{"as_of":"2026-08-10T17:11:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:fc35aa2682ca73c0fb5b9f504e6275285fdc618ef1312489df5952a3ce0ccddf","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":8,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":8,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":8,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":8,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-09T04:34:23.512068Z","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":"2026-07-04T18:10:02.082662Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-08-09T04:34:23.512068Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.03588","last_updated":"2025-07-09T10:02:13Z","snapshot_observed_at":"2026-08-10T05:06:14.205795Z","submitted_at":"2025-02-05T20:09:42Z","title":"Complementary Probes of Warped Extra Dimension: Colliders, Gravitational Waves and Primordial Black Holes from Phase Transitions","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-09T04:34:23.512068Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2502.03588"},"observation_digest":"sha256:b81cb49e3a59996608ffa9ed7e39c0cfa5232f6f6655ce5dd4e1a847116101c4","observation_id":"f8b77b85-106e-4807-a7f2-5a7445add6e7","resolution":{"observed_at":"2026-08-09T04:34:23.512068Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-08-08T14:17:20.977327Z","title":"Phase transition to RS: cool, not supercool,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.06965","last_updated":"2025-06-11T17:51:57Z","snapshot_observed_at":"2026-08-10T04:35:36.169514Z","submitted_at":"2025-02-10T19:02:33Z","title":"Conformal Freeze-in Dark Matter: 5D Dual and Phase Transition","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T14:17:20.977327Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2502.06965"},"observation_digest":"sha256:68443c960c308f00c87a09920a5fe776511c35373719939febf6c8bb1fc9f0be","observation_id":"414cb0d6-d66e-44f9-b0cb-b1d33ac94e51","resolution":{"observed_at":"2026-08-08T14:17:20.977327Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-08-03T18:46:27.256985Z","title":"Phase transition to RS: cool, not supercool,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2512.04177","last_updated":"2026-06-27T03:29:58Z","snapshot_observed_at":"2026-08-06T07:14:43.415261Z","submitted_at":"2025-12-03T19:00:12Z","title":"Inflation with a Growing Fifth Dimension","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-03T18:46:27.256985Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2512.04177"},"observation_digest":"sha256:ee4766846cf5233da922e7a6de6a16edd9e61ed0f7c93b899419f5de55c62105","observation_id":"4b7b5a4a-11bf-4b39-ae46-1d968b66ac3e","resolution":{"observed_at":"2026-08-03T18:46:27.256985Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":"2401.09633","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-07-04T18:10:02.082662Z","title":"Phase transition to RS: cool, not supercool","venue":null,"work_id":"eb3320a0-199f-42d0-a1d8-544b3c309e82","year":2024},"citing_paper":{"arxiv_id":"2603.24732","last_updated":"2026-07-29T15:25:46Z","snapshot_observed_at":"2026-08-02T17:37:37.143639Z","submitted_at":"2026-03-25T18:56:36Z","title":"Confinement in Holographic Theories at Finite Theta","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-05-14T23:57:30.735344Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2603.24732"},"observation_digest":"sha256:4fb83bcadecabd9869bbf909c698a13a9505bf1da549c02fdb141b8454bc1cd1","observation_id":"f017c2ae-6c0a-46a7-8e00-912561841920","resolution":{"observed_at":"2026-05-14T23:58:18.964080Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-08-02T17:37:39.093371Z","title":"Phase transition to RS: cool, not supercool,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2603.24732","last_updated":"2026-07-29T15:25:46Z","snapshot_observed_at":"2026-08-02T17:37:37.143639Z","submitted_at":"2026-03-25T18:56:36Z","title":"Confinement in Holographic Theories at Finite Theta","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-02T17:37:39.093371Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2603.24732"},"observation_digest":"sha256:dae90056374d61fa85c11e69abcbbc774e0f6d5f52dc5c6204149469e7b6b5e8","observation_id":"50d4f27c-c5cf-43b7-8255-ba2a78672b79","resolution":{"observed_at":"2026-08-02T17:37:39.093371Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":"2401.09633","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-07-04T18:10:02.082662Z","title":"Phase transition to RS: cool, not supercool","venue":null,"work_id":"eb3320a0-199f-42d0-a1d8-544b3c309e82","year":2024},"citing_paper":{"arxiv_id":"2604.06306","last_updated":"2026-04-07T18:00:00Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2026-04-07T18:00:00Z","title":"Uncool soft-wall transitions and gravitational waves","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-05-10T19:12:50.767365Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2604.06306"},"observation_digest":"sha256:44ee09416d0375f4f6e39946101eedf0b2ae9aa83b6ef656a07557468d5f8d1c","observation_id":"298709f6-42a4-4871-a60b-7a889c153fef","resolution":{"observed_at":"2026-05-10T23:20:52.156016Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":"2401.09633","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-07-04T18:10:02.082662Z","title":"Phase transition to RS: cool, not supercool","venue":null,"work_id":"eb3320a0-199f-42d0-a1d8-544b3c309e82","year":2024},"citing_paper":{"arxiv_id":"2606.25014","last_updated":"2026-07-08T17:34:31Z","snapshot_observed_at":"2026-07-12T12:25:42.844259Z","submitted_at":"2026-06-23T18:00:00Z","title":"Probing Confining Dark Sectors with Cosmological Perturbations","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-06-25T23:01:42.890617Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2606.25014"},"observation_digest":"sha256:43004b5f667ed31497214fc77d493feebc77467cb95089bcf11452688ce02da1","observation_id":"1ac0863d-ec95-45f4-b29e-dfe83fdf79dd","resolution":{"observed_at":"2026-07-04T18:10:02.084717Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.09633","snapshot_observed_at":"2026-07-12T12:25:43.531687Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2606.25014","last_updated":"2026-07-08T17:34:31Z","snapshot_observed_at":"2026-07-12T12:25:42.844259Z","submitted_at":"2026-06-23T18:00:00Z","title":"Probing Confining Dark Sectors with Cosmological Perturbations","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-07-12T12:25:43.531687Z"},"links":{"cited_paper":"/paper/2401.09633","citing_paper":"/paper/2606.25014"},"observation_digest":"sha256:098a945f829bfd7ce181ddd3e6e2659ed3f7c56795300322e8945392bfe2ad5e","observation_id":"278146e3-6a38-4381-bbf0-135107c2361d","resolution":{"observed_at":"2026-07-12T12:25:43.531687Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2401.09633/citation-record","integrity":"/paper/2401.09633/integrity","json":"/paper/2401.09633/citation-record.json","paper":"/paper/2401.09633"},"outbound":[],"paper":{"arxiv_id":"2401.09633","last_updated":"2025-08-25T20:35:36Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-10T04:40:36.012141Z","submitted_at":"2024-01-17T22:54:33Z","title":"Phase Transition to RS: Cool, not Supercool"},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 8 inbound Pith citation observations for arXiv:2401.09633."}