{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:KRSO62IAHAHCKFXZYSM7HRV7DH","short_pith_number":"pith:KRSO62IA","schema_version":"1.0","canonical_sha256":"5464ef6900380e2516f9c499f3c6bf19e017f3c11237d7038c2d5f9fb2d114af","source":{"kind":"arxiv","id":"1609.09078","version":3},"attestation_state":"computed","paper":{"title":"Simultaneous Explanation of the $R_K$ and $R_{D^{(*)}}$ Puzzles: a Model Analysis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alakabha Datta, Bhubanjyoti Bhattacharya, David London, Jean-Pascal Gu\\'evin, Ryoutaro Watanabe","submitted_at":"2016-09-28T20:00:02Z","abstract_excerpt":"$R_K$ and $R_{D^{(*)}}$ are two $B$-decay measurements that presently exhibit discrepancies with the SM. Recently, using an effective field theory approach, it was demonstrated that a new-physics model can simultaneously explain both the $R_K$ and $R_{D^{(*)}}$ puzzles. There are two UV completions that can give rise to the effective Lagrangian: (i) $VB$: a vector boson that transforms as an $SU(2)_L$ triplet, as in the SM, (ii) $U_1$: an $SU(2)_L$-singlet vector leptoquark. In this paper, we examine these models individually. A key point is that $VB$ contributes to $B^0_s$-${\\bar B}^0_s$ mixi"},"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":"1609.09078","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-09-28T20:00:02Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"cf7249a29412308280898c1de2fef2fbbc31a44850281d305dcd6edb295861d9","abstract_canon_sha256":"df05c0f588c1933074d2238dfaf1cf25f525c6c37963ee5e32fe8db34c41be8a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:15.487095Z","signature_b64":"i15nz1osH+D6PuCOaBsI9KDBSD3VE80+k+Mrsj6QG1Eptc30QZ4XIlC+gvVlhbevFHfNkeuV9gqqUnXAfMrQBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5464ef6900380e2516f9c499f3c6bf19e017f3c11237d7038c2d5f9fb2d114af","last_reissued_at":"2026-05-18T00:53:15.486671Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:15.486671Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simultaneous Explanation of the $R_K$ and $R_{D^{(*)}}$ Puzzles: a Model Analysis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alakabha Datta, Bhubanjyoti Bhattacharya, David London, Jean-Pascal Gu\\'evin, Ryoutaro Watanabe","submitted_at":"2016-09-28T20:00:02Z","abstract_excerpt":"$R_K$ and $R_{D^{(*)}}$ are two $B$-decay measurements that presently exhibit discrepancies with the SM. Recently, using an effective field theory approach, it was demonstrated that a new-physics model can simultaneously explain both the $R_K$ and $R_{D^{(*)}}$ puzzles. There are two UV completions that can give rise to the effective Lagrangian: (i) $VB$: a vector boson that transforms as an $SU(2)_L$ triplet, as in the SM, (ii) $U_1$: an $SU(2)_L$-singlet vector leptoquark. In this paper, we examine these models individually. A key point is that $VB$ contributes to $B^0_s$-${\\bar B}^0_s$ mixi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.09078","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1609.09078","created_at":"2026-05-18T00:53:15.486747+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.09078v3","created_at":"2026-05-18T00:53:15.486747+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.09078","created_at":"2026-05-18T00:53:15.486747+00:00"},{"alias_kind":"pith_short_12","alias_value":"KRSO62IAHAHC","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_16","alias_value":"KRSO62IAHAHCKFXZ","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_8","alias_value":"KRSO62IA","created_at":"2026-05-18T12:30:29.479603+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.09414","citing_title":"New physics searches via angular distributions of $ \\bar{B} \\to D^* (\\to D \\pi) \\tau (\\to \\ell \\nu_\\tau \\bar{\\nu}_\\ell) \\bar{\\nu}_\\tau$ decays","ref_index":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH","json":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH.json","graph_json":"https://pith.science/api/pith-number/KRSO62IAHAHCKFXZYSM7HRV7DH/graph.json","events_json":"https://pith.science/api/pith-number/KRSO62IAHAHCKFXZYSM7HRV7DH/events.json","paper":"https://pith.science/paper/KRSO62IA"},"agent_actions":{"view_html":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH","download_json":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH.json","view_paper":"https://pith.science/paper/KRSO62IA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.09078&json=true","fetch_graph":"https://pith.science/api/pith-number/KRSO62IAHAHCKFXZYSM7HRV7DH/graph.json","fetch_events":"https://pith.science/api/pith-number/KRSO62IAHAHCKFXZYSM7HRV7DH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH/action/storage_attestation","attest_author":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH/action/author_attestation","sign_citation":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH/action/citation_signature","submit_replication":"https://pith.science/pith/KRSO62IAHAHCKFXZYSM7HRV7DH/action/replication_record"}},"created_at":"2026-05-18T00:53:15.486747+00:00","updated_at":"2026-05-18T00:53:15.486747+00:00"}