José-María
Andrés Castán
*a,
Valid Mwatati
Mwalukuku
a,
Antonio J.
Riquelme
b,
Johan
Liotier
a,
Quentin
Huaulmé
a,
Juan A.
Anta
b,
Pascale
Maldivi
a and
Renaud
Demadrille
*a
aUniv. Grenoble Alpes, CEA, CNRS, IRIG-SyMMES, 38000 Grenoble, France. E-mail: renaud.demadrille@cea.fr
bDepartment of Physical, Chemical and Natural Systems, Universidad Pablo de Olavide, Carretera de Utrera km 1, Sevilla 41013, Spain
First published on 8th August 2022
Photochromic dyes possess unique properties that can be exploited in different domains, including optics, biomedicine and optoelectronics. Herein, we explore the potential of photochromic spiro-indoline naphthoxazine (SINO) and naphthopyran (NIPS) for application in photovoltaics. We designed and synthesized four new photosensitizers with a donor–pi–acceptor structure embedding SINO and NIPS units as photochromic cores. Their optical, photochromic and acidochromic properties were thoroughly studied to establish structure–properties relationships. Then, after unravelling the possible forms adopted depending on the stimuli, their photovoltaic properties were evaluated in DSSCs. Although the photochromic behavior is not always preserved, we elucidate the interplay between photochromic, acidochromic and photovoltaic properties and we demonstrate that these dyes can act as photosensitizers in DSSCs. We report a maximum power conversion efficiency of 2.7% with a NIPS-based dye, a tenfold improvement in comparison to previous works on similar class of compounds. This work opens new perspectives of developments for SINO and NIPS in optical and photovoltaic devices, and it provides novel research directions to design photochromic materials with improved characteristics.
However, these compounds could be particularly interesting for the design of semi-transparent devices because their reversible transformation between the two forms with different absorption would allow obtaining solar cells whose transparency could be modulated according to the light intensity.20 Such a property would be particularly appreciable in Building Integrated Photovoltaics (BIPV).21,22 Nevertheless, very few photochromes have been tested in photovoltaic devices. In 2015, a bis-thienylethene derivative was first used in dye-sensitized solar cells (DSSCs).23 For this type of molecules, the interconversion between the different photo-isomers is only possible by alternating ultraviolet and visible light irradiations. In addition, the colored isomer led to a poorer power conversion efficiency (PCE).
Photochromic dyes from the spirobenzopyran and spirobenzo and naphthoxazine families were also tested in DSSCs.24 Here again the isomerization process required intense ultraviolet irradiation and the molecules did not lead to the reversible optical properties expected within the device. Besides the fact that they were not stable, their photovoltaic performances were extremely low with PCEs below 0.1%. The low performance of these molecules can be explained by an unsuitable molecular design for this application. Indeed, in most of these systems, the anchor function was not conjugated with the photochromic core, which resulted in poor charge injection into the photoelectrode.
We have recently demonstrated that naphthopyran-based derivatives, when properly designed, show a high potential in semitransparent DSSCs.20 Push–pull photochromic naphthopyrans can sensitize efficiently TiO2-based mesoporous electrodes while keeping their reversible photochromic behavior after integration in complete devices. The resulting smart solar cells can generate electricity and self-adapt themselves depending on the light intensity in order to be more transparent under low light intensity.
In this work, we propose a new strategy for designing spiro-indoline naphthoxazine (SINO) and spiro-indoline naphthopyran (NIPS) dyes with the goal to explore their potential for solar cells. These two families of photochromic dyes are well known for their excellent switching kinetics and good resistance to photodegradation.25 As with diphenyl-naphthopyrans, the mechanism of the photochromic reaction of SINO and NIPS involves the cleavage and reformation of the carbon-oxygen single bond of the oxazine or pyran rings, respectively, as shown in Scheme 1. In the previous work on this type of dyes, the spiro-indoline benzopyran (BIPS) sensitizer carried the carboxylic anchor away from the conjugated system and its SINO counterpart did not even have a suitable anchoring function, leading to extremely poor performances in solar cells.24 For this reason, we designed two SINO and two NIPS photosensitizers following a donor–π–acceptor (D–π–A) structure (Scheme 1). Then, we investigated their optical and photochromic properties with the goal to establish new structure–properties relationships for this class of molecules. Then we used these molecules as photosensitizers in DSSCs to compare their photovoltaic performances.
Therefore, we carried out the synthesis of four derivatives: SINO-1, SINO-2, NIPS-1 and NIPS-2, whose structures and synthesis are depicted in Schemes 2 and 3. In the case of the SINO dyes, the 4-bromo-1-nitrosonaphthalen-2-ol precursor 1 was obtained from 4-bromonaphthalen-2-ol via direct nitrosilation in acid medium28 and it was directly used in the subsequent step without further purification. In the case of 4-formyl-3-hydroxynaphthalen-1-yl trifluoromethanesulfonate required for the synthesis of the NIPS derivatives, a less straightforward pathway was followed. First, naphthalene-1,3-diol was methylated in position 3 prior to introduce the triflate group in position 1.29 The carbonyl group was then introduced in position 4 through a Rieche formylation and eventually the alcohol was deprotected in the presence of boron tribromide to obtain the naphthol 5. On the other hand, to prepare the donating block 6, the Fischer's base was first brominated according to previously reported conditions30 and then the diphenylamine moiety was introduced through a Buchwald-Hartwig amination.
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Scheme 2 Synthetic pathway followed to obtain precursors 1, 5 and 6. DIPEA: N,N-diisopropylethylamine; Tf: trifluoromethylsulfonyl, dba: benzylideneacetone. |
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Scheme 3 Synthetic pathway used to obtain the new dyes SINO-1, SINO-2, NIPS-1 and NIPS-2. dppf: (diphenylphosphino)ferrocene. |
The condensations between the Fischer's bases and the naphthol derivatives were carried out in ethanol or toluene for the NIPS and SINO derivatives respectively to obtain intermediates 7–10 (Scheme 3). Finally, and in view of the lack of stability of the photochromes in the conditions used in the Knoevenagel condensations, the anchoring functions were directly introduced in the Suzuki coupling together with the phenyl spacer, for either the benzoic or the 2-cyano-3-phenylacrylic acceptors. This procedure, which is a deviation from the conventional synthetic way of introducing the anchoring functions, allowed obtaining the target molecules in a straightforward manner with overall yields between 5% and 18%.
Dye | λ max Tol CF (nm) | λ max Tol MC (nm) | λ max Tol MCH (nm) | λ max THF CF (nm) | λ max THF MC (nm) | λ max THF MCH (nm) | λ max DMF CF (nm) | λ max DMF MC (nm) | λ max DMF MCH (nm) |
---|---|---|---|---|---|---|---|---|---|
SINO-1 | 329 | 605 | 556 | 329 | 608 | 593 | 328 | 615 | 541 |
SINO-2 | 310 | 652 | 604 | 305 | 658 | 601 | 302 | 654 | 585 |
NIPS-1 | 367 | 569 | 499 | 325 | — | 512 | 325 | 579 | 488 |
NIPS-2 | 306 | — | 582 | 304 | — | 563 | 300 | — | 555 |
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Fig. 1 UV-vis absorption spectra of (a) SINO-1, (b) SINO-2, (c) NIPS-1 and (d) NIPS-2 in 2 × 10−5 M DMF solutions at 25 °C in the dark and under light using a 200–600 nm/200 W xenon lamp. |
In good agreement with different examples in the literature, both SINO derivatives exhibit a photochromic behavior upon irradiation. In these conditions, the ICT band of the open-form isomers emerges above 600 nm, slightly redshifted in the case of SINO-2. This effect is consistent with the higher push–pull effect induced by the two substituents. Compared to SINO compounds, their NIPS counterparts exhibited a limited photochromic behavior, a phenomenon that has been already reported for this type of derivatives.33 However, a slight band at ca. 570 nm could be observed under illumination in the case of NIPS-1, in both toluene and DMF, but surprisingly this compound was not photochromic when studied in THF. To the contrary, NIPS-2 does not show photochromic properties in any of the solvents. For SINO-1, SINO-2 and NIPS-1, it is noteworthy that the maxima of the absorption bands do not change much from one solvent to the other for either the CF or MC forms. It is also important to note that the three photochromic dyes can be colored with exposure to polychromatic light, an important aspect for the targeted application. Then, we investigated the thermal discoloration kinetics of the new compounds. Once the photostationary state (PSS) was reached under illumination (after circa 60 s), the irradiation source was turned off and the obtained discoloration curves were then modelled through the following equations with single and double exponentials respectively depending on the obtained experimental results:
The photochromic SINO derivatives showed extremely fast bleaching kinetics and the discoloration was even faster for NIPS-1. In all cases, no persistent colored isomers are formed after exposure to light (Table 2, Fig. 2 and Fig. S28, ESI†) and the solutions are fully decolored in less than 10 s for the SINO dyes and less than 1 s for the photochromic NIPS dye. However, they are more than 100 times faster compared to those of the best performing naphthopyran photochromic dyes in DSSCs, which make these molecules particularly appealing for application in semitransparent solar cells with dynamic optical properties. These values are in good accordance with the ones reported for unsubstituted SINO and NIPS.25 It is also noticeable that in every case a mono-exponential decay was obtained except for SINO-2, which exhibits the slowest kinetics and a bi-exponential decay in toluene likely due to the formation of different isomers.
Dye | k (s−1) Toluene | k (s−1) THF | k (s−1) DMF |
---|---|---|---|
SINO-1 | 0.59 | 1.2 | 0.77 |
SINO-2 | 0.58; 3.8 × 10−2* | 0.83 | 0.51 |
NIPS-1 | 28 | — | 8.1 |
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Fig. 2 Normalized discoloration curves of SINO-1, SINO-2 and NIPS-1, example given in DMF in 2 × 10−5 M solutions at 25 °C in the dark after irradiation 60 s with a 200–600 nm/200 W xenon lamp. |
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Scheme 4 Interconversion between the close (CF) and open protonated forms (MCH) of SINO (X = N) and NIPS (X = CH) derivatives in the presence of strong acids. |
We found that the four new derivatives revealed acidochromic properties in absence of light. In order to study the interaction between protons and our new SINO and NIPS molecules, a titration with HCl was carried out in THF in the dark (Fig. 3). It can be observed that the increase in the absorption of the band related to the MCH form when HCl is added. In addition, a sole isosbestic point was monitored in every case, suggesting that the protonation gives rise to a single compound, namely the MCH form.37,38 It appears from the spectra presented in Fig. 3 that the SINO compounds are less sensitive to acidic conditions compared to their NIPS analogs, as only a small fraction of the molecules undergoes the protonation reaction. For SINO-1, SINO-2 and NIPS-1, the absorption band of the MCH form in the visible is blue-shifted compared to the MC. The shifts varied between 15 and 70 nm for the SINO derivatives and from 70 to 90 nm for NIPS-1 depending on the solvent. In contrast to the CF and MC forms, the maxima of the bands associated with the MCH form are shifted depending on the solvent used due to its charged nature,39 although it does not follow a specific trend. This indicates that only MCH are subjected to solvatochromism. In addition, the acidochromism was found to greatly depend on the strength of the acid used. This observation confirms the results reported for the BIPS family.40 The acidochromic effect is observed when strong acids that can protonate the MC form are used. For instance, in the case of NIPS-1, the colored form was observed when acids with pKa below 0.5 were employed (i.e. nitric, sulfuric, hydrochloric and perchloric acids) but not in the case of “weaker” acids (i.e. trifluoroacetic, phosphoric or acetic acids) (Fig. S29, ESI†). Our experiments show that the nature of the acid plays a critical role on the protonation and the formation of the MCH. Further experiments are required to elucidate the exact role of the counter ions on the acidochromic properties of these dyes.
More interestingly, in stark contrast to the SINO compounds, the MCH forms of the NIPS exhibit a negative photochromic behavior.41 According to the literature of spiro-indoline benzopyrans, this process implies an E–Z isomerization followed by the deprotonation and the consequent ring closure.42
Although the effect is not intense in the case of NIPS-2, NIPS-1 reverts to its initial state under illumination and it is able to reopen quite rapidly in the dark (with a k of circa 2.6 × 10−2 s−1) (Fig. 4). The high reversibility of this process in THF has to be highlighted, as NIPS-1 bleaches almost quantitatively under illumination even reaching the same level of coloration in the dark showing no sign of photodegradation. Though this effect has been observed in the case of some spiro-indoline benzopyran derivatives,43 to the best of our knowledge, it has not been reported for NIPS compounds. It should also be noted that this negative photochromism observed in solution when acidic conditions and light are combined could be modulated by changing the solvent and the nature of the acid (see Fig. 4).
To conclude this section, it seems that the molecules once incorporated in a device in the presence of a liquid electrolyte, will be able to exist in multiple forms: either in a closed form, an open form of MC type but also in an open MCH form after protonation. For this reason, it is important to verify if the different possible forms of these molecules present energy levels appropriately positioned for an efficient sensitization of the oxide and an efficient regeneration by the redox mediator that we have chosen, namely the I3−/I− couple.44 The energy levels of the dyes are discussed in the next section.
Apart from the energy levels, the spatial distribution of the frontier orbitals is also a critical parameter because the efficiency of the injection and regeneration processes will strongly depend on it. Even though in all the CF the HOMO is localized on the donor and the LUMO on the acceptor showing a suitable electron distribution along the molecules, it is not the case for all the open forms. In the case of NIPS-1 and SINO-1, the HOMO and LUMO distributions of either the MC or MCH lie basically in the same region, i.e. the photochromic core, thus probably hampering the injection of electrons into the conduction band of the TiO2 electrode. However, though for the MC form of NIPS-2 and SINO-2 there is clearly a suitable spatial distribution between the donor and the acceptor for a charge transfer effect, we observe again the LUMO contribution in the central part of the molecule for their MCH forms, which may hinder the electron injection as well.
Dye | Electrolyte | J sc (mA cm−2) | V oc (V) | FF (%) | PCE (%) |
---|---|---|---|---|---|
SINO-1 | Homemade | 1.14 (1.09) | 0.31 (0.28) | 68 (67) | 0.24 (0.20) |
Iodolyte | 0.76 (0.76) | 0.54 (0.54) | 79 (78) | 0.32 (0.32) | |
SINO-2 | Homemade | 2.62 (2.53) | 0.31 (0.31) | 64 (64) | 0.51 (0.50) |
Iodolyte | 1.74 (1.70) | 0.53 (0.53) | 72 (72) | 0.66 (0.65) | |
NIPS-1 | Homemade | 1.94 (1.76) | 0.41 (0.38) | 66 (64) | 0.52 (0.42) |
Iodolyte | 0.92 (0.90) | 0.53 (0.52) | 77 (75) | 0.38 (0.35) | |
NIPS-2 | Homemade | 3.16 (3.14) | 0.40 (0.40) | 74 (74) | 0.94 (0.94) |
Iodolyte | 5.39 (5.11) | 0.64 (0.65) | 78 (80) | 2.73 (2.62) |
Referring to theoretical calculations in previous section, in the SINO series the formation of the MCH strongly decreases the ability to inject electrons into the conduction band of TiO2. Indeed, the LUMO level is lowered, thus reducing the driving force, and its spatial localization is quite far from the anchor group, not allowing a correct sensitization of the TiO2. This explains the poorer performance of SINO compared to their NIPS counterparts. The same problems appear with the NIPS compounds, but in that case, the LUMO energy level of the MCH is higher giving rise to a slightly higher driving force towards the injection. In contrast, when the commercial Iodolyte was used, the level of staining was considerably lower (Fig. 6). This is explained by its pH around 7, which allows the closed form to be present in the absence of illumination. In this case, the photochromic behavior is preserved for the molecules that were already demonstrated photochromic in solution, i.e. the two SINO derivatives and NIPS-1. In addition, Iodolyte contains additives such as tert-butylpyridine that is known to shift the TiO2 conduction band upwards thus increasing the Voc. However, in spite of all that, the overall performances of the three photochromes remain in the same range. According to theoretical calculations, the spatial distribution of the LUMO that delocalizes to the core of the molecule on the MC forms may explain this result for SINO-1 and NIPS-1. Surprisingly, in the case of NIPS-2, despite its lack of photochromic behavior and thus an absence of open MC form absorbing in the visible, a better current density was recorded contrarily to the other sensitizers. NIPS-2 demonstrates a Jsc higher than 5 mA cm−2 and a Voc over 0.6 V, thus leading to the highest PCE ever reported for this family of molecules: 2.73%. In addition, these devices are relatively stable as they are able to maintain their Voc after ca. 5000 h under ISOS-D1 ageing test45 though the Jsc is substantially reduced, resulting in an efficiency loss of 47% (Fig. S34, ESI†).
The lack of coloration of this device may indicate that most of NIPS-2 stays in its CF. To confirm the contribution of each form in NIPS-2/Iodolyte-based devices, the absorption patterns of 2 μm transparent devices made of both electrolytes were recorded (Fig. 7). It is noteworthy that when the homebased electrolyte is used, an intense absorption band appears in the visible corresponding to the formation of MCH, whereas with Iodolyte the device shows the typical yellow color of the Iodine based electrolyte and the absorption spectrum remains flat in the visible. In addition, as it can be observed in the incident photon to current efficiency (IPCE) spectrum of the 13 μm device composed of the homemade electrolyte (Fig. S35, ESI†), in spite of the great coloration, the injection of electrons related to the MCH form is negligible, in good agreement with the results provided by the theoretical calculations. This also demonstrates that the main contributor to the photogeneration is indeed the CF, favored by the good spatial distribution of its LUMO orbital. Then, to understand the electrolyte-driven behavior of the devices presented in Fig. 6 and Table 3, an electrochemical impedance investigation was carried out on the DSSCs made of the best performing dye, NIPS-2, and both electrolyte compositions. Charge transfer resistances were measured (see Fig. 8).
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Fig. 7 UV-Vis spectra and pictures of the respective devices of NIPS-2-based DSSCs on 2 μm transparent TiO2 electrodes using Iodolyte and our homebased electrolyte in the absence of illumination. |
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Fig. 8 Charge transfer resistances comparisons at the same quasi-Fermi level of 13 μm DSSCs made of NIPS-2 and both electrolytes (a) in the dark and (b) under operating conditions. |
The main arc of the impedance spectra (see Fig. S36a and b, ESI†) was fit to a single –RC– equivalent circuit element where the resistance is considered the charge transfer resistance (dark) or recombination resistance (RCT) and the capacitance is the chemical capacitance (Cμ). Both parameters are known to show an exponential voltage dependence following eqn (S1), (S2) and (Fig. S36c–f) (ESI†).46,47 The extracted α and β for the NIPS-2 DSSC using Iodolyte and the homebased electrolyte at dark conditions and under illumination are collected in Table S1 (ESI†). Typical values for α and β values normally reported for DSSCs are in the range of 0.15–0.35 for α and 0.5–0.8 for β.48–51 While the α parameter, which shows the average depth of the traps, remained within the range typical for a DSSC configuration irrespective of the redox couple used, β varied depending on the electrolyte.
When Iodolyte was employed, this parameter changed from 0.56 to 0.73 between the irradiation conditions but still within the DSSC typical values. However, when our homebased electrolyte was used in turn, β changed from 0.75 in the dark to 1.04 under operating conditions, which suggests a possible change in the dominant recombination pathway, which normally in DSSCs correspond to triiodide reduction.52,53 Whatever the redox couple, no TiO2 conducting band shift was induced at irradiation conditions (Fig. S36, ESI†). However, as it can be observed in Fig. S37 (ESI†), the change of the electrolyte induces a bandshift of +226 mV and +220 mV with Iodolyte under dark and white light irradiations, respectively, explaining the higher photovoltage observed in the reported JV curves. The Nyquists plots under irradiation, in which the size of the real part of the recombination arc is approximately equal to the recombination resistance, were compared applying a voltage correction to account for the bandshift, ensuring that both measurements were done at a similar electron concentration at the quasi-Fermi level (Fig. S38, ESI†). The diameter is larger in homebased electrolyte-based cells despite the high I2 concentration and the lower Voc therein. Certainly, the acidic homemade electrolyte gives rise to the protonated merocyanine form facilitating the interaction of the positively charged center with I3− hence lowering its local concentration at the photoanode compared to Iodolyte. This can also explain the change observed in the β values compared to the range usually reported for DSSCs.
Eventually, in an attempt to obtain the most performing semi-transparent device with the couple NIPS-2/Iodolyte, DSSCs were fabricated using a transparent 13 μm TiO2 anode (Fig. 9). On such thick electrodes, the coloration is more pronounced due to the formation of the MCH form with the remaining traces of acid, thus leading to slightly greenish electrodes. Despite of that, a PCE of 2.18% was then recorded while keeping the AVT at 52%, mostly absorbing below 500 nm, demonstrating once again that the majority of the molecules is in its CF as the transmittance at longer wavelengths is always kept above 50%. This corresponds to a light utilization efficiency (LUE) of 1.13. Then, to determine the aesthetic quality of the semi-transparent devices, the Commission Internationale de l’Eclairage (CIE) color coordinates were determined, as well as the color rendering index (CRI), which revealed an acceptable value of 80.4% (Fig. S39, ESI†).54,55 Therefore, despite its lack of photochromic behavior, this result shows that this type of dyes can be used in semi-transparent DSSCs. Eventually, though modest, they remain as the best results for SINO and NIPS derivatives in the literature.
These studies allow us to rationalize the behavior of these molecules when they are incorporated in solar cells. We demonstrate that the choice of the electrolyte is crucial as it drives the optical behavior of these compounds. The use of an acidic electrolyte suppresses the photochromic behavior in device whereas with a neutral pH electrolyte, the photochromic behavior is preserved. Although the photochromic behavior is not preserved in all devices with these dyes, these results show that they can be used in DSSCs. The results remain modest with a maximum PCE of 2.7%, but they are significantly improved compared to previous reports on spiropyran and spiroxazine derivatives in the literature. Eventually, the best performing dye, NIPS-2, despite its lack of photochromism, allowed obtaining a PCE of 2.7% in opaque solar cells and 2.2% in semi-transparent ones while showing an AVT at 52%.
This study is the first to investigate in details the complex relationships between photochromic, acidochromic and photovoltaic properties for these two families of dyes. The structure–property relationships that we establish in this study will undoubtedly be useful for the development of new photochromic compounds with optimized optoelectronic properties for applications in various fields, including photovoltaics.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2qm00375a |
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