Choose the extended supersymmetry normalization
The central charge in supersymmetry is antisymmetric in , because the full anticommutator is symmetric and is antisymmetric. In a massive one-particle state rest frame, , and the first anticommutator becomes .
A unitary skew-diagonalization of an antisymmetric matrix puts into blocks , with a remaining zero direction if is odd. For one block write , and label its two supersymmetries . The combinations
have
For example the mixed contribution to the first expression is . This is the phase-aligned version of taking a supercharge minus a unitary combination of its adjoints, as suggested by the hint.
For every operator and normalized state ,
Applying this to in every block proves the BPS bound
If the algebra is instead written with on its right side, the same result is ; the factor is purely a central-charge convention.
A BPS state saturates at least one of these inequalities. The corresponding zero-norm combinations of supercharges and their adjoints annihilate the representation, so part of supersymmetry is preserved. Its massive supermultiplet is shortened: each saturated block removes two complex fermionic oscillators, giving states from a spin- Clifford vacuum when blocks saturate, before any necessary CPT completion of a supermultiplet. It preserves of the real supercharges. Its mass is tied to the central charges in supersymmetry and remains protected while it stays on the same short branch. Stability is not unconditional: a wall of marginal stability can permit a charged BPS state to decay into other BPS states with the same total charge.

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