{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:O6XYSS6JSUPQ5LX3TK2TKKHNQR","short_pith_number":"pith:O6XYSS6J","schema_version":"1.0","canonical_sha256":"77af894bc9951f0eaefb9ab53528ed844021aaa8ec8dc4c096a5a00e8686de5b","source":{"kind":"arxiv","id":"1704.02707","version":1},"attestation_state":"computed","paper":{"title":"Majorana dynamical mean-field study of spin dynamics at finite temperatures in the honeycomb Kitaev model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Joji Nasu, Junki Yoshitake, Yasuyuki Kato, Yukitoshi Motome","submitted_at":"2017-04-10T04:29:03Z","abstract_excerpt":"A prominent feature of quantum spin liquids is fractionalization of the spin degree of freedom. Fractionalized excitations have their own dynamics in different energy scales, and hence, affect finite-temperature ($T$) properties in a peculiar manner even in the paramagnetic state harboring the quantum spin liquid state. We here present a comprehensive theoretical study of the spin dynamics in a wide $T$ range for the Kitaev model on a honeycomb lattice, whose ground state is such a quantum spin liquid. In this model, the fractionalization occurs to break up quantum spins into itinerant matter "},"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":"1704.02707","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-04-10T04:29:03Z","cross_cats_sorted":[],"title_canon_sha256":"3fcbc88bfb3444384adc9ba3c011deb33c467f048711e9e6da51ccd8f78b6527","abstract_canon_sha256":"433d6e2dd25fd4602fee95a46fbe7edcd04bc70040211445cbf0cba304f5455b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:41.638593Z","signature_b64":"jBNcHENHJBKa2tRnxSLUdO3xmTQ0z5hJrXJ67ZxQ0zCW1+tAL6RVErM/r4oOOF/KrGocGBn6r3bM5xD9UBWdBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"77af894bc9951f0eaefb9ab53528ed844021aaa8ec8dc4c096a5a00e8686de5b","last_reissued_at":"2026-05-18T00:38:41.638059Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:41.638059Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Majorana dynamical mean-field study of spin dynamics at finite temperatures in the honeycomb Kitaev model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Joji Nasu, Junki Yoshitake, Yasuyuki Kato, Yukitoshi Motome","submitted_at":"2017-04-10T04:29:03Z","abstract_excerpt":"A prominent feature of quantum spin liquids is fractionalization of the spin degree of freedom. Fractionalized excitations have their own dynamics in different energy scales, and hence, affect finite-temperature ($T$) properties in a peculiar manner even in the paramagnetic state harboring the quantum spin liquid state. We here present a comprehensive theoretical study of the spin dynamics in a wide $T$ range for the Kitaev model on a honeycomb lattice, whose ground state is such a quantum spin liquid. In this model, the fractionalization occurs to break up quantum spins into itinerant matter "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.02707","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":""},"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":"1704.02707","created_at":"2026-05-18T00:38:41.638149+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.02707v1","created_at":"2026-05-18T00:38:41.638149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.02707","created_at":"2026-05-18T00:38:41.638149+00:00"},{"alias_kind":"pith_short_12","alias_value":"O6XYSS6JSUPQ","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_16","alias_value":"O6XYSS6JSUPQ5LX3","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_8","alias_value":"O6XYSS6J","created_at":"2026-05-18T12:31:34.259226+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/O6XYSS6JSUPQ5LX3TK2TKKHNQR","json":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR.json","graph_json":"https://pith.science/api/pith-number/O6XYSS6JSUPQ5LX3TK2TKKHNQR/graph.json","events_json":"https://pith.science/api/pith-number/O6XYSS6JSUPQ5LX3TK2TKKHNQR/events.json","paper":"https://pith.science/paper/O6XYSS6J"},"agent_actions":{"view_html":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR","download_json":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR.json","view_paper":"https://pith.science/paper/O6XYSS6J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.02707&json=true","fetch_graph":"https://pith.science/api/pith-number/O6XYSS6JSUPQ5LX3TK2TKKHNQR/graph.json","fetch_events":"https://pith.science/api/pith-number/O6XYSS6JSUPQ5LX3TK2TKKHNQR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR/action/storage_attestation","attest_author":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR/action/author_attestation","sign_citation":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR/action/citation_signature","submit_replication":"https://pith.science/pith/O6XYSS6JSUPQ5LX3TK2TKKHNQR/action/replication_record"}},"created_at":"2026-05-18T00:38:41.638149+00:00","updated_at":"2026-05-18T00:38:41.638149+00:00"}