Kochen-Specker for two particles

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I've just saw Conway's lecture about "Free will" at princeton lectures online. It contains a nice explanation for the Kochen-Specker theorem for a spin-1 particle that is measured in 3 perpendicular directions (along symmetry directions).

I find it plausible that the state of a system changes locally(!) once a measurement is done. This would resolve the paradox of a single spin-1 particle (in Conways version at least).
I couldn't follow exactly what Conway said about two separated particles. If I assume that for whatever reason a measurement can change the state of the object, would it also resolve the problem for two separated particles? I assume that the measurement induced change of the object is only local.
Anyone got an easy reference about Kochen-Specker for two separated particles? Or someone knows what I mean with my first statement and has an answer to my second question?
 
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A:I believe that the resolution to the Kochen-Specker paradox for two separated particles is that each particle has its own set of possible outcomes for a given measurement, and these sets are not necessarily correlated with each other. That is, the outcome of one particle's measurement does not determine the outcome of the other, and thus there is no inconsistency.As for references, I would recommend starting with the original paper by Kochen and Specker (1967): "The Problem of Hidden Variables in Quantum Mechanics". It's not an especially easy read, but it's the seminal work on the subject. Another good reference is the book by Peres (1995): "Quantum Theory: Concepts and Methods". This provides an excellent overview of the topic, as well as a detailed discussion of the Kochen-Specker paradox.
 
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