{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:QNKXILM5GAOJNPXFKZ3P2ZFKUY","short_pith_number":"pith:QNKXILM5","canonical_record":{"source":{"id":"1507.00221","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-07-01T13:19:48Z","cross_cats_sorted":[],"title_canon_sha256":"b7392c32c95beba07c886ee972948c4a311d003f6799cc18a1fc29dfba1f4dd9","abstract_canon_sha256":"6e537284194c0437b96c375a81f40ba1ea2451c104e023192941ce12424123c5"},"schema_version":"1.0"},"canonical_sha256":"8355742d9d301c96bee55676fd64aaa63b75fc936f2317813f7a434d37219b16","source":{"kind":"arxiv","id":"1507.00221","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.00221","created_at":"2026-05-18T01:31:37Z"},{"alias_kind":"arxiv_version","alias_value":"1507.00221v1","created_at":"2026-05-18T01:31:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.00221","created_at":"2026-05-18T01:31:37Z"},{"alias_kind":"pith_short_12","alias_value":"QNKXILM5GAOJ","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"QNKXILM5GAOJNPXF","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"QNKXILM5","created_at":"2026-05-18T12:29:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:QNKXILM5GAOJNPXFKZ3P2ZFKUY","target":"record","payload":{"canonical_record":{"source":{"id":"1507.00221","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-07-01T13:19:48Z","cross_cats_sorted":[],"title_canon_sha256":"b7392c32c95beba07c886ee972948c4a311d003f6799cc18a1fc29dfba1f4dd9","abstract_canon_sha256":"6e537284194c0437b96c375a81f40ba1ea2451c104e023192941ce12424123c5"},"schema_version":"1.0"},"canonical_sha256":"8355742d9d301c96bee55676fd64aaa63b75fc936f2317813f7a434d37219b16","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:31:37.947638Z","signature_b64":"qZKaqqcXNrT4t+Oi9lze1vaFt7IdT4+giztSfxnmEk/TpFJSFDUrASS+fqG+zfpT+fw9iR0r8K6ltpKVdfyVAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8355742d9d301c96bee55676fd64aaa63b75fc936f2317813f7a434d37219b16","last_reissued_at":"2026-05-18T01:31:37.947134Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:31:37.947134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1507.00221","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:31:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wHYtS2pD6qdnk0r/0zGsrQk3Ij+l1RvrK6K3uj1/Sng8KVYmiuA6YE0vNHfaVL/JTwy6/hnzFB3gEhctiClnAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T23:28:17.870747Z"},"content_sha256":"191788a38492d3cedd44f31ded561493c47ca3bd80c7f20f94b9fc266425a6f5","schema_version":"1.0","event_id":"sha256:191788a38492d3cedd44f31ded561493c47ca3bd80c7f20f94b9fc266425a6f5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:QNKXILM5GAOJNPXFKZ3P2ZFKUY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Implications of N=4 superconformal symmetry in three spacetime dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Evgeny I. Buchbinder, Igor B. Samsonov, Sergei M. Kuzenko","submitted_at":"2015-07-01T13:19:48Z","abstract_excerpt":"We study implications of N=4 superconformal symmetry in three dimensions, thus extending our earlier results in arXiv:1503.04961 devoted to the N=1,2,3 cases. We show that the three-point function of the supercurrent in N=4 superconformal field theories contains two linearly independent forms. However, only one of these structures contributes to the three-point function of the energy-momentum tensor and the other one is present in those N=4 superconformal theories which are not invariant under the mirror map. We point out that general N=4 superconformal field theories admit two inequivalent fl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.00221","kind":"arxiv","version":1},"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":"2026-05-18T01:31:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nEE5lhnccreyVUkWjSxe4ML5eeI8VWw/q7hCOcwmZIORRLV34qYeariHIGQ8DiTmH9hQM9+WnSMO9nELx99sCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T23:28:17.871300Z"},"content_sha256":"bfe1df2e6e1835f606f3e076ca23e8aa845b5ed9739c047b6700f726dae5aa5e","schema_version":"1.0","event_id":"sha256:bfe1df2e6e1835f606f3e076ca23e8aa845b5ed9739c047b6700f726dae5aa5e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY/bundle.json","state_url":"https://pith.science/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY/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":"2026-05-31T23:28:17Z","links":{"resolver":"https://pith.science/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY","bundle":"https://pith.science/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY/bundle.json","state":"https://pith.science/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QNKXILM5GAOJNPXFKZ3P2ZFKUY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:QNKXILM5GAOJNPXFKZ3P2ZFKUY","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":"6e537284194c0437b96c375a81f40ba1ea2451c104e023192941ce12424123c5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-07-01T13:19:48Z","title_canon_sha256":"b7392c32c95beba07c886ee972948c4a311d003f6799cc18a1fc29dfba1f4dd9"},"schema_version":"1.0","source":{"id":"1507.00221","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.00221","created_at":"2026-05-18T01:31:37Z"},{"alias_kind":"arxiv_version","alias_value":"1507.00221v1","created_at":"2026-05-18T01:31:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.00221","created_at":"2026-05-18T01:31:37Z"},{"alias_kind":"pith_short_12","alias_value":"QNKXILM5GAOJ","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"QNKXILM5GAOJNPXF","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"QNKXILM5","created_at":"2026-05-18T12:29:37Z"}],"graph_snapshots":[{"event_id":"sha256:bfe1df2e6e1835f606f3e076ca23e8aa845b5ed9739c047b6700f726dae5aa5e","target":"graph","created_at":"2026-05-18T01:31:37Z","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 implications of N=4 superconformal symmetry in three dimensions, thus extending our earlier results in arXiv:1503.04961 devoted to the N=1,2,3 cases. We show that the three-point function of the supercurrent in N=4 superconformal field theories contains two linearly independent forms. However, only one of these structures contributes to the three-point function of the energy-momentum tensor and the other one is present in those N=4 superconformal theories which are not invariant under the mirror map. We point out that general N=4 superconformal field theories admit two inequivalent fl","authors_text":"Evgeny I. Buchbinder, Igor B. Samsonov, Sergei M. Kuzenko","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-07-01T13:19:48Z","title":"Implications of N=4 superconformal symmetry in three spacetime dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.00221","kind":"arxiv","version":1},"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":"sha256:191788a38492d3cedd44f31ded561493c47ca3bd80c7f20f94b9fc266425a6f5","target":"record","created_at":"2026-05-18T01:31:37Z","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":"6e537284194c0437b96c375a81f40ba1ea2451c104e023192941ce12424123c5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-07-01T13:19:48Z","title_canon_sha256":"b7392c32c95beba07c886ee972948c4a311d003f6799cc18a1fc29dfba1f4dd9"},"schema_version":"1.0","source":{"id":"1507.00221","kind":"arxiv","version":1}},"canonical_sha256":"8355742d9d301c96bee55676fd64aaa63b75fc936f2317813f7a434d37219b16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8355742d9d301c96bee55676fd64aaa63b75fc936f2317813f7a434d37219b16","first_computed_at":"2026-05-18T01:31:37.947134Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:31:37.947134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qZKaqqcXNrT4t+Oi9lze1vaFt7IdT4+giztSfxnmEk/TpFJSFDUrASS+fqG+zfpT+fw9iR0r8K6ltpKVdfyVAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:31:37.947638Z","signed_message":"canonical_sha256_bytes"},"source_id":"1507.00221","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:191788a38492d3cedd44f31ded561493c47ca3bd80c7f20f94b9fc266425a6f5","sha256:bfe1df2e6e1835f606f3e076ca23e8aa845b5ed9739c047b6700f726dae5aa5e"],"state_sha256":"79271bdd84e79b548cf8b6817397c7cced221e4c78df7f045e000f5918d6024f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z0s2H/VUerCbWBOFbSJqoYRF+ialonoJW+5Rmhe391Im/hX/yXboF4pfIrGu+oZI7Qy0c8/Kq5ywhinbb1BUBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T23:28:17.874301Z","bundle_sha256":"5b161e9525fd20d886ba71535d82078dcd328cd126c70ac9e7abb560267df948"}}