{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:AQFMPMOBOOMUV7MDC2MBWY5A7O","short_pith_number":"pith:AQFMPMOB","canonical_record":{"source":{"id":"2202.03471","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-07T19:20:32Z","cross_cats_sorted":[],"title_canon_sha256":"231fb880c5b8a8dbed062f234d1711bc99bee409aa7172e2147cb7f401db02fe","abstract_canon_sha256":"fb140d1d4d8cf3b87693ca0f5f2cd1e551961c28949848749944186a02833573"},"schema_version":"1.0"},"canonical_sha256":"040ac7b1c173994afd8316981b63a0fb8ec6fa07a2dde1300801841396421117","source":{"kind":"arxiv","id":"2202.03471","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.03471","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"arxiv_version","alias_value":"2202.03471v3","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.03471","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_12","alias_value":"AQFMPMOBOOMU","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_16","alias_value":"AQFMPMOBOOMUV7MD","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_8","alias_value":"AQFMPMOB","created_at":"2026-07-05T04:35:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:AQFMPMOBOOMUV7MDC2MBWY5A7O","target":"record","payload":{"canonical_record":{"source":{"id":"2202.03471","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-07T19:20:32Z","cross_cats_sorted":[],"title_canon_sha256":"231fb880c5b8a8dbed062f234d1711bc99bee409aa7172e2147cb7f401db02fe","abstract_canon_sha256":"fb140d1d4d8cf3b87693ca0f5f2cd1e551961c28949848749944186a02833573"},"schema_version":"1.0"},"canonical_sha256":"040ac7b1c173994afd8316981b63a0fb8ec6fa07a2dde1300801841396421117","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:35:43.411290Z","signature_b64":"HUhUOKTAbCm0+FShxZCic1N9IPPsmWgukA/lhF1RRxPXC708pUvLiUiCcjVI5h6fSpll6zCidXD6b+cFyuRFAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"040ac7b1c173994afd8316981b63a0fb8ec6fa07a2dde1300801841396421117","last_reissued_at":"2026-07-05T04:35:43.410829Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:35:43.410829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2202.03471","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T04:35:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hmg1tguIq0mdLCjwpJQSV0MVG22VYNixUOPX1wqKpUIPf1nun9Sa3gyyoSgJLgPG0/BvF1usRjJaj+e4oRg4Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T17:29:03.443484Z"},"content_sha256":"98f52d01a4dc3227f7b8e2303eaf8a3a7f120310f2dfe64b5e717d64e0b03b56","schema_version":"1.0","event_id":"sha256:98f52d01a4dc3227f7b8e2303eaf8a3a7f120310f2dfe64b5e717d64e0b03b56"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:AQFMPMOBOOMUV7MDC2MBWY5A7O","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A Scaling Limit for Line and Surface Defects","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Diego Rodriguez-Gomez","submitted_at":"2022-02-07T19:20:32Z","abstract_excerpt":"We study symmetry-breaking line defects in the Wilson-Fisher theory with $O(2N+1)$ global symmetry near four dimensions and symmetry-preserving surface defects in a cubic model with $O(2N)$ global symmetry near six dimensions. We introduce a scaling limit inspired by the large charge expansion in Conformal Field Theory. Using this, we compute the beta function for the defect coupling which allows to identify the corresponding Defect Conformal Field Theories. We also compute the correlation function of two parallel defects as well as correlation functions of certain defect operators with large "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.03471","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2202.03471/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T04:35:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sCpJhUYAs0h5ECOmeABSUKXSArQtTwUyeqJ/qO2PcBgGCorUlo87uD6eVkwcwVKZgPMIGbpvZ1ESXp9qqxtBCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T17:29:03.443992Z"},"content_sha256":"e9aa39339014cf6977048dea3e58db15cc4b4078386f649164d3748ea4457e1c","schema_version":"1.0","event_id":"sha256:e9aa39339014cf6977048dea3e58db15cc4b4078386f649164d3748ea4457e1c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O/bundle.json","state_url":"https://pith.science/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O/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":"2026-08-11T17:29:03Z","links":{"resolver":"https://pith.science/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O","bundle":"https://pith.science/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O/bundle.json","state":"https://pith.science/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AQFMPMOBOOMUV7MDC2MBWY5A7O/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:AQFMPMOBOOMUV7MDC2MBWY5A7O","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":"fb140d1d4d8cf3b87693ca0f5f2cd1e551961c28949848749944186a02833573","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-07T19:20:32Z","title_canon_sha256":"231fb880c5b8a8dbed062f234d1711bc99bee409aa7172e2147cb7f401db02fe"},"schema_version":"1.0","source":{"id":"2202.03471","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.03471","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"arxiv_version","alias_value":"2202.03471v3","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.03471","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_12","alias_value":"AQFMPMOBOOMU","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_16","alias_value":"AQFMPMOBOOMUV7MD","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_8","alias_value":"AQFMPMOB","created_at":"2026-07-05T04:35:43Z"}],"graph_snapshots":[{"event_id":"sha256:e9aa39339014cf6977048dea3e58db15cc4b4078386f649164d3748ea4457e1c","target":"graph","created_at":"2026-07-05T04:35:43Z","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/2202.03471/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study symmetry-breaking line defects in the Wilson-Fisher theory with $O(2N+1)$ global symmetry near four dimensions and symmetry-preserving surface defects in a cubic model with $O(2N)$ global symmetry near six dimensions. We introduce a scaling limit inspired by the large charge expansion in Conformal Field Theory. Using this, we compute the beta function for the defect coupling which allows to identify the corresponding Defect Conformal Field Theories. We also compute the correlation function of two parallel defects as well as correlation functions of certain defect operators with large ","authors_text":"Diego Rodriguez-Gomez","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-07T19:20:32Z","title":"A Scaling Limit for Line and Surface Defects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.03471","kind":"arxiv","version":3},"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":"sha256:98f52d01a4dc3227f7b8e2303eaf8a3a7f120310f2dfe64b5e717d64e0b03b56","target":"record","created_at":"2026-07-05T04:35:43Z","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":"fb140d1d4d8cf3b87693ca0f5f2cd1e551961c28949848749944186a02833573","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-02-07T19:20:32Z","title_canon_sha256":"231fb880c5b8a8dbed062f234d1711bc99bee409aa7172e2147cb7f401db02fe"},"schema_version":"1.0","source":{"id":"2202.03471","kind":"arxiv","version":3}},"canonical_sha256":"040ac7b1c173994afd8316981b63a0fb8ec6fa07a2dde1300801841396421117","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"040ac7b1c173994afd8316981b63a0fb8ec6fa07a2dde1300801841396421117","first_computed_at":"2026-07-05T04:35:43.410829Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:35:43.410829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HUhUOKTAbCm0+FShxZCic1N9IPPsmWgukA/lhF1RRxPXC708pUvLiUiCcjVI5h6fSpll6zCidXD6b+cFyuRFAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:35:43.411290Z","signed_message":"canonical_sha256_bytes"},"source_id":"2202.03471","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:98f52d01a4dc3227f7b8e2303eaf8a3a7f120310f2dfe64b5e717d64e0b03b56","sha256:e9aa39339014cf6977048dea3e58db15cc4b4078386f649164d3748ea4457e1c"],"state_sha256":"6631c2d32d573a3b525581d0b51b46ec826ba17da497761d8d17da6243604d61"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g6NoPYaDWOpfB56bzc2n+OPkpqfob+gRN5KlNlTkDTD78kWCqZpIa7WCjJ1k/luCR+k7ut1NUYbuRrsy+erEBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T17:29:03.447315Z","bundle_sha256":"b27dc6b580fa7a9fd09e95fd4850410c1d36d15ff91dd95a20788b468d1d2df6"}}