It is well known that,

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Theorem 1. For $f\in L^{2}(\mathbb H_{n}=\text{The Heisenberg group of dimesion } 2n+1)$ we have the expansion
$$f(z, s)= (2\pi)^{-n} \sum_{k=0}^{\infty} \int_{0}^{\infty}  f \ast e_{k}^{\lambda} (z, s)  |\lambda |^{n} d\lambda . $$;
where $\lambda \in \mathbb R^{\ast}$,$e_{k}^{\lambda}(z, s):= e^{i\lambda s}\phi_{k}(\sqrt{\mid \lambda \mid}z );$
where $\phi_{k}(z)= (2\pi)^{\frac {n}{2}} \sum_{|\alpha | = k} \Phi_{\alpha, \alpha}(z).$ and for each $\alpha, \beta \in \mathbb N^{n}$ and $z\in \mathbb C^{n}$, we define the special Hermite functions $\Phi_{\alpha, \beta }$ by
$$\Phi_{\alpha, \beta}(z):= (2\pi)^{-\frac{n}{2}} \int_{\mathbb R^{n}} e^{i x\cdot \xi}  \Phi_{\alpha}(\xi + \frac{y}{2}) \Phi_{\beta}(\xi- \frac{y}{2}) d\xi .$$

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Theorem 2. For $f\in L^{2}(\mathbb H_{n})$ we have
$$\parallel f \parallel_{2}^{2} = (2\pi)^{-n-1} \sum_{k=0}^{\infty} \int_{-\infty}^{\infty} \int_{\mathbb C^{n}} \mid f \ast e_{k}^{\lambda} (z, 0)\mid^{2}   \lambda ^{2n} dz  d\lambda . $$

\textbf{My question is}: Put $\eta= r+it, r>0$, and $ T_{\eta}f(z,s):= (2\pi)^{-n} \sum_{k=0}^{\infty} \int_{0}^{\infty} e^{-\eta(2k+n)|\lambda |}  f \ast e_{k}^{\lambda} (z, s)  |\lambda |^{n} d\lambda $.  Can we say this operator is bounded on $L^{2}(\mathbb H_{n})$, furthermore, on $L^{p}(\mathbb H_{n}), 1\leq p \leq \infty $ ?