Wang Jun, Lin Ying, Zou Huamin, Pu Shizhou, Shi Jing
Key Laboratory of Acoustic and Photonic Materials and Devices of the Ministry of Education, Department of Physics, Wuhan University, Wuhan 430072, People's Republic of China. Center for Electron Microscopy, Wuhan University, Wuhan 430072, People's Republic of China.
J Phys Condens Matter. 2009 Feb 18;21(7):075601. doi: 10.1088/0953-8984/21/7/075601. Epub 2009 Jan 13.
The effect of Co substitution for Cu on the structure and physical properties of Sr(14)(Cu(1-x)Co(x))(24)O(41) compounds was studied by analyzing the selected-area electron diffraction and convergent-beam electron diffraction patterns, and by measuring the magnetic susceptibility, the electrical resistivity and Raman spectra. It is found that the space group of the CuO(2) chain is changed from Amma to Ammm upon Co doping, but the structure of the Cu(2)O(3) ladder remains unchanged. This indicates that the displacement between two neighboring CuO(2) chains has disappeared due to Co doping. Once a small amount of Co ions are doped into the compound, exceptional changes in the Weiss temperature and in the number of dimers occur. The remarkable increase in the absolute value of the Weiss temperature indicates that the antiferromagnetic interaction in CuO(2) chains becomes very strong due to Co doping. The increase in the Curie coefficient and the number of dimers implies that the Co doping causes Zhang-Rice singlets in the chains to be decoupled into free spins Cu(2+) and holes. Then, the free spins Cu(2+) are coupled into dimers, and the holes transfer from chains to ladders, which causes the resistivity to decrease when the Co dopant concentration is low (x<0.10). When the Co dopant concentration is high (x>0.10), some Co ions are directly substituted for the Cu ions in the ladders, which results in an increase in resistivity with increasing Co dopant content.
通过分析选区电子衍射和会聚束电子衍射图案,并测量磁化率、电阻率和拉曼光谱,研究了用Co替代Cu对Sr(14)(Cu(1 - x)Co(x))(24)O(41)化合物结构和物理性质的影响。结果发现,Co掺杂后CuO(2)链的空间群从Amma变为Ammm,但Cu(2)O(3)梯子的结构保持不变。这表明由于Co掺杂,相邻两个CuO(2)链之间的位移消失了。一旦向该化合物中掺入少量Co离子,魏斯温度和二聚体数量就会发生异常变化。魏斯温度绝对值的显著增加表明,由于Co掺杂,CuO(2)链中的反铁磁相互作用变得非常强。居里系数和二聚体数量的增加意味着Co掺杂导致链中的张 - 赖斯单重态解耦为自由自旋Cu(2+)和空穴。然后,自由自旋Cu(2+)耦合形成二聚体,空穴从链转移到梯子上,这导致当Co掺杂浓度较低(x < 0.10)时电阻率降低。当Co掺杂浓度较高(x > 0.10)时,一些Co离子直接替代梯子中的Cu离子,这导致电阻率随Co掺杂含量的增加而增加。