Penrose's "The Road to Reality" - Objection to Broken Electroweak Symmetry?

  • Thread starter Thread starter torquil
  • Start date Start date
  • Tags Tags
    Penrose
torquil
Messages
648
Reaction score
2
Hi! This is for those who have read Penrose's "The Road to Reality" (btw, fantastic book).

In paragraph 25.8, on page 651, he writes something that I interpret as a critical remark regarding the spontaneous broken electroweak gauge symmetry.

Quote ( btw, he writes U(2) instead of the usual SU(2)xU(1) ):

"Also, there is the rather strange asymmetry between the roles of SU(3) and U(2) - in that SU(3) is taken to be exact, whereas U(2) is severely broken. Indeed, in my view, there does appear to be something strange about the particular way that U(2) is taken as a 'gauge group', which would seem to require an exact unbroken symmetry..."

Is he alluding to some problem regarding the EW theory that he does not write explictly? What does he mean by "... the particular way that U(2) is taken as a 'gauge group'"?

Anyone know/understand?

Best regards
Torquil
 
Physics news on Phys.org
A gauge theory requires massless vector bosons. The vector bosons of weak interactions are massive (to the extent the 80 GeV is not negligible). By forgetting this, G, S, and W won the Nobel prize.
 
Penrose doesn't like gauge symmetry breaking.

For Penrose's perspective, read the two sentences At the bottom of page 652 that begin with "The conventional perspective on electroweak ...," and then read sections 28.1, 28.2, and 28.3.
 
George Jones said:
Penrose doesn't like gauge symmetry breaking.

For Penrose's perspective, read the two sentences At the bottom of page 652 that begin with "The conventional perspective on electroweak ...," and then read sections 28.1, 28.2, and 28.3.

Ok, thanks. I'm in chapter 27 at the moment, so I'll have it in the back of my head when I get to those sections.

Torquil
 
clem said:
A gauge theory requires massless vector bosons. The vector bosons of weak interactions are massive (to the extent the 80 GeV is not negligible). By forgetting this, G, S, and W won the Nobel prize.

From wikipedia:

"In 1963 American physicist Sheldon Glashow proposed that the weak nuclear force and electricity and magnetism could arise from a partially unified electroweak theory. In 1967, Pakistani Abdus Salam and American Steven Weinberg independently revised Glashow's theory by having the masses for the W particle and Z particle arise through spontaneous symmetry breaking with the Higgs mechanism."

So maybe you could say that Glashow forgot it, then Salam and Weinberg remembered it later on :-)

Hopefully the LCH will be able to shed some light on the Higgs mechanism.

Torquil
 
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