@sol invictus:
What you are saying is not correct. Light does NOT redshift in de Sutter any more often than it blue shifts. The simplest way I can think of to show that to you is to point out that the expanding flat FRW coords, in which a(t) is a growing exponential, are no better than the contracting flat FRW coords, where a(t) is a decreasing exponential. But in those contracting coords, the same incorrect logic you are employing would indicate that all light blueshifts.
We need to be clear about the distinction between a spacetime and a coordinate
system. A spacetime admits any number of coordinate systems. Two different spacetimes are distinguished over some domain by the fact of not being coverable by the
same coordiante system.
Schwarzschild is a spacetime.
'Conformal' can refer either to a class of spacetimes coverable by a (set of) coordinate systems, or to the coordinate systems themselves.
De Sitter is a spacetime.
De Sitter can be written in conformal form, and therefore belongs to the class of conformal spacetimes, even if it is not written in conformal form (but in static or Rw form say).
The point of my original post is that in general one cannot say whether or not light red-shifts, blue-shifts or does neither without stating a
coordinate system (not a spacetime), which statement thereof is not physics. More specifically, there is no physical meaning to the statement that light red-shifts in de Sitter
spacetime, since red-shift depends on the coordinate system, which is not specified just by naming the spacetime.
Expressed in conformal coordinates plane waves do not change their wavelength or frequency in any of the RW spacetimes, including de Sitter spacetime.
In de Sitter spacetime expressed in RW coordinates (to use a shorthand) light red-shifts as it propagates due to the expansion of space due to the scale factor a(t) in the metric.
In de Sitter spacetime expressed in static de Sitter coordinates light red-shifts as it propagates due to a distant-dependent radial term in the metric.
Perhaps an even simpler way to say it is just that since there is a time translation invariance (which follows from the existence of a static coord system) there cannot be a preferred direction of time, or any preference for red over blueshifts.
The effect of the static de Sitter metric on erstwhile Minkowski spacetime plane waves (if you will) is not due to the present of an expanding scale factor, for of course there is none here. But this is not the only means by which a red-shift can occur. In this case the red-shift (or blue shift in anti-de Sitter) arises because the metric has a
spatial part - which, BTW, is not space-translation-invariant.
It is enough to know that the phase factor changes as
i*k*r -> i*g(r)_{ab}*k^{a}*r^{b}
We can write this as
i*k*r -> i*k'(r)_{a}*r^{a}
where now we have a pseudo-Minkowski 4-vector (with metric g = diag(1,-1,-1,-1)) k'(r):
k'(r)_{a} = g(r)_{ab}*k^{b}
that is a function of distance. That is, frequencies and wavelengths are continuously changing as the wave propagates.
(Actually, there is a metric-induced change in the potential amplitude also, but this is hardly likely to undo the red-shift induced in the phase factor.)