{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1991:LQSBQVRCLX6PHJHPRJIGFG2YWV","short_pith_number":"pith:LQSBQVRC","schema_version":"1.0","canonical_sha256":"5c241856225dfcf3a4ef8a50629b58b5705dff81bae41bac3189b0f12fdf9439","source":{"kind":"arxiv","id":"hep-th/9108008","version":1},"attestation_state":"computed","paper":{"title":"Novel Symmetries of Topological Conformal Field theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J. Sonnenschein, S. Yankielowicz","submitted_at":"1991-08-20T23:17:00Z","abstract_excerpt":"We show that various actions of topological conformal theories that were suggested recentely are particular cases of a general action. We prove the invariance of these models under transformations generated by nilpotent fermionic generators of arbitrary conformal dimension, $\\Q$ and $\\G$. The later are shown to be the $n^{th}$ covariant derivative with respect to ``flat abelian gauge field\" of the fermionic fields of those models. We derive the bosonic counterparts $\\W$ and $\\R$ which together with $\\Q$ and $\\G$ form a special $N=2$ super $W_\\infty$ algebra. The algebraic structure is discusse"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-th/9108008","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1991-08-20T23:17:00Z","cross_cats_sorted":[],"title_canon_sha256":"851841f2262a809a576cf46ee17c9c7e7e924d70ee594e37b52810a66314938a","abstract_canon_sha256":"42eb006fa75c6556035cb3ca3fd560127f579059c32fc65811795dcc517bf274"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:32:25.493366Z","signature_b64":"yT1XbOVyOIt+hPXxiWEr+GMpB+fZKBF6HYoQ+l5uwt2Ltb+A8T+VKYUw0VefuI2tyVsYQqJC/Fva53Tf9y/4Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c241856225dfcf3a4ef8a50629b58b5705dff81bae41bac3189b0f12fdf9439","last_reissued_at":"2026-07-04T14:32:25.492973Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:32:25.492973Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Novel Symmetries of Topological Conformal Field theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J. Sonnenschein, S. Yankielowicz","submitted_at":"1991-08-20T23:17:00Z","abstract_excerpt":"We show that various actions of topological conformal theories that were suggested recentely are particular cases of a general action. We prove the invariance of these models under transformations generated by nilpotent fermionic generators of arbitrary conformal dimension, $\\Q$ and $\\G$. The later are shown to be the $n^{th}$ covariant derivative with respect to ``flat abelian gauge field\" of the fermionic fields of those models. We derive the bosonic counterparts $\\W$ and $\\R$ which together with $\\Q$ and $\\G$ form a special $N=2$ super $W_\\infty$ algebra. The algebraic structure is discusse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9108008","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/9108008/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9108008","created_at":"2026-07-04T14:32:25.493029+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9108008v1","created_at":"2026-07-04T14:32:25.493029+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9108008","created_at":"2026-07-04T14:32:25.493029+00:00"},{"alias_kind":"pith_short_12","alias_value":"LQSBQVRCLX6P","created_at":"2026-07-04T14:32:25.493029+00:00"},{"alias_kind":"pith_short_16","alias_value":"LQSBQVRCLX6PHJHP","created_at":"2026-07-04T14:32:25.493029+00:00"},{"alias_kind":"pith_short_8","alias_value":"LQSBQVRC","created_at":"2026-07-04T14:32:25.493029+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV","json":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV.json","graph_json":"https://pith.science/api/pith-number/LQSBQVRCLX6PHJHPRJIGFG2YWV/graph.json","events_json":"https://pith.science/api/pith-number/LQSBQVRCLX6PHJHPRJIGFG2YWV/events.json","paper":"https://pith.science/paper/LQSBQVRC"},"agent_actions":{"view_html":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV","download_json":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV.json","view_paper":"https://pith.science/paper/LQSBQVRC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9108008&json=true","fetch_graph":"https://pith.science/api/pith-number/LQSBQVRCLX6PHJHPRJIGFG2YWV/graph.json","fetch_events":"https://pith.science/api/pith-number/LQSBQVRCLX6PHJHPRJIGFG2YWV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV/action/storage_attestation","attest_author":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV/action/author_attestation","sign_citation":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV/action/citation_signature","submit_replication":"https://pith.science/pith/LQSBQVRCLX6PHJHPRJIGFG2YWV/action/replication_record"}},"created_at":"2026-07-04T14:32:25.493029+00:00","updated_at":"2026-07-04T14:32:25.493029+00:00"}