{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:XLX73YLWEYX7ZAL6PY5THUUFGV","short_pith_number":"pith:XLX73YLW","schema_version":"1.0","canonical_sha256":"baeffde176262ffc817e7e3b33d285357d59b2b6cd69a1f5e8403a42ecc1d4f4","source":{"kind":"arxiv","id":"0910.4291","version":3},"attestation_state":"computed","paper":{"title":"Invisible Higgs decay with B\\to K\\nu\\bar{\\nu} constraint","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C.S. Kim, Guohuai Zhu, Kai Wang, Seong Chan Park","submitted_at":"2009-10-22T11:06:47Z","abstract_excerpt":"If the Higgs boson were the only particle within the LHC accessible range, precision measurement of the Higgs's properties would play a unique role in studying electroweak symmetry breaking as well as possible new physics. We try to use low energy experiments such as rare B decay to constrain a challenging decay mode of Higgs, in which a Higgs decays to a pair of light (\\approx 1 \\sim 2 GeV) SM singlet S and becomes invisible. By using the current experimental bound of rare decay B\\to K\\nu\\bar{\\nu} and computing the contribution of B\\to K SS to (the) B\\to K+\\cancel{E}, we obtain an upper bound"},"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":"0910.4291","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-10-22T11:06:47Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"928ef2703783787174397eff689682c67540cd2d37a2d2a8de635ec4cc087515","abstract_canon_sha256":"8288894e59eba9e679cdc044006d4f5ad8edd3a4f0d82bcb22e4be655c4a63d7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:13.135344Z","signature_b64":"M7h8A45jcQCU2DxipO8xmZW13/hjQ2HLx+x33xIN4eQ59MwbMYA3Ja76L0x1Q42/SgFyMWwcYs0q+/E6+0dNCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"baeffde176262ffc817e7e3b33d285357d59b2b6cd69a1f5e8403a42ecc1d4f4","last_reissued_at":"2026-05-18T02:34:13.134899Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:13.134899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Invisible Higgs decay with B\\to K\\nu\\bar{\\nu} constraint","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C.S. Kim, Guohuai Zhu, Kai Wang, Seong Chan Park","submitted_at":"2009-10-22T11:06:47Z","abstract_excerpt":"If the Higgs boson were the only particle within the LHC accessible range, precision measurement of the Higgs's properties would play a unique role in studying electroweak symmetry breaking as well as possible new physics. We try to use low energy experiments such as rare B decay to constrain a challenging decay mode of Higgs, in which a Higgs decays to a pair of light (\\approx 1 \\sim 2 GeV) SM singlet S and becomes invisible. By using the current experimental bound of rare decay B\\to K\\nu\\bar{\\nu} and computing the contribution of B\\to K SS to (the) B\\to K+\\cancel{E}, we obtain an upper bound"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0910.4291","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":"0910.4291","created_at":"2026-05-18T02:34:13.134963+00:00"},{"alias_kind":"arxiv_version","alias_value":"0910.4291v3","created_at":"2026-05-18T02:34:13.134963+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0910.4291","created_at":"2026-05-18T02:34:13.134963+00:00"},{"alias_kind":"pith_short_12","alias_value":"XLX73YLWEYX7","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_16","alias_value":"XLX73YLWEYX7ZAL6","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_8","alias_value":"XLX73YLW","created_at":"2026-05-18T12:26:02.257875+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV","json":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV.json","graph_json":"https://pith.science/api/pith-number/XLX73YLWEYX7ZAL6PY5THUUFGV/graph.json","events_json":"https://pith.science/api/pith-number/XLX73YLWEYX7ZAL6PY5THUUFGV/events.json","paper":"https://pith.science/paper/XLX73YLW"},"agent_actions":{"view_html":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV","download_json":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV.json","view_paper":"https://pith.science/paper/XLX73YLW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0910.4291&json=true","fetch_graph":"https://pith.science/api/pith-number/XLX73YLWEYX7ZAL6PY5THUUFGV/graph.json","fetch_events":"https://pith.science/api/pith-number/XLX73YLWEYX7ZAL6PY5THUUFGV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV/action/storage_attestation","attest_author":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV/action/author_attestation","sign_citation":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV/action/citation_signature","submit_replication":"https://pith.science/pith/XLX73YLWEYX7ZAL6PY5THUUFGV/action/replication_record"}},"created_at":"2026-05-18T02:34:13.134963+00:00","updated_at":"2026-05-18T02:34:13.134963+00:00"}