{"as_of":"2026-08-13T09:22:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:34739116653b3ac03e71704335c2c8541d70fba79873a81e06d9e5f70777490b","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":13,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":13,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":13,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":13,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T14:24:22.509507Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-04T07:19:38.487392Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-08-11T14:24:22.509507Z","title":"Frellesvig, The Loop-by-Loop Baikov Representation – Strategies and Implementation, 2412.01804","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.12057","last_updated":"2025-04-06T20:54:34Z","snapshot_observed_at":"2026-08-12T22:03:40.838147Z","submitted_at":"2024-12-16T18:32:32Z","title":"Calabi-Yau Feynman integrals in gravity: $\\varepsilon$-factorized form for apparent singularities","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-11T14:24:22.509507Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2412.12057"},"observation_digest":"sha256:0632363bc8d0cc4500ec3d1297af0f7cbf1932607729e3f19b97f487e6dab1e8","observation_id":"48bf9464-be32-4e40-a5bc-1802d328d200","resolution":{"observed_at":"2026-08-11T14:24:22.509507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-08-05T23:39:00.017332Z","title":"The loop-by-loop Baikov representation — Strategies and implementa- tion","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.05043","last_updated":"2025-08-07T05:53:15Z","snapshot_observed_at":"2026-08-10T04:28:13.242012Z","submitted_at":"2025-08-07T05:53:15Z","title":"Constitutive modeling of viscoelastic solids at large strains based on the theory of evolving natural configurations","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-05T23:39:00.017332Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2508.05043"},"observation_digest":"sha256:1da9845b57beca7589f13dbb97039c4fc48126a35e0947885b0159bdc2d1a9ab","observation_id":"81b3a1e7-46a8-417f-96f5-800e5e615186","resolution":{"observed_at":"2026-08-05T23:39:00.017332Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2511.15381","last_updated":"2026-05-11T16:23:12Z","snapshot_observed_at":"2026-07-06T22:36:24.466921Z","submitted_at":"2025-11-19T12:16:15Z","title":"New algorithms for Feynman integral reduction and $\\varepsilon$-factorised differential equations","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-05-17T20:59:19.615643Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2511.15381"},"observation_digest":"sha256:e6924b48083066757df1084b6b997accab73efb567260c4cd6526a21b95fa43a","observation_id":"b93a04fb-392b-4c6d-809f-4e84a3939206","resolution":{"observed_at":"2026-05-17T21:00:15.496375Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2512.13794","last_updated":"2026-05-11T15:09:48Z","snapshot_observed_at":"2026-07-06T22:39:04.164003Z","submitted_at":"2025-12-15T19:00:02Z","title":"The spectrum of Feynman-integral geometries at two loops","version":3},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-05-16T21:42:04.525894Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2512.13794"},"observation_digest":"sha256:d355c424e1b9eab8eeb5aa6d9f13b016a29500622f989c8790414e6e77bc54d1","observation_id":"915992db-c46e-4f78-81a6-ac614981f2f6","resolution":{"observed_at":"2026-05-16T21:43:34.995797Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-08-03T08:40:29.799012Z","title":"Frellesvig,The loop-by-loop Baikov representation — Strategies and implementation,JHEP04(2025) 111 [2412.01804]","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16256","last_updated":"2026-07-13T19:47:59Z","snapshot_observed_at":"2026-08-09T21:36:20.759595Z","submitted_at":"2026-01-22T19:00:01Z","title":"Conservative Black Hole Scattering at Fifth Post-Minkowskian and Second Self-Force Order","version":4},"reference_index":135,"source":"pdf_text","source_observed_at":"2026-08-03T08:40:29.799012Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2601.16256"},"observation_digest":"sha256:c93e4534d718b2f24811853a2f6bd2f7dcf5bd63eb3cb6ce4d4c6cdb32579a1c","observation_id":"0dad7420-e70b-4a6d-b2c6-ff8389f51982","resolution":{"observed_at":"2026-08-03T08:40:29.799012Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2602.06947","last_updated":"2026-04-09T15:42:30Z","snapshot_observed_at":"2026-07-31T17:35:32.003805Z","submitted_at":"2026-02-06T18:44:09Z","title":"The gravitational Compton amplitude at third post-Minkowskian order","version":2},"reference_index":167,"source":"pdf_text","source_observed_at":"2026-05-16T06:25:50.003086Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2602.06947"},"observation_digest":"sha256:f2aa5278318ad6366910be496696cf71fa1a666dbf38afc225d6f321121ee4be","observation_id":"05f78cff-7235-44be-9250-5f139c1d9d0e","resolution":{"observed_at":"2026-05-16T06:27:27.598686Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2604.08332","last_updated":"2026-04-09T15:06:06Z","snapshot_observed_at":"2026-07-06T22:57:26.678728Z","submitted_at":"2026-04-09T15:06:06Z","title":"Discrete symmetries of Feynman integrals","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-05-10T17:52:41.442686Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2604.08332"},"observation_digest":"sha256:2f0a4980753f64e35d37aa2ec6b69ef056524126fa2cadaecce55a028d7253a8","observation_id":"859cbf31-46a6-452b-802e-39566631f4ca","resolution":{"observed_at":"2026-05-11T05:55:58.369537Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2604.25270","last_updated":"2026-04-28T06:29:00Z","snapshot_observed_at":"2026-07-06T23:11:11.827339Z","submitted_at":"2026-04-28T06:29:00Z","title":"Integrand Analysis, Leading Singularities and Canonical Bases beyond Polylogarithms","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-05-07T16:07:21.257348Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2604.25270"},"observation_digest":"sha256:386c1d8f869071d3cc69cf00d1f6ae6cac66baea3ae28680ff54ffd64678b9e5","observation_id":"010aa8ca-16d0-46ca-8427-54abfc394074","resolution":{"observed_at":"2026-05-11T23:51:37.123376Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2605.07729","last_updated":"2026-05-08T13:35:27Z","snapshot_observed_at":"2026-07-06T23:20:06.574823Z","submitted_at":"2026-05-08T13:35:27Z","title":"Genus drop involving non-hyperelliptic curves in Feynman integrals","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-05-11T02:05:19.231407Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2605.07729"},"observation_digest":"sha256:32542d2c256342527ff2e53ce85d641413be076a8e354e91a756727f6b15aa8d","observation_id":"99072736-96fd-44fc-9dbf-35d927f5ac0b","resolution":{"observed_at":"2026-05-11T04:00:53.879392Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2605.29789","last_updated":"2026-05-28T11:40:07Z","snapshot_observed_at":"2026-08-12T17:24:53.124848Z","submitted_at":"2026-05-28T11:40:07Z","title":"Magic Relations and Critical Varieties of Feynman Integrals","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-06-29T06:40:09.724301Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2605.29789"},"observation_digest":"sha256:72e7c27d68fb0538c3939aa621ac5a5db97b868d14931dc1624ae7994f866242","observation_id":"c05fe383-ee06-42aa-b2a9-7aa97da5c9f5","resolution":{"observed_at":"2026-06-29T14:23:31.156645Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2606.21702","last_updated":"2026-06-19T19:21:28Z","snapshot_observed_at":"2026-08-09T18:57:43.505929Z","submitted_at":"2026-06-19T19:21:28Z","title":"Analytic results for heavy-quark contributions to charged-current DIS at NNLO","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-06-26T13:32:17.923022Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2606.21702"},"observation_digest":"sha256:23f7d0faa589dbc2fdb31e929d6abf40cfbe82bd2ffbe8a20702d6e56baeb407","observation_id":"527b9e1c-b469-4c62-913f-d275c78f0f68","resolution":{"observed_at":"2026-07-04T07:19:38.488974Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":"2412.01804","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-04T07:19:38.487392Z","title":"Frellesvig, JHEP 04, 111 (2025)","venue":null,"work_id":"388ad0ed-f2b0-4b90-9f88-2bc262f17789","year":2025},"citing_paper":{"arxiv_id":"2606.29612","last_updated":"2026-06-28T21:36:40Z","snapshot_observed_at":"2026-08-01T23:38:15.249654Z","submitted_at":"2026-06-28T21:36:40Z","title":"Landau's Leviathans","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-06-30T01:50:25.042094Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2606.29612"},"observation_digest":"sha256:d8d814d2721521b579d6a4fb622b753842c2d7dbbac13f771176273d54abbf0b","observation_id":"7ade3ab3-fd69-4a0f-8e2d-cd840c22cbb2","resolution":{"observed_at":"2026-06-30T03:04:14.570560Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.01804","snapshot_observed_at":"2026-07-12T03:09:19.132371Z","title":"Frellesvig,The loop-by-loop Baikov representation — Strategies and implementation, JHEP04(2025) 111, [2412.01804]","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03343","last_updated":"2026-07-03T14:00:23Z","snapshot_observed_at":"2026-08-13T02:45:22.101400Z","submitted_at":"2026-07-03T14:00:23Z","title":"First look at the evaluation of two-loop Feynman integrals for radiative return processes","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-07-12T03:09:19.132371Z"},"links":{"cited_paper":"/paper/2412.01804","citing_paper":"/paper/2607.03343"},"observation_digest":"sha256:89073c2617dd13ddbd2ec7fe7751a24e8aaa06fef84de9845ad07839267960da","observation_id":"a7024c51-6f51-4703-8a91-34fed78aa6d8","resolution":{"observed_at":"2026-07-12T03:09:19.132371Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2412.01804/citation-record","integrity":"/paper/2412.01804/integrity","json":"/paper/2412.01804/citation-record.json","paper":"/paper/2412.01804"},"outbound":[],"paper":{"arxiv_id":"2412.01804","last_updated":"2025-03-19T04:50:44Z","latest_version":3,"primary_category":"hep-th","snapshot_observed_at":"2026-08-12T00:52:31.295169Z","submitted_at":"2024-12-02T18:49:32Z","title":"The Loop-by-Loop Baikov Representation -- Strategies and Implementation"},"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":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 13 inbound Pith citation observations for arXiv:2412.01804."}