{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:AGMQZ4TTJW56E3KH2OD5ACICF6","short_pith_number":"pith:AGMQZ4TT","schema_version":"1.0","canonical_sha256":"01990cf2734dbbe26d47d387d009022f894ca61b77db83ab943727a947ccbd25","source":{"kind":"arxiv","id":"2008.02037","version":2},"attestation_state":"computed","paper":{"title":"Proximate ferromagnetic state in the Kitaev model material $\\alpha$-RuCl$_{3}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. J. Kim, B. Keimer, B. V. Lotsch, D. Weber, G. Khaliullin, H. Gretarsson, H. Kim, H. Liu, H. Suzuki, H. Takahashi, H. Yava\\c{s}, J. Bertinshaw, J. Chaloupka, K. F\\\"ursich, K. Ueda, L. Wang, M. Daghofer, M. Minola, S. Laha, Z. Yang","submitted_at":"2020-08-05T10:28:38Z","abstract_excerpt":"$\\alpha$-RuCl$_{3}$ is a major candidate for the realization of the Kitaev quantum spin liquid, but its zigzag antiferromagnetic order at low temperatures indicates deviations from the Kitaev model. We have quantified the spin Hamiltonian of $\\alpha$-RuCl$_{3}$ by a resonant inelastic x-ray scattering study at the Ru $L_{3}$ absorption edge. In the paramagnetic state, the quasi-elastic intensity of magnetic excitations has a broad maximum around the zone center without any local maxima at the zigzag magnetic Bragg wavevectors. This finding implies that the zigzag order is fragile and readily d"},"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":"2008.02037","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2020-08-05T10:28:38Z","cross_cats_sorted":[],"title_canon_sha256":"a9a624bd462400774bd8f2d79a827f3bb6d2e8d5a2aa8555c0cf7afc46799f41","abstract_canon_sha256":"d3faddcac10f2b9cf057cda711b1c15e14cfc6558f1ca99b86f9c0982e59c293"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:09:56.813959Z","signature_b64":"xXZjPuQD1+yTct1OrrX1EOj6wDUboE6wH4sBDMkZ3UqxQ3H/TWhZX3fMcDUvI6MdUCkUG75oTXnSR/GkBRc9DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"01990cf2734dbbe26d47d387d009022f894ca61b77db83ab943727a947ccbd25","last_reissued_at":"2026-07-05T03:09:56.813466Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:09:56.813466Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Proximate ferromagnetic state in the Kitaev model material $\\alpha$-RuCl$_{3}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. J. Kim, B. Keimer, B. V. Lotsch, D. Weber, G. Khaliullin, H. Gretarsson, H. Kim, H. Liu, H. Suzuki, H. Takahashi, H. Yava\\c{s}, J. Bertinshaw, J. Chaloupka, K. F\\\"ursich, K. Ueda, L. Wang, M. Daghofer, M. Minola, S. Laha, Z. Yang","submitted_at":"2020-08-05T10:28:38Z","abstract_excerpt":"$\\alpha$-RuCl$_{3}$ is a major candidate for the realization of the Kitaev quantum spin liquid, but its zigzag antiferromagnetic order at low temperatures indicates deviations from the Kitaev model. We have quantified the spin Hamiltonian of $\\alpha$-RuCl$_{3}$ by a resonant inelastic x-ray scattering study at the Ru $L_{3}$ absorption edge. In the paramagnetic state, the quasi-elastic intensity of magnetic excitations has a broad maximum around the zone center without any local maxima at the zigzag magnetic Bragg wavevectors. This finding implies that the zigzag order is fragile and readily d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2008.02037","kind":"arxiv","version":2},"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/2008.02037/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":"2008.02037","created_at":"2026-07-05T03:09:56.813524+00:00"},{"alias_kind":"arxiv_version","alias_value":"2008.02037v2","created_at":"2026-07-05T03:09:56.813524+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2008.02037","created_at":"2026-07-05T03:09:56.813524+00:00"},{"alias_kind":"pith_short_12","alias_value":"AGMQZ4TTJW56","created_at":"2026-07-05T03:09:56.813524+00:00"},{"alias_kind":"pith_short_16","alias_value":"AGMQZ4TTJW56E3KH","created_at":"2026-07-05T03:09:56.813524+00:00"},{"alias_kind":"pith_short_8","alias_value":"AGMQZ4TT","created_at":"2026-07-05T03:09:56.813524+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/AGMQZ4TTJW56E3KH2OD5ACICF6","json":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6.json","graph_json":"https://pith.science/api/pith-number/AGMQZ4TTJW56E3KH2OD5ACICF6/graph.json","events_json":"https://pith.science/api/pith-number/AGMQZ4TTJW56E3KH2OD5ACICF6/events.json","paper":"https://pith.science/paper/AGMQZ4TT"},"agent_actions":{"view_html":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6","download_json":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6.json","view_paper":"https://pith.science/paper/AGMQZ4TT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2008.02037&json=true","fetch_graph":"https://pith.science/api/pith-number/AGMQZ4TTJW56E3KH2OD5ACICF6/graph.json","fetch_events":"https://pith.science/api/pith-number/AGMQZ4TTJW56E3KH2OD5ACICF6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6/action/storage_attestation","attest_author":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6/action/author_attestation","sign_citation":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6/action/citation_signature","submit_replication":"https://pith.science/pith/AGMQZ4TTJW56E3KH2OD5ACICF6/action/replication_record"}},"created_at":"2026-07-05T03:09:56.813524+00:00","updated_at":"2026-07-05T03:09:56.813524+00:00"}