{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:V4ELUZPJE2NAGWUWRNKUNZAHVZ","short_pith_number":"pith:V4ELUZPJ","canonical_record":{"source":{"id":"hep-th/0005083","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2000-05-09T13:37:47Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a1e0b9fdf5b8e4f78f36509f1e3a273d760e168cfd3e6323cc684b715da1c792","abstract_canon_sha256":"c738ef6b02ec3daf604b744f4a3740b183aed71236415045ae1a2bd8496b9839"},"schema_version":"1.0"},"canonical_sha256":"af08ba65e9269a035a968b5546e407ae66ae2e7dc83c538ab75be63f515022f5","source":{"kind":"arxiv","id":"hep-th/0005083","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0005083","created_at":"2026-05-18T04:15:26Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0005083v2","created_at":"2026-05-18T04:15:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0005083","created_at":"2026-05-18T04:15:26Z"},{"alias_kind":"pith_short_12","alias_value":"V4ELUZPJE2NA","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"V4ELUZPJE2NAGWUW","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"V4ELUZPJ","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:V4ELUZPJE2NAGWUWRNKUNZAHVZ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0005083","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2000-05-09T13:37:47Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a1e0b9fdf5b8e4f78f36509f1e3a273d760e168cfd3e6323cc684b715da1c792","abstract_canon_sha256":"c738ef6b02ec3daf604b744f4a3740b183aed71236415045ae1a2bd8496b9839"},"schema_version":"1.0"},"canonical_sha256":"af08ba65e9269a035a968b5546e407ae66ae2e7dc83c538ab75be63f515022f5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:26.924868Z","signature_b64":"OnN8npK2g7TadwziPACEGIvpNe9deN6KBYG7Qoztbw/sBCxZ3XT5Wo/DzXZIb2k5H+sbyOAXSKk7+kpEQsdpAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af08ba65e9269a035a968b5546e407ae66ae2e7dc83c538ab75be63f515022f5","last_reissued_at":"2026-05-18T04:15:26.924516Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:26.924516Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0005083","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:15:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KEdAX9Knz5rX+HxMpZmv2/3ImBZwNYgu9ltZsFTHs6LFBP5RfVewUVSpGDBWrBMY0j5qSjwlTNUA2C0ObmZwAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T12:59:26.656650Z"},"content_sha256":"7347f51fb464eae849fb612688cd166b22522abdcdd4da23815386c3f11d4192","schema_version":"1.0","event_id":"sha256:7347f51fb464eae849fb612688cd166b22522abdcdd4da23815386c3f11d4192"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:V4ELUZPJE2NAGWUWRNKUNZAHVZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the Consistency of the Exact Renormalization Group Approach Applied to Gauge Theories in Algebraic Non-Covariant Gauges","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Michele Simionato","submitted_at":"2000-05-09T13:37:47Z","abstract_excerpt":"We study a class of Wilsonian formulations of non-Abelian gauge theories in algebraic non-covariant gauges where the Wilsonian infrared cutoff $\\Lambda$ is inserted as a mass term for the propagating fields. In this way the Ward-Takahashi identities are preserved to all scales. Nevertheless BRST-invariance in broken and the theory is gauge-dependent and unphysical at $\\Lambda\\neq0$. Then we discuss the infrared limit $\\Lambda\\to0$. We show that the singularities of the axial gauge choice are avoided in planar gauge and light-cone gauge. In addition the issue of infrared divergences is addresse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0005083","kind":"arxiv","version":2},"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":"2026-05-18T04:15:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mDksckMEN2BbPImoyrqTEUTaBnmAUxFL6Azr5KmgmU7CRfOGtzHJmwN1cYbiAR3elPSLtUizCrk6ghYAsErvCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T12:59:26.656989Z"},"content_sha256":"6b84dba8b027dbd325d9dd437c0b205f638056e98f048a33fd586303f73edbeb","schema_version":"1.0","event_id":"sha256:6b84dba8b027dbd325d9dd437c0b205f638056e98f048a33fd586303f73edbeb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ/bundle.json","state_url":"https://pith.science/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ/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":"2026-06-30T12:59:26Z","links":{"resolver":"https://pith.science/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ","bundle":"https://pith.science/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ/bundle.json","state":"https://pith.science/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/V4ELUZPJE2NAGWUWRNKUNZAHVZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:V4ELUZPJE2NAGWUWRNKUNZAHVZ","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":"c738ef6b02ec3daf604b744f4a3740b183aed71236415045ae1a2bd8496b9839","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2000-05-09T13:37:47Z","title_canon_sha256":"a1e0b9fdf5b8e4f78f36509f1e3a273d760e168cfd3e6323cc684b715da1c792"},"schema_version":"1.0","source":{"id":"hep-th/0005083","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0005083","created_at":"2026-05-18T04:15:26Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0005083v2","created_at":"2026-05-18T04:15:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0005083","created_at":"2026-05-18T04:15:26Z"},{"alias_kind":"pith_short_12","alias_value":"V4ELUZPJE2NA","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"V4ELUZPJE2NAGWUW","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"V4ELUZPJ","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:6b84dba8b027dbd325d9dd437c0b205f638056e98f048a33fd586303f73edbeb","target":"graph","created_at":"2026-05-18T04:15:26Z","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 study a class of Wilsonian formulations of non-Abelian gauge theories in algebraic non-covariant gauges where the Wilsonian infrared cutoff $\\Lambda$ is inserted as a mass term for the propagating fields. In this way the Ward-Takahashi identities are preserved to all scales. Nevertheless BRST-invariance in broken and the theory is gauge-dependent and unphysical at $\\Lambda\\neq0$. Then we discuss the infrared limit $\\Lambda\\to0$. We show that the singularities of the axial gauge choice are avoided in planar gauge and light-cone gauge. In addition the issue of infrared divergences is addresse","authors_text":"Michele Simionato","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2000-05-09T13:37:47Z","title":"On the Consistency of the Exact Renormalization Group Approach Applied to Gauge Theories in Algebraic Non-Covariant Gauges"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0005083","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":"sha256:7347f51fb464eae849fb612688cd166b22522abdcdd4da23815386c3f11d4192","target":"record","created_at":"2026-05-18T04:15:26Z","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":"c738ef6b02ec3daf604b744f4a3740b183aed71236415045ae1a2bd8496b9839","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2000-05-09T13:37:47Z","title_canon_sha256":"a1e0b9fdf5b8e4f78f36509f1e3a273d760e168cfd3e6323cc684b715da1c792"},"schema_version":"1.0","source":{"id":"hep-th/0005083","kind":"arxiv","version":2}},"canonical_sha256":"af08ba65e9269a035a968b5546e407ae66ae2e7dc83c538ab75be63f515022f5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"af08ba65e9269a035a968b5546e407ae66ae2e7dc83c538ab75be63f515022f5","first_computed_at":"2026-05-18T04:15:26.924516Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:15:26.924516Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OnN8npK2g7TadwziPACEGIvpNe9deN6KBYG7Qoztbw/sBCxZ3XT5Wo/DzXZIb2k5H+sbyOAXSKk7+kpEQsdpAg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:15:26.924868Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0005083","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7347f51fb464eae849fb612688cd166b22522abdcdd4da23815386c3f11d4192","sha256:6b84dba8b027dbd325d9dd437c0b205f638056e98f048a33fd586303f73edbeb"],"state_sha256":"d9bb3f58693bd6542422917e8d11aa103f4007e765db312ea1bff8297f8a2efe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"10lErxSWSDTPuAA5i9ZgAhh5UCi3ANj+FjpEGd7XYvjpXmq2Du6j7PXuKLHH+Kx+bDzt0rjHVqG7uJ4RIpVUDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-30T12:59:26.658822Z","bundle_sha256":"6dc90b8d001fa2fa64efa761da19e00b1f43f7808d37f578bc108197a81c5bc6"}}