{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:3SIK3GIMEMKDRMDEYNAD3KWGH4","short_pith_number":"pith:3SIK3GIM","schema_version":"1.0","canonical_sha256":"dc90ad990c231438b064c3403daac63f073972bb8c025224e50f7dc6af4f0f2c","source":{"kind":"arxiv","id":"1709.00654","version":2},"attestation_state":"computed","paper":{"title":"Most Strange Dibaryon from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"Hidekatsu Nemura, Kenji Sasaki, Noriyoshi Ishii, Shinya Gongyo, Sinya Aoki, Takashi Inoue, Takaya Miyamoto, Takumi Doi, Takumi Iritani, Tetsuo Hatsuda, Yoichi Ikeda","submitted_at":"2017-09-03T03:05:12Z","abstract_excerpt":"The $\\Omega\\Omega$ system in the $^1S_0$ channel (the most strange dibaryon) is studied on the basis of the (2+1)-flavor lattice QCD simulations with a large volume (8.1 fm)$^3$ and nearly physical pion mass $m_{\\pi}\\simeq 146$ MeV at a lattice spacing $a\\simeq 0.0846$ fm. We show that lattice QCD data analysis by the HAL QCD method leads to the scattering length $a_0 = 4.6 (6)(^{+1.2}_{-0.5}) {\\rm fm}$, the effective range $r_{\\rm eff} = 1.27 (3)(^{+0.06}_{-0.03}) {\\rm fm}$ and the binding energy $B_{\\Omega \\Omega} = 1.6 (6) (^{+0.7}_{-0.6}) {\\rm MeV}$. These results indicate that the $\\Omega"},"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":"1709.00654","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-09-03T03:05:12Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex","nucl-th"],"title_canon_sha256":"6edd7faf8bb19294708b6bd080eabe481fe52d8b9533d732d9c6aabb5b8dfbd7","abstract_canon_sha256":"08ddeb9cf26a77653f95ee751c0ca768a5732ed61de85011e0f8fe607831672a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:05.377200Z","signature_b64":"m9EpW2CAO9n6BiF4RgmRDpKaRuStZ4XG9+8Af4HLRwQJBg4Ta9fuQ2J5je+Pc4ArRjCpB6LxKI3JeyozBxyRBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc90ad990c231438b064c3403daac63f073972bb8c025224e50f7dc6af4f0f2c","last_reissued_at":"2026-05-18T00:15:05.376429Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:05.376429Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Most Strange Dibaryon from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"Hidekatsu Nemura, Kenji Sasaki, Noriyoshi Ishii, Shinya Gongyo, Sinya Aoki, Takashi Inoue, Takaya Miyamoto, Takumi Doi, Takumi Iritani, Tetsuo Hatsuda, Yoichi Ikeda","submitted_at":"2017-09-03T03:05:12Z","abstract_excerpt":"The $\\Omega\\Omega$ system in the $^1S_0$ channel (the most strange dibaryon) is studied on the basis of the (2+1)-flavor lattice QCD simulations with a large volume (8.1 fm)$^3$ and nearly physical pion mass $m_{\\pi}\\simeq 146$ MeV at a lattice spacing $a\\simeq 0.0846$ fm. We show that lattice QCD data analysis by the HAL QCD method leads to the scattering length $a_0 = 4.6 (6)(^{+1.2}_{-0.5}) {\\rm fm}$, the effective range $r_{\\rm eff} = 1.27 (3)(^{+0.06}_{-0.03}) {\\rm fm}$ and the binding energy $B_{\\Omega \\Omega} = 1.6 (6) (^{+0.7}_{-0.6}) {\\rm MeV}$. These results indicate that the $\\Omega"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.00654","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":"1709.00654","created_at":"2026-05-18T00:15:05.376547+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.00654v2","created_at":"2026-05-18T00:15:05.376547+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.00654","created_at":"2026-05-18T00:15:05.376547+00:00"},{"alias_kind":"pith_short_12","alias_value":"3SIK3GIMEMKD","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"3SIK3GIMEMKDRMDE","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"3SIK3GIM","created_at":"2026-05-18T12:30:58.224056+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.17813","citing_title":"Compositeness of near-threshold eigenstates with Coulomb plus short-range interactions","ref_index":88,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4","json":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4.json","graph_json":"https://pith.science/api/pith-number/3SIK3GIMEMKDRMDEYNAD3KWGH4/graph.json","events_json":"https://pith.science/api/pith-number/3SIK3GIMEMKDRMDEYNAD3KWGH4/events.json","paper":"https://pith.science/paper/3SIK3GIM"},"agent_actions":{"view_html":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4","download_json":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4.json","view_paper":"https://pith.science/paper/3SIK3GIM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.00654&json=true","fetch_graph":"https://pith.science/api/pith-number/3SIK3GIMEMKDRMDEYNAD3KWGH4/graph.json","fetch_events":"https://pith.science/api/pith-number/3SIK3GIMEMKDRMDEYNAD3KWGH4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4/action/storage_attestation","attest_author":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4/action/author_attestation","sign_citation":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4/action/citation_signature","submit_replication":"https://pith.science/pith/3SIK3GIMEMKDRMDEYNAD3KWGH4/action/replication_record"}},"created_at":"2026-05-18T00:15:05.376547+00:00","updated_at":"2026-05-18T00:15:05.376547+00:00"}