Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
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2.2. The thermal component 15<br />
Figure 2.1: Panel (a): Chandra observation of the massive (regular) cluster of galaxies A 1689<br />
(blue) superimposed on the optical image (yellow, Hubble Space Telescope). Panel (b): fitting of<br />
the surface brightness profile with a doubleβ model described in the inset. Taken from Xue & Wu<br />
(2002).<br />
gas temperatures increasing with the size and the mass of the environment. Typical temperatures<br />
for clusters, groups and in<strong>di</strong>vidual galaxies are given in Table 2.1.<br />
2.2.2 Morphology of the X-ray emitting gas<br />
Imaging of the X-ray emission from massive ellipticals, groups and clusters of galaxies has shown<br />
that the morphologies of the emitting gas are quite heterogeneous, but that they can be related to<br />
the dynamical state of the systems. Much of work has been carried out for galaxy clusters, but the<br />
conclusions can be extended to sparser environments such as groups of galaxies and field galaxies,<br />
which can be regarded as scaled-down version of rich clusters.<br />
Forman & Jones (1982) first proposed a classification into “regular” and “irregular” X-ray cluster<br />
morphologies, with a connection to the evolutionary state.<br />
Essentially, regular clusters are those which show approximately round, centrally condensed<br />
X-ray brightness <strong>di</strong>stributions, decreasing smoothly outwards. Their temperatures and X-ray<br />
luminosities are usually high and they often host a central dominant galaxy. Galaxy clusters<br />
belonging to this class are thought to be evolved systems which have undergone dynamical<br />
relaxation.<br />
When the X-ray emission can be approximated as regular, its surface brightness profile is well<br />
parametrized by the function:<br />
] −3β+1/2<br />
S (r)=S (0)<br />
[1+ r2<br />
(2.2)<br />
15<br />
r 2 c