Annu. Rev. Astron. Astrophys. 1984. 22: 157-184
Copyright © 1984 by . All rights reserved

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2. BASIC RESULTS

2.1. The Nature of Redshift

The standard theory assumes that electromagnetic radiation ("light" for short) travels on null geodesics (xa(lambda) : ka; bkb = 0, kaka = 0, where ka ident dxa / dlambda) in the space-time of general relativity and is characterized by the relations c = vlambda, E = hnu, relating the wavelength lambda, frequency nu, speed c, and energy E of a photon. Then the redshift z ident Deltalambda / lambda (where Deltalambda is the change in wavelength measured from spectra for light emitted at wavelength lambda) is a direct consequence of measurable time dilation between the source and the observer (25, 91, 111). There can be various sources for this time dilation.

In the cosmological context, there is assumed to be a well-defined average motion of matter at each point in the Universe, representing the "standard" motion of matter there (24, 25); galaxies moving in this standard way, characterized by a four-velocity ua (where ua ua = - 1), are called "fundamental particles," and an observer moving with four-velocity ua is denoted as a "fundamental observer." The cosmological redshift zc is the redshift observed when both the source and observer move with this velocity (at their respective space-time positions) and there are no local gravitational redshift effects. However, there will be local Doppler redshifts zDs, zDo if the source or observer is not moving at the standard velocity, and there may be local gravitational redshifts zGs, zGo generated at the source or the observer by local gravitational potential wells. (Notice that in each case the effect could be a blueshift rather than redshift; this corresponds to a negative value of z, and we shall assume this possibility without explicitly mentioning it.) These contributions to the total redshift z are not distinguishable from each other by any direct measurement of the received radiation; the measurable quantity is the total redshift z, given in terms of the other quantities by

Equation 1 (1)

The cosmological redshift depends on the path of the light ray from the source to the observer. One can distinguish two contributions. The first arises from the increase in relative distance of fundamental observers due to integrated local relative motion of matter [characterized by the expansion tensor thetaab = hac hbau(c; d) (24, 25), where hab ident gab + uaub projects into the rest-space orthogonal to ua]. The second arises from the noninertial motion of the fundamental observers, characterized by a nonzero acceleration vector udota ident ua; b ub (indicating that their world-lines are nongeodesic). The change of redshift when moving a distance dl, measured by a fundamental observer along a null geodesic in direction ea = hba kb / (uckc), obeys the equation (24, 25)

Equation 2a (2a)

Thus one can write

Equation 2b (2b)

where zEc is the usual Hubble (expansion) term (obtained by integrating the first term in Equation 2a), and zGc is what might be termed a "cosmological gravitational redshift" (obtained by integrating the second term).

In the FLRW models, it is assumed that the other redshift contributions are very small compared with the basic cosmological expansion effect. Then

Equation 3 (3)

where R(t) is the "radius function" of the Universe that represents the time behavior of the distance between any pair of fundamental particles as the Universe evolves (by the homogeneity and isotropy of these models, the distances between all pairs of fundamental particles scale in the same way); and te, t0 are the times of emission and observation of the light, respectively. The observation of systematic redshifts indicates that the Universe is expanding at the present time t0; so H0 ident (R -1 dR / dt)|0 > 0.

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