Abstract

Let (τ,Vτ)(τ,V_τ) be a spinor representation of Spin(n)\mathrm{Spin}(n) and let (σ,Vσ)(σ,V_σ) be a spinor representation of Spin(n−1)\mathrm{Spin}(n-1) that occurs in the restriction τ∣Spin(n−1)τ_{\mid \mathrm{Spin}(n-1)}. We consider the real hyperbolic space Hn(R)H^n(\mathbb R) as the rank one homogeneous space Spin0(1,n)/Spin(n)\mathrm{Spin}_0(1,n)/\mathrm{Spin}(n) and the spinor bundle ΣHn(R)ΣH^n(\mathbb R) over Hn(R)H^n(\mathbb R) as the homogeneous bundle Spin0(1,n)×Spin(n)Vτ\mathrm{Spin}_0(1,n)\times_{\mathrm{Spin}(n)} V_τ. Our aim is to characterize eigenspinors of the algebra of invariant differential operators acting on ΣHn(R)ΣH^n(\mathbb R) which can be written as the Poisson transform of LpL^p-sections of the bundle Spin(n)×Spin(n−1)Vσ\mathrm{Spin}(n)\times_{\mathrm{Spin}(n-1)} V_σ over the boundary Sn−1≃Spin(n)/Spin(n−1)S^{n-1}\simeq \mathrm{Spin}(n)/\mathrm{Spin}(n-1) of Hn(R)H^n(\mathbb R), for 1<p<∞1<p<\infty.

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