Circulant orbitals for atoms and molecules

Abstract
Circulant orbitals ϕ n for a closed-shell system are the orbitals obtained when the N canonical orthonormal Hartree-Fock orbitals λ [unk] are subjected to a unitary transformation which is the discrete Fourier transformation: ϕ n = 1/√ N Σ [unk] λ [unk] ω (n-1)([unk]-1) , where ω = exp(2πi/ N ). Electron densities associated with the orbitals ϕ n are each close to the average total electron density. The Fock matrix, diagonal for canonical orbitals, for circulant orbitals is a Hermitian circulant matrix, ε m, m+q = 1/ N Σ [unk] ε [unk] ω q ([unk]-1) , where the ε [unk] are the canonical orbital energies. The states ^F ϕ n are uniformly distributed on the surface of a sphere in Hilbert space.

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