{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:IUQMUDYAJX3F4IBB4765PAOTCO","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":"4a6585ee5ddd4103c0f0ed71519a2b32f76f52e4a89e3fdcc37b3687486805f3","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-07-20T14:59:20Z","title_canon_sha256":"99dae7cb798440c132c1ffd8bb25208454467df10e82311b97e1b213b5f1759a"},"schema_version":"1.0","source":{"id":"2607.18028","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.18028","created_at":"2026-07-21T02:22:12Z"},{"alias_kind":"arxiv_version","alias_value":"2607.18028v1","created_at":"2026-07-21T02:22:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.18028","created_at":"2026-07-21T02:22:12Z"},{"alias_kind":"pith_short_12","alias_value":"IUQMUDYAJX3F","created_at":"2026-07-21T02:22:12Z"},{"alias_kind":"pith_short_16","alias_value":"IUQMUDYAJX3F4IBB","created_at":"2026-07-21T02:22:12Z"},{"alias_kind":"pith_short_8","alias_value":"IUQMUDYA","created_at":"2026-07-21T02:22:12Z"}],"graph_snapshots":[{"event_id":"sha256:963c7f27aa13e46d18b20e045068c95f62f7fa4688b11a0401644699846302ba","target":"graph","created_at":"2026-07-21T02:22:12Z","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/2607.18028/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We revisit the problem of \\textit{real-time} quantum dynamics of the paradigmatic two dimensional transverse-field Ising model using the recently developed fuzzy sphere regularization scheme. By linearly ramping the transverse field from the paramagnetic phase to criticality, we study the finite-time scaling behavior of the squared order parameter $\\langle m_z^2 \\rangle$, the excitation energy density $Q$, and the two-point correlation function of $m_z$. We establish numerically that, at intermediate quench rate, $\\langle m_z^2 \\rangle$ follows the conventional Kibble-Zurek prediction set by t","authors_text":"Meng Zeng, Roderich Moessner, Shuai Yin","cross_cats":["cond-mat.stat-mech","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-07-20T14:59:20Z","title":"Universal Dynamic Scaling of 2D Quantum Ising Transition on the Fuzzy Sphere"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.18028","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":"sha256:21215342e680e2a11da37ead64dab236150512900ab7a89e45fe9ee1a8bfea3e","target":"record","created_at":"2026-07-21T02:22:12Z","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":"4a6585ee5ddd4103c0f0ed71519a2b32f76f52e4a89e3fdcc37b3687486805f3","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-07-20T14:59:20Z","title_canon_sha256":"99dae7cb798440c132c1ffd8bb25208454467df10e82311b97e1b213b5f1759a"},"schema_version":"1.0","source":{"id":"2607.18028","kind":"arxiv","version":1}},"canonical_sha256":"4520ca0f004df65e2021e7fdd781d3139f342abc242f565bd2a6fff3f2d6a025","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4520ca0f004df65e2021e7fdd781d3139f342abc242f565bd2a6fff3f2d6a025","first_computed_at":"2026-07-21T02:22:12.437958Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-21T02:22:12.437958Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NE22KMTLHumKIP2NNIqoAYgjmwRTFXMqAhVdt7yMOzbA2l1RTeICbGQxCvFLWyG5dKTjH2oVBWS/q0GQ5lxjAg==","signature_status":"signed_v1","signed_at":"2026-07-21T02:22:12.438808Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.18028","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:21215342e680e2a11da37ead64dab236150512900ab7a89e45fe9ee1a8bfea3e","sha256:963c7f27aa13e46d18b20e045068c95f62f7fa4688b11a0401644699846302ba"],"state_sha256":"f8afa3a5fe0ccb0a2fae67bb9aeccfad91310391027ca4860cdbdd04a5efc675"}