{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:ETHLMIVS5F4V3DTEIF76MWNRGQ","short_pith_number":"pith:ETHLMIVS","schema_version":"1.0","canonical_sha256":"24ceb622b2e9795d8e64417fe659b1342adcecd3168593471eb19ec84f743fb1","source":{"kind":"arxiv","id":"2206.11305","version":1},"attestation_state":"computed","paper":{"title":"The $B$ Anomalies, the $U_1$ Leptoquark and Dark Matter","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander Pukhov, David London, Genevi\\`eve B\\'elanger, Jacky Kumar","submitted_at":"2022-06-22T18:16:16Z","abstract_excerpt":"The present-day $B$-anomalies involving $b \\to s \\mu^+ \\mu^-$ or $b \\to c \\tau^- {\\bar\\nu}$ transitions can all be explained with the addition of a vector $U_1$ leptoquark with a mass of $M_{U_1} \\ge 1.8$ TeV. In the scalar singlet dark matter model (SSDMM), the DM is a scalar $S$ that couples to the Higgs via $\\lambda_{hS} \\, S^2|H|^2$. We update the fit to the data and find that the SSDMM is now viable only for $M_S \\ge\n  1.6$ TeV. In this paper, we assume that the DM also couples to the $U_1$ via $\\lambda_{U_1 S} \\, S^2 \\, U_{1\\mu}^{\\dagger} U^{\\mu}_1$. In addition to leading to DM annihila"},"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":"2206.11305","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-06-22T18:16:16Z","cross_cats_sorted":[],"title_canon_sha256":"88fd6b81550b1b9f9caeedb2f26eb4f0812b0e8cec1edd7a481147554e3be831","abstract_canon_sha256":"9ac823c1fe30dd29ec6e4b9f1fb045015beb9271ae3d3c47c8eef91b4eb2b49c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:37:38.353552Z","signature_b64":"k+EzA5wLLsPM6ViMXwj2hnVJYHorFWxvS7BWhhdakkLjMs2Rc8N17zWbAdAXdDG/Jjq6Zeq04Ya6KCjalVpDAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"24ceb622b2e9795d8e64417fe659b1342adcecd3168593471eb19ec84f743fb1","last_reissued_at":"2026-07-05T05:37:38.353069Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:37:38.353069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The $B$ Anomalies, the $U_1$ Leptoquark and Dark Matter","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander Pukhov, David London, Genevi\\`eve B\\'elanger, Jacky Kumar","submitted_at":"2022-06-22T18:16:16Z","abstract_excerpt":"The present-day $B$-anomalies involving $b \\to s \\mu^+ \\mu^-$ or $b \\to c \\tau^- {\\bar\\nu}$ transitions can all be explained with the addition of a vector $U_1$ leptoquark with a mass of $M_{U_1} \\ge 1.8$ TeV. In the scalar singlet dark matter model (SSDMM), the DM is a scalar $S$ that couples to the Higgs via $\\lambda_{hS} \\, S^2|H|^2$. We update the fit to the data and find that the SSDMM is now viable only for $M_S \\ge\n  1.6$ TeV. In this paper, we assume that the DM also couples to the $U_1$ via $\\lambda_{U_1 S} \\, S^2 \\, U_{1\\mu}^{\\dagger} U^{\\mu}_1$. In addition to leading to DM annihila"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.11305","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/2206.11305/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":"2206.11305","created_at":"2026-07-05T05:37:38.353127+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.11305v1","created_at":"2026-07-05T05:37:38.353127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.11305","created_at":"2026-07-05T05:37:38.353127+00:00"},{"alias_kind":"pith_short_12","alias_value":"ETHLMIVS5F4V","created_at":"2026-07-05T05:37:38.353127+00:00"},{"alias_kind":"pith_short_16","alias_value":"ETHLMIVS5F4V3DTE","created_at":"2026-07-05T05:37:38.353127+00:00"},{"alias_kind":"pith_short_8","alias_value":"ETHLMIVS","created_at":"2026-07-05T05:37:38.353127+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/ETHLMIVS5F4V3DTEIF76MWNRGQ","json":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ.json","graph_json":"https://pith.science/api/pith-number/ETHLMIVS5F4V3DTEIF76MWNRGQ/graph.json","events_json":"https://pith.science/api/pith-number/ETHLMIVS5F4V3DTEIF76MWNRGQ/events.json","paper":"https://pith.science/paper/ETHLMIVS"},"agent_actions":{"view_html":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ","download_json":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ.json","view_paper":"https://pith.science/paper/ETHLMIVS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.11305&json=true","fetch_graph":"https://pith.science/api/pith-number/ETHLMIVS5F4V3DTEIF76MWNRGQ/graph.json","fetch_events":"https://pith.science/api/pith-number/ETHLMIVS5F4V3DTEIF76MWNRGQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ/action/storage_attestation","attest_author":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ/action/author_attestation","sign_citation":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ/action/citation_signature","submit_replication":"https://pith.science/pith/ETHLMIVS5F4V3DTEIF76MWNRGQ/action/replication_record"}},"created_at":"2026-07-05T05:37:38.353127+00:00","updated_at":"2026-07-05T05:37:38.353127+00:00"}