2021
DOI: 10.1039/d1cp02227j
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Molecular excited state calculations with adaptive wavefunctions on a quantum eigensolver emulation: reducing circuit depth and separating spin states

Abstract: Using adaptive wavefunctions and spin restrictions to compute excited state energies of LiH in a VQE emulation greatly reduces ansatz depth, showing promise as a routine for molecular excited state calculations on near-term quantum computers.

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Cited by 17 publications
(24 citation statements)
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“…Equally we are interested in other types of UCC ansatze which involve higher-order correlation effects, such as MP3 or MP4, or triple excitation UCCSD(T) which could be important for strongly correlated systems and could improve further the accuracy as mentioned earlier 49 . We are also motivated to implement additional algorithms going beyond VQE, such as VQD (ADAPT-VQD) and QITE(ADAPT-QITE) that allow to determine excited state energies 105,72,73,106,107 .…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Equally we are interested in other types of UCC ansatze which involve higher-order correlation effects, such as MP3 or MP4, or triple excitation UCCSD(T) which could be important for strongly correlated systems and could improve further the accuracy as mentioned earlier 49 . We are also motivated to implement additional algorithms going beyond VQE, such as VQD (ADAPT-VQD) and QITE(ADAPT-QITE) that allow to determine excited state energies 105,72,73,106,107 .…”
Section: Discussionmentioning
confidence: 99%
“…Indeed, such approaches were also engineered not only for ground states but also to tackle excited states without undesired spin symmetry crossing over to lower states during VQE optimizations. They have been also used in connection with the variational Quantum Deflation algorithm (VQD), that is used to determine the energies of the ground and excited states 73 .…”
Section: Uccgsd and K-upccgsd Ansatze Uccgsdmentioning
confidence: 99%
“…10,11 Moreover, spin symmetry corresponding to the Ŝ2 operator is not conserved because the non-commuting spin components of unpaired two-body operators appear independently in the unitary product. 12 The ADAPT-VQE 13 algorithm, and its extensions, [14][15][16][17] iteratively build a UPS from a pool of one-and two-body fermionic operators, selecting the operator with the largest energy improvement at each step. Although promising, these approaches are not guaranteed to converge to the exact state 18,19 or identify the most accurate representation with the fewest number of operators, and can spontaneously break spin symmetry.…”
Section: Unitary Product Statesmentioning
confidence: 99%
“…In ref , we proposed a quantum algorithm for the calculation of the molecular excited states, which relies solely on the optimization of the ground state wave function, followed by the measurement of “excited” matrix elements. Alternative algorithms are reported in the literature, see, for instance, refs . Within this approach, excited states | n ⟩ are generated by applying an excitation operator of the general form to the ground state |0⟩ of the system, where | n ⟩ is the shorthand notation for the n th excited state of the electronic structure Hamiltonian.…”
Section: Calculation Of the Potential Energy Surfacesmentioning
confidence: 99%