Polarization and Bell measurments

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    Bell Polarization
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Discussion Overview

The discussion revolves around the behavior of polarized photons in relation to Bell test experiments, specifically addressing the implications of polarization alignment and the nature of entanglement. Participants explore the differences between photons passing through polarizers and the assumptions underlying Bell test measurements.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant questions the assumption that emitted pairs of photons must show a specific relationship in measurements when detectors are aligned, suggesting that mismatches can occur even with vertical polarization.
  • Another participant argues that if photons are known to be vertically polarized, they are no longer entangled, as they have already interacted with a vertical polarization filter.
  • A participant introduces notation to clarify the states of photons and their probabilities of passing through filters, emphasizing the role of superpositions in determining outcomes.
  • It is noted that in an EPR-type experiment, the pair of photons is in a superposition state that does not allow for mismatched outcomes, contrasting with the behavior of individual photons passing through filters.
  • There is a discussion about the implications of knowing or not knowing the polarization of photons and how this affects their interaction with filters.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between polarization, entanglement, and measurement outcomes. There is no consensus on whether emitted Bell test photons can mismatch at the detectors or the implications of known versus unknown polarization.

Contextual Notes

Participants reference various sources and concepts, including Dr. Chinese's statement on polarization alignment and Malus' law, but there are unresolved assumptions regarding the nature of entanglement and the conditions under which measurements are made.

bahamagreen
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There have been quite a few Bell threads lately, so I have been looking at them and various other sources. I'm missing something... any guidance appreciated.

Per Dr. Chinese's, "Once any photon passes through a polarizer lens, its polarization will be aligned exactly with the lens thereafter (even if it wasn't previously).".

Per Malus' and ubiquitous sites, of the photons passed through a vertical polarizer, some will pass a subsequent polarizer set to 45 degrees. I take this to mean that if a single vertically polarized photon may or may not pass a subsequent 45 degree filter, the same applies of any and all subsequent vertically polarized photons as well. So I am assuming that identically vertically polarized photons that encounter a 45 degree polarizing filter may or may not be passed; for example, of two subsequent such photons (I'll call them a "pair"), their passage or not though the filter does not have to match. If I assign all the possible pairs of a series, I will see some matching and some mismatching.

With respect to the simple Bell tests, this raises my question...

The question is, what is the difference between two vertically polarized photons going to a single 45 degree polarizing filter, and two photons identically emitted with vertical polarization, but going opposite directions to their respective but identically aligned 45 degree filters?

The Bell examples assume that the emitted pairs MUST show a specific and definite relationship between their measurements when the detectors are identically aligned, but two vertically polarized photons encountering a single 45 degree filter DO NOT have to be so... one may pass and the other may not, or vice versa, or both may pass, or neither.I'm not seeing why emitted Bell test photons can't mismatch at the detectors even if the detectors' filter alignments match (say both at 45 degrees) and the emitted pair are both polarized vertically. Why can't one pass and the other fail?
 
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bahamagreen said:
I'm not seeing why emitted Bell test photons can't mismatch at the detectors even if the detectors' filter alignments match (say both at 45 degrees) and the emitted pair are both polarized vertically. Why can't one pass and the other fail?

They can, if they are both polarized vertically. But if they are both known to be polarized vertically (or in any other directions for that matter), then they are no longer entangled, because they've already interacted with (been detected by) a vertical polarization filter.
 
bahamagreen said:
There have been quite a few Bell threads lately, so I have been looking at them and various other sources. I'm missing something... any guidance appreciated.

Per Dr. Chinese's, "Once any photon passes through a polarizer lens, its polarization will be aligned exactly with the lens thereafter (even if it wasn't previously).".

Per Malus' and ubiquitous sites, of the photons passed through a vertical polarizer, some will pass a subsequent polarizer set to 45 degrees. I take this to mean that if a single vertically polarized photon may or may not pass a subsequent 45 degree filter, the same applies of any and all subsequent vertically polarized photons as well. So I am assuming that identically vertically polarized photons that encounter a 45 degree polarizing filter may or may not be passed; for example, of two subsequent such photons (I'll call them a "pair"), their passage or not though the filter does not have to match. If I assign all the possible pairs of a series, I will see some matching and some mismatching.

With respect to the simple Bell tests, this raises my question...

The question is, what is the difference between two vertically polarized photons going to a single 45 degree polarizing filter, and two photons identically emitted with vertical polarization, but going opposite directions to their respective but identically aligned 45 degree filters?

The Bell examples assume that the emitted pairs MUST show a specific and definite relationship between their measurements when the detectors are identically aligned, but two vertically polarized photons encountering a single 45 degree filter DO NOT have to be so... one may pass and the other may not, or vice versa, or both may pass, or neither.

I'm not seeing why emitted Bell test photons can't mismatch at the detectors even if the detectors' filter alignments match (say both at 45 degrees) and the emitted pair are both polarized vertically. Why can't one pass and the other fail?

The difference is between
  • Each photon can be represented as a superposition of states.
  • The pair can be represented as a superposition of states.

Let me introduce a little bit of notation that I hope will clarify the situation.

  1. |D\rangle A photon in this state definitely passes a filter at 45 degrees, definitely does not pass a filter at 135 degrees.
  2. |\bar{D}\rangle A photon in this state definitely passes 135, definitely does not pass 45.

I didn't mention probabilities of passing (other than 0% and 100%), because the quantum-mechanical understanding of the probabilities is that they arise from superpositions. If you have a photon in the state

|\psi\rangle = \alpha |D\rangle + \beta |\bar{D}\rangle

then it will pass a 45 degree filter with probability |\alpha|^2, and will pass a 135 degree filter with probability |\beta|^2

A vertically polarized photon can be interpreted as a superposition of a 45 degree photon and a 135 degree photon:

|V\rangle = \frac{1}{\sqrt{2}}(|D\rangle + |\bar{D}\rangle)

(whether there is a + sign or a - sign or some other phase depends on how the various states are defined, but the above choice illustrates the point)

If I have a pair of vertically polarized photons, then they are described by the composite state:

|V\rangle |V\rangle = \frac{1}{2} |D\rangle |D\rangle + \frac{1}{2} |D\rangle |\bar{D}\rangle + \frac{1}{2} |\bar{D}\rangle |D\rangle + \frac{1}{2} |\bar{D}\rangle |\bar{D}\rangle

Squaring the coefficients tells us, since |\frac{1}{2}|^2 = \frac{1}{4}, that:
  1. There is a 25% probability that both photons will pass a 45 degree filter.
  2. There is a 25% probability that the first photon passes, but the second doesn't.
  3. There is a 25% probability that the second photon passes, but the first doesn't.
  4. There is a 25% probability that neither photon passes.

Now, in an EPR-type experiment, it's not that each photon is in a superposition, it's that the pair is in a superposition. The EPR state could be represented as:

\frac{1}{\sqrt{2}} (|D\rangle |D\rangle + |\bar{D}\rangle |\bar{D}\rangle)

In this state, there are no "crossed" states such as |D\rangle |\bar{D}\rangle or |\bar{D}\rangle |D\rangle. So there is 0% probability that one photon will pass the filter and the other will not.
 
Nugatory said:
They can, if they are both polarized vertically. But if they are both known to be polarized vertically (or in any other directions for that matter), then they are no longer entangled, because they've already interacted with (been detected by) a vertical polarization filter.

OK, but for the emitted pairs in the Bell tests isn't it assumed, thought, expected, or "known" that both will indicate the same polarity if a measurement is applied? Even if the particular polarization attribute is not known until a measurement, is it not the foundation of the experiment that both are the same polarity? Knowing that they are entangled implies this, right?

I'm not seeing the difference between two that have unknown but identical polarity, and two that have known identical polarity... in both cases the photons of each pair have the same polarity.

Simply knowing the polarity allowing the pair to interact with a filter differently, but not knowing the polarity making both of the pair interact with the filter identically... seems to suggest an attribute "known or unknown polarity"...

stevendaryl,

The notation is new to me, but I think I understand it.
What I don't understand is the last part...
You did not rule out that a superposition of two photons could be represented as the superposition of their composites.

Is that disallowed? That is,

\frac{1}{\sqrt{2}} (|V\rangle |V\rangle + |\bar{V}\rangle |\bar{V}\rangle)
 
Clearly, polarization entangled photons have different polarization than a pair vertically polarized. One pair's polarization is described by a single wave function. The other pair is described by 2 separate wave functions.

You might be interested in this: it is possible to create entangled photon pairs that are vertically (or horizontally) polarized. These pairs are NOT polarization entangled, but they are entangled as to momentum.

In fact, and somewhat counterintuitively, such pairs CAN be use to create polarization entangled pairs. This in commonly done as a matter of fact, by combining a stream of H> polarized pairs with a stream of V> polarized pairs. The trick is that they must be combined precisely so that it is not possible to determine whether the source was H> or V> polarized. See the following (great) reference, figure 2:

http://arxiv.org/abs/quant-ph/0205171
 
bahamagreen said:
You did not rule out that a superposition of two photons could be represented as the superposition of their composites.

Is that disallowed? That is,

\frac{1}{\sqrt{2}} (|V\rangle |V\rangle + |\bar{V}\rangle |\bar{V}\rangle)

The state \frac{1}{\sqrt{2}} (|V\rangle |V\rangle + |\bar{V}\rangle |\bar{V}\rangle) is a superposition of two mutually exclusive possibilities:

  1. Both photons are vertically polarized.
  2. Both photons are horizontally polarized (if you're using \bar{V} to mean horizontally polarized)

There is no possibility of one photon passing a vertical filter and the other photon passing a horizontal filter.

This is the state that would be produced if you generate a pair of entangled photons.

In contrast, the state \frac{1}{2} (|V\rangle |V\rangle + |\bar{V}\rangle |{V}\rangle + |V\rangle |\bar{V}\rangle + |\bar{V}\rangle |\bar{V}\rangle) is a superposition of four possibilities:

  1. Both photons are vertically polarized.
  2. The first is vertically polarized and the second is horizontally polarized.
  3. The first is horizontally polarized and the second is vertically polarized.
  4. Both are horizontally polarized.

For this state, there is a nonzero probability that one photon will pass a vertical filter, and the other will pass a horizontal filter.

This is the state that you would have if you generate two photons in the same single-particle state \frac{1}{\sqrt{2}} (|V\rangle + |\bar{V}\rangle

Being in the same state, initially, does not mean that the particles are entangle. Just the opposite; if each particle has a definite single-particle state, then the particles are NOT entangled. To be entangled means that the particles are not in definite single-particle states.

(One point of clarification: Mathematically, two particles are entangled if the composite state |\Psi\rangle CANNOT be represented as a product |\Psi\rangle = |\psi\rangle |\phi \rangle)
 

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