{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:JFHMVHDYLJG2QPRQQVNEJZYG7K","short_pith_number":"pith:JFHMVHDY","canonical_record":{"source":{"id":"1310.4185","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-15T20:03:52Z","cross_cats_sorted":[],"title_canon_sha256":"42781c4563014dd29681a485def5ac8f65bbff3f4d8097d178f01b9921033b51","abstract_canon_sha256":"41a088193e25b50f10c024fc03725a71488be883d38a938ddb12374e3082ae3e"},"schema_version":"1.0"},"canonical_sha256":"494eca9c785a4da83e30855a44e706fab8d8fe8ba5c7d40116898d1f85f5fdd4","source":{"kind":"arxiv","id":"1310.4185","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.4185","created_at":"2026-05-18T02:59:05Z"},{"alias_kind":"arxiv_version","alias_value":"1310.4185v3","created_at":"2026-05-18T02:59:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.4185","created_at":"2026-05-18T02:59:05Z"},{"alias_kind":"pith_short_12","alias_value":"JFHMVHDYLJG2","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_16","alias_value":"JFHMVHDYLJG2QPRQ","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_8","alias_value":"JFHMVHDY","created_at":"2026-05-18T12:27:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:JFHMVHDYLJG2QPRQQVNEJZYG7K","target":"record","payload":{"canonical_record":{"source":{"id":"1310.4185","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-15T20:03:52Z","cross_cats_sorted":[],"title_canon_sha256":"42781c4563014dd29681a485def5ac8f65bbff3f4d8097d178f01b9921033b51","abstract_canon_sha256":"41a088193e25b50f10c024fc03725a71488be883d38a938ddb12374e3082ae3e"},"schema_version":"1.0"},"canonical_sha256":"494eca9c785a4da83e30855a44e706fab8d8fe8ba5c7d40116898d1f85f5fdd4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:59:05.982055Z","signature_b64":"rS9b9S/BRyhUclClg3QDMLRjYCQBiJEN2aKgYSUHysX9SsoM0GPnioCGYQaPt2AGAtwJZxYEjP/7e+yzFEbIBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"494eca9c785a4da83e30855a44e706fab8d8fe8ba5c7d40116898d1f85f5fdd4","last_reissued_at":"2026-05-18T02:59:05.981284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:59:05.981284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.4185","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":"2026-05-18T02:59:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sFXf/pAkHwKLDTpxq9LC/4dBwA9fxMk4lnBbdMnuLwoBfF32mXKewKR1FeyZYPIYtmkz6X+OewNj78bbyugjAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T08:34:59.984934Z"},"content_sha256":"a518ca870fc7786360de56c2162c3320e55da4a1799b70c1d110241984272f8d","schema_version":"1.0","event_id":"sha256:a518ca870fc7786360de56c2162c3320e55da4a1799b70c1d110241984272f8d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:JFHMVHDYLJG2QPRQQVNEJZYG7K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Renormalization and redundancy in 2d quantum field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anatoly Konechny, Nicolas Behr","submitted_at":"2013-10-15T20:03:52Z","abstract_excerpt":"We analyze renormalization group (RG) flows in two-dimensional quantum field theories in the presence of redundant directions. We use the operator picture in which redundant operators are total derivatives. Our analysis has three levels of generality. We introduce a redundancy anomaly equation which is analyzed together with the RG anomaly equation previously considered by H.Osborn [8] and D.Friedan and A.Konechny [7]. The Wess-Zumino consistency conditions between these anomalies yield a number of general relations which should hold to all orders in perturbation theory. We further use conform"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.4185","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":""},"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":"2026-05-18T02:59:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"442twOjetpn6aIsd49t7XTUekPp5w6G7PHqfSL8YqPMFzZI46AhSG/7YwcBVW0c4H1Qg0LZSa/EnFeyTtrUXCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T08:34:59.985284Z"},"content_sha256":"095822fbbefbff60b656dbc68d45dba92bbb56fb7dbcdd1db87a6bad08e8c4f3","schema_version":"1.0","event_id":"sha256:095822fbbefbff60b656dbc68d45dba92bbb56fb7dbcdd1db87a6bad08e8c4f3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K/bundle.json","state_url":"https://pith.science/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K/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":"2026-06-07T08:34:59Z","links":{"resolver":"https://pith.science/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K","bundle":"https://pith.science/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K/bundle.json","state":"https://pith.science/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JFHMVHDYLJG2QPRQQVNEJZYG7K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:JFHMVHDYLJG2QPRQQVNEJZYG7K","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":"41a088193e25b50f10c024fc03725a71488be883d38a938ddb12374e3082ae3e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-15T20:03:52Z","title_canon_sha256":"42781c4563014dd29681a485def5ac8f65bbff3f4d8097d178f01b9921033b51"},"schema_version":"1.0","source":{"id":"1310.4185","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.4185","created_at":"2026-05-18T02:59:05Z"},{"alias_kind":"arxiv_version","alias_value":"1310.4185v3","created_at":"2026-05-18T02:59:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.4185","created_at":"2026-05-18T02:59:05Z"},{"alias_kind":"pith_short_12","alias_value":"JFHMVHDYLJG2","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_16","alias_value":"JFHMVHDYLJG2QPRQ","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_8","alias_value":"JFHMVHDY","created_at":"2026-05-18T12:27:49Z"}],"graph_snapshots":[{"event_id":"sha256:095822fbbefbff60b656dbc68d45dba92bbb56fb7dbcdd1db87a6bad08e8c4f3","target":"graph","created_at":"2026-05-18T02:59:05Z","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 analyze renormalization group (RG) flows in two-dimensional quantum field theories in the presence of redundant directions. We use the operator picture in which redundant operators are total derivatives. Our analysis has three levels of generality. We introduce a redundancy anomaly equation which is analyzed together with the RG anomaly equation previously considered by H.Osborn [8] and D.Friedan and A.Konechny [7]. The Wess-Zumino consistency conditions between these anomalies yield a number of general relations which should hold to all orders in perturbation theory. We further use conform","authors_text":"Anatoly Konechny, Nicolas Behr","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-15T20:03:52Z","title":"Renormalization and redundancy in 2d quantum field theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.4185","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:a518ca870fc7786360de56c2162c3320e55da4a1799b70c1d110241984272f8d","target":"record","created_at":"2026-05-18T02:59:05Z","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":"41a088193e25b50f10c024fc03725a71488be883d38a938ddb12374e3082ae3e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-15T20:03:52Z","title_canon_sha256":"42781c4563014dd29681a485def5ac8f65bbff3f4d8097d178f01b9921033b51"},"schema_version":"1.0","source":{"id":"1310.4185","kind":"arxiv","version":3}},"canonical_sha256":"494eca9c785a4da83e30855a44e706fab8d8fe8ba5c7d40116898d1f85f5fdd4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"494eca9c785a4da83e30855a44e706fab8d8fe8ba5c7d40116898d1f85f5fdd4","first_computed_at":"2026-05-18T02:59:05.981284Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:59:05.981284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rS9b9S/BRyhUclClg3QDMLRjYCQBiJEN2aKgYSUHysX9SsoM0GPnioCGYQaPt2AGAtwJZxYEjP/7e+yzFEbIBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:59:05.982055Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.4185","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a518ca870fc7786360de56c2162c3320e55da4a1799b70c1d110241984272f8d","sha256:095822fbbefbff60b656dbc68d45dba92bbb56fb7dbcdd1db87a6bad08e8c4f3"],"state_sha256":"1e5b2621095acd638a626e8eddc409ecbf70db7701e173ee10aae66d2ea416f4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g3hrYU0LeSwRciGCQ9ujOBoCXK/W/4gxspXOGzYl0Y/IcSVAYwRGcm4RsCh8SdClARdqBjm/5ZcEzWnVS/Z6Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T08:34:59.987194Z","bundle_sha256":"d758ff4b9dcba2aee8d2bc70f655eae3195882f335c4d078a4b7ad71162eda6d"}}