The second projection operator is Q1. It is the identity matrix - P1. It says that P1 and Q1 are complementary.
I have also proved that Q1=P2+P3 so for any number of n, Pn=sum of Qm, provided you miss m=n.
Then I tackle the idea that the Hamiltonian is also the sum of these projection operators multiplied by a factor. He calls this the SPECTRAL REPRESENTATION of the Hamiltonian - in other words, breaking the whole down into the bits that it is made of like white light is broken down into the component wavelength colours.
I've got as far as the commutator proof. The Hamiltonian commutes with the other projection operator Q.