- #36
zenith8
- 361
- 2
sokrates said:I think it's not fair to even dwell on this subject. We must immediately resort to 'Bertlmann's socks' argument whenever we, as the more knowledgeable, need to explain this to somebody.
Even the simplest things caused quite a stir in their times, but this just isn't important.
Sokrates - as has been pointed out to you several times, you're just wrong about this. Here is a summary of the current state of affairs:
We define nonlocality as a direct influence of one object on another, distant object, contrary to our expectation that an object is influenced directly only by its immediate surroundings.
Consider an EPR experiment, measuring spins. With parallel analyzers, we find that measurement of the spin on one side instantly predicts the result on the other. If you do not believe one side can have a causal influence on the other, you require the results on both sides to be determined in advance (the Bertlmann's socks argument). But this has implications for non-parallel settings (e.g. measure spin on axes 45 degrees apart in the two wings) which conflict with quantum mechanics (Bell).
Bell's analysis showed that any account of quantum phenomena needs to be non-local, not just any 'hidden variables' account i.e. nonlocality is implied by the predictions of standard quantum theory itself. Thus, if nature is governed by these predictions (which it is, according to real experiments) then nature is non-local. This is essentially because the many-particle wave function in the Schroedinger equation is defined on the configuration space of the system, an abstraction which combines or binds distant particles into a single irreducible reality.
So nonlocality - spooky action at a distance if you like - sounds strange and yet it is experimentally verifiable. If you want to refuse to believe it, what are your options?
(1) Loopholes: claim that improving detector efficiencies in the EPR-style experiments will invalidate the results. This is now widely understood to be desperate clutching-at-straws.
(2) Deny, in one way or another, that there is a material world - the description of which is the task of physics. Without objective reality, there is nothing to be objectively nonlocal. Despite its manifest ludicrousness, this has actually become a surprisingly fashionable viewpoint.
However, standard QM is not self-consistent due to the measurement problem. This is solvable only by granting real physical existence to theory objects. Standard QM is thus fundamentally an anti-realist stance - the wave function is just about probabilities, but probabilities of what? Something does travel - of course - along different paths in, say, an interference experiment; to refuse to call it 'real' is merely to play with words. Radical anti-realism can pretend to resolve interpretative paradoxes in virtually any context, e.g. Mach's rejection of grounding 'pressure' and 'temperature' in terms of real microscopic entities obviates the need to understand, say, convergence to thermodynamic equilibrium. More broadly, the philosophical doctrine of solipsism can 'solve' every problem in the history of science by just denying that anything but one's own mental experiences exist. This is ludicrously distant from the kind of solution we are interested in as scientists.
Instrumentalist Copenhagen QM is effectively 'an idea for making it easier to evade the implications of quantum theory for the nature of reality' (Deutsch). The positivist belief that empirical adequacy plus a formalized proof procedure is the best any theory can properly aspire to is - when you think about it - bizarre.
(3) Be a many-worlds person, then everything that can possibly happen happens in both branches of the experiment thus there can be no correlations. This makes two problems - nonlocality and macroscopic superpositions in measurement - go away, at the cost of believing in something apparently ludicrous (bazillions of ontologically-real extra universes) on the basis of assigning an entire universe to each term in a mathematical expansion.
(4) Allow time travel into the past (like in Cramer's transactional interpretation). But then we need to abandon the metaphysical picture of the past generating the future, and this is a step too far for most people.
(5) Make claims along the lines that the universe is necessarily Lorentz invariant and Lorentz invariance of a physical theory requires locality. However, this is just wrong as should be clear from the meaning: 'Lorentz invariance' describes the behaviour of a theory under certain transformations of the reference frame. 'Locality' implies there is no action at a distance. (Nonlocal Lorentz-invariant Wheeler-Feynman electrodynamics good counterexample to this).
(6) Claim that, in quantum field theory, the Equal Time Commutation Relations (operators which represent field quantities at space-like separation all commute) show that the theory contains no superluminal action. However, this is an empty claim. What it actually shows is that measurements on one side do not affect the long-term statistics on the other, that is that no signals can be sent from one region to the other by manipulating the apparatus on one side. However, superluminal influences are still required to explain the correlations between the two regions in an individual experiment.
To summarize finally the connection between non-locality and relativity, remember that although relativity is often taken to imply the existence of some sort of absolute speed limit, this is not actually the case. The fundamental feature of the Lorentz transformations is that they leave the speed of light invariant, not that they render it an insuperable boundary. Note that theories of tachyons and other superluminal transport do exist. We must therefore turn our attention to the question of the compatibility of non-locality with the relativistic picture of space-time. One can say that:
* Violation of Bell's inequality does not require superluminal matter or energy transport
* Violation of Bell's inequality does not entail the possibility of superluminal signalling (unless you believe in Bohm-Valentini style quantum nonequilibrium).
* Violation of Bell's inequality does require superluminal causal connections.
* Violation of Bell's inequality can be accomplished only if there is superluminal information transmission.
An excellent reference is Tim Maudlin's book 'Quantum non-locality and relativity' from where I adapted the previous four starred points.
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