Consider an experiment in which we prepare pairs of electrons. In each trial, one of the two electrons - let's name it the 'herald' - is sent to a detector C, and the other - let's name it 'signal' - to a detector D. The wave-function of the signal is therefore

(1) |ψ> = ψ(r) |1>,

i.e. in each trial of the experiment, when the detector C clicks, we know that a signal-electron is in the apparatus. Indeed, the detector D will report its detection.

Now, let's consider that the signal wave-packet is split into two copies which fly away from one another, one toward the detector DA, the other to the detector DB,

(2) |ψ> = 2-½ ψA(r) |1>A + 2-½ ψB(r) |1>B.

We know that the probability of getting a click in DA (DB) is ½, but in a given trial of the experiment we can't predict which one of DA and DB would click.

Then, let's ask ourselves what happens in a detector, for instance DA. The 'thing' that lands on the detector has all the properties of the type of particle named 'electron', i.e. mass, charge, spin, lepton number, etc. But, to the difference from the case in equation (1), the intensity of the wave-packet is now 1/2. It's not an 'entire' electron. Imagine that on a screen is projected a series of frames which interchange very quickly. The picture in the frame seems to be a table, but it is replaced very quickly by a blank frame, and so on. Then, can we say what we saw on the screen? A table, or blank?

The situation of the detector is quite analogous. So, will the detector report a detection, or will remain silent? What is your opinion?

For a deeper analysis see

Preprint Why is Quantum Mechanics Stochastic and Nonlocal? – Do We Ha...

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