{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:OXLYACQHYDE4QEBCFPDN5YTQSC","short_pith_number":"pith:OXLYACQH","canonical_record":{"source":{"id":"1308.4778","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-22T07:13:31Z","cross_cats_sorted":[],"title_canon_sha256":"0d9ac15c3e0efad98a9f7e333679474dd7b3e45ea01b15f4b017489f8c6b7db1","abstract_canon_sha256":"c1874f1886ad2727cb95c54f4d18d1b1b0926c62daa747b0aa6ffa3b8d0e4a06"},"schema_version":"1.0"},"canonical_sha256":"75d7800a07c0c9c810222bc6dee270909890a96e6ec65e039e7d04d9a4eb933f","source":{"kind":"arxiv","id":"1308.4778","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.4778","created_at":"2026-05-18T01:48:04Z"},{"alias_kind":"arxiv_version","alias_value":"1308.4778v3","created_at":"2026-05-18T01:48:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.4778","created_at":"2026-05-18T01:48:04Z"},{"alias_kind":"pith_short_12","alias_value":"OXLYACQHYDE4","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"OXLYACQHYDE4QEBC","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"OXLYACQH","created_at":"2026-05-18T12:27:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:OXLYACQHYDE4QEBCFPDN5YTQSC","target":"record","payload":{"canonical_record":{"source":{"id":"1308.4778","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-22T07:13:31Z","cross_cats_sorted":[],"title_canon_sha256":"0d9ac15c3e0efad98a9f7e333679474dd7b3e45ea01b15f4b017489f8c6b7db1","abstract_canon_sha256":"c1874f1886ad2727cb95c54f4d18d1b1b0926c62daa747b0aa6ffa3b8d0e4a06"},"schema_version":"1.0"},"canonical_sha256":"75d7800a07c0c9c810222bc6dee270909890a96e6ec65e039e7d04d9a4eb933f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:48:04.797205Z","signature_b64":"Ga5oYtMRU1679vbiPhx7m1ANdxKgKamX0ugl3Kay1d5mztsCTFDJBnonK9KQh/KDpHKZRZxE0GsdtBaRzHANDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"75d7800a07c0c9c810222bc6dee270909890a96e6ec65e039e7d04d9a4eb933f","last_reissued_at":"2026-05-18T01:48:04.796732Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:48:04.796732Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1308.4778","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:48:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gvi2aiqrMVJDH59e+Dl4FaPUA3/zkRJhz6Ia1Qjo+FzX2Oo5Ks1CPa0TCZNtjldnj14NVJg+9WFFQbhv+JslDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:29:59.350612Z"},"content_sha256":"fa0a6785cbac83a6215ed2a2e03370dac4a42c40283b729ff99bbc6d59b11da2","schema_version":"1.0","event_id":"sha256:fa0a6785cbac83a6215ed2a2e03370dac4a42c40283b729ff99bbc6d59b11da2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:OXLYACQHYDE4QEBCFPDN5YTQSC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Superspace formulation and correlation functions of 3d superconformal field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Amin A. Nizami, Tarun Sharma, V. Umesh","submitted_at":"2013-08-22T07:13:31Z","abstract_excerpt":"We study $3d$ SCFTs in the superspace formalism and discuss superfields and on-shell higher spin current multiplets in free $3d$ SCFTs with $\\mathcal{N}= 1,2,3,4$ and $6$ superconformal symmetry. For $\\mathcal{N}=1$ 3d SCFTs we determine the superconformal invariants in superspace needed for constructing 3-point functions of higher spin operators, find the non-linear relations between the invariants and consequently write down all the independent invariant structures, both parity even and odd, for various 3-point functions of higher spin operators."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.4778","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:48:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8qQKZkhU3jz1wxd1a0UVLtP0px0/xNyN350PJSe4SFsdhPBWcC1in5LWc+597OzaFwIYUry0I8jHk46vtG7tCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:29:59.351309Z"},"content_sha256":"2750d966a66cbd461e5023b8daa8105029f3ac7091851d817f9b3972440160ef","schema_version":"1.0","event_id":"sha256:2750d966a66cbd461e5023b8daa8105029f3ac7091851d817f9b3972440160ef"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OXLYACQHYDE4QEBCFPDN5YTQSC/bundle.json","state_url":"https://pith.science/pith/OXLYACQHYDE4QEBCFPDN5YTQSC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OXLYACQHYDE4QEBCFPDN5YTQSC/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-31T16:29:59Z","links":{"resolver":"https://pith.science/pith/OXLYACQHYDE4QEBCFPDN5YTQSC","bundle":"https://pith.science/pith/OXLYACQHYDE4QEBCFPDN5YTQSC/bundle.json","state":"https://pith.science/pith/OXLYACQHYDE4QEBCFPDN5YTQSC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OXLYACQHYDE4QEBCFPDN5YTQSC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:OXLYACQHYDE4QEBCFPDN5YTQSC","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"c1874f1886ad2727cb95c54f4d18d1b1b0926c62daa747b0aa6ffa3b8d0e4a06","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-22T07:13:31Z","title_canon_sha256":"0d9ac15c3e0efad98a9f7e333679474dd7b3e45ea01b15f4b017489f8c6b7db1"},"schema_version":"1.0","source":{"id":"1308.4778","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.4778","created_at":"2026-05-18T01:48:04Z"},{"alias_kind":"arxiv_version","alias_value":"1308.4778v3","created_at":"2026-05-18T01:48:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.4778","created_at":"2026-05-18T01:48:04Z"},{"alias_kind":"pith_short_12","alias_value":"OXLYACQHYDE4","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"OXLYACQHYDE4QEBC","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"OXLYACQH","created_at":"2026-05-18T12:27:54Z"}],"graph_snapshots":[{"event_id":"sha256:2750d966a66cbd461e5023b8daa8105029f3ac7091851d817f9b3972440160ef","target":"graph","created_at":"2026-05-18T01:48:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study $3d$ SCFTs in the superspace formalism and discuss superfields and on-shell higher spin current multiplets in free $3d$ SCFTs with $\\mathcal{N}= 1,2,3,4$ and $6$ superconformal symmetry. For $\\mathcal{N}=1$ 3d SCFTs we determine the superconformal invariants in superspace needed for constructing 3-point functions of higher spin operators, find the non-linear relations between the invariants and consequently write down all the independent invariant structures, both parity even and odd, for various 3-point functions of higher spin operators.","authors_text":"Amin A. Nizami, Tarun Sharma, V. Umesh","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-22T07:13:31Z","title":"Superspace formulation and correlation functions of 3d superconformal field theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.4778","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:fa0a6785cbac83a6215ed2a2e03370dac4a42c40283b729ff99bbc6d59b11da2","target":"record","created_at":"2026-05-18T01:48:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"c1874f1886ad2727cb95c54f4d18d1b1b0926c62daa747b0aa6ffa3b8d0e4a06","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-22T07:13:31Z","title_canon_sha256":"0d9ac15c3e0efad98a9f7e333679474dd7b3e45ea01b15f4b017489f8c6b7db1"},"schema_version":"1.0","source":{"id":"1308.4778","kind":"arxiv","version":3}},"canonical_sha256":"75d7800a07c0c9c810222bc6dee270909890a96e6ec65e039e7d04d9a4eb933f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"75d7800a07c0c9c810222bc6dee270909890a96e6ec65e039e7d04d9a4eb933f","first_computed_at":"2026-05-18T01:48:04.796732Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:48:04.796732Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ga5oYtMRU1679vbiPhx7m1ANdxKgKamX0ugl3Kay1d5mztsCTFDJBnonK9KQh/KDpHKZRZxE0GsdtBaRzHANDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:48:04.797205Z","signed_message":"canonical_sha256_bytes"},"source_id":"1308.4778","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fa0a6785cbac83a6215ed2a2e03370dac4a42c40283b729ff99bbc6d59b11da2","sha256:2750d966a66cbd461e5023b8daa8105029f3ac7091851d817f9b3972440160ef"],"state_sha256":"21575f49da68c969b3d26f75a484dc224c71aaa6fb1ef3a73b08b93e2161039a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Es9UGF8bDBpDaxtPPv4PID/hx2hN00yLdTWPaWwP98OFnvxQIzh4ZnW5WPj1i+qdWzHk1edU3OPCkWdt04jZBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T16:29:59.355970Z","bundle_sha256":"d4dc769580482dd5eb3a23dd55da604440958a6517a5b7a88a175e8a4b3d78f5"}}