I know that for a Fock State you can calculate the interference pattern, and that the distribution does not change with the intensity, in this case with n.
In this case, the intensity pattern has the same shape and only increase the intensity with n, thus for a fock state $|n\rangle$ the intensity follows the following distribution.
$I (r, t ) = n | f (r)|^2 [1 + cos \theta] $
Actually, the shape is the same for coherent state $|\alpha\rangle$
$I (r, t) = |α|^2 | f (r)|^2 [1 + cos\theta] $
Thus, the distribution of the interference doest not change,
What I wonder is, if you send a state $|n\rangle$ trough a double slit, could you see n simultaneous detections in the screen?
For example, for one photon $|1\rangle$, the way to measure this pattern is repeat the experiment several times, and as you record the detections the pattern appears. But you only detect a photon each time. In this case, since we have n photons ($|n\rangle$). I wonder if it is possible to detect in each iteration of the experiment n photons, or if the n photons hit the same point in the screen.
We can consider we have a screen that can detect 1 photon in each point of the screen.
I like the idea of model it as a beam splitter. However, since we have a whole screen of detection, I think the model should contain at least m detectors in the screen, didn't it?
– Tarek Peña Sep 21 '23 at 18:55