In double-slit experiments, path detection makes interference fringes disappear. How comes the detection screen does not? One observes that the fact of detecting the location of a particle path (which slit the particle went through) entails a collapse of the particle field (interference fringes disappear on the detection screen).
But, in every condition of the experiment, the detection screen does also give some information about the location of the particle. So how comes the detection screen does not trigger any collapse in the condition where slits are not observed?
Shouldn't the fact of hitting the screen entail some change in the particle field? How is the state of the field in the condition where slits are not monitored?
 A: Any edge deflects photons into areas with higher and lower density. To measure such a result different measurement instruments can be used. Beside a screen one may use a photodiode which is moved and the outcoming current shows the same intensity distribution like the pattern on a screen.
The detection of photons direct behind the slit destroys the interaction between the photons and the edge(s). Since a photon-photon interaction is very improbable you could use electrons, shooting them parallel to the wall with the slits. It will interfere the fringes. But why?
We know that the electrons we use for detection, interact with the photons after the edges. With the same certainty, we should assume that the photons and the surface electrons of the edges interacting.
Let's imagine an experiment. We shoot three electron beam and set up our photon beam perpendicular to it. We should get a result with an intensity distribution similar to the double slit (not the same, because only a small amount of photons meets the electrons).
Now, if you try to find out, which way the photon was going between the electron beams and you do this with an additional electron beam, clearly you’ll disturb the intensity distribution. Simply, we not have the sensitive enough measurement instrument.
A: The screen does trigger the collapse of the particle wave function to a specific point on the screen. The probability of collapse at a specific point is given by the magnitude squared of the wave function at the screen. Thus, when one carries experiment many times (shooting one particle after another), an interference pattern appears, in the form of darker areas where more particles have collapsed, and lighter areas where the probability of finding a particle is low.
It is for this reason that the descriptions of the double slit experiment always talk about a beam of particles, going through the trouble of explaining that the particles are shot one after another, so that we can neglect the interaction between them. Although a single particle is sufficient for setting the Schrödinger equation and calculating the interference pattern, it is not in practice sufficient for observing the interference. This is consistent with the canonical formulation of quantum mechanics, where the measurement is always done repeatedly on many objects, prepared in the identical quantum state.
However, as long as the place, where the collapse occurs on the screen, does not allow us to distinguish through which slit the particle has passed, the interference fringes are preserved.
