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International Congress of Mathematicians

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Converse Theorems, Functoriality, and Applications 125H (A) to the appropriate GLjv(A). The first lifting that resulted from the combination<strong>of</strong> the Converse Theorem and the Langlands-Shahidi method <strong>of</strong> controllingautomorphic F-functions was the weak lift for generic cuspidal representations fromS0 2 „ + i to GL 2 „ over a number field k obtained with Kim and Shahidi [2]. We cannow extend this to the following result.Theorem. [2, 3] Let H be a split classical group over k as above and n aglobally generic cuspidal representation o/H(A). Then there exists an automorphicrepresentation n <strong>of</strong> GLJV (A) for the appropriate N such that n^ is the local Langlandslift <strong>of</strong> n v for all archimedean places v and almost all non-archimedean placesv where n v is unramified.In these examples the local Langlands correspondence is not understood at theplaces v where n v is ramified and so we must use the technique <strong>of</strong> multiplicativityand stability <strong>of</strong> the local 7-factors as outlined in Section 3. Multiplicativity hasbeen established in generality by Shahidi [19] and in our first paper [2] we reliedon the stability <strong>of</strong> 7-factors for S0 2 „ + i from [5]. Recently Shahidi has establishedan expression for his local coefficients as Mellin transforms <strong>of</strong> Bessel functions insome generality, and in particular in the cases at hand one can combine this withthe results <strong>of</strong> [5] to obtain the necessary stability in the other cases, leading to theextension <strong>of</strong> the lifting to the other split classical groups [3].2. Tensor products. Let H = GL ro x GL„. Then L H = GL ro (C) x GL„(C).Then there is a natural simple tensor product map from GL TO (C) x GL n (C) toGL TOn (C). The associated functoriality from GL„ x GL TO to GL TO „ is the tensorproduct lifting. Now the associated local lifting is understood in principle since thelocal Langlands conjecture for GL„ has been solved. The question <strong>of</strong> global functorialityhas been recently solved in the cases <strong>of</strong> GL 2 x GL 2 to GL 4 by Ramakrishnan[17] and GL 2 x GL 3 to GL 6 by Kim and Shahidi [15, 16].Theorem. [17, 15] Let m be a cuspidal representation o/GL 2 (A) and 7r 2 acuspidal representation o/GL 2 (A) (respectively GL 3 (A)J. Then there is an automorphicrepresentation II o/GL 4 (A) (respectively GL 6 (A)) such that Il v is the localtensor product lift <strong>of</strong> m, v x 7r 2jt , at all places v.In both cases the authors are able to characterize when the lift is cuspidal.In the case <strong>of</strong> Ramakrishnan [17] n = m x 7r 2 with each 7r, cuspidal representation<strong>of</strong> GL 2 (A) and II is to be an automorphic representation <strong>of</strong> GL 4 (A). Toapply the Converse Theorem Ramakrishnan needs to control the analytic properties<strong>of</strong> L(s,U x n') for n' cuspidal representations <strong>of</strong> GLi(A) and GL 2 (A), that is,the Rankin triple product F-functions L(s,II x n') = L(s,ni x 7r 2 x n'). This hewas able to do using a combination <strong>of</strong> results on the integral representation for thisF-function due to Garrett, Rallis and Piatetski-Shapiro, and Ikeda and the work <strong>of</strong>Shahidi on the Langlands-Shahidi method.In the case <strong>of</strong> Kim and Shahidi [15, 16] 7r 2 is a cuspidal representation <strong>of</strong>GL 3 (A). Since the lifted representation II is to be an automorphic representation<strong>of</strong> GL 6 (A), to apply the Converse Theorem they must control the analytic properties<strong>of</strong> L(s, II x n') = L(s, 7Ti x 7T 2 x n') where now n' must run over appropriate cuspidalrepresentations <strong>of</strong> GL TO (A) with m = 1,2,3,4. The control <strong>of</strong> these triple productsis an application <strong>of</strong> the Langlands-Shahidi method <strong>of</strong> analysing F-functions and

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