With respect to the term 'generalized Kohn-Sham', we feel that it is appropriate. The generalized Kohn-Sham approach 67 relies on the basic idea of the original Kohn-Sham formalism by exploiting the Hohenberg-Kohn theorem to introduce a model system with the same groundstate density, in order to have access to quantities that help in the description of the electronic system. Such quantities can be energies, typically the 'noninteracting' kinetic energy or the exchange energy, but can also be orbital eigenvalues. The generalized Kohn-Sham approach generalizes the Kohn-Sham one in the sense that it extends the range of possible model systems. Like all proper generalizations, it contains the original Kohn-Sham approach as a special case. As also discussed in contribution (2.4.8), the generalized Kohn-Sham approach provides more flexibility and establishes a firm formal foundation for frequently used methods that do not calculate the exchange-correlation potential as a functional derivative with respect to the electron density, notably hybrid functional methods. And, as also discussed in contribution (4.1.5), a specific generalized-Kohn-Sham map need not be "crashed", but rather can be judiciously chosen, nonempirically, based on physical constraints.