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understanding bell's theorem: why hidden variables imply a linear relationship? |
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| Jun22-12, 11:42 AM | #239 |
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understanding bell's theorem: why hidden variables imply a linear relationship?
Understanding/checking Bell's theorem via scenario analysis
Theoretical simulation (of a case(s)) can be another way to understand/validate Bell's theorem. So lets take a scenario: If the entangled photons were oriented at say 0 degrees(see note below) and one polarizer (A) was at 0 degrees and the other (B) at 15 degrees. What is the logic, and calculations, we use to calculate the match prediction per LHV hypothesis? and per QM/actual? Note: per QM/QE - it is impossible to tell what degree the photons are oriented at because they are in an indeterminate state and as soon as we measure it, the entanglement breaks. That said.... lets assume hypothetically/theoretically. |
| Jun22-12, 05:02 PM | #240 |
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Le us represent the sets of photons as one set "w" for scenario (c), and three different sets ("x", "y","z") for scenario (b). The the probabilities for (c) are more accurately represented as P(A|w), P(B|w), P(C|w). Surely we can combine these probabilities into the same expression and obtain the trivial inequality P(C|w) <= P(A|w) + P(B|w). This makes sense because we are dealing with the same space "w" (aka, the same context, condition, etc). There is no question here. However the probabilities for scenario (b) are more accurately represented as P(A|x), P(B|y), P(C|z). You are saying that because for the specific physical scenario you described, P(A|x) = P(A|w) and P(B|y) = P(B|w) and P(C|z) = P(C|w), therefore P(C|z) <= P(A|x) + P(B|y) should be valid. But that is not very credible. The inequality is a deeper relationship between probabilities not just specific values of the probabilities. This is evident in the fact that P(ABC|w) is well defined and P(ABC|xyz) is not. There is nothing new here, this same issue was addressed by Boole 150 years ago. The article by Itamar Pitowsky I cited earlier goes into great details about this. Violation of inequality simply means the data are not from the same population. How does no-conspiracy enable you to recombine separate incompatible samples into a single one? It can't, they are not called incompatible for no reason.[/QUOTE] |
| Jun22-12, 07:00 PM | #241 |
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It seems so obvious to me. P(A|x)=.25, P(B|y)=.25, and P(C|z)=.75. Thus P(A|w)=.25, P(B|w)=.25, and P(C|w)=.75. And you agreed that P(C|w) ≤ P(A|w) + P(B|w). Then we reach the conclusion .75≤.25+.25. What do you think I'm doing wrong here? |
| Jun22-12, 08:59 PM | #242 |
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What is the explanation for that per QM/QE? Is it something like - Since the two particles are entangled and act as one prior to interaction (with the polarizer): the angle/orientation at both the polarizers will be "taken into account" and this causes the increase in mismatch. side note: Do the calculation involve some sort of "joint probabilities" ? |
| Jun23-12, 07:40 PM | #243 |
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And if you attempt to tell me what the joint probability P(ABC) is for both scenario (b) and (c) then you may start having a paradigm shift to understand the issue I have with your argument. I suppose your no-conspiracy condition implies that they two are equal. But that is impossible because P(ABC) is undefined for scenario (b). Let me even make it easier: your expression P(C|w) <= P(A|w) + P(B|w) is actually derived from the equality P(C|w) = P(A|w) + P(B|w) - P(AB|w) so let us stay with the equality for a moment. Please use your so called "no-conspiracay condition" to write down the equivalent equality for scenario (b) with appropriate notation. As soon as you start writing it you will realize that after the second term on the RHS you are stuck, there is no P(AB|..) term because A and B are incompatible experiments. So contrary to appearances, your "no-conspiracy" inequality P(C|z) <= P(A|x) + P(B|y) is nonsense. By writing it as an inequality, you have hidden the error of the impossible P(AB|..) term. And that means you are not allowed, ever, to use P(A|x), P(B|y) and P(C|z) in the same expression the way you do. You can only do that if the three are defined over the exact same probability space where the joint probabilities are well defined. Since you insist on doing the forbidden, don't blame anything else for violations. Going back to the inequality for a bit, if you insist on using the inquality and obtain a violation for scenario (b), such a violation means P(AB|..) is negative which is impossible! But of cause that is because you insisted on using an impossible probability P(AB|..) to start with so "garbage-in", "garbage out". This is what Boole published 150 years ago. Please read the article I cited earlier. |
| Jun23-12, 09:57 PM | #244 |
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1. The equation is meaningless in (b). 2. The equation is meaningful and correct in (c). 3. The equation in (c) implies the inequality in (c). 4. The inequality in (c) implies the inequality in (b) 5. The inequality is meaningful and correct in (b). Why do you see a contradiction in this? It's true that the equation doesn't apply to (b), but that is irrelevant. The reason the inequality applies to (b) is not because the equation applies to (b), but rather because the inequality applies to (c), which is ultimately because the equation applies to (c). |
| Jun24-12, 01:35 AM | #245 |
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Your argument is that no-conspirary allows you to conclude that the inequality P(C|w) <= P(A|w) + P(B|w) which is valid for scenario (c) must be valid for scenario (b), ie P(C|z) <= P(A|x) + P(B|y) because according to you the no-conspiracy implies that P(C|z) = P(C|w) and P(A|x)=P(A|w) and P(B|w)= P(B|y). This is your argument.
My argument is is the following: The inequality P(C|w) <= P(A|w) + P(B|w) is obtained from P(C|w) = P(A|w) + P(B|w) - 2P(AB|w). So if you are claiming that the inequality should apply to scenario (b) it means the equality should also apply. You can not take the inequality and reject the equality, the inequality is just a different view into the what is already there in the equality. What more do you want me to say if you refuse to see the fallacy. |
| Jun24-12, 04:04 PM | #246 |
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1. (P(A|w)+P(B|w)-P(C|w))/2=P(A & B|w) 2. P(A & B|w)≥0 3. (P(A|w)+P(B|w)-P(C|w))/2≥0 4. (P(A|x)+P(B|y)-P(C|z))/2≥0 Now I'm open in my "hiding" of a term. What I'm saying is that 1 and 2 imply 3, and even though 1 and 2 have no analogue for (b), it is nevertheless true that 3 implies 4. 1. P(C|w)≤P(A|w)+P(B|w) 2. P(A|x)=.25, P(B|y)=.25, P(C|z)=.75 3. P(A|x)=P(A|w), P(B|y)=P(B|w), P(C|z)=P(C|w) 4. P(A|w)=.25, P(B|w)=.25, P(C|w)=.75 5. .75 ≤ .25 + .25 What step do you think I'm going wrong in? |
| Jun25-12, 10:18 AM | #247 |
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2. P(A|x)=.25, P(B|y)=.25, P(C|z)=.75, P(AB|x?y?)=???????? 3. P(A|x)=P(A|w), P(B|y)=P(B|w), P(C|z)=P(C|w), P(AB|x?y?)=????????? 4. P(A|w)=.25, P(B|w)=.25, P(C|w)=.75, P(AB|w)=?? 5. .75 = .25 + .25 + ?????????????????? Steps (1), (2), (3), (4) and (5). You are hiding the dirt under the inequality "rug". Enough said. If you still do not understand my argument that's your problem. |
| Jun25-12, 10:32 AM | #248 |
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A short note that:
Bell's theorem, though fairly convincing, is not, as many of you are aware, the only "proof" of non-local action Other experiments, for example those listed below, also provide evidence of quantum entanglement - Two-photon interference - where interference is demonstrated (at a distance) without the entangled photons meeting at the beam-splitter which is not replicable via two (un-entangled) photons - Quantum entangled swapping - where photons are entangled (via their "twins") without ever meeting - improvements in Bell's test detection efficiency |
| Jun25-12, 10:46 AM | #249 |
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1. P(C|w)=P(A|w)+P(B|w)-2P(A & B)|w) 2. P(A|x)=.25, P(B|y)=.25, P(C|z)=.75 3. P(A|x)=P(A|w), P(B|y)=P(B|w), P(C|z)=P(C|w) (From no-conspiracy.) 4. P(A|w)=.25, P(B|w)=.25, P(C|w)=.75 (From 2 and 3) 5. .75 = .25 + .25 -2P(A & B|w) (From 1 and 4) 6. P(A & B|w) = -.125 (From 5) Now what step is in error? I am no longer "hiding" ill-defined probabilities like P(A & B|x) behind inequality signs. |
| Jun25-12, 05:28 PM | #250 |
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How many different ways do I have to explain this?
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