When does entanglement actually end?

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  • #51
So are we saying
1) That there needs (for entanglement to end - this thread) to be no mechanism involved, it happens.
2) We can never know the mechanism even if there is one (our brains are not correctly positioned to understand)
3) There is a mechanism which in the future we will probably find.
5) Its all solved, no need to discuss further.
4) Something else not in this list.
 
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  • #52
wawenspop said:
So are we saying
1) That there needs (for entanglement to end - this thread) to be no mechanism involved, it happens.
2) We can never know the mechanism even if there is one (our brains are not correctly positioned to understand)
3) There is a mechanism which in the future we will probably find.
5) Its all solved, no need to discuss further.
4) Something else not in this list.

Yes :wink:
 
  • #53
Thanks for the thoughtful replies. Just a few more points of clarification.

vanesch said:
If a classical physicist were looking at the experimental preparation, he'd see nothing else but "things that are set up to interact".
Maybe, maybe not. If the essence of quantum entanglement is the formal nonseparability corresponding to the statistical dependence produced by mutual interaction or common influence (and ultimately the filtering/measuring of the separated disturbances via a common global parameter), then (wrt to a simple Bell optical setup anyway) the cross-corrolation can also be understood in terms of analogy to a classical polariscopic setup.

The point is that the physical referent of the formal nonseparability is ultimately the statistical dependence that's produced via the experimental design.

vanesch said:
... two systems that are entangled have no "individual identity" anymore in their quantum-mechanical description.
Yes, but only if you're describing the simultaneous behavior of both systems wrt a global parameter. Otherwise, they still have an individual identity. It's just that the cross-correlation can't be understood without reference to the global parameter. This is the same state of affairs whether we're talking about it in terms of the qm formalism, or FLT or instantaneous influences between spacelike separated events, or the polariscope analogy.

vanesch said:
But again, that's a sheer property of the quantum-mechanical description.
For reasons I've stated, I'm thinking that maybe the essence of entanglement is not solely a property of the qm description. It depends on how one looks at it. As you say:

vanesch said:
... classical action-at-a-distance can mimic perfectly the quantum-mechanical entanglement (or, quantum-mechanical entanglement can mimic perfectly action-at-a-distance ; depends on your PoV).
So, the essence of this thing for which we have interchangeable formal descriptions is not one description or the other, but rather something or things that they have in common.

In any case, I will continue to refrain from using the term "entangled data".

Regarding my observation that your stance on this was possibly in conflict with your adherence to the MWI you wrote:

vanesch said:
I try to keep a distinction between what is "hard fact" and what are interpretational pictures. MWI is a way of giving a picture to the quantum-mechanical happening, which "explains" then of course entanglement and all that - but it's only that: a picture. It's not a hard fact.
I don't get any picture at all from the MWI approach. :smile:

vanesch said:
It is true that, through the quantum formalism, entangled states give rise to weird correlations which cannot always be explained by classical interaction, locality and some other reasonable assumptions (re Bell's theorem and all that).
The correlations are weird only if associated with the qm formalism or FTL or instantaneous propagations of some sort. When viewed via the polariscope analogy they are what one would expect for two identical waveforms being simultaneously analyzed by two identical filters. The correlation will vary as you vary the difference in the settings of the filters in a way that mimics the Malus Law results of polariscopic setups.

It's just that no value can be assigned to what's being filtered prior to a detection associated with some specific filter setting. This amounts to giving up the pseudo-objective view of reality that classical physics has allowed us to entertain.

In closing, I had written:
If the physical essence of quantum entanglement is interaction and mutual (common) influence, then in order to produce the correlations that correspond to quantum entanglement per quantum theory it would be necessary to duplicate the experimental conditions. A rose by any other name is still a rose.

To which you replied:
vanesch said:
I don't understand what you say here.
I have taken it that you are saying that the essence of quantum entanglement is the quantum theoretical formalism. I'm saying that maybe the formalism isn't the essence of it. So, even if you give it another name, or attribute different sorts of causes to it, we're still talking about, essentially, the same thing, and that thing is characterized not by the quantum formalism but by experimental designs which entangle two or more quanta and the resulting data which satisfies certain criteria.
 
  • #54
ThomasT said:
… a few more points of clarification.

The correlations are weird only if associated with the qm formalism or FTL or instantaneous propagations of some sort. When viewed via the polariscope analogy they are what one would expect for two identical waveforms being simultaneously analyzed by two identical filters. The correlation will vary as you vary the difference in the settings of the filters in a way that mimics the Malus Law results of polariscopic setups.

The problem here is stating that “When viewed via the polariscope analogy they are what one would expect …”
On what basis do you think there is an expectation that the “polariscope analogy” should produce the results that lead to Malus Law.
Malus Law is not built on an expectation – it is built from observations that can only be described as “weird”.
With the Horizontal polarized light re-measured at 90° to pass 100% of the light but at 0° pass no light and at 45° passing 50% of the light are all reasonable easy to explain expectations.
However results at 22.5° pass 15% f the light instead of 25% or 67.5° passing 85% instead of 75% cannot be said to be “expected”.
The classical assumption that Malus Law accurately defines or predicts what the results will be, is not the same as describing an expectation based on any rational description of why such “weird” results are produced.

Remember Malus Law does not address the behaviors of individual photons but the results of measuring many of them just as does QM Formalism.

SO IMO both Malus Law and EPR Correlations (both following the same Cos2 rule) are weird results defined by observation but not explained by Classical Expectations. And both are better explained by QM Formalism or equivalent interpretations of QM.
 
  • #55
RandallB said:
The problem here is stating that “When viewed via the polariscope analogy they are what one would expect …”
On what basis do you think there is an expectation that the “polariscope analogy” should produce the results that lead to Malus Law.
Malus Law is not built on an expectation – it is built from observations that can only be described as “weird”.

With the Horizontal polarized light re-measured at 90° to pass 100% of the light but at 0° pass no light and at 45° passing 50% of the light are all reasonable easy to explain expectations.
However results at 22.5° pass 15% f the light instead of 25% or 67.5° passing 85% instead of 75% cannot be said to be “expected”.
The classical assumption that Malus Law accurately defines or predicts what the results will be, is not the same as describing an expectation based on any rational description of why such “weird” results are produced.

Remember Malus Law does not address the behaviors of individual photons but the results of measuring many of them just as does QM Formalism.

SO IMO both Malus Law and EPR Correlations (both following the same Cos2 rule) are weird results defined by observation but not explained by Classical Expectations. And both are better explained by QM Formalism or equivalent interpretations of QM.
Thanks for your reply. After posting, I had some second thoughts on what I had written. I agree with the points you make here. What happens is that after doing lots of classical polariscope setups and becoming comfortable with the classical description, then one tends to think of these observations as not weird and that the nature of light isn't still a mystery. But, as you indicated, they are weird, and the quantum experimental phenomena have underlined the fact that the nature of light is still a mystery.

So, my comparison of simple optical Bell setups and results with a polariscope setup and results still doesn't solve the problem -- even if the analogy is correct.

Could it be that there's something wrong with the classical model of polarization viz the failure of local hidden variable models wrt EPR-Bell tests? I think I'll start a new thread on this. Is this topic appropriate for the quantum physics forum?
 
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  • #56
The correlation of states between entangled particles? There is no mass involved and no real information transmitted so SR cannot be violated and it is free to travel FTL. But, one may ask the question what is transmitted between the two particles that has no mass and carries no 'real' information (i.e. information that could introduce 'cause'). Looks mighty like nothing to me. Sure nothing can travel FTL. Why not?... (Yikes, what am I saying here!)

But whatever it is that maintains correlations does not depend on separation distancebetween particles, it seems. (realism and locality arguments). So, what is the mecahnism when the two particles are right on top of each other for maintaining correlation? It will probably be the same as when they are distant. There are no 'forces' involved, its more about probabilities.

When the Universe picks its probabilities for the two particles, how exactly does it do it? It will not be using a look up table or atomic distintegrations I assume. But, to be sure, that mechanism does not change with separation distance.
 
  • #57
Randall, after thinking about this some more, I'd like to address some of your comments.

RandallB said:
The problem here is stating that “When viewed via the polariscope analogy they are what one would expect …”
On what basis do you think there is an expectation that the “polariscope analogy” should produce the results that lead to Malus Law.

On the basis of sinusoidal wave models. One would expect the intensity of the wave transmitted by the analyzer in a polariscopic setup to be proportional to the square of the cosine of the angular difference between the transmission axes of the polarizer and the analyzer.

RandallB said:
Malus Law is not built on an expectation ...
I don't know, but I suspect that you're probably right that the original experimental discovery was not preceded by any theoretical prediction of it. But the experimental phenomenon lent itself quite readily to modelling in terms of sinusoidal functions. And, that's how propagating waves (whether light or matter) have continued to be modeled in both classical and quantum physics (using Fourier analysis where necessary for convenience).

RandallB said:
... – it is built from observations that can only be described as “weird”.
I've changed my mind on this. I don't think of the results of polariscopic setups as weird. This is just how one would expect EM waves to behave -- unless you or someone else can tell me what's weird about the standard EM wave model.

RandallB said:
With the Horizontal polarized light re-measured at 90° to pass 100% of the light but at 0° pass no light and at 45° passing 50% of the light are all reasonable easy to explain expectations.
However results at 22.5° pass 15% f the light instead of 25% or 67.5° passing 85% instead of 75% cannot be said to be “expected”.
They can if you're using the standard, classical model for it.

I'll agree that the relationship might have been surprising when first discovered. But during the past 150 years or thereabouts it has become increasingly less so. Now this might be attributed to just becoming familiar with a model that itself might be characterized as weird, but I don't think of it in that way. Viewed in terms of orthogonal plane wave components, the propagating wave is as visualizable as a surface wave from our everyday experience, sort of.

RandallB said:
The classical assumption that Malus Law accurately defines or predicts what the results will be, is not the same as describing an expectation based on any rational description of why such “weird” results are produced.
The classical model looks like a rational description to me.

RandallB said:
Remember Malus Law does not address the behaviors of individual photons but the results of measuring many of them just as does QM Formalism.
Yes, understood. When I use the term individual measurement I'm referring to the average of many trials.

RandallB said:
SO IMO both Malus Law and EPR Correlations (both following the same Cos2 rule) are weird results defined by observation but not explained by Classical Expectations. And both are better explained by QM Formalism or equivalent interpretations of QM.
I'm not saying that we have the option of using either a classical or qm model in the case of simple optical Bell tests, but the results do seem less weird to me (meaning, in part, that I don't have to worry about there really being FTL propagations of some sort) if I take those setups to be analogous to classical polariscopic setups (even though I then have to contend with those who say that Bell's theorem shows that it just can't be that both A and B are analysing the same disturbance simultaneously).

So, I guess we'll have to agree to disagree a little bit here -- unless you can convince me otherwise. My thinking on this remains open to criticism and direction to considerations I might be missing.
 
  • #58
ThomasT said:
I've changed my mind on this. I don't think of the results of polariscopic setups as weird. This is just how one would expect EM waves to behave -- unless you or someone else can tell me what's weird about the standard EM wave model.

They can if you're using the standard, classical model for it.

I'll agree that the relationship might have been surprising when first discovered. But during the past 150 years or thereabouts it has become increasingly less so. Now this might be attributed to just becoming familiar with a model that itself might be characterized as weird, but I don't think of it in that way. Viewed in terms of orthogonal plane wave components, the propagating wave is as visualizable as a surface wave from our everyday experience, sort of.

The classical model looks like a rational description to me.

The Malus Law comes from:
Actual_Amplitude = Initial_Amplitude CosB - classically reasonable assumption!

But intensity (related to number of particles observed)

Intensity = Amplitude squared

So classical AND quantum predicts:

Actual_Intensity = Initial_Intensity cos squared B - Malus AND QM predictions.

So Bell's Inequality is incorrectly assuming cos B instead of cos squared B
and so proves nothing at all! I knew it all the time!
 
  • #59
Epicurus3 said:
So Bell's Inequality is incorrectly assuming cos B instead of cos squared B and so proves nothing at all! I knew it all the time!

:smile: Before you jump to conclusions: Malus applies to light (spin 1 photons). Bell's argument used spin 1/2 particles (electrons), for which the related formula is cos(theta). A version of Bell's argument is easily fashioned for photons (which of course uses the cos^2 version), and the conclusion is the same: no local realistic theory can reproduce the results of QM (which has been experimentally validated in this respect).
 
  • #60
Bell was Irish and Irish physics is bound to be wrong.
 
  • #61
Epicurus3 said:
Bell was Irish and Irish physics is bound to be wrong.

Ah, but Padraig Harrington is Irish and he won 2 major golf championships this year!
 
  • #62
ThomasT said:
So, I guess we'll have to agree to disagree a little bit here
Sorry but I cannot agree to that.
I do not agree your approach as being based on rational modeling that can be considered acceptable science.
You are claiming classical “polariscopic” assumptions as an acceptable “not weird” or “Not Non-Local” solution that is as scientifically complete as QM.

The cos2 shape of your “Model” is based on measurements of light – not the modeling of individual photons. You cannot just apply the cos2 to individual photons, it is not a “classically reasonable assumption”. Planck demonstrated photons do not have variable intensities like light does.

The EPR paradox is based realistically modeling individual photon behaviors not the average result of measured light intensities. How does this “polariscopic” solution realistically model individual photon movements without even using a Einstein "local and realistic hidden variable". Can you describe those movements for anyone photon?

The “polariscopic” solution is simply an ineffective rebuttal against claims made by QM and the Bell proofs.
 
  • #63
Epicurus3 said:
So Bell's Inequality is incorrectly assuming cos B instead of cos squared B and so proves nothing at all! I knew it all the time!

A couple things you do not seem to know:
The shape of a cos and cos2 functions are exactly the same; one is centered on Zero, the other never goes negative, is centered on 0.5 and twice the Hz.
Also the Bell Inequality shape does not assume a cos and cos2 shape. The Bell Inequality is defined as a straight line that Classical or Local Realistic interpretation should not be able to cross.

It is the QM interpretation that uses a cos and cos2 function to violate that line depending on type of experiment being performed. Stern- Gerlach or Polarization.
 
  • #64
RandallB said:
You are claiming classical “polariscopic” assumptions as an acceptable “not weird” or “Not Non-Local” solution that is as scientifically complete as QM.
I'm claiming, first, that for a classical polariscopic setup the classical model of polarization works ok, and that it doesn't present a weird picture. I don't see how the classical model of polarization is weird or strange. If anyone thinks it is, then I'm interested to see why they think so.

I'm also claiming that the classical polariscopic setup provides an acceptable analogy to simple optical Bell setups -- that is, the two setups have several salient features in common.

RandallB said:
The cos2 shape of your “Model” is based on measurements of light – not the modeling of individual photons. You cannot just apply the cos2 to individual photons, it is not a “classically reasonable assumption”.
Photon detections require light emissions/transmissions of some sort, don't they? Given a polariscopic setup where individual photons are being detected, the intensity of the light transmitted by the analyzing polarizer is the number of photon detections per unit of time. The analog of this in a simple optical Bell setup is the number of coincidental photon detections per unit of time.

RandallB said:
How does this “polariscopic” solution realistically model individual photon movements without even using a Einstein "local and realistic hidden variable".
Hasn't quantum theory taught us that we can't effectively model, and predict the outcomes of, individual trials? The polariscope analogy isn't a solution to the hidden variable problem. It just provides a way of looking at Bell tests that seems to indicate that maybe experimental violations of Bell inequalities aren't telling us anything about nonlocality, because if one understands it as a rather more complicated polariscope, then FTL explanatory fictions are obviated.

RandallB said:
Can you describe those movements for anyone photon?
No.

RandallB said:
The “polariscopic” solution is simply an ineffective rebuttal against claims made by QM and the Bell proofs.
The polariscope analogy isn't aimed at rebutting any claims made by qm. In fact, it provides a way of looking at why, after a qualitative result (a photon detection at one end), the transmission axis of the polarizer associated with the detection can be taken as the principle axis of the disturbance incident on the other polarizer.
 
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  • #65
Epicurus3 said:
The Malus Law comes from:
Actual_Amplitude = Initial_Amplitude CosB - classically reasonable assumption!

But intensity (related to number of particles observed)

Intensity = Amplitude squared

So classical AND quantum predicts:

Actual_Intensity = Initial_Intensity cos squared B - Malus AND QM predictions.

So Bell's Inequality is incorrectly assuming cos B instead of cos squared B
and so proves nothing at all! I knew it all the time!
I'm not sure what you're saying, but it is true that Bell-type inequalities don't, taken by themselves, prove anything. They're mathematical identities. Tautologies.

However, the physical meaning of the experimental and theoretical violation of suitably derived and applied Bell inequalities is still an open question.
 
  • #66
ThomasT said:
The polariscope analogy isn't aimed at rebutting any claims made by qm. In fact, it provides a way of looking at why, after a qualitative result (a photon detection at one end), the transmission axis of the polarizer associated with the detection can be taken as the principle axis of the disturbance incident on the other polarizer.

We've been through this already. But in as much that this is a very plausible picture when it is *the same photon* that went through the first polarizer (and hence "got its principle axis turned into the polarizer direction" by interaction with that polarizer) it is not a surprise that when it arrives at the second polarizer, we find a relationship as given by Malus' law which depends on the difference of the axes of the first polarizer (now integrated into the photon itself after interaction) and the second polarizer (next interaction with the modified photon), I don't see how this can be an evident picture for two separate photons - even though they might start out with the same "principle axis" in the source. In what way will the twisting of the photon axis of the first photon by the first polarizer twist and turn the photon axis of the second one which is far away, so that it gets aligned with the orientation of the first polarizer, before it meets its own (second) polarizer ?
 
  • #67
ThomasT said:
Hasn't quantum theory taught us that we can't effectively model, and predict the outcomes of, individual trials? The polariscope analogy isn't a solution to the hidden variable problem. It just provides a way of looking at Bell tests that seems to indicate that maybe experimental violations of Bell inequalities aren't telling us anything about nonlocality, because if one understands it as a rather more complicated polariscope, then FTL explanatory fictions are obviated.
Well; yah – duh.
That is the whole point!
What your saying here is that your polariscope analogy is a “non-local & unrealistic“ classical interpretation that cannot describe movements for individual photons. I would call that a Classically Modified Copenhagen principle.
That is no less Weird than QM!
And since it does not, IMO, provide any usefully formalism to predicatively apply to physical sciences like chemistry and materials to help produce practical applications of new chemicals, semiconductors, etc. – I would say it not even as complete as QM claims to be.

You cannot hang your hat on an assertion like the polariscope analogy “seems to indicate that maybe” …
Just what are you claiming it does indicate for sure! And how is it not weird.

That you do not see what you have described as weird and non-local only means you have yet to grasp the full meaning behind what “Einstein Local” means.
I recommend that you and Epicurus3 take some time to ruminate on what “Local” means before continuing this pointless argument. Honestly if you cannot grasp the full meaning of Local you are not going to understand EPR; it will just be too advanced for you at this time.

Beyond that, I don’t think I can be of any more help for you on this; – good luck.
 
  • #68
RandallB said:
That you do not see what you have described as weird and non-local only means you have yet to grasp the full meaning behind what “Einstein Local” means.
I recommend that you and Epicurus3 take some time to ruminate on what “Local” means before continuing this pointless argument. Honestly if you cannot grasp the full meaning of Local you are not going to understand EPR; it will just be too advanced for you at this time.

Randall - Bells Theorem is a joke devised after a few Guinesses in a bar by an Irishman. It is ridiculously convoluted and has so many holes in it. "The number of particles which have A but not B plus the number which have B but not C is greater than or equal to the number which have A but not C." It is a clever joke!

You want to prove local variables cannot be true...? He fooled you all!

Of course, this post will be deleted! (because the truth is unbearable)

EDIT (vanesch): I won't delete this post, but it is not the kind of post that is constructive.
 
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  • #69
Epicurus3 said:
Of course, this post will be deleted! (because the truth is unbearable)
No it won't. And we'll try very hard not to lose sleep after your devastating coup de grace. :-p
 
  • #70
DaveC426913 said:
No it won't. And we'll try very hard not to lose sleep after your devastating coup de grace. :-p

If you understand superposition - as Bell did - then his Theroem follows from that with a bit of Sudoku level statistics.

The correlation between the states of two entangled particles is random for both particles as is clear from the wave equation. (not that they have secret states that only 'appear' when observed)

Bell realized that this statement (or similar, - better worded than mine) would not make a career for him, so he devised his joke intelligence test after a couple of beers and managed to make a career out of it. One of the guys in the same bar gave him the idea.

I have seen Bell interviewed - it was clear he had nothing more to contribute to physics than his little superposition side bar - and actually had a thin understanding of physics generally.

<flames on>
So let's hear no more about the subtley of Bell's Theorem PLEASE. Try AOP and pattern programming if you like convolution. Bell's is NOTHING MUCH, and follows from superposition directly.
<flames off>
 
  • #71
Epicurus3 said:
Bell's is NOTHING MUCH, and follows from superposition directly.
This makes absolutely no sense at all, and does little to explain your position.

Other than having an irrational bias against the Irish exactly what is your scientific position.
1) Local Realism is correct – and the Bell proofs against Local Realism are simplistic and flawed.
or
2) The Non-Local QM Copenhagen view is the most complete, but Bell and EPR-Bell experiments do nothing to refute Local Realism (but offering nothing to say why not).
Just state your position clearly:

To say “Bell's follows from superposition directly” only says that Bell agrees with QM’s ability to make predictions. It totally misses the point that Bell only addresses the viability of Local Realism; not the preference of one QM interpretation over another.

If by chance you think you are a Local Realist, you are representing the position irrationally – please read the sickly threads on the top of the forums and abide by the agreements you made on joining PF.
 
  • #72
DaveC426913 said:
No it won't. And we'll try very hard not to lose sleep after your devastating coup de grace. :-p

Well put. I assume that Epicurus3 is simply baiting us at some level.

Hey, there are people who don't think man has been to the moon either. No accounting for some folks' beliefs. No need to waste our time here with them either.
 
  • #73
Epicurus3 said:
If you understand superposition - as Bell did - then his Theroem follows from that with a bit of Sudoku level statistics.

The correlation between the states of two entangled particles is random for both particles as is clear from the wave equation. (not that they have secret states that only 'appear' when observed)

Bell realized that this statement (or similar, - better worded than mine) would not make a career for him, so he devised his joke intelligence test after a couple of beers and managed to make a career out of it. One of the guys in the same bar gave him the idea.

I have seen Bell interviewed - it was clear he had nothing more to contribute to physics than his little superposition side bar - and actually had a thin understanding of physics generally.

<flames on>
So let's hear no more about the subtley of Bell's Theorem PLEASE. Try AOP and pattern programming if you like convolution. Bell's is NOTHING MUCH, and follows from superposition directly.
<flames off>

Ok, your next post will have to contain something more of substance than a statement that Bell was a kind of Irish idiot, or I consider that you are just trolling.

You're warned.
 
  • #74
RandallB said:
This makes absolutely no sense at all, and does little to explain your position.

Other than having an irrational bias against the Irish exactly what is your scientific position.
1) Local Realism is correct – and the Bell proofs against Local Realism are simplistic and flawed.

'Local Realism is correct' - It would be impossible to tie a variable to ONE PARTICLE, because by superposition they could either one decohere - so a variable attached to either particle cannot work unless one can 'contact' the other. Such a local variable would tie a particle to one state - which is not the case. Its obvious from superpostition. So what are you trying to say? I believe that you cannot actually understand what a local variable means.(it means no contact between the two).

They used to think something like this, and this is also what you are still thinking, I assume from lack of clarity:

- 'one particle is actually always X state and the other always Y state, but this is hidden, until observed, so there may be a hidden variable in each particle which says what the particle ACTUALLY IS'. So, yes, yes, these particles have real spins and other states - bla bla bla - which is what they used to think in the 30s, and we know better now - particles do not have ANY state, or ALL states at once - they are in superposition, wave packet, coherent. When observed they pick a state at random. They have NOT got a state that is hidden. - what else can I say to you??

To me its obvious and clear - what's your problem? Stuck in sentences you cannot understand because you believe its so subtle. Sorry, its not. At least Bell's insn't. Come on - let's have some truth here. MAybe you are a physics Historian?

Bell's simply follows on from superposition and what's worse about it, it has so many experimental problems that it almost imposssible to handle in practice (see Thomas's endless whingings about the set up)

Bell's is a red herring and simply derived from his knowledge of superposition. It kind of proves superposition, but is experimentally very hard to do conclusively. A waste of peoples energy.
 
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  • #75
vanesch said:
We've been through this already. But in as much that this is a very plausible picture when it is *the same photon* that went through the first polarizer (and hence "got its principle axis turned into the polarizer direction" by interaction with that polarizer) it is not a surprise that when it arrives at the second polarizer, we find a relationship as given by Malus' law which depends on the difference of the axes of the first polarizer (now integrated into the photon itself after interaction) and the second polarizer (next interaction with the modified photon), I don't see how this can be an evident picture for two separate photons - even though they might start out with the same "principle axis" in the source. In what way will the twisting of the photon axis of the first photon by the first polarizer twist and turn the photon axis of the second one which is far away, so that it gets aligned with the orientation of the first polarizer, before it meets its own (second) polarizer ?

We're assuming that the optical disturbance (associated with each pair of detection attributes) between the two polarizers is one and the same thing during any given coincidence interval (although it is assumed to be varying randomly from interval to interval). That is, in a simple optical Bell setup, whatever is incident on polarizer A during a given coincidence interval is identical to what is incident on polarizer B during that same interval. The polariscopic (not necessarily classical per se -- ie. we could be accumulating single photon detections) analog of this assumption is that the optical disturbance transmitted by the first polarizer is identical to the optical disturbance incident on the second, or analyzing, polarizer.

This is the assumption that underlies the qm projection along the transmission axis associated with a detection.

In the polariscopic setup, the intensity of the transmission from the analyzing polarizer is a cos2 function of the difference between the transmission axes of the first and second polarizers. The amplitude of the resultant wave is altered by the rotation of either the second polarizer or the first polarizer.

This is what happens in Bell tests also. For essentially the same reason.
_____________________

Whether the above is acceptable or not, I've thought some more about your comments on the definition of quantum entanglement and I see your point that the only unambiguous meaning of the term quantum entanglement is its formal expression(s) within quantum theory.
 
  • #76
ThomasT said:
This is what happens in Bell tests also. For essentially the same reason.
NO
I suspect you still do not have a proper grasp of what Bell is asking an experiment to show and a LR (Local Realistic) description to explain.

Bell tests measure and summarize results from individual photons – NOT intensirtly levels from large groups of Photons (polariscopic method).
Sure – IF when B is measured at 22.5° while A is at 45° (If both were at 45° it gives 0% intensity correlation) you still saw 100% of the Photons – BUT at 15% of the proper energy of each photons energy level then yes your “Intensity” comparison would work. But the well known facts are quantum photon energy level don’t change intensity! You observe 15% of the photons not 15% of their each photons energy.

With A at 45° a random distribution of 50% V (0°) and 50% H (90°) could correctly predict 50% at H or V for the B test. A random distribution can also correctly predict 100% at 135° and 0% at 45°. BUT at 22.5° a polariscopic style random distribution can only predict 25% NOT 15°.

That is ON the Bell inequity line not a violation of it as is required to match the QM results.
 
  • #77
ThomasT said:
We're assuming that the optical disturbance (associated with each pair of detection attributes) between the two polarizers is one and the same thing during any given coincidence interval (although it is assumed to be varying randomly from interval to interval). That is, in a simple optical Bell setup, whatever is incident on polarizer A during a given coincidence interval is identical to what is incident on polarizer B during that same interval. The polariscopic (not necessarily classical per se -- ie. we could be accumulating single photon detections) analog of this assumption is that the optical disturbance transmitted by the first polarizer is identical to the optical disturbance incident on the second, or analyzing, polarizer.

Well, that's not going to work, as we discussed already. Imagine the polarizers at 90 degrees with respect to one another. As the incident disturbances are random, some will have "45 degrees", no ? Well, a 45 degree disturbance (which will be part of the set of random disturbances sent out) should have 50% probability (intensity whatever) to get through each polarizer. So in half of the cases where we saw something "left", we should also see something "right" for these distrubances, right ?
Well, that doesn't follow the cos^2 law, which tells us that there can NEVER be any click on the left when there is one on the right and vice versa. So even if there's only a small amount of "45 degree disturbances" in the lot that's randomly sent out to the left and the right, and half of them make "common clicks", this would violate the cos^2 law which says that never there can be any common clicks.

Again, the reason why we have a cos^2 law in the *successive* polarizers, is that the disturbance AFTER the first one has been aligned with the orientation of the first polarizer (and has "forgotten" its original incident orientation).
 
  • #78
vanesch said:
Well, that's not going to work, as we discussed already. Imagine the polarizers at 90 degrees with respect to one another. As the incident disturbances are random, some will have "45 degrees", no ? Well, a 45 degree disturbance (which will be part of the set of random disturbances sent out) should have 50% probability (intensity whatever) to get through each polarizer. So in half of the cases where we saw something "left", we should also see something "right" for these distrubances, right ?
I don't think this is the correct way to analyze the situation. Nothing can be said about the orientations of the incident disturbances or for that matter about anything that's qualitatively going on in individual trials independent of instrumental behavior. We only know if a detection is registered or not during a certain interval.

So, let's say that A detects first during some coincidence interval. The projected amplitude wrt the disturbance incident on B is assumed to be the same as A's which means that the probability of detection at B with polarizers aligned is 1, and with polarizers perpendicular to each other it's 0.

As the polarizer at B is rotated away from alignment with the polarizer at A, the amplitude of the transmitted component of the wave incident on the polarizer at B will vary as the cosine of the angular difference. The probability of detection at B is the intensity of the wave transmitted by the polarizer at B, which is the amplitude squared, which is cos2
Theta, which is Malus' Law -- which is the probability of coincidental detection.

Of course this probability has no physical meaning wrt any given individual trial, or coincidence interval or single pair of detection attributes. It's a statement regarding the expected frequency of coincidental detection given a large number of trials.

So, I don't think that your argument above renders the analogy invalid. Something else might, but not that.

vanesch said:
Again, the reason why we have a cos^2 law in the *successive* polarizers, is that the disturbance AFTER the first one has been aligned with the orientation of the first polarizer (and has "forgotten" its original incident orientation).
In either case (Bell test or polariscope), extending between the two polarizers is a disturbance or disturbances with common properties.

In the polariscopic setup, the first polarizer is the analog of polarizer A above (that is, it's the analog of whichever polarizer is associated with the first detection during some coincidence interval in a Bell test). Think of the disturbance between A and B in a Bell test as being transmitted by the polarizer that registers the initial detection in a given coincidence interval and incident on the other polarizer.
 
  • #79
ThomasT said:
I don't think this is the correct way to analyze the situation.
……
….. As the polarizer at B is rotated away from alignment with the polarizer at A, the amplitude of the transmitted component of the wave incident on the polarizer at B will vary as the cosine of the angular difference.
No once again – it is your way of analyzing the situation here that eliminates it from having any meaningful relation to BELL or “Entangelement”.

The only way you can use “amplitude” to allow your polariscopic to work is to select a detection coincidence interval at A that measures 1000 photons, and compare that to the same detection coincidence interval at B and use the B photon count as a measure of amplitude. Sure that will work – But is not an explanation entanglement and not at all what Bell is talking about as Bell requires quantum level (individual photon) comparisions. Until you understand that you will not be on the same page as vanesch or anyone else. Bell requires a Local Realistic description of the individual photon behaviors Not the apparent amplitude changes of groups of large numbers of photons.

The polariscopic Classical description can only be though of as a Classical Non-Local because it does not bring with it enough photon level detail to call it “Local”. And without that level of detail it can hardly be looked to for any help with the formalization of QM entanglement.
Remember Bell only addresses the viability of Local descriptions.
 
  • #80
RandallB said:
NO
I suspect you still do not have a proper grasp of what Bell is asking an experiment to show and a LR (Local Realistic) description to explain.
That's a definite possibility.

RandallB said:
Bell tests measure and summarize results from individual photons – NOT intensirtly levels from large groups of Photons (polariscopic method).
Intensity in Bell tests is the rate of coincidental detection per unit of time. The probabilities of coincidental detection refer to large numbers of individual trials. As the unit of time (and the number of trials) increases, the experimental results more closely approximate the predicted values.

The probability of individual detection at A or B for any and all individual trials remains 1/2.

RandallB said:
But the well known facts are quantum photon energy level don’t change intensity! You observe 15% of the photons not 15% of their each photons energy.
Yes, that's a hypothesis that seems to be supported by certain experimental results. I've got to think about this some more.

Without going into why, I'm confused again. Thanks for your replies, and vanesch and DrChinese and others.
 
  • #81
RandallB said:
No once again – it is your way of analyzing the situation here that eliminates it from having any meaningful relation to BELL or “Entangelement”.
I'm just talking about the similarities between the experimental setups.

RandallB said:
The only way you can use “amplitude” to allow your polariscopic to work is to select a detection coincidence interval at A that measures 1000 photons, and compare that to the same detection coincidence interval at B and use the B photon count as a measure of amplitude. Sure that will work ...
As I mentioned, the polariscopic setup can be one that counts individual photon detections.

RandallB said:
... But is not an explanation entanglement ...
I agree. Even if the analogy is valid, it still doesn't explain what entanglement is. But, if it is valid, then it's a stepping stone to understanding what it probably isn't and what it might be.

RandallB said:
... and not at all what Bell is talking about as Bell requires quantum level (individual photon) comparisions.
I don't know what you mean by this.

RandallB said:
Until you understand that you will not be on the same page as vanesch or anyone else.
Are you talking about the pairing process?

I've got to run -- will get to the rest of this later. Thanks.
 
  • #82
ThomasT said:
So, let's say that A detects first during some coincidence interval. The projected amplitude wrt the disturbance incident on B is assumed to be the same as A's which means that the probability of detection at B with polarizers aligned is 1, and with polarizers perpendicular to each other it's 0.

Why should the projected amplitude wrt to the disturbance incident on B be the same as A's ?
They should be the same, all right. But they should not be the same as the orientation of the polarizer, no ?

You do agree that the orientation of the light *changes* when it gets through a polarizer, right ? That it takes on the orientation of the polarizer ? Or not ? But how could the light at B *change* in accordance with the orientation of the polarizer at A ?

Because, consider the following setup:
one beam, 3 polarizers. The first one at 90 degrees, the second one at 45 degrees, the third one at 0 degrees. Does any light get through this setup or not ?
 
  • #83
ThomasT said:
As I mentioned, the polariscopic setup can be one that counts individual photon detections.
But you disrearded that when you earler said:

"As the polarizer at B is rotated away from alignment with the polarizer at A, the amplitude of the transmitted component of the wave incident on the polarizer at B will vary as the cosine of the angular difference."

Which would require that at some angle that individual photon deterction would require it deleiver only 15% of the energy in that photon.

Nothing Quantum or in Bell can accept that plan.
 
  • #84
peter0302 said:
Hehe, I can't really tell what side you're taking. :) But my answer is collapse can't be a physical process; it's just that quantum statistics don't conform to the laws of macro-statistics.

Wouldn't you rather throw out classical statistics than throw out relativity? :)

hmmm, maybe neither...
...as photons are bosons, can we use Bose-Einstein statistics?
Can we consider an entangled pair of photons as a Bose-Einstein condensate?
If we 'push it too hard' it collapses, but will 'reform' if the conditions are amenable.
 
  • #85
'kay...
...that went down well.

What about this...

...I get two 'bosons' into a 'space' for which they are too big to 'fit' they conform to Bose-Einstein statistics.

...if I make two 'bosons' from something that was in a 'space' in which they are too big to 'fit' (presuming that two photons created as an entanged pair from a single
photon take more 'space' than the original) what happens?

Assuming, presumably, that 'all things are still equal' (i.e. there is conservation of energy/momentum) does this seem correctly time-symmetric?

If so, could we appeal to Noether's theorem? (I'm not quite sure of the logic!...might be the wrong way round... does a conservation law imply a symmetry?)

I'm not fully familiar with the fermionic version of entanglement so this might seem stupid as a result of the mechanics of that.

Is this crackpottery? Probably...
 
  • #86
moving_on said:
'kay...
...that went down well.

What about this...

...I get two 'bosons' into a 'space' for which they are too big to 'fit' they conform to Bose-Einstein statistics.

...if I make two 'bosons' from something that was in a 'space' in which they are too big to 'fit' (presuming that two photons created as an entanged pair from a single
photon take more 'space' than the original) what happens?

Assuming, presumably, that 'all things are still equal' (i.e. there is conservation of energy/momentum) does this seem correctly time-symmetric?

If so, could we appeal to Noether's theorem? (I'm not quite sure of the logic!...might be the wrong way round... does a conservation law imply a symmetry?)

I'm not fully familiar with the fermionic version of entanglement so this might seem stupid as a result of the mechanics of that.

Is this crackpottery? Probably...

Photon not needing space because fermion already in hole wait for him.
 
  • #87
DrChinese said:
I haven't seen a paper which answers this particular question, maybe someone else has... (I have scanned the preprint archive but to no avail so far).

Most Bell tests use polarizing beam splitters (PBS) to check photons at Alice and Bob. Typical are 2 detectors at Alice and 2 at Bob. Results of all 4 are correlated and analyzed. You would normally say the entanglement ends once we know which way the photon goes through the beam splitter.

What if we takes the 2 beams at Alice and merge them back very precisely together again? I.e. such that it is no longer possible to tell which path the photon took through the PBS. I would expect that the resultant reconstructed beam (Alice) is still entangled with Bob. If you tested Alice and Bob at this point, I would expect us to see the perfect correlations and the Bell inequality violations per usual. Is this correct?

So when does the entanglement actually end? If what I am saying is right, the PBS is not actually capable of ending the entanglement itself. Instead, it is the detection of the photon - and what we know about it at that point - which ends the entanglement. I believe this is fully consistent with the QM prediction.



I have come to this thread rather late so I may have missed references to recent literature, if so I apologize for the duplication. There is a short review article Sudden Death of Entanglement by Ting Yu and J. H. Eberly in the 30 January 2009 issue of Science . Note: the article starts on page 598. The table of contents is in error --it says page 602. There are several other relevant articles in previous issues of Science :

J. H. Eberly and Ting Yu, The End of an Entanglement , Science . 27 April 2007, page 555.

M. P. Almeida, et. al. Environment-Induced Sudden Death of Entanglement , same issue of Science , page 579.

The longevity of entanglement is an active area of research because of its importance to the success of quantum computation and communication. One of the initial problems was to settle on a suitable measure of entanglement. It seems that the current consensus is to use a concept called concurrence { W. K. Wootters, Phys. Rev. Lett. 80 , 2245 (1998), see also Phys. Rev. Lett. 78 , 5022 (1997) and arXiv:quant-ph/9709029v2 13 Sep 1997 }

There is a long review article: Measures and dynamics of entangled states in Phys. Repts. 415 , 207 (2005), also arXiv:quant-ph/0505162v1 22 May 2005

Quantum entanglement for composite systems is often defined in terms of the density matix. See Appendix B of David J. Tannor, Introduction to Quantum Mechanics, A Time Dependent Perspective for a lucid synopsis.

I hope that you will find these references useful.
 
  • #88
AEM said:
J. H. Eberly and Ting Yu, The End of an Entanglement , Science . 27 April 2007, page 555.

http://www.sciencemag.org/cgi/content/abstract/316/5824/579
from the above quote:
"Using an all-optical experimental setup, we showed that, even when the environment-induced decay of each system is asymptotic, quantum entanglement may suddenly disappear. This sudden death constitutes yet another distinct and counterintuitive trait of entanglement."

The disappearance of entanglement appears to be unpredictable but sudden, ummmm..
 
  • #89
p764rds said:
http://www.sciencemag.org/cgi/content/abstract/316/5824/579
from the above quote:
"Using an all-optical experimental setup, we showed that, even when the environment-induced decay of each system is asymptotic, quantum entanglement may suddenly disappear. This sudden death constitutes yet another distinct and counterintuitive trait of entanglement."

The disappearance of entanglement appears to be unpredictable but sudden, ummmm..

Please, what's your point? Could you elaborate a little more?
 
  • #90
AEM said:
Please, what's your point? Could you elaborate a little more?

The results of exactly how entanglement ends - i.e. the exact ending time is unpredictable but it ends suddenly - is interesting.

sudden ending:
I would expect the end of entanglement to be instantaneous because otherwise there would be strange states of half entangled, quarter entangled until completely disentangled. There is nothing I know in QM that indicates this could happen. i.e. particles are entangled or not - no half way or phase lags. So it means, probably, that there is no 'inertia', so to speak, in the entangled states ending and occurring. It points to the hypothesis that the process of entanglement would probably be instantaneous too, but that was not tested. Would anyone expect different though?

unpredictable ending time:
This is a problem for quantum computing since it would limit the attainable clock speeds for computing. I would like to know if the entanglement end time has any variables associated with it and why is it unpredictable? It could be as simple as the probabilty of state observables between two particles (observer and observed) is the cause. So that when they approach each other there is no clear trigger point - only combined probabilities to condsider.
Could we also expect the same is true for entanglement starting? Is that also unpredictable but sudden?

Thats my take on it, and its only surmising possiblities from the paper quoted above.
 
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  • #91
As AEM said, the brazilian group of quantum optics at UFRJ has worked on this subject a lot.

Best regards

DaTario
 
  • #92
DaTario said:
As AEM said, the brazilian group of quantum optics at UFRJ has worked on this subject a lot.

Best regards

DaTario

I would expect that the disappearance of entanglement is sudden (instant) but the exact moment unpredictable. If it had been anything else I would be very confused.

Is it a big deal? I mean is it crucial in some way?
 
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