I'm working through Stephen Barnett's book on quantum information and have come across the following question (1.5, for anyone keeping track at home)
A particle counter records counts with an efficiency $\eta$. This means that each particle is detected with probability $\eta$ and missed with probability $1-\eta$. Let $N$ be the number of particles present and $n$ be the number detected. Show that
$$P(n|N) = \frac{N!}{(N-n)!n!}\eta^n(1-\eta)^{N-n}$$ [I did this part, no problem]
a) Calculate P(N|n) for
$$P(N) = e^{-\bar{N}}\frac{\bar{N}^N}{N!}$$
b) Calculate P(N|n) for all P(N) equally probable
c) Calculate P(N|n) given only that the mean number of particles present is $\bar{N}$.
My questions:
What does $P(N)$ denote? I recognize that question $a)$ is the Poisson distribution, so I assume that it's the probability of $N$ particles being detected, given a mean of $\bar{N}$. But this conflicts with the information in the first paragraph... It seems like $N$ is being used as a constant in the first paragraph, and now as a variable in the question.
Does $P(N|n)$ mean "the probability that $N$ particles are detected, given that $n$ are"?
Doesn't question $c)$ conflict with the fact that the first paragraph says that $N$ particles are present?