Local Langlands Correspondence and Weil Restriction (Joint Work with Roger Plymen)

Local Langlands Correspondence and Weil Restriction (Joint Work with Roger Plymen)

Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) Anne-Marie Aubert Institut de Math´ematiquesde Jussieu { Paris Rive Gauche C.N.R.S., Sorbonne Universit´e,et Universit´eParis Diderot 4 place Jussieu, 75005 Paris, France ALGEBRAIC AND ANALYTIC ASPECTS OF AUTOMORPHIC FORMS ICTS, Bangalore, India 25 February - 07 March, March 2019 Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 1 / 24 Ramification groups Let E=F be a finite and Galois extension extension of non-archimedean local fields, with degree denoted by d. Review of the ramification of the Galois group Γ = ΓE=F := Gal(E=F ) in the lower numbering : We have a decreasing sequence of normal subgroups of Γ : (∗) Γ = Γ−1 ⊇ Γ0 ⊇ Γ1 ⊇ Γ2 ⊇ · · · ⊇ Γi = Γi+1 = ··· = f1g where Γi is the group of elements in Γ acting trivially on the quotient of the ring of integers of E by the (i + 1)th power of its maximal ideal. If t is a real number ≥ −1, let Γt denote the ramification group Γi , where i is the smallest integer ≥ t. T We set Γt+ := t0>t Γt0 and we call t a break (or jump) of the filtration if Γt+ 6= Γt . Let b denote the largest ramification break in the filtration. Remark • E=F is unramified if and only if Γ0 = 1. In that case, b = −1. • E=F is tamely ramified if and only if Γ1 = 1. In that case, b = 0. Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 2 / 24 Properties of the Hasse-Herbrand function For t ≥ 0, we denote by (Γ0 :Γt ) the index of Γt in Γ0. For t 2 [−1; 0), we −1 set (Γ0 :Γt ) := (Γt :Γ0) . Let e = e(E=F ) denote the ramification index of E=F . The Hasse-Herbrand function 'E=F :[−1; 1) ! R is defined by Z u 1 'E=F (u) := dt: 0 (Γ0 :Γt ) It is continuous, piecewise linear, increasing and concave. Remark : Let the ramification breaks occur at b1, b2, :::, bk = b. We have b Z b 1 = dt e 0 (Γ0 : f1g) Z b1 1 Z b 1 = dt + ··· + dt 0 (Γ0 : f1g) bk−1 (Γ0 : f1g) Z b1 1 Z b 1 ≤ dt + ··· + dt 0 (Γ0 :Γb1 ) bk−1 (Γ0 :Γb) = 'E=F (b); Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 3 / 24 Properties of the Hasse-Herbrand function b so that 'E=F (b) − e ≥ 0, with equality if and only if b = 0. Proposition Let r > 0. Then we have b ' (er) = r + ' (b) − ≥ r; E=F E=F e where e = e(E=F ) denotes the ramification index of E=F . In particular, 'E=F (er) = r if and only if E=F is tamely ramified. Corollary We have ' (er) E=F ! 1 as r ! 1: r Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 4 / 24 Properties of the Hasse-Herbrand function For later use : Define an upper numbering on ramification groups by setting s Γ := Γt ; if s = 'E=F (t). Upper numbering behaves well with respect to quotients, i.e., if H is a normal subgroup of Γ, then (Γ=H)s = Γs H=H. The ramification in the upper numbering of the absolute Galois group ΓF := Gal(F =F ) is defined as follows : Γ(F )t := proj lim Gal(L=F )t with L running through the set of finite Galois extensions of F . The ramification in the upper numbering of the Weil group WF of F is then inherited from the ramification in the upper numbering of the absolute Galois group : t t WF ,! Γ(F ) : Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 5 / 24 Weil restriction Let X be an E-group scheme of finite type. The Weil restriction RE=F X is a finite type F -scheme satisfying the universal property : (RE=F X )(A) = X (E ⊗F A); for any F -algebra A. The Weil restriction exists as a F -scheme of finite type, and it has a natural F -group structure. Notation Let G be a split connected reductive group over E and let M := RE=F G. Let G _ be the Langlands dual group of G, that is, the complex Lie group with root system dual to that of G. Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 6 / 24 Weil restriction Examples _ G = GLn(C) if G = GLn(F ), _ _ G = PGLn(C) if G = SLn(F ) and G = SLn(C) if G = PGLn(F ), _ G = Sp2n(C) if G = SO2n+1(F ), _ G = SO2n+1(C) if G = Sp2n(F ), _ G = SO2n(C) if G = SO2n(F ). Next goal : to define the Langlands dual group M_ of M. Notation Let A be a group, A0 be a subgroup of A of finite index, and let D be an A0-module. Let D∗ be the group of maps f of A into D such that f (a0a) = a0f (a) for all a 2 A; a0 2 A0. Make D∗ into a A-module by setting ∗ A A (sf )a = f (as) with a; s 2 A. Write D = IndA0 (D) := IA0 (D). Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 7 / 24 Weil restriction Definition The Shapiro isomorphism is defined as follows : A0 1 ∗ 1 0 0 ShA : H (A; D ) ' H (A ; D); α 7! (θ ◦ α)jA ; ∗ where θ : D ! D is the morphism defined by θ(f ) = f (1A). Remark Let B be a group, µ: B ! A a homomorphism. Let B0 = µ−1(A0) and assume that µ induces a bijection B=B0 ! A=A0. Then f 7! µ ◦ f induces 0 A B an isomorphism µ : IA0 (D) ' IB0 (D). Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 8 / 24 Weil restriction The absolute Weil group WF of F It is a subgroup of the absolute Galois group Gal(F =F ). We have an exact sequence 1 ! IF ! Gal(F =F ) ! Gal(Fq=Fq) ! 1 where IF is the inertia group and Fq is the residual field of F . Q Then Gal(Fq=Fq) ' Zb = p Zp. WF is defined to be the inverse image of Z under Gal(F =F ) ! Gal(Fq=Fq). 0 0 Let WF denote the Weil-Deligne group of F defined as WF := WF n C with w · z = jjwjj · z for all w 2 WF ; z 2 C, where w acts on Fq as qjjwjj 0 x 7! x . Define similarly WE . Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 9 / 24 Weil restriction We will apply the previous Remark thrice. 0 0 0 0 0 • With A = WF , A = WE , B = WF , µ: WF ! WF then B = WE . The condition B=B0 ' A=A0 is satisfied. We infer that 0 WF _ WF _ Ind 0 G ' Ind G : WE WE 0 0 • With A = ΓF , A = ΓE , B = WF , µ: WF ! ΓF then B = WE . The condition B=B0 ' A=A0 is satisfied. We infer that IndWF G _ ' IndΓF G _: WE ΓE Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 10 / 24 Weil restriction 0 • With A = Gal(L=F ), A = Gal(L=E), B = ΓF , µ given by the projection 0 0 0 ΓF ! Gal(L=F ) then B = ΓE . The condition A=A ' B=B is satisfied. We infer that IndΓF G _ ' IndGal(L=F ) G _: ΓE Gal(L=E) Definition The common value will be denoted M_ : 0 _ WF _ WF _ ΓF _ Gal(L=F ) _ M := Ind G ' Ind 0 G ' Ind G ' Ind G : WE WE ΓE Gal(L=E) Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 11 / 24 Weil restriction Theorem [A-Plymen] 0 _ Assume that G = GLn and let λG : Irr G(E) ' Hom(WE ; G ) denote the LLC for G(E). 0 WF Set Sh := Sh 0 and let ι denote the natural bijection from Irr M(F ) to WE Irr G(E). Then −1 λM := Sh ◦ λG ◦ ι 1 0 _ defines a bijection from Irr M(F ) onto H (WF ; M ). The bijection λM should provide the LLC for M. When M is a torus, it is indeed the case (Langlands). Anne-Marie Aubert Local Langlands correspondence and Weil restriction (joint work with Roger Plymen) 12 / 24 The case of tori We will consider in this section the case n = 1, that is G = GL1. The × group GL1(E) = E = Gm is an affine algebraic variety with defining 2 × equation xy − 1 = 0 in affine space A . Upon restriction of scalars, E becomes a connected commutative algebraic group with defining equation 2d in the affine space A . This algebraic group M = RE=F Gm is a torus defined over F , called an induced torus. We have M(F ) = E ×. Theorem (Langlands) Let T be a torus defined over F . There is a unique family of homomorphisms × 1 _ λT : Hom(T(F ); C ) ! H (WF ; T ) with the following properties : (1) λT is additive functorial in T , i.e., it is a morphism between two additive functors from the category of tori over F to the category of abelian groups ; (2) For T = RE=F Gm where E=F is a finite separable extension, λT is the isomorphism described above.

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