{"paper":{"title":"Peculiar Phase Diagram with Isolated Superconducting Regions in ThFeAsN$_{1-x}$O$_x$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Bai-Zhuo Li, Cao Wang, Chun-Mu Feng, Dong-Ze Wang, Feng-Yuan Zhang, Fu-Xiang Zhang, Guang-han Cao, Hua-Fu Zhang, Jia-Lu Wang, Qiang Jing, Shu-Gang Tan, Yu-ke Li, Yu-Ping Sun, Yu-Xue Mei, Zhi-Cheng Wang","submitted_at":"2018-05-31T01:06:11Z","abstract_excerpt":"ThFeAsN$_{1-x}$O$_x$ ($0\\leq x\\leq0.6$) system with heavy electron doping has been studied by the measurements of X-ray diffraction, electrical resistivity, magnetic susceptibility and specific heat. The non-doped compound exhibits superconductivity at $T_\\mathrm{c}^\\mathrm{onset}=30$ K, which is possibly due to an internal uniaxial chemical pressure that is manifested by the extremely small value of As height with respect to the Fe plane. With the oxygen substitution, the $T_\\mathrm{c}$ value decreases rapidly to below 2 K for $0.1\\leq x\\leq0.2$, and surprisingly, superconductivity re-appears"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.12276","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"}