Breaking SU(3)xU(1) to SU(2) Exercise: A Search for Solutions

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SUMMARY

The discussion focuses on the exercise of Higgs breaking SU(3)xSU(2)xU(1) down to SU(2), highlighting the complexities involved in the process. Participants emphasize the importance of understanding Higgs content and the implications for U(1) symmetry, particularly whether it leads to the nonchiral U(1) of electromagnetism. The conversation also touches on the relationship between gauge symmetry breaking and compactifications of extra Kaluza-Klein dimensions, suggesting that breaking from the Standard Model to SU(2) may correspond to compactifying from higher dimensions. The need for specific boundary conditions and the nature of the compactification are noted as critical factors in this context.

PREREQUISITES
  • Understanding of Higgs mechanism in quantum field theory (QFT)
  • Familiarity with gauge symmetries, specifically SU(3), SU(2), and U(1)
  • Knowledge of Kaluza-Klein theory and compactification techniques
  • Basic concepts of chiral symmetry breaking in quantum chromodynamics (QCD)
NEXT STEPS
  • Research the Higgs mechanism in SU(3)xSU(2)xU(1) models
  • Explore Kaluza-Klein compactification methods and their implications for gauge theories
  • Study the relationship between gauge bosons and boundary conditions in orbifold compactifications
  • Investigate dynamical breaking of chiral QCD and its differences from Higgs mechanisms
USEFUL FOR

The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, gauge theories, and string theory, as well as graduate students seeking to deepen their understanding of symmetry breaking and compactification in high-energy physics.

arivero
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Can anyone provide a pointer to the exercise of higgs breaking SU(3)xSU(2)xU(1) down to SU(2)? I expect it to be solved somewhere in the web...
 
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It should be pretty easy. What is it, exactly, that you're interested in?
 
BenTheMan said:
It should be pretty easy. What is it, exactly, that you're interested in?

First, to check I am guessing it right. The Higgs content, etc. And what happens with U(1): do we forcefully get the nonchiral U(1) of electromagnetism, or does it depend of the breaking?

As you say, it is easy and one could expect to find it in some web of solved QFT exercises.

My long shot is to relate the breakings with the compactifications of extra Kaluza Klein dimensions. I would expect Standard Model ---> SU(2) to correspond with a compactification from dimension 10 or 11 to dimension 6.
 
arivero said:
First, to check I am guessing it right. The Higgs content, etc. And what happens with U(1): do we forcefully get the nonchiral U(1) of electromagnetism, or does it depend of the breaking?

Well, you don't necessarily have to get U(1) EM, because that is a very specific linear combination that survives.

As you say, it is easy and one could expect to find it in some web of solved QFT exercises.

My long shot is to relate the breakings with the compactifications of extra Kaluza Klein dimensions. I would expect Standard Model ---> SU(2) to correspond with a compactification from dimension 10 or 11 to dimension 6.

Well, it depends on what you're compactifying on. You can't break gauge symmetries if you compactify on a circle---you have to compactify on an orbifold. Then you have to figure out where the gauge bosons live, and how to assign them boundary conditions.
 
We'll just have to work it out, I doubt that you'd find it online anywhere. It seems like a non-standard textbook exercize.
 
Hello,

don't you have similar example from dynamical breaking of chiral QCD ?
 
Barmecides said:
Hello,

don't you have similar example from dynamical breaking of chiral QCD ?

Hmm, but there is not Higgs field involved there, is there? In any case I will check Donoghue et al. :smile:
 

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