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Extragalactic Astronomy and Cosmology: An Introduction

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9. The Universe at High Redshift<br />

356<br />

nearly completely hidden to the optical eye because of<br />

strong dust absorption.<br />

In this chapter, we will attempt to provide an impression<br />

of astronomy of the distant Universe, <strong>and</strong> shed<br />

light on some interesting aspects that are of particular<br />

importance for our underst<strong>and</strong>ing of the evolution of<br />

the Universe. This field of research is currently developing<br />

very rapidly, so we will simply address some of the<br />

main topics in this field today. We begin in Sect. 9.1 with<br />

a discussion of methods to specifically search for highredshift<br />

galaxies, <strong>and</strong> we will then focus on a method by<br />

which galaxy redshifts can be determined solely from<br />

photometric information in several b<strong>and</strong>s (thus, from the<br />

color of these objects). This method can be applied to<br />

deep sky images observed by HST, <strong>and</strong> we will present<br />

some of the results of these HST surveys. Finally, we<br />

will emphasize the importance of gravitational lenses as<br />

“natural telescopes”, which, due to their magnification,<br />

provide us with a deeper view into the Universe.<br />

Gaining access to new wavelength domains paves<br />

the way for the discovery of new kinds of sources;<br />

in Sect. 9.2 we will present galaxy populations which<br />

have been identified by submillimeter <strong>and</strong> NIR observations,<br />

<strong>and</strong> whose relation to the other known types<br />

of galaxies is yet to be uncovered. In Sect. 9.3 we will<br />

show that, besides the CMB, background radiation also<br />

exists at other wavelengths, but whose nature is considerably<br />

different from that of the CMB. The question of<br />

when <strong>and</strong> by what processes the Universe was reionized<br />

will be discussed in Sect. 9.4. Then, in Sect. 9.5,<br />

we will focus on the history of cosmic star formation,<br />

<strong>and</strong> show that at redshift z 1 the Universe was much<br />

more active than it is today – in fact, most of the stars<br />

which are observed in the Universe today were already<br />

formed in the first half of cosmic history. This empirical<br />

discovery is one of the aspects that one attempts<br />

to explain in the framework of models of galaxy formation<br />

<strong>and</strong> evolution. In Sect. 9.6 we will highlight<br />

some aspects of these models <strong>and</strong> their link to observations.<br />

Finally, we will discuss the sources of gamma-ray<br />

bursts. These are explosive events which, for a very<br />

short time, appear brighter than all other sources of<br />

gamma rays on the sky put together. For about 25 years<br />

the nature of these sources was totally unknown; even<br />

their distance estimates were spread over at least seven<br />

orders of magnitude. Only since 1997 has it been<br />

known that these sources are of extragalactic origin.<br />

9.1 Galaxies at High Redshift<br />

In this section we will first consider the question of how<br />

distant galaxies can be found, <strong>and</strong> how to identify them<br />

as such. The properties of these high-redshift galaxies<br />

can then be compared with those of galaxies in the<br />

local Universe, which were described in Chap. 3. The<br />

question then arises as to whether galaxies at high z,<strong>and</strong><br />

thus in the early Universe, look like local galaxies, or<br />

whether their properties are completely different. One<br />

might, for instance, expect that the mass <strong>and</strong> luminosity<br />

of galaxies are evolving with redshift. Examining the<br />

galaxy population as a function of redshift, one can trace<br />

the history of global cosmic star formation <strong>and</strong> analyze<br />

when most of the stars visible today have formed, <strong>and</strong><br />

how the density of galaxies changes as a function of<br />

redshift. We will investigate some of these questions in<br />

this <strong>and</strong> the following sections.<br />

9.1.1 Lyman-Break Galaxies (LBGs)<br />

How to Find High-Redshift Galaxies? Until about<br />

1995 only a few galaxies with z > 1 had been known;<br />

most of them were radio galaxies discovered by optical<br />

identification of radio sources. The most distant<br />

normal galaxy with z > 2 then was the source of the<br />

giant luminous arc in the galaxy cluster Cl 2244−02<br />

(see Fig. 6.31). Very distant galaxies are faint, <strong>and</strong> so<br />

the question arises of how galaxies at high z can be<br />

detected at all.<br />

The most obvious answer to this question may perhaps<br />

be by spectroscopy of a sample of faint galaxies.<br />

This method is not feasible though, since galaxies with<br />

R 22 have redshifts z 0.5, <strong>and</strong> spectra of galaxies<br />

with R > 22 are only observable with 4-m telescopes<br />

<strong>and</strong> with a very large investment of observing time.<br />

Also, the problem of finding a needle in a haystack<br />

arises: most galaxies with R 24.5 have redshifts z 2<br />

(a fact that was not known before 1995), so how can<br />

we detect the small fraction of galaxies with larger<br />

redshifts?<br />

Narrow-B<strong>and</strong> Photometry. A more systematic method<br />

that has been applied is narrow-b<strong>and</strong> photometry. Since<br />

hydrogen is the most abundant element in the Universe,

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