{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:XDG2KFEYB5DX6YP3DNBDXVCCKQ","short_pith_number":"pith:XDG2KFEY","schema_version":"1.0","canonical_sha256":"b8cda514980f477f61fb1b423bd44254066f529c79e9c9c535c94b100b474278","source":{"kind":"arxiv","id":"1206.5219","version":2},"attestation_state":"computed","paper":{"title":"Light Nuclei and Hypernuclei from Quantum Chromodynamics in the Limit of SU(3) Flavor Symmetry","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. Walker-Loud, E. Chang, H. W. Lin, K. Orginos, M. J. Savage, S. D. Cohen, S. R. Beane, T. C. Luu, W. Detmold","submitted_at":"2012-06-22T18:01:12Z","abstract_excerpt":"The binding energies of a range of nuclei and hypernuclei with atomic number A <= 4 and strangeness |s| <= 2, including the deuteron, di-neutron, H-dibaryon, 3He, Lambda 3He, Lambda 4He, and Lambda Lambda 4He, are calculated in the limit of flavor-SU(3) symmetry at the physical strange quark mass with quantum chromodynamics (without electromagnetic interactions). The nuclear states are extracted from Lattice QCD calculations performed with n_f=3 dynamical light quarks using an isotropic clover discretization of the quark-action in three lattice volumes of spatial extent L ~ 3.4 fm, 4.5 fm and "},"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":"1206.5219","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-06-22T18:01:12Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"7ae23b57bc1fcd136c5eb22a143fb212a6a5079bd0809443c2a28000951a07e9","abstract_canon_sha256":"2dd9371063e7bc9224e71ae345c0c22a089a565ae73521c9097e2974208e3bab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:17.613632Z","signature_b64":"L5X+65egBeMv8LZutNqVIuPfQcPevDCLOU5EWpTgyhjUMIfrPBSCu2PWqqM8gPUl0wOJdjWL/4WKKOladfLSCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b8cda514980f477f61fb1b423bd44254066f529c79e9c9c535c94b100b474278","last_reissued_at":"2026-05-18T03:31:17.612827Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:17.612827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light Nuclei and Hypernuclei from Quantum Chromodynamics in the Limit of SU(3) Flavor Symmetry","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. Walker-Loud, E. Chang, H. W. Lin, K. Orginos, M. J. Savage, S. D. Cohen, S. R. Beane, T. C. Luu, W. Detmold","submitted_at":"2012-06-22T18:01:12Z","abstract_excerpt":"The binding energies of a range of nuclei and hypernuclei with atomic number A <= 4 and strangeness |s| <= 2, including the deuteron, di-neutron, H-dibaryon, 3He, Lambda 3He, Lambda 4He, and Lambda Lambda 4He, are calculated in the limit of flavor-SU(3) symmetry at the physical strange quark mass with quantum chromodynamics (without electromagnetic interactions). The nuclear states are extracted from Lattice QCD calculations performed with n_f=3 dynamical light quarks using an isotropic clover discretization of the quark-action in three lattice volumes of spatial extent L ~ 3.4 fm, 4.5 fm and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.5219","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":"1206.5219","created_at":"2026-05-18T03:31:17.612957+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.5219v2","created_at":"2026-05-18T03:31:17.612957+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.5219","created_at":"2026-05-18T03:31:17.612957+00:00"},{"alias_kind":"pith_short_12","alias_value":"XDG2KFEYB5DX","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_16","alias_value":"XDG2KFEYB5DX6YP3","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_8","alias_value":"XDG2KFEY","created_at":"2026-05-18T12:27:27.928770+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2508.15912","citing_title":"$f$-mode Oscillations for Hyperons and H-dibaryons in Neutron Stars","ref_index":87,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16977","citing_title":"Two-nucleon systems at $m_{\\pi}\\approx292$ MeV from lattice QCD","ref_index":7,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ","json":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ.json","graph_json":"https://pith.science/api/pith-number/XDG2KFEYB5DX6YP3DNBDXVCCKQ/graph.json","events_json":"https://pith.science/api/pith-number/XDG2KFEYB5DX6YP3DNBDXVCCKQ/events.json","paper":"https://pith.science/paper/XDG2KFEY"},"agent_actions":{"view_html":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ","download_json":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ.json","view_paper":"https://pith.science/paper/XDG2KFEY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.5219&json=true","fetch_graph":"https://pith.science/api/pith-number/XDG2KFEYB5DX6YP3DNBDXVCCKQ/graph.json","fetch_events":"https://pith.science/api/pith-number/XDG2KFEYB5DX6YP3DNBDXVCCKQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ/action/storage_attestation","attest_author":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ/action/author_attestation","sign_citation":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ/action/citation_signature","submit_replication":"https://pith.science/pith/XDG2KFEYB5DX6YP3DNBDXVCCKQ/action/replication_record"}},"created_at":"2026-05-18T03:31:17.612957+00:00","updated_at":"2026-05-18T03:31:17.612957+00:00"}