{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:XRIZAVNF7ZNOZHEMSV2WJ6TQKF","short_pith_number":"pith:XRIZAVNF","schema_version":"1.0","canonical_sha256":"bc519055a5fe5aec9c8c957564fa705148bbcdb706e4149553a4e5bc263ebae5","source":{"kind":"arxiv","id":"2308.16793","version":2},"attestation_state":"computed","paper":{"title":"Hybrid Renormalization for Quasi Distribution Amplitudes of A Light Baryon","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Chao Han, Jia-Lu Zhang, Wei Wang, Yushan Su","submitted_at":"2023-08-31T15:11:11Z","abstract_excerpt":"We develop a hybrid scheme to renormalize quasi distribution amplitudes of a light baryon on the lattice, which combines the self-renormalization and ratio scheme. By employing self-renormalization, the UV divergences and linear divergence at large spatial separations in quasi distribution amplitudes are removed without introducing extra nonperturbative effects, while making a ratio with respect to the zero-momentum matrix element can properly remove the UV divergences in small spatial separations. As a specific application, distribution amplitudes of the $\\Lambda$ baryon made of $uds$ are inv"},"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":"2308.16793","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-08-31T15:11:11Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"424e215890aeb1d7b35c727d00d0549af4874ab1d74ea12673c61cf5dff33424","abstract_canon_sha256":"6e41273e5cdb0022ecf85ba5d9ba933366cab75a837c52272834335200cb87f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:21:44.206652Z","signature_b64":"bQpE+WKA+KtSClw35RDyZcK3eLMjlJpFBFs4JAgo376ozrc72KEKFYMCUD+HjdZiJ+o7XUrMzbqchXenne7uAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc519055a5fe5aec9c8c957564fa705148bbcdb706e4149553a4e5bc263ebae5","last_reissued_at":"2026-07-05T07:21:44.206267Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:21:44.206267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hybrid Renormalization for Quasi Distribution Amplitudes of A Light Baryon","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Chao Han, Jia-Lu Zhang, Wei Wang, Yushan Su","submitted_at":"2023-08-31T15:11:11Z","abstract_excerpt":"We develop a hybrid scheme to renormalize quasi distribution amplitudes of a light baryon on the lattice, which combines the self-renormalization and ratio scheme. By employing self-renormalization, the UV divergences and linear divergence at large spatial separations in quasi distribution amplitudes are removed without introducing extra nonperturbative effects, while making a ratio with respect to the zero-momentum matrix element can properly remove the UV divergences in small spatial separations. As a specific application, distribution amplitudes of the $\\Lambda$ baryon made of $uds$ are inv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2308.16793","kind":"arxiv","version":2},"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/2308.16793/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":"2308.16793","created_at":"2026-07-05T07:21:44.206320+00:00"},{"alias_kind":"arxiv_version","alias_value":"2308.16793v2","created_at":"2026-07-05T07:21:44.206320+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2308.16793","created_at":"2026-07-05T07:21:44.206320+00:00"},{"alias_kind":"pith_short_12","alias_value":"XRIZAVNF7ZNO","created_at":"2026-07-05T07:21:44.206320+00:00"},{"alias_kind":"pith_short_16","alias_value":"XRIZAVNF7ZNOZHEM","created_at":"2026-07-05T07:21:44.206320+00:00"},{"alias_kind":"pith_short_8","alias_value":"XRIZAVNF","created_at":"2026-07-05T07:21:44.206320+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.19091","citing_title":"Updated determination of light-cone distribution amplitudes of octet baryons in lattice QCD","ref_index":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF","json":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF.json","graph_json":"https://pith.science/api/pith-number/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/graph.json","events_json":"https://pith.science/api/pith-number/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/events.json","paper":"https://pith.science/paper/XRIZAVNF"},"agent_actions":{"view_html":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF","download_json":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF.json","view_paper":"https://pith.science/paper/XRIZAVNF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2308.16793&json=true","fetch_graph":"https://pith.science/api/pith-number/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/graph.json","fetch_events":"https://pith.science/api/pith-number/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/action/storage_attestation","attest_author":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/action/author_attestation","sign_citation":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/action/citation_signature","submit_replication":"https://pith.science/pith/XRIZAVNF7ZNOZHEMSV2WJ6TQKF/action/replication_record"}},"created_at":"2026-07-05T07:21:44.206320+00:00","updated_at":"2026-07-05T07:21:44.206320+00:00"}