Let L be the full laplacian on the Heisenberg group ${ℍ}^n$ of arbitrary dimension n. Then for $f\in L^2\left({ℍ}^n\right)$ such that ${(I-L)}^{s/2}f\in L^2\left({ℍ}^n\right)$, s > 3/4, for a $\varphi \in C_c\left({ℍ}^n\right)$ we have ${ʃ}_{{ℍ}^n}\left|\varphi \left(x\right)\right|su{p}_{0<t\le 1}{\left|e^{(\surd -1)tL}f\left(x\right)\right|}^{2}dx\le C_{\varphi }\parallel f{\parallel }_{W^s}^2$. On the other hand, the above maximal estimate fails for s < 1/4. If Δ is the sublaplacian on the Heisenberg group ${ℍ}^n$, then for every s < 1 there exists a sequence $f_n\in L^2\left({ℍ}^n\right)$ and $C_n>0$ such that ${(I-L)}^{s/2}{f}_n\in L^2\left({ℍ}^n\right)$ and for a $\varphi \in C_c\left({ℍ}^n\right)$ we have ${ʃ}_{{ℍ}^n}\left|\varphi \left(x\right)\right|su{p}_{0<t\le 1}{\left|e^{(\surd -1)t\Delta }{f}_n\left(x\right)\right|}^{2}dx\ge C_n\parallel f_n{\parallel }_{W^s}^2,li{m}_{n\to \infty }{C}_n=+\infty$.

Soient $F$ un corps local non archimédien, $N$ un entier $\ge 2$, $\underset{\_}{G}=GL\left(N\right)$, $n$ un entier $\ge 1$ et $\mathscr{H}\left(\underset{\_}{G}\right(F),K_F^n)$ l’algèbre de Hecke de $\underset{\_}{G}\left(F\right)$ relative au sous-groupe de congruence modulo ${𝒫}_F^n$ de $\underset{\_}{G}({𝒪}_F)$. On prouve une formule explicite pour les intégrales orbitales elliptiques des fonctions de $\mathscr{H}\left(\underset{\_}{G}\right(F),K_F^n)$. Grâce à cette formule, pour $\gamma \in \underset{\_}{G}\left(F\right)$ semi-simple régulier, on produit un entier $r=r(\gamma ,n)\ge n$ tel que pour tout corps local non archimédien $F^{\text{'}}$$r$-proche...

The purpose of this paper is to show how central extensions of (possibly infinite-dimensional) Lie algebras integrate to central extensions of étale Lie 2-groups in the sense of [Get09, Hen08]. In finite dimensions, central extensions of Lie algebras integrate to central extensions of Lie groups, a fact which is due to the vanishing of ${\pi }_2$ for each finite-dimensional Lie group. This fact was used by Cartan (in a slightly other guise) to construct the simply connected Lie group associated to each finite-dimensional...