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The Boltzmann equation for the CMB describes the transport
of the photons under Thomson scattering by the electrons. The
radiation is described by the intensity matrix: the time
average of the electric field tensor Ei* Ej over a time
long compared to the frequency of the light or equivalently as the
components of the photon density matrix (see [19] for
reviews). For radiation
propagating radially , so that
the intensity matrix exists on the subspace. The matrix can further
be decomposed in terms of the Pauli matrices
and the unit matrix on this subspace.
For our purposes, it is convenient to describe the polarization
in temperature fluctuation units rather than intensity,
where the analogous matrix becomes,
| |
(34) |
is the
temperature perturbation summed
over polarization states. Since ,it is the difference in temperature fluctuations polarized in
the and directions.
Similarly is the difference along
axes rotated by 45, ,and that between .Q and U thus represent linearly polarized
light in the north/south-east/west and
northeast/southwest-northwest/southeast directions on the sphere
respectively. V represents circularly polarized light
(in this section only,
not to be confused with vector metric perturbations).
Under a counterclockwise rotation of the axes
through an angle the intensity transforms as
.
and V remain distinct
while Q and U transform into one another. Since the
Pauli matrices transform as a more convenient
description is
| |
(35) |
where recall that (see Eqn. 1),
so that transforms into itself under rotation.
Thus Eqn. (2) implies that should
be decomposed into spin harmonics [3,4].
Since circular polarization cannot be generated by
Thomson scattering alone, we shall hereafter ignore V. It is then
convenient to reexpress the matrix as a vector
| |
(36) |
The Boltzmann equation describes the evolution of the vector
under the Thomson collisional term and gravitational redshifts in a perturbed metric
| |
(37) |
where we have used the fact that and that
in a flat universe photons propagate in straight lines .We shall now evaluate the Thomson scattering and gravitational
redshift terms.
Next: Scattering Matrix
Up: Radiation Transport
Previous: Radiation Transport
Wayne Hu
9/9/1997