Explanation of terminology: electroweak

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SUMMARY

The discussion clarifies the relationship between the electromagnetic (E&M) and weak interactions within the Standard Model (SM) gauge group, specifically ## U(1) \times SU(2) \times SU(3) ##. It establishes that U(1) represents weak hypercharge, while SU(2) pertains to weak isospin, leading to the conclusion that the electric charge is derived from a combination of these two generators. Although the weak and electromagnetic forces are interconnected, they do not share a single coupling constant, which complicates the notion of their unification. The conversation emphasizes the importance of understanding these distinctions to grasp the underlying physics of particle interactions.

PREREQUISITES
  • Understanding of the Standard Model of particle physics
  • Familiarity with gauge theory and gauge groups
  • Knowledge of the concepts of weak hypercharge and weak isospin
  • Basic grasp of particle interactions and coupling constants
NEXT STEPS
  • Study the implications of the Weinberg angle in electroweak theory
  • Explore the role of the Higgs mechanism in particle mass generation
  • Learn about the unification of forces in Grand Unified Theories (GUTs)
  • Investigate the mathematical framework of SU(2) and U(1) in quantum field theory
USEFUL FOR

This discussion is beneficial for physicists, students of particle physics, and anyone interested in the fundamental interactions of particles, particularly those exploring the nuances of electroweak unification and gauge theories.

dextercioby
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I'm not a specialist in this subject, so bear with me. I've always wondered why one claims that the electromagnetic and weak interactions are unified, but the strong one with the (unified) other two is not.
Mathematically, I'm aware that the full gauge group of the SM is ## U(1) \times SU(2) \times SU(3) ##, so one perceives all three interactions separately and on equal footing. In what exact sense are the weak and the em unified, but the strong not?

Thank you!
 
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Since this is an A, what do you think the U(1) and SU(2) are?
 
dextercioby said:
I'm not a specialist in this subject, so bear with me. I've always wondered why one claims that the electromagnetic and weak interactions are unified, but the strong one with the (unified) other two is not.
Mathematically, I'm aware that the full gauge group of the SM is ## U(1) \times SU(2) \times SU(3) ##, so one perceives all three interactions separately and on equal footing. In what exact sense are the weak and the em unified, but the strong not?

Thank you!
To follow up on Vanadium's post:

U(1) has one generator and SU(2) has three generators. The key questions are: The E&M gauge field is associated to which of these generators? The ## Z_0## is associated to which ones? What about the ##W^\pm##?
 
U(1) is the gauge group of electromagnetism, while SU(2)w is the gauge group of the weak interactions. The fields are all 4 vectors (co-vectors actually): the e-m potential A and Wa, a=1,2,3. SU(2) (just as SU(3) in QCD) enters through the adjoint representation of dimension 3.

One more time, why one claims that A and W are "unified", if the there's no single coupling constant and no global compact and connected gauge group which has the direct product U(1) x SU (2) as a subgroup?
 
dextercioby said:
U(1) is the gauge group of electromagnetism, while SU(2)w is the gauge group of the weak interactions. The fields are all 4 vectors (co-vectors actually): the e-m potential A and Wa, a=1,2,3. SU(2) (just as SU(3) in QCD) enters through the adjoint representation of dimension 3.

One more time, why one claims that A and W are "unified", if the there's no single coupling constant and no global compact and connected gauge group which has the direct product U(1) x SU (2) as a subgroup?
Actually, U(1) is not the gauge group of electromagnetism and SU(2) is not the gauge group of the weak interaction. That was the point I wanted to make. That U(1) is the weak hypercharge, not the electromagnetic U(1). What happens is that electromagnetism corresponds to a linear combination of the weak hypercharge generator and of the ##T_3## diagonal generator of the weak isospin SU(2), so that the electric charge is given by ##Q = T_3 + Y/2 ## where (by abuse of notation) here ##T_3## is the eigenvalue of the diagonal generator of the weak isospin SU(2), and Y is the hypercharge. The orthogonal linear combination corresponds to the ##Z_0## boson while the ##T_\pm## correspond to the ##W^\pm##. It is in that sense that the weak interaction and the electromagnetic force are deeply linked. Now, you are right that they do not not have the same coupling constant since the coupling constants of the hypercharge U(1) and the weak isospin are not equal and this shows up through the Weinberg angle, so I agree with you that saying they are "unified" is a stretch. But they are definitely deeply linked together, in the sense I just described.
 
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Thanks for pointing that essential aspect to me. Now I understand.
 
dextercioby said:
U(1) is the gauge group of electromagnetism, while SU(2)w is the gauge group of the weak interactions

And there's your problem. That's a broken symmetry. The real U(1) x SU(2) has the U(1) of weak hypercharge and the SU(2) of weak isospin. The physical photons and W, Z's are mixtures of these two (and the Higgs)m, which is where unification comes in.
 
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