{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:JKJZBJDF6AKT4SRZY3PEUR4JG5","short_pith_number":"pith:JKJZBJDF","schema_version":"1.0","canonical_sha256":"4a9390a465f0153e4a39c6de4a47893774e26d8d7a45bdbeb4adf4511139c58a","source":{"kind":"arxiv","id":"cond-mat/0207353","version":1},"attestation_state":"computed","paper":{"title":"Relativistic Nonextensive Thermodynamics","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Lavagno","submitted_at":"2002-07-15T09:53:52Z","abstract_excerpt":"Starting from the basic prescriptions of the Tsallis' nonextensive thermostatistics, i.e. generalized entropy and normalized q-expectation values, we study the relativistic nonextensive thermodynamics and derive a Boltzmann transport equation that implies the validity of the H-theorem where a local nonextensive four-entropy density is considered. Macroscopic thermodynamic functions and the equation of state for a perfect gas are derived at the equilibrium."},"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":"cond-mat/0207353","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-07-15T09:53:52Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"5eb6827018c628410df0c390605ab639c22b4719753ef4c91b8bc65829d64bca","abstract_canon_sha256":"2ae7f748a554d71917956c7ea791fe5260439eff7fc435c18e7aaad1672deab8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:03.294191Z","signature_b64":"pQGtz7+niaIO5rET9YefNfMtHk8qtoHDc5RjfoWhyFvXgpWz0vrgPAbdYAsbHkdDfSkp5TDmTw3BWRP5HkKcAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a9390a465f0153e4a39c6de4a47893774e26d8d7a45bdbeb4adf4511139c58a","last_reissued_at":"2026-05-18T01:40:03.293560Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:03.293560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Relativistic Nonextensive Thermodynamics","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Lavagno","submitted_at":"2002-07-15T09:53:52Z","abstract_excerpt":"Starting from the basic prescriptions of the Tsallis' nonextensive thermostatistics, i.e. generalized entropy and normalized q-expectation values, we study the relativistic nonextensive thermodynamics and derive a Boltzmann transport equation that implies the validity of the H-theorem where a local nonextensive four-entropy density is considered. Macroscopic thermodynamic functions and the equation of state for a perfect gas are derived at the equilibrium."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0207353","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":"cond-mat/0207353","created_at":"2026-05-18T01:40:03.293656+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0207353v1","created_at":"2026-05-18T01:40:03.293656+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0207353","created_at":"2026-05-18T01:40:03.293656+00:00"},{"alias_kind":"pith_short_12","alias_value":"JKJZBJDF6AKT","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_16","alias_value":"JKJZBJDF6AKT4SRZ","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_8","alias_value":"JKJZBJDF","created_at":"2026-05-18T12:25:50.845339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.17090","citing_title":"Non-extensive Hard Thermal Loop Resummation and Its Applications: Analysis in Zero and Finite Magnetic Fields","ref_index":67,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5","json":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5.json","graph_json":"https://pith.science/api/pith-number/JKJZBJDF6AKT4SRZY3PEUR4JG5/graph.json","events_json":"https://pith.science/api/pith-number/JKJZBJDF6AKT4SRZY3PEUR4JG5/events.json","paper":"https://pith.science/paper/JKJZBJDF"},"agent_actions":{"view_html":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5","download_json":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5.json","view_paper":"https://pith.science/paper/JKJZBJDF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0207353&json=true","fetch_graph":"https://pith.science/api/pith-number/JKJZBJDF6AKT4SRZY3PEUR4JG5/graph.json","fetch_events":"https://pith.science/api/pith-number/JKJZBJDF6AKT4SRZY3PEUR4JG5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5/action/storage_attestation","attest_author":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5/action/author_attestation","sign_citation":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5/action/citation_signature","submit_replication":"https://pith.science/pith/JKJZBJDF6AKT4SRZY3PEUR4JG5/action/replication_record"}},"created_at":"2026-05-18T01:40:03.293656+00:00","updated_at":"2026-05-18T01:40:03.293656+00:00"}