Laterally inhomogeneous barrier analysis of identically prepared Cd/CdS/n-Si/Au–Sb structures by SILAR method
In this study, CdS thin films have been deposited on n-Si substrate using a successive ionic layer adsorption and reaction (SILAR) method at room temperature. Structural properties have been investigated by means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) measurements. The XRD...
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Published in | Microelectronics and reliability Vol. 51; no. 12; pp. 2179 - 2184 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Kidlington
Elsevier Ltd
01.12.2011
Elsevier |
Subjects | |
Online Access | Get full text |
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Summary: | In this study, CdS thin films have been deposited on
n-Si substrate using a successive ionic layer adsorption and reaction (SILAR) method at room temperature. Structural properties have been investigated by means of X-ray diffraction (XRD) and scanning electron microscopy (SEM) measurements. The XRD and SEM investigations show that films are covered well, polycrystalline structure and good crystallinity levels. The
Cd/CdS/n-Si/Au–Sb structures (28 dots) have been identically prepared by the SILAR method. The effective barrier heights and ideality factors of these structures have been obtained from forward bias current–voltage (
I–V) and reverse bias capacitance voltage (
C–V) characteristics. The barrier height (BH) for the
Cd/CdS/n-Si/Au–Sb structure calculated from the
I–
V characteristics have ranged from 0.664
eV to 0.710
eV, and the ideality factor from 1.190 to 1.400. Lateral homogeneous barrier height has been determined approximately 0.719
eV from the experimental linear relationship between BHs and ideality factors. The experimental BH and ideality factor distributions obtained from the
I–V characteristics have been fitted by a Gaussian function, and their means of values have been found to be (0.683
±
0.01) eV and (1.287
±
0.05), respectively. The barrier height values obtained from the reverse bias
C
−2
–V characteristics have ranged from 0.720
eV to 0.865
eV and statistical analysis yields the mean (0.759
±
0.02) eV. Additionally, a doping concentration obtained from
C
−2
–V characteristics has been calculated (8.55
±
1.62)
×
10
14
cm
−3. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0026-2714 1872-941X |
DOI: | 10.1016/j.microrel.2011.04.020 |