{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:LUYPGQ6A4BGVXAJSWHD3F2NLXE","short_pith_number":"pith:LUYPGQ6A","schema_version":"1.0","canonical_sha256":"5d30f343c0e04d5b8132b1c7b2e9abb91a1e323eb468bf8016c9245442120d32","source":{"kind":"arxiv","id":"2107.07518","version":2},"attestation_state":"computed","paper":{"title":"Muonic Force Behind Flavor Anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Admir Greljo, Anders Eller Thomsen, Jure Zupan, Peter Stangl, Yotam Soreq","submitted_at":"2021-07-15T18:00:00Z","abstract_excerpt":"We develop an economical theoretical framework for combined explanations of the flavor physics anomalies involving muons: $(g-2)_\\mu$, $R_{K^{(*)}}$, and $b \\to s \\mu^+ \\mu^-$ angular distributions and branching ratios, that was first initiated by some of us in Ref. [1]. The Standard Model (SM) is supplemented with a lepton-flavored $\\mathrm{U}(1)_X$ gauge group. The $\\mathrm{U}(1)_X$ gauge boson with the mass of $\\mathcal{O}(0.1)$ GeV resolves the $(g-2)_\\mu$ tension. A TeV-scale leptoquark, charged under the $\\mathrm{U}(1)_X$, carries a muon number and mediates $B$-decays without prompting c"},"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":"2107.07518","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-07-15T18:00:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"da83ba44201b3be2515961014619792e1c68e067c8aea0369521949b50c2fcd7","abstract_canon_sha256":"d0c00d62ab355cb3d6d756aac21d9d085b5fc75f804ad06c8beb327869982877"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:23:36.181183Z","signature_b64":"/rfwNuQvunszMP6Z4gqbh/QTIAvnOKlKVwbTIYYYhFfbzLvzk0+OVcjVe3yta5lwAR+lTcvbzVL4mp4BpZErAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d30f343c0e04d5b8132b1c7b2e9abb91a1e323eb468bf8016c9245442120d32","last_reissued_at":"2026-07-05T04:23:36.180818Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:23:36.180818Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Muonic Force Behind Flavor Anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Admir Greljo, Anders Eller Thomsen, Jure Zupan, Peter Stangl, Yotam Soreq","submitted_at":"2021-07-15T18:00:00Z","abstract_excerpt":"We develop an economical theoretical framework for combined explanations of the flavor physics anomalies involving muons: $(g-2)_\\mu$, $R_{K^{(*)}}$, and $b \\to s \\mu^+ \\mu^-$ angular distributions and branching ratios, that was first initiated by some of us in Ref. [1]. The Standard Model (SM) is supplemented with a lepton-flavored $\\mathrm{U}(1)_X$ gauge group. The $\\mathrm{U}(1)_X$ gauge boson with the mass of $\\mathcal{O}(0.1)$ GeV resolves the $(g-2)_\\mu$ tension. A TeV-scale leptoquark, charged under the $\\mathrm{U}(1)_X$, carries a muon number and mediates $B$-decays without prompting c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.07518","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/2107.07518/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":"2107.07518","created_at":"2026-07-05T04:23:36.180880+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.07518v2","created_at":"2026-07-05T04:23:36.180880+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.07518","created_at":"2026-07-05T04:23:36.180880+00:00"},{"alias_kind":"pith_short_12","alias_value":"LUYPGQ6A4BGV","created_at":"2026-07-05T04:23:36.180880+00:00"},{"alias_kind":"pith_short_16","alias_value":"LUYPGQ6A4BGVXAJS","created_at":"2026-07-05T04:23:36.180880+00:00"},{"alias_kind":"pith_short_8","alias_value":"LUYPGQ6A","created_at":"2026-07-05T04:23:36.180880+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.05104","citing_title":"Weak decays of $B_s$ meson in self-consistent covariant light-front approach","ref_index":46,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE","json":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE.json","graph_json":"https://pith.science/api/pith-number/LUYPGQ6A4BGVXAJSWHD3F2NLXE/graph.json","events_json":"https://pith.science/api/pith-number/LUYPGQ6A4BGVXAJSWHD3F2NLXE/events.json","paper":"https://pith.science/paper/LUYPGQ6A"},"agent_actions":{"view_html":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE","download_json":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE.json","view_paper":"https://pith.science/paper/LUYPGQ6A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.07518&json=true","fetch_graph":"https://pith.science/api/pith-number/LUYPGQ6A4BGVXAJSWHD3F2NLXE/graph.json","fetch_events":"https://pith.science/api/pith-number/LUYPGQ6A4BGVXAJSWHD3F2NLXE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE/action/storage_attestation","attest_author":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE/action/author_attestation","sign_citation":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE/action/citation_signature","submit_replication":"https://pith.science/pith/LUYPGQ6A4BGVXAJSWHD3F2NLXE/action/replication_record"}},"created_at":"2026-07-05T04:23:36.180880+00:00","updated_at":"2026-07-05T04:23:36.180880+00:00"}