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Intersection behavior of the current–voltage ( I–V ) characteristics of the (Au/Ni)/HfAlO 3 /n-Si (MIS) structure depends on the lighting intensity
Journal of Materials Science: Materials in Electronics ( IF 2.8 ) Pub Date : 2020-07-06 , DOI: 10.1007/s10854-020-03868-9
Engin Arslan , Yosef Badali , Şemsettin Altındal , Ekmel Özbay

The current–voltage (I–V) and capacitance–voltage (C–V) behaviors of the (Au/Ni)/HfAlO3/n-Si (MIS) junctions at room temperature under white light with various intensities were investigated. The ln(I)–V curves show two linear behavior regions at about 1 V before and after the point of intersection that can be defined as two separate current-conduction (CMs) Mechanisms. The values of the ideality factor (n) and the zero-bias barrier height (ΦB0) were extracted using the slope and intercept of the ln(I)–V curve before and after the intersection point based on lighting power. Although the ΦB0 values decrease with increasing light power, n increases for two regions, and there is a strong linear relationship between them. The values of photo-current (Iph) increase with the increasing lighting power due to the formation of electron–hole pairs. The slope of the double-logarithmic Iph–P was changed from 0.422 to 0.852, respectively, at − 2 V and − 9 V, which indicates the ongoing distribution of Nss. In addition, the profile of surface states (Nss) ionized by light was obtained from the capacitance measured in dark and under lighting at 1 MHz. The Nss–V curve has two characteristic peaks that correspond to the region of depletion and accumulation due to a special distribution of Nss and their restructuring and reordering under the effects of lighting and an electric field.



中文翻译:

(Au / Ni)/ HfAlO 3 / n-Si(MIS)结构的电流-电压(IV)特性的相交行为取决于照明强度

的电流-电压(I-V )和电容-电压(C-V )的(金/镍)的行为/ HfAlO中3在白光下使用各种强度室温/正硅(MIS)结进行了研究。ln(I)– V曲线显示了在相交点前后大约1 V处的两个线性行为区域,可以将其定义为两个独立的电流传导(CMs)机制。根据照明功率,使用相交之前和之后的ln(I-V曲线的斜率和截距,提取理想因子(n)和零偏置势垒高度(ΦB0)的值。虽然ΦB0值随光功率的增加而减小,两个区域的n增大,并且它们之间存在很强的线性关系。由于电子-空穴对的形成,光电流(I ph)的值随照明功率的增加而增加。双对数I ph –P的斜率在− 2 V和− 9 V处分别从0.422变为0.852,这表明N ss正在进行分布。另外,由光电离的表面状态(N ss)的轮廓是从在黑暗中和在1 MHz下在光照下测得的电容获得的。所述Ñ SS -V由于N ss的特殊分布及其在光照和电场作用下的重构和重新排序,该曲线具有两个特征峰,分别对应于耗尽和累积区域。

更新日期:2020-07-06
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