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Don Danilov

Publications and source records attributed to Don Danilov.

3 recordsLinked to original sources

Open-shell Configuration State Functions as trial states for phaseless auxiliary-field quantum Monte Carlo

The accurate description of open-shell states in molecular systems poses challenges for approximate electronic structure methods. One emerging approach is to variationally optimize the orbitals of a single user-selected Configuration State Function (CSF), i.e., a linear combination of Slater determinants that is constructed as an eigenstate of the total spin operator. In this work we explore the use of these orbital-optimized single CSFs as trial wavefunctions in phaseless auxiliary-field quantum Monte Carlo (ph-AFQMC), a stochastic method that recovers electron correlation by evolving an initial state in imaginary time, subject to a constraint imposed by the trial state. We investigate the symmetric stretch of H-He-H, a series of small $p$-block compounds with diradicaloid singlet states, twisted ethene conformers, and a bimetallic iron-sulfur complex. We find that accurate energetics are obtained for states dominated by open-shell character, and that for certain atoms and diatomics the accuracy can be significantly improved when the trial is made to also preserve the relevant angular momentum symmetries. Furthermore, our study reveals that the open-shell CSF trial is suboptimal when the target electronic state reflects a significant mixture of ionic and covalent character, e.g., at shorter bond lengths in H-He-H and for the superexchange-stabilized ground state of [2Fe-2S]$^{2+}$. Our findings suggest that ph-AFQMC using CSF trial states is a promising method for many (but not all) strongly correlated molecular states, especially given its relatively low computational cost, and that it provides a reasonable non-perturbative way to recover some of the dynamic correlation that is otherwise missing in the CSF.

physics.chem-ph↗

Selecting optimal unrestricted Hartree-Fock trial wavefunctions for phaseless auxiliary-field quantum Monte Carlo: Accuracy and limitations in modeling three iron-sulfur clusters

Phaseless auxiliary-field quantum Monte Carlo (ph-AFQMC) has emerged as a promising electronic structure method for correlated electronic systems. However, the quality of its predictions depends critically on the choice of trial wavefunction, and it is not obvious how to make an optimal choice especially for strongly correlated states of large systems. Mean-field wavefunctions are compelling trial wavefunction candidates as they map directly to chemical concepts and can be obtained with $O(N^4)$ cost. Yet in the strongly correlated regime one faces a symmetry dilemma and the existence of multiple nearly-degenerate solutions. In this work we investigate active space models of [2Fe-2S]$^{2+}$, mixed-valent [4Fe-4S]$^{2+}$, and [4Fe-4S]$^{4+}$ and explore the sensitivity of ph-AFQMC to the choice of unrestricted Hartree-Fock trial wavefunction. We find that chemical properties and physical symmetries, rather than the variational energy, ought to guide the choice of mean-field trial for ph-AFQMC (or reference state for coupled cluster models), and show that surprisingly accurate ground-state energies for these systems can be obtained. However, in all cases we find a rapidly vanishing overlap between the stochastic wavefunction and the UHF trial, indicating that the trials are suboptimal importance functions. By analogy to a similar situation in the stretched helium dimer cation, we show how this sampling bias pushes ph-AFQMC towards artificially negative energies, which evidently can be compensated for by the phaseless bias in certain cases.

physics.chem-ph↗

Enhancing the accuracy and efficiency of sample-based quantum diagonalization with phaseless auxiliary-field quantum Monte Carlo

Quantum Selected Configuration Interaction (QSCI) and an extended protocol known as Sample-based Quantum Diagonalization (SQD) have emerged as promising algorithms to solve the electronic Schrödinger equation with noisy quantum computers. In QSCI/SQD a quantum circuit is repeatedly prepared on the quantum device, and measured configurations form a subspace of the many-body Hilbert space in which the Hamiltonian is diagonalized classically. For the dissociation of N$_2$ and a model $\mathrm{[2Fe-2S]}$ cluster (correlating 10 electrons in 26 orbitals and 30 electrons in 20 orbitals, respectively) we show that a non-perturbative stochastic approach, phaseless auxiliary-field quantum Monte Carlo (ph-AFQMC), using truncated SQD trial wavefunctions obtained from quantum hardware can recover a substantial amount (e.g., O(100) mHa) of correlation energy and alleviate the possible sampling redundancy of the QSCI/SQD procedure. Extrapolation of the ph-AFQMC energy versus the energy variance of the SQD trial wavefunctions has the potential to further improve the energy accuracy.

quant-ph↗