{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:Y4HBKFWYLK3GDFKMWEF7W5IKYB","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":"5d5e8c5b3238952df9c447ba6a2c9305179791b9339eba134aa54df1528d03be","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-02-15T18:19:02Z","title_canon_sha256":"1f006d614f791503f5528852c52abbfbd9583989babbe41ea28f6397c94521ba"},"schema_version":"1.0","source":{"id":"2202.07627","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.07627","created_at":"2026-07-05T04:50:53Z"},{"alias_kind":"arxiv_version","alias_value":"2202.07627v2","created_at":"2026-07-05T04:50:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.07627","created_at":"2026-07-05T04:50:53Z"},{"alias_kind":"pith_short_12","alias_value":"Y4HBKFWYLK3G","created_at":"2026-07-05T04:50:53Z"},{"alias_kind":"pith_short_16","alias_value":"Y4HBKFWYLK3GDFKM","created_at":"2026-07-05T04:50:53Z"},{"alias_kind":"pith_short_8","alias_value":"Y4HBKFWY","created_at":"2026-07-05T04:50:53Z"}],"graph_snapshots":[{"event_id":"sha256:7d37e032bcb8547391ada86662603bdcfb8cf81ba80ba3e71685674365c65f8f","target":"graph","created_at":"2026-07-05T04:50:53Z","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/2202.07627/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We continue our study of large charge limits of the defect CFT defined by the half-BPS Wilson loop in planar $\\mathcal{N}=4$ supersymmetric Yang-Mills theory. In this paper, we compute $1/J$ corrections to the correlation function of two heavy insertions of charge $J$ and two light insertions, in the double scaling limit where the charge $J$ and the 't Hooft coupling $\\lambda$ are sent to infinity with the ratio $J/\\sqrt{\\lambda}$ fixed. Holographically, they correspond to quantum fluctuations around a classical string solution with large angular momentum, and can be computed by evaluating Gre","authors_text":"Bendeguz Offertaler, Shota Komatsu, Simone Giombi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-02-15T18:19:02Z","title":"Large Charges on the Wilson Loop in $\\mathcal{N}=4$ SYM: II. Quantum Fluctuations, OPE, and Spectral Curve"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.07627","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":"sha256:1c52cdb77e56e39f78f081cb4ff050ca16f4308b7421a0b392ac7ba3a2c354bc","target":"record","created_at":"2026-07-05T04:50:53Z","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":"5d5e8c5b3238952df9c447ba6a2c9305179791b9339eba134aa54df1528d03be","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-02-15T18:19:02Z","title_canon_sha256":"1f006d614f791503f5528852c52abbfbd9583989babbe41ea28f6397c94521ba"},"schema_version":"1.0","source":{"id":"2202.07627","kind":"arxiv","version":2}},"canonical_sha256":"c70e1516d85ab661954cb10bfb750ac041f979d80b49fe0fd41adce8d2cade0b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c70e1516d85ab661954cb10bfb750ac041f979d80b49fe0fd41adce8d2cade0b","first_computed_at":"2026-07-05T04:50:53.216363Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:50:53.216363Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/flWv4HNXjHA6c2qubPy6OCiYo/29NDrFdAtLDMfZf3hOwpQkS8E/1GtVjTOrxlXrGUMSw5t7qZjeOMIqtycAw==","signature_status":"signed_v1","signed_at":"2026-07-05T04:50:53.216721Z","signed_message":"canonical_sha256_bytes"},"source_id":"2202.07627","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1c52cdb77e56e39f78f081cb4ff050ca16f4308b7421a0b392ac7ba3a2c354bc","sha256:7d37e032bcb8547391ada86662603bdcfb8cf81ba80ba3e71685674365c65f8f"],"state_sha256":"d4f201113df0dac51ddf48c08b480b83f072494e7c06f54f266a63729ea260a4"}