Polarization and crystallography

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Discussion Overview

The discussion revolves around the concepts of principal section and optic axis in the context of crystallography and optical properties of crystals. Participants explore the definitions and implications of these terms, particularly in relation to birefringence and the behavior of light in different crystal structures.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant asks for clarification on the principal section and optic axis of a crystal.
  • Another participant suggests that the optic axis for a biaxial crystal is the direction where the extraordinary refractive index equals the ordinary refractive index.
  • A different participant explains that in uniaxial crystals, the refractive index varies with polarization and can be represented by an ellipsoid, with the optic axis being the long axis of this ellipsoid.
  • This participant also describes how different propagation directions lead to different refractive indices for orthogonal polarization components, resulting in birefringence.
  • A link to an external resource is provided for further reading on the optic axis of a crystal.
  • Another external link is shared that defines the principal section as a plane passing through the optical axis of a crystal.
  • A participant expresses difficulty in understanding the explanations and requests more specificity.
  • Further clarification is provided regarding the relationship between wave propagation directions and the intersection with the ellipsoid, emphasizing that light traveling along the optic axis experiences a uniform refractive index.
  • One participant acknowledges understanding after the explanations provided.

Areas of Agreement / Disagreement

There is no explicit consensus reached among participants, as some express confusion and seek further clarification, while others provide technical explanations that may not be fully understood by all.

Contextual Notes

Participants note the necessity of understanding the mathematical representation of optical properties and the implications of different crystal structures on light propagation, indicating that some assumptions may not be fully articulated.

rahulmotan
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Can anyone explain what is principal section and optic axis of a crystal?
Any help wud be highly appreciated.
Thank You
 
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Off the top of my head, the optic axis is the direction (for a biaxial crystal) along which n_e = n_o. I'd have to look up the other one.
 
You will have to do a little reading to fully understand it if you haven't yet seen the tensor representation of crystal properties and optical properties in particular. But the essential point is that refractive index can vary for different polarizations in a material. For a uniaxial crystal, which is the most typical case, it turns out that you can represent the refractive index by drawing an ellipsoid with a=b =/= c if a,b,c are the three semimajor axes. Then if you draw a vector from the center to any point on the surface, that length will be inversely related to the value of the refractive index felt for a wave with polarization pointing in that direction. So, the optic axis of the material is the long axis of this ellipse, and if the wave is propagating along the optic axis, it will feel the same refractive index regardless of polarization. Therefore there is no birefringence experienced by the wave.

For any other direction of propagation, the refractive index will depend on the polarization state (draw a vector in the direction of propagation, and draw the ellipse normal to it which intersects the ellipsoid). In this case, two orthogonal polarization components will experience two refractive indices - called the ordinary and extraordinary index. If the wave impinges on the crystal at an angle, the different refractive indices will cause the two polarization components to refract at different angles, leading to two spatially separated beams, the visible manifestation of birefringence.

Again, you'll have to read through the math to see why the refractive index can be represented by this ellipse. It's not difficult but you just have to go through it.

So if one central intersection of the ellipsoid is a circle, the section orthogonal to that is the principal section. That's just terminology, I had to look that up as well. But the principal section will tell you the wave vector which experiences the most pronounced birefringence.
 
thank you for replying but it wud be better if u wud make it more specific...because i cudnt get evrything of wat u wrote...i found it tough to understand!:confused:
 
I_Indicatrix_uniaxial.jpg


Look at the picture on the right. The three arrows coming out of the ellipsoid are the propagation directions of three different waves. Each has a plane normal to the direction which intersects the ellipsoid, forming an ellipse (or circle). The polarization can lie anywhere in the plane of that ellipse. It's length is related to the refractive index. So you can see that the wave traveling straight up (ie, along the optic axis) has the same refractive index for all polarizations, since the intersection with the ellipsoid is a circle. Any other direction, the two perpendicular polarization components will experience a different refractive index.

I can't be more specific. Maybe I shouldn't be trying to explain the optical indicatrix to you, but if you want to understand it on this level you will have to read about it. The simplest answer is just that, traveling along the optic axis, light will travel at one speed. Travelling in any other direction, light will split into two beams with slightly different speeds.
 
thank u vry much got it...:D
 

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