We theoretically identify the chemical thermodynamic boundary conditions that will produce n-type CuInSe2 via halogen doping. Remarkably, we find that due to the low formation energies of the intrinsic defects, VCu and InCu in CuInSe2, the growth conditions that maximize the halogen donor incorporation do not yield n-type conductivity, whereas the conditions that maximize the concentration of the intrinsic donor InCu do yield n-type conductivity. Under the latter conditions, however, the contribution of the halogen donors to the net donor concentration stays significantly below that of InCu.

1.
K.
Ramanathan
,
F. S.
Hasoon
,
S.
Smith
,
D. L.
Young
,
M. A.
Contreras
,
P. K.
Johnson
,
A. O.
Pudov
, and
J. R.
Sites
,
J. Phys. Chem. Solids
64
,
1495
(
2003
).
3.
P.
Migliorato
,
L. J.
Shay
,
H. M.
Kasper
, and
S.
Wagner
,
J. Appl. Phys.
46
,
1777
(
1975
).
4.
P. W.
Yu
,
Y. S.
Park
, and
J. T.
Grant
,
Appl. Phys. Lett.
28
,
214
(
1976
).
5.
T.
Tanaka
,
T.
Yamaguchi
,
T.
Ohshima
,
H.
Itoh
,
A.
Wakahara
, and
A.
Yoshida
,
Sol. Energy Mater. Sol. Cells
75
,
109
(
2003
). Used ion implantation of Cl, finding electron concentrations up to 3×1016cm3.
6.
A.
Zunger
,
Appl. Phys. Lett.
83
,
57
(
2003
).
7.
S. B.
Zhang
,
S. H.
Wei
, and
A.
Zunger
,
Phys. Rev. Lett.
78
,
4059
(
1997
).
8.
U.
Rau
and
H. W.
Schock
,
Appl. Phys. A: Mater. Sci. Process.
69
,
131
(
1999
).
9.
S.
Lany
and
A.
Zunger
,
Phys. Rev. Lett.
93
,
156404
(
2004
).
10.
J.
Ihm
,
A.
Zunger
, and
M. L.
Cohen
,
J. Phys. C
12
,
4409
(
1979
).
11.
G.
Kresse
and
J.
Furthmüller
,
Comput. Mater. Sci.
6
,
15
(
1996
);
G.
Kresse
and
J.
Joubert
,
Phys. Rev. B
59
,
1758
(
1999
).
12.
A. I.
Liechtenstein
,
V. I.
Anisimov
, and
J.
Zaane
,
Phys. Rev. B
52
,
R5468
(
1995
).
13.
G.
Makov
and
M. C.
Payne
,
Phys. Rev. B
51
,
4014
(
1995
).
14.
C.
Persson
,
Y. J.
Zhao
,
S.
Lany
, and
A.
Zunger
(unpublished).
15.

Instead of using the simplification np=exp(EgkT), as used in most textbook examples, the Fermi–Dirac distribution function is integrated numerically to obtain n and p. Accordingly, there is no assumption necessary that EF is separated from the band edges by ΔEkT.

16.
A. M.
Gabor
,
J. R.
Tuttle
,
D. S.
Albin
,
M. A.
Contreras
,
R.
Noufi
, and
A. M.
Hermann
,
Appl. Phys. Lett.
65
,
198
(
1994
).
You do not currently have access to this content.