- #1
Herr Malus
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Homework Statement
We want to deduce the index of refraction for a plane electromagnetic wave propagating (along the z direction) in a plasma with an applied static, uniform magnetic field B=B 0 [tex]\widehat{z}[/tex]. Show that the index of refraction for right and left circularly polarised light satisfies: n 2 r,l=1-[tex]\omega2[/tex]/[[tex]\omega[/tex]([tex]\omega[/tex][tex]\pm[/tex][tex]\omegaB[/tex]
Where [tex]\omegaB[/tex] is the cyclotron frequency.
There then follow parts 2 and 3 regarding getting the dispersion relation and conductivity/suspceptibility and dielectric constant.
Homework Equations
Since this is a plasma, [tex]\omega0[/tex]=[tex]\gamma[/tex]=0
So we have m[tex]\partial2[/tex]x=q(E+vxB)
The Attempt at a Solution
So I took the equation for a right circular polarised E along with an x of the form x=x0e-i[tex]\omega[/tex]t, and placed it alongside the given B in the equation above. This basically gave me a whole mess of algebra to sort through, but I got down to:
r0=-[tex]\omega -2 [/tex]((qE0eikx/m-i[tex]\omega[/tex][tex]\omegaB[/tex]r0)[tex]\widehat{x}[/tex]+(qE 0 eikx/m+i [tex]\omega[/tex] [tex]\omegaB[/tex]r0)[tex]\widehat{y}[/tex])
I'm not even sure if this is the right direction and my class textbook, Griffiths, has a derivation which doesn't seem useful since it arrives at n through the relation between k and [tex]\omega[/tex]. Any help, or even a good source for the math behind plasma physics in this area would be greatly appreciated.
Cheers.