Efficient dye-sensitized solar cells with an organic photosensitizer featuring orderly conjugated ethylenedioxythiophene and dithienosilole blocks

Article abstract of DOI:10.1021/cm9036988

In view of the limited ruthenium resource, metal-free organic dyes may play a prominent role in the coming large-scale application of cost-effective dye-sensitized solar cells, if their efficiency and stability can be considerably improved. In this paper we utilized a binary jr-conjugated spacer of ethylenedioxythiophene and dithienosilole to construct a high molar absorption coefficient push-pull dye, characteristic of an intramolecular charge-transfer band peaking at 584 nm measured in chloroform. In comparison with the standard ruthenium sensitizer Z907, this metal-free chromophore C219 endowed a nanocrystalline titania film with an evident light-harvesting enhancement, leading to an unprecedented 10.0-10.3% efficiency at the AM1.5G conditions for dyesensitized solar cells with nonruthenium dyestuffs, although a highly volatile electrolyte was used. Transient absorption measurements have revealed that even if the kinetics of back-electron transfer and dye regeneration are considerably different for Z907 and C219, the branching ratios of these two charge-transfer channels are over 35 for both dyes, ensuring a high yield of net charge separation at the titania/dye/electrolyte interface. A solvent-free ionic liquid cell with C219 as the sensitizer exhibited an impressive efficiency of 8.9% under a low light intensity of 14.39 mW cm ^-2, making it very favorable for the indoor application of flexible dye-sensitized solar cells.

Full text of DOI:10.1021/cm9036988

Chem. Mater. 2010, 22, 1915–1925 1915
DOI:10.1021/cm9036988
Efficient Dye-Sensitized Solar Cells with an Organic Photosensitizer
Featuring Orderly Conjugated Ethylenedioxythiophene and Dithienosilole
Blocks
Wangdong Zeng,†,‡ Yiming Cao,† Yu Bai,† Yinghui Wang,† Yushuai Shi,† Min Zhang,†
Fangfang Wang,† Chunyue Pan,‡ and Peng Wang*,†
†State Key Laboratory of Polymer Physics and Chemistry, Changchun Institute of Applied Chemistry,
Chinese Academy of Sciences, Changchun 130022, China and ‡College of Chemistry and Chemical
Engineering, Central South University, Changsha 410083, China
Received December 8, 2009. Revised Manuscript Received December 20, 2009
In view of the limited ruthenium resource, metal-free organic dyes may play a prominent role in the
coming large-scale application of cost-effective dye-sensitized solar cells, if their efficiency and
stability can be considerably improved. In this paper we utilized a binary π-conjugated spacer of
ethylenedioxythiophene and dithienosilole to construct a high molar absorption coefficient
push-pull dye, characteristic of an intramolecular charge-transfer band peaking at 584 nm measured
in chloroform. In comparison with the standard ruthenium sensitizer Z907, this metal-free
chromophore C219 endowed a nanocrystalline titania film with an evident light-harvesting enhance-
ment, leading to an unprecedented 10.0-10.3% efficiency at the AM1.5G conditions for dye-
sensitized solar cells with nonruthenium dyestuffs, although a highly volatile electrolyte was used.
Transient absorption measurements have revealed that even if the kinetics of back-electron transfer
and dye regeneration are considerably different for Z907 and C219, the branching ratios of these two
charge-transfer channels are over 35 for both dyes, ensuring a high yield of net charge separation at
the titania/dye/electrolyte interface. A solvent-free ionic liquid cell with C219 as the sensitizer
exhibited an impressive efficiency of 8.9% under a low light intensity of 14.39 mW cm-2, making it
very favorable for the indoor application of flexible dye-sensitized solar cells.
1. Introduction
material innovation and device engineering, a state of the
art DSC has achieved a validated efficiency of 11.1%
measured at the AM1.5G conditions, albeit the utiliza-
tion of a highly volatile electrolyte.3
Photovoltaic cells have great potential for a low-carbon
energy supply but so far remain expensive relative to
other technologies. Greatly increased penetration of solar
cells into global energy markets requires an expansion in
attention from designs of high efficiency devices to those
that can deliver significantly lower cost per kilowatt-
hour.1 In the past years, tremendous research efforts have
been devoted to dye-sensitized solar cells2 (DSCs) during
the surging on cost-effective and resource-unlimited
photovoltaic technologies. It is also valuable to note that
the production of DSC key materials are more environ-
mentally friendly and energy-saving in contrast to the
traditional silicon technology. The foremost feature of
DSCs consists in a nanoporous semiconducting film
grafted with light-harvesting dye molecules, which could
be either immersed in a redox electrolyte or filled by a
hole-transporter. This charming assembly of low-cost
materials can perform the functions of light absorption,
charge generation, and charge transport, efficiently convert-
ing light energy to electricity. On the basis of continuous
With a view to the limited ruthenium resource, metal-
free organic dyes have attracted considerable attention in
recent years owing to their excellent flexibility in terms of
molecular tailoring. In this regard, enormous studies have
been focused on energy-level engineering of chromo-
phores to attain a capability of panchromatic light-har-
vesting.4 Furthermore, these dyestuffs need to be
controllably grafted onto a nanostructured semiconduct-
ing film with favorable stacking modes and energy align-
ments, which have significant influences on multichanel
charge-transfer kinetics, determing the ultimate cell effi-
cienies. In this contribution, we report a very promising
sensitizer coded C219 and presented in Figure 1. A
distinguishable feature of this amphiphilic push-pull
chromophore consists in a binary π-conjugated spacer,
apart from the blocks of a lipophilic alkoxy-substituted
triphenylamine electron-donor (D) and a hydrophilic
cyanoacrylic acid electron-acceptor (A). Here electron-
rich 3,4-ethylenedioxythiophene unit (EDOT) is con-
nected to D to lift up the highest occupied molecular
*To whom correspondence should be addressed. E-mail: peng.wang@
ciac.jl.cn.
(1) Wadia, C.; Alivisatos, A. P.; Kammen, D. M. Environ. Sci.
Technol. 2009, 43, 2072.
(3) Chiba, Y.; Islam, A.; Watanabe, Y.; Komiya, R.; Koide, N.; Han,
L. Jpn. J. Appl. Phys. 2006, 45 (Part 2), L638.
€
(2) O’Regan, B.; Gratzel, M. Nature 1991, 353, 737.
r
2010 American Chemical Society
Published on Web 01/22/2010
pubs.acs.org/cm

1916 Chem. Mater., Vol. 22, No. 5, 2010
Zeng et al.
photosensitizers in DSCs. Moreover, the introduction
of dihexyl-substituted DTS featuring a tetrahedral silicon
center will not affect the planarity of π-conjugated spacer
but may significantly reduce the π-π stacking of dye
molecules on nanocrystals. An aggregation of dye mole-
cules on nanocrystals may lead to a dissipative intermo-
lecular charge transfer, which could have an adverse
effect on the cell efficiency.4o,6 Even with a preliminary
optimization this novel photosensitizer C219 has already
achieved a strikingly high efficiency of 10.0-10.3% mea-
sured under irradiation of AM1.5G full sunlight, in
contrast to 9.3% attained with the standard amphiphilic
ruthenium dye Z907 (Figure 1).
2. Experimental Section
2.1. Materials. All solvents and reagents, unless otherwise
stated, were of puriss quality and used as received. n-Butyl-
ithium, 2-cyanoacetic acid, guanidinium thiocyanate (GNCS),
tert-butylpyridine (TBP), and 3R,7R-dihyroxy-5β-cholic acid
(cheno) were purchased from Fluka. 3,30-Di-n-hexylsilylene-
2,20-bithiophene (1),7 1-(2-ethylhexyloxy)-4-iodobenzene (4),8
2-(tributylstannyl)-3,4-(ethylenedioxy)thiophene,9 and Z90710
were synthesized according to the corresponding literature
methods. The synthesis of 1,3-dimethylimidazolium iodide
(DMII) and 1-ethyl-3-methylimidazolium iodide (EMII) was
described in our previous paper.11 The scattering TiO2 paste
(WER2-O) and 1-ethyl-3-methylimidazolium tetracyanoborate
(EMITCB) were received as gifts from Dyesol. The synthetic
route of C219 is outlined in Scheme 1 and the details are
described as follows.
Figure 1. Molecular structures of Z907 and C219.
orbital (HOMO) properly, and dihexyl-substituted
dithienosilole (DTS)5 conjugated with A keeps a suitable
lowest unoccupied molecular orbital (LUMO). This is the
first time that DTS has been used in the design of
(4) For example, see: (a) Hara, K.; Kurashige, M.; Dan-oh, Y.;
Kasada, C.; Shinpo, A.; Suga, S.; Sayama, K.; Arakawa, H. New
J. Chem. 2003, 27, 783. (b) Kitamura, T.; Ikeda, M.; Shigaki, K.; Inoue,
T.; Anderson, N. A.; Ai, X.; Lian, T.; Yanagida, S. Chem. Mater. 2004,
16, 1806. (c) Horiuchi, T.; Miura, H.; Sumioka, K.; Uchida, S. J. Am.
Chem. Soc. 2004, 126, 12218. (d) Thomas, K. R. J.; Lin, J. T.; Hsu,
Y.-C.; Ho, K.-C. Chem. Commun. 2005, 4098. (e) Chen, Y.; Zeng, Z.;
Li, C.; Wang, W.; Wang, X.; Zhang, B. New. J. Chem. 2005, 29, 773.
(f) Hagberg, D. P.; Edvinsson, T.; Marinado, T.; Boschloo, G.; Hagfeldt,
A.; Sun, L. Chem. Commun. 2006, 2245. (g) Li, S.-L.; Jiang, K.-J.;
Shao, K.-F.; Yang, L.-M. Chem. Commun. 2006, 2792. (h) Koumura,
N.; Wang, Z.-S.; Mori, S.; Miyashita, M.; Suzuki, E.; Hara, K. J. Am.
Chem. Soc. 2006, 128, 14256. (i) Kim, S.; Lee, J. W.; Kang, S. O.; Ko,
J.; Yum, J.-H.; Fantacci, S.; De Angellis, F.; Di Censo, D.; Nazeeruddin,
Synthesis of 3,30-Di-n-hexylsilylene-2,20-bithiophene-5-carbal-
dehyde (2). To a cold solution of 1 (1.46 g, 4.03 mmol) and N,N-
dimethylformide (0.35 g, 4.84 mmol) in 1,2-dichloroethane
(10 mL) at 0 °C was added phosphorus chloride oxide (0.74 g,
4.84 mmol). The reaction solution was heated to 80 °C, stirred
for 4 h, and then saturated sodium acetate aqueous solution
(20 mL) added. The mixture was further stirred at room
temperature for 30 min. The crude product was extracted into
dichloromethane, and the organic layer was washed with brine
and water, and dried over anhydrous sodium sulfate. After
removing solvent under reduced pressure, the residue was
purified by column chromatography (dichloromethane/petro-
leum ether 60-90 °C, 2/1, v/v) on silica gel to yield a colorless oil
€
M. K.; Gratzel, M. J. Am. Chem. Soc. 2006, 128, 16701. (j) Wang,
Z.-S.; Cui, Y.; Hara, K.; Dan-oh, Y.; Kasada, C.; Shinpo, A. Adv.
Mater. 2007, 19, 1138. (k) Edvinsson, T.; Li, C.; Pschirer, N.;
€
Schoneboom, J.; Eickemeyer, F.; Sens, R.; Boschloo, G.; Herrmann,
A.; M€ullen, K.; Hagfeldt, A. J. Phys. Chem. C 2007, 111, 15137. (l) Ito,
S.; Miura, H.; Uchida, S.; Takata, M.; Sumioka, K.; Liska, P.; Comte, P.;
ꢀ
€
Pechy, P.; Gratzel, M. Chem. Commun. 2008, 5194. (m) Thomas, K. R.
J.; Hsu, Y.-C.; Lin, J. T.; Lee, K.-M.; Ho, K.-C.; Lai, C.-H.; Cheng,
Y.-M.; Chou, P.-T. Chem. Mater. 2008, 20, 1830. (n) Zhou, G.;
1
(96% yield). H NMR (600 MHz, DMSO-d6) δ: 9.87 (s, 1H),
8.05 (s, 1H), 7.41 (d, J = 4.8 Hz, 1H), 7.12 (d, J = 4.8 Hz, 1H),
1.30 (m, 4H), 1.21 (m, 4H), 1.16 (m, 8H), 0.95 (t, J = 6.8 Hz,
4H), 0.78 (t, J = 6.8 Hz, 6H). 13C NMR (150 MHz, DMSO-d6)
δ: 183.73, 156.85, 146.86, 146.58, 144.06, 142.81, 141.18, 130.63,
€
Pschirer, N.; Schoneboom, J. C.; Eickemeyer, F.; Baumgarten, M.;
M€ullen, K. Chem. Mater. 2008, 20, 1808. (o) Wang, Z.-S.; Koumura,
N.; Cui, Y.; Takahashi, M.; Sekiguchi, H.; Mori, A.; Kubo, T.; Furube,
A.; Hara, K. Chem. Mater. 2008, 20, 3993. (p) Lin, J. T.; Chen, P.-C.;
Yen, Y.-S.; Hsu, Y.-C.; Chou, H.-H.; Yeh, M.-C. P. Org. Lett. 2009, 11,
97. (q) Tian, H.; Yang, X.; Cong, J.; Chen, R.; Liu, J.; Hao, Y.; Hagfeldt,
A.; Sun, L. Chem. Commun. 2009, 6288. (r) Tian, H.; Yang, X.; Chen,
R.; Hagfeldt, A.; Sun, L. Energy Environ. Sci. 2009, 2, 674. (s) Teng,
C.; Yang, X.; Yuan, C.; Li, C.; Chen, R.; Tian, H.; Li, S.; Hagfeldt, A.;
Sun, L. Org. Lett. 2009, 11, 5542. (t) Kumaresan, D.; Thummel, R. P.;
Bura, T.; Ulrich, G.; Ziessel, R. Chem.;Eur. J. 2009, 15, 6335.
(u) Wang, Z.-S.; Koumura, N.; Cui, Y.; Miyashita, M.; Mori, S.; Hara,
K. Chem. Mater. 2009, 21, 2810. (v) Song, J.; Zhang, F.; Li, C.; Liu,
W.; Li, B.; Huang, Y.; Bo, Z. J. Phys. Chem. C 2009, 113, 13391. (w)
(6) Wang, X.-F.; Kitao, O.; Zhou, H.; Tamiaki, H.; Sasaki, S.-i. J.
Phys. Chem. C 2009, 113, 7954.
(7) (a) Lu, G.; Usta, H.; Risko, C.; Wang, L.; Facchetti, A.; Ratner, M.
A.; Marks, T. J. J. Am. Chem. Soc. 2008, 130, 7670. (b) Hou, J. H.;
Chen, H.- Y.; Zhang, S. Q.; Li, G.; Yang, Y. J. Am. Chem. Soc. 2008,
130, 16144. (c) Beaujuge, P. M.; Pisula, W.; Tsao, H. N.; Ellinger, S.;
M€ullen, K.; Reynolds, J. R. J. Am. Chem. Soc. 2009, 131, 7514. (d)
Huo, L.; Chen, H.-Y.; Hou, J.; Chen, T. L.; Yang, Y. Chem. Commun.
2009, 5570.
ꢁ
Preat, J.; Michaux, C.; Jacquemin, D.; Perpete, E. A. J. Phys. Chem. C
2009, 113, 16821. (x) Li, Q.; Lu, L.; Zhong, C.; Shi, J.; Huang, Q.; Jin,
X.; Peng, T.; Qin, J.; Li, Z. J. Phys. Chem. B 2009, 113, 14588. (y) Liu,
B.; Zhu, W.; Zhang, Q.; Wu, W.; Xu, M.; Ning, Z.; Xie, Y.; Tian, H.
Chem. Commun. 2009, 1766 and references cited therein. (z) Mishra,
(8) Hiroko, Y.; Ikuyoshi, T.; Kazuchika, O.; Takeshi, E. Mol. Cryst.
Liq. Cryst. A 2001, 369, 47.
(9) Zhu, S. S.; Swager, T. M. J. Am. Chem. Soc. 1997, 119, 12568.
(10) Wang, P.; Wenger, B.; Humphry-Baker, R.; Moser, J.-E.; Teuscher,
J.; Kantlehner, W.; Mezger, J.; Stoyanov, E. V.; Zakeeruddin, S. M.;
€
A.; Fischer, M. K. R.; Bauerle, P. Angew. Chem., Int. Ed. 2009, 48,
€
Gratzel, M. J. Am. Chem. Soc. 2005, 127, 6850.
(11) Cao, Y.; Zhang, J.; Bai, Y.; Li, R.; Zakeeruddin, S. M.; Gratzel, M.;
2474 and references cited therein.
(5) (a) Ohshita, J. Macromol. Chem. Phys. 2009, 210, 1360. (b) Zhan, X.;
Barlow, S.; Marder, S. R. Chem. Commun. 2009, 1948.
€
Wang, P. J. Phys. Chem. C 2008, 112, 13775.

Article
Chem. Mater., Vol. 22, No. 5, 2010 1917
Scheme 1. Synthetic Route of the C219 Dyea
a Reagents: (i) POCl3, DMF, 1,2-dichloroethane; (ii) NBS, DMF; (iii) 4-bromoaniline, CuCl, 1,10-phenathroline, KOH, toluene; (iv) 2-(tributylstannyl)-
3,4-(ethylenedioxy)thiophene, Pd(PPh3)2Cl2, toluene; (v) n-BuLi, tributylstannyl chloride, THF; (vi) 3, Pd(PPh3)2Cl2, toluene; (vii) cyanoacetic acid,
piperidine, CHCl3.
130.24, 31.85, 30.70, 23.43, 21.84, 13.80, 10.91. MS (ESI) m/z
calcd for C21H30OS2Si: 390.15. Found: 391.20 ([MþH]þ). Anal.
Calcd for C21H30OS2Si: C, 64.56; H, 7.74. Found: C, 64.57; H,
7.71.
Synthesis of 4-(3,4-Ethylenedioxythiophene-5-yl)-N,N-bis-
(4-(2-ethylhexyloxy)phenyl)aniline (6). A mixture of 5 (9.60 g,
16.55 mmol), 2-(tributylstannyl)-3,4-(ethylenedioxy)thiophene
(10.70 g, 24.82 mmol), Pd(PPh3)2Cl2 (1.16 g, 1.65 mmol) and
150 mL of anhydrous toluene was refluxed for 16 h under argon.
The crude product was extracted into dichloromethane, and the
organic layer was washed with water and dried over anhydrous
sodium sulfate. After removing solvent under reduced pressure,
the residue was purified by column chromatography
(dichloromethane/petroleum ether 60-90 °C, 1/25, v/v) on silica
gel to yield a yellow oil (63% yield). 1H NMR (600 MHz,
DMSO-d6) δ: 7.44 (d, J = 8.8 Hz, 2H), 6.99 (d, J = 8.8 Hz,
4H), 6.90 (d, J = 8.8 Hz, 4H), 6.79 (d, J = 8.8 Hz, 2H), 6.48
(s, 1H), 4.26 (m, 2H), 4.24 (m, 2H), 3.82 (t, J = 6.0 Hz, 4H), 1.66
(m, 2H), 1.40 (m, 8H), 1.30 (m, 8H), 0.89 (m, 12H). 13C NMR
(150 MHz, DMSO-d6) δ: 155.16, 146.73, 141.90, 139.77, 137.05,
126.12, 126.04, 124.70, 119.63, 116.02, 115.32, 96.05, 70.31,
64.32, 63.86, 38.60, 29.76, 28.18, 23.18, 22.09, 13.44, 10.57.
MS (ESI) m/z calcd for C40H51NO4S: 641.35. Found: 642.35
([MþH]þ). Anal. Calcd for C40H51NO4S: C, 74.84; H, 8.01.
Found: C, 74.88; H, 8.04.
Synthesis of 50-Bromo-3,30-di-n-hexylsilylene-2,20-bithiophene-
5-carbaldehyde (3). To a cold solution of 2 (1.50 g, 3.84 mmol) in
N,N-dimethylformide (30 mL) was added N-bromosuccinimide
(0.77 g, 4.33 mmol) at 0 °C under argon. The reaction mixture
was warmed to room temperature, stirred for 4 h, and then water
(50 mL) added. The crude product was extracted into dichloro-
methane, and the organic layer was dried over anhydrous sodium
sulfate. After removing solvent under reduced pressure, the residue
was purified by column chromatography (dichloromethane/petro-
leum ether 60-90 °C, 2/1, v/v) on silica gel to yield a yellowish oil
(97% yield). 1H NMR (600 MHz, DMSO-d6) δ: 9.89 (s, 1H), 8.07
(s, 1H), 7.43 (s, 1H), 1.31 (m, 4H), 1.22 (m, 4H), 1.17 (m, 8H), 0.96
(t, J = 6.8 Hz, 4H), 0.79 (t, J = 6.8 Hz, 6H). 13C NMR (150 MHz,
DMSO-d6) δ: 183.90, 155.64, 147.41, 147.32, 144.54, 142.17, 140.95,
133.67, 114.74, 31.83, 30.65, 23.30, 21.85, 13.80, 10.73. MS (ESI) m/z
calcd for C21H29BrOS2Si: 468.06. Found: 469.10 ([MþH]þ). Anal.
Calcd for C21H29BrOS2Si: C, 53.71; H, 6.22. Found: C, 53.73;
H, 6.25.
Synthesis of 50-{2-{4-[N,N-Bis(4-(2-ethylhexyloxy)phenyl)-
amino]phenyl}-3,4-ethylenedioxythiophene-5-yl}-3,30-di-n-hexylsi-
lylene-2,20-bithiophene-5-carbaldehyde (8). Compound 6 (2.00 g,
3.11 mmol) dissolved in 15 mL of anhydrous THF was treated
dropwise with n-butyllithium (1.6 M, 2.13 mL, 3.42 mmol) at
-78 °C under argon. The solution was stirred at -78 °C for 1 h
and tributylstannyl chloride (1.32 g, 4.04 mmol) added. The
mixture was warmed to room temperature and stirred for 6 h.
The reaction was terminated by adding water and the mixture
was extracted with dichloromethane and dried over anhydrous
sodium sulfate. The solvent was evaporated to obtain the crude
7 as a brown oil and used in the further reaction. The 70% yield
Synthesis of 4-Bromo-N,N-bis((4-(2-ethyl)hexyloxy)phenyl)-
aniline (5). To a stirred solution of 4 (70.00 g, 210.70 mmol),
4-bromoaniline (14.50 g, 84.28 mmol), and 1,10-phenanthroline
(3.03 g, 16.85 mmol) in toluene (350 mL) at 100 °C were added
potassium hydroxide (37.83 g, 674.24 mmol) and cuprous
chloride (1.67 g, 16.85 mmol) under argon. The reaction mixture
was refluxed at 120 °C overnight and water (200 mL) added. The
crude product was extracted into dichloromethane, and the
organic layer was washed with water and dried over anhydrous
sodium sulfate. After removing solvent under reduced pressure,
the residue was purified by column chromatography (ethyl
acetate/petroleum ether 60-90 °C, 1/30, v/v) on silica gel to
yield a yellowish oil (58% yield). 1H NMR (600 MHz, DMSO-
d6) δ: 7.30 (d, J = 8.0 Hz, 2H), 7.01 (d, J = 8.0 Hz, 4H), 6.91 (d,
J = 8.0 Hz, 4H), 6.65 (d, J = 8.0 Hz, 2H), 3.82 (t, J = 4.0 Hz,
4H), 1.66 (m, 2H), 1.42 (m, 8H), 1.30 (m, 8H), 0.88 (m, 12H). 13C
NMR (150 MHz, DMSO-d6) δ: 155.65, 147.85, 139.46, 131.61,
126.83, 120.62, 115.53, 110.80, 70.08, 38.68, 29.90, 28.41, 23.28,
22.46, 13.09, 10.88. MS (ESI) m/z calcd for C34H46BrNO2:
579.27. Found: 580.25 ([MþH]þ). Anal. Calcd for
C34H46BrNO2: C, 70.33; H, 7.99; N, 2.41. Found: C, 70.32; H,
7.89; N, 2.40.
1
of 7 was roughly estimated according to H NMR data. To a
solution of 7 (1.01 g, 1.09 mmol) and 3 (0.87 g, 1.86 mmol) in
toluene (20 mL), Pd(PPh3)2Cl2 (0.13 g, 0.18 mmol) was added.
The mixture was refluxed at 110 °C for 14 h under argon. The
crude compound was extracted into ethyl acetate, washed with
brine and water, and dried over anhydrous sodium sulfate.
After removing solvent under reduced pressure, the residue
was purified by column chromatography (ethyl acetate/petro-
leum ether 60-90 °C, 1:10, v/v) on silica gel to yield a red powder
1
(96% yield). H NMR (600 MHz, DMSO-d6) δ: 9.86 (s, 1H),
7.99 (s, 1H), 7.49 (d, J = 8.4 Hz, 2H), 7.32 (s, 1H), 7.03

1918 Chem. Mater., Vol. 22, No. 5, 2010
Zeng et al.
(d, J = 9.0 Hz, 4H), 6.91 (d, J = 9.0 Hz, 4H), 6.81 (d, J = 8.4 Hz,
2H), 4.44 (m, 2H), 4.37 (m, 2H), 3.85 (t, J = 6.6 Hz, 4H), 1.69
(m, 2H), 1.42 (m, 8H), 1.33 (m, 12H), 1.24 (m, 4H), 1.19 (m, 8H),
0.99 (m, 4H), 0.91 (m, 12H), 0.81 (t, J = 6.6 Hz, 6H). 13C NMR
(150 MHz, DMSO-d6) δ: 182.82, 156.73, 155.39, 147.22, 144.30,
143.66, 142.02, 140.31, 139.50, 138.71, 138.43, 137.20, 126.35,
126.26, 124.97, 123.46, 119.13, 115.39, 114.97, 106.89, 70.34,
64.81, 64.34, 38.59, 31.43, 30.35, 29.74, 28.17, 23.17, 23.07,
22.06, 21.47, 13.42, 13.35, 10.70, 10.56. MS (ESI) m/z calcd
for C61H79NO5S3Si: 1029.49. Found: 1030.50 ([MþH]þ). Anal.
Calcd for C61H79NO5S3Si: C, 71.09; H, 7.73; N, 1.36. Found: C,
71.11; H, 7.75; N, 1.34.
a sand-blasting drill, was sealed with a Bynel sheet and a thin
glass cover by heating. Two electrolytes were used for device
evaluations. EL01: 1.0 M DMII, 50 mM LiI, 30 mM I2, 0.5 M
TBP, and 0.1 M GNCS in the 85/15 mixture of acetonitrile and
valeronitrile; EL02: DMII/EMII/EMITCB/I2/TBP/GNCS (molar
ratio: 12/12/16/1.67/3.33/0.67), where the iodide and triiodide
concentrations are 3.18 and 0.24 M, respectively.
2.3. Calculation. The ground-state geometry of C219 was
fully optimized by the density functional theory (DFT) method13
with Beck’s three-parameter functional and Lee-Yang-Parr
functional14 (B3LYP) and the 6-31G basis set was used for all
atoms.15 The electronic transitions were calculated by time-
dependent density functional theory (TDDFT) method16 based
on the optimized ground-state structure. All calculations were
performed with the Gaussian03 program package.
Synthesis of 2-Cyano-3-{50-{2-{4-[N,N-bis(4-(2-ethylhexyloxy)-
phenyl)amino]phenyl}-3,4-ethylenedioxythiophene-5-yl}-3,30-di-
n-hexylsilylene-2,20-bithiophene-5-yl}acrylic Acid (C219). To a
stirred solution of compound 8 (1.06 g, 1.03 mmol) and cya-
noacetic acid (0.26 g, 3.09 mmol) in chloroform (30 mL) was
added piperidine (0.61 g, 7.21 mmol). The reaction mixture was
refluxed under argon for 12 h and then acidified with 2 M
hydrochloric acid aqueous solution (40 mL). The crude product
was extracted into chloroform, washed with water, and dried
over anhydrous sodium sulfate. After removing solvent under
reduced pressure, the residue was purified by flash chromato-
graphy with chloroform and methanol/chloroform (1/10, v/v)
in turn as eluent to yield a purple powder (89%). 1H NMR
(600 MHz, DMSO-d6) δ: 13.49 (s, 1H), 8.45 (s, 1H), 8.00 (s, 1H),
7.48 (d, J = 8.8 Hz, 2H), 7.34 (s, 1H), 7.00 (d, J = 8.8 Hz, 4H),
6.90 (d, J = 8.8 Hz, 4H), 6.78 (d, J = 8.8 Hz, 2H), 4.44 (m, 2H),
4.37 (m, 2H), 3.82 (d, J = 5.2 Hz, 4H), 1.66 (m, 2H), 1.42
(m, 16H), 1.22 (m, 16H), 0.97 (m, 4H), 0.90 (m, 12H), 0.78 (t,
J = 6.4 Hz, 6H). 13C NMR (150 MHz, DMSO-d6) δ: 163.98,
158.37, 155.50, 147.92, 147.37, 146.56, 144.42, 143.20, 142.09,
139.53, 139.38, 139.16, 137.38, 136.38, 126.67, 126.48, 125.20,
123.44, 119.16, 117.01, 115.45, 107.06, 95.12, 70.08, 65.10, 64.57,
38.69, 31.86, 30.69, 29.90, 28.41, 23.37, 23.29, 22.45, 21.86,
13.87, 13.80, 10.87. ATR-FTIR: 1680 cm-1 (COOH), 2214
cm-1 (CN). MS (ESI) m/z calcd for C64H80N2O6S3Si: 1096.49.
Found: 1097.61 ([MþH]þ). Anal. Calcd for C64H80N2O6S3Si:
C, 70.03; H, 7.35; N, 2.55. Found: C, 70.02; H, 7.36; N, 2.54.
2.2. Device Fabrication. A screen-printed single or double
layer film of interconnected titania particles was used as the
negative electrode. A transparent layer of 20-nm-sized titania
particles was first printed on the fluorine-doped SnO2 (FTO,
Nippon Sheet Glass, Solar, 4 mm thick) conducting glass
electrode and further coated by a second layer of scattering
titania particles if needed. The film thickness was measured by a
benchtop Ambios XP-1 stylus profilometer. The detailed pre-
paration procedures of titania nanocrystals, pastes for screen-
printing, and nanostructured titania films have been reported in
a previous paper.12 A cycloidal titania electrode (∼0.28 cm2) was
stained by immersing it into a dye solution (150 μM C219 and
300 μM cheno in chlorobenzene, 3-4 h; 300 μM Z907 and
300 μM cheno in the 1:1 mixture of acetonitrile and tert-butanol,
overnight). After washing with acetonitrile and drying by air
flow, the dye-coated titania electrode was assembled with a
thermally platinized FTO (TEC 15 Ω/0, Libbey-Owens-Ford
Industries, 2.2 mm thick) electrode. The electrodes were sepa-
rated by a 30-μm-thick Bynel (DuPont) hot-melt gasket and
sealed up by heating. The internal space was filled with a liquid
electrolyte using a vacuum backfilling system. The electrolyte-
injecting hole on the counter electrode glass substrate made with
2.4. UV-Vis, Voltammetric, Photoluminescence, and Transi-
ent Absorption Measurements. Electronic absorption spectra
were recorded on a UNICO WFZ UV-2802PC/PCS spectro-
meter. A CHI660C electrochemical workstation was used for
square-wave voltammetric measurements in combination with a
mini three-electrode electrochemical cell equipped with a 5-μm-
radius Pt ultramicroelectrode as working electrode. A Pt wire
and a silver wire were used as counter and quasi-reference
electrodes, respectively. The redox potentials were calibrated
with ferrocene as the internal reference. Photoluminescence
spectra and decays were measured with a LifeSpec-II fluores-
cence spectrometer equipped with an EPL405 laser diode.
Transient absorption measurements were carried out with a
LP920 laser flash spectrometer in conjunction with a nanose-
cond tunable OPOLett-355II laser. The sample was kept at a 45°
angle to the excitation beam. The probe light from a pulsed
xenon arc lamp was passed through various optical elements,
samples, and a monochromator before being detected by a fast
photomultiplier tube and recorded with a TDS 3012C digital
signal analyzer.
2.5. Photovoltaic Measurements and Stability Tests. A Keithley
2400 source meter and a Zolix Omni-λ300 monochromator
equipped with a 500 W xenon lamp were used to measure
photocurrent action spectra, with a wavelength sampling inter-
val of 10 nm and a current sampling time of 2 s under the full
computer control. Monochromatic incident photon-to-col-
lected electron conversion efficiency (IPCE) is defined by IPCE-
(λ)=hcJsc/eφλ, where h is the Planck constant, c is the light speed
in vacuum, e is the electronic charge, λ is the wavelength, Jsc is
the short-circuit photocurrent density, and φ is the incident
radiative flux. A Hamamatsu S1337-1010BQ silicon diode used
for IPCE measurements was calibrated in National Institute of
Metrology, China. A model LS1000-4S-AM1.5G-1000W solar
simulator (Solar Light Company, USA) in combination with a
metal mesh was employed to give an irradiance of 100 mW
cm-2. The light intensity was tested with a PMA2144 pyrano-
meter and a calibrated PMA 2100 dose control system. J-V
characteristics were obtained by applying a bias potential to a
testing cell and measuring dark current and photocurrent with a
Keithley 2602 source meter under the full computer control. The
measurements were fully automated using Labview 8.0. A metal
mask with an aperture area of 0.158 cm2 was covered on a testing
(13) Runge, E.; Gross, E. K. U. Phys. Rev. Lett. 1984, 52, 997.
(14) (a) Becke, A. D. J. Chem. Phys. 1993, 98, 5648. (b) Lee, C.; Yang, W.;
Parr, R. G. Phys. Rev. B 1988, 37, 785.
(15) Hay, P. J.; Wadt, W. R. J. Chem. Phys. 1985, 82, 299.
(16) (a) Matsuzawa, N. N.; Ishitani, A. J. Phys. Chem. A 2001, 105,
4953. (b) Stratmann, R. E.; Scuseria, G. E. J. Chem. Phys. 1998, 109,
8218.
(12) Wang, P.; Zakeeruddin, S. M.; Comte, P.; Charvet, R.; Humphry-
€
Baker, R.; Gratzel, M. J. Phys. Chem. B 2003, 107, 14336.

Article
Chem. Mater., Vol. 22, No. 5, 2010 1919
Figure 2. (A) Electronic absorption spectra of Z907 and C219 in DMF and photoluminescence spectrum of C219 in DMF obtained with a laser excitation
at 405 nm. (B) Absorption spectra of Z907 and C219 anchored on a 2.4 μm thick mesoporous titania film.
cell during all measurements. An antireflection film (λ < 380 nm,
ARKTOP, ASAHI Glass) is adhered to the DSC photoanode
during IPCE and J-V measurements. A homemade hea-
ting-cooling system was used for temperature-dependent ex-
periments. Solar cells covered with a 50 μm thick of polyester
film (Preservation Equipment Ltd., UK) as a 400 nm UV cutoff
filter were irradiated at open circuit under a Suntest CPS plus
lamp (ATLAS GmbH, 100 mW cm-2) in ambient air at 60 °C.
J-V measurements were carried out at room temperature after
allowing the cells to cool down and equilibrate for 30 min.
2.6. Electrical Impedance Measurements. Electrical impe-
dance experiments were carried out in the dark with an IM6ex
electrochemical workstation, with a frequency range from 50
dye-sensitized solar cells away from irradiation of UV
photons, assuring a long haul device operation. This
consideration is based on our observation on an evident
deterioration of cell efficiencies if UV light is not filtered.
We deduce that this should be ascribed to structural
modifications of dye molecules, which are probably
attacked by high-energy holes in the photoexcited titania
nanocrystals. In this regard, an antireflection film can be
coated onto DSCs, filtering UV photons and reducing the
reflection of visible photons simultaneously. Therefore,
in DSCs, the sensitizer normally functions as the only
light-absorption component making a contribution to the
subsequent charge generation.
mHz to 100 kHz and
a
potential modulation of
10 mV. The obtained impedance spectra were fitted with the
Z-view software (v2.80, Scribner Associates Inc.) in terms of
appropriate equivalent circuits. A homemade heating-cooling
system was used for temperature-dependent measurements.
2.7. Transient Photoelectrical Measurements. In transient
photoelectrical decay experiments, a steady light was supplied
with a white light-emitting diode (LED) array while a perturbing
light pulse was provided with a red LED array controlled by a
fast solid-state switch. Both white and red lights were irradiated
on the photoanode side of a testing cell. The red pulse was
carefully controlled by the driving potential of diodes to keep the
modulated photovoltage below 5 mV. We used red light as a
probe to generate a photovoltage perturbation near the open-
circuit photovoltage (Voc) of the cell under the white light and
measured the voltage decay process thereafter. Normally, the
transient signals follow a single exponential decay, therefore the
recombination rate constant, kr, can be extracted from the slope
of the semilogarithmic plot. The capacitance (Cμ) of the titania
interface at the Voc is calculated by Cμ = ΔQ/ΔV, where ΔV is
the peak of the photovoltage transient and ΔQ is the number of
electron injected during the red light flash. The latter is obtained
by integrating a short-circuit photocurrent transient generated
from an identical red pulse. The electron density (de) in the
titania film under a given white light intensity was determined by
charge extraction technique. A homemade heating-cooling
system was used for temperature-dependent measurements.
Therefore, we first measured the electronic absorption
spectrum of C219 dissolved in DMF to have a prelimin-
ary evaluation on its light-harvesting capacity, in com-
parison with the standard amphiphilic ruthenium dye
Z907. As presented in Figure 2A, the molar extinction
coefficient (ε) of 57.5 ꢀ 103 M-1 cm-1 at 493 nm
measured for C219 is over four times higher than that
of 12.2 ꢀ 103 M-1 cm-1 at 521 nm for Z907. In view of the
strong influence of solvent polarities on charge-transfer
transitions of organic push-pull chromophores,18 we
further measured the absorption of C219 in chloroform
to have a systematic comparison with other metal-free
photosensitizers reported in our previous work19 and the
details are collected in Table S1 of the Supporting In-
formation. Among these dyes, the low-energy electronic
transition of C219 arises at the longest wavelength of 584
nm, demonstrating a sound advancement in terms of
enhancing the near-infrared light-harvesting. More im-
portantly, C219 bestows significantly improved light
(18) Meier, H. Angew. Chem., Int. Ed. 2005, 44, 2482.
(19) (a) Wang, M.; Xu, M.; Shi, D.; Li, R.; Gao, F.; Zhang, G.; Yi, Z.;
€
Humphry-Baker, R.; Wang, P.; Zakeeruddin, S. M.; Gratzel, M.
Adv. Mater. 2008, 20, 4460. (b) Qin, H.; Wenger, S.; Xu, M.; Gao, F.;
€
Jing, X.; Wang, P.; Zakeeruddin, S. M.; Gratzel, M. J. Am. Chem. Soc.
2008, 130, 9202. (c) Shi, D.; Pootrakuchote, N.; Yi, Z.; Xu, M.;
Zakeeruddin, S. M.; Gr€atzel, M.; Wang, P. J. Phys. Chem. C 2008,
112, 17478. (d) Xu, M.; Li, R.; Pootrakulchote, N.; Shi, D.; Guo, J.; Yi,
Z.; Zakeeruddin, S. M.; Gratzel, M.; Wang, P. J. Phys. Chem. C 2008,
112, 19770. (e) Xu, M.; Wenger, S.; Bara, H.; Shi, D.; Li, R.; Zhou, Y.;
3. Results and Discussion
€
3.1. Electronic Absorption and Energy Level. Distinct
from photocatalytic degradation of organic pollutants
realized by a direct band excitation of titania nano-
crystals with high-energy photons,17 it is pertinent to keep
€
Zakeeruddin, S. M.; Gratzel, M.; Wang, P. J. Phys. Chem. C 2009, 113,
2966. (f) Li, R.; Lv, X.; Shi, D.; Zhou, D.; Cheng, X.; Zhang, G.; Wang,
P. J. Phys. Chem. C 2009, 113, 7469. (g) Zhang, G.; Bai, Y.; Li, R.; Shi,
€
D.; Wenger, S.; Zakeeruddin, S. M.; Gratzel, M.; Wang, P. Energy
Environ. Sci. 2009, 2, 92. (h) Zhang, G.; Bala, H.; Cheng, Y.; Shi, D.;
Lv, X.; Yu, Q.; Wang, P. Chem. Commun. 2009, 2198.
(17) Legrini, O.; Oliveros, E.; Braun, A. M. Chem. Rev. 1993, 93, 671.

1920 Chem. Mater., Vol. 22, No. 5, 2010
Zeng et al.
Figure 3. Contour representations of (A) LUMO, (B) HOMO, and (C) HOMO-1 of C219. All the iodensity surface values are fixed at 0.04.
absorption coefficients (Figure 2B) upon a titania film in
contrast to Z907, ensuring a good light absorption even if
a thin active layer must be used for efficient device
operation.19a On the other hand, a reduction in film
thickness can improve the open-circuit photovoltage,
benefiting from an uplifted electron-Fermi level of a
titania negative electrode because of the intensified elec-
tron density under a given light intensity.
electron-withdrawing cyanoacrylic acid fragment. More-
over, both HOMO and LUMO exhibit overlapping ex-
tension to the EDOT and DST spacers, enhancing the
electronic coupling parallel to the electronic transition
dipole moment between the two states, which in turn
augments the oscillator strength between these two elec-
tronic states.
The DMF solution of C219 has a strong red emission
centered at 688 nm, featuring a single exponential lifetime
of 1.23 ns derived from our picosecond time-correlated
single photon counting (TCSPC) measurements. The
excitation transition energy (E0-0) was roughly estimated
to be 2.19 eV from the intersection of absorption and
photoluminescence spectra. The redox potentials of Z907
and C219 in DMF were accurately measured by employ-
ing the ultramicroelectrode technique in conjunction with
square-wave voltammetry. The HOMO and LUMO va-
lues versus vacuum were transformed via the equation
The electronic absorption origins are scrutinized by
calculating the singlet electronic transitions with the
TDDFT method in Gaussian03W program suite. Calcu-
lation results show that the visible absorption of C219
stems from the π f π* transitions mostly from HOMO to
LUMO and subsidiarily from HOMO-1 to LUMO. The
isodensity surface plots of HOMO, HOMO-1, and
LUMO are presented in Figure 3. HOMO of C219 is
populated over the triphenylamine, EDOT, and DTS
blocks with considerable contribution from the former,
whereas LUMO is delocalized through the EDOT, DTS,
and cyanoacrylic acid fragments with sizable contribu-
tion from the latter. This spatially directed separation of
HOMO and LUMO is an ideal condition for dye-sensi-
tized solar cells, which not only facilitates ultrafast inter-
facial electron injection from excited dyes to titania but
also slows down recombination of injected electrons with
oxidized dye cations because of their remoteness. In
addition, the hole localization on the triphenylamine
fragment facilitates the electron donor to approach,
promoting the fast dye regeneration. It is valuable to note
that the σ*-π*-interactions typically observed for the
small silole structures5 are actually not inspected for the
LUMO of C219, likely because of the energetic stabiliza-
tion of carbon-backbone-based π*-orbital by the strong
E
LUMO/HOMO= -e(4.88þVredox),20 where Vredox is the
onset potential versus ferrocene of reduction or oxidiza-
tion of sensitizers. The energy offsets of LUMOs (-3.35
eV for Z907; -3.47 eV for C219) of dye molecules with
respect to the titania conduction band edge (-4.00 eV)21
provide thermodynamic driving forces for charge genera-
tion. The energy offsets of HOMOs (-4.99 eV for Z907;
-4.96 eV for C219) relative to that (-4.60 eV)19g of iodide
supply negative Gibbs energy changes for dye regenera-
tion reaction. Through a systematic comparison on elec-
trochemical data (see Table S1 in the Supporting
(20) Yan, Q.; Zhou, Y.; Ni, B.; Ma, Y.; Wang, J.; Pei, J.; Cao, Y. J. Org.
Chem. 2008, 73, 5328.
€
€
(21) (a) Hagfeldf, A.; Gratzel, M. Chem. Rev. 1995, 95, 49. (b) Gratzel, M.
Nature 2001, 414, 338.

Article
Chem. Mater., Vol. 22, No. 5, 2010 1921
Figure 4. (A) Transient absorption changes recorded at 210 ns upon nanosecond pulsed laser excitation of dye-coated titania films immersed in EL01.
(B) Absorption changes after applying a small positive bias to dye-coated titania films immersed in EMITFSI. (C) Time-resolved absorption traces of dye-
coated titania films in the 85/15 mixed solvent of acetonitrile (AN) and valeronitrile (VN) and in EL01. Smooth solid lines are single exponential fits of
experimental data. Absorbance changes were measured at a probe wavelength of 782 nm upon 540 nm (for Z907) or 606 nm (for C219) pulsed laser
excitation (7 ns full width half-maximum pulse duration, 2 Hz repetition rate, 1.35 ꢀ 1014 photons cm-2 pulse fluence). Signals shown were obtained by
averaging over 1600 laser shots.
Information) of all organic dyes reported by our group so
far, it is clear that the C219 dye has a relative small
HOMO/LUMO gap of 1.49 eV, generally consistent with
its low-energy absorption peak. The influence of π-con-
jugation spacer on HOMOs and LUMOs of chromo-
phores can also be easily perceived from Table S1 in the
Supporting Information.
absorption spectra to the electronic absorptions of oxi-
dized dye cations. Note that the concomitant electrons in
titania exhibit relatively weak absorptions throughout
this spectral region (ε780 = 3400 M-1 cm-1).22
On the basis of transient absorption measurements, we
selected a 780 nm monochromatic light to probe the
kinetics of charge recombination of trapped electrons in
titania with oxidized dye cations, and that of interception
of oxidized dye cations by iodide ions (electron donor),
i.e., dye regeneration. To a large extent the kinetic com-
petition between these two charge-transfer channels are
widely believed to determine IPCEs of DSCs, along with
the yields of light absorption, electron injection, and
charge collection.23 The excitation wavelength and flu-
ence were carefully controlled in our kinetic measure-
ments to ensure that ∼1.35 ꢀ 1014 photons cm-2 was
absorbed by dye-coated films during every laser pulse,
which is close to the light intensity of device operation.
Because no electron donor is existent in the 85/15 mixture
3.2. Transient Absorption Spectra and Charge-Transfer
Kinetics. A 2.5 μm thick dye-coated transparent titania
film on glass slide was employed to make a dummy cell in
combination with an acetonitrile electrolyte EL01 for
transient absorption spectra measurements. The absorp-
tion changes in the spectral range from 530 to 830 nm
(Figure 4A) were recorded at 210 ns using a white probe
light, upon nanosecond pulsed laser excitation. We assign
these long-lived negative signals to the bleaching of
ground-state dye molecules. In consideration of less than
30 ns photoluminescence traces of dye-coated zirconia
films, we rule out any contribution from dye emission to
the positive signals. At the titania/dye interface, an ultra-
fast charge generation from organic excitons ejects elec-
trons into titania nanocrystals and leaves holes on dye
molecules, producing oxidized dye cations. With the aid
of spectroelectrochemical measurements (Figure 4B) on
dye-coated film immersed in 1-ethyl-3-methylimidazo-
lium bis(trifluoromethanesulfonyl)imide (EMITFSI),
we could ascribe the positive changes in the transient
€
(22) Rothenburger, G.; Fitzmaurice, D.; Gratzel, M. J. Phys. Chem.
1992, 96, 5983.
(23) (a) Tachibana, Y.; Moser, J. E.; Gratzel, M.; Klug, D. R.; Durrant,
€
J. R. J. Phys. Chem. 1996, 100, 20056. (b) Haque, S. A.; Tachibana, Y.;
€
Willis, R. L.; Moser, J. E.; Gratzel, M.; Klug, D. R.; Durrant, J. R. J.
€
Phys. Chem. B 2000, 104, 538. (c) Pelet, S.; Moser, J. E.; Gratzel, M. J.
Phys. Chem. B 2000, 104, 1791. (d) Wang, P.; Klein, C.; Moser, J.-E.;
Humphry-Baker, R.; Cevey-Ha, N.-L.; Charvet, R.; Comte, P.;
€
Zakeeruddin, S. M.; Gratzel, M. J. Phys. Chem. B 2004, 108, 17553.

1922 Chem. Mater., Vol. 22, No. 5, 2010
Zeng et al.
Figure 5. (A) Photocurrent action spectra of cells made from Z907 and C219 in combination with an acetonitrile based electrolyte EL01. (B) J-V
characteristics of cells measured under irradiation of 100 mW cm-2 AM1.5G sunlight. An antireflection film was adhered to cells during measurements.
EL01 is composed of 1.0 M DMII, 50 mM LiI, 30 mM I2, 0.5 M TBY, and 0.1 M GNCS in the 85/15 mixture of acetonitrile and valeronitrile.
Table 1. Detailed Photovoltaic Parametersa of DSCs with Z907 and C219
Using a Solvent-Free Ionic Liquid Electrolyte
of acetonitrile and valeronitrile, the absorption decays
reflect the kinetics of recombination of injected electrons
dye
Pin (mW cm-2
)
Jsc (mA cm-2
)
Voc (mV)
FF
η (%)
with oxidized dye cations. The absorption traces in
Figure 4C can be well-fitted by a single exponential decay
function, with a lifetime (τb) of 194 μs for Z907 cations
and 994 μs for C219 cations. When the dye-coated titania
films are submerged in EL01 with a high concentration of
iodide ions, the decays (Figure 4C) are significantly
accelerated, characteristic of a single exponential lifetime
(τr) of 2.3 μs for Z907 cations and that of 27.1 μs for C219
cations. Even if the rate constants of both back-electron
transfer and dye-regeneration are dissimilar in the cases
of Z907 and C219, the τb/τr branching ratios of over 35 for
both dyes imply that at least 97% of oxidized dye cations
are intercepted by electron donation from iodide, result-
ing in very efficient dye-regeneration and therefore high-
yield net charge separation.
Z907
14.39
26.14
53.26
100
14.39
26.14
53.26
100
2.13
3.80
7.50
13.34
2.52
4.47
8.65
14.96
660.1
678.0
698.8
713.0
641.3
659.1
677.5
693.0
0.796
0.784
0.769
0.752
0.791
0.783
0.762
0.736
7.8
7.7
7.6
7.2
8.9
8.8
8.4
7.6
C219
a The spectral distribution of our light resource simulates AM 1.5G
solar emission with a mismatch less than 5%. Lights at different
intensities were obtained by attenuating the AM1.5G full sunlight with
a set of neutral meshes. Incident power intensity, Pin; short-circuit
photocurrent density, Jsc; open-circuit photovoltage, Voc; fill factor,
FF; total power conversion efficiency, η. Cell area tested with a metal
mask: 0.158 cm2. An antireflection film was adhered to testing cells
during measurements. The composition of solvent-free ionic liquid
electrolyte EL02 is as follows: DMII/EMII/EMITCB/I2/TBP/GNCS
(molar ratio: 12/12/16/1.67/3.33/0.67).
3.3. Photovoltaic Performance. Our previous work24
has shown that both thickness and architecture of titania
films have significant influences on efficiencies of DSCs
fabricated from EL01 and Z907, owing to fairly low light
absorption coefficients of this dye in the whole visible and
near-infrared region. However in combination with a
state of the art double-layer titania film, 9.0-9.5%
efficiencies can be indeed attained with Z907 by using
an acetonitrile based electrolyte.10,24 Considerable effi-
ciency superiorities of C219 with respect to Z907 were
observed in our prior experiments using a thin transpar-
ent titania film. However, in this paper, we will utilize a
double-layer film (7 þ 5) with a 7 μm thick nanoporous
layer and a 5-μm-thick scattering layer for comparisons,
having an impartial evaluation on the status of metal-free
organic photosensitizers relative to the standard amphi-
philic ruthenium dye Z907, which has already been
applied in the first commercial product of DSCs.25
As depicted in Figure 5A, IPCE maxima of both dyes
are close to 95% after coating our cells with an antire-
flection film. If the light loss caused by reflection of
smooth glass was not attenuated, ∼4% lower IPCEs were
observed in our measurements on thousands of cells.
Notably, the photocurrent action spectrum of C219
departures evidently from the thin-film absorption spec-
trum (see Figure S3 of the Supporting Information),
featuring a broad plateau from 500 to 590 nm because
of close to unity light-harvesting by the double-layer cell
architecture in this spectral region. It is valuable to note
that the infrared IPCEs of C219 are still low in compar-
ison with that of Z907, highlighting the future necessary
efforts on narrowing the energy gap of metal-free organic
dyes. J-V characteristics were further measured under
irradiation of AM1.5G full sunlight and presented in
Figure 5B. The short-circuit photocurrent density (Jsc),
open-circuit photovoltage (Voc), and fill factor (FF) of a
cell made from Z907 are 16.84 mA cm-2, 773 mV, and
0.715, respectively, yielding an overall conversion effi-
ciency (η) of 9.3%, well-consistent with previously re-
ported data.10,24 In contrast, photovoltaic parameters
(Jsc, Voc, FF, and η) of the C219 cell are 17.94 mA
cm-2, 770 mV, 0.730, and 10.1%. Two batches of 10 cells
show an efficiency range from 10.0 to 10.3%. The im-
proved photocurrent of C219 relative to Z907 is in good
accord with the preceding IPCE measurements. This is
the first time greater than 10% efficiency has been
reached by dye-sensitized solar cells with a nonruthen-
ium photosensitizer.4,19 We remark that under the same
(24) Cao, Y.; Bai, Y.; Yu, Q.; Cheng, Y.; Liu, S.; Shi, D.; Gao, F.; Wang,
P. J. Phys. Chem. C 2009, 113, 6290.
(25) http://www.g24i.com.

Article
Chem. Mater., Vol. 22, No. 5, 2010 1923
Figure 6. (A) Photocurrent action spectra of cells made from Z907 and C219 in combination with a solvent-free ionic liquid electrolyte EL02. (B) J-V
characteristics ofcellsmeasured underirradiation of100mWcm-2 AM1.5Gsunlight. Anantireflectionfilm wasadheredtocellsduringmeasurements. The
composition of solvent-free ionic liquid electrolyte EL02 is as follows: DMII/EMII/EMITCB/I2/TBP/GNCS (molar ratio: 12/12/16/1.67/3.33/0.67).
Figure 7. Temperature-dependent photovoltaic parameters of a DSC made with C219 in combination with a solvent-free ionic liquid electrolyte EL02.
conditions, a reference cell with a new generation high-
absorption ruthenium dye C106 shows an efficiency of
11.3%,24 still leaving the performance of organic dyes
behind. Photovoltaic data on all other metal-free organic
dyes19 reported by our group are also collected in Table
S1 in the Supporting Information for a preliminary
understanding. Note that these comparisons must be
taken very carefully because several solvents for the dye
bath and different cheno concentrations, staining time,
washing solvents, and even the base tetra-n-butyl-
amonium hydroxide have been applied in our device
fabrication, which have a significant influence on cell
parameters. Unfortunately, we do not find a very good
rationale during optimization of dye staining, which
should be closely related to the dye-uploaded amount
and perhaps dye-anchoring mode. We think that the
latter could have a strong impact on multichannel
charge transfer kinetics. The complicated interfacial
chemistry and intrinsic physics behind these need to
be fully addressed in some further joint studies with
advanced scanning probe microscopic, computational,
photophysical, and optoelectronic methods. Whatever,
widening the spectral response of DSCs is the first critical
step to significantly improve cell performance close to the
challenging 15% efficiency, because presently the main
limiting factor on the inferior efficiency of DSCs with
respect to crystalline solar cells is a much lower photo-
current owing to an insufficient light-harvesting of photo-
sensitizers.
We believe that a substantial improvement in device
efficiency is still desirable to lower the cost per kilowatt-
hour of energy supply with dye-sensitized solar panels in
the near future. Nevertheless, stable, low-cost, flexible,
and lightweight DSCs based on a plastic matrix are
attractive, even if their efficiencies are moderate, i.e., in
the 5-10% range. However, for these devices, the use of
organic solvents is likely prohibitive as they would perme-
ate across the polymeric cell walls. Thus we also studied
the performance of C219 and Z907 in conjunction with
a solvent-free ionic liquid electrolyte (see Figure 6). In
contrast to the acetonitrile cells, a slight decrease in IPCE
maxima (∼90%) was noted for the ionic liquid cells, apart
from a clear diminishment in the blue region due to a high
concentration of triiodide in our ionic liquid electrolyte

1924 Chem. Mater., Vol. 22, No. 5, 2010
Zeng et al.
EL02. Note that the light absorption by triiodide does not
contribute to photocurrents in DSCs. Moreover, in any
part of the whole spectrum the Z907 cell with EL02 does
not exhibit higher IPCEs anymore than the C219 cell.
This was further rationalized by the electronic absorption
measurements of dummy cells. As shown in Figure S3
of the Supporting Information, the C219-coated film
immersed in EL02 can harvest more low-energy photons
than that in EL01, probably because of the sensitive
response of C219 to the dielectric change of these two
electrolytes. Photovoltaic parameters (Jsc, Voc, FF, and η)
of the C219 cell with a solvent-free ionic liquid electrol-
yte under the AM 1.5G full sunlight (100 mW cm-2) are
14.96 mA cm-2, 693 mV, 0.736, and 7.6%, respectively. In
contrast, the Z907 cell has an efficiency of 7.2% at the
same condition. At low light intensities of 14.39 mW cm-2
and 26.14 mW cm-2 attenuated by a set of metal meshes,
very impressive efficiency of 8.9% and 8.8% has been
reached with C219. This is very favorable for the practical
indoor application of flexible devices, which are fre-
quently operated under reduced light intensities and for
which ionic liquids are the electrolytes of choice.26 We
have noted that the measured photocurrent densities
under the full sunlight for both cells are significantly
lower than the overlap integral currents of the IPCE
curves with the standard AM1.5G solar emission spec-
trum. As listed in Table 1, there is a clear nonlinear
dependence of short-circuit photocurrent on light inten-
sity, implying that photocurrents of our ionic liquid cells
with Z907 and C219 could be limited by the slow trans-
port of redox mediators in this viscous electrolyte. More-
over, a solvent-free DSC with C219 as sensitizer exhibits
an excellent stability (Figure S4 of the Supporting In-
formation), keeping more than 93% of its initial effi-
ciency after 1000 h of aging under the full sunlight soaking
at 60 °C.
For the outdoor application of dye-sensitized solar
cells, the cell may operate at various temperatures. There-
by, we also measured J-V characteristics of a solvent-free
ionic liquid cell made from C219 at various temperatures.
As presented in Figure 7A, the short-circuit photo-
current augments with temperature from 10 to 45 °C
but saturates upon a further temperature improvement.
Our electrical impedance measurements27 have shown
that the electron diffusion length (Ln) is shortened at
a high temperature (Figure 8A), indicating that the
increase of photocurrent with temperature is probably
not related to a better charge collection yield. In addition,
we did not observe a light-harvesting enhancement for
cells at a high temperature. At the moment, we could not
rule out whether the temperature-dependent photocur-
rent tendency is also related to the net charge generation
yield, which needs to be addressed in our future studies.
Figure 8. Temperature-dependent (A) electron diffusion length versus
density of states (DOS) measured with electrical impedance spectroscopy,
(B) chemical capacitance, and (C) charge recombination constant derived
from measurements on transient photovoltage and photocurrent decays.
As the viscosity of EL02 becomes low with temperature,
the dependence of photocurrent on temperature could be
ascribed to the limit of electrolyte transport at low
temperatures. Furthermore, poor fill factors were ob-
served at 10 and 15 °C because of the relatively large cell
serial resistances, including electrolyte diffusion resis-
tances, charge-transfer resistances on the counter elec-
trode, and electron transport resistances in the
semiconducting titania film. The overall power conver-
sion efficiencies at temperatures from 10 to 55 °C are over
7%, with a maximum of 8.0% at 35 °C due to a trade-off
among Jsc, FF, and Voc.
To comprehend the adverse effect of raising tempera-
ture on cell photovoltage, we resorted to the transient
photoelectrical decay technique28 to measure interfacial
chemical capacitance (Cμ) and charge recombination
kinetics. As presented in Figure 8B, at a set of tempera-
tures the capacitance closely related to surface states
(26) Shi, D.; Pootrakuchote, N.; Li, R.; Guo, J.; Wang, Y.; Zakeeruddin,
€
S. M.; Gratzel, M.; Wang, P. J. Phys. Chem. C 2008, 112,
17046.
(27) (a) Bisquert, J. J. Phys. Chem. B 2002, 106, 325. (b) Bisquert, J. Phys.
Chem. Chem. Phys. 2003, 5, 5360. (c) Bisquert, J. Phys. Chem. Chem.
Phys. 2008, 10, 49.

Article
Chem. Mater., Vol. 22, No. 5, 2010 1925
under the conduction band edge of titania increases
exponentially with the enlargement of Voc, which was
generated by applying a gradually enhanced white light
intensity. At a given Voc, the apparently higher Cμ at a
higher temperature could be attributed to more deep
surface states because the calculated equilibrium poten-
tial of EL02 at 55 °C has a less than 10 mV negative shift
relative to that at 10 °C. As shown in Figure 8C, at a given
electron density (de) the charge recombination rate (kr)
becomes fast with temperature, which could be mainly
caused by the enhanced diffusion coefficients of triiodide
anions and electrons in the titania film, implying a
bimolecular interfacial recombination process. It is likely
that at a high temperature, deep electron-traps and fast
interfacial charge recombination kinetics together lead to
a decreased open-circuit photovoltage.
nonruthenium dyestuffs. This achievement should con-
siderably stimulate further efforts on energy-level engi-
neering of organic chromophores, catching up with the
high performance of ruthenium dyes. More importantly,
a solvent-free ionic liquid cell based on this new dye has
achieved a high efficiency of 8.9% under a low light
intensity of 14.39 mW cm-2, making it very promising
for the practical indoor application of flexible dye-sensi-
tized solar cells. We are now systematically optimizing
electrolyte compositions and device architectures to ex-
plore the full potential of this encouraging organic sensi-
tizer. Systematic studies on the intrinsic role of conjugated
spacers on multichannel charge transfer kinetics and sur-
face states of titania nanocrystals are needed to shed light
on the structure-activity relationship for the future de-
velopment of more efficient photosensitizers.
4. Conclusions
Acknowledgment. The National Key Scientific Program
(2007CB936700), the National Science Foundation of China
(50973105 and 50773078), the CAS Knowledge Innovation
Program (KGCX2-YW-326), and the CAS Hundred Talents
Program are acknowledged for financial support. M.Z.
thanks the State Key Laboratory of Theoretical and Com-
putational Chemistry, Jilin University for the computational
resources. We are grateful to Dyesol for supplying the
scattering paste and EMITCB, and to DuPont Packaging
and Industrial Polymers for supplying the Bynel film.
To summarize, we have prepared a high molar absorp-
tion coefficient organic push-pull dye featuring a binary
conjugated spacer of ethylenedioxythiophene and dithie-
nosilole, apart from the blocks of a lipophilic alkoxy-
substituted triphenylamine and a hydrophilic cya-
noacrylic acid. On the basis of this amphiphilic photo-
sensitizer and a volatile electrolyte, we have set a new
benchmark of 10.0-10.3% efficiency measured at the
AM1.5G conditions for dye-sensitized solar cells with
Note Added after ASAP Publication. There was an error in
Figure 4C in the version published ASAP January 22, 2010; the
corrected version was published ASAP January 26, 2010.
(28) (a) O’Regan, B. C.; Lenzmann, F. J. Phys. Chem. B 2004, 108, 4342.
(b) O'Regan, B. C.; Scully, S.; Mayer, A. C.; Palomares, E.; Durrant, J.
J. Phys. Chem. B 2005, 109, 4616. (c) O'Regan, B. C.; Durrant, J. R.
J. Phys. Chem. B 2006, 110, 8544. (d) Bailes, M.; Cameron, P. J.;
Lobato, K.; Peter, L. M. J. Phys. Chem. B 2005, 109, 15429.
(e) Kopidakis, N.; Neale, N. R.; Frank, A. J. J. Phys. Chem. B 2006,
110, 12485. (f) Walker, A. B.; Peter, L. M.; Lobato, K.; Cameron, P. J.
J. Phys. Chem. B 2006, 110, 25504. (g) Quintana, M.; Edvinsson, T.;
Hagfeldt, A.; Boschloo, G. J. Phys. Chem. C 2007, 111, 1035.
Supporting Information Available: ATR-FTIR spectrum,
square-wave voltammogram, additional spectral, and photo-
voltaic data (PDF). This material is available free of charge via
the Internet at http://pubs.acs.org.