Going further, the unbroken Standard Model does not feature electric charge. Instead, electric charge emerges from the breaking of electroweak symmetry. Every unbroken-SM multiplet has three gauge-symmetry quantum numbers:
- The QCD multiplicity (strictly speaking: 2 quantum numbers)
- The weak isospin I
- The weak hypercharge Y
WIS behaves like 3D angular momentum, thus the name. Multiplet members have WIS-component value I
3 values -I, -I+1, -I+2, ..., I-1, I.
WHC behaves like electric charge - it's the average electric charge of a multiplet.
The members' electric charges are
Q = I
3 + Y
or
Q = -I + Y, -I + 1 + Y, -I + 2 + Y, ..., I - 1 + Y, I + Y
Standard-Model particles: (WIS, WHC) -> Q's
L = left-handed, R = right-handed
- L quark: (1/2, 1/6) -> -1/3, 2/3
- R down quark: (0, -1/3) -> -1/3
- R up quark: (0, 2/3) -> 2/3
- L lepton: (1/2, -1/2) -> -1, 0
- R electron: (0, -1) -> -1
- R neutrino: (0, 0) -> 0
- QCD particle: gluon: (0, 0) -> 0
- WIS particle: W: (1, 0) -> -1, 0, 1
- WHC particle: B: (0, 0) -> 0
- down Higgs particle: (1/2, -1/2) -> -1, 0
- up Higgs particle (1/2, 1/2) -> 0, 1 (SM: conjugate of down Higgs, MSSM: separate particle)
Antiparticles: same I, reverse-sign Y, L <-> R
However, that puts the problem back a step, and the weak hypercharges have even more fractional values. But there's a solution. From QCD multiplets' quantum numbers can be deduced "triality", a quantity that adds modulo 3. Gluons and colorless particles have triality 0, quarks triality 1, and antiquarks triality 2. Hadrons have triality 0. From the SM particles, one can deduce this expression for the weak hypercharge:
Y = - (triality)/3 + I + (integer)
For the electric charge, that gives us
Q = - (triality)/3 + (integer)
That Y expression is a consequence of some GUT's, like Georgi-Glashow, Pati-Salam, and their supersets.