{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:Y3AZ3CSEB6I6QLXQL3HRTWF5HT","short_pith_number":"pith:Y3AZ3CSE","schema_version":"1.0","canonical_sha256":"c6c19d8a440f91e82ef05ecf19d8bd3cfd8134277c6ab073d437848c428f9686","source":{"kind":"arxiv","id":"1703.03426","version":3},"attestation_state":"computed","paper":{"title":"Two Higgs Doublet Models and $b\\to s$ exclusive decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Damir Be\\v{c}irevi\\'c, Federico Mescia, Olcyr Sumensari, Pere Arnan","submitted_at":"2017-03-09T19:06:31Z","abstract_excerpt":"We computed the leading order Wilson coefficients relevant to all the exclusive $b\\to s\\ell^+\\ell^-$ decays in the framework of Two Higgs Doublet Model (2HDM) with a softly broken $\\mathbb{Z}_2$ symmetry by including the $\\mathcal{O}(m_b)$ corrections. We elucidate the issue of appropriate matching between the full and the effective theory when dealing with the (pseudo-)scalar operators for which keeping the external momenta different from zero is necessary. We then make a phenomenological analysis by using the measured $\\mathcal{B}(B_s\\to \\mu^+\\mu^-)$ and $\\mathcal{B}(B\\to K \\mu^+\\mu^-)_{\\mat"},"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":"1703.03426","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-03-09T19:06:31Z","cross_cats_sorted":[],"title_canon_sha256":"63d49d10e70ef81897aca6658437bdf88dff22a65b78a5e8e34e543c49f74eff","abstract_canon_sha256":"682d7a7d5b9982abdcc337f705e87f3d6c211eaed388c0852c17801f637e4b18"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:00.818652Z","signature_b64":"s/Un0QtjFGCzhHd6GYuW2f/Dd+ZeDnU5Ndn/ez38U6Rmb6FtpXQJGFLiKA3ex8F0F4Fw0DkCb7BypBnsVgT9DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c6c19d8a440f91e82ef05ecf19d8bd3cfd8134277c6ab073d437848c428f9686","last_reissued_at":"2026-05-18T00:26:00.817996Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:00.817996Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two Higgs Doublet Models and $b\\to s$ exclusive decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Damir Be\\v{c}irevi\\'c, Federico Mescia, Olcyr Sumensari, Pere Arnan","submitted_at":"2017-03-09T19:06:31Z","abstract_excerpt":"We computed the leading order Wilson coefficients relevant to all the exclusive $b\\to s\\ell^+\\ell^-$ decays in the framework of Two Higgs Doublet Model (2HDM) with a softly broken $\\mathbb{Z}_2$ symmetry by including the $\\mathcal{O}(m_b)$ corrections. We elucidate the issue of appropriate matching between the full and the effective theory when dealing with the (pseudo-)scalar operators for which keeping the external momenta different from zero is necessary. We then make a phenomenological analysis by using the measured $\\mathcal{B}(B_s\\to \\mu^+\\mu^-)$ and $\\mathcal{B}(B\\to K \\mu^+\\mu^-)_{\\mat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.03426","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":"1703.03426","created_at":"2026-05-18T00:26:00.818104+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.03426v3","created_at":"2026-05-18T00:26:00.818104+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.03426","created_at":"2026-05-18T00:26:00.818104+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y3AZ3CSEB6I6","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y3AZ3CSEB6I6QLXQ","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y3AZ3CSE","created_at":"2026-05-18T12:31:56.362134+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.14099","citing_title":"Electro-Weak Phase Transitions and Collider Signals in the Aligned 2-Higgs Doublet Model","ref_index":75,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT","json":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT.json","graph_json":"https://pith.science/api/pith-number/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/graph.json","events_json":"https://pith.science/api/pith-number/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/events.json","paper":"https://pith.science/paper/Y3AZ3CSE"},"agent_actions":{"view_html":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT","download_json":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT.json","view_paper":"https://pith.science/paper/Y3AZ3CSE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.03426&json=true","fetch_graph":"https://pith.science/api/pith-number/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/graph.json","fetch_events":"https://pith.science/api/pith-number/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/action/storage_attestation","attest_author":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/action/author_attestation","sign_citation":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/action/citation_signature","submit_replication":"https://pith.science/pith/Y3AZ3CSEB6I6QLXQL3HRTWF5HT/action/replication_record"}},"created_at":"2026-05-18T00:26:00.818104+00:00","updated_at":"2026-05-18T00:26:00.818104+00:00"}