“…As before, (A.25) j ℓ (λ) = |μ p · · ·μ ℓ | . (1, 5, 7, 9, 10, 11) 1 : 1, 3 1 (3,4,7,8,11,12) 2 : 2, 4 1 (2, 5, 7, 9, 10, 12) 2 : 1, 3, 5 2 * (1, 6, 8, 9, 10, 11) 0 : 1 0 (3, 5, 7, 9, 11, 12) 3 : 1, 3, 4 2 (2, 6, 8, 9, 10, 12) 1 : 1, 5 1 * (4, 5, 7, 10, 11, 12) 1 : 3 1 (3,6,8,9,11,12) 2 : 1, 4 1 (4, 6, 8, 10, 11, 12) 2 : 1, 3 1 (5,6,9,10,11,12) 1 : 2 1 * (7,8,9,10,11,12) As an example, Table 2 lists the partitions and corresponding a : J and r values for the Schubert varieties of S 6 = Spin 12 C/P 6 . The discussion above yields the following.…”