{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:HCBGVADQSRJYXAAS2JRLSNKS6O","short_pith_number":"pith:HCBGVADQ","schema_version":"1.0","canonical_sha256":"38826a807094538b8012d262b93552f3a19cf2b6858804e0d1e910878c5bdaff","source":{"kind":"arxiv","id":"2402.08636","version":3},"attestation_state":"computed","paper":{"title":"Finite density QCD equation of state: critical point and lattice-based $T'$-expansion","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Claudia Ratti, Damien Price, Elena Bratkovskaya, Johannes Jahan, Micheal Kahangirwe, Mikhail Stephanov, Olga Soloveva, Paolo Parotto, Pierre Moreau, Steffen A. Bass","submitted_at":"2024-02-13T18:03:29Z","abstract_excerpt":"We present a novel construction of the QCD equation of state (EoS) at finite baryon density. Our work combines a recently proposed resummation scheme for lattice QCD results with the universal critical behavior at the QCD critical point. This allows us to obtain a family of equations of state in the range $0 \\leq \\mu_B \\leq 700$ MeV and 25 MeV $\\leq T \\leq 800$ MeV, which match lattice QCD results near $\\mu_B=0$ while featuring a critical point in the 3D Ising model universality class. The position of the critical point can be chosen within the range accessible to beam-energy scan heavy-ion co"},"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":"2402.08636","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"nucl-th","submitted_at":"2024-02-13T18:03:29Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4033c6216441e0504789f8e57a3cb2ec17912dcb92fcc5070b1324c6c587fa2c","abstract_canon_sha256":"53e0bdf92d30b5b34436f5ff4717fcfab96739f2765caeed89ebaf1d54f85ba8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:30:31.673383Z","signature_b64":"3Ba1afzFZJsNXoS1yUkxTmkyqSK2NLh8sKQ2K+2F6T5m9uyXZyKYcI+xVYNiu4Lvc0yRijgj1IlZJAY38DxDDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38826a807094538b8012d262b93552f3a19cf2b6858804e0d1e910878c5bdaff","last_reissued_at":"2026-07-05T08:30:31.672842Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:30:31.672842Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite density QCD equation of state: critical point and lattice-based $T'$-expansion","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Claudia Ratti, Damien Price, Elena Bratkovskaya, Johannes Jahan, Micheal Kahangirwe, Mikhail Stephanov, Olga Soloveva, Paolo Parotto, Pierre Moreau, Steffen A. Bass","submitted_at":"2024-02-13T18:03:29Z","abstract_excerpt":"We present a novel construction of the QCD equation of state (EoS) at finite baryon density. Our work combines a recently proposed resummation scheme for lattice QCD results with the universal critical behavior at the QCD critical point. This allows us to obtain a family of equations of state in the range $0 \\leq \\mu_B \\leq 700$ MeV and 25 MeV $\\leq T \\leq 800$ MeV, which match lattice QCD results near $\\mu_B=0$ while featuring a critical point in the 3D Ising model universality class. The position of the critical point can be chosen within the range accessible to beam-energy scan heavy-ion co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.08636","kind":"arxiv","version":3},"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/2402.08636/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":"2402.08636","created_at":"2026-07-05T08:30:31.672909+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.08636v3","created_at":"2026-07-05T08:30:31.672909+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.08636","created_at":"2026-07-05T08:30:31.672909+00:00"},{"alias_kind":"pith_short_12","alias_value":"HCBGVADQSRJY","created_at":"2026-07-05T08:30:31.672909+00:00"},{"alias_kind":"pith_short_16","alias_value":"HCBGVADQSRJYXAAS","created_at":"2026-07-05T08:30:31.672909+00:00"},{"alias_kind":"pith_short_8","alias_value":"HCBGVADQ","created_at":"2026-07-05T08:30:31.672909+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26326","citing_title":"Studying the QCD Matter produced in Heavy-Ion Collisions using the MUSES Calculation Engine","ref_index":108,"is_internal_anchor":false},{"citing_arxiv_id":"2606.17204","citing_title":"Scaling of the Surface Free Energy as a Probe of the QCD Critical Region","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2504.18764","citing_title":"Symmetry Energy Expansion with Strange Dense Matter","ref_index":90,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20196","citing_title":"Chiral first order phase transition at finite baryon density and zero temperature from self-consistent pole masses in the linear sigma model with quarks","ref_index":57,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O","json":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O.json","graph_json":"https://pith.science/api/pith-number/HCBGVADQSRJYXAAS2JRLSNKS6O/graph.json","events_json":"https://pith.science/api/pith-number/HCBGVADQSRJYXAAS2JRLSNKS6O/events.json","paper":"https://pith.science/paper/HCBGVADQ"},"agent_actions":{"view_html":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O","download_json":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O.json","view_paper":"https://pith.science/paper/HCBGVADQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.08636&json=true","fetch_graph":"https://pith.science/api/pith-number/HCBGVADQSRJYXAAS2JRLSNKS6O/graph.json","fetch_events":"https://pith.science/api/pith-number/HCBGVADQSRJYXAAS2JRLSNKS6O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O/action/storage_attestation","attest_author":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O/action/author_attestation","sign_citation":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O/action/citation_signature","submit_replication":"https://pith.science/pith/HCBGVADQSRJYXAAS2JRLSNKS6O/action/replication_record"}},"created_at":"2026-07-05T08:30:31.672909+00:00","updated_at":"2026-07-05T08:30:31.672909+00:00"}