{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1991:7X2JIS7CXO43GEVM4TBYSZLJL2","short_pith_number":"pith:7X2JIS7C","schema_version":"1.0","canonical_sha256":"fdf4944be2bbb9b312ace4c38965695e8784bccfb05df10987267f956751306b","source":{"kind":"arxiv","id":"hep-th/9108021","version":2},"attestation_state":"computed","paper":{"title":"The big picture","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M.T. Hatsuda, N. Berkovits, W. Siegel","submitted_at":"1991-08-26T21:15:24Z","abstract_excerpt":"We discuss the conformal field theory and string field theory of the NSR superstring using a BRST operator with a nonminimal term, which allows all bosonic ghost modes to be paired into creation and annihilation operators. Vertex operators for the Neveu-Schwarz and Ramond sectors have the same ghost number, as do string fields. The kinetic and interaction terms are the same for Neveu-Schwarz as for Ramond string fields, so spacetime supersymmetry is closer to being manifest. The kinetic terms and supersymmetry don't mix levels, simplifying component analysis and gauge fixing."},"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/9108021","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1991-08-26T21:15:24Z","cross_cats_sorted":[],"title_canon_sha256":"bf2a85307bdb9f41e8d27b28434d5afd3c6e303260fc1697d70bcc29038c246d","abstract_canon_sha256":"a74f6442f64878f41e1cb5019ae1b0d73741bfe0e5ff1725440fa13a48d209b5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:54:58.701462Z","signature_b64":"vXkdlFhb9mrxM2uyyHCZjuGO9rUajYjy9VPBynWpH/bYg8/UTNZz+ULUE6lcFEddoBwq5zgenb2mdyPbewEQCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fdf4944be2bbb9b312ace4c38965695e8784bccfb05df10987267f956751306b","last_reissued_at":"2026-07-04T15:54:58.701091Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:54:58.701091Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The big picture","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M.T. Hatsuda, N. Berkovits, W. Siegel","submitted_at":"1991-08-26T21:15:24Z","abstract_excerpt":"We discuss the conformal field theory and string field theory of the NSR superstring using a BRST operator with a nonminimal term, which allows all bosonic ghost modes to be paired into creation and annihilation operators. Vertex operators for the Neveu-Schwarz and Ramond sectors have the same ghost number, as do string fields. The kinetic and interaction terms are the same for Neveu-Schwarz as for Ramond string fields, so spacetime supersymmetry is closer to being manifest. The kinetic terms and supersymmetry don't mix levels, simplifying component analysis and gauge fixing."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9108021","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9108021/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/9108021","created_at":"2026-07-04T15:54:58.701153+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9108021v2","created_at":"2026-07-04T15:54:58.701153+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9108021","created_at":"2026-07-04T15:54:58.701153+00:00"},{"alias_kind":"pith_short_12","alias_value":"7X2JIS7CXO43","created_at":"2026-07-04T15:54:58.701153+00:00"},{"alias_kind":"pith_short_16","alias_value":"7X2JIS7CXO43GEVM","created_at":"2026-07-04T15:54:58.701153+00:00"},{"alias_kind":"pith_short_8","alias_value":"7X2JIS7C","created_at":"2026-07-04T15:54:58.701153+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/7X2JIS7CXO43GEVM4TBYSZLJL2","json":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2.json","graph_json":"https://pith.science/api/pith-number/7X2JIS7CXO43GEVM4TBYSZLJL2/graph.json","events_json":"https://pith.science/api/pith-number/7X2JIS7CXO43GEVM4TBYSZLJL2/events.json","paper":"https://pith.science/paper/7X2JIS7C"},"agent_actions":{"view_html":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2","download_json":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2.json","view_paper":"https://pith.science/paper/7X2JIS7C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9108021&json=true","fetch_graph":"https://pith.science/api/pith-number/7X2JIS7CXO43GEVM4TBYSZLJL2/graph.json","fetch_events":"https://pith.science/api/pith-number/7X2JIS7CXO43GEVM4TBYSZLJL2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2/action/storage_attestation","attest_author":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2/action/author_attestation","sign_citation":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2/action/citation_signature","submit_replication":"https://pith.science/pith/7X2JIS7CXO43GEVM4TBYSZLJL2/action/replication_record"}},"created_at":"2026-07-04T15:54:58.701153+00:00","updated_at":"2026-07-04T15:54:58.701153+00:00"}