Why is Higgs particle a doublet

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SUMMARY

The Higgs particle is a complex doublet under the weak isospin SU(2) symmetry, which is essential for the Higgs mechanism to provide mass to gauge boson fields. The hypercharge Y=1/2 is crucial for maintaining massless states in the unbroken Standard Model, where left-handed and right-handed fermions require the Higgs field to bridge gauge-multiplet mismatches. The coupling terms involving the Higgs field facilitate the generation of Dirac masses for charged elementary fermions, confirming the necessity of the Higgs particle in the Standard Model framework.

PREREQUISITES
  • Understanding of the Standard Model of particle physics
  • Familiarity with gauge theories and symmetries
  • Knowledge of weak isospin (I) and weak hypercharge (Y)
  • Basic grasp of Dirac mass terms and fermion fields
NEXT STEPS
  • Study the Higgs mechanism in detail, focusing on its role in mass generation
  • Explore the implications of gauge-multiplet mismatches in particle physics
  • Learn about the mathematical formulation of the Standard Model, including symmetry breaking
  • Investigate the differences between the Higgs field and the Higgs boson
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Particle physicists, theoretical physicists, and students studying the Standard Model and Higgs mechanism will benefit from this discussion.

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In demonstrating that Higgs mechanism gives mass to gauge boson fields, we used the fact that hypercharge Y=1/2, which is due to "Higgs particle is a complex doublet of the weak isospin SU(2) symmetry". But why?

In other words, can you show the details about why the Higgs field has charge +1/2 under the weak hypercharge U(1) symmetry?
 
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That's because in the unbroken Standard Model, everything must be massless except perhaps the Higgs particle. This is because left-handed and right-handed parts have gauge-multiplet mismatches, and the Higgs particle is necessary for bridging this gap.


The Standard Model's charged elementary fermions have mass terms that look like this:
(mass) . (left-handed part of EF field) . (right-handed part of EF field)+ + Hermitian conjugate (+ = HC)

In the unbroken SM, the EF fields break down into these gauge multiplets:
Left-handed quark, I = 1/2, Y = 1/6
Right-handed up quark, I = 0, Y = 2/3
Right-handed down quark, I = 0, Y = -1/3
Left-handed lepton, I = 1/2, Y = -1/2
Right-handed neutrino (if it exists), I = 0, Y = 0
Right-handed electron, I = 0, Y = -1
I = weak isospin, Y = weak hypercharge
Hermitian conjugate, same I, - Y

I'm ignoring generations here for simplicity. The muon and the tau are essentially additional flavors of electron, etc.

Electric charge Q = I3 + Y
I3 = -I to I in integer steps, like angular momentum

That makes bare Dirac masses impossible in the Standard Model, or at least so it seems. A left-handed part and a right-handed part, when combined, have I = 1/2 and Y = +- 1. That means that there must be some additional field with I = 1/2 and Y = 1 or -1 to cancel that out and make a proper interaction term. That field is the Higgs particle, with I = 1/2, Y = 1.

We get Higgs-coupling terms
(Higgs) . (coupling) . (left-handed quark) . (right-handed up quark)+
(Higgs)+ . (coupling) . (left-handed quark) . (right-handed down quark)+
(Higgs) . (coupling) . (left-handed lepton) . (right-handed neutrino)+
(Higgs)+ . (coupling) . (left-handed lepton) . (right-handed electron)+

Their (I,Y) sets:
(1/2,1/2) . (1/2,1/6) . (0,-2/3)
(1/2,-1/2) . (1/2,1/6) . (0,1/3)
(1/2,1/2) . (1/2,-1/2) . (0,0)
(1/2,-1/2) . (1/2,-1/2) . (0,1)

If the Higgs particle has a nonzero vacuum field value, then that field value can combine with the coupling to make a Dirac mass.
 
It seems like you are confusing "Higgs field" with "Higgs boson". You add a complex doublet field (4 degrees of freedom), and are left with but a single Higgs boson.
 

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