{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:5E5EWLWVSORRLERZICDSRXMAK3","short_pith_number":"pith:5E5EWLWV","schema_version":"1.0","canonical_sha256":"e93a4b2ed593a3159239408728dd8056d8bdbbbb5cf010786d6231a4a563c3f2","source":{"kind":"arxiv","id":"1302.2987","version":2},"attestation_state":"computed","paper":{"title":"Structure and Flow of the Nucleon Eigenstates in Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Anthony G. Williams, Derek B. Leinweber, M. Selim Mahbub, Peter J. Moran, Waseem Kamleh","submitted_at":"2013-02-13T06:02:53Z","abstract_excerpt":"A determination of the excited energy eigenstates of the nucleon, $s=c{1}{2}$, $I={1}{2}$, $N^{\\pm}$, is presented in full QCD using 2+1 flavor PACS-CS gauge configurations. The correlation-matrix method is used and is built using standard nucleon interpolators employing smearings at the fermion sources and sinks. We develop and demonstrate a new technique that allows the eigenvectors obtained to be utilized to track the propagation of the intrinsic nature of energy-states from one quark mass to the next. This approach is particularly useful for larger dimension correlation matrices where more"},"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":"1302.2987","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-02-13T06:02:53Z","cross_cats_sorted":[],"title_canon_sha256":"9ee8518a9fe4eae2636f08fe3fd4134cd144159d033cb07c04e120e9492b5a83","abstract_canon_sha256":"f41a8538db9a4474af1a08ca67520e6d4d9c39bb5958ddc42b02b13f62735df7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:19:59.051716Z","signature_b64":"Tthitxufh0DRNHkHYLXOTMAxuQM9C8wIyMOdMaYodbRmfl1fe9E98xJmQYCOeehKis9PfwR08LUV+NYkVnskDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e93a4b2ed593a3159239408728dd8056d8bdbbbb5cf010786d6231a4a563c3f2","last_reissued_at":"2026-05-18T03:19:59.051154Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:19:59.051154Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Structure and Flow of the Nucleon Eigenstates in Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Anthony G. Williams, Derek B. Leinweber, M. Selim Mahbub, Peter J. Moran, Waseem Kamleh","submitted_at":"2013-02-13T06:02:53Z","abstract_excerpt":"A determination of the excited energy eigenstates of the nucleon, $s=c{1}{2}$, $I={1}{2}$, $N^{\\pm}$, is presented in full QCD using 2+1 flavor PACS-CS gauge configurations. The correlation-matrix method is used and is built using standard nucleon interpolators employing smearings at the fermion sources and sinks. We develop and demonstrate a new technique that allows the eigenvectors obtained to be utilized to track the propagation of the intrinsic nature of energy-states from one quark mass to the next. This approach is particularly useful for larger dimension correlation matrices where more"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.2987","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":"1302.2987","created_at":"2026-05-18T03:19:59.051251+00:00"},{"alias_kind":"arxiv_version","alias_value":"1302.2987v2","created_at":"2026-05-18T03:19:59.051251+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.2987","created_at":"2026-05-18T03:19:59.051251+00:00"},{"alias_kind":"pith_short_12","alias_value":"5E5EWLWVSORR","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_16","alias_value":"5E5EWLWVSORRLERZ","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_8","alias_value":"5E5EWLWV","created_at":"2026-05-18T12:27:34.582898+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.10038","citing_title":"Understanding the structure of nucleon excitations from their wavefunctions","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3","json":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3.json","graph_json":"https://pith.science/api/pith-number/5E5EWLWVSORRLERZICDSRXMAK3/graph.json","events_json":"https://pith.science/api/pith-number/5E5EWLWVSORRLERZICDSRXMAK3/events.json","paper":"https://pith.science/paper/5E5EWLWV"},"agent_actions":{"view_html":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3","download_json":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3.json","view_paper":"https://pith.science/paper/5E5EWLWV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1302.2987&json=true","fetch_graph":"https://pith.science/api/pith-number/5E5EWLWVSORRLERZICDSRXMAK3/graph.json","fetch_events":"https://pith.science/api/pith-number/5E5EWLWVSORRLERZICDSRXMAK3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3/action/storage_attestation","attest_author":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3/action/author_attestation","sign_citation":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3/action/citation_signature","submit_replication":"https://pith.science/pith/5E5EWLWVSORRLERZICDSRXMAK3/action/replication_record"}},"created_at":"2026-05-18T03:19:59.051251+00:00","updated_at":"2026-05-18T03:19:59.051251+00:00"}