One loop Fermi Constant running

tomperson
Messages
4
Reaction score
0
Hi

I am attempting to calculate the mass of the W boson according to one loop energies using the equation,

Mw2=(πα/GF√2)/sin2θw(1-Δr)

where (Δr)top=(3GFMt2)/8√2π2tan2θw

using values:-

α=α(MZ)=(127.916)-1
GF=1.16634×10-5
sin2θw=0.23116 => tan2θw=sin2θw/cos2θw=sin2θw/(1-sin2θw)=0.300661
Mt=172.9

This gives the result Mw=72.2922, which is very wrong.

I suspect at least part of the discrepancy comes from the fact that the Tree Level Fermi Constant has been used, yet many hours of scouring the Internet has not revealed any running values of it. Is my assumption correct, or is there something more fundamentally wrong with what I have done?

I appreciate any assistance you can lend.
 
Physics news on Phys.org
You probably made a mistake plugging numbers in (that formula is ugly). I find 81.6, which is a bit better (WolframAlpha).

I haven't seen much about the definition of a running G_F, but apparently the reported value is measured from the muon lifetime using eq 10.4 in http://pdg.lbl.gov/2011/reviews/rpp2011-rev-standard-model.pdf Looking at that, it looks like any running of the weak coupling is accounted for by the radiative corrections there. In other words, perhaps

G_F = \frac{\sqrt{2} g_2^2(M_Z)}{8M_W^2}

is the reported value.

If that's not the case, it doesn't seem like G_F runs too much. With

g_2^2 = \frac{4\pi \alpha}{\sin^2\theta_W},

I find G_F(M_Z) = 1.1622\cdot 10^{-5} ~\mathrm{GeV}^{-2}, which is very close to the reported value.
 
Thank you. Maths is great until numbers get involved :3
 
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