Léon Aline, Kircher Oliver, Fichtner Maximilian, Rothe Jörg, Schild Dieter
Institut für Nanotechnologie, Forschungszentrum Karlsruhe GmbH, P.O. Box 36 40, 76021 Karlsruhe, Germany.
J Phys Chem B. 2006 Jan 26;110(3):1192-200. doi: 10.1021/jp055100b.
X-ray absorption and X-ray photoelectron spectroscopy are used to investigate NaAlH4 doped with 5 mol % of Ti on the basis of either TiCl3 or Ti13.6THF by ball milling. X-ray photoelectron spectroscopy (XPS) analysis of TiCl3 or Ti colloid doped samples indicates that Ti species do not remain on the sample surface but are driven into the material with increasing milling time. The surface concentration of Ti continues to decrease during subsequent cycles under hydrogen. After several cycles, it reaches a constant value of 0.5 at. % independently of the nature of the precursor. Moreover, metallic aluminum is already present at the surface after 2 min of ball milling in the case of TiCl3 doped Na-alanate, whereas it is totally absent in the case of Ti colloid doped samples at any milling time. Upon cycling, the atomic concentration of metallic Al at the surface evolves with the reaction under hydrogen, in contrast to the Ti concentration. Analysis of the binding energies of samples doped with TiCl3 or Ti colloid, after eight desorption/absorption cycles, reveals that the Na, O, and Ti environment remains the same, while the Al environment undergoes changes. According to the extended X-ray absorption fine structure (EXAFS) analysis of TiCl3 doped Na-alanate, the local structure around Ti during the first cycle is close to that of metallic Ti but in a more distorted state. In the case of the Ti colloid doped sample, a stripping of the oxygen shell occurs. After eight cycles, a similar intermetallic phase between Ti and Al is present in the hydrogenated state of TiCl3 or Ti colloid doped samples. The local structure around Ti atoms after eight cycles consists of Al and Ti backscatterers with a Ti-Al distance of 2.79 angstroms and a Ti-Ti distance of 3.88 angstroms. This local structure is not exactly the TiAl3 phase because it differs significantly from the alloy phase in its fine structure and lacks long-range order. Volumetric measurements performed on these samples indicate that the formation of this local structure is responsible for the reduction of the reversible hydrogen capacity with the increasing number of cycles. Moreover, the formation of the alloy-like phase is correlated with a decrease of the desorption/absorption reaction rate.
采用X射线吸收光谱和X射线光电子能谱,对通过球磨法制备的、掺杂5 mol% Ti(基于TiCl3或Ti13.6THF)的NaAlH4进行研究。对掺杂TiCl3或Ti胶体的样品进行X射线光电子能谱(XPS)分析表明,随着球磨时间的增加,Ti物种并未保留在样品表面,而是被驱入材料内部。在随后的氢气循环过程中,Ti的表面浓度持续下降。经过几个循环后,无论前驱体的性质如何,其表面浓度均达到0.5原子%的恒定值。此外,对于掺杂TiCl3的Na-铝酸盐,球磨2分钟后表面即已存在金属铝,而对于掺杂Ti胶体的样品,在任何球磨时间下表面均完全不存在金属铝。与Ti浓度不同,在循环过程中,表面金属Al的原子浓度随氢气反应而变化。对经过八次脱附/吸收循环的掺杂TiCl3或Ti胶体的样品的结合能进行分析表明,Na、O和Ti的环境保持不变,而Al的环境发生了变化。根据对掺杂TiCl3的Na-铝酸盐的扩展X射线吸收精细结构(EXAFS)分析,第一个循环中Ti周围的局部结构接近金属Ti,但处于更扭曲的状态。对于掺杂Ti胶体的样品,氧壳层发生了剥离。经过八次循环后,在掺杂TiCl3或Ti胶体的样品的氢化状态下,Ti和Al之间存在类似的金属间相。八次循环后Ti原子周围的局部结构由Al和Ti背散射体组成,Ti-Al距离为2.79埃,Ti-Ti距离为3.88埃。这种局部结构并不完全是TiAl3相,因为其精细结构与合金相有显著差异且缺乏长程有序。对这些样品进行的体积测量表明,这种局部结构的形成导致了可逆储氢容量随循环次数增加而降低。此外,类合金相的形成与脱附/吸收反应速率的降低相关。