{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:LBF4AWLHFRSCMECSQAAD47YO7A","short_pith_number":"pith:LBF4AWLH","canonical_record":{"source":{"id":"1712.02800","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-12-07T19:00:08Z","cross_cats_sorted":[],"title_canon_sha256":"6a6f33e72913614fbef79f74728c5ca86d9dda4e8d73ef6d98e446402b3a545a","abstract_canon_sha256":"64aabaf97aef056fe60892cb526a3e334a257385ded71701ac990bfd5ecdab10"},"schema_version":"1.0"},"canonical_sha256":"584bc059672c6426105280003e7f0ef801a533f711c2b136593635581bcb9c41","source":{"kind":"arxiv","id":"1712.02800","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.02800","created_at":"2026-05-18T00:04:59Z"},{"alias_kind":"arxiv_version","alias_value":"1712.02800v3","created_at":"2026-05-18T00:04:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.02800","created_at":"2026-05-18T00:04:59Z"},{"alias_kind":"pith_short_12","alias_value":"LBF4AWLHFRSC","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LBF4AWLHFRSCMECS","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LBF4AWLH","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:LBF4AWLHFRSCMECSQAAD47YO7A","target":"record","payload":{"canonical_record":{"source":{"id":"1712.02800","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-12-07T19:00:08Z","cross_cats_sorted":[],"title_canon_sha256":"6a6f33e72913614fbef79f74728c5ca86d9dda4e8d73ef6d98e446402b3a545a","abstract_canon_sha256":"64aabaf97aef056fe60892cb526a3e334a257385ded71701ac990bfd5ecdab10"},"schema_version":"1.0"},"canonical_sha256":"584bc059672c6426105280003e7f0ef801a533f711c2b136593635581bcb9c41","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:59.936999Z","signature_b64":"cCbTdmfj4H92jGbrPrq+Va0su5l3XB+/nHk63ZQxw3pmLaXtYn18tNtQBTbPjYN/t963qHN2I/0lRyd7q7UPDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"584bc059672c6426105280003e7f0ef801a533f711c2b136593635581bcb9c41","last_reissued_at":"2026-05-18T00:04:59.936581Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:59.936581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1712.02800","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":"2026-05-18T00:04:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ohg19SjurWPsZQyFXxrGJVX2s7EgKp4dn19K2fn+3/mx0AH7NVYI17IlNUTWnZq4b2UOEZ5MlnLfPkyZ44ahAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:09:14.354656Z"},"content_sha256":"58a0c0949a068f2be2a40b9efc2ec8d9d5d70092bad2f7f127ed7a5d6302227f","schema_version":"1.0","event_id":"sha256:58a0c0949a068f2be2a40b9efc2ec8d9d5d70092bad2f7f127ed7a5d6302227f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:LBF4AWLHFRSCMECSQAAD47YO7A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On Superconformal Four-Point Mellin Amplitudes in Dimension $d>2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Xinan Zhou","submitted_at":"2017-12-07T19:00:08Z","abstract_excerpt":"We present a universal treatment for imposing superconformal constraints on Mellin amplitudes for $\\mathrm{SCFT_d}$ with $3\\leq d\\leq 6$. This leads to a new technique to compute holographic correlators, which is similar but complementary to the ones introduced in [1,2]. We apply this technique to theories in various spacetime dimensions. In addition to reproducing known results, we obtain a simple expression for next-next-to-extremal four-point functions in $AdS_7\\times S^4$. We also use this machinery on $AdS_4\\times S^7$ and compute the first holographic one-half BPS four-point function. We"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.02800","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":"2026-05-18T00:04:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0XYF44gngfsrkhqld3meUYm2+y7DabCsRZoVMI9uj/MdRYQMI3NZ2x5uiw35O6o1sF20X3X7c3ZqyKniHH3JCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:09:14.355336Z"},"content_sha256":"7d2cbef6a351ca5b8213c442688465aadc7c7b4957ee773302da71fc287ad044","schema_version":"1.0","event_id":"sha256:7d2cbef6a351ca5b8213c442688465aadc7c7b4957ee773302da71fc287ad044"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LBF4AWLHFRSCMECSQAAD47YO7A/bundle.json","state_url":"https://pith.science/pith/LBF4AWLHFRSCMECSQAAD47YO7A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LBF4AWLHFRSCMECSQAAD47YO7A/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":"2026-05-30T06:09:14Z","links":{"resolver":"https://pith.science/pith/LBF4AWLHFRSCMECSQAAD47YO7A","bundle":"https://pith.science/pith/LBF4AWLHFRSCMECSQAAD47YO7A/bundle.json","state":"https://pith.science/pith/LBF4AWLHFRSCMECSQAAD47YO7A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LBF4AWLHFRSCMECSQAAD47YO7A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:LBF4AWLHFRSCMECSQAAD47YO7A","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":"64aabaf97aef056fe60892cb526a3e334a257385ded71701ac990bfd5ecdab10","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-12-07T19:00:08Z","title_canon_sha256":"6a6f33e72913614fbef79f74728c5ca86d9dda4e8d73ef6d98e446402b3a545a"},"schema_version":"1.0","source":{"id":"1712.02800","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.02800","created_at":"2026-05-18T00:04:59Z"},{"alias_kind":"arxiv_version","alias_value":"1712.02800v3","created_at":"2026-05-18T00:04:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.02800","created_at":"2026-05-18T00:04:59Z"},{"alias_kind":"pith_short_12","alias_value":"LBF4AWLHFRSC","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LBF4AWLHFRSCMECS","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LBF4AWLH","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:7d2cbef6a351ca5b8213c442688465aadc7c7b4957ee773302da71fc287ad044","target":"graph","created_at":"2026-05-18T00:04:59Z","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 present a universal treatment for imposing superconformal constraints on Mellin amplitudes for $\\mathrm{SCFT_d}$ with $3\\leq d\\leq 6$. This leads to a new technique to compute holographic correlators, which is similar but complementary to the ones introduced in [1,2]. We apply this technique to theories in various spacetime dimensions. In addition to reproducing known results, we obtain a simple expression for next-next-to-extremal four-point functions in $AdS_7\\times S^4$. We also use this machinery on $AdS_4\\times S^7$ and compute the first holographic one-half BPS four-point function. We","authors_text":"Xinan Zhou","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-12-07T19:00:08Z","title":"On Superconformal Four-Point Mellin Amplitudes in Dimension $d>2$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.02800","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":"sha256:58a0c0949a068f2be2a40b9efc2ec8d9d5d70092bad2f7f127ed7a5d6302227f","target":"record","created_at":"2026-05-18T00:04:59Z","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":"64aabaf97aef056fe60892cb526a3e334a257385ded71701ac990bfd5ecdab10","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-12-07T19:00:08Z","title_canon_sha256":"6a6f33e72913614fbef79f74728c5ca86d9dda4e8d73ef6d98e446402b3a545a"},"schema_version":"1.0","source":{"id":"1712.02800","kind":"arxiv","version":3}},"canonical_sha256":"584bc059672c6426105280003e7f0ef801a533f711c2b136593635581bcb9c41","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"584bc059672c6426105280003e7f0ef801a533f711c2b136593635581bcb9c41","first_computed_at":"2026-05-18T00:04:59.936581Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:59.936581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cCbTdmfj4H92jGbrPrq+Va0su5l3XB+/nHk63ZQxw3pmLaXtYn18tNtQBTbPjYN/t963qHN2I/0lRyd7q7UPDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:59.936999Z","signed_message":"canonical_sha256_bytes"},"source_id":"1712.02800","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:58a0c0949a068f2be2a40b9efc2ec8d9d5d70092bad2f7f127ed7a5d6302227f","sha256:7d2cbef6a351ca5b8213c442688465aadc7c7b4957ee773302da71fc287ad044"],"state_sha256":"764798877ad2f25d553d18f08113b49d4ee2a51045ad127de10371e28d13052d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Lopq6c86dqi+x2/1uL9+SV64/agk7ZHGXfiVYNCNyKtZb8LxguFDiaXCIptjTRa6nzXJMjke/PqPRGSJdzbWCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T06:09:14.358782Z","bundle_sha256":"79fbc7bd80b236a1056c938026be03da1fb13324f19dbcec8d9f55e23cb3b597"}}