{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JBOQR47LJSSNUYAP4WNRWNUSY6","short_pith_number":"pith:JBOQR47L","schema_version":"1.0","canonical_sha256":"485d08f3eb4ca4da600fe59b1b3692c7afc2644d3bf2b04eea51e6ea5c877e57","source":{"kind":"arxiv","id":"1612.08867","version":2},"attestation_state":"computed","paper":{"title":"$B^0\\to K^{\\ast 0}\\mu^+\\mu^-$ Decay in the Aligned Two-Higgs-Doublet Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Quan-Yi Hu, Xin-Qiang Li, Ya-Dong Yang","submitted_at":"2016-12-28T12:23:25Z","abstract_excerpt":"In the aligned two-Higgs-doublet model, we perform a complete one-loop computation of the short-distance Wilson coefficients $C_{7,9,10}^{(\\prime)}$, which are the most relevant ones for $b\\to s\\ell^+\\ell^-$ transitions. It is found that, when the model parameter $\\left|\\varsigma_u\\right|$ is much smaller than $\\left|\\varsigma_d\\right|$, the charged-scalar contributes mainly to chirality-flipped $C_{9,10}^\\prime$, with the corresponding effects being proportional to $\\left|\\varsigma_d\\right|^2$. Numerically, the charged-scalar effects fit into two categories: (A) $C_{7,9,10}^\\mathrm{H^\\pm}$ ar"},"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":"1612.08867","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-28T12:23:25Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3f7863dd152b3d0583ff22b56f597d37363f18cb3b785ffc4deb7c11ecc7586b","abstract_canon_sha256":"d9b4ed883a2b1187a8e4de26bf3c4ba92fd04c258e323df08599ae9f0bfee058"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:43.529258Z","signature_b64":"ri7JUmfUbCzSPDZhPlTQ2boATceAPTsEao7C/FwkQF6EIDGeqlUbLlSlhVdbU6rLqW4kcuq7WiBIUxGq+igUBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"485d08f3eb4ca4da600fe59b1b3692c7afc2644d3bf2b04eea51e6ea5c877e57","last_reissued_at":"2026-05-18T00:45:43.528627Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:43.528627Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$B^0\\to K^{\\ast 0}\\mu^+\\mu^-$ Decay in the Aligned Two-Higgs-Doublet Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Quan-Yi Hu, Xin-Qiang Li, Ya-Dong Yang","submitted_at":"2016-12-28T12:23:25Z","abstract_excerpt":"In the aligned two-Higgs-doublet model, we perform a complete one-loop computation of the short-distance Wilson coefficients $C_{7,9,10}^{(\\prime)}$, which are the most relevant ones for $b\\to s\\ell^+\\ell^-$ transitions. It is found that, when the model parameter $\\left|\\varsigma_u\\right|$ is much smaller than $\\left|\\varsigma_d\\right|$, the charged-scalar contributes mainly to chirality-flipped $C_{9,10}^\\prime$, with the corresponding effects being proportional to $\\left|\\varsigma_d\\right|^2$. Numerically, the charged-scalar effects fit into two categories: (A) $C_{7,9,10}^\\mathrm{H^\\pm}$ ar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.08867","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":""},"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":"1612.08867","created_at":"2026-05-18T00:45:43.528728+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.08867v2","created_at":"2026-05-18T00:45:43.528728+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.08867","created_at":"2026-05-18T00:45:43.528728+00:00"},{"alias_kind":"pith_short_12","alias_value":"JBOQR47LJSSN","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_16","alias_value":"JBOQR47LJSSNUYAP","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_8","alias_value":"JBOQR47L","created_at":"2026-05-18T12:30:22.444734+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.26370","citing_title":"$\\Lambda_b\\to\\Lambda^{(*)}\\nu{\\bar\\nu}$ and $b\\to s$ $B$ decays","ref_index":51,"is_internal_anchor":true},{"citing_arxiv_id":"2605.08861","citing_title":"$B$ anomalies and the tauphilic leptoquark model","ref_index":60,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6","json":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6.json","graph_json":"https://pith.science/api/pith-number/JBOQR47LJSSNUYAP4WNRWNUSY6/graph.json","events_json":"https://pith.science/api/pith-number/JBOQR47LJSSNUYAP4WNRWNUSY6/events.json","paper":"https://pith.science/paper/JBOQR47L"},"agent_actions":{"view_html":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6","download_json":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6.json","view_paper":"https://pith.science/paper/JBOQR47L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.08867&json=true","fetch_graph":"https://pith.science/api/pith-number/JBOQR47LJSSNUYAP4WNRWNUSY6/graph.json","fetch_events":"https://pith.science/api/pith-number/JBOQR47LJSSNUYAP4WNRWNUSY6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6/action/storage_attestation","attest_author":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6/action/author_attestation","sign_citation":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6/action/citation_signature","submit_replication":"https://pith.science/pith/JBOQR47LJSSNUYAP4WNRWNUSY6/action/replication_record"}},"created_at":"2026-05-18T00:45:43.528728+00:00","updated_at":"2026-05-18T00:45:43.528728+00:00"}