{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:3HPFV732UXBMLYAKFJ7453Q33W","short_pith_number":"pith:3HPFV732","schema_version":"1.0","canonical_sha256":"d9de5aff7aa5c2c5e00a2a7fceee1bdd9f90ffa3f80d8fc9c698b828e9103735","source":{"kind":"arxiv","id":"1803.07795","version":2},"attestation_state":"computed","paper":{"title":"Phenomenological study on the decay widths of $\\Upsilon(nS)\\rightarrow \\bar{d}^{\\ast}(2380)+X$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Chao-Yi L\\\"u, D. M. Li, P. N. Shen, P. Wang, Y. B. Dong, Z. Y. Zhang","submitted_at":"2018-03-21T08:33:56Z","abstract_excerpt":"The decay widths of $\\Upsilon(nS)$ $\\rightarrow$ $\\bar{d}^{\\ast}(2380)+X$ with $n=1,2,3$ are studied in a phenomenological way. With the help of crossing symmetry, the decay widths are obtained by investigating the imaginary part of the forward scattering amplitudes between $d^\\ast$ and $\\Upsilon(nS)$. The wave functions of $d^\\ast$ and deuteron obtained in previous studies are used for calculating the amplitude. The interaction between $d^{\\ast}$ ($d$) and $\\Upsilon$ is governed by the quark-meson interaction where the coupling constant is determined by fitting the observed widths of $\\Upsilo"},"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":"1803.07795","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-21T08:33:56Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"e74b259eb58abdcc8e88a94008e5bd313873c3f48f543261bf65bfa6d3215f08","abstract_canon_sha256":"58673aace28912196af9a335f56fe20cd66369e241a81ffe6edec0a947735958"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:51.711983Z","signature_b64":"RmTMbCwZoarmMVe+ZTB46usuD+x1XQusdZqgcGa0HjKf9gqvLbVc0YC8INvVoFCGmNO6yzGQfGxmKD3jDIg4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9de5aff7aa5c2c5e00a2a7fceee1bdd9f90ffa3f80d8fc9c698b828e9103735","last_reissued_at":"2026-05-18T00:15:51.711384Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:51.711384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenological study on the decay widths of $\\Upsilon(nS)\\rightarrow \\bar{d}^{\\ast}(2380)+X$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Chao-Yi L\\\"u, D. M. Li, P. N. Shen, P. Wang, Y. B. Dong, Z. Y. Zhang","submitted_at":"2018-03-21T08:33:56Z","abstract_excerpt":"The decay widths of $\\Upsilon(nS)$ $\\rightarrow$ $\\bar{d}^{\\ast}(2380)+X$ with $n=1,2,3$ are studied in a phenomenological way. With the help of crossing symmetry, the decay widths are obtained by investigating the imaginary part of the forward scattering amplitudes between $d^\\ast$ and $\\Upsilon(nS)$. The wave functions of $d^\\ast$ and deuteron obtained in previous studies are used for calculating the amplitude. The interaction between $d^{\\ast}$ ($d$) and $\\Upsilon$ is governed by the quark-meson interaction where the coupling constant is determined by fitting the observed widths of $\\Upsilo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.07795","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":"1803.07795","created_at":"2026-05-18T00:15:51.711492+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.07795v2","created_at":"2026-05-18T00:15:51.711492+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.07795","created_at":"2026-05-18T00:15:51.711492+00:00"},{"alias_kind":"pith_short_12","alias_value":"3HPFV732UXBM","created_at":"2026-05-18T12:32:02.567920+00:00"},{"alias_kind":"pith_short_16","alias_value":"3HPFV732UXBMLYAK","created_at":"2026-05-18T12:32:02.567920+00:00"},{"alias_kind":"pith_short_8","alias_value":"3HPFV732","created_at":"2026-05-18T12:32:02.567920+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/3HPFV732UXBMLYAKFJ7453Q33W","json":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W.json","graph_json":"https://pith.science/api/pith-number/3HPFV732UXBMLYAKFJ7453Q33W/graph.json","events_json":"https://pith.science/api/pith-number/3HPFV732UXBMLYAKFJ7453Q33W/events.json","paper":"https://pith.science/paper/3HPFV732"},"agent_actions":{"view_html":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W","download_json":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W.json","view_paper":"https://pith.science/paper/3HPFV732","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.07795&json=true","fetch_graph":"https://pith.science/api/pith-number/3HPFV732UXBMLYAKFJ7453Q33W/graph.json","fetch_events":"https://pith.science/api/pith-number/3HPFV732UXBMLYAKFJ7453Q33W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W/action/storage_attestation","attest_author":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W/action/author_attestation","sign_citation":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W/action/citation_signature","submit_replication":"https://pith.science/pith/3HPFV732UXBMLYAKFJ7453Q33W/action/replication_record"}},"created_at":"2026-05-18T00:15:51.711492+00:00","updated_at":"2026-05-18T00:15:51.711492+00:00"}