“…In the k < n case, W n = 0 so there is no choice for σ n ; in the k = n case, there are (up to G W -conjugacy) three choices for σ n , namely σ n = id W n , σ n = −id W n , and σ n having eigenvalues 1 and −1; the respective values of (w + , w − ) are (2, 0), (0, 2) and (1,1). Also note that the defining equations (3.6) of Λ A 2n−1 (V, W ) now take a simpler form, since Γ i = Δ i = 0 for i / ∈ {k, 2n − k}.…”