{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ZKPHN7C7UQ3U4NUKEXP6ABCYX6","short_pith_number":"pith:ZKPHN7C7","schema_version":"1.0","canonical_sha256":"ca9e76fc5fa4374e368a25dfe00458bfaab956d4b116d7597aaf067d3d3d95ac","source":{"kind":"arxiv","id":"2404.12109","version":1},"attestation_state":"computed","paper":{"title":"Revisiting holographic model for thermal and dense QCD with a critical point","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Li Li, Qingxuan Fu, Song He, Zhibin Li","submitted_at":"2024-04-18T11:48:33Z","abstract_excerpt":"To quantitatively provide reliable predictions for the hot and dense QCD matter, a holographic model should be adjusted to describe first-principles lattice results available at vanishing baryon chemical potential. The equation of state from two well-known lattice groups, the HotQCD collaboration and the Wuppertal-Budapest (WB) collaboration, shows visible differences at high temperatures. We revisit the Einstein-Maxwell-dilaton (EMD) holographic model for hot QCD with 2+1 flavors and physical quark masses by fitting lattice QCD data from the WB collaboration. Using the parameterization for th"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2404.12109","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-18T11:48:33Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"171882dbac97eb6a89f9a956e450fc156816756c451103d0d21d618cf5fbd607","abstract_canon_sha256":"961e2174c0eec912838c159b44b3feb7a4e25372161169cd35a4661375dff58b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:26:42.321191Z","signature_b64":"jiXJrTZXOUPQU0q/XoBM1oOfye+SazZqHYIiovulSE2aSkmB67zhdTWdfckt2TO1duAwQSgGi+9kmc9woiDjDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca9e76fc5fa4374e368a25dfe00458bfaab956d4b116d7597aaf067d3d3d95ac","last_reissued_at":"2026-07-05T11:26:42.320701Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:26:42.320701Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting holographic model for thermal and dense QCD with a critical point","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Li Li, Qingxuan Fu, Song He, Zhibin Li","submitted_at":"2024-04-18T11:48:33Z","abstract_excerpt":"To quantitatively provide reliable predictions for the hot and dense QCD matter, a holographic model should be adjusted to describe first-principles lattice results available at vanishing baryon chemical potential. The equation of state from two well-known lattice groups, the HotQCD collaboration and the Wuppertal-Budapest (WB) collaboration, shows visible differences at high temperatures. We revisit the Einstein-Maxwell-dilaton (EMD) holographic model for hot QCD with 2+1 flavors and physical quark masses by fitting lattice QCD data from the WB collaboration. Using the parameterization for th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.12109","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2404.12109/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2404.12109","created_at":"2026-07-05T11:26:42.320760+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.12109v1","created_at":"2026-07-05T11:26:42.320760+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.12109","created_at":"2026-07-05T11:26:42.320760+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZKPHN7C7UQ3U","created_at":"2026-07-05T11:26:42.320760+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZKPHN7C7UQ3U4NUK","created_at":"2026-07-05T11:26:42.320760+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZKPHN7C7","created_at":"2026-07-05T11:26:42.320760+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.23834","citing_title":"Thermodynamics and transport in holographic QCD with Gauss-Bonnet corrections","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6","json":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6.json","graph_json":"https://pith.science/api/pith-number/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/graph.json","events_json":"https://pith.science/api/pith-number/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/events.json","paper":"https://pith.science/paper/ZKPHN7C7"},"agent_actions":{"view_html":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6","download_json":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6.json","view_paper":"https://pith.science/paper/ZKPHN7C7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.12109&json=true","fetch_graph":"https://pith.science/api/pith-number/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/graph.json","fetch_events":"https://pith.science/api/pith-number/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/action/storage_attestation","attest_author":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/action/author_attestation","sign_citation":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/action/citation_signature","submit_replication":"https://pith.science/pith/ZKPHN7C7UQ3U4NUKEXP6ABCYX6/action/replication_record"}},"created_at":"2026-07-05T11:26:42.320760+00:00","updated_at":"2026-07-05T11:26:42.320760+00:00"}