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Astron. Astrophys. 363, 415-424 (2000)

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Appendix A: structure integral for the y parameter

The structure integral for the SZ effect is given by the expression

[EQUATION]

where [FORMULA] is the density profile of the electrons, [FORMULA] the central density of the cluster and l the maximum extension of the hot gas on the line of sight [FORMULA], in units of the core radius [FORMULA]. With an ellipsoidal density profile, we obtain

[EQUATION]

where [FORMULA] and l are given in units of the core radius [FORMULA]. With the definition of a function G and transforming the variable of integration from [FORMULA] to [FORMULA] such that

[EQUATION]

we obtain after some algebra the structure integral

[EQUATION]

Finally, with a last change of variable,

[EQUATION]

we get

[EQUATION]

with

[EQUATION]

The structure integral turns out to be

[EQUATION]

where we introduced the Beta and the incomplete Beta functions defined by

[EQUATION]

and

[EQUATION]

with the Gamma and the incomplete Gamma-functions [FORMULA] and [FORMULA], respectively.

[FORMULA]-ray surface brightness

The structure integral for the X-ray surface brightness is given by

[EQUATION]

With the same transformations, as given above, we get

[EQUATION]

Appendix B: projection effects on the [FORMULA] parameter

The rotation in the ([FORMULA])-plane around [FORMULA] with an angle [FORMULA] leads to the density profile:

[EQUATION]

The rotation angle [FORMULA] is the angle between the major half axis of the rotated ellipse in the [FORMULA] plane and the [FORMULA]-axis. The line of sight is taken to be along the [FORMULA]-axis.

To investigate the projection effects we will compare a rotated cluster with respect to the [FORMULA] axis with its projection on the ([FORMULA]) 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]

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]

with

[EQUATION]

and

[EQUATION]

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]

where [FORMULA] is the maximum value that we get along the [FORMULA] axis in units of [FORMULA]

[EQUATION]

Moreover, [FORMULA] and [FORMULA].

The projected structure integral for the y parameter turns out to be

[EQUATION]

with

[EQUATION]

[FORMULA]-ray surface brightness

For the structure integral of the X-ray surface brightness we find in the case of the rotated cluster

[EQUATION]

and for the projected case

[EQUATION]

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© European Southern Observatory (ESO) 2000

Online publication: December 11, 2000
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