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Fourier and Helgason Fourier transforms for Vector Bundle-valued Differential Forms on Homogeneous Spaces

Olufemi O. Oyadare

Abstract

We employ the perspective of the functional equation satisfied by the classical Fourier transform to derive the Helgason Fourier transform map $Ω^{l}(G/K,W)\longrightarrowΩ^{k}(G/K\times G/P,V[χ]):f\longmapsto \widehat{f}:G/K\times G/P\mapsto V[χ]:(x,b)\longmapsto\widehat{f}(x,b)$ (for $W-$valued differential forms $f\in Ω^{l}(G/K,W)$) as the $G-$ invariant vector bundle-valued differential form $\widehat{f}$ on the product space $G/K\times G/P$ whose image under the vector bundle-valued Poisson transform is the fibre convolution-integral $\varphi^{U^{σ,ν}}_{τ,l,k}* f$ on $G/K,$ where $\varphi^{U^{σ,ν}}_{τ,l,k}$ is the $W-$valued $τ-$spherical $l-$form on $G/K.$ Explicitly, we prove that $$\widehat{f}_{l,k,\varepsilon(λ)}(x,b)=({\bf C_{o}λ)}^{-1}\circβ^{V}(λ))\circ(\int_{G/K}\varphi^{U^{σν},t}_{λ,l,k}\wedgeπ^{*}_{K}f)(x),$$ where $b\in G/P$ is a consequence of the boundary map $β^{V}(λ),$ ${\bf C_{o}(λ)}$ is the vector bundle-valued Harish-Chandra $c-$function and for some $λ-$linear relation, $\varepsilon(λ).$ The Fourier transform is found to be the map $Ω^{l}G/K,W)\longrightarrowΩ^{k}(G/K\times G/P,W)$ $:f\mapsto f^{\triangle}:$ $G/P\times G/K\longrightarrow W$ $:(b,x)\longmapsto f^{\triangle}(b,x)$ and is then established to be explicitly given as $f^{\triangle}_{l,k,\upsilon(λ)}(b,x)=$ $$\int_{G/P}φ_{k,l,λ}\wedgeπ^{*}_{P}(({\bf C_{o}(λ)}^{-1}\circβ^{V}λ))\circ(\int_{G/K}\varphi^{U^{σν},t}_{λ,l,k}\wedgeπ^{*}_{K}f)(x)),$$ where $\upsilon(λ)$ is some $λ-$linear relation.

Fourier and Helgason Fourier transforms for Vector Bundle-valued Differential Forms on Homogeneous Spaces

Abstract

We employ the perspective of the functional equation satisfied by the classical Fourier transform to derive the Helgason Fourier transform map (for valued differential forms ) as the invariant vector bundle-valued differential form on the product space whose image under the vector bundle-valued Poisson transform is the fibre convolution-integral on where is the valued spherical form on Explicitly, we prove that where is a consequence of the boundary map is the vector bundle-valued Harish-Chandra function and for some linear relation, The Fourier transform is found to be the map and is then established to be explicitly given as where is some linear relation.

Paper Structure

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