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arXiv:2604.25333

Sign Embedding Quantum Algorithms for Matrix Equations and Matrix Functions

Yanqiao Wang, Jin-Peng Liu

quant-phmath.NASubmitted Apr 28, 2026• Announced Apr 29, 2026• 0 citations• Revised Sep 21, 2026 (v2)
v1 · Apr 28, 2026v2 · Sep 21, 2026
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Abstract

We develop operator-output quantum algorithms for matrix equations and matrix functions using matrix-sign embeddings. For each problem, an augmented matrix $M$ is chosen so that the target operator is a block of $\text{sign}(M)$ or is recovered from blocks of $(I-\text{sign}(M))/2$. We approximate the half-plane sign by a logarithmic-sinc formula and implement the shifted inverse families by scaled multiplexing with node-dependent rebalancing. For ordinary Sylvester equations, this yields a block-encoding of the solution with query complexity linear in the relevant conditioning parameters and logarithmic in the inverse error tolerance, under either a field-of-values (FoV) gap or a strip-resolvent bound. The same method extends to generalized Sylvester and Lyapunov equations, principal square and inverse square roots, matrix geometric means, and continuous-time algebraic Riccati equations (CARE), with explicit query-complexity and block-encoding-normalization bounds that cover non-normal and non-diagonalizable cases.

Comments
81 pages, 3 figures, 6 tables

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Determining whether every trajectory of the linear system x˙=Ax\dot{x}=Axx˙=Ax converges to zero (or, equivalently, whether AAA is Hurwitz stable) is a fundamental problem in control theory. It arises, for example, in verifying the stability of feedback controllers and state observers, as well as of linearized dynamical models. We study the quantum query complexity of deciding whether a matrix A∈Cn×nA\in\mathbb{C}^{n\times n}A∈Cn×n is Hurwitz stable, given an exact normalized block-encoding of AAA. The query complexity is characterized in terms of the system dimension nnn and a supplied lower bound 0<ν≤ωA0<ν\leq ω_A0<ν≤ωA​ on the imaginary-axis distance ωA:=min⁡t∈Rσmin⁡(A−itI)ω_A:=\min_{t\in\mathbb{R}}σ_{\min}(A-\mathrm{i}tI)ωA​:=mint∈R​σmin​(A−itI), where σmin⁡(A)σ_{\min}(A)σmin​(A) is the smallest singular value of AAA. We prove a query-complexity lower bound of Ω(n/ν)Ω(\sqrt{n}/ν)Ω(n​/ν), which holds even when AAA is restricted to be real and diagonal. For general matrices with nonzero ωAω_AωA​, we encode an approximation of the right-half-plane spectral projector sign⁡+(A):=(I+sign⁡(A))/2\operatorname{sign}^+(A):=(I+\operatorname{sign}(A))/2sign+(A):=(I+sign(A))/2 as a block of a matrix inverse, where AAA is Hurwitz if and only if the projector is zero. To test this, we produce a quantum algorithm which determines if a (β,b,1/(4n))(β,b,1/(4\sqrt{n}))(β,b,1/(4n​))-block-encoded projector matrix (like sign⁡+(A)\operatorname{sign}^+(A)sign+(A)) is zero or not; for constant success probability, it has complexity Θ(βn)Θ(β\sqrt{n})Θ(βn​). When the zero test is applied to specific approximations of sign⁡+(A)\operatorname{sign}^+(A)sign+(A), this yields an upper bound of O(nν−2log⁡(n/ν))O(\sqrt{n}ν^{-2}\log(\sqrt{n}/ν))O(n​ν−2log(n​/ν)) queries in the general case, and O(nν−1log⁡n)O(\sqrt{n}ν^{-1}\log n)O(n​ν−1logn) when AAA is Hermitian or normal. The latter upper bound matches the lower bound up to a logarithmic factor. Thus the dimension dependence of quantum Hurwitz testing is nearly optimal, while the remaining factor in the non-normal case isolates an open conditioning gap.
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