A finite-shot perturbation bound is proved showing that, after overlap thresholding, the eigenvalue sensitivity is controlled by the condition number of the retained overlap matrix rather than by a worst-case dimension factor.
Abstract
Quantum subspace diagonalization methods are promising algorithms for quantum chemistry on near-term quantum computers. These methods can estimate low-lying energies of molecular systems using shallow quantum circuits, at the cost of many circuit repetitions to estimate the projected matrix elements. Errors in these matrix elements can be converted into much larger eigenvalue errors by an ill-conditioned overlap matrix. We study this bottleneck for the nonorthogonal quantum eigensolver (NOQE), which constructs a compact multireference subspace from dressed unrestricted Hartree-Fock states. We prove a finite-shot perturbation bound showing that, after overlap thresholding, the eigenvalue sensitivity is controlled by the condition number of the retained overlap matrix rather than by a worst-case dimension factor. With a scalable thresholding scheme, the upper bound on the per-matrix-element shot count required to reach a target accuracy scales as $\mathcal{O}(M)$, improving on the previously known $\mathcal{O}(M^3)$ bound, where $M$ is the number of reference states. Numerical experiments on hydrogen chains and rings suggest that, in practice, the measurement cost of structured NOQE instances can grow even more slowly than this linear bound.
The Monte Carlo Projective Quantum Eigensolver (MC-PQE) was recently introduced as an alternative to hybrid algorithms like the variational quantum eigensolver (VQE). By using a quantum Monte Carlo-inspired scheme for energy estimation, MC\nobreakdash-PQE was found to decrease the required measurement cost relative to...
A protocol for approximating the measurement distributions of quantum states, extending beyond standard observable estimation is introduced, and tightened gate complexity bounds for practically relevant systems, including those with k-local interactions, long-tailed matrix ensembles, and conserved quantities are provid...
Arul Rhik Mazumder, James D. Watson, Samson Wang· 0 citations
Nonorthogonal variational quantum simulation (NOVQS) is introduced, which applies linear combinations of parameterized quantum states to real- and imaginary-time evolutions and provides a flexible route to enhancing wavefunction expressivity under circuit-depth constraints.
A novel QST protocol that utilizes Kirkwood-Dirac (KD) quasiprobability to reconstruct quantum states, which enables state reconstruction with only two complementary rank-one projective measurements, thus significantly reducing the measurement cost.
Xiang Li, Yong Wang, Li-Jun Liu et al.· 0 citations
Quantum subspace diagonalization (QSD) is a near-term strategy for electronic-structure problems that avoids the deep, heavily optimized circuits of the variational quantum eigensolver by preparing a small basis, measuring a subspace Hamiltonian on hardware, and diagonalizing it classically. We benchmark two QSD varian...
Matt Trippy, R. Guo, A. Bhalla· Low-Dimensional Materials an...· 0 citations
A quantum algorithm efficient for ranges of wave lengths, with complexity in the spatial dimension and discretization and query bounds containing {\it no} negative powers of the small wavelength, which can capture the correct physical observables even if the spatial grid does not resolve the frequency, hence defying th...
Shi Jin, Chu-Wen Ma· 0 citations
We use cookies to run the site and, with your consent, for analytics and to show ads.
See our Cookie Policy.