{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:NHHX3ZD3BZSBN3Q642LL3H7MIX","short_pith_number":"pith:NHHX3ZD3","schema_version":"1.0","canonical_sha256":"69cf7de47b0e6416ee1ee696bd9fec45d928bb55e92289132a4029a608a83835","source":{"kind":"arxiv","id":"1105.5193","version":2},"attestation_state":"computed","paper":{"title":"Charged bottomonium-like states $Z_b(10610)$ and $Z_b(10650)$ and the $\\Upsilon(5S)\\to \\Upsilon(2S)\\pi^+\\pi^-$ decay","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, Shi-Lin Zhu, Xiang Liu","submitted_at":"2011-05-26T02:57:25Z","abstract_excerpt":"Inspired by the newly observed two charged bottomonium-like states, we consider the possible contribution from the intermediate $Z_b(10610)$ and $Z_b(10650)$ states to the $\\Upsilon(5S)\\to \\Upsilon(2S)\\pi^+\\pi^-$ decay process, which naturally explains Belle's previous observation of the anomalous $\\Upsilon(2S)\\pi^+\\pi^-$ production near the peak of $\\Upsilon(5S)$ at $\\sqrt s=10.87$ GeV [K.F. Chen {\\it et al}. (Belle Collaboration), Phys. Rev. Lett. {\\bf 100}, 112001 (2008)]. The resulting $d\\Gamma(\\Upsilon(5S)\\to \\Upsilon(2S)\\pi^+\\pi^-)/dm_{\\pi^+\\pi^-}$ and $d\\Gamma(\\Upsilon(5S)\\to \\Upsilon(2"},"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":"1105.5193","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-05-26T02:57:25Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"973090f4baedbb95699a8fb05c0cdfbffa81239a621948845438cd52cee976a3","abstract_canon_sha256":"092d672c86d8b0c45a78516cc293ae4df056d7b892a7d6037e221c155456482c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:11:08.382160Z","signature_b64":"EeuPVekQ69Ne4Re90n93/Tlj8c9GReTW8fQjjs2Vie2mzcLys/PV4EF2yVD3fwnWpPrtnQ37CMTJlWDX3hZtAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"69cf7de47b0e6416ee1ee696bd9fec45d928bb55e92289132a4029a608a83835","last_reissued_at":"2026-05-18T04:11:08.381411Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:11:08.381411Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charged bottomonium-like states $Z_b(10610)$ and $Z_b(10650)$ and the $\\Upsilon(5S)\\to \\Upsilon(2S)\\pi^+\\pi^-$ decay","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, Shi-Lin Zhu, Xiang Liu","submitted_at":"2011-05-26T02:57:25Z","abstract_excerpt":"Inspired by the newly observed two charged bottomonium-like states, we consider the possible contribution from the intermediate $Z_b(10610)$ and $Z_b(10650)$ states to the $\\Upsilon(5S)\\to \\Upsilon(2S)\\pi^+\\pi^-$ decay process, which naturally explains Belle's previous observation of the anomalous $\\Upsilon(2S)\\pi^+\\pi^-$ production near the peak of $\\Upsilon(5S)$ at $\\sqrt s=10.87$ GeV [K.F. Chen {\\it et al}. (Belle Collaboration), Phys. Rev. Lett. {\\bf 100}, 112001 (2008)]. The resulting $d\\Gamma(\\Upsilon(5S)\\to \\Upsilon(2S)\\pi^+\\pi^-)/dm_{\\pi^+\\pi^-}$ and $d\\Gamma(\\Upsilon(5S)\\to \\Upsilon(2"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.5193","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":"1105.5193","created_at":"2026-05-18T04:11:08.381538+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.5193v2","created_at":"2026-05-18T04:11:08.381538+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.5193","created_at":"2026-05-18T04:11:08.381538+00:00"},{"alias_kind":"pith_short_12","alias_value":"NHHX3ZD3BZSB","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"NHHX3ZD3BZSBN3Q6","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"NHHX3ZD3","created_at":"2026-05-18T12:26:37.096874+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/NHHX3ZD3BZSBN3Q642LL3H7MIX","json":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX.json","graph_json":"https://pith.science/api/pith-number/NHHX3ZD3BZSBN3Q642LL3H7MIX/graph.json","events_json":"https://pith.science/api/pith-number/NHHX3ZD3BZSBN3Q642LL3H7MIX/events.json","paper":"https://pith.science/paper/NHHX3ZD3"},"agent_actions":{"view_html":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX","download_json":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX.json","view_paper":"https://pith.science/paper/NHHX3ZD3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.5193&json=true","fetch_graph":"https://pith.science/api/pith-number/NHHX3ZD3BZSBN3Q642LL3H7MIX/graph.json","fetch_events":"https://pith.science/api/pith-number/NHHX3ZD3BZSBN3Q642LL3H7MIX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX/action/storage_attestation","attest_author":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX/action/author_attestation","sign_citation":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX/action/citation_signature","submit_replication":"https://pith.science/pith/NHHX3ZD3BZSBN3Q642LL3H7MIX/action/replication_record"}},"created_at":"2026-05-18T04:11:08.381538+00:00","updated_at":"2026-05-18T04:11:08.381538+00:00"}