{"as_of":"2026-08-11T02:31:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:11df7ceeb560a074e5b2477d236a0297d34cb330bcd231febce8534a1cc5810d","coverage":[{"denominator":71,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":71,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T10:37:18.887788Z","state":"measured"},{"denominator":71,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":71,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+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/2509.03947/citation-record","integrity":"/paper/2509.03947/integrity","json":"/paper/2509.03947/citation-record.json","paper":"/paper/2509.03947"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1906.00936","last_updated":"2020-04-16T15:47:10Z","snapshot_observed_at":"2026-07-30T16:44:03.301968Z","submitted_at":"2019-06-03T17:29:52Z","title":"Mapping the Phases of Quantum Chromodynamics with Beam Energy Scan","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.00936","snapshot_observed_at":"2026-08-05T10:37:18.698651Z","title":"Bzdak, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.698651Z"},"links":{"cited_paper":"/paper/1906.00936","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:ff40b29d7c88fcc750ae3f663528a254d54c1f34fcaf807c68af93668cc74c2c","observation_id":"b34ad4c5-5de2-4e33-8981-57a2c350451f","resolution":{"observed_at":"2026-08-05T10:37:18.698651Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.04801","last_updated":"2018-02-23T09:27:32Z","snapshot_observed_at":"2026-07-06T06:23:14.334711Z","submitted_at":"2018-02-13T19:00:00Z","title":"Heavy Ion Collisions: The Big Picture, and the Big Questions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.04801","snapshot_observed_at":"2026-08-05T10:37:18.702091Z","title":"Busza, K","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.702091Z"},"links":{"cited_paper":"/paper/1802.04801","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:d69a890af19b7651e966f9860016dbdec409ec305239f6723ab4689ca21f2501","observation_id":"4a8992fb-8cf3-4fe8-8091-c673ab44267c","resolution":{"observed_at":"2026-08-05T10:37:18.702091Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.02224","last_updated":"2022-11-08T01:52:13Z","snapshot_observed_at":"2026-08-09T11:27:18.295957Z","submitted_at":"2022-11-04T02:15:29Z","title":"Long Range Plan: Dense matter theory for heavy-ion collisions and neutron stars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.02224","snapshot_observed_at":"2026-08-05T10:37:18.705106Z","title":"Lovato et al., Long Range Plan: Dense matter theory for heavy-ion collisions and neutron stars, 2211.02224","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.705106Z"},"links":{"cited_paper":"/paper/2211.02224","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:97dd1bca9866d8f80954f52b788a2bd945c995fcbdca17b723dae363925ed6a0","observation_id":"89a7304b-a89c-4c4a-876b-32d3939acc5b","resolution":{"observed_at":"2026-08-05T10:37:18.705106Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.00468","last_updated":"2022-05-01T13:51:31Z","snapshot_observed_at":"2026-08-07T03:46:32.901659Z","submitted_at":"2022-05-01T13:51:31Z","title":"QCD at finite temperature and density within the fRG approach: An overview","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.00468","snapshot_observed_at":"2026-08-05T10:37:18.708065Z","title":"Fu, QCD at finite temperature and density within the fRG approach: an overview, Commun","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.708065Z"},"links":{"cited_paper":"/paper/2205.00468","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:4950f521ed8c1ef7ac31831b7ece51777fd241b29da79591372513a3c49df823","observation_id":"1fa4f94f-b705-4784-9da7-014bd546e1b3","resolution":{"observed_at":"2026-08-05T10:37:18.708065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.15503","last_updated":"2021-02-16T10:50:04Z","snapshot_observed_at":"2026-08-09T08:58:45.497553Z","submitted_at":"2020-10-29T11:56:03Z","title":"Overview of the QCD phase diagram -- Recent progress from the lattice","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.15503","snapshot_observed_at":"2026-08-05T10:37:18.711038Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.711038Z"},"links":{"cited_paper":"/paper/2010.15503","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:906994cc49b61f7abfefb6cad921d43836ea03f390b833c05afb3ea832677aa8","observation_id":"363e41b1-a74e-407e-ad1e-4da0bf7a962b","resolution":{"observed_at":"2026-08-05T10:37:18.711038Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.10183","last_updated":"2024-05-06T23:37:53Z","snapshot_observed_at":"2026-08-11T01:54:29.948971Z","submitted_at":"2024-02-15T18:37:33Z","title":"The QCD phase diagram and Beam Energy Scan physics: a theory overview","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.10183","snapshot_observed_at":"2026-08-05T10:37:18.713911Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.713911Z"},"links":{"cited_paper":"/paper/2402.10183","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:608eea7da6b25fa4f7022bf860bce47d23cde83c73e557beaf6fca83ea61341c","observation_id":"65364e0f-330b-4d2e-92eb-48108c759475","resolution":{"observed_at":"2026-08-05T10:37:18.713911Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.00789","last_updated":"2020-04-02T03:07:51Z","snapshot_observed_at":"2026-08-07T19:47:26.493217Z","submitted_at":"2020-04-02T03:07:51Z","title":"A Study of the Properties of the QCD Phase Diagram in High-Energy Nuclear Collisions","version":1},"cited_work":{"arxiv_id":"2004.00789","doi":null,"metadata_source":"pith","pith_arxiv_id":"2004.00789","snapshot_observed_at":"2026-08-05T10:37:19.462025Z","title":"A Study of the Properties of the QCD Phase Diagram in High-Energy Nuclear Collisions","venue":"nucl-ex","work_id":"25eccd8e-6572-4e6b-bc32-68cbddef01e3","year":2020},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.716802Z"},"links":{"cited_paper":"/paper/2004.00789","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:06c3f0cfd06a509072ac74c9495fc8194386ff55d1dee8fea9c3b2abdf99987b","observation_id":"c1499a3c-3bac-4efc-9527-47a4620722c7","resolution":{"observed_at":"2026-08-05T10:37:19.465137Z","resolver_source":"local_arxiv","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":"1004.4187","last_updated":"2010-04-23T17:30:24Z","snapshot_observed_at":"2026-07-06T02:05:58.319217Z","submitted_at":"2010-04-23T17:30:24Z","title":"Energy Budget of Cosmological First-order Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1004.4187","snapshot_observed_at":"2026-08-05T10:37:18.719683Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.719683Z"},"links":{"cited_paper":"/paper/1004.4187","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:0888ef4a6207c7ecee5174c00883c8d9194b6360e9b3cccb8f27ead187f637cc","observation_id":"3a570b78-eb30-4c87-a660-1fe5bb0159c7","resolution":{"observed_at":"2026-08-05T10:37:18.719683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1105.0832","last_updated":"2011-10-10T16:55:38Z","snapshot_observed_at":"2026-07-06T02:27:16.398598Z","submitted_at":"2011-05-04T14:05:01Z","title":"A little inflation at the cosmological QCD phase transition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.0832","snapshot_observed_at":"2026-08-05T10:37:18.722642Z","title":"Boeckel and J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.722642Z"},"links":{"cited_paper":"/paper/1105.0832","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:50e8d3e19dbafe304ce1606146f1900155c7d56c7bed416ffae29920e4826f22","observation_id":"993069d2-4c56-4cf8-aa6a-5716980b4b24","resolution":{"observed_at":"2026-08-05T10:37:18.722642Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.06239","last_updated":"2016-04-01T10:50:20Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2015-12-19T12:44:06Z","title":"Science with the space-based interferometer eLISA. II: Gravitational waves from cosmological phase transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.06239","snapshot_observed_at":"2026-08-05T10:37:18.725237Z","title":"Caprini et al., Science with the space-based interferometer eLISA","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.725237Z"},"links":{"cited_paper":"/paper/1512.06239","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:c37f489619e501bacd8d627b09fac730bda0b048ebea88ee15b2ebbfaf9f78b2","observation_id":"f054dba2-7ff2-43d6-b8e6-ece1679996e1","resolution":{"observed_at":"2026-08-05T10:37:18.725237Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.16755","last_updated":"2023-09-28T18:00:04Z","snapshot_observed_at":"2026-07-06T16:25:09.382064Z","submitted_at":"2023-09-28T18:00:04Z","title":"Gravitational Waves from Composite Dark Sectors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.16755","snapshot_observed_at":"2026-08-05T10:37:18.727838Z","title":"Pasechnik, M","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.727838Z"},"links":{"cited_paper":"/paper/2309.16755","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:69e6a85835a819889dd0e321dc08dee18654202da399001d49a98b6e454004a5","observation_id":"0a04fb89-691e-4ffe-880b-eaec8337431d","resolution":{"observed_at":"2026-08-05T10:37:18.727838Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.05637","last_updated":"2022-01-14T11:58:31Z","snapshot_observed_at":"2026-08-01T15:38:56.675364Z","submitted_at":"2021-06-10T10:20:25Z","title":"Primordial black hole production during first-order phase transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.05637","snapshot_observed_at":"2026-08-05T10:37:18.730496Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.730496Z"},"links":{"cited_paper":"/paper/2106.05637","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:e1a5a1316fe4a6ff069bd1c261dff6dbdbab41c2b6cac09b576aaae47e9da69e","observation_id":"182f7f95-f496-49e4-8719-5e52b4ef9e22","resolution":{"observed_at":"2026-08-05T10:37:18.730496Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.13809","last_updated":"2023-02-11T05:56:08Z","snapshot_observed_at":"2026-08-06T05:54:43.603290Z","submitted_at":"2022-09-28T03:33:57Z","title":"Gravitational waves and primordial black holes from chirality imbalanced QCD first-order phase transition with $\\mathcal {P}$ and $\\mathcal {CP}$ violation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.13809","snapshot_observed_at":"2026-08-05T10:37:18.733014Z","title":"Shao and M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.733014Z"},"links":{"cited_paper":"/paper/2209.13809","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:6bdc2a7bcdf11546f9d7cbc2d062ec7edfee1996ac7fc12fc1e7970e4a9b8c57","observation_id":"0e90e469-2e7e-429d-a73c-77f3fec24ef9","resolution":{"observed_at":"2026-08-05T10:37:18.733014Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9806219","last_updated":"1999-03-09T22:15:39Z","snapshot_observed_at":"2026-08-10T04:16:38.504057Z","submitted_at":"1998-06-01T22:15:40Z","title":"Signatures of the Tricritical Point in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9806219","snapshot_observed_at":"2026-08-05T10:37:18.735574Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.735574Z"},"links":{"cited_paper":"/paper/hep-ph/9806219","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:0d1b84b12d82326ddcbd8c280c20c9964e55203ca8272db5ebfa3d6372960cc0","observation_id":"d0264ef0-2d59-4762-ad34-970d42c62d69","resolution":{"observed_at":"2026-08-05T10:37:18.735574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.07065","last_updated":"2017-10-14T17:32:56Z","snapshot_observed_at":"2026-07-06T05:27:25.871020Z","submitted_at":"2017-01-24T19:59:25Z","title":"Bulk Properties of the Medium Produced in Relativistic Heavy-Ion Collisions from the Beam Energy Scan Program","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.07065","snapshot_observed_at":"2026-08-05T10:37:18.738232Z","title":"Adamczyk et al., Bulk Properties of the Medium Produced in Relativistic Heavy-Ion Collisions from the Beam Energy Scan Program, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.738232Z"},"links":{"cited_paper":"/paper/1701.07065","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:31eff3f949fc5dadcdd45eb2e260a114c810d3a9761f6d7f85ce3764b6782c07","observation_id":"e89a17fd-9c39-47bc-84ed-8b5250635925","resolution":{"observed_at":"2026-08-05T10:37:18.738232Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.01056","last_updated":"2022-04-03T11:46:50Z","snapshot_observed_at":"2026-07-06T12:56:07.820484Z","submitted_at":"2022-04-03T11:46:50Z","title":"Exploring terra incognita in the phase diagram of strongly interacting matter -- Experiments at FAIR and NICA","version":1},"cited_work":{"arxiv_id":"2204.01056","doi":null,"metadata_source":"pith","pith_arxiv_id":"2204.01056","snapshot_observed_at":"2026-08-05T10:37:19.386368Z","title":"Exploring terra incognita in the phase diagram of strongly interacting matter -- Experiments at FAIR and NICA","venue":"nucl-ex","work_id":"0e6bcb34-4928-4bb7-8589-68567c610a6b","year":2022},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.740788Z"},"links":{"cited_paper":"/paper/2204.01056","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:e99b1840ea9fef25711a010ecd76726090d442e870cf7458ad4a507c246d697c","observation_id":"694bafdb-0d27-4086-9154-88b6547ce7f9","resolution":{"observed_at":"2026-08-05T10:37:19.389808Z","resolver_source":"local_arxiv","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":"2110.04462","last_updated":"2021-10-09T05:38:48Z","snapshot_observed_at":"2026-07-06T11:56:03.791657Z","submitted_at":"2021-10-09T05:38:48Z","title":"Extension of the J-PARC Hadron Experimental Facility: Third White Paper","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.04462","snapshot_observed_at":"2026-08-05T10:37:18.743542Z","title":"Aoki et al., Extension of the J-PARC Hadron Experimental Facility: Third White Paper, 2110.04462","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.743542Z"},"links":{"cited_paper":"/paper/2110.04462","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:423a41adc12201066ddddb94a62090e30974f7b6a4e20c670dc3d3591f56bdfd","observation_id":"fdbecbbf-7bb8-42dd-81d8-6829da7a7b46","resolution":{"observed_at":"2026-08-05T10:37:18.743542Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0204010","last_updated":"2002-09-02T13:38:39Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2002-04-09T14:27:19Z","title":"The QCD thermal phase transition in the presence of a small chemical potential","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0204010","snapshot_observed_at":"2026-08-05T10:37:18.746251Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.746251Z"},"links":{"cited_paper":"/paper/hep-lat/0204010","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:fbfe5f0ef18e848822144d47abc97359a5ad43c8584db14325abab280638910e","observation_id":"8fc3c086-4d84-45a0-9c2e-cea844671e17","resolution":{"observed_at":"2026-08-05T10:37:18.746251Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0501030","last_updated":"2005-03-14T10:06:42Z","snapshot_observed_at":"2026-07-07T03:42:39.583570Z","submitted_at":"2005-01-30T11:10:35Z","title":"Thermodynamics of Two Flavor QCD to Sixth Order in Quark Chemical Potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0501030","snapshot_observed_at":"2026-08-05T10:37:18.748783Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.748783Z"},"links":{"cited_paper":"/paper/hep-lat/0501030","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:da223e195cee61cf77f23c903c774b226959f5ef302eece40c0c27581a5a8cb7","observation_id":"55785940-e001-4d32-9f2b-a740f0d8d396","resolution":{"observed_at":"2026-08-05T10:37:18.748783Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.04325","last_updated":"2017-03-09T17:04:57Z","snapshot_observed_at":"2026-07-06T05:26:19.801141Z","submitted_at":"2017-01-16T15:24:41Z","title":"The QCD Equation of State to $\\mathcal{O}(\\mu_B^6)$ from Lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.04325","snapshot_observed_at":"2026-08-05T10:37:18.751316Z","title":"Bazavov et al., The QCD Equation of State toO(µ6 B) from Lattice QCD, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.751316Z"},"links":{"cited_paper":"/paper/1701.04325","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:4dcf25569d1952f75f521ec95572a534772be2d87ad2d66cfee6ba345595b222","observation_id":"68ea7a9b-5ab7-4885-a82c-0bd16733a145","resolution":{"observed_at":"2026-08-05T10:37:18.751316Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.06660","last_updated":"2021-02-12T18:03:41Z","snapshot_observed_at":"2026-08-06T03:16:38.181001Z","submitted_at":"2021-02-12T18:03:41Z","title":"Lattice QCD equation of state at finite chemical potential from an alternative expansion scheme","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.06660","snapshot_observed_at":"2026-08-05T10:37:18.753846Z","title":"Borsányi, Z","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.753846Z"},"links":{"cited_paper":"/paper/2102.06660","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:4431acb522ac4ca6f89b44b94cca0ef199ce7b088b6038970205abbea60f41e2","observation_id":"f94f26bc-cafa-4221-8c14-6e767cabfe75","resolution":{"observed_at":"2026-08-05T10:37:18.753846Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9403224","last_updated":"1997-08-11T23:07:07Z","snapshot_observed_at":"2026-07-07T04:16:50.792121Z","submitted_at":"1994-03-03T22:34:27Z","title":"Dyson-Schwinger Equations and the Application to Hadronic Physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9403224","snapshot_observed_at":"2026-08-05T10:37:18.756746Z","title":null,"venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.756746Z"},"links":{"cited_paper":"/paper/hep-ph/9403224","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:fcff07280cfe4e3cc74d9ec729da51273ca98e49e2a2e29b727a4bc1e2d2c7aa","observation_id":"02849d20-0f00-4332-8023-ef33194e6a83","resolution":{"observed_at":"2026-08-05T10:37:18.756746Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1011.2876","last_updated":"2010-11-12T10:57:17Z","snapshot_observed_at":"2026-07-06T02:19:06.235766Z","submitted_at":"2010-11-12T10:57:17Z","title":"Phase diagram and critical endpoint for strongly-interacting quarks","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1011.2876","snapshot_observed_at":"2026-08-05T10:37:18.759458Z","title":null,"venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.759458Z"},"links":{"cited_paper":"/paper/1011.2876","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:23afd2709c4f85dd12944f85ff612af03bd598f5155b3ec52bde76b0461d723b","observation_id":"cd759948-2b64-4439-b93a-8748bceb944f","resolution":{"observed_at":"2026-08-05T10:37:18.759458Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.3797","last_updated":"2014-07-03T03:22:12Z","snapshot_observed_at":"2026-08-08T12:04:17.025127Z","submitted_at":"2014-03-15T12:42:52Z","title":"Locate QCD Critical End Point in a Continuum Model Study","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.3797","snapshot_observed_at":"2026-08-05T10:37:18.762067Z","title":"Shi, Y .-L","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.762067Z"},"links":{"cited_paper":"/paper/1403.3797","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:cc00fa952b6cfdbe689e946e98c9bbb2ee80050afe497ab10a76fead38e3b65b","observation_id":"32e628e8-0658-480e-84c6-b30f764c9939","resolution":{"observed_at":"2026-08-05T10:37:18.762067Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.01675","last_updated":"2016-07-06T15:33:18Z","snapshot_observed_at":"2026-07-06T05:02:37.459715Z","submitted_at":"2016-07-06T15:33:18Z","title":"QCD phase transitions via a refined truncation of Dyson-Schwinger equations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.01675","snapshot_observed_at":"2026-08-05T10:37:18.764762Z","title":"Gao and Y .-x","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.764762Z"},"links":{"cited_paper":"/paper/1607.01675","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:afa234e57c16f85413c1237bd5fff92d331fb827c86057d775641bccc095331b","observation_id":"2a3cd65d-0fc9-4f4a-b87b-aba35ebe04c7","resolution":{"observed_at":"2026-08-05T10:37:18.764762Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9804290","last_updated":"1998-07-21T15:47:04Z","snapshot_observed_at":"2026-07-07T04:29:09.115226Z","submitted_at":"1998-04-15T03:51:30Z","title":"On the Phase Diagram of QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9804290","snapshot_observed_at":"2026-08-05T10:37:18.767510Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.767510Z"},"links":{"cited_paper":"/paper/hep-ph/9804290","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:c25844e36173f1e8f30a7ef678260d3b90c8eaa446d845b82e0dd883e140b87b","observation_id":"878c2497-0aeb-4911-bb57-8c070ba35f57","resolution":{"observed_at":"2026-08-05T10:37:18.767510Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9401310","last_updated":"1994-01-23T02:49:05Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"1994-01-23T02:49:05Z","title":"QCD Phenomenology based on a Chiral Effective Lagrangian","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9401310","snapshot_observed_at":"2026-08-05T10:37:18.770072Z","title":"Hatsuda and T","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.770072Z"},"links":{"cited_paper":"/paper/hep-ph/9401310","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:a05ede65086f4fc3a34220bc59d5af7218c870b7f99816f5a5c24d83ab857c9e","observation_id":"f4a30420-6822-429b-92e0-1b1027fa034d","resolution":{"observed_at":"2026-08-05T10:37:18.770072Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9903048","last_updated":"1999-09-08T10:13:25Z","snapshot_observed_at":"2026-07-07T06:41:51.118586Z","submitted_at":"1999-03-19T16:27:50Z","title":"The phase diagram and bulk thermodynamical quantities in the NJL model at finite temperature and density","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/9903048","snapshot_observed_at":"2026-08-05T10:37:18.772604Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.772604Z"},"links":{"cited_paper":"/paper/nucl-th/9903048","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:12591f26615e8c6e7984d409e0efd2d0abc269bce658ed6326cc5552b79630ea","observation_id":"dd14ecf3-8c3e-4e62-8c73-ecb7a90373a1","resolution":{"observed_at":"2026-08-05T10:37:18.772604Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.0539","last_updated":"2010-06-01T14:39:07Z","snapshot_observed_at":"2026-08-08T14:53:38.265649Z","submitted_at":"2010-05-04T14:27:36Z","title":"Simulating QCD at finite density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.0539","snapshot_observed_at":"2026-08-05T10:37:18.775189Z","title":"de Forcrand, Simulating QCD at finite density, PoS LA T2009(2009) 010, [1005.0539]","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.775189Z"},"links":{"cited_paper":"/paper/1005.0539","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:ba5938b270f8dd0d8dbe8fefc845d109942ab307f4e4b2ca7772c8ac5a5a5cdd","observation_id":"962bf1f1-2440-4d7e-9823-65f02fc3c785","resolution":{"observed_at":"2026-08-05T10:37:18.775189Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.05274","last_updated":"2015-04-21T01:51:31Z","snapshot_observed_at":"2026-08-10T06:44:47.943637Z","submitted_at":"2015-04-21T01:51:31Z","title":"Thermodynamics of strong-interaction matter from Lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.05274","snapshot_observed_at":"2026-08-05T10:37:18.777848Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.777848Z"},"links":{"cited_paper":"/paper/1504.05274","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:78b7924c7fbac8b201139cdc66b301cfb53c0f4049dcb60c5e603bdf885a5d93","observation_id":"3c367264-9a16-43c6-9e79-b48e03e0f9de","resolution":{"observed_at":"2026-08-05T10:37:18.777848Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":"2026-08-05T10:37:18.780482Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.780482Z"},"links":{"cited_paper":"/paper/hep-th/9711200","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:5e70b0f609f2326f65a879b3e58060c3224d72aeeb5de8d71b46259ddc057d0a","observation_id":"14eaeab3-7e90-4fbb-86da-d69beaa995c3","resolution":{"observed_at":"2026-08-05T10:37:18.780482Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9802109","last_updated":"1998-03-27T22:25:16Z","snapshot_observed_at":"2026-07-07T05:15:59.969374Z","submitted_at":"1998-02-16T18:38:17Z","title":"Gauge Theory Correlators from Non-Critical String Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9802109","snapshot_observed_at":"2026-08-05T10:37:18.783161Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.783161Z"},"links":{"cited_paper":"/paper/hep-th/9802109","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:2c5ecf3e07cbe49dffd632c6395ed9021ed2eef620e13eb268c86d91e43c1140","observation_id":"048e2daa-8da7-4adc-9ea7-e60ae1078e42","resolution":{"observed_at":"2026-08-05T10:37:18.783161Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9802150","last_updated":"1998-04-06T20:45:58Z","snapshot_observed_at":"2026-08-02T14:27:11.943858Z","submitted_at":"1998-02-20T22:41:01Z","title":"Anti De Sitter Space And Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9802150","snapshot_observed_at":"2026-08-05T10:37:18.786065Z","title":"Witten, Anti de Sitter space and holography, Adv","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.786065Z"},"links":{"cited_paper":"/paper/hep-th/9802150","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:fa14ea2c6e69c59736dd699d7dca569f5a1884090d3538d111e0c5a3fdb011b1","observation_id":"4e80437c-16d5-4999-ab92-ab36f5c5bd66","resolution":{"observed_at":"2026-08-05T10:37:18.786065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0309213","last_updated":"2003-09-23T19:51:32Z","snapshot_observed_at":"2026-08-10T08:23:19.220388Z","submitted_at":"2003-09-23T19:51:32Z","title":"Holography and hydrodynamics: diffusion on stretched horizons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0309213","snapshot_observed_at":"2026-08-05T10:37:18.788510Z","title":"Kovtun, D","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.788510Z"},"links":{"cited_paper":"/paper/hep-th/0309213","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:0becfc73e81239b8ba3230ea5fc3c47d882e78f4606a5dab17c17cb409cca604","observation_id":"a482c1ae-4039-43f8-82c6-f9f845f93f6b","resolution":{"observed_at":"2026-08-05T10:37:18.788510Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0311175","last_updated":"2003-11-19T18:24:20Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2003-11-19T18:24:20Z","title":"Universality of the shear viscosity in supergravity","version":1},"cited_work":{"arxiv_id":"hep-th/0311175","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0311175","snapshot_observed_at":"2026-08-05T10:37:19.228556Z","title":"Universality of the shear viscosity in supergravity","venue":"hep-th","work_id":"0b3873db-0d26-421c-8636-e81f31b42f4f","year":2003},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.791175Z"},"links":{"cited_paper":"/paper/hep-th/0311175","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:bad913f6c2e92fd82da084766103b6e047be03c733e99ccb049c772880b058dc","observation_id":"422bffd7-98ba-423d-a505-42d713445132","resolution":{"observed_at":"2026-08-05T10:37:19.231638Z","resolver_source":"local_arxiv","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":"0808.2354","last_updated":"2008-10-03T13:38:07Z","snapshot_observed_at":"2026-07-06T01:46:46.102553Z","submitted_at":"2008-08-18T08:45:27Z","title":"Viscosity Bound, Causality Violation and Instability with Stringy Correction and Charge","version":3},"cited_work":{"arxiv_id":"0808.2354","doi":null,"metadata_source":"pith","pith_arxiv_id":"0808.2354","snapshot_observed_at":"2026-08-05T10:37:19.217185Z","title":"Viscosity Bound, Causality Violation and Instability with Stringy Correction and Charge","venue":"hep-th","work_id":"b3c2c1b1-9cbf-4e3f-8d32-6ed29e526022","year":2008},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.793708Z"},"links":{"cited_paper":"/paper/0808.2354","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:8674929e2d68e6b1c8f2b2de143ea34977eb3f080cbd5a6acc022643051a9d64","observation_id":"07a16d20-979e-405a-bc53-e9a3880264dd","resolution":{"observed_at":"2026-08-05T10:37:19.220171Z","resolver_source":"local_arxiv","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":"0903.3246","last_updated":"2010-01-17T12:26:06Z","snapshot_observed_at":"2026-07-06T01:51:38.873738Z","submitted_at":"2009-03-18T22:37:42Z","title":"Lectures on holographic methods for condensed matter physics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.3246","snapshot_observed_at":"2026-08-05T10:37:18.796183Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.796183Z"},"links":{"cited_paper":"/paper/0903.3246","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:2e7d0dc897e32986772e2781a16d830c96d507288c7db71b5abe9b8ee0210161","observation_id":"feb17755-b2b1-4756-8589-b7b7fba5fbcb","resolution":{"observed_at":"2026-08-05T10:37:18.796183Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0904.1975","last_updated":"2009-07-27T17:32:17Z","snapshot_observed_at":"2026-07-06T01:52:44.885713Z","submitted_at":"2009-04-13T17:44:46Z","title":"Lectures on Holographic Superfluidity and Superconductivity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0904.1975","snapshot_observed_at":"2026-08-05T10:37:18.798714Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.798714Z"},"links":{"cited_paper":"/paper/0904.1975","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:908d23e8c2c0b48178bea1045d0f9b8372cf03a5bc9945e35e97ac1c86b78f64","observation_id":"195ea242-298e-4b06-8570-dc468af19d22","resolution":{"observed_at":"2026-08-05T10:37:18.798714Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.00437","last_updated":"2015-05-07T07:58:29Z","snapshot_observed_at":"2026-07-06T04:07:53.933121Z","submitted_at":"2015-02-02T11:09:36Z","title":"Introduction to Holographic Superconductor Models","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.00437","snapshot_observed_at":"2026-08-05T10:37:18.801198Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.801198Z"},"links":{"cited_paper":"/paper/1502.00437","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:70077ffea5fd6f4c343e24b279f3f7e86322c7bd7f3fd25c163cda943dbe5149","observation_id":"e18a51ed-c705-4494-bee1-f6626a64f1aa","resolution":{"observed_at":"2026-08-05T10:37:18.801198Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0711.4467","last_updated":"2007-12-17T09:50:13Z","snapshot_observed_at":"2026-07-06T01:32:58.861290Z","submitted_at":"2007-11-28T10:54:19Z","title":"Mesons in Gauge/Gravity Duals - A Review","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0711.4467","snapshot_observed_at":"2026-08-05T10:37:18.803783Z","title":"Erdmenger, N","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.803783Z"},"links":{"cited_paper":"/paper/0711.4467","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:ef159b65485c69036144506385d0fbd2850ea563599e65d2a75f01fc1dffded9","observation_id":"c195bd10-ca6b-45e8-9cd4-581554cf905f","resolution":{"observed_at":"2026-08-05T10:37:18.803783Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T10:37:18.806469Z","title":"Casalderrey-Solana, H","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.806469Z"},"links":{"citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:ae2a1154e573a6005f086a5063d4cf0ebb31aa4779682489728e21f6dd90d6a2","observation_id":"01759354-64e7-46ff-b50b-d124dd0dcbed","resolution":{"observed_at":"2026-08-05T10:37:18.806469Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.8131","last_updated":"2015-02-13T18:20:52Z","snapshot_observed_at":"2026-08-07T12:32:55.511762Z","submitted_at":"2014-07-30T17:23:56Z","title":"Light-Front Holographic QCD and Emerging Confinement","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.8131","snapshot_observed_at":"2026-08-05T10:37:18.808917Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.808917Z"},"links":{"cited_paper":"/paper/1407.8131","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:80ff78087438179899b1145e780e10402b03e4b9ecc841f262e72fd086f15486","observation_id":"c73f00c2-b52c-457c-95e6-1dd360a2d496","resolution":{"observed_at":"2026-08-05T10:37:18.808917Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.3723","last_updated":"2014-05-18T23:45:16Z","snapshot_observed_at":"2026-07-06T03:41:10.318277Z","submitted_at":"2014-04-14T19:47:02Z","title":"QCD and strongly coupled gauge theories: challenges and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.3723","snapshot_observed_at":"2026-08-05T10:37:18.811448Z","title":"Brambilla et al., QCD and Strongly Coupled Gauge Theories: Challenges and Perspectives, Eur","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.811448Z"},"links":{"cited_paper":"/paper/1404.3723","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:866e996b0640b11f719caeb4eca94ef759b42b7d5d90af4c3eef101e6f3cee40","observation_id":"d2c25300-9312-46bc-a1c1-97bd4c8b4855","resolution":{"observed_at":"2026-08-05T10:37:18.811448Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1012.1864","last_updated":"2010-12-27T19:58:57Z","snapshot_observed_at":"2026-07-06T02:20:23.825275Z","submitted_at":"2010-12-08T21:04:33Z","title":"A holographic critical point","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1012.1864","snapshot_observed_at":"2026-08-05T10:37:18.813984Z","title":"DeWolfe, S","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.813984Z"},"links":{"cited_paper":"/paper/1012.1864","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:6986044dc10d8449fa93619d48e397609ca851bed072559d4271083d11688cc5","observation_id":"13323606-9253-4755-be9b-e35564300c2e","resolution":{"observed_at":"2026-08-05T10:37:18.813984Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.2029","last_updated":"2011-08-09T20:00:00Z","snapshot_observed_at":"2026-07-06T02:32:11.304324Z","submitted_at":"2011-08-09T20:00:00Z","title":"Dynamic critical phenomena at a holographic critical point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.2029","snapshot_observed_at":"2026-08-05T10:37:18.816567Z","title":"DeWolfe, S","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.816567Z"},"links":{"cited_paper":"/paper/1108.2029","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:d0344978f1927b2929265cc2b73f48f5e88776a3871ad4c933368829c687e84c","observation_id":"e4ca835a-7c2f-4fe9-b467-71caf98fc2b8","resolution":{"observed_at":"2026-08-05T10:37:18.816567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.09062","last_updated":"2020-10-04T15:37:58Z","snapshot_observed_at":"2026-08-11T00:42:57.166529Z","submitted_at":"2020-06-16T10:45:47Z","title":"Thermodynamics of heavy quarkonium in magnetic field background","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.09062","snapshot_observed_at":"2026-08-05T10:37:18.819139Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.819139Z"},"links":{"cited_paper":"/paper/2006.09062","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:2024cb9d83badafd83e0d5c980b8b5529fe6eaf0dd5a981ac02996d0564c9869","observation_id":"f3c23bc7-15d1-41ec-9403-0e975a5ba257","resolution":{"observed_at":"2026-08-05T10:37:18.819139Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05558","last_updated":"2017-07-17T17:08:39Z","snapshot_observed_at":"2026-07-06T05:38:20.294763Z","submitted_at":"2017-04-18T22:47:21Z","title":"Dynamical vs. equilibrium properties of the QCD phase transition: a holographic perspective","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.05558","snapshot_observed_at":"2026-08-05T10:37:18.821615Z","title":"Rougemont, R","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.821615Z"},"links":{"cited_paper":"/paper/1704.05558","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:1efdeb5a33feb7341245e6b27f91ed3504bf43088dfcc71e2ebd3397a4474d2a","observation_id":"3250f605-0afe-47a1-8180-008db2639bc8","resolution":{"observed_at":"2026-08-05T10:37:18.821615Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.00139","last_updated":"2022-12-06T19:33:48Z","snapshot_observed_at":"2026-08-10T13:38:14.801852Z","submitted_at":"2022-02-28T23:27:14Z","title":"Transport coefficients of the quark-gluon plasma at the critical point and across the first-order line","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.00139","snapshot_observed_at":"2026-08-05T10:37:18.824245Z","title":"Grefa, M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.824245Z"},"links":{"cited_paper":"/paper/2203.00139","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:bb1d66d7bc1ea94fe7b997ac4d93d7750243abda3e45be59f8449a5b0eec99ae","observation_id":"eb65620b-c942-400d-b3c1-6a1fda6763ac","resolution":{"observed_at":"2026-08-05T10:37:18.824245Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.06556","last_updated":"2016-04-05T02:49:30Z","snapshot_observed_at":"2026-08-03T00:32:15.339149Z","submitted_at":"2015-07-23T16:42:11Z","title":"Energy loss, equilibration, and thermodynamics of a baryon rich strongly coupled quark-gluon plasma","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.06556","snapshot_observed_at":"2026-08-05T10:37:18.827019Z","title":"Rougemont, A","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.827019Z"},"links":{"cited_paper":"/paper/1507.06556","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:d9f67cc3a9fbad73ad3532f5d7fe39d83aa0bbf046774b9983619e817ad5a08f","observation_id":"bdc8de1c-f329-4b98-abdb-fd459b3cad96","resolution":{"observed_at":"2026-08-05T10:37:18.827019Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.04147","last_updated":"2025-04-05T11:38:09Z","snapshot_observed_at":"2026-08-07T16:08:24.604862Z","submitted_at":"2025-04-05T11:38:09Z","title":"Signals of critical end point from jet quenching and quark energy loss in holographic QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.04147","snapshot_observed_at":"2026-08-05T10:37:18.829696Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.829696Z"},"links":{"cited_paper":"/paper/2504.04147","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:73506b2999b015d837c71eb9c7d5f170258420b24e889d46979faa6b1b216195","observation_id":"376649cd-2094-4085-964b-dd7edf7911c4","resolution":{"observed_at":"2026-08-05T10:37:18.829696Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.0385","last_updated":"2013-01-03T07:44:46Z","snapshot_observed_at":"2026-07-06T03:03:11.822245Z","submitted_at":"2013-01-03T07:44:46Z","title":"Phase Structure in a Dynamical Soft-Wall Holographic QCD Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.0385","snapshot_observed_at":"2026-08-05T10:37:18.832437Z","title":"He, S.-Y","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.832437Z"},"links":{"cited_paper":"/paper/1301.0385","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:aa83af797e9150f46159d40d1940d3f05f412a09b0b3a6bd539851003520f50e","observation_id":"b3d2a5d4-a2dd-44dd-82df-29c2acbe8cc1","resolution":{"observed_at":"2026-08-05T10:37:18.832437Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.1865","last_updated":"2014-06-07T06:25:08Z","snapshot_observed_at":"2026-08-05T16:03:16.649648Z","submitted_at":"2014-06-07T06:25:08Z","title":"A Refined Holographic QCD Model and QCD Phase Structure","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.1865","snapshot_observed_at":"2026-08-05T10:37:18.835031Z","title":"Yang and P.-H","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.835031Z"},"links":{"cited_paper":"/paper/1406.1865","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:0f4ce843b78b550649a8a0747f45dd55ecf8077295f9bce9d58b2f346fbf3732","observation_id":"899634bd-9493-482b-abf4-757da6df00ea","resolution":{"observed_at":"2026-08-05T10:37:18.835031Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.06731","last_updated":"2018-01-19T14:45:32Z","snapshot_observed_at":"2026-08-06T22:17:15.031925Z","submitted_at":"2017-02-22T10:09:03Z","title":"Holographic QCD phase diagram with critical point from Einstein-Maxwell-dilaton dynamics","version":3},"cited_work":{"arxiv_id":"1702.06731","doi":null,"metadata_source":"pith","pith_arxiv_id":"1702.06731","snapshot_observed_at":"2026-08-05T10:37:19.080914Z","title":"Holographic QCD phase diagram with critical point from Einstein-Maxwell-dilaton dynamics","venue":"hep-ph","work_id":"6701d8f5-458b-48c0-94fd-f7e381e5a8ac","year":2017},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.837609Z"},"links":{"cited_paper":"/paper/1702.06731","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:a389c2692a2393f490225933b5a0e4f66a502993e537d0a83b23ac3a0f2bf461","observation_id":"6cdd1c3f-4786-4a99-97b5-754c5edcbf0d","resolution":{"observed_at":"2026-08-05T10:37:19.084407Z","resolver_source":"local_arxiv","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":"1706.00455","last_updated":"2017-11-10T01:45:56Z","snapshot_observed_at":"2026-07-06T05:45:13.627570Z","submitted_at":"2017-06-01T18:52:43Z","title":"Critical point in the phase diagram of primordial quark-gluon matter from black hole physics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.00455","snapshot_observed_at":"2026-08-05T10:37:18.840109Z","title":"Critelli, J","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.840109Z"},"links":{"cited_paper":"/paper/1706.00455","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:e52cb0d119ad964508a06b3c028314a0d6b3919093931d62ff3af79e4478dd00","observation_id":"b4c0df21-bbf3-4848-bd70-e0a426481fff","resolution":{"observed_at":"2026-08-05T10:37:18.840109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.12042","last_updated":"2021-07-14T01:52:56Z","snapshot_observed_at":"2026-08-10T21:45:58.915348Z","submitted_at":"2021-02-24T03:18:41Z","title":"Hot and dense quark-gluon plasma thermodynamics from holographic black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.12042","snapshot_observed_at":"2026-08-05T10:37:18.842648Z","title":"Grefa, J","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.842648Z"},"links":{"cited_paper":"/paper/2102.12042","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:896ea90e714c7eb9e02bedc4887ad8ba5021569e49d003209e8c927cc6deed55","observation_id":"0e94600f-f34a-4915-a2f5-2c0495b9a6bd","resolution":{"observed_at":"2026-08-05T10:37:18.842648Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02004","last_updated":"2023-02-18T02:28:23Z","snapshot_observed_at":"2026-08-06T23:31:30.629556Z","submitted_at":"2022-01-06T10:38:14Z","title":"Probing QCD critical point and induced gravitational wave by black hole physics","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.02004","snapshot_observed_at":"2026-08-05T10:37:18.848230Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.848230Z"},"links":{"cited_paper":"/paper/2201.02004","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:66b39da4a8a433ba5a968c5ed89d01d3fff68b224b1eb120ce5dbadcb16f4436","observation_id":"586fd0d0-b4cc-462a-a3cc-0568c5ec118b","resolution":{"observed_at":"2026-08-05T10:37:18.848230Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.13874","last_updated":"2023-06-05T14:05:52Z","snapshot_observed_at":"2026-08-11T02:08:35.116657Z","submitted_at":"2023-05-23T09:50:05Z","title":"Holographic study of higher-order baryon number susceptibilities at finite temperature and density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.13874","snapshot_observed_at":"2026-08-05T10:37:18.850906Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.850906Z"},"links":{"cited_paper":"/paper/2305.13874","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:16d7f60d2668c2cfddfb97bd4c977fd4c6bcfefe6dbd715d8d9e36160d6243bf","observation_id":"90e8bf0e-a05f-43d9-bb24-6fdcdfe8c1e3","resolution":{"observed_at":"2026-08-05T10:37:18.850906Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.03885","last_updated":"2023-11-27T14:27:38Z","snapshot_observed_at":"2026-08-06T23:54:18.851365Z","submitted_at":"2023-07-08T03:30:02Z","title":"Hot QCD Phase Diagram From Holographic Einstein-Maxwell-Dilaton Models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.03885","snapshot_observed_at":"2026-08-05T10:37:18.853405Z","title":"Rougemont, J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.853405Z"},"links":{"cited_paper":"/paper/2307.03885","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:bd92fdc2e7e4a2980302a7091ea6d2636e0da7ca5894ee73f01a5bcf13ba7140","observation_id":"7cdbd7e3-be80-4aca-bf9f-6844144fd7e3","resolution":{"observed_at":"2026-08-05T10:37:18.853405Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0801.2977","last_updated":"2008-01-18T21:23:56Z","snapshot_observed_at":"2026-07-06T01:34:43.058222Z","submitted_at":"2008-01-18T21:23:56Z","title":"Breaking an Abelian gauge symmetry near a black hole horizon","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0801.2977","snapshot_observed_at":"2026-08-05T10:37:18.856090Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.856090Z"},"links":{"cited_paper":"/paper/0801.2977","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:2fc7963fde96f1675944082b6a03650bb6f66a94bc9b1cd08e8559b5416d00c1","observation_id":"0afec266-391a-4050-8e3e-1ad8f9da3c2c","resolution":{"observed_at":"2026-08-05T10:37:18.856090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0810.1563","last_updated":"2008-10-09T03:40:28Z","snapshot_observed_at":"2026-08-03T01:49:40.027254Z","submitted_at":"2008-10-09T03:40:28Z","title":"Holographic Superconductors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0810.1563","snapshot_observed_at":"2026-08-05T10:37:18.858725Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.858725Z"},"links":{"cited_paper":"/paper/0810.1563","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:9838e2f958bd2d5adea50c2f36b3c69e93960516622c00de08c27b89f5b96dc7","observation_id":"93575549-557e-4fa2-a95b-19ff4697ba9d","resolution":{"observed_at":"2026-08-05T10:37:18.858725Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.3295","last_updated":"2008-03-22T21:33:37Z","snapshot_observed_at":"2026-08-06T15:11:28.876708Z","submitted_at":"2008-03-22T21:33:37Z","title":"Building an AdS/CFT superconductor","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.3295","snapshot_observed_at":"2026-08-05T10:37:18.861408Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.861408Z"},"links":{"cited_paper":"/paper/0803.3295","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:ee8ccab77e952ea42d91971129ab1a83a842b25bb0b44cff34e058f257951811","observation_id":"8718b286-e5eb-40c2-8531-915573e5242c","resolution":{"observed_at":"2026-08-05T10:37:18.861408Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.05065","last_updated":"2025-02-09T00:39:53Z","snapshot_observed_at":"2026-08-06T16:43:27.214105Z","submitted_at":"2024-10-07T14:22:39Z","title":"The underlying black hole phase transitions in an Einstein-Maxwell-dilaton model with a holographic critical point","version":3},"cited_work":{"arxiv_id":"2410.05065","doi":null,"metadata_source":"pith","pith_arxiv_id":"2410.05065","snapshot_observed_at":"2026-08-05T10:37:18.999514Z","title":"The underlying black hole phase transitions in an Einstein-Maxwell-dilaton model with a holographic critical point","venue":"hep-th","work_id":"cbb17323-56ac-4319-a822-27485c7d9603","year":2024},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.863933Z"},"links":{"cited_paper":"/paper/2410.05065","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:fcd3413495bcfebc6a74b75d144df935ddd6dea5421026e7458092f6e13dde7d","observation_id":"ae094561-852d-4221-a1ef-9358b3361917","resolution":{"observed_at":"2026-08-05T10:37:19.004583Z","resolver_source":"local_arxiv","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":"1902.05079","last_updated":"2019-08-26T15:26:51Z","snapshot_observed_at":"2026-08-05T07:16:18.554881Z","submitted_at":"2019-02-13T19:00:04Z","title":"Spontaneous scalarisation of charged black holes: coupling dependence and dynamical features","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.05079","snapshot_observed_at":"2026-08-05T10:37:18.866704Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.866704Z"},"links":{"cited_paper":"/paper/1902.05079","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:a32a0ba3226ed6e9e0db25692e638026e0859338dcff2316f5d51a7f013e2586","observation_id":"8d21d3c6-ed89-4a80-890a-ac4616635f7f","resolution":{"observed_at":"2026-08-05T10:37:18.866704Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.05190","last_updated":"2018-06-19T08:51:40Z","snapshot_observed_at":"2026-08-03T17:47:57.271173Z","submitted_at":"2018-06-13T18:00:02Z","title":"Spontaneous scalarisation of charged black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.05190","snapshot_observed_at":"2026-08-05T10:37:18.869394Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.869394Z"},"links":{"cited_paper":"/paper/1806.05190","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:86f977435d3abd1bfae6cb74d5113b024bdbc9587e60cd5fca987bb00249993e","observation_id":"b77d365a-a213-4c98-bde9-2d876b7d0c91","resolution":{"observed_at":"2026-08-05T10:37:18.869394Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0404261","last_updated":"2004-05-13T18:34:19Z","snapshot_observed_at":"2026-07-07T04:50:31.853301Z","submitted_at":"2004-04-30T18:36:23Z","title":"Black Holes with Scalar Hair and Asymptotics in N=8 Supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0404261","snapshot_observed_at":"2026-08-05T10:37:18.872138Z","title":"Hertog and K","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.872138Z"},"links":{"cited_paper":"/paper/hep-th/0404261","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:0ca30f33bec1acd81264834169fa1cadf054a26bf6f2d9dc12e6c0361d27392c","observation_id":"76ed94d5-7e45-46ed-89b0-216b5b5e1465","resolution":{"observed_at":"2026-08-05T10:37:18.872138Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.2833","last_updated":"2011-03-21T02:01:27Z","snapshot_observed_at":"2026-07-06T02:24:51.089060Z","submitted_at":"2011-03-15T03:00:53Z","title":"Analytical Studies on Holographic Superconductors in Gauss-Bonnet Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.2833","snapshot_observed_at":"2026-08-05T10:37:18.874868Z","title":"Li, R.-G","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.874868Z"},"links":{"cited_paper":"/paper/1103.2833","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:9c0c9da5c45cbfb53f5325e726eee6d7c2f9052761475afc2adbd2812d8a61c9","observation_id":"73f8907d-6be8-4f7c-a787-8bb635292566","resolution":{"observed_at":"2026-08-05T10:37:18.874868Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.10659","last_updated":"2020-10-14T08:39:29Z","snapshot_observed_at":"2026-08-09T01:59:15.931114Z","submitted_at":"2020-06-18T16:34:36Z","title":"Spontaneous Holographic Scalarization of Black Holes in Einstein-Scalar-Gauss-Bonnet Theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.10659","snapshot_observed_at":"2026-08-05T10:37:18.877581Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.877581Z"},"links":{"cited_paper":"/paper/2006.10659","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:ad1e5eebc15498a9652181ef16af8ff1f539d998100194d0ab8449409cd983f7","observation_id":"8d065c82-7961-4c63-9136-d4bf22aabf56","resolution":{"observed_at":"2026-08-05T10:37:18.877581Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.09846","last_updated":"2024-05-15T18:36:19Z","snapshot_observed_at":"2026-07-06T17:17:15.712197Z","submitted_at":"2024-01-18T10:03:47Z","title":"Phase structure of holographic superconductors in an Einstein-scalar-Gauss-Bonnet theory with spontaneous scalarization","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.09846","snapshot_observed_at":"2026-08-05T10:37:18.880099Z","title":"Guo, W.-L","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.880099Z"},"links":{"cited_paper":"/paper/2401.09846","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:3d0f618a563f0ef25078a475aa78de36e48f47da6811ed7b2b77fe0961d80dac","observation_id":"c90c5121-452d-4abc-a702-8a2af52c8d46","resolution":{"observed_at":"2026-08-05T10:37:18.880099Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.01950","last_updated":"2020-05-12T09:06:01Z","snapshot_observed_at":"2026-07-06T08:34:55.890866Z","submitted_at":"2019-11-05T17:20:53Z","title":"Scalarization of asymptotically Anti-de Sitter black holes with applications to holographic phase transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1911.01950","snapshot_observed_at":"2026-08-05T10:37:18.882631Z","title":"Brihaye, B","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.882631Z"},"links":{"cited_paper":"/paper/1911.01950","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:aa9c0e0b47dfa9d89cc3fd84d90760897b2296a9cb179ffe90eea6130aa21651","observation_id":"c33afbf1-561d-4199-93ae-b7d0d92f22f1","resolution":{"observed_at":"2026-08-05T10:37:18.882631Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9511071","last_updated":"1995-11-10T18:17:34Z","snapshot_observed_at":"2026-08-05T00:23:32.893452Z","submitted_at":"1995-11-10T18:17:34Z","title":"Dilatonic Black Holes in Higher Curvature String Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9511071","snapshot_observed_at":"2026-08-05T10:37:18.885211Z","title":"Kanti, N","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.885211Z"},"links":{"cited_paper":"/paper/hep-th/9511071","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:a6c004aa1e5de8cba54173e3c7084073311190907ee61933fb930b9f258b256f","observation_id":"08a8d8f5-add6-439f-8efb-002ae5b15277","resolution":{"observed_at":"2026-08-05T10:37:18.885211Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9606034","last_updated":"1996-06-19T04:18:00Z","snapshot_observed_at":"2026-08-10T08:41:26.570716Z","submitted_at":"1996-06-17T04:12:46Z","title":"Dilatonic Black Holes with Gauss-Bonnet Term","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9606034","snapshot_observed_at":"2026-08-05T10:37:18.887788Z","title":"Torii, H","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-05T10:37:18.887788Z"},"links":{"cited_paper":"/paper/gr-qc/9606034","citing_paper":"/paper/2509.03947"},"observation_digest":"sha256:1c4c93e5d32078f541d7428f9a617b7d797ee6e1e047f6da82d66218d659cdf6","observation_id":"c1d64458-1330-473c-abfa-30f1cec9ff85","resolution":{"observed_at":"2026-08-05T10:37:18.887788Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2509.03947","last_updated":"2025-09-04T07:17:05Z","latest_version":1,"primary_category":"hep-th","snapshot_observed_at":"2026-08-06T11:04:32.394190Z","submitted_at":"2025-09-04T07:17:05Z","title":"A Critical Point on the Hairy Black Hole Phase Boundary in the Improved Holographic Einstein-Maxwell-Dilaton Theory"},"reference_resolution":{"displayed":71,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":65,"verified_exact":6,"verified_fuzzy":0},"total_outbound_references":71},"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 11 August 2026, this Paper Citation Record lists 71 of 71 outbound references and 0 inbound Pith citation observations for arXiv:2509.03947."}