{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:TKSTSL5JUSLWMBGWLWH3V25BED","short_pith_number":"pith:TKSTSL5J","canonical_record":{"source":{"id":"1409.8330","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-29T21:19:46Z","cross_cats_sorted":[],"title_canon_sha256":"4de7f29b7a89826d9ff7239ed32cb305b38af70a04b87a0422e1aab63c02378f","abstract_canon_sha256":"fbf589bdfdca8eb6d6d5342ea6a06d59d063cd4472ade35697db90bcaf05921a"},"schema_version":"1.0"},"canonical_sha256":"9aa5392fa9a4976604d65d8fbaeba120c1708a794f0842c020190f7de20d238b","source":{"kind":"arxiv","id":"1409.8330","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.8330","created_at":"2026-05-18T01:41:54Z"},{"alias_kind":"arxiv_version","alias_value":"1409.8330v1","created_at":"2026-05-18T01:41:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.8330","created_at":"2026-05-18T01:41:54Z"},{"alias_kind":"pith_short_12","alias_value":"TKSTSL5JUSLW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"TKSTSL5JUSLWMBGW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"TKSTSL5J","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:TKSTSL5JUSLWMBGWLWH3V25BED","target":"record","payload":{"canonical_record":{"source":{"id":"1409.8330","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-29T21:19:46Z","cross_cats_sorted":[],"title_canon_sha256":"4de7f29b7a89826d9ff7239ed32cb305b38af70a04b87a0422e1aab63c02378f","abstract_canon_sha256":"fbf589bdfdca8eb6d6d5342ea6a06d59d063cd4472ade35697db90bcaf05921a"},"schema_version":"1.0"},"canonical_sha256":"9aa5392fa9a4976604d65d8fbaeba120c1708a794f0842c020190f7de20d238b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:54.208697Z","signature_b64":"aVq2F+kPu5biTqCs7LV1r2ej6ulNL7P6ixS+cGFTJX3d1WBUKZ4zSnGNWXwoxOS0u79K+i08wOf9bsEXO/aDAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9aa5392fa9a4976604d65d8fbaeba120c1708a794f0842c020190f7de20d238b","last_reissued_at":"2026-05-18T01:41:54.208227Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:54.208227Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.8330","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:41:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Pwz23ESqz3wp/7ceTRE6bmT3t2GMXqM1/GBc2TKffKMV0YVUwATCN2SIoDo/pxPg+Y4GskLclIm2jfqhXtpvAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T17:37:57.803745Z"},"content_sha256":"1b7de899ecea2c9bc7d29bfe59e2cf288fa508595fbe1cdf8c418117f7c52bf7","schema_version":"1.0","event_id":"sha256:1b7de899ecea2c9bc7d29bfe59e2cf288fa508595fbe1cdf8c418117f7c52bf7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:TKSTSL5JUSLWMBGWLWH3V25BED","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analyzing high-energy factorization beyond next-to-leading logarithmic accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giulio Falcioni, Leonardo Vernazza, Lorenzo Magnea, Vittorio Del Duca","submitted_at":"2014-09-29T21:19:46Z","abstract_excerpt":"We provide a complete and detailed study of the high-energy limit of four-parton scattering amplitudes in QCD, giving explicit results at two loops and higher orders, and going beyond next-to-leading logarithmic (NLL) accuracy. Building upon recent results, we use the techniques of infrared factorization to investigate the failure of the simplest form of Regge factorization, starting at next-to-next-to-leading logarithmic accuracy (NNLL) in ln(s/|t|). We provide detailed accounts and explicit expressions for the terms responsible for this breaking in the case of two-loop and three-loop quark a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.8330","kind":"arxiv","version":1},"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":"2026-05-18T01:41:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aVFCv3ETMP4HkMRu5cNfxYIrVsWXUHUvRSMTialricaoOCgEvnESv3i/OVnOGkjWp+7stBLCi4O9EitMOcRNBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T17:37:57.804121Z"},"content_sha256":"996cd407bce91779a95df69fcc482790658df508b4d9aed6109fae6d5e638467","schema_version":"1.0","event_id":"sha256:996cd407bce91779a95df69fcc482790658df508b4d9aed6109fae6d5e638467"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TKSTSL5JUSLWMBGWLWH3V25BED/bundle.json","state_url":"https://pith.science/pith/TKSTSL5JUSLWMBGWLWH3V25BED/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TKSTSL5JUSLWMBGWLWH3V25BED/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":"2026-06-05T17:37:57Z","links":{"resolver":"https://pith.science/pith/TKSTSL5JUSLWMBGWLWH3V25BED","bundle":"https://pith.science/pith/TKSTSL5JUSLWMBGWLWH3V25BED/bundle.json","state":"https://pith.science/pith/TKSTSL5JUSLWMBGWLWH3V25BED/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TKSTSL5JUSLWMBGWLWH3V25BED/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:TKSTSL5JUSLWMBGWLWH3V25BED","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":"fbf589bdfdca8eb6d6d5342ea6a06d59d063cd4472ade35697db90bcaf05921a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-29T21:19:46Z","title_canon_sha256":"4de7f29b7a89826d9ff7239ed32cb305b38af70a04b87a0422e1aab63c02378f"},"schema_version":"1.0","source":{"id":"1409.8330","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.8330","created_at":"2026-05-18T01:41:54Z"},{"alias_kind":"arxiv_version","alias_value":"1409.8330v1","created_at":"2026-05-18T01:41:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.8330","created_at":"2026-05-18T01:41:54Z"},{"alias_kind":"pith_short_12","alias_value":"TKSTSL5JUSLW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"TKSTSL5JUSLWMBGW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"TKSTSL5J","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:996cd407bce91779a95df69fcc482790658df508b4d9aed6109fae6d5e638467","target":"graph","created_at":"2026-05-18T01:41:54Z","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 provide a complete and detailed study of the high-energy limit of four-parton scattering amplitudes in QCD, giving explicit results at two loops and higher orders, and going beyond next-to-leading logarithmic (NLL) accuracy. Building upon recent results, we use the techniques of infrared factorization to investigate the failure of the simplest form of Regge factorization, starting at next-to-next-to-leading logarithmic accuracy (NNLL) in ln(s/|t|). We provide detailed accounts and explicit expressions for the terms responsible for this breaking in the case of two-loop and three-loop quark a","authors_text":"Giulio Falcioni, Leonardo Vernazza, Lorenzo Magnea, Vittorio Del Duca","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-29T21:19:46Z","title":"Analyzing high-energy factorization beyond next-to-leading logarithmic accuracy"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.8330","kind":"arxiv","version":1},"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":"sha256:1b7de899ecea2c9bc7d29bfe59e2cf288fa508595fbe1cdf8c418117f7c52bf7","target":"record","created_at":"2026-05-18T01:41:54Z","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":"fbf589bdfdca8eb6d6d5342ea6a06d59d063cd4472ade35697db90bcaf05921a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-29T21:19:46Z","title_canon_sha256":"4de7f29b7a89826d9ff7239ed32cb305b38af70a04b87a0422e1aab63c02378f"},"schema_version":"1.0","source":{"id":"1409.8330","kind":"arxiv","version":1}},"canonical_sha256":"9aa5392fa9a4976604d65d8fbaeba120c1708a794f0842c020190f7de20d238b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9aa5392fa9a4976604d65d8fbaeba120c1708a794f0842c020190f7de20d238b","first_computed_at":"2026-05-18T01:41:54.208227Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:54.208227Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aVq2F+kPu5biTqCs7LV1r2ej6ulNL7P6ixS+cGFTJX3d1WBUKZ4zSnGNWXwoxOS0u79K+i08wOf9bsEXO/aDAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:54.208697Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.8330","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1b7de899ecea2c9bc7d29bfe59e2cf288fa508595fbe1cdf8c418117f7c52bf7","sha256:996cd407bce91779a95df69fcc482790658df508b4d9aed6109fae6d5e638467"],"state_sha256":"a01e737c191766c601ca46f409bb28ef7476c59d887ec1e2a54dd26ecf498079"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0OecCehILI5M3KKgqlnHd9Jke0ILtLnhZdZZNb1CDSehWiKIoEfn5RAMSnsFeWxOgKRWULk2HfMtgkBxR6ZeDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T17:37:57.806088Z","bundle_sha256":"872a510ba9f0042e8e6af7bbc37a2c8068e241dc73fe94f425e28d6f235adde4"}}