Abstract

Computing quantum state fidelity will be important to verify and characterize states prepared on a quantum computer. In this work, we propose novel lower and upper bounds for the fidelity F(ρ,σ)F(ρ,σ) based on the "truncated fidelity" F(ρm,σ)F(ρ_m, σ), which is evaluated for a state ρmρ_m obtained by projecting ρρ onto its mm-largest eigenvalues. Our bounds can be refined, i.e., they tighten monotonically with mm. To compute our bounds, we introduce a hybrid quantum-classical algorithm, called Variational Quantum Fidelity Estimation, that involves three steps: (1) variationally diagonalize ρρ, (2) compute matrix elements of σσ in the eigenbasis of ρρ, and (3) combine these matrix elements to compute our bounds. Our algorithm is aimed at the case where σσ is arbitrary and ρρ is low rank, which we call low-rank fidelity estimation, and we prove that a classical algorithm cannot efficiently solve this problem. Finally, we demonstrate that our bounds can detect quantum phase transitions and are often tighter than previously known computable bounds for realistic situations.

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