I have designed an experiment. Without going into detail it resolves around the double slit quantum eraser experiments. If we can infer the location of a particle without actually measuring it, does it remain in a quantum state? After all, we have not measured or detected that particle in any way. If not, it can not be the act of measuring it, but merely the fact we know about it that effects its quantum state. This does not fit any model I know of. If it is true that you do not need to measure or detect a particle to affect its state, what implications does that have for quantum mechanics?
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A particle is always in a quantum state. The only thing that causes that quantum state to change in the manner known as a "measurement" (or wavefunction collapse) is an actual interaction with another particle. The mere fact that you know or don't know something about the quantum state is irrelevant. |
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This is a famous intuitive paradox in quantum mechanics, the null-result measurement. There are many examples:
All of these examples have the property that the quantum measurement fails, nothing happens, and yet the wavefunction collapses becuase the null result reveals to you that the quantum wavefunction is not in the state you are checking. The ultimate version of this is the Elitzur-Vaidman bomb-tester, which is a device which confirms whether a mirror is doing a measurement, without the mirror ever successfully getting a measurement outcome. The way it is usually stated, you have a bunch of bombs set off by a very sensitive mirror, that detects the recoil of a single photon. You also have duds, which are just ordinary mirrors that don't do a measurement on the photon. Can you tell them apart without exploding the bombs? The answer is yes, and this is an extreme example of doing a counterfactual measurement in QM--- you can tell if the mirror would measure the photon, were you to shine it, without having any appreciable probability of the mirror actually detecting anything. This property is not paradoxical in many-worlds derived intepretations, because all that is going on is that the detector is entangling with the particle, and the branch where the detector doesn't go off is special, in that it only has a particle relative state which is collapsed. This is the standard way of understanding these effects in modern interpretations, and these only differ in philosophy regarding what causes the collapse, or if it happens at all. In other interpretations, you can consider this as an indication that the quantum state is a measure of information about the particle, since getting information about the particle's position affects the wavefunction, or else not. This is all philosophy, so I don't think it is so important. |
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So basically we can view this as a particle being carried on a wave. The wave is an actual physical thing, in the same way that a magnetic field is real, or a gravitational field is real, albeit nothing we can actually see - we can just infer it is there because we see how it affects other things. So I see this wave spreading out in every direction from the source, like when you throw a pebble into a pool, but the particle it carries is only going in one direction, ie, through one or other of the slits. Of course we don't know this until later when certain measurements are not made/made. Until then it is everywhere on that wave front. And the act of measuring, but failing to detect a particle as the wave carrying that particle passes through the detector causes the whole wave to collapse, leaving in it's wake a Newtonian particle which just continues on it's way all the way to the detector. So we can - again - have an effect on a particle remotely. Sort of the opposite of twinning. You collapse the wave by failing to detect a particle here, and the particle which is over there loses uncertainty. So the question is: how do we measure a particle to find out if it is in a quantum state or not?! LOL IS this a philosophical quantum paradox? ;O) |
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