Why 1964 Higgs? Uncovering the Motivation Behind Its Postulation

  • Thread starter Thread starter DonBonbon
  • Start date Start date
  • Tags Tags
    Higgs
DonBonbon
Messages
2
Reaction score
0
Layman, I have a problem to understand the Higgs' motivation back then at 1964.

The Higgs as I understand was postulated to explain how spontaneous breaking of gauge symmetry takes place in nature, which in turn explains why other elementary particles have mass.
This all make perfect sense as of today...But, and here comes my lack of knowledge, at that time there was no W+/-, nor Z and no electroweak unification, so why to bother?
What was the problem these paper tried to tackle?
Was it 'only' to explain the mass mechanism via yet unknown vector bosons?...Or did they (the 3 groups) really aimed that high?
Was it intentional or was it like pure curiosity 'Lie Groups' that then became a necessity?

NB - no diminutive by pure curiosity, to the contrary.
 
Physics news on Phys.org
Did you read the paper? Higgs makes it clear in the 1st paragraph (which I will not type in) exactly what he is doing.
 
Thanks...I actually could find only the 19 October publication, that of July 27, I could not found online.
It was not that obvious to me however - does Higgs stated his intention to show that Goldstone vector boson can acquire mass under gauge fields as well?
i.e. does he say something like: "these particles have mass and therefore 'are real objects' and can be experimentally tested one day?"
I'm not suggesting that massless particles are not real...I extrapolate (based on remark Pauli once made to Yang about the mass of this particles), that the lack of mass was a problem.
Do am anywhere near the zone?
 
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