Author: D.E. Ruiz
Abstract: Even diffraction aside, the well-known
equations of geometrical optics (GO) are not entirely
accurate. Traditional GO treats wave rays
as classical particles, which are completely described
by their coordinates and momenta, but rays have another
degree of freedom, namely, polarization. The polarization
degree of freedom manifests itself as an effective (classical)
spin that can be assigned to rays and can affect the wave
dynamics accordingly. A well-known example of
associated effects is wave-mode conversion, which can be
interpreted as spin precession. However, there are also other,
less-known manifestations of the wave spin, such as
polarization-driven bending of ray trajectories. This
work presents an extension and
reformulation of GO as a first-principle
Lagrangian theory, whose effective-gauge Hamiltonian
governs all the aforementioned polarization phenomena
simultaneously. As an example, the theory is
applied to describe the polarization-driven
divergence of right-hand and left-hand circularly polarized
electromagnetic waves in weakly magnetized plasma.
Submitted to: Physics of Plasmas
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