kote said:
There is no possible explanation using finite three-dimensional local variables that can explain the predictions of QM (and observed correlations). To put it another way, if you're measuring the spin of two entangled electrons, there is no possible definition of spin as a property of electrons that can explain the results of experiments, no matter how the spin of two particles interact with each other during entanglement.
We observe correlations that are simply not possible if spin is a property of electrons unless there is nonlocal signaling. It's all tied to http://plato.stanford.edu/entries/bell-theorem/" .
Pardon me for disagreeing. Bell theorem violation in entangled pairs does not imply non-local signaling. Entanglement is simply
a priori strong quantum correlation of two systems. This correlation is obtained at the cost of knowing anything about the actual "state" of each individual particle in an entangled pair.
It is true that we cannot due to Bell inequality violation describe the pair in the classical sense of local objective properties. But this doesn't imply non-local signaling. Rather we must invoke non-local signaling in order to recover a "classical" local description and still violate Bell's inequality.
Let's take the example of a pair of totally anti-correlated electrons created at the origin. To keep things simple let's confine them to channels running along the z-axis and ignore x and y components of momentum and position.
The total momentum and spin and center of mass is zero. Now we are in a quandary as to how to label these two electrons. All we have to distinguish them is values for observables. We may consider for example the z-component of momentum and speak of the rising electron vs the descending electron. Or we may consider the z-component of spin and speak of the up electron and the down electron, or we may consider some other component of spin and e.g. refer to the spin x+ and spin x - electron.
In each of these cases we are factoring the two electron system into distinct pairs in a non-mutually consistent way. The spin z+ electron will be in a superposition of x spins.
These different factorizations show that we are not talking about local reality, not about reality at all as such. You must abandon the "state of reality" concept when dealing with quantum systems. This would be necessary if non-local effects were present anyway since any prior observed state could be changed by some future act, i.e. future acts could change the past and any concept of "reality" goes right out the window. But we can abandon classical "reality" and still keep local causality.
Back to the OP's question and the implied question in the title. Does entanglement violate Heisenberg's Uncertainty Principle?
Lets use the z-component of momentum as our labels A = rising electron and B = descending electron.
Now the question is, how does measuring say the z-component of spin for the A electron and the x-component of spin for the B electron not violate HUP?
Since spin components in the different cardinal directions do not commute HUP says we cannot know (=measure) the component of spin in say both the z and x directions.
Lets say we measured the z-component of spin for the A electron and let's say it's spin up. This means we know the z-component we would measure for the B electron if we choose to measure it. So far no HUP violation. Now we choose what to measure...
Case 1: We choose to measure the z-component of spin for the B electron and sure enough it is spin down. No HUP violation there!
Case 2: We choose to measure the x-component of spin for the B electron... just prior to measuring it we don't have a clue what the value will be so no HUP violation yet.
Once we make the measurement (and let's say we got a neg. value) then we loose information about subsequent z-component measurements and HUP is still in force.
Critical to this preservation of HUP is that by virtue of the two particles being entangled,
all specific information about either part of the two particles must be unknown. It is actually another application of HUP. The observable for the pair which defines them as anti-correlated does not commute with any of the single particle observables whose values have been so correlated.
You cannot go back and apply HUP conterfactually by saying "well we know the z-component of electron A was +, and now we know if we had gone back and instead measured the x component it would have been + as well." This is a true statement but HUP does not apply because by going back and changing the assumption about what you actually did you also go back and change the assumption that you know what the z-component is. In QM you only know what you measure and Heisenberg's uncertainty principle only applies to measurements not counterfactual hypotheses.
In short, "what we know" about a quantum system depends on "what we do" (measure). Changing assumptions about "what was done" changes "what was known". It's a subtle question of logic you must pay attention to when working with thought experiments vs. actual experiments.