Polarized light - QM vs. classical?

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Discussion Overview

The discussion revolves around the behavior of polarized light as it passes through multiple polarizing filters. Participants explore the implications of this phenomenon from both classical and quantum mechanical perspectives, questioning how the arrangement and orientation of filters affect light transmission.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes the setup of three polarized filters and notes that light passes through more effectively when a diagonal filter is added between two perpendicular filters.
  • Another participant asks for clarification on the polarization state of light after passing through the diagonal filter.
  • A participant explains that the polarization direction can be represented as a vector, which can be decomposed into components that interact with the filters.
  • There is a discussion about the order of filters affecting the outcome, with a participant asserting that the polarization after the diagonal filter will be diagonal, allowing some light to pass through the final filter.
  • One participant expresses confusion about how adding a filter can lead to more light transmission, suggesting that the nature of polarizing filters is more complex than simply acting as light filters.
  • A thought experiment is proposed regarding the effect of adding multiple filters, hinting at the complexity of the situation.
  • Another participant explains the electromagnetic wave perspective, detailing how the electric field's orientation relates to polarization and how the intensity of light changes according to Malus's law.
  • One participant expresses disappointment at the realization that the phenomenon may not be a direct application of quantum mechanics.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and confusion regarding the classical explanation of polarized light and its behavior through filters. Some express uncertainty about the implications of quantum mechanics in this context, while others focus on the classical interpretations.

Contextual Notes

Participants acknowledge the complexity of how polarizing filters interact with light, with discussions hinting at unresolved assumptions about the nature of polarization and the effects of multiple filters.

Who May Find This Useful

This discussion may be of interest to those studying optics, electromagnetic theory, or the foundational concepts of quantum mechanics as they relate to light behavior.

DaveC426913
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Could someone 'splain this phenomenon?

I place two polarized filters (A and B) at right angles to each other so that the first filter passes light that's polarized vertically, while the second passes light that's polarized horizontally. No light gets all the way through. OK so far.

I now place a third polarized filter (C) between the first two. This one I angle so that it's diagonal (45 degrees from both A and B). Suddenly, some light gets through!

Obviously, the act of polarizing the light as it passes through the first filter is having an effect on its subsequent polarization.

Can someone explain what is happening?

I read somewhere that this is a clear demonstration of QM. Is there a classical explanation?
 
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let me ask you one question- what is the light polarization after filter C?
 
The direction of linear polarization (after A) can be defined by a single vector. This vector can be seen as the sum of two perpendicular vectors, of which only one goes through C. This remaining vector can then also be seen as a sum of two perpendicular vectors, only one of which goes through B.
 
Sorry, I was a little ambiguous in my diagram.

For purposes of discussion, light will pass through B *then* through A (left to right).
So that when C is added, light goes B > C > A. (In reality, it doesn't matter. It will work both ways BCA or ACB, but let's keep our numbers straight.)

So, what is the polarization after C? (i.e. en route from C to A).

Actually, I don't know. Well, I guess what's remaining will be diagonally polarized. So when it gets to A, some of it wil get through.

But perhaps I'm also not being clear about something else. There is MORE light coming through after passing through A+B+C than there was after passing through any two filters (A+B, A+C or B+C). How is that possible?


"The direction of linear polarization (after A) can be defined by a single vector. This vector can be seen as the sum of two perpendicular vectors, of which only one goes through C. This remaining vector can then also be seen as a sum of two perpendicular vectors, only one of which goes through B."

I see how that works (oddly enough), so I guess the problem is I don't understand how polarization actually manifests in light.
 
This confusion arises when polaroids are though of filters, because of the inevitable paradox that arises, i.e. if I add a filter, I get more light through. Polaroids are actually a little more complicated than that as they rotate the polarisation vector of the incident field.

As an interesting thought experiment, consider the situation where there are many polaroids in between A and B, (possibly an infinite number?).

Claude.
 
Claude Bile said:
As an interesting thought experiment, consider the situation where there are many polaroids in between A and B, (possibly an infinite number?).Claude.

Yes well, I'll leave that until afrter I understand the basic model with just 3, OK?

OK, so light passing through a polarizing filter does change the nature of the light?

This is not a QM effect then? It is merely classical physics?
 
If you think of the light as an electromagnetic wave, the orientation of its E field represents its polarization angle. The nature of an ordinary dichroic polarizer is to strongly absorb the E field in one direction, allowing the field perpendicular to that direction to pass through. The light that makes it through the polarizing "filter" has its field realigned with the polarization of the filter. Ignoring loss, if polarized light ([itex]E_0[/itex]) passes through a dichroic filter at an angle [itex]\theta[/itex], the transmitted beam is now polarized parallel to the orientation of the filter's axis and has a field strength of [itex]E_0 \cos\theta[/itex]. The intensity of the beam is reduced to [itex]I_0\cos^2\theta[/itex]--the law of Malus.

As Claude points out, it does seem kind of weird that adding a filter could increase the amount of light transmitted; but if you look at it step by step, it makes sense. Each filter reduces the intensity of the light passing through it, but that change in polarization angle makes all the difference.
 
OK cool.

And drat. I thought I was looking at a direct application of QM.
 

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