Lowell S. Brown
Plasmas may be created that contain different species which
are at different temperatures. This happens, for example,
when a plasma experiences a laser pulse which preferentially
heats the light electrons that have the larger scattering
cross section. The Coulomb interactions between the two
species brings them into equilibrium at a common temperature.
To compute the rate at which equilibrium is approached in a
dilute plasma , we exploit a novel technique employing
dimensional continuation that has been introduced recently.
The Boltzmann equation correctly describes the short-distance,
hard collision interactions for spatial dimensions ,
but it has a soft, long-distance, infrared divergence when
the spatial dimension
approaches 3 from above. The
Lenard-Balescu equation correctly describes the dynamically
screened, soft, long-distance interactions when
,
but it has a short-distance, hard, ultraviolet divergence
when
approaches 3 from below. As explained in detail
in previous work, as as reviewed here, the analytical
continuation of the sum of the rates computed from the
Boltzmann equation for
and from the Lenard-Balescu
equation for
yields the correct result for the
physical limit at
dimensions. We use this method to
compute the rate at which two species come into thermal
equilibrium for arbitrary mass ratios and for arbitrary
initial temperature ratios.
See [physics/9911056] for all the details.