{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:HARZYKXLIOQN2LIAM2EGRU733G","short_pith_number":"pith:HARZYKXL","schema_version":"1.0","canonical_sha256":"38239c2aeb43a0dd2d00668868d3fbd9b1ce67c61f40b9e34438db019bbda300","source":{"kind":"arxiv","id":"1908.08333","version":1},"attestation_state":"computed","paper":{"title":"Intrinsic three-body nuclear interaction from a constituent quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Aaron Park, Su Houng Lee","submitted_at":"2019-08-22T12:23:23Z","abstract_excerpt":"We study the short distance part of the intrinsic three-nucleon interaction in a constituent quark model with color-spin interaction. For that purpose we first calculate the transformation coefficient between the tribaryon configuration and their corresponding three baryon basis. Using a formula for the intrinsic three-body interaction in terms of a tribaryon configuration, we find that after subtracting the corresponding two-baryon contributions, the intrinsic three-body interaction vanishes in flavor SU(3) symmetric limit for all quantum numbers for the three nucleon states. We further find "},"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":"1908.08333","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-08-22T12:23:23Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"cdf7c6891bfec0a77c906c7e6f99a62b6c301036eab0865eacd7ff981828a665","abstract_canon_sha256":"321cc94d93e7c4f27e4155290099fafa3a4802e4c10391ac1e1c32615b659967"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:18:39.707658Z","signature_b64":"SPNGBizLlx9HjnUYpdX3+Ht6PXfAqQUKhH3bazH5pSW5+Z1CRNwtagTjfacOLKT090raTuzVuYEsmfR1EqrJDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38239c2aeb43a0dd2d00668868d3fbd9b1ce67c61f40b9e34438db019bbda300","last_reissued_at":"2026-07-05T00:18:39.707165Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:18:39.707165Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Intrinsic three-body nuclear interaction from a constituent quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Aaron Park, Su Houng Lee","submitted_at":"2019-08-22T12:23:23Z","abstract_excerpt":"We study the short distance part of the intrinsic three-nucleon interaction in a constituent quark model with color-spin interaction. For that purpose we first calculate the transformation coefficient between the tribaryon configuration and their corresponding three baryon basis. Using a formula for the intrinsic three-body interaction in terms of a tribaryon configuration, we find that after subtracting the corresponding two-baryon contributions, the intrinsic three-body interaction vanishes in flavor SU(3) symmetric limit for all quantum numbers for the three nucleon states. We further find "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.08333","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/1908.08333/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":"1908.08333","created_at":"2026-07-05T00:18:39.707231+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.08333v1","created_at":"2026-07-05T00:18:39.707231+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.08333","created_at":"2026-07-05T00:18:39.707231+00:00"},{"alias_kind":"pith_short_12","alias_value":"HARZYKXLIOQN","created_at":"2026-07-05T00:18:39.707231+00:00"},{"alias_kind":"pith_short_16","alias_value":"HARZYKXLIOQN2LIA","created_at":"2026-07-05T00:18:39.707231+00:00"},{"alias_kind":"pith_short_8","alias_value":"HARZYKXL","created_at":"2026-07-05T00:18:39.707231+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/HARZYKXLIOQN2LIAM2EGRU733G","json":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G.json","graph_json":"https://pith.science/api/pith-number/HARZYKXLIOQN2LIAM2EGRU733G/graph.json","events_json":"https://pith.science/api/pith-number/HARZYKXLIOQN2LIAM2EGRU733G/events.json","paper":"https://pith.science/paper/HARZYKXL"},"agent_actions":{"view_html":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G","download_json":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G.json","view_paper":"https://pith.science/paper/HARZYKXL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.08333&json=true","fetch_graph":"https://pith.science/api/pith-number/HARZYKXLIOQN2LIAM2EGRU733G/graph.json","fetch_events":"https://pith.science/api/pith-number/HARZYKXLIOQN2LIAM2EGRU733G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G/action/storage_attestation","attest_author":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G/action/author_attestation","sign_citation":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G/action/citation_signature","submit_replication":"https://pith.science/pith/HARZYKXLIOQN2LIAM2EGRU733G/action/replication_record"}},"created_at":"2026-07-05T00:18:39.707231+00:00","updated_at":"2026-07-05T00:18:39.707231+00:00"}