{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:XOTHRUUWCHQ2OSH3LAYSSNHH4P","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":"50f5e1d836049d85a2278cd5ca72d375d3151e16a1d5b0783156c99acf5e04a2","cross_cats_sorted":["cond-mat.stat-mech","hep-ph"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-26T15:44:26Z","title_canon_sha256":"a174e1f0f5c51b79b99a833e4bd4c7fb1d0bbb92607a00e40a1524b14a793f1f"},"schema_version":"1.0","source":{"id":"2202.13165","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.13165","created_at":"2026-07-05T04:35:44Z"},{"alias_kind":"arxiv_version","alias_value":"2202.13165v1","created_at":"2026-07-05T04:35:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.13165","created_at":"2026-07-05T04:35:44Z"},{"alias_kind":"pith_short_12","alias_value":"XOTHRUUWCHQ2","created_at":"2026-07-05T04:35:44Z"},{"alias_kind":"pith_short_16","alias_value":"XOTHRUUWCHQ2OSH3","created_at":"2026-07-05T04:35:44Z"},{"alias_kind":"pith_short_8","alias_value":"XOTHRUUW","created_at":"2026-07-05T04:35:44Z"}],"graph_snapshots":[{"event_id":"sha256:cb4ba16dcfa67e3b5a8230356308dc54b54742665912ef542bf4da33c96701e5","target":"graph","created_at":"2026-07-05T04:35:44Z","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/2202.13165/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the analytic properties of the fixed charge expansion for a number of conformal field theories in different space-time dimensions. The models investigated here are $O(N)$ and $QED_3$. We show that in $d=3-\\epsilon$ dimensions the contribution to the $O(N)$ fixed charge $Q$ conformal dimensions obtained in the double scaling limit of large charge and vanishing $\\epsilon$ is non-Borel summable, doubly factorial divergent, and with order $\\sqrt{Q}$ optimal truncation order. By using resurgence techniques we show that the singularities in the Borel plane are related to worldline ins","authors_text":"Francesco Sannino, Jahmall Bersini, Mat\\'ias Torres, Oleg Antipin","cross_cats":["cond-mat.stat-mech","hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-26T15:44:26Z","title":"The analytic structure of the fixed charge expansion"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.13165","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":"sha256:487b72317aa7ebf9e37ce3ae17e846ab4a4ebbd19ac3fcb36ec8aef19c1274c7","target":"record","created_at":"2026-07-05T04:35:44Z","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":"50f5e1d836049d85a2278cd5ca72d375d3151e16a1d5b0783156c99acf5e04a2","cross_cats_sorted":["cond-mat.stat-mech","hep-ph"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-26T15:44:26Z","title_canon_sha256":"a174e1f0f5c51b79b99a833e4bd4c7fb1d0bbb92607a00e40a1524b14a793f1f"},"schema_version":"1.0","source":{"id":"2202.13165","kind":"arxiv","version":1}},"canonical_sha256":"bba678d29611e1a748fb58312934e7e3c5f01de8a716c226243c5dbf726a6d87","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bba678d29611e1a748fb58312934e7e3c5f01de8a716c226243c5dbf726a6d87","first_computed_at":"2026-07-05T04:35:44.261017Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:35:44.261017Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vlbf4KYP3Hx/GJ4fPWoJCYeTjKnTPsHOh5MtXzTGiqGIJ1xr1TKUrCsf2kaYbvneKrp9fhDmCcLwmXkhRd6mAw==","signature_status":"signed_v1","signed_at":"2026-07-05T04:35:44.261503Z","signed_message":"canonical_sha256_bytes"},"source_id":"2202.13165","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:487b72317aa7ebf9e37ce3ae17e846ab4a4ebbd19ac3fcb36ec8aef19c1274c7","sha256:cb4ba16dcfa67e3b5a8230356308dc54b54742665912ef542bf4da33c96701e5"],"state_sha256":"4740d3c489a91a69a397b2b8a2c94a4bc6f4a5a912bbdf14fc320ae32275251a"}