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and Cosmology

Extragalactic Astronomy and Cosmology: An Introduction

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2.6 The Galactic Center<br />

83<br />

Fig. 2.38. Determination of the mass M(r) within a radius r<br />

from Sgr A ∗ , as measured by the radial velocities <strong>and</strong> proper<br />

motions of stars in the central cluster. Mass estimates obtained<br />

from individual stars (S14, S2, S12) are given by the points<br />

with error bars for small r. The other data points were derived<br />

from the kinematic analysis of the observed proper motions<br />

of the stars, where different methods have been applied. As<br />

can be seen, these methods produce results that are mutually<br />

compatible, so that the mass profile plotted here can be<br />

regarded to be robust. The solid curve is the best-fit model,<br />

representing a point mass of 2.9 × 10 6 M ⊙ plus a star cluster<br />

with a central density of 3.6 × 10 6 M ⊙ /pc 3 (the mass profile<br />

of this star cluster is indicated by the dash-dotted curve). The<br />

dashed curve shows the mass profile of a hypothetical cluster<br />

with a very steep profile, n ∝ r −5 , <strong>and</strong> a central density of<br />

2.2 × 10 17 M ⊙ pc −3<br />

the same modulation time-scale. Observing the Galactic<br />

center simultaneously in the NIR <strong>and</strong> the X-rays<br />

revealed a clear correlation of the corresponding light<br />

curves; for example, simultaneous flares were found in<br />

these two wavelength regimes. These flares have similar<br />

light profiles, indicating a similar origin of their<br />

radiation. The consequences of these observations for<br />

the nature of the central black hole will be discussed<br />

in Sect. 5.4.6, after we have introduced the concept of<br />

black holes in a bit more detail. Flares were also observed<br />

at mm-wavelengths; their time-scale appears to<br />

be longer than that at higher frequencies, as expected<br />

if the emission comes from a more extended source<br />

component.<br />

2.6.5 The Proper Motion of Sgr A ∗<br />

From a series of VLBI observations of the position of<br />

Sgr A ∗ , covering eight years, the proper motion of this<br />

compact radio source was measured with very high precision.<br />

To do this, the position of Sgr A ∗ was determined<br />

relative to two compact extragalactic radio sources. Due<br />

to their large distances these are not expected to show

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