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Symmetry breaking

Choose the map before branching

Two su(2) embeddings in su(3) give different physical multiplets.

A subgroup name is not enough

Branching restricts a representation along a specified homomorphism. The abstract groups alone do not identify that map. Kernel, image, and charge conventions are part of the calculation.

The regular map

The regular block inclusion sends U to diag(U,1). It is injective. Restricting the fundamental and adjoint gives:

3↓SU(2)=2⊕1,8↓SU(2)=3⊕2⊕2⊕1\mathbf3\downarrow\mathrm{SU}(2)=\mathbf2\oplus\mathbf1,\qquad \mathbf8\downarrow\mathrm{SU}(2)=\mathbf3\oplus\mathbf2\oplus\mathbf2\oplus\mathbf1

The principal map

The spin-one representation defines the principal homomorphism from SU(2) to SU(3). Its kernel is {±I} and its image is SO(3). The same parent representations now restrict as follows:

3↓SO(3)=3,8↓SO(3)=3⊕5\mathbf3\downarrow\mathrm{SO}(3)=\mathbf3,\qquad\mathbf8\downarrow\mathrm{SO}(3)=\mathbf3\oplus\mathbf5

Verify the result

Start from the fundamental times its conjugate, which is the sum of the singlet and adjoint. Restrict both factors, then remove the singlet. The regular and principal results both have dimension eight, but different spin content. The principal restriction contains only integer spins, as required by the kernel.

3⊗3‾=1⊕8\mathbf3\otimes\overline{\mathbf3}=\mathbf1\oplus\mathbf8

Work with the actual map

Embeddings and branching contrasts the regular and principal maps. Continue to the SU(5) worked restriction and retain its abelian charges and finite kernel.

Sources and further reading

This guide connects sourced reference material with supported calculations. Source curation and automated checks do not constitute completed independent expert review. Read the editorial method.