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Interpolating between the Bose-Einstein and the Fermi-Dirac distributions in odd dimensions
We consider the response of a uniformly accelerated monopole detector that is
coupled to a superposition of an odd and an even power of a quantized, massless
scalar field in flat spacetime in arbitrary dimensions. We show that, when the
field is assumed to be in the Minkowski vacuum, the response of the detector is
characterized by a Bose-Einstein factor in even spacetime dimensions, whereas a
Bose-Einstein as well as a Fermi-Dirac factor appear in the detector response
when the dimension of spacetime is odd. Moreover, we find that, it is possible
to interpolate between the Bose-Einstein and the Fermi-Dirac distributions in
odd spacetime dimensions by suitably adjusting the relative strengths of the
detector's coupling to the odd and the even powers of the scalar field. We
point out that the response of the detector is always thermal and we, finally,
close by stressing the apparent nature of the appearance of the Fermi-Dirac
factor in the detector response.Comment: RevTeX, 7 page
Quasiparticle relaxation rate and shear viscosity of superfluid 3He-A_1 at low temperatures
Quasiparticle relaxation rate,, and the shear viscosity tensor
of the A_1-phase of superfluid 3He are calculated at low temperatures and
melting pressure, by using Boltzmann equation approach in momentum space. The
collision integral is written in terms of inscattering and outscattering
collision integrals. The interaction between normal and Bogoliubov
quasiparticles is considered in calculating transition probabilities in the
binary, decay and coalescence processes. We obtain that both
and are proportional to
>. The shear viscosities , and are
proportional to . The constant of proportionality of the shear
viscosity tensor is in nearly good agreement with the experimental results of
Roobol et al., and our exact theoretical calculation.Comment: 8 pages, some typos were correcte
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