I have recently begun to study John Kingsman's "Poisson processes", and in the first chapter, the author defines $\mathbb{P}${$X$ = $n$} = $\pi_{n}$($\mu$) = $\mu^{n}e^{-\mu}/n!$
"Differentiating with respect to $\mu$, we have
$\frac{d\pi_{n}}{d\mu}$ = $\pi_{n-1} - \pi_{n}$ with the convention that $\pi_{-1}=0$.
Thus $\frac{d}{d\mu} \sum_{k=0}^n \pi_k = -\pi_n$.
Integrating from $0$ to $\mu$ gives the useful identity
$\sum_{k=0}^n \pi_k(\mu) = 1 - \int_0^{\mu} \pi_n(\lambda) d\lambda~ \qquad$(*) "
How does one get to the observation (*)? Integrating with respect to $\mu$ or $\lambda$? Where does the $1$ come from?
I am grateful for any tip or piece of advice
In general if $f'(x)=g(x)$ then - if $g$ is a suitable function - we may conclude at first hand that: $$f(x)=\int_0^xg(t)dt+c$$for some constant $c$.
Substituting $x=0$ reveals that $f(0)=c$ so that apparantly:$$f(x)=\int_0^xg(t)dt+f(0)$$
Something similar happens here.
Be aware that $\sum_{k=0}^n\pi_k(0)=1$.