Understanding SU(2) Adjoint Repr of Algebra

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SUMMARY

The discussion focuses on the adjoint representation of the su(2) algebra, which is defined by the structure constants ε_{ijk}. The adjoint representation corresponds to 3 generators, resulting in a 3x3 matrix representation that acts on 3-component vectors, confirming it as a spin J=1 representation. The conversation also clarifies that the spin-1/2 representation is isomorphic to the fundamental representation, which is built on C2, despite the initial assumption that it requires two generators.

PREREQUISITES
  • Understanding of Lie algebras, specifically su(2)
  • Familiarity with matrix representations of algebraic structures
  • Knowledge of representation theory, particularly spin representations
  • Basic concepts of isomorphism in algebra
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The discussion is beneficial for theoretical physicists, mathematicians specializing in algebra, and students studying quantum mechanics or representation theory, particularly those interested in the properties of Lie algebras and their representations.

ChrisVer
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Well I am trying to understand the adjoint representation of the su(2) algebra.
We know that the algebra is given:
[itex][X_{i}, X_{j}]= ε_{ij}^{k} X_{k}[/itex]
(maybe I forgot an [itex]i[/itex] but I am not sure).

The adjoint representation is then ( in the matrix representation) defined by the [itex]ε_{ijk}[/itex] structure constants, via the identification [itex]X_{i}= [ε_{i}]_{j}^{k}[/itex]. Correct? Because by that we have:
[itex](adX_{i})^{k}_{j}= ad X_{i} X_{j}|_{X_{k}} = [X_{i}, X_{j}]|_{X_{k}}=[ε_{i}]_{j}^{k}[/itex]

Now begins my question/problem. The matrices of [itex][ε_{i}]_{j}^{k}[/itex] are of dimension [itex]j_{max}\times k_{max}[/itex] so equal to the number of generators [itex]X_{i}[/itex].

The su(2) algebra has [itex]n^{2}-1=4-1=3[/itex] generators, so the adjoint representation can be seen as [itex]3\times3[/itex] matrices, so it naturally acts on 3 component vectors. That means that the adjoint representation is 3 dimensional representation and so it is the spin J=1. (?)
Is there another way to prove the last sentence? Eg using the existing isomorphism between su(2)-so(3) algebras? And one more question, what happens with the spin-1/2? The spin 1/2 representation (if my logic was correct) could only exist if the number of generators are 2!
Can someone help? :confused::blushing:
 
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ChrisVer said:
[...]
The su(2) algebra has [itex]n^{2}-1=4-1=3[/itex] generators, so the adjoint representation can be seen as [itex]3\times3[/itex] matrices, so it naturally acts on 3 component vectors. That means that the adjoint representation is 3 dimensional representation and so it is the spin J=1. (?) [...]

Yes. The adjoint rep. is isomorphic to the standard weight =1 representation.

ChrisVer said:
[...]Is there another way to prove the last sentence? Eg using the existing isomorphism between su(2)-so(3) algebras? [...]

You don't need it. Just write down the 3 generators of each representation and compare them. The basis of the rep. space is (1,0,0), (0,1,0) and (0,0,1).

ChrisVer said:
[...] And one more question, what happens with the spin-1/2? The spin 1/2 representation (if my logic was correct) could only exist if the number of generators are 2!
Can someone help? :confused::blushing:

No. The dimension (weight) of the representation has to do with the dimension of the vector space on which the representation is built. Actually spin/weight 1/2 rep. is isomorphic to the fundamental representation. Both are built on C2.
 

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