Some quantum erasure experiments involve polarization of photons. In one such experiment with a double slit, a horizontal polarizer is used in front of one slit, and a vertical polarizer is used for the second slit and the idea is that then horizontal or vertical polarization of the photon coming out of the double slit "marks" which path it took and so interference pattern disappears. Then the experimenter goes on to erase that which-path information in some way to restore interference. So it seems to me that a photon detector by itself does not work as an eraser and that a horizontally polarized photon entering a photon detector leaves something very different in the detector or the environment than a vertically polarized photon entering the same detector. How is it that a detector that usually cannot tell apart different incoming directions of photons can somehow tell apart different polarization?
The key point here is the notion of distinguishability. If the two paths are made distinguishable, by associating different polarization to each path, then there is no way for the two amplitudes to interfere when they meet again because the "which-path" information is present. It doesn't matter whether or not the observer decide to actually look at the information.
You're right, if one uses a detector such as a CCD camera, it won't tell you what was the polarization of an incoming photon, so you're not actually retrieving the "which-path" information. But still, since this information is available, you won't observe interference, unless you make the information disappear again, using a diagonal polarizer for instance.
It is very important to keep in mind that the double slit interference is a quantum mechanical phenomenon. The ideal would be to solve the quantum mechanical problem and get the wavefunction , i.e. photon , two slit field pattern, screen , detector and impose the boundary conditions to get the system wave function and see the probability of the photon hitting the screen.
This has not been done as far as I know mathematically. What is being done is various experiments that lead to reasonable conclusions on what is happening when boundary conditions are changed by inserting different detectors and measuring more variables.
In this experiment, for example, Which-way detector unlocks some mystery of the double-slit experiment
shows the importance of changing boundary conditions. If the detector is set up for measuring polarization it is a different detector and a different state function of the system gives the probabilities of detection.
We arrived at the conclusion that the microlevel of nature is quantum mechanical and quantum mechanics was discovered because of the odd probabilistic behavior of the results of experiments on elementary particles , which photons and electrons are. One cannot use the deterministic intuition of classical mechanics to describe experiments on elementary particles.
I see that I have not answered the question of
Polarisation is not a simple state. Polarization of the beam is built up by photons, but the beam polarization is perpendicular to the direction of the wave while the photon polarization is plus or minus on its direction of motion.
Photon are always polarized along their direction of motion. There can be no vertical or horizontal polarization for a single photon. It will just be tagged as a photon that went through the classical filter of horizontal or vertical polarization.
It is a pictorial example of how the classical wave, light, is built up by the quantum mechanical photons. Light is a confluence of zillions of photons.## Heading
In your description " horizontal polarizer is used in front of one slit, and a vertical polarizer is used for the second slit" the polarizers are light poarizers, which means a system of filters. To detect a point of arrival of the photon one needs a screen or a corresponding electronic surface. The two requirements cannot be met in one detector , to catch an individual photon and extrapolate its direction and also get its polarization. It would be a different experiment with two detectors and one photon at a time passing the slit, different quantum mechanical setup.