{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:OAHQUMMXNBEQPUUPMOW74UPK4K","short_pith_number":"pith:OAHQUMMX","canonical_record":{"source":{"id":"1302.0816","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-04T19:45:33Z","cross_cats_sorted":[],"title_canon_sha256":"2904fb7fd2b55beaf1451e7d256ba29232d91cbf87876d17f2f2fefc04a1610c","abstract_canon_sha256":"388adb662d4d96d0278d2b1c0b3e03a1da8c04318b75146d4bffe58c296a9d79"},"schema_version":"1.0"},"canonical_sha256":"700f0a3197684907d28f63adfe51eae2908009b1017d4b6c1751bf2b1b35fbd8","source":{"kind":"arxiv","id":"1302.0816","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.0816","created_at":"2026-05-18T00:03:59Z"},{"alias_kind":"arxiv_version","alias_value":"1302.0816v2","created_at":"2026-05-18T00:03:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.0816","created_at":"2026-05-18T00:03:59Z"},{"alias_kind":"pith_short_12","alias_value":"OAHQUMMXNBEQ","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"OAHQUMMXNBEQPUUP","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"OAHQUMMX","created_at":"2026-05-18T12:27:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:OAHQUMMXNBEQPUUPMOW74UPK4K","target":"record","payload":{"canonical_record":{"source":{"id":"1302.0816","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-04T19:45:33Z","cross_cats_sorted":[],"title_canon_sha256":"2904fb7fd2b55beaf1451e7d256ba29232d91cbf87876d17f2f2fefc04a1610c","abstract_canon_sha256":"388adb662d4d96d0278d2b1c0b3e03a1da8c04318b75146d4bffe58c296a9d79"},"schema_version":"1.0"},"canonical_sha256":"700f0a3197684907d28f63adfe51eae2908009b1017d4b6c1751bf2b1b35fbd8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:59.800972Z","signature_b64":"OSxaqSNF+x13FSzxqkSK95TbheFKzZ+J7AYZZVeu8pPAlKlRYGmMrJj5mTFDmEB1d4tkFFpm96gM7jk5moobDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"700f0a3197684907d28f63adfe51eae2908009b1017d4b6c1751bf2b1b35fbd8","last_reissued_at":"2026-05-18T00:03:59.800448Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:59.800448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.0816","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":"2026-05-18T00:03:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"43ylzn5y9YHpNhxDufKMq2Jgjvb+A+kal0bMgq6KIO2WOcPzvtTQP8KqgkOb4V/dRASMOvAdTYyWZ6lYXNU3Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T07:36:06.944746Z"},"content_sha256":"9683b9f93e900951dcba6e98813bf8bb4eee4c5b6933aa412ab10cf21558df6f","schema_version":"1.0","event_id":"sha256:9683b9f93e900951dcba6e98813bf8bb4eee4c5b6933aa412ab10cf21558df6f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:OAHQUMMXNBEQPUUPMOW74UPK4K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamics of Higher Spin Black Holes in AdS$_3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jan de Boer, Juan I. Jottar","submitted_at":"2013-02-04T19:45:33Z","abstract_excerpt":"We discuss the thermodynamics of recently constructed three-dimensional higher spin black holes in SL(N,R)\\times SL(N,R) Chern-Simons theory with generalized asymptotically-anti-de Sitter boundary conditions. From a holographic perspective, these bulk theories are dual to two-dimensional CFTs with W_N symmetry algebras, and the black hole solutions are dual to thermal states with higher spin chemical potentials and charges turned on. Because the notion of horizon area is not gauge-invariant in the higher spin theory, the traditional approaches to the computation of black hole entropy must be r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.0816","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":"2026-05-18T00:03:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0Re2PVnBVR6TaQQknvYabH4cgeAsgOSNCxNHPrB5C7Vx5Z93x9hdl4Rp7YXKcJtpl1zx6Y1iVmKZZOI6YI+zAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T07:36:06.945092Z"},"content_sha256":"5888ca23fc6df883bf338f6cedef16887a75d6924444b255eaade18e0422e68a","schema_version":"1.0","event_id":"sha256:5888ca23fc6df883bf338f6cedef16887a75d6924444b255eaade18e0422e68a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OAHQUMMXNBEQPUUPMOW74UPK4K/bundle.json","state_url":"https://pith.science/pith/OAHQUMMXNBEQPUUPMOW74UPK4K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OAHQUMMXNBEQPUUPMOW74UPK4K/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":"2026-05-28T07:36:06Z","links":{"resolver":"https://pith.science/pith/OAHQUMMXNBEQPUUPMOW74UPK4K","bundle":"https://pith.science/pith/OAHQUMMXNBEQPUUPMOW74UPK4K/bundle.json","state":"https://pith.science/pith/OAHQUMMXNBEQPUUPMOW74UPK4K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OAHQUMMXNBEQPUUPMOW74UPK4K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:OAHQUMMXNBEQPUUPMOW74UPK4K","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":"388adb662d4d96d0278d2b1c0b3e03a1da8c04318b75146d4bffe58c296a9d79","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-04T19:45:33Z","title_canon_sha256":"2904fb7fd2b55beaf1451e7d256ba29232d91cbf87876d17f2f2fefc04a1610c"},"schema_version":"1.0","source":{"id":"1302.0816","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.0816","created_at":"2026-05-18T00:03:59Z"},{"alias_kind":"arxiv_version","alias_value":"1302.0816v2","created_at":"2026-05-18T00:03:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.0816","created_at":"2026-05-18T00:03:59Z"},{"alias_kind":"pith_short_12","alias_value":"OAHQUMMXNBEQ","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"OAHQUMMXNBEQPUUP","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"OAHQUMMX","created_at":"2026-05-18T12:27:54Z"}],"graph_snapshots":[{"event_id":"sha256:5888ca23fc6df883bf338f6cedef16887a75d6924444b255eaade18e0422e68a","target":"graph","created_at":"2026-05-18T00:03:59Z","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 discuss the thermodynamics of recently constructed three-dimensional higher spin black holes in SL(N,R)\\times SL(N,R) Chern-Simons theory with generalized asymptotically-anti-de Sitter boundary conditions. From a holographic perspective, these bulk theories are dual to two-dimensional CFTs with W_N symmetry algebras, and the black hole solutions are dual to thermal states with higher spin chemical potentials and charges turned on. Because the notion of horizon area is not gauge-invariant in the higher spin theory, the traditional approaches to the computation of black hole entropy must be r","authors_text":"Jan de Boer, Juan I. Jottar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-04T19:45:33Z","title":"Thermodynamics of Higher Spin Black Holes in AdS$_3$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.0816","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":"sha256:9683b9f93e900951dcba6e98813bf8bb4eee4c5b6933aa412ab10cf21558df6f","target":"record","created_at":"2026-05-18T00:03:59Z","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":"388adb662d4d96d0278d2b1c0b3e03a1da8c04318b75146d4bffe58c296a9d79","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-04T19:45:33Z","title_canon_sha256":"2904fb7fd2b55beaf1451e7d256ba29232d91cbf87876d17f2f2fefc04a1610c"},"schema_version":"1.0","source":{"id":"1302.0816","kind":"arxiv","version":2}},"canonical_sha256":"700f0a3197684907d28f63adfe51eae2908009b1017d4b6c1751bf2b1b35fbd8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"700f0a3197684907d28f63adfe51eae2908009b1017d4b6c1751bf2b1b35fbd8","first_computed_at":"2026-05-18T00:03:59.800448Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:03:59.800448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OSxaqSNF+x13FSzxqkSK95TbheFKzZ+J7AYZZVeu8pPAlKlRYGmMrJj5mTFDmEB1d4tkFFpm96gM7jk5moobDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:03:59.800972Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.0816","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9683b9f93e900951dcba6e98813bf8bb4eee4c5b6933aa412ab10cf21558df6f","sha256:5888ca23fc6df883bf338f6cedef16887a75d6924444b255eaade18e0422e68a"],"state_sha256":"71c574c9595434cfce083825c9f896be69fc4578038b3d69f3184637c7503ab4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P9KZK7qJO8RM83CAE2JkhDCBA9doGCsdis4e27VrdXpgxj6Un3YDbg+ieJoP6z9FhkUnTSOTzlvdEp2NCFmADQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T07:36:06.947020Z","bundle_sha256":"483c3d85e27fd5b0b9f00d0981d9333dd6a35d5f0737cd42a4e8291da5b432c5"}}