{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:KQFY2L25NIA2Z7H7VA7EFZFP2G","short_pith_number":"pith:KQFY2L25","schema_version":"1.0","canonical_sha256":"540b8d2f5d6a01acfcffa83e42e4afd184e76efbb1eaf5a5cb5bd27414d4acbf","source":{"kind":"arxiv","id":"2108.01865","version":3},"attestation_state":"computed","paper":{"title":"Three-point functions of a superspin-2 current multiplet in 3D, N=1 superconformal theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Benjamin J. Stone, Evgeny I. Buchbinder","submitted_at":"2021-08-04T06:28:54Z","abstract_excerpt":"We consider $\\mathcal{N=1}$ superconformal field theories in three-dimensions possessing a conserved current multiplet $\\mathcal{F}_{ (\\alpha_{1} \\alpha_{2} \\alpha_{3} \\alpha_{4}) }$ which we refer to as the superspin-2 current multiplet. At the component level it contains a conserved spin-2 current different from the energy-momentum tensor and a conserved fermionic higher spin current of spin 5/2. Using a superspace formulation, we calculate correlation functions involving $\\mathcal{F}$, focusing particularly on the three-point function $ \\langle \\mathcal{F} \\mathcal{F} \\mathcal{F} \\rangle $."},"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":"2108.01865","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-08-04T06:28:54Z","cross_cats_sorted":[],"title_canon_sha256":"be3dbf5031ef87c201482de4544a9d08477387ffcf93a33373f84bb731f89cc8","abstract_canon_sha256":"ebbafcf017bf04d81e0c9d88ebc1c262ce26b759d714fc33c58d09d511176c3e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:31:29.404461Z","signature_b64":"i3paXENv0IMJmuW7YGb2xHJxv8CO+lliwEsbcoZblzW9YEN8nobzx73ZojQdu6Fn9yOgLIR/EoOHRD0NmfPTBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"540b8d2f5d6a01acfcffa83e42e4afd184e76efbb1eaf5a5cb5bd27414d4acbf","last_reissued_at":"2026-07-05T03:31:29.404043Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:31:29.404043Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three-point functions of a superspin-2 current multiplet in 3D, N=1 superconformal theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Benjamin J. Stone, Evgeny I. Buchbinder","submitted_at":"2021-08-04T06:28:54Z","abstract_excerpt":"We consider $\\mathcal{N=1}$ superconformal field theories in three-dimensions possessing a conserved current multiplet $\\mathcal{F}_{ (\\alpha_{1} \\alpha_{2} \\alpha_{3} \\alpha_{4}) }$ which we refer to as the superspin-2 current multiplet. At the component level it contains a conserved spin-2 current different from the energy-momentum tensor and a conserved fermionic higher spin current of spin 5/2. Using a superspace formulation, we calculate correlation functions involving $\\mathcal{F}$, focusing particularly on the three-point function $ \\langle \\mathcal{F} \\mathcal{F} \\mathcal{F} \\rangle $."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2108.01865","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2108.01865/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2108.01865","created_at":"2026-07-05T03:31:29.404097+00:00"},{"alias_kind":"arxiv_version","alias_value":"2108.01865v3","created_at":"2026-07-05T03:31:29.404097+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2108.01865","created_at":"2026-07-05T03:31:29.404097+00:00"},{"alias_kind":"pith_short_12","alias_value":"KQFY2L25NIA2","created_at":"2026-07-05T03:31:29.404097+00:00"},{"alias_kind":"pith_short_16","alias_value":"KQFY2L25NIA2Z7H7","created_at":"2026-07-05T03:31:29.404097+00:00"},{"alias_kind":"pith_short_8","alias_value":"KQFY2L25","created_at":"2026-07-05T03:31:29.404097+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.21633","citing_title":"Lectures on the Spinor and Twistor Formalism in 3D Conformal Field Theory","ref_index":89,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G","json":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G.json","graph_json":"https://pith.science/api/pith-number/KQFY2L25NIA2Z7H7VA7EFZFP2G/graph.json","events_json":"https://pith.science/api/pith-number/KQFY2L25NIA2Z7H7VA7EFZFP2G/events.json","paper":"https://pith.science/paper/KQFY2L25"},"agent_actions":{"view_html":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G","download_json":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G.json","view_paper":"https://pith.science/paper/KQFY2L25","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2108.01865&json=true","fetch_graph":"https://pith.science/api/pith-number/KQFY2L25NIA2Z7H7VA7EFZFP2G/graph.json","fetch_events":"https://pith.science/api/pith-number/KQFY2L25NIA2Z7H7VA7EFZFP2G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G/action/storage_attestation","attest_author":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G/action/author_attestation","sign_citation":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G/action/citation_signature","submit_replication":"https://pith.science/pith/KQFY2L25NIA2Z7H7VA7EFZFP2G/action/replication_record"}},"created_at":"2026-07-05T03:31:29.404097+00:00","updated_at":"2026-07-05T03:31:29.404097+00:00"}