In weak fields, the polarization plane of light in a Berry-dipole metal rocks as θ(z) ≈ θ0 cos(Ω z/λ), with Ω proportional to the light intensity.
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Non-linear Faraday Precession of Light Polarization in Time-Reversal Invariant Materials
In weak fields, the polarization plane of light in a Berry-dipole metal rocks as θ(z) ≈ θ0 cos(Ω z/λ), with Ω proportional to the light intensity.