ZnO thin films doped with various amounts of In impurities were prepared by magnetron sputtering at a substrate temperature of 150°C. The shift in optical bandgap of the In-doped ZnO films is studied as a function of carrier concentration. Nominally doped ZnO films exhibit an increase in the measured optical band gap known as the Burstein-Moss effect. Dominant band gap narrowing is observed with increased doping. XPS and TOFSIMS analyses confirm that In is incorporated in the ZnO material. The In 3d peaks show that no metallic In is present as a result of heavy doping. The XRD phase analysis shows a preferential c-axis growth but a shift of the ZnO (002) peak to lower 2-theta values with increasing FWHM as the carrier concentration increases indicates the decline in the quality of crystallinity. An elongation of the c lattice constant is also observed and is likely to be caused by intersitital In as the amount of In dopants increases. The incorporation of In induces a semiconductor-metal transition between the carrier concentrations of 3.58 – 5.61×1019 cm−3 and structural changes in the ZnO host material.

1.
A. P.
Roth
,
J. B.
Webb
and
D. F.
Williams
,
Phys. Rev. B
25
,
7836
7839
(
1982
).
2.
K. J.
Kim
and
Y. R.
Park
,
Appl. Phys. Lett.
78
,
475
477
(
2001
).
3.
J.
Chastain
,
Handbook of x-ray photoelectron spectroscopy
(
Physical Electronics USA
,
Minnesota
,
1995
) pp
124
125
.
4.
D. J.
Goyal
,
C.
Agashe
,
M. G.
Takwale
and
V. G.
Bhide
,
J. Mater. Res.
8
,
1052
1056
(
1993
).
5.
K. G.
Saw
,
K.
Ibrahim
,
Y. T.
Lim
and
M. K.
Chai
,
Thin Solid Films
515
,
2879
2884
(
2007
).
6.
B.
Kumar
and
H.
Gong
,
J. Appl. Phys.
97
,
063706
(
2005
).
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