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This pull requests allows for frozen core orbitals. This is implemented by modifying the slice for occupied orbitals:
self.o = slice(0,system.n) -> slice(nfrozen,system.n),
where nfrozen now is an argument to the constructor of the system class. The parameter nfrozen just gives the number of electrons to freeze, so it does not discriminate between restricted or general type systems. This has the potential pitfall that, for example nfrozen=1 effectively freezes the lowest lying doubly occupied orbital for a restricted system, while freezing just 1 spin-orbital for a general system. We have support for going from a restricted to a general system, thus we should make a choice if this automatically should mean that nfrozen is multiplied by 2 (I think this is most sensible, but maybe it is debatable).
Note that system.n, system.l and system.m are unchanged and that the number of virtual orbitals (self.m) is unaffected by the frozen core. However, it should be noted that when the reference energy and the fock matrix is constructed all occupied orbitals have to be used. This is handled explicitly in these methods.