{"as_of":"2026-08-23T08:25:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:56fd77464a9d92338659e55f8c59cd5e297c40189e19fbae894b186826fa4509","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":25,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":25,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-23T06:30:58.430688+00:00","state":"measured"},{"denominator":25,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":25,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-16T12:06:26.605202Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-07-09T19:16:27.841086Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-12T19:35:19.549578Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.10652","last_updated":"2026-05-26T10:39:09Z","snapshot_observed_at":"2026-08-19T22:16:31.304828Z","submitted_at":"2024-11-16T01:18:27Z","title":"String-Breaking Dynamics in Quantum Adiabatic and Diabatic Processes","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-12T19:35:19.549578Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2411.10652"},"observation_digest":"sha256:e6e6040e4fda5e0199adffe22ecfd9e867e9ac1e6dc9d4b92b1770496f41e1b2","observation_id":"49873568-58bb-4de8-9771-0e1e755fb2da","resolution":{"observed_at":"2026-08-12T19:35:19.549578Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-10T22:51:15.783277Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.00604","last_updated":"2025-07-28T08:53:00Z","snapshot_observed_at":"2026-08-18T12:03:47.296622Z","submitted_at":"2024-12-31T19:00:06Z","title":"String breaking dynamics in Ising chain with local vibrations","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-10T22:51:15.783277Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2501.00604"},"observation_digest":"sha256:35ba0b3c58cef26c64bca36e1a6f99ac57d18731b784d3c44418a0562c647e3c","observation_id":"5cd99989-99b4-4449-b14c-4671950aa637","resolution":{"observed_at":"2026-08-10T22:51:15.783277Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-10T00:03:59.955474Z","title":"Ciavarella,String Breaking in the Heavy Quark Limit with Scalable Circuits, 2411.05915","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.18301","last_updated":"2025-02-17T14:11:23Z","snapshot_observed_at":"2026-08-18T09:38:04.529710Z","submitted_at":"2025-01-30T12:22:11Z","title":"Tensor-network toolbox for probing dynamics of non-Abelian gauge theories","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-10T00:03:59.955474Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2501.18301"},"observation_digest":"sha256:ba8a4d00417df75a285e1f2c6424777843528ce24d02628e54bd1b8f2fc4f0f1","observation_id":"81744e72-f42c-403e-8d27-71b206f04999","resolution":{"observed_at":"2026-08-10T00:03:59.955474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-09T12:01:56.456387Z","title":"String breaking in the heavy quark limit with scalable circuits","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.02502","last_updated":"2025-02-04T17:16:16Z","snapshot_observed_at":"2026-08-13T19:56:02.122052Z","submitted_at":"2025-02-04T17:16:16Z","title":"Developing techniques for Simulation of SU(3) Quantum Field Theories on State-of-the-Art Quantum Devices","version":1},"reference_index":173,"source":"pdf_text","source_observed_at":"2026-08-09T12:01:56.456387Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2502.02502"},"observation_digest":"sha256:1988397445fa6bcd783272684b4b1b2330bc203295f42f3ebbc86dd63ad890c8","observation_id":"90b4e06e-a475-45d1-8aaf-6f8fb28546b9","resolution":{"observed_at":"2026-08-09T12:01:56.456387Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-16T12:06:26.605202Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13760","last_updated":"2025-04-18T15:52:31Z","snapshot_observed_at":"2026-08-21T03:54:42.529410Z","submitted_at":"2025-04-18T15:52:31Z","title":"Realizing string breaking dynamics in a $Z_2$ lattice gauge theory on quantum hardware","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-16T12:06:26.605202Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2504.13760"},"observation_digest":"sha256:7b586cc7784358cc6b687b8c19f2dfb593f4444e5dda105b48bf5c03cfbef279","observation_id":"f781137d-207e-40a6-8855-987291199130","resolution":{"observed_at":"2026-08-16T12:06:26.605202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-16T10:57:23.689949Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.17000","last_updated":"2025-04-23T18:00:04Z","snapshot_observed_at":"2026-08-18T22:17:50.776746Z","submitted_at":"2025-04-23T18:00:04Z","title":"Bosonic vs. Fermionic Matter in Quantum Simulations of $2+1$D Gauge Theories","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-16T10:57:23.689949Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2504.17000"},"observation_digest":"sha256:de5775533b14964d930fdfe4a1b607a266c5d598ba90473c432f4e57d2c123cf","observation_id":"8623d634-2af0-4862-8496-125867c2ba5d","resolution":{"observed_at":"2026-08-16T10:57:23.689949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2505.04704","last_updated":"2026-05-21T17:13:44Z","snapshot_observed_at":"2026-08-15T04:14:22.486764Z","submitted_at":"2025-05-07T18:00:42Z","title":"Disorder-Free Localization and Fragmentation in a Non-Abelian Lattice Gauge Theory","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-05-22T16:42:43.646374Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2505.04704"},"observation_digest":"sha256:d4b04b3748343f94d0aac49d1019268f24423d760baca5c4bbfa04a16865c2ec","observation_id":"37536cad-7d7f-47cf-b782-92055cf690a6","resolution":{"observed_at":"2026-05-22T16:44:59.996124Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-15T21:34:11.758553Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.09607","last_updated":"2025-05-14T17:57:25Z","snapshot_observed_at":"2026-08-19T14:35:11.088429Z","submitted_at":"2025-05-14T17:57:25Z","title":"Quantum simulation of bubble nucleation across a quantum phase transition","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-15T21:34:11.758553Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2505.09607"},"observation_digest":"sha256:c92d228e784060a2d235e109cc80370a04c801488d5418d8252a8657430c096d","observation_id":"c08b8c95-f20e-4846-a6c3-2ef93aabdea0","resolution":{"observed_at":"2026-08-15T21:34:11.758553Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-07T13:59:56.436675Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.20387","last_updated":"2025-05-26T18:00:00Z","snapshot_observed_at":"2026-08-16T12:25:25.279382Z","submitted_at":"2025-05-26T18:00:00Z","title":"Observation of hadron scattering in a lattice gauge theory on a quantum computer","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-07T13:59:56.436675Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2505.20387"},"observation_digest":"sha256:dd0475f2b90eff8c9c491d25fd3d4e8c6f44ee0078b56e10d24992676e6cee6f","observation_id":"6cc17913-65b9-48b9-a589-73f78f5a9cb4","resolution":{"observed_at":"2026-08-07T13:59:56.436675Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-07T14:02:15.469466Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.20408","last_updated":"2025-05-26T18:00:49Z","snapshot_observed_at":"2026-08-12T14:10:49.199204Z","submitted_at":"2025-05-26T18:00:49Z","title":"Quantum computation of hadron scattering in a lattice gauge theory","version":1},"reference_index":193,"source":"pdf_text","source_observed_at":"2026-08-07T14:02:15.469466Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2505.20408"},"observation_digest":"sha256:3e9180a25ef4d5f091e1bdf86102a963fe6f64d9d0ecd65f9cd0f88d5a82ba88","observation_id":"9b4a1fad-15bb-42ab-bc22-0318697eed04","resolution":{"observed_at":"2026-08-07T14:02:15.469466Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-07T12:08:17.955974Z","title":"String breaking in the heavy quark limit with scalable circuits,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2506.00755","last_updated":"2026-06-23T15:29:30Z","snapshot_observed_at":"2026-08-13T19:36:43.637391Z","submitted_at":"2025-05-31T23:50:27Z","title":"Exponential speedup in quantum simulation of Kogut-Susskind Hamiltonian via orbifold lattice","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-07T12:08:17.955974Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2506.00755"},"observation_digest":"sha256:7662505d5e181248497d172e7059eb17b800079c54bb7e168b7bf1805da727b9","observation_id":"cc790813-3349-41f3-b82a-13a5f83fd8fc","resolution":{"observed_at":"2026-08-07T12:08:17.955974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-15T19:32:48.931158Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2506.16559","last_updated":"2025-06-19T19:28:21Z","snapshot_observed_at":"2026-08-16T12:25:26.716434Z","submitted_at":"2025-06-19T19:28:21Z","title":"Obtaining continuum physics from dynamical simulations of Hamiltonian lattice gauge theories","version":1},"reference_index":110,"source":"pdf_text","source_observed_at":"2026-08-15T19:32:48.931158Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2506.16559"},"observation_digest":"sha256:f42a489502d5d9d8eb28e8d31c77da9c901b3cb18c77a67fab87b226d256124e","observation_id":"b2d79f57-6a5c-45c1-acec-74d05b47ea67","resolution":{"observed_at":"2026-08-15T19:32:48.931158Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-15T18:50:17.442544Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.18966","last_updated":"2025-06-23T18:00:00Z","snapshot_observed_at":"2026-08-16T12:32:06.165659Z","submitted_at":"2025-06-23T18:00:00Z","title":"Universal framework with exponential speedup for the quantum simulation of quantum field theories including QCD","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-15T18:50:17.442544Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2506.18966"},"observation_digest":"sha256:f566372e638b640b2fb83bc95ad468f4d42884b5f5b9eae7da238a13bd1a7836","observation_id":"ddabe949-507f-4bc9-81a4-97f8e28ab57e","resolution":{"observed_at":"2026-08-15T18:50:17.442544Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-06T20:53:51.028427Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_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},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T20:53:51.028427Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2507.01950"},"observation_digest":"sha256:a17419acd962d4309d74701e2a87fdaaa3593ed15be4921f509764551b4c5919","observation_id":"a0b823f0-7113-4d08-80ce-4fc0967435e2","resolution":{"observed_at":"2026-08-06T20:53:51.028427Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-06T16:56:33.299383Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.12589","last_updated":"2025-07-16T19:16:49Z","snapshot_observed_at":"2026-08-13T19:28:55.734750Z","submitted_at":"2025-07-16T19:16:49Z","title":"Efficient Qudit Circuit for Quench Dynamics of $2+1$D Quantum Link Electrodynamics","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-06T16:56:33.299383Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2507.12589"},"observation_digest":"sha256:b686119a61485a494401164abd84643ac664a0e14a003312fe5e34d2719a29e9","observation_id":"06b8c943-cd16-4d18-b8be-0aaf10edd783","resolution":{"observed_at":"2026-08-06T16:56:33.299383Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-06T16:50:03.384022Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.12614","last_updated":"2025-07-16T20:15:36Z","snapshot_observed_at":"2026-08-12T14:11:33.130172Z","submitted_at":"2025-07-16T20:15:36Z","title":"Probing Hadron Scattering in Lattice Gauge Theories on Qudit Quantum Computers","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T16:50:03.384022Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2507.12614"},"observation_digest":"sha256:0f1a24210d79d2c32f39f1a07d1f78c8de5c260bb451d94bbb723e238d02c5a2","observation_id":"cdc98456-4d79-4347-bd7f-c51e66f4b6d8","resolution":{"observed_at":"2026-08-06T16:50:03.384022Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2511.00154","last_updated":"2026-05-12T11:54:39Z","snapshot_observed_at":"2026-08-17T09:14:10.518415Z","submitted_at":"2025-10-31T18:00:46Z","title":"Hadronic scattering in (1+1)D SU(2) lattice gauge theory from tensor networks","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-05-18T02:22:05.111871Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2511.00154"},"observation_digest":"sha256:9713fcaa7ccbe5855e5464e41393fbe7fb51334146a14024253637820bd7a5de","observation_id":"81a6dd0e-2f2c-421c-b708-708f9dc70d8d","resolution":{"observed_at":"2026-05-18T02:22:18.767012Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2512.05210","last_updated":"2026-04-13T22:53:29Z","snapshot_observed_at":"2026-08-11T04:27:30.333121Z","submitted_at":"2025-12-04T19:31:09Z","title":"A Framework for Quantum Simulations of Energy-Loss and Hadronization in Non-Abelian Gauge Theories: SU(2) Lattice Gauge Theory in 1+1D","version":3},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-05-17T01:03:51.668159Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2512.05210"},"observation_digest":"sha256:73c2db726061ee6cca51b613b1eb78ca58a50d569923ee488b81f9d76c1e087c","observation_id":"165d8a54-2119-47c0-95b4-05227e85b423","resolution":{"observed_at":"2026-05-17T01:08:48.269401Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2601.08825","last_updated":"2026-04-13T22:01:35Z","snapshot_observed_at":"2026-08-15T09:59:45.563563Z","submitted_at":"2026-01-13T18:57:53Z","title":"The Quantum Complexity of String Breaking in the Schwinger Model","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-16T14:36:15.190389Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2601.08825"},"observation_digest":"sha256:4bfbc117c0dd16ffdfa806f81749f9547a7b72faebcf958dc82f49bd86b9bd52","observation_id":"67fd894c-33d3-466f-a0c3-8ccb176f674b","resolution":{"observed_at":"2026-05-16T14:38:00.346986Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2603.23948","last_updated":"2026-07-31T15:10:43Z","snapshot_observed_at":"2026-08-19T18:33:50.311485Z","submitted_at":"2026-03-25T05:09:36Z","title":"Local Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-05-15T01:07:14.594657Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2603.23948"},"observation_digest":"sha256:fd17c2db8c699b14559830f05f48b4d32596d38bae85b970fceb80882b24206b","observation_id":"604064dd-2cd8-4d18-8d52-deaa093014ec","resolution":{"observed_at":"2026-05-15T01:08:25.422882Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-03T02:32:39.651755Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2603.23948","last_updated":"2026-07-31T15:10:43Z","snapshot_observed_at":"2026-08-19T18:33:50.311485Z","submitted_at":"2026-03-25T05:09:36Z","title":"Local Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-03T02:32:39.651755Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2603.23948"},"observation_digest":"sha256:24bd0b903100beec0c88ea6a5f3209fc28f7a7cdda186889c1152cb9b093935d","observation_id":"8421a24d-1251-4547-bff7-49a8cdcfab52","resolution":{"observed_at":"2026-08-03T02:32:39.651755Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2605.04210","last_updated":"2026-07-24T17:20:56Z","snapshot_observed_at":"2026-08-15T20:15:59.720085Z","submitted_at":"2026-05-05T18:48:47Z","title":"Nonlocal Nonstabilizerness from Holographic Schwinger Pair Production","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-05-08T17:28:37.365629Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2605.04210"},"observation_digest":"sha256:487633a63c28299ae584df06e17d843a025ec2e908308b42176cae522a4c333e","observation_id":"6373ea41-ca48-45ef-a844-af99cd691666","resolution":{"observed_at":"2026-05-11T17:31:08.387690Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-02T15:00:13.043935Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2605.04210","last_updated":"2026-07-24T17:20:56Z","snapshot_observed_at":"2026-08-15T20:15:59.720085Z","submitted_at":"2026-05-05T18:48:47Z","title":"Nonlocal Nonstabilizerness from Holographic Schwinger Pair Production","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-02T15:00:13.043935Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2605.04210"},"observation_digest":"sha256:072f744c1530701cb4e9285e8ae7c4f8470f63a10e75e506822f904793bd47fb","observation_id":"858d2457-3575-4947-bfd2-7d1227597459","resolution":{"observed_at":"2026-08-02T15:00:13.043935Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":"2411.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-07-09T19:16:27.841086Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","venue":"quant-ph","work_id":"efe072f0-c557-4539-9160-ce6231db0b41","year":2024},"citing_paper":{"arxiv_id":"2607.07143","last_updated":"2026-07-08T08:37:32Z","snapshot_observed_at":"2026-07-11T23:18:56.751737Z","submitted_at":"2026-07-08T08:37:32Z","title":"Hints for string breaking in QCD","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-07-09T19:08:55.847030Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2607.07143"},"observation_digest":"sha256:fa9c913b3ba08ad711e0738c39af2e8da71bc95f21b674ef69c3db7193da9748","observation_id":"b48c1995-d32e-40e7-8798-89a3ca49e40a","resolution":{"observed_at":"2026-07-09T19:16:27.843517Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05915","snapshot_observed_at":"2026-08-01T05:56:53.655427Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.27550","last_updated":"2026-07-30T00:50:25Z","snapshot_observed_at":"2026-08-20T00:37:55.375143Z","submitted_at":"2026-07-30T00:50:25Z","title":"Confinement and String Breaking in the Compact Abelian Higgs Model","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-01T05:56:53.655427Z"},"links":{"cited_paper":"/paper/2411.05915","citing_paper":"/paper/2607.27550"},"observation_digest":"sha256:d340167e0c6de2a8d2a5401a1d501741a9ed4c64fa5b059efd32cfa9bf53b823","observation_id":"407c114f-63e1-4649-9073-71072ca94706","resolution":{"observed_at":"2026-08-01T05:56:53.655427Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2411.05915/citation-record","integrity":"/paper/2411.05915/integrity","json":"/paper/2411.05915/citation-record.json","paper":"/paper/2411.05915"},"outbound":[],"paper":{"arxiv_id":"2411.05915","last_updated":"2025-02-10T22:00:56Z","latest_version":2,"primary_category":"quant-ph","snapshot_observed_at":"2026-08-21T11:42:30.448733Z","submitted_at":"2024-11-08T19:00:27Z","title":"String Breaking in the Heavy Quark Limit with Scalable Circuits"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"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":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"thesis":"As of 23 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 25 inbound Pith citation observations for arXiv:2411.05915."}