[Home]History of Cosmic Background Radiation

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Revision 16 . . (edit) December 7, 2001 8:13 am by (logged).196.209.xxx
Revision 15 . . December 7, 2001 8:13 am by (logged).196.209.xxx [CBR in general, not just CMBR]
Revision 14 . . (edit) December 7, 2001 8:04 am by (logged).196.209.xxx
Revision 13 . . December 6, 2001 5:54 am by The ansible [fixed link to anisotropic]
Revision 12 . . December 6, 2001 5:07 am by AstroNomer
Revision 11 . . (edit) December 6, 2001 2:48 am by (logged).191.188.xxx
Revision 10 . . (edit) December 6, 2001 2:48 am by (logged).191.188.xxx
Revision 9 . . (edit) October 5, 2001 2:58 am by Mike dill
  

Difference (from prior major revision) (minor diff, author diff)

Changed: 1,13c1,13
The Cosmic Background Radiation is a form of radiation that fills the whole of the universe. It has the characteristics of Black Body radiation of a temperature of 2.726 Kelvin. It has a frequency on the microwave range.

This radiation is regarded as the best available evidence of the Big Bang theory -- it gives a snapshot of the Universe when the temperature dropped enough to allow electrons? and protons? to
form hydrogen atoms, thus making the universe transparent to radiation. When it originated some 300,000 years after the Big Bang -- this point in time is generally known as the "last scattering surface" -- the temperature of the Universe
was about 6000 K. Since then it has dropped because of the expansion of the Universe, which cools radiation inversely proportional to the fourth power of the Universe's [scale length]?.

One of the microwave background's most salient features is a high degree of isotropy. There are some anisotropies, the most pronounced of which is the dipole anisotropy at a level of about 10-4 at a scale of 180 degrees of arc. It is due to the motion of the observer against the CBR, which is some 700 km/s for the Earth.

Much smaller variations due to external physics also exist; the
Sunyaev-Zel'dovic-Effect? is one of the major factors here.
Even more interesting are anisotropies at a level of roughly 1/100000 and on a scale of a few arcminutes. Those very small variations correspond to the density fluctuations at the last scattering surface and give valuable information about the seeds for the large scale structures we observe now.

The CBR was predicted by Murray Gell-Mann? in the 1940s and was independently discovered in the 1950s by Penzias and Wilson, who received a Nobel Prize for this discovery. Since the cosmic microwave radiation is rather difficult to observe with ground-based instruments, CMB research makes increasing use of space-borne experiments. Probably still the most famous of these is the Cosmic Background Explorer (COBE?) that was flown in 1992-1996.
We any patch of the sky is observed where no individual
sources can be discerned, and the effects of the
interplanetary dust, and interstellar matter are taken into
account, there is still is radiation,
this radiation is known as Cosmic Background Radiation.
The origen of this radiation depends on the region of the
spectrum that we are observing. Certainly the most famous
component is the Cosmic microwave background radiation,
a reminder of epoch where the universe, still hot, became
transparent for the first time to radiation.
The are also background in the infrared, x-rays, etc., with
different causes, and most of them ultimately reducible to
unresolved individual sources.

Removed: 16d15
Cosmic microwave background radiation

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