Intelligent Materials for Solar CellsView this Special Issue
Substitution of Carbazole Modified Fluorenes as π-Extension in Ru(II) Complex-Influence on Performance of Dye-Sensitized Solar Cells
A new high molar extinction coefficient ruthenium(II) bipyridyl complex “cis-Ru(4,-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,-bipyridine)(2,-bipyridine-4,-dicarboxylic acid)(NCS)2, BPFC” has been synthesized and characterized by FT-IR, -NMR, and ESI-MASS spectroscopes. The sensitizer showed molar extinction coefficient of M−1cm−1, larger as compared to the reference N719, which showed M−1cm−1. The test cells fabricated using BPFC sensitizer employing high performance volatile electrolyte, (E01) containing 0.05 M I2, 0.1 M LiI, 0.6 M 1,2-dimethyl-3-n-propylimidazolium iodide, 0.5 M 4-tert-butylpyridine in acetonitrile solvent, exhibited solar-to-electric energy conversion efficiency (η) of 4.65% (short-circuit current density () = 11.52 mA/cm2, open-circuit voltage () = 566 mV, fill factor = 0.72) under Air Mass 1.5 sunlight, lower as compared to the reference N719 sensitized solar cell, fabricated under similar conditions, which exhibited η-value of 6.5% ( = 14.3 mA/cm2, = 640 mV, fill factor = 0.71). UV-Vis measurements conducted on TiO2 films showed decreased film absorption ratios for BPFC as compared to those of reference N719. Staining TiO2 electrodes immediately after sonication of dye solutions enhanced film absorption ratios of BPFC relative to those of N719. Time-dependent density functional theory (TD-DFT) calculations show higher oscillation strengths for 4,-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,-bipyridine relative to 2,-bipyridine-4,-dicarboxylic acid and increased spectral response for the corresponding BPFC complex.
Dye sensitized solar cells (DSSCs) attracted intense attention among scientific as well as industrial organizations because of their high photon-to-electricity conversion efficiency and low cost compared to traditional photoelectrochemical cells [1–5]. Since Graetzel introduced the first highly efficient nanocrystalline TiO2 sensitized solar cell based on ruthenium(II) bipyridyl complex, N3 as sensitizer, there have been several modifications to improve the overall performance of the test cell devices [6–22]. Among all the components employed in DSSC, sensitizer plays a key role in photovoltaic performance in respect of efficiency and long-term durability. The important tunable properties of sensitizers for high efficient DSSCs are broad absorption (400 to 900 nm) and high molar extinction coefficient (thin films and solid state DSSCs), thermal and photochemical stability (long durable), compatibility with TiO2 semiconductor conduction band (efficient electron injection) and redox electrolyte (efficient dye regeneration), nonplanar molecular structure, and so forth [6, 8, 22–24]. Thiophene containing oligomers have been extensively explored as the active organic materials for OFET applications due to the ease in chemical modification of the structures, allowing fine-tuning their optical and electronic properties . They exhibit high field-effect mobility, which have been related to both, the close packing through π-interactions and the high degree of local order of molecules . Thiphene oligomers display poor stability especially in the solid state, limiting their practical applications, where as fluorine-based oligomers showed both improved stability and lower HOMO level as compared to thiophene oligomers. Endcaping of oligofluorenes with diphenylamino group has been shown to offer advantages in terms of lowering their first ionization potentials, enhancing thermal stability and inducing good amorphous morphological stability . Thus, fluorene unit as the core is known to display interesting chemical and electronic characteristics. We have been engaged in our laboratory to synthesize durable and high efficient new organic, phthalocyanine as well as ruthenium(II) bipyridyl dyes, [22–24, 28–32] and came across a report of super sensitizer, where carbazole was incorporated on ancillary bipyridyl through conjugation of thiophene moiety . And as a part of our continued efforts in this area of research, we became interested to synthesize a new ruthenium(II) bipyridyl complex BPFC by introducing 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine as an ancillary ligand, and the influence of increased conjugation length on photovoltaic performance and thermal stability was evaluated relative to N719 sensitizer. Multiple performance increasing features such as alkyl groups (n-butyl and t-butyl), triarylamine equivalent (carbazole), biphenyl group in fluorene as extended conjugation have been incorporated in the new ruthenium(II) complex BPFC for achieving better overall performance.
2. Results and Discussion
Structure of the new ruthenium(II) bipyridyl sensitizer is shown in Figure 1 and the series of steps involved in synthesis of the complex are illustrated in Scheme 1. The new substituted π-conjugated ancillary bipyridyl ligand “4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine” (L1) was prepared in accordance to the reported classical reactions. Fluorene, procured from Sigma-Aldrich, was directly used in the bromination reaction to obtain 2-bromofluorene (1), which was subjected to bromine lithium exchange reaction with n-butyllithium (n-BuLi) followed by addition of n-butylbromide to obtain 2-bromo-9,9-dibutyl-9H fluorene (2). This was further reacted with triisopropylborate in presence of n-BuLi to form 9, 9-dibutyl-9H-fluoren-2-ylboronic acid (3). The boronic acid derivative was coupled with 4,4′-dibromo-2,2′-bipyridine under palladium catalyzed Suzuki conditions to afford 4,4-bis(9,9-dibutyl-9H-fluorene-2-yl)- bipyridine. The bipyridyl derivative thus obtained was treated with elemental iodine to afford 4,4′-bis(9,9-dibutyl-7-iodo-9H-fluoren-2-yl)-2,2′-bipyridine (5). The diiodo compound, on further reaction with 3,6-di-tert-butyl-9H-carbazole resulted crude L1, which was purified on silica gel column chromatography to obtain pure L1. The ancillary ligand L1 was subjected to complexation with [RuCl2p-cymene2]2 in DMF and followed by addition of 2,2′-bipyridine-4,4′-dicarboxylic acid and excess ammonium thiocyanate resulted the formation of crude BPFC. The complex was purified on Sephadex LH-20 column chromatography. The intermediates formed during the several classical reactions and the final ruthenium complex are characterized by FT-IR, 1H-NMR, UV-Vis and ESI-MASS spectroscopes. The reference sensitizer, N719, was synthesized in accordance to the procedure reported.
2.1.1. Synthesis of 2-Bromofluorene (1)
To a solution of fluorene (0.500 g, 1.8 mmoL) in dry acetone was added N-bromosuccinimide (0.320 g, 1.8 mmol) under nitrogen atmosphere. After maintaining at 80°C for 3 hours, cool to room temperature and ice water was added and then extracted with dichloromethane. The crude compound was purified on silica gel column chromatography using hexane/ethyl acetate mixture in 9/1 as eluent. Yield: 90% 1H NMR (δH/ppm in CDCl3): 7.75–7.65 (m, 3H), 7.45–7.20 (m, 4H). Chemical formula C13H10Br: ESI-MS: Calcd for (M + H)+: 246, found: 246 (28%).
2.1.2. Synthesis of 2-Bromo-9,9-Dibutyl-9H-Fluorine (2)
To a mechanically stirred mixture of 2-bromofluorene (0.980 g, 4 mmol), powdered KOH (1.200 g, 20 mmol), KI (0.066 g, 0.4 mmol), and DMSO (20 mL) were added and cooled to 10°C. Bromobutane (1.076 mL, 10 mmol) was added drop wise over 45 minutes. The color of the reaction mixture turned from red to light purple. After the temperature increased to 20°C, the reaction mixture was left over night, with stirring, poured into water and the precipitate obtained was extracted into dichloromethane. The organic extract was washed with brine solution and water and then concentrated with rotavapour. The compound was purified on silica gel column chromatography using hexane/ethyl acetate mixture in 9/1 as eluent. Yield: 90% 1H NMR (δH/ppm in CDCl3): 7.75–7.65 (m, 3H), 7.45–7.20 (m, 4H), 1.99 (m, 2H), 1.50 (t, 4H), 1.30 (t, 4H), 0.73 (t, 6H), 0.60 (s, 6H). Chemical formula C21H25Br: ESI-MS: Calcd for (M + H)+: 357, found: 357 (100%).
2.1.3. Synthesis of 9,9-Dibutyl-9H-Fluoren-2-Ylboronic Acid (3)
To a 100 mL two neck glass flask containing 2 (0.500 g, 1.4 mmol) in dry THF (20 mL) and a magnetic stirrer bar at –78°C, n-BuLi (1.05 mL, 1.05 mmol) was added under nitrogen atmosphere while maintaining good stirring. After stirring for 1 hour, triisopropylborate (0.484 mL, 2.1 mmol) was added. After stirring for further 2 hours, the reaction mixture was first quenched with water and then aqueous HCl (6 M, 20 mL) was added drop wise fashion until the solution turned acidic and then extracted with dichloromethane. The combined organic layers were dried over anhydrous sodium sulphate and concentrated with rotavapour. Purification was carried out by column chromatography on silica gel using hexane/ethyl acetate mixture (4/6 v/v) as eluent. Yield: 50%. 1H NMR (δH/ppm in CDCl3): 7.70 (d, 1H), 7.62 (s, 1H), 7.42–7.27 (m, 5H), 1.99 (s, 2H), 1.92 (m, 4H), 1.10 (t, 4H), 0.73 (t, 6H), 0.60 (s, 6H). Chemical formula C21H27BO2, ESI-MS: Calcd for (M + H)+: 323, found: 323 (100%).
2.1.4. Synthesis of 4,4-Bis(9,9-Dibutyl-9H-Fluorene-2-yl)--Bipyridine (4)
In a 25 mL one-necked round bottom flask equipped with a condenser were placed 3 (0.440 g, 1.375 mmol), barium hydroxide octahydrate (1.355 g, 4.297 mmol), and palladium tetrakis triphenyl phosphine (0.106 g, 0.091 mmol). The reaction flask was evacuated and filled with nitrogen gas, and is charged with 1.4-dioxane (4 mL), water (1.35 mL) and 4,4′-dibromo-2,2′-bipyridine (0.180 g, 0.573 mmol). The reaction mixture was refluxed for 24 hours under nitrogen gas and then cooled to room temperature. The dioxane was removed and the contents were poured into dichloromethane, the precipitate was removed through filter paper, and the organic layer was washed with 1 M-NaOH aqueous solution, NaCl (100 mL) and dried over sodium sulphate. After concentration on rotavapour, small quantity of methanol was added. The precipitate formed was filtered and purified on column chromatography with silica gel using mixture dichloromethane/methanol, (9/1 v/v) to obtain the pure product as pale yellow solid Yield 50%. 1H NMR (500 MHz, CDCl3) 8.70 (d, 1H), 8.63 (s, 1H), 7.80 (d, 1H), 7.60 (d, 1H), 7.29–6.63 (m, 6H), 2.0 ( m, 4H), 1.50 (m, 4H), 1.10 (m, 4H), 0.86 (s, 6H). Chemical formula (C52H56N2), ESI-MS: Calcd for (M + H)+: 709, found: 709 (70%).
2.1.5. Synthesis of 4,4-Bis(9,9-Dibutyl-7-Iodo-9H-Fluorene-2-yl)--Bipyridine (5)
A mixture of 4 (0.200 g, 0.282 mmol), iodine (0.172 g, 0.677 mmol), conc H2SO4 (0.036 mL) and water (0.013 mL) in glacial acetic acid (10 mL) were taken into 1-neck 100 mL round bottom flask. Then, the mixture was stirred at 80°C under nitrogen gas for 4 hours, and then, the reaction mixture was cooled to room temperature. The solution was poured into large amount of ice cool water. The resulting mixture was extracted with dichloromethane and then washed with water and then dried over Na2SO4 and concentrated on rotavapour, small quantity of methanol was added. The precipitate formed was separated and purified on column chromatography with silica gel using mixture (DCM/methanol, 9/1) to obtain the pure product as pale yellow solid Yield 45%. 1H NMR (δH/ppm in CDCl3) 8.8 (d, 2H), 8.75 (s, 2H), 7.6–7.8 (m, 8H), 7.5 (d, 2H), 7.25 (s, 4H), 2.0 (t, 8H), 1.15 (m, 16H), 0.78 (t, 12H). Chemical formula (C52H54I2N2), ESI-MS: Calcd for (M + H)+: 961, found: 961 (75%).
2.1.6. Synthesis of 4,4-Bis(9,9-Dibutyl-7,7 Di tert-butyl Carbazole-9H-Fluorene-2-yl)-[2,2]-Bipyridinyl (6)
In a 2-neck 250 mL round bottom flask containing 4,4-bis(9,9-dibutyl-7-iodo-9H-fluorene-2-yl)-[2,2]-bipyridinyl (0.100 g, 0.104 mmol), di-tert-butyl carbazole (0.087 g, 0.312 mmol), copper bronze (0.005 g, 0.084 mmol), and K2CO3 (0.067 g, 0.487 mmol) freshly distilled nitrobenzene was added, and the contents were stirred under N2 atmosphere under reflux at 210°C for 24 hours. After cooling to room temperature the reaction mixture was concentrated on the rotavapour for complete removal of nitrobenzene. The crude reaction mixture was then subjected to purification on silica gel column chromatography using ethyl acetate/methanol (9/1) as eluent, 45% yield. 1H NMR (δH/ppm in CDCl3) 8.81 (d, 2H), 8.79 (s, 2H), 7.54–7.85 (m, 18H), 7.35 (d, 4H), 7.12 (d, 4H), 2.0 (t, 8H), 1.50 (m, 16H), 1.35 (s, 36H), 0.86 (t, 12H). Chemical formula (C92H102N4), ESI-MS: Calcd for (M)+: 1263, found: 1263 (100%).
2.1.7. Synthesis of Ruthenium(II) Complex
Compound 6 (0.100 g, 0.079 mmol) and dichloro (p-cymene) ruthenium(II) dimer (0.024 g, 0.039 mmol) in DMF were heated at 60°C for a period of 4 hours under nitrogen in dark. Subsequently 4,4′-dicarboxylic acid-2,2′-bipyridine (0.019 g, 0.079 mmol) was added and the reaction mixture was heated to 140°C for another 4 hours. To the resulting dark green solution, solid NH4NCS (0.180 g, 2.37 mmol) was added and then the reaction mixture was further heated for another 4 hours at 140°C. After rotaevaporation of DMF, water (250 mL) was added to get precipitate. The precipitate was kept in refrigerator overnight, filtered and washed with distilled water and then dried in vacuum desiccator. The crude compound was dissolved in methanol and dichloromethane mixture and further purified on sephadex LH-20 column using methanol/dichloromethane mixture (3/2 v/v) as eluent. The main band was collected and concentrated with rotavapour. Yield: 65%. 1H NMR (δH/ppm in CD3OD + CDCl3) 9.48 (d, 1H), 9.39 (d, 1H), 8.82 (s, 1H), 8.69 (s, 1H), 8.56 (s, 1H), 8.41 (s, 1H), 7.30–8.30 (m, 29H), 7.18 (d, 1H), 1.8 (t, 8H), 1.35 (s, 36H), 1.15 (m, 16H), and 0.85 (t, 12H). Chemical formula RuC109H116N8O4S2, ESI-MASS: Calcd for (M + H) +: 1768, found: 1768 (72%).
2.2. Fabrication of Test Cells
Fluorine-doped SnO2 (FTO) conducting glass plates (Nippon Sheet Glass, 4 mm thick, 8 Ω/sq) were cleaned with a detergent solution followed by rinsing with water and ethanol and then treated in a UV-O3 system to remove organics and other contaminants. A compact layer, which will facilitate a good mechanical contact between the nanocrystalline TiO2 and the conducting FTO matrix, was coated over the cleaned plates using a 40 mM TiCl4 aqueous solution, and then, the plates were heated at 70°C for 30 minutes. The working electrodes are composed with 9 μm thickness of 18 nm TiO2 particles (D18T) as transparent layer over which 4.8 μm thickness of 400 nm anatase TiO2 particles (CCIC, HPW-400) as scattering layer. The TiO2-coated films were gradually heated under an air flow at 325°C for 5 minutes, at 375°C for 5 minutes, at 450°C for 15 minutes, and at 500°C for 15 minutes. While cooling, when the temperature attained to around 90°C, the electrodes were immersed in 0.3 mM dye solutions of ethanol and soaked for 16 hours under the dark. The dye-sensitized TiO2 electrodes were rinsed with ethanol to remove the unadsorbed dye molecules and then dried under nitrogen gas. The counter electrodes were prepared by coating an FTO plate (TEC 15, 2.2 mm thickness, Libbey-Owens-Ford Industries) with a drop of H2PtCl6 solution (2 mg of Pt in 1 mL of ethanol) and heating it at 430°C for 15 minutes. The dye sensitized TiO2 electrode and Pt counter electrode were assembled into a sealed sandwich type cell by heating with a hot-melt surlyn film (Surlyn 1702, 25 μm thickness, Du-Pont) as a spacer in-between the electrodes. The liquid electrolyte of E01 (I2 0.05 M, LiI 0.1 M, DMPII 0.6 M, and TBP 0.5 M in acetonitrile) was filled through the predrilled hole present on the counter electrode, and then, the hole was sealed with a Surlyn disk and a thin glass to avoid leakage of the electrolyte.
2.3. Absorption and Emission Properties
The electronic absorption spectrum of BPFC sensitizer recorded in ethanol is shown in Figure 2(a), and the spectrum was compared with that of the reference N719 sensitizer. The complex exhibited one absorption band at longer wavelength region and a shoulder type band in short wavelength region. The molar extinction coefficient of low-energy absorption band of BPFC is 18.5 × 103 M−1 cm−1, which is larger as compared to that of reference N719 sensitizer that showed molar extinction coefficient of 14.4 × 103 M−1 cm−1. Compared to N719, the increase in π-conjugation length by introduction of 4, 4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine in BPFC complex increases the molar extinction coefficient and the spectral response of the new complex. The high-energy shoulder type absorption band of the complex with increased molar extinction coefficient could be attributed to the π-π* transitions of fluorene segments which exhibit strong absorption at around 400 nm.
The high-energy absorption band of ruthenium(II)-bipyridyl complexes is contributed by two components: one is metal to ligand charge transfer transition, while the other one is π-π* transitions of the ancillary bipyridyl ligand, L1. The 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine (L1) exhibits two absorption bands, one at around 303 nm and the other one at 322 nm and these characteristic absorption bands exists even in BPFC complex but slightly at higher wavelengths. This indicates that the π-π* transitions in the ancillary bipyridyl ligand, L1 are strong and significantly contributing to the high-energy absorption band of BPFC complex. The emission spectra of BPFC sensitizer was recorded in ethanol by exciting the complex with its absorption maxima of low-energy absorption band. The emission spectrum was analyzed by Gaussian reconvolution method to integrate emission peak to estimate the emission maxima.
Besides the molar extinction coefficient, the other important property, that is, quantity of dye absorped on TiO2 films and the pattern of dye absorpsion, also influences the light-harvesting capability and the photovoltaic performance of DSSC devices. The molecular diagonal diameter and geometrical structure of any dye vary with respect to π-system substituted on one of the bipyridine moieties of N719. As compared to simple 2,2′-bipyridine-4,4′-dicarboxylic acid in N3, the 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine in BPFC complex largely increases the diagonal molecular size, and hence, it is expected to show significant effect on film absorptions of BPFC. Therefore, the film absorption measurements over TiO2 surface were carried out by staining 7.0 μm thick TiO2 (18 NRT layered) films in 0.3 mM dye solutions prepared in ethanol for a period of 16 hours under dark. The absorption spectrum of BPFC-sensitized TiO2 film was recorded and was compared with that of N719 sensitized TiO2 film (Figure 2(b)). The measurements indicate that the dye molecules are anchored on TiO2 surface, and the film absorbencies for both the dyes are similar. To compare the anchoring pattern and surface morphology of the new sensitizer, the absorbance maxima of low energy absorption band of BPFC sensitizer is normalized by the corresponding absorbance maxima of N719, while their molar extinction coefficients are normalized by the molar extinction coefficient of N719. The film absorbance ratio of BPFC calculated is lower than that of N719 indicating its lower packing density of the dye molecules on TiO2 surface. Staining TiO2 electrodes immediately after sonication of BPFC dye solution showed much higher film absorption ratios as compared to those TiO2 films stained for prolonged soaking times in the BPFC dye solutions, and this indicates the necessity of sonication before staining the TiO2 electrodes, particularly when sensitizers with larger diagonal diameter are employed.
2.4. Electrochemical Properties
In dye-sensitized solar cells, favorite energy offset between dye and titania is a basic requirement for any high-efficiency solar cell, in which the sensitizer’s immediate charge generation yield from the excited state has a direct influence on the performance of DSSC device. To measure the electrochemical properties of BPFC dye, cyclic voltammetry was employed using tetra-butyl ammonium perchlorate (0.1 M in acetonitrile) as an electrolyte and ferrocene as an internal standard at 0.42 V versus SCE (Figure 3). The oxidation and reduction potentials of BPFC are 0.79 V and −0.80 V, respectively. The more positive potential of the sensitizer, relative to I-/I3- redox couple in the electrolyte provide a large thermodynamic driving force for the regeneration of the dye by iodide. Based on absorption and emission spectra, the excitation transition energy () of BPFC was estimated to be 1.87 eV and the standard potential (φ0(S+/S*)) calculated from the relation of [φ0(S+/S) = φ0(S+/S*)–] for the sensitizer was −1.08 V versus SCE. So, φ0(S+/S*) value is more negative (or higher in energy) than the conduction band edge of TiO2 providing a thermodynamic driving force to inject electron from the dye to TiO2.
2.5. Computational Studies
In order to augment the molar extinction coefficient with the π-conjugation extension through 4, 4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine (L1) in BPFC relative to 2,2′-bipyridine -4,4′-dicarboxylic acid in N719 complex, the electronic ground state of fully protonated complex is optimized. To see the influence of the ancillary ligand, L1 on the corresponding ruthenium(II) complex, the electronic ground state of the ligand was optimized using B3LYP/6-31G(d) method. Based on the optimized structures, TD-DFT calculations were performed to see the optical properties of the ligand and the corresponding ruthenium(II) complex. The unoccupied (LUMO+4 to LUMO) and occupied (HOMO to HOMO+4) orbitals of L1 are shown in Figure 4. The HOMO and HOMO−1 orbitals of L1 are degenerate and the π-orbitals are almost delocalized among carbazole modified fluorenes on ancillary bipyridine, which lifts their energy levels. In case of HOMO−2 and HOMO−3, the π-orbitals are almost localized on the carbazole chromophore. In case of LUMO to LUMO+2 orbitals of L1, the π*-orbitals are delocalized over π-system with maximum components on the bipyridine, which depresses their energy levels. LUMO+3 and LUMO+4 have π*-orbitals localized on carbazole chromophore. The TD-DFT excitation calculations performed for the optimized ground state of the ancillary bipyridyl ligand, L1 shows basically two π-π* transitions with significant oscillation strengths at 303 and 322 nm, respectively, as observed in the case of the absorption spectrum of the ancillary ligand, L1.
The unoccupied (LUMO to LUMO+4) and occupied (HOMO to HOMO−4) frontier orbitals of BPFC are shown in Figure 5. The first three occupied (HOMO to HOMO−2) orbitals of BPFC exhibit ruthenium t2g character with size mixing from thiocyanate ligand and with π-bonding orbitals of 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine (L1). The π-clouds for HOMO−3 orbital for both the dyes are nonbonding combination localized on the NCS ligands. The HOMO−4 and HOMO−5 of BPFC are combinations of π-bonding orbitals localized over carbazole moiety of 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine. In HOMO and HOMO−1 orbitals of the new ancillary bipyridine, the π-orbitals are more delocalized over the π-system and bipyridine, and this favors lifting their energy levels. The conjugation length of BPFC resulted in increase in the molar extinction coefficient of MLCT absorption bands, which could probably due to lifting their occupied molecular orbitals energy levels as compared to those of N719. In case of LUMO, the electron distribution move toward anchoring groups, while assuming similar molecular orbital geometry when adsorbed on TiO2 surface, the close position of the LUMO to the anchoring moieties is expected to enhance the overlap with the 3d orbitals of TiO2 leading to favored electron injection.
2.6. Thermal Stability
One of the parameters desired to sustain the initial photovoltaic performance of the DSSC over a long period is the high thermal stability of the ruthenium(II) sensitizer. In order to evaluate the thermal stability of the new sensitizer relative to N719, TGA analysis were performed using a TGA/SDTA thermal system (Mettler Toledo, Switzerland) at heating rate of 10°C/min in the temperature range of 50–600°C under N2 atmosphere (flow rate of 30 mL/min) and the influence of 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine on thermal stability of BPFC complex was studied. Film samples ranging from 8 to 10 mg were placed in the sample pan and heated, while weight loss and temperature difference were recorded as a function of temperature. The thermogram of BPFC obtained under identical conditions with that of N719 was compared. Figure 6 shows the derivative of % conversion with respect to temperature, in which both the thermograms of BPFC and N719 initially follow similar trend up to around 200°C and after this, BPFC loses its mass quickly and hence a decrease in thermal stability by around 50°C was observed as compared to that of N719. This indicates that the substitution of 4,4-bis(9,9-dibutyl-9H-fluorene-2-yl)- bipyridine reduces the thermal stability of the ruthenium(II) sensitizer.
2.7. Photovoltaic Properties
To study the influence of 4,4′-bis(9,9-dibutyl-7-(3,6-di-tert-butyl-9H-carbazol-9-yl)-9H-fluoren-2-yl)-2,2′-bipyridine as π-conjugation extension on the photovoltaic performance of DSSC relative to 2,2′-bipyridine-4,4′-bicarboxylic acid, double-layer titania film (9.0 + 4.8 μm) 0.16 cm2 active area TiO2 electrodes and high-efficiency liquid electrolyte were employed for fabrication of DSSC test cells. The fabrication and evaluation of DSSC test cells were in accordance to the procedures already reported and the volatile electrolyte, (E01) containing 0.05 M I2, 0.1 M LiI, 0.6 M 1,2-dimethyl-3-n-propylimidazolium iodide, 0.5 M 4-tert-butylpyridine in acetonitrile solvent was employed . The incident photon-to-current conversion efficiency (IPCE) of the sensitizer plotted as a function of excited wavelength was compared with that of N719 sensitized solar cell, fabricated and evaluated under identical conditions (Figure 7). The photocurrent action spectrum of BPFC showed broad plateau IPCE spectrum with exceeding IPCE of 55%, while that of N719 exhibited maximum IPCE reaching 78%. The BPFC sensitizer gives short-circuit photocurrent density (), open-circuit voltage (), and fill factor (ff) of 11.52 mAcm2, 566 mV, and 0.72, respectively, yielding an overall energy conversion efficiency (η) of 4.65%, while the test device fabricated under identical conditions with N719 dye gave of 14.36 mA/cm2, of 640 mV, and ff of 0.71 yielding an overall energy conversion efficiency of 6.5%. When compared to N719 sensitized solar cell, BPFC-sensitized solar cell is expected to show lower power conversion efficiency due to lower and lower IPCE of BPFC relative to that of N719 (Table 1).
The new sensitizer BPFC was carefully designed considering the following (1) The alkylgroups (two n-butyl and two t-butyl on each pyridyl of ancillary ligand) not only increase the solubility of the sensitizer in organic solvents but also serve as electron donating apart from inhibiting water induced desorption of the sensitizer from the TiO2. (2) Carbazole is a triarylamine equivalent which is known to improve the efficiency of the sensitizer. (3) The biphenyl group in Fluorene moiety serves as extended conjugation for enhancing the molar extinction coefficient and provides aromatic stability to the molecule. (4) The bipyridine dicarboxylic acid provides excellent anchoring of the complex on to the TiO2 surface facilitating easy electron injection. Thus, the multiple performance increasing features of the BPFC sensitizer makes the ruthenium(II) complex unique for DSSC application and showed solar-to-electric energy conversion efficiency (η) 4.6%, while under similar fabrication and measurement conditions, standard N719 showed 6.5% efficiency. The new ruthenium(II) bipyridyl sensitizer showed relatively high molar extinction coefficient. Upon sensitization with nano-crystalline TiO2, the dye showed decreased film absorption ratios, whereas staining the TiO2 electrodes with freshly sonicated dye solutions showed relatively increased film absorption ratios on TiO2 surface. The lower solar-to-electrical energy conversion efficiency could be result of lower IPCE value and lower film absorption ratios. Design and development of super sensitizers with similar high performance features but with less bulky nature are under progress.
C. S. Rao thanks IICT-AIC collaborative project for a fellowship. T. Suresh thanks CSIR, New Delhi, for senior research fellowship. M. Chandrasekharam thanks DST, New Delhi for the grant of the project entitled “Advancing the efficiency and production potential of Excitonic Solar Cells (APEX)” under UK-DST consortium.
A. Hagfeld and M. Grätzel, “Light-induced redox reactions in nanocrystalline systems,” Chemical Reviews, vol. 95, no. 1, pp. 49–68, 1995.View at: Google Scholar
B. O'Regan and M. Grätzel, “A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO2 films,” Nature, vol. 353, no. 6346, pp. 737–740, 1991.View at: Google Scholar
M. K. Nazeeruddin, A. Kay, I. Rodicio et al., “Conversion of light to electricity by cis-X2bis(2,2'-bipyridyl-4,4'-dicarboxylate)ruthenium(II) charge-transfer sensitizers (X = Cl-, Br-, I-, CN-, and SCN-) on nanocrystalline titanium dioxide electrodes,” Journal of the American Chemical Society, vol. 115, no. 14, pp. 6382–6390, 1993.View at: Google Scholar
S. M. Zakeeruddin, M. K. Nazeeruddin, R. Humpry Baker et al., “Design, synthesis, and application of amphiphilic ruthenium polypyridyl photosensitizers in solar cells based on nanocrystalline TiO2 films,” Langmuir, vol. 18, no. 3, pp. 952–954, 2002.View at: Google Scholar
P. Wang, S. M. Zakeeruddin, J. E. Moser, M. K. Nazeeruddin, T. Sekiguchi, and M. Grätzel, “A stable quasi-solid-state dye-sensitized solar cell with an amphiphilic ruthenium sensitizer and polymer gel electrolyte,” Nature Materials, vol. 2, no. 6, pp. 402–407, 2003.View at: Publisher Site | Google Scholar
D. Kuang, C. Klein, S. Ito et al., “High molar extinction coefficient ion-coordinating ruthenium sensitizer for efficient and stable mesoscopic Dye-sensitized solarCells,” Advanced Functional Materials, vol. 17, pp. 154–160, 2007.View at: Google Scholar
K. J. Jiang, N. Masaki, J. B. Xia, S. Noda, and S. Yanagida, “A novel ruthenium sensitizer with a hydrophobic 2-thiophen-2-yl-vinyl- conjugated bipyridyl ligand for effective dye sensitized TiO2 solar cells,” Chemical Communications, no. 23, pp. 2460–2462, 2006.View at: Publisher Site | Google Scholar
C.-Y. Chen, S.-J. Wu, C.-G. Wu, J.-G. Chen, and K.-C. Ho, “A ruthenium complex with superhigh light-harvesting capacity for dye-sensitized solar cells,” Angewandte Chemie—International Edition, vol. 118, pp. 5954–5957, 2006.View at: Google Scholar
D. Kuang, C. Klein, S. Ito et al., “High effiiciency and stable mesoscopic Dye-sensitized solar cells based on a high molar extinction cofficient Ru-sensitizer and non-volatile electrolyte,” Advanced Materials, vol. 19, pp. 1133–1137, 2007.View at: Google Scholar
F. Matar, T. H. Ghaddar, K. Walley, T. DosSantos, J. R. Durrant, and B. O'Regan, “A new ruthenium polypyridyl dye, TG6, whose performance in dye-sensitized solar cells is surprisingly close to that of N719, the ‘dye to beat’ for 17 years,” Journal of Materials Chemistry, vol. 18, no. 36, pp. 4246–4253, 2008.View at: Publisher Site | Google Scholar
F. Gao, Y. Wang, D. Shi et al., “Enhance the optical absorptivity of nanocrystalline TiO2 film with high molar extinction coefficient ruthenium sensitizers for high performance dye-sensitized solar cells,” Journal of the American Chemical Society, vol. 130, no. 32, pp. 10720–10728, 2008.View at: Publisher Site | Google Scholar
M. Chandrasekharam, C. Srinivasarao, T. Suresh et al., “High spectral response heteroleptic ruthenium (II) complexes as sensitizers for dye sensitized solar cells,” Journal of Chemical Sciences, vol. 123, pp. 37–46, 2011.View at: Google Scholar
L. Giribabu, M. Chandrasekheram, M. L. Kantham et al., “Conjugated organic dyes for dye-sensitized solar cells,” Indian Journal of Chemistry—Section A, vol. 45, no. 3, pp. 629–634, 2006.View at: Google Scholar
M. Chandrasekharam, G. Rajkumar, C. Srinivasa Rao et al., “Molecular engineered fluorene substituted Ru-complex for efficient mesoscopic dye sensitized solar cells,” vol. 2, 2011, Advances in Natural Sciences: Nanoscience and Nanotechnology. Accepted.View at: Google Scholar
M. Chandrasekharam, G. Rajkumar, C. Srinivasa Rao et al., “Polypyridyl Ru(II)-sensitizers with extended π-system enhances the performance of Dye sensitized solar cells,” Synthetic Metals, vol. 161, pp. 1098–1104, 2011.View at: Google Scholar
M. Chandrasekharam, G. Rajkumar, C. Srinivasa Rao, P. Yella Reddy, and M. Lakshmi Kantam, “Change of Dye bath for sensitisation of nanocrystalline TiO2 films: enhances performance of Dye-sensitized solar cells,” Advances in OptoElectronics, vol. 2011, Article ID 376369, 9 pages.View at: Google Scholar