{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:JDDM5X3LGRAFYAOXFZ5CMOYW7H","short_pith_number":"pith:JDDM5X3L","schema_version":"1.0","canonical_sha256":"48c6cedf6b34405c01d72e7a263b16f9dcd4b386f8e211b85b0db9aee8e0d86b","source":{"kind":"arxiv","id":"hep-ph/9602260","version":2},"attestation_state":"computed","paper":{"title":"Big Bang nucleosynthesis and physics beyond the Standard Model","license":"","headline":"","cross_cats":["astro-ph","nucl-th"],"primary_cat":"hep-ph","authors_text":"Subir Sarkar (Oxford)","submitted_at":"1996-02-08T20:51:34Z","abstract_excerpt":"The Hubble expansion of galaxies, the $2.73\\dK$ blackbody radiation background and the cosmic abundances of the light elements argue for a hot, dense origin of the universe --- the standard Big Bang cosmology --- and enable its evolution to be traced back fairly reliably to the nucleosynthesis era when the temperature was of $\\Or(1)$ MeV corresponding to an expansion age of $\\Or(1)$ sec. All particles, known and hypothetical, would have been created at higher temperatures in the early universe and analyses of their possible effects on the abundances of the synthesized elements enable many inte"},"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":"hep-ph/9602260","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-02-08T20:51:34Z","cross_cats_sorted":["astro-ph","nucl-th"],"title_canon_sha256":"6c08c60789b5efb209071dc4aa2be153080cbcb0abcbeecc348d2a94dd0ddab7","abstract_canon_sha256":"cb3b06bd5c9087897c7ff1d3c05c47b5ff97b60bc17c0aa06f08f7fe0408d391"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:37.593485Z","signature_b64":"L2+eqWRSd6oc6DSSUx7tsub3T+eW5clmnU/pdkNVTF5++xa4EkXDdC0vW9LM2LN78UiMpaGzsinU7c1FDnxdBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48c6cedf6b34405c01d72e7a263b16f9dcd4b386f8e211b85b0db9aee8e0d86b","last_reissued_at":"2026-05-18T04:28:37.593014Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:37.593014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Big Bang nucleosynthesis and physics beyond the Standard Model","license":"","headline":"","cross_cats":["astro-ph","nucl-th"],"primary_cat":"hep-ph","authors_text":"Subir Sarkar (Oxford)","submitted_at":"1996-02-08T20:51:34Z","abstract_excerpt":"The Hubble expansion of galaxies, the $2.73\\dK$ blackbody radiation background and the cosmic abundances of the light elements argue for a hot, dense origin of the universe --- the standard Big Bang cosmology --- and enable its evolution to be traced back fairly reliably to the nucleosynthesis era when the temperature was of $\\Or(1)$ MeV corresponding to an expansion age of $\\Or(1)$ sec. All particles, known and hypothetical, would have been created at higher temperatures in the early universe and analyses of their possible effects on the abundances of the synthesized elements enable many inte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9602260","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":""},"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":"hep-ph/9602260","created_at":"2026-05-18T04:28:37.593088+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9602260v2","created_at":"2026-05-18T04:28:37.593088+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9602260","created_at":"2026-05-18T04:28:37.593088+00:00"},{"alias_kind":"pith_short_12","alias_value":"JDDM5X3LGRAF","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"JDDM5X3LGRAFYAOX","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"JDDM5X3L","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.27521","citing_title":"From WIMP to FIMP during reheating: collider vs non-collider probes for p-wave annihilation","ref_index":59,"is_internal_anchor":true},{"citing_arxiv_id":"2604.09843","citing_title":"Induced Multi-phase Inflation with Reheating: Leptogenesis and Dark Matter Production in Metric versus Palatini","ref_index":74,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04870","citing_title":"Probing Unification Scenarios with Big Bang Nucleosynthesis","ref_index":3,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H","json":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H.json","graph_json":"https://pith.science/api/pith-number/JDDM5X3LGRAFYAOXFZ5CMOYW7H/graph.json","events_json":"https://pith.science/api/pith-number/JDDM5X3LGRAFYAOXFZ5CMOYW7H/events.json","paper":"https://pith.science/paper/JDDM5X3L"},"agent_actions":{"view_html":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H","download_json":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H.json","view_paper":"https://pith.science/paper/JDDM5X3L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9602260&json=true","fetch_graph":"https://pith.science/api/pith-number/JDDM5X3LGRAFYAOXFZ5CMOYW7H/graph.json","fetch_events":"https://pith.science/api/pith-number/JDDM5X3LGRAFYAOXFZ5CMOYW7H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H/action/storage_attestation","attest_author":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H/action/author_attestation","sign_citation":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H/action/citation_signature","submit_replication":"https://pith.science/pith/JDDM5X3LGRAFYAOXFZ5CMOYW7H/action/replication_record"}},"created_at":"2026-05-18T04:28:37.593088+00:00","updated_at":"2026-05-18T04:28:37.593088+00:00"}