{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:NSLVQZUPIMSMSMR4OMPCH5M3YX","short_pith_number":"pith:NSLVQZUP","schema_version":"1.0","canonical_sha256":"6c9758668f4324c9323c731e23f59bc5e2084db76e36699d0c34e25d412baf82","source":{"kind":"arxiv","id":"2103.12504","version":2},"attestation_state":"computed","paper":{"title":"On the single leptoquark solutions to the $B$-physics anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Andrei Angelescu, Damir Be\\v{c}irevi\\'c, Darius A. Faroughy, Florentin Jaffredo, Olcyr Sumensari","submitted_at":"2021-03-23T13:06:33Z","abstract_excerpt":"We revisit the possibilities of accommodating the experimental indications of the lepton flavor universality violation in $b$-hadron decays in the minimal scenarios in which the Standard Model is extended by the presence of a single $\\mathcal{O}(1\\,\\mathrm{TeV})$ leptoquark state. To do so we combine the most recent low energy flavor physics constraints, including $R_{K^{(\\ast)}}^\\mathrm{exp}$ and $R_{D^{(\\ast)}}^\\mathrm{exp}$, and combine them with the bounds on the leptoquark masses and their couplings to quarks and leptons as inferred from the direct searches at the LHC and the studies of t"},"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":"2103.12504","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-03-23T13:06:33Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"6d46faa0b9bf4a97a9eafe8636f3192c7c8cad4beb01131ca5a8bfff5007b2ef","abstract_canon_sha256":"b59ac348ece99fda07ca8f01157b75096d9ca4222dd6ba618ad6005cb707313e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:16:11.249461Z","signature_b64":"lKB0v0BXx+HurC+MP1vj9hT9gUFiRuu5SBkt+jegeBuTBRVofLuPT0jARtIn130OWvTJ9NUb9h0MFLKNQDpZAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6c9758668f4324c9323c731e23f59bc5e2084db76e36699d0c34e25d412baf82","last_reissued_at":"2026-07-05T03:16:11.248963Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:16:11.248963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the single leptoquark solutions to the $B$-physics anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Andrei Angelescu, Damir Be\\v{c}irevi\\'c, Darius A. Faroughy, Florentin Jaffredo, Olcyr Sumensari","submitted_at":"2021-03-23T13:06:33Z","abstract_excerpt":"We revisit the possibilities of accommodating the experimental indications of the lepton flavor universality violation in $b$-hadron decays in the minimal scenarios in which the Standard Model is extended by the presence of a single $\\mathcal{O}(1\\,\\mathrm{TeV})$ leptoquark state. To do so we combine the most recent low energy flavor physics constraints, including $R_{K^{(\\ast)}}^\\mathrm{exp}$ and $R_{D^{(\\ast)}}^\\mathrm{exp}$, and combine them with the bounds on the leptoquark masses and their couplings to quarks and leptons as inferred from the direct searches at the LHC and the studies of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.12504","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/2103.12504/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":"2103.12504","created_at":"2026-07-05T03:16:11.249024+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.12504v2","created_at":"2026-07-05T03:16:11.249024+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.12504","created_at":"2026-07-05T03:16:11.249024+00:00"},{"alias_kind":"pith_short_12","alias_value":"NSLVQZUPIMSM","created_at":"2026-07-05T03:16:11.249024+00:00"},{"alias_kind":"pith_short_16","alias_value":"NSLVQZUPIMSMSMR4","created_at":"2026-07-05T03:16:11.249024+00:00"},{"alias_kind":"pith_short_8","alias_value":"NSLVQZUP","created_at":"2026-07-05T03:16:11.249024+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21642","citing_title":"Probing Light Dark Fermions in $B \\to D^{(*)}\\ell X_{\\rm inv}$ via Rate Distributions","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02067","citing_title":"Search for a leptoquark in events with a hadronically decaying $\\tau$-lepton and missing transverse momentum using $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2509.26370","citing_title":"$\\Lambda_b\\to\\Lambda^{(*)}\\nu{\\bar\\nu}$ and $b\\to s$ $B$ decays","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2605.08861","citing_title":"$B$ anomalies and the tauphilic leptoquark model","ref_index":80,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX","json":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX.json","graph_json":"https://pith.science/api/pith-number/NSLVQZUPIMSMSMR4OMPCH5M3YX/graph.json","events_json":"https://pith.science/api/pith-number/NSLVQZUPIMSMSMR4OMPCH5M3YX/events.json","paper":"https://pith.science/paper/NSLVQZUP"},"agent_actions":{"view_html":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX","download_json":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX.json","view_paper":"https://pith.science/paper/NSLVQZUP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.12504&json=true","fetch_graph":"https://pith.science/api/pith-number/NSLVQZUPIMSMSMR4OMPCH5M3YX/graph.json","fetch_events":"https://pith.science/api/pith-number/NSLVQZUPIMSMSMR4OMPCH5M3YX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX/action/storage_attestation","attest_author":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX/action/author_attestation","sign_citation":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX/action/citation_signature","submit_replication":"https://pith.science/pith/NSLVQZUPIMSMSMR4OMPCH5M3YX/action/replication_record"}},"created_at":"2026-07-05T03:16:11.249024+00:00","updated_at":"2026-07-05T03:16:11.249024+00:00"}