Originally posted by: kongking
Originally posted by: User1001
didn't fermi used to produce the most.
Fermilab and CERN are the only places to my knowlege that have ever made the stuff. Not sure who started doing it first.
If you don't require complete antiatoms, we've made it in tiny quantities since the 30's. Fermilab has the been the highest energy accelerator for some years, but the LHC at CERN will take the top position in a few years.
I have a question, shouldn't there be an equal ammount of antimatter as matter? I know that after the big bang, there was nearly the same ammount of both matter and antimatter, and that much of it has annihilated. But shouldn't annihilations transform an equal ammount of both matter and matter into energy? So why has antimatter almost gone extinct?
Good question.
There is only a very small amount of matter. There are about a billion photons for every proton or neutron. The photons may have been produced by matter-antimatter annhilation in the first few moments of the universe. Your question is why are there any protons left over, without an equal amount of antiprotons.
The reason is that the symmetry between matter and antimatter isn't perfect. The strong nuclear, electromagnetic, and gravitation forces treat antimatter identically to matter (with the obvious difference that the charge is opposite), but the weak nuclear force treats them differently by about 2 parts in 1000 in certain particle decays, such as those of neutral K and B mesons.
I'll have to get a bit technical now, by introducing symmetries under two operations:
[*]
P Parity transformations, i.e. mirror reflections of space.
[*]
C Charge conjugation, i.e. reverse the electric charge of a particle.
We expected physics to be invariant under parity transformations, but it turns out that there is a fundamental difference between left and right in nature that we can observe in particle decays. It turns out that the symmetry is restored if we also turn particles into antiparticles by applying the C operation, giving us the CP symmetry.
In 1964, we discovered that the weak force violates CP symmetry. CP symmetry should prevent the K0 meson from decaying into a p+p- pair, but occasionally (about 2 times in 1000), the K0 does decay that way. The discoverers won the Nobel Prize.
More recently, several special accelerator extensions were built, called B factories, such as the BaBar project at SLAC, to examine CP violation in B0 mesons, where it was predicted to also occur from our experience with K0s. Recent results point towards CP violation in B0 mesons as well. If CP symmetry held, a B0 should decay equally into K+pi- and K-pi+ pairs, but experiments show us that B0 prefers to decay to K+pi-.
It's a very small asymmetry, but the ratio of matter to photons indicates that the difference in amounts of matter and antimatter was very small too.