Why does the Bell inequality give 1/4 in quantum mechanics but 1/3 classically?

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jerromyjon
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I went through a paper last week about the Bell inequality and how it is incompatible with QM. Something along the lines of probability in classical regards being 1/3 but in quantum mechanics it is 1/4. It went into some basic principles of how this is determined through quantum entanglement to be 2 separate variables measured on 2 entangled particles. OK then. I file it away in the pile labeled "not fully understood". But then something doesn't sit right... wouldn't 2 variables with 2 possible values be 1/4 chance of any of the 4 possible "states" occurring? That's just classical probability.
 
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Why would 2 variables with two possible values have a 1/4 probability of each combination of values? Is the probability that a randomly selected person is male and not retired equal to 1/4 ?
 
I was trying to explain it in a simple boolean manner, 0 or 1, true or false, heads or tails fits best... 2 coins with 2 possible states. 25% both heads 25% heads/tails 25% tails/heads 25% both tails.
 
jerromyjon said:
I was trying to explain it in a simple boolean manner, 0 or 1, true or false, heads or tails fits best... 2 coins with 2 possible states. 25% both heads 25% heads/tails 25% tails/heads 25% both tails.

That's clear. Now what is the question? Are you asking why ordinary probability theory gives an answer of 1/3 in the quantum entanglement problem? To answer that I, myself, would need to hear a statement of the entanglement problem you read about. Perhaps someone else knows the problem just from the mention of the word "entaglement".
 
I just absorbed another version found in another thread here: http://www.felderbooks.com/papers/bell.html
It makes the same case of what should be 5/9 chance turns out 50/50.

But just before reading that version I had the "aha!" moment and realized this is because entanglement gives 100% (or close to, ideally) chance of pairs being opposite spin in any 1 of the 3 axes. We can only measure 1. So then we double up pairs, and we measure 2 axes on 1 of each pair. Then when we think we can predict what the measurements of the other pair will be it turns out random?
 
I'm still not sure if I explained that well enough or correctly, or if the original paper by Bell? would provide any additional insight. All I am trying to do is relate what is expected locally (meaning classically as in all 3 axes in 1 particle should always be the opposite spin in all 3 axes of entangled pairs) to what truly occurs non-locally (the measurements in the other 2 axes is affected in the pair by measuring the first axis on the first particle). This is truly the gist of the inequality, is it not?
 
I haven't finished reading it yet, but can I assume there is verification that we know for sure a singlet state that we've partnered that we can measure vectors A,B and verify we know what C is or is that inferred from Bell's Theorem exclusively?
 
I don't think anyone understands your question or what article you are referring to, since there are now 3 references in the thread.
 
Forget it I'm good thanks for the links everyone.
 
Detection-Loophole-Free Test of Quantum Nonlocality, and Applications, arXiv:1306.5772)

Here's a recent proof...