Finite-$N$ BMN index across all vacuum sectors

We compute the finite-$N$ Witten index of BMN matrix quantum mechanics after summing over all partition-labeled supersymmetric vacuum sectors. Starting from the unitary-matrix integral for each sector, we develop two complementary evaluation methods: a symmetric-group character expansion, which reduces each fixed fugacity order to a finite combinatorial sum, and a residue expansion in which the contributing poles are organized by rooted trees, with a colored-tree generalization for multi-partition sectors. Direct integration and constant-term extraction provide independent checks in explicit examples. We evaluate every vacuum sector for $N\leq 9$. In the equal-fugacity expansion, the coefficients near charges $j\sim N^2$ show entropy growth of order $N^2$, and the sector sum does not cancel this growth. The finite-$N$ data also reveal a nontrivial sectoral organization: near $j=N^2$, the sector giving the largest contribution changes with $N$, from single-partition sectors at small rank to double-partition sectors starting at $N=5$. We call this phenomenon dominance switching. These results provide a quantitative finite-$N$ foundation for using the BMN index as a diagnostic of protected plane-wave black-hole microstates and suggest a bulk interpretation in terms of plane-wave black holes dressed by macroscopic M2 giant gravitons, analogous to dual dressed black holes in $AdS_5\times S^5$.