{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:XWMLKLVIKICANTICD33VPNSOSR","short_pith_number":"pith:XWMLKLVI","canonical_record":{"source":{"id":"1011.1509","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2010-11-05T20:51:12Z","cross_cats_sorted":[],"title_canon_sha256":"3b649ef8888f0ed5de09c4dcf8b7eb57735243721b431a99f6cdc5c680e93059","abstract_canon_sha256":"4bd82f51ce7e3646d18ec0a46ba21cc825dd71d77e4cf81c06994ef149d9db37"},"schema_version":"1.0"},"canonical_sha256":"bd98b52ea8520406cd021ef757b64e945880904fde5250fcff04991caf1bbac9","source":{"kind":"arxiv","id":"1011.1509","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.1509","created_at":"2026-05-18T02:23:37Z"},{"alias_kind":"arxiv_version","alias_value":"1011.1509v1","created_at":"2026-05-18T02:23:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.1509","created_at":"2026-05-18T02:23:37Z"},{"alias_kind":"pith_short_12","alias_value":"XWMLKLVIKICA","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_16","alias_value":"XWMLKLVIKICANTIC","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_8","alias_value":"XWMLKLVI","created_at":"2026-05-18T12:26:17Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:XWMLKLVIKICANTICD33VPNSOSR","target":"record","payload":{"canonical_record":{"source":{"id":"1011.1509","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2010-11-05T20:51:12Z","cross_cats_sorted":[],"title_canon_sha256":"3b649ef8888f0ed5de09c4dcf8b7eb57735243721b431a99f6cdc5c680e93059","abstract_canon_sha256":"4bd82f51ce7e3646d18ec0a46ba21cc825dd71d77e4cf81c06994ef149d9db37"},"schema_version":"1.0"},"canonical_sha256":"bd98b52ea8520406cd021ef757b64e945880904fde5250fcff04991caf1bbac9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:23:37.490047Z","signature_b64":"AiiWhw/jN2Ic1aS2w2X9QfqN2CA7Ka9T+Lu6DhKZ802ENP3zIcXWKJ8oIR+qSjTezBjnjCM8kB9MUHkA/MasDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd98b52ea8520406cd021ef757b64e945880904fde5250fcff04991caf1bbac9","last_reissued_at":"2026-05-18T02:23:37.489508Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:23:37.489508Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1011.1509","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:23:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VdCPEeKvNf0OxQx2yC0puT9vOuBP6joPvAEFKXMmnLDKYCu4BVXc5acyc6t7FnAsrYJLceJVZ+2GSxTbWhJeDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T05:52:23.284903Z"},"content_sha256":"09fb1e6a9b0e98f23dc815efec4ceffab1d45d5029e6176527dcabbdfb6a12d4","schema_version":"1.0","event_id":"sha256:09fb1e6a9b0e98f23dc815efec4ceffab1d45d5029e6176527dcabbdfb6a12d4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:XWMLKLVIKICANTICD33VPNSOSR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nucleon, Delta and Omega excited state spectra at three pion mass values","license":"http://creativecommons.org/licenses/publicdomain/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"B\\'alint Jo\\'o, Colin Morningstar, David G. Richards, Eric Engelson, Huey-Wen Lin, John Bulava, Robert G. Edwards, Stephen J. Wallace","submitted_at":"2010-11-05T20:51:12Z","abstract_excerpt":"The energies of the excited states of the Nucleon, Delta and Omega are computed in lattice QCD, using two light quarks and one strange quark on anisotropic lattices. The calculations are performed at three values of the pion mass: 392(4), 438(3) and 521(3) MeV. We employ the variational method with a basis of about ten interpolating operators enabling six energies to be distinguished clearly in each irreducible representation of the octahedral group. We compare our calculations of nucleon excited states with the low-lying experimental spectrum. There is reasonable agreement for the pattern of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.1509","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:23:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e5EEq8ih8Yzw8d4jsnp/73eTz/Okmd8iOsXwan79Rdq5plmLmH7I4MF1A5F/APEWkx8zC5lAV7Ddszz+lx68Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T05:52:23.285249Z"},"content_sha256":"7bd5499bd2f055880b9d3d23cbbb0720faf4cbf438a8e594c60316ffd1ca3a50","schema_version":"1.0","event_id":"sha256:7bd5499bd2f055880b9d3d23cbbb0720faf4cbf438a8e594c60316ffd1ca3a50"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XWMLKLVIKICANTICD33VPNSOSR/bundle.json","state_url":"https://pith.science/pith/XWMLKLVIKICANTICD33VPNSOSR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XWMLKLVIKICANTICD33VPNSOSR/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-30T05:52:23Z","links":{"resolver":"https://pith.science/pith/XWMLKLVIKICANTICD33VPNSOSR","bundle":"https://pith.science/pith/XWMLKLVIKICANTICD33VPNSOSR/bundle.json","state":"https://pith.science/pith/XWMLKLVIKICANTICD33VPNSOSR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XWMLKLVIKICANTICD33VPNSOSR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:XWMLKLVIKICANTICD33VPNSOSR","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4bd82f51ce7e3646d18ec0a46ba21cc825dd71d77e4cf81c06994ef149d9db37","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2010-11-05T20:51:12Z","title_canon_sha256":"3b649ef8888f0ed5de09c4dcf8b7eb57735243721b431a99f6cdc5c680e93059"},"schema_version":"1.0","source":{"id":"1011.1509","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.1509","created_at":"2026-05-18T02:23:37Z"},{"alias_kind":"arxiv_version","alias_value":"1011.1509v1","created_at":"2026-05-18T02:23:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.1509","created_at":"2026-05-18T02:23:37Z"},{"alias_kind":"pith_short_12","alias_value":"XWMLKLVIKICA","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_16","alias_value":"XWMLKLVIKICANTIC","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_8","alias_value":"XWMLKLVI","created_at":"2026-05-18T12:26:17Z"}],"graph_snapshots":[{"event_id":"sha256:7bd5499bd2f055880b9d3d23cbbb0720faf4cbf438a8e594c60316ffd1ca3a50","target":"graph","created_at":"2026-05-18T02:23:37Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The energies of the excited states of the Nucleon, Delta and Omega are computed in lattice QCD, using two light quarks and one strange quark on anisotropic lattices. The calculations are performed at three values of the pion mass: 392(4), 438(3) and 521(3) MeV. We employ the variational method with a basis of about ten interpolating operators enabling six energies to be distinguished clearly in each irreducible representation of the octahedral group. We compare our calculations of nucleon excited states with the low-lying experimental spectrum. There is reasonable agreement for the pattern of ","authors_text":"B\\'alint Jo\\'o, Colin Morningstar, David G. Richards, Eric Engelson, Huey-Wen Lin, John Bulava, Robert G. Edwards, Stephen J. Wallace","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2010-11-05T20:51:12Z","title":"Nucleon, Delta and Omega excited state spectra at three pion mass values"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.1509","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:09fb1e6a9b0e98f23dc815efec4ceffab1d45d5029e6176527dcabbdfb6a12d4","target":"record","created_at":"2026-05-18T02:23:37Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4bd82f51ce7e3646d18ec0a46ba21cc825dd71d77e4cf81c06994ef149d9db37","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2010-11-05T20:51:12Z","title_canon_sha256":"3b649ef8888f0ed5de09c4dcf8b7eb57735243721b431a99f6cdc5c680e93059"},"schema_version":"1.0","source":{"id":"1011.1509","kind":"arxiv","version":1}},"canonical_sha256":"bd98b52ea8520406cd021ef757b64e945880904fde5250fcff04991caf1bbac9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bd98b52ea8520406cd021ef757b64e945880904fde5250fcff04991caf1bbac9","first_computed_at":"2026-05-18T02:23:37.489508Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:23:37.489508Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AiiWhw/jN2Ic1aS2w2X9QfqN2CA7Ka9T+Lu6DhKZ802ENP3zIcXWKJ8oIR+qSjTezBjnjCM8kB9MUHkA/MasDw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:23:37.490047Z","signed_message":"canonical_sha256_bytes"},"source_id":"1011.1509","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:09fb1e6a9b0e98f23dc815efec4ceffab1d45d5029e6176527dcabbdfb6a12d4","sha256:7bd5499bd2f055880b9d3d23cbbb0720faf4cbf438a8e594c60316ffd1ca3a50"],"state_sha256":"61deff18479b71b8f7f714a843e9181915f9605412733535d7e26c39694298f6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wIMeTYiODR8Ebt+S//sbx/BxWgx2xwv+H05EG+eXZlmSdZTwjmlpxaouQBUT1ropQJRXGRA9api06hvsK6lmAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T05:52:23.287435Z","bundle_sha256":"e508d8309cfda78940abf8f745d6462e8d4d21d223e74c43aa9159a7b08cc03e"}}