{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:OHOCXHSQ7YVCA2X6VRLLL7CHSH","short_pith_number":"pith:OHOCXHSQ","schema_version":"1.0","canonical_sha256":"71dc2b9e50fe2a206afeac56b5fc4791c2c2d80d9f5fd71006d7600b11ac5293","source":{"kind":"arxiv","id":"1109.2889","version":1},"attestation_state":"computed","paper":{"title":"The Deuteron and Exotic Two-Body Bound States from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Parreno, A. Torok, A. Walker-Loud (NPLQCD Collaboration), E. Chang, H. W. Lin, K. Orginos, M. J. Savage, S. R. Beane, T. C. Luu, W. Detmold","submitted_at":"2011-09-13T19:31:25Z","abstract_excerpt":"Results of a high-statistics, multi-volume Lattice QCD exploration of the deuteron, the di-neutron, the H-dibaryon, and the Xi-Xi- system at a pion mass of m ~ 390 MeV are presented. Calculations were performed with an anisotropic n_f = 2+1 Clover discretization in four lattice volumes of spatial extent L ~ 2.0, 2.5, 3.0 and 4.0 fm, with a lattice spacing of b_s ~ 0.123 fm in the spatial-direction, and b_t ~ b_s/3.5 in the time-direction. The Xi-Xi- is found to be bound by B_{Xi-Xi-} = 14.0(1.4)(6.7) MeV, consistent with expectations based upon phenomenological models and low-energy effective "},"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":"1109.2889","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2011-09-13T19:31:25Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"b329d71b4e058b830fdc068ec8c979350e6a05d65e7438337c54714d2f14e09a","abstract_canon_sha256":"a4cc243449a5aaf04ba481422a1a22441b542ecf70bd46a334d12c34e51946bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:02.203370Z","signature_b64":"qU/PdYEx5CIapew75mGzhDNqVg7MMDcuxiblbK+ZLgWp5WKu6ILDkKcwcJ4PvkaDvRNNYhaz026or0hYX4XLCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"71dc2b9e50fe2a206afeac56b5fc4791c2c2d80d9f5fd71006d7600b11ac5293","last_reissued_at":"2026-05-18T03:23:02.202898Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:02.202898Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Deuteron and Exotic Two-Body Bound States from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Parreno, A. Torok, A. Walker-Loud (NPLQCD Collaboration), E. Chang, H. W. Lin, K. Orginos, M. J. Savage, S. R. Beane, T. C. Luu, W. Detmold","submitted_at":"2011-09-13T19:31:25Z","abstract_excerpt":"Results of a high-statistics, multi-volume Lattice QCD exploration of the deuteron, the di-neutron, the H-dibaryon, and the Xi-Xi- system at a pion mass of m ~ 390 MeV are presented. Calculations were performed with an anisotropic n_f = 2+1 Clover discretization in four lattice volumes of spatial extent L ~ 2.0, 2.5, 3.0 and 4.0 fm, with a lattice spacing of b_s ~ 0.123 fm in the spatial-direction, and b_t ~ b_s/3.5 in the time-direction. The Xi-Xi- is found to be bound by B_{Xi-Xi-} = 14.0(1.4)(6.7) MeV, consistent with expectations based upon phenomenological models and low-energy effective "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.2889","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":""},"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":"1109.2889","created_at":"2026-05-18T03:23:02.202973+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.2889v1","created_at":"2026-05-18T03:23:02.202973+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.2889","created_at":"2026-05-18T03:23:02.202973+00:00"},{"alias_kind":"pith_short_12","alias_value":"OHOCXHSQ7YVC","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"OHOCXHSQ7YVCA2X6","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"OHOCXHSQ","created_at":"2026-05-18T12:26:37.096874+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":11,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH","json":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH.json","graph_json":"https://pith.science/api/pith-number/OHOCXHSQ7YVCA2X6VRLLL7CHSH/graph.json","events_json":"https://pith.science/api/pith-number/OHOCXHSQ7YVCA2X6VRLLL7CHSH/events.json","paper":"https://pith.science/paper/OHOCXHSQ"},"agent_actions":{"view_html":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH","download_json":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH.json","view_paper":"https://pith.science/paper/OHOCXHSQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.2889&json=true","fetch_graph":"https://pith.science/api/pith-number/OHOCXHSQ7YVCA2X6VRLLL7CHSH/graph.json","fetch_events":"https://pith.science/api/pith-number/OHOCXHSQ7YVCA2X6VRLLL7CHSH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH/action/storage_attestation","attest_author":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH/action/author_attestation","sign_citation":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH/action/citation_signature","submit_replication":"https://pith.science/pith/OHOCXHSQ7YVCA2X6VRLLL7CHSH/action/replication_record"}},"created_at":"2026-05-18T03:23:02.202973+00:00","updated_at":"2026-05-18T03:23:02.202973+00:00"}