EPR Debate: Nature Agrees with Einstein

  • Thread starter Thread starter JohnBarchak
  • Start date Start date
  • Tags Tags
    Epr
  • #51
DrChinese said:
Yes, sure, you can make any prediction you want to.

I will repeat: QM itself does NOT lead to negative probabilities. LR does if it matches the predictions of QM. These are two completely different scenarios even though they sound like they are the same. Local reality makes assumptions that QM does not.
OK I must be missing something on the assumtions: - before we run a test how can we accept a LR prediction of "anything it wants". We don't need to run a test to reject invalid predictions as we should be able to show a prediction to be invalid, based on the standards of the predicting theroy.
SO predictions are invalid or acceptable based on: -- First let's review:

[1] A+ B+ C+
[2] A+ B+ C-
[3] A+ B- C+
[4] A+ B- C-
[5] A- B+ C+
[6] A- B+ C-
[7] A- B- C+
[8] A- B- C-
Total probability 1.0 100% of 8 permutations

Three tests holding one Variable unknown (??)
Each test 4 permutations for 100%
Predictions: (C using 22.5 Degrees)
Test ?? - Corr - - NonCorr - Predict - BY:
A&B (C) [1,2,7,8] [3,4,5,6] 1.0 0.0 : QM & LR both
A&C (B) [1,3,6,8] [2,4,5,7] .14 .86 : QM ;; LR?
B&C (A) [1,4,5,8] [2,3,6,7] .14 .86 : QM ;; LR?
Statistical Math gives us:
A&B(NonCorr) + A&C(Corr) – B&C(NonCorr) = [1,3,6,8] + [3,4,5,6] - [1,4,5,8]
Result 0.0 + .14 - .86 = [1][3][6][8] + [3][4][5][6] - [1][4][5][8]
[3] [3] [6] [6] = -.72
[3][6]= -.36 or - 36% (Negative probability !)
(I can see where 45 degrees or 0.5 & 0.5 would not reveal this problem)

Before we even consider running a test, we know the LR (Local Realist) cannot predict .14 & .86 due to the negative probability that would predict for permutations [3][6] together! The LR position must agree with the validity of the Statistical Math as being a requirement part of the LR and a prediction of .14 & .86 on its face would be contrary to the LR view and assumtions BECAUSE: ...?

However from the QM view the Statistical Math is not even considered or referred to since the assumption and principal view of QM does not agree that the above Statistical Math would apply to this case at all BECAUSE: ...?

Therefore before running the test we know that the only realistic prediction that the LR based on LR assumtions & view (and such test results validate the LR view) WOULD BE: ...?
 
Physics news on Phys.org
  • #52
RandallB said:
1. Before we even consider running a test, we know the LR (Local Realist) cannot predict .14 & .86 due to the negative probability that would predict for permutations [3][6] together!

2. The LR position must agree with the validity of the Statistical Math as being a requirement part of the LR and a prediction of .14 & .86 on its face would be contrary to the LR view and assumtions BECAUSE: ...?

3. However from the QM view the Statistical Math is not even considered or referred to since the assumption and principal view of QM does not agree that the above Statistical Math would apply to this case at all BECAUSE: ...?

4. Therefore before running the test we know that the only realistic prediction that the LR based on LR assumtions & view (and such test results validate the LR view) WOULD BE: ...?

1. Yes, exactly, this is what Bell pointed out.

2. Because, as you showed, negative probabilities result and that is an un-physical result.

3. Because QM already had the Heisenberg Uncertainty Relations (with its h), and had accepted that there were limits to the description of physical reality. (The realist position is that there is no absolute limit.)

4. LR must predict differing values from QM, since the .14 and .86 are the predictions of QM. So the LR advocate has a problem as now QM and LR must go their separate ways.

Keep in mind that we are in the world of "designer" theories in which theories can be constructed ad hoc to fit various scenarios. Of course, 99.99% of these are totally useless and most of those are a complete waste of time. QM is the .01% that is useful.

So if you (or someone else) want to construct a theory which can be disproven before testing, then there is no law against it other than it wastes time. There are also those who hold out hope that all existing published EPR tests will somehow be thrown out in the future.
 
  • #53
DrChinese said:
There are also those who hold out hope that all existing published EPR tests will somehow be thrown out in the future.
Yes, for example me, and not without good reason.

I've studied many reports of actual experiments and discovered alternative local realist explanations for all the results. In some experiments it's just a matter of the data having been adjusted in a manner that makes sense under QM but not under local realism. The adjustment increases the Bell test statistics, turning (in the specific instances for which I have the data) results that comply with the inequality into ones that do not. In other experiments, the "detection" or "fair sampling" loophole is open. This loophole crept into the experiments as a result of sleight of hand! It is related to the use of an inequality for which an unbiased estimate demands that each term be divided by the number of emitted pairs. The test used in practice involves division by the number of detected pairs and is simply not valid.

There are other loopholes, different ones (or combinations of them) being relevant in different experiments. See my website or a page I contributed to wikipedia:
http://en.wikipedia.org/wiki/Bell_test_loopholes

Caroline
http://freespace.virgin.net/ch.thompson1/
 
Last edited by a moderator:
  • #54
Caroline Thompson said:
In some experiments it's just a matter of the data having been adjusted in a manner that makes sense under QM but not under local realism.

Caroline:
DrChinese's comment:
"LR must predict differing values from QM, since the .14 and .86 are the predictions of QM."
Makes no sense to me.
Just because one method/theory (QM) makes a prediction (A legit one based on that theory) cannot be justification for denying any other approach from making exactly the same prediction as long as it's legit within that other theory.
A credible argument as to why LR is wrong should at least define the prediction LR must make (Say for 22.5 degrees), within the definition of LR.
I guess Dr Chinise dosn't know or care as he's in a position to already "know" that even if it agrees with QM it's wrong.

You have at least implied that there are results that if reached during testing would support LR over QM. (Hence your concern over the apparent "adjusted" data favoring QM).

My main question then: in an example like 22.5 degrees, does LR make a prediction different than QM?
What is it ??
Are we talking about a tiny difference like .001% or less that is making this so hard to test?


Personally I wonder about the usefulness of Polarization testing, because it seems to me that a classical view, as I'd see it, would agree with 14% and 85% that QM predicts. But I suspect my "classical view" may not be consistent with the rules for LR. I can deal with that later.
For now I'd be impressed if someone could just explain what the LR prediction actually is for 22.5 degrees.

RB
 
  • #55
RandallB said:
Caroline:
DrChinese's comment:
"LR must predict differing values from QM, since the .14 and .86 are the predictions of QM."
Makes no sense to me.
Just because one method/theory (QM) makes a prediction (A legit one based on that theory) cannot be justification for denying any other approach from making exactly the same prediction as long as it's legit within that other theory.
A credible argument as to why LR is wrong should at least define the prediction LR must make (Say for 22.5 degrees), within the definition of LR.
I guess Dr Chinise dosn't know or care as he's in a position to already "know" that even if it agrees with QM it's wrong.

I will repeat: Bell's Theorem (and not DrChinese) precludes LR and QM from making the same predictions.

Also: As I have said before, some LR theories make predictions outside of the Bell Inequality. I have repeatedly asked for other values to discuss. In one of these provided by Caroline, the difference between LR and QM is large: 1.000 for QM vs. .7500 for LR at 0 degrees; .8536 for QM vs. .6768 for LR at 22.5 degrees (correlated cases). However, they agree at 45 degrees.
 
  • #56
DrChinese said:
I will repeat: Bell's Theorem (and not DrChinese) precludes LR and QM from making the same predictions.

Also: As I have said before, some LR theories make predictions outside of the Bell Inequality. I have repeatedly asked for other values to discuss. In one of these provided by Caroline, the difference between LR and QM is large: 1.000 for QM vs. .7500 for LR at 0 degrees; .8536 for QM vs. .6768 for LR at 22.5 degrees (correlated cases). However, they agree at 45 degrees.
You're just not reading me, DrChinese! The figures are meaningless. The idea that LR predicts just one figure is wrong: LR represents the genuine scientific approach to modelling the real world, and it is absolutely right and proper that it should give a different result for each experiment. The exact experimental conditions vary.

That's one point. The other is that if the experimenters in practice pursue the aim of obtaining as high a visibility to their coincidence curves as they can (by using suitably low beam intensities, for instance, with the nominal aim of obtaining the "single photon level"), then they will land up, if they are lucky, with curves of almost 100% visibility. They will be very nearly exactly sinusoidal. Both LR and QM agree on this, so naturally there is no problem for LR theory in agreeing with your figures and with experiment, so long as we look only at the normalised data, where the normalisation is done with respect to the detected pairs! Had we normalised with respect to the emitted pairs, the figures would have looked very different. All coincidence rates would have been well below the QM prediction.

As far as I know, there has been only one exception to this -- the Rowe et al experiment using trapped ions. Here almost every emission was detected, so the two methods of normalisation coincide. As the whole world recognises, though, the experiment did not satisfy the basic requirements of a Bell test: the ions were very close together, the settings of the detectors may not have been independent, and the measurements made did not even pretend to be independent. [See M Rowe et al, “Experimental violation of a Bell’s inequality with efficient detection”, Nature 409, 791 (2001)]

Caroline
http://freespace.virgin.net/ch.thompson1/
 
Last edited by a moderator:
  • #57
Caroline Thompson said:
You're just not reading me, DrChinese! The figures are meaningless. The idea that LR predicts just one figure is wrong: LR represents the genuine scientific approach to modelling the real world, and it is absolutely right and proper that it should give a different result for each experiment. The exact experimental conditions vary.

That's one point. The other is that if the experimenters in practice pursue the aim of obtaining as high a visibility to their coincidence curves as they can (by using suitably low beam intensities, for instance, with the nominal aim of obtaining the "single photon level"), then they will land up, if they are lucky, with curves of almost 100% visibility. They will be very nearly exactly sinusoidal. Both LR and QM agree on this, so naturally there is no problem for LR theory in agreeing with your figures and with experiment, so long as we look only at the normalised data, where the normalisation is done with respect to the detected pairs! Had we normalised with respect to the emitted pairs, the figures would have looked very different. All coincidence rates would have been well below the QM prediction.

I recognize that you postulate added parameters in experimental situations - one being beam intensity. So you should be able to put this in terms of a specific prediction, shouldn't you? I simply ask for a value to compare against the experimental results so we can rule a specific theory as "in" or "out". As best I see, all current LR theories are ruled out by experiment. But perhaps your added parameters would fix everything (although I personally don't see how that is possible).

Assume the added parameter "beam intensity" comes into the equation. You state that QM and your LR theories give identical predictions when this parameter is low. But this would then violate the Bell Inequality, no?
 
  • #58
DrChinese said:
I recognize that you postulate added parameters in experimental situations - one being beam intensity. So you should be able to put this in terms of a specific prediction, shouldn't you?
I'm afraid not. In the general formula for the local realist prediction we have a function that gives, effectively, the probability of detection as a function of intensity. The exact form of this function depends on the particular make of detector used. The only way I can think of to find this function is to do some supplementary tests using different input intensities and seeing what happens. You have to be careful, though, what physical mechanism you use to vary the intensity! You'd expect one answer if you vary the number of pulses per second, a different one if you vary the strength of each individual pulse. It is mainly the latter that is of interest for Bell tests. The polariser, in the "classical" model, is assumed to reduce the intensity of the indivual pulses.

I simply ask for a value to compare against the experimental results so we can rule a specific theory as "in" or "out". As best I see, all current LR theories are ruled out by experiment. But perhaps your added parameters would fix everything (although I personally don't see how that is possible).
You're absolutely right! Take account of all the messy details and your LR solution will reveal itself.

Assume the added parameter "beam intensity" comes into the equation. You state that QM and your LR theories give identical predictions when this parameter is low. But this would then violate the Bell Inequality, no?
I can't guarantee exact equality of the predicitions, only agreement with experiment. Yes, the results may very well violate an invalid Bell inequality, but they will never violate a valid one.

Caroline
 
  • #59
I've read through this thread, perhaps not quite carefully enough, and here's where my head is at at the moment:
- QM can predict the outcome of an experiment (accurately)
- LR can match the outcome of an experiment (accurately)
- QM's predictions apply across a range of experiments, of several different kinds
- LR cannot make 'before the experiment' predictions (the exact details are unknowable?)
- QM's predictions are general, with no ad hoc components
- LR's post-experiment analyses are ad hoc
- both QM and LR analyses of experimental results are consistent with the Bell inequality
- there have been no experiments conducted - to date - which proponents of LR regard as definitive tests of the Bell Inequality
- there have been many experiments conducted - to date - which proponents of QM regard as definitive test of the Bell Inequality
- proponents of LR have not (yet) proposed an experiment (or class of experiment) which, if conducted properly, would yield a good result which would unambiguously distinguish LR from QM
- proponents of QM have proposed many experiments which, if conducted properly, would yield good results which would unambiguously distinguish LR from QM.
 
  • #60
Hi Nereid

Hmmm ... Most of your points seem correct. However, I think the position re proposals for experiments that would in fact discriminate between QM and LR is that local realists (and there are, unfortunately, not many of these who have the courage to stand up and be counted) have from time to time suggested such experiments and been ignored. [The journals have not been helpful re publicising them.]

I think one could prove the matter one way or the other if only a sufficiently comprehensive set of tests were to be done, covering a wide range of parameters.

Caroline
http://freespace.virgin.net/ch.thompson1/
 
Last edited by a moderator:
  • #61
Nereid
The seemingly circular logic needed to get to where your head is at oddly enough makes the most sense to me. I’m still not sure I have a clear understanding of the LR.
So allow me my translate and you or someone can let me know if I have the LR right.

In the case of “entangled particles” for polarization testing this would be a pair of photons generated simultaneously and heading in opposite directions. With a “LR” observing one of these in Area A while the other is headed off though area B.
LR and QM both agree that the testing in area A (just sending the photon through a polarizing filter) permanent changes that photon, and is no longer the same as it was prior to arriving at the filter.
However, QM claims by going through the filter in area A the photon actually traveling in area B is affected and can test differently then it would have, were no testing to be done on the photon in area A.

LR presumes the testing in area A has had no affect at all on the other photon in area B.

-- Just want to be sure I have this basics of how each view understands “entanglement”.
And if I’m understanding the above correctly would it be proper to say the LR view disagrees with the idea of “entanglement”?
 
  • #62
RandallB said:
---And if I’m understanding the above correctly would it be proper to say the LR view disagrees with the idea of “entanglement”?

Hello--I have been watching here for some time--very interesting postings. Please excuse my posts until I get the hang of the system-

One additional question relating to the above quote: Is it also proper to say that the LR view disagrees with the concept of "Superposition" and that of the Photon being a particle? I read a lot of history in here-but never saw this addressed.. Thanks,Photongod
 
  • #63
RandallB,

However, QM claims by going through the filter in area A the photon actually traveling in area B is affected and can test differently then it would have, were no testing to be done on the photon in area A.

QM doesn't claim that. It claims you will know of the state of particle B only if you measure it, and further notes that when it is measured, you find correspondence to particle A.
 
  • #64
Quantum Mechanics Meets Reality

It is clear that the quantum world is non-local. But that world has almost nothing to do with reality.

In "Towards Quantum Information Theory in Space and Time", http://arxiv.org/PS_cache/quant-ph/pdf/0203/0203030.pdf
Igor V. Volovich shows us that modern quantum information theory deals with an idealized situation where the spacetime dependence of quantum phenomena is neglected.

In "Local Realism, Contextualism and Loopholes in Bell`s Experiments"
http://arxiv.org/PS_cache/quant-ph/pdf/0212/0212127.pdf
Volovich and Andrei Khrennikov demonstrate that if we include into the quantum mechanical formalism the space-time structure in the standard way then quantum mechanics might be consistent with Einstein's local realism.

Volovich is of the opinion that QM can be fixed. To me, that seems
roughly equivalent to trying to fix the Titanic, but let's look at his
proposal.

Quantum Mechanics Meets Reality
Igor Volovich, in "Seven Principles of Quantum Mechanics", looks at
bringing QM closer to reality:

"INTRODUCTION
Most discussions of foundations and interpretations of quantum
mechanics take place around the meaning of probability, measurements,
reduction of the state and entanglement. The list of basic axioms of
quantum mechanics as it was formulated by von Neumann [1] includes
only general mathematical formalism of the Hilbert space and its statistical interpretation, see also [2]-[6]. From this point of view any mathematical proposition on properties of operators in the Hilbert space can be considered as a quantum mechanical result. From our point of view such an approach is too general to be called foundations of Quantum mechanics.

We have to introduce more structures to treat a mathematical scheme
as quantum mechanics. These remarks are important for practical
purposes. If we would agree about the basic axioms of quantum mechanics and if one proves a proposition in this framework then it could be considered as a quantum mechanical result. Otherwise it can be a mathematical result without immediate relevance to quantum theory. An important example of such a case is related with Bell's inequalities. It is known that the correlation function of two spins computed in the four-dimensional Hilbert space does not satisfy the Bell inequalities. This result is often interpreted as the proof that quantum mechanics is inconsistent with Bell's inequalities. However from the previous discussion it should be clear that such a claim is justified only if we agree to treat the four-dimensional Hilbert space as describing a physical quantum mechanical system. In quantum information theory qubit, i.e. the two-dimensional Hilbert space, is considered as a fundamental notion.

Let us note however that in fact the finite-dimensional Hilbert space should be considered only as a convenient approximation for a quantum mechanical system and if we want to investigate fundamental properties of quantum mechanics then we have to work in an infinitedimensional Hilbert space because only there the condition of locality in space and time can be formulated. There are such problems where we can not reduce the infinite-dimensional Hilbert space to a finite-dimensional subspace.

We shall present a list from seven axioms of quantum mechanics. The
axioms are well known from various textbooks but normally they are not combined together. Then, these axioms define an axiomatic quantum
mechanical framework. If some proposition is proved in this framework then it could be considered as an assertion in axiomatic quantum mechanics. Of course, the list of the axioms can be discussed but I feel that if we fix the list it can help to clarify some problems in the foundations of quantum mechanics.

For example, as we shall see, the seven axioms do not admit a nontrivial realization in the four-dimensional Hilbert space. This axiomatic framework requires an infinite-dimensional Hilbert space. One can prove that Bell's inequalities might be consistent with the correlation function of the localized measurements of spin computed in the infinite-dimensional Hilbert space [16, 20]. Therefore in this sense we can say that axiomatic quantum mechanics is consistent with Bell's inequalities and with local realism. It is well known that there are no Bell's type experiments without loopholes, so there is no
contradiction between Bell's inequalities, axiomatic quantum mechanics and experiments, see [21].

There is a gap between an abstract approach to the foundations and the very successful pragmatic approach to quantum mechanics which is essentially reduced to the solution of the Schroedinger equation. If we will be able to fill this gap then perhaps it will be possible to get a progress in the investigations of foundations because in fact the study of solutions of the Schroedinger equation led to the deepest and greatest achievements of quantum mechanics.

In this note it is proposed that the key notion which can help to build a bridge between the abstract formalism of the Hilbert space and the practically useful formalism of quantum mechanics is the notion of the ordinary three-dimensional space. It is suggested that the spatial properties of quantum system should be included into the list of basic axioms of quantum mechanics together with the standard notions of the Hilbert space, observables and states. Similar approach is well known in quantum field theory but it is not very much used when we consider foundations of quantum mechanics.

Quantum mechanics is essentially reduced to the solution of the Schroedinger equation. However in many discussions of the foundations of quantum mechanics not only the Schroedinger equation is not considered but even the space-time coordinates are not mentioned (see for example papers in [6]). Such views to the foundations of quantum mechanics are similar to the consideration of foundations of electromagnetism but without mentioning the Maxwell equations.

Here I present a list from seven basic postulates of quantum mechanics which perhaps can serve as a basis for further discussions.
The axioms are: Hilbert space, measurements, time, space, composite
systems, Bose-Fermi alternative, internal symmetries. In particular the list includes the axiom describing spatial properties of quantum system which play a crucial role in the standard formalism of quantum mechanics. Formulations of the axioms are based on the material from [1]-[20]. The main point of the note is this: quantum mechanics is a physical theory and therefore its foundations are placed not in the Hilbert space but in space and time."

The complete paper may be found at:
http://arxiv.org/PS_cache/quant-ph/pdf/0212/0212126.pdf

References
[1] John von Neumann. Mathematical Foundations of Quantum Mechanics,
Princeton University Press, 1955.
[2] I. Segal. Mathematical Foundations of Quantum Field Theory,
Benjamin, New York, 1964.
[3] G.W. Mackey. The Mathematical Foundations of Quantum Mechanics,
W.A. Benjamin, Inc., 1963.
[4] A. Peres. Quantum Theory: Concepts and Methods, Kluwer,
Dordrecht, 1995.
[5] P. Bush, P. Lahti, P. Mittelstaedt. The Quantum Theory of
Measurement. Springer, 1996.
[6] Quantum Theory: Reconsideration of Foundations, Ed. A.Khrennikov,
Vaxjo University Press, 2002.
[7] P.A.M. Dirac. The Principles of Quantum Mechanics, Oxford Univ.
Press, 1930.
[8] N.N. Bogoluibov, A.A. Logunov, A.I. Oksak, I. Todorov. General
Principles of Quantum Field Theory, Nauka, Moscow, 1987.
[9] R.F. Streater, A.S. Wightman. PCT, Spin, Statistics and All That,
Benjamin, New York, 1964.
[10] R. Haag. Local Quantum Physics. Fields, Particles, Algebras.
Springer, 1996.
[11] L. Landau, M. Lifschic. Quantum Mchenics, Nauka, Moscow, 1974
[12] J. Sakurai. Modern Quantum Mechanics, 1985
[13] Andrei Khrennikov. Non-Archimedean Analysis: Quantum Paradoxes,
Dynamical Systems and Biological Models. Kluwer Academic Publishers,
1997.
[14] H. Araki. Mathematical Theory of Quantum Fields, Oxford Univ.
Press, 1999.
[15] R. Gill. On Quantum Statistical Inference,
http://www.math.uu.nl/people/gill/
[16] I. Volovich. Quantum Cryptography in Space and Bells Theorem,
in: Foundations of Probability and Physics, Ed. A. Khrennikov, World
Sci.,2001, pp.364-372.
[17] L. Accardi, Yu.G. Lu, I. Volovich. Quantum Theory and Its
Stochastic Limit, Springer, 2002.
[18] M. Ohya, I.V. Volovich. Quantum Computer, Information,
Teleportation, Cryptography, to be published.
[19] A. Khrennikov, I. Volovich. Einstein, Podolsky and Rosen versus
Bohm and Bell, http://arxiv.org/abs/quant-ph/0211078.
[20] I.V. Volovich. Towards Quantum Information Theory in Space and
Time, http://arxiv.org/abs/quant-ph/0203030.
[21] A. Khrennikov, I.V. Volovich. Local Realism, Contextualism and
Loopholes in Bells Experiments,
http://arxiv.org/abs/quant-ph/0212127.
 
Last edited by a moderator:
  • #65
RandallB said:
Nereid
The seemingly circular logic needed to get to where your head is at oddly enough makes the most sense to me. I’m still not sure I have a clear understanding of the LR.
So allow me my translate and you or someone can let me know if I have the LR right.

1. However, QM claims by going through the filter in area A the photon actually traveling in area B is affected and can test differently then it would have, were no testing to be done on the photon in area A.

2. LR presumes the testing in area A has had no affect at all on the other photon in area B.

-- Just want to be sure I have this basics of how each view understands “entanglement”.
And if I’m understanding the above correctly would it be proper to say the LR view disagrees with the idea of “entanglement”?

1. QM view... is silent about the mechanics. The setup of the QM prediction is "as if" a measurement at A changes the photon at B to match. Or it could have been "as if" a measurement at B changes the photon at A to match. No one really is saying, and that is the objection many have with QM. Anyway, if you follow the picture through to the conclusion, you end up believing you are witnessing non-local causation. But this is really a result of the picture. (There are other possible interpretations as well that lead to the same results. That is why I say "as if" which is a big consideration.)

You know the setup is done as I describe above because the correlation formula is cos^2\theta which comes once the polarization is known on one side. I.e. once you know the results on side A, you can predict the statistics observed on side B. And vice versa.

2. LR view... there is no "one" LR view. There are many depending on the hidden variables you wish to postulate. The most simplistic view is that there is a real polarization which is definite as of when the photons are created. But there are literally an infinite number of other possibilities. Since Bell, it has been acknowledged that the fundamental problems with any LR theory appear insurmountable.
 
  • #66
JohnBarchak said:
Volovich is of the opinion that QM can be fixed. To me, that seems roughly equivalent to trying to fix the Titanic, but let's look at his
proposal.

..."Therefore in this sense we can say that axiomatic quantum mechanics is consistent with Bell's inequalities and with local realism. It is well known that there are no Bell's type experiments without loopholes, so there is no contradiction between Bell's inequalities, axiomatic quantum mechanics and experiments, see [21].

[21] A. Khrennikov, I.V. Volovich. Local Realism, Contextualism and
Loopholes in Bells Experiments,
http://arxiv.org/abs/quant-ph/0212127.

This is absolutely nothing, John. Any EPR paper that assumes that published experimental results are in error as its premise is stating a well-known position argued by Caroline Thompson and others. And that conclusion is further clouded by the authors arguing that in an infinite-dimensional space, LR wouldn't violate Bell's Inequality anyway.

If folks are going to feel better about LR and Bell by assuming that a) the universe has infinite dimensions; or b) that published repeatable results are in error... well, I say have a nice day.

As to the idea that QM can be "fixed", I would point out the old saying "if it ain't broke, don't fix it." Other than violating some folks' sense of what is right, what is wrong with QM?

More importantly, where is the better theory? You know, the one with more decimal places... We all know there are a thousand "promising" ideas out there, we are simply waiting for ONE actual such theory to materialize. Any theory which makes the same predictive results as QM in all particulars is merely an ad hoc theory, and nothing more. Show me a testable prediction which differs from QM, and then you will have something.
 
  • #67
Principle of Local Action

I accept your challenge. Einstein's Principle of Local Action has never been violated and it is clearly at odds with QM:

Principle of Local Action
In 1948, very early atomic age, Albert Einstein was in the twilight of his career. He published an article in the journal Dialectica. He hoped that his clear definition of locality and explanation of why locality is an essential part of the scientific method would be a major part of his legacy.

Here is Einstein's Principle of Local Action
"The following idea characterises the relative independence of objects far apart in space (A and B): external influence on A has no direct influence on B; this is known as the Principle of Local Action, which is used consistently only in field theory. If this axiom were to be completely abolished, the idea of the existence of quasienclosed systems, and thereby the postulation of laws which can be checked empirically in the accepted sense, would become impossible."

The import of this principle is that without the Principle of Local Action, science, engineering and law as practiced today would not be viable. In fact, if the Principle of Local Action were to be completely abolished, the Bell Test experiments would have no validity since the test apparatus could be influenced (in unknown ways) by events at the other side of the universe. It should be clear that Bell Test experiments cannot disprove the Principle of Local Action. To make it perfectly clear, the Principle of Local Action would be needed to disprove the Principle of Local Action.

All the best
John B.
 
  • #68
DrChinese said:
This is absolutely nothing, John. Any EPR paper that assumes that published experimental results are in error as its premise is stating a well-known position argued by Caroline Thompson and others.
Unless Volovich has changed his tune since I last corresponded with him, this is not what he claims. I must say I'm inclined to think you are right in dismissing his ideas, though. I could not find much of value in the paper we were discussing (http://arxiv.org/abs/quant-ph/0009058).

And that conclusion is further clouded by the authors arguing that in an infinite-dimensional space, LR wouldn't violate Bell's Inequality anyway.
I don't know where that idea came from, but it must be remembered that the hidden variables can have any number of components. If they have an infinite number that does not necessarily condemn the theory. The "dimensions" here are merely mathematical, with no assumption that they have any geometrical meaning.

As to the idea that QM can be "fixed", I would point out the old saying "if it ain't broke, don't fix it." Other than violating some folks' sense of what is right, what is wrong with QM?
["Some folk" being, in this instance, almost every living human being! Those who are blessed by ignorance of QM would surely never dream of accepting the possibility of non-local effects!

More importantly, where is the better theory? You know, the one with more decimal places...
Under that criterion we might find ourselves accepting Ptolemy!

We all know there are a thousand "promising" ideas out there, we are simply waiting for ONE actual such theory to materialize. Any theory which makes the same predictive results as QM in all particulars is merely an ad hoc theory, and nothing more. Show me a testable prediction which differs from QM, and then you will have something.
Again and again I've told you: simply repeat a Bell test experiments more comprehensively, doing a designed set of related experiments to investigate how the coincidence rates vary as you vary all the relevant parameters! Simply find out by trial and error what parameters matter (the experimenters will already know these!). They will be found to include those built into the local realist model: parameters controlling the response of a detector to variations in individual input pulse intensity etc..

QM predicts that the CHSH test statistic does not vary as you vary the beam intensity. LR predicts that it is most unlikely to stay constant. It is likely to increase as the beam intensity decreases. [NB: the beam intensity needs to be varied by a method such as the introduction of attenuating plates, so that (under wave theory) each individual pulse of light (treated under QM as a single "photon") is reduced in intensity]

Caroline
 
  • #69
JohnBarchak said:
I accept your challenge. Einstein's Principle of Local Action has never been violated and it is clearly at odds with QM:

Principle of Local Action
In 1948, very early atomic age, Albert Einstein was in the twilight of his career. He published an article in the journal Dialectica. He hoped that his clear definition of locality and explanation of why locality is an essential part of the scientific method would be a major part of his legacy.

Here is Einstein's Principle of Local Action
"The following idea characterises the relative independence of objects far apart in space (A and B): external influence on A has no direct influence on B; this is known as the Principle of Local Action, which is used consistently only in field theory. If this axiom were to be completely abolished, the idea of the existence of quasienclosed systems, and thereby the postulation of laws which can be checked empirically in the accepted sense, would become impossible."

The import of this principle is that without the Principle of Local Action, science, engineering and law as practiced today would not be viable. In fact, if the Principle of Local Action were to be completely abolished, the Bell Test experiments would have no validity since the test apparatus could be influenced (in unknown ways) by events at the other side of the universe. It should be clear that Bell Test experiments cannot disprove the Principle of Local Action. To make it perfectly clear, the Principle of Local Action would be needed to disprove the Principle of Local Action.

All the best
John B.

Good try, but there is no conflict between this and QM. If there is, where is the experiment?
 
  • #70
Caroline Thompson said:
Under that criterion we might find ourselves accepting Ptolemy!

Except that is going the wrong direction. I said MORE decimals places, not less.

It's all about the usefulness of the theory. Theory is never reality - not ever. All theory is a model of a subset of reality to which the theory applies, under limited conditions and with specific limits on its applicability. QM is useful and has no superior (read: more useful) competitors at this time other than ad hoc theories yielding identical predictions.
 
  • #71
[NB: the beam intensity needs to be varied by a method such as the introduction of attenuating plates, so that (under wave theory) each individual pulse of light (treated under QM as a single "photon") is reduced in intensity]

Look, I know I've just jumped in on this thread, but don't you see that you're not testing QM and your theory under the same conditions if you use 'intensity' in the wrong sense of the word?

I don't know what your theory says, but in modern physics the intensity of a *source* is related to the *number* of photons being emitted. This doesn't change the ENERGY of each photon - just keep that in mind. This is part of the reason why 'intensity' is gradually being replaced by the word 'irradiance', see for example Hecht, Optics. It's about the energy being delivered by photons per second rather than the amplitude of some wave.

So, to reduce the intensity of a light source you reduce the number of photons emitted. To reduce the intensity of a classical electromagnetic wave you reduce the amplitude. These two approaches OVERLAP in the classical limit, but the latter is NOT valid at low light levels, especially at optical frequencies. Photoelectric effect experiments clearly show that this 'intensity proportional to photon density' idea is correct, as is the idea that photons carry quanta of energy that cannot be reduced just by turning down the light.

Any theory which does *not* define intensity in terms of energy being delivered per second by lumped energy carriers contradicts experiment. This, naturally, includes classical electromagnetism.


Kane
 
  • #72
DrChinese said:
Good try, but there is no conflict between this and QM. If there is, where is the experiment?

I assume from your answer that the Principle of Local Action which
"characterises the relative independence of objects far apart in space (A and B): external influence on A has no direct influence on B"
is in agreement with QM and that QM is a local theory.

The experiments are being done minute by minute in chemistry, biology, physics and all the other sciences - the Principle of Local Action has never been violated.

All the best
John B.
 
  • #73
JohnBarchak said:
I assume from your answer that the Principle of Local Action which
"characterises the relative independence of objects far apart in space (A and B): external influence on A has no direct influence on B"
is in agreement with QM and that QM is a local theory.

The experiments are being done minute by minute in chemistry, biology, physics and all the other sciences - the Principle of Local Action has never been violated.

All the best
John B.

QM is not a local realistic theory. What is the experiment that will distinguish QM from Einstein's Locality? I know of no such experiment. I realize you coyly say "experiments" done every day prove this locality but this is also true with QM.

It is totally false, anyway, to assume that non-locality has implications which negate everyday experience. We don't know. Perhaps there are space dimensions such that every point in the universe is nearby in that spatial dimension? The point is that the simplistic local realism contemplated by EPR is non-existent. How is that any weirder than special or general relativity? It is what it is.
 
  • #74
Kane O'Donnell said:
Any theory which does *not* define intensity in terms of energy being delivered per second by lumped energy carriers contradicts experiment. This, naturally, includes classical electromagnetism.

Hi Kane,

For your information: "local realists" know that they are in trouble once they accept the existence of photons, so they deny it, but this usually comes out very late in the discussion. Having some experience in discussing with them it is a useful question to be clear on that first.
The reasoning presented is usually that they have "local realist models" that explain in a natural way the Aspect like experiment (exploiting the efficiency loophole). In doing so, they usually use classical EM, and the fact that counters are square-law devices responding to classical intensity (say, the Poynting vector). This can indeed sound convincing, if you do not explicitly talk about photons. However, if you then ask them how they interpret OTHER experiments, like the anti-coincidence experiments, then they tell you that there is no problem in it, in that the photon is send left or right in a deterministic way in the beam splitter. When you then ask how you can get interference between the two split beams, you get as an answer that this is explained by classical EM. However, they fail to come up with a coherent scheme which can explain/predict all these experiments in one single vision, as does QM. But you can be busy for tens of posts before realizing that they in fact deny photons.

cheers,
Patrick.
 
  • #75
Thanks very much Patrick. I'm not particularly familiar with EPR paradox and similar things, but I can't see how the existence of photons can be denied in any model which seeks to coherently explain all aspects of the interaction of light and matter. In particular, since classical EM can be *recovered* from quantum theory in the low-frequency, long wavelength limit, I don't see how any experiment that is 'explained' by classical EM cannot also be explained from the photon point of view.

I would guess that the only way that one could distinguish between classical EM and quantum theory in the experiments that have been discussed is to use extremely low intensity devices - is it then the problem that detector efficiency limits our ability to get results?

Kane
 
  • #76
Kane O'Donnell said:
I would guess that the only way that one could distinguish between classical EM and quantum theory in the experiments that have been discussed is to use extremely low intensity devices - is it then the problem that detector efficiency limits our ability to get results?

No, there are very clear experiments proving the existence of photons.
Have a look at the following experiment:

Am. J. Phys. Vol 72, No 9 (1210), September 2004 by Thorn et al.

What they do is the following:

They send an entangled photon pair (from a PDC xtal) in two optical fibres.
One photon goes to the "trigger" detector, to open the coincidence time window for the second one.
The second one goes onto a 50-50 beam splitter and each arm goes onto a photon detector (D1 and D2).
The trick is to show that during the coincidence window with the trigger, at most ONE D1 or D2 triggers, and that coincidences trigger-D1-D2 are extremely rare.
This cannot be explained by classical EM. Indeed, even assuming that out of the Xtal come two correlated intensity bunches, one triggering the photodetector "trigger", then the intensity of the second bunch is divided equally (beamsplitter) on D1 and D2. So, due to the finite efficiency of D1 and D2 of "clicking" on incoming classical intensity, you should find a statistical distribution between "no click", "D1 OR D2 click" and "D1 AND D2 click". THIS IS NOT OBSERVED. The (D1 AND D2) click ratio is strongly suppressed as compared to what one should expect by an "intensity response" of the photodectors, and the very low remaining coincidence is explained by the finite duration of the time window of coincidence (and hence the Poissonian probability of capturing 2 photon pairs).

You CAN explain this experiment classically if you somehow turn your 50-50 beamsplitter into a random "left-right" switch (but you should then explain how it comes that a beam splitter suddenly works that way!). But then you cannot explain why exactly that same beamsplitter, with exactly the same beam, can give interference patterns between the two arms (if you remove the photodetectors D1 and D2). Indeed, if all the intensity goes randomly left or right in the beam splitter (the only way to explain the anticoincidence), then every possible interference is excluded.

The nice thing about this paper is that you do not need to correct any data: the raw data of coincidence clicks are clean enough to prove the point.

cheers,
Patrick.
 
Last edited:
  • #77
That's very impressive - I didn't know that there were experiments of that form that can be used as evidence for the quantum mechanical view of light. Still, there's no need to convince me, of course, I've seen enough laser theory to know that you'd have a hard time explaining stimulated emission without a photon viewpoint.

I'm afraid I don't have much to contribute to the LR discussion, but thanks for your information, Patrick.

Kane
 
  • #78
Kane O'Donnell said:
That's very impressive - I didn't know that there were experiments of that form that can be used as evidence for the quantum mechanical view of light. Still, there's no need to convince me, of course, I've seen enough laser theory to know that you'd have a hard time explaining stimulated emission without a photon viewpoint.

I'm afraid I don't have much to contribute to the LR discussion, but thanks for your information, Patrick.

Kane

Oh sure! I posted the info about this article on 09-07-2004 (on here and in my journal entry) and vanesch gets the credit for it! :) :)

Take note that experiements such as this are no longer "exotic". In fact, this particular paper was describing an experiment done for an undergraduate advanced lab!

Zz.
 
  • #79
ZapperZ said:
Oh sure! I posted the info about this article on 09-07-2004 (on here and in my journal entry) and vanesch gets the credit for it! :) :)

Take note that experiements such as this are no longer "exotic". In fact, this particular paper was describing an experiment done for an undergraduate advanced lab!

Zz.

Here is a direct link to the paper: http://marcus.whitman.edu/~beckmk/QM/grangier/Thorn_ajp.pdf . The authors make an extremely persuasive case.

Mark Beck (Whitman University) is one of the co-authors. He is working on a series of similar tests using PDCs, including tests of Bell Inequalities. As Vanesch states, these are for undergraduate courses specifically which I think is very exciting.

-------------

As to the arguments for local realism: there is no purpose whatsoever to attacking a useful theory like QM unless something better can be put forth in its place. This would be the case EVEN IF (however unlikely) QM was wrong in some particular... because it would still have the exact same utility regardless. As is true with Newtonian gravity after GR.

No one is asserting that we know everything there is to know about QM, or that as currently stated it is final. All we do say is: The EPR paradox - that the possibility of a more complete specification of the system was demonstrated - has been resolved. Result: it has not been demonstrated to be a consequence of QM. Perhaps in the future, someone WILL demonstrate a more complete specification of the system.
 
Last edited by a moderator:
  • #80
DrChinese said:
Here is a direct link to the paper: http://marcus.whitman.edu/~beckmk/QM/grangier/Thorn_ajp.pdf . The authors make an extremely persuasive case.

Mark Beck (Whitman University) is one of the co-authors. He is working on a series of similar tests using PDCs, including tests of Bell Inequalities. As Vanesch states, these are for undergraduate courses specifically which I think is very exciting.

You may want to read a new paper that also described not just one, but a set of undergraduate experiments (5 to be exact) similar to the one here.[1] I have included a short description of it in the latest entry of my journal.

It is unfortunate that many people who freely and continuously come up with apparent "lack of evidence" for the existence of photons either do not understand, nor have ever perform experiments such as these. I am glad that such experiments, which would have been rather daunting to be performed at this level years ago, are becoming more common and accessible.

Zz.

[1] E. J. Galvez et al. Am. J. Phys. v.73, p.127 (2005).
 
Last edited by a moderator:
  • #81
The only thing the beamsplitter test proves is that photons are particles not waves.
And I can see where Bell can “disprove” the classical view, IF the view is restricted to a classical EM or WAVE view.
But cannot there be a classical view of the “particle”. As in:
*An individual photon is polarized based by its spin, on an axis perpendicular to its travel with V H D etc. alignments.
* V photons always absorbed by H filter, always passed by a V filter.
* Diagonal filters destroy the old spin on a V or H photon allowing it to pass based the position of the field of ‘whatever’ is spinning and how (maybe like a baton in the hand of a majorette) when it interacts with the D filter. With passing being a function related to cos^2\theta.
*And if successful in passing, allowing the spin to continue only inline with the angle of the diagonal filter not the original V or H alignment. The greater the amount of spin realignment required the less likely the photon will pass through.
(This isn’t a QM view is it?)

Now I may be an amateur to even imagine such an explanation. But it seems more classical in context than QM. It would not require adherence to Bell Statistical math. And also resolves the “polarization paradox”. Maybe QM also explains the “polarization paradox” also, but so far I’ve not found that anywhere.

So if this could be a true part of a classical explanation of the particle. The EPR test won’t be capable of eliminating either view as both use cos^2\theta.
This only shows the need for a better test, it certainly does not confirm the LR view.

PS: “polarization paradox”
Light totally blocked by filters V H also V H D
But light goes through filters V D H
 
  • #82
RandallB said:
The only thing the beamsplitter test proves is that photons are particles not waves.
And I can see where Bell can “disprove” the classical view, IF the view is restricted to a classical EM or WAVE view.
But cannot there be a classical view of the “particle”.

No, Bell absolutely applies in this situation. Photons are still photons, which is what is measured in every experiment. Also, recall that the EPR and Bell papers themselves discussed spin 1/2 particles (electrons).

The LR crowd tried to escape the Bell results by claiming there was no evidence that photons were quantized. That never made any sense, but these experiments prove it conclusively. The "table top" experiment Vanesch mentions saw a violation of the classical (Maxwell) predictions by 100+ standard deviations, and very close agreement with QM.

Wave theory predicted: >=1.0000
QM predicted: .0000
Actual: .0118
 
  • #83
Of Einstein, Podolsky, Rosen, Bohm and Bell

I have yet to encounter a proponent of quantum theory who has even a basic understanding of the EPR gedanken experiment - but I guess Bohr did give absolution to quantum people from having to understand anything. Most think that it has something to do with the Bohm/Bell proposed experiments involving spin or polarization. None appear to realize that the EPR gedanken experiment and the Bohm/Bell proposed experiments are fundamentally different. Actually, the EPR gedanken experiment involves the breakup of a molecule of two identical
atoms. The two resulting particles move in opposite directions at the same speed (classical conservation), so their positions and momenta are obviously correlated in continuous Einstein 4 space. Bell proved absolutely nothing as far as the original EPR gedanken experiment. For those who want to believe that Bell proved something, please call it the Bell gedanken experiment for photons or for Bohm's electron spin gedanken experiment, call it EPRB.

The main thing to remember is that Bohr's denial of the EPR "elements of reality" was essentially a denial of the scientific method and the principles of engineering. If the functional relationship between the two particles in the EPR gedanken experiment is not real, then almost nothing in science or the principles of engineering can be
considered real. We are left with mysticism and voodoo. It is incredible that rational people even consider the denial the EPR "elements of reality". I think that Einstein was in a state of shock until the day he died.

Of Einstein, Podolsky, Rosen, Bohm and Bell

In "Einstein, Podolsky and Rosen versus Bohm and Bell", Andrei Khrennikov and Igor Volovich explain how the EPR gedanken experiment and the Bohm/Bell proposed experiments are fundamentally different:

"In 1935 Einstein, Podolsky and Rosen (EPR) advanced an argument about incompleteness of quantum mechanics [1]. They proposed a gedanken experiment involving a system of two particles spatially separated but correlated in position and momentum and argued that two non-commuting variables (position and momentum of a particle) can have simultaneous physical reality. They concluded that the description of physical reality given by quantum mechanics, which does not permit such a simultaneous reality, is incomplete.

Though the EPR work dealt with continuous variables most of the further activity have concentrated almost exclusively on systems of discrete spin variables following to the Bohm [2] and Bell [3] works.

Bell's theorem [3] states that there are quantum spin correlation functions that can not be represented as classical correlation functions of separated random variables. It has been interpreted as incompatibility of the requirement of locality with the statistical predictions of quantum mechanics [3]. For a recent discussion of Bell's theorem see, for example [4] - [17] and references therein. It is now widely accepted, as a result of Bell's theorem and related experiments, that "Einstein`s local realism" must be rejected. For a discussion of the role of locality in the three dimensional space see, however, [16, 17].

The original EPR system involving continuous variables has been considered by Bell in [18]. He has mentioned that if one admits "measurement" of arbitrary "observables" on arbitrary states then it is easy to mimic his work on spin variables (just take a two-dimensional subspace and define an analogue of spin operators). The
problem which he was discussing in [18] is narrower problem, restricted to measurement of positions only, on two non-interacting spinless particles in free space. Bell used the Wigner distribution approach to quantum mechanics. The original EPR state has a nonnegative Wigner distribution. Bell argues that it gives a local,
classical model of hidden variables and therefore the EPR state should not violate local realism. He then considers a state with nonpositive Wigner distribution and demonstrates that this state violates local realism.

Bell's proof of violation of local realism in phase space has been criticized in [19] because of the use of an unnormalizable Wigner distribution. Then in [20] it was demonstrated that the Wigner function of the EPR state, though positive definite, provides an evidence of the nonlocal character of this state if one measures a
displaced parity operator.

In this note we apply to the original EPR problem the method which was used by Bell in his well known paper [3]. He has shown that the correlation function of two spins cannot be represented by classical correlations of separated bounded random variables. This Bell's theorem has been interpreted as incompatibility of local realism with quantum mechanics. We shall show that, in contrast to Bell's theorem for spin correlation functions, the correlation function of positions (or momenta) of two particles always admits a representation in the form of classical correlation of separated random variables. This result looks rather surprising since one thinks that the Bohm-Bell reformulation of the EPR paradox is equivalent to the original one."

The entire paper may be found at:
http://arxiv.org/PS_cache/quant-ph/pdf/0211/0211078.pdf

References
[1] A. Einstein, B. Podolsky, and N. Rosen, Phys. Rev. 47(1935)777.
[2] D. Bohm, Quantum Theory, Prentice-Hall, Englewood Cliffs, 1951.
[3] J.S. Bell, Physics, 1, 195 (1964).
[4] J.F. Clauser, A. Shimony, Report. Progr. Physics, 41(1978)1881.
[5] J.F.Clauser, M.A. Horne, A. Shimony, and R.A. Holt,
Phys.Rev.Lett. 23,880 (1969)
[6] G. Weihs, T. Jennewein, C. Simon, H. Weinfurter, A. Zeilinger ,
Phys.Rev.Lett. 81
(1998) 5039-5043.
[7] S.L. Braunstein, A.Mann, and M. Revzen, Phys. Rev. Lett, 68, 3259
(1992)
[8] D. Collins, N. Gisin, N. Linden, S. Massar, S. Popescu, Phys.
Rev. Lett. 88, 040404
(2002).
[9] M. D. Reid, Phys. Rev. Lett, 84, 2765 (2000)
[10] A. Beige, W. J. Munro, P. L. Knight, Phys. Rev. A 62, 052102
(2000)
[11] Z.-B. Chen, J.-W. Pan, G. Hou, and Y.-D. Zhang, Phys. Rev. Lett.
88, 040406 (2002)
[12] A. Kuzmich, I.A. Walmsley, and L. Mandel, Phys. Rev. Lett, 85,
1349 (2000)
[13] H. Jeong, W. Son, M. S. Kim, D. Ahn, C. Brukner, quant-
ph/0210110.
[14] A. Yu. Khrennikov, Foundations of Physics, 32, 1159-1174 (2002).
[15] A.Yu. Khrennikov, Il Nuovo Cimento, B 115, N.2, 179-184, (1999).
[16] I. V. Volovich, in : Foundations of Probability and Physics, Ed.
A. Khrennikov, World Sci. 2001, pp.364-372.
[17] I. V. Volovich, quant-ph/0203030.
[18] J.S. Bell, Speakable and unspeakable in quantum mechanics,
Cambridge University
Press, Cambridge, 1987, p.196.
[19] L.M. Johansen, Phys. Lett. A236(1997)173
[20] K. Banaszek, K. Wodkiewicz , Phys. Rev. A 58, 4345 (1998)
 
Last edited by a moderator:
  • #84
JohnBarchak said:
I have yet to encounter a proponent of quantum theory who has even a basic understanding of the EPR gedanken experiment - but I guess Bohr did give absolution to quantum people from having to understand anything. Most think that it has something to do with the Bohm/Bell proposed experiments involving spin or polarization. None appear to realize that the EPR gedanken experiment and the Bohm/Bell proposed experiments are fundamentally different. Actually, the EPR gedanken experiment involves the breakup of a molecule of two identical
atoms. The two resulting particles move in opposite directions at the same speed (classical conservation), so their positions and momenta are obviously correlated in continuous Einstein 4 space. Bell proved absolutely nothing as far as the original EPR gedanken experiment. For those who want to believe that Bell proved something, please call it the Bell gedanken experiment for photons or for Bohm's electron spin gedanken experiment, call it EPRB.

The main thing to remember is that Bohr's denial of the EPR "elements of reality" was essentially a denial of the scientific method and the principles of engineering. If the functional relationship between the two particles in the EPR gedanken experiment is not real, then almost nothing in science or the principles of engineering can be
considered real. We are left with mysticism and voodoo. It is incredible that rational people even consider the denial the EPR "elements of reality". I think that Einstein was in a state of shock until the day he died.

etc. etc.

John,

You adeptness at quoting long tracts of others' work with no value added is acknowledged.

1) You continue to ignore the challenge I have laid out for you: Describe a specific experiment that separates the men from the boys. You say that your position is so incredibly amazing that the rest of us are too dumb to comprehend (I apparently lack "basic understanding"); well, perhaps that door swings both ways. I am not impressed by claims of brilliance. Actual brilliance impresses me. Where is yours? Show us a specific experiment, we've heard enough big claims from you already.

2) You state that "most" think EPR had to do with "spin or polarization". I think instead that most folks here know the following: EPR thought they had demonstrated that QM was not complete because a more complete specification of the system was possible. I don't think it ever occurred to EPR that something like the Bell Theorem would come along. Clearly, if the entangled particles have specific definite attributes as EPR envisioned them, then a more complete specification IS possible (in principle). You are free to ignore Bell and say it does not disprove EPR. But you are splitting hairs while everyone else has passed you by and left you in the dust. Bell says that the hypothesis that a more complete specification of the system is possible (in the manner of the EPR paradox) is falsifiable via experiment. Experiment performed, hypothesis rejected.
 
  • #85
Please clarify for me - does QM satisfy Einstein's Principle of Local Action or does it not? You can't sit on the fence forever.

All the best
John B.
 
  • #86
JohnBarchak said:
Please clarify for me - does QM satisfy Einstein's Principle of Local Action or does it not? You can't sit on the fence forever.

All the best
John B.

a) In my personal opinion, it does. I tend to believe in local non-reality. A light cone limits propagation of causes towards effects. Particles do not have precise definite real attributes outside of the context of a measurement.

b) Others think that reality is non-local. (A reasonable position, too, IMHO.) In that case, there are instances in which what appears non-local from one space-time perspective is local from another. In that case, the other side of the universe is close if you could approach from the correct dimension.

In either case, the QM formalism is sufficient to be useful.

Now, when are you going to address my challenge? An experiment to separate your use of hyperbole into something of substance?
 
  • #87
Dehmelt's Penning trap capture of an electron, which in Dehmelt's words was "drastically at odds with the famous Physicist Heisenberg's claim that an electron truly at rest could not be localized and could be found anywhere in space." This totally blows away QM.

The Aspect experiment is used as proof of the non-local character of physics. If the Principle of Local Action were to be completely abolished, the Bell Test experiments would have no validity since the test apparatus could be influenced (in unknown ways) by events at the other side of the universe. Since a counter example experiment to the Principle of Local Action has never been found, this totally blows away QM. Remember that for superposition to work, spooky action at a distance MUST occur. Actually, it never occurs.

I've got many more examples if you want to hear about them.
 
  • #88
JohnBarchak said:
Dehmelt's Penning trap capture of an electron, which in Dehmelt's words was "drastically at odds with the famous Physicist Heisenberg's claim that an electron truly at rest could not be localized and could be found anywhere in space." This totally blows away QM.

The Aspect experiment is used as proof of the non-local character of physics. If the Principle of Local Action were to be completely abolished, the Bell Test experiments would have no validity since the test apparatus could be influenced (in unknown ways) by events at the other side of the universe. Since a counter example experiment to the Principle of Local Action has never been found, this totally blows away QM. Remember that for superposition to work, spooky action at a distance MUST occur. Actually, it never occurs.

I've got many more examples if you want to hear about them.

Your logic blows me away. Where is the beef, John? You talk the talk, but...

A quote by Dehmelt is not experimental evidence of anything - you fail to address the most basic of challenges. Give an experiment that falsifies QM. Or give a description of an actual experiment that separates your view from QM. (Oh, and make sure your theory gives identical predictions in all other places.)

Unless you are God, I do not see how any of us have the power to enforce OR abolish the "Principle of Local Action". No one, least of all myself, has said that a cause can be made to propagate outside a light cone. So what is your point?

Spooky action at a distance is one *possible* consequence of Aspect. Aspect happened. Do you simply refuse to accept experimental results you do not care for? If so, save us a lot of time right now and tell us what you believe instead of hiding behind a curtain.
 
  • #89
RandallB said:
The only thing the beamsplitter test proves is that photons are particles not waves.

I would drop the "not waves", but indeed, it means that there is some entity that "doesn't split". So you "detect a photon or you don't detect it", and you do not detect 3/4 of a photon.

Once this is accepted, you can say that a photodetector clicks when it sees a photon, with a certain efficiency, and that that efficiency can slightly depend on the energy of the photon (easily checked: it is the quantum efficiency as a function of frequency), it can eventually depend on the polarization (easily checked, usually this is flat) and of course it depends in a trivial way on position: you hit the photocathode or you miss it :-) But if you are not too clumsy an experimentalist, you restrict the impact zone to the middle portion of the photocathode, where you are independent of position.
And there is nothing else the efficiency can depend upon.

And I can see where Bell can “disprove” the classical view, IF the view is restricted to a classical EM or WAVE view.
But cannot there be a classical view of the “particle”. As in:
*An individual photon is polarized based by its spin, on an axis perpendicular to its travel with V H D etc. alignments.
* V photons always absorbed by H filter, always passed by a V filter.
* Diagonal filters destroy the old spin on a V or H photon allowing it to pass based the position of the field of ‘whatever’ is spinning and how (maybe like a baton in the hand of a majorette) when it interacts with the D filter. With passing being a function related to cos^2\theta.
*And if successful in passing, allowing the spin to continue only inline with the angle of the diagonal filter not the original V or H alignment. The greater the amount of spin realignment required the less likely the photon will pass through.

But is it EXACTLY to such a situation that Bell applies, and this is exactly quantum mechanics ! Indeed, the photons that pass have the polarization of the last filter.
Now, the correlations mentioned in Bell correspond to the correlations of clicks when we choose two different angles for the polarizers in the two beams.
For instance, we know that the polarizations are "opposite" in the two photons of a photon pair. So if one polarizer is horizontal, and let's pass, and the other one is vertical, it should let pass. "100% correlation" but of course not in practice because of the finite efficiencies.
If one polarizer is horizontal, and the other one under 45 degrees, there is no correlation (50%), in that, if you know the first photon passed horizontal, the other one is vertical and upon a 45 degree polarizer it has 50% chance of passing (and yes, it will then come out as a 45 degree photon, but we don't care about that).
If you accept an independent finite efficiency for detecting a photon, as explained above, then you can extract the ideal correlations from the measurements ; for instance, if the efficiency of the detectors are, say, 34%, and in the case of X - Y you expect 100% ideal correlation, you should find 34% correlation in your data (because each time the photon got through, it had a chance of 34 % of clicking).
When you do that for different angles, you find a clear violation of the Bell inequalities. These are the Aspect like experiments.

There is no reasonable way in which these efficiencies should suddenly be a function of polarization (while you can check that, by using a polarized beam and looking at the average click rate when you turn it). But LR proponents say that it is STILL possible that in this kinds of experiments the efficiencies change exactly in the way to make us think that if they weren't we had a violation of Bell's inequalities. And indeed, theoretically such a possibility must be considered for a "loophole free" test. So this is the famous "efficiency loophole".

cheers,
Patrick.
 
  • #90
With 10% efficiency on photon detection, the total inability to determine how many photons are involved, and the total inability to determine the energy involved, it is absolutely amazing that anyone concluded anything. I do not blame Aspect; he was not the one making the incredible claims.

All the best
John B.
 
  • #91
vanesch said:
And indeed, theoretically such a possibility must be considered for a "loophole free" test. So this is the famous "efficiency loophole".

cheers,
Patrick.

Vanesch,

I freely acknowledge the "detection loophole" and the "fair sampling" assumption (see more on that, next post, reference probably stolen from you already anyway). The question, don't you think, is what is its significance?

We could also have a leap year loophole. Scientific experiments run in a leap year give different results than other years. Or if run in the Southern hemisphere. Or in *France*, for god's sake. :smile: The point is, why is it that only EPR tests should have such loopholes heaped upon them? Why not double slit experiments, etc. etc.

This same thing - creating ad hoc evidentiary requirements - is also done to evolutionary theory. (Next we will be hearing about "intelligent design" in EPR experiments.) I guess, to be fair, special relativity (and the "one way speed of light" controversy) gets some of the same heaped upon it.

It seems to me that improvements in technology (and therefore leading to experiments with greater accuracy) render such "loopholes" as rapidly approaching moot status. I guess the great thing about science is that nothing is ever quite 100.0000% settled.
 
Last edited:
  • #92
JohnBarchak said:
With 10% efficiency on photon detection, the total inability to determine how many photons are involved, and the total inability to determine the energy involved, it is absolutely amazing that anyone concluded anything. I do not blame Aspect; he was not the one making the incredible claims.

All the best
John B.

You are way behind:

Experimental violation of a Bell's Inequality with efficient detection
M. A. Rowe, et al
Nature, vol 409, February 2001

CHSH value of 2.25+/-.03 where 2.00 is the max allowed by local realistic theories. "...the high detection efficiency of our apparatus eliminates the so-called detection loophole. ... The result above was obtained using the outcomes of every experiment, so that no fair sampling hypothesis was required."

By the way, there is nothing weird about drawing strong conclusions from small samples. There is a branch of science called "statistics" ... you might learn from its study!
 
Last edited:
  • #93
DrChinese said:
We could also have a leap year loophole. Scientific experiments run in a leap year give different results than other years. Or if run in the Southern hemisphere. Or in *France*, for god's sake. :smile: The point is, why is it that only EPR tests should have such loopholes heaped upon them? Why not double slit experiments, etc. etc.

This same thing - creating ad hoc evidentiary requirements - is also done to evolutionary theory. (Next we will be hearing about "intelligent design" in EPR experiments.) I guess, to be fair, special relativity (and the "one way speed of light" controversy) gets some of the same heaped upon it.

Exactly. That's why I stopped discussing with these people ; we have two fundamentally different ways of viewing of how science works. Science works (in my opinion, which is, I think, well-informed on the question) on two requirements:
1) logical consistency and sufficient generality of a theory (which is essentially a way of mapping "things in the lab" onto a mathematical model, within boundaries, but not tied to specific lab situations ad hoc)
2) agreement between numerical predictions by said theory in given circumstances describing and experiment and the actual outcomes of those experiment.

The logical consequence is that you can disprove specific theories (either because they don't satisfy 1) or because they fail on 2)), or even specific classes of theories which is just a loop over 1) and 2). But you can never PROVE a theory, nor can you disprove one particular aspect of what could be contained in 1).

And it is exactly that what many people try to do, or accuse "scientists" to fail to do. No, you cannot *absolutely prove* QM, or the *existence of photons*. You can only show that theories using this make accurate predictions and satisfy up to date 1) and 2), and compare this to other theories which satisfy also 1) (such as classical optics). You cannot prove the inexistence of LR theories if the class is too wide.

What they should do, in order to be taken seriously, is to produce specific theories, or classes of theories, that contain their pet principle, and satisfy 1) and 2). But they rarely (if ever) do.

They just say: hey, for _this_ specific experimental result, I can think up a theory that respects my pet principle and produces the same results - if I'm allowed to change the behaviour of all known apparatus. But for the next experiment, they do the same, but with DIFFERENT theories and different behaviour of the apparatus. This means that their view doesn't satisfy 1).

The nicest attempts that I've seen were "stochastic Electrodynamics". I think it has a problem with thermodynamics, and with the rest of quantum theory, but at least it tried to construct an equivalent theory in optics having LR.

cheers,
Patrick.
 
  • #94
DrChinese said:
You are way behind:

Experimental violation of a Bell's Inequality with efficient detection
M. A. Rowe, et al
Nature, vol 409, February 2001"

YOU are the one who brought up Aspect!
 
  • #95
MY "Classical view" of the photon as a particle
vanesch said:
But is it EXACTLY to such a situation that Bell applies, and this is exactly quantum mechanics ! Indeed, the photons that pass have the polarization of the last filter. .
So if my "Classical view of a particle" is QM, can you help me understand the mechanics of how QM explains a photon changes its polarization as it goes through a filter?

ALSO
For instance, we know that the polarizations are "opposite" in the two photons of a photon pair. So if one polarizer is horizontal, and let's pass, and the other one is vertical, it should let pass. "100% correlation"
Patrick.
Just to confirm a point (maybe only important to the testers) but somewhere I'd picked up the idea that entangled photons came out with the same polarization. Testers must set there 0 degeres mark for correlation in test areas A and B 90 degrees apart from each other, correct?

Thanks, I think I'm getting it.
 
  • #96
RandallB said:
1. MY "Classical view" of the photon as a particle
So if my "Classical view of a particle" is QM, can you help me understand the mechanics of how QM explains a photon changes its polarization as it goes through a filter?

2. ALSOJust to confirm a point (maybe only important to the testers) but somewhere I'd picked up the idea that entangled photons came out with the same polarization. Testers must set there 0 degeres mark for correlation in test areas A and B 90 degrees apart from each other, correct?

Thanks, I think I'm getting it.

1. Vanesch can probably answer this better. As far as I know, there is no real "mechanical" explanation of spin intrinsics. It just is. This is one of the elements of QM that some find objectionable. By analogy, it is no different than what happens when an electron moves from one orbital to another. It just does.

2. I always refer to 0 degrees as the correlated case because it is easier to discuss. Actually the spins are crossed - i.e. 90 degrees apart - but that is easily compensated for as you state.
 
  • #97
JohnBarchak said:
YOU are the one who brought up Aspect!

?

OK, here is another simple question for you to evade: do you or do you not accept the results of Aspect as proof of a violation of Bell's Inequality?

If the answer is NO, then: do you or do you not accept the results of Rowe as proof of a violation of Bell's Inequality?
 
  • #98
RandallB said:
MY "Classical view" of the photon as a particle
So if my "Classical view of a particle" is QM, can you help me understand the mechanics of how QM explains a photon changes its polarization as it goes through a filter?

Because in quantum mechanics, an x-polarized photon can just as well be seen as a superposition of a 45 degree left, and a 45 degree right polarized photon. And then only one of the two components gets true. It is not that there is a mechanistic explanation of something "tilting" the axis of polarization. In QM formalism, it is just a "change of basis". But you touch indeed upon one of the most bizarre properties of QM. In fact, all these things are different expressions of THE bizarre property of QM, namely the superposition principle. And it is the cornerstone of QM which gives rise to about all of its results.
However, in this particular case, the analogy with classical optics is striking: you wouldn't argue that something "tilted" the plane of the E-field when it went through a polarizer, right ? Well, exactly the same thing applies to the photon.

ALSOJust to confirm a point (maybe only important to the testers) but somewhere I'd picked up the idea that entangled photons came out with the same polarization. Testers must set there 0 degeres mark for correlation in test areas A and B 90 degrees apart from each other, correct?

In fact, both occur. Some parametric down converters are of type I, and then indeed, both have the same polarization. Others are of type II, and then they are perpendicularly polarized. (or was it the opposite?).

cheers,
Patrick.
 
  • #99
DrChinese said:
... do you or do you not accept the results of Rowe as proof of a violation of Bell's Inequality?
I think it is in http://arxiv.org/abs/quant-ph/0102139 that Lev Vaidman explains why, though an inequality was violated, we don't have to interpret it as illustrating entanglement: the ions in Rowe's experiment were very close together. The measurements on them could not be considered (as required for the Bell inequality) to be independent.

Cat
 
  • #100
Cat said:
I think it is in http://arxiv.org/abs/quant-ph/0102139 that Lev Vaidman explains why, though an inequality was violated, we don't have to interpret it as illustrating entanglement: the ions in Rowe's experiment were very close together. The measurements on them could not be considered (as required for the Bell inequality) to be independent.

Cat

Lev doesn't think that experiment has eliminated the detection ("fair sampling") issue because of the locality issue. But that is merely one person's opinion.

It is clear to me from the Rowe and Aspect experiments (and others such as Weihs):

a. Locality: the Inequality is violated whether or not the apparatus is space-like separated, per Weihs. (Requiring this never made any sense in the first place, because it requires the existence of physical effects never otherwise witnessed.)

b. Fair Sampling: the Inequality is violated whether or not a fair sample is obtained, per Rowe. (Requiring a complete sample never made sense to me either, as a large subsample should not possibly show more correlations than are actually present in the full population.)

Combining these two, you know that locality and sampling are not factors in the correlated events. That should be sufficient to address the lingering doubts of most scientists.
 
Back
Top