{"as_of":"2026-08-12T06:12:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6c5c1f2a1d2ab811a6f4935981cb030c948292bbf822c5d4f58e2591c4be44fa","coverage":[{"denominator":9,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":9,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-10T14:17:09.763632Z","state":"measured"},{"denominator":9,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":9,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-11T06:34:44.6726+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2501.15533/citation-record","integrity":"/paper/2501.15533/integrity","json":"/paper/2501.15533/citation-record.json","paper":"/paper/2501.15533"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-th/9711200","last_updated":"1998-01-22T15:42:41Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"1997-11-27T23:53:13Z","title":"The Large N Limit of Superconformal Field Theories and Supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9711200","snapshot_observed_at":"2026-08-10T14:17:09.728195Z","title":"The Large N limit of superconformal field theories and supergravity,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.728195Z"},"links":{"cited_paper":"/paper/hep-th/9711200","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:000f9c8d816b4d57ccad990495806cb225949b79b865ad0b7a8713e6752b79f1","observation_id":"2a59e066-a1da-4da7-bca1-9d82d396d65e","resolution":{"observed_at":"2026-08-10T14:17:09.728195Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.04611","last_updated":"2024-05-07T18:49:53Z","snapshot_observed_at":"2026-07-06T18:11:13.757248Z","submitted_at":"2024-05-07T18:49:53Z","title":"Plasma-Plasma Third Order Phase Transition from type IIB Supergravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.04611","snapshot_observed_at":"2026-08-10T14:17:09.733347Z","title":"Plasma-Plasma Third Order Phase Transition from Type IIB Supergravity,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.733347Z"},"links":{"cited_paper":"/paper/2405.04611","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:9f7692b02b124262844dee6e01c0ac512608e351882da1685b16eaf3076f2445","observation_id":"1f8c9401-cfd9-4366-aab0-07291bb5a9d9","resolution":{"observed_at":"2026-08-10T14:17:09.733347Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9810227","last_updated":"1998-12-02T22:50:41Z","snapshot_observed_at":"2026-07-07T05:18:11.555260Z","submitted_at":"1998-10-28T00:56:55Z","title":"Non-Extreme Black Holes of Five Dimensional N=2 AdS Supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9810227","snapshot_observed_at":"2026-08-10T14:17:09.737721Z","title":"Nonextreme black holes of five-dimensional N=2 AdS supergravity,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.737721Z"},"links":{"cited_paper":"/paper/hep-th/9810227","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:a4c370f9fdded0e23f4a919f79b6a1d271a3e749c107cbbb034dcfcdd8d39efd","observation_id":"aea8a627-949e-4754-9c4f-fb9efb817b43","resolution":{"observed_at":"2026-08-10T14:17:09.737721Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.01562","last_updated":"2019-10-04T11:05:26Z","snapshot_observed_at":"2026-08-10T15:58:12.313729Z","submitted_at":"2019-07-02T18:00:07Z","title":"Novel color superconducting phases of $\\cal{N}$ = 4 super Yang-Mills at strong coupling","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.01562","snapshot_observed_at":"2026-08-10T14:17:09.742197Z","title":"Novel color superconducting phases of N = 4 super Yang-Mills at strong coupling,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.742197Z"},"links":{"cited_paper":"/paper/1907.01562","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:1179828b11243169e437fe4bb0a2ab30806568c90ef6e2929da62834cc56f218","observation_id":"544d4d1f-0b00-481f-80b6-87297b56c44e","resolution":{"observed_at":"2026-08-10T14:17:09.742197Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9803002","last_updated":"1998-03-19T18:56:26Z","snapshot_observed_at":"2026-08-01T23:29:08.567443Z","submitted_at":"1998-03-01T00:26:14Z","title":"Wilson loops in large N field theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9803002","snapshot_observed_at":"2026-08-10T14:17:09.746562Z","title":"Wilson loops in large N field theories,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.746562Z"},"links":{"cited_paper":"/paper/hep-th/9803002","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:7d751a2d88459b438b402c27d5f18be435d021da8affa80c80859ebb72afd468","observation_id":"e37f9f66-15d1-4a6b-ab18-f280d6d0f622","resolution":{"observed_at":"2026-08-10T14:17:09.746562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9803137","last_updated":"1998-04-01T15:25:44Z","snapshot_observed_at":"2026-08-08T12:04:36.892953Z","submitted_at":"1998-03-17T19:01:35Z","title":"Wilson Loops in the Large N Limit at Finite Temperature","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9803137","snapshot_observed_at":"2026-08-10T14:17:09.751157Z","title":"Wilson loops in the large N limit at finite temperature,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.751157Z"},"links":{"cited_paper":"/paper/hep-th/9803137","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:d2d57500df7e170539568e31223fc1fb2a3093b3637f33547d157fbc2a204a36","observation_id":"26499220-bdef-47bb-964a-7053db80b8e7","resolution":{"observed_at":"2026-08-10T14:17:09.751157Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.12403","last_updated":"2025-01-13T15:38:01Z","snapshot_observed_at":"2026-08-10T20:40:14.519913Z","submitted_at":"2025-01-13T15:38:01Z","title":"The ordered phase of charged N=4 SYM plasma from STU","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.12403","snapshot_observed_at":"2026-08-10T14:17:09.755588Z","title":"The ordered phase of charged N=4 SYM plasma from STU,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.755588Z"},"links":{"cited_paper":"/paper/2501.12403","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:3103d48a5421e732b8cf801c6758bf88731eab984407bc512a1ca11d1e5e5f6c","observation_id":"8a0f6a78-2882-4ad0-af63-c7271117e167","resolution":{"observed_at":"2026-08-10T14:17:09.755588Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.01856","last_updated":"2025-01-12T00:58:13Z","snapshot_observed_at":"2026-08-11T15:16:28.831895Z","submitted_at":"2025-01-03T15:11:43Z","title":"The ordered phase of charged N=4 SYM plasma","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.01856","snapshot_observed_at":"2026-08-10T14:17:09.759689Z","title":"The ordered phase of charged N=4 SYM plasma,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.759689Z"},"links":{"cited_paper":"/paper/2501.01856","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:13e1435c5944b28dfb0ef70cc4aed09c723faba40370061c0e79ff0c7d0a9f9f","observation_id":"b235b9dd-81cd-4b3e-84c5-70082f633944","resolution":{"observed_at":"2026-08-10T14:17:09.759689Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.12353","last_updated":"2024-12-20T18:44:53Z","snapshot_observed_at":"2026-08-11T20:01:47.873069Z","submitted_at":"2024-12-16T20:50:17Z","title":"Instability in ${\\cal N}=4$ supersymmetric Yang-Mills theory at finite density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.12353","snapshot_observed_at":"2026-08-10T14:17:09.763632Z","title":"Instability in N = 4 supersymmetric Yang-Mills theory at finite density,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-10T14:17:09.763632Z"},"links":{"cited_paper":"/paper/2412.12353","citing_paper":"/paper/2501.15533"},"observation_digest":"sha256:c1f1dfc8ef8936d6695c09a223c17a64436b0087032b42e25fda1b43381357eb","observation_id":"f8b548d6-4d7f-4fa8-bfe9-e7ccc46a0c11","resolution":{"observed_at":"2026-08-10T14:17:09.763632Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2501.15533","last_updated":"2026-05-26T02:46:51Z","latest_version":3,"primary_category":"hep-th","snapshot_observed_at":"2026-08-10T15:35:56.418662Z","submitted_at":"2025-01-26T13:55:02Z","title":"Quark-Antiquark Potential as a Probe for Holographic Phase Transitions"},"reference_resolution":{"displayed":9,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":9,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":9},"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":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 12 August 2026, this Paper Citation Record lists 9 of 9 outbound references and 0 inbound Pith citation observations for arXiv:2501.15533."}