5 rep of SU(5) under SU(3)XSU(2)XU(1)

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SUMMARY

The discussion focuses on the transformation of the 5 representation of SU(5) under the gauge group SU(3)×SU(2)×U(1), specifically expressed as 5 → (3,1,-1/3) ⊕ (1,2,+1/2). This notation indicates the decomposition of the SU(5) representation into components corresponding to SU(3), SU(2), and U(1) representations. Key references include Georgi's "Lie Algebras In Particle Physics" for a comprehensive understanding of Grand Unified Theories (GUTs) and the Georgi–Glashow model. The discussion also highlights the importance of mastering Clebsch-Gordon decomposition and Young Tableaux for representation theory.

PREREQUISITES
  • Understanding of SU(5) and its role in Grand Unified Theories (GUTs)
  • Familiarity with representation theory, specifically Clebsch-Gordon decomposition
  • Knowledge of Young Tableaux and their application in particle physics
  • Basic concepts of gauge groups, particularly SU(3), SU(2), and U(1)
NEXT STEPS
  • Study Georgi's "Lie Algebras In Particle Physics" for detailed insights on SU(5) and SO(10) GUTs
  • Learn about the Clebsch-Gordon coefficients and their application in decomposing representations
  • Explore the mathematical framework of Young Tableaux in representation theory
  • Investigate the implications of SU(3) → SU(2)×U(1) transformations in particle physics
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Particle physicists, theoretical physicists, and students studying Grand Unified Theories and representation theory in the context of gauge groups.

LAHLH
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Hi,

What does is mean to say under SU(3)XSU(2)XU(1) the 5 representation of SU(5) transforms as

5\to(3,1,-1/3) \oplus (1,2,+1/2)

I can't work out what this (a,b,c) notation means exactly; could anyone point me to a link or chapter of a book that could explain what's going on here?

thanks
 
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This decomposes the representation into an outer product of representations of SU(3), SU(2) and SU(1). For example (3,1,-1/3) means 3 ⊗ 1 ⊗ -1/3, the triplet of SU(3), the singlet of SU(2) and weak hypercharge -1/3.
 
Bill_K gave the answer for what the notation means. As for references, you can start with
Wikipedia. The SU(5) model is known as the Georgi–Glashow model and is a simple example of a GUT.

Probably the best intro textbook for this topic is Georgi's Lie Algebras In Particle Physics, where both the SU(5) and SO(10) GUTs are discussed in detail.
 
So I understand how to do a Clebsch-Gordon decomp and the rules of Young-Tableaux, for example I'm happy doing things like 8\otimes 8=\bar{10} \oplus 8 \oplus 8\oplus 1 (well reasonably happy..)...so here we are just decomposing the outer product of two or more representations of a single group into the direct sum of other representations of the group.

I started having a look at p183 of Georgi where he discusses SU(3)\to SU(2)\times U(1), as I think this is a simpler example of the mathematics I need to understand my original post? I'm not sure I follow what is going on in this section (12.3) however, despite feeling I reasonably well understand the previous Young Tableaux stuff. What is he doing to obtain the figure associated with (12.16) and (12.17)?
 

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