{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:DKN5C6XBEYMBE6VYTSETHKAKO4","short_pith_number":"pith:DKN5C6XB","schema_version":"1.0","canonical_sha256":"1a9bd17ae12618127ab89c8933a80a7707182fe4dcb711b3412d58bfb7c5b07b","source":{"kind":"arxiv","id":"nucl-th/9710014","version":2},"attestation_state":"computed","paper":{"title":"Thermodynamics of Delta resonances","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"B. Friman, W. N\\\"orenberg (GSI), W. Weinhold","submitted_at":"1997-10-06T12:36:35Z","abstract_excerpt":"The thermodynamic potential of a system of pions and nucleons is computed including the piN interactions in the P33 channel. A consistent treatment of the width of the resonance in this channel, the Delta(1232) resonance, is explored in detail. In the low-density limit we recover the leading term of the virial expansion for the thermodynamic potential. An instructive diagrammatic interpretation of the contributions to the total baryon number is presented. Furthermore, we examine within a fireball model the consequences for the pion spectra in heavy-ion collisions at intermediate energies, incl"},"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":"nucl-th/9710014","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1997-10-06T12:36:35Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"5e7a2d27aa52d9f130c6c6b7d66a2cd591ba2d43c4f3054aa56eae29f017adb6","abstract_canon_sha256":"1b73dcf08480762aa2abaafb6dcaf640155ecac534cc49f2f8e4ae2ee2475493"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:05:53.993043Z","signature_b64":"FRIcsZFtsx7nDdDr7I07IvRpBDBu1s1E7QgjHSYpwvuFDItfaQQW3lpeg9jSTBz2C9rNjCOtyd0TFzI+uZ6mDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a9bd17ae12618127ab89c8933a80a7707182fe4dcb711b3412d58bfb7c5b07b","last_reissued_at":"2026-07-04T16:05:53.992702Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:05:53.992702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics of Delta resonances","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"B. Friman, W. N\\\"orenberg (GSI), W. Weinhold","submitted_at":"1997-10-06T12:36:35Z","abstract_excerpt":"The thermodynamic potential of a system of pions and nucleons is computed including the piN interactions in the P33 channel. A consistent treatment of the width of the resonance in this channel, the Delta(1232) resonance, is explored in detail. In the low-density limit we recover the leading term of the virial expansion for the thermodynamic potential. An instructive diagrammatic interpretation of the contributions to the total baryon number is presented. Furthermore, we examine within a fireball model the consequences for the pion spectra in heavy-ion collisions at intermediate energies, incl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9710014","kind":"arxiv","version":2},"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/nucl-th/9710014/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":"nucl-th/9710014","created_at":"2026-07-04T16:05:53.992761+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9710014v2","created_at":"2026-07-04T16:05:53.992761+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9710014","created_at":"2026-07-04T16:05:53.992761+00:00"},{"alias_kind":"pith_short_12","alias_value":"DKN5C6XBEYMB","created_at":"2026-07-04T16:05:53.992761+00:00"},{"alias_kind":"pith_short_16","alias_value":"DKN5C6XBEYMBE6VY","created_at":"2026-07-04T16:05:53.992761+00:00"},{"alias_kind":"pith_short_8","alias_value":"DKN5C6XB","created_at":"2026-07-04T16:05:53.992761+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.18879","citing_title":"Baselines for Abelian Charge Fluctuations in Nuclear Collisions:Theory and Comparison with Experimental Data","ref_index":55,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4","json":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4.json","graph_json":"https://pith.science/api/pith-number/DKN5C6XBEYMBE6VYTSETHKAKO4/graph.json","events_json":"https://pith.science/api/pith-number/DKN5C6XBEYMBE6VYTSETHKAKO4/events.json","paper":"https://pith.science/paper/DKN5C6XB"},"agent_actions":{"view_html":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4","download_json":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4.json","view_paper":"https://pith.science/paper/DKN5C6XB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9710014&json=true","fetch_graph":"https://pith.science/api/pith-number/DKN5C6XBEYMBE6VYTSETHKAKO4/graph.json","fetch_events":"https://pith.science/api/pith-number/DKN5C6XBEYMBE6VYTSETHKAKO4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4/action/storage_attestation","attest_author":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4/action/author_attestation","sign_citation":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4/action/citation_signature","submit_replication":"https://pith.science/pith/DKN5C6XBEYMBE6VYTSETHKAKO4/action/replication_record"}},"created_at":"2026-07-04T16:05:53.992761+00:00","updated_at":"2026-07-04T16:05:53.992761+00:00"}