{"as_of":"2026-08-17T20:12:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:b21e9ab06fef8dcc985379d7171d68a598cd4d1058ba0add32411264de434129","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":5,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":5,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-17T06:30:58.91139+00:00","state":"measured"},{"denominator":5,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":5,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-10T15:42:20.786629Z","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":"2026-07-01T23:46:24.540842Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2406.17468","last_updated":"2024-06-25T11:13:14Z","snapshot_observed_at":"2026-08-17T07:37:45.413700Z","submitted_at":"2024-06-25T11:13:14Z","title":"Tachyonic production of dark relics: classical lattice vs. quantum 2PI in Hartree truncation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.17468","snapshot_observed_at":"2026-08-10T15:42:20.786629Z","title":"Kainulainen, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.13811","last_updated":"2025-01-23T16:32:20Z","snapshot_observed_at":"2026-08-16T22:12:40.825427Z","submitted_at":"2025-01-23T16:32:20Z","title":"Inflaton Self Resonance, Oscillons, and Gravitational Waves in Small Field Polynomial Inflation","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-10T15:42:20.786629Z"},"links":{"cited_paper":"/paper/2406.17468","citing_paper":"/paper/2501.13811"},"observation_digest":"sha256:68173294a7d1d5a092ae879fa902d2235ae0f96f833c6a9bc3f3f899e34b888c","observation_id":"c8dc1b6b-5232-436c-9ddd-b172c236cedb","resolution":{"observed_at":"2026-08-10T15:42:20.786629Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.17468","last_updated":"2024-06-25T11:13:14Z","snapshot_observed_at":"2026-08-17T07:37:45.413700Z","submitted_at":"2024-06-25T11:13:14Z","title":"Tachyonic production of dark relics: classical lattice vs. quantum 2PI in Hartree truncation","version":1},"cited_work":{"arxiv_id":"2406.17468","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.17468","snapshot_observed_at":"2026-07-01T23:46:24.540842Z","title":"Kainulainen, S","venue":null,"work_id":"61a1ce27-7c74-47e9-bf4a-cbd9b652650e","year":2024},"citing_paper":{"arxiv_id":"2601.07670","last_updated":"2026-05-14T14:26:24Z","snapshot_observed_at":"2026-08-05T04:12:23.424751Z","submitted_at":"2026-01-12T15:51:11Z","title":"Tachyonic gravitational dark matter production after inflation","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-05-16T14:59:59.375201Z"},"links":{"cited_paper":"/paper/2406.17468","citing_paper":"/paper/2601.07670"},"observation_digest":"sha256:8fc219e5f5253047c5bbd7448c9a2c7ff06e7270178d4185494dc417e9bf769d","observation_id":"888a30be-2223-41a5-806c-9baf4f3de3f1","resolution":{"observed_at":"2026-05-16T15:01:03.574547Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.17468","last_updated":"2024-06-25T11:13:14Z","snapshot_observed_at":"2026-08-17T07:37:45.413700Z","submitted_at":"2024-06-25T11:13:14Z","title":"Tachyonic production of dark relics: classical lattice vs. quantum 2PI in Hartree truncation","version":1},"cited_work":{"arxiv_id":"2406.17468","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.17468","snapshot_observed_at":"2026-07-01T23:46:24.540842Z","title":"Kainulainen, S","venue":null,"work_id":"61a1ce27-7c74-47e9-bf4a-cbd9b652650e","year":2024},"citing_paper":{"arxiv_id":"2604.05078","last_updated":"2026-04-06T18:29:45Z","snapshot_observed_at":"2026-08-16T21:46:05.639695Z","submitted_at":"2026-04-06T18:29:45Z","title":"Gravitational Waves from Matter Perturbations of Spectator Scalar Fields","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-05-10T19:14:15.636565Z"},"links":{"cited_paper":"/paper/2406.17468","citing_paper":"/paper/2604.05078"},"observation_digest":"sha256:0af7505ed2a1145a0d357ef55a103c8a82079069ba2e49792aa16d715321199a","observation_id":"78ea7679-9f3c-40ca-8b82-1c8e30f12ac7","resolution":{"observed_at":"2026-05-10T23:20:50.809908Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.17468","last_updated":"2024-06-25T11:13:14Z","snapshot_observed_at":"2026-08-17T07:37:45.413700Z","submitted_at":"2024-06-25T11:13:14Z","title":"Tachyonic production of dark relics: classical lattice vs. quantum 2PI in Hartree truncation","version":1},"cited_work":{"arxiv_id":"2406.17468","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.17468","snapshot_observed_at":"2026-07-01T23:46:24.540842Z","title":"Kainulainen, S","venue":null,"work_id":"61a1ce27-7c74-47e9-bf4a-cbd9b652650e","year":2024},"citing_paper":{"arxiv_id":"2604.16085","last_updated":"2026-04-17T14:14:55Z","snapshot_observed_at":"2026-07-06T23:03:30.601598Z","submitted_at":"2026-04-17T14:14:55Z","title":"Thermal effects on Dark Matter production during cosmic reheating","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-05-10T08:31:08.029870Z"},"links":{"cited_paper":"/paper/2406.17468","citing_paper":"/paper/2604.16085"},"observation_digest":"sha256:ebe25d803aca400e8a8edfb9c45719bcabdd7c8d5c10c3c5a8f5b112eb76740a","observation_id":"3bdc9bd0-b6df-4b95-8748-4d04b348b232","resolution":{"observed_at":"2026-05-10T08:58:13.672900Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.17468","last_updated":"2024-06-25T11:13:14Z","snapshot_observed_at":"2026-08-17T07:37:45.413700Z","submitted_at":"2024-06-25T11:13:14Z","title":"Tachyonic production of dark relics: classical lattice vs. quantum 2PI in Hartree truncation","version":1},"cited_work":{"arxiv_id":"2406.17468","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2406.17468","snapshot_observed_at":"2026-07-01T23:46:24.540842Z","title":"Kainulainen, S","venue":null,"work_id":"61a1ce27-7c74-47e9-bf4a-cbd9b652650e","year":2024},"citing_paper":{"arxiv_id":"2606.02039","last_updated":"2026-06-01T10:29:45Z","snapshot_observed_at":"2026-08-17T11:58:54.281837Z","submitted_at":"2026-06-01T10:29:45Z","title":"Tachyonic particle production: quantum 2PI formalism with momentum exchanging collisions","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-06-28T13:51:55.523108Z"},"links":{"cited_paper":"/paper/2406.17468","citing_paper":"/paper/2606.02039"},"observation_digest":"sha256:32ef12dacd5c464ceec0c4b2098764ca335384b4ca9d73c09302da545fb58799","observation_id":"753fec0b-6049-4d7f-b7f0-6573c92143bd","resolution":{"observed_at":"2026-07-01T23:46:24.542646Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2406.17468/citation-record","integrity":"/paper/2406.17468/integrity","json":"/paper/2406.17468/citation-record.json","paper":"/paper/2406.17468"},"outbound":[],"paper":{"arxiv_id":"2406.17468","last_updated":"2024-06-25T11:13:14Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-17T07:37:45.413700Z","submitted_at":"2024-06-25T11:13:14Z","title":"Tachyonic production of dark relics: classical lattice vs. quantum 2PI in Hartree truncation"},"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":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"thesis":"As of 17 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 5 inbound Pith citation observations for arXiv:2406.17468."}