{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:2HNODWKZIP5VGEBWQ2VHX275GZ","short_pith_number":"pith:2HNODWKZ","canonical_record":{"source":{"id":"hep-ph/0107029","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-04T00:44:30Z","cross_cats_sorted":[],"title_canon_sha256":"a593599068894bb697737fa92065b4d5563398a9cd21c9aca0f279d66ae37145","abstract_canon_sha256":"828dda0c00b9dfd5e3622d2f4c9098dc10cf3cfd8d2fa453b2b8b594c8d4cf53"},"schema_version":"1.0"},"canonical_sha256":"d1dae1d95943fb53103686aa7bebfd3653266f08b06689a6cbbe96b7bde6e49f","source":{"kind":"arxiv","id":"hep-ph/0107029","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0107029","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0107029v2","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0107029","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"pith_short_12","alias_value":"2HNODWKZIP5V","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"2HNODWKZIP5VGEBW","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"2HNODWKZ","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:2HNODWKZIP5VGEBWQ2VHX275GZ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0107029","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-04T00:44:30Z","cross_cats_sorted":[],"title_canon_sha256":"a593599068894bb697737fa92065b4d5563398a9cd21c9aca0f279d66ae37145","abstract_canon_sha256":"828dda0c00b9dfd5e3622d2f4c9098dc10cf3cfd8d2fa453b2b8b594c8d4cf53"},"schema_version":"1.0"},"canonical_sha256":"d1dae1d95943fb53103686aa7bebfd3653266f08b06689a6cbbe96b7bde6e49f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:57.325212Z","signature_b64":"rdASK1ZOfhoYWogrbhRUPTtLm+TIahLWcCZU1JLtwgoVe1EoTCf8ohYHhNlbrGBLKDZ0l1plVubCXzk2lRAeDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1dae1d95943fb53103686aa7bebfd3653266f08b06689a6cbbe96b7bde6e49f","last_reissued_at":"2026-05-18T00:36:57.324776Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:57.324776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0107029","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":"2026-05-18T00:36:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T1qdftvIjStoFsxjX5tbAhYNpK8O7N2S7XDqL9DhMFQK6Mzcz49AOEGPdEfMHCZO+2slc3wjDXOUXuY3kENEDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T00:28:24.632347Z"},"content_sha256":"9f584719779cb1b169b062d734abdc240b8dd21da092b74fe208d1969d51cb56","schema_version":"1.0","event_id":"sha256:9f584719779cb1b169b062d734abdc240b8dd21da092b74fe208d1969d51cb56"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:2HNODWKZIP5VGEBWQ2VHX275GZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gluons, quarks, and the transition from nonperturbative to perturbative QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anthony G. Williams, Derek B. Leinweber, Frederic D.R. Bonnet, James M. Zanotti, Jon Ivar Skullerud, Patrick O. Bowman","submitted_at":"2001-07-04T00:44:30Z","abstract_excerpt":"Lattice-based investigations of two fundamental QCD quantities are described, namely the gluon and quark propagators in Landau gauge. We have studied the Landau gauge gluon propagator using a variety of lattices with spacings from a = 0.17 to 0.41 fm. We demonstrate that it is possible to obtain scaling behavior over a very wide range of momenta and lattice spacings and to explore the infinite volume and continuum limits. These results confirm that the Landau gauge gluon propagator is infrared finite. We study the Landau gauge quark propagator in quenched QCD using two forms of the O(a)-improv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0107029","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":"2026-05-18T00:36:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IAG/jcnMu/RcmNakkb1uTtb8OImv+E7eWizPaZ2pPRLeqosp/qlj0t1PN4vcQ+LE1Q2AYGUxEY9kgJ0HnbWbCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T00:28:24.633051Z"},"content_sha256":"dc30740ccc01d463fdd5ce795f2e6c059eca954aac63aa87b1c1885d89f85365","schema_version":"1.0","event_id":"sha256:dc30740ccc01d463fdd5ce795f2e6c059eca954aac63aa87b1c1885d89f85365"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2HNODWKZIP5VGEBWQ2VHX275GZ/bundle.json","state_url":"https://pith.science/pith/2HNODWKZIP5VGEBWQ2VHX275GZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2HNODWKZIP5VGEBWQ2VHX275GZ/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":"2026-05-27T00:28:24Z","links":{"resolver":"https://pith.science/pith/2HNODWKZIP5VGEBWQ2VHX275GZ","bundle":"https://pith.science/pith/2HNODWKZIP5VGEBWQ2VHX275GZ/bundle.json","state":"https://pith.science/pith/2HNODWKZIP5VGEBWQ2VHX275GZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2HNODWKZIP5VGEBWQ2VHX275GZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:2HNODWKZIP5VGEBWQ2VHX275GZ","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":"828dda0c00b9dfd5e3622d2f4c9098dc10cf3cfd8d2fa453b2b8b594c8d4cf53","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-04T00:44:30Z","title_canon_sha256":"a593599068894bb697737fa92065b4d5563398a9cd21c9aca0f279d66ae37145"},"schema_version":"1.0","source":{"id":"hep-ph/0107029","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0107029","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0107029v2","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0107029","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"pith_short_12","alias_value":"2HNODWKZIP5V","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"2HNODWKZIP5VGEBW","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"2HNODWKZ","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:dc30740ccc01d463fdd5ce795f2e6c059eca954aac63aa87b1c1885d89f85365","target":"graph","created_at":"2026-05-18T00:36:57Z","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-based investigations of two fundamental QCD quantities are described, namely the gluon and quark propagators in Landau gauge. We have studied the Landau gauge gluon propagator using a variety of lattices with spacings from a = 0.17 to 0.41 fm. We demonstrate that it is possible to obtain scaling behavior over a very wide range of momenta and lattice spacings and to explore the infinite volume and continuum limits. These results confirm that the Landau gauge gluon propagator is infrared finite. We study the Landau gauge quark propagator in quenched QCD using two forms of the O(a)-improv","authors_text":"Anthony G. Williams, Derek B. Leinweber, Frederic D.R. Bonnet, James M. Zanotti, Jon Ivar Skullerud, Patrick O. Bowman","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2001-07-04T00:44:30Z","title":"Gluons, quarks, and the transition from nonperturbative to perturbative QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0107029","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":"sha256:9f584719779cb1b169b062d734abdc240b8dd21da092b74fe208d1969d51cb56","target":"record","created_at":"2026-05-18T00:36:57Z","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":"828dda0c00b9dfd5e3622d2f4c9098dc10cf3cfd8d2fa453b2b8b594c8d4cf53","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-04T00:44:30Z","title_canon_sha256":"a593599068894bb697737fa92065b4d5563398a9cd21c9aca0f279d66ae37145"},"schema_version":"1.0","source":{"id":"hep-ph/0107029","kind":"arxiv","version":2}},"canonical_sha256":"d1dae1d95943fb53103686aa7bebfd3653266f08b06689a6cbbe96b7bde6e49f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d1dae1d95943fb53103686aa7bebfd3653266f08b06689a6cbbe96b7bde6e49f","first_computed_at":"2026-05-18T00:36:57.324776Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:57.324776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rdASK1ZOfhoYWogrbhRUPTtLm+TIahLWcCZU1JLtwgoVe1EoTCf8ohYHhNlbrGBLKDZ0l1plVubCXzk2lRAeDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:57.325212Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0107029","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9f584719779cb1b169b062d734abdc240b8dd21da092b74fe208d1969d51cb56","sha256:dc30740ccc01d463fdd5ce795f2e6c059eca954aac63aa87b1c1885d89f85365"],"state_sha256":"3786de20c11befdbb3b0be66258824e521fd7d422922eff82085101e357b8c49"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RRbFak1XuqT7ajqYOgSVKYYWu/LUl3b8XTpX1e7DPHmOj9RTmgQX1ykfs0t0UHpe+o/i4vJDGIIgJW+XceKuAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T00:28:24.636903Z","bundle_sha256":"0dc301e62465e2a447c8ff94e46534a25bc99dd14319a2f4039c20be1ab54e4a"}}