- #1
danja347
- 22
- 0
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
[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