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Let $H_n$ be the (2n+1)-dimensional Heisenberg group, let p,q be two non-negative integers satisfying p+q=n and let G be the semidirect product of U(p,q) and $H_n$. So $L^2\left(H_n\right)$ has a natural structure of G-module. We obtain a decomposition of $L^2\left(H_n\right)$ as a direct integral of irreducible representations of G. On the other hand, we give an explicit description of the joint spectrum σ(L,iT) in $L^2\left(H_n\right)$ where $L={\sum }_{j=1}^p(X_j^2+Y_j^2)-{\sum }_{j=p+1}^n(X_j^2+Y_j^2)$, and where $X_1,Y_1,...,X_n,Y_n,T$ denotes the standard basis of the Lie algebra of $H_n$. Finally, we obtain a spectral characterization of the...

Let 𝓢(Hₙ) be the space of Schwartz functions on the Heisenberg group Hₙ. We define a spherical transform on 𝓢(Hₙ) associated to the action (by automorphisms) of U(p,q) on Hₙ, p + q = n. We determine its kernel and image and obtain an inversion formula analogous to the Godement-Plancherel formula.

Let Hₙ be the (2n+1)-dimensional Heisenberg group, let p,q ≥ 1 be integers satisfying p+q=n, and let $L={\sum }_{j=1}^p(X{²}_j+Y{²}_j)-{\sum }_{j=p+1}^n(X{²}_j+Y{²}_j)$, where X₁,Y₁,...,Xₙ,Yₙ,T denotes the standard basis of the Lie algebra of Hₙ. We compute explicitly a relative fundamental solution for L.

Let m: ℝ → ℝ be a function of bounded variation. We prove the $L^p\left(ℝ\right)$-boundedness, 1 < p < ∞, of the one-dimensional integral operator defined by $T_{m}f\left(x\right)=p.v.\int k(x-y)m(x+y)f\left(y\right)dy$ where $k\left(x\right)={\sum }_{j\in \mathbb{Z}}{2}^j{\phi }_j\left(2^{j}x\right)$ for a family of functions ${{\phi }_j}_{j\in \mathbb{Z}}$ satisfying conditions (1.1)-(1.3) given below.