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Fourier expansion along geodesics on Riemann surfaces

Anton Deitmar (2014)

Open Mathematics

For an eigenfunction of the Laplacian on a hyperbolic Riemann surface, the coefficients of the Fourier expansion are described as intertwining functionals. All intertwiners are classified. A refined growth estimate for the coefficients is given and a summation formula is proved.

Functoriality and the Inverse Galois problem II: groups of type B n and G 2

Chandrashekhar Khare, Michael Larsen, Gordan Savin (2010)

Annales de la faculté des sciences de Toulouse Mathématiques

This paper contains an application of Langlands’ functoriality principle to the following classical problem: which finite groups, in particular which simple groups appear as Galois groups over ? Let be a prime and t a positive integer. We show that that the finite simple groups of Lie type B n ( k ) = 3 D S O 2 n + 1 ( 𝔽 k ) d e r if 3 , 5 ( mod 8 ) and G 2 ( k ) appear as Galois groups over , for some k divisible by t . In particular, for each of the two Lie types and fixed we construct infinitely many Galois groups but we do not have a precise control...

Geometric theta-lifting for the dual pair 𝕊𝕆 2 m , 𝕊 p 2 n

Sergey Lysenko (2011)

Annales scientifiques de l'École Normale Supérieure

Let X be a smooth projective curve over an algebraically closed field of characteristic  > 2 . Consider the dual pair H = SO 2 m , G = Sp 2 n over X with H split. Write Bun G and Bun H for the stacks of G -torsors and H -torsors on X . The theta-kernel Aut G , H on Bun G × Bun H yields theta-lifting functors F G : D ( Bun H ) D ( Bun G ) and F H : D ( Bun G ) D ( Bun H ) between the corresponding derived categories. We describe the relation of these functors with Hecke operators. In two particular cases these functors realize the geometric Langlands functoriality for the above pair (in the non ramified case)....

Induction automorphe globale pour les corps de nombres

Guy Henniart (2012)

Bulletin de la Société Mathématique de France

Soit F un corps de nombres et soit E une extension cyclique de F , de degré d . L’induction automorphe associe à une représentation automorphe cuspidale τ de GL m ( 𝔸 E ) une représentation automorphe π de GL m d ( 𝔸 F ) , induite de cuspidale. La représentation π est caractérisée par le fait qu’à presque toute place v de F , le facteur L ( π v , s ) est le produit des facteurs L ( τ w , s ) , w parcourant les places de E au–dessus de v . Par la correspondance conjecturale de Langlands, cette opération doit correspondre à l’induction, de E à F , des...

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