Several years after the SZE was first proposed
(Sunyaev &
Zel'dovich, 1972;
Sunyaev &
Zel'dovich, 1970)
it was recognized that the distance to a cluster could be
determined with a measure of its SZE and X-ray emission
(Birkinshaw,
1979;
Cavaliere et
al., 1977;
Cavaliere &
Fusco-Femiano, 1978;
Boynton &
Murray, 1978;
Gunn et al., 1978;
Silk & White,
1978).
The distance is determined by exploiting the
different density dependences of the SZE and X-ray emissions. The
SZE is proportional to the first power of the density;
TSZE
~
d
ne Te, where ne is
the electron density, Te
is the electron temperature, and
d
is along the
line-of-sight.
The distance dependence is made explicit with the substitution
d
= DA
d
,
where DA is the angular-diameter distance of the cluster.
The X-ray emission is proportional to the second power of the density;
Sx ~
d
ne2
eH,
where
eH is
the X-ray cooling function. The angular-diameter distance is solved for
by eliminating the electron density,
(3) yielding
![]() |
(6) |
where these quantities have been evaluated along the line of sight
through the center of the cluster (subscript 0) and
c refers
to a characteristic scale of the cluster along the line of sight,
whose exact meaning depends on the density model adopted. Only the
characteristic scale of the cluster in the plane of the sky is
measured, so one must relate the characteristic scales along the line of
sight
and in the plane of the sky. For detailed treatments of this calculation,
see Birkinshaw et
al. (1991)
and Reese et
al. (2002);
Reese et al. (2000).
Combined
with the redshift of the cluster and the geometry of the Universe, one
may determine the Hubble parameter, with the inverse dependences on
the observables as that of DA. With a sample of galaxy
clusters,
one fits the cluster distances versus redshift to the theoretical
angular-diameter distance relation, with the Hubble constant as the
normalization (see, e.g., Fig. 6).
![]() |
Figure 6. SZE-determined distances versus
redshift. The theoretical angular diameter distance relation is plotted
for three different cosmologies, assuming
H0 = 60 km s-1 Mpc-1:
|
3 Similarly, one could eliminate DA in favor of the central density, ne0. Back.