{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,9,24]],"date-time":"2025-09-24T08:47:06Z","timestamp":1758703626223},"reference-count":23,"publisher":"Verein zur Forderung des Open Access Publizierens in den Quantenwissenschaften","license":[{"start":{"date-parts":[[2024,3,13]],"date-time":"2024-03-13T00:00:00Z","timestamp":1710288000000},"content-version":"unspecified","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"funder":[{"name":"NSF CCF","award":["006667"],"award-info":[{"award-number":["006667"]}]}],"content-domain":{"domain":["quantum-journal.org"],"crossmark-restriction":false},"short-container-title":["Quantum"],"abstract":"<jats:p>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 <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mo fence=\"false\" stretchy=\"false\">&amp;#x2308;<\/mml:mo><mml:mn>2<\/mml:mn><mml:mi>L<\/mml:mi><mml:mo>+<\/mml:mo><mml:mn>2<\/mml:mn><mml:mo>+<\/mml:mo><mml:mi>l<\/mml:mi><mml:mi>o<\/mml:mi><mml:msub><mml:mi>g<\/mml:mi><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msub><mml:mo stretchy=\"false\">(<\/mml:mo><mml:mi>d<\/mml:mi><mml:mo stretchy=\"false\">)<\/mml:mo><mml:mo>+<\/mml:mo><mml:mfrac><mml:mi>L<\/mml:mi><mml:mrow><mml:mn>2<\/mml:mn><mml:mi>d<\/mml:mi><\/mml:mrow><\/mml:mfrac><mml:mo fence=\"false\" stretchy=\"false\">&amp;#x2309;<\/mml:mo><\/mml:math> time steps, where <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>L<\/mml:mi><\/mml:math> refers to the system size and <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>d<\/mml:mi><\/mml:math> 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 <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>3<\/mml:mn><mml:mi>L<\/mml:mi><mml:mo>+<\/mml:mo><mml:mn>8<\/mml:mn><\/mml:math> steps and the X-cube fracton model in <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>12<\/mml:mn><mml:mi>L<\/mml:mi><mml:mo>+<\/mml:mo><mml:mn>11<\/mml:mn><\/mml:math> 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.<\/jats:p>","DOI":"10.22331\/q-2024-03-13-1276","type":"journal-article","created":{"date-parts":[[2024,3,13]],"date-time":"2024-03-13T11:07:55Z","timestamp":1710328075000},"page":"1276","update-policy":"http:\/\/dx.doi.org\/10.22331\/q-crossmark-policy-page","source":"Crossref","is-referenced-by-count":2,"title":["Quantum circuits for toric code and X-cube fracton model"],"prefix":"10.22331","volume":"8","author":[{"given":"Penghua","family":"Chen","sequence":"first","affiliation":[{"name":"Department of Physics and Astronomy, Purdue University, West Lafayette"}]},{"given":"Bowen","family":"Yan","sequence":"additional","affiliation":[{"name":"Department of Physics and Astronomy, Purdue University, West Lafayette"}]},{"given":"Shawn X.","family":"Cui","sequence":"additional","affiliation":[{"name":"Department of Physics and Astronomy, Purdue University, West Lafayette"},{"name":"Department of Mathematics, Purdue University, West Lafayette"}]}],"member":"9598","published-online":{"date-parts":[[2024,3,13]]},"reference":[{"key":"0","doi-asserted-by":"publisher","unstructured":"Miguel Aguadoand Guifre Vidal ``Entanglement renormalization and topological order&apos;&apos; 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