{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:QTVBCZ5SVTMF4CJY6IEU6YSXAC","short_pith_number":"pith:QTVBCZ5S","schema_version":"1.0","canonical_sha256":"84ea1167b2acd85e0938f2094f625700a1f71d92ef73c5b5b6e7cd13a018cf75","source":{"kind":"arxiv","id":"2110.07156","version":1},"attestation_state":"computed","paper":{"title":"Simple BSM explanations of $a_\\mu$ in light of the FNAL muon $g-2$ measurement","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Csaba Bal\\'azs, Dominik St\\\"ockinger, Douglas Jacob, Hyejung St\\\"ockinger-Kim, Peter Athron, Wojciech Kotlarski","submitted_at":"2021-10-14T05:08:09Z","abstract_excerpt":"Now that the Fermilab muon $g-2$ experiment has released the results of its Run-1 data, which agrees with the results of the Brookhaven experiment, one can examine the potential of simple extensions to explain the combined $4.2\\sigma$ discrepancy between the SM prediction and experiment. This proceeding examines a single-, two-, and three-field extension of the standard model and examines their ability to explain the muon $g-2$ anomaly, and where possible, produce a dark matter candidate particle with the observed relic density. This is based on work carried out for Ref. [1]. It is found that "},"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":"2110.07156","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ph","submitted_at":"2021-10-14T05:08:09Z","cross_cats_sorted":[],"title_canon_sha256":"790bcad4d81f401e5eb0cc574093799d058d39dbb0d5a97439e341c2c1c0e9ba","abstract_canon_sha256":"e69c141e68594dfc8785ff23de9acc3126e7643655e80ac8dbe17a0b18022458"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:22:39.429405Z","signature_b64":"8/i+nx7hywK/PrsRa8cjlNuQl586wMhjBDM1COqhkRBVLvmeamo2trVZt3PUYhN+cPYBp4khgON4KmmKrjuzBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84ea1167b2acd85e0938f2094f625700a1f71d92ef73c5b5b6e7cd13a018cf75","last_reissued_at":"2026-07-05T03:22:39.429020Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:22:39.429020Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simple BSM explanations of $a_\\mu$ in light of the FNAL muon $g-2$ measurement","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Csaba Bal\\'azs, Dominik St\\\"ockinger, Douglas Jacob, Hyejung St\\\"ockinger-Kim, Peter Athron, Wojciech Kotlarski","submitted_at":"2021-10-14T05:08:09Z","abstract_excerpt":"Now that the Fermilab muon $g-2$ experiment has released the results of its Run-1 data, which agrees with the results of the Brookhaven experiment, one can examine the potential of simple extensions to explain the combined $4.2\\sigma$ discrepancy between the SM prediction and experiment. This proceeding examines a single-, two-, and three-field extension of the standard model and examines their ability to explain the muon $g-2$ anomaly, and where possible, produce a dark matter candidate particle with the observed relic density. This is based on work carried out for Ref. [1]. It is found that "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.07156","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/2110.07156/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":"2110.07156","created_at":"2026-07-05T03:22:39.429072+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.07156v1","created_at":"2026-07-05T03:22:39.429072+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.07156","created_at":"2026-07-05T03:22:39.429072+00:00"},{"alias_kind":"pith_short_12","alias_value":"QTVBCZ5SVTMF","created_at":"2026-07-05T03:22:39.429072+00:00"},{"alias_kind":"pith_short_16","alias_value":"QTVBCZ5SVTMF4CJY","created_at":"2026-07-05T03:22:39.429072+00:00"},{"alias_kind":"pith_short_8","alias_value":"QTVBCZ5S","created_at":"2026-07-05T03:22:39.429072+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/QTVBCZ5SVTMF4CJY6IEU6YSXAC","json":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC.json","graph_json":"https://pith.science/api/pith-number/QTVBCZ5SVTMF4CJY6IEU6YSXAC/graph.json","events_json":"https://pith.science/api/pith-number/QTVBCZ5SVTMF4CJY6IEU6YSXAC/events.json","paper":"https://pith.science/paper/QTVBCZ5S"},"agent_actions":{"view_html":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC","download_json":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC.json","view_paper":"https://pith.science/paper/QTVBCZ5S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.07156&json=true","fetch_graph":"https://pith.science/api/pith-number/QTVBCZ5SVTMF4CJY6IEU6YSXAC/graph.json","fetch_events":"https://pith.science/api/pith-number/QTVBCZ5SVTMF4CJY6IEU6YSXAC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC/action/storage_attestation","attest_author":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC/action/author_attestation","sign_citation":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC/action/citation_signature","submit_replication":"https://pith.science/pith/QTVBCZ5SVTMF4CJY6IEU6YSXAC/action/replication_record"}},"created_at":"2026-07-05T03:22:39.429072+00:00","updated_at":"2026-07-05T03:22:39.429072+00:00"}