Peschke Simon, Weippert Valentin, Senyshyn Anatoliy, Mühlbauer Martin Johann, Janka Oliver, Pöttgen Rainer, Holenstein Stefan, Luetkens Hubertus, Johrendt Dirk
Department Chemie, Ludwig-Maximilians-Universität München , D-81377 München, Germany.
Heinz Maier-Leibnitz Zentrum, Technische Universität München , Lichtenbergstrasse 1, D-85747 Garching, Germany.
Inorg Chem. 2017 Feb 20;56(4):2241-2247. doi: 10.1021/acs.inorgchem.6b02895. Epub 2017 Feb 9.
The rare-earth chromium(II) oxyselenides RECrSeO (RE = La-Nd) were synthesized in eutectic NaI/KI fluxes, and their crystal structures were determined by single-crystal and powder X-ray diffraction (PbHgClO-type, C2/m, Z = 2). The magnetic structure of LaCrSeO was solved and refined from neutron powder diffraction data. Main building blocks are chains of edge-sharing CrSeO octahedra linked together by two edge-sharing ORECr tetrahedra forming infinite ribbons. The Jahn-Teller instability of divalent Cr (d) leads to structural phase transitions at 200 and 130 K in LaCrSeO and CeCrSeO, respectively. RECrSeO are Curie-Weiss paramagnetic above T ≈ 14-17 K. Neutron powder diffraction reveals anti-ferromagnetic ordering of the Cr moments in LaCrSeO below T = 12.7(3) K with an average ordered moment of 3.40(4) μ/Cr at 4 K, which was confirmed by muon spin rotation experiments.
稀土氧硒化铬(II)RECrSeO(RE = La - Nd)是在共晶NaI/KI助熔剂中合成的,其晶体结构通过单晶和粉末X射线衍射确定(PbHgClO型,C2/m,Z = 2)。LaCrSeO的磁结构由中子粉末衍射数据解析并精修。主要结构单元是由两个共边的ORECr四面体连接在一起的共边CrSeO八面体链,形成无限长带。二价Cr(d)的 Jahn - Teller 不稳定性分别导致LaCrSeO和CeCrSeO在200 K和130 K发生结构相变。RECrSeO在T≈14 - 17 K以上为居里 - 外斯顺磁体。中子粉末衍射表明,LaCrSeO在T = 12.7(3) K以下Cr磁矩呈反铁磁有序排列,在4 K时平均有序磁矩为3.40(4) μ/Cr,这一点通过μ子自旋旋转实验得到了证实。