{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:5VIWCPTKEX32KVQOY7OSULZQWE","short_pith_number":"pith:5VIWCPTK","canonical_record":{"source":{"id":"1702.04353","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-14T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"374732b31cbe88951511fa34c94586248e137a2cba86e7ec95370a927ea0e5bf","abstract_canon_sha256":"6ed8ee8627b88a18811bade43722b6411cce83a2264d88f74d64bf0a544250e9"},"schema_version":"1.0"},"canonical_sha256":"ed51613e6a25f7a5560ec7dd2a2f30b13198af1c980111056fcfbcd35cc38589","source":{"kind":"arxiv","id":"1702.04353","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.04353","created_at":"2026-05-18T00:41:37Z"},{"alias_kind":"arxiv_version","alias_value":"1702.04353v2","created_at":"2026-05-18T00:41:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.04353","created_at":"2026-05-18T00:41:37Z"},{"alias_kind":"pith_short_12","alias_value":"5VIWCPTKEX32","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"5VIWCPTKEX32KVQO","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"5VIWCPTK","created_at":"2026-05-18T12:31:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:5VIWCPTKEX32KVQOY7OSULZQWE","target":"record","payload":{"canonical_record":{"source":{"id":"1702.04353","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-14T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"374732b31cbe88951511fa34c94586248e137a2cba86e7ec95370a927ea0e5bf","abstract_canon_sha256":"6ed8ee8627b88a18811bade43722b6411cce83a2264d88f74d64bf0a544250e9"},"schema_version":"1.0"},"canonical_sha256":"ed51613e6a25f7a5560ec7dd2a2f30b13198af1c980111056fcfbcd35cc38589","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:37.001055Z","signature_b64":"W90d6A7rme5W2qAW7i+VJGwQhF83CUGUEAQs3Y06GKBqNCoZ7ynvAJQV431ezPNNCIGWgwP2z3XpfJ5Otk80BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed51613e6a25f7a5560ec7dd2a2f30b13198af1c980111056fcfbcd35cc38589","last_reissued_at":"2026-05-18T00:41:37.000402Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:37.000402Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.04353","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":"2026-05-18T00:41:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cZd7DFk/ACVHEN0ttdy2QalPN0ta076ZL10XK3TC7HsjAc0YESSCNEVuGlalS1VNdG30f+/L23H4OhDx1IMxBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:29:53.025019Z"},"content_sha256":"58e97160c714c339da583ef3922238ad0014077eb364740b6e2718c1ea88bac9","schema_version":"1.0","event_id":"sha256:58e97160c714c339da583ef3922238ad0014077eb364740b6e2718c1ea88bac9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:5VIWCPTKEX32KVQOY7OSULZQWE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polarised Black Holes in ABJM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Joao Penedones, Jorge E. Santos, Lauren Greenspan, Miguel S. Costa","submitted_at":"2017-02-14T19:00:00Z","abstract_excerpt":"We numerically construct asymptotically $AdS_4$ solutions to Einstein-Maxwell-dilaton theory. These have a dipolar electrostatic potential turned on at the conformal boundary $S^2\\times \\mathbb{R}_t$. We find two classes of geometries: $AdS$ soliton solutions that encode the full backreaction of the electric field on the $AdS$ geometry without a horizon, and neutral black holes that are \"polarised\" by the dipolar potential. For a certain range of the electric field $\\mathcal{E}$, we find two distinct branches of the $AdS$ soliton that exist for the same value of $\\mathcal{E}$. For the black ho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.04353","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":"2026-05-18T00:41:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9OZKYZummPwOXQtm1tdl522Hve4LcBJD6R772osq0LCUqa8NRY7Bs/n2EA1JT4C2HFFc2ye6SjxyfTb/TH5TBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:29:53.025711Z"},"content_sha256":"8f262c65d1ffef2d20385f1de0eac630c27ee7e0423f8ced580d9733cb3cff4d","schema_version":"1.0","event_id":"sha256:8f262c65d1ffef2d20385f1de0eac630c27ee7e0423f8ced580d9733cb3cff4d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5VIWCPTKEX32KVQOY7OSULZQWE/bundle.json","state_url":"https://pith.science/pith/5VIWCPTKEX32KVQOY7OSULZQWE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5VIWCPTKEX32KVQOY7OSULZQWE/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":"2026-05-27T04:29:53Z","links":{"resolver":"https://pith.science/pith/5VIWCPTKEX32KVQOY7OSULZQWE","bundle":"https://pith.science/pith/5VIWCPTKEX32KVQOY7OSULZQWE/bundle.json","state":"https://pith.science/pith/5VIWCPTKEX32KVQOY7OSULZQWE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5VIWCPTKEX32KVQOY7OSULZQWE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:5VIWCPTKEX32KVQOY7OSULZQWE","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":"6ed8ee8627b88a18811bade43722b6411cce83a2264d88f74d64bf0a544250e9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-14T19:00:00Z","title_canon_sha256":"374732b31cbe88951511fa34c94586248e137a2cba86e7ec95370a927ea0e5bf"},"schema_version":"1.0","source":{"id":"1702.04353","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.04353","created_at":"2026-05-18T00:41:37Z"},{"alias_kind":"arxiv_version","alias_value":"1702.04353v2","created_at":"2026-05-18T00:41:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.04353","created_at":"2026-05-18T00:41:37Z"},{"alias_kind":"pith_short_12","alias_value":"5VIWCPTKEX32","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"5VIWCPTKEX32KVQO","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"5VIWCPTK","created_at":"2026-05-18T12:31:00Z"}],"graph_snapshots":[{"event_id":"sha256:8f262c65d1ffef2d20385f1de0eac630c27ee7e0423f8ced580d9733cb3cff4d","target":"graph","created_at":"2026-05-18T00:41:37Z","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 numerically construct asymptotically $AdS_4$ solutions to Einstein-Maxwell-dilaton theory. These have a dipolar electrostatic potential turned on at the conformal boundary $S^2\\times \\mathbb{R}_t$. We find two classes of geometries: $AdS$ soliton solutions that encode the full backreaction of the electric field on the $AdS$ geometry without a horizon, and neutral black holes that are \"polarised\" by the dipolar potential. For a certain range of the electric field $\\mathcal{E}$, we find two distinct branches of the $AdS$ soliton that exist for the same value of $\\mathcal{E}$. For the black ho","authors_text":"Joao Penedones, Jorge E. Santos, Lauren Greenspan, Miguel S. Costa","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-14T19:00:00Z","title":"Polarised Black Holes in ABJM"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.04353","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":"sha256:58e97160c714c339da583ef3922238ad0014077eb364740b6e2718c1ea88bac9","target":"record","created_at":"2026-05-18T00:41:37Z","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":"6ed8ee8627b88a18811bade43722b6411cce83a2264d88f74d64bf0a544250e9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-14T19:00:00Z","title_canon_sha256":"374732b31cbe88951511fa34c94586248e137a2cba86e7ec95370a927ea0e5bf"},"schema_version":"1.0","source":{"id":"1702.04353","kind":"arxiv","version":2}},"canonical_sha256":"ed51613e6a25f7a5560ec7dd2a2f30b13198af1c980111056fcfbcd35cc38589","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ed51613e6a25f7a5560ec7dd2a2f30b13198af1c980111056fcfbcd35cc38589","first_computed_at":"2026-05-18T00:41:37.000402Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:41:37.000402Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"W90d6A7rme5W2qAW7i+VJGwQhF83CUGUEAQs3Y06GKBqNCoZ7ynvAJQV431ezPNNCIGWgwP2z3XpfJ5Otk80BA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:41:37.001055Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.04353","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:58e97160c714c339da583ef3922238ad0014077eb364740b6e2718c1ea88bac9","sha256:8f262c65d1ffef2d20385f1de0eac630c27ee7e0423f8ced580d9733cb3cff4d"],"state_sha256":"8dfea821638e515e20206da2df9a1f980337c126dbfd81a7bd3677c8d03761dc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rOlHhJvYC0tPeM19fEeNkHFvM2bpXD4+WsjF2q+4BHOM8dB9uWayd/3veCjq6ULD7vyBXYHNPb2kP3VpPRqKBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T04:29:53.029374Z","bundle_sha256":"0d98b3436c0cf8a735ccef1851327b48ff0cb3c7fdfc561c51cac03c6b85d980"}}