{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:TK6KXHNJPI2SP44AMDJ75ADCHQ","short_pith_number":"pith:TK6KXHNJ","schema_version":"1.0","canonical_sha256":"9abcab9da97a3527f38060d3fe80623c2c2a556c9690e7b01c609e32578eb0d0","source":{"kind":"arxiv","id":"2006.01383","version":1},"attestation_state":"computed","paper":{"title":"S-wave kaon-nucleon potentials with all-to-all propagators in the HAL QCD method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Kotaro Murakami, Sinya Aoki, Yutaro Akahoshi","submitted_at":"2020-06-02T04:25:05Z","abstract_excerpt":"In this paper, employing an all-to-all quark propagator technique, we investigate the kaon-nucleon interactions in lattice QCD. We calculate the S-wave kaon-nucleon potentials at the leading order in the derivative expansion in the time-dependent HAL QCD method, using (2+1)-flavor gauge configurations at the lattice spacing $a \\approx 0.09$ fm on $32^3 \\times 64$ lattices and the pion mass $m_{\\pi} \\approx 570$ MeV. We take the one-end trick for all-to-all propagators, which allows us to put the zero momentum hadron operators at both source and sink and to smear quark operators at the source. "},"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":"2006.01383","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2020-06-02T04:25:05Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"a6d603c95ef44b0159d2d1bf9ba23bcd3a7b6ffa10582d1db0e481b55b18e3b6","abstract_canon_sha256":"af7efe9b06e4429dfd451080f241201ca7fbc484738f3a52ac159210be0d345f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:35:33.225273Z","signature_b64":"dtnS0Ew2ffrMjGZdwZ6m538DUGX62hswrqgtG8tYRXU6iVs3CaJkDeEEZ5/r/g/CYCHhP+vgVqGlSktdDtYVDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9abcab9da97a3527f38060d3fe80623c2c2a556c9690e7b01c609e32578eb0d0","last_reissued_at":"2026-07-05T01:35:33.224747Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:35:33.224747Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"S-wave kaon-nucleon potentials with all-to-all propagators in the HAL QCD method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Kotaro Murakami, Sinya Aoki, Yutaro Akahoshi","submitted_at":"2020-06-02T04:25:05Z","abstract_excerpt":"In this paper, employing an all-to-all quark propagator technique, we investigate the kaon-nucleon interactions in lattice QCD. We calculate the S-wave kaon-nucleon potentials at the leading order in the derivative expansion in the time-dependent HAL QCD method, using (2+1)-flavor gauge configurations at the lattice spacing $a \\approx 0.09$ fm on $32^3 \\times 64$ lattices and the pion mass $m_{\\pi} \\approx 570$ MeV. We take the one-end trick for all-to-all propagators, which allows us to put the zero momentum hadron operators at both source and sink and to smear quark operators at the source. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2006.01383","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/2006.01383/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":"2006.01383","created_at":"2026-07-05T01:35:33.224819+00:00"},{"alias_kind":"arxiv_version","alias_value":"2006.01383v1","created_at":"2026-07-05T01:35:33.224819+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2006.01383","created_at":"2026-07-05T01:35:33.224819+00:00"},{"alias_kind":"pith_short_12","alias_value":"TK6KXHNJPI2S","created_at":"2026-07-05T01:35:33.224819+00:00"},{"alias_kind":"pith_short_16","alias_value":"TK6KXHNJPI2SP44A","created_at":"2026-07-05T01:35:33.224819+00:00"},{"alias_kind":"pith_short_8","alias_value":"TK6KXHNJ","created_at":"2026-07-05T01:35:33.224819+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.00838","citing_title":"$S$-wave kaon-nucleon interactions from lattice QCD at the physical point","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ","json":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ.json","graph_json":"https://pith.science/api/pith-number/TK6KXHNJPI2SP44AMDJ75ADCHQ/graph.json","events_json":"https://pith.science/api/pith-number/TK6KXHNJPI2SP44AMDJ75ADCHQ/events.json","paper":"https://pith.science/paper/TK6KXHNJ"},"agent_actions":{"view_html":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ","download_json":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ.json","view_paper":"https://pith.science/paper/TK6KXHNJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2006.01383&json=true","fetch_graph":"https://pith.science/api/pith-number/TK6KXHNJPI2SP44AMDJ75ADCHQ/graph.json","fetch_events":"https://pith.science/api/pith-number/TK6KXHNJPI2SP44AMDJ75ADCHQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ/action/storage_attestation","attest_author":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ/action/author_attestation","sign_citation":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ/action/citation_signature","submit_replication":"https://pith.science/pith/TK6KXHNJPI2SP44AMDJ75ADCHQ/action/replication_record"}},"created_at":"2026-07-05T01:35:33.224819+00:00","updated_at":"2026-07-05T01:35:33.224819+00:00"}