Is action at a distance possible as envisaged by the EPR Paradox.

  • #851
billschnieder said:
So then according to Bell, the P on the LHS ie equivalent to P(AB|a,b) in standard notation, where as we have agreed before a and b are place-holders for a specific value of the "random variables" a and b.

I thought you guys were using a, b as measurement settings, not hidden variables. Where/when did you switch to this notation? Lambda represents the hidden variables.
 
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  • #852
DrChinese said:
I thought you guys were using a, b as measurement settings, not hidden variables. Where/when did you switch to this notation? Lambda represents the hidden variables.
I'm still using them to mean measurement settings--perhaps Bill is too, and just called them "random variables" because it's assumed the measurement settings are to be chosen randomly by the two experimenters on each trial.
 
  • #853
Sorry, I haven't been able to keep up with this thread. I'm out of town this week and without access to his papers, but a couple of people have asked me to explain where Kracklauer is mistaken.

Again, my last exchange with him was some years ago concerning one of his published papers. In that paper I pointed out to him that his statistics assumed information concerning the detector settings at all sites was available at all sites. He confirmed this was correct. I told him that there is no mystery if this is true (and sent him a quote from Mermin to this effect, since I'm not an authority). I told him that experimentalists understand that this would have to be avoided and change polarizer settings at very high frequencies so that information concerning settings at remote sites is not available prior to recording relevant outcomes. He said I didn't know what I was talking about, so I sent him a quote from one of Aspect's papers making this same claim and never heard from him again.

That's all I know about Kracklauer.

I may not be able to tend to PF in the immediate future because I'm teaching, doing research and preparing for a conference in July. I'll get back to you after my summer research students and class are finished :-)
 
  • #854
JesseM said:
OK, this is another minor quibble, the left side is actually an expectation value. I noted earlier in post #790 that A and B in (2) were just written as functions rather than probabilities

I neglected to note there that he allows the function A(a,λ) (and likewise B(b,λ)) to take values +1 or -1 depending on the measurement result (+1 for spin-up when measured with setting a and -1 for spin-down when measured with setting a, for example). So the notation P(a,b) on the left side of the equation is the expectation value for the product of A and B, which would be equivalent to a weighted sum of four different probabilities: P(A=+1, B=+1|ab)*(+1*+1) + P(A=+1, B=-1|ab)*(+1*-1) + P(A=-1, B=+1|ab)*(-1*+1) + P(A=-1, B=-1|ab)*(-1*-1)

There now appears to be two different meanings ascribed to what Bell is doing in equation (2), which I asked you earlier several times:
1) Bell is marginalizing with respect to λ.
2) Bell is calculating an expectation value for the probability P(AB|ab)
Which one is it? I see only a single integral and no summation, and you need one for each if you are doing both.
 
  • #855
billschnieder said:
There now appears to be two different meanings ascribed to what Bell is doing in equation (2), which I asked you earlier several times:
1) Bell is marginalizing with respect to λ.
2) Bell is calculating an expectation value for the probability P(AB|ab)
Which one is it? I see only a single integral and no summation, and you need one for each if you are doing both.
Yes, I didn't notice before that the left side of (2) was an expectation value rather than a straight probability. But it's not quite an expectation value for P(AB|ab) as you suggest, it's actually an expectation value for A*B, which is equivalent to a sum over all possible combinations of values for A and B of the quantity A*B*P(AB|a,b). Remember, though, Bell is assuming that the value of A and B is completely determined by the values of a, b, and λ. So, the integral on the right of (2) is exactly equivalent to the following weighted sum of four integrals:

(+1)*(+1)\int P(A=+1, B=+1|a,b,\lambda)P(\lambda)\,d\lambda +
(+1)*(-1)\int P(A=+1, B=-1|a,b,\lambda)P(\lambda)\,d\lambda +
(-1)*(+1)\int P(A=-1, B=+1|a,b,\lambda)P(\lambda)\,d\lambda +
(-1)*(-1)\int P(A=+1, B=+1|a,b,\lambda)P(\lambda)\,d\lambda

The reason this works is because for any given value of λ, say λ=λi, three of the probabilities in the four integrals above will be equal to zero, while the other probability will be equal to 1. So by splitting up the single integral into the four above, you aren't overcounting or undercounting A*B*P(λ) for any specific value of λ, you're counting it exactly once. This is easier to see if you suppose λ can only take a discrete set of values from 0 to N, so the integral on the right side of (2) can be replaced by the sum \sum_{i=0}^N A(a,\lambda_i)*B(b,\lambda_i)*P(\lambda_i). Then if a,b,λ completely determine the values of A and B (which each take one of two values +1 or -1), that means the four-term sum (+1)*(+1)*P(A=+1,B=+1|a,b,λi) + (+1)*(-1)*P(A=+1,B=-1|a,b,λi) + (-1)*(+1)*P(A=-1,B=+1|a,b,λi) + (-1)*(-1)*P(A=-1,B=-1|a,b,λi) will always be equal to A(a,λi)B(b,λi) for each specific value of λi [for example, if a,b,λi determine that A=+1 and B=-1, then (+1)*(+1)*P(A=+1,B=+1|a,b,λi) + (+1)*(-1)*P(A=+1,B=-1|a,b,λi) + (-1)*(+1)*P(A=-1,B=+1|a,b,λi) + (-1)*(-1)*P(A=-1,B=-1|a,b,λi) = (+1)*(+1)*0 + (+1)*(-1)*1 + (-1)*(+1)*0 + (-1)*(-1)*0 = (+1)*(-1) = A(a,λi)B(b,λi)]. So, if we substitute the four-term sum in for the individual term A(a,λi)B(b,λi) in the sum over all possible values of λ I wrote above, we get:

\sum_{i=0}^N [(+1)*(+1)*P(A=+1,B=+1|a,b,\lambda_i)\,+\,(+1)*(-1)*P(A=+1,B=-1|a,b,\lambda_i)+ \,(-1)*(+1)*P(A=-1,B=+1|a,b,\lambda_i)\,+\,(-1)*(-1)*P(A=-1,B=-1|a,b,\lambda_i)]*P(\lambda_i)

Which can be split up into the following four sums:

\sum_{i=0}^N (+1)*(+1)*P(A=+1,B=+1|a,b,\lambda_i)*P(\lambda_i) +
\sum_{i=0}^N (+1)*(-1)*P(A=+1,B=-1|a,b,\lambda_i)*P(\lambda_i) +
\sum_{i=0}^N (-1)*(+1)*P(A=-1,B=+1|a,b,\lambda_i)*P(\lambda_i) +
\sum_{i=0}^N (-1)*(-1)*P(A=-1,B=-1|a,b,\lambda_i)*P(\lambda_i)

...which is just the discrete version of the four integrals I wrote before.

So, the left side is an expectation value which can be broken up into a weighted sum of four probabilities of the form P(AB|ab), and the right side can be broken up into a weighted sum of four integrals or sums over all possible values of λ of terms of the form P(AB|a,b,λ). For example, on the left side one of the four weighted probabilities is (+1)*(-1)*P(A=+1,B=-1|ab), and on the right side one of the four weighted integrals is (+1)*(-1)\int P(A=+1, B=-1|a,b,\lambda)P(\lambda)\,d\lambda. So if you take the marginalization equation P(A=+1,B=-1|a,b) = \int P(A=+1, B=-1|a,b,\lambda)P(\lambda)\,d\lambda and then multiply both sides by A*B=(+1)*(-1) and add this equation to three other marginalization equations where both sides have been multiplied by the corresponding value of A*B, you get something mathematically equivalent to equation (2) in Bell's proof.
 
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  • #856
JesseM said:
But it's not quite an expectation value for P(AB|ab) as you suggest, it's actually an expectation value for A*B, which is equivalent to a sum over all possible combinations of values for A and B of the quantity A*B*P(AB|a,b)...

One unanswered question and a few comments:
This "thing" which Bell calculates in equation (2), which you now say is an expectation value and from my initial glimpse of your explanation, it appears to be. Is the equation as it stands indicating that the numerical value represents what is obtained by measuring a specific pair of settings (ai, bi) a large number of times, or is it indicating that expectation value is what will be obtained my measuring a large number of different pairs of angles (ai,bi)? Or do you think the two are equivalent.

As a follow up of the above, in order to understand what you understand the expected value to mean: If I perform a survey in which respondents answer either ("yes") or ("no") and I know that both outcomes are equally likely, what would you say the expectation value of the survey result?
 
  • #857
billschnieder said:
One unanswered question and a few comments:
This "thing" which Bell calculates in equation (2), which you now say is an expectation value and from my initial glimpse of your explanation, it appears to be. Is the equation as it stands indicating that the numerical value represents what is obtained by measuring a specific pair of settings (ai, bi) a large number of times, or is it indicating that expectation value is what will be obtained my measuring a large number of different pairs of angles (ai,bi)? Or do you think the two are equivalent.
The first, I think he's calculating the expectation value for some specific pair of settings. If he wanted to talk about the expectation value for a variety of different ai's I think he'd need to have a sum over different values of i in there.
billschnieder said:
As a follow up of the above, in order to understand what you understand the expected value to mean: If I perform a survey in which respondents answer either ("yes") or ("no") and I know that both outcomes are equally likely, what would you say the expectation value of the survey result?
You have to assign a number to each possibility to have an expectation value. For instance, if you let yes=1 and no=2, then if they're equally likely the expectation value is 1.5, but if you let yes=-1 and no=-1, the expectation value is 0. In Bell's case he's doing something like "result of particle's measurement is spin-up"=+1 and "result of particle's measurement is spin-down"=-1.
 
  • #858
JesseM said:
The first, I think he's calculating the expectation value for some specific pair of settings. If he wanted to talk about the expectation value for a variety of different ai's I think he'd need to have a sum over different values of i in there.
JesseM said:
The first, I think he's calculating the expectation value for some specific pair of settings. If he wanted to talk about the expectation value for a variety of different ai's I think he'd need to have a sum over different values of i in there.
So then, let us consider a specific pair of settings (a, b), and presume that we have calculated an expectation value from equation (2) of Bell's paper, say E(a,b). From what you have explained above, there is going to be a specific probability distribution P(λi) over which E(a,b) was obtained, since the corresponding P(AB|ab) which you obtained your E(a,b) from, was obtained by marginalizing over a specific P(λi) . Do you agree?

Fast forward to then to the resulting CHSH inequality
|E(a,b) + E(a,b') + E(a',b) - E(a',b')| <= 2

In your opinion then, is the P(λi) the same for each of the above terms, or do you believe it doesn't matter.
 
  • #859
billschnieder said:
So then, let us consider a specific pair of settings (a, b), and presume that we have calculated an expectation value from equation (2) of Bell's paper, say E(a,b). From what you have explained above, there is going to be a specific probability distribution P(λi) over which E(a,b) was obtained, since the corresponding P(AB|ab) which you obtained your E(a,b) from, was obtained by marginalizing over a specific P(λi) . Do you agree?
If we wanted to calculate a precise expectation value, yes we'd need a specific probability distribution on the hidden variables, as well as knowledge of what value of A and B went with each possible value of λ. However, the inequalities he derives would apply to any specific choice of probability distribution in a local realist universe.
billschnieder said:
Fast forward to then to the resulting CHSH inequality
|E(a,b) + E(a,b') + E(a',b) - E(a',b')| <= 2

In your opinion then, is the P(λi) the same for each of the above terms, or do you believe it doesn't matter.
The same probability distribution should apply to each of the four terms, but the inequality should hold regardless of the specific probability distribution (assuming the universe is a local realist one and the specific experimental conditions assumed in the derivation apply).
 
  • #860
JesseM said:
The same probability distribution should apply to each of the four terms, but the inequality should hold regardless of the specific probability distribution (assuming the universe is a local realist one and the specific experimental conditions assumed in the derivation apply).
So then, if it was found that it is possible in a local realist universe for P(λi) to be different for at least one of the terms in the inequality, above, then the inequality will not apply to those situations where P(λi) is not the same. In other words, the inequalities above are limited to only those cases for which a uniform P(λi) can be guaranteed between all terms within the inequality. Do you disagree?

Do you believe, P(λi) is always uniform between all the terms in the inequality, when calculating from data acquired in Aspect-type experiments?
 
  • #861
billschnieder said:
So then, if it was found that it is possible in a local realist universe for P(λi) to be different for at least one of the terms in the inequality, above, then the inequality will not apply to those situations where P(λi) is not the same.
When you suggest the possibility that P(λi) could be "different for at least one of the terms in the inequality", that would imply that P(λi) depends on the choice of detector settings, since each expectation value is defined relative to a particular combination of detector settings. Am I understanding correctly, or are you talking about something else?

If I am understanding you right, note that it's generally accepted that one of the assumptions needed in Bell's theorem is something called the "no-conspiracy assumption", which says the decisions about detector settings should not be correlated with the values of the hidden variables. For example, this page on EPR/Bell says:
Assumption 4. The choices between the measurement setups in the left and right wings are entirely autonomous, that is, they are independent of each other and of the assumed elements of reality that determine the measurement outcomes.

Otherwise the following conspiracy is possible: something in the world pre-determines which measurement will be performed and what will be the outcome. We assume however that there is no such a conspiracy in our world.
And later on the same page:
a. Conspiracy
There is an easy resolution of the EPR/Bell paradox, if we allow the conspiracy that was prohibited by Assumption 4 (Brans 1988; Szabó 1995). It is hard to believe, however, that the “free” decisions of the laboratory assistants in the left and right wings depend on the value of the hidden variable which also determines the spins of the two particles.
Likewise the fairly rigorous-looking derivation Minimal assumption derivation of a Bell-type inequality mentions this assumption on p. 6:
D. No conspiracy

The events of type C^{+-}_{ii} are not supposed to be influenced by the measuring operations Li and Rj . One reason for this assumption is that the measurement operations can be chosen arbitrarily before the particles enter the magnetic field of the Stern-Gerlach magnets and that an event of type C^{+-}_{ii} is assumed to happen before the particles arrive at the magnets. Therefore a causal influence of the measurement operations on events of type C^{+-}_{ii} would be tantamount to backward causation. Also an inverse statement is supposed to hold: The event types C^{+-}_{ii} are assumed not to be causally relevant for the measurement operations. This is meant to rule out some kind of “cosmic conspiracy” that whenever an event of type C^{+-}_{ii} is instantiated, the experimenter would be “forced” to use certain measurement operations. This causal independence between C^{+-}_{ii} and the measurement operations is assumed to imply the corresponding statistical independence. The same is assumed to hold also for conjunctions of common cause event types. We refer to this condition as no conspiracy (NO-CONS).
So, I agree the inequality can only be assumed to hold if the choice of detector settings and the value of the hidden variables are statistically independent (which means the probability distribution P(λi) does not change depending on the detector settings), but this is explicitly included as an assumption in the more rigorous modern derivations. If you dispute that a "conspiracy" of the type being ruled out here would in fact have some very physically implausible features so that it's reasonable to rule it out, I can give you some more detailed arguments for why it's so implausible.
 
  • #862
You are wondering off now, JesseM. Try not to pre-empt the discussion. The question I asked should have a straightforward answer. The reason why P(λi) might be different shouldn't affect the answer you give to my question. If you believe P(λi) will be different when a conspiracy is involved, then you should have no problem admitting that Bell's inequalities do not apply to situations in which there is conspiracy.

Here it is again:

So then, if it was found that it is possible in a local realist universe for P(λi) to be different for at least one of the terms in the inequality, above, then the inequality will not apply to those situations where P(λi) is not the same. In other words, the inequalities above are limited to only those cases for which a uniform P(λi) can be guaranteed between all terms within the inequality. Do you disagree?

Do you believe P(λi) can different between the terms in a locally causal universe if and only if conspiracy is involved?
 
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  • #863
billschnieder said:
You are wondering off now, JesseM. Try not to pre-empt the discussion.
You are acting like a bully, Bill. You don't have dictatorial control over the terms of "the discussion", we are both allowed to contribute whatever we think is relevant. If you want to be a dictator who gets to tell me what I am and am not allowed to discuss, what questions from you I must answer, but who refuses to address topics/questions I think are relevant if you don't immediately spot the relevance yourself, I'm not going to participate in that sort of game.
billschnieder said:
The reason why P(λi) might be different shouldn't affect the answer you give to my question.
True, but for anyone following along it may still help their understanding of the physical meaning of what we're talking about to point out that the only way P(λi) could be different for the four expectation values would be if there are different probability distributions for different combinations of detector settings. We can show this with pure math, no physical reasoning whatsoever. After all, as I explained in post #855, E(a,b) for some specific pair of detector settings a and b is just defined as (sum over all possible values of A and B) of A*B*P(AB|a,b), or equivalently the same sum but for A*B*P(A,B,a,b)/P(a,b). And we can marginalize P(A,B,a,b) over λ by setting it equal to \int P(A,B,\lambda,a,b)\,d\lambda, which by the chain rule of probability is equal to \int P(A,B|\lambda,a,b)P(\lambda|a,b)P(a|b)P(b)\,d\lambda, and P(a|b)P(b) = P(a,b) so this reduces to \int P(A,B|\lambda,a,b)P(\lambda|a,b)P(a,b)\,d\lambda. So, (sum over all possible values of A and B) of A*B*P(A,B,a,b)/P(a,b) is equal to (sum over all possible values of A and B) of (A*B/P(a,b))*\int P(A,B|\lambda,a,b)P(\lambda|a,b)P(a,b)\,d\lambda, and dividing out P(a,b) gives (sum over all possible values of A and B) of A*B\int P(A,B|\lambda,a,b)P(\lambda|a,b)\,d\lambda. This looks just like the sum of four integrals in #855 which I said was equivalent to the right side of equation (2) in Bell's paper, except with P(λ|a,b) substituted in for P(λ). Along the same lines, if you wanted to calculate the expectation value for a different pair of settings like a' and b', (sum over all possible values of A and B) of A*B\int P(A,B|\lambda,a&#039;,b&#039;)P(\lambda|a&#039;,b&#039;)\,d\lambda. So, if there was a different P(λ) for each version of equation (2) calculating the expectation value for each possible pair of detector settings, just using pure math we can see that the only way this could happen was if P(λ|a,b) for one pair of detector settings is different than P(λ|a',b') for a different pair of detector settings.
billschnieder said:
If you believe P(λi) will be different when a conspiracy is involved, then you should have no problem admitting that Bell's inequalities do not apply to situations in which there is conspiracy.
Didn't I already "admit" that in my last post? Read again:
So, I agree the inequality can only be assumed to hold if the choice of detector settings and the value of the hidden variables are statistically independent (which means the probability distribution P(λi) does not change depending on the detector settings)
billschnieder said:
Do you believe P(λi) can different between the terms if and only if conspiracy is involved?
Yes, since "conspiracy" is just defined as P(λ|a,b) being different from P(λ). I showed above using pure math (no physics) that P(λ) can be different between the integrals Bell uses to calculate expectation values only if P(λ|a,b) is different from P(λ), i.e if there is a "conspiracy".
 
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  • #864
JesseM said:
You are acting like a bully, Bill. You don't have dictatorial control over the terms of "the discussion"
I haven't twisted your arm to force you to comply with my requests. All I am trying to do is have a focused discussion, which apparently is very very difficult for you to do. You have been cooperating until now, why the sudden change of heart. I ask you a simple question to which you either agree or disagree, and you go back and pull already settled issues, raise new issues, with tons of equations into the response as if you want to drown the the real issue. I understand you like to write a lot and you have every right, but for once could you please make an effort to just stick to the point?

So then, I will assume that the last few posts did not happen, and I will consider that the responses moving forward are as follows:
So then, if it was found that it is possible in a local realist universe for P(λi) to be different for at least one of the terms in the inequality, above, then the inequality will not apply to those situations where P(λi) is not the same. In other words, the inequalities above are limited to only those cases for which a uniform P(λi) can be guaranteed between all terms within the inequality. Do you disagree?
... I agree ...
Do you believe P(λi) can different between the terms if and only if conspiracy is involved?
Yes ...
See how short and to the point this would have been. You would have saved yourself all the typing effort, and to boot, we don't have to start a new rabbit trail about the meaning of "conspiracy"! Your answer presented as precisely above would already have incorporated your view about what "conspiracy" means, but the fact that it is precise enables use to continue the discussion on topic. But if you now define conspiracy in a manner that I don't agree with, I will be forced to challenge it because if I don't it may appear as though I agree with that definition, then we end up 20 posts later, discussing whose definition of "conspiracy" is correct, having left the original topic. The more you write, the more things need to be challenged in your posts and the more off-topic the discussions will get. This is why I insist that the discussion be focused. I hope you will recognize and respect this, otherwise there is no point continuing this discussion.
 
  • #865
billschnieder said:
I haven't twisted your arm to force you to comply with my requests.
The only way a person can "twist someone's arm" over the internet is by adopting a demanding or aggressive tone whenever the other person doesn't comply with their requests, and that's exactly what you've done.
billschnieder said:
All I am trying to do is have a focused discussion, which apparently is very very difficult for you to do. You have been cooperating until now, why the sudden change of heart. I ask you a simple question to which you either agree or disagree, and you go back and pull already settled issues, raise new issues, with tons of equations into the response as if you want to drown the the real issue.
Again, I bring these things up because I want anyone else reading the discussion to understand exactly what various conditions entail. I have answered your questions, and you are perfectly free to ignore the extra points I make if they don't seem relevant to you, so there is absolutely no need for you to berate me and imply I am trying to obscure the issue just because I don't confine myself to the shortest possible answers. Like I said, it just seems like bullying for the sake of bullying, unless you can give a practical rationale for why including some extra points in a post that already answers all the questions you asked is going to prevent you from developing whatever point you intend to make.
billschnieder said:
So then, I will assume that the last few posts did not happen, and I will consider that the responses moving forward are as follows:
So then, if it was found that it is possible in a local realist universe for P(λi) to be different for at least one of the terms in the inequality, above, then the inequality will not apply to those situations where P(λi) is not the same. In other words, the inequalities above are limited to only those cases for which a uniform P(λi) can be guaranteed between all terms within the inequality. Do you disagree?

... I agree ...

Do you believe P(λi) can different between the terms if and only if conspiracy is involved?

Yes ...
See how short and to the point this would have been. You would have saved yourself all the typing effort, and to boot, we don't have to start a new rabbit trail about the meaning of "conspiracy"!
There is no "rabbit trail" about the meaning, it's a technical term with a single well-defined meaning in the context of a discussion of assumptions needed in deriving Bell inequalities. "Conspiracy" in this context is defined in terms of P(λ) being different from P(λ|ab) (i.e. a statistical dependence between hidden variables and measurement state), I was just pointing out that this official definition is actually equivalent to your own comment about P(λ) being different for different expectation values, but it's not instantly obvious that they're equivalent, so for pedagogical reasons I was explaining why (again, even if this explanation is not interesting to you it may be helpful for others reading).

And speaking of "short and to the point", there's no need for you to elaborately berate me about how much time I could have saved or how you will "assume that the last few posts did not happen", you could just quote the part of the posts that are relevant to you and respond to that.
billschnieder said:
Your answer presented as precisely above would already have incorporated your view about what "conspiracy" means, but the fact that it is precise enables use to continue the discussion on topic.
But as I said, it wouldn't have made clear how the standard definition relates to the fact that P(λ) can only differ for different expectation values if a "conspiracy is involved" (which is not the standard way of defining it).
billschnieder said:
But if you now define conspiracy in a manner that I don't agree with, I will be forced to challenge it because if I don't it may appear as though I agree with that definition, then we end up 20 posts later, discussing whose definition of "conspiracy" is correct, having left the original topic.
There would be no need for an extended debate about the meaning of a technical term like "conspiracy", a condition that can be expressed as a simple equation, any more than there would about other technical terms that can be expressed in terms of equations like "energy" or "force". Our debate about "probability" was because we weren't debating the purely mathematical aspects (like the fact that the sum of probabilities of all possible outcomes must always be 1, and individual probabilities can never be negative), but were debating philosophical interpretations of the meaning of the mathematical symbols and how they apply to the real world.
billschnieder said:
The more you write, the more things need to be challenged in your posts and the more off-topic the discussions will get. This is why I insist that the discussion be focused. I hope you will recognize and respect this, otherwise there is no point continuing this discussion.
I don't recognize that the hypothetical you mention actually applies to this discussion. In fact you didn't need to challenge anything in my definition of the no-conspiracy assumption, so going on about how I need to keep it short is completely gratuitous here. In other situations where you have challenged me on less straightforward mathematical issues, I would say that the debates were central to the main issues we were disagreeing about, like how the frequentist definition of a "population" of hypothetical experiments shows why an Aspect-type experiment will naturally be a "fair sample", something you were continually asserting it wouldn't be unless we precisely controlled for the values of all hidden variables (just bringing this up as an example, the actual debate on this point can continue on the other thread).
 
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  • #866
Well JesseM,
Thank you then for your cooperation so far, and I won't bother you again. Unfortunately I can not continue the discussion like this when you are unable to stay on topic. Despite my complaints, you continue in like manner as if though secretly hope I will abandon the discussion. So you get your wish. Anyone else following the discussion who is interested in finding out where I was going with the line of questioning is welcome to PM me.
 
  • #867
billschnieder said:
Despite my complaints, you continue in like manner as if though secretly hope I will abandon the discussion. So you get your wish.
It's not my wish that the discussion stop, it's just that you haven't provided any practical justification for why I should change my posting style (as I already pointed out, I did answer all your questions so nothing is stopping you from just responding to the parts of my posts that are relevant to your argument and ignoring the rest), and your requests amount to little more than "shut up and answer exactly the way I tell you to, not the way you want to" (and the tone of your requests is only marginally more civil than that). Again it pretty much just seems like bullying to me, and while I'm happy to continue the discussion in a civil and adult manner, I'm not going to cede total control over my own posting style just because you bark orders at me.
 
  • #868
DevilsAvocado said:
Could you please show me one title, link, or paper-id?
One? There's a bunch, and they're legit. As ajw1 pointed out, you're the one who provided the links in the first place. (thanks again) You might consider clicking on the links to some of the papers and actually reading them.

--- snip ---

DevilsAvocado said:
... Crackpot Kracklauer is just too much, and I will never back off from this, never.
What is it? Do you have some personal history with this guy or something?

DevilsAvocado said:
Supporting Crackpot Kracklauer must be against all and everything in Physics Forums Global Guidelines ...
You've presented what so far seems to be a groundless personal attack on a physicist who's got some interesting papers (several in peer reviewed journals), the conclusions of which are, apparently, contrary to certain views which, apparently, you've emotionally bonded with. So, who's the crackpot deviating from the PF guidelines?

Now, DA, I'm not saying you're a crackpot, in fact my understanding is that you've gotten into the Bell-EPR stuff relatively recently. This was the case, at one time or another, for everyone (including Zeilinger, DrC, Kracklauer, RUTA, JesseM, and even Einstein and Bell) who's been interested in the implications of a certain, call it 'realistic', view of how theories of quantum experimental phenomena might be formulated. These considerations involve semantics, logic and physics. What I ask of you is that you not attack anyone as a 'crackpot' until you fully understand everything involved in their particular view. This will take some time. As DrC might confirm, I've revisited this topic several times, have changed my approach (my way of thinking about it) several times, and I'm still not sure that I fully understand everything involved. So, please, don't be so quick to dismiss someone as a 'crackpot' unless and until you fully understand exactly what it is that they're saying. And, when you do fully understand the arguments involved, then I think that you will just deal with the arguments.
I hope that you stay interested in this and continue to learn, as I hope to do.

In connection with this, I think it's important that I learn as much about OPDC as I can. That's my next agenda, and so after my next few posts in this thread I won't be contributing to it.
 
  • #869
DrC, thanks for your elaboration on your 'requirement' for candidate local realistic models of entanglement. I still don't understand what you're saying. I think the best thing to do is to start a new thread on this. Which I will do tonight.
 
  • #870
JesseM, thanks for your thoughtful post #842. I don't want to nitpick (but I will be thinking about the questions you've posed). I want you to understand why I don't understand why some people present Bell's theorem as implying that nature is nonlocal. I look at the experimental setups involved and I see a local optical 'explanation' for the observed correlations. I've talked to maybe two dozen working experimental physicists about this and they agree.

As far as the form of Bell's (2) is concerned, it represents the experimental situation in a factorable form, which means that it reduces to an expression that the data sets A and B are independent. Is this how you see it?

Should I start a new thread on this?
 
  • #871
RUTA said:
... his statistics assumes that knowledge of detector settings is available at both detection sites.

ThomasT said:
This 'global' knowledge is available via the data processing and analysis. Isn't it?

RUTA said:
I wrote him a detailed email explaining that experiments change polarization settings at very high frequencies precisely so info about Alice's detector settings is not available to Bob and vice versa.

ThomasT said:
While it's true that the settings are changed rapidly and randomly, it's also true that for any given time-matched pair of detection attributes there's an associated pair of polarizer settings. The statistics associated with any given run would include all of that. "Wouldn't they?

I've only just glanced at the paper so far. If you can point out where his error appears, that would be appreciated.

RUTA said:
Sorry, I haven't been able to keep up with this thread. I'm out of town this week and without access to his papers, but a couple of people have asked me to explain where Kracklauer is mistaken.

Again, my last exchange with him was some years ago concerning one of his published papers. In that paper I pointed out to him that his statistics assumed information concerning the detector settings at all sites was available at all sites. He confirmed this was correct. I told him that there is no mystery if this is true (and sent him a quote from Mermin to this effect, since I'm not an authority). I told him that experimentalists understand that this would have to be avoided and change polarizer settings at very high frequencies so that information concerning settings at remote sites is not available prior to recording relevant outcomes. He said I didn't know what I was talking about, so I sent him a quote from one of Aspect's papers making this same claim and never heard from him again.

That's all I know about Kracklauer.

I may not be able to tend to PF in the immediate future because I'm teaching, doing research and preparing for a conference in July. I'll get back to you after my summer research students and class are finished :-)
Please reply to my specific questions.

You stated that Kracklauer's "statistics assumed information concerning the detector settings at all sites was available at all sites." Isn't it true that at the conclusion of a run this info is available ... to the global observer, the experimenter? So, I'm suggesting that maybe Kracklauer's objection to your criticism was valid.

As I've asked, if you can point out the specific error in Kracklauer's analysis, then that woud be appreciated.
 
  • #872
ThomasT said:
JesseM, thanks for your thoughtful post #842. I don't want to nitpick (but I will be thinking about the questions you've posed). I want you to understand why I don't understand why some people present Bell's theorem as implying that nature is nonlocal. I look at the experimental setups involved and I see a local optical 'explanation' for the observed correlations. I've talked to maybe two dozen working experimental physicists about this and they agree.
Well, can you present your local optical explanation in detail, either here or on a new thread? You'll need to present it in enough quantitative detail that we can calculate what measurement outcome will occur (or what the probability is for different outcomes) given knowledge of a detector settings and the local hidden variables at the location of the measurement (like the 'polarization vector' of the particle being measured, if that's your hidden variable).
ThomasT said:
As far as the form of Bell's (2) is concerned, it represents the experimental situation in a factorable form, which means that it reduces to an expression that the data sets A and B are independent. Is this how you see it?
No, A and B are not independent in their marginal probabilities (which determine the actual observed frequencies of different measurement outcomes), only in their probabilities conditioned on λ. I've asked whether you understand the distinction a bunch of times and you never answer. If you'd like to see a numerical example where there's a statistical dependence in marginal probabilities but not when conditioned on some other variable I could easily provide it.
 
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  • #873
ThomasT said:
Please reply to my specific questions.

You stated that Kracklauer's "statistics assumed information concerning the detector settings at all sites was available at all sites." Isn't it true that at the conclusion of a run this info is available ... to the global observer, the experimenter? So, I'm suggesting that maybe Kracklauer's objection to your criticism was valid.

As I've asked, if you can point out the specific error in Kracklauer's analysis, then that woud be appreciated.

That the information is available AFTER the fact doesn't bear on a possible CAUSE for the correlations. The point is that the detector setting at site A is NOT available to site B BEFORE the detection event occurs at site B. If this information is available prior to detection, the correlations in the outcomes can be orchestrated to violate Bell's inequality. No one disputes this fact -- you have to keep the outcome at each site dependent ONLY upon information AT THAT SITE to have the conundrum about their correlations.

Thus, there are generally two ways to account for EPR-Bell correlations. 1) The detection events are separable and you have superluminal exchange of information. 2) The detection events are not separable, e.g., the spin of the entangled electrons is not a property of each electron. The first property is often called "locality" and the second property "realism."

Kracklauer's statistics simply assumed detector setting information was available at each site prior to detection outcomes. When I discussed this with him at a conference, he was adamant that the outcome at each site was contingent upon outcomes and settings at other sites so the "proper" statistics had to contain this fact. His whole argument was that we needed to use the "proper" statistics and the mystery would disappear. His "proper" statistics just assume global knowledge of detector settings. But, unless he has a proposal for how this information is available, he has done nothing to resolve the mystery. How is this information available? FTL signals or nonseparability? Or both? What is the mechanism? All he had was a statistical counterpart to the mystery, although it could be published if no one else had pointed this out. But, nothing was "resolved."
 
  • #874
ThomasT said:
One? There's a bunch, and they're legit. As ajw1 pointed out, you're the one who provided the links in the first place. (thanks again) You might consider clicking on the links to some of the papers and actually reading them.

Here’s http://arxiv.org/find/all/1/all:+Kracklauer/0/1/0/all/0/1" of Crackpot Kracklauer’s 21 papers on arXiv.org. Where is the "bunch" of peer reviewed papers? These two are peer reviewed before 2000:

egz343.png


And the only one peer reviewed after 2000, is this one:

2whmntl.png


These 2 mumbling pages of a rebuttal of http://en.wikipedia.org/wiki/David_Mermin" , and this was his last paper that made it thru a scientific journal.

(Note that http://www.springer.com/physics/journal/10701" , which resulted in the takeover of Gerard ‘t Hooft as Editor-in-Chief in 2007.)


ThomasT said:
What is it? Do you have some personal history with this guy or something?

The question is why you risk all your credibility for a 100% crackpot as A. F. Kracklauer? Didn’t you watch the http://video.google.com/videoplay?docid=-1112934842741515675" ? Crackpot Kracklauer thinks QM mainstream physics are wrong! And we are not talking a little 'disagreement' around Bell (2) – everything is wrong according to Crackpot Kracklauer!

A completely lost "independent researcher" with a crazy homepage at freehosting.com, and you are supporting this guy!? Why??

I know you dislike nonlocality very much, and are fighting to find a "solution". But don’t you think this is a 'little' too "far out"? This man has a mental problem:
A. F. Kracklauer - Non-loco Physics
"Loco'' (Spanish for 'crazy'). Contemporary Physics is vexed by some really "loco'' ideas, with nonlocality and asymmetric aging leading the list.
...
A second motivation is sociological. Some see a mutual interplay between fundamental science and the development of civilization. If this notion is accepted, then physics, as a social enterprise, has some responsibility to support those things making positive contributions to civilization by being the exemplar of rationality, contrary to the current fashion of spewing forth ever new and more exotic pop-psycho-sci-fi contrivances, i.e., loco ideas.


Convinced yet? No? How about this 'excellent' paper by Crackpot Kracklauer?


(Edit: Crackpot Kracklauer’s fancy host freehosting.com doesn’t allow direct linking to PDF, use http://www.google.com/search?hl=en&...ing.com/ws01.pdf&aq=f&aqi=&aql=&oq=&gs_rfai=" instead.)
http://www.nonloco-physics.000freehosting.com/ws01.pdf"
ABSTRACT. Of the various “complimentarities” or “dualities” evident in Quantum Mechanics (QM), among the most vexing is that afflicting the character of a ‘wave function,’ which at once is to be something ontological because it diffracts at material boundaries, and something epistemological because it carries only probabilistic information. Herein a description of a paradigm, a conceptual model of physical effects, will be presented, that, perhaps, can provide an understanding of this schizophrenic nature of wave functions. It is based on Stochastic Electrodynamics (SED), a candidate theory to elucidate the mysteries of QM. The fundamental assumption underlying SED is the supposed existence of a certain sort of random, electromagnetic background, the nature of which, it is hoped, will ultimately account for the behavior of atomic scale entities as described usually by QM.
In addition, the interplay of this paradigm with Bell’s ‘no-go’ theorem for local, realistic extentions of QM will be analyzed.

Have you ever heard of the "SCHIZOPHRENIC NATURE of wave functions" before?


Still not convinced? How about this?

(Edit: Crackpot Kracklauer’s fancy host freehosting.com doesn’t allow direct linking to PDF, use http://www.google.com/search?hl=en&....pdf&btnG=Search&aq=f&aqi=&aql=&oq=&gs_rfai=" instead.)
http://www.nonloco-physics.000freehosting.com/abort.pdf"
Does quantum mechanics have anything to do with abortion? Something, maybe. Quantum mechanics is the theory that encodes the mathematical patterns involved in the chemical bond. The chemical bond, in turn, writ big, or rather, writ oft, is the tool for assembling DNA, the crucial stuff of living matter. So, as the non plus ultra of life, the quantum mechanical chemical bond, may well have some relevance to abortion too, as an event affecting life.

When did you last hear a "scientist" speculate around quantum mechanics and ABORTION?

As I said – this is the worst crackpot I have ever seen, and I think you should make it very clear that you are not backing up this man and his totally crazy ideas. This is not science.


ThomasT said:
So, who's the crackpot deviating from the PF guidelines?

I think you owe me an apology.
 
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  • #875
DevilsAvocado said:
As I said – this is the worst crackpot I have ever seen,...
There's worse, much worse... :smile:
 
  • #876
my_wan said:
There's worse, much worse... :smile:

Please! Don’t tell me! I don’t think I can take it anymore...
(What’s next? A Bayesian 'cranky theory' "proving" that the Earth is flat and in the center of the Solar system and the Universe! :biggrin:)
 
  • #877
A. F. Kracklauer - Non-loco Physics
"Loco'' (Spanish for 'crazy'). Contemporary Physics is vexed by some really "loco'' ideas, with nonlocality and asymmetric aging leading the list.
...
A second motivation is sociological. Some see a mutual interplay between fundamental science and the development of civilization. If this notion is accepted, then physics, as a social enterprise, has some responsibility to support those things making positive contributions to civilization by being the exemplar of rationality, contrary to the current fashion of spewing forth ever new and more exotic pop-psycho-sci-fi contrivances, i.e., loco ideas.
Just noticed this--apparently the guy wants to disprove relativistic time dilation as well! You can see him making some ridiculous arguments against time dilation experiments (which have established 'asymmetric aging' beyond any reasonable doubt) in publication 4, "analysis of and remedy for asymmetric aging (twin paradox)", on this page of his site.
 
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  • #878
RUTA said:
Thus, there are generally two ways to account for EPR-Bell correlations. 1) The detection events are separable and you have superluminal exchange of information. 2) The detection events are not separable, e.g., the spin of the entangled electrons is not a property of each electron. The first property is often called "locality" and the second property "realism."

Great description, RUTA!

To those that try to dissect the words and formulae of Bell (and I count myself in that group sometimes): You can see from RUTA's description that locality and separability can have meanings and implications that can somewhat be interchanged by your choice of base definitions or perspectives.

For example: Norsen (mentioned earlier in the discussion here) sees Bell (2) as defining separability, and he equates that with locality. So separability is spatial/temporal. On the other hand, RUTA is classifying separability according to wave functions. Particles that share a wave function do not have independent (separable) observables - which leans towards the realistic side of the subject.

Further: Norsen sees lack of separability as automatically indicating we live in a non-local universe. Thus c is not a constraint on influences from elsewhere. On the other hand, RUTA (and I probably shouldn't supply words when RUTA can speak for himself) might tend to see lack of separability as indicative that the observer and observed systems are themselves not independent. This perspective was specifically mentioned in the 1935 EPR paper, although EPR rejected this option as not "reasonable" (because that would make the reality of one system dependent on the nature of observation made on another). Unreasonable or not, if it is considered as an option then there are no contradictions with Bell.

Lastly, there is the issue of mechanism. Once you reject local realism, can you account for the "how"? In the Bohmian view, there is action at a distance and c is not respected. Apparently, and I am not suitably versed in this department, the action potential of one particle upon another does not diminish with distance. In the view of RUTA (see more on Relational Blockworld at http://arxiv.org/abs/0908.4348 ): the mechanism can be accounted for without action at distance. However, there are elements whereby the future and the past interact; and this provides the basis for what might appear as action at a distance (even though c is fully respected). I don't think "interact" is the correct word as RBW is sort of Zen-like in its description; there are no events exactly. But I will ask RUTA to correct any misconceptions I have introduced; ditto on the Bohmian side: Maaneli, Demystifier?

So this is some very interesting stuff.
 
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  • #879
ThomasT said:
I look at the experimental setups involved and I see a local optical 'explanation' for the observed correlations. I've talked to maybe two dozen working experimental physicists about this and they agree.

So you are saying that there are a number (24 that you know) of people who all are familiar with the same local realistic mechanism for explaining entanglement "optically". And yet I have never even heard of this. Does it have a name so I can look it up? Or is just "the mechanism everybody else knows about" that hasn't yet been published? Or maybe... just maybe... you should consider supplying a reference when you make claims like this.
 
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  • #880
DevilsAvocado said:
21 papers on arXiv.org. Where is the "bunch" of peer reviewed papers? These two are peer reviewed before 2000
...
And the only one peer reviewed after 2000, is this one:
...

Either you are just being dishonest, or you can not count, or maybe you do not know what a peer reviewed article means, or you do not know how to find peer reviewed articles. Here is a list from the page you linked to.

  • On the nature of information-erasing , Journal of Modern Optics, Volume 54, Numbers 16-17, November 2007 , pp. 2365-2371(7)
  • Nonlocality, Bell's Ansatz and Probability Optics and Spectroscopy. 103 (3) 451-450 (2007)
  • "What's wrong with this rebuttal,"Found. Phys. Lett. 19 (6) 625-629 (2006).
  • ``Quantum'' beats in classical physics,, J. of Russian Laser Research 26 (6) 524-529 (2005)
  • Oh Photon, Photon, whither art thou gone?, in: Proceedings of SPIE, 5866 (2005).
  • EPR-B correlations: non-locality or geometry?, J. Nonlinear Math. Phys. 11(Supp.) 104-109 (2004).
  • EPR-B correlations: quantum mechanics or just geometry?, J. Opt. B (Semiclass. & Quant.) 6 S544-S548 (2004)
  • Exclusion of correlation in the theorem of Bell, in: Foundations of Probability and Physics-2, 385-398
  • One less quantum mystery, J. Opt. B (Semiclass. & Quant.) 4, S469-S472 (2002)
  • Is entanglement always entangled?, J. Opt. B (Semiclass. & Quant.) 4, S121-S126 (2002)
  • ``Complementarity'' or Schizophrenia: is Probability in Quantum Mechanics Information or Onta?, in: Foundations of Probability and Physics, 219-235 (2001)
  • The Improbability of Non-locality, Phys. Essays, 15(2) 162-171 (2002)
  • La `theorem' de Bell, est-elle al plus grand meprise de l'histoire de la physique?, Ann. Fond. L. de Broglie 25(2) 193-207 (2000)
  • Pilot wave steerage: a mechanism and test, Found. Phys. Lett. 12(2) 441-453 (1999).
  • Objective Local Models for Would-be Nonlocal Physics, in: Instantaneous aad: Pro & Contra, 363-372 (1999).
  • An Intuitive Paradigm for Quantum Mechanics, Phys. Essays 5 (2) 226-234 (1992)
  • A theory of the electromagnetic two-body interaction. J. Math. Phys. 19(4) 838-841 (1978)
  • Comment on: Classical derivation of Planck Spectrum, Phys. Rev. D 14, 654-655 (1976)
  • On the Imaginable Content of de Broglie Waves, Scientia, 109 ,111-120 (1974).
  • Comment on: Derivation of Schroedinger's Equation from Newtonian Mechanics, Phys. Rev. D 10(4) 1358-1360 (1974).
  • A geometric proof of no-interaction theorems, J.Math Phys. 17(5) 693-694 (1974)

Ad-hominem http://dictionary.reference.com/browse/ad+hominem
1. appealing to one's prejudices, emotions, or special interests rather than to one's intellect or reason.
2. attacking an opponent's character rather than answering his argument.
http://en.wikipedia.org/wiki/Ad_hominem
Ad hominem abusive
Ad hominem abusive usually involves insulting or belittling one's opponent, but can also involve pointing out factual but ostensible character flaws or actions which are irrelevant to the opponent's argument. This tactic is logically fallacious because insults and even true negative facts about the opponent's personal character have nothing to do with the logical merits of the opponent's arguments or assertions.
...
Guilt by association
Guilt by association can sometimes also be a type of ad hominem fallacy, if the argument attacks a source because of the similarity between the views of someone making an argument and other proponents of the argument.
This form of the argument is as follows:

Source A makes claim P.
Group B also make claim P.
Therefore, source A is a member of group B.
Fallacy -- http://en.wikipedia.org/wiki/Fallacy
In logic and rhetoric, a fallacy is a misconception resulting from incorrect reasoning in argumentation. By accident or design, fallacies may exploit emotional triggers in the listener or interlocutor (e.g. appeal to emotion), or take advantage of social relationships between people (e.g. argument from authority). Fallacious arguments are often structured using rhetorical patterns that obscure the logical argument
 
  • #881
  • #882
JesseM said:
Just noticed this--apparently the guy wants to disprove relativistic time dilation as well! You can see him making some ridiculous arguments against time dilation experiments (which have established 'asymmetric aging' beyond any reasonable doubt) in publication 4, "analysis of and remedy for asymmetric aging (twin paradox)", on this page of his site.


Well, what can I say?? The man is a "crackpot miracle"... It’s not only QM that’s "totally wrong"! Albert Einstein also goes down the Crackpot-Kracklauer-Drain??

(I sure hope Crackpot Kracklauer doesn’t use GPS in his car, because this would not work without QM atomic clocks + SR/GR correction for time dilation effects and gravitational frequency shift!)

This is remarkable... ThomasT & billschnieder thinks Crackpot Kracklauer is a "great scientist"...


JesseM, I really admire yours (and DrC’s) enormous patience and great skills, in trying to educate users like billschnieder. To me it looks like ThomasT has shown some willingness to an honest intellectual discussion and some openness to input and logical argumentation. But billschnieder on the other hand, is a wall of weird preconceptions, mainly based on the crazy ideas of Crackpot Kracklauer. That’s why your discussion ended the way it did. You did all you could – but it was a dead end from the beginning.

And there are other terrible examples of billschnieder’s 'technique' in other threads on PF (I tried to warn you).

I’m only a layman. I don’t have the great skills and deep knowledge you and many others here posses. But I do think I have one 'skill' – common sense and ability to judge what’s reasonable or not (which some "sophisticated gentlemen" in this thread apparently lacks).

Crackpot Kracklauer is not reasonable.


I must apologize to all "casual readers" for this "unpleasant episode" in this thread. I generally don’t find it interesting or productive to start "fights". But this was an exception, and someone had to push the "alarm button".

I hope we all can continue to discuss the matters of EPR and Bell's Theorem in an open, stimulating and productive way, as before.

I’m working on some "new" material from John Bell himself, never shown or discussed on PF. I think (hope) everyone will find it (very) interesting. I’m a little short of time at the moment, but I hope I can get it ready for 'publishing' ASAP.

Again – Sorry for the latest "mess".

/DA
 
  • #883
DrChinese said:
Great description, RUTA!

I agree! Captain RUTA is a great teacher! And most of all I admire him for implementing this little 'tips':

"Everything should be made as simple as possible, but not simpler" -- Albert Einstein
 
  • #884
billschnieder said:
Ad-hominem
Fallacy

Please billschnieder, you are making a fool of yourself.
 
  • #886
DevilsAvocado said:
... And the only one peer reviewed after 2000, is this one: ...
Are you being intentionally dishonest about this? All anyone has to do is go to the guy's website and click on the links to see that what you're saying wrt the number of papers he's published (since 1999) in peer reviewed journals is false. There's at least 8 by my count, maybe more. A couple were published in the same journals that Stuckey (RUTA) has published in.

DevilsAvocado said:
The question is why you risk all your credibility for a 100% crackpot as A. F. Kracklauer? ... A completely lost "independent researcher" with a crazy homepage at freehosting.com, and you are supporting this guy!? Why??
Where did I say that I support his ideas? I did say that some of his stuff looked like it might be interesting, and that he seemed to have a clear writing style.

I don't like what I see as your personal attack on someone whose views you happen to oppose. I'm not familiar with Kracklauer's stuff, but I intend to get around to reading it. Until then, I can't speak to whether or not I think any of his ideas or arguments are right or wrong. But even if I eventually conclude that ALL of his ideas and arguments are wrong, I certainly won't be calling him names because of it.

For a while in this thread you were following a line of reasoning, and I was enjoying your posts (even if I didn't agree with all your reasoning or tentative conclusions -- though some I did agree with -- not that that matters). But I don't see the utility in your current line of personal attacks. You can pursue your political agenda in another forum (or maybe not). Anyway, this is a science forum, and this is a thread about the grounds for assuming that nature is nonlocal. If you want to make an argument, or present an idea about that, then fine, but the personal stuff is annoying. Bottom line, I don't care if Kracklauer is crazy or not. If he's got any good ideas then I want to know about them. Eventually, though probably not real soon, I'll find out for myself.

DevilsAvocado said:
I know you dislike nonlocality very much, and are fighting to find a "solution".
I couldn't care less if nonlocality or ftl exist or not. In fact, it would be very exciting if they did. But the evidence just doesn't support that conclusion.

The scientific method requires two basic questions be answered whenever some new property of reality or some paradigm changing, revolutionary view of reality is proposed. (1) What do you mean, and (2) how do you know? If you'd like to contribute to the effort to answer those questions, to discern the truth from the fiction wrt nonlocality and related considerations, then that would be a welcome change from your recent postings.

DevilsAvocado said:
But don’t you think this is a 'little' too "far out"? This man has a mental problem:

A. F. Kracklauer - Non-loco Physics
"Loco'' (Spanish for 'crazy'). Contemporary Physics is vexed by some really "loco'' ideas, with nonlocality and asymmetric aging leading the list.
...
A second motivation is sociological. Some see a mutual interplay between fundamental science and the development of civilization. If this notion is accepted, then physics, as a social enterprise, has some responsibility to support those things making positive contributions to civilization by being the exemplar of rationality, contrary to the current fashion of spewing forth ever new and more exotic pop-psycho-sci-fi contrivances, i.e., loco ideas.
Well, he's saying that physical science should be an exemplar of rationality. Nothing crazy about that. Now, I will say that my superficial impression of his ideas on asymmetric or differential aging seems to be contrary to the way I've learned to think about it. That is, I believe that differential aging is pretty much a demonstrated fact of nature. But, I haven't read his paper(s) on this yet. So, I don't know exactly what he's saying about this, or his arguments. By themselves, the above quotes don't seem crazy. Even if they're grossly wrong, that doesn't imply that the guy is crazy. And if he has an agenda, even a personal one, that influences his approach and reasoning, well, I don't think that's at all unusual, and certainly not an indicator of 'mental illness'. Maybe in your imagination there are scientists whose work isn't influenced by 'nonscientific' factors.

"Complementarity" or Schizophrenia: is Probability in Quantum Mechanics Information or Onta?
ABSTRACT. Of the various “complimentarities” or “dualities” evident in Quantum Mechanics (QM), among the most vexing is that afflicting the character of a ‘wave function,’ which at once is to be something ontological because it diffracts at material boundaries, and something epistemological because it carries only probabilistic information. Herein a description of a paradigm, a conceptual model of physical effects, will be presented, that, perhaps, can provide an understanding of this schizophrenic nature of wave functions. It is based on Stochastic Electrodynamics (SED), a candidate theory to elucidate the mysteries of QM. The fundamental assumption underlying SED is the supposed existence of a certain sort of random, electromagnetic background, the nature of which, it is hoped, will ultimately account for the behavior of atomic scale entities as described usually by QM.
In addition, the interplay of this paradigm with Bell’s ‘no-go’ theorem for local, realistic extentions of QM will be analyzed.
I think the title was intended to get attention -- so that people would actually read the paper. Nothing crazy about that. Despite the fact that he might be, strictly speaking, using the term 'schizophrenia' incorrectly, I don't have an opinion wrt the merits of the content of the paper, not having read it yet. Have you read it?

The quantum mechanics of abortion
Does quantum mechanics have anything to do with abortion? Something, maybe. Quantum mechanics is the theory that encodes the mathematical patterns involved in the chemical bond. The chemical bond, in turn, writ big, or rather, writ oft, is the tool for assembling DNA, the crucial stuff of living matter. So, as the non plus ultra of life, the quantum mechanical chemical bond, may well have some relevance to abortion too, as an event affecting life.
When I first read this, I thought that maybe the guy really is crazy -- like maybe another abortion nut or whatever. But since the paper was only one page, I read it. He seems to be making a very reasonable social commentary.

He concludes with:

In any case, in the end quantum mechanics throws little light on these standards, except from its essentially probabilistic nature. This feature tells us that bond formation needs no ‘breath of life,’ or other mystical ingredient, it is a random event, it just happens, sometimes for no good reason. All the above seems to imply that science and logic can not be used to unequivocably evaluate abortion ethically. For what it’s worth, the morally superior stance, surely is the one which, no matter how and when life starts and ends, tends to cause people to turn to it less often. Practically this means avoiding unwanted pregnancies beforehand by promoting reproductive hygiene, and then providing material and financial support for single or disadvantaged mothers who failed with prevention afterwards. It is regrettable that an all too common sort of mental confusion, especially in the voting booth, leads ‘right-to-lifers’ themselves to become opponents of these practical means to actually reduce the occasions for abortion, thereby serving effectively as champions of the ‘evil’ they themselves disparage!

DevilsAvocado said:
When did you last hear a "scientist" speculate around quantum mechanics and ABORTION?

As I said – this is the worst crackpot I have ever seen, and I think you should make it very clear that you are not backing up this man and his totally crazy ideas. This is not science.
Right. It's not science. Nor, I think, is it meant to be taken as such. It's an essay that presents some interesting and reasonable observations by a scientist with an active social conscience. Keep in mind that the US is full of Christian fanatics who would twist any scientific finding or paradigm to support their religious agendas. Kracklauer's program, it seems to me so far, is to oppose that sort of thing and also to oppose what some might see as an increasing tendency toward metaphysical constructions and 'mysticism' in 'mainstream' physics.

So, if that's all you've got, then 'case dismissed', as they say. From what I've seen so far, I think you owe Kracklauer and the contributors to, and observers of, this thread an apology. However, if you really just want to discredit the guy, then keep digging. That should at least keep you busy, and hopefully not posting your personal attacks, for a while. But keep in mind that your posts regarding Kracklauer are quite off topic. Maybe, eventually, some thoughtful moderator is going to inform you of that.
 
  • #887
JesseM said:
Well, can you present your local optical explanation in detail, either here or on a new
thread? You'll need to present it in enough quantitative detail that we can calculate
what measurement outcome will occur (or what the probability is for different outcomes)
given knowledge of a detector settings and the local hidden variables at the location of
the measurement (like the 'polarization vector' of the particle being measured, if that's
your hidden variable).
It isn't 'my' optical explanation. It's optics. There's two polarizers, a and b. They can both be on side A, or both be on side B, or one on each side. There's a randomly varying optical vector extending between the two polarizers. The resultant, measured, joint intensity of the light (the coincident photon flux) will vary as cos^2 (a-b). Of course the exact calculation will depend on the setup, but the point is that whenever crossed polarizers are jointly analyzing light from a random source, then this optical law applies.

I'm no expert, so if there's something essentially wrong with this, then let me know. If it's, in principle, ok, then I don't see any reason to suppose that anything nonlocal or ftl is happening.

Further, as DrC pointed out, a slight rotation of a wave plate is all that's necessary to produce polarization entanglement in certain OPDC Bell tests. Again, this doesn't suggest anything nonlocal or ftl to me. Does it to you?

So, this is the first problem I have with the assumption of nonlocality -- that there's nothing wrt Bell test setups and results, sans Bell's theorem (Bell inequalities) which warrants the assumption of nonlocality. If you put both polarizers on side A or side B, you get the same results as when you put one polarizer at A and one at B. But we don't think that anything nonlocal is going on when we have both polarizers on side A or side B. These are just simple polariscopic setups. But the joint results are the same as when we have one polarizer at A and one at B. So, why does this latter setup require a 'nonlocal' explanation? Well, the way I currently think about it, it doesn't.

The same sort of reasoning applies to OPDC setups where a slight rotation of a wave plate produces entanglement statistics wrt joint polarization measurements. Should I assume that this slight rotation has somehow precipitated nonlocal or ftl 'communications' in some realm underlying that of electromagnetic radiation? This just seems a bit silly to me. But if you can convince me otherwise, then I'm all ears, so to speak.

JesseM said:
No, A and B are not independent in their marginal probabilities (which determine the
actual observed frequencies of different measurement outcomes), only in their
probabilities conditioned on λ. I've asked whether you understand the distinction a
bunch of times and you never answer.
I don't think the distinction matters. No matter how it's parsed, or how one chooses to express probability analogs for Bell's (2), the bottom line is that the joint probability is being modeled as the product of the separate probabilities. So, no matter what was intended, the form of Bell's (2) effectively models the two resultant data sets as independent. This was Bell's explicit expression of locality. The problem is that its intended function as an expression of locality is superceded by its effective function as an expression of statistical independence between the data sets.
 
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  • #888
DrChinese said:
So you are saying that there are a number (24 that you know) of people who all are familiar with the same local realistic mechanism for explaining entanglement "optically". And yet I have never even heard of this. Does it have a name so I can look it up? Or is just "the mechanism everybody else knows about" that hasn't yet been published? Or maybe... just maybe... you should consider supplying a reference when you make claims like this.
I was referring to casual conversations over the course of 8 or 9 years. So, no, you wouldn't have heard of 'it'. I would describe an optical Bell test setup, recount the results, and ask them if they thought the results indicated that any sort of 'nonlocal' or ftl 'communication' was necessary to understand them, and they would say no. I don't know exactly how many physicists I engaged in these conversations, but the impression I got was that none of them thought that anything mysterious (beyond the mystery of light itself) was going on in the experiments we discussed. The consensus was that it's just optics as usual -- ie., the correlations are due to the joint analysis of random polarizations by crossed polarizers.

Positing the existence of disturbances propagating at > c^9 (or 'instantaneously', whatever that might mean) is a nifty way to account for the correlations in optical Bell tests, but it just seems to me, and apparently lots of others (including Mermin, Jaynes, 't Hooft, etc.), to be too simplistic a solution to the conundra presented by the various interpretations of Bell's theorem. Anyway, those who do choose to advocate nonlocality as an 'explanation' are then left with the formidable task of explaining the explanation. So far, it's just metaphysics. But don't get me wrong, I like metaphysical speculations. It's just that I like them to be well grounded in accepted physics -- and, unfortunately, nonlocality isn't.

DrChinese said:
...if you accept Malus - combined with the assumption that there is a specific but unknown polarization for entangled photons - then probably you would conclude that Bell (2) is false.
Well, Malus Law is an empirically well established optical law. And since we know from experiments that, assuming that nature is evolving in accordance with the principle of local action, Bell's (2) is false, then what should we conclude? That there is some nonlocal or ftl 'mechanism' at work in entanglement situations, or that Bell's (2) simply misrepresents the experimental situation? What's being suggested is that the latter alternative is the more reasonable hypothesis, and that this hypothesis has yet to be definitively dismissed.
 
  • #889
ThomasT said:
It isn't 'my' optical explanation. It's optics. There's two polarizers, a and b. They can both be on side A, or both be on side B, or one on each side. There's a randomly varying optical vector extending between the two polarizers. The resultant, measured, joint intensity of the light (the coincident photon flux) will vary as cos^2 (a-b)
Your claim here is completely ill-defined. What is "joint intensity" supposed to mean in the context of optics? It appears to be completely meaningless in the context of classical optics, where there are no probabilities and thus no joint probabilities. Now, it's true that if the polarization of a light beam is v and the angle of the polarizer is a, then in classical optics the reduction in intensity as the light goes through the polarizer will be cos^2(a-v), that's just Malus' law. In quantum physics intensity is proportional to photon number, so are you suggesting that for a beam with polarization v passing through a polarizer at angle a, each photon has a probability of cos^2(a-v) of passing through the polarizer? And then the "joint intensity" would be based on imagining photons are sent to the different detectors in pairs, so the probability both photons make it through the detectors would be cos^2(a-v)*cos^2(b-v)? If so, this would not give a probability of cos^2(a-b) that both photons make it through (I showed this in my third-to-last paragraph of this post, a section you never responded to even when I reposted that paragraph in a later post).
ThomasT said:
I don't think the distinction matters. No matter how it's parsed, or how one chooses to express probability analogs for Bell's (2), the bottom line is that the joint probability is being modeled as the product of the separate probabilities.
Huh? The joint probability P(AB) is not being modeled as the product of P(A)*P(B) by Bell's equation. Do you disagree?
 
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  • #890
ThomasT said:
I was referring to casual conversations over the course of 8 or 9 years. So, no, you wouldn't have heard of 'it'. I would describe an optical Bell test setup, recount the results, and ask them if they thought the results indicated that any sort of 'nonlocal' or ftl 'communication' was necessary to understand them, and they would say no. I don't know exactly how many physicists I engaged in these conversations, but the impression I got was that none of them thought that anything mysterious (beyond the mystery of light itself) was going on in the experiments we discussed. The consensus was that it's just optics as usual -- ie., the correlations are due to the joint analysis of random polarizations by crossed polarizers.

Once again, you completely ignored the fact that this is false and you have NO reference for an outlandish statement. I would like to see this from any textbook. Quit stating your opinion by placing it in the mouth of unnamed others.

Reference, citation = ??
 
  • #891
JesseM said:
Huh? The joint probability P(AB) is not being modeled as the product of P(A)*P(B) by Bell's equation. Do you disagree?

ThomasT doesn't follow this correctly and keeps returning to something that is completely wrong. So this is intended for ThomasT:

1) If optics were the ruling issue, we would see Product State statistics. And those are different than what are observed. Product State stats are .5(.5+cos^2(theta)).

2) Entangled state statistics APPEAR to match Malus but that is something of a coincidence. Yes, it is cos^2(theta). And that is the Malus formula. But that is where it ends. If Malus applied, you would actually get the formula in 1) above.

Entanglement is a PURELY quantum effect and there is NO optical analog. I don't know how many different ways I can say this to make ThomasT understand it.
 
  • #892
DrC,
Perhaps you can be more clear. When you say:
1) If optics were the ruling issue, we would see Product State statistics.

Is this not essentially equivalent to saying, based on optics alone, that given theta = x then 2theta = 2x?, or some linear multiple for all theta. Malus law doesn't work this way even in standard optics.

I don't see using Malus law to show the same behavior pattern as relevant in resolving the issue, but neither does calling a one to one quantitative correspondence only an apparent match make much sense to me. As noted, by itself it doesn't resolve the realism issue, and standard optics allows a greater range of presumptions about how this result might be classical. The simplest of such presumptions being unequivocally ruled out by EPR correlation experiments. Yet perhaps you could be more specific in claiming an exact numerical match is an illusion.

Perhaps the rebuttal should involve the extra constraints BI imposes on possible mechanisms, rather than simply claiming the a quantitative correspondence is an illusion. Because I really don't think you can demonstrate that Malus law, standard optics, allows arbitrary choices of theta that leads to linear polarizer path statistics.

To illustrate, consider a standard polarized beam of light. Take the polarization of the light beam to be something other than theta = 0, and offset the polarizer/detector from the light beam on that same coordinate system. It breaks Malus law when you demand arbitrary coordinate choices, even in standard optics. This same demand that is insisted on to model EPR correlations that is also broken in standard optics.

Yes, I think these issues are fundamentally related. No, I don't think simply pointing out the relationship within standard optics, by itself, represents a resolution to the issue. The fact that it could be interpreted differently within the context of standard optics ignores the extra properties/things relationship constraints that EPR correlation experiments are sensitive to.
 
  • #893
my_wan said:
I don't see using Malus law to show the same behavior pattern as relevant in resolving the issue, but neither does calling a one to one quantitative correspondence only an apparent match make much sense to me.
"One to one quantitative correspondence" between what and what? the cos^2 in Malus' law is for the difference between the angle of a polarizer and the polarization angle of a beam hitting it at the same location, the cos^2 in entanglement experiments is for the difference in angles between two polarizers at completely different locations making measurements on different particles. There's no way to use the first cos^2 law to derive the second one, whatever ThomasT may think.
my_wan said:
As noted, by itself it doesn't resolve the realism issue, and standard optics allows a greater range of presumptions about how this result might be classical.
Why a "greater range of presumptions"? Standard optics can be derived from Maxwell's laws, which is a perfect example of a local realist theory of physics, so Bell's theorem definitely applies to anything in optics (and it's impossible to use classical optics to get a violation of Bell inequalities).
my_wan said:
To illustrate, consider a standard polarized beam of light. Take the polarization of the light beam to be something other than theta = 0, and offset the polarizer/detector from the light beam on that same coordinate system. It breaks Malus law when you demand arbitrary coordinate choices, even in standard optics. This same demand that is insisted on to model EPR correlations that is also broken in standard optics.
Malus' law is only based on the difference in angle between the beam and the polarizer, so it doesn't get violated depending on how your coordinate system defines the angle of the beam. Are you suggesting otherwise?
 
  • #894
DrChinese said:
Once again, you completely ignored the fact that this is false and you have NO reference for an outlandish statement.
Ok, so you don't think that a randomly varying polarization vector being jointly analyzed by crossed polarizers is a good way to think about it? Then how about when you put both polarizers on the same side? How would you think about that situation?

DrChinese said:
1) If optics were the ruling issue, we would see Product State statistics. And those are different than what are observed. Product State stats are .5(.5+cos^2(theta)).
2) Entangled state statistics APPEAR to match Malus but that is something of a coincidence. Yes, it is cos^2(theta). And that is the Malus formula. But that is where it ends. If Malus applied, you would actually get the formula in 1) above.
3) Entanglement is a PURELY quantum effect and there is NO optical analog.
1) Well, these are optics experiments, so why wouldn't optics be the ruling issue?
2) Do you think that Malus Law doesn't apply in quantum optics?
3) Statements like this don't do it for me. The goal is to understand the correlations, not keep them mysterious. If you want to think that something nonlocal or ftl kicks in simply because single photons are being detected, or because a polarizer has been moved, or a wave plate adjusted, then ok. I guess we'll just have to agree to disagree about the prospects for a better understanding of quantum optical experiments, and quantum entanglement.
 
  • #895
JesseM said:
Your claim here is completely ill-defined.
I'm somewhat noted for that.

JesseM said:
What is "joint intensity" supposed to mean in the context of optics?
We're talking about optical Bell tests, right? I think I phrased it as the 'coincidental photon flux'.

In certain optical Bell tests the coincidence rate is proportional to cos^2(a-b). From your knowledge of quantum optics, do you think that that indicates or requires that something nonlocal or ftl is happening in those experiments?

JesseM said:
The joint probability P(AB) is not being modeled as the product of P(A)*P(B) by Bell's equation. Do you disagree?
My thinking has been that it reduces to that. Just a stripped down shorthand for expressing Bell's separability requirement. If you don't think that's ok, then how would you characterize the separability of the joint state (ie., the expression of locality) per Bell's (2)?
 
  • #896
ThomasT said:
3) Statements like this don't do it for me. The goal is to understand the correlations, not keep them mysterious. If you want to think that something nonlocal or ftl kicks in simply because single photons are being detected, or because a polarizer has been moved, or a wave plate adjusted, then ok.
Bell's theorem doesn't depend on the fact that "single photons are being detected", but it does require that each measurement setting can yield one of two binary outcomes akin to "spin-up" and "spin-down". You are free to design your detectors in a classical optics experiment so that they can only yield two outcomes rather than a continuous range of intensities--for example, you design it so that if the intensity of the light that made it through the polarizer was above a certain threshold a red light would go off, and if the intensity was at or below that threshold a green light would go off. Likewise you might design the detector so the probability or a red light going off vs. a green light going off would depend on the reduction in intensity as the light went through the polarizer--say if the intensity was reduced by 70%, there'd be a 70% chance the red light would go off and a 30% chance the green light would go off.

But no matter how you design the experiment, as long as each detector setting can yield only one of two possible results, and the two measurements are made at a spacelike separation, no experiment which obeys the laws of classical optics will violate Bell's inequalities. Do you disagree? If you do, please give specifics on the design of the experiment you are imagining, detailing how the light's polarization and the detector setting determine which of two outcomes occur on each trial (as I did in the two examples above). If you can't fill in these basic details, then your claims that there is an "optical" explanation for Bell-inequality-violating quantum correlations are obviously not very well thought-out.
 
  • #897
JesseM said:
There's no way to use the first cos^2 law to derive the second one, whatever ThomasT may think.
I'm just trying to understand the correlation between the angular difference in the polarizer settings and coincidental detection. It doesn't 'seem' mysterious. That is, the optics principle that applies to the observed coincidence count when both polarizers are on one side, would seem to be applicable when there's one polarizer on each side.
 
  • #898
JesseM said:
"One to one quantitative correspondence" between what and what? the cos^2 in Malus' law is for the difference between the angle of a polarizer and the polarization angle of a beam hitting it at the same location, the cos^2 in entanglement experiments is for the difference in angles between two polarizers at completely different locations making measurements on different particles.
The cos^2 in Malus Law is the functional relationship between the angular difference of two polarizer settings and the measured intensity of the light transmitted by the analyzing polarizer.

You can demonstrate Malus Law in an optical Bell test by simply taking the polarizer on side A and putting it on side B.

Interestingly, P(AB) remains .5cos^2(a-b) when this is done, and we wouldn't think that anything nonlocal was happening in that situation -- would we?
 
  • #899
my_wan said:
To illustrate, consider a standard polarized beam of light. Take the polarization of the light beam to be something other than theta = 0, and offset the polarizer/detector from the light beam on that same coordinate system. It breaks Malus law when you demand arbitrary coordinate choices, even in standard optics. This same demand that is insisted on to model EPR correlations that is also broken in standard optics.
I don't understand what you're saying here.
 
  • #900
my_wan said:
DrC,
Perhaps you can be more clear. When you say:
1) If optics were the ruling issue, we would see Product State statistics.

Is this not essentially equivalent to saying, based on optics alone, that given theta = x then 2theta = 2x?, or some linear multiple for all theta. Malus law doesn't work this way even in standard optics.

I don't see using Malus law to show the same behavior pattern as relevant in resolving the issue, but neither does calling a one to one quantitative correspondence only an apparent match make much sense to me. As noted, by itself it doesn't resolve the realism issue, and standard optics allows a greater range of presumptions about how this result might be classical. The simplest of such presumptions being unequivocally ruled out by EPR correlation experiments. Yet perhaps you could be more specific in claiming an exact numerical match is an illusion.

Perhaps the rebuttal should involve the extra constraints BI imposes on possible mechanisms, rather than simply claiming the a quantitative correspondence is an illusion. Because I really don't think you can demonstrate that Malus law, standard optics, allows arbitrary choices of theta that leads to linear polarizer path statistics.

To illustrate, consider a standard polarized beam of light. Take the polarization of the light beam to be something other than theta = 0, and offset the polarizer/detector from the light beam on that same coordinate system. It breaks Malus law when you demand arbitrary coordinate choices, even in standard optics. This same demand that is insisted on to model EPR correlations that is also broken in standard optics.

Yes, I think these issues are fundamentally related. No, I don't think simply pointing out the relationship within standard optics, by itself, represents a resolution to the issue. The fact that it could be interpreted differently within the context of standard optics ignores the extra properties/things relationship constraints that EPR correlation experiments are sensitive to.

The issue is that in standard optics, there is NOT perfect correlation of light beams - even when they are created together with symmetric (or anti-symmetric) polarizations. So as you mention, the "extra properties" are only present in an entangled (EPR) state. There is nothing optically that relates too this and that is why I am trying to drive the point home. Which is that there are no classical optics that have the EPR state present. The EPR state only occurs with a suitable superposition, and there is no classical analog to this. (Specifically, the states must be indistinguishable.)
 

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