{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:5YIVSENTAXG4AKNR3ZWH6ONNOE","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":"b850338c7076607950c1561b09602595e7fe0bad0ce7ccbaf540f943420be78f","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T15:10:18Z","title_canon_sha256":"86690aa99d61d5c276ec47dd384285a21d044ceebc735de1bb7f2e2d1b9a8f89"},"schema_version":"1.0","source":{"id":"2605.16034","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.16034","created_at":"2026-05-20T00:01:50Z"},{"alias_kind":"arxiv_version","alias_value":"2605.16034v1","created_at":"2026-05-20T00:01:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.16034","created_at":"2026-05-20T00:01:50Z"},{"alias_kind":"pith_short_12","alias_value":"5YIVSENTAXG4","created_at":"2026-05-20T00:01:50Z"},{"alias_kind":"pith_short_16","alias_value":"5YIVSENTAXG4AKNR","created_at":"2026-05-20T00:01:50Z"},{"alias_kind":"pith_short_8","alias_value":"5YIVSENT","created_at":"2026-05-20T00:01:50Z"}],"graph_snapshots":[{"event_id":"sha256:4a6fb05ce14a97f75bbbb4e8b318fc551aa92729dedfe173b7cee5b7c8ca5d27","target":"graph","created_at":"2026-05-20T00:01:50Z","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":[{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T17:33:41.564572Z","status":"skipped","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T16:41:55.540989Z","status":"completed","version":"1.0.0"}],"endpoint":"/pith/2605.16034/integrity.json","findings":[],"snapshot_sha256":"bd2250e60cb73d80ff676c402d0ee3c6e456bb4952b35b57983c95a6fde6a42b","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the Sudakov form factor and the four-point scattering amplitude on the Coulomb branch of planar $\\mathcal{N}=4$ SYM as functions of the Coulomb-branch parameters and kinematic invariants. This setup provides a controlled probe of the interpolation between on- and off-shell regimes of infrared-sensitive quantities in gauge theories. We identify a novel scaling limit in which both observables exhibit double-logarithmic behavior governed by a walking anomalous dimension. As the mass scales are varied, this walking anomalous dimension interpolates between the cusp anomalous dimension of t","authors_text":"Alexander Zhiboedov, Andrei V. Belitsky, Elisabetta Armanini, Kelian H\\\"aring, Luis F. Alday","cross_cats":["hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T15:10:18Z","title":"Walking Sudakov: From Cusp to Octagon"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.16034","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":"sha256:303ea8e824179db2b020e9449c004345c946888823f677c54f289d0dee053f12","target":"record","created_at":"2026-05-20T00:01:50Z","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":"b850338c7076607950c1561b09602595e7fe0bad0ce7ccbaf540f943420be78f","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T15:10:18Z","title_canon_sha256":"86690aa99d61d5c276ec47dd384285a21d044ceebc735de1bb7f2e2d1b9a8f89"},"schema_version":"1.0","source":{"id":"2605.16034","kind":"arxiv","version":1}},"canonical_sha256":"ee115911b305cdc029b1de6c7f39ad710c4882013df6e530a3792631d59c5a6f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ee115911b305cdc029b1de6c7f39ad710c4882013df6e530a3792631d59c5a6f","first_computed_at":"2026-05-20T00:01:50.091907Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:01:50.091907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"i7aGW9xSw6+Xdl5UCyA2e40m3O8DsNl5Bzu7D4oPkwJksozijOCXeeOFxeKafxVJG386rpBi02lMpe3QVuejAg==","signature_status":"signed_v1","signed_at":"2026-05-20T00:01:50.092484Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.16034","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:303ea8e824179db2b020e9449c004345c946888823f677c54f289d0dee053f12","sha256:4a6fb05ce14a97f75bbbb4e8b318fc551aa92729dedfe173b7cee5b7c8ca5d27"],"state_sha256":"c5f45101be0776a33ba38358b0f2c4a06aed6a3e8949a6c45004862d2a7b6ea2"}