Polarization of light -- Determine the thickness of the crystal

Click For Summary
SUMMARY

The thickness of the crystal required to convert linearly polarized light to circularly polarized light is calculated using the formula d = λ/(4(n1 - n2)), resulting in a thickness of 856 nm. The incoming light, polarized at 45 degrees, can be treated as a combination of two eigen-polarizations due to birefringence. The key to achieving circular polarization lies in the phase difference accumulated by each component as it passes through the crystal. The problem specifically asks for the thickness that results in a 1/4 wave phase shift, which is the only necessary calculation.

PREREQUISITES
  • Understanding of birefringence in crystals
  • Knowledge of linear and circular polarization of light
  • Familiarity with phase differences in wave optics
  • Basic principles of Fresnel reflection and transmission
NEXT STEPS
  • Study the principles of birefringence in calcite crystals
  • Learn about the mathematical derivation of phase shifts in polarized light
  • Explore the differences between linear, circular, and elliptical polarization
  • Investigate the application of Fresnel equations in optical systems
USEFUL FOR

Optical physicists, students studying wave optics, and anyone interested in the properties of polarized light and its applications in crystal optics.

Karl Karlsson
Messages
104
Reaction score
12
Homework Statement
A double-breaking material can be used to convert linearly polarized light at right angles to circularly polarized. It is desired to utilize this to change the polarization of light at wavelength 589 nm. Calcite, or its full name, calcium carbonate (CaCO3) is an example of a double-breaking crystal. For the current wavelength, the refractive index is 1.658 for light polarized along the optical axis and 1.486 for light polarized perpendicular to the optical axis. The crystal is oriented so that the optical axis lies in the plane of the surface and the polarization direction of the incident linearly polarized light forms the angle 45 degrees towards the optical axis in the plane of the crystal. Determine the minimum thickness of the crystal required for outgoing light to be circularly polarized.
Relevant Equations
I assume Fresnel's formulas. Circularly polarized light in vector form:
(0, E*cos(kx - wt), E*cos(kx - wt +- pi/2)). Malus law (maybe)

Maybe (I don't know). Bragg condition for interference from an array (since it's a crystal, I don't know if that matters).
I don't even know where to start with this problem. What kind of slit makes linearly polarized light circularly polarized?

The correct answer is d = lambda/(4(n1 - n2)) = 856nm. But how do I get there?

Thanks in beforehand!
 
Physics news on Phys.org
The incoming light polarized at 45 degrees is halfway between the ordinary and extraordinary axes. You can treat it as a sum of two waves aligned along each of the axes. Now, how much phase does each part accumulate passing through a thickness t of the calcite?
 
Karl Karlsson said:
I don't even know where to start with this problem. What kind of slit makes linearly polarized light circularly polarized?
This is the key. Do you know what circularly polarised light is? How does it differ from linear polarized light, or unpolarized (randomly polarised) light.
 
Ooh, i must read wrong i thought i was some slit. Below is my attempt:
IMG_0594.jpeg

However the light is only elliptically polarized and not circular or maybe they meant elliptically polarized light
 
Karl Karlsson said:
However the light is only elliptically polarized and not circular or maybe they meant elliptically polarized light

The light entering is at 45 degrees to the optical axis. It can be treated as a sum of two components. The two components have the same amplitude (because 45 degrees). The two components are eigen-polarizations of the birefringence. The crystal will not convert one to the other. The only thing it can do is change the relative phases. Of course you can get circular polarization.

The only thing I understood on the page was your correct calculation of the thickness based on the path length difference to wind up 1/4 wave out of phase. That is all you need. That is all the problem asked for.

I have no idea what you did at the top. Down at the bottom I have no idea why you think one of the two electric fields needs to be divided by a square root of two. If that is you creating the two parts out of the original 45 degree amplitude, why is only one of them a square root of two smaller than the original?
 
I think your application of Fresnel reflection/transmission is inappropriate here. Since you have normal incidence, it will not discriminate between p and s waves - or IMO there are no p and s, since all polarizations are perpendicular to the surface.
As KK says, just work out the thickness for 1/4 wave difference, as you did. Nothing in the question requires anything more.
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 43 ·
2
Replies
43
Views
4K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 20 ·
Replies
20
Views
3K
Replies
12
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K