Bloch Functions: Explaining the Bloch-Floquet Theorem

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Discussion Overview

The discussion revolves around the Bloch-Floquet theorem, particularly its application in the context of periodic dielectric crystals and its implications for wave propagation. Participants explore the origins of the theorem, its conditions for application, and seek resources for further reading.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Homework-related

Main Points Raised

  • One participant presents a mathematical formulation related to wave propagation in periodic dielectric crystals and seeks clarification on the Bloch-Floquet theorem.
  • Another participant suggests using online resources for additional information, providing a specific link as a reference.
  • It is proposed that the essence of the theorem is that solutions to periodic variations in refractive index must also be periodic, which is described as a logical conclusion.
  • A suggestion is made to consult specific textbooks, such as 'Solid State Physics' by Ashcroft & Mermin or Kittel, which contain derivations of Bloch's Theorem.
  • One participant offers an insight into Bloch's theorem, emphasizing the relationship between the probability of finding an electron in a periodic potential and the phase of the wave function, which varies with the lattice vector.
  • A participant expresses gratitude for the responses and indicates an improving understanding of the topic.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the explanations or applications of the Bloch-Floquet theorem, with multiple viewpoints and resources suggested. The discussion remains open-ended with various interpretations and insights shared.

Contextual Notes

Some assumptions about the periodicity and its implications for wave functions are discussed, but these remain unresolved and dependent on further clarification and definitions.

danja347
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For propagation in a periodic dielectric crystal i can by combining Maxwells equations under certain conditions get:

[tex] \bold{\nabla}\times{1\over\epsilon(\bold{x})}\bold{\nabla}\times\bold{H}=\left({\omega\over{c}}\right)^2\bold{H}[/tex]

I can apply Bloch-Floquet theorem and then draw a lot of conclusion.
Where does Bloch-Floquet theorem come from, when can I apply it and how can it be explained?
Please help or give references to where i can read about it.

Thanks!

/Daniel
 
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Why not try google.For example the first search resualt I got is:

http://www.elettra.trieste.it/experiments/beamlines/lilit/htdocs/people/luca/tesihtml/node7.html
 
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The essence of the theorem is, that any solution to a periodic variation in the refractive index, must itself be periodic (To me, this is a fairly logical conclusion).

There is a wealth of information about this theorem, as it is not only used in photonic crystals, but also to study bandgaps in metals and semi-conductors.

As for the google, I thought the 3rd one down was pretty good (A little more layman for those that don't have a large mathematics background).

Claude.
 
Also, if you have access to a library, find 'Solid State Physics' by Ashcroft & Mermin or Kittel. Both have derivations of Bloch's Theorem.
 
Here's an insight into Bloch's theorem that most texts do not mention:

The idea is that in a period potential, the probablilty of finding an electron at some location should be equal to the probability of finding the electron at all other places which are identical due to periodicity- and this makes sense. Here's the punchline - since the lwavefunctionl^2 gives the probability, this means that at all those places the wave function can differ only by a phase. The not so obvious thing is that this is not just any phase, but a phase whose argument is a function of the lattice vector.
 
Thank you all for you replies... I think I am getting a better and better understandning about how things work!

So, thanks again!

/Daniel
 

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