peter0302 said:
Ok I understand your argument but I think your premise is that Bohr and CI are correct in that physical reality is _solely_ defined by what the human experimenter sees.
Let me ask you a question then - what experimental evidence would, in your mind, disprove CI in favor of, say, a pilot wave theory or TI?
No experiment can do this, as these interpretations are, as far as quantum theory is concerned, IDENTICAL in their experimental predictions. It is only when one would find / or not find a DEVIATION from the predictions of the quantum formalism (and we all agree that the Afshar experiment doesn't CONTRADICT the predictions of the quantum FORMALISM), and after one would have build a NEW theory, that some interpretations might lend themselves better to the change than others. But as long as standard quantum mechanics prevails, all interpretations are empirically indistinguishable - because they are ALL compatible with the quantum formalism.
And let me ask you another question. And I know this sounds stupid but I do not intend it to be facetious. The air molecules immediately beyond the slit "know" which slit the photon went through do they not? Let's put two clear pieces of glass beyond the slit. Those, too, "know" which slit the photon went through. Yet we'll still see the interference pattern right?
No ! The point is that nothing interacts in an irreversible way (that means, is in a different physical quantum state) after the experiment. Actually, if this IS the case, then the interference doesn't appear anymore. The quantum-mechanical explanation for this is that, if the state of another system (glass plate or anything), has interacted with the original photon system in such a way as to entangle with it, that we have the following:
|glassplate0> (|slit 1> + |slit 2> ) before.
after irreversible interaction:
|glassplate +> |slit 1> + |glassplate -> |slit 2>
Now, you can easily work out that concerning the photon system only (reduced density matrix), all observables to "slit 1 and slit 2" will behave as if the state changed from:
"|slit 1> + |slit 2> " into a statistical mixture of 50% slit 1 and 50% slit 2.
This is what one calls "decoherence". Another way of seeing this is that the sum |slit 1> + |slit 2> happens in the hilbert space of the photon only and gives you a new vector in that hilbert space which can be "longer or shorter", while the entangled state has "orthogonal components" of the other system added to it, so any norm will just add the amplitudes squared.
So from the moment that there is interaction which leaves another system in a state which is "dependent on which way" (which means, in quantum speak, that this other system entangled with our system under study - the photon - during interaction). At that point, interference (the getting longer or shorter of the sum) disappears, because we now add the amplitudes squared.
Now let's put a miniature single photon source beyond each slit which, when it receives a photon, emits an _identical_ one and records the receipt. Suddenly we won't see an interference pattern.
Nope, we WILL see interference. That's btw what happens in a laser amplifier.
Why? Because human beings (as opposed to inanimate molecules) now "know" which slit the photon went through? So somehow the quantum state evolution depends on whether a human made the observaiton instead of a molecule? Does anybody really believe that?
No, not at all. The state of the emitter will be identical whether or not it "absorbed and re-emitted" an identical photon or not, and hence will not entangle with the photon. So the photon system remains unentangled, and will hence show interference.
However, if something entangles with the photon system (be it a single air molecule, or anything) then the interference will disappear.
This phenomenon is called decoherence.
EDIT: btw, this is the reason why "macroscopic quantum experiments" are so difficult to do - or impossible even. The "signature" of quantum mechanics is interference: that is: we have a system in a superposition of states which look classical, and we let this superposition evolve in such a way that it becomes a "classically observable state".
We have initially a system in |A> + |B> (say, "slit 1" and "slit 2"), and we evolve it, by setting up an experiment, that this evolves into a new state which is observable (hit at peak of interference pattern, or at bottom, or focus through a lens at one detector, or another).
So, |A> + |B> evolves into |C>.
If we can now design or change the setup such that we have initially:
|A> - |B> (that is the same states, but with a different phase relation), and we can have it evolve in a DIFFERENT observable state |D> (shifted interference pattern, other detector, ...) so that:
|A> - |B> evolves into |D>
then we have the typical setup which demonstrates quantum interference in the following way:
If we apply only |A>, then we find 50% |C> and 50% |D>
If we only apply |B>, then we find 50% |C> and 50% |D>
If we now apply |A> + |B> then we only find |C>
and if we apply |A> - |B> then we only find |D>
Clearly, if we had a statistical mixture of 50% A and 50% B, we wouldn't find "only C" or "only D", so this demonstrates without ambiguity that there was a superposition of states, and not a mixture at the start.
ALL quantum interference experiments are somehow modeled on this.
But the difficulty with these experiments is that NOTHING may entangle with A or B during the evolution, not even a single molecule of air. If this happens, then this molecule will "entangle" and
|A> + |B> will evolve into |mol1> |A> + |mol2> |B>
and this will give rise to 50% |C> and 50% |D>.
So the slightest entanglement will screw up your quantum interference experiment.
The "bigger" your quantum systems, the more difficult it is to preserve it from interaction during evolution (even with a single molecule or photon or ...). For macroscopic systems, it is totally impossible to avoid this beyond extremely short timescales. Even the cosmic microwave background will end up interacting with the system. This is why quantum interference is hard or impossible to observe for bigger systems.