{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:ZZQCKNTZBKN4DAG4OSZX3C6SEY","short_pith_number":"pith:ZZQCKNTZ","canonical_record":{"source":{"id":"2207.09474","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-19T18:00:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"052d37a9a2ca05954f080fd137c3004e599c7c283bf1e07408c21d71e26c64b7","abstract_canon_sha256":"48d11fa043b4b6fe259056ca6676bb37d933b1ca6531abb6fe5e53fdc30336d1"},"schema_version":"1.0"},"canonical_sha256":"ce602536790a9bc180dc74b37d8bd22600b6d4c29fc62b98ae20ecdd84d01dff","source":{"kind":"arxiv","id":"2207.09474","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2207.09474","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"arxiv_version","alias_value":"2207.09474v3","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.09474","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"pith_short_12","alias_value":"ZZQCKNTZBKN4","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"pith_short_16","alias_value":"ZZQCKNTZBKN4DAG4","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"pith_short_8","alias_value":"ZZQCKNTZ","created_at":"2026-07-05T06:06:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:ZZQCKNTZBKN4DAG4OSZX3C6SEY","target":"record","payload":{"canonical_record":{"source":{"id":"2207.09474","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-19T18:00:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"052d37a9a2ca05954f080fd137c3004e599c7c283bf1e07408c21d71e26c64b7","abstract_canon_sha256":"48d11fa043b4b6fe259056ca6676bb37d933b1ca6531abb6fe5e53fdc30336d1"},"schema_version":"1.0"},"canonical_sha256":"ce602536790a9bc180dc74b37d8bd22600b6d4c29fc62b98ae20ecdd84d01dff","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:06:40.457623Z","signature_b64":"wj5SqAxJyNK43hlHd5OJ7IMbgJZ0H9XxNVKmp/0G1Xv5JekIlVZmFEABhML5WmWeVL4uuMeXUCxT+ccwMAXJBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce602536790a9bc180dc74b37d8bd22600b6d4c29fc62b98ae20ecdd84d01dff","last_reissued_at":"2026-07-05T06:06:40.457088Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:06:40.457088Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2207.09474","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":"2026-07-05T06:06:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9O3sapZYaeWKFRO8OrDXTUThcV3NvCdxhCii6Dmf56Tw5bGHqwB48fHFzoTec71e6oG7+x3W9fBKHLm+Rcs8Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T01:19:53.150509Z"},"content_sha256":"8485069d7982b633354a134065846e8b6149260ada5173767f15639cd6ca82d3","schema_version":"1.0","event_id":"sha256:8485069d7982b633354a134065846e8b6149260ada5173767f15639cd6ca82d3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:ZZQCKNTZBKN4DAG4OSZX3C6SEY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conformal field theory for particle physicists","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Marc Gillioz","submitted_at":"2022-07-19T18:00:04Z","abstract_excerpt":"This is a set of introductory lecture notes on conformal field theory. Unlike most existing reviews on the subject, CFT is presented here from the perspective of a unitary quantum field theory in Minkowski space-time. It begins with a non-perturbative formulation of quantum field theory (Wightman axioms), and then gradually focuses on the implications of scale and special conformal symmetry, all the way to the modern conformal bootstrap. This approach includes topics often left out, such as subtleties of conformal transformations in Minkowski space-time, the construction of Wightman functions "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.09474","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/2207.09474/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":"2026-07-05T06:06:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"brJfwdtfLccTjNpeTkVqMUkAAYlwcjae2PHcWqXCzZvk5U7jxq1sToBzkPuou1Hxz2e2aLxj+8NP5nRUWta1CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T01:19:53.151409Z"},"content_sha256":"a91d4cbce7363e4b2abb12c1bcb8bbac2579ef7519b92e3f0faa59ea06f98b72","schema_version":"1.0","event_id":"sha256:a91d4cbce7363e4b2abb12c1bcb8bbac2579ef7519b92e3f0faa59ea06f98b72"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY/bundle.json","state_url":"https://pith.science/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY/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":"2026-08-16T01:19:53Z","links":{"resolver":"https://pith.science/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY","bundle":"https://pith.science/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY/bundle.json","state":"https://pith.science/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZZQCKNTZBKN4DAG4OSZX3C6SEY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:ZZQCKNTZBKN4DAG4OSZX3C6SEY","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":"48d11fa043b4b6fe259056ca6676bb37d933b1ca6531abb6fe5e53fdc30336d1","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-19T18:00:04Z","title_canon_sha256":"052d37a9a2ca05954f080fd137c3004e599c7c283bf1e07408c21d71e26c64b7"},"schema_version":"1.0","source":{"id":"2207.09474","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2207.09474","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"arxiv_version","alias_value":"2207.09474v3","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.09474","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"pith_short_12","alias_value":"ZZQCKNTZBKN4","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"pith_short_16","alias_value":"ZZQCKNTZBKN4DAG4","created_at":"2026-07-05T06:06:40Z"},{"alias_kind":"pith_short_8","alias_value":"ZZQCKNTZ","created_at":"2026-07-05T06:06:40Z"}],"graph_snapshots":[{"event_id":"sha256:a91d4cbce7363e4b2abb12c1bcb8bbac2579ef7519b92e3f0faa59ea06f98b72","target":"graph","created_at":"2026-07-05T06:06:40Z","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/2207.09474/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"This is a set of introductory lecture notes on conformal field theory. Unlike most existing reviews on the subject, CFT is presented here from the perspective of a unitary quantum field theory in Minkowski space-time. It begins with a non-perturbative formulation of quantum field theory (Wightman axioms), and then gradually focuses on the implications of scale and special conformal symmetry, all the way to the modern conformal bootstrap. This approach includes topics often left out, such as subtleties of conformal transformations in Minkowski space-time, the construction of Wightman functions ","authors_text":"Marc Gillioz","cross_cats":["hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-19T18:00:04Z","title":"Conformal field theory for particle physicists"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.09474","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":"sha256:8485069d7982b633354a134065846e8b6149260ada5173767f15639cd6ca82d3","target":"record","created_at":"2026-07-05T06:06:40Z","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":"48d11fa043b4b6fe259056ca6676bb37d933b1ca6531abb6fe5e53fdc30336d1","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-19T18:00:04Z","title_canon_sha256":"052d37a9a2ca05954f080fd137c3004e599c7c283bf1e07408c21d71e26c64b7"},"schema_version":"1.0","source":{"id":"2207.09474","kind":"arxiv","version":3}},"canonical_sha256":"ce602536790a9bc180dc74b37d8bd22600b6d4c29fc62b98ae20ecdd84d01dff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ce602536790a9bc180dc74b37d8bd22600b6d4c29fc62b98ae20ecdd84d01dff","first_computed_at":"2026-07-05T06:06:40.457088Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:06:40.457088Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wj5SqAxJyNK43hlHd5OJ7IMbgJZ0H9XxNVKmp/0G1Xv5JekIlVZmFEABhML5WmWeVL4uuMeXUCxT+ccwMAXJBw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:06:40.457623Z","signed_message":"canonical_sha256_bytes"},"source_id":"2207.09474","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8485069d7982b633354a134065846e8b6149260ada5173767f15639cd6ca82d3","sha256:a91d4cbce7363e4b2abb12c1bcb8bbac2579ef7519b92e3f0faa59ea06f98b72"],"state_sha256":"95aa7f765836a5c26e5d43c93e347d34d9bb6bc26387916423639661f9937060"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kNeoTGdEJFRyfujd4Y/Sdkl5z4NcvvRsfoBkOQLHSp/NA2yc75Pn88/ztDS4ik48gzpabqXU0hADJboPRbotBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T01:19:53.164539Z","bundle_sha256":"ce1c5c2557a81c65738242a433a0ccfd60a98f05448d921c075b421ca676905c"}}