The Wilkinson Microwave Anisotropy Probe WMAP team in 2003 released a full-sky map of the oldest light in the universe, extending to more detail the results obtained in 1992 by the COBE instrument. "Warmer" (red) and "cooler" (blue) spots enhance anisotropies in the low ppm range. The oval shape projection displays the whole sky. This microwave pattern is from 379,000 years after the Big Bang, over 13 billion years ago.

Looking to the bottom of time

If you can't imagine a four-dimensional space-time (can you? I can't), at least some cosmological facts may be envisioned by scaling down the problem to a lower level. Let's imagine we are living on the surface of a sphere without knowing it. That shouldn't be too difficult, since we did exactly that for many millenia. Now let's imagine a very distant view, and let's assume further that photons are allowed to travel only in the surface of the sphere. What would happen if we would peer into really very far? Of course you might expect that a very enduring photon should eventually travel around the whole "universe", and finally we should be able to see our own behind.
We have just overlooked one tiny detail in our nice thought experiment: We forgot that the photon takes some time for this journey. A whole lot of time. Such a long time that it is very unlikely that we would ever live to see our own behind. What would we see? Our world as it was 100 years ago? 1000 years ago? No chance. We wouldn't see anything of "our world". In reality, the Hubble Space Telescope looks back into space-time by more than 10 billion years, and it still doesn't see itself from behind. At that time, there was no mankind yet, there was no earth, there was no sun. Most likely, there wasn't even our Milky Way as we know it. But still it hasn't looked to the end of time.
What would we see if we looked to the end of time? Well, the COBE Differential Microwave Radiometer has done that, at least almost so (Partridge 1992). In 1964, Penzias & Wilson stumbled over a curious phenomenon, that earned them each a quarter of the physics Nobel Price in 1978. From all directions of the sky, a faint but remarkebly homogenous microwave radiation can be recorded, spectrally equivalent to the heat radiation from a black body with a temperature of exactly 2.728 ± 0.002 K (cited in Dodelson et al. 1996). The satellite-born COBE instrument screened the cosmic space in all directions and detected slight anisotropies in that background radiation, in the range of 10 ppm. What kind of "black body" was the source of this radiation?
The theory goes like this (Hu et al. 1997): All these photons originated at the same time, due to the same event. At the time of their generation, their energy spectrum corresponded to a temperature of 3 000 (three thousand) K. Cooling down to 2.728 (i.e. slightly below 3) K took them about 13.7 billion years. These photons correspond to the first light of the developing universe, emanated 379 000 years after the Big Bang. Before that time, the universe was too hot to allow the formation of atoms and was dominated by a particle soup hindering the photons to travel relevant distances. Only after the formation of (hydrogen) atoms the universe became transparent to light. Maybe you feel reminded now of Genesis 1:3 (God said, "Let there be light," and there was light). Now we know that this didn't happen on the second day of creation, but in its 379 000th year.
The anisotropies recorded by COBE are regarded as the "seeds of cosmic structure", a reflection of the first density fluctuations in the primordial particle soup. Later, these fluctuations gave rise to the formation of the first stars, and are believed to have founded the large-scale distribution of galaxy clusters as observed today (Boughn & Crittenden 2003). The origin of the cosmic microwave background marks the earliest event in the history of our universe that theoretically could be seen. Beyond that moment, the universe was pitch-dark. In other words: We cannot see to the very bottom of time, not even with a super-Hubble telescope. The last picture we see, allthough cosmologists are happy with anisotropies in the 10 ppm range, is blurred and devoid of explicit structure - and surely is not showing our behind.
More...

6/05 <          MB 6/05          > 6/05

S.Boughn & R.Crittenden (2004) A correlation between the cosmic microwave background and large-scale structure in the universe. Nature 427: 45-47
S.Dodelson, E.I.Gates, M.S.Turner (1996) Cold dark matter. Science 274: 69-75
W.Hu, N.Sugiyama, J.Silk (1997) The physics of microwave background anisotropies. Nature 386: 37-43
R.B.Partridge (1992) The seeds of cosmic structure. Science 257: 178-179