Belik Alexei A, Azuma Masaki, Matsuo Akira, Kindo Koichi, Takano Mikio
Institute for Chemical Research, Kyoto University, Uji, Japan.
Inorg Chem. 2005 May 16;44(10):3762-6. doi: 10.1021/ic050164m.
The crystal structure of isostructural SrCuV(2)O(7) and BaCuV(2)O(7) consists of one-dimensional (1D) zigzag chains of Cu atoms with next-nearest-neighbor interaction. The main intrachain interaction was found to be ferromagnetic and estimated at 4.6 K (Hamiltonian H approximately -2J). SrCuV(2)O(7) and BaCuV(2)O(7) are new examples in the scanty family of 1D ferromagnets. Isothermal magnetization measurements at 0.08 K and specific heat data showed that MCuV(2)O(7) exhibits antiferromagnetic long-range ordering at T(N) = 1.36 K for SrCuV(2)O(7) and T(N) = 1.47 K for BaCuV(2)O(7). Spin-flop transitions were observed in the antiferromagnetic state at 0.08 K near 0.5 kOe in SrCuV(2)O(7) and 2 kOe in BaCuV(2)O(7). In air, SrCuV(2)O(7) and BaCuV(2)O(7) melted incongruently above 983 and 1018 K, respectively.
同结构的SrCuV₂O₇和BaCuV₂O₇的晶体结构由具有次近邻相互作用的一维(1D)之字形铜原子链组成。发现链内主要相互作用为铁磁性,估计为4.6 K(哈密顿量H≈ -2J)。SrCuV₂O₇和BaCuV₂O₇是一维铁磁体这一稀少家族中的新例子。在0.08 K下的等温磁化测量和比热数据表明,对于SrCuV₂O₇,MCuV₂O₇在TN = 1.36 K时表现出反铁磁长程序,对于BaCuV₂O₇,TN = 1.47 K。在0.08 K时,在反铁磁态中观察到自旋翻转转变,在SrCuV₂O₇中接近0.5 kOe,在BaCuV₂O₇中为2 kOe。在空气中,SrCuV₂O₇和BaCuV₂O₇分别在983 K和1018 K以上不一致地熔化。