I don't understand the following statement: Any pair of Dirac spinors verifies $(\bar{\Psi}_1\Psi_2)^\dagger=\bar{\Psi}_2\Psi_1$ and it is valid for both commuting and anti-commuting (Grassmann-valued) components.
In the case of Grassmanian number, shouldn't I add an extra sign when I flip them? Is there anything else to take into account in the case of Majorana spinors?