{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:3R47DZWNLLXLKNA7AYWBOAOH2F","short_pith_number":"pith:3R47DZWN","schema_version":"1.0","canonical_sha256":"dc79f1e6cd5aeeb5341f062c1701c7d14add4fa4c7d0ae280263fc4783334901","source":{"kind":"arxiv","id":"1402.1458","version":1},"attestation_state":"computed","paper":{"title":"Thermalization of Hadrons via Hagedorn States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Greiner, K. Gallmeister, M. Beitel","submitted_at":"2014-02-06T19:06:20Z","abstract_excerpt":"Hagedorn states are characterized by being very massive hadron-like resonances and by not being limited to quantum numbers of known hadrons. To generate such a zoo of different Hagedorn states, a covariantly formulated bootstrap equation is solved by ensuring energy conservation and conservation of baryon number $B$, strangeness $S$ and electric charge $Q$. The numerical solution of this equation provides Hagedorn spectra, which enable to obtain the decay width for Hagedorn states needed in cascading decay simulations. A single (heavy) Hagedorn state cascades by various two-body decay channels"},"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":"1402.1458","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-06T19:06:20Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"688bf2ee4e424ef0198e2af919d489c76797664b6b8481db16767ed5f0d75a7d","abstract_canon_sha256":"8aaf1f7a7951fb65bf6a3efa7e0659d968fd50d9027168e3a5014d5a3593158c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:40:10.761912Z","signature_b64":"qVjjdyk/O5LLVswx5Og8fhqhkqx4DsXsDLg5ciZprLF7ANWqHso7lb7GZ8TRZDXNn4XfTBVO+IgLRfDP63wcAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc79f1e6cd5aeeb5341f062c1701c7d14add4fa4c7d0ae280263fc4783334901","last_reissued_at":"2026-05-18T02:40:10.761420Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:40:10.761420Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermalization of Hadrons via Hagedorn States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Greiner, K. Gallmeister, M. Beitel","submitted_at":"2014-02-06T19:06:20Z","abstract_excerpt":"Hagedorn states are characterized by being very massive hadron-like resonances and by not being limited to quantum numbers of known hadrons. To generate such a zoo of different Hagedorn states, a covariantly formulated bootstrap equation is solved by ensuring energy conservation and conservation of baryon number $B$, strangeness $S$ and electric charge $Q$. The numerical solution of this equation provides Hagedorn spectra, which enable to obtain the decay width for Hagedorn states needed in cascading decay simulations. A single (heavy) Hagedorn state cascades by various two-body decay channels"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.1458","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":"1402.1458","created_at":"2026-05-18T02:40:10.761491+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.1458v1","created_at":"2026-05-18T02:40:10.761491+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.1458","created_at":"2026-05-18T02:40:10.761491+00:00"},{"alias_kind":"pith_short_12","alias_value":"3R47DZWNLLXL","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"3R47DZWNLLXLKNA7","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"3R47DZWN","created_at":"2026-05-18T12:28:11.866339+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/3R47DZWNLLXLKNA7AYWBOAOH2F","json":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F.json","graph_json":"https://pith.science/api/pith-number/3R47DZWNLLXLKNA7AYWBOAOH2F/graph.json","events_json":"https://pith.science/api/pith-number/3R47DZWNLLXLKNA7AYWBOAOH2F/events.json","paper":"https://pith.science/paper/3R47DZWN"},"agent_actions":{"view_html":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F","download_json":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F.json","view_paper":"https://pith.science/paper/3R47DZWN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.1458&json=true","fetch_graph":"https://pith.science/api/pith-number/3R47DZWNLLXLKNA7AYWBOAOH2F/graph.json","fetch_events":"https://pith.science/api/pith-number/3R47DZWNLLXLKNA7AYWBOAOH2F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F/action/storage_attestation","attest_author":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F/action/author_attestation","sign_citation":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F/action/citation_signature","submit_replication":"https://pith.science/pith/3R47DZWNLLXLKNA7AYWBOAOH2F/action/replication_record"}},"created_at":"2026-05-18T02:40:10.761491+00:00","updated_at":"2026-05-18T02:40:10.761491+00:00"}