{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:BN2JMV64HE5K4IAL4PD6JDYIHF","short_pith_number":"pith:BN2JMV64","schema_version":"1.0","canonical_sha256":"0b749657dc393aae200be3c7e48f083945f6d1eabbd8e5078d09e2b638b6b125","source":{"kind":"arxiv","id":"2212.09454","version":3},"attestation_state":"computed","paper":{"title":"Leptogenesis via Inflaton Mass Terms in Non-Minimally Coupled Inflation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"John McDonald, Kit Lloyd-Stubbs","submitted_at":"2022-12-19T13:47:15Z","abstract_excerpt":"We consider a model of baryogenesis based on adding lepton number-violating quadratic mass terms to the inflaton potential of a non-minimally coupled inflation model. The $L$-violating mass terms generate a lepton asymmetry in a complex inflaton field via the mass term Affleck-Dine mechanism, which is transferred to the Standard Model (SM) sector when the inflaton decays to right-handed (RH) neutrinos. The model is minimal in that it requires only the SM sector, RH neutrinos, and a non-minimally coupled inflaton sector. We find that baryon isocurvature fluctuations can be observable in metric "},"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":"2212.09454","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-12-19T13:47:15Z","cross_cats_sorted":["astro-ph.CO","gr-qc","hep-th"],"title_canon_sha256":"e4a7c585c0800ca51d232e66b7469bd0b9091bff572ae2fc9b85cc8af3ca88ba","abstract_canon_sha256":"8acbafb097a3b307c5481a5e8ee85d9cfd3b4b476f03f0e3caa3c7a585e531bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:29:37.550377Z","signature_b64":"bjSxsVArTTSQrWhr4J64/LZ7BSZJWbkXYJGMZuEWL/pDM1sRx3NqhIHq/BbQlR9jMjHhkiqOjLixNYfxTFN2Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0b749657dc393aae200be3c7e48f083945f6d1eabbd8e5078d09e2b638b6b125","last_reissued_at":"2026-07-05T06:29:37.549892Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:29:37.549892Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Leptogenesis via Inflaton Mass Terms in Non-Minimally Coupled Inflation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"John McDonald, Kit Lloyd-Stubbs","submitted_at":"2022-12-19T13:47:15Z","abstract_excerpt":"We consider a model of baryogenesis based on adding lepton number-violating quadratic mass terms to the inflaton potential of a non-minimally coupled inflation model. The $L$-violating mass terms generate a lepton asymmetry in a complex inflaton field via the mass term Affleck-Dine mechanism, which is transferred to the Standard Model (SM) sector when the inflaton decays to right-handed (RH) neutrinos. The model is minimal in that it requires only the SM sector, RH neutrinos, and a non-minimally coupled inflaton sector. We find that baryon isocurvature fluctuations can be observable in metric "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.09454","kind":"arxiv","version":3},"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/2212.09454/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":"2212.09454","created_at":"2026-07-05T06:29:37.549952+00:00"},{"alias_kind":"arxiv_version","alias_value":"2212.09454v3","created_at":"2026-07-05T06:29:37.549952+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.09454","created_at":"2026-07-05T06:29:37.549952+00:00"},{"alias_kind":"pith_short_12","alias_value":"BN2JMV64HE5K","created_at":"2026-07-05T06:29:37.549952+00:00"},{"alias_kind":"pith_short_16","alias_value":"BN2JMV64HE5K4IAL","created_at":"2026-07-05T06:29:37.549952+00:00"},{"alias_kind":"pith_short_8","alias_value":"BN2JMV64","created_at":"2026-07-05T06:29:37.549952+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2508.10103","citing_title":"Leptogenesis and neutrino mass with one right-handed neutrino and Higgs inflaton","ref_index":54,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF","json":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF.json","graph_json":"https://pith.science/api/pith-number/BN2JMV64HE5K4IAL4PD6JDYIHF/graph.json","events_json":"https://pith.science/api/pith-number/BN2JMV64HE5K4IAL4PD6JDYIHF/events.json","paper":"https://pith.science/paper/BN2JMV64"},"agent_actions":{"view_html":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF","download_json":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF.json","view_paper":"https://pith.science/paper/BN2JMV64","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2212.09454&json=true","fetch_graph":"https://pith.science/api/pith-number/BN2JMV64HE5K4IAL4PD6JDYIHF/graph.json","fetch_events":"https://pith.science/api/pith-number/BN2JMV64HE5K4IAL4PD6JDYIHF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF/action/storage_attestation","attest_author":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF/action/author_attestation","sign_citation":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF/action/citation_signature","submit_replication":"https://pith.science/pith/BN2JMV64HE5K4IAL4PD6JDYIHF/action/replication_record"}},"created_at":"2026-07-05T06:29:37.549952+00:00","updated_at":"2026-07-05T06:29:37.549952+00:00"}