{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:F6LS3JPME4V75XMMYO65IGHFEE","short_pith_number":"pith:F6LS3JPM","schema_version":"1.0","canonical_sha256":"2f972da5ec272bfedd8cc3bdd418e521196b5838dac134a860acb795e121884c","source":{"kind":"arxiv","id":"1203.3320","version":1},"attestation_state":"computed","paper":{"title":"Baryon-baryon interaction of strangeness S=-1 sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"for HAL QCD Collaboration, Hidekatsu Nemura","submitted_at":"2012-03-15T11:10:41Z","abstract_excerpt":"We present our recent studies on hyperon-nucleon (YN) interactions in the strangeness S=-1 that $p\\Lambda, \\Sigma^0 p$ and $\\Sigma^+ n$, by extracting corresponding potentials through Nambu-Bethe-Salpeter wave functions. We calculate $\\Lambda N$ and $\\Sigma N$ potentials in the isospin I=3/2 channel, using the $N_f=2+1$ gauge configurations generated by PACS-CS collaboration and employing an improved method to obtain potentials in lattice QCD simulations. For the $^1S_0$ channel, the central $\\Sigma N (I=3/2, ^1S_0)$ potential and the central $\\Lambda N (^1S_0)$ potential are found to be very "},"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":"1203.3320","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-03-15T11:10:41Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"3ab71fd9bedd38227a48c19d1f82732e8ec6375edce42026a03a2239db2a0efb","abstract_canon_sha256":"4a7305c71935d7ab35b8f5c838c395a1f2f9142ac4eb3c04ac6cfedda279a736"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:00:02.132554Z","signature_b64":"v80SoBc7HSYjcqPybw8QCCL2SDZ/FZ7pTf4RUZMCcv48EHR9b2wJEpQYomOM6+oBy4fd5rhoUYQJrTwsQevKBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f972da5ec272bfedd8cc3bdd418e521196b5838dac134a860acb795e121884c","last_reissued_at":"2026-05-18T04:00:02.131782Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:00:02.131782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon-baryon interaction of strangeness S=-1 sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"for HAL QCD Collaboration, Hidekatsu Nemura","submitted_at":"2012-03-15T11:10:41Z","abstract_excerpt":"We present our recent studies on hyperon-nucleon (YN) interactions in the strangeness S=-1 that $p\\Lambda, \\Sigma^0 p$ and $\\Sigma^+ n$, by extracting corresponding potentials through Nambu-Bethe-Salpeter wave functions. We calculate $\\Lambda N$ and $\\Sigma N$ potentials in the isospin I=3/2 channel, using the $N_f=2+1$ gauge configurations generated by PACS-CS collaboration and employing an improved method to obtain potentials in lattice QCD simulations. For the $^1S_0$ channel, the central $\\Sigma N (I=3/2, ^1S_0)$ potential and the central $\\Lambda N (^1S_0)$ potential are found to be very "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.3320","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":""},"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":"1203.3320","created_at":"2026-05-18T04:00:02.131905+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.3320v1","created_at":"2026-05-18T04:00:02.131905+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.3320","created_at":"2026-05-18T04:00:02.131905+00:00"},{"alias_kind":"pith_short_12","alias_value":"F6LS3JPME4V7","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"F6LS3JPME4V75XMM","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"F6LS3JPM","created_at":"2026-05-18T12:27:04.183437+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/F6LS3JPME4V75XMMYO65IGHFEE","json":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE.json","graph_json":"https://pith.science/api/pith-number/F6LS3JPME4V75XMMYO65IGHFEE/graph.json","events_json":"https://pith.science/api/pith-number/F6LS3JPME4V75XMMYO65IGHFEE/events.json","paper":"https://pith.science/paper/F6LS3JPM"},"agent_actions":{"view_html":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE","download_json":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE.json","view_paper":"https://pith.science/paper/F6LS3JPM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.3320&json=true","fetch_graph":"https://pith.science/api/pith-number/F6LS3JPME4V75XMMYO65IGHFEE/graph.json","fetch_events":"https://pith.science/api/pith-number/F6LS3JPME4V75XMMYO65IGHFEE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE/action/storage_attestation","attest_author":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE/action/author_attestation","sign_citation":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE/action/citation_signature","submit_replication":"https://pith.science/pith/F6LS3JPME4V75XMMYO65IGHFEE/action/replication_record"}},"created_at":"2026-05-18T04:00:02.131905+00:00","updated_at":"2026-05-18T04:00:02.131905+00:00"}