(The question arises from playing with translating series into integrals)
I wanted to see, what it means to have a "continuous" relative for powerseries and other series; the most simple one perhaps
$$ \begin{array} {} f_1(x) = \sum _{k=0}^\infty x^k = {1 \over 1-x} &\to & g_1(x)= \int_0^\infty x^t \,dt = - { 1\over \log(x) } \end{array}$$
I couldn't get this
$$ \begin{array} {} f_2(x)=\sum _{k=0}^\infty {x^k \over k!} = \exp(x) &\to& g_2(x)=\int_0^\infty { x^t\over \Gamma(1+t) } \,dt =\text{ ???} \end{array}$$ by, for instance, Wolfram alpha...
and I'd like to proceed to some more general
$$ \begin{array} {} f_\varphi(x)=\sum _{k=0}^\infty \varphi(k) x^k &\to& g_\varphi(x)=\int_0^\infty \varphi(t) x^t \,dt =\text{ ???} \end{array}$$ where $\varphi(k)$ is some meaningful function producing common sets of coefficients for the power series.
Playing a bit with numerical evaluations for $f_2(x),g_2(x)$ so far did not uncover anything obvious, but I am interested, whether there are some relations known; for instance whether there are relations between $g_2(x) \cdot g_2(y)$ perhaps analoguously to $ f_2(x) \cdot f_2(y) = f_2(x+y)$ or the like.
Is there something known about it? Is there a possibly a list of sums/integrals-relations done elsewhere?
In general, I'd like to get more intuition about this; it reminds me that I should possibly re-read in the explanations for the Euler/MacLaurin-summation formula where the "dance between discrete and continuous" (as it is a title of a nice article about the work of Delabaere on Euler's divergent series) has a similar relevance. (But this is possibly too much for this Q&A-site ...)
Here's a thought: rewrite $g_2$ as
$$\int_0^{\infty} dt \frac{e^{-t \log{(1/x)}}}{t \Gamma(t)}$$
Now, $\frac1{t \Gamma(t)}$ is an entire function and therefore has the following Taylor series representation in the whole complex plane:
$$\frac1{t \Gamma(t)} = \sum_{k=0}^{\infty} a_k t^k$$
where $a_0=1$, $a_1=\gamma$, and for $k \ge 2$, the $a_k$ satisfy
$$a_k = \frac{a_1 a_{k-1}-\sum_{j=2}^{k} (-1)^j \zeta(j) a_{k-j}}{k} $$
Integrate and get the following
$$g_2(x) = \sum_{k=0}^{\infty} a_k \frac{k!}{\left ( \log{\frac1{x}}\right )^{k+1}} $$