Dynkin index

In mathematics, the Dynkin index

\chi_{\lambda}

of a representation |\lambda| of the Lie algebra g that has a highest weight \lambda is defined as follows

\chi_{\lambda}=\frac{\dim(|\lambda|)}{2\dim(g)}(\lambda, \lambda %2B2\rho)

where the Weyl vector

\rho=\frac{1}{2}\sum_{\alpha\in \Delta^%2B} \alpha

is equal to half of the sum of all the positive roots of g. In the particular case where \lambda is the highest root, meaning that |\lambda| is the adjoint representation, \chi_{\lambda} is equal to the dual Coxeter number.

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