{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:C525M56BPOI7OALD6RO5UPVNGH","short_pith_number":"pith:C525M56B","canonical_record":{"source":{"id":"nucl-th/0006020","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2000-06-12T21:15:19Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"2f5269ebf02ea3c5eaf1ed07c8c9c421b9ce35eb810e430ccbf7cc5d2e0b308b","abstract_canon_sha256":"fd9a0b705f5d57e6581e5709fcc1df1ec1b0ed8f9da910b5f5b583cbe79357b3"},"schema_version":"1.0"},"canonical_sha256":"1775d677c17b91f70163f45dda3ead31d6b08080c1e728d173b0b8781cb303d6","source":{"kind":"arxiv","id":"nucl-th/0006020","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0006020","created_at":"2026-05-18T00:36:53Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0006020v2","created_at":"2026-05-18T00:36:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0006020","created_at":"2026-05-18T00:36:53Z"},{"alias_kind":"pith_short_12","alias_value":"C525M56BPOI7","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"C525M56BPOI7OALD","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"C525M56B","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:C525M56BPOI7OALD6RO5UPVNGH","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0006020","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2000-06-12T21:15:19Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"2f5269ebf02ea3c5eaf1ed07c8c9c421b9ce35eb810e430ccbf7cc5d2e0b308b","abstract_canon_sha256":"fd9a0b705f5d57e6581e5709fcc1df1ec1b0ed8f9da910b5f5b583cbe79357b3"},"schema_version":"1.0"},"canonical_sha256":"1775d677c17b91f70163f45dda3ead31d6b08080c1e728d173b0b8781cb303d6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:53.170490Z","signature_b64":"RwxTzz7oi1lI8FIthv5j5a0UyyegnaOUf4ZAS1R6FQPy9+Vu85AkRQPVsEVh+JmRgh/1f0lIBAb/jiLoIaz2DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1775d677c17b91f70163f45dda3ead31d6b08080c1e728d173b0b8781cb303d6","last_reissued_at":"2026-05-18T00:36:53.169989Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:53.169989Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0006020","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":"2026-05-18T00:36:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Yr1W4YBl5jOIZguy1nBlsdEDX63oAOgFV9JNqZO/jKjX4xBR32lA9/hOz5U2RXfVCkX0Ed8Af08UpWl8EJUmCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T13:11:32.009553Z"},"content_sha256":"76c07940f60b5a07427cfba8b493a4f4e40c25894b2430490d13430bc305e9a5","schema_version":"1.0","event_id":"sha256:76c07940f60b5a07427cfba8b493a4f4e40c25894b2430490d13430bc305e9a5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:C525M56BPOI7OALD6RO5UPVNGH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lattice Gauge Theory - QCD from Quarks to Hadrons","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"nucl-th","authors_text":"D.G. Richards (Old Dominion University, Jefferson Laboratory)","submitted_at":"2000-06-12T21:15:19Z","abstract_excerpt":"Lattice Gauge Theory enables an ab initio study of the low-energy properties of Quantum Chromodynamics, the theory of the strong interaction. I begin these lectures by presenting the lattice formulation of QCD, and then outline the benchmark calculation of lattice QCD, the light-hadron spectrum. I then proceed to explore the predictive power of lattice QCD, in particular as it pertains to hadronic physics. I will discuss the spectrum of glueballs, exotics and excited states, before investigating the study of form factors and structure functions. I will conclude by showing how lattice QCD can b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0006020","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":"2026-05-18T00:36:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"azkbtWnDml/al9sC6TAwveDsDJ6IW0pUWRDBqat8JjFr8Bwd3dO3wTgsGfplkKEPKE20oQMrASmKf5+gch9TDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T13:11:32.009898Z"},"content_sha256":"92ac9b7e6fead53af6b51194aa1ec3797bf89bc8aecb2a3d472e82a89052a8f9","schema_version":"1.0","event_id":"sha256:92ac9b7e6fead53af6b51194aa1ec3797bf89bc8aecb2a3d472e82a89052a8f9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C525M56BPOI7OALD6RO5UPVNGH/bundle.json","state_url":"https://pith.science/pith/C525M56BPOI7OALD6RO5UPVNGH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C525M56BPOI7OALD6RO5UPVNGH/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":"2026-06-29T13:11:32Z","links":{"resolver":"https://pith.science/pith/C525M56BPOI7OALD6RO5UPVNGH","bundle":"https://pith.science/pith/C525M56BPOI7OALD6RO5UPVNGH/bundle.json","state":"https://pith.science/pith/C525M56BPOI7OALD6RO5UPVNGH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C525M56BPOI7OALD6RO5UPVNGH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:C525M56BPOI7OALD6RO5UPVNGH","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":"fd9a0b705f5d57e6581e5709fcc1df1ec1b0ed8f9da910b5f5b583cbe79357b3","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"nucl-th","submitted_at":"2000-06-12T21:15:19Z","title_canon_sha256":"2f5269ebf02ea3c5eaf1ed07c8c9c421b9ce35eb810e430ccbf7cc5d2e0b308b"},"schema_version":"1.0","source":{"id":"nucl-th/0006020","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0006020","created_at":"2026-05-18T00:36:53Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0006020v2","created_at":"2026-05-18T00:36:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0006020","created_at":"2026-05-18T00:36:53Z"},{"alias_kind":"pith_short_12","alias_value":"C525M56BPOI7","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"C525M56BPOI7OALD","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"C525M56B","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:92ac9b7e6fead53af6b51194aa1ec3797bf89bc8aecb2a3d472e82a89052a8f9","target":"graph","created_at":"2026-05-18T00:36:53Z","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":"Lattice Gauge Theory enables an ab initio study of the low-energy properties of Quantum Chromodynamics, the theory of the strong interaction. I begin these lectures by presenting the lattice formulation of QCD, and then outline the benchmark calculation of lattice QCD, the light-hadron spectrum. I then proceed to explore the predictive power of lattice QCD, in particular as it pertains to hadronic physics. I will discuss the spectrum of glueballs, exotics and excited states, before investigating the study of form factors and structure functions. I will conclude by showing how lattice QCD can b","authors_text":"D.G. Richards (Old Dominion University, Jefferson Laboratory)","cross_cats":["hep-lat"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2000-06-12T21:15:19Z","title":"Lattice Gauge Theory - QCD from Quarks to Hadrons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0006020","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":"sha256:76c07940f60b5a07427cfba8b493a4f4e40c25894b2430490d13430bc305e9a5","target":"record","created_at":"2026-05-18T00:36:53Z","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":"fd9a0b705f5d57e6581e5709fcc1df1ec1b0ed8f9da910b5f5b583cbe79357b3","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"nucl-th","submitted_at":"2000-06-12T21:15:19Z","title_canon_sha256":"2f5269ebf02ea3c5eaf1ed07c8c9c421b9ce35eb810e430ccbf7cc5d2e0b308b"},"schema_version":"1.0","source":{"id":"nucl-th/0006020","kind":"arxiv","version":2}},"canonical_sha256":"1775d677c17b91f70163f45dda3ead31d6b08080c1e728d173b0b8781cb303d6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1775d677c17b91f70163f45dda3ead31d6b08080c1e728d173b0b8781cb303d6","first_computed_at":"2026-05-18T00:36:53.169989Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:53.169989Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RwxTzz7oi1lI8FIthv5j5a0UyyegnaOUf4ZAS1R6FQPy9+Vu85AkRQPVsEVh+JmRgh/1f0lIBAb/jiLoIaz2DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:53.170490Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0006020","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:76c07940f60b5a07427cfba8b493a4f4e40c25894b2430490d13430bc305e9a5","sha256:92ac9b7e6fead53af6b51194aa1ec3797bf89bc8aecb2a3d472e82a89052a8f9"],"state_sha256":"7742a25ecc888cbab239e95b8508fbcb1550ae6c196e8662c6b66e57646e3321"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pwRmtKtewEReJcofrWjmaJWygud8mlVjrEs9eYsSoBHQtaBg51FMJMErwFezrZ7xCH9uXpqRooDAG36ZBqMrDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T13:11:32.011917Z","bundle_sha256":"5c0fe8fac0bf356c2cb1d7a5a49ac3b36a912d0e0521a03dfa01361271dfc3b7"}}