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This paper establishes a rigorous lower bound for Quantum Linear System (QLS) solvers that explicitly captures the dependence on matrix sparsity ($s$), correcting previous folklore assumptions about query complexity. By proving an $\Omega(\kappa\sqrt{s})$ limit, the work provides a critical theoretical foundation for understanding the fundamental performance limits of quantum algorithms in machine learning and differential equation solving. This result is essential for researchers aiming to optimize QLS solvers and accurately assess their potential advantages over classical methods.
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Sparsity-dependent Complexity Lower Bound of Quantum Linear System Solvers

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arXiv:2601.16697v2 Announce Type: replace 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 $\kappa$ and sparsity $s$ of the linear system, and the target error $\epsilon$. To date, the best known query-complexity lower bound is $\Omega(\kappa\log(1/\epsilon))$, 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 The original proof of this lower bound is attributed to Harrow and Kothari, but their result is unpublished.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 $\Omega( \kappa \sqrt{s}\log(1/\epsilon))$. In this work, we establish the rigorous lower bound capturing the sparsity dependence of QLS. We prove the lower bound of $\Omega(\kappa\sqrt{s})$ for any quantum algorithm that solves QLS with constant error. While the dependence on all parameters $\kappa,s,\epsilon$ remains an open problem, our result provides a crucial stepping stone toward the complete 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 $\kappa$ and sparsity $s$ of the linear system, and the target error $\epsilon$. To date, the best known query-complexity lower bound is $\Omega(\kappa\log(1/\epsilon))$, 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 $\Omega( \kappa \sqrt{s}\log(1/\epsilon))$. In this work, we establish the rigorous lower bound capturing the sparsity dependence of QLS. We prove the lower bound of $\Omega(\kappa\sqrt{s})$ for any quantum algorithm that solves QLS with constant error. While the dependence on all parameters $\kappa,s,\epsilon$ remains an open problem, our result provides a crucial stepping stone toward the complete characterization of QLS complexity.

arXiv:2601.16697 [quant-ph]

(or arXiv:2601.16697v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2601.16697 Focus to learn more arXiv-issued DOI via DataCite

Quantum Sci. Technol. 11 035063 (2026)

https://doi.org/10.1088/2058-9565/ae89e0 Focus to learn more DOI(s) linking to related resources

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