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Annual Report 2011 Max Planck Institute for Astronomy

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30 II. Highlights<br />

II.3 In what Galaxies do Black Holes live in the Early Universe?<br />

Using state-of-the-art technology and sophisticated<br />

data analysis tools, a team from MPIA has developed a<br />

new and powerful technique to directly determine the<br />

mass of a galaxy hosting an active supermassive central<br />

black hole at a distance of nearly 9 billion light-years<br />

from Earth. This pioneering method promises a new<br />

approach <strong>for</strong> studying the co-evolution of galaxies and<br />

their central black holes, which typically relies on mass<br />

determinations.<br />

One of the most intriguing developments in astronomy<br />

over the last few decades is the realization that not only<br />

do most galaxies contain central black holes of gigantic<br />

size, but also that the mass of these central black holes<br />

are directly related to the mass of their host galaxies.<br />

These scaling relations with the black hole mass have<br />

been found to exist with the galaxy’s stellar or dynamical<br />

bulge mass, total luminosity and stellar velocity dispersion.<br />

It has recently been realized that these correlations<br />

are expected as a consequence of the current standard<br />

model of galaxy evolution, the so-called hierarchical<br />

model, as astronomers from MPIA have shown (Jahnke<br />

& Macciò <strong>2011</strong>, ApJ, 734, 92). In this standard model of<br />

galaxy <strong>for</strong>mation galaxies evolve and grow by ingesting<br />

smaller galaxies, or through mergers with galaxies of<br />

comparable size. As a a consequence of this hierarchical<br />

<strong>for</strong>mation, the individual relations between bulge and<br />

black hole mass are averaged out, creating a nearly universal<br />

ratio between the two properties in every galaxy.<br />

One of the most robust methods to study how galaxies<br />

and black holes evolve relative to each other is to trace<br />

these scaling relations through cosmic time. This can<br />

pixel<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

a<br />

–21.4<br />

log (F(Ha) / (W/m<br />

–21<br />

2 ))<br />

–20.6<br />

0.5<br />

10<br />

E<br />

20 30 40 50 60<br />

pixel<br />

N<br />

b<br />

0.5<br />

10<br />

L(Ha) [10 42 ]<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

–0.1<br />

620<br />

640 660 680 700 720<br />

Wavelength [nm]<br />

Fig. II.3.1: Spectrum around Hα <strong>for</strong> the quasar SDSS<br />

J090543.56+043347.3, centered on the active nucleus. From<br />

the combination of width (red arrow) and luminosity (integral<br />

above the zero level between the blue lines) of the Hα line<br />

the black hole mass can be inferred (Greene & Ho 2005,<br />

ApJ, 630, 122). The use of Hα <strong>for</strong> this purpose reduces the<br />

systematic uncertainties present in the prior estimates using<br />

the MgII line.<br />

Fig. II.3.2: SDSS J090543.56+043347.3: (a) Extracted emission<br />

line flux distribution, (b) Hα line width and (c) resulting<br />

velocity field, in all cases after removal of the bright nucleus,<br />

overlaid in contours.<br />

50<br />

Ha line width [km/s]<br />

110 170<br />

E<br />

20 30 40 50 60<br />

pixel<br />

N<br />

c<br />

V [km/s]<br />

–150 50<br />

0.5<br />

10<br />

E<br />

250<br />

20 30 40 50 60<br />

pixel<br />

N<br />

Credit: Katherine J. Inskip<br />

Credit: Katherine J. Inskip

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