{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:MINZ7TG6TBROD6IR3JBRYFHIKX","short_pith_number":"pith:MINZ7TG6","canonical_record":{"source":{"id":"2204.05262","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-11T17:04:27Z","cross_cats_sorted":[],"title_canon_sha256":"6a66dae801c7fdffe6393635e5f53628121ec2879113cead3817812e0da9735d","abstract_canon_sha256":"56c4c93d3d9f6d58696150ca15c7fb82d610f808882c6213656ec2546a446c3a"},"schema_version":"1.0"},"canonical_sha256":"621b9fccde9862e1f911da431c14e855dc0c3845c4a6b4628558999b1b0cbd2c","source":{"kind":"arxiv","id":"2204.05262","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.05262","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"arxiv_version","alias_value":"2204.05262v4","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.05262","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"pith_short_12","alias_value":"MINZ7TG6TBRO","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"pith_short_16","alias_value":"MINZ7TG6TBROD6IR","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"pith_short_8","alias_value":"MINZ7TG6","created_at":"2026-07-05T05:24:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:MINZ7TG6TBROD6IR3JBRYFHIKX","target":"record","payload":{"canonical_record":{"source":{"id":"2204.05262","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-11T17:04:27Z","cross_cats_sorted":[],"title_canon_sha256":"6a66dae801c7fdffe6393635e5f53628121ec2879113cead3817812e0da9735d","abstract_canon_sha256":"56c4c93d3d9f6d58696150ca15c7fb82d610f808882c6213656ec2546a446c3a"},"schema_version":"1.0"},"canonical_sha256":"621b9fccde9862e1f911da431c14e855dc0c3845c4a6b4628558999b1b0cbd2c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:24:11.140676Z","signature_b64":"XjCySFcBW8MIjPbMGSS0EJnC0EQ255jcP+nId3zHPkf700S0ROQEzSIvC54QtEbjc9jmT7CUg9J2bSZSLfWSBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"621b9fccde9862e1f911da431c14e855dc0c3845c4a6b4628558999b1b0cbd2c","last_reissued_at":"2026-07-05T05:24:11.140197Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:24:11.140197Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2204.05262","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T05:24:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uZZsdX28sFySlhTgkBZurFH81ozrZcf9gbEmkSKYWqb3yXAB+TKPkZmaFY4gF5kTU/UAHZA4FAOke5FXEF6kAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-21T19:50:28.271196Z"},"content_sha256":"b09d41c4197b03f93159d5a4486072ff17753f7737aa386317fe131fc033e087","schema_version":"1.0","event_id":"sha256:b09d41c4197b03f93159d5a4486072ff17753f7737aa386317fe131fc033e087"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:MINZ7TG6TBROD6IR3JBRYFHIKX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Line Operators in Chern-Simons-Matter Theories and Bosonization in Three Dimensions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Amit Sever, Barak Gabai, De-liang Zhong","submitted_at":"2022-04-11T17:04:27Z","abstract_excerpt":"We study Chern-Simons theories at large $N$ with either bosonic or fermionic matter in the fundamental representation. The most fundamental operators in these theories are mesonic line operators, the simplest example being Wilson lines ending on fundamentals. We classify the conformal line operators along an arbitrary smooth path as well as the spectrum of conformal dimensions and transverse spins of their boundary operators at finite 't Hooft coupling. These line operators are shown to satisfy first-order chiral evolution equations, in which a smooth variation of the path is given by a factor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.05262","kind":"arxiv","version":4},"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/2204.05262/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":"2026-07-05T05:24:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DhZkIzCVxYnn+Lgu05ToaK48BErBchbVM/OSCg+061xSE9Lv+Gmk0dnQxf6SSNzDPlTqWqupubDkVNMF2QJYBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-21T19:50:28.271545Z"},"content_sha256":"facb5f2a505c2b935722d6cc583b700594bc9592f48b40415c9bfa5a0c58c56c","schema_version":"1.0","event_id":"sha256:facb5f2a505c2b935722d6cc583b700594bc9592f48b40415c9bfa5a0c58c56c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MINZ7TG6TBROD6IR3JBRYFHIKX/bundle.json","state_url":"https://pith.science/pith/MINZ7TG6TBROD6IR3JBRYFHIKX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MINZ7TG6TBROD6IR3JBRYFHIKX/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":"2026-08-21T19:50:28Z","links":{"resolver":"https://pith.science/pith/MINZ7TG6TBROD6IR3JBRYFHIKX","bundle":"https://pith.science/pith/MINZ7TG6TBROD6IR3JBRYFHIKX/bundle.json","state":"https://pith.science/pith/MINZ7TG6TBROD6IR3JBRYFHIKX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MINZ7TG6TBROD6IR3JBRYFHIKX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:MINZ7TG6TBROD6IR3JBRYFHIKX","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":"56c4c93d3d9f6d58696150ca15c7fb82d610f808882c6213656ec2546a446c3a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-11T17:04:27Z","title_canon_sha256":"6a66dae801c7fdffe6393635e5f53628121ec2879113cead3817812e0da9735d"},"schema_version":"1.0","source":{"id":"2204.05262","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.05262","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"arxiv_version","alias_value":"2204.05262v4","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.05262","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"pith_short_12","alias_value":"MINZ7TG6TBRO","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"pith_short_16","alias_value":"MINZ7TG6TBROD6IR","created_at":"2026-07-05T05:24:11Z"},{"alias_kind":"pith_short_8","alias_value":"MINZ7TG6","created_at":"2026-07-05T05:24:11Z"}],"graph_snapshots":[{"event_id":"sha256:facb5f2a505c2b935722d6cc583b700594bc9592f48b40415c9bfa5a0c58c56c","target":"graph","created_at":"2026-07-05T05:24:11Z","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/2204.05262/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study Chern-Simons theories at large $N$ with either bosonic or fermionic matter in the fundamental representation. The most fundamental operators in these theories are mesonic line operators, the simplest example being Wilson lines ending on fundamentals. We classify the conformal line operators along an arbitrary smooth path as well as the spectrum of conformal dimensions and transverse spins of their boundary operators at finite 't Hooft coupling. These line operators are shown to satisfy first-order chiral evolution equations, in which a smooth variation of the path is given by a factor","authors_text":"Amit Sever, Barak Gabai, De-liang Zhong","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-11T17:04:27Z","title":"Line Operators in Chern-Simons-Matter Theories and Bosonization in Three Dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.05262","kind":"arxiv","version":4},"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:b09d41c4197b03f93159d5a4486072ff17753f7737aa386317fe131fc033e087","target":"record","created_at":"2026-07-05T05:24:11Z","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":"56c4c93d3d9f6d58696150ca15c7fb82d610f808882c6213656ec2546a446c3a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-11T17:04:27Z","title_canon_sha256":"6a66dae801c7fdffe6393635e5f53628121ec2879113cead3817812e0da9735d"},"schema_version":"1.0","source":{"id":"2204.05262","kind":"arxiv","version":4}},"canonical_sha256":"621b9fccde9862e1f911da431c14e855dc0c3845c4a6b4628558999b1b0cbd2c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"621b9fccde9862e1f911da431c14e855dc0c3845c4a6b4628558999b1b0cbd2c","first_computed_at":"2026-07-05T05:24:11.140197Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:24:11.140197Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XjCySFcBW8MIjPbMGSS0EJnC0EQ255jcP+nId3zHPkf700S0ROQEzSIvC54QtEbjc9jmT7CUg9J2bSZSLfWSBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T05:24:11.140676Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.05262","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b09d41c4197b03f93159d5a4486072ff17753f7737aa386317fe131fc033e087","sha256:facb5f2a505c2b935722d6cc583b700594bc9592f48b40415c9bfa5a0c58c56c"],"state_sha256":"07e27bec4aa5e0484deaaffe09f6266ffda00548f9ccd427fc5785da0d5d63c7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2NMHJv7F1fq259FeY7FVFqQAbTc0ecYmpzfU/nzhtjETJBbpOFyzWwJOsMWtrvh47gRZe0JCbuZsnperVscnAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-21T19:50:28.276005Z","bundle_sha256":"32df1efbd9fba9ae10b602ca010763d5e7156d6bc8c841e27864d86c8aa5437a"}}