{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:TOBYC4SRNFLA77VJF4FRGDU6ZA","short_pith_number":"pith:TOBYC4SR","schema_version":"1.0","canonical_sha256":"9b8381725169560ffea92f0b130e9ec83ee947132854e7309f8aac4420880675","source":{"kind":"arxiv","id":"1410.1384","version":1},"attestation_state":"computed","paper":{"title":"Baryon spin-flavor structure from an analysis of lattice QCD results of the baryon spectrum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Ishara P. Fernando, Jose L. Goity","submitted_at":"2014-10-06T14:24:16Z","abstract_excerpt":"The excited baryon masses are analyzed in the framework of the $1/N_c$ expansion using the available physical masses and also the masses obtained in lattice QCD for different quark masses. The baryon states are organized into irreducible representations of $SU(6)\\times O(3)$, where the $[{\\bf{56}},\\ell^P=0^+]$ ground state and excited baryons, and the $[{\\bf{56}},2^+]$ and $[{\\bf{70}},1^-]$ excited states are analyzed. The analyses are carried out to order 1/Nc and first order in the quark masses. The issue of state identifications is discussed. Numerous parameter independent mass relations re"},"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":"1410.1384","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-10-06T14:24:16Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"8f23adcfa65acdd3c0059335f56a3638ea96e591e047599fa6061feae2ceffdd","abstract_canon_sha256":"603921fbfcdbc706c6e040c512fab2110d7fbb4e34eab9417e72dc4195d9e2b1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:52.210287Z","signature_b64":"fpQL9tddH5Y5v3ceLopkSSk/HkO+VqvT4he8OgUmaQ4RtD9xCWXTI2jTDRUlKqX2oXcwqtIxND2AgCB3d8Y5Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b8381725169560ffea92f0b130e9ec83ee947132854e7309f8aac4420880675","last_reissued_at":"2026-05-18T01:41:52.209594Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:52.209594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon spin-flavor structure from an analysis of lattice QCD results of the baryon spectrum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Ishara P. Fernando, Jose L. Goity","submitted_at":"2014-10-06T14:24:16Z","abstract_excerpt":"The excited baryon masses are analyzed in the framework of the $1/N_c$ expansion using the available physical masses and also the masses obtained in lattice QCD for different quark masses. The baryon states are organized into irreducible representations of $SU(6)\\times O(3)$, where the $[{\\bf{56}},\\ell^P=0^+]$ ground state and excited baryons, and the $[{\\bf{56}},2^+]$ and $[{\\bf{70}},1^-]$ excited states are analyzed. The analyses are carried out to order 1/Nc and first order in the quark masses. The issue of state identifications is discussed. Numerous parameter independent mass relations re"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.1384","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":"1410.1384","created_at":"2026-05-18T01:41:52.209712+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.1384v1","created_at":"2026-05-18T01:41:52.209712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.1384","created_at":"2026-05-18T01:41:52.209712+00:00"},{"alias_kind":"pith_short_12","alias_value":"TOBYC4SRNFLA","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"TOBYC4SRNFLA77VJ","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"TOBYC4SR","created_at":"2026-05-18T12:28:49.207871+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA","json":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA.json","graph_json":"https://pith.science/api/pith-number/TOBYC4SRNFLA77VJF4FRGDU6ZA/graph.json","events_json":"https://pith.science/api/pith-number/TOBYC4SRNFLA77VJF4FRGDU6ZA/events.json","paper":"https://pith.science/paper/TOBYC4SR"},"agent_actions":{"view_html":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA","download_json":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA.json","view_paper":"https://pith.science/paper/TOBYC4SR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.1384&json=true","fetch_graph":"https://pith.science/api/pith-number/TOBYC4SRNFLA77VJF4FRGDU6ZA/graph.json","fetch_events":"https://pith.science/api/pith-number/TOBYC4SRNFLA77VJF4FRGDU6ZA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA/action/storage_attestation","attest_author":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA/action/author_attestation","sign_citation":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA/action/citation_signature","submit_replication":"https://pith.science/pith/TOBYC4SRNFLA77VJF4FRGDU6ZA/action/replication_record"}},"created_at":"2026-05-18T01:41:52.209712+00:00","updated_at":"2026-05-18T01:41:52.209712+00:00"}