{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:6CGKPEB6TOOLEEQWEYRP472D6I","short_pith_number":"pith:6CGKPEB6","schema_version":"1.0","canonical_sha256":"f08ca7903e9b9cb212162622fe7f43f20ecb61c05c43f52111994298e79a73d7","source":{"kind":"arxiv","id":"1805.03966","version":2},"attestation_state":"computed","paper":{"title":"Lattice QCD study of the $H$ dibaryon using hexaquark and two-baryon interpolators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Francis, Ch. Miao, H. Wittig, J.R. Green, P.M. Junnarkar, T.D. Rae","submitted_at":"2018-05-10T13:29:20Z","abstract_excerpt":"We present a lattice QCD spectroscopy study in the isospin singlet, strangeness $-2$ sectors relevant for the conjectured $H$ dibaryon. We employ both local and bilocal interpolating operators to isolate the ground state in the rest frame and in moving frames. Calculations are performed using two flavors of O($a$)-improved Wilson fermions and a quenched strange quark. Our initial point-source method for constructing correlators does not allow for bilocal operators at the source; nevertheless, results from using these operators at the sink indicate that they provide an improved overlap onto the"},"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":"1805.03966","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-05-10T13:29:20Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"09baeb0517b5bc19e9d18b2bf940211029a6b169ce19d289ad9e19a7b4bfa33a","abstract_canon_sha256":"63e594a09f0acffda8c4abff236b40641168ac36dfbcced0c1416d48456e723b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:34.191716Z","signature_b64":"GpeD4nF4bjnw6d3Azih+OQRIjLegW6aSDUe3+6YbELSZkyVNx+g2j2P100NdoySi8Q83C0UNRiEQ1Bu58p6zDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f08ca7903e9b9cb212162622fe7f43f20ecb61c05c43f52111994298e79a73d7","last_reissued_at":"2026-05-17T23:48:34.191117Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:34.191117Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice QCD study of the $H$ dibaryon using hexaquark and two-baryon interpolators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Francis, Ch. Miao, H. Wittig, J.R. Green, P.M. Junnarkar, T.D. Rae","submitted_at":"2018-05-10T13:29:20Z","abstract_excerpt":"We present a lattice QCD spectroscopy study in the isospin singlet, strangeness $-2$ sectors relevant for the conjectured $H$ dibaryon. We employ both local and bilocal interpolating operators to isolate the ground state in the rest frame and in moving frames. Calculations are performed using two flavors of O($a$)-improved Wilson fermions and a quenched strange quark. Our initial point-source method for constructing correlators does not allow for bilocal operators at the source; nevertheless, results from using these operators at the sink indicate that they provide an improved overlap onto the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.03966","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":""},"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":"1805.03966","created_at":"2026-05-17T23:48:34.191194+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.03966v2","created_at":"2026-05-17T23:48:34.191194+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.03966","created_at":"2026-05-17T23:48:34.191194+00:00"},{"alias_kind":"pith_short_12","alias_value":"6CGKPEB6TOOL","created_at":"2026-05-18T12:32:08.215937+00:00"},{"alias_kind":"pith_short_16","alias_value":"6CGKPEB6TOOLEEQW","created_at":"2026-05-18T12:32:08.215937+00:00"},{"alias_kind":"pith_short_8","alias_value":"6CGKPEB6","created_at":"2026-05-18T12:32:08.215937+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.16977","citing_title":"Two-nucleon systems at $m_{\\pi}\\approx292$ MeV from lattice QCD","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I","json":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I.json","graph_json":"https://pith.science/api/pith-number/6CGKPEB6TOOLEEQWEYRP472D6I/graph.json","events_json":"https://pith.science/api/pith-number/6CGKPEB6TOOLEEQWEYRP472D6I/events.json","paper":"https://pith.science/paper/6CGKPEB6"},"agent_actions":{"view_html":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I","download_json":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I.json","view_paper":"https://pith.science/paper/6CGKPEB6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.03966&json=true","fetch_graph":"https://pith.science/api/pith-number/6CGKPEB6TOOLEEQWEYRP472D6I/graph.json","fetch_events":"https://pith.science/api/pith-number/6CGKPEB6TOOLEEQWEYRP472D6I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I/action/storage_attestation","attest_author":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I/action/author_attestation","sign_citation":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I/action/citation_signature","submit_replication":"https://pith.science/pith/6CGKPEB6TOOLEEQWEYRP472D6I/action/replication_record"}},"created_at":"2026-05-17T23:48:34.191194+00:00","updated_at":"2026-05-17T23:48:34.191194+00:00"}