aiqbench analysis
This paper demonstrates a significant theoretical breakthrough in quantum circuit complexity, proving that constant-depth circuits with arbitrary-width Toffoli gates can efficiently prepare any logarithmic-qubit state without relying on FANOUT or QRAM resources. The result improves upon previous constructions by reducing the required circuit size from doubly exponential to polynomial scaling, highlighting the computational power of nonlocal interactions within restricted quantum architectures.
QAC0 Can Prepare Every Logarithmic-Qubit State
arXiv:2609.17408v1 Announce Type: new Abstract: $\mathsf{QAC}^0$ is the class of constant-depth $\mathrm{poly}(n)$-ancilla circuits obtained by extending $\mathsf{QNC}^0$, the class of local circuits, to include nonlocal interactions via arbitrary width Toffoli gates. It is believed to be weaker than its counterpart, $\mathsf{QNC}^0_f$, obtained by including arbitrary-width FANOUT gates instead ($\mathsf{QAC}^0 \subseteq \mathsf{QNC}^0_f$ [Moo99]). In this note, we show that every $O(\log n)$-qubit state can be exactly and cleanly prepared by a $\mathrm{poly}(n)$-ancilla $\mathsf{QAC}^0$ circuit. Previous known $\mathrm{poly}(n)$-ancilla circuits for arbitrary such states are only known via additional access to either FANOUT or QRAM (indexing) gates [Ros21b, GGJ26b], neither of which are known to be in $\mathsf{QAC}^0$. Equivalently, prior constructions of arbitrary $n$-qubit states in $\mathsf{QAC}^0$ require doubly exponential size and we obtain an exponential factor improvement.
Abstract:$\mathsf{QAC}^0$ is the class of constant-depth $\mathrm{poly}(n)$-ancilla circuits obtained by extending $\mathsf{QNC}^0$, the class of local circuits, to include nonlocal interactions via arbitrary width Toffoli gates. It is believed to be weaker than its counterpart, $\mathsf{QNC}^0_f$, obtained by including arbitrary-width FANOUT gates instead ($\mathsf{QAC}^0 \subseteq \mathsf{QNC}^0_f$ [Moo99]). In this note, we show that every $O(\log n)$-qubit state can be exactly and cleanly prepared by a $\mathrm{poly}(n)$-ancilla $\mathsf{QAC}^0$ circuit. Previous known $\mathrm{poly}(n)$-ancilla circuits for arbitrary such states are only known via additional access to either FANOUT or QRAM (indexing) gates [Ros21b, GGJ26b], neither of which are known to be in $\mathsf{QAC}^0$. Equivalently, prior constructions of arbitrary $n$-qubit states in $\mathsf{QAC}^0$ require doubly exponential size and we obtain an exponential factor improvement.
arXiv:2609.17408 [quant-ph]
(or arXiv:2609.17408v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.17408 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
arXivLabs is a framework that allows collaborators to develop and share new arXiv features directly on our website.
Both individuals and organizations that work with arXivLabs have embraced and accepted our values of openness, community, excellence, and user data privacy. arXiv is committed to these values and only works with partners that adhere to them.
Have an idea for a project that will add value for arXiv's community? Learn more about arXivLabs.
Full text under the publisher's open licence · 211 words
Related coverage

Researchers Prepare Logarithmic-Qubit States with Efficient Circuits
Quantum Zeitgeist · Sep 18, 2026
News Archive 2026
Quantum Computing Report · Jul 25, 2026
A Single Fixed Shallow Circuit for Classical Shadows of Arbitrary n-Qubit States
arXiv · Sep 9, 2026

Cryptographically Relevant Quantum Computer (CRQC): The Threat Timeline
Quantum Zeitgeist · May 23, 2026