At the instant $t = 0$ a certain radioactive focus starts emitting particles. The infinitesimal probability that the focus emits a particle in the differential interval is $\lambda dt$. Let $N_t$ also be the random variable 'number of particles emitted by the focus in the time interval $[0,t]$'. Hence, we have that the probability distribution that $N_t$ follows is a Poisson one:
$$P_n = e^{-\lambda t} \frac{(\lambda t)^n}{n!}$$
However, imagine we wanted to calculate the probability distribution of the continuous random variable $T_n$ 'moment $t$ at which the focus emits the nth particle'.
How would we calculate this probability distribution? How would it be related to the Poisson one above?
I know it has to be a gamma distribution, but I don't know how to get to that conclusion.
Many thanks.
Attempt:
$$P[T_n \leq t]=P[N_t\geq n]=1-P[N_t\leq n-1] = 1 - e^{-\lambda t} \sum_{i = 1}^{n-i = 0} \frac{(\lambda t)^{n-i}}{(n-i)!}$$
How could I get to the following expression?
$$\rho_n(t)= \frac{1}{(n-1)!}\lambda^nt^{n-1}e^{-\lambda t}$$