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The generalization of Hardy uncertainty principle for the windowed Bochner–Fourier transform on the Heisenberg group is proved. We consider a Bochner measurable function Ψ : G → X {\Psi:G\to X} , where X is a completely separable Hilbert space X and Let G be a completely separable, unimodular, connected nilpotent Lie group. We establish that if ϕ ∈ C C ( G ) {\phi\in C_{C}(G)} is a non-trivial window function and Ψ ∈ L 2 ( G ) {\Psi\in L^{2}(G)} satisfies ∥ V ϕ ( Ψ ) ( g , χ ) ∥ HB ≤ c 2 ( g ) exp ( - β ∥ χ ∥ 2 ) \|V_{\phi}(\Psi)(g,\chi)\|_{\rm HB}\leq c_{2}(g)\exp(-\beta\|\chi\|^{2}) , β > 0 {\beta>0} , then Ψ = 0 {\Psi=0} almost everywhere.
The generalization of Hardy uncertainty principle for the windowed Bochner–Fourier transform on the Heisenberg group is proved. We consider a Bochner measurable function Ψ : G → X {\Psi:G\to X} , where X is a completely separable Hilbert space X and Let G be a completely separable, unimodular, connected nilpotent Lie group. We establish that if ϕ ∈ C C ( G ) {\phi\in C_{C}(G)} is a non-trivial window function and Ψ ∈ L 2 ( G ) {\Psi\in L^{2}(G)} satisfies ∥ V ϕ ( Ψ ) ( g , χ ) ∥ HB ≤ c 2 ( g ) exp ( - β ∥ χ ∥ 2 ) \|V_{\phi}(\Psi)(g,\chi)\|_{\rm HB}\leq c_{2}(g)\exp(-\beta\|\chi\|^{2}) , β > 0 {\beta>0} , then Ψ = 0 {\Psi=0} almost everywhere.
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