{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:LVNSXMBYVKMAXMYMFNAH53NIOA","short_pith_number":"pith:LVNSXMBY","schema_version":"1.0","canonical_sha256":"5d5b2bb038aa980bb30c2b407eeda87015f5b882f5485b5f65e2812bcda2d23f","source":{"kind":"arxiv","id":"1712.01669","version":1},"attestation_state":"computed","paper":{"title":"Competition between spin-orbit coupling, magnetism, and dimerization in the honeycomb iridates: $\\alpha$-Li$_{2}$IrO$_{3}$ under pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. A. Tsirlin, A. Jesche, C. A. Kuntscher, D. I. Khomskii, F. Freund, I. I. Mazin, J. Ebad-Allah, M. Altmeyer, M. Hanfland, P. Gegenwart, R. Valent\\'i, V. Hermann","submitted_at":"2017-12-05T14:40:17Z","abstract_excerpt":"Single-crystal x-ray diffraction studies with synchrotron radiation on the honeycomb iridate $\\alpha$-Li$_{2}$IrO$_{3}$ reveal a pressure-induced structural phase transition with symmetry lowering from monoclinic to triclinic at a critical pressure of $P_{c}$ = 3.8 GPa. According to the evolution of the lattice parameters with pressure, the transition mainly affects the $ab$ plane and thereby the Ir hexagon network, leading to the formation of Ir--Ir dimers. These observations are independently predicted and corroborated by our \\textit{ab initio} density functional theory calculations where we"},"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":"1712.01669","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-12-05T14:40:17Z","cross_cats_sorted":[],"title_canon_sha256":"56804841bb0420ac95baccdda9cf3fa541f3a35ad75fcf1c4d7c442c6c473af0","abstract_canon_sha256":"a22f8259696e5d907ec6f67e96b2f5a24505ddd4deaa0799c07bd787438f4457"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:15.016307Z","signature_b64":"kh73zLCBbj/bngkzB2AYuRKXnXjA5Y3fpRfTHtm86kF6C8LFGToqWa0/AtLxYL1jT2LGGcC7wvQS20lI9MqxDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d5b2bb038aa980bb30c2b407eeda87015f5b882f5485b5f65e2812bcda2d23f","last_reissued_at":"2026-05-18T00:24:15.015680Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:15.015680Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Competition between spin-orbit coupling, magnetism, and dimerization in the honeycomb iridates: $\\alpha$-Li$_{2}$IrO$_{3}$ under pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. A. Tsirlin, A. Jesche, C. A. Kuntscher, D. I. Khomskii, F. Freund, I. I. Mazin, J. Ebad-Allah, M. Altmeyer, M. Hanfland, P. Gegenwart, R. Valent\\'i, V. Hermann","submitted_at":"2017-12-05T14:40:17Z","abstract_excerpt":"Single-crystal x-ray diffraction studies with synchrotron radiation on the honeycomb iridate $\\alpha$-Li$_{2}$IrO$_{3}$ reveal a pressure-induced structural phase transition with symmetry lowering from monoclinic to triclinic at a critical pressure of $P_{c}$ = 3.8 GPa. According to the evolution of the lattice parameters with pressure, the transition mainly affects the $ab$ plane and thereby the Ir hexagon network, leading to the formation of Ir--Ir dimers. These observations are independently predicted and corroborated by our \\textit{ab initio} density functional theory calculations where we"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.01669","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":"1712.01669","created_at":"2026-05-18T00:24:15.015768+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.01669v1","created_at":"2026-05-18T00:24:15.015768+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.01669","created_at":"2026-05-18T00:24:15.015768+00:00"},{"alias_kind":"pith_short_12","alias_value":"LVNSXMBYVKMA","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"LVNSXMBYVKMAXMYM","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"LVNSXMBY","created_at":"2026-05-18T12:31:28.150371+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/LVNSXMBYVKMAXMYMFNAH53NIOA","json":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA.json","graph_json":"https://pith.science/api/pith-number/LVNSXMBYVKMAXMYMFNAH53NIOA/graph.json","events_json":"https://pith.science/api/pith-number/LVNSXMBYVKMAXMYMFNAH53NIOA/events.json","paper":"https://pith.science/paper/LVNSXMBY"},"agent_actions":{"view_html":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA","download_json":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA.json","view_paper":"https://pith.science/paper/LVNSXMBY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.01669&json=true","fetch_graph":"https://pith.science/api/pith-number/LVNSXMBYVKMAXMYMFNAH53NIOA/graph.json","fetch_events":"https://pith.science/api/pith-number/LVNSXMBYVKMAXMYMFNAH53NIOA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA/action/storage_attestation","attest_author":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA/action/author_attestation","sign_citation":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA/action/citation_signature","submit_replication":"https://pith.science/pith/LVNSXMBYVKMAXMYMFNAH53NIOA/action/replication_record"}},"created_at":"2026-05-18T00:24:15.015768+00:00","updated_at":"2026-05-18T00:24:15.015768+00:00"}