{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:4TIYG6HQYBBTX3QKZGC3HTZQ47","short_pith_number":"pith:4TIYG6HQ","schema_version":"1.0","canonical_sha256":"e4d18378f0c0433bee0ac985b3cf30e7fbe5acc3808704fb14dc75088ec01c67","source":{"kind":"arxiv","id":"1403.7167","version":2},"attestation_state":"computed","paper":{"title":"More on Ramond-Ramond, SYM, WZ couplings and their corrections in IIA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Ehsan Hatefi","submitted_at":"2014-03-27T18:45:21Z","abstract_excerpt":"We obtain the closed form of the correlation function of one current and four spin operators (with different chiralities ) in type IIA superstring theory. The complete form of the S-matrix of one gauge , two fermions (with different chiralities) and one closed string Ramond-Ramond for all order $\\alpha'$ type IIA has been explored. Moreover, we make use of a different gauge fixing to be able to find out all the closed forms of $<V_{C} V_{A}V_{\\bar\\psi}V_{\\psi} >$ correlators. An infinite number of $t,s-$channel fermion poles of this S-matrix in the field theory of IIA is generated. Unlike the "},"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":"1403.7167","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-03-27T18:45:21Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"5ccc31942aa5e4fd4cae0b9eb4226af518f497cf3a913708aaba7ace1eb49ccb","abstract_canon_sha256":"a11205c1f4c13e7b1e2a726b461e5682f565550b7a4f23cf049f68f0f908aaea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:01.011829Z","signature_b64":"BmoL6IlO3wKIHELUJ3JAgKEJBvGPj7pE/0RcvMFSO5x0TTcl1gDkYSZ1z2QVJPCRYDpRDoXqYpVHJu+9pjhMCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4d18378f0c0433bee0ac985b3cf30e7fbe5acc3808704fb14dc75088ec01c67","last_reissued_at":"2026-05-18T02:39:01.011150Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:01.011150Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"More on Ramond-Ramond, SYM, WZ couplings and their corrections in IIA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Ehsan Hatefi","submitted_at":"2014-03-27T18:45:21Z","abstract_excerpt":"We obtain the closed form of the correlation function of one current and four spin operators (with different chiralities ) in type IIA superstring theory. The complete form of the S-matrix of one gauge , two fermions (with different chiralities) and one closed string Ramond-Ramond for all order $\\alpha'$ type IIA has been explored. Moreover, we make use of a different gauge fixing to be able to find out all the closed forms of $<V_{C} V_{A}V_{\\bar\\psi}V_{\\psi} >$ correlators. An infinite number of $t,s-$channel fermion poles of this S-matrix in the field theory of IIA is generated. Unlike the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.7167","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":""},"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":"1403.7167","created_at":"2026-05-18T02:39:01.011245+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.7167v2","created_at":"2026-05-18T02:39:01.011245+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.7167","created_at":"2026-05-18T02:39:01.011245+00:00"},{"alias_kind":"pith_short_12","alias_value":"4TIYG6HQYBBT","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_16","alias_value":"4TIYG6HQYBBTX3QK","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_8","alias_value":"4TIYG6HQ","created_at":"2026-05-18T12:28:14.216126+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/4TIYG6HQYBBTX3QKZGC3HTZQ47","json":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47.json","graph_json":"https://pith.science/api/pith-number/4TIYG6HQYBBTX3QKZGC3HTZQ47/graph.json","events_json":"https://pith.science/api/pith-number/4TIYG6HQYBBTX3QKZGC3HTZQ47/events.json","paper":"https://pith.science/paper/4TIYG6HQ"},"agent_actions":{"view_html":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47","download_json":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47.json","view_paper":"https://pith.science/paper/4TIYG6HQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.7167&json=true","fetch_graph":"https://pith.science/api/pith-number/4TIYG6HQYBBTX3QKZGC3HTZQ47/graph.json","fetch_events":"https://pith.science/api/pith-number/4TIYG6HQYBBTX3QKZGC3HTZQ47/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47/action/storage_attestation","attest_author":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47/action/author_attestation","sign_citation":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47/action/citation_signature","submit_replication":"https://pith.science/pith/4TIYG6HQYBBTX3QKZGC3HTZQ47/action/replication_record"}},"created_at":"2026-05-18T02:39:01.011245+00:00","updated_at":"2026-05-18T02:39:01.011245+00:00"}