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Max Planck Institute for Astronomy - Annual Report 2007

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seems consistent with the present value. Only beyond<br />

z 1.7 are there indications that black holes were more<br />

massive than today relative to their galaxies in the early<br />

universe. Accordingly, the black holes would have first<br />

grown quickly – their galaxies building their masses only<br />

later and more slowly.<br />

However, because of selection effects, the uncertainties<br />

of this method are still so high that these results could<br />

possibly be insignificant. Further, methodically independent<br />

approaches are necessary in order to obtain a coherent<br />

picture at these and other redshifts. To achieve this,<br />

the MPIA astronomers have started among other things<br />

an observing program using the VLT and Si n F o n i (the<br />

near infrared integral field spectrograph with camera),<br />

<strong>for</strong> which they make use of MPIAʼs guaranteed observing<br />

time from building the pa r S e c laser guidance system<br />

HE1104–1805 Host galaxy Einstein Ring<br />

(after point source removal)<br />

A<br />

B<br />

lensing galaxy<br />

3<br />

III.2 In What Type of Galaxies Do Quasars III.X Live? Titel 77<br />

that supports Si n F o n i. The initial goal is to determine dynamic<br />

galaxy masses <strong>for</strong> four quasars, three of which are<br />

gravitationally lensed. Through Si n F o n i, extended line<br />

emission in the host galaxy is measured in order to derive<br />

the velocity field present there and thus dynamically<br />

determine the included masses. This method differs in<br />

principle from the above-described approach and is also<br />

complementary to the mass determinations based on the<br />

33 FOV<br />

Source plane velocity field Image plane velocity field<br />

Fig. III.2.8: The lense system HE1104-1805. Top left: the optical<br />

image (HST), top right: the image of the host galaxy after<br />

subtraction of the quasar core pulled apart near an Einstein<br />

ring, right bottom: a velocity field likely observed according<br />

to the lens model, and left bottom: the velocity field calculated<br />

back into the source plane.<br />

3 3<br />

3

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