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CMMUNICATION
This journal is © The Royal Society of Chemistry [year] [journal], [year], [vol], 00–00 | 1
Dual Functional Additive for HTM Layer in Perovskite Solar Cells
Hong Zhang,a Yantao Shi,*
a Feng Yan,
b Liang Wang,
a Kai Wang,
a Yujin Xing,
a Qingshun Dong,
a and
Tingli Ma*a,c
Received (in XXX, XXX) Xth XXXXXXXXX 20XX, Accepted Xth XXXXXXXXX 20XX
DOI: 10.1039/b000000x 5
The ionic liquid N-butyl-N’-(4-pyridylheptyl)imidazolium
bis(trifluoromethane)sulfonimide (BuPyIm-TFSI) was used as
a dual-functional additive to improve the electrical properties
of the hole-transporting material (HTM) for perovskite solar
cells. BuPyIm-TFSI improved the conductivity of HTM and 10
reduced dark current of the solar cell simultaneously, thereby
greatly increasing the power conversion efficiency.
As a typical 3rd generation photovoltaic cell, mesoscopic solar
cells have been studied intensively since 1991.1 However, no
breakthroughs are available for conventional dye-sensitized solar 15
cells (DSCs), regardless of the many so-called strategies that have
been tested experimentally or theoretically. In 2012, this stagnant
situation was successfully overcome by using organolead halide
perovskites as sensitizer in all-solid-state mesoscopic solar cells.2
Up to now, power conversion efficiencies (PCEs) of higher than 20
15% have been reported by the groups of H. J. Snaith3 and M.
Grätzel,4 either based on a 3D porous framework or a 2D planar
structure. Undoubtedly, perovskite solar cells open up a new and
promising avenue for future thin-film solar cell development.5
Perovskite solar cells generally comprise a conductive 25
substrate, a compact TiO2 layer, an organolead halide perovskite
light-absorption layer (single or combined with a porous scaffold),
a hole-transporting layer (HTM), and a metal cathode (Ag or Au).
As of this writing, studies have mainly focused on designing
scaffold layers,6 optimizing the perovskite layer,3, 4, 7 exploring 30
alternative structures,8 and probing into inherent mechanisms.9
As one of the key components in perovskite solar cells, HTM
separates photo-excited electron-hole pairs and transports the
holes to the external circuit. Thus photovoltaic performance of
perovskite solar cells is highly dependent on the properties of 35
HTM in which 2,2′,7,7′-tetrakis(N,N-di-p--methoxyphenyl-
amine)9,9′-spirobifluorene (spiro-OMeTAD) is currently widely
used as the matrix for hole transportation.2-7 However, spiro-
MeOTAD alone in HTM is insufficient for obtaining high PCEs
because of low conductivity and other problems. Adding different 40
kinds of functional additives to spiro-MeOTAD can further
improve the properties of HTM and ensure the high efficiency
perovskite solar cells. For example, lithium10 or cobalt salts4 are
frequently used for p-doping to increase the hole concentration.
Despite the high volatility and unpleasant smell, TBP (4-tert-45
butylpyridine) is usually added into HTM to suppress charge-
recombination, as in traditional DSCs.11 For the first time, we use
a stable ionic liquid N-butyl-N’-(4-pyridylheptyl)imidazolium
bis(trifluoromethane) sulfonimide (BuPyIm-TFSI) as a dual-
functional additive to simultaneously improve the electrical 50
property of HTM and suppress charge combination in perovskite
solar cells. BuPyIm-TFSI improved the conductivity of HTM and
reduced the dark current of the solar cell.The PCE greatly
increased from 3.83% (with no additive in HTM) to 7.91%, and
these rates are comparable to those in conventional HTM 55
containing lithium salt and TBP. Moreover, using such dual-
functional additive can effectively simplify the components of
HTM and help reduce the production cost.
Fig. 1. Molecular structures of the BuPyIm-TFSI and spiro-OMeTAD 60
Molecular structures of BuPyIm-TFSI and spiro-MeOTAD are
shown in Fig. 1, the molecular structure of BuPyIm-TFSI was
characterized by NMR spectra in Supporting Information. As
illustrated in Fig. 1, BuPyIm-TFSI is an ionic liquid and its cation
comprises imidazolyl, pyridyl and alkyl chains that are used to 65
either link or modify the two heteroatom rings. Unlike ordinary
organic additives, ionic liquids are nearly non-volatile and
usually have excellent stability. As shown in Fig. 2a, subsequent
thermal gravimetric analysis indicated that the decomposition
temperature of BuPyIm-TFSI was higher than 300°C. 70
Undoubtedly, such satisfactory thermal stability will be
meaningful to the long-term durability of perovskite solar cells.
More importantly, the elaborate structural design enables dual
function of the BuPyIm-TFSI. On one hand, based on the
mechanism proposed by H. J. Snaith, free proton can be released 75
from imidazolyl for p-doping and thus increase the conductivity
of HTM by partial oxidation of spiro-MeOTAD.12 On the other
hand, pyridyl can function in the same way as TBP to suppress
the charge recombination that occurs at the TiO2/perovskite
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2 | Journal Name, [year], [vol], 00–00 This journal is © The Royal Society of Chemistry [year]
Table 1 Photovoltaic parameters of the peroviskite solar cells under 100 mWcm-2 light illumination.
HTM Compositions VOC (V) JSC (mA cm-2) FF PCE (%)
HTM1 Pristine spiro 0.63±0.03 12.26±0.20 0.50±0.08 3.83 ±0.20
HTM2 Spiro+BuPyIm-TFSI 0.87±0.04 16.26±0.30 0.56±0.03 7.91 ±0.30
HTM3 Spiro+Li+TBP 0.91±0.05 15.56±0.50 0.57±0.05 8.16±0.25
Fig. 2. (a) Thermal gravimetric analysis curves of BuPyIm-TFSI; (b) J-V 5
curves of CE/HTM/CE devices for different HTM.
interface.
In total, three HTM samples we prepared and designated as
HTM1, HTM2 and HTM3, respectively. HTM1 contained only
spiro-MeOTAD, whereas HTM2 contained BuPyIm-TFSI and 10
spiro-MeOTAD. For comparison, we prepared HTM3 using
spiro-MeOTAD, lithium salt (LiTFSI) and TBP based on
published works.4 Conductivities of these three HTMs were
characterized using linear sweep voltammetry by sandwiching
HTM between two platinum electrodes, as reported previously.13 15
As shown in Fig. 2b, BuPyIm-TFSI improved the conductive
property of HTM2 compared with HTM1 and HTM3. Based on a
previously reported theory, an ionic liquid such as BuPyIm-TFSI
is considered as Brϕnsted acid and can release free protons to
facilitate the oxidization of spiro-MeOTAD, which increase the 20
hole concentration and the subsequent conductivity of HTM.12
We fabricated our perovskite solar cells using a previously
described method, in which one sequential deposition route was
used to well control the morphology of CH3NH3PbI3.4 The cross
section and the top view of the perovskite solar cells are shown in 25
Fig. 3. In addition to the necessary layer of dense TiO2, we also
added one mesoporous layer of anatase TiO2 (approximately 300
nm thick) to support the CH3NH3PbI3, which was prepared by
two deposition steps using PbI2 and CH3NH3I solutions
consecutively. The formation of CH3NH3PbI3 was confirmed by 30
XRD spectroscopy (Fig. S1). We also verified that the perovskite
was uniformly distributed throughout the mesoporous TiO2 films
by performing cross-sectional scanning electron microscopy with
elemental mapping via energy dispersive X-ray analysis (Fig. S2)
35
Fig. 3. (a) Cross-sectional SEM image of a complete photovoltaic device
based on HTM2. (b) SEM image of the top view of perovskite layer.
Photovoltaic performance of the perovskite solar cells based on
HTM1, HTM2, and HTM3 was measured under AM 1.5, 100
mW/cm2 light illumination. J-V curves of these three perovskite 40
solar cells are illustrated in Fig. 4 and the detailed parameters
have been summarized in Table 1. All of the above mentioned
measurements were repeated more than three times. HTM2-based
perovskite solar cells showed a much better performance than
HTM1-based ones that contained only spiro-MeOTAD. The open-45
circuit voltage (Voc) and short-circuit current density (Jsc) of
HTM1-based perovskite solar cells were ca. 0.63 V and 12.26 mA
cm-2, respectively. The Voc and Jsc values were greatly enhanced
to ca. 0.87 V and 16.26 mA cm-2, respectively, in HTM2-based
perovskite solar cells with BuPyIm-TFSI. The fill factor, which 50
reflects the inherent resistance and the degree of chare
recombination, also increased from ca. 0.50 to 0.56. HTM2-based
perovskite solar cells achieved a PCE of 7.91% because of the
improved parameters, and this PCE value was much higher than
that of HTM1-based cells (3.83%).This result was comparable to 55
that obtained for HTM3-based cells containing LiTFSI and TBP,
as shown in Table 1.
Fig. 4. J-V curves of the peroviskite solar cells employing different HTM.
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This journal is © The Royal Society of Chemistry [year] Journal Name, [year], [vol], 00–00 | 3
To better understand the inherent mechanism underlying the
improvements in HTM2-based perovskite solar cells, we first
provide insight into the process of charge recombination by
characterizing the dark current shown in Fig. 4. An HTM2-based
solar cell exhibited a much lower dark current density than an 5
HTM1-based solar cell, indicating that BuPyIm-TFSI can
suppress charge recombination. Similar to the pronounced effect
of TBP on the interfaces of either perovsikte/TiO2 in perovskite
solar cells or dye/TiO2 in traditional solid state DSCs, BuPyIm-
TFSI also form a barrier layer that retards charge recombination 10
between electrons in TiO2 and holes in the HTM.
Fig. 5. IPCEs of the peroviskite solar cells employing different HTM
Incident photon-to-current conversion efficiencies (IPCEs) of
our perovskite solar cells were characterized and shown in Fig. 5. 15
For this type of solar cells, the spectrum rang, within which
sunlight can be effectively converted into electricity, is very wide.
The spectrum ranged from 300 nm to higher than 750 nm, with
the maximum at ca. 520 nm. Compared with HTM1-based solar
cells, HTM2- and HTM3-based perovskite solar cells 20
demonstrated higher IPCE within this broad range, especially
from 350 nm to 750 nm, where more than 50% of the photons can
be successfully converted into electricity. This result was in
agreement with J-V measurements.
In summary, the validity of ionic liquid BuPyIm-TFSI is 25
reported for the first time as a stable and dual-functional additive
to enhance HTM conductivity and suppress charge combination
in perovskite solar cells simultaneously. Various
characterizations were carried out and some relevant mechanisms
were determined to support our conclusions. BuPyIm-TFSI in 30
HTM improved photovoltaic parameters, such as photocurrent,
photovoltage, and fill factor. The PCE was enhanced remarkably.
Using such dual functional additive can effectively simplify the
components of HTM and help reduce production cost.
This work is supported by the National Natural Science 35
Foundation of China (Grant No. 51273032), Doctoral Found of
Ministry of Education of China (Grant No. 2110041110003),
International Science & Technology Cooperation Program of Chi
na (Grant No. 2013DFA51000),Fundamental Research Funds for
the Central Universities (Grant No. DUT12RC(3)57) and Open 40
Project Program of the State Key Laboratory of Physical
Chemical of Solid Surfaces, Xiamen University (Grant No.
201210). This research was also supported by the State Key
Laboratory of Fine Chemicals of China. We also thank Prof. Yi
Xiao and Mr. Youdi Zhang for helping evaporate sliver electrode. 45
Notes and references
a State Key Laboratory of Fine Chemicals, School of Chemistry, Dalian
University of Technology (DUT), 2 Linggong Rd., 116024, Dalian, P. R.
China. Fax: +86-411-84986230; Tel: +86-411-84986230;
E-mail: [email protected]; [email protected] 50 b Jiangsu Key Laboratory of Advanced Functional Polymer Design and
Application, Department of Polymer Science and Engineering, College of Chemistry, Chemical Engineering and Materials Science, Soochow
University, Suzhou, 215123, P. R. China c Graduate School of Life Science and Systems Engineering,Kyushu 55
Institute of Technolog, 2-4 Hibikino, Wakamatsu, Kitakyushu, Fukuoka,
808-0196, Japan
† Electronic Supplementary Information (ESI) available: [Experimental
details, fabrication and characterization of devices].See
DOI: 10.1039/b000000x/ 60
1 (a) O’Regan, M. Grätzel, Nature 1991, 353, 24; (b) A. Hagfeldt, G.
Boschloo, L. Sun, L. Kloo, H. Pettersson, Chem. Rev. 2010, 110,
6595; (c) W. Chen, Y. Qiu, S. Yang, Phys. Chem. Chem.
Phys., 2012, 14, 10872; (d) H. Zhang, Y. Shi, L. Wang, C. Wang, H.
Zhou, W. Guo and T. Ma, Chem. Commun., 2013, 49, 9003; (e) D. Xu, 65
X. Chen, L. Wang, L. Qiu, H. Zhang and F. Yan, Electrochim. Acta,
2013,106, 181.
2 (a) H.-S. Kim, C.-R. Lee, J.-H. Im, K.-B. Lee, T. Moehl,
A.Marchioro,S.-J. Moon, R. Humphry-Baker, J.-H. Yum, J. E. Moser,
M. Grätzel and N.-G. Park, Sci. Rep. , 2012, 2, 1; (b) M. M. Lee, J. 70
Teuscher, T. Miyasaka, T. N. Murakami and H. J. Snaith, Science,
2012, 338 , 643;
3 M. Liu, M. B. Johnston and H. J. Snaith, Nature, 2013, 501, 395.
4 J. Burschka, N. Pellet, S.-J. Moon, R. Humphry-Baker, P. Gao, M. K.
Nazeeruddin and M. Grätzel, Nature, 2013,499, 316 . 75
5 (a) N.-G. Park, J. Phys. Chem. Lett., 2013, 4, 2423; (b) B. Cai, Y.
Xing, Z. Yang, W.-H. Zhang and J. Qiu, Energy Environ. Sci., 2013,
6, 1480; (c) H. Chen, X. Pan, W. Liu, M. Cai, D. Kou, Z. Huo, X. X.
Fang and S. Dai, Chem. Commun., 2013, 49, 7277.
6 (a) J. M. Ball, M. M. Lee, A. Hey and H. Snaith, Energy 80
Environ.Sci.,2013, 6, 1739; (b) J. Qiu, Y. Qiu, K. Yan, M. Zhong, C.
Mu, H. Yan and S. Yang, Nanoscale, 2013, 5, 3245; (c) D. Bi, L.
Häggman, G. Boschloo, L. Yang, E. M. Johansson and A. Hagfeldt,
RSC Adv., 2013, 3, 18762; (d) M. J. Carnie, C. Charbonnaeu, M. L.
Davies, J. Troughton, T. M. Watson, K. Wojciechowski, H. Snaith 85
and D. A. Worsley, Chem. Commun., 2013,49, 7893.
7 (a) J. H. Noh, S. H. Im, J. H. Heo, T. N. Mandal and S. I. Seok,
Nano lett., 2013, 13, 1764; (b) G. E. Eperon, V. M. Burlakov, P.
Docampo, A. Goriely and H. J. Snaith, Adv. Funct. Mater., 2013,
DOI: 10.1002/adfm.201302090. 90
8 (a) W. A. Laban and L. Etgar, Energy Environ. Sci. , 2013, 6, 3249;
(b) W. Li, J. Li, L. Wang, G. Niu, R. Gao and Y. Qiu, J. Mater.
Chem. A, 2013, 1, 11735; (c) Z. Ku, Y. Rong, M. Xu, T. Liu and H.
Han, Sci. Rep., 2013, DOI: 10.1038/srep03132; (d) J. You, Z. Hong,
Y. Yang, Q. Chen, M. Cai, T.-B. Song, C.-C. Chen, S. Lu, Y. Liu, H. 95
Zhou and Y. Yang, ACS Nano, 2014. 8,1674.
9 (a) H.-S. Kim, I. Mora-Sero, V. Gonzalez-Pedro, F. Fabregat-
Santiago, E. J. Juarez-Perez, N.-G. Park and J. Bisquert, Nature
commun., 2013, DOI:10.1038/ncomms3242; (b) G. Xing, N.
Mathews, S. Sun, S. S. Lim, Y. M. Lam, M. Grätzel, S. Mhaisalkar 100
and T. C. Sum, Science, 2013, 342, 344.
10 A. Abate, T. Leijtens, S. Pathak, J. Teuscher, R. Avolio, M. E.
Errico, J. Kirkpatrik, J. M. Ball, P. Docampo, I. McPherson and H. J.
Snaith, Phys. Chem. Chem. Phys., 2013,15, 257.
11 W.H. Howie, J.E. Harris, J.R. Jennings, L.M. Peter, Sol. Energy 105
Mater. Sol. Cells, 2007, 91, 424.
12 A. Abate, D. J. Hollman, J. Teuscher, S. Pathak, R. Avolio, G.
D’Errico, G. Vitiello, S. Fantacci and H. J. Snaith, J. Am. Chem. Soc.
, 2013, 135, 13538.
13 M. Xu, Y. Rong, Z. Ku, A. Mei, X. Li and H. Han, J. Phys. Chem. C, 110
2013, 117, 22492.
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View Article OnlineDOI: 10.1039/C3CC49458F
The ionic liquid N-butyl-N’-(4-pyridylheptyl) imidazolium bis(trifluoromethane) sulfonimide
(BuPyIm-TFSI) was used as an additive to improve HTM conductivity and reduce dark current of
the solar cell simultaneously, thereby greatly increasing the power conversion efficiency.
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View Article OnlineDOI: 10.1039/C3CC49458F