{"paper":{"title":"Magnetic Field and Pressure Phase Diagrams of Uranium Heavy-Fermion Compound U$_2$Zn$_{17}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Etsuji Yamamoto, Kiyohiro Sugiyama, Koichi Kindo, Masayuki Hagiwara, Naoyuki Tateiwa, Shugo Ikeda, Tatsuma D. Matsuda, Yoshichika Onuki, Yoshinori Haga","submitted_at":"2011-01-05T04:40:37Z","abstract_excerpt":"We have performed magnetization measurements at high magnetic fields of up to 53 T on single crystals of a uranium heavy-fermion compound U$_2$Zn$_{17}$ grown by the Bridgman method. In the antiferromagnetic state below the N\\'{e}el temperature $T_{\\rm N}$ = 9.7 K, a metamagnetic transition is found at $H_c$ $\\simeq$ 32 T for the field along the [11$\\bar{2}$0] direction ($a$-axis). The magnetic phase diagram for the field along the [11$\\bar{2}$0] direction is given. The magnetization curve shows a nonlinear increase at $H_m$ $\\simeq$ 35 T in the paramagnetic state above $T_{\\rm N}$ up to a cha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.0879","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"}