2
$\begingroup$

My professor defined the Clebsch-Gordan series as the direct sum decomposition of the tensor product of two representations of the Lie group SU(2):

$$ D_{j_1} \otimes D_{j_2} = D_{j_1+j_2} \oplus D_{j_1+j_2-1} \oplus ... \oplus D_{|j_1-j_2|} $$

I think it's an interesting fact that the trivial representation $D_0$ will be in the tensor product if and only if $j_1=j_2$.

Is there an intuitive explanation for that? What common property of all systems with $j_1=j_2$ leads to the trivial representation being part of the tensor product?

This question could be generalized to a similar fact about $D_{1/2}$ and $D_1$.

$\endgroup$

2 Answers 2

2
$\begingroup$

Generically, given a representation $V$ of a group, the tensor representation $V\otimes V$ will decompose into the symmetric and antisymmetric parts $$ V\otimes V = \Lambda^2 V \oplus S^2 V$$ and in the case of the rotation group (or its universal cover), the symmetric 2-tensors have a certain invariant under rotations - their trace! So when $j_1 = j_2$, the tensor representation is really the 2-tensors (think: matrices) on the $D_{j_1}$ space, and the trace part of the matrices forms the trivial subrepresentation.

If $j_1 \neq j_2$, the tensor representation is not simply such sqaure matrices on the original space, so we can't speak of a trace, and we don't have a trivial subrepresentation.

$\endgroup$
1
$\begingroup$

Yes. To obtain a scalar (or the trivial representation) one must multiply a representation $D^{\lambda}$ by its conjugate $D^{\lambda^*}$: the weights in the conjugate representation $\lambda^*$ are the negative of those in $\lambda$, and the scalar occurs when combining conjugate functions, so,as to produce a final function with weight $0$.

In $SU(2)$ all representations are self conjugate, so $\lambda^*$ is equivalent to $\lambda$, and indeed the weights in $\lambda$ runs from $-\lambda$ to $\lambda$, so that any weight and its negative are in the representation. This means that, to get a scalar, you need to have $\lambda_1=\lambda_2$.

In other groups, v.g. $SU(3)$, not all irreps are self-conjugate. To get a scalar one must then combine two properly conjugate irreps, such as $(1,0)$ and $(0,1)$. Indeed $(1,0)\otimes (0,1)=(0,0)\oplus (1,1)$ etc.

$\endgroup$

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service and acknowledge you have read our privacy policy.

Not the answer you're looking for? Browse other questions tagged or ask your own question.