In the 1930Ős, following the discovery of the expanding
universe, attempts began to extrapolate back to the beginning of the expansion.
Running the expansion backward (in theory) led to the idea of a hot, dense
early universe, too hot to be anything but a plasma, perhaps hot enough to
cause fusion, and happening at a particular time. The idea appeared ridiculous
to most scientists. How could there be a beginning? Did the laws of physics
begin then too? At the time, most scientists thought that the universe was
infinitely old. The Hubble law ended the static universe model, but it was
hoped that some infinite age model would replace it.
The first logical, self-consistent calculation was done in
the 1940Ős, by George Gamow, Alpher and Herman. At first they started with an
equal mix of protons and neutrons. They didnŐt try to explain the origin of
this mix, or claim it was realistic. They calculated the reactions that would
happen at temperature of several million K, and hoped to discover the origin of
all the elements, given some original mix of protons and neutrons.
The results were unexpected:
- They
couldnŐt make any element but He, and a small amount of deuterium (H with
a neutron bound to the proton in the nucleus.)
- They
soon realized the heat radiation in the early universe had no place to go!
If it was hot, there would have to be radiation, and it would still be
everywhere today.
- They
calculated the present temperature as around 5K, not exactly, but
certainly greater than 1K.
At the same time, Fred Hoyle, Gold, Bondi and others
developed the Steady State theory, consistent with General Relativity with an
extra constant, which would be expanding but constantly creating matter and not
changing density. Hoyle was partly motivated by religion – he was an atheist
and didnŐt like the idea of a creation event. Hoyle named the origin idea the
ŇBig BangÓ. It was derogatory, but not for long. (The word ŇYankeeÓ was
derogatory too, but it outlasted its inventors and their empire.)
The modern theory is more developed and more interesting
than the original.
- The
modern theory is developed partly from actual measurements of the cosmic
radiation predicted by Alpher, Herman, and Gamow.
- It
makes no assumptions about the original mix. A hot enough environment will
contain every elementary particle and anti-particle, in equal numbers.
Photons are just part of the mix.
- As
things cool off (in a second or so!) particles and antiparticles
annihilate until only photons and neutrinos are left. The photons become
the 5K temperature radiation deduced above.
- Um,
well, there are a few particles too. These are our protons, neutrons, and
electrons.
- The
proton-neutron ratio is not 50-50, and is not arbitrary. It follows from
the calculations. The protons donŐt last in isolation, but are found in He
nuclei.
- The
exact ratio of H to He depends, to a few percent, on the number of
families of neutrinos. By the time it became possible to measure that
number in accelerators, the cosmic theory needed the number to be three,
or just possibly 4. By then it was actually a test of the Big Bang theory.
When measured, the number of neutrino families was indeed found to be
three.
- The
deuterium fraction depends on the initial (and thus the present) density
of protons & neutrons. This ŇbaryonicÓ matter is about 4% of the
critical density. Most of it (about 75%) is outside the galaxies.