“…By [26,Section I.6], nilpotent orbits corresponding to the partition [(2n+1)(2n−1)1 3 ] are parametrized by certain quadratic forms {β 2n+1 , β 2n−1 , q V 0 }, corresponding to the parts (2n+1), (2n−1) and 1 3 , where β 2n+1 and β 2n−1 are square classes, and q V 0 is the quadratic form in 3 variables on V 0 (see Section 2.1). This parametrization can be refined according to [13,Proposition 8.1], that is, E τ ⊗σ actually has a non-zero generalized Whittaker-Fourier coefficient attached to the nilpotent O, corresponding to the partition [(2n + 1)(2n − 1)1 3 ] and parametrized by quadratic forms {β, −β, q V 0 } for some β ∈ F × . Note that the normalization of the bilinear form for the irreducible representation of sl 2 (C) of dimension i in [13] differs from the one in [26] by the factor (−1) [(i−1)/2] (See [13,Section 7]).…”