{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:CWALBMUZAF2MXXRM6HV7JX6X2W","short_pith_number":"pith:CWALBMUZ","schema_version":"1.0","canonical_sha256":"1580b0b2990174cbde2cf1ebf4dfd7d5b89b2ce52716a1ac9d4a01ff6972b96a","source":{"kind":"arxiv","id":"2606.09757","version":1},"attestation_state":"computed","paper":{"title":"Partial Pressure Contributions of Hadron Families to the QCD Equation of State","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alejandro Florez, Angel R. Nava Acuna, Claudia Ratti, Johannes Jahan, Jonathan Gonzales, Naman Mehndiratta","submitted_at":"2026-06-08T17:17:05Z","abstract_excerpt":"Lattice simulations provide the thermodynamics of quantum chromodynamics (QCD) as a function of the temperature, at zero-to-moderate values of the baryonic chemical potential. However, the contribution of single hadronic species cannot be directly isolated from lattice calculations. In this work, we find linear combinations of up to fourth order susceptibilities which isolate the contribution of hadrons to the QCD pressure according to their baryon number $B$, electric charge $Q$ and strangeness $S$ content. These combinations are valid, provided that the thermodynamics of a strongly-interacti"},"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":"2606.09757","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ph","submitted_at":"2026-06-08T17:17:05Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"b3cf0927d046532be089d7befd5985a4841c656acf4b3ef2a48f17dc85167567","abstract_canon_sha256":"058e2a5d14abed2f3d7c0607dbce8f74ba287cad6387702ef03304d74427c25f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-09T02:09:07.970094Z","signature_b64":"GHTbdS8b34PJ4CrsJzKp+6oJ/n0F+Lv8NRoeMkfEHoEfHl+quRNFyw2gh0nhvlMc/nqfU+Fx5bSKWh52uFy6Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1580b0b2990174cbde2cf1ebf4dfd7d5b89b2ce52716a1ac9d4a01ff6972b96a","last_reissued_at":"2026-06-09T02:09:07.969241Z","signature_status":"signed_v1","first_computed_at":"2026-06-09T02:09:07.969241Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Partial Pressure Contributions of Hadron Families to the QCD Equation of State","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alejandro Florez, Angel R. Nava Acuna, Claudia Ratti, Johannes Jahan, Jonathan Gonzales, Naman Mehndiratta","submitted_at":"2026-06-08T17:17:05Z","abstract_excerpt":"Lattice simulations provide the thermodynamics of quantum chromodynamics (QCD) as a function of the temperature, at zero-to-moderate values of the baryonic chemical potential. However, the contribution of single hadronic species cannot be directly isolated from lattice calculations. In this work, we find linear combinations of up to fourth order susceptibilities which isolate the contribution of hadrons to the QCD pressure according to their baryon number $B$, electric charge $Q$ and strangeness $S$ content. These combinations are valid, provided that the thermodynamics of a strongly-interacti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.09757","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/2606.09757/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":"2606.09757","created_at":"2026-06-09T02:09:07.969373+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.09757v1","created_at":"2026-06-09T02:09:07.969373+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.09757","created_at":"2026-06-09T02:09:07.969373+00:00"},{"alias_kind":"pith_short_12","alias_value":"CWALBMUZAF2M","created_at":"2026-06-09T02:09:07.969373+00:00"},{"alias_kind":"pith_short_16","alias_value":"CWALBMUZAF2MXXRM","created_at":"2026-06-09T02:09:07.969373+00:00"},{"alias_kind":"pith_short_8","alias_value":"CWALBMUZ","created_at":"2026-06-09T02:09:07.969373+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W","json":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W.json","graph_json":"https://pith.science/api/pith-number/CWALBMUZAF2MXXRM6HV7JX6X2W/graph.json","events_json":"https://pith.science/api/pith-number/CWALBMUZAF2MXXRM6HV7JX6X2W/events.json","paper":"https://pith.science/paper/CWALBMUZ"},"agent_actions":{"view_html":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W","download_json":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W.json","view_paper":"https://pith.science/paper/CWALBMUZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.09757&json=true","fetch_graph":"https://pith.science/api/pith-number/CWALBMUZAF2MXXRM6HV7JX6X2W/graph.json","fetch_events":"https://pith.science/api/pith-number/CWALBMUZAF2MXXRM6HV7JX6X2W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W/action/storage_attestation","attest_author":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W/action/author_attestation","sign_citation":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W/action/citation_signature","submit_replication":"https://pith.science/pith/CWALBMUZAF2MXXRM6HV7JX6X2W/action/replication_record"}},"created_at":"2026-06-09T02:09:07.969373+00:00","updated_at":"2026-06-09T02:09:07.969373+00:00"}