Dynkin index

In mathematics, the Dynkin index $I({\lambda })$ of a finite-dimensional highest-weight representation of a compact simple Lie algebra ${\mathfrak {g}}$ with highest weight $\lambda$ is defined by

${\text{Tr}}_{V_{\lambda }}=2I(\lambda ){\text{Tr}}_{V_{0}},$

where $V_{0}$ is the 'defining representation', which is most often taken to be the fundamental representation if the Lie algebra under consideration is a matrix Lie algebra.

The notation ${\text{Tr}}_{V}$ is the trace form on the representation $\rho :{\mathfrak {g}}\rightarrow {\text{End}}(V)$ . By Schur's lemma, since the trace forms are all invariant forms, they are related by constants, so the index is well-defined.

Since the trace forms are bilinear forms, we can take traces to obtain^{[citation needed]}

I(\lambda )={\frac {\dim V_{\lambda }}{2\dim {\mathfrak {g}}}}(\lambda ,\lambda +2\rho )

where the Weyl vector

\rho ={\frac {1}{2}}\sum _{\alpha \in \Delta ^{+}}\alpha

is equal to half of the sum of all the positive roots of ${\mathfrak {g}}$ . The expression $(\lambda ,\lambda +2\rho )$ is the value of the quadratic Casimir in the representation $V_{\lambda }$ . The index $I(\lambda )$ is always a positive integer.

In the particular case where $\lambda$ is the highest root, so that $V_{\lambda }$ is the adjoint representation, the Dynkin index $I(\lambda )$ is equal to the dual Coxeter number.