{"as_of":"2026-08-10T05:49:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:5b83d96d12d6be4070f1601a6dcb21aca1a113e4697d418621fd6e37bde6c444","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":10,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":10,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+00:00","state":"measured"},{"denominator":10,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":10,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T14:22:24.888770Z","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":"2026-06-29T16:53:40.719034Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-08-08T14:22:24.888770Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.06935","last_updated":"2025-06-02T05:31:17Z","snapshot_observed_at":"2026-08-08T14:38:50.495220Z","submitted_at":"2025-02-10T19:00:00Z","title":"Collective flavor conversions are interactions of neutrinos with quantized flavor waves","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T14:22:24.888770Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2502.06935"},"observation_digest":"sha256:d68d2f795ce31932e2273d023d8d1061c0e5de6dd509fb33a040c119673d4f7c","observation_id":"fc836f1c-20b4-48e2-afa3-91d1010db690","resolution":{"observed_at":"2026-08-08T14:22:24.888770Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-08-07T05:49:17.978576Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2506.07017","last_updated":"2025-07-25T07:27:58Z","snapshot_observed_at":"2026-08-09T15:02:22.481724Z","submitted_at":"2025-06-08T06:47:31Z","title":"Comparative Testing of Subgrid Models for Fast Neutrino Flavor Conversions in Core-collapse Supernova Simulations","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-07T05:49:17.978576Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2506.07017"},"observation_digest":"sha256:ac82f8652adb56393bdaf706d0a7514cda3c9a75d549ddf7c1d0670d9c6feddc","observation_id":"cae56266-560c-455d-b365-4f9f0e049f9e","resolution":{"observed_at":"2026-08-07T05:49:17.978576Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-08-03T08:55:31.902761Z","title":"Fiorillo and G.G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.15372","last_updated":"2026-06-11T08:58:56Z","snapshot_observed_at":"2026-08-07T18:02:44.585556Z","submitted_at":"2026-01-21T19:00:00Z","title":"Single-wave solutions of the neutrino fast flavor system. Part I. Mechanical properties","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T08:55:31.902761Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2601.15372"},"observation_digest":"sha256:f314d8a0c63066fb136665b4b3a5857c8546e7d7591b16b901b9b565f2e28c57","observation_id":"517fa344-c74c-4e8d-ade7-7a43f83164af","resolution":{"observed_at":"2026-08-03T08:55:31.902761Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-08-03T08:01:32.480206Z","title":"Fiorillo and G.G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.18880","last_updated":"2026-06-11T15:05:04Z","snapshot_observed_at":"2026-08-03T08:01:28.938226Z","submitted_at":"2026-01-26T19:00:03Z","title":"Single-wave solutions of the neutrino fast flavor system. Part II. Weak instabilities and their resonant behavior","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T08:01:32.480206Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2601.18880"},"observation_digest":"sha256:4bb0c4a278285f10e3c9c8bb8afb4b3a8b457746afad78f5c5fce0142369ec04","observation_id":"8fdc0c10-2886-43f6-885a-d3a7be0970cc","resolution":{"observed_at":"2026-08-03T08:01:32.480206Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":"2406.06708","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-06-29T16:53:40.719034Z","title":"Fiorillo and G.G","venue":null,"work_id":"d304a570-58b8-45ba-a284-4428b1cccc8a","year":2024},"citing_paper":{"arxiv_id":"2604.06404","last_updated":"2026-04-07T19:37:20Z","snapshot_observed_at":"2026-07-06T22:54:53.308309Z","submitted_at":"2026-04-07T19:37:20Z","title":"Neutrino transport and flavor instabilities in a post-merger disk","version":1},"reference_index":116,"source":"pdf_text","source_observed_at":"2026-05-10T18:35:42.044621Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2604.06404"},"observation_digest":"sha256:a278821ac79b9ff8fee33729ef3bb282b127fae16868ae52f21c1afd796face4","observation_id":"7177e523-19a6-4437-9b85-572aa898ee3a","resolution":{"observed_at":"2026-05-11T00:20:52.894866Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":"2406.06708","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-06-29T16:53:40.719034Z","title":"Fiorillo and G.G","venue":null,"work_id":"d304a570-58b8-45ba-a284-4428b1cccc8a","year":2024},"citing_paper":{"arxiv_id":"2604.18689","last_updated":"2026-07-24T10:42:41Z","snapshot_observed_at":"2026-08-06T14:51:31.468285Z","submitted_at":"2026-04-20T18:00:03Z","title":"Flavomons in Matter Gradients: Ray Tracing and Amplitude Evolution","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-05-10T04:00:00.056270Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2604.18689"},"observation_digest":"sha256:8920a4e11ed6c7fb626b479588311f34de142f1e40d497a0a85d1095e601b3ed","observation_id":"485ce507-5368-41ce-a4ef-1bc618ff09d8","resolution":{"observed_at":"2026-05-11T12:16:04.481366Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-08-02T15:54:27.536806Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2604.18689","last_updated":"2026-07-24T10:42:41Z","snapshot_observed_at":"2026-08-06T14:51:31.468285Z","submitted_at":"2026-04-20T18:00:03Z","title":"Flavomons in Matter Gradients: Ray Tracing and Amplitude Evolution","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-02T15:54:27.536806Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2604.18689"},"observation_digest":"sha256:c403ce88340e47859858cd88523f843932bc8ccf9e363d64f54feaf6e970ca07","observation_id":"a8da8969-effc-4434-8cc2-4310fc93e8b9","resolution":{"observed_at":"2026-08-02T15:54:27.536806Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":"2406.06708","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-06-29T16:53:40.719034Z","title":"Fiorillo and G.G","venue":null,"work_id":"d304a570-58b8-45ba-a284-4428b1cccc8a","year":2024},"citing_paper":{"arxiv_id":"2604.25687","last_updated":"2026-04-28T14:18:05Z","snapshot_observed_at":"2026-07-06T23:11:30.068819Z","submitted_at":"2026-04-28T14:18:05Z","title":"Collective neutrino-antineutrino pair oscillations","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-05-07T15:58:06.378902Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2604.25687"},"observation_digest":"sha256:58a0021b7e60a19776119a4476b0d29a712aaf6bc4a4f794e608671fe6be6c78","observation_id":"129ace98-eac5-4095-852a-4b37e2288be8","resolution":{"observed_at":"2026-05-12T00:01:13.428430Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":"2406.06708","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-06-29T16:53:40.719034Z","title":"Fiorillo and G.G","venue":null,"work_id":"d304a570-58b8-45ba-a284-4428b1cccc8a","year":2024},"citing_paper":{"arxiv_id":"2605.27506","last_updated":"2026-05-26T18:00:01Z","snapshot_observed_at":"2026-08-01T09:04:58.580049Z","submitted_at":"2026-05-26T18:00:01Z","title":"Neutrino-antineutrino superfluidity","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-06-29T16:50:27.099389Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2605.27506"},"observation_digest":"sha256:492c28575a0548cbadbe56fe1252bfd4ac33e56d4c662049c88d7bb48e11588b","observation_id":"6fce5a84-34f1-4284-bdc0-d35ddf89b73c","resolution":{"observed_at":"2026-06-29T16:53:40.720322Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.06708","snapshot_observed_at":"2026-08-01T23:35:14.009070Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.15392","last_updated":"2026-07-16T18:43:32Z","snapshot_observed_at":"2026-08-06T08:46:15.300374Z","submitted_at":"2026-07-16T18:43:32Z","title":"Solar-System Abundances of $p$-Nuclides Probe Collective Neutrino Oscillations in Supernovae","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-01T23:35:14.009070Z"},"links":{"cited_paper":"/paper/2406.06708","citing_paper":"/paper/2607.15392"},"observation_digest":"sha256:1b2021cfefb150a3b17a1fb461330eeb3a6bcbf531c391ea6df562bab125ad88","observation_id":"01dfa101-63f0-4305-8b46-c571db9a9d5c","resolution":{"observed_at":"2026-08-01T23:35:14.009070Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2406.06708/citation-record","integrity":"/paper/2406.06708/integrity","json":"/paper/2406.06708/citation-record.json","paper":"/paper/2406.06708"},"outbound":[],"paper":{"arxiv_id":"2406.06708","last_updated":"2024-09-30T07:51:29Z","latest_version":3,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-10T05:12:25.781616Z","submitted_at":"2024-06-10T18:16:28Z","title":"Theory of neutrino fast flavor evolution. Part I. Linear response theory and stability conditions"},"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":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 10 inbound Pith citation observations for arXiv:2406.06708."}