Preparing topological states with finite depth simultaneous commuting gates

We present protocols for preparing two-dimensional Abelian and non-Abelian topologically ordered states by employing finite depth unitary circuits composed of long-ranged, simultaneous, and mutually commuting two-qubit gates. Our protocols are motivated by recent proposals for circuits in trapped ion systems, which allow each qubit to participate in multiple gates simultaneously. Our circuits are shown to be optimal, in the sense that the number of two-qubit gates and ancilla qubits scales as $O({L}^{2})$, where $L$ is the linear size of the system. Examples include the ground states of the toric code, certain Kitaev quantum-double models, and string-net models. Going beyond two dimensions, we extend our scheme to more general Calderbank-Shor-Steane codes. As an application, we present protocols for realizing the three-dimensional Haah's code and X-cube fracton models.

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Publication Details

Journal
Physical review. B./Physical review. B
Published
2025-03-28
DOI
https://doi.org/10.1103/physrevb.111.115160
Citations
1
Primary Topic
Advanced Memory and Neural Computing
Type
article
Field-Weighted Citation Impact
0.73

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article

Preparing topological states with finite depth simultaneous commuting gates

Yarden Sheffer, Ady Stern, Erez Berg
1 citations
Physical review. B./Physical review. B
Advanced Memory and Neural Computing
0.73
article

Preparing topological states with finite depth simultaneous commuting gates

Yarden Sheffer, Ady Stern, Erez Berg
article en
1 citations

Abstract

We present protocols for preparing two-dimensional Abelian and non-Abelian topologically ordered states by employing finite depth unitary circuits composed of long-ranged, simultaneous, and mutually commuting two-qubit gates. Our protocols are motivated by recent proposals for circuits in trapped ion systems, which allow each qubit to participate in multiple gates simultaneously. Our circuits are shown to be optimal, in the sense that the number of two-qubit gates and ancilla qubits scales as $O({L}^{2})$, where $L$ is the linear size of the system. Examples include the ground states of the toric code, certain Kitaev quantum-double models, and string-net models. Going beyond two dimensions, we extend our scheme to more general Calderbank-Shor-Steane codes. As an application, we present protocols for realizing the three-dimensional Haah's code and X-cube fracton models.

Physical review. B./Physical review. BVol. 111(11)
Weizmann Institute of Science (IL)
Deutsche Forschungsgemeinschaft, Israel Science Foundation, Horizon 2020, Kavli Institute for Theoretical Physics, University of California, Santa Barbara
Openalex Percentile: Top 30%
Advanced Memory and Neural Computing
0.73
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