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Spectral Projections and Paley–Wiener Theorem for the Unit Ball in \(\mathbb {C}^{n}\)

  • Noureddine Imesmad

摘要

For \(\nu \in \mathbb {R}\) ν R , we consider the invariant Laplacians \(\Delta _{\nu }\) Δ ν in the unit complex ball    \({\mathcal {B}}^{n}=(SU(n,1)/S(U(n)\times U(1))\) B n = ( S U ( n , 1 ) / S ( U ( n ) × U ( 1 ) ) \(\begin{aligned} \Delta _{\nu }= & {} 4(1-|z|^{2})\Bigg \{\sum _{i,j=1}^{n}(\delta _{ij}-z_{i}\bar{z_{j}})\dfrac{\partial ^{2}}{\partial z_{i}\partial \bar{z_{j}}}-\frac{\nu }{2}\sum _{j=1}^{n}z_{j}\dfrac{\partial }{\partial z_{j}}+\frac{\nu }{2}\sum _{j=1}^{n}\bar{z_{j}}\dfrac{\partial }{\partial \bar{z_{j}}}+\frac{\nu ^2}{4}\Bigg \} \end{aligned}\) Δ ν = 4 ( 1 - | z | 2 ) { i , j = 1 n ( δ ij - z i z j ¯ ) 2 z i z j ¯ - ν 2 j = 1 n z j z j + ν 2 j = 1 n z j ¯ z j ¯ + ν 2 4 } and the spectral projectors \({\mathcal {Q}}_{\lambda ,\nu }\) Q λ , ν associated to \(\Delta _{\nu }\) Δ ν defined by \(\begin{aligned} {\mathcal {Q}}_{\lambda ,\nu }f= & {} |{\textbf{c}}_{\nu }(\lambda )|^{-2}f*\varphi _{\lambda ,\nu }(z), \end{aligned}\) Q λ , ν f = | c ν ( λ ) | - 2 f φ λ , ν ( z ) , where \(\varphi _{\lambda ,\nu }\) φ λ , ν is the \(S(U(n)\times U(1))\) S ( U ( n ) × U ( 1 ) ) -invariant eigenfunction of \(\Delta _{\nu }\) Δ ν and \({\textbf{c}}_{\nu }(\lambda )\) c ν ( λ ) the Harish-Chandra function. The goal of this paper is to give an image characterization of \({\mathcal {Q}}_{\lambda ,\nu }\) Q λ , ν of \({\mathcal {C}}_{c}^{\infty }({\mathcal {B}}^{n})\) C c ( B n ) and \(L^{2}({\mathcal {B}}^{n},(1-|z|^2)^{-n-1}dm(z))\) L 2 ( B n , ( 1 - | z | 2 ) - n - 1 d m ( z ) ) .