Belik Alexei A, Azuma Masaki, Takano Mikio
Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu 611-0011, Japan.
Inorg Chem. 2003 Dec 15;42(25):8572-8. doi: 10.1021/ic034825w.
Magnetic properties of SrCuP2O7 and PbCu(1-x)ZnxP2O7 (x=0, 0.1, and 0.5) were studied by magnetic susceptibility, chiT, and specific heat, Cp(T). Both data showed that magnetism of SrCuP2O7 and PbCuP2O7 can be described by the one-dimensional (1D) uniform chain model despite the structural features suggesting the presence of zigzag chains with next-nearest-neighbor interactions. The chiT data were fitted by the Bonner-Fisher curve (plus temperature independent and Curie-Weiss terms) with g=2.20 and J/kB=9.38 K for SrCuP2O7 and g=2.17 and J/kB=8.41 K for PbCuP2O7 (Hamiltonian H=J SigmaSiS(i+1)). Magnetic specific heat, Cm(T), exhibited one broad maximum due to short-range ordering and one sharp peak at TN=1.64 K for SrCuP2O7 and TN=1.15 K for PbCuP2O7 due to long-range antiferromagnetic ordering. The characteristic values of the broad maxima on the Cm(T) curves (Cmax and TC(max)) were in good agreement with the theoretical calculations for the uniform 1D S=1/2 Heisenberg chain. Magnetic properties of PbCu0.9Zn0.1P2O7 still obeyed the 1D uniform chain model but those of PbCu0.5Zn0.5P2O7 did not. In air, SrCuP2O7 was stable at least up to 1373 K while PbCuP2O7 melted incongruently above 1180 K.
通过磁化率(χT)和比热(Cp(T))研究了SrCuP2O7和PbCu(1 - x)ZnxP2O7(x = 0、0.1和0.5)的磁性。两项数据均表明,尽管结构特征表明存在具有次近邻相互作用的锯齿链,但SrCuP2O7和PbCuP2O7的磁性可用一维(1D)均匀链模型来描述。对于SrCuP2O7,χT数据由Bonner - Fisher曲线(加上与温度无关的项和居里 - 外斯项)拟合,g = 2.20,J/kB = 9.38 K;对于PbCuP2O7,g = 2.17,J/kB = 8.41 K(哈密顿量H = JΣSiS(i + 1))。磁比热Cm(T)由于短程有序呈现一个宽峰,对于SrCuP2O7在TN = 1.64 K处以及对于PbCuP2O7在TN = 1.15 K处由于长程反铁磁有序呈现一个尖锐峰。Cm(T)曲线上宽峰的特征值(Cmax和TC(max))与均匀1D S = 1/2海森堡链的理论计算结果吻合良好。PbCu0.9Zn0.1P2O7的磁性仍服从1D均匀链模型,但PbCu0.5Zn0.5P2O7的磁性则不然。在空气中,SrCuP2O7至少在1373 K以下是稳定的,而PbCuP2O7在高于1180 K时会发生不一致熔化。