Let $f \in L^2(\mathbb{R}, (1/\sqrt{2 \pi})\exp(-x^2/2))$ be such that $0 \leq f(x) \leq 1$. We know that the (normalized) Hermite polynomials are a complete orthonormal basis for this space. Therefore we let \begin{equation} f_n(x) = \sum_{i=0}^n \langle f, H_i\rangle\ H_i(x) = \sum_{i=0}^n c_i H_i(x), \end{equation} where \begin{equation} c_i = \langle f, H_i \rangle = \int H_i(x) f(x) \frac{1}{\sqrt{2 \pi}} \exp(-x^2/2)\ \mathrm{d} x = \int H_i(x) f(x)\ \phi(x) \mathrm{d} x, \end{equation} where $\phi(x) = (1/\sqrt{2 \pi}) \exp(-x^2/2)$. Consider now the integral \begin{equation} d_i = \int H_i(x) f(x)\ \phi(x-\mu) \mathrm{d} x \end{equation} $d_i$ is the Hermite coefficient with respect to a translated Gaussian.
Question: Is there an upper bound for $|c_i - d_i|$? Ideally it would be something in the form $|c_i - d_i| \leq A c_i$.
My guess would be that there should exist some fixed constant $A$ such that \begin{equation} |c_i - d_i| \leq A |c_i| \exp(\mu^2). \end{equation}
I know that this question could be formulated only in terms of integrals but I thought that providing more context could be helpful.
Any pointers to relevant literature are welcome.