{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:J65NBUDKOF5NQTLG7ETKMIVMX4","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":"c375043b1a8e8823d44c3dde0c378f65014a2867f419339bfe580ee5adebb7f2","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.supr-con","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-04-12T09:56:21Z","title_canon_sha256":"ded1858494c973a20da4b2b8943ad2200097ed5551c5823f6a5be351170ecda1"},"schema_version":"1.0","source":{"id":"2204.05671","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.05671","created_at":"2026-07-05T04:30:08Z"},{"alias_kind":"arxiv_version","alias_value":"2204.05671v3","created_at":"2026-07-05T04:30:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.05671","created_at":"2026-07-05T04:30:08Z"},{"alias_kind":"pith_short_12","alias_value":"J65NBUDKOF5N","created_at":"2026-07-05T04:30:08Z"},{"alias_kind":"pith_short_16","alias_value":"J65NBUDKOF5NQTLG","created_at":"2026-07-05T04:30:08Z"},{"alias_kind":"pith_short_8","alias_value":"J65NBUDK","created_at":"2026-07-05T04:30:08Z"}],"graph_snapshots":[{"event_id":"sha256:7dd2cabe4d9d4124e9ed9693dbf45cd3adb89f940f64d585001654dc94072b22","target":"graph","created_at":"2026-07-05T04:30:08Z","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/2204.05671/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Two-dimensional $p+ i p$ superconductors and superfluids are systems that feature chiral behavior emerging from the Cooper pairing of electrons or neutral fermionic atoms with non-zero angular momentum. Their realization has been a longstanding goal because they offer great potential utility for quantum computation and memory. However, they have so far eluded experimental observation both in solid state systems as well as in ultracold quantum gases. Here, we propose to leverage the tremendous control offered by rotating two-dimensional trapped-ion crystals in a Penning trap to simulate the dyn","authors_text":"Ana Maria Rey, Athreya Shankar, Emil A. Yuzbashyan, John J. Bollinger, Peter Zoller, Victor Gurarie","cross_cats":["cond-mat.quant-gas","cond-mat.supr-con","physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-04-12T09:56:21Z","title":"Simulating dynamical phases of chiral $p+ i p$ superconductors with a trapped ion magnet"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.05671","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":"sha256:2e8cf9b7e3ed54637d159290194546f25ceb65c132193821ff30d7ca12ac137b","target":"record","created_at":"2026-07-05T04:30:08Z","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":"c375043b1a8e8823d44c3dde0c378f65014a2867f419339bfe580ee5adebb7f2","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.supr-con","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-04-12T09:56:21Z","title_canon_sha256":"ded1858494c973a20da4b2b8943ad2200097ed5551c5823f6a5be351170ecda1"},"schema_version":"1.0","source":{"id":"2204.05671","kind":"arxiv","version":3}},"canonical_sha256":"4fbad0d06a717ad84d66f926a622acbf2569d16d3328e9021e4961563090db84","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4fbad0d06a717ad84d66f926a622acbf2569d16d3328e9021e4961563090db84","first_computed_at":"2026-07-05T04:30:08.411072Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:30:08.411072Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"K/+VJZ5fGvNj9JYNj61v6IgBj1o0uraT38tGeWmHg//5YHhu1NlE9seEOSSfvwtivEAQN9TvlHETcXixHf4NDw==","signature_status":"signed_v1","signed_at":"2026-07-05T04:30:08.411604Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.05671","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2e8cf9b7e3ed54637d159290194546f25ceb65c132193821ff30d7ca12ac137b","sha256:7dd2cabe4d9d4124e9ed9693dbf45cd3adb89f940f64d585001654dc94072b22"],"state_sha256":"23d93e9a2f40d1fbef8f822b01bbf628041fa25ea25c0cbef5caed43fcd9861a"}