Verma Kuldeep Chand, Kotnala R K
Centre of Advanced Study in Physics, Department of Physics, Panjab University, Chandigarh 160 014, India.
Phys Chem Chem Phys. 2016 Jul 14;18(26):17565-74. doi: 10.1039/c6cp02283a. Epub 2016 Jun 16.
We report the defects/vacancies that attribute to room temperature ferromagnetism in SnO2 in contrast to ZnO [Phys. Chem. Chem. Phys., 2016, 18, 5647], which has observed ferromagnetic ordering below room temperature, since both the systems involve similar dopant Fe, Co, and Ce ions. The Fe, Co, Ce doped SnO2 nanostructures were synthesized by a sol-gel process. The Rietveld refinement of the X-ray diffraction data detects a rutile SnO2 structure, with structural defects due to the deformation of the unit cell with doping. The pure, Fe and Co doped SnO2 have nanoparticle formation that is induced to nanorods with Ce co-doping. However, ZnO retained a nanorod-type shape with Fe and Co ions and changed to nanoparticles with Ce co-doping. The rutile SnO2 structure and defect formation with Fe, Co, and Ce ions is also confirmed with Raman vibrational modes. The observed lattice defects due to oxygen vacancies are shown by the photoluminescence study. The weak room temperature ferromagnetism is observed with Fe and Co ions in SnO2, which is enhanced with Ce ions. The zero field (ZFC) and field cooling magnetic measurements indicate an improvement in magnetization with a cusp in the ZFC curve at low temperature, observed due to an antiferromagnetic transition. It also induced variations in the magnetic coercive field due to the phenomenon of superparamagnetism, spin glasses, and magnetic clustered growth. This can be further confirmed with ac magnetic susceptibility measurements that show magnetic transitions as well as frequency dispersive and dependent behaviors of χ'(T)/χ''(T). However, the Fe, Co, Ce doped ZnO exhibit paramagnetic behavior at room temperature due to favorable antiferromagnetic interactions and have a ferromagnetic transition at low temperature with little ferromagnetic cluster growth.
我们报道了与ZnO [《物理化学化学物理》,2016年,第18卷,第5647页] 相比,SnO₂ 中归因于室温铁磁性的缺陷/空位,由于这两个体系都涉及类似的掺杂剂Fe、Co和Ce离子,而ZnO在室温以下观察到了铁磁有序。通过溶胶-凝胶法合成了Fe、Co、Ce掺杂的SnO₂ 纳米结构。X射线衍射数据的Rietveld精修检测到金红石型SnO₂ 结构,由于掺杂导致晶胞变形而存在结构缺陷。纯的、Fe和Co掺杂的SnO₂ 形成纳米颗粒,Ce共掺杂会诱导其形成纳米棒。然而,ZnO在Fe和Co离子存在下保持纳米棒形状,Ce共掺杂时变为纳米颗粒。Fe、Co和Ce离子导致的金红石型SnO₂ 结构和缺陷形成也通过拉曼振动模式得到证实。光致发光研究表明了由于氧空位导致的观察到的晶格缺陷。在SnO₂ 中观察到Fe和Co离子具有弱室温铁磁性,Ce离子会增强这种铁磁性。零场(ZFC)和场冷磁测量表明,在低温下ZFC曲线出现尖峰,磁化强度有所提高,这是由于反铁磁转变所致。由于超顺磁性、自旋玻璃和磁簇生长现象,它还引起了磁矫顽场的变化。这可以通过交流磁化率测量进一步证实,该测量显示了磁转变以及χ'(T)/χ''(T)的频率色散和频率依赖性行为。然而,Fe、Co、Ce掺杂的ZnO在室温下由于有利的反铁磁相互作用而表现出顺磁性行为,并且在低温下具有铁磁转变,铁磁簇生长很少。