{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:6AGWFRYF2OW7UGKOMU6RKJMF6I","short_pith_number":"pith:6AGWFRYF","schema_version":"1.0","canonical_sha256":"f00d62c705d3adfa194e653d152585f218b4ef62fdc07ef551cb7e64d1b73036","source":{"kind":"arxiv","id":"hep-th/0509165","version":1},"attestation_state":"computed","paper":{"title":"Pure-spinor superstrings in d=2,4,6","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Niclas Wyllard","submitted_at":"2005-09-21T13:41:25Z","abstract_excerpt":"We continue the study of the d=2,4,6 pure-spinor superstring models introduced in [1]. By explicitly solving the pure-spinor constraint we show that these theories have vanishing central charge and work out the (covariant) current algebra for the Lorentz currents. We argue that these super-Poincare covariant models may be thought of as compactifications of the superstring on CY_{4,3,2}, and take some steps toward making this precise by constructing a map to the RNS superstring variables. We also discuss the relation to the so called hybrid superstrings, which describe the same type of compacti"},"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/0509165","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-09-21T13:41:25Z","cross_cats_sorted":[],"title_canon_sha256":"dc92a132bc83b3468631d7534279c43013f2fc27c75e6d6c9bebf37b6cfd5073","abstract_canon_sha256":"516e91e198d26da3a0928db196d9a68aaf39341ac3feb1efc4b55d3d1a7c2598"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:56:20.026565Z","signature_b64":"A71kjRSTGTIyIV+QIPE3cxmNXdMW7k8MayxZHE/J5NvonZQEh0ByseNg1K/HbAKWviC0HwLOjEcpByMdYdVsBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f00d62c705d3adfa194e653d152585f218b4ef62fdc07ef551cb7e64d1b73036","last_reissued_at":"2026-07-04T16:56:20.026163Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:56:20.026163Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pure-spinor superstrings in d=2,4,6","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Niclas Wyllard","submitted_at":"2005-09-21T13:41:25Z","abstract_excerpt":"We continue the study of the d=2,4,6 pure-spinor superstring models introduced in [1]. By explicitly solving the pure-spinor constraint we show that these theories have vanishing central charge and work out the (covariant) current algebra for the Lorentz currents. We argue that these super-Poincare covariant models may be thought of as compactifications of the superstring on CY_{4,3,2}, and take some steps toward making this precise by constructing a map to the RNS superstring variables. We also discuss the relation to the so called hybrid superstrings, which describe the same type of compacti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0509165","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/0509165/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/0509165","created_at":"2026-07-04T16:56:20.026224+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0509165v1","created_at":"2026-07-04T16:56:20.026224+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0509165","created_at":"2026-07-04T16:56:20.026224+00:00"},{"alias_kind":"pith_short_12","alias_value":"6AGWFRYF2OW7","created_at":"2026-07-04T16:56:20.026224+00:00"},{"alias_kind":"pith_short_16","alias_value":"6AGWFRYF2OW7UGKO","created_at":"2026-07-04T16:56:20.026224+00:00"},{"alias_kind":"pith_short_8","alias_value":"6AGWFRYF","created_at":"2026-07-04T16:56:20.026224+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.06194","citing_title":"Vertex operators for the superstring with manifest $d=6$ $\\mathcal{N}=1$ supersymmetry","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I","json":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I.json","graph_json":"https://pith.science/api/pith-number/6AGWFRYF2OW7UGKOMU6RKJMF6I/graph.json","events_json":"https://pith.science/api/pith-number/6AGWFRYF2OW7UGKOMU6RKJMF6I/events.json","paper":"https://pith.science/paper/6AGWFRYF"},"agent_actions":{"view_html":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I","download_json":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I.json","view_paper":"https://pith.science/paper/6AGWFRYF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0509165&json=true","fetch_graph":"https://pith.science/api/pith-number/6AGWFRYF2OW7UGKOMU6RKJMF6I/graph.json","fetch_events":"https://pith.science/api/pith-number/6AGWFRYF2OW7UGKOMU6RKJMF6I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I/action/storage_attestation","attest_author":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I/action/author_attestation","sign_citation":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I/action/citation_signature","submit_replication":"https://pith.science/pith/6AGWFRYF2OW7UGKOMU6RKJMF6I/action/replication_record"}},"created_at":"2026-07-04T16:56:20.026224+00:00","updated_at":"2026-07-04T16:56:20.026224+00:00"}