Quantum circuits for toric code and X-cube fracton model

We propose a systematic and efficient quantum circuit composed solely of Clifford gates for simulating the ground state of the surface code model. This approach yields the ground state of the toric code in $\lceil 2L+2+log_{2}(d)+\frac{L}{2d} \rceil$ time steps, where $L$ refers to the system size a...

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Main Authors: Penghua Chen, Bowen Yan, Shawn X. Cui
Format: Article
Language:English
Published: Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften 2024-03-01
Series:Quantum
Online Access:https://quantum-journal.org/papers/q-2024-03-13-1276/pdf/
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author Penghua Chen
Bowen Yan
Shawn X. Cui
author_facet Penghua Chen
Bowen Yan
Shawn X. Cui
author_sort Penghua Chen
collection DOAJ
description We propose a systematic and efficient quantum circuit composed solely of Clifford gates for simulating the ground state of the surface code model. This approach yields the ground state of the toric code in $\lceil 2L+2+log_{2}(d)+\frac{L}{2d} \rceil$ time steps, where $L$ refers to the system size and $d$ represents the maximum distance to constrain the application of the CNOT gates. Our algorithm reformulates the problem into a purely geometric one, facilitating its extension to attain the ground state of certain 3D topological phases, such as the 3D toric model in $3L+8$ steps and the X-cube fracton model in $12L+11$ steps. Furthermore, we introduce a gluing method involving measurements, enabling our technique to attain the ground state of the 2D toric code on an arbitrary planar lattice and paving the way to more intricate 3D topological phases.
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spelling doaj.art-2613a04d31a24068aaa2b95b771c54032024-03-13T11:07:24ZengVerein zur Förderung des Open Access Publizierens in den QuantenwissenschaftenQuantum2521-327X2024-03-018127610.22331/q-2024-03-13-127610.22331/q-2024-03-13-1276Quantum circuits for toric code and X-cube fracton modelPenghua ChenBowen YanShawn X. CuiWe propose a systematic and efficient quantum circuit composed solely of Clifford gates for simulating the ground state of the surface code model. This approach yields the ground state of the toric code in $\lceil 2L+2+log_{2}(d)+\frac{L}{2d} \rceil$ time steps, where $L$ refers to the system size and $d$ represents the maximum distance to constrain the application of the CNOT gates. Our algorithm reformulates the problem into a purely geometric one, facilitating its extension to attain the ground state of certain 3D topological phases, such as the 3D toric model in $3L+8$ steps and the X-cube fracton model in $12L+11$ steps. Furthermore, we introduce a gluing method involving measurements, enabling our technique to attain the ground state of the 2D toric code on an arbitrary planar lattice and paving the way to more intricate 3D topological phases.https://quantum-journal.org/papers/q-2024-03-13-1276/pdf/
spellingShingle Penghua Chen
Bowen Yan
Shawn X. Cui
Quantum circuits for toric code and X-cube fracton model
Quantum
title Quantum circuits for toric code and X-cube fracton model
title_full Quantum circuits for toric code and X-cube fracton model
title_fullStr Quantum circuits for toric code and X-cube fracton model
title_full_unstemmed Quantum circuits for toric code and X-cube fracton model
title_short Quantum circuits for toric code and X-cube fracton model
title_sort quantum circuits for toric code and x cube fracton model
url https://quantum-journal.org/papers/q-2024-03-13-1276/pdf/
work_keys_str_mv AT penghuachen quantumcircuitsfortoriccodeandxcubefractonmodel
AT bowenyan quantumcircuitsfortoriccodeandxcubefractonmodel
AT shawnxcui quantumcircuitsfortoriccodeandxcubefractonmodel