{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:LAXINVVM373XSK543X3LQDNGGI","short_pith_number":"pith:LAXINVVM","canonical_record":{"source":{"id":"1709.07025","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-09-20T18:21:22Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"9058ba7d7f815c931ced2c74bf24b980a7087c43594e8e7b4be6838af018da6c","abstract_canon_sha256":"6279ce6900de253016eb2eb32183dd97c6f7f56e4ab675acc6359c97a1d3c78c"},"schema_version":"1.0"},"canonical_sha256":"582e86d6acdff7792bbcddf6b80da6322ab2a7dc206c2546d808386aa935272a","source":{"kind":"arxiv","id":"1709.07025","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.07025","created_at":"2026-05-18T00:17:19Z"},{"alias_kind":"arxiv_version","alias_value":"1709.07025v2","created_at":"2026-05-18T00:17:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07025","created_at":"2026-05-18T00:17:19Z"},{"alias_kind":"pith_short_12","alias_value":"LAXINVVM373X","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LAXINVVM373XSK54","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LAXINVVM","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:LAXINVVM373XSK543X3LQDNGGI","target":"record","payload":{"canonical_record":{"source":{"id":"1709.07025","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-09-20T18:21:22Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"9058ba7d7f815c931ced2c74bf24b980a7087c43594e8e7b4be6838af018da6c","abstract_canon_sha256":"6279ce6900de253016eb2eb32183dd97c6f7f56e4ab675acc6359c97a1d3c78c"},"schema_version":"1.0"},"canonical_sha256":"582e86d6acdff7792bbcddf6b80da6322ab2a7dc206c2546d808386aa935272a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:17:19.120656Z","signature_b64":"zlFKc+FEmiIz5w/x6c3lEiVDSbEaq7G+VQykoLSlk1jsYbK1zAc4xOQRiFBnmRcmZ4LuWUMQcUjmi8hWUJvHBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"582e86d6acdff7792bbcddf6b80da6322ab2a7dc206c2546d808386aa935272a","last_reissued_at":"2026-05-18T00:17:19.120227Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:17:19.120227Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.07025","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:17:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9d/QVCVDwi0XNgFwr7VairrsQq7NjrHXUf/m4zA/HjsAkTpvqqw9D22LCG9ONdqTyQpzZNtiNftp3hhqUlzrDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T04:56:29.051097Z"},"content_sha256":"57dba8e3fbcb2104683730165770c30a4bf8329dbc93e1c11232264e4eb34f34","schema_version":"1.0","event_id":"sha256:57dba8e3fbcb2104683730165770c30a4bf8329dbc93e1c11232264e4eb34f34"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:LAXINVVM373XSK543X3LQDNGGI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Testing holography using lattice super-Yang--Mills on a 2-torus","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"David Schaich, Raghav G. Jha, Simon Catterall, Toby Wiseman","submitted_at":"2017-09-20T18:21:22Z","abstract_excerpt":"We consider maximally supersymmetric SU(N) Yang--Mills theory in Euclidean signature compactified on a flat two-dimensional torus with anti-periodic (`thermal') fermion boundary conditions imposed on one cycle. At large N, holography predicts that this theory describes certain black hole solutions in Type IIA and IIB supergravity, and we use lattice gauge theory to test this. Unlike the one-dimensional quantum mechanics case where there is only the dimensionless temperature to vary, here we emphasize there are two more parameters which determine the shape of the flat torus. While a rectangular"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07025","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:17:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O5yTKTr22z0kYBUAVGJVur1huz6DWRft5Gy0p6MfvK/11xq7EYkttPgtDE0GCaG3bfu9nVrcENuyiSlgqdZuCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T04:56:29.051491Z"},"content_sha256":"b7a8479dbf0e82fb9d7150b5b2125581b001d48b5941f29483779197b7e27a52","schema_version":"1.0","event_id":"sha256:b7a8479dbf0e82fb9d7150b5b2125581b001d48b5941f29483779197b7e27a52"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LAXINVVM373XSK543X3LQDNGGI/bundle.json","state_url":"https://pith.science/pith/LAXINVVM373XSK543X3LQDNGGI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LAXINVVM373XSK543X3LQDNGGI/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":"2026-06-08T04:56:29Z","links":{"resolver":"https://pith.science/pith/LAXINVVM373XSK543X3LQDNGGI","bundle":"https://pith.science/pith/LAXINVVM373XSK543X3LQDNGGI/bundle.json","state":"https://pith.science/pith/LAXINVVM373XSK543X3LQDNGGI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LAXINVVM373XSK543X3LQDNGGI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:LAXINVVM373XSK543X3LQDNGGI","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":"6279ce6900de253016eb2eb32183dd97c6f7f56e4ab675acc6359c97a1d3c78c","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-09-20T18:21:22Z","title_canon_sha256":"9058ba7d7f815c931ced2c74bf24b980a7087c43594e8e7b4be6838af018da6c"},"schema_version":"1.0","source":{"id":"1709.07025","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.07025","created_at":"2026-05-18T00:17:19Z"},{"alias_kind":"arxiv_version","alias_value":"1709.07025v2","created_at":"2026-05-18T00:17:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07025","created_at":"2026-05-18T00:17:19Z"},{"alias_kind":"pith_short_12","alias_value":"LAXINVVM373X","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LAXINVVM373XSK54","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LAXINVVM","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:b7a8479dbf0e82fb9d7150b5b2125581b001d48b5941f29483779197b7e27a52","target":"graph","created_at":"2026-05-18T00:17:19Z","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 consider maximally supersymmetric SU(N) Yang--Mills theory in Euclidean signature compactified on a flat two-dimensional torus with anti-periodic (`thermal') fermion boundary conditions imposed on one cycle. At large N, holography predicts that this theory describes certain black hole solutions in Type IIA and IIB supergravity, and we use lattice gauge theory to test this. Unlike the one-dimensional quantum mechanics case where there is only the dimensionless temperature to vary, here we emphasize there are two more parameters which determine the shape of the flat torus. While a rectangular","authors_text":"David Schaich, Raghav G. Jha, Simon Catterall, Toby Wiseman","cross_cats":["hep-lat"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-09-20T18:21:22Z","title":"Testing holography using lattice super-Yang--Mills on a 2-torus"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07025","kind":"arxiv","version":2},"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":"sha256:57dba8e3fbcb2104683730165770c30a4bf8329dbc93e1c11232264e4eb34f34","target":"record","created_at":"2026-05-18T00:17:19Z","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":"6279ce6900de253016eb2eb32183dd97c6f7f56e4ab675acc6359c97a1d3c78c","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-09-20T18:21:22Z","title_canon_sha256":"9058ba7d7f815c931ced2c74bf24b980a7087c43594e8e7b4be6838af018da6c"},"schema_version":"1.0","source":{"id":"1709.07025","kind":"arxiv","version":2}},"canonical_sha256":"582e86d6acdff7792bbcddf6b80da6322ab2a7dc206c2546d808386aa935272a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"582e86d6acdff7792bbcddf6b80da6322ab2a7dc206c2546d808386aa935272a","first_computed_at":"2026-05-18T00:17:19.120227Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:17:19.120227Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zlFKc+FEmiIz5w/x6c3lEiVDSbEaq7G+VQykoLSlk1jsYbK1zAc4xOQRiFBnmRcmZ4LuWUMQcUjmi8hWUJvHBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:17:19.120656Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.07025","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:57dba8e3fbcb2104683730165770c30a4bf8329dbc93e1c11232264e4eb34f34","sha256:b7a8479dbf0e82fb9d7150b5b2125581b001d48b5941f29483779197b7e27a52"],"state_sha256":"e572518c09261829658b7fb1c2805bf0c12a1edca525acbb059411699f1f48df"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hTR9JLZpmnAsPlBqMghPXF6MGnhlc5fu5KHHfJEOU7ZJGXCs2JPJU1Mg2DrArkXSH32NmJKK5B8nXalFsh/8CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T04:56:29.053839Z","bundle_sha256":"6fd1cafedea699b694347517e72adfdd5198fefa4b3458124dfe30a3c29296c1"}}