{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:GCSJ3IKEYJQ5AWFFCTH47VU2P5","short_pith_number":"pith:GCSJ3IKE","canonical_record":{"source":{"id":"hep-th/0404092","kind":"arxiv","version":5},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-04-13T18:04:55Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"0c80a6a2bc0d884ce7a673762411c4b07365c72e93ea88ef7a377b38601fface","abstract_canon_sha256":"6c8910de7208cff336902fb82306d3889531f00baa57571f51ab8ba2b7e8eb37"},"schema_version":"1.0"},"canonical_sha256":"30a49da144c261d058a514cfcfd69a7f7cc3255c335a4b71ec665e14f01a2440","source":{"kind":"arxiv","id":"hep-th/0404092","version":5},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0404092","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0404092v5","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0404092","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"pith_short_12","alias_value":"GCSJ3IKEYJQ5","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"GCSJ3IKEYJQ5AWFF","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"GCSJ3IKE","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:GCSJ3IKEYJQ5AWFFCTH47VU2P5","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0404092","kind":"arxiv","version":5},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-04-13T18:04:55Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"0c80a6a2bc0d884ce7a673762411c4b07365c72e93ea88ef7a377b38601fface","abstract_canon_sha256":"6c8910de7208cff336902fb82306d3889531f00baa57571f51ab8ba2b7e8eb37"},"schema_version":"1.0"},"canonical_sha256":"30a49da144c261d058a514cfcfd69a7f7cc3255c335a4b71ec665e14f01a2440","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:58.869691Z","signature_b64":"qnIruPpPe9ca4r+odp7mqo3M8UL+fjB6ibVSc/aSQswNPvZs0dqg7iJTFI9/oGGEUhhF8CYSUxScFAVD5YiECQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30a49da144c261d058a514cfcfd69a7f7cc3255c335a4b71ec665e14f01a2440","last_reissued_at":"2026-05-18T01:05:58.869033Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:58.869033Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0404092","source_version":5,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:05:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"R45gCeuLiNfOeDa4mp3Fu50DJI5e1c1u8nbgbJ3yxhflFVmKvip/GosyhPaKgxxnIqTcRq4fgZTESgOjjWnxBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T01:10:45.417248Z"},"content_sha256":"e6861e69237282e240ee7fdbfe371b38a9c9ab3b562037e686ffdecc10e65d3a","schema_version":"1.0","event_id":"sha256:e6861e69237282e240ee7fdbfe371b38a9c9ab3b562037e686ffdecc10e65d3a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:GCSJ3IKEYJQ5AWFFCTH47VU2P5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Three-loop universal anomalous dimension of the Wilson operators in N=4 SUSY Yang-Mills model","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"A.I. Onishchenko (Wayne State U. & Moscow, A.V. Kotikov (Dubna, INP), ITEP), JINR), L.N. Lipatov (St. Petersburg, V.N. Velizhanin (St. Petersburg","submitted_at":"2004-04-13T18:04:55Z","abstract_excerpt":"We present results for the three-loop universal anomalous dimension of Wilson twist-2 operators in the N=4 Supersymmetric Yang-Mills model. These results are obtained by extracting the most complicated contributions from the three loop non-singlet anomalous dimensions in QCD which were calculated recently. Their singularities at j=1 agree with the predictions obtained from the BFKL equation for N=4 SYM in the next-to-leading order. The asymptotics of universal anomalous dimension at large j is in an agreement with the expectations based on an interpolation between weak and strong coupling regi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0404092","kind":"arxiv","version":5},"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":"2026-05-18T01:05:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KI0+SSSXppsn35sd/RSHEOTpIo3qzmqUHJfqtau80M2Cq2nrD5fsRbhE059RovnjpSbPArjoaj+/BS3317HHCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T01:10:45.417620Z"},"content_sha256":"6c8c9194cf0ff864db3c7c3dbf3ca64abc2c017cb651cf459571eb2eb6aa631d","schema_version":"1.0","event_id":"sha256:6c8c9194cf0ff864db3c7c3dbf3ca64abc2c017cb651cf459571eb2eb6aa631d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5/bundle.json","state_url":"https://pith.science/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5/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":"2026-06-04T01:10:45Z","links":{"resolver":"https://pith.science/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5","bundle":"https://pith.science/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5/bundle.json","state":"https://pith.science/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GCSJ3IKEYJQ5AWFFCTH47VU2P5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:GCSJ3IKEYJQ5AWFFCTH47VU2P5","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":"6c8910de7208cff336902fb82306d3889531f00baa57571f51ab8ba2b7e8eb37","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2004-04-13T18:04:55Z","title_canon_sha256":"0c80a6a2bc0d884ce7a673762411c4b07365c72e93ea88ef7a377b38601fface"},"schema_version":"1.0","source":{"id":"hep-th/0404092","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0404092","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0404092v5","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0404092","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"pith_short_12","alias_value":"GCSJ3IKEYJQ5","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"GCSJ3IKEYJQ5AWFF","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"GCSJ3IKE","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:6c8c9194cf0ff864db3c7c3dbf3ca64abc2c017cb651cf459571eb2eb6aa631d","target":"graph","created_at":"2026-05-18T01:05:58Z","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":"We present results for the three-loop universal anomalous dimension of Wilson twist-2 operators in the N=4 Supersymmetric Yang-Mills model. These results are obtained by extracting the most complicated contributions from the three loop non-singlet anomalous dimensions in QCD which were calculated recently. Their singularities at j=1 agree with the predictions obtained from the BFKL equation for N=4 SYM in the next-to-leading order. The asymptotics of universal anomalous dimension at large j is in an agreement with the expectations based on an interpolation between weak and strong coupling regi","authors_text":"A.I. Onishchenko (Wayne State U. & Moscow, A.V. Kotikov (Dubna, INP), ITEP), JINR), L.N. Lipatov (St. Petersburg, V.N. Velizhanin (St. Petersburg","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2004-04-13T18:04:55Z","title":"Three-loop universal anomalous dimension of the Wilson operators in N=4 SUSY Yang-Mills model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0404092","kind":"arxiv","version":5},"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:e6861e69237282e240ee7fdbfe371b38a9c9ab3b562037e686ffdecc10e65d3a","target":"record","created_at":"2026-05-18T01:05:58Z","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":"6c8910de7208cff336902fb82306d3889531f00baa57571f51ab8ba2b7e8eb37","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2004-04-13T18:04:55Z","title_canon_sha256":"0c80a6a2bc0d884ce7a673762411c4b07365c72e93ea88ef7a377b38601fface"},"schema_version":"1.0","source":{"id":"hep-th/0404092","kind":"arxiv","version":5}},"canonical_sha256":"30a49da144c261d058a514cfcfd69a7f7cc3255c335a4b71ec665e14f01a2440","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"30a49da144c261d058a514cfcfd69a7f7cc3255c335a4b71ec665e14f01a2440","first_computed_at":"2026-05-18T01:05:58.869033Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:05:58.869033Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qnIruPpPe9ca4r+odp7mqo3M8UL+fjB6ibVSc/aSQswNPvZs0dqg7iJTFI9/oGGEUhhF8CYSUxScFAVD5YiECQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:05:58.869691Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0404092","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e6861e69237282e240ee7fdbfe371b38a9c9ab3b562037e686ffdecc10e65d3a","sha256:6c8c9194cf0ff864db3c7c3dbf3ca64abc2c017cb651cf459571eb2eb6aa631d"],"state_sha256":"115fc6f61708d89d24f45535a9ae9b85fb855d517c67454cefd1c15fac464b19"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KTre2SHJdHQUcgrEmIDh/z91FHNGMeu3+B8H4+4cP93FQUuSY4gF4cFFEgTXBqC+sbqAm/nHYVR46x2u6Kq1Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T01:10:45.419580Z","bundle_sha256":"2a02293d88588ee039dac9d9d1e7c2a157c9130d3c220a7b921e736c25bc95e5"}}