{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:Z4HPNR5MLZGKHBYNMX43ARPTGF","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":"99d1fc5b7f63e2b9ed0f5ce22c71e4ac322aab28ac9061b57b0fb4806ff18f03","cross_cats_sorted":["cond-mat.stat-mech","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-02-03T19:00:00Z","title_canon_sha256":"23437b054dca78569fe97c3452adefcd26823fdb992958fd6800bffed1612ccd"},"schema_version":"1.0","source":{"id":"2502.01723","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.01723","created_at":"2026-07-05T10:09:18Z"},{"alias_kind":"arxiv_version","alias_value":"2502.01723v1","created_at":"2026-07-05T10:09:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.01723","created_at":"2026-07-05T10:09:18Z"},{"alias_kind":"pith_short_12","alias_value":"Z4HPNR5MLZGK","created_at":"2026-07-05T10:09:18Z"},{"alias_kind":"pith_short_16","alias_value":"Z4HPNR5MLZGKHBYN","created_at":"2026-07-05T10:09:18Z"},{"alias_kind":"pith_short_8","alias_value":"Z4HPNR5M","created_at":"2026-07-05T10:09:18Z"}],"graph_snapshots":[{"event_id":"sha256:354418952a7f6e3aa44d1d6900b01e3ab55deb1f38df07a82ef485e00ef56422","target":"graph","created_at":"2026-07-05T10:09:18Z","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/2502.01723/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In the large$-N$ limit, no known no-go theorem rules out thermal time crystals that spontaneously break continuous time-translation, unlike in the large volume limit. If thermal time crystals exist in holographic CFTs, they would correspond to ensemble-dominating black holes with eternally time-varying exterior geometries. We point out that recent work on a conjectured non-linear instability of slowly rotating Kerr-AdS$_4$ produced viable candidates for such states. Then we show that the existence of holographic microcanonical time crystals would imply violations of the AdS Penrose inequality ","authors_text":"{\\AA}smund Folkestad","cross_cats":["cond-mat.stat-mech","gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-02-03T19:00:00Z","title":"Holographic Time Crystals vs Penrose"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.01723","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:cef8dcb7144aac361293ededca71625d2fbcdb41011147f0a828d2d21b26256c","target":"record","created_at":"2026-07-05T10:09:18Z","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":"99d1fc5b7f63e2b9ed0f5ce22c71e4ac322aab28ac9061b57b0fb4806ff18f03","cross_cats_sorted":["cond-mat.stat-mech","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-02-03T19:00:00Z","title_canon_sha256":"23437b054dca78569fe97c3452adefcd26823fdb992958fd6800bffed1612ccd"},"schema_version":"1.0","source":{"id":"2502.01723","kind":"arxiv","version":1}},"canonical_sha256":"cf0ef6c7ac5e4ca3870d65f9b045f331747c8675c8c5248bb5737768ff269cf6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cf0ef6c7ac5e4ca3870d65f9b045f331747c8675c8c5248bb5737768ff269cf6","first_computed_at":"2026-07-05T10:09:18.214681Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:09:18.214681Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QS5HZHRX3HXJt50YGkqX4kwi43Z/qVvtojnbxqxZkT4FuiEhKXg5Pjzk290rCUZDwlicTIlGAAEAAzkpRbJTBw==","signature_status":"signed_v1","signed_at":"2026-07-05T10:09:18.215167Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.01723","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cef8dcb7144aac361293ededca71625d2fbcdb41011147f0a828d2d21b26256c","sha256:354418952a7f6e3aa44d1d6900b01e3ab55deb1f38df07a82ef485e00ef56422"],"state_sha256":"b1652f56b4a66da8d6659740141c54405bb0b3e06498d0de67af7c42c2c8b07b"}