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Article

Push–Pull Zinc Phthalocyanine Bearing Hexa-Tertiary Substituted Carbazolyl Donor Groups for Dye-Sensitized Solar Cells

by
Basma Ghazal
1,2,
Kobra Azizi
3,
Ewies F. Ewies
2,
Ahmed S. A. Youssef
4,
Valid Mwatati Mwalukuku
5,
Renaud Demadrille
5,*,
Tomás Torres
3,6,* and
Saad Makhseed
1,*
1
Department of Chemistry, Kuwait University, P.O. Box 5969, Safat 13060, Kuwait
2
Organometallic and Organometalloid Chemistry Department, National Research Centre, Cairo 12622, Egypt
3
Departamento de Química Orgánica, Universidad Autónoma de Madrid, Cantoblanco, 28049 Madrid, Spain
4
Department of Chemistry, Faculty of Science, Ain Shams University, Abbassia, P.O. 11566, Cairo, Egypt
5
CEA-Univ. Grenoble Alpes-CNRS, IRIG, SyMMES, 38000 Grenoble, France
6
IMDEA-Nanociencia, Campus de Cantoblanco, 28049 Madrid, Spain
*
Authors to whom correspondence should be addressed.
Molecules 2020, 25(7), 1692; https://doi.org/10.3390/molecules25071692
Submission received: 15 February 2020 / Revised: 27 March 2020 / Accepted: 2 April 2020 / Published: 7 April 2020
(This article belongs to the Special Issue Recent Advances in Dye-Sensitized Solar Cells)
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Abstract

:
An asymmetrical, push–pull phthalocyanine bearing bulky tert-butylcarbazolyl moieties as electron donor and carboxylic acid as anchoring group was synthetized and tested as a photosensitizer in dye-sensitized solar cells (DSSC). The new photosensitizer was characterized by 1H and 13C NMR, UV–Vis and mass spectrometry. The bulky tert-butylcarbazolyl moieties avoid the aggregation of the phthalocyanine dye. DFT studies indicate that the HOMO is delocalized throughout the π-electron system of the substituted phthalocyanine and the LUMO is located on the core of the molecule with a sizable electron density distribution on carboxyl groups. The new dye has been used as a photosensitizer in transparent and opaque dye-sensitized solar cells, which exhibit poor efficiencies related to a low Jsc.

Graphical Abstract

1. Introduction

Dye-sensitized solar cells (DSSCs) are an effective alternative for delivering clean energy from the sun compared to traditional power cells [1,2,3,4]. Numerous efforts are currently being directed toward the development of optimized light harvesters capable of utilizing the entire range of the solar spectrum, including the infrared portion lost in present silicon-based PV technology. These efforts have the potential to improve the efficiency in solar energy conversion of dye-sensitized solar cells (DSSCs) via the so-called panchromatic sensitization.
In a DSSC, the photosensitizer is a crucial element not only because it is responsible for the photon harvesting of the solar cell, but also because it drives the electron transfer at the TiO2/dye/electrolyte interfaces [5]. For this reason, it is of tremendous importance to accurately control not only the absorption but also the energy levels of the dyes. The structure engineering of organic dyes offers this possibility, and organic photosensitizers usually show superior absorption compared to ruthenium dyes. For this reason, a plethora of organic dyes have been developed in the last decade, leading to the improvement of the device performances and robustness [6,7].
The new generation of DSSCs use donor–π–acceptor (D–π–A) sensitizers with high molar absorptivity, which allow the use of TiO2 thin films, leading to improvements in the open circuit voltage VOC when used with cobalt–based or copper–based redox mediators [1,8,9,10]. The production of efficient D–π–A sensitizers involves the design of panchromatic dyes with high absorption in the red and near-infrared regions as well as low aggregation [11]. Also, the ability of such dyes to establish strong electronic communication between the lowest unoccupied molecular orbitals (LUMOs) of the dye and the TiO2 conduction band ensures efficient electron injection from the excited photosensitizer into the semiconductor. Phthalocyanines (Pcs) represent one of the most prospective class of functional materials incorporated in DSSCs, owing to their high photochemical and electrochemical stabilities and extremely intense absorption band in the red-NIR region (i.e., the maximum solar flux of photons within this optical window region) [12,13]. Moreover, a strong light harvesting capability and high absorption at λ = 600–800 nm is the most photon-rich part of the sunlight.
The most successful ZnPcs sensitizers identified to date are asymmetrically substituted molecules of A3B type, characterized by three of the four isoindole subunits (called A), that makes up the Pc macrocycle as identical and bulky with electron-donating groups, whereas one or more anchoring groups (called B) are capable of interacting with the metal oxide semiconductor [14,15]. The aim of this A3B design is to combine steric suppression of dye aggregation, favorable electronic push–pull effects, and optimized binding mode of the dye with the semiconductor layer surface. Nazeeruddin, Torres et al., proposed this initially, using peripherally A3B form-bearing tert-butyl donors and -COOH anchoring groups that were able to achieve power conversion efficiencies up to 3.5% [15]. Molecular engineering toward Pc-based efficient DSSCs reported by Giribabu et al. involved substitution of the A3B ZnPcs with six butyloxy groups at the alpha peripheral positions and double carboxyl structures. Contrary to what was expected, the designed structures led to lower efficiency of 1.13% as the result of a low LUMO level, unsuitable for efficient electron injection [16,17]. Kimura et al. designed bulky, electron rich aryl substituents rotated with respect to the macrocycle plane. Even though the aggregation was strongly reduced, they reached the optimum PCE of 1.59% [18]. On the other hand, Torres, Nazeeruddin, Mori, Kimura et al. demonstrated the interest of a A3B ZnPc family, with electron-rich 2,6-disubstituted phenoxy groups, as a donor A, and one electron withdrawing -COOH group, with or without a rigid alkyne spacer between the dye and the anchoring group, as the acceptor B, reporting impressive power conversion efficiencies up to 6.1% (TT40) [19,20] and 6.4% (PcS20) [21,22,23] under simulated one-sun illumination. Regardless of continuous improvements in this field, the full potential of ZnPcs as a photosensitizer is yet to be realized in DSSCs and further developments are required.
Amino groups including NH2, NHR, -NR2, NHAr, and NAr2 have been tested as good donor groups to enhance the photovoltaic performance of asymmetrical ZnPcs (A3B) based on their higher LUMO levels, lower energy gaps, and red-shifted absorption bands [24,25]. Moreover, the presence of new absorption bands in the 400–600 nm region, where the molar absorption coefficient of the macrocycle is minimum, should make them good candidates as panchromatic sensitizers. Along the same lines are rational molecular designs by Giribabu et al. who prepared asymmetrical A3B Pc bearing three bulky electron-donating triphenylamines and two carboxyl units [24]. Regardless of the adequate optical design of the sensitizer, it exhibited poor performance. Meanwhile, the IPCE (Incident Photon-to-electron Conversion Efficiency) spectra showed broader, red-shifted, and better response [1,24]. Several attempts have been reported to enhance the overall power conversion efficiency PCE along with adequate optical properties [25,26]. Using a different approach, Kimura et al. described the direct annulation of carbazole entities with the Pc core and revealed an influence of carbazole groups on the photophysical and electrochemical properties as well as on their performance in DSSC [27], in addition to interesting wide light-harvesting properties in the 400–800 nm range. Recently, we reported an octa-substituted carbazolyl phthalocyanines with a broad absorption band observed in the 450–500 nm range [28,29]. The steric hindrance imposed by bulky tert-butyl groups on the carbazole substituents are expected to suppress the undesirable molecular aggregation while at the same time acting as electron-donating units. This should provide excellent absorption in the NIR region.
Herein, we have designed and synthesized an asymmetrical phthalocyanine (tCzZnPc1) bearing six tert-butylcarbazolyl moieties and one carboxyl group, and this new molecule was incorporated for the first time in DSSCs as a photosensitizer.

2. Results and Discussion

2.1. Synthesis

The synthetic route to tCzZnPc1 is depicted in Scheme 1. The molecule has been prepared according to Zn(II)-templated cyclization on a mixture of 4,5-bis(3,6-di-tert-butyl-9H-carbazol-9-yl)phthalonitrile (1) and 4-(hydroxymethyl)phthalonitrile (2) as building blocks, (molar ratio 4:1) to afford the A3B ZnPc (3) in 14% yield. The dehydrogenation of hydroxymethyl phthalocyanine 3 was performed in zinc oxide and potassium hydroxide solution in mesitylene to give tCzZnPc1 in 92% overall yield and hydrogen gas was the only byproduct (for more details, see the Materials and Methods section). The catalytically active species in the solution is believed to be the corresponding zinc alkoxide from the reaction of alcohol with zinc oxide and potassium hydroxide. Decomposition of the alkoxide would result in zinc hydride and the corresponding aldehyde, which can give rise to the carboxylate and the starting alcohol by either a Cannizzaro reaction or a Tishchenko reaction in the presence of KOH [30].
Both 3 and tCzZnPc1 complexes are freely soluble in most organic solvents. Structural identification of both was achieved by 1H (Figure 1), and 13C NMR spectroscopies as well as UV-Vis and MALDI-TOF spectrometry. The UV-Vis spectra of 3 (Figure S4) and tCzZnPc1 were detected in THF and exhibited the classic Q-band of phthalocyanines, and typical shape of monomeric systems. A red-shift of this Q-band, regarding common substituted phthalocyanines, at around 707 nm was observed. The intensity of this absorption in both 3 and tCzZnPc1 is low, particularly in the last one. A strong absorption around ~340 nm, due to the carbazole moieties, appeared overlapping in the B-band region in tCzZnPc1 (Figure 4a), which was observed before in a previously prepared symmetrical octacarbazolylphthalocyanine Pc [25]. In our particular case, the intensity of the Q-band in tCzZnPc1 is low in comparison with the strong absorption of the six carbazole moieties which absorb in the region of 340 nm. On the other hand, it is well known that phthalocyanines bearing bulky groups can be highly distorted, with deviation of the planarity, which can affect the intensity of this band.
Having proved the synthetic feasibility of A3B tCzZnPc1 substituted with six tert-butylcarbazolyl moieties, we then examined the electronic compatibility of tCzZnPc1 for use as a sensitizer in a DSSC configuration. The architecture of a DSSC requires the favorable energy alignment of all functional components of the electrochemical circuit, such as the electron transport material (ETM), the sensitizer, and the redox couple responsible for the regeneration of the photo-oxidized dye. Theoretical calculations were carried out to understand the geometrical configuration, electronic distributions, and frontier orbital energies of tCzZnPc1 using TD−DFT on CAM-B3LYP exchange–correlation functional [31] coupled with the double-zeta quality LANL2DZ basis set [32] for all atoms. tCzZnPc1 reveals good spatial orbitals separation. The HOMO levels of the dye are delocalized over pyrrolic α- and β-pyrrolic carbons in the studied complexes along with high contribution of carbazole donor moieties. Meanwhile, the LUMO levels are delocalized at the core, with contributions from either the α- and β-pyrrolic carbon atoms, or from meso- and inner-nitrogen atoms along with a sizable electron density distribution on carboxylic anchoring group (Figure 2).

2.2. Photovoltaic Performance

In order to evaluate the potential of the newly synthesized molecules for photovoltaic applications, semi-transparent and opaque DSSCs were fabricated following a standard procedure. The opaque solar cells refer to devices that include an additional TiO2 layer (particle size ~ 400 nm) of about 3 to 4 µm thick above the mesoporous TiO2, whereas the “transparent solar cells” contain only the mesoporous TiO2 layer of 13 µm-thick layer (particle size ~ 15–20 nm). The devices show an active area of 0.36 cm2. The complete treatment of the electrodes are fully described in the experimental section. Immediately after the treatment, the photoanodes were sensitized through immersion in the dyeing solution for 16 h at room temperature with varying dye concentration of tCzZnPc1 = 0.2 and 0.5 mM, with/without CDCA co-adsorption due to the bulkiness of our dye, in CHCl3/EtOH 1/1, v/v. The CDCA coadsorption was done with the dye/CDCA ratio of 1:5. Platinized counter electrodes were employed in this study and the cells were filled with an electrolyte (Solaronix Iodolyte HI-30) via the pre-drilled hole using a vacuum pump. To improve the current collection, a metal contact along the cell edges was deposited using an ultrasonic solder. Before measurements, the AM1.5G solar simulator was calibrated using a reference silicon photodiode equipped with an IR-cutoff filter (KG-3, Schott). The current–voltage characteristics of the cells were measured under dark and under AM 1.5G (1000 W·m−2) irradiation condition. The devices were masked prior to measurements to attain an illuminated active area of 0.36 cm2 (Figure 3).
From the HOMO and LUMO energy levels determined by cyclic voltammetry in solution, it is clear that the molecule can be used as a photosensitizer in a classical DSSC configuration. Experimental HOMO and LUMO energy levels are found in relatively good agreement with the results from the modeling. We determined a HOMO energy level located at -5.40 eV and a LUMO level located at −3.50 eV. Taking into account that the conduction band energy level of the semiconductor is around −4.1 eV and the redox potential of the I−/I3− is around −3.9 eV, the driving force for the electron photoinjection is higher than 0.5 eV, and the driving force for the regeneration of the dye is higher than 0.3 eV.
Despite this, the photovoltaic parameters of the solar cells fabricated in this work were quite disappointing (see Table 1). One should note that the electrodes are yellowish after sensitization, showing that the absorption of the dye overlaps strongly with the one of the iodine-based electrolytes. The highest performance was achieved with an opaque device. The best cell exhibited a Jsc of 1.05 mA.cm−2, Voc of 542 mV, and FF of 70.8%, leading to a power conversion efficiency of 0.40%. Surprisingly, the transparent solar cells showed a quite similar PCE around 0.35% with a Jsc of 0.91 mA.cm−2, Voc of 538 mV, and FF of 71.7%. These results were reproducible over three devices. The use of chenodeoxycholic, which is often employed to reduce aggregation of the dyes on TiO2 surface, did not improve the performances of the cells. This result was expected because of the presence of the twelve tertbutyl groups on the molecule that are supposed to totally suppress aggregation phenomenon. Unfortunately, the very poor performances and the low Jsc impede accurate IPCE analysis of the solar cells.
In order to find the reason behind the poor efficiency of this new Zn-phthalocyanine derivative, we have measured the molar absorption coefficient in THF solution and the absorption spectrum of the molecule after adsorption on TiO2 mesoporous transparent electrodes (see Figure 4) and calculated the dye loading on the opaque photoelectrodes.
These measurements demonstrate that the molecule has poor absorption in the visible range. After grafting the molecule on TiO2, the absorption spectrum is slightly enlarged with an absorption edge close to 600 nm, but the absorption feature corresponding to the Q-band disappears. In addition, a very low dye-loading of 6.069 × 10−8 moles·cm−2 was estimated on the 13 + 4 µm-thick photoelectrodes. These results can explain the low Jsc values and consequently low performance of the molecule. Our preliminary results on this class of molecules indicate that the introduction of bulky substituents is a good strategy to reduce the dye aggregation but their low absorption in the visible range and the low amount of dyes attached on the surface lead to poor photovoltaic performances.

3. Materials and Methods

3.1. General Methods and Characterization Techniques

Carbazole, deuterated dimethylsulfoxide (DMSO-d6), cesium fluoride (CsF), anhydrous zinc acetate, ZnO, and KOH were purchased from Sigma-Aldrich. 5,6-Dichlorophthalonitrile was obtained from TCI (Toshima, Japan). Mesitylene (solvent) from Sigma-Aldrich was stored over activated 4Å molecular sieves (HPLC grade) and degassed with N2-vacuum before use. Anhydrous solvents were either supplied from Sigma-Aldrich and used as they were received and dried with 4Å molecular sieves (Panreac) or dried as described by Perrin [33]. TLC was performed using polygram sil G/UV 254 (0.2 mm thick, E. Merck, Darmstadt, Germany) TLC plates and visualization was carried out by ultraviolet light at 254 and 350 nm. Column chromatography was performed using Merck silica gel 60, 230–400 of mesh size 0.040–0.063 mm, Merck and eluents are indicated for each particular case. Gel permeation chromatography (GPC) was performed using Bio-Beads S-X1 (200400 mesh, Bio-Rad, Hercules, CA, USA). NMR spectra were recorded on a Bruker Ascend 400 spectrometer.
1H and 13C NMR spectra were recorded using Bruker DPX 600 at 600 and 150 MHz, respectively, while for oxidized complex, the NMR spectra were recorded on a Bruker Ascend 400 spectrometer. The IR spectra were obtained using Jasco 6300 FTIR. UV–Vis spectra were recorded with a Varian Cary 5 or Shimadzu UV-2600 spectrophotometer. MALDI-TOF MS was performed on a Bruker ultrafleXtreme using RP 700-3500-Da LP-700-3500-Da methods and 2, 5-dihydroxybenzoic acid (DHB) as the matrix on a ground steel plate. The MALDI-TOF mass data for Pcs are presented as the mass of the most intense peak in the cluster instead of exact mass. LC–MS was performed on a Waters ACQUITY UPLC system equipped with PDA and SQD2 electrospray MS detector. The parameters of operation were column: Thermo Accucore C18 (2.6 µm, 2.1 × 50 mm); column temp: 50 °C; flowrate: 0.6 mL/min;solvent A: 5mM NH4Ac in water; solvent B: 5mM NH4Ac in acetonitrile/water (95:5).

3.2. Computational Details

The starting geometries of Pz tCzZnPc1 were optimized using CAM-B3LYP/LANL2DZ [31,32] for all atoms. Frequency calculation was used to confirm the energy minima in optimized geometry. Chloroform was used as a solvent in all of the single point DFT–PCM and TDDFT–DCM calculations were performed using the polarizable continuum model (PCM) to study the solvation effects [34]. The first 100 excited states of each compound were calculated in all TDDFT–PCM calculations. All DFT calculations were conducted using the Gaussian 09 software package [35], and the GaussView program [36] was used for the molecular orbital analysis.

3.3. Synthesis

Compounds 4,5-bis(3,6-di-tert-butyl-9H-carbazol-9-yl)phthalonitrile (1) and 4-(hydroxymethyl)phthalonitrile (2), [37] have been prepared according to published procedures.
Tri-tert-butylcarbazolyl-hydroxymethylphthalocyaninatozinc(II) (3): A mixture of 4,5-bis(3,6-di-tert-butyl-9H-carbazol-9-yl)phthalonitrile (1) (737 mg, 4 mmol), 4-hydroxymethylphthalonitrile (2) [37] (158 mg, 1 mmol) and Zn(AcO)2 (330 mg, 1.5 mmol) in DMAE (4 mL) was refluxed during 24 h. The solvent was evaporated under reduced pressure, and the crude product was purified by column chromatography (SiO2, ethyl acetate/cyclohexane 9:1) to afford 3 as a deep green solid (130 mg, 14%); m.p. > 300 °C; 1H NMR (600 MHz, DMSO-d6) δ = 9.82 (d, 6H), 9.82 (s, 1H), 9.43 (d, 2H), 8.58 (s, 1H), 7.96–7.79 (m, 12H), 7.39–7.30 (m, 12H), 7.13–7.05 (m, 12H), 6.07 (bs, 3H), 1.37–1.30 (brs, 108H). 1H NMR (600 MHz, benzene-d6) δ = 10.37 (s, 1H), 10.25–10.18 (b, 6H), 9.46 (bs, 2H), 7.98–7.84 (m, 12H), 7.45–7.06 (m, 24), 4.69 (s, 3H), 0.91-0.29 (brs, 108H). 13C NMR (100 MHz, DMSO-d6) δ = 168.4, 143.3, 139.1, 138.2, 137.8, 132.8, 127.4, 124.0, 123.8, 123.4, 123.2, 109.5, 31.7, 31.6 ppm. UV-Vis (THF) λmax (nm) (log ε (dm3 mol−1 cm−1)): 707 (5.5), 350 (5.1). MS (MALDI-TOF, DHB on ground steel plate): m/z: 2272.56.
Tri-tert-butylcarbazolyl-carboxylphthalocyaninatozinc(II) (tCzZnPc1): Zinc oxide (0.4 mg, 0.004 mmol) and potassium hydroxide (2.8 mg, 0,04 mmol) were placed in an oven-dried tube, which was placed in a Radley carousel. The tube was subjected to vacuum and then filled with nitrogen gas (repeated three times). Vacuum was applied again, and the carousel heated to 170 °C for 1 h. Subsequently, the tube was refilled with nitrogen gas. Anhydrous and degassed mesitylene (2 mL) was added and the mixture heated to reflux. 3 (0.02 mmol, 40 mg) that previously was dissolved in degassed mesitylene (1 mL) was added dropwise by syringe, and the reaction was refluxed with stirring under a flow of nitrogen for 24 h. The mixture was cooled down to room temperature and the mesitylene was evaporated under vacuum. The precipitate was acidified with 16% aqueous hydrochloric acid. The aqueous layer was extracted with ethyl acetate (3 × 5 mL). The combined organic layers were dried over sodium sulfate and concentrated in vacuum to give tCzZnPc1 as a pure compound (36 mg, 92%). m.p. > 300 °C; 1H NMR (400 MHz, DMSO-d6) δ = 11.72 (s, 1H), 7.96–7.76 (m, 12H), 7.32–6.92 (m, 33H), 1.30 (brs, 109H). 13C NMR (100 MHz, DMSO-d6) δ = 168.4, 143.3, 139.1, 138.2, 137.8, 132.8, 127.4, 124.0, 123.8, 123.4, 123.2, 109.5, 34.7, 32.1 ppm. UV-Vis (THF) λmax (nm) (log ε(dm3 mol−1 cm−1)): 707 (3.7), 355 (4.5 sh). MS (MALDI-TOF, DHB on ground steel plate): m/z: 2285.74.

3.4. Photovoltaics

The devices reported in this paper were prepared using the following procedure. TiO2 thin films with specific thickness and a total area of 0.36 cm2 were screen printed in Solaronix (Switzerland) using a TiO2 nanoparticles paste (Ti-nanoxide HT/SP). The “opaque solar cells” are based on a 13µm-thick mesoporous TiO2 layer with an additional 4 µm-thick scattering (Solaronix, Ti-Nanoxide R/SP) whereas the “transparent solar cells” contain only the 13 µm-thick mesoporous TiO2 layer. The electrodes are cleaned with absolute ethanol beforehand and dried under an argon flow. The photoanodes are then treated by immersion into a freshly prepared 4.1 mmol·L−1 TiO2 aqueous suspension at 70 °C for 20 min. The electrodes are then cooled down to room temperature, rinsed with distilled water followed by absolute ethanol, and then drying under an argon flux. The electrodes are then sintered under air at 500 °C for 20 min. The photoanodes are then cooled down to 80 °C and sensitized through immersion in the dyeing solution for 16 h at room temperature with varying dye concentration of tCzZnPc1 = 0.2 and 0.5 mM, with/without CDCA co-adsorption, due to the bulkiness of our dye, in CHCl3/EtOH 1/1, v/v. The CDCA coadsorption was done with the dye: CDCA ratio of 1:5. The drilled counter electrodes are coated with a thin layer of platisol (Solaronix, Switzerland) and charred under air at 500 °C using the same heating procedure as described above. The sensitized photoanode is rinsed with dichloromethane, absolute ethanol, and dried under an argon flux. Both electrodes are then sandwiched together using a suryln thermogluing polymer (60 µm thick) using a heating press at 105 °C for 16 s. The cell is then filled with an electrolyte (Solaronix Iodolyte HI-30) via the pre-drilled hole using a vacuum pump. The electrolyte injection hole on the counter electrode is then sealed with the aid of a surlyn underneath the thin glass cover using heat. Lastly, contact along the cell edges is created.
Before measurements, the AM1.5G simulator was calibrated using a reference silicon photodiode equipped with an IR-cutoff filter (KG-3, Schott). The current–voltage characteristics of the cells were measured under dark and under AM 1.5G (1000 W m−2) irradiation condition, achieved by applying an external potential bias to the cell while measuring the generated photocurrent with a Keithley model 2400 digital source meter (Beaverton, OR, USA). The devices were masked prior to measurements to attain an illuminated active area of 0.36 cm2.

4. Conclusions

An asymmetrical, push–pull phthalocyanine bearing six bulky tert-butylcarbazolyl electron donor units and a carboxylic acid anchoring group were synthetized and tested as photosensitizer in dye-sensitized solar cells (DSSC). DFT and electrochemical studies indicate that the electronic distribution in the dye is appropriate for electron injection into the titanium dioxide. The new dye has been used as photosensitizer in transparent and opaque dye-sensitized solar cells, which exhibit poor efficiencies related to a low Jsc. These preliminary results indicate that the introduction of bulky carbazolyl substituents is a good strategy to reduce the dye aggregation but its low absorption in the visible range and the low amount of dyes attached on the TiO2 surface may explain the poor photovoltaic parameters.

Supplementary Materials

The following are available online at https://www.mdpi.com/1420-3049/25/7/1692/s1, Mass spectra: Figures S1 and S2; NMR spectrum: Figure S3; Absorption and Emission spectra: Figures S4 to S13; Electrochemical data: Figures S14 to S18.

Author Contributions

B.G. and K.A. synthesized and characterized the materials; V.M.M. performed the photovoltaic measurements; E.F.E. and A.S.A.Y. contributed to the methodology; R.D., T.T., and S.M. designed the work and coordinated the research and, together with B.G., they wrote the manuscript; all authors contributed to and commented on the manuscript. All authors have read and agreed to the published version of the manuscript.

Funding

This work was financially supported by the Kuwait Foundation for the Advancement of Science (Grant Number PN18-12-SC01) and the RSP unit general facilities of the Faculty of Science GFS (GS 01/01, GS 03/01, GS 01/03, GS 01/05, and GS 02/13) (S.M.). T.T. thanks MINECO (project CTQ2017-85393-P) and ERA-NET/European Commission/MINECO, (UNIQUE, SOLAR-ERA.NET Cofund 2 N° 008/PCI2019-111889-2). R.D. acknowledges ANR for funding through ODYCE project. (Grant agreement No ANR-14-OHRI-0003-01). RD thanks European Research Council (ERC) for funding. This project has received funding from the European Union’s Horizon 2020 research and innovation program (grant agreement No 832606)—Project PISCO.

Acknowledgments

T.T. thanks Victor Mariñas for experimental help related to UV–Visible and Cyclic Voltammetry measurements. V.M.M. thanks the French Embassy in Kenya through Campus France for a scholarship grant. S.M. thanks the Chemistry Department for using MALDI-TOF.

Conflicts of Interest

The authors declare no conflict of interest.

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Sample Availability: Samples of the compounds are not available from the authors.
Molecules 25 01692 sch001 550
Scheme 1. Synthetic route to peripherally substituted A3B tCz-ZnPc with carboxylic anchoring group (i) Zn(AcO)2, DMAE, reflux (ii) ZnO, KOH, mesitylene, reflux.
Scheme 1. Synthetic route to peripherally substituted A3B tCz-ZnPc with carboxylic anchoring group (i) Zn(AcO)2, DMAE, reflux (ii) ZnO, KOH, mesitylene, reflux.
Molecules 25 01692 sch001
Molecules 25 01692 g001 550
Figure 1. 1H NMR spectrum for A3B tCzZnPc1 (in DMSO-d6).
Figure 1. 1H NMR spectrum for A3B tCzZnPc1 (in DMSO-d6).
Molecules 25 01692 g001
Molecules 25 01692 g002 550
Figure 2. The Gouterman’s molecular orbitals of tCzZnPc1 calculated at CAM-B3LYP/LANL2DZ level of theory, and the calculated values of HOMO and LUMO energy levels in a vacuum and in CHCl3.
Figure 2. The Gouterman’s molecular orbitals of tCzZnPc1 calculated at CAM-B3LYP/LANL2DZ level of theory, and the calculated values of HOMO and LUMO energy levels in a vacuum and in CHCl3.
Molecules 25 01692 g002
Molecules 25 01692 g003 550
Figure 3. (a) Energy band diagram of the DSSC fabricated in this work. (b) Current–voltage curves of an opaque tCzZnPc1-based device recorded in the dark (black line) and under irradiation (red line) under AM 1.5G (1000 W·m−2) irradiation condition.
Figure 3. (a) Energy band diagram of the DSSC fabricated in this work. (b) Current–voltage curves of an opaque tCzZnPc1-based device recorded in the dark (black line) and under irradiation (red line) under AM 1.5G (1000 W·m−2) irradiation condition.
Molecules 25 01692 g003
Molecules 25 01692 g004 550
Figure 4. (a) Absorption in solution tCzZnPc1 (THF, 25 °C, 10−5 M), and (b) after adsorption on a 4µm-thick transparent TiO2 mesoporous electrode.
Figure 4. (a) Absorption in solution tCzZnPc1 (THF, 25 °C, 10−5 M), and (b) after adsorption on a 4µm-thick transparent TiO2 mesoporous electrode.
Molecules 25 01692 g004
Table
Table 1. Photovoltaic parameters of the best solar cells and mean values over 3 cells (in parenthesis).
Table 1. Photovoltaic parameters of the best solar cells and mean values over 3 cells (in parenthesis).
DyeCellsJSC (mA·cm−2)VOC (V)FF (%)PCE (%)
tCzZnPc1Opaque1.05 (0.98)0.54 (0.54)70.8 (69.8)0.40 (0.37)
tCzZnPc1Transparent0.91 (0.77)0.54 (0.51)71.7 (73.3)0.35 (0.29)

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MDPI and ACS Style

Ghazal, B.; Azizi, K.; Ewies, E.F.; Youssef, A.S.A.; Mwalukuku, V.M.; Demadrille, R.; Torres, T.; Makhseed, S. Push–Pull Zinc Phthalocyanine Bearing Hexa-Tertiary Substituted Carbazolyl Donor Groups for Dye-Sensitized Solar Cells. Molecules 2020, 25, 1692. https://doi.org/10.3390/molecules25071692

AMA Style

Ghazal B, Azizi K, Ewies EF, Youssef ASA, Mwalukuku VM, Demadrille R, Torres T, Makhseed S. Push–Pull Zinc Phthalocyanine Bearing Hexa-Tertiary Substituted Carbazolyl Donor Groups for Dye-Sensitized Solar Cells. Molecules. 2020; 25(7):1692. https://doi.org/10.3390/molecules25071692

Chicago/Turabian Style

Ghazal, Basma, Kobra Azizi, Ewies F. Ewies, Ahmed S. A. Youssef, Valid Mwatati Mwalukuku, Renaud Demadrille, Tomás Torres, and Saad Makhseed. 2020. "Push–Pull Zinc Phthalocyanine Bearing Hexa-Tertiary Substituted Carbazolyl Donor Groups for Dye-Sensitized Solar Cells" Molecules 25, no. 7: 1692. https://doi.org/10.3390/molecules25071692

APA Style

Ghazal, B., Azizi, K., Ewies, E. F., Youssef, A. S. A., Mwalukuku, V. M., Demadrille, R., Torres, T., & Makhseed, S. (2020). Push–Pull Zinc Phthalocyanine Bearing Hexa-Tertiary Substituted Carbazolyl Donor Groups for Dye-Sensitized Solar Cells. Molecules, 25(7), 1692. https://doi.org/10.3390/molecules25071692

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