High symmetry points and lines in Brillioun Zone

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SUMMARY

The discussion focuses on high symmetry points and lines within the Brillouin Zone (BZ) in solid state physics. Participants emphasize the importance of group theory in understanding crystallographic symmetries, referencing Kittel's book and Tinkham's "Group Theory in Quantum Mechanics" as essential resources. Key symmetry points such as Gamma, X, L, K, U, W, and lines like Sigma, Lambda, and Delta are highlighted for their significance in solid state spectroscopic experiments. Understanding these concepts is crucial for interpreting phenomena like x-ray diffraction and electron paramagnetic resonance (EPR).

PREREQUISITES
  • Basic understanding of solid state physics concepts
  • Familiarity with Kittel's "Introduction to Solid State Physics"
  • Knowledge of group theory as it applies to crystallographic symmetries
  • Basic quantum mechanics principles
NEXT STEPS
  • Study Tinkham's "Group Theory in Quantum Mechanics" for crystallographic symmetry
  • Learn about the significance of symmetry operations in solid state physics
  • Research the application of high symmetry points in solid state spectroscopic techniques
  • Explore the mathematical framework of point groups and their representations
USEFUL FOR

Students and researchers in solid state physics, particularly those interested in crystallography, group theory, and spectroscopic analysis.

Log
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Hi,

I've seen pictures like this one: http://www.lcst-cn.org/Solid%20State%20Physics/Ch25.files/image002.gif
Is there any good explanation somewhere on this subject?

I'm using Kittel's book but there's nothing in there on this.
 
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Log said:
Is there any good explanation somewhere on this subject?

I'm using Kittel's book but there's nothing in there on this.

What explanation exactly do you need? An explanation on what a Brillouin zone is?

Zz.
 
I know that a Brillioun Zone is a Wigner Seitz cell in k-space, but what are the symmetry points and lines?

How are these used and what physical significance do they have?

How are they chosen?

I've read the first 6 chapters in Kittel. I don't think we're required to know this in the course I'm taking, just asking out of curiosity. :)
 
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You need to study a little group theory as it applies to crystallographic symmetries. It is surprisingly easy to understand. I leaned it from the book by Micheal Tinkham "Group Theory in Quantum Mechanics". Basically, the geometric structure of the Wigner Seitz cell is subsumed to an irreducible representation of the geometry by the symmetry group operators of rotation, reflection, and inversion.

This technique is fundamental to the interpretation of almost all solid state spectroscopic experiments (i.e. x-ray diffraction, EPR etc).
 
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I have been thinking about buying that book actually, it seems quite interesting. How much mathematics and QM is required to understand it?

I have Ashcroft as well. There's a section on point groups and such but the notation is different, is this the same thing as high symmetry points? I didn't bother reading it yet as the subject seemed to be different. I bought the book as a supplement but haven't been using it that much.

My understanding is only basic so far. I know some basic QM and I'm studying Kittel.
 
The first four chapters or so of Tinkham are related to crystallographic symmetry groups. The math is not hard at all. If you can do the problems in Kittel, you can work through Tinkham. I suggest you read the first few chapters and try to work the problems. The time spent studying group theory will be enormously beneficial to your understanding of solid state physics.
 
Look at the point group of the crystal.

Then pick a point within the BZ, e.g. one of the special points (Gamma, X, L, K, U, W) or along one of the special lines (Sigma, Lambda, Delta), or any other point.

Then figure out which of the symmetry operations of the point group project that point onto itself (or itself+reciprocal lattice vector).

What do you get?
 

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