{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:3HSQX5WEUX76RPLFNQUECJ2FOJ","short_pith_number":"pith:3HSQX5WE","canonical_record":{"source":{"id":"1401.0010","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-30T21:00:04Z","cross_cats_sorted":[],"title_canon_sha256":"40171c0b1cb3121271ae668173a58b3e80f2eb58c85aae633f002cb2ac3403b7","abstract_canon_sha256":"c0ca56ce69b9afde670d223769a5fd06a2f32fc7640760d9406c5d7a4d8f9e6f"},"schema_version":"1.0"},"canonical_sha256":"d9e50bf6c4a5ffe8bd656c284127457260655dabae1fffde5955b6186fc7bd86","source":{"kind":"arxiv","id":"1401.0010","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.0010","created_at":"2026-05-18T01:45:35Z"},{"alias_kind":"arxiv_version","alias_value":"1401.0010v2","created_at":"2026-05-18T01:45:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.0010","created_at":"2026-05-18T01:45:35Z"},{"alias_kind":"pith_short_12","alias_value":"3HSQX5WEUX76","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3HSQX5WEUX76RPLF","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3HSQX5WE","created_at":"2026-05-18T12:27:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:3HSQX5WEUX76RPLFNQUECJ2FOJ","target":"record","payload":{"canonical_record":{"source":{"id":"1401.0010","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-30T21:00:04Z","cross_cats_sorted":[],"title_canon_sha256":"40171c0b1cb3121271ae668173a58b3e80f2eb58c85aae633f002cb2ac3403b7","abstract_canon_sha256":"c0ca56ce69b9afde670d223769a5fd06a2f32fc7640760d9406c5d7a4d8f9e6f"},"schema_version":"1.0"},"canonical_sha256":"d9e50bf6c4a5ffe8bd656c284127457260655dabae1fffde5955b6186fc7bd86","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:35.064122Z","signature_b64":"YHOIr9OG7+IrjeIvJL120Subco7vtBR2QscYIya6Gzs9joC9/R8bzXwjah1/koGxe2LYg4KsBqqSvGxYUbqFAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9e50bf6c4a5ffe8bd656c284127457260655dabae1fffde5955b6186fc7bd86","last_reissued_at":"2026-05-18T01:45:35.063415Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:35.063415Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.0010","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":"2026-05-18T01:45:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dPuKuwLfEIO2/kpheD1hCxarPEWhbwvCq8RiHNDyVlTpgORYw+43lToeJV/Q67qmUSa5RacbITUUfs6njvwTAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T04:03:19.059563Z"},"content_sha256":"5a72ae5e02fc002a6182602426a644c8c1e1ff5c1fe980a9df2f96c8f6543b29","schema_version":"1.0","event_id":"sha256:5a72ae5e02fc002a6182602426a644c8c1e1ff5c1fe980a9df2f96c8f6543b29"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:3HSQX5WEUX76RPLFNQUECJ2FOJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scalar Charges in Asymptotic AdS Geometries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Hai-Shan Liu, H. Lu","submitted_at":"2013-12-30T21:00:04Z","abstract_excerpt":"We show that for n-dimensional Einstein gravity coupled to a scalar field with mass-squared m_0^2=-n(n-2)/(4\\ell^2), the first law of thermodynamics of (charged) AdS black holes will be modified by the boundary conditions of the scalar field at asymptotic infinity. Such scalars can arise in gauged supergravities in four and six dimensions, but not in five or seven. The result provides a guiding principle for constructing designer black holes and solitons in general dimensions, where the properties of the dual field theories depend on the boundary conditions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.0010","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":"2026-05-18T01:45:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nsdhUD+imbp/ONQmQRxBFE0/r+btGYwPZyBICfhATH0PtYgAvsBSUy1+tvq5Q80IKeMM6QWw4r7E7LqfcNdUCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T04:03:19.060232Z"},"content_sha256":"273eafe34b2edb231719ec383cb91930eda1a264019f7667ba23be6261defb0e","schema_version":"1.0","event_id":"sha256:273eafe34b2edb231719ec383cb91930eda1a264019f7667ba23be6261defb0e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ/bundle.json","state_url":"https://pith.science/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ/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":"2026-05-22T04:03:19Z","links":{"resolver":"https://pith.science/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ","bundle":"https://pith.science/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ/bundle.json","state":"https://pith.science/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3HSQX5WEUX76RPLFNQUECJ2FOJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:3HSQX5WEUX76RPLFNQUECJ2FOJ","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":"c0ca56ce69b9afde670d223769a5fd06a2f32fc7640760d9406c5d7a4d8f9e6f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-30T21:00:04Z","title_canon_sha256":"40171c0b1cb3121271ae668173a58b3e80f2eb58c85aae633f002cb2ac3403b7"},"schema_version":"1.0","source":{"id":"1401.0010","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.0010","created_at":"2026-05-18T01:45:35Z"},{"alias_kind":"arxiv_version","alias_value":"1401.0010v2","created_at":"2026-05-18T01:45:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.0010","created_at":"2026-05-18T01:45:35Z"},{"alias_kind":"pith_short_12","alias_value":"3HSQX5WEUX76","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3HSQX5WEUX76RPLF","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3HSQX5WE","created_at":"2026-05-18T12:27:32Z"}],"graph_snapshots":[{"event_id":"sha256:273eafe34b2edb231719ec383cb91930eda1a264019f7667ba23be6261defb0e","target":"graph","created_at":"2026-05-18T01:45:35Z","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 show that for n-dimensional Einstein gravity coupled to a scalar field with mass-squared m_0^2=-n(n-2)/(4\\ell^2), the first law of thermodynamics of (charged) AdS black holes will be modified by the boundary conditions of the scalar field at asymptotic infinity. Such scalars can arise in gauged supergravities in four and six dimensions, but not in five or seven. The result provides a guiding principle for constructing designer black holes and solitons in general dimensions, where the properties of the dual field theories depend on the boundary conditions.","authors_text":"Hai-Shan Liu, H. Lu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-30T21:00:04Z","title":"Scalar Charges in Asymptotic AdS Geometries"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.0010","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":"sha256:5a72ae5e02fc002a6182602426a644c8c1e1ff5c1fe980a9df2f96c8f6543b29","target":"record","created_at":"2026-05-18T01:45:35Z","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":"c0ca56ce69b9afde670d223769a5fd06a2f32fc7640760d9406c5d7a4d8f9e6f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-30T21:00:04Z","title_canon_sha256":"40171c0b1cb3121271ae668173a58b3e80f2eb58c85aae633f002cb2ac3403b7"},"schema_version":"1.0","source":{"id":"1401.0010","kind":"arxiv","version":2}},"canonical_sha256":"d9e50bf6c4a5ffe8bd656c284127457260655dabae1fffde5955b6186fc7bd86","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d9e50bf6c4a5ffe8bd656c284127457260655dabae1fffde5955b6186fc7bd86","first_computed_at":"2026-05-18T01:45:35.063415Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:45:35.063415Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YHOIr9OG7+IrjeIvJL120Subco7vtBR2QscYIya6Gzs9joC9/R8bzXwjah1/koGxe2LYg4KsBqqSvGxYUbqFAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:45:35.064122Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.0010","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5a72ae5e02fc002a6182602426a644c8c1e1ff5c1fe980a9df2f96c8f6543b29","sha256:273eafe34b2edb231719ec383cb91930eda1a264019f7667ba23be6261defb0e"],"state_sha256":"e285c855d6187045c25bf6ebcb69bcb0140dc7bdd360f1fb500d01bbc94dd520"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jpasK3qYCbC/lIniElBmVvlZFkoVjXffIQ1rSh35N99HQuuLJKAnvUE9EpeSUThhQKW6vA85QSjxBg9vFdkCDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T04:03:19.064009Z","bundle_sha256":"39e0e7086b182b12c7917df1df1d53ea1a98b0f3d69fddce3cc245e473ed5ad3"}}