Browse > Article

a-Si:H Photodiode Using Alumina Thin Film Barrier  

Hur Chang-Wu (Mokwon University)
Dimitrijev Sima (Mokwon University)
Abstract
A photodiode capable of obtaining a sufficient photo/ dark current ratio at both forward bias state and reverse bias state is proposed. The photodiode includes a glass substrate, an aluminum film formed as a lower electrode over the glass substrate, an alumina film formed as an insulator barrier over the aluminum film, a hydrogenated amorphous silicon film formed as a photo conduction layer over a portion of the alumina film, and a transparent conduction film formed as an upper electrode over the hydro-generated amorphous silicon film. A good quality alumina $(Al_2O_3)$ film is formed by oxidation of aluminum film using electrolyte solution of succinic acid. Alumina is used as a potential barrier between amorphous silicon and aluminum. It controls dark-current restriction. In case of photodiodes made by changing the formation condition of alumina, we can obtain a stable dark current $(\~10^{-12}A)$ in alumina thickness below $1000{\AA}$. At the reverse bias state of the negative voltage in ITO (Indium Tin Oxide), the photo current has substantially constant value of $5{\times}10^{-9}$ A at light scan of 100 1x. On the other hand, the photo/dark current ratios become higher at smaller thicknesses of the alumina film. Therefore, the alumina film is used as a thin insulator barrier, which is distinct from the conventional concept of forming the insulator barrier layer near the transparent conduction film. Also, the structure with the insulator thin barrier layer formed near the lower electrode, opposed to the ITO film, solves the interface problem of the ITO film because it provides an improved photo current/dark current ratio.
Keywords
hydrogenated amorphous silicon film; photodiode; insulator barrier; alumina film;
Citations & Related Records
연도 인용수 순위
  • Reference
1 K. Aflatooni, R. Hornsey, A. Nathan, 'Reverse current instabilities in amorphous silicon Schottky diodes: modeling and experiments,' IEEE Trans. Electron Devices, vol.46, 1999, pp.1417-1422   DOI   ScienceOn
2 A. Nathan, 'High performance Schottky photodiode based on polycrystalline ITO deposited at room temperature,' IEEE Workshop on Charge-Coupled Devices and Advanced Image Sensor, Karuizawa, Japan, June, 1999, pp. 10-12
3 Q. Ma, 'ITO/a-Si:H Schottky photodiode with low leakage current and high stability,' Mat. Res. Soc. Symposium B, Sanfrancisco, April, 1999, pp.5-9
4 M. Ristova, Y. Kuo, H. H. Lee, S. Lee and Y. J. Tewg, 'Amorphous Silicon Photodiodes for Image Sensing,' Applied Surface Science, 218, 44-53, 2003   DOI   ScienceOn
5 M.Hoheisel, N.Brutscher, 'The interface a-Si:H/ITO structure and properties,' J. Non-crys. Sil, vol.7, 1987, pp.959-964
6 B.W.Park, J.L.Choi, and C.W.Hur, 'Micro-crystal silicon in image sensor,' MRS, vol.283, 1992, pp. 609-612   DOI
7 J.McGil, O.Prache, 'a-Si:H alloy contact image sensor,' SID Digest, 1989, pp.252-255
8 S.Ri, H.Fujioka, K.Fujino, 'a-Si:H image sensor : characteristics of an ITO/a-Si:H junction,' MRS, Vol. 118, 1998, pp.451-455