{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:BAMOCG5ZX6WFG7KFUYJ2J7LOMN","short_pith_number":"pith:BAMOCG5Z","schema_version":"1.0","canonical_sha256":"0818e11bb9bfac537d45a613a4fd6e636a1a0c8c82a7e7530f19d47367f98b90","source":{"kind":"arxiv","id":"1907.10019","version":1},"attestation_state":"computed","paper":{"title":"Double type-II seesaw accompanied by Dirac fermionic dark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Pei-Hong Gu","submitted_at":"2019-07-23T17:24:20Z","abstract_excerpt":"In the type-II seesaw mechanism, the neutrino mass generation could be tested experimentally if the Higgs triplet is at the TeV scale and has a small cubic coupling to the standard model Higgs doublet. We show such small triplet-doublet coupling and the cosmic baryon asymmetry can be simultaneously induced by an additional seesaw mechanism involving a $U(1)_{B-L}$ gauge symmetry. Meanwhile, three neutral fermions for cancelling the gauge anomalies can form a stable Dirac fermionic dark matter besides an acceptably massless fermion."},"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":"1907.10019","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-23T17:24:20Z","cross_cats_sorted":[],"title_canon_sha256":"eae75b800cca8e378195ff67e50fa8e70798f20c98301e66a3d374d6f27b2f36","abstract_canon_sha256":"9e4ea734f9e101be87cf3f6accdc52e91a53146b83f1b75c3d4098975a71933f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:33:14.399722Z","signature_b64":"f+wPBHLdXtNK5RPTqO8IrvljOFO6USH/J/r/jH+SEuGZ/dB0VfhDPGO2mnHU1oZSm/pO8uQmNfCmPdyQS6OHCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0818e11bb9bfac537d45a613a4fd6e636a1a0c8c82a7e7530f19d47367f98b90","last_reissued_at":"2026-07-05T00:33:14.399209Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:33:14.399209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Double type-II seesaw accompanied by Dirac fermionic dark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Pei-Hong Gu","submitted_at":"2019-07-23T17:24:20Z","abstract_excerpt":"In the type-II seesaw mechanism, the neutrino mass generation could be tested experimentally if the Higgs triplet is at the TeV scale and has a small cubic coupling to the standard model Higgs doublet. We show such small triplet-doublet coupling and the cosmic baryon asymmetry can be simultaneously induced by an additional seesaw mechanism involving a $U(1)_{B-L}$ gauge symmetry. Meanwhile, three neutral fermions for cancelling the gauge anomalies can form a stable Dirac fermionic dark matter besides an acceptably massless fermion."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.10019","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/1907.10019/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":"1907.10019","created_at":"2026-07-05T00:33:14.399273+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.10019v1","created_at":"2026-07-05T00:33:14.399273+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.10019","created_at":"2026-07-05T00:33:14.399273+00:00"},{"alias_kind":"pith_short_12","alias_value":"BAMOCG5ZX6WF","created_at":"2026-07-05T00:33:14.399273+00:00"},{"alias_kind":"pith_short_16","alias_value":"BAMOCG5ZX6WFG7KF","created_at":"2026-07-05T00:33:14.399273+00:00"},{"alias_kind":"pith_short_8","alias_value":"BAMOCG5Z","created_at":"2026-07-05T00:33:14.399273+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.03795","citing_title":"Neutrino mass generation via the inverse seesaw mechanism in a $U(1)_{B-L}$ gauge extension","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN","json":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN.json","graph_json":"https://pith.science/api/pith-number/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/graph.json","events_json":"https://pith.science/api/pith-number/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/events.json","paper":"https://pith.science/paper/BAMOCG5Z"},"agent_actions":{"view_html":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN","download_json":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN.json","view_paper":"https://pith.science/paper/BAMOCG5Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.10019&json=true","fetch_graph":"https://pith.science/api/pith-number/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/graph.json","fetch_events":"https://pith.science/api/pith-number/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/action/storage_attestation","attest_author":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/action/author_attestation","sign_citation":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/action/citation_signature","submit_replication":"https://pith.science/pith/BAMOCG5ZX6WFG7KFUYJ2J7LOMN/action/replication_record"}},"created_at":"2026-07-05T00:33:14.399273+00:00","updated_at":"2026-07-05T00:33:14.399273+00:00"}