Geometric Structure for the Principal Series of a Split Reductive P-Adic Group with Connected Centre

Total Page:16

File Type:pdf, Size:1020Kb

Geometric Structure for the Principal Series of a Split Reductive P-Adic Group with Connected Centre Geometric structure for the principal series of a split reductive p-adic group with connected centre Aubert, Anne-Marie and Baum, Paul and Plymen, Roger and Solleveld, Maarten 2015 MIMS EPrint: 2015.77 Manchester Institute for Mathematical Sciences School of Mathematics The University of Manchester Reports available from: http://eprints.maths.manchester.ac.uk/ And by contacting: The MIMS Secretary School of Mathematics The University of Manchester Manchester, M13 9PL, UK ISSN 1749-9097 GEOMETRIC STRUCTURE FOR THE PRINCIPAL SERIES OF A SPLIT REDUCTIVE p-ADIC GROUP WITH CONNECTED CENTRE ANNE-MARIE AUBERT, PAUL BAUM, ROGER PLYMEN, AND MAARTEN SOLLEVELD Abstract. Let G be a split reductive p-adic group with connected cen- tre. We show that each Bernstein block in the principal series of G admits a definite geometric structure, namely that of an extended quo- tient. For the Iwahori-spherical block, this extended quotient has the form T ==W where T is a maximal torus in the Langlands dual group of G and W is the Weyl group of G. Contents 1. Introduction 1 2. Extended quotient 3 3. The group W s as a Weyl group 4 4. Comparison of different parameters 5 4.1. Varieties of Borel subgroups 5 4.2. Enhanced Langlands parameters 7 4.3. Affine Springer parameters 8 5. Structure theorem 10 6. Correcting cocharacters and L-packets 13 References 15 1. Introduction Let G be a split reductive p-adic group with connected centre, and let G = G_ denote the Langlands dual group. Then G is a complex reductive group. Let T be a maximal torus in G and let W be the common Weyl group of G and G. We can form the quotient variety T=W and, familiar from noncommutative geometry [Kha, p.77], the noncommu- tative quotient algebra O(T ) o W: Date: August 1, 2015. 2010 Mathematics Subject Classification. 20G05, 22E50. Key words and phrases. reductive p-adic group, representation theory, geometric struc- ture, local Langlands conjecture. The second author was partially supported by NSF grant DMS-0701184. 1 2 A.-M. AUBERT, P. BAUM, R. PLYMEN, AND M. SOLLEVELD Within periodic cyclic homology (a noncommutative version of de Rham theory) there is a canonical isomorphism ∗ HP∗(O(T ) o W ) ' H (T ==W ; C) where T ==W denotes the extended quotient of T by W , see x2. In this sense, the extended quotient T ==W , a complex algebraic variety, is a more concrete version of the noncommutative quotient algebra O(T ) o W . Returning to the p-adic group G, let Irr(G)i denote the subset of the smooth dual Irr(G) comprising all the irreducible smooth Iwahori-spherical representations of G. We prove in this article that there is a continuous bijective map, satisfying several constraints, as follows: T ==W ' Irr(G)i: We note that there is nothing in the classical representation theory of G to indicate that Irr(G)i admits such a geometric structure. Nevertheless, such a structure was conjectured by the present authors in [ABPS], and so this article is a confirmation of that conjecture, for the single point i in the Bernstein spectrum of G. We prove, more generally, that, subject to constraints itemized in [ABPS], and subject to the Condition 3.1 on the residual characteristic, there is a continuous bijective map T s==W s ' Irr(G)s for each point s in the Bernstein spectrum for the principal series of G, see Theorem 5.2. Here, T s and W s are the complex torus and the finite group attached to s. This, too, is a confirmation of the geometric conjecture in [ABPS]. Let WF denote the Weil group of F . A Langlands parameter Φ for the principal series of G should have Φ(WF ) contained in a maximal torus of G. In particular, it should suffice to consider parameters Φ such that Φ WF ab ∼ × factors through WF = F , that is, such that Φ factors as follows: × Φ: WF × SL2(C) ! F × SL2(C) ! G: Such a parameter is enhanced in the following way. Let ρ be an irreducible representation of the component group of the centralizer of the image of Φ: ρ 2 Irr π0(ZG(im Φ)): The pair (Φ; ρ) will be called an enhanced Langlands parameter. We rely on Reeder's classification of the constituents of a given principal series representation of G, see [Ree, Theorem 1, p.101-102]. Reeder's the- orem amounts to a local Langlands correspondence for the principal series of G. Reeder uses only enhanced Langlands parameters with a particular geometric origin, namely those which occur in the homology of a certain variety of Borel subgroups of G. This condition is essential, see, for exam- ple, the discussion, in [ABP2], of the Iwahori-spherical representations of the exceptional group G2. In Theorem 4.7 we show how to replace the enhanced Langlands param- eters of this kind, namely those of geometric origin, by the affine Springer GEOMETRIC STRUCTURE 3 parameters defined in x4.3. These affine Springer parameters are defined in terms of data attached to the complex reductive group G { in this sense, the affine Springer parameters are independent of the cardinality q of the residue field of F . The scene is now set for us to prove the first theorem of geometric structure, namely Theorem 5.1, from which our main structure theorem, Theorem 5.2 follows. We also relate our basic structure theorem with L-packets in the principal series of G, see Theorem 6.2. An earlier, less precise version of our conjecture was formulated in [ABP1]. That version was proven in [Sol1] for Bernstein components which are de- scribed nicely by affine Hecke algebras. These include the principal series of split groups (with possibly disconnected centre), symplectic and orthogonal groups and also inner forms of GLn. Acknowledgements. Thanks to Mark Reeder for drawing our attention to the article of Kato [Kat]. We thank Joseph Bernstein, David Kazhdan, George Lusztig, and David Vogan for enlightening comments and discus- sions. 2. Extended quotient Let Γ be a finite group acting on a complex affine variety X by automor- phisms, Γ × X ! X: The quotient variety X=Γ is obtained by collapsing each orbit to a point. For x 2 X; Γx denotes the stabilizer group of x: Γx = fγ 2 Γ: γx = xg: Let c(Γx) denote the set of conjugacy classes of Γx. The extended quotient is obtained from X=Γ by replacing the orbit of x by c(Γx). This is done as follows: Set Xe = f(γ; x) 2 Γ × X : γx = xg. It is an affine variety and a subvariety of Γ × X. The group Γ acts on Xe: Γ × Xe ! Xe α(γ; x) = (αγα−1; αx); α 2 Γ; (γ; x) 2 X:e The extended quotient, denoted X==Γ, is X=e Γ. Thus the extended quotient X==Γ is the usual quotient for the action of Γ on Xe. The projection Xe ! X; (γ; x) 7! x is Γ-equivariant and so passes to quotient spaces to give a morphism of affine varieties ρ: X==Γ ! X=Γ: This map will be referred to as the projection of the extended quotient onto the ordinary quotient. The inclusion X,! Xe x 7! (e; x) e = identity element of Γ 4 A.-M. AUBERT, P. BAUM, R. PLYMEN, AND M. SOLLEVELD is Γ-equivariant and so passes to quotient spaces to give an inclusion of affine varieties X=Γ ,! X==Γ. This article will be dominated by extended quotients of the form T ==W or, more generally, extended quotients of the form T s==W s. 3. The group W s as a Weyl group Let G be a connected reductive p-adic group over F , which is F -split and has connected centre. Let T be a F -split maximal torus in G. Let G, T denote the Langlands dual groups of G, T . The principal series consists of all G-representations that are obtained with parabolic induction from characters of T . We will suppose that the residual characteristic p of F satisfies the hypothesis in [Roc, p. 379], for all reductive subgroups H ⊂ G containing T : Condition 3.1. If the root system R(H; T ) is irreducible, then the restric- tion on the residual characteristic p of F is as follows: • for type An p > n + 1 • for types Bn;Cn;Dn p 6= 2 • for type F4 p 6= 2; 3 • for types G2;E6 p 6= 2; 3; 5 • for types E7;E8 p 6= 2; 3; 5; 7: If R(H; T ) is reducible, one excludes primes attached to each of its irreducible factors. Since R(H; T ) is a subset of R(G; T ) =∼ R(G; T )_, these conditions are fulfilled when they hold for R(G; T ). We denote the collection of all Bernstein components of G of the form s = [T ; χ]G by B(G; T ) and call these the Bernstein components in the principal series. The union [ Irr(G; T ) := Irr(G)s s2B(G;T ) is by definition the set of all irreducible subquotients of principal series representations of G. Choose a uniformizer $F 2 F . There is a bijection t 7! ν between points in T and unramified characters of T , determined by the relation ν(λ($F )) = λ(t) ∗ [T ,χ] where λ 2 X∗(T ) = X (T ). The space Irr(T ) T is in bijection with T via t 7! ν 7! χ⊗ν. Hence Bernstein's torus T s is isomorphic to T .
Recommended publications
  • Shtukas for Reductive Groups and Langlands Correspondence for Functions Fields
    SHTUKAS FOR REDUCTIVE GROUPS AND LANGLANDS CORRESPONDENCE FOR FUNCTIONS FIELDS VINCENT LAFFORGUE This text gives an introduction to the Langlands correspondence for function fields and in particular to some recent works in this subject. We begin with a short historical account (all notions used below are recalled in the text). The Langlands correspondence [49] is a conjecture of utmost impor- tance, concerning global fields, i.e. number fields and function fields. Many excellent surveys are available, for example [39, 14, 13, 79, 31, 5]. The Langlands correspondence belongs to a huge system of conjectures (Langlands functoriality, Grothendieck’s vision of motives, special val- ues of L-functions, Ramanujan-Petersson conjecture, generalized Rie- mann hypothesis). This system has a remarkable deepness and logical coherence and many cases of these conjectures have already been es- tablished. Moreover the Langlands correspondence over function fields admits a geometrization, the “geometric Langlands program”, which is related to conformal field theory in Theoretical Physics. Let G be a connected reductive group over a global field F . For the sake of simplicity we assume G is split. The Langlands correspondence relates two fundamental objects, of very different nature, whose definition will be recalled later, • the automorphic forms for G, • the global Langlands parameters , i.e. the conjugacy classes of morphisms from the Galois group Gal(F =F ) to the Langlands b dual group G(Q`). b For G = GL1 we have G = GL1 and this is class field theory, which describes the abelianization of Gal(F =F ) (one particular case of it for Q is the law of quadratic reciprocity, which dates back to Euler, Legendre and Gauss).
    [Show full text]
  • Contents 1 Root Systems
    Stefan Dawydiak February 19, 2021 Marginalia about roots These notes are an attempt to maintain a overview collection of facts about and relationships between some situations in which root systems and root data appear. They also serve to track some common identifications and choices. The references include some helpful lecture notes with more examples. The author of these notes learned this material from courses taught by Zinovy Reichstein, Joel Kam- nitzer, James Arthur, and Florian Herzig, as well as many student talks, and lecture notes by Ivan Loseu. These notes are simply collected marginalia for those references. Any errors introduced, especially of viewpoint, are the author's own. The author of these notes would be grateful for their communication to [email protected]. Contents 1 Root systems 1 1.1 Root space decomposition . .2 1.2 Roots, coroots, and reflections . .3 1.2.1 Abstract root systems . .7 1.2.2 Coroots, fundamental weights and Cartan matrices . .7 1.2.3 Roots vs weights . .9 1.2.4 Roots at the group level . .9 1.3 The Weyl group . 10 1.3.1 Weyl Chambers . 11 1.3.2 The Weyl group as a subquotient for compact Lie groups . 13 1.3.3 The Weyl group as a subquotient for noncompact Lie groups . 13 2 Root data 16 2.1 Root data . 16 2.2 The Langlands dual group . 17 2.3 The flag variety . 18 2.3.1 Bruhat decomposition revisited . 18 2.3.2 Schubert cells . 19 3 Adelic groups 20 3.1 Weyl sets . 20 References 21 1 Root systems The following examples are taken mostly from [8] where they are stated without most of the calculations.
    [Show full text]
  • Geometric Structure in Smooth Dual and Local Langlands Conjecture
    GEOMETRIC STRUCTURE IN SMOOTH DUAL AND LOCAL LANGLANDS CONJECTURE ANNE-MARIE AUBERT, PAUL BAUM, ROGER PLYMEN, AND MAARTEN SOLLEVELD Contents 1. Introduction1 2. p-adic Fields2 3. The Weil Group5 4. Local Class Field Theory5 5. Reductive p-adic Groups6 6. The Smooth Dual7 7. Split Reductive p-adic Groups8 8. The Local Langlands Conjecture9 9. The Hecke Algebra { Bernstein Components 12 10. Cuspidal Support Map { Tempered Dual 14 11. Extended Quotient 15 12. Approximate Statement of the ABPS conjecture 16 13. Extended quotient of the second kind 16 14. Comparison of the two extended quotients 18 15. Statement of the ABPS conjecture 19 16. Two Theorems 23 17. Appendix : Geometric Equivalence 25 17.1. k-algebras 26 17.2. Spectrum preserving morphisms of k-algebras 27 17.3. Algebraic variation of k-structure 28 17.4. Definition and examples 28 References 30 1. Introduction The subject of this article is related to several branches of mathematics: number theory, representation theory, algebraic geometry, and non-commutative geometry. We start with a review of basic notions of number theory: p-adic field, the Weil group of a p-adic field, and local class field theory (sections 2-4). In sections 5, 6, 7, we recall some features of the theory of algebraic groups over p-adic fields and of their representations. In particular, we introduce the smooth dual Irr(G) of a reductive group G over a p-adic field F . The smooth dual Irr(G) is the set of equivalence classes of irreducible smooth representations of G, and is the main Paul Baum was partially supported by NSF grant DMS-0701184.
    [Show full text]
  • The Langlands Dual Group and Electric-Magnetic Duality
    The Langlands dual group and Electric-Magnetic Duality Aswin Balasubramanian DESY (Theory) & U. Hamburg (Dept. of Math) Nov 10, 2015 DESY Fellows Meeting Aswin Balasubramanian The Langlands dual group and Electric-Magnetic Duality I will provide the motivation by answering a specific question : How does the Langlands Dual Group enter physics and what new things can we learn from its appearance ? Talk is mostly motivational and historical in nature. Outline My hope is to answer the question : Why should physicists pay attention to aspects of Langlands Duality ? Aswin Balasubramanian The Langlands dual group and Electric-Magnetic Duality Talk is mostly motivational and historical in nature. Outline My hope is to answer the question : Why should physicists pay attention to aspects of Langlands Duality ? I will provide the motivation by answering a specific question : How does the Langlands Dual Group enter physics and what new things can we learn from its appearance ? Aswin Balasubramanian The Langlands dual group and Electric-Magnetic Duality Outline My hope is to answer the question : Why should physicists pay attention to aspects of Langlands Duality ? I will provide the motivation by answering a specific question : How does the Langlands Dual Group enter physics and what new things can we learn from its appearance ? Talk is mostly motivational and historical in nature. Aswin Balasubramanian The Langlands dual group and Electric-Magnetic Duality Does this extend to a quantum duality ? Not immediately, since U(1) gauge theories by themselves are not well defined(\not UV complete"). But, you could embed the U(1) theory in a non abelian gauge theory.
    [Show full text]
  • Parameters and Duality for the Metaplectic Geometric Langlands Theory
    PARAMETERS AND DUALITY FOR THE METAPLECTIC GEOMETRIC LANGLANDS THEORY D. GAITSGORY AND S. LYSENKO For Sasha Beilinson Abstract. This is a corrected version of the paper, and it differs substantially from the original one. We introduce the space of parameters for the metaplectic Langlands theory as factorization gerbes on the affine Grassmannian, and develop metaplectic Langlands duality in the incarnation of the metaplectic geometric Satake functor. We formulate a conjecture in the context of the global metaplectic Langlands theory, which is a metaplectic version of the \vanishing theorem" of [Ga5, Theorem 4.5.2]. Introduction 0.1. What is this paper about? The goal of this paper is to provide a summary of the metaplectic Langlands theory. Our main objectives are: {Description of the set (rather, space) of parameters for the metaplectic Langlands theory; {Construction of the metaplectic Langlands dual (see Sect. 0.1.6 for what we mean by this); {The statement of the metaplectic geometric Satake. 0.1.1. The metaplectic setting. Let F be a local field and G an algebraic group over F. The classical representation theory of locally compact groups studies (smooth) representations of the group G(F) on vector spaces over another field E. Suppose now that we are given a central extension (0.1) 1 ! E× ! G^(F) ! G(F) ! 1: We can then study representations of G^(F) on which the central E× acts by the tautological char- acter. We will refer to (0.1) as a local metaplectic extension of G(F), and to the above category of representations as metaplectic representations of G(F) corresponding to the extension (0.1).
    [Show full text]
  • Betti Geometric Langlands
    BETTI GEOMETRIC LANGLANDS DAVID BEN-ZVI AND DAVID NADLER Abstract. We introduce and survey a Betti form of the geometric Langlands conjecture, parallel to the de Rham form developed by Beilinson-Drinfeld and Arinkin-Gaitsgory, and the Dolbeault form of Donagi-Pantev, and inspired by the work of Kapustin-Witten in supersymmetric gauge the- ory. The conjecture proposes an automorphic category associated to a compact Riemann surface X and complex reductive group G is equivalent to a spectral category associated to the underly- ing topological surface S and Langlands dual group G∨. The automorphic category consists of suitable C-sheaves on the moduli stack BunG(X) of G-bundles on X, while the spectral category ∨ consists of suitable O-modules on the character stack LocG∨ (S) of G -local systems on S. The conjecture is compatible with and constrained by the natural symmetries of both sides coming from modifications of bundles and local systems. On the one hand, cuspidal Hecke eigensheaves in the de Rham and Betti sense are expected to coincide, so that one can view the Betti conjecture as offering a different “integration measure” on the same fundamental objects. On the other hand, the Betti spectral categories are more explicit than their de Rham counterparts and one might hope the conjecture is less challenging. The Betti program also enjoys symmetries coming from topological field theory: it is expected to extend to an equivalence of four-dimensional topological field theories, and in particular, the conjecture for closed surfaces is expected to reduce to the case of the thrice-punctured sphere.
    [Show full text]
  • Langlands Program, Field Theory, and Mirror Symmetry
    Langlands Program, Field Theory, and Mirror Symmetry Kazuki Ikeda Department of Physics, Osaka University, Toyonaka, Osaka 560-0043, Japan [email protected] Abstract This article aims to give a self-contained introduction to the Langlands program in math and physics. Initially the Langlands correspondences are purely mathematical conjecture, however, recently there have been several related works from physics side. Giving some basic facts from mathematical side, we review those recent advances towards the Langlands program mostly from physical viewpoints, and see the physical geometric Langlands correspondence is indeed analogous to the picture we have in mathematics. Starting with N = 4 super Yang-Mills theory on a four-dimensional manifold, we claim that the geometrical Langlands duality is physically understandable via mirror symmetries between (electric and magnetic) branes associated with the boundaries of the manifold. Main references are [26, 55]. Contents 1 introduction 4 2 Langlands program in math 8 2.1 The Langlands conjecture over number fields . 8 2.1.1 Preliminaries . 8 2.1.2 Automorphic forms and Hecke operators on SL2(Z)............... 9 2.1.3 Congruence subgroup of SL2(Z) and Hecke operators . 12 2.1.4 Remarks on history . 13 2.1.5 Automorphic representation on GL2(AQ)..................... 16 2.1.6 Elliptic curves . 20 2.1.7 Galois representation . 25 2.2 The geometric Langlands Program . 29 2.2.1 Geometric interpretation of the Langlands program . 29 2.2.2 Flat bundles and local systems . 31 2.2.3 D-module . 33 2.2.4 Schubert variety . 35 2.2.5 More on Hecke operators .
    [Show full text]
  • Twisted Whittaker Models for Metaplectic Groups Sergey Lysenko
    Twisted Whittaker models for metaplectic groups Sergey Lysenko To cite this version: Sergey Lysenko. Twisted Whittaker models for metaplectic groups. Geometric And Functional Anal- ysis, 2017, 27 (2), pp.289-372. 10.1007/s00039-017-0403-1. hal-01227086v2 HAL Id: hal-01227086 https://hal.archives-ouvertes.fr/hal-01227086v2 Submitted on 9 Jun 2021 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Twisted Whittaker models for metaplectic groups Sergey Lysenko Geometric and Functional Analysis GAFA ISSN 1016-443X Geom. Funct. Anal. DOI 10.1007/s00039-017-0403-1 1 23 Your article is protected by copyright and all rights are held exclusively by Springer International Publishing. This e-offprint is for personal use only and shall not be self- archived in electronic repositories. If you wish to self-archive your article, please use the accepted manuscript version for posting on your own website. You may further deposit the accepted manuscript version in any repository, provided it is only made publicly available 12 months after official publication or later and provided acknowledgement is given to the original source of publication and a link is inserted to the published article on Springer's website.
    [Show full text]
  • Bourbaki-Gauge.Pdf
    S´eminaire BOURBAKI Juin 2009 61`eme ann´ee, 2008-2009, no 1010 GAUGE THEORY AND LANGLANDS DUALITY by Edward FRENKEL INTRODUCTION In the late 1960s Robert Langlands launched what has become known as the Lang- lands Program with the ambitious goal of relating deep questions in Number Theory to Harmonic Analysis [L]. In particular, Langlands conjectured that Galois represen- tations and motives can be described in terms of the more tangible data of automor- phic representations. A striking application of this general principle is the celebrated Shimura–Taniyama–Weil conjecture (which implies Fermat’s Last Theorem), proved by A. Wiles and others, which says that information about Galois representations associ- ated to elliptic curves over Q is encoded in the Fourier expansion of certain modular forms on the upper-half plane. One of the most fascinating and mysterious aspects of the Langlands Program is the appearance of the Langlands dual group. Given a reductive algebraic group G, one constructs its Langlands dual LG by applying an involution to its root data. Under the Langlands correspondence, automorphic representations of the group G correspond to Galois representations with values in LG. Surprisingly, the Langlands dual group also appears in Quantum Physics in what looks like an entirely different context; namely, the electro-magnetic duality. Looking at the Maxwell equations describing the classical electromagnetism, one quickly notices that they are invariant under the exchange of the electric and magnetic fields. It is natural to ask whether this duality exists at the quantum level. In quantum theory there is an important parameter, the electric charge e.
    [Show full text]
  • Arxiv:Math/0201073V6 [Math.RT] 11 Feb 2020 ..Mndoyad”Ihs Egt Ros Hrceiainof Characterization Arrows: Weight” ”Highest and Monodromy 3.3
    PERVERSE SHEAVES ON AFFINE FLAGS AND LANGLANDS DUAL GROUP SERGEY ARKHIPOV AND ROMAN BEZRUKAVNIKOV Though he goeth on his way weeping that beareth the measure of seed, he shall come home with joy, bearing his sheaves. Psalm 126 ”Shir ha-maalot” (Song of Ascendance) Contents 1. Introduction 2 1.1. Basic notations and motivation 2 1.2. More notations 5 1.3. The monoidal functor 5 1.4. Compatibility with Frobenius 6 1.5. Anti-spherical quotient category 6 1.6. Iwahori-Whittaker category 6 2. Comparisonofanti-sphericalandWhittakercategories 7 3. Construction of the monoidal functor F 10 3.1. Plan of the construction 10 3.2. Central and Wakimoto sheaves: definition of the functor F¯ 11 3.3. Monodromy and ”highest weight” arrows: characterization of the functor F˜ 12 3.4. Tannakian and Drinfeld-Plucker formalism 13 3.5. Proof of Proposition 1 15 arXiv:math/0201073v6 [math.RT] 11 Feb 2020 3.6. Filtration of central sheaves by Wakimoto sheaves 16 3.7. Factoring F˜ to F 21 4. Proof of Theorem 1 23 4.1. Intermediate statements 23 4.2. Proof of Theorem 3 23 4.3. Proof of Proposition 8: category P0 and the regular orbit 24 4.4. Proof of Proposition 7 26 4.5. Proof of Theorem 2 29 4.6. Application: Whittaker integrals of central sheaves 29 5. Appendix 30 5.1. Sketch of proof of Theorem 5 30 5.2. Sketch of proof of Theorem 8 31 1 2 SERGEYARKHIPOVANDROMANBEZRUKAVNIKOV References 32 Abstract. This is the first in a series of papers devoted to describing the category of sheaves on the affine flag manifold of a simple algebraic group in terms of the Langlands dual group.
    [Show full text]
  • Integral Homology of Loop Groups Via Langlands Dual Groups
    REPRESENTATION THEORY An Electronic Journal of the American Mathematical Society Volume 15, Pages 347–369 (April 20, 2011) S 1088-4165(2011)00399-X INTEGRAL HOMOLOGY OF LOOP GROUPS VIA LANGLANDS DUAL GROUPS ZHIWEI YUN AND XINWEN ZHU Abstract. Let K be a connected compact Lie group, and G its complexifi- cation. The homology of the based loop group ΩK with integer coefficients is naturally a Z-Hopf algebra. After possibly inverting 2 or 3, we identify Z ∨ ∨ H∗(ΩK, ) with the Hopf algebra of algebraic functions on Be ,whereB is ∨ ∨ a Borel subgroup of the Langlands dual group scheme G of G and Be is the centralizer in B∨ of a regular nilpotent element e ∈ Lie B∨. We also give a similar interpretation for the equivariant homology of ΩK under the maximal torus action. 1. Introduction Let K be a connected compact Lie group and G its complexification. Let ΩK be the based loop space of K. Then the homology H∗(ΩK, Z) is a Hopf algebra over Z. The goal of this paper is to describe this Hopf algebra canonically in terms of the Langlands dual group of G. The rational (co)homology of ΩK is easy since rationally K is the product of spheres. However, the integral (co)homology is much more subtle: H∗(ΩK, Z) is not a finitely generated Z-algebra, and the simplest example H∗(Ω SU(2), Z) involves divided power structures. The integral (co)homology of ΩK has been studied extensively by different methods. The first method was pioneered by Bott (cf.
    [Show full text]
  • Arxiv:1803.03791V1 [Math.AG]
    SHTUKAS FOR REDUCTIVE GROUPS AND LANGLANDS CORRESPONDENCE FOR FUNCTION FIELDS VINCENT LAFFORGUE This text gives an introduction to the Langlands correspondence for function fields and in particular to some recent works in this subject. We begin with a short historical account (all notions used below are recalled in the text). The Langlands correspondence [Lan70] is a conjecture of utmost importance, concerning global fields, i.e. number fields and function fields. Many excellent surveys are available, for example [Gel84, Bum97, BeGe03, Tay04, Fre07, Art14]. The Langlands correspondence belongs to a huge system of conjectures (Lang- lands functoriality, Grothendieck’s vision of motives, special values of L-functions, Ramanujan-Petersson conjecture, generalized Riemann hypothesis). This system has a remarkable deepness and logical coherence and many cases of these con- jectures have already been established. Moreover the Langlands correspondence over function fields admits a geometrization, the “geometric Langlands program”, which is related to conformal field theory in Theoretical Physics. Let G be a connected reductive group over a global field F . For the sake of simplicity we assume G is split. The Langlands correspondence relates two fundamental objects, of very differ- ent nature, whose definition will be recalled later, • the automorphic forms for G, • the global Langlands parameters , i.e. the conjugacy classes of morphisms from the Galois group Gal(F /F ) to the Langlands dual group G(Qℓ). b For G = GL1 we have G = GL1 and this is class field theory, which describes the abelianization of Gal(Fb /F ) (one particular case of it for Q is the law of quadratic reciprocity, which dates back to Euler, Legendre and Gauss).
    [Show full text]