{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:VFVFPHQXGCH7HZ52HU2PYVPEZD","short_pith_number":"pith:VFVFPHQX","schema_version":"1.0","canonical_sha256":"a96a579e17308ff3e7ba3d34fc55e4c8dd8fed3c6d5b120ad65d826fef3feb07","source":{"kind":"arxiv","id":"1605.01386","version":1},"attestation_state":"computed","paper":{"title":"Composite operators and form factors in N=4 SYM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dmitry Chicherin, Emery Sokatchev","submitted_at":"2016-05-04T19:16:01Z","abstract_excerpt":"We construct the most general composite operators of N = 4 SYM in Lorentz harmonic chiral ($\\approx$ twistor) superspace. The operators are built from the SYM supercurvature which is nonpolynomial in the chiral gauge prepotentials. We reconstruct the full nonchiral dependence of the supercurvature. We compute all tree-level MHV form factors via the LSZ redcution procedure with on-shell states made of the same supercurvature."},"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":"1605.01386","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-05-04T19:16:01Z","cross_cats_sorted":[],"title_canon_sha256":"06535a501e4396082ad61b719b81276ac2f0856b6a100963180d0f658b3e54c3","abstract_canon_sha256":"bd369fd7f03724fcbfb2595caa5d5d4ee0e6963ac576c80c6e7c720f1e3b5981"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:41.852697Z","signature_b64":"b9uUqMwMB16rca9gbZLrl4gN64BQDq/40G4r0HNXeWPIlTs4uMGD3i1+ImdGZeqmKwuO5TPleja/+ASojcFJDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a96a579e17308ff3e7ba3d34fc55e4c8dd8fed3c6d5b120ad65d826fef3feb07","last_reissued_at":"2026-05-18T00:41:41.852227Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:41.852227Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Composite operators and form factors in N=4 SYM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dmitry Chicherin, Emery Sokatchev","submitted_at":"2016-05-04T19:16:01Z","abstract_excerpt":"We construct the most general composite operators of N = 4 SYM in Lorentz harmonic chiral ($\\approx$ twistor) superspace. The operators are built from the SYM supercurvature which is nonpolynomial in the chiral gauge prepotentials. We reconstruct the full nonchiral dependence of the supercurvature. We compute all tree-level MHV form factors via the LSZ redcution procedure with on-shell states made of the same supercurvature."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.01386","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":"1605.01386","created_at":"2026-05-18T00:41:41.852300+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.01386v1","created_at":"2026-05-18T00:41:41.852300+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.01386","created_at":"2026-05-18T00:41:41.852300+00:00"},{"alias_kind":"pith_short_12","alias_value":"VFVFPHQXGCH7","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_16","alias_value":"VFVFPHQXGCH7HZ52","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_8","alias_value":"VFVFPHQX","created_at":"2026-05-18T12:30:48.956258+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.17168","citing_title":"Associativity is enough: an all-orders 2d chiral algebra for 4d form factors","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD","json":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD.json","graph_json":"https://pith.science/api/pith-number/VFVFPHQXGCH7HZ52HU2PYVPEZD/graph.json","events_json":"https://pith.science/api/pith-number/VFVFPHQXGCH7HZ52HU2PYVPEZD/events.json","paper":"https://pith.science/paper/VFVFPHQX"},"agent_actions":{"view_html":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD","download_json":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD.json","view_paper":"https://pith.science/paper/VFVFPHQX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.01386&json=true","fetch_graph":"https://pith.science/api/pith-number/VFVFPHQXGCH7HZ52HU2PYVPEZD/graph.json","fetch_events":"https://pith.science/api/pith-number/VFVFPHQXGCH7HZ52HU2PYVPEZD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD/action/storage_attestation","attest_author":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD/action/author_attestation","sign_citation":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD/action/citation_signature","submit_replication":"https://pith.science/pith/VFVFPHQXGCH7HZ52HU2PYVPEZD/action/replication_record"}},"created_at":"2026-05-18T00:41:41.852300+00:00","updated_at":"2026-05-18T00:41:41.852300+00:00"}