{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:AS54FUZBVYOEH4R7WDCJ66IA6U","short_pith_number":"pith:AS54FUZB","schema_version":"1.0","canonical_sha256":"04bbc2d321ae1c43f23fb0c49f7900f5148706632a5b6b3cf585ebb215f177a4","source":{"kind":"arxiv","id":"2103.13149","version":2},"attestation_state":"computed","paper":{"title":"Inverse seesaw and $(g-2)$ anomalies in $B-L$ extended two Higgs doublet model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiroshi Okada, Tanmoy Mondal","submitted_at":"2021-03-24T12:49:14Z","abstract_excerpt":"We propose a gauged $U(1)_{B-L}$ extended two Higgs doublet model to explain both neutrino mass and lepton anomalous magnetic moments ($g-2$). Neutrino mass is generated via an inverse seesaw mechanism by introducing singlet fermions. Especially, we update the result of muon $g-2$ in light of the very recent report by E989 experiment at Fermilab, indicating $a_\\mu^{\\rm FNAL}=116592040(54)\\times 10^{-11}$. Combining BNL result, we have the following deviation from the standard model prediction $\\Delta a_\\mu=(2.51\\pm 5.9)\\times10^{-10}$ at 4.2 $\\sigma$. Thanks to an appropriate assignment for $U"},"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":"2103.13149","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-03-24T12:49:14Z","cross_cats_sorted":[],"title_canon_sha256":"36a63182567de3ee64fdd56643e14d4409bc2632461e72423ddbcd93b99e6f81","abstract_canon_sha256":"dd192e4c0e54d059630360def7e8ade88fa614804ff3e69442e0af0d28751a3b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:11:44.658164Z","signature_b64":"fCbYfnpjfsVoiiH34Po2p2XdfKuw/TKiICdIcoHSvytqIFJZefm3B7usKecu13hKAzjrEwX1W66wnDSxyHSFBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04bbc2d321ae1c43f23fb0c49f7900f5148706632a5b6b3cf585ebb215f177a4","last_reissued_at":"2026-07-05T04:11:44.657679Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:11:44.657679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inverse seesaw and $(g-2)$ anomalies in $B-L$ extended two Higgs doublet model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiroshi Okada, Tanmoy Mondal","submitted_at":"2021-03-24T12:49:14Z","abstract_excerpt":"We propose a gauged $U(1)_{B-L}$ extended two Higgs doublet model to explain both neutrino mass and lepton anomalous magnetic moments ($g-2$). Neutrino mass is generated via an inverse seesaw mechanism by introducing singlet fermions. Especially, we update the result of muon $g-2$ in light of the very recent report by E989 experiment at Fermilab, indicating $a_\\mu^{\\rm FNAL}=116592040(54)\\times 10^{-11}$. Combining BNL result, we have the following deviation from the standard model prediction $\\Delta a_\\mu=(2.51\\pm 5.9)\\times10^{-10}$ at 4.2 $\\sigma$. Thanks to an appropriate assignment for $U"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.13149","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2103.13149/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":"2103.13149","created_at":"2026-07-05T04:11:44.657738+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.13149v2","created_at":"2026-07-05T04:11:44.657738+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.13149","created_at":"2026-07-05T04:11:44.657738+00:00"},{"alias_kind":"pith_short_12","alias_value":"AS54FUZBVYOE","created_at":"2026-07-05T04:11:44.657738+00:00"},{"alias_kind":"pith_short_16","alias_value":"AS54FUZBVYOEH4R7","created_at":"2026-07-05T04:11:44.657738+00:00"},{"alias_kind":"pith_short_8","alias_value":"AS54FUZB","created_at":"2026-07-05T04:11:44.657738+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U","json":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U.json","graph_json":"https://pith.science/api/pith-number/AS54FUZBVYOEH4R7WDCJ66IA6U/graph.json","events_json":"https://pith.science/api/pith-number/AS54FUZBVYOEH4R7WDCJ66IA6U/events.json","paper":"https://pith.science/paper/AS54FUZB"},"agent_actions":{"view_html":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U","download_json":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U.json","view_paper":"https://pith.science/paper/AS54FUZB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.13149&json=true","fetch_graph":"https://pith.science/api/pith-number/AS54FUZBVYOEH4R7WDCJ66IA6U/graph.json","fetch_events":"https://pith.science/api/pith-number/AS54FUZBVYOEH4R7WDCJ66IA6U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U/action/storage_attestation","attest_author":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U/action/author_attestation","sign_citation":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U/action/citation_signature","submit_replication":"https://pith.science/pith/AS54FUZBVYOEH4R7WDCJ66IA6U/action/replication_record"}},"created_at":"2026-07-05T04:11:44.657738+00:00","updated_at":"2026-07-05T04:11:44.657738+00:00"}