Sparsity-dependent Complexity Lower Bound of Quantum Linear System Solvers
Hitomi Mori, Yuta Kikuchi, Marcello Benedetti, Matthias Rosenkranz
TL;DR
This work advances the understanding of quantum linear system solver complexity by establishing a sparsity-dependent lower bound $Ω(κ sqrt{s})$ for QLS under sparse-access. It also provides a detailed reduction-based derivation of the standard bound $Ω(κ log(1/ε))$ via a reduction from the unbounded-error PARITY problem, clarifying historical uncertainties around the Harrow–Kothari result. The constructions relate the QLS problem to Boolean-query tasks, yielding κ ≈ Θ(n) and s ≈ Θ(m) in the reductions, and show that current techniques separate the ε, κ, and s dependencies. The paper highlights open questions toward a joint lower bound in all three parameters and outlines potential directions for achieving a comprehensive characterization of QLS complexity.
Abstract
Quantum linear system (QLS) solvers are a fundamental class of quantum algorithms used in many potential quantum computing applications, including machine learning and solving differential equations. The performance of quantum algorithms is often measured by their query complexity, which quantifies the number of oracle calls required to access the input. The main parameters determining the complexity of QLS solvers are the condition number $κ$ and sparsity $s$ of the linear system, and the target error $ε$. To date, the best known query-complexity lower bound is $Ω(κ\log(1/ε))$, which establishes the optimality of the most recent QLS solvers. The original proof of this lower bound is attributed to Harrow and Kothari, but their result is unpublished. Furthermore, when discussing a more general lower bound including the sparsity $s$ of the linear system, it has become folklore that it should read as $Ω( κ\sqrt{s}\log(1/ε))$. In this work, we establish the rigorous lower bound capturing the sparsity dependence of QLS. We prove the lower bound of $Ω(κ\sqrt{s})$ for any quantum algorithm that solves QLS with constant error. While the dependence on all parameters $κ,s,ε$ remains an open problem, our result provides a crucial stepping stone toward the complete characterization of QLS complexity.
