aiqbench analysis
This paper introduces a novel quantum algorithm for solving linear systems ($Ax=b$) by leveraging dissipation as a core primitive rather than relying on traditional unitary evolution. By constructing a purely dissipative Lindbladian, the authors achieve dimension-independent mixing times and provide a concrete implementation strategy for digital quantum computers using block encoding. This approach offers a distinct pathway to quantum linear algebra that could be advantageous for near-term hardware where error correction is limited.
A Simple Quantum Linear-System Solver via Dissipation
arXiv:2609.12284v1 Announce Type: new Abstract: Dissipation has been recently demonstrated as a powerful primitive for designing quantum algorithms. We apply this viewpoint directly to linear-system solving, $Ax=b$. We construct a simple purely dissipative Lindbladian whose unique fixed point encodes the linear-system solution. We prove dimension-independent trace-distance mixing in $\Theta(\kappa^2\log(1/\eps))$ time. We then show how to run this Lindbladian on digital quantum computers via collective block encoding and Lindbladian simulation, resulting in an $O\!\left(\kappa^2\log(1/\eps) \frac{\log(\kappa/\eps)}{\log\log(\kappa/\eps)}\right)$ query complexity for both $U_A$, the block encoding of $A$, and $U_b$, the $|b\rangle$ state preparation unitary.
Abstract:Dissipation has been recently demonstrated as a powerful primitive for designing quantum algorithms. We apply this viewpoint directly to linear-system solving, $Ax=b$. We construct a simple purely dissipative Lindbladian whose unique fixed point encodes the linear-system solution. We prove dimension-independent trace-distance mixing in $\Theta(\kappa^2\log(1/\eps))$ time. We then show how to run this Lindbladian on digital quantum computers via collective block encoding and Lindbladian simulation, resulting in an $O\!\left(\kappa^2\log(1/\eps) \frac{\log(\kappa/\eps)}{\log\log(\kappa/\eps)}\right)$ query complexity for both $U_A$, the block encoding of $A$, and $U_b$, the $|b\rangle$ state preparation unitary.
arXiv:2609.12284 [quant-ph]
(or arXiv:2609.12284v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.12284 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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Full text under the publisher's open licence · 177 words
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