{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:BUWS5N6ANM7AFT6JI3XLWDO4AC","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":"802334bf695d6ba6e9529b9e1410e43dcf14304440a3fb03d94303ed719aeafb","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2022-10-27T15:09:36Z","title_canon_sha256":"0e57c49575b6227ec03160be94c9096b736aef7f3dce1508d0ff3ebc107bb455"},"schema_version":"1.0","source":{"id":"2210.15526","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.15526","created_at":"2026-07-05T06:31:06Z"},{"alias_kind":"arxiv_version","alias_value":"2210.15526v2","created_at":"2026-07-05T06:31:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.15526","created_at":"2026-07-05T06:31:06Z"},{"alias_kind":"pith_short_12","alias_value":"BUWS5N6ANM7A","created_at":"2026-07-05T06:31:06Z"},{"alias_kind":"pith_short_16","alias_value":"BUWS5N6ANM7AFT6J","created_at":"2026-07-05T06:31:06Z"},{"alias_kind":"pith_short_8","alias_value":"BUWS5N6A","created_at":"2026-07-05T06:31:06Z"}],"graph_snapshots":[{"event_id":"sha256:c38e134961bbd97ea78cd631c8bcddfe189f36387c180f32f7b161402c26fac9","target":"graph","created_at":"2026-07-05T06:31:06Z","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/2210.15526/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Quantum simulation of quasicrystals in synthetic bosonic matter now paves the way to the exploration of these intriguing systems in wide parameter ranges. Yet thermal fluctuations in such systems compete with quantum coherence, and significantly affect the zero-temperature quantum phases. Here we determine the thermodynamic phase diagram of interacting bosons in a two-dimensional, homogeneous quasicrystal potential. Our results are found using quantum Monte Carlo simulations. Finite-size scaling is carefully considered and the quantum phases are systematically distinguished from thermal phases","authors_text":"Hepeng Yao, Laurent Sanchez-Palencia, Zhaoxuan Zhu","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2022-10-27T15:09:36Z","title":"Thermodynamic Phase Diagram of Two-Dimensional Bosons in a Quasicrystal Potential"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.15526","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":"sha256:5c4d9afb274966a0549c6ed2fd9aed6850f3c0ecc9de9bc786efe6e4dd79f167","target":"record","created_at":"2026-07-05T06:31:06Z","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":"802334bf695d6ba6e9529b9e1410e43dcf14304440a3fb03d94303ed719aeafb","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2022-10-27T15:09:36Z","title_canon_sha256":"0e57c49575b6227ec03160be94c9096b736aef7f3dce1508d0ff3ebc107bb455"},"schema_version":"1.0","source":{"id":"2210.15526","kind":"arxiv","version":2}},"canonical_sha256":"0d2d2eb7c06b3e02cfc946eebb0ddc00a983671342fcaa10acb00aa57541d928","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0d2d2eb7c06b3e02cfc946eebb0ddc00a983671342fcaa10acb00aa57541d928","first_computed_at":"2026-07-05T06:31:06.421305Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:31:06.421305Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IsHUfnU188un0Vl572sTbZTGafWpaPDWrlLORmOA3kJp68307FygUhYVPrHdIfZikm+z02CkYcLQYcecVvd5BA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:31:06.421780Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.15526","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5c4d9afb274966a0549c6ed2fd9aed6850f3c0ecc9de9bc786efe6e4dd79f167","sha256:c38e134961bbd97ea78cd631c8bcddfe189f36387c180f32f7b161402c26fac9"],"state_sha256":"226cb5e3c3006f208cfede4a6166fe3d37bbfc200aa9a5fa6f57a798bfd6b870"}