利用混合DFT技术确定BiVO4|NiOOH界面的波段对准

J. Conesa
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引用次数: 0

摘要

了解半导体之间的带偏移是很重要的,这对于确定界面上电子转移的方向至关重要。通常有两种方法用于根据第一原理确定方向:交替放置接触的板料(它们之间没有空白空间)和在存在真空空间的情况下对每个材料表面进行单独计算。第一种方法可能由于外延匹配不足而导致扭曲,这可能导致带隙变化,第二种方法可能忽略了界面上的电子转移,这在具有非常不同的平均电负性的系统中可能很重要。这也可能意味着电子密度溢出到真空空间中,而这在实际界面中是不存在的。本文采用两种方法对BiVO4/NiOOH界面进行了研究,并对研究结果进行了比较;这里的结果与光电化学有关。该方法基于混合密度泛函理论方法,给出了与实验值一致的体相带隙值(在一种情况下,一个值反映了理论值)。混合dft导出的能带位置之间的距离和相应的哈特里静电势分布被传递到界面上。这有助于确定价带和导带的适当位置(如C. G. Van de Walle和R. M. Martin, Phys所建议的)。Rev. B 1987, 35, 8154)。保证了界面是非极性的(Tasker准则:P.W. Tasker, J. Phys。[j] .固体物理学报,1999,12(2):481 - 481。
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Determining the Band Alignment at the BiVO4|NiOOH Interface Using the Hybrid DFT Technique
It is important to understand the band offsets between semiconductors, which are crucial to determine the direction of electron transfer at the interfaces. Two methods are normally used to determine the direction from the first principles: alternating slabs put in contact (without empty spaces between them) and separate calculations for each material surface in the presence of vacuum spaces. The first method may introduce distortions due to insufficient epitaxial match, which may lead to bandgap changes, and the second may neglect electron transfer at the interface, which may be important in systems exhibiting very different average electronegativities. This can also imply a spill of electronic density into the vacuum spaces, which will not be present at real interfaces. Herein, both approaches were used to study the BiVO4/NiOOH interface, and the results were compared; the results are here relevant for photoelectrochemistry. The method is based on hybrid Density Functional Theory methods which give for the bulk phases Bandgap values that agree with the experimental ones (in one case, a value reflecting the theoretical value). The distances between the (hybrid DFT-derived) band positions and the corresponding profiles of the Hartree electrostatic potential were transferred to the interfaces. This helps determining the appropriate positions of the valence and conduction bands (as has been suggested by C. G. Van de Walle & R. M. Martin, Phys. Rev. B 1987, 35, 8154). It is ensured that the interfaces are nonpolar (Tasker’s criterion: P.W. Tasker, J. Phys. C: Solid State Phys. 1979, 12, 4977).
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