“…In the framework of variational quantum algorithms, there has been considerable effort in obtaining excited states. ,,− Among them, the most prominent approach is perhaps variational quantum deflation (VQD), which introduces the following modification to the Hamiltonian to determine the κth excited state Ĥ false( κ false) = Ĥ + ∑ λ = 0 κ − 1 α | Ψ λ false⟩ false⟨ Ψ λ | where α = prefix− ⟨ Ψ λ | Ĥ | Ψ λ ⟩ is typically chosen. This modified Hamiltonian ensures approximate orthogonality between |Ψ λ ⟩ (λ = 0, 1, 2, ..., κ), which are the ground state, and the first, second, ..., and κth excited states, obtained by the corresponding VQE calculations.…”