Ludwig-Maximilians-Universität München, Department Chemie, München, Germany.
Phys Chem Chem Phys. 2012 Sep 7;14(33):11610-25. doi: 10.1039/c2cp41139c. Epub 2012 Jul 17.
The electrical conductivity of aluminium doped zinc oxide (AZO, ZnO:Al) materials depends on doping induced defects and grain structure. This study aims at relating macroscopic electrical conductivity of AZO nanoparticles with their atomic structure, which is non-trivial because the derived materials are heavily disordered and heterogeneous in nature. For this purpose we synthesized AZO nanoparticles with different doping levels and narrow size distribution by a microwave assisted polyol method followed by drying and a reductive treatment with forming gas. From these particles electrically conductive, optically transparent films were obtained by spin-coating. Characterization involved energy-dispersive X-ray analysis, wet chemical analysis, X-ray diffraction, electron microscopy and dynamic light scattering, which provided a basis for a detailed structural solid-state NMR study. A multinuclear ((27)Al, (13)C, (1)H) spectroscopic investigation required a number of 1D MAS NMR and 2D MAS NMR techniques (T(1)-measurements, (27)Al-MQMAS, (27)Al-(1)H 2D-PRESTO-III heteronuclear correlation spectroscopy), which were corroborated by quantum chemical calculations with an embedded cluster method (EEIM) at the DFT level. From the combined data we conclude that only a small part of the provided Al is incorporated into the ZnO structure by substitution of Zn. The related (27)Al NMR signal undergoes a Knight shift when the material is subjected to a reductive treatment with forming gas. At higher (formal) doping levels Al forms insulating (Al, H and C containing) side-phases, which cover the surface of the ZnO:Al particles and increase the sheet resistivity of spin-coated material. Moreover, calculated (27)Al quadrupole coupling constants serve as a spectroscopic fingerprint by which previously suggested point-defects can be identified and in their great majority be ruled out.
掺铝氧化锌(AZO,ZnO:Al)材料的电导率取决于掺杂诱导的缺陷和晶粒结构。本研究旨在将 AZO 纳米粒子的宏观电导率与其原子结构联系起来,由于所得到的材料在性质上严重无序和不均匀,因此这并非易事。为此,我们通过微波辅助多元醇法合成了不同掺杂水平和窄粒径分布的 AZO 纳米粒子,然后进行干燥和还原处理。从这些粒子中通过旋涂法获得了导电且光学透明的薄膜。表征涉及能量色散 X 射线分析、湿化学分析、X 射线衍射、电子显微镜和动态光散射,为详细的结构固态 NMR 研究提供了基础。多核((27)Al、(13)C、(1)H)光谱研究需要多种 1D MAS NMR 和 2D MAS NMR 技术(T(1)-测量、(27)Al-MQMAS、(27)Al-(1)H 2D-PRESTO-III 异核相关光谱),这些技术通过嵌入簇方法(EEIM)在 DFT 水平上的量子化学计算得到了证实。从综合数据中我们得出结论,只有一小部分提供的 Al 通过取代 Zn 掺入 ZnO 结构中。当材料用形成气体进行还原处理时,相关的(27)Al NMR 信号会经历 Knight 位移。在较高的(形式)掺杂水平下,Al 形成绝缘(含 Al、H 和 C)侧相,覆盖 ZnO:Al 粒子的表面并增加旋涂材料的方阻。此外,计算出的(27)Al 四极耦合常数可用作光谱指纹,可识别先前提出的点缺陷,并在大多数情况下排除它们。