Understanding SU(2) Adjoint Repr of Algebra

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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.