{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:KTSKKWCE7FAI7HCB64EO23OVYH","short_pith_number":"pith:KTSKKWCE","schema_version":"1.0","canonical_sha256":"54e4a55844f9408f9c41f708ed6dd5c1e027be4f7978d9ed7e5b79806a7a5b95","source":{"kind":"arxiv","id":"2305.19189","version":1},"attestation_state":"computed","paper":{"title":"Classification of Classical Spin Liquids: Detailed Formalism and Suite of Examples","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Andriy H. Nevidomskyy, Han Yan, Owen Benton, Roderich Moessner","submitted_at":"2023-05-30T16:33:20Z","abstract_excerpt":"The hallmark of highly frustrated systems is the presence of many states close in energy to the ground state. Fluctuations between these states can preclude the emergence of any form of order and lead to the appearance of spin liquids. Even on the classical level, spin liquids are not all alike: they may have algebraic or exponential correlation decay, and various forms of long wavelength description, including vector or tensor gauge theories. Here, we introduce a classification scheme, allowing us to fit the diversity of classical spin liquids (CSLs) into a general framework as well as predic"},"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":"2305.19189","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-05-30T16:33:20Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"54bcd7d436ce0d8522a00c783e3d2e6eb756f39962c839d72697a855facf3b40","abstract_canon_sha256":"f9bbfc96ed2f3f73f79ecdf74536434521f05dd3e530efb3ce0ca8c290cf46ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:15:39.304772Z","signature_b64":"AmBxdd9ftBQBG2f+3GtI9oQ+a5w3S/YJ5lXXLXYABNwspnEzVXUmsOoFig5JKqypV1qlLC99ywiD/JQNFghrDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"54e4a55844f9408f9c41f708ed6dd5c1e027be4f7978d9ed7e5b79806a7a5b95","last_reissued_at":"2026-07-05T06:15:39.304347Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:15:39.304347Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Classification of Classical Spin Liquids: Detailed Formalism and Suite of Examples","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Andriy H. Nevidomskyy, Han Yan, Owen Benton, Roderich Moessner","submitted_at":"2023-05-30T16:33:20Z","abstract_excerpt":"The hallmark of highly frustrated systems is the presence of many states close in energy to the ground state. Fluctuations between these states can preclude the emergence of any form of order and lead to the appearance of spin liquids. Even on the classical level, spin liquids are not all alike: they may have algebraic or exponential correlation decay, and various forms of long wavelength description, including vector or tensor gauge theories. Here, we introduce a classification scheme, allowing us to fit the diversity of classical spin liquids (CSLs) into a general framework as well as predic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.19189","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/2305.19189/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":"2305.19189","created_at":"2026-07-05T06:15:39.304401+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.19189v1","created_at":"2026-07-05T06:15:39.304401+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.19189","created_at":"2026-07-05T06:15:39.304401+00:00"},{"alias_kind":"pith_short_12","alias_value":"KTSKKWCE7FAI","created_at":"2026-07-05T06:15:39.304401+00:00"},{"alias_kind":"pith_short_16","alias_value":"KTSKKWCE7FAI7HCB","created_at":"2026-07-05T06:15:39.304401+00:00"},{"alias_kind":"pith_short_8","alias_value":"KTSKKWCE","created_at":"2026-07-05T06:15:39.304401+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2508.06606","citing_title":"Classical fracton spin liquid and Hilbert space fragmentation in a 2D spin-$1/2$ model","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2510.17258","citing_title":"Real space decay of flat band projectors from compact localized states","ref_index":62,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH","json":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH.json","graph_json":"https://pith.science/api/pith-number/KTSKKWCE7FAI7HCB64EO23OVYH/graph.json","events_json":"https://pith.science/api/pith-number/KTSKKWCE7FAI7HCB64EO23OVYH/events.json","paper":"https://pith.science/paper/KTSKKWCE"},"agent_actions":{"view_html":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH","download_json":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH.json","view_paper":"https://pith.science/paper/KTSKKWCE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.19189&json=true","fetch_graph":"https://pith.science/api/pith-number/KTSKKWCE7FAI7HCB64EO23OVYH/graph.json","fetch_events":"https://pith.science/api/pith-number/KTSKKWCE7FAI7HCB64EO23OVYH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH/action/storage_attestation","attest_author":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH/action/author_attestation","sign_citation":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH/action/citation_signature","submit_replication":"https://pith.science/pith/KTSKKWCE7FAI7HCB64EO23OVYH/action/replication_record"}},"created_at":"2026-07-05T06:15:39.304401+00:00","updated_at":"2026-07-05T06:15:39.304401+00:00"}