In a physics problem I'm currently considering generating functions containing the term $1/\sqrt{t^2}$, where earlier in the derivation I have restricted my attention to the cases $\lvert xt\rvert<\frac12$ (by expanding a geometric series).
Suppose I have produced \begin{equation} G(x,t)=\frac{\sqrt{(1-2xt)^2}}{2(1-2xt)\sqrt{t^2}}\exp\left(\frac{(1-2xt)^2}{4t^2}\right)\Gamma\left(\frac12,\frac{(1-2xt)^2}{4t^2}\right) \end{equation} Finding the $n$'th coefficient requires taking the $n$'th derivative with respect to $t$, dividing by $n!$, and setting $t=0$.
What are the considerations for treating these derivatives of the absolute value in a generating function in the distributional sense, and what does the existence of $\sqrt{t^2}$ in $G$ mean for what the coefficients encode? For what purpose may I argue that its derivative is a sign function, it's second derivative a delta distribution etc.? And if we may argue that it is "legal" to call this a $\delta$ distribution: what is the meaning of that, since I will not be considering any integrals?
Derivation:
\begin{align} \exp\left(-\frac{\partial_x^2}4\right)\left(\frac1{1-2xt}\right) &= \exp\left(-\partial_x^2/4\right)\left(1-2xt\right)^{-1}\\ &= \sum_{m\geq0}\left(-\frac14\right)^m \frac{(2t)^{2m}}{\left(1-2xt\right)^{1+2m}}\frac{(2m)!}{m!}\\ &= \frac1{1-2xt}\sum_{m\geq0}(-)^m(2m-1)!! \left(\frac{\left(1-2xt\right)^{2}}{2t^{2}}\right)^{-m}\\ &= \frac1{1-2xt}\frac{\exp\left(\frac{(1-2xt)^2}{4t^2}\right)\Gamma\left(\frac12,\frac{(1-2xt)^2}{4t^2}\right)}{\sqrt{2\frac{2t^2}{(1-2xt)^2}}} \end{align} but also \begin{align} \exp\left(-\frac{\partial_x^2}4\right)\sum_{n\geq0} (2xt)^n &= \sum_{n\geq0}2^n t^n\sum_{m\leq n/2} \left(-1\right)^m\left(\frac12\right)^{2m}\frac{\Gamma(1+n)}{m!\Gamma(1+n-2m)}(x)^{n-2m}\\ &=\sum_{n\geq0}t^nH_n(x) \end{align}
