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2.1. Distances of Extragalactic Objects

Our only means of obtaining information and therefore knowledge of the structure and dynamics of the Universe (on all different scales) are through the electromagnetic radiation that we receive. Therefore it is of primary importance to define a system of measuring luminosities taking also into account that the Universe expands and that light loses energy through a variety of processes.

If we assume that light propagates with no loss of energy, then the apparent luminosity of a source l, is related to its absolute luminosity L, by:

Equation 36 (36)

where r is the distance to the source. We can see the extreme importance of determining the pair (l, L), since such knowledge would provide the distance of the source, r.

Due to historical mostly reasons we use a logarithmic brightness system by which an object with a magnitude of 1 is 100 times brighter than an object with a magnitude 6. We have:

Equation 37 (37)

where m is the apparent magnitude and M the absolute one. Therefore, using (36) we have:

Equation 38 (38)

where c1,2 are constants which depend on the filter used and c3 is that value for which m = m at a distance of 10 parsecs (see section 2.3) from the Earth, and thus c3 = -5. In extragalactic astronomy, instead of pc, we use Mpc and therefore (38) becomes:

Equation 39 (39)

The above definitions are somewhat ideal, since in the real world we do not observe the total apparent magnitude, but that corresponding to the particular range of spectral frequencies, that our detector is sensitive to, and those allowed to pass through Earth's atmosphere. If we detect lnu over a range of frequencies (nu ± delta nu), then the observed apparent magnitude is m = -2.5 log10 integdeltanu lsub>nu dnu + c. However, neither the atmosphere nor the detectors have a sharp nu limit and therefore it is better to model these effects by a sensitivity mask Fnu, and the observed apparent magnitude is then:

Equation 40 (40)

If Fnu = 1 then the apparent (or absolute) magnitude of a source is called the bolometric magnitude.

How do the above definitions change by taking into account the fact that the Universe expands? To answer this we need a metric of space-time, which in our case is the Robertson-Walker metric. Since light travels along null-geodesics, a fundamental concept of distance can be defined by the corresponding light-travel time, which is called proper distance. If a light signal is emitted at a galaxy curlyG1 from the coordinate position (r1, theta0, phi0) at time t = 0 and received by an observer at curlyG0 at (r0, theta0, phi0), then these events are connected only by the light signal and since all observers must measure the same speed of light, it defines a very fundamental concept of distance. Obviously, it depends on the curvature of space, and since ds = 0 we have from (1):

Equation 41 (41)

In the expanding Universe framework, the expressions (36) and (38) change, to:

Equation 42 (42)

where dL ident dpro(1 + z) is the luminosity distance. It is obvious that the distance measure of an extragalactic object depends on the underlying Cosmology. A proper derivation of the luminosity distance (cf. [183], [112]) provides the following expression:

Equation 43 (43)

where Omega contains all the contributions (mass, energy density, curvature). Another important distance definition is that of the angular-diameter. It is based on the fact that a length l, subtends a smaller angle, theta, the further away it is (l propto 1 / theta) and it is given from: relation to:

Equation 44 (44)

Note that this notion of distance is used to derive the CMB power spectrum predictions of the different cosmological models (see section 3.1).

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