Astron. Astrophys. 363, 415-424 (2000)
Appendix A: structure integral for the y parameter
The structure integral for the SZ effect is given by the
expression
![[EQUATION]](img209.gif)
where is the density profile of
the electrons, the central density of
the cluster and l the maximum extension of the hot gas on the
line of sight , in units of the core
radius . With an ellipsoidal density
profile, we obtain
![[EQUATION]](img211.gif)
where and l are given in
units of the core radius . With the
definition of a function G and transforming the variable of
integration from to
such that
![[EQUATION]](img214.gif)
we obtain after some algebra the structure integral
![[EQUATION]](img215.gif)
Finally, with a last change of variable,
![[EQUATION]](img216.gif)
we get
![[EQUATION]](img217.gif)
with
![[EQUATION]](img218.gif)
The structure integral turns out to be
![[EQUATION]](img219.gif)
where we introduced the Beta and the incomplete Beta functions
defined by
![[EQUATION]](img220.gif)
and
![[EQUATION]](img221.gif)
with the Gamma and the incomplete Gamma-functions
and
, respectively.
-ray surface brightness
The structure integral for the X-ray surface brightness is
given by
![[EQUATION]](img225.gif)
With the same transformations, as given above, we get
![[EQUATION]](img226.gif)
Appendix B: projection effects on the parameter
The rotation in the ( )-plane
around with an angle
leads to the density profile:
![[EQUATION]](img228.gif)
The rotation angle is the angle
between the major half axis of the rotated ellipse in the
plane and the
-axis. The line of sight is taken to
be along the -axis.
To investigate the projection effects we will compare a rotated
cluster with respect to the axis with
its projection on the ( ) plane,
corresponding to the sky plane. We assume an infinite extension and an
isothermal profile.
The rotated structure integral for the y parameter
turns out to be
![[EQUATION]](img230.gif)
After some algebra and with the same kind of variable changes as in
Appendix A, we get (assuming an infinite cluster extension for the
structure integral):
![[EQUATION]](img231.gif)
with
![[EQUATION]](img232.gif)
and
![[EQUATION]](img233.gif)
On the other hand, the projection of this cluster on the observed
sky plane in the infinite cluster extension case leads to the density
profile
![[EQUATION]](img234.gif)
where is the maximum value that
we get along the axis in units of
![[EQUATION]](img236.gif)
Moreover, and
.
The projected structure integral for the y parameter
turns out to be
![[EQUATION]](img239.gif)
with
![[EQUATION]](img240.gif)
-ray surface brightness
For the structure integral of the X-ray surface brightness
we find in the case of the rotated cluster
![[EQUATION]](img241.gif)
and for the projected case
![[EQUATION]](img242.gif)
© European Southern Observatory (ESO) 2000
Online publication: December 11, 2000
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