{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:X237J7HTCD7NHS77VLHEIS2G7Z","short_pith_number":"pith:X237J7HT","canonical_record":{"source":{"id":"hep-lat/0401033","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-30T17:32:00Z","cross_cats_sorted":[],"title_canon_sha256":"d2d9e5f759095a3abbed4cfcca52245fe2528846d89015005cf8d932c0e6f9b4","abstract_canon_sha256":"549743146f7cbf967878b1999a9ffe7d67263f94f5c0ef1c1592e74b2c8d3971"},"schema_version":"1.0"},"canonical_sha256":"beb7f4fcf310fed3cbffaace444b46fe7d4498346e9f3c6fd6beea6782409937","source":{"kind":"arxiv","id":"hep-lat/0401033","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0401033","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0401033v2","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0401033","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"pith_short_12","alias_value":"X237J7HTCD7N","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"pith_short_16","alias_value":"X237J7HTCD7NHS77","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"pith_short_8","alias_value":"X237J7HT","created_at":"2026-07-04T16:47:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:X237J7HTCD7NHS77VLHEIS2G7Z","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0401033","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-30T17:32:00Z","cross_cats_sorted":[],"title_canon_sha256":"d2d9e5f759095a3abbed4cfcca52245fe2528846d89015005cf8d932c0e6f9b4","abstract_canon_sha256":"549743146f7cbf967878b1999a9ffe7d67263f94f5c0ef1c1592e74b2c8d3971"},"schema_version":"1.0"},"canonical_sha256":"beb7f4fcf310fed3cbffaace444b46fe7d4498346e9f3c6fd6beea6782409937","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:47:59.250184Z","signature_b64":"5P4yyQkpZfP3Qfo54VfS76NIsOEM0qWB4MH/hzAcATd7FimB9VkKHC0Lnv2otJAyN5soSzRZuZ6OTmsy4ZevDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"beb7f4fcf310fed3cbffaace444b46fe7d4498346e9f3c6fd6beea6782409937","last_reissued_at":"2026-07-04T16:47:59.249782Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:47:59.249782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0401033","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":"2026-07-04T16:47:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MgrQDbPqOHm+VYMoL1STZTGz/P/ndgEXxq9bUMSdxKBXNE7odxGGxFZSTnQ7PzghTTR1sjcm/KkiEUfPjJtgDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-14T10:30:46.312068Z"},"content_sha256":"8a5034a8d6bc93e0f4c4ab8f676ea1b4b8c19964caf4739ff8e336b62fa4278c","schema_version":"1.0","event_id":"sha256:8a5034a8d6bc93e0f4c4ab8f676ea1b4b8c19964caf4739ff8e336b62fa4278c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:X237J7HTCD7NHS77VLHEIS2G7Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Renormalization Constants of Quark Operators for the Non-Perturbatively Improved Wilson Action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D.Becirevic, G.Martinelli, J.Reyes, M.Papinutto, V.Gimenez, V.Lubicz","submitted_at":"2004-01-30T17:32:00Z","abstract_excerpt":"We present the results of an extensive lattice calculation of the renormalization constants of bilinear and four-quark operators for the non-perturbatively O(a)-improved Wilson action. The results are obtained in the quenched approximation at four values of the lattice coupling by using the non-perturbative RI/MOM renormalization method. Several sources of systematic uncertainties, including discretization errors and final volume effects, are examined. The contribution of the Goldstone pole, which in some cases may affect the extrapolation of the renormalization constants to the chiral limit, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0401033","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0401033/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T16:47:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VlxBDwesMKObT7+cUiryByZwf7+5ieVibDfJEnA0nS00/JtSB0rzrj4xezMC9R55rUcpLjGKOTMc+VsMvHguDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-14T10:30:46.312465Z"},"content_sha256":"fd8f162038c13a2edef91da3f80a40826c5034afa82a0608b49681c3b689e0db","schema_version":"1.0","event_id":"sha256:fd8f162038c13a2edef91da3f80a40826c5034afa82a0608b49681c3b689e0db"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/X237J7HTCD7NHS77VLHEIS2G7Z/bundle.json","state_url":"https://pith.science/pith/X237J7HTCD7NHS77VLHEIS2G7Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/X237J7HTCD7NHS77VLHEIS2G7Z/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":"2026-07-14T10:30:46Z","links":{"resolver":"https://pith.science/pith/X237J7HTCD7NHS77VLHEIS2G7Z","bundle":"https://pith.science/pith/X237J7HTCD7NHS77VLHEIS2G7Z/bundle.json","state":"https://pith.science/pith/X237J7HTCD7NHS77VLHEIS2G7Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/X237J7HTCD7NHS77VLHEIS2G7Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:X237J7HTCD7NHS77VLHEIS2G7Z","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":"549743146f7cbf967878b1999a9ffe7d67263f94f5c0ef1c1592e74b2c8d3971","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-30T17:32:00Z","title_canon_sha256":"d2d9e5f759095a3abbed4cfcca52245fe2528846d89015005cf8d932c0e6f9b4"},"schema_version":"1.0","source":{"id":"hep-lat/0401033","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0401033","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0401033v2","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0401033","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"pith_short_12","alias_value":"X237J7HTCD7N","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"pith_short_16","alias_value":"X237J7HTCD7NHS77","created_at":"2026-07-04T16:47:59Z"},{"alias_kind":"pith_short_8","alias_value":"X237J7HT","created_at":"2026-07-04T16:47:59Z"}],"graph_snapshots":[{"event_id":"sha256:fd8f162038c13a2edef91da3f80a40826c5034afa82a0608b49681c3b689e0db","target":"graph","created_at":"2026-07-04T16:47:59Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-lat/0401033/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the results of an extensive lattice calculation of the renormalization constants of bilinear and four-quark operators for the non-perturbatively O(a)-improved Wilson action. The results are obtained in the quenched approximation at four values of the lattice coupling by using the non-perturbative RI/MOM renormalization method. Several sources of systematic uncertainties, including discretization errors and final volume effects, are examined. The contribution of the Goldstone pole, which in some cases may affect the extrapolation of the renormalization constants to the chiral limit, ","authors_text":"D.Becirevic, G.Martinelli, J.Reyes, M.Papinutto, V.Gimenez, V.Lubicz","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2004-01-30T17:32:00Z","title":"Renormalization Constants of Quark Operators for the Non-Perturbatively Improved Wilson Action"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0401033","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":"sha256:8a5034a8d6bc93e0f4c4ab8f676ea1b4b8c19964caf4739ff8e336b62fa4278c","target":"record","created_at":"2026-07-04T16:47:59Z","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":"549743146f7cbf967878b1999a9ffe7d67263f94f5c0ef1c1592e74b2c8d3971","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-30T17:32:00Z","title_canon_sha256":"d2d9e5f759095a3abbed4cfcca52245fe2528846d89015005cf8d932c0e6f9b4"},"schema_version":"1.0","source":{"id":"hep-lat/0401033","kind":"arxiv","version":2}},"canonical_sha256":"beb7f4fcf310fed3cbffaace444b46fe7d4498346e9f3c6fd6beea6782409937","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"beb7f4fcf310fed3cbffaace444b46fe7d4498346e9f3c6fd6beea6782409937","first_computed_at":"2026-07-04T16:47:59.249782Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:47:59.249782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5P4yyQkpZfP3Qfo54VfS76NIsOEM0qWB4MH/hzAcATd7FimB9VkKHC0Lnv2otJAyN5soSzRZuZ6OTmsy4ZevDA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:47:59.250184Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0401033","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8a5034a8d6bc93e0f4c4ab8f676ea1b4b8c19964caf4739ff8e336b62fa4278c","sha256:fd8f162038c13a2edef91da3f80a40826c5034afa82a0608b49681c3b689e0db"],"state_sha256":"f9737ba1ebe34a1402d5777848f9aaa9ff16175fe8ad01cf52023b444990a499"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GCG4dkmv4irH5PNrEOr+7u+EwX4lUOUyFu2VbMVpjTPKoHOS58B7c5qZzl+U4EQZlpAsiNRqt136N6f9meZdBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-14T10:30:46.315053Z","bundle_sha256":"101cf345a7e3bc8b6e3a6c19b9ce5414518df4dfeeb6618afc25077674cf7146"}}