woensdag 14 december 2011

Higgs-boson at 126 GeV

I wish I could understand this comment on Slashdot

"
If you assume no Higgs then you end up with a Lagrangian without any mass terms (because if you put those in you break the local gauge symmetries). However when you do the calculation of e.g. e+e- --> W+W- you have to use the fact that the electron has a mass in the Feynman calculation. This non-zero mass causes you you have a "left over" term which does not cancel in the high energy limit and causes you to break unitarity.

The Higgs mechanism gets around this by adding a new diagram e+e- --> H --> W+W- which precisely cancels the electron mass term. The reason the cancellation is perfect is because the electron gets its mass from coupling to the non-zero Higgs vacuum expectation value.

So effectively you are correct in that the reason the model fails at high energy is because you use the electron mass in the cross-section calculation but have no electron mass term in the Lagrangian so you are not being consistent....but you cannot simply stick a mass term in there without adding symmetry breaking interactions which are not observed in nature. Hence you have to add a Higgs field with a non-zero vacuum expectation value which in turn adds more than just the effective mass terms.

Hope that is comprehensible - it is hard to explain in just typed text!
"
by Roger W Moore

I think I need to recap some of my physics learnings books for that.....