Why EM and weak interaction are unified

karlzr
Messages
129
Reaction score
2
In SM, people say the ##SU(2)\otimes U(1)## theory unify the EM and weak interaction. I understand that the two interactions both originate from the electroweak theory in a mixed way. But does this mean they are unified? Since when we talk about unification like GUT, we require the couplings run to the same value at a high unification scale. I don't see it in electroweak theory. So how should we interpret the difference?
 
Physics news on Phys.org
Yes, you can justifiably complain that the electroweak theory does not really unify anything since it still has two independent gauge groups, SU(2) and U(1), with independent couplings. Ideally we might have hoped that both forces would arise from a single gauge group. GUTs are more ambitious and seek to derive the SU(3), SU(2), and U(1) of the Standard Model from a single gauge group.
 
The weak and EM couplings are the same alpha=1/137. However the weak interaction depends on
alpha/(M_W^2+Q^2), while EM is alpha/Q^2, so the weak looks weak at low energies.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top