Why is entanglement necessary for understanding quantum mechanics?

In summary, the conversation discusses the concept of entanglement in quantum mechanics, where two particles can be connected in such a way that measuring one instantly affects the other, regardless of the distance between them. This phenomenon has been proven through various experiments, such as the Bell's Theorem and related experiments. The need for this property arises from the fact that classical physics cannot explain the perfect anti-correlation observed in entangled particles. The evidence for this phenomenon was first observed through experiments involving entangled pairs of particles, and it has been a subject of ongoing research in the scientific community.
  • #71
Jabbu said:
When we say we emitted a single photon through a single polarizer and [itex]\theta[/itex] = 30 degrees, it means polarizer absolute angle can be anything, as long as photon is either 30 degrees clockwise or 30 degrees anticlockwise polarized relative to the polarizer absolute axis. Right?

Yes, in the sense that we can choose to call any angle we wish "zero" and (for example) ##\theta_A=10##, ##\theta_B=70##, ##\omega_A=-35##, ##\omega_B=55## is the same situation with a different zero point ##\theta_A=20##, ##\theta_B=80##, ##\omega_A=-25##, ##\omega_B=65##.

But you're still missing the point. We set one polarizer to angle ##\theta_A## and second polarizer to angle ##\theta_B##. There are no values ##\omega_A## and ##\omega_B## such that for all ##\theta_A## and ##\theta_B##:
1) Malus's law for ##\theta_A-\omega_A## matches the experimental results at polarizer A AND
2) Malus's law for ##\theta_B-\omega_B## matches the experimental results at polarizer B AND
3) ##\omega_A## and ##\omega_B## are at right angles to one another.

That's how we know that the photons do not have definite polarizations ##\omega_A## and ##\omega_B## when they're created.
 
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  • #72
stevendaryl said:
No, [itex]\theta_A[/itex] has nothing to do with any "initial polarization". The filter can turn about an axis. There is one point on the axis that is labeled [itex]0[/itex], and the angle is measured relative to that. Of course, to be meaningful, [itex]\theta_B[/itex] and [itex]\theta_A[/itex] have to be measured relative to the same zero point. But the zero point has nothing to do with the polarization of the light.

http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/polcross.html
http://en.wikipedia.org/wiki/Malus's_law#Malus.27_law_and_other_properties
http://en.wikipedia.org/wiki/Photon_polarization

Theta is always defined as the angle between the light's initial polarization and the axis of the polarizer, otherwise it would be arbitrary. Where did you ever see theta refers to some absolute polarizer angle unrelated to light polarization?


As I said earlier, you can change [itex]\theta_A[/itex] and [itex]\theta_B[/itex] in the middle of the experiment, and it makes no difference (in the entangled case). All that matters is [itex]\theta_A - \theta_B[/itex] at the time the photons pass through Alice's and Bob's filter.

Of course you can change [itex]\theta_A[/itex] and [itex]\theta_B[/itex] whenever you want, just keep photons polarization constant and rotate the polarizers. Yes, all that matters is [itex]\theta_A - \theta_B[/itex] at the time the photons pass through Alice's and Bob's filter. But does it mean the result is predetermined exclusively by the polarizers and photons don't even matter at all?


That would be true if Malus' law worked for individual photons, but it doesn't. That's what I've been telling you---Malus' law does not work. The QM prediction (for entangled photons) only involves [itex]\theta_A - \theta_B[/itex]. It does NOT involve any polarization angle for the photons. (Because there is no such angle.)

Why do you think Malus law would work for a light beam with 10 billion photons but not for a single photon? If each one of 10 billion vertically polarized photons have 50% chance to pass through polarizer rotated at 45 degrees relative angle, then a single photon has to have that same chance as well. I see you're saying [itex]\theta_A and \theta_B[/itex] are absolute polarizer angles, but I don't understand why would you think something like that.
 
  • #73
Jabbu said:
Theta is always defined as the angle between the light's initial polarization and the axis of the polarizer

That is not correct. Malus' law does not apply in EPR experiments. In EPR experiments, there IS no "initial polarization"
 
  • #74
Jabbu said:
Why do you think Malus law would work for a light beam with 10 billion photons but not for a single photon?

You're comparing two different experiments:

(1) You start with light having a known polarization. In that case, the photons are NOT entangled. In that case, Malus' law works.

(2) You start with a pair of entangled photons. In that case, Malus' law does NOT work.

Both cases are described by QM, but only the first case is described by Malus' law. The two theories make the same prediction in the first case, but not the second case.

Once again, Malus' law does not describe entangled photons. The case where you are talking about, with a light beam consisting of 10 billion photons, does not involve entangled photons.
 
  • #75
Jabbu said:
If each one of 10 billion vertically polarized photons have 50% chance to pass through polarizer rotated at 45 degrees relative angle, then a single photon has to have that same chance as well. I see you're saying [itex]\theta_A and \theta_B[/itex] are absolute polarizer angles, but I don't understand why would you think something like that.

No one is disputing that for polarized photons, and that is entirely the point. But entangled photons lack a specific polarization until they are measured. As a result, their statistics are different. Because you keep mentioning Malus, you are confusing things. Malus applies to the example above just fine.

a. Take a stream of photons polarized at 0 degrees (call that vertical), and send the stream through a polarizer at 45 degrees. Malus (applied to classical light) and QM make the same predictions: cos^2(45)= .5.

b. Take 2 vertical photons and run them through polarizers at 45 degrees, and the chance they will match is: .25 (++ case) + .25 (-- case) = .5. Malus (applied to classical light) and QM make the same predictions again.

c. Take 2 Type I polarization entangled photons and run them through polarizers at 45 degrees, and the chance they will match is: 0 (++ case) + 0 (-- case) = 0. Note that by coincidence (although it is related), the result is per the formula 1-cos^2(theta) where theta is 0 degrees. Yes, it seems to be the same formula as per a. but we arrive at that point by a completely different logic set. And you won't get the correct answer using a classical model a la Malus. You cannot just say "I will use the QM formula on my classical model" - that is called hand-waving.

So this is the point we are making, the statistics are different for entangled photons than what you are modeling. Work it out and you will conclude the same.
 
  • #76
stevendaryl said:
You're comparing two different experiments:

(1) You start with light having a known polarization. In that case, the photons are NOT entangled. In that case, Malus' law works.

(2) You start with a pair of entangled photons. In that case, Malus' law does NOT work.

Both cases are described by QM, but only the first case is described by Malus' law. The two theories make the same prediction in the first case, but not the second case.

Once again, Malus' law does not describe entangled photons. The case where you are talking about, with a light beam consisting of 10 billion photons, does not involve entangled photons.

For the entangled photons, couldn't I take the reduced density matrix for one, so that its polarization would be a local observable, and effectively equivalent to a statistical mixture of photons with definite polarization, to which I can then apply Malus's Law?
 
  • #77
atyy said:
For the entangled photons, couldn't I take the reduced density matrix for one, so that its polarization would be a local observable, and effectively equivalent to a statistical mixture of photons with definite polarization, to which I can then apply Malus's Law?

Yes, that's equivalent (as far as the answer you get) to the "collapse" interpretation, where after a measurement, the photons are in a definite polarization state. The point is that you can't get the right answer from Malus' law alone. The thread started with someone asking what's weird about QM, when the predictions for EPR are the same as the classical predictions (Malus' law).
 
  • #78
atyy said:
For the entangled photons, couldn't I take the reduced density matrix for one, so that its polarization would be a local observable, and effectively equivalent to a statistical mixture of photons with definite polarization, to which I can then apply Malus's Law?

Not unless you first run it through a polarizer to reduce it. Otherwise, you just get what appears to be a statistical mixture of H and V photons.
 
  • #79
DrChinese said:
Not unless you first run it through a polarizer to reduce it. Otherwise, you just get what appears to be a statistical mixture of H and V photons.

The idea is if I have a statistical mixture only of H photons, then I can treat the mixture with Malus's Law. Similarly, if I have a mixture only of V photons, I can treat the mixture with Malus's Law. Since I have effectively a statistical mixture of H and V photons, the result should be a statistical mixture of Malus's Law applied to H photons and Malus's Law applied to V photons.
 
  • #80
stevendaryl said:
Yes, that's equivalent (as far as the answer you get) to the "collapse" interpretation, where after a measurement, the photons are in a definite polarization state. The point is that you can't get the right answer from Malus' law alone. The thread started with someone asking what's weird about QM, when the predictions for EPR are the same as the classical predictions (Malus' law).

Yes, I agree. I just thought maybe it's confusing to Jabbu to have been told both that Malus's Law does and does not apply to single photons in the quantum case (I think Nugatory said that in post #22, and he was probably thinking of the reduced density matrix). Anyway, I thought maybe this idea that one can effectively apply Malus's Law to single photons even in the entangled quantum case, can help make the entangled quantum case closer to classical case, so that one can see how they really diverge.
 
  • #81
atyy said:
Yes, I agree. I just thought maybe it's confusing to Jabbu to have been told both that Malus's Law does and does not apply to single photons in the quantum case (I think Nugatory said that in post #22, and he was probably thinking of the reduced density matrix). Anyway, I thought maybe this idea that one can effectively apply Malus's Law to single photons even in the entangled quantum case, can help make the entangled quantum case closer to classical case, so that one can see how they really diverge.

Yes. I guess there are two different facts about quantum polarization experiments: What happens at individual filters can be explained by Malus' law. But correlations between two different filters is an additional piece of information that is not explained by Malus' law (unless you add the "collapse" interpretation).
 
  • #82
stevendaryl said:
In an EPR experiment, we don't produce polarized photons. There is some atomic reaction (radioactive decay) that produces two photons. One photon goes through (or is blocked by) Alice's filter, and the other goes through (or is blocked by) Bob's filter. Alice's and Bob's filter angles are measured relative to an arbitrary zero point, not relative to any initial photon polarization. When a particle decays, there is no associated "polarization angle".

But it is constant. I believe that's how the setup is calibrated. You rotate the polarizer until the detector starts reading all zeros or all ones, where zeros mean the polarizer is at 90 degrees relative to photons polarization, and all ones means they are perfectly aligned and theta = 0, so there you set the zero point, deliberately, not arbitrarily.

If photon polarization was random, then when we change polarizer angle from vertical to horizontal, why does it matter? Photons with random polarization is unpolarized light, they have 50% chance to go through regardless of the polarizer absolute rotation.
 
  • #83
Jabbu said:
But it is constant. I believe that's how the setup is calibrated. You rotate the polarizer until the detector starts reading all zeros or all ones, where zeros mean the polarizer is at 90 degrees relative to photons polarization, and all ones means they are perfectly aligned and theta = 0, so there you set the zero point, deliberately, not arbitrarily.

That is not what is done in EPR-type experiments. Once again, in the EPR experiment, you don't start with polarized light. You start with some particle decaying.

If photon polarization was random, then when we change polarizer angle from vertical to horizontal, why does it matter? Photons with random polarization is unpolarized light, they have 50% chance to go through regardless of the polarizer absolute rotation.

The point is that in the case of an entangled pair of photons, the polarization seems random, in the sense that Alice's filter passes 50% of the photons that reach it, and Bob's filter also passes 50% of its photons. But in another sense it is not random: If Alice and Bob have the same filter settings, and a photon passes Alice's filter, it will, with 100% probability, also pass Bob's filter. If a photon is blocked by Alice's filter, it will, with 100% probability, also be blocked by Bob's filter.
 
  • #84
stevendaryl said:
That is not correct. Malus' law does not apply in EPR experiments. In EPR experiments, there IS no "initial polarization"

Absolute theta is arbitrary by itself no matter what experiment. It would be like entering 38 every time into the equation and still get different results. Do you have any reference that defines theta as absolute polarizer angle and unrelated to light polarization?
 
  • #85
Jabbu said:
Absolute theta is arbitrary by itself no matter what experiment. It would be like entering 38 every time into the equation and still get different results.

Alice's angle [itex]\theta_A[/itex] is arbitrary, and Bob's angle [itex]\theta_B[/itex] is arbitrary, but the difference [itex]\theta_A - \theta_B[/itex] is the relevant quantity that enters in the QM prediction:

Probability that Alice's result is the same as Bob's result = [itex]cos^2(\theta_A - \theta_B)[/itex]

Do you have any reference that defines theta as absolute polarizer angle and unrelated to light polarization?

As I said, in EPR, you don't start with polarized light. The formula can't possibly be related to light polarization, because the light isn't polarized.
 
  • #86
Jabbu said:
But it is constant. I believe that's how the setup is calibrated. You rotate the polarizer until the detector starts reading all zeros or all ones, where zeros mean the polarizer is at 90 degrees relative to photons polarization, and all ones means they are perfectly aligned and theta = 0, so there you set the zero point, deliberately, not arbitrarily.

In that case your belief is wrong. The quantity which is entangled is necessarily ill defined. polarization entangled photons are umpolarized on their own. Momentum entangled photons have a broad distribution of individual momenta. Energy-entangled photons are spectrally broad.

Jabbu said:
If photon polarization was random, then when we change polarizer angle from vertical to horizontal, why does it matter? Photons with random polarization is unpolarized light, they have 50% chance to go through regardless of the polarizer absolute rotation.

That point was already covered. The relative angle between the polarizers and the relative angle of polarization between the two photons matter. This relative angle is well defined. The single photon polarizations are not.

Let us remove most of the details and focus on the absolutely basic stuff and a strongly simplified scenario. We have a light source emitting two photons and the polarizations have to be orthogonal in the end. Now we set the polarizers to some fixed settings (say 0°/90°) and compare two basic scenarios:

1) The source emits two photons of well defined polarization. Sometimes 0°/90°. Sometimes 45°/135°. Sometimes 157°/247°. You can get the expected correlation by applying Malus' law independently to each photon and polarizer setting.

2) The source emits two photons, but the polarization is undefined. If the first measurement at a polarizer results in transmission, the polarizer forces the photon to acquire a polarization matching that of the polarizer setting and the other photon instantaneously "jumps" to the orthogonal polarization.

Leaving all details on real physics aside, do you agree that these two scenarios will give different coincidence count rates?
 
  • #88
stevendaryl said:
Alice's angle [itex]\theta_A[/itex] is arbitrary, and Bob's angle [itex]\theta_B[/itex] is arbitrary, but the difference [itex]\theta_A - \theta_B[/itex] is the relevant quantity that enters in the QM prediction:

Probability that Alice's result is the same as Bob's result = [itex]cos^2(\theta_A - \theta_B)[/itex]

So if the equation carries no information about photons, does it not mean the result is predetermined by polarizers alone?


As I said, in EPR, you don't start with polarized light. The formula can't possibly be related to light polarization, because the light isn't polarized.

From all the papers I've seen I don't remember anyone suggested anything like that.

When detectors A and B read:

A: 1 1 1 1 1 1 1 1 1 1..
B: 0 0 0 0 0 0 0 0 0 0..

relative angle between photons A polarization and polarizer A is theta_A = 0?
relative angle between photons B polarization and polarizer B is theta_B = 90?
Correlation = ?


A: 1 1 0 1 0 1 0 0 1 0...
B: 0 0 1 1 0 0 0 0 0 0...

relative angle between photon A polarization and polarizer A is theta_A = 45?
relative angle between photon B polarization and polarizer B is theta_B = ?
Correlation = ?
 
  • #89
Jabbu said:
So if the equation carries no information about photons, does it not mean the result is predetermined by polarizers alone?

Now you're getting to what's strange about EPR. It seems as if Bob's result depends on Alice's filter setting.

From all the papers I've seen I don't remember anyone suggested anything like that.

Did you ever read anything about EPR that suggested that the twin photons are polarized?
 
  • #90
Jabbu said:
When detectors A and B read:

A: 1 1 1 1 1 1 1 1 1 1..
B: 0 0 0 0 0 0 0 0 0 0..

relative angle between photons A polarization and polarizer A is theta_A = 0?
relative angle between photons B polarization and polarizer B is theta_B = 90?
Correlation = ?

I think you're getting two different experiments confused. In the EPR experiment, both Alice and Bob detect 50% of the photons, regardless of [itex]\theta_A[/itex] or [itex]\theta_B[/itex]. What's of interest are the correlations. If [itex]\theta_A = \theta_B[/itex], then there is 100% correlation. if [itex]\theta_B = \theta_A + 90^o[/itex], then there is 100% anti-correlation.
 
  • #92
Cthugha said:
Let us remove most of the details and focus on the absolutely basic stuff and a strongly simplified scenario. We have a light source emitting two photons and the polarizations have to be orthogonal in the end.

I think I may have gotten a detail wrong in the two-photon EPR case. Or maybe you did. What I thought was that the two photons had the SAME polarizations. rather than polarizations that differ by 90 degrees.
 
  • #93
Jabbu said:
But it is constant. I believe that's how the setup is calibrated. You rotate the polarizer until the detector starts reading all zeros or all ones, where zeros mean the polarizer is at 90 degrees relative to photons polarization, and all ones means they are perfectly aligned and theta = 0, so there you set the zero point, deliberately, not arbitrarily.
No, that is not how it works. The source does not have any preferred direction, so no matter how you rotate the source or one of the directors you will get a random stream of zeroes and ones at that detector as half the photons pass and half don't (which is, BTW, consistent with Malus's law for photons of random orientation reaching the polarizer).

If photon polarization was random, then when we change polarizer angle from vertical to horizontal, why does it matter? Photons with random polarization is unpolarized light, they have 50% chance to go through regardless of the polarizer absolute rotation.

Changing the angle of the polarizer does not matter, because you get a 50% pass rate no matter what angle you choose. However, the angle between the two polarizers does matter, and indeed that's what the whole thing is about. If the two polarizers are oriented at 90 degrees relative to one another, then every time we get a 1 at the left-hand polarizer we'll get a 1 at the right-hand polarizer; if they are oriented at zero degrees relative to each other, then every time we get a 1 at the left-hand polarizer we get a 0 at the right-hand polarizer; but if we look at the results from only one of them, we'll see a random stream of ones and zeroes.

For any in-between angle: If the A detector reads 1, the B detector will give a 0 or 1 result with the probability predicted by Malus's law if ##\omega_B## is at right angles to ##\theta_A##; and if the A detector reads 0 the B detector will give a 0 or 1 result with the probability predicted by Malus's law if ##\omega_B## is equal to ##\theta_A##.
 
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  • #94
stevendaryl said:
I think I may have gotten a detail wrong in the two-photon EPR case. Or maybe you did. What I thought was that the two photons had the SAME polarizations. rather than polarizations that differ by 90 degrees.

Oh, both are possible, depending on whether you have a type I or type II spdc crystal.

My main point was just to remove a bit of the discussion on the physical details of entanglement and steer Jabbu towards the point of the realism assumption. The fact that it makes a real measurable difference whether you assume that particles are emitted with well defined properties right from the start or whether you assume that these properties become well defined only during the first measurement made.
 
  • #95
Jabbu said:
They say probability is cos^2(theta_2 - theta_1), where theta 1 and 2 are light polarization and polarizer angle. That's what I've been saying, it's Malus's law.

No, it does not say that. On the previous page, it says:

What if we measured polarizations at arbitrary angles [itex]\theta_1[/itex], [itex]\theta_2[/itex]?

[itex]\theta_1[/itex] and [itex]\theta_2[/itex] are the orientations of the filters. That's clearly what's being shown in the figure on page 8.

Read through to page 13. They clearly say that the QM prediction is different from what would be expected classically.
 
  • #96
Cthugha said:
That point was already covered. The relative angle between the polarizers and the relative angle of polarization between the two photons matter. This relative angle is well defined. The single photon polarizations are not.

I was talking about only one polarizer. Detector readings are recorded separately for each polarizer and streams of data, when theta = 0 and correlation = 100%, look like this:

A: 1 1 1 1 1 1 1 1 1 1...
B: 1 1 1 1 1 1 1 1 1 1...

Can angle between photons A polarization and polarizer A be anything else but zero degrees?


Let us remove most of the details and focus on the absolutely basic stuff and a strongly simplified scenario. We have a light source emitting two photons and the polarizations have to be orthogonal in the end. Now we set the polarizers to some fixed settings (say 0°/90°) and compare two basic scenarios:

1) The source emits two photons of well defined polarization. Sometimes 0°/90°. Sometimes 45°/135°. Sometimes 157°/247°. You can get the expected correlation by applying Malus' law independently to each photon and polarizer setting.

2) The source emits two photons, but the polarization is undefined. If the first measurement at a polarizer results in transmission, the polarizer forces the photon to acquire a polarization matching that of the polarizer setting and the other photon instantaneously "jumps" to the orthogonal polarization.

Leaving all details on real physics aside, do you agree that these two scenarios will give different coincidence count rates?

The simplest case is to take a single setup where for example theta_A = -30 and theta_B = +30 degrees. QM predicts 25% correlation (75% discordance), and Malus law is supposed to give different result, right? So what result Malus law predicts and how do you arrive at it?
 
  • #97
stevendaryl said:
I think you're getting two different experiments confused. In the EPR experiment, both Alice and Bob detect 50% of the photons, regardless of [itex]\theta_A[/itex] or [itex]\theta_B[/itex]. What's of interest are the correlations. If [itex]\theta_A = \theta_B[/itex], then there is 100% correlation. if [itex]\theta_B = \theta_A + 90^o[/itex], then there is 100% anti-correlation.

If photons always had 50% chance it would always yield the same correlation. Correlation here is a simple relation between two probabilities. If both probabilities are constant the correlation stays constant.

A: 1 1 1 1 1 1 1 1 1 1...
B: 0 0 0 0 0 0 0 0 0 0...

These two sequences represent two probabilities: 100% and 0%, how do you calculate correlation between them?
 
  • #98
Jabbu said:
I was talking about only one polarizer. Detector readings are recorded separately for each polarizer and streams of data, when theta = 0 and correlation = 100%, look like this:

A: 1 1 1 1 1 1 1 1 1 1...
B: 1 1 1 1 1 1 1 1 1 1...

Can angle between photons A polarization and polarizer A be anything else but zero degrees?

Those are not realistic runs for EPR. As I said, in the photon version of EPR, both Alice and Bob get 50% transmission rates. So a more likely run would look like:


For [itex]\theta_A - \theta_B = 0[/itex]:

A: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1
B: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1

(They agree 100% of the time)

For [itex]\theta_A - \theta_B = 45^o[/itex]:

A: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1
B: 0 0 0 1 1 0 1 1 0 1 1 1 1 1 0 0 0 0 1 0

(They agree 50% of the time)
 
  • #99
Jabbu said:
If photons always had 50% chance it would always yield the same correlation. Correlation here is a simple relation between two probabilities.

No, what I've been talking about is the probability that Alice and Bob get the same result (either 0 or 1). For the runs that you gave:

A: 1 1 1 1 1 1 1 1 1 1...
B: 0 0 0 0 0 0 0 0 0 0...

That number would be 0. The quantum prediction is [itex]cos^2(\theta_A - \theta_B)[/itex]
 
  • #100
stevendaryl said:
No, it does not say that. On the previous page, it says:

But when light polarization is constant those angles are still relative to light polarization even if you change them randomly and the result is the same, the meaning stays the same.
 
  • #101
Jabbu said:
But when light polarization is constant those angles are still relative to light polarization even if you change them randomly and the result is the same, the meaning stays the same.

It doesn't make any sense to assume that the light polarization is constant. That's because no matter what angle is chosen for [itex]\theta_1[/itex], only 50% of the photons are transmitted, and 50% are blocked. If the polarization were constant, then there would be some angle that would produce 100% transmission.
 
  • #102
stevendaryl said:
Those are not realistic runs for EPR. As I said, in the photon version of EPR, both Alice and Bob get 50% transmission rates. So a more likely run would look like:


For [itex]\theta_A - \theta_B = 0[/itex]:

A: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1
B: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1

(They agree 100% of the time)

For [itex]\theta_A - \theta_B = 45^o[/itex]:

A: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1
B: 0 0 0 1 1 0 1 1 0 1 1 1 1 1 0 0 0 0 1 0

(They agree 50% of the time)

So that's where we disagree, very subtle difference. How do you calculate correlation? Sequence length is 20, there is 10 matching pairs of ones and 10 matching pairs of zeros, how do you get 100% out of that?
 
  • #103
Jabbu said:
So that's where we disagree, very subtle difference. How do you calculate correlation? Sequence length is 20, there is 10 matching pairs of ones and 10 matching pairs of zeros, how do you get 100% out of that?

That's 50%. That's what I said. Once again:

Case 1: [itex]\theta_A - \theta_B = 0^o[/itex]

A: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1
B: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1

That's 100% agreement.

Case 2: [itex]\theta_A - \theta_B = 45^o[/itex]

A: 0 0 1 0 1 1 1 1 1 0 0 1 0 1 0 0 0 1 0 1
B: 0 0 0 1 1 0 1 1 0 1 1 1 1 1 0 0 0 0 1 0

That's 50% agreement.
 
  • #104
stevendaryl said:
I think I may have gotten a detail wrong in the two-photon EPR case. Or maybe you did. What I thought was that the two photons had the SAME polarizations. rather than polarizations that differ by 90 degrees.

As Cthugha says, it is dependent on the type.

Type I: The entangled pairs are of the same polarization. It takes 2 crystals oriented perpendicular to get the desired effect.

Type II: The entangled pairs are of the orthogonal (opposite) polarization. Only 1 crystal is needed for this.

(I get this backwards all the time.)
 
  • #105
stevendaryl said:
Now you're getting to what's strange about EPR. It seems as if Bob's result depends on Alice's filter setting.

If there is no any information about photons in that equation then the equation doesn't know whether photons are entangled or not, would it not make the same prediction?
 

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