{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:Z36YQ7UBNGPFQQTFWTZWJDM2GD","short_pith_number":"pith:Z36YQ7UB","canonical_record":{"source":{"id":"1307.7022","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-26T12:59:25Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3377f20ff2d04f6b6e4470c3609625ac84c1c9e6f586d9763434d8224d277f9e","abstract_canon_sha256":"fa1a4d3b4bb41299ebf0293ad2293a44a516868229cc9bc8a4a87ed5758013b5"},"schema_version":"1.0"},"canonical_sha256":"cefd887e81699e584265b4f3648d9a30e87430c3325a3b38b78222bfff910160","source":{"kind":"arxiv","id":"1307.7022","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.7022","created_at":"2026-05-18T02:39:01Z"},{"alias_kind":"arxiv_version","alias_value":"1307.7022v2","created_at":"2026-05-18T02:39:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.7022","created_at":"2026-05-18T02:39:01Z"},{"alias_kind":"pith_short_12","alias_value":"Z36YQ7UBNGPF","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"Z36YQ7UBNGPFQQTF","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"Z36YQ7UB","created_at":"2026-05-18T12:28:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:Z36YQ7UBNGPFQQTFWTZWJDM2GD","target":"record","payload":{"canonical_record":{"source":{"id":"1307.7022","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-26T12:59:25Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3377f20ff2d04f6b6e4470c3609625ac84c1c9e6f586d9763434d8224d277f9e","abstract_canon_sha256":"fa1a4d3b4bb41299ebf0293ad2293a44a516868229cc9bc8a4a87ed5758013b5"},"schema_version":"1.0"},"canonical_sha256":"cefd887e81699e584265b4f3648d9a30e87430c3325a3b38b78222bfff910160","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:01.300670Z","signature_b64":"Z/Q1tlZP3U0LIjZ6JbM81uOko06dfbc/MM47+SptwjGX7BgtPuRjuchsDVwn9kS6+ceoUdx+dINoQPwmJwCCAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cefd887e81699e584265b4f3648d9a30e87430c3325a3b38b78222bfff910160","last_reissued_at":"2026-05-18T02:39:01.300071Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:01.300071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1307.7022","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:39:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RK5hJfbPR8ZL1+IQoLN/i9W1409lOVJaJTp0a4PYDcD8tfltYcABss+zNF+3GLkCc88y2edNKcwaXus8zcXODw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:35:50.804904Z"},"content_sha256":"62f785727cc50efa018d730b35c9b45df60444492d21892cc0dce431518a2fb5","schema_version":"1.0","event_id":"sha256:62f785727cc50efa018d730b35c9b45df60444492d21892cc0dce431518a2fb5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:Z36YQ7UBNGPFQQTFWTZWJDM2GD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spectroscopy of triply-charmed baryons from lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Michael Peardon, M. Padmanath, Nilmani Mathur, Robert G. Edwards","submitted_at":"2013-07-26T12:59:25Z","abstract_excerpt":"The spectrum of excitations of triply-charmed baryons is computed using lattice QCD including dynamical light quark fields. Calculations are performed on anisotropic lattices with temporal and spatial spacings a_t = 0.0351(2) and a_s ~ 0.12 fm respectively and with pion mass of about 390 MeV. The spectrum obtained has baryonic states with well-defined total spin up to 7/2 and the low-lying states closely resemble the expectation from models with an SU(6)X O(3) symmetry. Energy splittings between extracted states, including those due to spin-orbit coupling in the heavy quark limit are computed "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.7022","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:39:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XMXH1LAm4nB6k1BqucwfE5z2NQMBKaIBdmhybY9gI+f4cVzMVOjsIaZxOfb6V2oEqG0y1m0gZERIBhJqyD8oAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:35:50.805591Z"},"content_sha256":"3f348a31092f5e950af2ef13ea8fb132776ddc2c98b980a788271cee586059b3","schema_version":"1.0","event_id":"sha256:3f348a31092f5e950af2ef13ea8fb132776ddc2c98b980a788271cee586059b3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD/bundle.json","state_url":"https://pith.science/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD/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":"2026-05-27T21:35:50Z","links":{"resolver":"https://pith.science/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD","bundle":"https://pith.science/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD/bundle.json","state":"https://pith.science/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Z36YQ7UBNGPFQQTFWTZWJDM2GD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:Z36YQ7UBNGPFQQTFWTZWJDM2GD","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":"fa1a4d3b4bb41299ebf0293ad2293a44a516868229cc9bc8a4a87ed5758013b5","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-26T12:59:25Z","title_canon_sha256":"3377f20ff2d04f6b6e4470c3609625ac84c1c9e6f586d9763434d8224d277f9e"},"schema_version":"1.0","source":{"id":"1307.7022","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.7022","created_at":"2026-05-18T02:39:01Z"},{"alias_kind":"arxiv_version","alias_value":"1307.7022v2","created_at":"2026-05-18T02:39:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.7022","created_at":"2026-05-18T02:39:01Z"},{"alias_kind":"pith_short_12","alias_value":"Z36YQ7UBNGPF","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"Z36YQ7UBNGPFQQTF","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"Z36YQ7UB","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:3f348a31092f5e950af2ef13ea8fb132776ddc2c98b980a788271cee586059b3","target":"graph","created_at":"2026-05-18T02:39:01Z","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 spectrum of excitations of triply-charmed baryons is computed using lattice QCD including dynamical light quark fields. Calculations are performed on anisotropic lattices with temporal and spatial spacings a_t = 0.0351(2) and a_s ~ 0.12 fm respectively and with pion mass of about 390 MeV. The spectrum obtained has baryonic states with well-defined total spin up to 7/2 and the low-lying states closely resemble the expectation from models with an SU(6)X O(3) symmetry. Energy splittings between extracted states, including those due to spin-orbit coupling in the heavy quark limit are computed ","authors_text":"Michael Peardon, M. Padmanath, Nilmani Mathur, Robert G. Edwards","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-26T12:59:25Z","title":"Spectroscopy of triply-charmed baryons from lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.7022","kind":"arxiv","version":2},"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":"sha256:62f785727cc50efa018d730b35c9b45df60444492d21892cc0dce431518a2fb5","target":"record","created_at":"2026-05-18T02:39:01Z","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":"fa1a4d3b4bb41299ebf0293ad2293a44a516868229cc9bc8a4a87ed5758013b5","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-26T12:59:25Z","title_canon_sha256":"3377f20ff2d04f6b6e4470c3609625ac84c1c9e6f586d9763434d8224d277f9e"},"schema_version":"1.0","source":{"id":"1307.7022","kind":"arxiv","version":2}},"canonical_sha256":"cefd887e81699e584265b4f3648d9a30e87430c3325a3b38b78222bfff910160","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cefd887e81699e584265b4f3648d9a30e87430c3325a3b38b78222bfff910160","first_computed_at":"2026-05-18T02:39:01.300071Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:39:01.300071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Z/Q1tlZP3U0LIjZ6JbM81uOko06dfbc/MM47+SptwjGX7BgtPuRjuchsDVwn9kS6+ceoUdx+dINoQPwmJwCCAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:39:01.300670Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.7022","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:62f785727cc50efa018d730b35c9b45df60444492d21892cc0dce431518a2fb5","sha256:3f348a31092f5e950af2ef13ea8fb132776ddc2c98b980a788271cee586059b3"],"state_sha256":"a277fb2fe14ed838d269c0592040e60ef4a60d8a4b297fcfe132d05eef759904"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Bc2jTS6NBukOxuqtIZoge7nwoVHXLS5AagH6XT3KSJP47OGm9sbn7Dpdz7DCf+pSaK8tw7r/MIkBJdwHI9sADg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T21:35:50.809083Z","bundle_sha256":"73c057d39a967fd8126ee515cc88286033524df089a8b9b6e7075fc8c204b670"}}