{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:2H4YNCRYWHBHBV2S6QAEKJULK2","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":"cbe9622092769794e762d004cc4b9e470af65a979656dcc15fa232573e8e1a78","cross_cats_sorted":["cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2021-03-19T04:37:43Z","title_canon_sha256":"f39866564334b147dc731e1f4f844ddd215dfa4675a04099952a99350d786b64"},"schema_version":"1.0","source":{"id":"2103.10628","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.10628","created_at":"2026-07-05T04:19:21Z"},{"alias_kind":"arxiv_version","alias_value":"2103.10628v3","created_at":"2026-07-05T04:19:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.10628","created_at":"2026-07-05T04:19:21Z"},{"alias_kind":"pith_short_12","alias_value":"2H4YNCRYWHBH","created_at":"2026-07-05T04:19:21Z"},{"alias_kind":"pith_short_16","alias_value":"2H4YNCRYWHBHBV2S","created_at":"2026-07-05T04:19:21Z"},{"alias_kind":"pith_short_8","alias_value":"2H4YNCRY","created_at":"2026-07-05T04:19:21Z"}],"graph_snapshots":[{"event_id":"sha256:65466482fcd56b074050e0cd745e8ff3337444b0f1906ec89edca2422f5f96fc","target":"graph","created_at":"2026-07-05T04:19:21Z","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/2103.10628/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a quantum circuit with measurements and post-selection that exhibits a panoply of space- and/or time-ordered phases, from ferromagnetic order to spin-density waves to time crystals. Unlike the time crystals that have been found in unitary models, those that occur here are \\emph{incommensurate} with the drive frequency. The period of the incommensurate time-crystal phase may be tuned by adjusting the circuit parameters. We demonstrate that the phases of our quantum circuit, including the inherently non-equilibrium dynamical ones, correspond to complex-temperature equilibrium phases o","authors_text":"Chris A. Hooley, Daniel P. Arovas, Sankhya Basu, Sarang Gopalakrishnan, Vadim Oganesyan","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2021-03-19T04:37:43Z","title":"Fisher zeros and persistent temporal oscillations in non-unitary quantum circuits"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.10628","kind":"arxiv","version":3},"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":"sha256:1d0560d743341f0d2db81d8521d65ef1d6dd6cf51bf75bf394ec713cd6efaac5","target":"record","created_at":"2026-07-05T04:19:21Z","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":"cbe9622092769794e762d004cc4b9e470af65a979656dcc15fa232573e8e1a78","cross_cats_sorted":["cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2021-03-19T04:37:43Z","title_canon_sha256":"f39866564334b147dc731e1f4f844ddd215dfa4675a04099952a99350d786b64"},"schema_version":"1.0","source":{"id":"2103.10628","kind":"arxiv","version":3}},"canonical_sha256":"d1f9868a38b1c270d752f40045268b5682f1a18b861a2056d1253b107b27ca4e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d1f9868a38b1c270d752f40045268b5682f1a18b861a2056d1253b107b27ca4e","first_computed_at":"2026-07-05T04:19:21.758138Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:19:21.758138Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IIdFMrPeaxJmYanrdXcFWI5W54qEP09vYUTXyJXg5yKUozotcJBJ+jYBaY+luXu9ug6d3x9n/qKEtdj3rYbSDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:19:21.758694Z","signed_message":"canonical_sha256_bytes"},"source_id":"2103.10628","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1d0560d743341f0d2db81d8521d65ef1d6dd6cf51bf75bf394ec713cd6efaac5","sha256:65466482fcd56b074050e0cd745e8ff3337444b0f1906ec89edca2422f5f96fc"],"state_sha256":"62bdf8dd2ea1141f63e7fe1f0a4b529725fb599672df65832ccb75ee6121068f"}