24.07.2014 Views

pdf - SRON

pdf - SRON

pdf - SRON

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

CHAPTER 1: INTRODUCTION<br />

1.6.2 Space density of AGN<br />

As we have seen before, AGN can be detected at cosmological distances thanks<br />

to their large luminosity and hence they are of great interest to study the Universe<br />

at earlier epochs. However, all observations have a limiting flux for detection,<br />

such that an object with a flux below this limit cannot be distinguished<br />

from the background. The limiting luminosity for detection varies with distance<br />

so that we end up seeing different populations of AGN at different redshifts.<br />

The luminosity function enables us to represent what is observed in<br />

terms of different distances and luminosities, and is thus defined as the number<br />

of objects detected per unit comoving volume per unit luminosity. In general,<br />

the luminosity function will be a function of both luminosity and redshift. The<br />

comoving volume is the volume that a region of space would have if it were<br />

observed at the present epoch. Hence, the comoving volume is independent<br />

of the expansion of the Universe and therefore there is no density evolution of<br />

objects caused by this cosmological expansion.<br />

Evolution in the comoving space density or luminsity of AGN is seen as a<br />

change in the luminosity function. This can be described in different forms:<br />

• Pure Luminosity Evolution (PLE): In PLE, the number of AGN per unit<br />

comoving volume remains constant while the luminosity of each AGN<br />

evolves, at a rate that is the same for AGN of all luminosities. In the<br />

framework of a PLE model, the luminosity function retains its shape at all<br />

redshifts and depends only on the evolution law and the luminosity function<br />

at zero redshift. It has been a fairly succesful model for the evolution<br />

of AGN at radio ([56], [169], [198]), optical ([27], [26], [106], [107], [108],<br />

[205]) and X-ray ([51], [25], [118], [171]) wavelengths, although deviations<br />

from this model have been seen at high redshifts and overproductions of<br />

the X-ray background have been reported ([157], [224]).<br />

• Pure Density Evolution (PDE): In PDE, the number of AGN per unit comoving<br />

volume is assumed to evolve while the distribution of luminosities remains<br />

constant. This model has failed to fit the current observations well<br />

since it clearly overpredicts the measured cosmic X-ray background (e.g.<br />

[99], [157], [224]) and therefore has been ruled out as a possible description<br />

of the evolution of AGN.<br />

• Luminosity-dependent Density Evolution (LDDE): In LDDE, both the num-<br />

22

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!