{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XXTFSGKFXYAIBWQ6YVO2R4WV33","short_pith_number":"pith:XXTFSGKF","schema_version":"1.0","canonical_sha256":"bde6591945be0080da1ec55da8f2d5dedd0c70b95179484a6c740ff9766fc952","source":{"kind":"arxiv","id":"1711.09863","version":1},"attestation_state":"computed","paper":{"title":"van der Waals Interactions and Hadron Resonance Gas: Role of resonance widths modeling on conserved charges fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Horst Stoecker, Mark I. Gorenstein, Paolo Alba, Volodymyr Vovchenko","submitted_at":"2017-11-27T18:21:42Z","abstract_excerpt":"The quantum van der Waals (QvdW) extension of the ideal hadron resonance gas (HRG) model which includes the attractive and repulsive interactions between baryons -- the QvdW-HRG model -- is applied to study the behavior of the baryon number related susceptibilities in the crossover temperature region. Inclusion of the QvdW interactions leads to a qualitatively different behavior of susceptibilities, in many cases resembling lattice QCD simulations. It is shown that for some observables, in particular for $\\chi_{11}^{BQ} / \\chi_2^B$, effects of the QvdW interactions essentially cancel out. It i"},"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":"1711.09863","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-11-27T18:21:42Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"dc7d5e20cea3bafc957d1437284691574c098f602a007a078e0e91bbc76d2a05","abstract_canon_sha256":"2d62f6ad194c001c2bbedbcaef5ee1b76a849e4b12d1f8fec104250108d71f1a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:09.458039Z","signature_b64":"xJI+BaaPRksSU32N2YJ4tCuKQn2rzvvtnmnqvJ0HbXv41f1yvBFPxOngMysg0I73oseHqGncdHaVp4ySjgKNAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bde6591945be0080da1ec55da8f2d5dedd0c70b95179484a6c740ff9766fc952","last_reissued_at":"2026-05-18T00:21:09.457594Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:09.457594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"van der Waals Interactions and Hadron Resonance Gas: Role of resonance widths modeling on conserved charges fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Horst Stoecker, Mark I. Gorenstein, Paolo Alba, Volodymyr Vovchenko","submitted_at":"2017-11-27T18:21:42Z","abstract_excerpt":"The quantum van der Waals (QvdW) extension of the ideal hadron resonance gas (HRG) model which includes the attractive and repulsive interactions between baryons -- the QvdW-HRG model -- is applied to study the behavior of the baryon number related susceptibilities in the crossover temperature region. Inclusion of the QvdW interactions leads to a qualitatively different behavior of susceptibilities, in many cases resembling lattice QCD simulations. It is shown that for some observables, in particular for $\\chi_{11}^{BQ} / \\chi_2^B$, effects of the QvdW interactions essentially cancel out. It i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.09863","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":""},"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":"1711.09863","created_at":"2026-05-18T00:21:09.457681+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.09863v1","created_at":"2026-05-18T00:21:09.457681+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.09863","created_at":"2026-05-18T00:21:09.457681+00:00"},{"alias_kind":"pith_short_12","alias_value":"XXTFSGKFXYAI","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"XXTFSGKFXYAIBWQ6","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"XXTFSGKF","created_at":"2026-05-18T12:31:56.362134+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/XXTFSGKFXYAIBWQ6YVO2R4WV33","json":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33.json","graph_json":"https://pith.science/api/pith-number/XXTFSGKFXYAIBWQ6YVO2R4WV33/graph.json","events_json":"https://pith.science/api/pith-number/XXTFSGKFXYAIBWQ6YVO2R4WV33/events.json","paper":"https://pith.science/paper/XXTFSGKF"},"agent_actions":{"view_html":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33","download_json":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33.json","view_paper":"https://pith.science/paper/XXTFSGKF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.09863&json=true","fetch_graph":"https://pith.science/api/pith-number/XXTFSGKFXYAIBWQ6YVO2R4WV33/graph.json","fetch_events":"https://pith.science/api/pith-number/XXTFSGKFXYAIBWQ6YVO2R4WV33/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33/action/storage_attestation","attest_author":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33/action/author_attestation","sign_citation":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33/action/citation_signature","submit_replication":"https://pith.science/pith/XXTFSGKFXYAIBWQ6YVO2R4WV33/action/replication_record"}},"created_at":"2026-05-18T00:21:09.457681+00:00","updated_at":"2026-05-18T00:21:09.457681+00:00"}