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When you get particles decaying you should get as much anti-matter created as matter, anti-matter being the opposite of matter. Well, the reaction and charge has to be OPPOSITE - so for that to happen, matter and anti-matter has to be created in equal amounts, you see? Conservation of matter can't create stuff out of thin air, right?
Well, if that's true, then it should stand to reason that we should have as much matter here as anti-matter. Well, look around - what have you got? Matter. Quite a lot of it. But no anti-matter! It's not here! So where's it all gone? Where's the fundamental asymmetry?
Well, when a k-meson or "kaon" decays, you should get a completely symmetrical result - which would be a three pion group. However, sometimes, it'll decay into a two pion group! AH WHAT DA HELL! No-one knows why this happens but it does.
So, apply this rule to about five seconds after the Big Bang, sometime during the Vacuum Era. With this asymmetric tendacy in the middle of all our beautiful symmetry, it could explain why there's so much matter here - but no anti-matter!
woooooooo
Well, if that's true, then it should stand to reason that we should have as much matter here as anti-matter. Well, look around - what have you got? Matter. Quite a lot of it. But no anti-matter! It's not here! So where's it all gone? Where's the fundamental asymmetry?
Well, when a k-meson or "kaon" decays, you should get a completely symmetrical result - which would be a three pion group. However, sometimes, it'll decay into a two pion group! AH WHAT DA HELL! No-one knows why this happens but it does.
So, apply this rule to about five seconds after the Big Bang, sometime during the Vacuum Era. With this asymmetric tendacy in the middle of all our beautiful symmetry, it could explain why there's so much matter here - but no anti-matter!
woooooooo
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