{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:7BKTZWMZ2E6LLRP7WS76WWX6ML","short_pith_number":"pith:7BKTZWMZ","schema_version":"1.0","canonical_sha256":"f8553cd999d13cb5c5ffb4bfeb5afe62c292c8909d14dfa0b2050266c3afd96e","source":{"kind":"arxiv","id":"1211.0512","version":1},"attestation_state":"computed","paper":{"title":"The minimal scenario of leptogenesis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Pasquale Di Bari, Steve Blanchet","submitted_at":"2012-11-02T18:14:37Z","abstract_excerpt":"We review the main features and results of thermal leptogenesis within the type I seesaw mechanism, the minimal extension of the Standard Model explaining neutrino masses and mixing. After presenting the simplest approach, the vanilla scenario, we discuss various important developments in recent years, such as the inclusion of lepton and heavy neutrino flavour effects, a description beyond a hierarchical heavy neutrino mass spectrum and an improved kinetic description within the density matrix and the closed-time-path formalisms. We also discuss how leptogenesis can ultimately represent an imp"},"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":"1211.0512","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-11-02T18:14:37Z","cross_cats_sorted":[],"title_canon_sha256":"392bec4a0d087eb5545e887d3c6d06b4d5467ed4939bcc492471a8b5d6782700","abstract_canon_sha256":"54143444fbfc6dcc751f8aa5987549c3e586d80c51a0016096c2cf4a8e59b3ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:53:26.496051Z","signature_b64":"i75YNILtH8ohY7AX1Gf1jYdl3zUu5JkaSitKwJjsEvHSMrCDjmcnM+EgJdDL45+wwqgo3XvnMV9hYQ30UysKDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f8553cd999d13cb5c5ffb4bfeb5afe62c292c8909d14dfa0b2050266c3afd96e","last_reissued_at":"2026-05-18T01:53:26.495352Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:53:26.495352Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The minimal scenario of leptogenesis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Pasquale Di Bari, Steve Blanchet","submitted_at":"2012-11-02T18:14:37Z","abstract_excerpt":"We review the main features and results of thermal leptogenesis within the type I seesaw mechanism, the minimal extension of the Standard Model explaining neutrino masses and mixing. After presenting the simplest approach, the vanilla scenario, we discuss various important developments in recent years, such as the inclusion of lepton and heavy neutrino flavour effects, a description beyond a hierarchical heavy neutrino mass spectrum and an improved kinetic description within the density matrix and the closed-time-path formalisms. We also discuss how leptogenesis can ultimately represent an imp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.0512","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":"1211.0512","created_at":"2026-05-18T01:53:26.495484+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.0512v1","created_at":"2026-05-18T01:53:26.495484+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.0512","created_at":"2026-05-18T01:53:26.495484+00:00"},{"alias_kind":"pith_short_12","alias_value":"7BKTZWMZ2E6L","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"7BKTZWMZ2E6LLRP7","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"7BKTZWMZ","created_at":"2026-05-18T12:26:56.085431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.09571","citing_title":"Einstein-Cartan pseudoscalaron inflation, reheating and nonthermal leptogenesis","ref_index":69,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19434","citing_title":"$SO(10)$-inspired leptogenesis","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML","json":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML.json","graph_json":"https://pith.science/api/pith-number/7BKTZWMZ2E6LLRP7WS76WWX6ML/graph.json","events_json":"https://pith.science/api/pith-number/7BKTZWMZ2E6LLRP7WS76WWX6ML/events.json","paper":"https://pith.science/paper/7BKTZWMZ"},"agent_actions":{"view_html":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML","download_json":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML.json","view_paper":"https://pith.science/paper/7BKTZWMZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.0512&json=true","fetch_graph":"https://pith.science/api/pith-number/7BKTZWMZ2E6LLRP7WS76WWX6ML/graph.json","fetch_events":"https://pith.science/api/pith-number/7BKTZWMZ2E6LLRP7WS76WWX6ML/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML/action/storage_attestation","attest_author":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML/action/author_attestation","sign_citation":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML/action/citation_signature","submit_replication":"https://pith.science/pith/7BKTZWMZ2E6LLRP7WS76WWX6ML/action/replication_record"}},"created_at":"2026-05-18T01:53:26.495484+00:00","updated_at":"2026-05-18T01:53:26.495484+00:00"}