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This research demonstrates that depolarizing noise in one-dimensional quantum circuits allows for efficient classical parallel simulation, effectively eliminating the previously observed quantum advantage in this specific geometric configuration. By showing that noisy 1D shallow circuits can be replicated by randomized AC0-classical circuits, the study clarifies the boundaries of where genuine quantum superiority might emerge compared to higher-dimensional setups.
Surse care acoperăarXiv, Quantum Zeitgeist, The Quantum Insider, LessWrong
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Parallel classical simulation of noisy shallow circuits: no quantum advantage in 1D

arXiv3 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2609.39448v1 Announce Type: new Abstract: We consider quantum circuits consisting of $d$ layers of nearest-neighbor two-qubit gates acting on $n$ qubits arranged on a line, where every qubit is independently depolarized with a constant probability before each layer. We describe a randomized parallel algorithm which samples from the output distribution of any such circuit to within total variation error $\delta$, with parallel runtime $2^{O(d)}\log\log(n/\delta)$ and $n 2^{O(d)}$ elementary real-arithmetic operations. Without noise, the same approach gives an exact sampler with parallel runtime $O(\log n)$. For constant depth, we further show that the input/output behavior of the noisy quantum circuit is reproduced up to a constant error by a randomized $\mathsf{AC}^0$-circuit, that is, a Boolean circuit of polynomial size and constant depth with unbounded fan-in AND and OR gates and NOT gates. Consequently, every relation problem solved by a noisy constant-depth quantum circuit in one dimension is also solved, with essentially the same success probability, by a randomized $\mathsf{AC}^0$-circuit. This rules out, for noisy circuits in one dimension, the unconditional quantum advantage established for noisy shallow circuits in two and three dimensions, where polynomial-size classical circuits over the same gate set require depth $\Omega(\log n/\log\log n)$. Our algorithm exploits the fact that depolarizing noise cuts a one-dimensional circuit into independent pieces of logarithmic width, each of which can be sampled exactly in parallel.

Abstract:We consider quantum circuits consisting of $d$ layers of nearest-neighbor two-qubit gates acting on $n$ qubits arranged on a line, where every qubit is independently depolarized with a constant probability before each layer. We describe a randomized parallel algorithm which samples from the output distribution of any such circuit to within total variation error $\delta$, with parallel runtime $2^{O(d)}\log\log(n/\delta)$ and $n 2^{O(d)}$ elementary real-arithmetic operations. Without noise, the same approach gives an exact sampler with parallel runtime $O(\log n)$. For constant depth, we further show that the input/output behavior of the noisy quantum circuit is reproduced up to a constant error by a randomized $\mathsf{AC}^0$-circuit, that is, a Boolean circuit of polynomial size and constant depth with unbounded fan-in AND and OR gates and NOT gates. Consequently, every relation problem solved by a noisy constant-depth quantum circuit in one dimension is also solved, with essentially the same success probability, by a randomized $\mathsf{AC}^0$-circuit. This rules out, for noisy circuits in one dimension, the unconditional quantum advantage established for noisy shallow circuits in two and three dimensions, where polynomial-size classical circuits over the same gate set require depth $\Omega(\log n/\log\log n)$. Our algorithm exploits the fact that depolarizing noise cuts a one-dimensional circuit into independent pieces of logarithmic width, each of which can be sampled exactly in parallel.

arXiv:2609.39448 [quant-ph]

(or arXiv:2609.39448v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.39448 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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