I was dealing with a problem where a delta approximating function is given. Apart from the fact that this delta approximating functions has the form $$g_\epsilon(x) = \epsilon^{-3}g(\epsilon^{-1}x)\tag{1}$$ and that $g\in L^1(\mathbb{R}^3)\cap L^2(\mathbb{R}^3)$ with $\int g(x)\,\mathrm{d}^3x = 1$, no specific form of the $g_\epsilon$ is given. What i then was trying to evaluate is the integral $$\int g_\epsilon(x)f(x)\,\mathrm{d}^3x\tag{2}$$ for which i would imagine that $$\lim_{\epsilon\to 0}\int g_\epsilon(x)f(x)\,\mathrm{d}^3x = f(0)\tag{3}$$ but I'm not quite sure what to do with the integral $(2)$ which is what interests me.
What i can say about $(2)$? And, if there's one, what's an explicit form of that integral?
Maybe a bit of context could help. I'm trying to study the resolvent of an hamiltonian which contains a term $$\mu_\epsilon(g_\epsilon, \cdot)g_\epsilon\qquad \mu_\epsilon\in \mathbb{R}$$ and to do so i'm trying to find the action of the hamiltonian in Fourier space by computing the integral $$\mu_\epsilon\int(g_\epsilon, f)g_\epsilon(x)e^{-ikx}\,\mathrm{d}^3x = \int g_\epsilon(x) e^{-ikx}\,\mathrm{d}^3x\int \overline{g_\epsilon}(y)f(y)\,\mathrm{d}^3 y$$ where the second integral is what I'm trying to understand.
The integral in (2) is $\int_{\Bbb R^3}g(x)f(\epsilon y)\mathrm{d}^3y$. For sufficiently nice $f$ continuous at $0$ with finite $f(0)$, we can move a $\lim_{\epsilon\to0^+}$ operator inside the integral. This gives $\int_{\Bbb R^3}g(x)f(0)\mathrm{d}^3y=f(0)\int_{\Bbb R^3}g(x)\mathrm{d}^3y=f(0)$.