{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:ATDG5ROXJ2JR6NSJWMOHNIQN3O","short_pith_number":"pith:ATDG5ROX","schema_version":"1.0","canonical_sha256":"04c66ec5d74e931f3649b31c76a20ddba80d509ccaf77d7ce7a69208c62eeb9f","source":{"kind":"arxiv","id":"hep-ph/9611440","version":1},"attestation_state":"computed","paper":{"title":"Baryogenesis from baryon number violating scalar interactions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. P. Bowes, R. R. Volkas","submitted_at":"1996-11-26T22:15:54Z","abstract_excerpt":"In the following work we consider the possibility of explaining the observed baryon number asymmetry in the universe from simple baryon number violating modifications, involving massive scalar bosons, to the Standard Model. In these cases baryon number violation is mediated through a combination of Yukawa and scalar self-coupling interactions. Starting with a previously compiled catalogue of baryon-number violating extensions of the Standard Model, we identify the minimal subsets which can induce a $B-L$ asymmetry and thus be immune to sphaleron washout. For each of these models, we identify t"},"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/9611440","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-11-26T22:15:54Z","cross_cats_sorted":[],"title_canon_sha256":"c7548de864104335cfafa4f7dd263e498e9959528a13b58a33844ea047bbcc73","abstract_canon_sha256":"3044b2f40e40832b8f404b1fbe44db3d10c7aa34f62ce90159ffbfb6e372c15d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:00.443598Z","signature_b64":"QEJwxQ1772Jq5JzwfX7PxG1NO6OKBAtlJZ7J3RqbqhU/zrIqQ1UsA0DCjp8XNrtP2VIaJxlOqRxf/TZDOVybAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04c66ec5d74e931f3649b31c76a20ddba80d509ccaf77d7ce7a69208c62eeb9f","last_reissued_at":"2026-07-04T16:02:00.443236Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:00.443236Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryogenesis from baryon number violating scalar interactions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. P. Bowes, R. R. Volkas","submitted_at":"1996-11-26T22:15:54Z","abstract_excerpt":"In the following work we consider the possibility of explaining the observed baryon number asymmetry in the universe from simple baryon number violating modifications, involving massive scalar bosons, to the Standard Model. In these cases baryon number violation is mediated through a combination of Yukawa and scalar self-coupling interactions. Starting with a previously compiled catalogue of baryon-number violating extensions of the Standard Model, we identify the minimal subsets which can induce a $B-L$ asymmetry and thus be immune to sphaleron washout. For each of these models, we identify t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9611440","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9611440/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":"hep-ph/9611440","created_at":"2026-07-04T16:02:00.443293+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9611440v1","created_at":"2026-07-04T16:02:00.443293+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9611440","created_at":"2026-07-04T16:02:00.443293+00:00"},{"alias_kind":"pith_short_12","alias_value":"ATDG5ROXJ2JR","created_at":"2026-07-04T16:02:00.443293+00:00"},{"alias_kind":"pith_short_16","alias_value":"ATDG5ROXJ2JR6NSJ","created_at":"2026-07-04T16:02:00.443293+00:00"},{"alias_kind":"pith_short_8","alias_value":"ATDG5ROX","created_at":"2026-07-04T16:02:00.443293+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.25989","citing_title":"EFT Pathways to $|\\Delta B| =2$: Chiral Constructions and Phenomenology","ref_index":36,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O","json":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O.json","graph_json":"https://pith.science/api/pith-number/ATDG5ROXJ2JR6NSJWMOHNIQN3O/graph.json","events_json":"https://pith.science/api/pith-number/ATDG5ROXJ2JR6NSJWMOHNIQN3O/events.json","paper":"https://pith.science/paper/ATDG5ROX"},"agent_actions":{"view_html":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O","download_json":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O.json","view_paper":"https://pith.science/paper/ATDG5ROX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9611440&json=true","fetch_graph":"https://pith.science/api/pith-number/ATDG5ROXJ2JR6NSJWMOHNIQN3O/graph.json","fetch_events":"https://pith.science/api/pith-number/ATDG5ROXJ2JR6NSJWMOHNIQN3O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O/action/storage_attestation","attest_author":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O/action/author_attestation","sign_citation":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O/action/citation_signature","submit_replication":"https://pith.science/pith/ATDG5ROXJ2JR6NSJWMOHNIQN3O/action/replication_record"}},"created_at":"2026-07-04T16:02:00.443293+00:00","updated_at":"2026-07-04T16:02:00.443293+00:00"}