{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:Q3ZWPU3NFP2TBGNVRMMSWBQBVF","short_pith_number":"pith:Q3ZWPU3N","schema_version":"1.0","canonical_sha256":"86f367d36d2bf53099b58b192b0601a96dba694424740c1f01e8724fff9400ee","source":{"kind":"arxiv","id":"hep-th/0703084","version":1},"attestation_state":"computed","paper":{"title":"Bootstrap in Supersymmetric Liouville Field Theory. I. NS Sector","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.Belavin, Al.Zamolodchikov, A.Neveu, V.Belavin","submitted_at":"2007-03-08T17:26:54Z","abstract_excerpt":"A four point function of basic Neveu-Schwarz exponential fields is constructed in the N = 1 supersymmetric Liouville field theory. Although the basic NS structure constants were known previously, we present a new derivation, based on a singular vector decoupling in the NS sector. This allows to stay completely inside the NS sector of the space of states, without referencing to the Ramond fields. The four-point construction involves also the NS blocks, for which we suggest a new recursion representation, the so-called elliptic one. The bootstrap conditions for this four point correlation functi"},"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/0703084","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-03-08T17:26:54Z","cross_cats_sorted":[],"title_canon_sha256":"228f58a2ae42bbcf94400a6ac982aa2b0f50577ead70e9189642a4a547fb8ad8","abstract_canon_sha256":"0aecb83aa1624bc62e7dfa9b48197ef753d715682d7454ac65df031b8b84fd5e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:28:54.048466Z","signature_b64":"MVpjI4oCI6pYY0HRDb85REXrnW2375tNil7jYT1a7EAdkXzvxmnlBK14s6RbVVg0LY4KAvYjiGDzIM98EhilBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"86f367d36d2bf53099b58b192b0601a96dba694424740c1f01e8724fff9400ee","last_reissued_at":"2026-07-04T15:28:54.048054Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:28:54.048054Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bootstrap in Supersymmetric Liouville Field Theory. I. NS Sector","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.Belavin, Al.Zamolodchikov, A.Neveu, V.Belavin","submitted_at":"2007-03-08T17:26:54Z","abstract_excerpt":"A four point function of basic Neveu-Schwarz exponential fields is constructed in the N = 1 supersymmetric Liouville field theory. Although the basic NS structure constants were known previously, we present a new derivation, based on a singular vector decoupling in the NS sector. This allows to stay completely inside the NS sector of the space of states, without referencing to the Ramond fields. The four-point construction involves also the NS blocks, for which we suggest a new recursion representation, the so-called elliptic one. The bootstrap conditions for this four point correlation functi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0703084","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/0703084/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/0703084","created_at":"2026-07-04T15:28:54.048117+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0703084v1","created_at":"2026-07-04T15:28:54.048117+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0703084","created_at":"2026-07-04T15:28:54.048117+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q3ZWPU3NFP2T","created_at":"2026-07-04T15:28:54.048117+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q3ZWPU3NFP2TBGNV","created_at":"2026-07-04T15:28:54.048117+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q3ZWPU3N","created_at":"2026-07-04T15:28:54.048117+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.26038","citing_title":"The Super Virasoro Minimal String from 3d Supergravity","ref_index":57,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF","json":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF.json","graph_json":"https://pith.science/api/pith-number/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/graph.json","events_json":"https://pith.science/api/pith-number/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/events.json","paper":"https://pith.science/paper/Q3ZWPU3N"},"agent_actions":{"view_html":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF","download_json":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF.json","view_paper":"https://pith.science/paper/Q3ZWPU3N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0703084&json=true","fetch_graph":"https://pith.science/api/pith-number/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/graph.json","fetch_events":"https://pith.science/api/pith-number/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/action/storage_attestation","attest_author":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/action/author_attestation","sign_citation":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/action/citation_signature","submit_replication":"https://pith.science/pith/Q3ZWPU3NFP2TBGNVRMMSWBQBVF/action/replication_record"}},"created_at":"2026-07-04T15:28:54.048117+00:00","updated_at":"2026-07-04T15:28:54.048117+00:00"}