Saiker said:
All these videos and articles about the Double Slit Experiment say that if we "look" where the single photons go, they act like particles and if we don't "look" they act like waves, creating the interference pattern...
BUT
What does it mean to "look"? We're not using our eyes or any camera after all. How do these detectors work? Don't they have to interact with the photon in order to measure it? If so, doesn't that interaction change the behaviour of the photon and affect the experiment results?
It's not right but popularizations of science. Photons never behave like particles nor like waves. Photons are single-particle Fock states of the electromagnetic field. You cannot simplify it from this statement without getting it somehow wrong. Forget classical pictures about photons. They are as far from classical objects as something can be. You are not even able to define position observables (neither mathematically nor experimentally in the real world). All you can predict and finally also measure in the real world are detection probabilities given a single-photon state, and comparing experiment with theory (Quantum Electrodynamics, QED) in this case leads to results that are among the best of entire physics today. Some quantities like the Lambshift of hydrogen or the anomalous magnetic moment of the electron coincide between theory and experiment at an accuracy of ~12 siginificant digits or so.
The interference patterns, you talk about, occur for doing a double-slit experiment with single photons for many times, if you do not register somehow, through which slit the photon has gone. Of course, given that we don't have a position observable for photons, we have to define, what we mean with that, and that can be done only by describing concrete experimental setups.
One way to get which-way information is to begin with linearly polarized photons and then set a quarter-wave plate in each of the slits, one oriented with ##+\pi/4##, the other with ##-\pi/4## angle relative to the polarization direction of the photons. Then, if the photon goes to the first (second) slit it's right-circular (left-circular) polarized, and thus its polarization state (helicity ##h=\pm 1##) clearly indicates through which slit the photon came. But now the "partial beams" of photons cannot interfere anymore, because the polarization states are orthogonal to each other, and if you have a superposition of two orthogonal states, they cannot interfere, because
$$\langle 1 + -1|1+-1 \rangle=\langle 1|1 \rangle + \langle 1|-1 \rangle+\langle -1|1 \rangle+\langle -1|-1 \rangle=\langle 1|1 \rangle+\langle -1|-1 \rangle,$$
i.e., there are no mixed terms between photons coming from slit 1 (helicity ##+1## state) and those coming from slit 2 (helicity ##-1## state). So gaining "which-way information" (in this physically well-defined sense) destroys the interference pattern.
If you distort the relative angles of the quarter-wave plates in the slits, you gain only some which-way information, i.e., it's not certain any more through which slit each photon comes, but for a given polarization indicates that it with some more probability it came from a specific slit. Now the polarization states are not orthogonal anymore and you get some interference back, i.e., a somewhat washed-out interference pattern. If you put the quarter-wave plates in the same direction all photons coming to either of the slits have the same polarization, and thus you cannot get any which-way information anymore, but you get the best contrast for the interference pattern possible.