Simultaneous estimation of multiple eigenvalues with short-depth quantum circuit on early fault-tolerant quantum computers

We introduce a multi-modal, multi-level quantum complex exponential least squares (MM-QCELS) method to simultaneously estimate multiple eigenvalues of a quantum Hamiltonian. The circuit depth and the total cost exhibit Heisenberg-limited scaling. The quantum circuit uses one ancilla qubit, and under suitable initial state conditions, the circuit depth can be much shorter than that of quantum phase estimation (QPE) type circuits. As a result, this method is well-suited for early fault-tolerant quantum computers. Our approach extends and refines the quantum complex exponential least squares (QCELS) method, recently developed for estimating a single dominant eigenvalue [Ding and Lin, arXiv:2211.11973]. Our theoretical analysis for estimating multiple eigenvalues also tightens the bound for single dominant eigenvalue estimation. Numerical results suggest that compared to QPE, the circuit depth can be reduced by around two orders of magnitude under several settings for estimating ground-state and excited-state energies of certain quantum systems

Even shorter quantum circuit for phase estimation on early fault-tolerant quantum computers with applications to ground-state energy estimation

We develop a phase estimation method with a distinct feature: its maximal runtime (which determines the circuit depth) is $\delta/\epsilon$, where $\epsilon$ is the target precision, and the preconstant $\delta$ can be arbitrarily close to $0$ as the initial state approaches the target eigenstate. The total cost of the algorithm satisfies the Heisenberg-limited scaling $\widetilde{\mathcal{O}}(\epsilon^{-1})$. This is different from all previous proposals, where $\delta \gtrsim \pi$ is required even if the initial state is an exact eigenstate. As a result, our algorithm may significantly reduce the circuit depth for performing phase estimation tasks on early fault-tolerant quantum computers. The key technique is a simple subroutine called quantum complex exponential least squares (QCELS). Our algorithm can be readily applied to reduce the circuit depth for estimating the ground-state energy of a quantum Hamiltonian, when the overlap between the initial state and the ground state is large. If this initial overlap is small, we can combine our method with the Fourier filtering method developed in [Lin, Tong, PRX Quantum 3, 010318, 2022], and the resulting algorithm provably reduces the circuit depth in the presence of a large relative overlap compared to $\epsilon$. The relative overlap condition is similar to a spectral gap assumption, but it is aware of the information in the initial state and is therefore applicable to certain Hamiltonians with small spectral gaps. We observe that the circuit depth can be reduced by around two orders of magnitude in numerical experiments under various settings

Single-ancilla ground state preparation via Lindbladians

We design an early fault-tolerant quantum algorithm for ground state preparation. As a Monte Carlo-style quantum algorithm, our method features a Lindbladian where the target state is stationary, and its evolution can be efficiently implemented using just one ancilla qubit. Our algorithm can prepare the ground state even when the initial state has zero overlap with the ground state, bypassing the most significant limitation of methods like quantum phase estimation. As a variant, we also propose a discrete-time algorithm, which demonstrates even better efficiency, providing a near-optimal simulation cost for the simulation time and precision. Numerical simulation using Ising models and Hubbard models demonstrates the efficacy and applicability of our method