{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:QZVN7SPGPZDVCZGFAYA56UXT5P","short_pith_number":"pith:QZVN7SPG","schema_version":"1.0","canonical_sha256":"866adfc9e67e475164c50601df52f3ebca79bb2d2a346804e09166b8d94e32f5","source":{"kind":"arxiv","id":"2606.29413","version":1},"attestation_state":"computed","paper":{"title":"Exploring $K\\Xi^*$ and $K^*\\Xi$ molecular states and the triangle singularity in the $K^- p \\to K \\Xi(1530)$ reaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bing-Song Zou, Fei Huang, Ke Wang","submitted_at":"2026-06-28T14:23:39Z","abstract_excerpt":"We investigate the $K^- p \\to K \\Xi(1530)$ reaction within an effective Lagrangian approach, exploring possible $K \\Xi^*$ and $K^* \\Xi$ hadronic molecular states and the role of the triangle singularity (TS). The $\\Lambda(2050)3/2^-$ is interpreted as a $K \\Xi^*$ molecule, whereas a $K^* \\Xi$ molecule with $I(J^P)=0(3/2^-)$ and mass about 2150~MeV denoted as $\\Lambda(2150)$ can generate a TS through triangle-loop diagrams with intermediate $K^*$, $\\Xi$, and $\\pi$. The peak structure observed in the cross section near $\\sqrt{s}=2.25$ GeV is analyzed in terms of both the $\\Sigma(2250)$ resonance"},"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":"2606.29413","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-06-28T14:23:39Z","cross_cats_sorted":[],"title_canon_sha256":"d590d993ecb380d675d0e16707912a6de17c613501b476610339eda9ddfd7c04","abstract_canon_sha256":"8801b252ec043fcfdd0688944e439f7984aff3fc90ff80c3400b8549a62e1198"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-30T01:18:05.282624Z","signature_b64":"q1uefrS95LVUh8fBQQDJPNnfsuYedAe+FTxBnUxR/z7J/Byt+nBqx1WY59VODOTzxjHQdawg/5p0rnVMNAerCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"866adfc9e67e475164c50601df52f3ebca79bb2d2a346804e09166b8d94e32f5","last_reissued_at":"2026-06-30T01:18:05.282036Z","signature_status":"signed_v1","first_computed_at":"2026-06-30T01:18:05.282036Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring $K\\Xi^*$ and $K^*\\Xi$ molecular states and the triangle singularity in the $K^- p \\to K \\Xi(1530)$ reaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bing-Song Zou, Fei Huang, Ke Wang","submitted_at":"2026-06-28T14:23:39Z","abstract_excerpt":"We investigate the $K^- p \\to K \\Xi(1530)$ reaction within an effective Lagrangian approach, exploring possible $K \\Xi^*$ and $K^* \\Xi$ hadronic molecular states and the role of the triangle singularity (TS). The $\\Lambda(2050)3/2^-$ is interpreted as a $K \\Xi^*$ molecule, whereas a $K^* \\Xi$ molecule with $I(J^P)=0(3/2^-)$ and mass about 2150~MeV denoted as $\\Lambda(2150)$ can generate a TS through triangle-loop diagrams with intermediate $K^*$, $\\Xi$, and $\\pi$. The peak structure observed in the cross section near $\\sqrt{s}=2.25$ GeV is analyzed in terms of both the $\\Sigma(2250)$ resonance"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.29413","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/2606.29413/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":"2606.29413","created_at":"2026-06-30T01:18:05.282119+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.29413v1","created_at":"2026-06-30T01:18:05.282119+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.29413","created_at":"2026-06-30T01:18:05.282119+00:00"},{"alias_kind":"pith_short_12","alias_value":"QZVN7SPGPZDV","created_at":"2026-06-30T01:18:05.282119+00:00"},{"alias_kind":"pith_short_16","alias_value":"QZVN7SPGPZDVCZGF","created_at":"2026-06-30T01:18:05.282119+00:00"},{"alias_kind":"pith_short_8","alias_value":"QZVN7SPG","created_at":"2026-06-30T01:18:05.282119+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/QZVN7SPGPZDVCZGFAYA56UXT5P","json":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P.json","graph_json":"https://pith.science/api/pith-number/QZVN7SPGPZDVCZGFAYA56UXT5P/graph.json","events_json":"https://pith.science/api/pith-number/QZVN7SPGPZDVCZGFAYA56UXT5P/events.json","paper":"https://pith.science/paper/QZVN7SPG"},"agent_actions":{"view_html":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P","download_json":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P.json","view_paper":"https://pith.science/paper/QZVN7SPG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.29413&json=true","fetch_graph":"https://pith.science/api/pith-number/QZVN7SPGPZDVCZGFAYA56UXT5P/graph.json","fetch_events":"https://pith.science/api/pith-number/QZVN7SPGPZDVCZGFAYA56UXT5P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P/action/storage_attestation","attest_author":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P/action/author_attestation","sign_citation":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P/action/citation_signature","submit_replication":"https://pith.science/pith/QZVN7SPGPZDVCZGFAYA56UXT5P/action/replication_record"}},"created_at":"2026-06-30T01:18:05.282119+00:00","updated_at":"2026-06-30T01:18:05.282119+00:00"}