{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:UVP5DLS4ANLLMKWS7SG2G4UYPP","short_pith_number":"pith:UVP5DLS4","schema_version":"1.0","canonical_sha256":"a55fd1ae5c0356b62ad2fc8da372987bd41cd0e286d1a4c037fdb1d32d0ef07b","source":{"kind":"arxiv","id":"2010.07900","version":1},"attestation_state":"computed","paper":{"title":"Dynamic fingerprint of fractionalized excitations in single-crystalline Cu$_3$Zn(OH)$_6$FBr","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cai Liu, Dapeng Yu, Fei Ye, Hu Zhang, Jia-Wei Mei, Junfeng Dai, Jun Zhang, Le Wang, Lianglong Huang, Miao-Ling Lin, Patrick A. Lee, Ping-Heng Tan, Qiye Liu, Wenrui Jiang, Xingqiang Shi, Ying Fu, Zhanyang Hao","submitted_at":"2020-10-15T17:25:58Z","abstract_excerpt":"Quantum spin liquid (QSL) represents a new class of condensed matter states characterized by the long-range many-body entanglement of topological orders. The most prominent feature of the elusive QSL state is the existence of fractionalized spin excitations. Subject to the strong quantum fluctuations, the spin-1/2 antiferromagnetic system on a kagome lattice is the promising candidate for hosting a QSL ground state, but the structurally ideal realization is rare. Here, we report Raman scattering on the single crystalline Cu$_3$Zn(OH)$_6$FBr, and confirm that the ideal kagome structure remains "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2010.07900","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2020-10-15T17:25:58Z","cross_cats_sorted":[],"title_canon_sha256":"5684a13b1767f3af74901a02935b68ebec7d08381d78c4b200ddc13585da47c8","abstract_canon_sha256":"da6b6e61ecdcb19444828d05bd16643da14338caa2d38c40e0f61d3a7a685886"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:47:26.635412Z","signature_b64":"fULkoVOvQ9SZQAtSS57m0qjv+h8LZLK8XTRWqD1/WaF0mcRMTLIEjDVAr4G48NQR9wSwRiZtIH+cMwmPr4kdCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a55fd1ae5c0356b62ad2fc8da372987bd41cd0e286d1a4c037fdb1d32d0ef07b","last_reissued_at":"2026-07-05T02:47:26.634960Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:47:26.634960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamic fingerprint of fractionalized excitations in single-crystalline Cu$_3$Zn(OH)$_6$FBr","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cai Liu, Dapeng Yu, Fei Ye, Hu Zhang, Jia-Wei Mei, Junfeng Dai, Jun Zhang, Le Wang, Lianglong Huang, Miao-Ling Lin, Patrick A. Lee, Ping-Heng Tan, Qiye Liu, Wenrui Jiang, Xingqiang Shi, Ying Fu, Zhanyang Hao","submitted_at":"2020-10-15T17:25:58Z","abstract_excerpt":"Quantum spin liquid (QSL) represents a new class of condensed matter states characterized by the long-range many-body entanglement of topological orders. The most prominent feature of the elusive QSL state is the existence of fractionalized spin excitations. Subject to the strong quantum fluctuations, the spin-1/2 antiferromagnetic system on a kagome lattice is the promising candidate for hosting a QSL ground state, but the structurally ideal realization is rare. Here, we report Raman scattering on the single crystalline Cu$_3$Zn(OH)$_6$FBr, and confirm that the ideal kagome structure remains "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.07900","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2010.07900/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2010.07900","created_at":"2026-07-05T02:47:26.635018+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.07900v1","created_at":"2026-07-05T02:47:26.635018+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.07900","created_at":"2026-07-05T02:47:26.635018+00:00"},{"alias_kind":"pith_short_12","alias_value":"UVP5DLS4ANLL","created_at":"2026-07-05T02:47:26.635018+00:00"},{"alias_kind":"pith_short_16","alias_value":"UVP5DLS4ANLLMKWS","created_at":"2026-07-05T02:47:26.635018+00:00"},{"alias_kind":"pith_short_8","alias_value":"UVP5DLS4","created_at":"2026-07-05T02:47:26.635018+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP","json":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP.json","graph_json":"https://pith.science/api/pith-number/UVP5DLS4ANLLMKWS7SG2G4UYPP/graph.json","events_json":"https://pith.science/api/pith-number/UVP5DLS4ANLLMKWS7SG2G4UYPP/events.json","paper":"https://pith.science/paper/UVP5DLS4"},"agent_actions":{"view_html":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP","download_json":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP.json","view_paper":"https://pith.science/paper/UVP5DLS4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.07900&json=true","fetch_graph":"https://pith.science/api/pith-number/UVP5DLS4ANLLMKWS7SG2G4UYPP/graph.json","fetch_events":"https://pith.science/api/pith-number/UVP5DLS4ANLLMKWS7SG2G4UYPP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP/action/storage_attestation","attest_author":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP/action/author_attestation","sign_citation":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP/action/citation_signature","submit_replication":"https://pith.science/pith/UVP5DLS4ANLLMKWS7SG2G4UYPP/action/replication_record"}},"created_at":"2026-07-05T02:47:26.635018+00:00","updated_at":"2026-07-05T02:47:26.635018+00:00"}