{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:NHM45IOFBESRRRY7YHURSXPIY5","short_pith_number":"pith:NHM45IOF","schema_version":"1.0","canonical_sha256":"69d9cea1c5092518c71fc1e9195de8c76dddc9cba736c1fecaac18c9baae5c80","source":{"kind":"arxiv","id":"2201.07374","version":3},"attestation_state":"computed","paper":{"title":"Analysis of $B_s\\to\\phi\\nu\\bar{\\nu}$ at CEPC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Lingfeng Li, Manqi Ruan, Yudong Wang, Yuexin Wang","submitted_at":"2022-01-19T01:20:27Z","abstract_excerpt":"The rare $b\\to s\\nu\\bar{\\nu}$ decays are sensitive to contributions of new physics (NP) and helpful to resolve the puzzle of multiple $B$ flavor anomalies. In this work, we propose to study the $b\\to s\\nu\\bar{\\nu}$ transition at a future lepton collider operating at the $Z$ pole through the $B_s \\to \\phi\\nu\\bar{\\nu}$ decay. Using the $B_s\\to\\phi$ decay form factors from lattice simulations, we first update the SM prediction of BR($B_s \\to \\phi\\nu\\bar{\\nu})_{\\mathrm{SM}}=(9.93\\pm 0.72)\\times 10^{-6}$ and the corresponding $\\phi$ longitudinal polarization fraction $F_{L,{\\mathrm{SM}}}=0.53\\pm 0."},"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":"2201.07374","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-01-19T01:20:27Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4d68a4ee8fcbb92111abecc1f220c53c6c46df9d0adbf27636a22ae57364bd3d","abstract_canon_sha256":"2ad1c0ce6e42f3baaed2f5ba0e9c36654ab9a07db0eae00c7a3ebcecab9049ea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:44:42.024005Z","signature_b64":"5cM58Ad8X6QedNyR1TJBt9w4C5ltbuzfWStZBrb39yfAuD2FQkYl24Ptdta1yL2L8bihs1D5kuAS/6y9oC2eAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"69d9cea1c5092518c71fc1e9195de8c76dddc9cba736c1fecaac18c9baae5c80","last_reissued_at":"2026-07-05T04:44:42.023597Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:44:42.023597Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of $B_s\\to\\phi\\nu\\bar{\\nu}$ at CEPC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Lingfeng Li, Manqi Ruan, Yudong Wang, Yuexin Wang","submitted_at":"2022-01-19T01:20:27Z","abstract_excerpt":"The rare $b\\to s\\nu\\bar{\\nu}$ decays are sensitive to contributions of new physics (NP) and helpful to resolve the puzzle of multiple $B$ flavor anomalies. In this work, we propose to study the $b\\to s\\nu\\bar{\\nu}$ transition at a future lepton collider operating at the $Z$ pole through the $B_s \\to \\phi\\nu\\bar{\\nu}$ decay. Using the $B_s\\to\\phi$ decay form factors from lattice simulations, we first update the SM prediction of BR($B_s \\to \\phi\\nu\\bar{\\nu})_{\\mathrm{SM}}=(9.93\\pm 0.72)\\times 10^{-6}$ and the corresponding $\\phi$ longitudinal polarization fraction $F_{L,{\\mathrm{SM}}}=0.53\\pm 0."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2201.07374","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2201.07374/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":"2201.07374","created_at":"2026-07-05T04:44:42.023667+00:00"},{"alias_kind":"arxiv_version","alias_value":"2201.07374v3","created_at":"2026-07-05T04:44:42.023667+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2201.07374","created_at":"2026-07-05T04:44:42.023667+00:00"},{"alias_kind":"pith_short_12","alias_value":"NHM45IOFBESR","created_at":"2026-07-05T04:44:42.023667+00:00"},{"alias_kind":"pith_short_16","alias_value":"NHM45IOFBESRRRY7","created_at":"2026-07-05T04:44:42.023667+00:00"},{"alias_kind":"pith_short_8","alias_value":"NHM45IOF","created_at":"2026-07-05T04:44:42.023667+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.08089","citing_title":"Time-Dependent Precision Measurement of $B_s^0\\rightarrow \\phi \\mu^+\\mu^-$ Decay at FCC-$ee$","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5","json":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5.json","graph_json":"https://pith.science/api/pith-number/NHM45IOFBESRRRY7YHURSXPIY5/graph.json","events_json":"https://pith.science/api/pith-number/NHM45IOFBESRRRY7YHURSXPIY5/events.json","paper":"https://pith.science/paper/NHM45IOF"},"agent_actions":{"view_html":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5","download_json":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5.json","view_paper":"https://pith.science/paper/NHM45IOF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2201.07374&json=true","fetch_graph":"https://pith.science/api/pith-number/NHM45IOFBESRRRY7YHURSXPIY5/graph.json","fetch_events":"https://pith.science/api/pith-number/NHM45IOFBESRRRY7YHURSXPIY5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5/action/storage_attestation","attest_author":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5/action/author_attestation","sign_citation":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5/action/citation_signature","submit_replication":"https://pith.science/pith/NHM45IOFBESRRRY7YHURSXPIY5/action/replication_record"}},"created_at":"2026-07-05T04:44:42.023667+00:00","updated_at":"2026-07-05T04:44:42.023667+00:00"}