For the computation of the lower (attracting) fixpoint $L_0$ for $b^{L_0} = L_0 $ (where the base $b$ is in the range for convergence $1 \lt b \lt e^{1/e}$) there is the simple formula $$L_0 = \exp(-W(-\log(b))) \qquad \qquad \text{where $W$ is the Lambert-W-function}$$ or if we directly use the logs for $b$ and $L$ writing $\beta := \log(b)$ and $\lambda := \log(L)$ $$\lambda_0 = -W(-\beta) \phantom{\qquad \qquad \text{where $W$ is the Lambert-W-function}}$$ (This has also the nice property that $\beta = \lambda_0 / L_0 $ or $b=L_0^{1/L_0}$.)
I think there is a related formula for the upper (repelling) fixpoint $L_1$ too, but I can't remember it from the top of my head (some simple variations didn't work so far). Before beginning a long search in older texts and program-sources (the searchkey were much un-sharp) - could someone refresh my memory? A reference would suffice...
Example: let $b=\sqrt 2$ then $L_0 = 2$ because $b^2 = 2$ and $L_1=4$ because $b^4 = 4$
Remark: I know how to approximate $L_1$ using the Newton-algorithm - I specifically think to remember that there is some variant with the Lambert W (which is what I want here)
Yes. If you use the other real-valued branch of $W$, denoted $W_{-1}$, you will get this fixed point:
$$\lambda_U = -W_{-1}(-\beta)$$
and
$$L_U = \exp(-W_{-1}(-\log(b)))$$.
But I do not know if or believe that $W_{-1}$ can be expressed through $W = W_0$, the principal branch (unlike simpler multivalued relations like $\sqrt{...}$ and $\log$ in the complex plane.).