ELECTROWEAK THEORY

 


Steven Weinberg (1933 - 2021)

Sheldon Glashow (1932 - )

Abdus Salam (1926 - 1996)








In a landmark 1967 paper, “A Model of Leptons,” often considered the first paper about the Standard Model, Weinberg noted that any theory of weak interactions must involve only leptons (and quarks) with left-handed chirality.  The equal number of right-handed leptons and quarks must be projected out.  The coupling to weak charge requires defining weak isospin and weak hypercharge.  The left-handed leptons form doublets, while the right handed ones are singlets, and the same applies to quarks.  In the same paper Weinberg indicated a way to to unify electromagnetic and weak interactions for leptons and introduced the concept of spontaneous symmetry breaking with gauge fields to generate the masses of the weak bosons.






e = g sinθw = g′ cosθw. The Weinberg angle is a coupling constant, and runs with momentum transfer like all the others.

Note that before SSB there are two independent coupling constants, g′ and g. One way to relate them to parameters after SSB is to think of the coupling constant g vanishing, but a new parameter, the Weinberg angle θW  appearing to determine what linear combination of the neutral vector bosons W0 and B0 turns into the massive Z boson and what combination turns into the massless γ.  Because the Weinberg angle is a form of coupling constant, its value "runs" with momentum transfer.

Helicity states can be described with the same formalism used for intrinsic spin-1/2, namely two-entry column vectors and 2 x 2 matrix operators.



The existence of the very-high-mass weak bosons offers many precision tests of the Standard Model of Particles and Fields.




Epic discovery of the Higgs Boson. This was the last missing piece of the Standard Model.


By the way, where does the Higgs boson get its mass?






The quest for further unifications beyond the electroweak sent physics, beginning in the 1970s, down a rabbit hole from which it has never quite emerged, despite the total and complete failure of ALL such efforts. Where do we go next?


A HISTORY OF ELECTROWEAK UNIFICATION

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