{"as_of":"2026-08-23T00:05:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:48b0d45ef47adf8d9baf16d16ddc73108d0aacd655d19713aec625b5a74c9dde","coverage":[{"denominator":63,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":63,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-02T16:07:18.246040Z","state":"measured"},{"denominator":64,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":64,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-22T06:32:14.747728+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T01:17:54.895830Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.17874","snapshot_observed_at":"2026-08-04T01:17:54.895830Z","title":"Sekiyama and L","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.00165","last_updated":"2026-07-31T18:00:01Z","snapshot_observed_at":"2026-08-17T14:48:21.840397Z","submitted_at":"2026-07-31T18:00:01Z","title":"Arbitrary-Distance Quantum Error Correction with Gauss's Law for $\\mathbb Z_2$ Lattice Gauge Theory","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-04T01:17:54.895830Z"},"links":{"cited_paper":"/paper/2604.17874","citing_paper":"/paper/2608.00165"},"observation_digest":"sha256:5b6eec267fb934b3c8d322fe8327b5220f260e75b6401a4321e0a66ea5f99b81","observation_id":"59a4ec03-6c28-49ea-a8b6-cd56b84a2d3a","resolution":{"observed_at":"2026-08-04T01:17:54.895830Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2604.17874/citation-record","integrity":"/paper/2604.17874/integrity","json":"/paper/2604.17874/citation-record.json","paper":"/paper/2604.17874"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:17.980981Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:17.980981Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:0d5d678dc0925d42d6835ba3a315c6f56911e6112e98fa14b211393c51b1e2ee","observation_id":"d8cd48e5-77a4-47f6-aa93-91d9313cd41f","resolution":{"observed_at":"2026-08-02T16:07:17.980981Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:17.986001Z","title":"supportD partitionD=DX ⊔ D¯X YY Y Y Z Z Z Y YX I X X Pauli assignment forDX andD¯X FIG","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:17.986001Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:5346cbeecbcc7d5d1561f8761e88ba84e921fbd891c9dad83de9f0b862245e8c","observation_id":"fe2dc73d-9243-4a7a-b1b7-a8abd5200b09","resolution":{"observed_at":"2026-08-02T16:07:17.986001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.3633","last_updated":"2011-11-21T15:59:05Z","snapshot_observed_at":"2026-08-15T04:28:50.822364Z","submitted_at":"2011-11-15T20:48:13Z","title":"Quantum Algorithms for Quantum Field Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.3633","snapshot_observed_at":"2026-08-02T16:07:17.990939Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:17.990939Z"},"links":{"cited_paper":"/paper/1111.3633","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:73c26782cf44ad0755ea57c58212dffeef2a2c015fb7c8beb89e241d59aae28b","observation_id":"c715cd4a-5047-47a8-be34-6edb8585bc99","resolution":{"observed_at":"2026-08-02T16:07:17.990939Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.03381","last_updated":"2022-04-07T11:59:15Z","snapshot_observed_at":"2026-08-16T17:08:36.977912Z","submitted_at":"2022-04-07T11:59:15Z","title":"Quantum Simulation for High Energy Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.03381","snapshot_observed_at":"2026-08-02T16:07:17.995635Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:17.995635Z"},"links":{"cited_paper":"/paper/2204.03381","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:bdc62039a535a36dede4b4ba2934e42d8bc34e2db7ca0e5d0093f0cc8587d4f0","observation_id":"31c98337-3209-4f88-a06d-3c381920a2fe","resolution":{"observed_at":"2026-08-02T16:07:17.995635Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.03236","last_updated":"2023-07-06T18:01:02Z","snapshot_observed_at":"2026-08-17T21:01:01.758171Z","submitted_at":"2023-07-06T18:01:02Z","title":"Quantum Computing for High-Energy Physics: State of the Art and Challenges. Summary of the QC4HEP Working Group","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.03236","snapshot_observed_at":"2026-08-02T16:07:18.000618Z","title":"Di Meglioet al., Quantum Computing for High- Energy Physics: State of the Art and Challenges, PRX Quantum5, 037001 (2024), arXiv:2307.03236 [quant-ph]","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.000618Z"},"links":{"cited_paper":"/paper/2307.03236","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:7386c032fea4e79ca979686ce15a519926971182069048ac2dade0c854a7be4e","observation_id":"b365bdb5-2e5e-4602-a299-c2c34424778b","resolution":{"observed_at":"2026-08-02T16:07:18.000618Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.005320Z","title":"Davoudi, Tasi/cern/kitp lecture notes on” toward quantum computing gauge theories of nature”, arXiv preprint arXiv:2507.15840 (2025)","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.005320Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:5540fac2a0525b4bd4048f655f0cbdd42c1058ebb9d65b475eb1a018fb841874","observation_id":"cc79c465-0290-4b0b-bbaa-b5c3263dd729","resolution":{"observed_at":"2026-08-02T16:07:18.005320Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2509.03586","last_updated":"2025-09-03T18:00:29Z","snapshot_observed_at":"2026-08-14T13:38:38.720636Z","submitted_at":"2025-09-03T18:00:29Z","title":"Quantum simulation of out-of-equilibrium dynamics in gauge theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2509.03586","snapshot_observed_at":"2026-08-02T16:07:18.009576Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.009576Z"},"links":{"cited_paper":"/paper/2509.03586","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:14d817893fe15c5336df2fde9f73373711a3d29cc2842f9a4453ccb480f13a14","observation_id":"0aa8701d-9654-4580-a033-91c685533438","resolution":{"observed_at":"2026-08-02T16:07:18.009576Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.03023","last_updated":"2019-09-16T03:49:17Z","snapshot_observed_at":"2026-08-21T18:00:21.079545Z","submitted_at":"2018-04-09T14:36:50Z","title":"Variational ansatz-based quantum simulation of imaginary time evolution","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.03023","snapshot_observed_at":"2026-08-02T16:07:18.014017Z","title":"McArdle, T","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.014017Z"},"links":{"cited_paper":"/paper/1804.03023","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:ed87d41328bfe28f82272b3f9e905b6659ecdc72637862765fcb0d5dfd6a9d01","observation_id":"2637bdc7-58fd-4814-810b-47edb58164c2","resolution":{"observed_at":"2026-08-02T16:07:18.014017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.019054Z","title":"Gomes, A","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.019054Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:3bb10041c4717df67f6a927257d23d3139c392ac3cb96b35bb86ebdae8412934","observation_id":"918993b9-c317-4563-b124-492aea0ae32a","resolution":{"observed_at":"2026-08-02T16:07:18.019054Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.023251Z","title":"Gacon, J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.023251Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:7e135fc2c4a91d87f6518920b37d98debcd02b6b8d996527a01e2b191df10231","observation_id":"25953c5a-0c21-4fc5-854c-5a72fe4f3621","resolution":{"observed_at":"2026-08-02T16:07:18.023251Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.07653","last_updated":"2020-02-16T19:23:19Z","snapshot_observed_at":"2026-08-21T09:00:41.926559Z","submitted_at":"2019-01-23T00:01:34Z","title":"Determining eigenstates and thermal states on a quantum computer using quantum imaginary time evolution","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.07653","snapshot_observed_at":"2026-08-02T16:07:18.027586Z","title":"Motta, C","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.027586Z"},"links":{"cited_paper":"/paper/1901.07653","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:462d76b4a87b55df946359facb4466f38a1a80b7bd943fcc9315af6dfd68ba52","observation_id":"2c9e0ad0-4c18-4d41-ae02-4398439e40ec","resolution":{"observed_at":"2026-08-02T16:07:18.027586Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.032130Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.032130Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:e54b4155c5fe48fdbbd0eeca390cc71e5016b887e5ade996d1d89f998381db55","observation_id":"76e9cc39-4416-48d5-9938-aee351cd361b","resolution":{"observed_at":"2026-08-02T16:07:18.032130Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.06161","last_updated":"2023-04-11T08:55:39Z","snapshot_observed_at":"2026-08-21T18:07:58.096273Z","submitted_at":"2023-03-10T19:00:33Z","title":"Simulating non-unitary dynamics using quantum signal processing with unitary block encoding","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.06161","snapshot_observed_at":"2026-08-02T16:07:18.036095Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.036095Z"},"links":{"cited_paper":"/paper/2303.06161","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:1489ff1b136c54ba590521b53467bafb90a9f01ec07638eb16896748c668575d","observation_id":"3ee5ea8d-8cbf-4f98-bd34-4138a2cc3be6","resolution":{"observed_at":"2026-08-02T16:07:18.036095Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.00908","last_updated":"2026-07-14T09:43:29Z","snapshot_observed_at":"2026-08-06T21:00:27.600861Z","submitted_at":"2025-07-01T16:11:47Z","title":"Quantum Imaginary-Time Evolution with Polynomial Resources in Evolution Time","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.00908","snapshot_observed_at":"2026-08-02T16:07:18.040428Z","title":"Zhang, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.040428Z"},"links":{"cited_paper":"/paper/2507.00908","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:15bf9ecd6934098f05e5b816e5739ebea2100655890bfbc87e6ad53d5450a0f5","observation_id":"30554ddc-b5c5-46ec-ba6a-48a306045b23","resolution":{"observed_at":"2026-08-02T16:07:18.040428Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.045035Z","title":"Gluza, J","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.045035Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:048f2da2129d062efef97f312418f18d2e9ddd64ef576060def5b443da598eb5","observation_id":"d0da3345-4f9f-4282-a28f-e2f3faf624b3","resolution":{"observed_at":"2026-08-02T16:07:18.045035Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.09726","last_updated":"2020-09-02T10:05:17Z","snapshot_observed_at":"2026-08-15T00:19:07.912266Z","submitted_at":"2020-06-17T08:56:06Z","title":"Probabilistic Nonunitary Gate in Imaginary Time Evolution","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.09726","snapshot_observed_at":"2026-08-02T16:07:18.049528Z","title":"Liu, J.-G","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.049528Z"},"links":{"cited_paper":"/paper/2006.09726","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:02c55a63efcdce57bb1e491616cad62923d25ad9b9a98700fe0630543f7ac2f0","observation_id":"0a9d4507-f730-4aa8-8acd-d7cf98146789","resolution":{"observed_at":"2026-08-02T16:07:18.049528Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.053714Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.053714Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:f911b21496ef2f8b025c1dccb99e0a4358da36c6322119f5f2557b5c1c99c64a","observation_id":"186f073b-e70a-4912-a3c2-b53376f7185a","resolution":{"observed_at":"2026-08-02T16:07:18.053714Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.057690Z","title":"Kosugi, Y","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.057690Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:ebb37472e6fb72f59984557af5570b18a916c5b372a36ab55815390bd4d65867","observation_id":"c98e29b2-74da-4bfe-8cb2-38990a084ace","resolution":{"observed_at":"2026-08-02T16:07:18.057690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.00791","last_updated":"2021-07-02T01:45:29Z","snapshot_observed_at":"2026-08-16T18:12:51.611084Z","submitted_at":"2021-07-02T01:45:29Z","title":"Quantum Imaginary Time Evolution Algorithm for Quantum Field Theories with Continuous Variables","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.00791","snapshot_observed_at":"2026-08-02T16:07:18.062046Z","title":"Yeter-Aydeniz, E","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.062046Z"},"links":{"cited_paper":"/paper/2107.00791","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:3d0cce044ee33203e56629385f03ccde03d38e7cf398d1c3dd8673c4ae9517bb","observation_id":"1c1e3ce4-1c58-4d1d-9c59-9f2552a46f35","resolution":{"observed_at":"2026-08-02T16:07:18.062046Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.066561Z","title":"Yeter-Aydeniz, R","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.066561Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:addc409291cb76710432d8da34c1270378c2ba8a1105c4251fbf785730330652","observation_id":"ec756303-f471-430d-8288-25f7e81d0718","resolution":{"observed_at":"2026-08-02T16:07:18.066561Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.070599Z","title":"Gomes, F","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.070599Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:5ec00949859149aff6a106cdd6ec7671a84c09a411fb1d0c21914ba36bb2abac","observation_id":"b98f5eb7-7ce0-474d-8995-99f5d1906ca0","resolution":{"observed_at":"2026-08-02T16:07:18.070599Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.074966Z","title":"Nishi, T","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.074966Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:429a45629a65d25bc56e118edcb23d6252b56d531812399e543a745c8a390b4f","observation_id":"2988c652-a455-4bd4-8bae-557510bf3313","resolution":{"observed_at":"2026-08-02T16:07:18.074966Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.079541Z","title":"Huang, Y","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.079541Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:d76af045b778abe98f6c7a51b63881661b43c3a5b04b93bbb72f19b783455e5f","observation_id":"661b98ce-65ee-4f06-b23f-6cf83e6405a6","resolution":{"observed_at":"2026-08-02T16:07:18.079541Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2510.15781","last_updated":"2026-06-30T07:42:46Z","snapshot_observed_at":"2026-08-09T20:07:33.676909Z","submitted_at":"2025-10-17T16:04:06Z","title":"Adaptive time Compressed QITE (ACQ) and its geometrical interpretation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2510.15781","snapshot_observed_at":"2026-08-02T16:07:18.084062Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.084062Z"},"links":{"cited_paper":"/paper/2510.15781","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:468cf991219730c6b30e0396ca00c85be142f2e8c7ac9a9ed8f2a75e1d6be15a","observation_id":"17674351-7f0a-471e-8084-2962671a5d1a","resolution":{"observed_at":"2026-08-02T16:07:18.084062Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.03542","last_updated":"2020-09-08T06:49:08Z","snapshot_observed_at":"2026-08-17T20:36:44.565593Z","submitted_at":"2020-09-08T06:49:08Z","title":"Quantum Computation of Finite-Temperature Static and Dynamical Properties of Spin Systems Using Quantum Imaginary Time Evolution","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.03542","snapshot_observed_at":"2026-08-02T16:07:18.088285Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.088285Z"},"links":{"cited_paper":"/paper/2009.03542","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:6c83ee6a69637b3dcda4233ace12005ef09debb9f3e5cafbd6f8f56793c2aa20","observation_id":"600c408b-4b61-4cf2-8a49-85e7f7214108","resolution":{"observed_at":"2026-08-02T16:07:18.088285Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.11616","last_updated":"2023-11-20T09:00:10Z","snapshot_observed_at":"2026-08-16T14:41:56.005588Z","submitted_at":"2023-11-20T09:00:10Z","title":"Quantum Simulation of Finite Temperature Schwinger Model via Quantum Imaginary Time Evolution","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.11616","snapshot_observed_at":"2026-08-02T16:07:18.092572Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.092572Z"},"links":{"cited_paper":"/paper/2311.11616","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:6f73661963d9e8a4dbe7b88d7c4784e347d9eb2d47c9b41718e47f1db9204225","observation_id":"1620b0ed-34b2-49f3-920a-428cf4eb4135","resolution":{"observed_at":"2026-08-02T16:07:18.092572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.13112","last_updated":"2022-08-28T01:26:10Z","snapshot_observed_at":"2026-08-16T16:36:28.024371Z","submitted_at":"2022-08-28T01:26:10Z","title":"Toward Quantum Computing Phase Diagrams of Gauge Theories with Thermal Pure Quantum States","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.13112","snapshot_observed_at":"2026-08-02T16:07:18.097083Z","title":"Davoudi, N","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.097083Z"},"links":{"cited_paper":"/paper/2208.13112","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:51513e4172b0dfc983616be9e64216d0302b7469c3ad027c6301a0ea8d82143d","observation_id":"73dbaf62-ba84-498c-9372-f9b831c1182a","resolution":{"observed_at":"2026-08-02T16:07:18.097083Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2603.10932","last_updated":"2026-05-18T10:38:50Z","snapshot_observed_at":"2026-08-14T16:07:59.907982Z","submitted_at":"2026-03-11T16:17:10Z","title":"Gauge-invariant QMETTS with mutually unbiased physical bases for $Z_2$ lattice gauge theories at finite temperature and density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2603.10932","snapshot_observed_at":"2026-08-02T16:07:18.101269Z","title":"Maeno, Efficient construction ofZ 2 gauge-invariant bases for the quantum minimally entangled typical ther- mal states algorithm, arXiv preprint arXiv:2603.10932 (2026)","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.101269Z"},"links":{"cited_paper":"/paper/2603.10932","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:787ca86fc5a30fbc0572f7e795ef26bf2919c4acd8abe34c81021036d1773a55","observation_id":"26f02f8b-c1dc-425c-8dfa-346f414e3306","resolution":{"observed_at":"2026-08-02T16:07:18.101269Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.13598","last_updated":"2023-07-25T16:00:34Z","snapshot_observed_at":"2026-08-17T00:02:03.277818Z","submitted_at":"2023-07-25T16:00:34Z","title":"Symmetry enhanced variational quantum imaginary time evolution","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.13598","snapshot_observed_at":"2026-08-02T16:07:18.105333Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.105333Z"},"links":{"cited_paper":"/paper/2307.13598","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:b0e79624f3086337ad907f3d0619f9b4611639c3d888fc9eb12e3f29bdbb33a3","observation_id":"931218a7-4656-4fb1-8029-d1cba25ccd6b","resolution":{"observed_at":"2026-08-02T16:07:18.105333Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.109698Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.109698Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:91eac122d2c7d3ae650f86a208920a4a56429361745fbba514d25a1bee4e6049","observation_id":"5c6cdc6f-d8ff-4dbf-9395-a131dbf074ea","resolution":{"observed_at":"2026-08-02T16:07:18.109698Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.113666Z","title":null,"venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.113666Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:f1899d3b645394dd8731651adc4f5d25f0befaf150c0b96cc65e41f0793a2068","observation_id":"b9cd7ae1-3146-43b6-93e5-c5a9b32ccd87","resolution":{"observed_at":"2026-08-02T16:07:18.113666Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.117766Z","title":null,"venue":null,"work_id":null,"year":1971},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.117766Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:75c502551649fe3b9e909adc2ec2eb02018efcbddb11892bc3039fa882019f23","observation_id":"97350058-f9c3-42d1-b958-efb107ef8827","resolution":{"observed_at":"2026-08-02T16:07:18.117766Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.121698Z","title":null,"venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.121698Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:dbb3790d2b68e0cc4a6295c4cf3d3a8d35666dd65e151dd4309d024e250e90c6","observation_id":"6714825c-c6ce-4eab-bfae-dcae47a2c3ba","resolution":{"observed_at":"2026-08-02T16:07:18.121698Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.17929","last_updated":"2025-01-29T19:00:04Z","snapshot_observed_at":"2026-08-19T13:51:44.785936Z","submitted_at":"2025-01-29T19:00:04Z","title":"String Breaking in a $2+1$D $\\mathbb{Z}_2$ Lattice Gauge Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.17929","snapshot_observed_at":"2026-08-02T16:07:18.125724Z","title":"Borla, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.125724Z"},"links":{"cited_paper":"/paper/2501.17929","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:50f845371b61fb19b266acce03b3836ddde3e3b13e17c89aeda04159782b8f65","observation_id":"de791c61-a537-4f57-ac93-ddb1c55e9662","resolution":{"observed_at":"2026-08-02T16:07:18.125724Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.01950","last_updated":"2025-07-02T17:57:52Z","snapshot_observed_at":"2026-08-17T20:25:15.469415Z","submitted_at":"2025-07-02T17:57:52Z","title":"String Breaking Dynamics and Glueball Formation in a $2+1$D Lattice Gauge Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.01950","snapshot_observed_at":"2026-08-02T16:07:18.130249Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.130249Z"},"links":{"cited_paper":"/paper/2507.01950","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:3bd178030753be5fedcf52b96da2f59a68b1c4dd2c56897d9e47b4a6e9df0229","observation_id":"31aa8242-d995-415f-bb52-86c8b01e7a99","resolution":{"observed_at":"2026-08-02T16:07:18.130249Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0506009","last_updated":"2005-06-20T14:27:33Z","snapshot_observed_at":"2026-07-07T03:42:44.613480Z","submitted_at":"2005-06-07T20:09:13Z","title":"Matrix product representation of gauge invariant states in a Z_2 lattice gauge theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0506009","snapshot_observed_at":"2026-08-02T16:07:18.134539Z","title":"Sugihara, Matrix product representation of gauge in- variant states in aZ 2 lattice gauge theory, JHEP07, 022, arXiv:hep-lat/0506009","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.134539Z"},"links":{"cited_paper":"/paper/hep-lat/0506009","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:1319be928d9c66d12847addf9e7f5f19059c5bc5250c950d89679e04963b1e48","observation_id":"83c43311-e173-47b3-8e80-500c3ada92b6","resolution":{"observed_at":"2026-08-02T16:07:18.134539Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.4145","last_updated":"2011-04-11T19:12:24Z","snapshot_observed_at":"2026-08-15T05:13:07.798463Z","submitted_at":"2010-07-23T15:01:54Z","title":"Entanglement renormalization and gauge symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.4145","snapshot_observed_at":"2026-08-02T16:07:18.138970Z","title":"Tagliacozzo and G","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.138970Z"},"links":{"cited_paper":"/paper/1007.4145","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:bcc8b5da55918beb1630583d9ba09ba45f89de7ec542410727e30bb5aeaa3f7c","observation_id":"d7069132-1f55-4f7f-be02-91e5ea68a639","resolution":{"observed_at":"2026-08-02T16:07:18.138970Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.6543","last_updated":"2013-07-24T19:38:01Z","snapshot_observed_at":"2026-08-15T00:09:11.357103Z","submitted_at":"2013-07-24T19:38:01Z","title":"Exact blocking formulas for spin and gauge models","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.6543","snapshot_observed_at":"2026-08-02T16:07:18.143306Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.143306Z"},"links":{"cited_paper":"/paper/1307.6543","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:dfbbc91d19ed2e6eac63c03c88bbfd72834e9f2775682f067f3f556cc383bad4","observation_id":"b9d053c9-74aa-43ed-9364-56db1a3a2dbc","resolution":{"observed_at":"2026-08-02T16:07:18.143306Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.20566","last_updated":"2025-08-10T14:19:56Z","snapshot_observed_at":"2026-08-16T12:46:37.452019Z","submitted_at":"2025-03-26T14:04:21Z","title":"Accurate Gauge-Invariant Tensor Network Simulations for Abelian Lattice Gauge Theory in (2+1)D: ground state and real-time dynamics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.20566","snapshot_observed_at":"2026-08-02T16:07:18.147606Z","title":"Wu and W.-Y","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.147606Z"},"links":{"cited_paper":"/paper/2503.20566","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:c5256a09dbccb58aebbc1212804c9aeb1cf30c5bc64b79e367b70b9e1e571bd3","observation_id":"bc7d0a22-1296-40b3-9f3b-ebcd27c4c35f","resolution":{"observed_at":"2026-08-02T16:07:18.147606Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.19027","last_updated":"2025-07-18T21:28:51Z","snapshot_observed_at":"2026-08-16T12:47:14.345422Z","submitted_at":"2025-03-24T18:00:04Z","title":"Tensor-network study of the roughening transition in a (2 + 1)D $\\mathbb{Z}_2$ lattice gauge theory with matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.19027","snapshot_observed_at":"2026-08-02T16:07:18.152078Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.152078Z"},"links":{"cited_paper":"/paper/2503.19027","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:879c9c054e920b48f10915991d0bb67a3521f37376b557b49405cbc2151f75f7","observation_id":"ef017b29-cda6-4d49-948f-260b85b23dd8","resolution":{"observed_at":"2026-08-02T16:07:18.152078Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.17142","last_updated":"2025-07-01T01:46:37Z","snapshot_observed_at":"2026-08-16T13:15:23.985301Z","submitted_at":"2024-09-25T17:59:05Z","title":"Visualizing Dynamics of Charges and Strings in (2+1)D Lattice Gauge Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.17142","snapshot_observed_at":"2026-08-02T16:07:18.156221Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.156221Z"},"links":{"cited_paper":"/paper/2409.17142","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:3365e9e470867e02c6390edfa8f372f155efe1d75bbf3adab837bdcb8f492aaf","observation_id":"8ac996b8-17b5-45ad-904d-85e55ba888b0","resolution":{"observed_at":"2026-08-02T16:07:18.156221Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.11395","last_updated":"2021-02-01T09:16:16Z","snapshot_observed_at":"2026-08-11T20:52:26.219060Z","submitted_at":"2020-08-26T06:18:46Z","title":"Real-time simulation of (2+1)-dimensional lattice gauge theory on qubits","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.11395","snapshot_observed_at":"2026-08-02T16:07:18.160611Z","title":"Yamamoto, Real-time simulation of (2+1)- dimensional lattice gauge theory on qubits, PTEP 2021, 013B06 (2021), arXiv:2008.11395 [hep-lat]","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.160611Z"},"links":{"cited_paper":"/paper/2008.11395","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:fdaacf28aa1fdc1c60984e30c5487268c577378eb386ebaec86eef027d5d034b","observation_id":"286eab95-fb0a-44b6-88ff-82f3c45a10d6","resolution":{"observed_at":"2026-08-02T16:07:18.160611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.165056Z","title":"Alexandrou, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.165056Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:516a0a4e408077faf6d5ccc9d0ec94cc652d9cb8c4b37a75bd36cea8de7bee2d","observation_id":"16aec55b-a551-4fd5-87e7-92b9629cbb7f","resolution":{"observed_at":"2026-08-02T16:07:18.165056Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.19203","last_updated":"2026-07-24T10:50:27Z","snapshot_observed_at":"2026-08-17T22:46:03.563560Z","submitted_at":"2025-07-25T12:16:02Z","title":"Barren-plateau free variational quantum simulation of Z2 lattice gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.19203","snapshot_observed_at":"2026-08-02T16:07:18.169066Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.169066Z"},"links":{"cited_paper":"/paper/2507.19203","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:1ce55736c517c96dc1e9be8e6dae9ae0777084ef3e04c49801743fbb7374a9bb","observation_id":"06358abb-6a95-4ef8-be6d-5a64e7255a32","resolution":{"observed_at":"2026-08-02T16:07:18.169066Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.07435","last_updated":"2026-04-08T18:00:00Z","snapshot_observed_at":"2026-07-06T22:55:41.978450Z","submitted_at":"2026-04-08T18:00:00Z","title":"Observation of glueball excitations and string breaking in a $2+1$D $\\mathbb{Z}_2$ lattice gauge theory on a trapped-ion quantum computer","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.07435","snapshot_observed_at":"2026-08-02T16:07:18.172963Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.172963Z"},"links":{"cited_paper":"/paper/2604.07435","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:99661a91535612b5ec5291af676bbcb536ca52d9bfee68342f1dd7c9ab8618fa","observation_id":"5b3250c7-ecbb-4e69-99e6-bfc1e630b803","resolution":{"observed_at":"2026-08-02T16:07:18.172963Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.177043Z","title":"Emonts, A","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.177043Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:e15661ca1c32fb270ef92a665f7798adca3b4a5779f0f1c401571cbdaddd0c20","observation_id":"d4917d07-aa3d-4831-b117-e045ffa276e4","resolution":{"observed_at":"2026-08-02T16:07:18.177043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.180942Z","title":"Irmejs, M.-C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.180942Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:6679688554896167bdc1fa391b3291f4e91fc2eb406c4e3cdd8ccf1502f77040","observation_id":"c22e01f3-c2c0-4381-bb75-c35d65bb5edc","resolution":{"observed_at":"2026-08-02T16:07:18.180942Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.184830Z","title":"Lumia, P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.184830Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:62a11ecf4e14baf9452cc5eec47e4fe755901a6ac7ecc8003b53369591033373","observation_id":"60019613-b741-4c99-84f2-5ba13bc5285a","resolution":{"observed_at":"2026-08-02T16:07:18.184830Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.08088","last_updated":"2025-07-10T18:01:27Z","snapshot_observed_at":"2026-08-18T02:20:52.875611Z","submitted_at":"2025-07-10T18:01:27Z","title":"Real-Time Dynamics in a (2+1)-D Gauge Theory: The Stringy Nature on a Superconducting Quantum Simulator","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.08088","snapshot_observed_at":"2026-08-02T16:07:18.188764Z","title":"Cobos, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.188764Z"},"links":{"cited_paper":"/paper/2507.08088","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:e94079d45f5f891935588cf657264e6a9b9286fea4a6daa00637003a8c7069b6","observation_id":"7edffc8e-a1d0-4f84-bf7f-7dafa74d058e","resolution":{"observed_at":"2026-08-02T16:07:18.188764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.192893Z","title":"Mueller, T","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.192893Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:ccd1f2d90192a08d85e190aa97d0e52d931af2f7454c6fd12d458613904dcba3","observation_id":"55ee3daf-3080-4c5e-9241-0334f2cd1122","resolution":{"observed_at":"2026-08-02T16:07:18.192893Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.13410","last_updated":"2022-03-13T05:45:56Z","snapshot_observed_at":"2026-08-17T03:23:39.028808Z","submitted_at":"2021-08-27T07:08:35Z","title":"Digital quantum simulation and Pseudoquantum Simulation of $\\mathbb{Z}_2$ Gauge Higgs Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.13410","snapshot_observed_at":"2026-08-02T16:07:18.197005Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.197005Z"},"links":{"cited_paper":"/paper/2108.13410","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:7ba7bb2634f064712ac969f7eb19ec72884df42491eaa5b3fb81c0fb55af700e","observation_id":"6b3ec060-74e1-458b-a8b1-7e4488d1fb58","resolution":{"observed_at":"2026-08-02T16:07:18.197005Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.201099Z","title":"Wiese, Ultracold quantum gases and lattice sys- tems: quantum simulation of lattice gauge theories, An- nalen der Physik525, 777 (2013)","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.201099Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:a96917ef5d755a06428f1c3b5ef5c7747cfd2158e243478884303ca78f0ca054","observation_id":"6186c292-fa73-4d46-89b6-66989f33e79a","resolution":{"observed_at":"2026-08-02T16:07:18.201099Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.23853","last_updated":"2025-05-29T01:56:52Z","snapshot_observed_at":"2026-08-19T01:54:53.360457Z","submitted_at":"2025-05-29T01:56:52Z","title":"Roughening and dynamics of an electric flux string in a (2+1)D lattice gauge theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.23853","snapshot_observed_at":"2026-08-02T16:07:18.205169Z","title":"Di Marcantonio, S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.205169Z"},"links":{"cited_paper":"/paper/2505.23853","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:41f78903074af29a3d892f66c3ed7ca80b3da68d2776178b2264742bc362a792","observation_id":"d0b2ad06-9fd1-4fda-8aa5-b4fdeeab4aeb","resolution":{"observed_at":"2026-08-02T16:07:18.205169Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.209160Z","title":"Homeier, A","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.209160Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:ab0a7b92233b2e4d7045d32ed0f47f358f251088c1510e8f1f58084991a9b260","observation_id":"38478f8d-705d-4672-8b46-2ae2eab9d949","resolution":{"observed_at":"2026-08-02T16:07:18.209160Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.213271Z","title":"Gonz´ alez-Cuadra, L","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.213271Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:45e7a19e417bc3fde611b4793393e1bb8332a78e1f8c0b684fe472f219a65e0f","observation_id":"f76b63c9-26c9-423d-b688-38c7cf93b8d7","resolution":{"observed_at":"2026-08-02T16:07:18.213271Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.217098Z","title":"Sukeno and T","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.217098Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:6afba69f34c02008d4aed7ef2ac071c8f2891fdcc3975f6f2eeaecc15a49f3f1","observation_id":"707a334c-3705-488e-a7c3-e0409b4ade58","resolution":{"observed_at":"2026-08-02T16:07:18.217098Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.221379Z","title":"Borla, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.221379Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:80c50639c54cff00ae140f34623ca8445e22989b80379eb61ef7e035e25dca67","observation_id":"cd05970a-bd0e-4033-9440-c8aa3783a570","resolution":{"observed_at":"2026-08-02T16:07:18.221379Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.225580Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.225580Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:109707802f776b99d5d23426badb399bdf630a0f8dadf4047ce8600dc6c9ce9d","observation_id":"3a9c00da-32ba-4c03-b002-894a1b934d3c","resolution":{"observed_at":"2026-08-02T16:07:18.225580Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.229647Z","title":"Kogut and L","venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.229647Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:6e311241493f16f8a2a3619b0bb3978721b62fb51c00b224e97c8083f9841016","observation_id":"5d20b683-3ff8-45d3-82b7-eb5d509e7fce","resolution":{"observed_at":"2026-08-02T16:07:18.229647Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.233656Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.233656Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:59564df34640c1de67d99321d96fe23a2a1b834bc2d105a12b0d4b02b109d11a","observation_id":"ba6a383e-ad36-4966-88d8-046222a3cc7a","resolution":{"observed_at":"2026-08-02T16:07:18.233656Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"quant-ph/0110143","last_updated":"2001-10-24T20:02:14Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2001-10-24T20:02:14Z","title":"Topological quantum memory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"quant-ph/0110143","snapshot_observed_at":"2026-08-02T16:07:18.237715Z","title":"Dennis, A","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.237715Z"},"links":{"cited_paper":"/paper/quant-ph/0110143","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:e2c757e62d48e2dbb96a762ab207c45999e31a27e8701a163f749e9ce59b40ed","observation_id":"56941caa-cc73-4c8b-8ac5-7c1aadeb890d","resolution":{"observed_at":"2026-08-02T16:07:18.237715Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"quant-ph/0310089","last_updated":"2003-10-14T01:57:22Z","snapshot_observed_at":"2026-08-19T13:36:49.794405Z","submitted_at":"2003-10-14T01:57:22Z","title":"Efficient simulation of one-dimensional quantum many-body systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"quant-ph/0310089","snapshot_observed_at":"2026-08-02T16:07:18.241925Z","title":"Vidal, Efficient simulation of one-dimensional quan- tum many-body systems, Phys","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.241925Z"},"links":{"cited_paper":"/paper/quant-ph/0310089","citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:b63cb6e6031c54f4889bf2c1caa70c98cbeccaa7d725427cde04c96ce943c550","observation_id":"e8c9d023-9f4b-4e6f-88d9-2223bcf43eeb","resolution":{"observed_at":"2026-08-02T16:07:18.241925Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T16:07:18.246040Z","title":"Fishman, S","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution","version":3},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-02T16:07:18.246040Z"},"links":{"citing_paper":"/paper/2604.17874"},"observation_digest":"sha256:7df1995784b72bc04b0c37bcbf78a1a93d3ecb2f7d20f6c3739a61b62c892d21","observation_id":"540939d6-e8f6-490b-b582-8f47c2a64dae","resolution":{"observed_at":"2026-08-02T16:07:18.246040Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2604.17874","last_updated":"2026-07-22T08:37:09Z","latest_version":3,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-15T00:24:38.027771Z","submitted_at":"2026-04-20T06:37:05Z","title":"Ground state preparation in $(2+1)$-dimensional pure $\\mathbb{Z}_2$ lattice gauge theory via deterministic quantum imaginary time evolution"},"reference_resolution":{"displayed":63,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":63,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":63},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+00:00","source":"retraction_watch"}],"thesis":"As of 23 August 2026, this Paper Citation Record lists 63 of 63 outbound references and 1 inbound Pith citation observation for arXiv:2604.17874."}