{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:UZ4HDNIA4ISV2RSMA3HULZONQS","short_pith_number":"pith:UZ4HDNIA","canonical_record":{"source":{"id":"2102.09439","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-18T16:00:06Z","cross_cats_sorted":[],"title_canon_sha256":"cd7d80576012940d0753307bfc9b156b6c322a7eeb2b5ae5dfa8ee8ca3150c7a","abstract_canon_sha256":"ca0aef962df6c76c7a715ccb8235b1230ef2995147c223a68467f51d45a93b4d"},"schema_version":"1.0"},"canonical_sha256":"a67871b500e2255d464c06cf45e5cd849f68c90b61f9e552cd53563322694435","source":{"kind":"arxiv","id":"2102.09439","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2102.09439","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"arxiv_version","alias_value":"2102.09439v1","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.09439","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"pith_short_12","alias_value":"UZ4HDNIA4ISV","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"pith_short_16","alias_value":"UZ4HDNIA4ISV2RSM","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"pith_short_8","alias_value":"UZ4HDNIA","created_at":"2026-07-05T03:28:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:UZ4HDNIA4ISV2RSMA3HULZONQS","target":"record","payload":{"canonical_record":{"source":{"id":"2102.09439","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-18T16:00:06Z","cross_cats_sorted":[],"title_canon_sha256":"cd7d80576012940d0753307bfc9b156b6c322a7eeb2b5ae5dfa8ee8ca3150c7a","abstract_canon_sha256":"ca0aef962df6c76c7a715ccb8235b1230ef2995147c223a68467f51d45a93b4d"},"schema_version":"1.0"},"canonical_sha256":"a67871b500e2255d464c06cf45e5cd849f68c90b61f9e552cd53563322694435","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:28:13.216320Z","signature_b64":"Hp9KPREBVmPg3WSE8PrGytkmnKMsbDYKJNodvPi/SYG4JJCnfKssWpPdJ7v4Oi6WfxFk+ZdhBNWSx2wB3OY2DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a67871b500e2255d464c06cf45e5cd849f68c90b61f9e552cd53563322694435","last_reissued_at":"2026-07-05T03:28:13.215836Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:28:13.215836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2102.09439","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T03:28:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P+Q0qJwqUpsAhk11JfZiwG6idfGAFagc1nqPGQnLEoX4zrv45yg4Iae/QXBkkoadhe+KfCDPo7xE2s7bF335CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T13:02:05.038669Z"},"content_sha256":"3396a284643613f29281389bcfc50b50cd99d7912cb017d7c0a4f3b5c3659e14","schema_version":"1.0","event_id":"sha256:3396a284643613f29281389bcfc50b50cd99d7912cb017d7c0a4f3b5c3659e14"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:UZ4HDNIA4ISV2RSMA3HULZONQS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Probing black hole microstructure with the kinetic turnover of phase transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Jin Wang, Kun Zhang, Ran Li","submitted_at":"2021-02-18T16:00:06Z","abstract_excerpt":"By treating black hole as the macroscopic stable state on the free energy landscape, we propose that the stochastic dynamics of the black hole phase transition can be effectively described by the Langevin equation or equivalently by the Fokker-Planck equation in phase space. We demonstrate the turnover of the kinetics for the charged anti-de Sitter black hole phase transition, which shows that the mean first passage time is linear with the friction in the high damping regime and inversely proportional to the friction in the low damping regime. The fluctuations in the kinetics are shown to be l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.09439","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2102.09439/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T03:28:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b0EdHJD9w3zxaW5r/S3Q86CWfOcA4AOl09bA9FRlpr/d7JegybpieqZ/90jUiRUhWOXdeBqGSVjw1B/d7dPUDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T13:02:05.039195Z"},"content_sha256":"b223df2b6f0b4bada11258e5dbe0c36432c1191455fdfaa8d6604c0df637e7f4","schema_version":"1.0","event_id":"sha256:b223df2b6f0b4bada11258e5dbe0c36432c1191455fdfaa8d6604c0df637e7f4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UZ4HDNIA4ISV2RSMA3HULZONQS/bundle.json","state_url":"https://pith.science/pith/UZ4HDNIA4ISV2RSMA3HULZONQS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UZ4HDNIA4ISV2RSMA3HULZONQS/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":"2026-08-06T13:02:05Z","links":{"resolver":"https://pith.science/pith/UZ4HDNIA4ISV2RSMA3HULZONQS","bundle":"https://pith.science/pith/UZ4HDNIA4ISV2RSMA3HULZONQS/bundle.json","state":"https://pith.science/pith/UZ4HDNIA4ISV2RSMA3HULZONQS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UZ4HDNIA4ISV2RSMA3HULZONQS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:UZ4HDNIA4ISV2RSMA3HULZONQS","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":"ca0aef962df6c76c7a715ccb8235b1230ef2995147c223a68467f51d45a93b4d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-18T16:00:06Z","title_canon_sha256":"cd7d80576012940d0753307bfc9b156b6c322a7eeb2b5ae5dfa8ee8ca3150c7a"},"schema_version":"1.0","source":{"id":"2102.09439","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2102.09439","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"arxiv_version","alias_value":"2102.09439v1","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.09439","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"pith_short_12","alias_value":"UZ4HDNIA4ISV","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"pith_short_16","alias_value":"UZ4HDNIA4ISV2RSM","created_at":"2026-07-05T03:28:13Z"},{"alias_kind":"pith_short_8","alias_value":"UZ4HDNIA","created_at":"2026-07-05T03:28:13Z"}],"graph_snapshots":[{"event_id":"sha256:b223df2b6f0b4bada11258e5dbe0c36432c1191455fdfaa8d6604c0df637e7f4","target":"graph","created_at":"2026-07-05T03:28:13Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2102.09439/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"By treating black hole as the macroscopic stable state on the free energy landscape, we propose that the stochastic dynamics of the black hole phase transition can be effectively described by the Langevin equation or equivalently by the Fokker-Planck equation in phase space. We demonstrate the turnover of the kinetics for the charged anti-de Sitter black hole phase transition, which shows that the mean first passage time is linear with the friction in the high damping regime and inversely proportional to the friction in the low damping regime. The fluctuations in the kinetics are shown to be l","authors_text":"Jin Wang, Kun Zhang, Ran Li","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-18T16:00:06Z","title":"Probing black hole microstructure with the kinetic turnover of phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.09439","kind":"arxiv","version":1},"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":"sha256:3396a284643613f29281389bcfc50b50cd99d7912cb017d7c0a4f3b5c3659e14","target":"record","created_at":"2026-07-05T03:28:13Z","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":"ca0aef962df6c76c7a715ccb8235b1230ef2995147c223a68467f51d45a93b4d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-18T16:00:06Z","title_canon_sha256":"cd7d80576012940d0753307bfc9b156b6c322a7eeb2b5ae5dfa8ee8ca3150c7a"},"schema_version":"1.0","source":{"id":"2102.09439","kind":"arxiv","version":1}},"canonical_sha256":"a67871b500e2255d464c06cf45e5cd849f68c90b61f9e552cd53563322694435","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a67871b500e2255d464c06cf45e5cd849f68c90b61f9e552cd53563322694435","first_computed_at":"2026-07-05T03:28:13.215836Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:28:13.215836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Hp9KPREBVmPg3WSE8PrGytkmnKMsbDYKJNodvPi/SYG4JJCnfKssWpPdJ7v4Oi6WfxFk+ZdhBNWSx2wB3OY2DA==","signature_status":"signed_v1","signed_at":"2026-07-05T03:28:13.216320Z","signed_message":"canonical_sha256_bytes"},"source_id":"2102.09439","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3396a284643613f29281389bcfc50b50cd99d7912cb017d7c0a4f3b5c3659e14","sha256:b223df2b6f0b4bada11258e5dbe0c36432c1191455fdfaa8d6604c0df637e7f4"],"state_sha256":"eccfbdf0f289cd351d2721b6cbf319bd080c1e00a1f300a3d4644bc18a3b7647"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ERaejzE8/zY2OC4WnOAzXS1fbDk6Ckw3ldlQ7ChQ2E9Y4BmA6KV+XuTh+Si2BuCqJXEMhwX/iFf5SUuWvNkBAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T13:02:05.043401Z","bundle_sha256":"302943cf2fe4982aee928ba14ca697968e7e8dec7442ab00e25f80fd9d93f663"}}