Definition The group of unitary operators $u(\theta)$ on $L^2(\mathbb R^3)$ given by $(u(\theta)\Phi)(r) =\Phi(\theta) \equiv e^{\frac{3\theta}{2}}\Phi(e^\theta r)$ is called the group of dilation operators on $\mathbb R^3.$
Let $H$ be a compact operator and $R(z) \equiv(H-z)^{-1}$ the resolvent. Define $R(z,\theta)$ by $R(z,\theta) \equiv u(\theta)R(z)u(\theta)^{-1}$. Let us define also $\mathcal O \equiv \{\theta \in \mathbb C: (u(\theta)\Phi)(r)$ for $\theta \in \mathbb R$ has an analytic continuation $ \}$
In this article A Class of Analytic Perturbations for One-body Schrδdinger Hamiltonians they were able to show that the function $\Psi_z(\theta)=(\phi(\theta) ,R(z,\theta)\phi(\theta))$ is meromorphic in $z$ for $z \in \mathcal C^{++} \equiv \{z \in \mathbb C : Im \ z > 0 ,\ Re \ z > 0 \} $ and $\theta \in \mathcal O^\epsilon \equiv \{\theta \in \mathcal O: Im \ \theta > \epsilon \}$
Now since for $\theta \in \mathbb R,\ u(\theta)$ is unitary we have that
$\Psi_z \equiv (\Phi,R(z)\Phi)=\Psi_z(\theta)$
from this they claim that $\Psi_z(\theta)$ that for fixed $z \in \mathcal C^{++}$ and $\theta \in \mathcal O^\epsilon$ the function $\Psi_z(\theta)$ is constant in $\theta$.
My question is why is $\Psi_z(\theta)$ constant for fixed $z \in \mathcal C^{++}$ and $\theta \in \mathcal O^\epsilon$ ?