{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:NWRMGHHMNYXZQHZFIGLC3JY4DB","short_pith_number":"pith:NWRMGHHM","schema_version":"1.0","canonical_sha256":"6da2c31cec6e2f981f2541962da71c18653eb4bcf712034c327e0934078a2c42","source":{"kind":"arxiv","id":"1110.0375","version":3},"attestation_state":"computed","paper":{"title":"$J/\\psi \\rightarrow p\\bar{p}\\phi$ decay in the isobar resonance model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Bing-Song Zou, Jian-Ping Dai, Ju-Jun Xie, Peng-Nian Shen","submitted_at":"2011-10-03T15:09:59Z","abstract_excerpt":"Based on the effective Lagrangian approach, the $ J/\\psi \\to p \\bar{p} \\phi$ decay is studied in an isobar resonance model with the assumption that the $\\phi$-meson is produced from intermediate nucleon resonances. The contributions from the $N^*_{1/2^-}(1535)$, $N^*_{3/2^+}(1900)$, $N^*_{1/2^-}(2090)$ and $N^*_{1/2^+}(2100)$ states are considered. In terms of the coupling constants $g^{2}_{\\phi N N^{*}}$ and $g^{2}_{\\phi N N^{*}}$ extracted from the data of the partial decay widths of the $N^*$s to the $N\\pi$ channel, the reaction cross section of the $\\pi^{-}p\\rightarrow n\\phi$ process and t"},"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":"1110.0375","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-10-03T15:09:59Z","cross_cats_sorted":[],"title_canon_sha256":"55ac21da2f1005a2ef03390b1285f5ae30a1e9ed93802bdc676f83daffede5b5","abstract_canon_sha256":"8744fcbf5cc2b6fa4dab1cd06201224049ab0fbd958ae7ca4651c8a6ef401f4f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:13.275025Z","signature_b64":"0SICF5YDNzXITALEb6BU0nKvLvf4p5XHfj1iqPhhYlT2SI8bKwBbtvz5zfLFeud3ybEuhOsT9htnrn7+XuF9Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6da2c31cec6e2f981f2541962da71c18653eb4bcf712034c327e0934078a2c42","last_reissued_at":"2026-05-18T03:23:13.274569Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:13.274569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$J/\\psi \\rightarrow p\\bar{p}\\phi$ decay in the isobar resonance model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Bing-Song Zou, Jian-Ping Dai, Ju-Jun Xie, Peng-Nian Shen","submitted_at":"2011-10-03T15:09:59Z","abstract_excerpt":"Based on the effective Lagrangian approach, the $ J/\\psi \\to p \\bar{p} \\phi$ decay is studied in an isobar resonance model with the assumption that the $\\phi$-meson is produced from intermediate nucleon resonances. The contributions from the $N^*_{1/2^-}(1535)$, $N^*_{3/2^+}(1900)$, $N^*_{1/2^-}(2090)$ and $N^*_{1/2^+}(2100)$ states are considered. In terms of the coupling constants $g^{2}_{\\phi N N^{*}}$ and $g^{2}_{\\phi N N^{*}}$ extracted from the data of the partial decay widths of the $N^*$s to the $N\\pi$ channel, the reaction cross section of the $\\pi^{-}p\\rightarrow n\\phi$ process and t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.0375","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":"1110.0375","created_at":"2026-05-18T03:23:13.274631+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.0375v3","created_at":"2026-05-18T03:23:13.274631+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.0375","created_at":"2026-05-18T03:23:13.274631+00:00"},{"alias_kind":"pith_short_12","alias_value":"NWRMGHHMNYXZ","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"NWRMGHHMNYXZQHZF","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"NWRMGHHM","created_at":"2026-05-18T12:26:37.096874+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.11873","citing_title":"Maximizing Reachability via Shifting of Temporal Paths","ref_index":268,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB","json":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB.json","graph_json":"https://pith.science/api/pith-number/NWRMGHHMNYXZQHZFIGLC3JY4DB/graph.json","events_json":"https://pith.science/api/pith-number/NWRMGHHMNYXZQHZFIGLC3JY4DB/events.json","paper":"https://pith.science/paper/NWRMGHHM"},"agent_actions":{"view_html":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB","download_json":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB.json","view_paper":"https://pith.science/paper/NWRMGHHM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.0375&json=true","fetch_graph":"https://pith.science/api/pith-number/NWRMGHHMNYXZQHZFIGLC3JY4DB/graph.json","fetch_events":"https://pith.science/api/pith-number/NWRMGHHMNYXZQHZFIGLC3JY4DB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB/action/storage_attestation","attest_author":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB/action/author_attestation","sign_citation":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB/action/citation_signature","submit_replication":"https://pith.science/pith/NWRMGHHMNYXZQHZFIGLC3JY4DB/action/replication_record"}},"created_at":"2026-05-18T03:23:13.274631+00:00","updated_at":"2026-05-18T03:23:13.274631+00:00"}