{"as_of":"2026-08-07T19:07:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:d28d5f9b62ec32e63f3c759b079b6d3ec5f016ff7e3878f0f2437a266f6b047e","coverage":[{"denominator":73,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":73,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T18:13:00.864648Z","state":"measured"},{"denominator":74,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":74,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-07T06:34:17.273281+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-01T13:22:35.819653Z","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":[{"citation":{"cited_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.09113","snapshot_observed_at":"2026-08-01T13:22:35.819653Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.19149","last_updated":"2026-07-21T14:45:47Z","snapshot_observed_at":"2026-08-07T05:12:54.762322Z","submitted_at":"2026-07-21T14:45:47Z","title":"Flavor-Dependent QCD Critical Endpoint and Dual-Channel Fluctuations from Multi-Charge Holography","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-01T13:22:35.819653Z"},"links":{"cited_paper":"/paper/2507.09113","citing_paper":"/paper/2607.19149"},"observation_digest":"sha256:e0a6e5b7bc124135fa90e125dfb96482d063ffc36b51dee4e8959f180e341fcc","observation_id":"62e7acb9-b978-4a25-a2d4-fedb7f79157a","resolution":{"observed_at":"2026-08-01T13:22:35.819653Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2507.09113/citation-record","integrity":"/paper/2507.09113/integrity","json":"/paper/2507.09113/citation-record.json","paper":"/paper/2507.09113"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1711.01261","last_updated":"2018-06-08T16:23:20Z","snapshot_observed_at":"2026-07-06T06:07:38.769231Z","submitted_at":"2017-11-03T17:48:04Z","title":"Cluster Expansion Model for QCD Baryon Number Fluctuations: No Phase Transition at $\\mu_B / T < \\pi$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.01261","snapshot_observed_at":"2026-08-06T18:12:58.788365Z","title":"Cluster Expansion Model for QCD Baryon Number Fluctuations: No Phase Transition at µB/T < π,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.788365Z"},"links":{"cited_paper":"/paper/1711.01261","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:9f28dcf70ded623a6dcc782e0315dc12a769d671d77ba70403106c3b4dd64481","observation_id":"b52c9710-a9ae-4cc8-a571-0f2157caf644","resolution":{"observed_at":"2026-08-06T18:12:58.788365Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.02821","last_updated":"2020-02-07T14:48:56Z","snapshot_observed_at":"2026-08-02T21:42:56.588707Z","submitted_at":"2020-02-07T14:48:56Z","title":"The QCD crossover at finite chemical potential from lattice simulations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.02821","snapshot_observed_at":"2026-08-06T18:12:58.823653Z","title":"QCD Crossover at Finite Chemical Potential from Lattice Simulations,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.823653Z"},"links":{"cited_paper":"/paper/2002.02821","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:34f24293270a46d334a639d143b089638cc86fdadde482e6c37b234b647509a6","observation_id":"4187f9bc-2fba-489d-a395-96b1286fac18","resolution":{"observed_at":"2026-08-06T18:12:58.823653Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.08530","last_updated":"2020-04-03T16:26:21Z","snapshot_observed_at":"2026-08-03T20:56:53.418807Z","submitted_at":"2020-01-23T14:07:31Z","title":"Skewness, kurtosis and the 5th and 6th order cumulants of net baryon-number distributions from lattice QCD confront high-statistics STAR data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.08530","snapshot_observed_at":"2026-08-06T18:12:58.843296Z","title":"Skewness, kurtosis, and the fifth and sixth order cumulants of net baryon-number distributions from lattice QCD confront high-statistics STAR data,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.843296Z"},"links":{"cited_paper":"/paper/2001.08530","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:9d2087a24e5ab94f37d3894875686efb0d120cfcf669dbd444df747d0a88db75","observation_id":"a08dd179-39df-4140-9373-d52aa1d1033d","resolution":{"observed_at":"2026-08-06T18:12:58.843296Z","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":"2026-08-06T18:12:58.866807Z","title":"Lattice QCD equation of state at finite chemical potential from an alternative expansion scheme,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.866807Z"},"links":{"cited_paper":"/paper/2102.06660","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:9041a4b1869e0c582133e5f6e191446e786811fcd457381ab726c59c19e257c7","observation_id":"7da9fcb3-7539-4053-ad76-464de47e95b9","resolution":{"observed_at":"2026-08-06T18:12:58.866807Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.09043","last_updated":"2023-07-20T09:12:27Z","snapshot_observed_at":"2026-08-03T16:18:01.549670Z","submitted_at":"2022-12-18T09:30:14Z","title":"Equation of state and speed of sound of (2+1)-flavor QCD in strangeness-neutral matter at non-vanishing net baryon-number density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.09043","snapshot_observed_at":"2026-08-06T18:12:58.901738Z","title":"Equation of state and speed of sound of (2+1)-flavor QCD in strangeness-neutral matter at non-vanishing net baryon-number density,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.901738Z"},"links":{"cited_paper":"/paper/2212.09043","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:b8aa3ca24fab5c0ea51d8ad8a1fbd9b127f3b6c81585ffe36dae3f728e860c81","observation_id":"4a4dd03e-5956-4423-b0cb-904af70502e3","resolution":{"observed_at":"2026-08-06T18:12:58.901738Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.03590","last_updated":"2021-11-05T16:23:24Z","snapshot_observed_at":"2026-08-06T14:07:46.197465Z","submitted_at":"2021-11-05T16:23:24Z","title":"Lattice Constraints on the QCD Chiral Phase Transition at Finite Temperature and Baryon Density","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.03590","snapshot_observed_at":"2026-08-06T18:12:58.937784Z","title":"Lattice Constraints on the QCD Chiral Phase Transition at Finite Temperature and Baryon Density,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.937784Z"},"links":{"cited_paper":"/paper/2111.03590","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:d0f96cbd75710079a1dc1baf3fd0751045debca8b0a41a58b122574f986c7c66","observation_id":"8caaccbf-b070-4573-834b-1a67c197654e","resolution":{"observed_at":"2026-08-06T18:12:58.937784Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0904.2089","last_updated":"2009-12-29T11:28:34Z","snapshot_observed_at":"2026-07-06T01:52:34.964765Z","submitted_at":"2009-04-14T10:11:20Z","title":"Third moments of conserved charges as probes of QCD phase structure","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0904.2089","snapshot_observed_at":"2026-08-06T18:12:58.974142Z","title":"Third moments of conserved charges as probes of QCD phase structure,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:58.974142Z"},"links":{"cited_paper":"/paper/0904.2089","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:4b771a14d37eb7f4cfd7b313f0e8a2d74078f2dd7138a191ed19ca8420cc1d8e","observation_id":"5d5e8890-56fd-4868-909f-6dbe6fc636fd","resolution":{"observed_at":"2026-08-06T18:12:58.974142Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6871","last_updated":"2012-02-15T14:22:36Z","snapshot_observed_at":"2026-07-06T02:38:26.924581Z","submitted_at":"2011-11-29T16:10:35Z","title":"QCD critical region and higher moments for three flavor models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6871","snapshot_observed_at":"2026-08-06T18:12:59.009953Z","title":"QCD critical region and higher moments for three flavor models,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.009953Z"},"links":{"cited_paper":"/paper/1111.6871","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:7369a95c5344f563eff06fd378f26f6f664967bd9d7a0b3e19827b588ae149ca","observation_id":"c2d392bc-dede-49a0-8fc9-6b86c887dd34","resolution":{"observed_at":"2026-08-06T18:12:59.009953Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.07903","last_updated":"2016-12-20T09:51:20Z","snapshot_observed_at":"2026-07-06T05:08:26.261632Z","submitted_at":"2016-08-29T03:32:31Z","title":"Susceptibilities of Conserved Charges within a Modified Nambu-Jona-Lasinio Model","version":4},"cited_work":{"arxiv_id":"1608.07903","doi":null,"metadata_source":"pith","pith_arxiv_id":"1608.07903","snapshot_observed_at":"2026-08-06T18:13:03.704100Z","title":"Susceptibilities of Conserved Charges within a Modified Nambu-Jona-Lasinio Model","venue":"hep-ph","work_id":"5084854b-f1bb-4f6c-a5eb-dc2ff1fdec1a","year":2016},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.047135Z"},"links":{"cited_paper":"/paper/1608.07903","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:a36aff407d7e32b30eeb73672de0fa369f4e48cc86e7fae6ce4fa9e22b0792b2","observation_id":"679f9de8-bdb3-4d1a-9ca8-deee6c39bb58","resolution":{"observed_at":"2026-08-06T18:13:03.782653Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1610.09981","last_updated":"2016-10-31T15:45:40Z","snapshot_observed_at":"2026-07-06T05:16:49.234920Z","submitted_at":"2016-10-31T15:45:40Z","title":"Susceptibilities from a black hole engineered EoS with a critical point","version":1},"cited_work":{"arxiv_id":"1610.09981","doi":null,"metadata_source":"pith","pith_arxiv_id":"1610.09981","snapshot_observed_at":"2026-08-06T18:13:03.467504Z","title":"Susceptibilities from a black hole engineered EoS with a critical point","venue":"nucl-th","work_id":"11ffa205-5a07-4213-a1e0-9d0e59f4979b","year":2016},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.082242Z"},"links":{"cited_paper":"/paper/1610.09981","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:25e620594fb36ae8079e74cf77658a31fe1bdcd2c9dfcfa3a49091397c8d60c1","observation_id":"6ef59b85-148d-403a-8026-d8a1aef08e52","resolution":{"observed_at":"2026-08-06T18:13:03.571413Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1702.08674","last_updated":"2017-02-28T07:22:31Z","snapshot_observed_at":"2026-07-06T05:31:40.572534Z","submitted_at":"2017-02-28T07:22:31Z","title":"Identifying the presence of the critical end point in QCD phase diagram by higher order susceptibilities","version":1},"cited_work":{"arxiv_id":"1702.08674","doi":null,"metadata_source":"pith","pith_arxiv_id":"1702.08674","snapshot_observed_at":"2026-08-06T18:13:03.255173Z","title":"Identifying the presence of the critical end point in QCD phase diagram by higher order susceptibilities","venue":"hep-ph","work_id":"994639fd-d89d-4286-8641-0afb9a92beeb","year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.117562Z"},"links":{"cited_paper":"/paper/1702.08674","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:c33febd8e7b6eff40109dffc82082a33749b926589bd85c1faa814423a5e3984","observation_id":"56f0cf31-d194-4f6c-bdf7-425ee14d6d6c","resolution":{"observed_at":"2026-08-06T18:13:03.346483Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1706.02238","last_updated":"2017-06-07T16:21:18Z","snapshot_observed_at":"2026-07-06T05:45:57.083160Z","submitted_at":"2017-06-07T16:21:18Z","title":"Locating the QCD critical end point through the peaked baryon number susceptibilities along the freeze-out line","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.02238","snapshot_observed_at":"2026-08-06T18:12:59.145906Z","title":"Locating the QCD critical end point through the peaked baryon number susceptibilities along the freeze-out line,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.145906Z"},"links":{"cited_paper":"/paper/1706.02238","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:451759308c0a56e78f220a2f1e0bfa76fe446c054362aaed473767edacc781b7","observation_id":"bca622d8-2667-4123-8181-27e010147b3e","resolution":{"observed_at":"2026-08-06T18:12:59.145906Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.09215","last_updated":"2019-01-29T19:27:24Z","snapshot_observed_at":"2026-07-06T06:20:35.413488Z","submitted_at":"2018-01-28T11:58:41Z","title":"The kurtosis of net baryon number fluctuations from a realistic Polyakov--Nambu--Jona-Lasinio model along the experimental freeze-out line","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.09215","snapshot_observed_at":"2026-08-06T18:12:59.181849Z","title":"The kurtosis of net baryon number fluctuations from a realistic Polyakov–Nambu–Jona-Lasinio model along the experimental freeze-out line,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.181849Z"},"links":{"cited_paper":"/paper/1801.09215","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:7d095077c4df3bfccbc0c3700c9dc72d0befd23e26222ad40eee5d1a4c5f5bd2","observation_id":"979d7e1d-dcfe-4698-8705-04d0c6008f8a","resolution":{"observed_at":"2026-08-06T18:12:59.181849Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.06035","last_updated":"2022-02-27T03:42:07Z","snapshot_observed_at":"2026-08-06T20:47:04.908240Z","submitted_at":"2021-01-15T09:54:04Z","title":"Hyper-order baryon number fluctuations at finite temperature and density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.06035","snapshot_observed_at":"2026-08-06T18:12:59.217207Z","title":"Hyper-order baryon number fluctuations at finite temperature and density,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.217207Z"},"links":{"cited_paper":"/paper/2101.06035","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:a9c6854a47318ce543d26b92c277361dd068b61ff67c14d9a58e418e49f01e18","observation_id":"c53420b3-601f-4dce-a695-000b034203b8","resolution":{"observed_at":"2026-08-06T18:12:59.217207Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.12010","last_updated":"2023-02-23T13:29:41Z","snapshot_observed_at":"2026-08-03T17:50:01.849791Z","submitted_at":"2023-02-23T13:29:41Z","title":"Nonextensive effects on QCD chiral phase diagram and baryon-number fluctuations within Polyakov-Nambu-Jona-Lasinio model","version":1},"cited_work":{"arxiv_id":"2302.12010","doi":null,"metadata_source":"pith","pith_arxiv_id":"2302.12010","snapshot_observed_at":"2026-08-06T18:13:03.045400Z","title":"Nonextensive effects on QCD chiral phase diagram and baryon-number fluctuations within Polyakov-Nambu-Jona-Lasinio model","venue":"hep-ph","work_id":"729e675f-0293-48c7-8be3-468211bd1cf5","year":2023},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.246052Z"},"links":{"cited_paper":"/paper/2302.12010","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:d863676ebba3bdf22bdf6625cf7e3883836dd1eb66b511e803d52b2a08092dfa","observation_id":"27c49f2a-2e45-4989-801a-e0bed9a40bf3","resolution":{"observed_at":"2026-08-06T18:13:03.092727Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2305.13874","last_updated":"2023-06-05T14:05:52Z","snapshot_observed_at":"2026-07-06T15:31:18.144952Z","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":"2026-08-06T18:12:59.282322Z","title":"Holographic study of higher-order baryon number susceptibilities at finite temperature and density,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.282322Z"},"links":{"cited_paper":"/paper/2305.13874","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:f3168c43c50cc700b30d8fa33b835adc70f10dae3d9a20ac34c7ff90ea5b8458","observation_id":"a3b48173-31f0-4672-ac76-1475c8617380","resolution":{"observed_at":"2026-08-06T18:12:59.282322Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1104.1627","last_updated":"2011-04-08T19:16:19Z","snapshot_observed_at":"2026-07-06T02:26:03.723768Z","submitted_at":"2011-04-08T19:16:19Z","title":"On the sign of kurtosis near the QCD critical point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.1627","snapshot_observed_at":"2026-08-06T18:12:59.318887Z","title":"On the sign of kurtosis near the QCD critical point,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.318887Z"},"links":{"cited_paper":"/paper/1104.1627","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:7a3319aed22e273e99221d43d656dda34c205c160c024fc5442e1157f6787dbc","observation_id":"34a5d477-921e-4868-97a8-90bf97b6fa67","resolution":{"observed_at":"2026-08-06T18:12:59.318887Z","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":"2026-08-06T18:12:59.353069Z","title":"Bulk Properties of the Medium Produced in Relativistic Heavy-Ion Collisions from the Beam Energy Scan Program,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.353069Z"},"links":{"cited_paper":"/paper/1701.07065","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:4f5189a37b55fe0dc38d8858cf84bb903ee25a9d4ce7c4a82b4171c2da5b21c6","observation_id":"d52b3471-bdbc-4e9d-bf44-8e1a8389c73d","resolution":{"observed_at":"2026-08-06T18:12:59.353069Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.01021","last_updated":"2017-05-02T15:27:31Z","snapshot_observed_at":"2026-07-06T05:40:29.102400Z","submitted_at":"2017-05-02T15:27:31Z","title":"Baryon susceptibilities from a holographic equation of state","version":1},"cited_work":{"arxiv_id":"1705.01021","doi":null,"metadata_source":"pith","pith_arxiv_id":"1705.01021","snapshot_observed_at":"2026-08-06T18:13:02.867831Z","title":"Baryon susceptibilities from a holographic equation of state","venue":"nucl-th","work_id":"c1da10fc-14f5-4718-a6ac-a74d98023445","year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.388764Z"},"links":{"cited_paper":"/paper/1705.01021","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:38556a60eaa4c98a97c7497e7ec7289a0c7762d7d97091f9e4297334cd9df5ae","observation_id":"e2a55f84-72e7-4d82-b57c-abcfc93aff44","resolution":{"observed_at":"2026-08-06T18:13:02.901550Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1808.01931","last_updated":"2019-01-12T01:11:39Z","snapshot_observed_at":"2026-07-06T06:54:15.356839Z","submitted_at":"2018-08-06T14:36:34Z","title":"Quark matter under rotation in the NJL model with vector interaction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.01931","snapshot_observed_at":"2026-08-06T18:12:59.422718Z","title":"Quark matter under rotation in the NJL model with vector interaction,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.422718Z"},"links":{"cited_paper":"/paper/1808.01931","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:7ed9aebcdf251c3ce7ded1caf69b5631d34ed1da96404e584e85a5aae98fe61d","observation_id":"bb3a507f-a06f-4c30-b285-dd23874322cd","resolution":{"observed_at":"2026-08-06T18:12:59.422718Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T18:13:04.012491Z","title":"QCD Matter and Phase Transitions under Extreme Conditions,","venue":null,"work_id":"559c8337-96d6-4aab-82fb-50cf05127eb5","year":2023},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.444841Z"},"links":{"citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:da1ddeb92451b57b23f085d1120e9d76216f1a1d5e10da2a38234b3f2227e03d","observation_id":"80f20276-a343-4d11-844b-d6130af7a595","resolution":{"observed_at":"2026-08-06T18:13:04.050946Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2504.00817","last_updated":"2025-04-01T14:05:36Z","snapshot_observed_at":"2026-08-07T16:17:21.057561Z","submitted_at":"2025-04-01T14:05:36Z","title":"Precision Measurement of (Net-)proton Number Fluctuations in Au+Au Collisions at RHIC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.00817","snapshot_observed_at":"2026-08-06T18:12:59.473216Z","title":"Precision Measurement of (Net-)proton Number Fluctuations in Au+Au Collisions at RHIC,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.473216Z"},"links":{"cited_paper":"/paper/2504.00817","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:e7ae9d351bc99dce8cd9d99b82d742036a285d6565eadbd64c56ba7bee32f19a","observation_id":"69bdf748-23bb-4d41-97f0-6e2467122064","resolution":{"observed_at":"2026-08-06T18:12:59.473216Z","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":"2026-08-06T18:12:59.493313Z","title":"A holographic critical point,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.493313Z"},"links":{"cited_paper":"/paper/1012.1864","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:0f92bce17e10f4ad10be45e8dd3a4f5693c1e127700b158197593f6b27c05a17","observation_id":"fdee6e2e-0d46-410d-8be9-382a59ed73e8","resolution":{"observed_at":"2026-08-06T18:12:59.493313Z","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":"2026-08-06T18:12:59.524644Z","title":"Dynamic critical phenomena at a holographic critical point,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.524644Z"},"links":{"cited_paper":"/paper/1108.2029","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:bc546fbf0510f95c834826079bec656bc5828918738b45c3157ba92e72ebac26","observation_id":"60cc3a81-4cac-4281-8f29-2547bea69d89","resolution":{"observed_at":"2026-08-06T18:12:59.524644Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1201.0820","last_updated":"2012-02-26T06:03:03Z","snapshot_observed_at":"2026-08-02T08:11:43.584059Z","submitted_at":"2012-01-04T04:59:06Z","title":"A hQCD model and its phase diagram in Einstein-Maxwell-Dilaton system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.0820","snapshot_observed_at":"2026-08-06T18:12:59.556649Z","title":"A hQCD model and its phase diagram in Einstein-Maxwell-Dilaton system,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.556649Z"},"links":{"cited_paper":"/paper/1201.0820","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:9cec32ca2c99f9e549a4d64f98114e79762166aee1937260845f3bdcbc504c5d","observation_id":"a2138aef-b812-4e3c-bead-52263239bcb5","resolution":{"observed_at":"2026-08-06T18:12:59.556649Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.4512","last_updated":"2013-01-24T02:33:10Z","snapshot_observed_at":"2026-07-06T02:55:58.956343Z","submitted_at":"2012-09-20T12:37:55Z","title":"Some aspects of QGP phase in a hQCD model","version":2},"cited_work":{"arxiv_id":"1209.4512","doi":null,"metadata_source":"pith","pith_arxiv_id":"1209.4512","snapshot_observed_at":"2026-08-06T18:13:02.628545Z","title":"Some aspects of QGP phase in a hQCD model","venue":"hep-th","work_id":"ea33fe8e-96aa-4aaf-ad59-5448ccc12f8f","year":2012},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.591864Z"},"links":{"cited_paper":"/paper/1209.4512","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:e8f1db48af6d63ef471ddafa0a55cb5a9105f115a49bd66679b0552f1689e816","observation_id":"6a370424-ec4f-421f-92da-98c69c98ca5d","resolution":{"observed_at":"2026-08-06T18:13:02.725689Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1311.6675","last_updated":"2013-11-26T14:01:59Z","snapshot_observed_at":"2026-07-06T03:29:14.869368Z","submitted_at":"2013-11-26T14:01:59Z","title":"A holographic calculation of the electric conductivity of the strongly coupled quark-gluon plasma near the deconfinement transition","version":1},"cited_work":{"arxiv_id":"1311.6675","doi":null,"metadata_source":"pith","pith_arxiv_id":"1311.6675","snapshot_observed_at":"2026-08-06T18:13:02.480698Z","title":"A holographic calculation of the electric conductivity of the strongly coupled quark-gluon plasma near the deconfinement transition","venue":"hep-th","work_id":"d47aaacf-a029-49c5-97e2-b76f4455d803","year":2013},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.617675Z"},"links":{"cited_paper":"/paper/1311.6675","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:e673fdbf4845a75e6f07e6960f5ebfd0cb11d947987809a7dd60dc80c31deff9","observation_id":"d429a537-1168-45ac-8371-14b9bc928781","resolution":{"observed_at":"2026-08-06T18:13:02.569660Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"2026-08-06T18:12:59.647035Z","title":"A Refined Holographic QCD Model and QCD Phase Structure,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.647035Z"},"links":{"cited_paper":"/paper/1406.1865","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:fa6ba258eface43a845fc1c140b37d735fc23fac5215cced1a37f8c5ca5ab351","observation_id":"ab0e83aa-5dc4-48ec-a7d5-880cbadd8f56","resolution":{"observed_at":"2026-08-06T18:12:59.647035Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":"2026-08-06T18:12:59.678245Z","title":"Critical point in the phase diagram of primordial quark-gluon matter from black hole physics,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.678245Z"},"links":{"cited_paper":"/paper/1706.00455","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:cb6ee4e2fe67f3f41a1148d61406fb12fd607072dfc4d50cec32b790da978311","observation_id":"0f49b534-5f11-4135-beb4-d16836caaffb","resolution":{"observed_at":"2026-08-06T18:12:59.678245Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.03470","last_updated":"2017-12-10T04:10:06Z","snapshot_observed_at":"2026-08-01T16:20:28.325904Z","submitted_at":"2017-12-10T04:10:06Z","title":"Gravitation waves from QCD and electroweak phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.03470","snapshot_observed_at":"2026-08-06T18:12:59.704247Z","title":"Gravitation waves from QCD and electroweak phase transitions,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.704247Z"},"links":{"cited_paper":"/paper/1712.03470","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:6618e6624831f96689afa0e6915be4bae2742d809b4920f32c924e687ea63c8e","observation_id":"7207f55f-22fc-46ad-9cae-981d34cdf0c1","resolution":{"observed_at":"2026-08-06T18:12:59.704247Z","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":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.06731","snapshot_observed_at":"2026-08-06T18:12:59.736299Z","title":"Holographic QCD phase diagram with critical point from Einstein–Maxwell-dilaton dynamics,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.736299Z"},"links":{"cited_paper":"/paper/1702.06731","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:8c912348d05157f77b72f7062047629a4c564ef7c1b223d2c99221594a208208","observation_id":"ebe0eb89-ac64-4bb8-861f-16fe5356b207","resolution":{"observed_at":"2026-08-06T18:12:59.736299Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12525","last_updated":"2018-10-30T04:40:37Z","snapshot_observed_at":"2026-07-06T07:11:21.870009Z","submitted_at":"2018-10-30T04:40:37Z","title":"Chiral phase transition and QCD phase diagram from AdS/QCD","version":1},"cited_work":{"arxiv_id":"1810.12525","doi":null,"metadata_source":"pith","pith_arxiv_id":"1810.12525","snapshot_observed_at":"2026-08-06T18:13:02.321217Z","title":"Chiral phase transition and QCD phase diagram from AdS/QCD","venue":"hep-ph","work_id":"7d90cdb0-1e60-42d4-ba75-d52121ecec91","year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.763055Z"},"links":{"cited_paper":"/paper/1810.12525","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:fc21bef559c047dee9aa28a0a196164107b9a9b6a44784e791f7045e0e472d9f","observation_id":"d22d7944-e998-4178-a9e4-ae9158676e95","resolution":{"observed_at":"2026-08-06T18:13:02.358687Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2006.08810","last_updated":"2020-12-04T01:31:46Z","snapshot_observed_at":"2026-07-06T09:29:27.671659Z","submitted_at":"2020-06-15T22:38:23Z","title":"Criticality from Einstein-Maxwell-dilaton holography at finite temperature and density","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.08810","snapshot_observed_at":"2026-08-06T18:12:59.793744Z","title":"Criticality from Einstein-Maxwell-dilaton holography at finite temperature and density,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.793744Z"},"links":{"cited_paper":"/paper/2006.08810","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:4d3820fb56a28d658a955fae6c1fe0e3bc91ca4af380e5f95eef47a04c4459f2","observation_id":"a1c0f290-0afe-45b8-87d0-71ae32526e87","resolution":{"observed_at":"2026-08-06T18:12:59.793744Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.05694","last_updated":"2020-11-24T08:36:28Z","snapshot_observed_at":"2026-08-07T18:43:20.902975Z","submitted_at":"2020-09-12T01:04:08Z","title":"Analytic Study on Chiral Phase Transition in Holographic QCD","version":2},"cited_work":{"arxiv_id":"2009.05694","doi":null,"metadata_source":"pith","pith_arxiv_id":"2009.05694","snapshot_observed_at":"2026-08-06T18:13:02.200242Z","title":"Analytic Study on Chiral Phase Transition in Holographic QCD","venue":"hep-th","work_id":"dc2d090f-d001-4118-858c-02365a19abc2","year":2020},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.822053Z"},"links":{"cited_paper":"/paper/2009.05694","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:0d744c371a0ea3c5fa36139497078f887b33834f0af5d95992f61e3fcf8fc1c3","observation_id":"ad177a64-3012-4a55-858b-5f01b81a7a1b","resolution":{"observed_at":"2026-08-06T18:13:02.222845Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2102.12042","last_updated":"2021-07-14T01:52:56Z","snapshot_observed_at":"2026-08-07T10:59:51.049420Z","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":"2026-08-06T18:12:59.855014Z","title":"Hot and dense quark-gluon plasma thermodynamics from holographic black holes,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.855014Z"},"links":{"cited_paper":"/paper/2102.12042","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:9acb7a8ebf3b6075fb16f27710eca11a0c46c41d85761c0cd6b7bf7b27cd1813","observation_id":"769aceb8-8cee-4db0-8f4e-d8d235d136c6","resolution":{"observed_at":"2026-08-06T18:12:59.855014Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.14094","last_updated":"2024-01-09T15:24:11Z","snapshot_observed_at":"2026-07-31T02:34:42.950727Z","submitted_at":"2022-10-25T15:23:32Z","title":"Gravitational Waves and Primordial Black Hole Productions from Gluodynamics by Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.14094","snapshot_observed_at":"2026-08-06T18:12:59.892544Z","title":"Gravitational waves and primordial black hole productions from gluodynamics by holography,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.892544Z"},"links":{"cited_paper":"/paper/2210.14094","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:e566be7aa835818b58b17a34d9fab8c5dd544a761ad7787f84385dd1827fa266","observation_id":"648de60e-f91b-4c28-92c0-8f68151646e4","resolution":{"observed_at":"2026-08-06T18:12:59.892544Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12564","last_updated":"2022-07-25T22:42:31Z","snapshot_observed_at":"2026-07-06T13:35:14.805149Z","submitted_at":"2022-07-25T22:42:31Z","title":"QCD Equilibrium and Dynamical Properties from Holographic Black Holes","version":1},"cited_work":{"arxiv_id":"2207.12564","doi":null,"metadata_source":"pith","pith_arxiv_id":"2207.12564","snapshot_observed_at":"2026-08-06T18:13:02.066087Z","title":"QCD Equilibrium and Dynamical Properties from Holographic Black Holes","venue":"nucl-th","work_id":"8ff8f5df-884c-4159-b268-65fa6c99502b","year":2022},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.917832Z"},"links":{"cited_paper":"/paper/2207.12564","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:00da53c4b55f02e24efcae284f8ae64259233dc63bbc80dfcdcf0e0c20e1913f","observation_id":"65e17cce-2517-489d-9647-cd6311f59439","resolution":{"observed_at":"2026-08-06T18:13:02.095867Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.06417","last_updated":"2024-03-30T02:34:06Z","snapshot_observed_at":"2026-08-06T03:48:45.332452Z","submitted_at":"2024-01-12T07:26:10Z","title":"Machine learning holographic black hole from lattice QCD equation of state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.06417","snapshot_observed_at":"2026-08-06T18:12:59.939532Z","title":"Machine learning holographic black hole from lattice QCD equation of state,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.939532Z"},"links":{"cited_paper":"/paper/2401.06417","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:86cee4a11dc81d664ffb47680f3c831ed2ee4a1b2e8249d5376541f5f7672be9","observation_id":"48350c7d-7139-4d63-9f8d-7cc2828e1732","resolution":{"observed_at":"2026-08-06T18:12:59.939532Z","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":"2026-08-06T18:12:59.959206Z","title":"Probing QCD critical point and induced gravitational wave by black hole physics,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.959206Z"},"links":{"cited_paper":"/paper/2201.02004","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:6a3343d9be7c3ef9910273f4e15fe305d0005297bfea65ec27efd123f10b9516","observation_id":"daa4a7d3-5dca-4a6d-b3f3-a9eb83af5625","resolution":{"observed_at":"2026-08-06T18:12:59.959206Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.00579","last_updated":"2024-11-08T14:08:15Z","snapshot_observed_at":"2026-08-02T18:35:46.201234Z","submitted_at":"2023-09-01T16:49:46Z","title":"Bayesian location of the QCD critical point from a holographic perspective","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.00579","snapshot_observed_at":"2026-08-06T18:12:59.993927Z","title":"Bayesian location of the QCD critical point from a holographic perspective,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:59.993927Z"},"links":{"cited_paper":"/paper/2309.00579","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:aaa08004895fb4e070ed5f5d79b3f7a22f6087e89811183a2e713e0bf9c17b3d","observation_id":"3a49d47a-2bd1-490e-b0e7-a57cb9729603","resolution":{"observed_at":"2026-08-06T18:12:59.993927Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.03784","last_updated":"2024-12-03T09:29:36Z","snapshot_observed_at":"2026-07-06T18:57:52.401361Z","submitted_at":"2024-08-07T14:09:25Z","title":"Neural Network Modeling of Heavy-Quark Potential from Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.03784","snapshot_observed_at":"2026-08-06T18:13:00.021227Z","title":"Neural network modeling of heavy-quark potential from holography,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.021227Z"},"links":{"cited_paper":"/paper/2408.03784","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:99e84b675dbf8f877296c19b9c8f01f07f45cbfb31a4337fec6e4146cb697d36","observation_id":"9cefeb99-2c3f-476d-9103-379e024e8309","resolution":{"observed_at":"2026-08-06T18:13:00.021227Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.17763","last_updated":"2025-06-29T05:07:39Z","snapshot_observed_at":"2026-08-02T18:35:47.345182Z","submitted_at":"2025-01-29T16:54:47Z","title":"Bayesian Inference of the Critical Endpoint in 2+1-Flavor System from Holographic QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.17763","snapshot_observed_at":"2026-08-06T18:13:00.055158Z","title":"Bayesian Inference of the Critical Endpoint in 2+1-Flavor System from Holographic QCD,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.055158Z"},"links":{"cited_paper":"/paper/2501.17763","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:ec0db47932be13b404edb51297ad4012b90119a3246f5d291d34f7be4b9f603c","observation_id":"25c8a61c-c1b5-4ee7-bb74-1095b776ee5b","resolution":{"observed_at":"2026-08-06T18:13:00.055158Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.17642","last_updated":"2025-03-22T04:14:57Z","snapshot_observed_at":"2026-08-07T16:44:36.516107Z","submitted_at":"2025-03-22T04:14:57Z","title":"High-precise determination of critical exponents in holographic QCD","version":1},"cited_work":{"arxiv_id":"2503.17642","doi":null,"metadata_source":"pith","pith_arxiv_id":"2503.17642","snapshot_observed_at":"2026-08-06T18:13:01.885133Z","title":"High-precise determination of critical exponents in holographic QCD","venue":"hep-ph","work_id":"0670a65d-6b5b-47c6-bec1-1b8c78d40d87","year":2025},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.087845Z"},"links":{"cited_paper":"/paper/2503.17642","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:1cd9cdb2b958f24f069820e0a2dc5f39a2ee6c82e6bf31042e47b6e804f7d859","observation_id":"fcc069ed-bcf1-46eb-b8e9-f66a1a64c892","resolution":{"observed_at":"2026-08-06T18:13:01.918719Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2402.02944","last_updated":"2024-07-16T22:46:05Z","snapshot_observed_at":"2026-07-06T17:25:26.813696Z","submitted_at":"2024-02-05T12:17:52Z","title":"Holographic entanglement properties in the QCD phase diagram from EMD models","version":3},"cited_work":{"arxiv_id":"2402.02944","doi":null,"metadata_source":"pith","pith_arxiv_id":"2402.02944","snapshot_observed_at":"2026-08-06T18:13:01.822215Z","title":"Holographic entanglement properties in the QCD phase diagram from EMD models","venue":"hep-th","work_id":"d2775480-55ae-4140-ad4a-4bf33974d328","year":2024},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.122246Z"},"links":{"cited_paper":"/paper/2402.02944","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:a12f1640dc51ce3cf15fda3bb7232853bf3c5defe0c94cb438dbaee4b654da45","observation_id":"3300c9b7-2d1a-4d72-ad46-0a75cc1506ed","resolution":{"observed_at":"2026-08-06T18:13:01.846988Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"2026-08-06T18:13:00.150347Z","title":"Jet quenching and quark energy loss from holographic QCD,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.150347Z"},"links":{"cited_paper":"/paper/2504.04147","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:3e2f1c99f6440bb2a4589a6d0578c71a59ca51f833e015a121a13f764d75d7f4","observation_id":"fe35e7c7-4fb0-4246-8768-40c3b410f187","resolution":{"observed_at":"2026-08-06T18:13:00.150347Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9307038","last_updated":"1993-07-29T16:37:13Z","snapshot_observed_at":"2026-07-07T03:24:21.295752Z","submitted_at":"1993-07-29T16:37:13Z","title":"Black Hole Entropy is Noether Charge","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9307038","snapshot_observed_at":"2026-08-06T18:13:00.178887Z","title":"Black hole entropy is the Noether charge,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.178887Z"},"links":{"cited_paper":"/paper/gr-qc/9307038","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:21d77bbd4d5060d5ff7591cbc6dfd9d17f9b53dc9d0afd3be256381ba9056673","observation_id":"bacfaac6-053d-429a-8d87-cde7e9360b69","resolution":{"observed_at":"2026-08-06T18:13:00.178887Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9403028","last_updated":"1994-03-15T18:18:00Z","snapshot_observed_at":"2026-08-03T09:59:16.103624Z","submitted_at":"1994-03-15T18:18:00Z","title":"Some Properties of Noether Charge and a Proposal for Dynamical Black Hole Entropy","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9403028","snapshot_observed_at":"2026-08-06T18:13:00.212856Z","title":"Some properties of Noether charge and a proposal for dynamical black hole entropy,","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.212856Z"},"links":{"cited_paper":"/paper/gr-qc/9403028","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:b4816223c8d8291c527f09b4824e479c043df564964578095d6f520a4f322adf","observation_id":"7f0c20e1-4c65-48af-be6a-8995c68edd76","resolution":{"observed_at":"2026-08-06T18:13:00.212856Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.0010","last_updated":"2014-01-13T00:47:42Z","snapshot_observed_at":"2026-07-06T03:32:13.149972Z","submitted_at":"2013-12-30T21:00:04Z","title":"Scalar Charges in Asymptotic AdS Geometries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.0010","snapshot_observed_at":"2026-08-06T18:13:00.239155Z","title":"Scalar Charges in Asymptotic AdS Geometries,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.239155Z"},"links":{"cited_paper":"/paper/1401.0010","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:ebac8ec4a58f46122644af0217a1a71504f854e5b72ca916ff9aa928bfebc2bd","observation_id":"a004e46d-e0ef-4ae2-ab04-27cea66a19cc","resolution":{"observed_at":"2026-08-06T18:13:00.239155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.1514","last_updated":"2015-07-08T08:13:19Z","snapshot_observed_at":"2026-08-02T07:37:23.914948Z","submitted_at":"2014-08-07T08:41:50Z","title":"Thermodynamics of AdS Black Holes in Einstein-Scalar Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.1514","snapshot_observed_at":"2026-08-06T18:13:00.261462Z","title":"Thermodynamics of AdS Black Holes in Einstein-Scalar Gravity,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.261462Z"},"links":{"cited_paper":"/paper/1408.1514","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:0d059ddbd51e73b8a4cce4df78979b6fc18d91bf79f4759d82758b164cfed1c0","observation_id":"8dd75566-d8e9-488e-a498-4fec0e98bc1d","resolution":{"observed_at":"2026-08-06T18:13:00.261462Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.02329","last_updated":"2017-09-10T10:18:27Z","snapshot_observed_at":"2026-07-06T05:54:25.300709Z","submitted_at":"2017-08-07T23:02:46Z","title":"Holographic Heat Current as Noether Current","version":2},"cited_work":{"arxiv_id":"1708.02329","doi":null,"metadata_source":"pith","pith_arxiv_id":"1708.02329","snapshot_observed_at":"2026-08-06T18:13:01.639014Z","title":"Holographic Heat Current as Noether Current","venue":"hep-th","work_id":"6d221ae9-1293-4a06-8405-de1f5b13d588","year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.286525Z"},"links":{"cited_paper":"/paper/1708.02329","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:b0d2b5607ff1026f33a8ac58c4c21088383c3567c6abdfb84b78e931a29dabbd","observation_id":"6e918bed-910e-422c-83ba-635de28b907d","resolution":{"observed_at":"2026-08-06T18:13:01.676750Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2008.05597","last_updated":"2022-01-27T02:48:11Z","snapshot_observed_at":"2026-07-06T09:46:45.172185Z","submitted_at":"2020-08-12T23:05:52Z","title":"On Thermodynamics of AdS Black Holes with Scalar Hair","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.05597","snapshot_observed_at":"2026-08-06T18:13:00.319328Z","title":"On Thermodynamics of AdS Black Holes with Scalar Hair,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.319328Z"},"links":{"cited_paper":"/paper/2008.05597","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:b0f1c3b05309dd091744c7d76f82192c8e12f1af63419aadeb8326ac9b7cb48e","observation_id":"fd6cf61d-2d49-419f-9cda-2166e1c1e176","resolution":{"observed_at":"2026-08-06T18:13:00.319328Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.8393","last_updated":"2015-10-28T19:12:59Z","snapshot_observed_at":"2026-08-01T20:42:32.197083Z","submitted_at":"2014-12-29T17:03:27Z","title":"Heavy Ion Collisions: Achievements and Challenges","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.8393","snapshot_observed_at":"2026-08-06T18:13:00.348122Z","title":"Strongly coupled quark-gluon plasma in heavy ion collisions,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.348122Z"},"links":{"cited_paper":"/paper/1412.8393","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:e66178935f57be02837c12b35328ed8fcecb98af5ee710b34f2d0cb7ff3f09c4","observation_id":"f37a8255-a736-45c0-9ac2-bec4d09b3ae6","resolution":{"observed_at":"2026-08-06T18:13:00.348122Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.2527","last_updated":"2009-05-16T01:48:46Z","snapshot_observed_at":"2026-07-06T01:51:46.872173Z","submitted_at":"2009-03-14T04:45:29Z","title":"Shear viscosity, instability and the upper bound of the Gauss-Bonnet coupling constant","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.2527","snapshot_observed_at":"2026-08-06T18:13:00.373865Z","title":"Shear viscosity, instability and the upper bound of the Gauss-Bonnet coupling constant,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.373865Z"},"links":{"cited_paper":"/paper/0903.2527","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:848dc361ef51d43dc82d8b8646101a68ced73b8b801ac972d8f77dc310e6cdd0","observation_id":"2bf68503-9d53-4fe5-9b79-0d22c00809be","resolution":{"observed_at":"2026-08-06T18:13:00.373865Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.1499","last_updated":"2014-12-03T16:56:45Z","snapshot_observed_at":"2026-07-06T02:49:31.528390Z","submitted_at":"2012-06-07T14:00:41Z","title":"Higher-derivative scalar-vector-tensor theories: black holes, Galileons, singularity cloaking and holography","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.1499","snapshot_observed_at":"2026-08-06T18:13:00.393193Z","title":"Higher-derivative scalar-vector-tensor theories: black holes, Galileons, singularity cloaking and holography,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.393193Z"},"links":{"cited_paper":"/paper/1206.1499","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:d635dcaf35de33ca64532b36f1c48ca66b5a025ed5650e45c78df18cb63c3a7c","observation_id":"12d2afec-e970-49ec-86c8-760c3fb0656d","resolution":{"observed_at":"2026-08-06T18:13:00.393193Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.07870","last_updated":"2018-01-29T04:54:28Z","snapshot_observed_at":"2026-07-06T06:20:01.257212Z","submitted_at":"2018-01-24T06:18:59Z","title":"Note on Noether charge and holographic transports","version":2},"cited_work":{"arxiv_id":"1801.07870","doi":null,"metadata_source":"pith","pith_arxiv_id":"1801.07870","snapshot_observed_at":"2026-08-06T18:13:01.503859Z","title":"Note on Noether charge and holographic transports","venue":"hep-th","work_id":"198e52fc-39ca-4405-80be-c5de13334102","year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.416087Z"},"links":{"cited_paper":"/paper/1801.07870","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:f6308d8a0d1daaaca9c75b67a467aedc3d7062ed85e39e888767bfecc146057c","observation_id":"d98f4e33-1b9e-4b43-ade3-ad679e9c2fca","resolution":{"observed_at":"2026-08-06T18:13:01.524449Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"2026-08-06T18:13:00.440951Z","title":"Hot QCD Phase Diagram From Holographic Einstein-Maxwell-Dilaton Models,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.440951Z"},"links":{"cited_paper":"/paper/2307.03885","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:140c7b5a3c1176da9756f53c254500e2f777940541eb97676d245a844499eab6","observation_id":"2bd5a8dc-5aaa-46e3-8b61-1889f70c47a2","resolution":{"observed_at":"2026-08-06T18:13:00.440951Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.02394","last_updated":"2024-11-01T05:39:33Z","snapshot_observed_at":"2026-08-04T20:49:01.934738Z","submitted_at":"2024-05-03T18:00:01Z","title":"Refining holographic models of the quark-gluon plasma","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.02394","snapshot_observed_at":"2026-08-06T18:13:00.485793Z","title":"Refining holographic models of the quark-gluon plasma,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.485793Z"},"links":{"cited_paper":"/paper/2405.02394","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:2492f912fd4976e68aa1536c40ca2ab8ae30811b65599295956437fcf6db973e","observation_id":"d71a3451-4e2c-44eb-9c52-9c8ff7a4a7a8","resolution":{"observed_at":"2026-08-06T18:13:00.485793Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.0784","last_updated":"2012-08-11T12:57:36Z","snapshot_observed_at":"2026-07-06T02:44:00.307419Z","submitted_at":"2012-03-04T23:06:00Z","title":"Fluctuations and Correlations of net baryon number, electric charge, and strangeness: A comparison of lattice QCD results with the hadron resonance gas model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.0784","snapshot_observed_at":"2026-08-06T18:13:00.512142Z","title":"Fluctuations and Correlations of net baryon number, electric charge, and strangeness: A comparison of lattice QCD results with the 23 hadron resonance gas model,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.512142Z"},"links":{"cited_paper":"/paper/1203.0784","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:8497d9ba005e7ffa45e6913cab2b2c89446d4708c75bfe027daa6187d66fbbb6","observation_id":"d329fb67-874d-4827-affe-d29cbad0e8b7","resolution":{"observed_at":"2026-08-06T18:13:00.512142Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.6387","last_updated":"2014-11-24T21:18:03Z","snapshot_observed_at":"2026-08-02T02:23:39.687183Z","submitted_at":"2014-07-23T20:48:29Z","title":"The equation of state in (2+1)-flavor QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.6387","snapshot_observed_at":"2026-08-06T18:13:00.533642Z","title":"Equation of state in ( 2+1 )-flavor QCD,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.533642Z"},"links":{"cited_paper":"/paper/1407.6387","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:7766222ddfe48e4ada9a19201d4f08b48532be5b06d1a0153425a4796d392a21","observation_id":"59712499-443f-426d-878c-52752b554110","resolution":{"observed_at":"2026-08-06T18:13:00.533642Z","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":"2026-08-06T18:13:00.559854Z","title":"The QCD Equation of State to O(µ6 B) from Lattice QCD,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.559854Z"},"links":{"cited_paper":"/paper/1701.04325","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:01c38f52f92bbe5788a2e6772d29039436437585a10a688124b113057359012a","observation_id":"11a30d92-c15b-4b49-b700-302c9523dc1c","resolution":{"observed_at":"2026-08-06T18:13:00.559854Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.09184","last_updated":"2022-05-02T02:23:42Z","snapshot_observed_at":"2026-08-04T16:03:56.525381Z","submitted_at":"2022-02-18T13:26:59Z","title":"Taylor expansions and Pad\\'e approximants for cumulants of conserved charge fluctuations at non-vanishing chemical potentials","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.09184","snapshot_observed_at":"2026-08-06T18:13:00.578900Z","title":"Taylor expansions and Pad´ e approximants for cumulants of conserved charge fluctuations at nonvanishing chemical potentials,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.578900Z"},"links":{"cited_paper":"/paper/2202.09184","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:0faf7465f9d4b7c483866564b4db313e7505d57f4514a692463cd17015f076d6","observation_id":"ccbdf12a-cd8d-4d32-9a2e-2f68e4c0cfa2","resolution":{"observed_at":"2026-08-06T18:13:00.578900Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.07134","last_updated":"2016-11-22T03:08:44Z","snapshot_observed_at":"2026-07-06T05:19:35.141404Z","submitted_at":"2016-11-22T03:08:44Z","title":"Energy Dependence of Moments of Net-Proton, Net-Kaon, and Net-Charge Multiplicity Distributions at STAR","version":1},"cited_work":{"arxiv_id":"1611.07134","doi":null,"metadata_source":"pith","pith_arxiv_id":"1611.07134","snapshot_observed_at":"2026-08-06T18:13:01.323036Z","title":"Energy Dependence of Moments of Net-Proton, Net-Kaon, and Net-Charge Multiplicity Distributions at STAR","venue":"hep-ex","work_id":"08be9b7b-55eb-4134-a78d-f2a35ce5e022","year":2016},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.606670Z"},"links":{"cited_paper":"/paper/1611.07134","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:058de9c6d8ceefbf2080e5fc8b1611e1fdf6b2189707d28431048d6875e0d06b","observation_id":"ef46aa49-b18c-4e38-88ba-ca6fbee7f735","resolution":{"observed_at":"2026-08-06T18:13:01.355964Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T18:13:00.626786Z","title":"Measurements of Proton High Order Cumulants in √sNN = 3 GeV Au+Au Collisions and Implications for the QCD Critical Point,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.626786Z"},"links":{"citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:5f0583d8fc6102e8d0932de4d22c234276a5ca6a68e76eebfe35be4c2f3df838","observation_id":"3007e395-5905-4091-a11a-d2dba8cb0af0","resolution":{"observed_at":"2026-08-06T18:13:00.626786Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1501.00006","last_updated":"2015-02-13T02:21:24Z","snapshot_observed_at":"2026-07-06T04:05:02.363433Z","submitted_at":"2014-12-30T21:00:11Z","title":"Thermodynamical First Laws of Black Holes in Quadratically-Extended Gravities","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.00006","snapshot_observed_at":"2026-08-06T18:13:00.639799Z","title":"Thermodynamical First Laws of Black Holes in Quadratically-Extended Gravities,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.639799Z"},"links":{"cited_paper":"/paper/1501.00006","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:52edd371c0bd7f38c9d8f4b74a48d03ad9eea87a4580111c532b73633b477f68","observation_id":"77a52902-3c6a-423c-88e7-828aabc1e513","resolution":{"observed_at":"2026-08-06T18:13:00.639799Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.08282","last_updated":"2016-09-14T01:39:42Z","snapshot_observed_at":"2026-07-06T04:54:23.035745Z","submitted_at":"2016-04-28T01:41:16Z","title":"AdS and Lifshitz Scalar Hairy Black Holes in Gauss-Bonnet Gravity","version":3},"cited_work":{"arxiv_id":"1604.08282","doi":null,"metadata_source":"pith","pith_arxiv_id":"1604.08282","snapshot_observed_at":"2026-08-06T18:13:01.090010Z","title":"AdS and Lifshitz Scalar Hairy Black Holes in Gauss-Bonnet Gravity","venue":"hep-th","work_id":"22a7ae3c-5222-40ad-8c63-7a88bad05a52","year":2016},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.662089Z"},"links":{"cited_paper":"/paper/1604.08282","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:886255c7685283b7373426634df339534affdb2134f05dd4e2570241eb0e2b53","observation_id":"368d6ae5-8161-47bd-ad39-50b3f2188dac","resolution":{"observed_at":"2026-08-06T18:13:01.114469Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0712.0805","last_updated":"2008-06-13T15:39:13Z","snapshot_observed_at":"2026-07-06T01:36:33.294493Z","submitted_at":"2007-12-05T20:51:34Z","title":"Viscosity Bound Violation in Higher Derivative Gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.0805","snapshot_observed_at":"2026-08-06T18:13:00.683870Z","title":"Viscosity Bound Violation in Higher Derivative Gravity,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.683870Z"},"links":{"cited_paper":"/paper/0712.0805","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:306652916b63bfb5229931b3d4ce68f989dc4073e5080f4b00e39e1c4444ef08","observation_id":"4a22f968-a70a-4914-bbd5-7bef67bfce55","resolution":{"observed_at":"2026-08-06T18:13:00.683870Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.12109","last_updated":"2024-04-18T11:48:33Z","snapshot_observed_at":"2026-07-06T18:02:06.709537Z","submitted_at":"2024-04-18T11:48:33Z","title":"Revisiting holographic model for thermal and dense QCD with a critical point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.12109","snapshot_observed_at":"2026-08-06T18:13:00.715166Z","title":"Revisiting holographic model for thermal and dense QCD with a critical point,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.715166Z"},"links":{"cited_paper":"/paper/2404.12109","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:911b6a2f1d3367969a051b058990dcbc2447116c6400589d8fc5e9c161caaba1","observation_id":"619a4602-ba6a-4b11-a80c-9af5be7c75b9","resolution":{"observed_at":"2026-08-06T18:13:00.715166Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.04681","last_updated":"2020-04-09T17:04:22Z","snapshot_observed_at":"2026-07-06T09:11:17.430597Z","submitted_at":"2020-04-09T17:04:22Z","title":"Freeze-out and thermalization in relativistic heavy ion collisions","version":1},"cited_work":{"arxiv_id":"2004.04681","doi":null,"metadata_source":"pith","pith_arxiv_id":"2004.04681","snapshot_observed_at":"2026-08-06T18:13:01.005225Z","title":"Freeze-out and thermalization in relativistic heavy ion collisions","venue":"hep-ph","work_id":"12d22a5d-fdaf-431f-b157-6e5973341fa1","year":2020},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.729791Z"},"links":{"cited_paper":"/paper/2004.04681","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:6b1a408f1c4039d0b899e43aab9cd639b49ba64b1ec1d33c4e49ce896b97c3f5","observation_id":"7d82c56f-ea5a-46cf-b8eb-29088b0fccef","resolution":{"observed_at":"2026-08-06T18:13:01.025972Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2407.09335","last_updated":"2024-10-02T14:19:24Z","snapshot_observed_at":"2026-08-04T15:52:03.764749Z","submitted_at":"2024-07-12T15:13:12Z","title":"Strangeness-Correlations on the pseudo-critical line in (2+1)-flavor QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.09335","snapshot_observed_at":"2026-08-06T18:13:00.749602Z","title":"Strangeness-correlations on the pseudocritical line in (2+1)-flavor QCD,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.749602Z"},"links":{"cited_paper":"/paper/2407.09335","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:48ce1c112250b6dafda68c8af75ae2d193a55cdc9433beeb1d13b3da1e5e3dfd","observation_id":"27e9679a-fc1a-4f35-94ad-28698fb0937b","resolution":{"observed_at":"2026-08-06T18:13:00.749602Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9803035","last_updated":"1998-03-19T18:17:56Z","snapshot_observed_at":"2026-08-03T18:04:57.514835Z","submitted_at":"1998-03-17T19:07:10Z","title":"Microscopic Models for Ultrarelativistic Heavy Ion Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/9803035","snapshot_observed_at":"2026-08-06T18:13:00.781883Z","title":"Microscopic models for ultrarelativistic heavy ion collisions,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.781883Z"},"links":{"cited_paper":"/paper/nucl-th/9803035","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:91e59f85201c0e83997b297b776cc7278c5f94d1da4d54be18a97e8aeb8433c9","observation_id":"aa66fc8d-793a-402b-9a9a-cae439baab0a","resolution":{"observed_at":"2026-08-06T18:13:00.781883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9909407","last_updated":"1999-09-16T21:08:53Z","snapshot_observed_at":"2026-07-07T04:34:27.949726Z","submitted_at":"1999-09-16T21:08:53Z","title":"Relativistic Hadron-Hadron Collisions in the Ultra-Relativistic Quantum Molecular Dynamics Model (UrQMD)","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9909407","snapshot_observed_at":"2026-08-06T18:13:00.808128Z","title":"Relativistic hadron hadron collisions in the ultrarelativistic quantum molecular dynamics model,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.808128Z"},"links":{"cited_paper":"/paper/hep-ph/9909407","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:431e3c6fd05fa6b32fc196e608823d1b47362f68fb73cbc2cbcb575d8a8ab97e","observation_id":"e91d1215-7dfc-43d5-9b27-b9c861939027","resolution":{"observed_at":"2026-08-06T18:13:00.808128Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.4931","last_updated":"2009-11-25T18:32:35Z","snapshot_observed_at":"2026-08-03T11:51:27.773359Z","submitted_at":"2009-11-25T18:32:35Z","title":"The horn, the hadron mass spectrum and the QCD phase diagram - the statistical model of hadron production in central nucleus-nucleus collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.4931","snapshot_observed_at":"2026-08-06T18:13:00.837846Z","title":"The Horn, the hadron mass spectrum and the QCD phase diagram: The Statistical model of hadron production in central nucleus-nucleus collisions,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.837846Z"},"links":{"cited_paper":"/paper/0911.4931","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:8ee7679d74f957e56629821b62678bc5f122c8743ff73f08dc133510be9e10b9","observation_id":"b9a4ae07-9dbc-4375-8720-425ca2cb008e","resolution":{"observed_at":"2026-08-06T18:13:00.837846Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.09425","last_updated":"2018-07-04T19:26:49Z","snapshot_observed_at":"2026-08-01T17:16:21.331977Z","submitted_at":"2017-10-25T19:00:35Z","title":"Decoding the phase structure of QCD via particle production at high energy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.09425","snapshot_observed_at":"2026-08-06T18:13:00.864648Z","title":"Decoding the phase structure of QCD via particle production at high energy,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-06T18:13:00.864648Z"},"links":{"cited_paper":"/paper/1710.09425","citing_paper":"/paper/2507.09113"},"observation_digest":"sha256:385b49f6083df3f7bbf13ecda7b00ffd821bc9a523a27b5aaf2019ce9f2eb126","observation_id":"c91e3a7e-6eb9-4014-a36d-c91e9834790d","resolution":{"observed_at":"2026-08-06T18:13:00.864648Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2507.09113","last_updated":"2025-07-12T01:58:31Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-07T18:20:10.572724Z","submitted_at":"2025-07-12T01:58:31Z","title":"Phase transition of hot dense QCD Matter from a refined holographic EMD model"},"reference_resolution":{"displayed":73,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":55,"verified_exact":17,"verified_fuzzy":1},"total_outbound_references":73},"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":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"thesis":"As of 7 August 2026, this Paper Citation Record lists 73 of 73 outbound references and 1 inbound Pith citation observation for arXiv:2507.09113."}