{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:BZTA3EP2IQS4YIGEJDHUA4CFVD","short_pith_number":"pith:BZTA3EP2","canonical_record":{"source":{"id":"hep-th/9405136","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-05-20T19:02:26Z","cross_cats_sorted":[],"title_canon_sha256":"f6246fa0d8623fedb3fc723a4645e53896137ceafcdf19f657b8517ff4c5e63c","abstract_canon_sha256":"d21905abd56fbae57629a129588bc2fbc244632b45a9a010f5b9fc6755859294"},"schema_version":"1.0"},"canonical_sha256":"0e660d91fa4425cc20c448cf407045a8c8641abec63086da10847997ee8d40f3","source":{"kind":"arxiv","id":"hep-th/9405136","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9405136","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9405136v1","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9405136","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"pith_short_12","alias_value":"BZTA3EP2IQS4","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"pith_short_16","alias_value":"BZTA3EP2IQS4YIGE","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"pith_short_8","alias_value":"BZTA3EP2","created_at":"2026-07-04T15:57:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:BZTA3EP2IQS4YIGEJDHUA4CFVD","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9405136","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-05-20T19:02:26Z","cross_cats_sorted":[],"title_canon_sha256":"f6246fa0d8623fedb3fc723a4645e53896137ceafcdf19f657b8517ff4c5e63c","abstract_canon_sha256":"d21905abd56fbae57629a129588bc2fbc244632b45a9a010f5b9fc6755859294"},"schema_version":"1.0"},"canonical_sha256":"0e660d91fa4425cc20c448cf407045a8c8641abec63086da10847997ee8d40f3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:57:45.365064Z","signature_b64":"GCB+AZOig0ePFKhxXvFjh+kIVJD09pdlJeRddwy+AdgK+NOzMrSRNN39BGTSkXutVEFdE76X1rD6uqJP8iJ3Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e660d91fa4425cc20c448cf407045a8c8641abec63086da10847997ee8d40f3","last_reissued_at":"2026-07-04T15:57:45.364717Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:57:45.364717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9405136","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":"2026-07-04T15:57:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qJ0We3Ml89+6nU8zIynVLwP3xqysDSOuzZ2F6Q5cbd9ruCxsZiJeCfVhfjgl46bomn2GHTIuFomMMfqsiq20BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T07:11:22.995074Z"},"content_sha256":"ff5a735e13195e308f3610f75d76a08e1f1eeb411a7662599a5f87f5aad76c08","schema_version":"1.0","event_id":"sha256:ff5a735e13195e308f3610f75d76a08e1f1eeb411a7662599a5f87f5aad76c08"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:BZTA3EP2IQS4YIGEJDHUA4CFVD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Continous Spins in 2D Gravity: Chiral Vertex Operators and Local Fields","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jean-Loup Gervais, Jens Schnittger","submitted_at":"1994-05-20T19:02:26Z","abstract_excerpt":"We construct the exponentials of the Liouville field with continuous powers within the operator approach. Their chiral decomposition is realized using the explicit Coulomb-gas operators we introduced earlier. {}From the quantum-group viewpoint, they are related to semi-infinite highest or lowest weight representations with continuous spins. The Liouville field itself is defined, and the canonical commutation relations verified, as well as the validity of the quantum Liouville field equations.\n  In a second part, both screening charges are considered. The braiding of the chiral components is de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9405136","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/9405136/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":"2026-07-04T15:57:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Xpaoq9zNPcu5VrmyuwRFoFlgmDt8MUYZx1MuqWom7ntjNJhZwD2U6NjcrM62ZLBQX1sbK8y3N5bcyxv6on4VAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T07:11:22.995865Z"},"content_sha256":"47ac5890a2a2a9ba79889e1dcd533c1277d81f9c66a56701c64b87ddc1eba096","schema_version":"1.0","event_id":"sha256:47ac5890a2a2a9ba79889e1dcd533c1277d81f9c66a56701c64b87ddc1eba096"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD/bundle.json","state_url":"https://pith.science/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD/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":"2026-08-09T07:11:23Z","links":{"resolver":"https://pith.science/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD","bundle":"https://pith.science/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD/bundle.json","state":"https://pith.science/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BZTA3EP2IQS4YIGEJDHUA4CFVD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:BZTA3EP2IQS4YIGEJDHUA4CFVD","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":"d21905abd56fbae57629a129588bc2fbc244632b45a9a010f5b9fc6755859294","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1994-05-20T19:02:26Z","title_canon_sha256":"f6246fa0d8623fedb3fc723a4645e53896137ceafcdf19f657b8517ff4c5e63c"},"schema_version":"1.0","source":{"id":"hep-th/9405136","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9405136","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9405136v1","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9405136","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"pith_short_12","alias_value":"BZTA3EP2IQS4","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"pith_short_16","alias_value":"BZTA3EP2IQS4YIGE","created_at":"2026-07-04T15:57:45Z"},{"alias_kind":"pith_short_8","alias_value":"BZTA3EP2","created_at":"2026-07-04T15:57:45Z"}],"graph_snapshots":[{"event_id":"sha256:47ac5890a2a2a9ba79889e1dcd533c1277d81f9c66a56701c64b87ddc1eba096","target":"graph","created_at":"2026-07-04T15:57:45Z","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/9405136/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We construct the exponentials of the Liouville field with continuous powers within the operator approach. Their chiral decomposition is realized using the explicit Coulomb-gas operators we introduced earlier. {}From the quantum-group viewpoint, they are related to semi-infinite highest or lowest weight representations with continuous spins. The Liouville field itself is defined, and the canonical commutation relations verified, as well as the validity of the quantum Liouville field equations.\n  In a second part, both screening charges are considered. The braiding of the chiral components is de","authors_text":"Jean-Loup Gervais, Jens Schnittger","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1994-05-20T19:02:26Z","title":"Continous Spins in 2D Gravity: Chiral Vertex Operators and Local Fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9405136","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:ff5a735e13195e308f3610f75d76a08e1f1eeb411a7662599a5f87f5aad76c08","target":"record","created_at":"2026-07-04T15:57:45Z","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":"d21905abd56fbae57629a129588bc2fbc244632b45a9a010f5b9fc6755859294","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1994-05-20T19:02:26Z","title_canon_sha256":"f6246fa0d8623fedb3fc723a4645e53896137ceafcdf19f657b8517ff4c5e63c"},"schema_version":"1.0","source":{"id":"hep-th/9405136","kind":"arxiv","version":1}},"canonical_sha256":"0e660d91fa4425cc20c448cf407045a8c8641abec63086da10847997ee8d40f3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0e660d91fa4425cc20c448cf407045a8c8641abec63086da10847997ee8d40f3","first_computed_at":"2026-07-04T15:57:45.364717Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:57:45.364717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GCB+AZOig0ePFKhxXvFjh+kIVJD09pdlJeRddwy+AdgK+NOzMrSRNN39BGTSkXutVEFdE76X1rD6uqJP8iJ3Aw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:57:45.365064Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9405136","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff5a735e13195e308f3610f75d76a08e1f1eeb411a7662599a5f87f5aad76c08","sha256:47ac5890a2a2a9ba79889e1dcd533c1277d81f9c66a56701c64b87ddc1eba096"],"state_sha256":"2c44f0b4db61c6a291f0f2771c558eb3726f6a179870782e2ce27c80747a327e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UTXzPU+dMj6MJ6pIRplUhf5NH/lL/tSWkh5fpnC52f9DlB5UzNmgOBo8I58vSYvwuuYZ5XbaR80zhgXaTNvCBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T07:11:23.054716Z","bundle_sha256":"f7f4ac3e44c63384be733aae741b77e4179bbd5349ae982a9844204edd37456b"}}