{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DF5PCQTR3SPRNRWANYE73ALYOL","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":"f7168179aa6a85e057994019bd85bab75b6de13fda1782f509a462ad4ff1839a","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-04-16T13:55:58Z","title_canon_sha256":"e532d59dfe973b917fcaa83f84783caf554302bd85dafb88390b6f2e49e543fd"},"schema_version":"1.0","source":{"id":"2404.10576","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.10576","created_at":"2026-07-05T08:38:59Z"},{"alias_kind":"arxiv_version","alias_value":"2404.10576v1","created_at":"2026-07-05T08:38:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.10576","created_at":"2026-07-05T08:38:59Z"},{"alias_kind":"pith_short_12","alias_value":"DF5PCQTR3SPR","created_at":"2026-07-05T08:38:59Z"},{"alias_kind":"pith_short_16","alias_value":"DF5PCQTR3SPRNRWA","created_at":"2026-07-05T08:38:59Z"},{"alias_kind":"pith_short_8","alias_value":"DF5PCQTR","created_at":"2026-07-05T08:38:59Z"}],"graph_snapshots":[{"event_id":"sha256:df95d1f48b37bb4eca2428bc546e5dafa917858efa6ea6964882a038d66e1054","target":"graph","created_at":"2026-07-05T08:38:59Z","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/2404.10576/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The phase transition between gapped topological phases represents a class of unconventional criticality beyond the Landau paradigm. However, recent research has shifted attention to topological phases without a bulk gap, where the phase transitions between them are still elusive. In this work, based on large-scale density matrix renormalization group techniques, we investigate the critical behaviors of the extended quantum XXZ model obtained by the Kennedy-Tasaki transformation. Using fidelity susceptibility as a diagnostic, we obtain a complete phase diagram, which includes both topological n","authors_text":"Han-Ze Li, Hao-Long Zhang, Sheng Yang, Xue-Jia Yu","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-04-16T13:55:58Z","title":"Quantum phase transition and critical behavior between the gapless topological phases"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.10576","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:bb474ab56f3bce0ebbdb7f7a8e4a423c9b1b6c858317761bf05e7ee9ca7f716f","target":"record","created_at":"2026-07-05T08:38:59Z","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":"f7168179aa6a85e057994019bd85bab75b6de13fda1782f509a462ad4ff1839a","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-04-16T13:55:58Z","title_canon_sha256":"e532d59dfe973b917fcaa83f84783caf554302bd85dafb88390b6f2e49e543fd"},"schema_version":"1.0","source":{"id":"2404.10576","kind":"arxiv","version":1}},"canonical_sha256":"197af14271dc9f16c6c06e09fd817872f554297c8a7637a6940b206b7b56ed68","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"197af14271dc9f16c6c06e09fd817872f554297c8a7637a6940b206b7b56ed68","first_computed_at":"2026-07-05T08:38:59.219012Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:38:59.219012Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"w4KjvdppMk3N7TMidm6D69gv98pwlmJOzGPSV+jHv5stE4Hm4L3qBr0WERh/uhwY1pJNJB7laoNSOHVnXGASDw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:38:59.219539Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.10576","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bb474ab56f3bce0ebbdb7f7a8e4a423c9b1b6c858317761bf05e7ee9ca7f716f","sha256:df95d1f48b37bb4eca2428bc546e5dafa917858efa6ea6964882a038d66e1054"],"state_sha256":"495311f1a18c9569ee04a492bc13c8d328fc6d179c303db9b128113eefb82d4e"}