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This journal is c The Royal Society of Chemistry 2012 Chem. Commun., 2012, 48, 9501–9503 9501
Cite this: Chem. Commun., 2012, 48, 9501–9503
Employing electrostatic self-assembly of tailored nickel sulfide
nanoparticles for quasi-solid-state dye-sensitized solar cells with Pt-free
counter electrodesw
Won Seok Chi, Joung Woo Han, Sungeun Yang, Dong Kyu Roh, Hyunjoo Lee* and
Jong Hak Kim*
Received 26th June 2012, Accepted 7th August 2012
DOI: 10.1039/c2cc34559e
A low cost, low-temperature processable, highly efficient nickel
sulfide counter electrode is demonstrated. Using the tailored,
preformed nickel sulfide nanoparticles and electrostatic self-
assembly, a novel counter electrode was fabricated that exceeded
the efficiency of a conventional Pt-based cell.
Dye-sensitized solar cells (DSSCs) are promising photovoltaic
devices due to their high efficiency and low cost.1 Considerable
efforts have been made to boost the efficiency and stability of
cells based on structural control of the TiO2 photoelectrode,2–4
development of efficient redox couples,5,6 synthesis of new
sensitizers7,8 and development of a stable solid electrolyte.9–11
One of the current issues of DSSCs is the use of platinum (Pt) as
a counter electrode, which is a noble metal with low abundance
and high cost, limiting large-scale manufacture. Furthermore,
heat treatments are needed to increase the electrocatalytic activity
and conductivity of Pt, precluding the use of flexible plastic
substrates. Thus, the development of new, Pt-free counter
electrodes has recently received considerable attention.12–23
Carbon-based materials with a high surface area such as
mesoporous carbon or carbon nanotubes (CNTs),12,13 and
conjugated conducting polymers are representative alternative
materials to Pt, but their electrocatalytic activities are lower
than that of Pt.14,15 Recently, inorganic compounds such as
metal oxides,16,17 nitrides,18 carbides19 and sulfides20–23 have
been investigated due to the possibility of generating diverse,
new nanomaterials with simple fabrication processes. Among
them, nickel sulfide is one of the most efficient catalytic
substances. Meng’s group prepared nickel sulfide layered on
F-doped tin oxide (FTO) glass via an electro-deposition
method and obtained an efficiency (6.82%) slightly lower than
that of a Pt-based cell (7.00%) upon using a liquid electrolyte.20
Lam’s group also prepared Ni3S2-coated counter electrodes
through an annealing process after drop-casting a nickel and sulfur
precursor mixture solution; they obtained an efficiency (7.01%)
slightly lower than that of the comparable Pt-based cell (7.32%)
with a liquid electrolyte.21 These previous papers have proved
that nickel sulfide is a prospective stable catalyst that can
substitute for the Pt counter electrode. However, there have
been no reports on the efficiency of metal sulfide counter
electrodes exceeding that of conventional Pt electrodes. This is
presumably because (1) the adhesion properties between the
FTO substrate and metal sulfides were not strong enough to
reduce the interfacial resistance of the electrode/electrolyte, and
(2) the metal sulfides were not small enough to provide high
electrocatalytic activity.
Here, we report a low cost, low-temperature processable,
highly efficient nickel sulfide counter electrode exceeding the
efficiency of the comparable Pt-based cell. Nickel sulfide
nanoparticles with two different atomic ratios and morphologies
were synthesized through wet-chemistry, which enables mass
production of electrode materials and facile fabrication of the
electrode. The preformed nanoparticles turned out to have distinct
surface charges, enabling facile deposition on the electrode
through electrostatic self-assembly of nanoparticles, which is
responsible for strong adhesion between the FTO substrate
and the nickel sulfide nanoparticles.
Fig. 1a and b shows transmission electron microscopy
(TEM) images of Ni3S2 and NiS nanoparticles, respectively.
Most Ni3S2 nanoparticles have an octahedral shape with an
average size of 30 nm, whereas the rod-shaped nanoparticles
with an average length of 50 nm were dominantly found in the
NiS. The insets in Fig. 1a and b are the high resolution (HR) TEM
images of Ni3S2 andNiS, which more clearly show their shape and
size. Energy dispersive X-ray spectroscopy (EDX) analysis with
TEM revealed that the atomic ratio of Ni to S was almost 3 : 2
and 1 : 1 for Ni3S2 and NiS, respectively (Table S1, ESIw).Interestingly, the surface charges of the preformed nickel
sulfide nanoparticles were significantly different, depending on
the atomic ratio and morphology. The zeta potential values of
the nickel sulfides were measured, as shown in Fig. S1 and
Table S2 (ESIw). The zeta potential of NiS nanoparticles was
+28.4 mV in ethanol solution, which was more than two-fold
greater than that of the Ni3S2 nanoparticles (+11.3 mV).
Nickel sulfide nanoparticles with a positive surface charge
would effectively attach to the negatively charged FTO glass
Department of Chemical and Biomolecular Engineering,Yonsei University, 262 Seongsanno, Seodaemun-gu, Seoul 120-749,South Korea. E-mail: [email protected], [email protected] Electronic supplementary information (ESI) available. See DOI:10.1039/c2cc34559e
ChemComm Dynamic Article Links
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9502 Chem. Commun., 2012, 48, 9501–9503 This journal is c The Royal Society of Chemistry 2012
via electrostatic interaction.24 Thus, the NiS nanoparticles
with a higher positive surface charge were expected to be more
strongly adhered to the FTO glass than the Ni3S2 nano-
particles. These speculations were visually confirmed in the
SEM images (Fig. 1c and d) and photos (Fig. 1f). Under the
same experimental conditions, the loading of NiS nano-
particles (0.02 � 0.005 mg cm�2) was always greater than that
of Ni3S2 (0.01 � 0.007 mg cm�2) due to the greater surface
charge of the former (Scheme S1, ESIw). It should be noted
that the Pt counter electrode is formed through a chemical
reduction process directly from the precursor (H2PtCl6), which
follows a completely different mechanism compared to that of
the nickel sulfide electrodes (Fig. 1e).
The detailed properties of nickel sulfides such as crystallinity
and element composition were characterized using X-ray
diffraction (XRD) and X-ray photoelectron spectroscopy
(XPS), as shown in Fig. S2 and S3 (ESIw), respectively.25
The nickel sulfides were utilized as a catalyst in counter
electrodes for quasi-solid-state DSSCs (qssDSSCs), which
have advantages in terms of lighter weight and improved
long-term stability compared to liquid DSSCs. Furthermore,
the process temperature (200 1C) of nickel sulfides is much
lower than that of Pt (450 1C), which enables the use of flexible
substrates, which are preferred for qssDSSCs. It should also be
noted that the interfacial contact between electrode and
electrolyte plays a very crucial role in determining the perfor-
mance of solid or qssDSSCs.4,9
The qssDSSC fabricated with NiS displayed higher efficiency
(6.8% at 100 mW cm�2), which is one of the highest values
observed for qssDSSCs4,9,10 and approximately 1.2-fold greater
than that of a conventional Pt electrode (5.8%). As far as we
know, this is the first report of nickel sulfide counter electrodes
exceeding the efficiency of Pt-based cells (Fig. 2 and Table 1).20,21
The efficiency improvement is mostly due to the increased FF
value, resulting from the reduced interfacial resistance of the cell
and larger electrocatalytic activity, which will be characterized
in detail. Jsc values were not different among the cells, but the
Voc values of nickel sulfides were slightly lower than that of Pt.
This might result from recombination due to the presence of
some free nickel sulfide nanoparticles less strongly bound to
the FTO substrate.20
The internal resistance and charge transfer kinetics of
qssDSSCs fabricated with different counter electrodes were
investigated using electrochemical impedance spectroscopy (EIS)
analysis. EIS was performed under dark conditions, as shown in
Fig. S4 (ESIw). The dark EIS data indicate that the recombination
resistance of the Pt counter electrode is greater than that of the
nickel sulfide electrode, which explains the slightly lower Voc
values of nickel sulfide-based cells compared to Pt-based cells.26
EIS was also performed under 1 sun in order to investigate the
interfacial resistance of the cells, as shown in Fig. S5 (ESIw).27,28 Asmaller Rs value indicates that the catalytic material is more
strongly attached to the FTO glass substrate.19 The Rs values of
NiS, Ni3S2 and Pt were 13.8, 14.7 and 16.4 O, respectively,indicating that the strength of adhesion to the FTO is NiS >
Ni3S2 > Pt, which is consistent with the zeta potential results.
The Rct1 value can be related to the electrocatalytic activity
of materials. Cyclic voltammetry (CV) was performed on the
catalysts to investigate the electrocatalytic activity for the
reduction of I3 at the counter electrode, as shown in Fig. 3.
Fig. 1 TEM images of (a) Ni3S2 and (b) NiS nanoparticles. The insets
in (a) and (b) show HR-TEM images of each particle. SEM images of
(c) Ni3S2, (d) NiS and (e) Pt on FTO glass. (f) Photos of three counter
electrodes (Ni3S2, NiS, Pt).
Fig. 2 J–V curves of qssDSSCs with different counter electrodes
under one sun and dark conditions.
Table 1 Photovoltaic parameters of DSSCs with different counterelectrodes
SampleVoc
a
(V)Jsc
b
(mA cm�2) FFcZ(%)
Rsd
(O)Rct1
e
(O)CPE1
f
(mF)
NiS 0.75 13.5 0.65 6.8 13.8 8.5 55.6Ni3S2 0.75 13.4 0.59 5.9 14.7 22.1 26.7Pt 0.77 13.5 0.55 5.8 16.4 19.4 24.6
a Voc: open circuit voltage. b Jsc: short circuit current density.c FF: fill
factor. d Rs: series resistance. e Rct1: charge transfer resistance 1.f CPE1: constant phase element of capacitance corresponding to Rct1.
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This journal is c The Royal Society of Chemistry 2012 Chem. Commun., 2012, 48, 9501–9503 9503
All three electrodes showed two similar pairs of redox peaks,
indicating their similar roles as a catalyst.
I3� + 2e� 2 3I� (1)
3I2 + 2e� 2 2I3� (2)
Reaction (1) corresponds to the cathodic peak around �0.3 V
and an anodic peak around 0.0 V, whereas reaction (2)
corresponds to a cathodic peak around 0.25 V and an anodic
peak around 0.43 V. The cathodic peak of reaction (1) is the
most important peak, indicating the reduction of I3 at the
counter electrode with electrolyte in DSSCs.20,21 The cathodic
peak position in reaction (1) appeared at a more positive potential
for NiS compared to Pt, demonstrating superior catalytic activity of
NiS compared to Pt. TheRct1 values of NiS, Ni3S2 and Pt were 8.5,
22.1 and 19.4 O, respectively, indicating that NiS has the greatest
electrocatalytic activity, which is in good agreement with the CV
results. The CPE1 values were ordered as follows: NiScNi3S2 >
Pt, based on FTO surface coverage and consistent with the SEM
images. The small interfacial resistance at the counter electrodes
as well as the greater electrocatalytic activity of NiS is responsible
for a high FF of 0.65, resulting in higher efficiency (6.8%) than
the Pt-based cell. On the other hand, better adhesion of N3S2to the FTO glass compensated for its lower electrocatalytic
activity relative to Pt, leading to an efficiency (5.9%) compar-
able to that of a Pt-based cell (5.8%). We also found that the
monolayered, deep coverage of nickel sulfides on the FTO
glass via the electrostatic self-assembly using the drop-casting
method is most important for improving the cell performance,
as seen in Fig. S6 and Table S3 (ESIw).In conclusion, we have demonstrated a low cost, low-
temperature processable, highly efficient nickel sulfide counter
electrode. The counter electrode comprised of the tailored,
preformed nickel sulfide nanoparticles via electrostatic self-
assembly showed an efficiency of 6.8% at 100 mW cm�2. The
observed efficiency is one of the highest values for qssDSSCs4,9,10
and much greater than that of a conventional Pt electrode
(5.8%). In particular, the rod-shaped NiS nanoparticles exhibited
higher electrocatalytic activity than Pt. Furthermore, the electro-
static self-assembly method allowed the preformed nanoparticles
to attach more strongly to the FTO glass, leading to reduced
interfacial resistances of the cells. The low-cost, highly catalytic
nanomaterials and facile fabrication methods should have
enormous potential to pioneer nano-scale energy devices with
high energy conversion performance.
We acknowledge the financial support of a National Research
Foundation (NRF) grant funded by the Korean government
(MEST) through No. 2012R1A2A2A02011268 and the Korea
Center for Artificial Photosynthesis (KCAP) (NRF-2009-
C1AAA001-2009-0093879).
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Fig. 3 Cyclic voltammograms of Ni3S2, NiS and Pt electrodes in
10 mM LiI, 1 mM I2, 0.1 M LiClO4 in acetonitrile solution at a scan
rate of 50 mV s�1.
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