In mathematics, the Dynkin index
                              x                      λ                                  of a representation with highest weight                               |                λ                  |                         of a compact simple Lie algebra                                           g                                   that has a highest weight                     λ                 is defined by
                                          t            r                          (                  t                      a                                    t                      b                          )        =        2                  x                      λ                                    g                      a            b                                  evaluated in the representation                               |                λ                  |                        . Here                               t                      a                                   are the matrices representing the generators, and                               g                      a            b                                   is given by
                                          t            r                          (                  t                      a                                    t                      b                          )        =        2                  g                      a            b                                  evaluated in the defining representation.
By taking traces, we find that
                              x                      λ                          =                                            dim                                            |                            λ                              |                                                    2              dim                                                              g                                                                    (        λ        ,        λ        +        2        ρ        )                where the Weyl vector
                    ρ        =                              1            2                                    ∑                      α            ∈                          Δ                              +                                                    α                is equal to half of the sum of all the positive roots of                                           g                                  . The expression                     (        λ        ,        λ        +        2        ρ        )                 is the value quadratic Casimir in the representation                               |                λ                  |                        . The index                               x                      λ                                   is always a positive integer.
In the particular case where                     λ                 is the highest root, meaning that                               |                λ                  |                         is the adjoint representation,                               x                      λ                                   is equal to the dual Coxeter number.