Minimizing spatial hole burning

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Discussion Overview

The discussion centers on minimizing spatial hole burning in a linear laser cavity filled with a gain medium. Participants explore the implications of using birefringent materials and polarization changes within the cavity, examining theoretical approaches and potential devices for achieving this goal.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Niles proposes that changing the polarization of the intracavity field could minimize spatial hole burning due to the differing optical path lengths for P- and S-polarized beams.
  • Another participant questions whether points A and B are inside the cavity and suggests that a quarter waveplate could be used to achieve the desired polarization changes, referencing a technique proposed by Siegman.
  • Niles expresses skepticism about the effectiveness of the quarter waveplate, arguing that it would result in a complete phase shift, returning the polarization to its original state after reflection.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the effectiveness of the proposed methods for minimizing spatial hole burning, with differing views on the practicality and implications of using quarter waveplates and the nature of the cavity.

Contextual Notes

There are unresolved assumptions regarding the design and functionality of the proposed devices, as well as the implications of polarization changes on the standing wave patterns within the cavity.

Niles
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Hi

Say I am looking at a linear laser cavity consisting of a gain medium filling the *entire* cavity, please refer to the attached picture. The cavity will have standing waves in it, which will result in spatial hole burning of the gain medium at the antinodes of the optical field.

Say the intracavity field starts out by being P-polarized at point A. Then it propagates to point B, where I put a device that changes the polarization to S. Then it propagates back to point where, where a device makes it P-polarized again, etc..

Assuming the gain-medium is birefringent, this should in principle minimize spatial hole burning, right? Because the optical path length of P- and S-polarized beams are different, so the standing-wave pattern would also change as well?


Niles.
 
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Interesting thought.. Do you consider the points A and B to be inside the cavity as well? (By the way, I don't see any picture attached.)
Any thoughts about how such a "device" would look like?
Normally you'd use a Halfwaveplate to rotate polarization. This will, however, not work in your case. But a quartewaveplate could do the trick.
The latter has been proposed by Siegman, named twisted-mode-technique, see Applied Optics, Vol. 4, Issue 1, pp. 142-143 (1965) It works in the inverse way as you suggested: The polarization within the gain medium will be circular.

I also think that with your suggestion you will implicitely create a ring-cavity (there won't be any standing waves at all because p- and s-polarizations won't interfere).
 
I forgot the attachment, thanks to berkeman for letting me know. In principle the gain medium should fill the whole cavity.


Niles.
 

Attachments

  • cavity.PNG
    cavity.PNG
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Thanks. I haven't thought much about how I would do it in practice, I just thoight of the theory. But you say quarter waveplates? I don't see how that could work. So first time it passes through and becomes circular, then changes direction when reflection of the mirror, and then it gets a 90 degree phase shift again, which is a total of 360 degrees. So we just end up with the same as initially?
 

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