Kim et al.
Synthesis of CZTS Nanoparticles for Low-Cost Solar Cells
peaks were analyzed and compared with the data of
JCPDS card No 26-0575 for tetragonal CZTS (referred
Figure 6 shows the XRD patterns of the CZTS nanopar-
ticles synthesized for various reaction times. The diffrac-
tion peaks related to the secondary CuS and ternary
Cu SnS were observed because of Cu too rich and
Sn poor system. However, the additional secondary or
ternary phases were not formed, although the reaction time
increases.
2
0
as red box ꢀ). Other secondary or ternary XRD peaks
were referred CuS as empty orange circle (ꢀ), Cu S as
2
3
4
2
2
orange dot (•), Cu Sn S as purple upper triangle (ꢁ),
2
3 7
Cu SnS as black clover (♣) and Cu SnS as left trian-
3
4
4
4
2
1
gle ( ). All the samples exhibited the strongest peak near
ꢀ
2
ꢂ = 28ꢃ5 , which correspond to (1 1 2) plane of tetrago-
nal CZTS, and several small peaks associated with CZTS
phase. In addition, some secondary and ternary phases
were observed from the XRD patterns. This may be due
to non-stoichiometric composition of Cu rich and S poor,
as shown in Figure 3. As the reaction temerature was
higher, the intensity of the (1 1 2) plane peak increased,
indicating improvement of crystallinity. When the reac-
4
. CONCLUSION
The effects of synthesis conditions including reaction tem-
perature and time on the properties of the CZTS nanopar-
ticles. As the synthesis temperature and time increased,
the nanoparticles became larger. The CZTS nanoparticles
with uniform size were obtained at the reaction tempera-
ꢀ
ture of 240 C. In addition, the significant deviation from
ꢀ
tion temperature further increased over 300 C, a strong
the stoichiometry of CZTS was observed for longer reac-
tion times. From the XRD analysis, the strongest peak cor-
responded to (1 1 2) plane of tetragonal CZTS and some
peaks associated with secondary and ternary phases were
observed, regardless of the synthesis conditions. In parti-
clular, a strong diffraction peak appeared corresponded the
ꢀ
diffraction peak appeared at 2ꢂ = 32ꢃ1 , which is related
to the secondary SnS phase. The formation of SnS phase
is attributed to thermal decomposition of CZTS, as the fol-
1
7ꢁ19
lowing reaction,
or abnormal stoichiometry states of
Cu rich, Sn and S poor.
ꢀ
secondary SnS phase over 300 C.
Cu ZnSnS ꢄsꢀ → Cu S ꢄsꢀ+ZnS ꢄsꢀ+1/2 S ꢄgꢀ (1)
2
4
2
2
Acknowledgment: This work was supported by a grant
from the Korea Research Foundation (KRF), funded by the
Korean government (MEST) (No. 2012R1A1A2008591).
Figure 4 shows the SEM images of the CZTS nanopar-
ticles synthesized for various times. Frome the figures, the
nanoparticles became larger when the reaction time was
longer.
Figure 5 shows the EDS analysis of CZTS nanoparti-
Delivered by Ingenta to: IMn c aMd da i st it oe nr , Ut hn ii sv ew r so ir tky was also supported by the Human
IP: 188.72.126.103 On: Mon, 09 May 2016 12:06:07
Resources Development program (No. 20144030200580)
Copyright: American Scientific Publishers
of the Korea Institute of Energy Technology Evaluation
and Planning (KETEP) grant funded by the Korean gov-
ernment Ministry of Trade, Industry and Energy.
cles synthesized for various times. When the reaction time
increased, the ratio of Cu and S increased. In particular, the
significant deviation from the stoichiometry of CZTS due
to higher Cu ratio than 4 was observed for 300 min, com-
pared to the results of the reaction temperature, as shown
in Figure 2. This is attributed to smaller chalcogen loss
References and Notes
1. P. Jackson, D. Hariskos, E. Lotter, S. Paetel, R. Wuerz, R. Menner,
W. Wischmann, and M. Powalla, Prog. Photovolt: Res. Appl. 19, 894
ꢀ
than Sn loss at the reaction temperature of 240 C, as seen
(2011).
in Figure 5(b).
2
. S. Taunier, J. Sicx-Kurdi, P. P. Grand, A. Chomont, O. Ramdani,
L. Parissi, P. Panheleux, N. Naghavi, C. Hubert, M. Ben-Farah, J. P.
Fauvarque, J. Connolly, O. Roussel, P. Mogensen, E. Mahé, J. F.
Guillemoles, D. Lincot, and O. Kerrec, Thin Solid Films 480, 526
3
00 min
(2005).
3
. D. Herrmann, P. Kratzert, S. Weeke, M. Zimmer, J. D. Reiss,
R. Hunger, P. Lindbergy, E. Wallin, O. Lundberg, and L. Stolt,
Proceedings of the 40th IEEE Photovotaic Specialist Conference
(
PVSC), Denver (2014), p. 2775.
2
10 min
4
. G. Yue, D. Lu, B. Cheng, B. Sang, and B.J. Stanbery, Proceedings
of the 40th IEEE Photovotaic Specialist Conference (PVSC), Denver
(
2014), p. 2056.
1
95 min
80 min
5
. J. J. Scragg, P. J. Dale, L. M. Peter, G. Zoppi, and I. Forbes, Phys.
Stat. Sol. (b) 245, 1772 (2008).
. L. Guen, J. Sol. Stat. Chem. 35, 10 (1980).
6
1
7. K. Ito and T. Nakazawa, Jpn. J. Appl. Phys. 27, 2094 (1988).
8
9
. C. H. Henry, J. Appl. Phys. 51, 4494 (1980).
. K. Tanaka, N. Moritake, and H. Uchiki, Sol. Energ. Mat. Sol. Cells
91, 1199 (2007).
10
20
30
40
50
60
70
80
90
1
0. J. J. Scragg, P. J. Dale, and L. M. Peter, Jpn. J. Appl. Phys. 40, 500
2θ (degrees)
(2001).
Figure 6. XRD patterns of the CZTS nanoparticles synthesized for var-
ious reaction times.
11. M. A. Contreras, M. J. Romero, B. To, F. Hasoon, R. Noufi, S. Ward,
and K. Ramanathan, Thin Solid Films 403–404, 204 (2002).
J. Nanosci. Nanotechnol. 16, 5082–5086, 2016
5085