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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:
[X_{i}, X_{j}]= ε_{ij}^{k} X_{k}
(maybe I forgot an i but I am not sure).
The adjoint representation is then ( in the matrix representation) defined by the ε_{ijk} structure constants, via the identification X_{i}= [ε_{i}]_{j}^{k}. Correct? Because by that we have:
(adX_{i})^{k}_{j}= ad X_{i} X_{j}|_{X_{k}} = [X_{i}, X_{j}]|_{X_{k}}=[ε_{i}]_{j}^{k}
Now begins my question/problem. The matrices of [ε_{i}]_{j}^{k} are of dimension j_{max}\times k_{max} so equal to the number of generators X_{i}.
The su(2) algebra has n^{2}-1=4-1=3 generators, so the adjoint representation can be seen as 3\times3 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?

We know that the algebra is given:
[X_{i}, X_{j}]= ε_{ij}^{k} X_{k}
(maybe I forgot an i but I am not sure).
The adjoint representation is then ( in the matrix representation) defined by the ε_{ijk} structure constants, via the identification X_{i}= [ε_{i}]_{j}^{k}. Correct? Because by that we have:
(adX_{i})^{k}_{j}= ad X_{i} X_{j}|_{X_{k}} = [X_{i}, X_{j}]|_{X_{k}}=[ε_{i}]_{j}^{k}
Now begins my question/problem. The matrices of [ε_{i}]_{j}^{k} are of dimension j_{max}\times k_{max} so equal to the number of generators X_{i}.
The su(2) algebra has n^{2}-1=4-1=3 generators, so the adjoint representation can be seen as 3\times3 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?

