → P such that π = π ϕ (a bundle AA || π AA || π0 isomorphism) that is compatible with the group ac- A |~ | tion, i.e. ϕ(x.g) = ϕ(x).g for all x ∈ M and g ∈ G. M This gives an equivalence relation on the set of principal G-bundles over M and the set of equivalence classes will be denoted PrinG(M). example: covering spaces Let π : M˜ → M be a normal covering space, i.e. the group G(M) of deck transformations acts transitively on each π−1(x). This is a principal G(M)-bundle where G(M) is equipped with the discrete topology.