{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NBAZFE6CAJ72N7MQLBUD6WB637","short_pith_number":"pith:NBAZFE6C","schema_version":"1.0","canonical_sha256":"68419293c2027fa6fd9058683f583edfe2ead4348d5e2fb41bdd1feeb620b157","source":{"kind":"arxiv","id":"1805.04413","version":2},"attestation_state":"computed","paper":{"title":"Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"I. L. Buchbinder, Konstantinos Koutrolikos, S. James Gates Jr.","submitted_at":"2018-05-11T14:15:21Z","abstract_excerpt":"We give an explicit superspace construction of higher spin conserved supercurrents built out of $4D,\\mathcal{N}=1$ massless supermultiplets of arbitrary spin. These supercurrents are gauge invariant and generate a large class of cubic interactions between a massless supermultiplet with superspin $Y_1=s_1+1/2$ and two massless supermultiplets of arbitrary superspin $Y_2$. These interactions are possible only for $s_1\\geq 2Y_2$. At the equality, the supercurrent acquires its simplest form and defines the supersymmetric, higher spin extension of the linearized Bel-Robinson tensor."},"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":"1805.04413","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-11T14:15:21Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"b92d731e748828018a1141dd8e7a8140af6996f3e76c3922d94162f681ca9b28","abstract_canon_sha256":"5b540d22bae4bfb0005cb4a44f358ea9827c9907a14fcdfe60544dc6a077ffed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:07:07.303956Z","signature_b64":"fGBR4wD2FBV2idMEHP4ieZW966SpURULLHm82IFEUQtesWCoqxPy9mIL22R9hnx0WHX+2Jbx5SILVIHJqLb6CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"68419293c2027fa6fd9058683f583edfe2ead4348d5e2fb41bdd1feeb620b157","last_reissued_at":"2026-05-18T00:07:07.303341Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:07:07.303341Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"I. L. Buchbinder, Konstantinos Koutrolikos, S. James Gates Jr.","submitted_at":"2018-05-11T14:15:21Z","abstract_excerpt":"We give an explicit superspace construction of higher spin conserved supercurrents built out of $4D,\\mathcal{N}=1$ massless supermultiplets of arbitrary spin. These supercurrents are gauge invariant and generate a large class of cubic interactions between a massless supermultiplet with superspin $Y_1=s_1+1/2$ and two massless supermultiplets of arbitrary superspin $Y_2$. These interactions are possible only for $s_1\\geq 2Y_2$. At the equality, the supercurrent acquires its simplest form and defines the supersymmetric, higher spin extension of the linearized Bel-Robinson tensor."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.04413","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":"1805.04413","created_at":"2026-05-18T00:07:07.303423+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.04413v2","created_at":"2026-05-18T00:07:07.303423+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.04413","created_at":"2026-05-18T00:07:07.303423+00:00"},{"alias_kind":"pith_short_12","alias_value":"NBAZFE6CAJ72","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NBAZFE6CAJ72N7MQ","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NBAZFE6C","created_at":"2026-05-18T12:32:40.477152+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/NBAZFE6CAJ72N7MQLBUD6WB637","json":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637.json","graph_json":"https://pith.science/api/pith-number/NBAZFE6CAJ72N7MQLBUD6WB637/graph.json","events_json":"https://pith.science/api/pith-number/NBAZFE6CAJ72N7MQLBUD6WB637/events.json","paper":"https://pith.science/paper/NBAZFE6C"},"agent_actions":{"view_html":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637","download_json":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637.json","view_paper":"https://pith.science/paper/NBAZFE6C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.04413&json=true","fetch_graph":"https://pith.science/api/pith-number/NBAZFE6CAJ72N7MQLBUD6WB637/graph.json","fetch_events":"https://pith.science/api/pith-number/NBAZFE6CAJ72N7MQLBUD6WB637/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637/action/storage_attestation","attest_author":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637/action/author_attestation","sign_citation":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637/action/citation_signature","submit_replication":"https://pith.science/pith/NBAZFE6CAJ72N7MQLBUD6WB637/action/replication_record"}},"created_at":"2026-05-18T00:07:07.303423+00:00","updated_at":"2026-05-18T00:07:07.303423+00:00"}