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Each higher spin-3/2 current contains the above antisymmetric second rank tensor and three symmetric (and traceless) second rank tensors (i.e. three antisymmetric almost complex structures contracted by the above antisymmetric tensor) in the product of spin-1/2 and spin-1 Kac-Moody currents r"},"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":"1411.0356","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-03T04:07:45Z","cross_cats_sorted":[],"title_canon_sha256":"9639358e7047536ad776b8fb58065310a8cdfa0df7e2931470c55108757f2f94","abstract_canon_sha256":"485f4e268752fd12bbe1cfa930aacd798a9ac6f7e3083d5a5fe3b05a00ebbb35"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:36.066728Z","signature_b64":"8TgTQz+q5ZV/NR5iQqQ/n3rhfqXQig7w99TgfD/q3LLRGfYFXVz+PQEKYbxLj2vhU9jSCmWcUBs+D8O7POXGDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c143e7df644a00db7d3e889f019f9e5a4a2b5dc81cf740710d17026c099a57b1","last_reissued_at":"2026-05-18T01:41:36.066074Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:36.066074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher Spin Currents in Wolf Space for Generic N","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Changhyun Ahn, Hyunsu Kim","submitted_at":"2014-11-03T04:07:45Z","abstract_excerpt":"We obtain the 16 higher spin currents with spins (1,3/2,3/2,2),(3/2, 2,2, 5/2), (3/2,2,2, 5/2) and (2,5/2,5/2,3) in the N=4 superconformal Wolf space coset SU(N+2)/[SU(N) x SU(2) x U(1)]. 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