{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:PWODIIGOXXQ5KLLJTCWTNDNOEG","short_pith_number":"pith:PWODIIGO","schema_version":"1.0","canonical_sha256":"7d9c3420cebde1d52d6998ad368dae21852d77ec1a95e961c263e320b2a898ee","source":{"kind":"arxiv","id":"1611.03262","version":2},"attestation_state":"computed","paper":{"title":"Dzyaloshinsky-Moriya interaction and the ground state in S=3/2 perfect kagome lattice antiferromagnet $\\mathbf{KCr_3(OH)_6(SO_4)_2}$ (Cr-jarosite) studied by X-band and high-frequency ESR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hirohiko Sato, Hitoshi Ohta, Koji Okuta, Naoki Takahashi, Ryohei Nakata, Sakai Toru, Shigeo Hara, Shohei Ikeda, Susumu Okubo, Takahiro Sakurai, Tokuro Shimokawa, Wei-Min Zhang","submitted_at":"2016-11-10T11:28:00Z","abstract_excerpt":"A single crystal S=3/2 perfect kagome lattice antiferromagnet $\\mathrm{KCr_3(OH)_6(SO_4)_2}$ (Cr-jarosite) has been studied by X-band and high-frequency electron spin resonance (ESR). The g-values perpendicular to the kagome plane (c-axis) and in the plane are determined to be $g_c=1.9704 \\pm 0.0002$ and $g_\\xi=1.9720 \\pm 0.0003$, respectively, by high-frequency ESR observed at 265 K. Antiferromagnetic resonances (AFMR) with the antiferromagnetic gap of 120 GHz are observed at 1.9 K, which is below $T_N$=4.5 K. The analysis of AFMR modes by the conventional molecular field theory shows $d_p=0."},"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":"1611.03262","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-11-10T11:28:00Z","cross_cats_sorted":[],"title_canon_sha256":"dc1320e033c10a21bdbfeab160a8b34208447213310eb3c627a10c8add4d20b6","abstract_canon_sha256":"d2b4d549fbdc0093a0fcf8aed79fb2dae7dad5e6df23c2bfb56f26554a7cf06d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:52:33.866211Z","signature_b64":"3QwXxQDSrlSYDleaO+RViGNnBOmx3rodohhPoxZXCd9dwwxtRZIUU8R2yyle22BeMZ32T3F0Qu8mKDzheteqBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d9c3420cebde1d52d6998ad368dae21852d77ec1a95e961c263e320b2a898ee","last_reissued_at":"2026-05-18T00:52:33.865649Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:52:33.865649Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dzyaloshinsky-Moriya interaction and the ground state in S=3/2 perfect kagome lattice antiferromagnet $\\mathbf{KCr_3(OH)_6(SO_4)_2}$ (Cr-jarosite) studied by X-band and high-frequency ESR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hirohiko Sato, Hitoshi Ohta, Koji Okuta, Naoki Takahashi, Ryohei Nakata, Sakai Toru, Shigeo Hara, Shohei Ikeda, Susumu Okubo, Takahiro Sakurai, Tokuro Shimokawa, Wei-Min Zhang","submitted_at":"2016-11-10T11:28:00Z","abstract_excerpt":"A single crystal S=3/2 perfect kagome lattice antiferromagnet $\\mathrm{KCr_3(OH)_6(SO_4)_2}$ (Cr-jarosite) has been studied by X-band and high-frequency electron spin resonance (ESR). The g-values perpendicular to the kagome plane (c-axis) and in the plane are determined to be $g_c=1.9704 \\pm 0.0002$ and $g_\\xi=1.9720 \\pm 0.0003$, respectively, by high-frequency ESR observed at 265 K. Antiferromagnetic resonances (AFMR) with the antiferromagnetic gap of 120 GHz are observed at 1.9 K, which is below $T_N$=4.5 K. The analysis of AFMR modes by the conventional molecular field theory shows $d_p=0."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.03262","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":""},"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":"1611.03262","created_at":"2026-05-18T00:52:33.865735+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.03262v2","created_at":"2026-05-18T00:52:33.865735+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.03262","created_at":"2026-05-18T00:52:33.865735+00:00"},{"alias_kind":"pith_short_12","alias_value":"PWODIIGOXXQ5","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"PWODIIGOXXQ5KLLJ","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"PWODIIGO","created_at":"2026-05-18T12:30:39.010887+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/PWODIIGOXXQ5KLLJTCWTNDNOEG","json":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG.json","graph_json":"https://pith.science/api/pith-number/PWODIIGOXXQ5KLLJTCWTNDNOEG/graph.json","events_json":"https://pith.science/api/pith-number/PWODIIGOXXQ5KLLJTCWTNDNOEG/events.json","paper":"https://pith.science/paper/PWODIIGO"},"agent_actions":{"view_html":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG","download_json":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG.json","view_paper":"https://pith.science/paper/PWODIIGO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.03262&json=true","fetch_graph":"https://pith.science/api/pith-number/PWODIIGOXXQ5KLLJTCWTNDNOEG/graph.json","fetch_events":"https://pith.science/api/pith-number/PWODIIGOXXQ5KLLJTCWTNDNOEG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG/action/storage_attestation","attest_author":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG/action/author_attestation","sign_citation":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG/action/citation_signature","submit_replication":"https://pith.science/pith/PWODIIGOXXQ5KLLJTCWTNDNOEG/action/replication_record"}},"created_at":"2026-05-18T00:52:33.865735+00:00","updated_at":"2026-05-18T00:52:33.865735+00:00"}