B2.20

Electrodynamics | Part II, 2003

A plane electromagnetic wave of frequency ω\omega and wavevector k\mathbf{k} has an electromagnetic potential given by

Aa=Aϵaei(kxωt)A^{a}=A \epsilon^{a} e^{i(\mathbf{k} \cdot \mathbf{x}-\omega t)}

where AA is the amplitude of the wave and ϵa\epsilon^{a} is the polarization vector. Explain carefully why there are two independent polarization states for such a wave, and why k2=ω2|\mathbf{k}|^{2}=\omega^{2}.

A wave travels in the positive zz-direction with polarization vector ϵa=(0,1,i,0)\epsilon^{a}=(0,1, i, 0). It is incident at z=0z=0 on a plane surface which conducts perfectly in the xx-direction, but not at all in the yy-direction. Find an expression for the electromagnetic potential of the radiation that is reflected from this surface.

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