{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1993:HVQGZBHRI6LLXAHBJ3AMNIE2ZN","short_pith_number":"pith:HVQGZBHR","canonical_record":{"source":{"id":"hep-th/9307027","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-07-05T14:40:00Z","cross_cats_sorted":[],"title_canon_sha256":"b97400af45d4aa8cb39fe7dfc3f3c9f66a25b4b345ccb94e19f2d7945fe048ea","abstract_canon_sha256":"798f339adac247f12c0cec7b63543c9373a356570073c9abbd1857d179420337"},"schema_version":"1.0"},"canonical_sha256":"3d606c84f14796bb80e14ec0c6a09acb60e1570f0d89052af465e8c2028345c7","source":{"kind":"arxiv","id":"hep-th/9307027","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9307027","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9307027v1","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9307027","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"pith_short_12","alias_value":"HVQGZBHRI6LL","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"pith_short_16","alias_value":"HVQGZBHRI6LLXAHB","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"pith_short_8","alias_value":"HVQGZBHR","created_at":"2026-07-04T15:56:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1993:HVQGZBHRI6LLXAHBJ3AMNIE2ZN","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9307027","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-07-05T14:40:00Z","cross_cats_sorted":[],"title_canon_sha256":"b97400af45d4aa8cb39fe7dfc3f3c9f66a25b4b345ccb94e19f2d7945fe048ea","abstract_canon_sha256":"798f339adac247f12c0cec7b63543c9373a356570073c9abbd1857d179420337"},"schema_version":"1.0"},"canonical_sha256":"3d606c84f14796bb80e14ec0c6a09acb60e1570f0d89052af465e8c2028345c7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:56:15.811604Z","signature_b64":"72OvbVV4DaTflh3LHlYbeyBO/pT0z3o7jOt85Vd2e/RuLQgLPSfl0eU5m527rVzFtXTo07u3kKb50D3+UipDDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3d606c84f14796bb80e14ec0c6a09acb60e1570f0d89052af465e8c2028345c7","last_reissued_at":"2026-07-04T15:56:15.811270Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:56:15.811270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9307027","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:56:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n5DwvSebWyqNBiJ44ebiTOMUjxaJ9lLhlv2J1gsP+wNrrpQHIIa6Ku6sX1ra5uSxrtyDUu2rbTQ8mzdHrcjCCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T15:14:07.702406Z"},"content_sha256":"aed3619f67eb9f4379ab9cd68e17de94057add5217f6ac0fe55022e93bbdd05d","schema_version":"1.0","event_id":"sha256:aed3619f67eb9f4379ab9cd68e17de94057add5217f6ac0fe55022e93bbdd05d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1993:HVQGZBHRI6LLXAHBJ3AMNIE2ZN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The WZNW Model at Two Loops","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. de Wit, M.T. Grisaru, P. van Nieuwenhuizen","submitted_at":"1993-07-05T14:40:00Z","abstract_excerpt":"We study perturbatively the (conformal) WZNW model. At one loop we compute one-particle irreducible two- and three-point current correlation functions, both in the conventional version and in the classically equivalent, chiral, nonlocal, induced version of the model. At two loops we compute the two-point function and find that it vanishes (modulo infrared-induced logarithms). We use dimensional regularization and the $R^*$ operation for removing infrared divergences. The outcome of the calculations is insensitive to the treatment of the $\\varepsilon^{\\m\\n}$ tensor as a two-dimensional or $d$-d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9307027","kind":"arxiv","version":1},"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/hep-th/9307027/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":"2026-07-04T15:56:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J0BMCoEXg0w515qF1HAlrNtkGtNJcXFB2hJ22m7jZ1cx47o6YYYfulteZW6dkra1UnlUcO0FaTdYBPR3jmzNAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T15:14:07.702995Z"},"content_sha256":"45936acf661c0a97eda65bc48eef39a4e24eaf6f1116611e344c5d8c80212d37","schema_version":"1.0","event_id":"sha256:45936acf661c0a97eda65bc48eef39a4e24eaf6f1116611e344c5d8c80212d37"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN/bundle.json","state_url":"https://pith.science/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN/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":"2026-08-13T15:14:07Z","links":{"resolver":"https://pith.science/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN","bundle":"https://pith.science/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN/bundle.json","state":"https://pith.science/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HVQGZBHRI6LLXAHBJ3AMNIE2ZN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1993:HVQGZBHRI6LLXAHBJ3AMNIE2ZN","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":"798f339adac247f12c0cec7b63543c9373a356570073c9abbd1857d179420337","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1993-07-05T14:40:00Z","title_canon_sha256":"b97400af45d4aa8cb39fe7dfc3f3c9f66a25b4b345ccb94e19f2d7945fe048ea"},"schema_version":"1.0","source":{"id":"hep-th/9307027","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9307027","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9307027v1","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9307027","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"pith_short_12","alias_value":"HVQGZBHRI6LL","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"pith_short_16","alias_value":"HVQGZBHRI6LLXAHB","created_at":"2026-07-04T15:56:15Z"},{"alias_kind":"pith_short_8","alias_value":"HVQGZBHR","created_at":"2026-07-04T15:56:15Z"}],"graph_snapshots":[{"event_id":"sha256:45936acf661c0a97eda65bc48eef39a4e24eaf6f1116611e344c5d8c80212d37","target":"graph","created_at":"2026-07-04T15:56:15Z","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/hep-th/9307027/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study perturbatively the (conformal) WZNW model. At one loop we compute one-particle irreducible two- and three-point current correlation functions, both in the conventional version and in the classically equivalent, chiral, nonlocal, induced version of the model. At two loops we compute the two-point function and find that it vanishes (modulo infrared-induced logarithms). We use dimensional regularization and the $R^*$ operation for removing infrared divergences. The outcome of the calculations is insensitive to the treatment of the $\\varepsilon^{\\m\\n}$ tensor as a two-dimensional or $d$-d","authors_text":"B. de Wit, M.T. Grisaru, P. van Nieuwenhuizen","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1993-07-05T14:40:00Z","title":"The WZNW Model at Two Loops"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9307027","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:aed3619f67eb9f4379ab9cd68e17de94057add5217f6ac0fe55022e93bbdd05d","target":"record","created_at":"2026-07-04T15:56:15Z","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":"798f339adac247f12c0cec7b63543c9373a356570073c9abbd1857d179420337","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1993-07-05T14:40:00Z","title_canon_sha256":"b97400af45d4aa8cb39fe7dfc3f3c9f66a25b4b345ccb94e19f2d7945fe048ea"},"schema_version":"1.0","source":{"id":"hep-th/9307027","kind":"arxiv","version":1}},"canonical_sha256":"3d606c84f14796bb80e14ec0c6a09acb60e1570f0d89052af465e8c2028345c7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3d606c84f14796bb80e14ec0c6a09acb60e1570f0d89052af465e8c2028345c7","first_computed_at":"2026-07-04T15:56:15.811270Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:56:15.811270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"72OvbVV4DaTflh3LHlYbeyBO/pT0z3o7jOt85Vd2e/RuLQgLPSfl0eU5m527rVzFtXTo07u3kKb50D3+UipDDw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:56:15.811604Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9307027","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:aed3619f67eb9f4379ab9cd68e17de94057add5217f6ac0fe55022e93bbdd05d","sha256:45936acf661c0a97eda65bc48eef39a4e24eaf6f1116611e344c5d8c80212d37"],"state_sha256":"ade400b5084ec426cd2eacb972627a85db95a0ef98cbc78efbea56ccd57efd41"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6HECeVRuUm0LXkuoO5FC/7zO5cBNrmU1r8A7s3j5vtwePO1bOgQryVs9uNV3xmCCq7fsMk15ZqDzFXMNfm++BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T15:14:07.711369Z","bundle_sha256":"c19ad3fc70f59576560aa3f55cfa4fe856a5eb8b28366a573e00f7010e3f8955"}}