Quantum Simulation of Molecules without Fermionic Encoding of the Wave Function
arXiv:2101.11607 · doi:10.1088/1367-2630/ac3573
Abstract
Molecular simulations generally require fermionic encoding in which fermion statistics are encoded into the qubit representation of the wave function. Recent calculations suggest that fermionic encoding of the wave function can be bypassed, leading to more efficient quantum computations. Here we show that the energy can be expressed as a functional of the two-electron reduced density matrix (2-RDM) where the 2-RDM is a unique functional of the unencoded -qubit-particle wave function. Contrasts are made with current hardware-efficient methods. An application to computing the ground-state energy and 2-RDM of H is presented.
References in corpus (17)
- Supplementary information for "Quantum supremacy using a programmable superconducting processor"
- Simulated Quantum Computation of Molecular Energies
- Hartree-Fock on a superconducting qubit quantum computer
- Exact Parameterization of Fermionic Wave Functions via Unitary Coupled Cluster Theory
- The Pauli principle revisited
- Global Method for Electron Correlation
- Quantum Solver of Contracted Eigenvalue Equations for Scalable Molecular Simulations on Quantum Computing Devices
- Pinning of Fermionic Occupation Numbers
- Quantum-classical hybrid algorithm using an error-mitigating -representability condition to compute the Mott metal-insulator transition
- Generalized Pauli conditions on the spectra of one-electron reduced density matrices of atoms and molecules
- Preparation of an Exciton Condensate of Photons on a 53-Qubit Quantum Computer
- Quasipinning and selection rules for excitations in atoms and molecules
- Dual-Cone Variational Calculation of the 2-Electron Reduced Density Matrix
- Pinning of fermionic occupation numbers: Higher spatial dimensions and spin
- Exact Two-body Expansion of the Many-particle Wave Function
- Efficient Two-Electron Ansatz for Benchmarking Quantum Chemistry on a Quantum Computer
- Test of the unitary coupled-cluster variational quantum eigensolver for a simple strongly correlated condensed-matter system