Mellin Barnes Like Integral Representation:
$\def\M{\operatorname M} \def\B{\operatorname B}$
We apply the Mellin Inversion theorem on the exponentially decreasing branch of $f^{-1}(x)=h(x)$:

$$f(x)=-e^{-x}\ln(x)\implies h(x)=\M_x^{-1}(\M_s(h(t))$$
The Mellin transform uses $e^y$’s Maclaurin series and integration by parts:
$$\M_s(h(t))=\int_0^\infty h(t)t^{s-1}dt=\frac{(-1)^s}{s!}\int_0^1 e^{-st}\ln^s(t)dt=\Gamma(s)\sum_{n=0}^\infty\frac{(-s)^n}{(n+1)^{s+1}n!}$$
Therefore:
$$\bbox[5px,border: 3.5px solid blue]{f(x)=\frac{e^x}{\ln(x)}\implies f^{-1}(x)=\frac1{2\pi i}\int_{c-i\infty}^{c+i\infty}(-x)^s f_{-s-1}(-s)ds,f_a(x)=\sum_{n=0}^\infty \frac{(n+1)^ax^n}{n!}}$$
The integral of the summand nor the sum itself has a closed form yet, but $f_a(x)$ relates to the Bell polynomial $\B_n(x)$ for $a\in\Bbb N$. The Mathematica code
InverseMellinTransform[Gamma[s]*Sum[(-s)^n/((n+1)^(s+1)n!),{n,0,b}],s,-1/x] for large $b$ and given $x$ verifies the result:

Series Solution:
Using the Bell polynomial and Lagrange reversion gives this series for the same branch of the inverse function:
$$\bbox[5px,border: 3.5px solid blue]{f(x)=\frac{e^x}{\ln(x)}\implies f^{-1}(x)=\sum_{n=1}\frac{e^\frac nx}{n!}\B_{n-1}\left(\frac nx\right)}$$
shown here