By the Lagrange Inversion Theorem, one can derive the series expansion for the principal branch of $W_0(x)$: $$W_0(x)= \sum_{n=1}^{\infty} \frac{(-n)^{n-1}x^n}{n!}, \, |x| \leq \frac1e$$
For $x \in \mathbb{R}$.
Is there also a series expansion for $W_{-1}(x)$? If so, how can it be derived?
Lagrange reversion:
$$\text W_{-1}(z)=\ln(z)-2i\pi-\ln(\ln(z)-2i\pi)-\sum_{n=1}^\infty\sum_{m=1}^n\frac{S_n^{(m-n+1)}\ln^m(\ln(z)-2i\pi)}{(2\pi i-\ln(z))^nm!}\tag1$$
from The Generalized Lambert function from Wolfram Functions and the Stirling numbers of the first kind $S_n^{(m)}$. If both sums go to $\infty$, then they are interchangeable. The derivation uses Lagrange reversion:
$$We^W=z\implies W=\ln(z)-2\pi i -\ln(W)\implies W_{-1}(z)=\ln(z)-2\pi i+\sum_{n=1}^\infty\frac{(-1)^n}{n!}\left.\frac{d^{n-1}\ln^n(a)}{da^{n-1}}\right|_{a=\ln(z)-2\pi i}$$
Differentiating gives a pattern with factorial power $u^{(v)}$:
$$\frac{d^{n-1}}{dx^{n-1}}\ln^n(x)=x^{1-n}\sum_{m=1}^{n-1}n^{(m)}S_{n-1}^{(m)}\ln^{n-m}(x)$$
The $n=1$ term does not fit this formula, so remove $\ln(\ln(z)-2\pi i)$ and simplify:
$$W_{-1}(z)=\ln(z)-2\pi i-\ln(\ln(z)-2\pi i)+\sum_{n=2}^\infty\sum_{m=1}^{n-1}\frac{S_{n-1}^{(m)}(-1)^n\ln^{n-m}(\ln(z)-2\pi i)}{(\ln(z)-2\pi i)^{n-1}(n-m)!}$$
which works. Then, some index shift gives $(1)$.
Inverse gamma regularized:
$$-Q^{-1}(2,-ez)-1\mathop=^{-\frac1e\le z<0}\text W_{-1}(z)=…-\frac{43}{135}(ex+1)^2-\frac{11}{72}(2ex+2)^\frac32-\frac23(ex+1)-\sqrt{2ex+2}-1 $$
From the series expansion of Inverse Gamma Regularized. Please correct me and give me feedback.
The series coefficients have a recurrence relation mentioned in quantile mechanics