{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:WYVHUGNKYG3LG5HR2N5ZKLSD5C","short_pith_number":"pith:WYVHUGNK","schema_version":"1.0","canonical_sha256":"b62a7a19aac1b6b374f1d37b952e43e8a8767abafb9e2ce1d83546b503da4aa3","source":{"kind":"arxiv","id":"nucl-th/9807082","version":1},"attestation_state":"computed","paper":{"title":"Soft-core hyperon-nucleon potentials","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"ANL), Japan), Th. A. Rijken (Nijmegen), V. G. J. Stoks (CSSM, Y. Yamamoto (Tsuru","submitted_at":"1998-07-31T00:56:19Z","abstract_excerpt":"A new Nijmegen soft-core OBE potential model is presented for the low-energy YN interactions. Besides the results for the fit to the scattering data, which largely defines the model, we also present some applications to hypernuclear systems using the G-matrix method. An important innovation with respect to the original soft-core potential is the assignment of the cut-off masses for the baryon-baryon-meson (BBM) vertices in accordance with broken SU(3)$_F$, which serves to connect the NN and the YN channels. As a novel feature, we allow for medium strong breaking of the coupling constants, usin"},"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":"nucl-th/9807082","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1998-07-31T00:56:19Z","cross_cats_sorted":[],"title_canon_sha256":"a28e2ab52e900cb049772fb9aaf8c5c72d75aee5ea8ffbb044104b28c1c133f0","abstract_canon_sha256":"fb670c062a3b4bcec5602b9e1e5c6baa96b68502de1933651d84749ab3870401"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:29.033035Z","signature_b64":"Ajk6d5n1kekdI2pCu9HS6uV3FpFFje6xKJW8g+jGhlr9WAGNujZcGSDqQoj7+w5M8HPtFBsl6X8Wo8z9/ZDMBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b62a7a19aac1b6b374f1d37b952e43e8a8767abafb9e2ce1d83546b503da4aa3","last_reissued_at":"2026-07-04T15:23:29.032565Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:29.032565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Soft-core hyperon-nucleon potentials","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"ANL), Japan), Th. A. Rijken (Nijmegen), V. G. J. Stoks (CSSM, Y. Yamamoto (Tsuru","submitted_at":"1998-07-31T00:56:19Z","abstract_excerpt":"A new Nijmegen soft-core OBE potential model is presented for the low-energy YN interactions. Besides the results for the fit to the scattering data, which largely defines the model, we also present some applications to hypernuclear systems using the G-matrix method. An important innovation with respect to the original soft-core potential is the assignment of the cut-off masses for the baryon-baryon-meson (BBM) vertices in accordance with broken SU(3)$_F$, which serves to connect the NN and the YN channels. As a novel feature, we allow for medium strong breaking of the coupling constants, usin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9807082","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/nucl-th/9807082/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":"nucl-th/9807082","created_at":"2026-07-04T15:23:29.032622+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9807082v1","created_at":"2026-07-04T15:23:29.032622+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9807082","created_at":"2026-07-04T15:23:29.032622+00:00"},{"alias_kind":"pith_short_12","alias_value":"WYVHUGNKYG3L","created_at":"2026-07-04T15:23:29.032622+00:00"},{"alias_kind":"pith_short_16","alias_value":"WYVHUGNKYG3LG5HR","created_at":"2026-07-04T15:23:29.032622+00:00"},{"alias_kind":"pith_short_8","alias_value":"WYVHUGNK","created_at":"2026-07-04T15:23:29.032622+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.11808","citing_title":"Nonexistence of hidden-charm pentaquarks in $J/\\psi$ photoproduction","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28285","citing_title":"Probing hidden-charm pentaquarks from the $\\pi N\\rightarrow J/\\psi N$ reaction","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C","json":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C.json","graph_json":"https://pith.science/api/pith-number/WYVHUGNKYG3LG5HR2N5ZKLSD5C/graph.json","events_json":"https://pith.science/api/pith-number/WYVHUGNKYG3LG5HR2N5ZKLSD5C/events.json","paper":"https://pith.science/paper/WYVHUGNK"},"agent_actions":{"view_html":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C","download_json":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C.json","view_paper":"https://pith.science/paper/WYVHUGNK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9807082&json=true","fetch_graph":"https://pith.science/api/pith-number/WYVHUGNKYG3LG5HR2N5ZKLSD5C/graph.json","fetch_events":"https://pith.science/api/pith-number/WYVHUGNKYG3LG5HR2N5ZKLSD5C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C/action/storage_attestation","attest_author":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C/action/author_attestation","sign_citation":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C/action/citation_signature","submit_replication":"https://pith.science/pith/WYVHUGNKYG3LG5HR2N5ZKLSD5C/action/replication_record"}},"created_at":"2026-07-04T15:23:29.032622+00:00","updated_at":"2026-07-04T15:23:29.032622+00:00"}