Belik Alexei A
International Center for Materials Nanoarchitectonics (WPI-MANA) and Research Center for Functional Materials, National Institute for Materials Science (NIMS) , 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan.
Inorg Chem. 2016 Dec 5;55(23):12348-12356. doi: 10.1021/acs.inorgchem.6b02237. Epub 2016 Nov 11.
Solid solutions BiMnCrO (0 ≤ x ≤ 1) have been prepared at 6 GPa and 1370-1620 K. Their structural properties have been studied with synchrotron X-ray powder diffraction, and their physical properties have been investigated by dc/ac magnetic, specific heat, dielectric, and differential scanning calorimetry measurements. A magnetic phase diagram of BiMnCrO is established. A phase with orbital ordering observed in BiMnO is suppressed at x > 0.1, accompanied by a drop in the ferromagnetic Curie temperature T from 101 K for x = 0 to 76 K for x = 0.15 and sharp changes in the lattice parameters. The T value monotonically decreases up to x = 0.3 (with T = 53 K). For intermediate compositions with x = 0.4, 0.5, spin-glass magnetic properties are found at 28 and 24 K, respectively. The Néel temperature T linearly increases from 36 K for x = 0.6 to 111 K for x = 1.0. A spin-reorientation transition is observed at 61 K for x = 0.9 and 72 K for x = 1.0. Re-entrant spin-glass transitions are also observed for samples with x = 0.3, 0.6, 0.7 by ac susceptibility at low temperatures. At high temperatures, a structural phase transition from C2/c to Pnma symmetry is observed for all compositions with a monotonic change of the phase transition temperature. The magnetic phase diagram from the BiMnO-rich side (x ≤ 0.5) resembles a phase diagram of BiMnScO solid solutions, indicating that the nature of substituting cations (magnetic or nonmagnetic) is not crucial for doped BiMnO.
在6吉帕斯卡压力和1370 - 1620开尔文温度下制备了固溶体BiMnCrO(0≤x≤1)。利用同步辐射X射线粉末衍射研究了它们的结构性质,并通过直流/交流磁性、比热、介电和差示扫描量热法测量研究了它们的物理性质。建立了BiMnCrO的磁相图。在BiMnO中观察到的具有轨道有序的相在x > 0.1时受到抑制,同时铁磁居里温度T从x = 0时的101 K下降到x = 0.15时的76 K,并且晶格参数发生急剧变化。T值单调下降直至x = 0.3(T = 53 K)。对于x = 0.4、0.5的中间成分,分别在28 K和24 K发现了自旋玻璃磁性。奈尔温度T从x = 0.6时的36 K线性增加到x = 1.0时的111 K。在x = 0.9时于61 K和x = 1.0时于72 K观察到自旋重取向转变。通过低温下的交流磁化率还观察到x = 0.3、0.6、0.7的样品出现再入自旋玻璃转变。在高温下,对于所有成分都观察到从C2/c到Pnma对称性的结构相变,且相变温度单调变化。从富BiMnO一侧(x≤0.5)的磁相图类似于BiMnScO固溶体的相图,表明取代阳离子的性质(磁性或非磁性)对于掺杂的BiMnO并不关键。