{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:XZV55EP6SCFIYHSHUNASB74EAU","short_pith_number":"pith:XZV55EP6","schema_version":"1.0","canonical_sha256":"be6bde91fe908a8c1e47a34120ff8405183a60d44d9231e2d3c0803d0c02cb72","source":{"kind":"arxiv","id":"2311.16920","version":1},"attestation_state":"computed","paper":{"title":"$\\Xi(1620)$ production in $K^- p$ scattering process","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, Quan-Yun Guo, Zi-Li Yue","submitted_at":"2023-11-28T16:24:57Z","abstract_excerpt":"In the present work, the production of $\\Xi(1620)$ in the $K^- p$ scattering process is investigated by using an effective Lagrangian approach, where $\\Xi(1620)$ is considered as a $\\bar{K} \\Lambda$ molecular state. Our estimations indicate that the cross sections for $K^-p\\to K^+ \\Xi(1620)^-$ are $(1.48 ^{+ 1.12}_{-0.69}) \\ \\mathrm{\\mu b}$ at $P_K=2.8 \\ \\mathrm{GeV}$, where the uncertainties are resulted from the variation of the model parameter. As for the $K^-p\\to K^+ \\pi^0 \\Xi^-$ process, the cross sections are estimated to be $(0.61 ^{+0.47}_{-0.29})\\ \\mathrm{\\mu b}$ at $P_K =2.8 \\ \\mathr"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2311.16920","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-11-28T16:24:57Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"d6a2f7153298b32763c1a0a1e400e1efaf10df0b281cbe7a1d8329fd8e3e6b85","abstract_canon_sha256":"48c07336058d1232131123f72441db2c8edbfa1082a90e8c97fa4cc41f74c941"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:17:48.312542Z","signature_b64":"gGYjNheB/uz3hPrgX34txb52J7zR4jTLuacQhUpW/31o7zDWZcO1h1FYnrEVbaA9zj7ysZUbxx0yaLRiT+61Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be6bde91fe908a8c1e47a34120ff8405183a60d44d9231e2d3c0803d0c02cb72","last_reissued_at":"2026-07-05T07:17:48.312052Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:17:48.312052Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\Xi(1620)$ production in $K^- p$ scattering process","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, Quan-Yun Guo, Zi-Li Yue","submitted_at":"2023-11-28T16:24:57Z","abstract_excerpt":"In the present work, the production of $\\Xi(1620)$ in the $K^- p$ scattering process is investigated by using an effective Lagrangian approach, where $\\Xi(1620)$ is considered as a $\\bar{K} \\Lambda$ molecular state. Our estimations indicate that the cross sections for $K^-p\\to K^+ \\Xi(1620)^-$ are $(1.48 ^{+ 1.12}_{-0.69}) \\ \\mathrm{\\mu b}$ at $P_K=2.8 \\ \\mathrm{GeV}$, where the uncertainties are resulted from the variation of the model parameter. As for the $K^-p\\to K^+ \\pi^0 \\Xi^-$ process, the cross sections are estimated to be $(0.61 ^{+0.47}_{-0.29})\\ \\mathrm{\\mu b}$ at $P_K =2.8 \\ \\mathr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.16920","kind":"arxiv","version":1},"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/2311.16920/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":"2311.16920","created_at":"2026-07-05T07:17:48.312104+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.16920v1","created_at":"2026-07-05T07:17:48.312104+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.16920","created_at":"2026-07-05T07:17:48.312104+00:00"},{"alias_kind":"pith_short_12","alias_value":"XZV55EP6SCFI","created_at":"2026-07-05T07:17:48.312104+00:00"},{"alias_kind":"pith_short_16","alias_value":"XZV55EP6SCFIYHSH","created_at":"2026-07-05T07:17:48.312104+00:00"},{"alias_kind":"pith_short_8","alias_value":"XZV55EP6","created_at":"2026-07-05T07:17:48.312104+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/XZV55EP6SCFIYHSHUNASB74EAU","json":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU.json","graph_json":"https://pith.science/api/pith-number/XZV55EP6SCFIYHSHUNASB74EAU/graph.json","events_json":"https://pith.science/api/pith-number/XZV55EP6SCFIYHSHUNASB74EAU/events.json","paper":"https://pith.science/paper/XZV55EP6"},"agent_actions":{"view_html":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU","download_json":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU.json","view_paper":"https://pith.science/paper/XZV55EP6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.16920&json=true","fetch_graph":"https://pith.science/api/pith-number/XZV55EP6SCFIYHSHUNASB74EAU/graph.json","fetch_events":"https://pith.science/api/pith-number/XZV55EP6SCFIYHSHUNASB74EAU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU/action/storage_attestation","attest_author":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU/action/author_attestation","sign_citation":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU/action/citation_signature","submit_replication":"https://pith.science/pith/XZV55EP6SCFIYHSHUNASB74EAU/action/replication_record"}},"created_at":"2026-07-05T07:17:48.312104+00:00","updated_at":"2026-07-05T07:17:48.312104+00:00"}