{"as_of":"2026-08-08T03:38:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:b56871d3b74947428163c6e7a198d38013ed1ab0883b9e9cded44f1b2d355697","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":4,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":4,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-07T06:34:17.273281+00:00","state":"measured"},{"denominator":4,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":4,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T16:57:35.201848Z","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":"2026-07-04T21:10:08.523144Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2405.05316","last_updated":"2024-05-08T18:00:02Z","snapshot_observed_at":"2026-07-06T18:11:43.528130Z","submitted_at":"2024-05-08T18:00:02Z","title":"Higher Berry Curvature from the Wave Function I: Schmidt Decomposition and Matrix Product States","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.05316","snapshot_observed_at":"2026-08-06T16:57:35.201848Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.12546","last_updated":"2025-07-16T18:00:49Z","snapshot_observed_at":"2026-08-07T21:43:15.054655Z","submitted_at":"2025-07-16T18:00:49Z","title":"Space of conformal boundary conditions from the view of higher Berry phase: Flow of Berry curvature in parametrized BCFTs","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T16:57:35.201848Z"},"links":{"cited_paper":"/paper/2405.05316","citing_paper":"/paper/2507.12546"},"observation_digest":"sha256:e442a44a056521c39532b85d66e69fedbae7f9435d7b0a65065df3599a5c6e44","observation_id":"fca37c6a-8627-4f1a-bfb4-fd40b7d3f304","resolution":{"observed_at":"2026-08-06T16:57:35.201848Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.05316","last_updated":"2024-05-08T18:00:02Z","snapshot_observed_at":"2026-07-06T18:11:43.528130Z","submitted_at":"2024-05-08T18:00:02Z","title":"Higher Berry Curvature from the Wave Function I: Schmidt Decomposition and Matrix Product States","version":1},"cited_work":{"arxiv_id":"2405.05316","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2405.05316","snapshot_observed_at":"2026-07-04T21:10:08.523144Z","title":"Sommer, X","venue":null,"work_id":"278764ea-fb60-4c0d-a571-54bfdace74a5","year":2024},"citing_paper":{"arxiv_id":"2602.13627","last_updated":"2026-05-12T22:47:49Z","snapshot_observed_at":"2026-07-31T01:10:52.998012Z","submitted_at":"2026-02-14T06:35:33Z","title":"Higher Connection in Open String Field Theory","version":3},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-05-15T22:56:16.855782Z"},"links":{"cited_paper":"/paper/2405.05316","citing_paper":"/paper/2602.13627"},"observation_digest":"sha256:81884904bf6446f65a3b0ac61dc721b157068ca3d39472942d637e6a814e4566","observation_id":"a67ecffe-19da-47ba-970c-4bcba0b9ddf4","resolution":{"observed_at":"2026-05-15T22:56:49.857766Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2405.05316","last_updated":"2024-05-08T18:00:02Z","snapshot_observed_at":"2026-07-06T18:11:43.528130Z","submitted_at":"2024-05-08T18:00:02Z","title":"Higher Berry Curvature from the Wave Function I: Schmidt Decomposition and Matrix Product States","version":1},"cited_work":{"arxiv_id":"2405.05316","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2405.05316","snapshot_observed_at":"2026-07-04T21:10:08.523144Z","title":"Sommer, X","venue":null,"work_id":"278764ea-fb60-4c0d-a571-54bfdace74a5","year":2024},"citing_paper":{"arxiv_id":"2605.03891","last_updated":"2026-05-05T15:48:37Z","snapshot_observed_at":"2026-07-06T23:16:44.876986Z","submitted_at":"2026-05-05T15:48:37Z","title":"Parameterized Families of Toric Code Phase: $em$-duality family and higher-order anyon pumping","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-05-07T04:07:13.027020Z"},"links":{"cited_paper":"/paper/2405.05316","citing_paper":"/paper/2605.03891"},"observation_digest":"sha256:f187aa907238fbc7112171bd6506a3f03a9f8ade067a90ca45ddfd019b751630","observation_id":"33379428-8dd4-4050-806f-04ecb155e39b","resolution":{"observed_at":"2026-05-12T10:41:31.235283Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2405.05316","last_updated":"2024-05-08T18:00:02Z","snapshot_observed_at":"2026-07-06T18:11:43.528130Z","submitted_at":"2024-05-08T18:00:02Z","title":"Higher Berry Curvature from the Wave Function I: Schmidt Decomposition and Matrix Product States","version":1},"cited_work":{"arxiv_id":"2405.05316","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2405.05316","snapshot_observed_at":"2026-07-04T21:10:08.523144Z","title":"Sommer, X","venue":null,"work_id":"278764ea-fb60-4c0d-a571-54bfdace74a5","year":2024},"citing_paper":{"arxiv_id":"2606.26096","last_updated":"2026-06-24T17:59:57Z","snapshot_observed_at":"2026-07-07T00:00:26.827253Z","submitted_at":"2026-06-24T17:59:57Z","title":"Higher Berry curvature, second Chern numbers and magnetoelectric coupling in crystalline insulators","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-06-25T19:07:05.145214Z"},"links":{"cited_paper":"/paper/2405.05316","citing_paper":"/paper/2606.26096"},"observation_digest":"sha256:f68a7fd2ce7af18a44c5db40fc4eab1f9b7b4978b9c3714892efa7a34db0de90","observation_id":"cce917f0-aba8-4890-b4a1-b42809bfd9e5","resolution":{"observed_at":"2026-07-04T21:10:08.525252Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2405.05316/citation-record","integrity":"/paper/2405.05316/integrity","json":"/paper/2405.05316/citation-record.json","paper":"/paper/2405.05316"},"outbound":[],"paper":{"arxiv_id":"2405.05316","last_updated":"2024-05-08T18:00:02Z","latest_version":1,"primary_category":"cond-mat.str-el","snapshot_observed_at":"2026-07-06T18:11:43.528130Z","submitted_at":"2024-05-08T18:00:02Z","title":"Higher Berry Curvature from the Wave Function I: Schmidt Decomposition and Matrix Product States"},"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":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2405.05316."}