{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:7DGY33TIWX2NDBYHZ4D575FCIT","short_pith_number":"pith:7DGY33TI","schema_version":"1.0","canonical_sha256":"f8cd8dee68b5f4d18707cf07dff4a244c3971412705a181942874fe73c38376c","source":{"kind":"arxiv","id":"1104.2605","version":1},"attestation_state":"computed","paper":{"title":"Super Yang-Mills Theory as a Twistor Matrix Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Herman Verlinde, Jonathan J. Heckman","submitted_at":"2011-04-13T20:03:36Z","abstract_excerpt":"We introduce a covariant finite regulator for N = 4 super Yang-Mills theory on S^4. Our formulation is based on holomorphic Chern-Simons theory on twistor space. By switching on a large background flux, the twistor space dissolves into a fuzzy geometry, with a finite number of points. The large N continuum limit of the matrix model naturally approaches ordinary N = 4 SYM. We comment on the relation between our model and the 4D quantum Hall effect."},"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":"1104.2605","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-13T20:03:36Z","cross_cats_sorted":[],"title_canon_sha256":"26715d8d013d74e25fd97eaa15002670653d719b13a0d28ba5d7424539f444db","abstract_canon_sha256":"cc6e242c1b16667e1ea2fd321fadc1aafde29bbaddd8412836a67711cfa5162a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:24:27.238753Z","signature_b64":"OIVT4HCEMsPB80gjb+K/QRSJ6SfRN2bbhIAcYpQ9iMN3FIOXRIYiEHOgavTTf3i6+fEFv96qh4mdnmh4MZlKBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f8cd8dee68b5f4d18707cf07dff4a244c3971412705a181942874fe73c38376c","last_reissued_at":"2026-05-18T04:24:27.238156Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:24:27.238156Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Super Yang-Mills Theory as a Twistor Matrix Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Herman Verlinde, Jonathan J. Heckman","submitted_at":"2011-04-13T20:03:36Z","abstract_excerpt":"We introduce a covariant finite regulator for N = 4 super Yang-Mills theory on S^4. Our formulation is based on holomorphic Chern-Simons theory on twistor space. By switching on a large background flux, the twistor space dissolves into a fuzzy geometry, with a finite number of points. The large N continuum limit of the matrix model naturally approaches ordinary N = 4 SYM. We comment on the relation between our model and the 4D quantum Hall effect."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.2605","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":""},"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":"1104.2605","created_at":"2026-05-18T04:24:27.238236+00:00"},{"alias_kind":"arxiv_version","alias_value":"1104.2605v1","created_at":"2026-05-18T04:24:27.238236+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.2605","created_at":"2026-05-18T04:24:27.238236+00:00"},{"alias_kind":"pith_short_12","alias_value":"7DGY33TIWX2N","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"7DGY33TIWX2NDBYH","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"7DGY33TI","created_at":"2026-05-18T12:26:22.705136+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/7DGY33TIWX2NDBYHZ4D575FCIT","json":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT.json","graph_json":"https://pith.science/api/pith-number/7DGY33TIWX2NDBYHZ4D575FCIT/graph.json","events_json":"https://pith.science/api/pith-number/7DGY33TIWX2NDBYHZ4D575FCIT/events.json","paper":"https://pith.science/paper/7DGY33TI"},"agent_actions":{"view_html":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT","download_json":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT.json","view_paper":"https://pith.science/paper/7DGY33TI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1104.2605&json=true","fetch_graph":"https://pith.science/api/pith-number/7DGY33TIWX2NDBYHZ4D575FCIT/graph.json","fetch_events":"https://pith.science/api/pith-number/7DGY33TIWX2NDBYHZ4D575FCIT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT/action/storage_attestation","attest_author":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT/action/author_attestation","sign_citation":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT/action/citation_signature","submit_replication":"https://pith.science/pith/7DGY33TIWX2NDBYHZ4D575FCIT/action/replication_record"}},"created_at":"2026-05-18T04:24:27.238236+00:00","updated_at":"2026-05-18T04:24:27.238236+00:00"}