Abstract
Molecular photosensitizers based on the anthranil core were synthesized through a six-step linear synthesis featuring a Suzuki coupling at the C7 position and a controlled C3–H arylation. The introduction of donor and acceptor groups allowed the synthesis of unsymmetrical photosensitizers that were then investigated, revealing different spectroscopic and optoelectronic properties. Transient spectroscopy of excited species indicated that placing the acceptor at C7 and the donor group at C3 altered the energy levels around the anthranil core, making these dyes attractive for photovoltaic applications.


With the energy demand rising every day, our society needs to focus on pursuing strategies to move away from fossil-based systems and promote low-carbon and renewable resources to produce energy, such as wind and solar. One of the most promising approaches to indoor powering utilities for converting light into electricity is dye-sensitized solar cells (DSSCs), which have reached a power conversion efficiency (PCE) of 15.2% thanks to optimized molecular photosensitizers. The three leading families of photosensitizers for DSSCs include Ru(II) polypyridyl complexes, Zn porphyrin derivatives, and metal-free organic dyes. Through careful design and synthesis, the properties of the organic photosensitizers can be tuned to obtain a high absorption coefficient and a broad spectral response to enhance the photovoltaic performance.
The chemical architecture of an organic photosensitizer involves an electron donor (D) group linked to an electron acceptor (A) moiety through a π-conjugated bridge (π). To date, the most popular π-conjugated linkers are chromophores, such as BODIPY, isoindigo, and porphyrins and N- and/or S-heterocycles, such as benzothiadiazole, quinoxaline, diketopyrrolopyrrole, and benzotriazole. Among them, electron-deficient benzo[c][2,1,3]thiadiazole 1 is one of the most widely studied units for DSSCs due to its capability to tune the energy bandgap to maximize the light absorption, allowing for record PCEs in cosensitized DSSCs. , Almost all of the benzothiadiazole-based molecules for DSSCs present a typical substitution pattern where the donor/acceptor (D/A) groups are at the 4 and 7 positions. Under this approach, Zhang et al. recently reported the synthesis of a simple D-π-A dye 2, the MS5 compound commercialized by Dyenamo, that enabled the fabrication of a cosensitized DSSC with a PCE of 13.5% and a V oc of 1.24 V (Figure ).
1.
Structures of benzo[c][2,1,3]thiadiazole 1 and commercial dye MS5 2.
The benzothiadiazole structure combines a five-membered ring containing N and S atoms and a benzene ring. Both rings possess different electron densities; however, the donor/acceptor groups can only be placed at the benzene ring, leading to a symmetrical substitution pattern at positions 4 and 7 such as in MS5.
After scouting different heterocycles, we identified a chemical entity that could be used as π-conjugated bridge in the synthesis of new photosensitizers, having a five-membered ring heterocycle that has a C–H bond available for further substitutions and is fused with a benzene ring.
Thus, we envisioned that the anthranil core 3 would be suitable to place one group (donor/acceptor) at the five-membered ring and the other group at the benzene ring (Figure ), preparing novel molecular photosensitizers with different charge transfer properties, e.g., by placing the donor group at the electron rich ring and the acceptor group at the electron poor ring, or vice versa.
2.

Frontier molecular orbitals for 1 and 3 according to density functional theory (DFT).
Anthranils (2,1-benzisoxazoles) were discovered in the 1960s, and they have been privileged scaffolds for medicinal chemistry and versatile building blocks for the synthesis of more complex structures. , However, to the best of our knowledge, they have not been used in materials science or in DSSCs. Compared with 1, the anthranil core 3 possesses similar HOMO–LUMO energy levels and a moderate electron density at the isoxazole ring that ensures its use as a π-conjugated bridge (Figure ). Moreover, from a synthetic point of view, the desired substitution in this skeleton involves the challenging formation of two C–C bonds, which motivated us to consider potential synthetic routes to functionalize the C3 and C7 positions at the anthranil core.
Our synthetic approach started with the synthesis of the corresponding bromo-substituted anthranil 5 (78%) through a reductive cyclization of commercial o-nitrobenzaldehyde 4 using SnCl2 as a reductive agent under smooth reaction conditions (Scheme ). Then, the reactive site at C7 in derivative 5 allowed us to select the Suzuki–Miyaura coupling as the second step in our synthetic plan over the C–H arylation reaction. In this order, we first introduce the corresponding donor/acceptor moiety at the C7 position using the synthetic boronic ester 6 to insert the triphenylamine core as a donor group and give the intermediate 7 in 85% yield, while with the commercial boronic acid 8 the intermediate with the benzoic acid–methyl ester moiety as the acceptor group was obtained in 75% yield (Scheme ).
1. Preparation of Anthranil Derivatives with the Donor (7) and Acceptor (9) Moieties at the C7 Position.
Considering the difficulty of accessing aryl diazonium tetrafluoroborates and the regioselectivity issues of the recently reported metal-free C–H arylation of anthranils, we decided to explore a Pd catalytic system, optimizing the reaction conditions for the selective C3-arylation on compound 5 by first using the commercial anthranil 5′ and 4-bromoanisole 10′ as model substrates (Table ). We successfully obtained our desired product 11′ in 88% yield using Pd(OAc)2 as a catalyst and KOAc as the base and performing the reaction at 150 °C for 24 h in DMA as a solvent (entry 8, Table ).
1. Optimization of Reaction Conditions for the C–H Arylation Using Model Substrates 5′ and 10′ .
| Entry | Cat. (mol %) | Ligand (mol %) | Base (2 equiv) | Solvent (5 mL) | T (°C) | Time (h) | Yield (%) |
|---|---|---|---|---|---|---|---|
| 1 | Pd2dba3 (1) | K2CO3 | DMA | 150 | 24 | NR | |
| 2 | Pd2dba3 (1) | Cs2CO3 | DMA | 150 | 24 | NR | |
| 3 | PdCl2 (1) | PPh3 (1.5) | KOAc | DMA | 150 | 24 | 40 |
| 4 | Pd(PPh3)4 (1) | KOAc | DMA | 150 | 24 | 21 | |
| 5 | Pd2dba3 (1) | NaOtBu | DMA | 150 | 24 | 45 | |
| 6 | Pd2dba3 (1) | KOtBu | DMA | 150 | 24 | 40 | |
| 7 | Pd(OAc)2 (1) | P(t-Bu)3 (1.5) | KOAc | DMA | 150 | 24 | 32 |
| 8 | Pd(OAc)2 (1) | KOAc | DMA | 150 | 24 | 88 | |
| 9 | Pd(OAc)2 (1) | KOAc | DMF | 150 | 24 | 44 | |
| 10 | Pd(OAc)2 (1) | KOAc | DMA | 120 | 24 | 30 | |
| 11 | Pd(OAc)2 (1) | KOAc | DMA | 150 | 12 | 40 | |
| 12 | Pd(OAc)2 (10) | KOAc | DMA | 150 | 24 | 51 |
Reaction conditions on a 1 mmol scale: anthranil 5′ (1.5 equiv), bromoanisole 10′ (1 equiv), base (2 equiv), solvent (5 mL), temperature, and time.
Isolated yields.
NR: No Reaction.
11a′ was identified by GC-MS upon increasing the catalyst loading.
Subsequent modifications to the standard conditions revealed that palladium catalysts such as Pd2dba3, PdCl2, and Pd(PPh3)4, combined with common phosphine ligands like PPh3 and P(t-Bu)3, did not lead to yields of the desired product over 40%. Furthermore, the use of bases such as K2CO3, Cs2CO3, NaOtBu, and KOtBu to promote the abstraction of the C–H bond at C3 was ineffective in comparison to KOAc.
Regarding the solvent, DMA was chosen in the first place as an aprotic and high-boiling-point reaction media to perform the experiments described in Table . Attempts to change to DMF decreased the yield of 11′ to 44% under the same conditions: catalyst, base and temperature (entry 9, Table ).
A decrease in the reaction temperature (120 °C) or reaction time (12 h) dramatically decreased the reaction yields compared to the standard conditions. Finally, increasing the catalyst loading (10 mol %) favored the in situ ring opening of the starting anthranil, forming byproducts derived from nitrene and ketene intermediates.
With the optimized reaction conditions, we applied this protocol to couple the donor substrate 7 with the commercial ethyl 4-bromobenzoate 10, obtaining the D-anthranil-A intermediate 11 in an excellent yield (88%) due to the enriched electron density over the anthranil core given by the attached triphenylamine group present at the C7 position of substrate 7 (Scheme ).
2. C3-Arylation on the Donor Anthranil Core 7 to give the D-Anthranil-A intermediate 11 .
On the other hand, when the same protocol for the C3 arylation was applied to substrate 9 with the commercial 4-bromo-N,N-diphenylaniline 12, which resulted in a moderate yield of desired A-anthranil-D intermediate 13 (70%) due to the formation of a byproduct 13′ in considerable amounts (27%). In this case, the formation of the side product was promoted by the presence of the acceptor benzoate moiety at the C7 position of anthranil 9, reducing the reactivity of the C3–H bond and favoring the ring opening of the five-membered ring of the anthranil to give the corresponding aldehyde 13′ (Scheme ).
3. C3-Arylation on the Aceptor Anthranil Core 9 to give the D–Anthranil–A Intermediate 13 and the Byproduct 13′ .
The final steps of our synthetic approach for the synthesis of the novel anthranil-based photosensitizers were directed toward the construction of the bulky donor moiety: the N-(2′,4′-bis(dodecyloxy)-[1,1′-biphenyl]-4-yl)-2′,4′-bis(dodecyloxy)-N-phenyl-[1,1′-biphenyl]-4-amine fragment, also known as the Hagfeldt donor. Thus, intermediates 11 and 13 were subjected to a selective aromatic dibromination using NBS in DMF to afford compounds 14 (73%) and 18 (93%) in good to excellent yields (Scheme ).
4. Di-Bromination at the Diphenyl Moiety in Anthranil Derivatives 11 and 13 .
Compounds 14 and 15 were used then as the starting material for the Suzuki–Miyaura coupling with the synthetic boronate ester 16 to introduce the 2,4-bis(dodecyloxy)benzene moiety, furnishing the unsymmetric anthranil benzoates 17 (72%) and 18 (81%) in good yields bearing the donor and acceptor groups at the C3 and C7 positions (Scheme a). Finally, hydrolysis was performed under basic and mild conditions to give the desired photosensitizers LM14 19 and CP104 20 with excellent yields of 90% and 97%, respectively (Scheme a). Our target compounds were obtained on a 300 mg scale in a linear seven-step synthetic route and with satisfactory overall yields of 27% and 29%, respectively, for 19 and 20.
5.

a (a) Construction of the Hagfeldt donor fragment in the anthranil core to complete the synthesis of photosensitizers 19 and 20. (b) Change in the light emission during the chemical transformation of intermediates 7 and 9 into photosensitizers 19 and 20, respectively (THF at 365 nm).
In the synthesis of 19 and 20, we noticed that during the introduction of the donor and acceptor groups into the structure of anthranil 5, the resulting intermediates started to exhibit interesting photoluminescence properties due to having different groups attached to various positions of the anthranil core (Scheme b). In the case of photosensitizer 19 and its intermediates, we observed that by having the donor group at the C7 position and the acceptor group at C3, the emission of 7 moved from 497 nm (blue) to 643 nm (red) through all the chemical transformations to access the final compound 19 (Figure S1). This effect can be explained by the fact that in 19, the acceptor group at C3 is directly attached to the more electron-dense ring of the anthranil core, favoring the movement of charges from the donor to the acceptor moiety and resulting in a lower energy gap between the HOMO and LUMO of 19 in comparison with those of 20. On the other side, having the donor group at the C3 position of 20 completely changes the distribution of the electron density in the molecule through the anthranil bridge, affecting the movement of charges and increasing the energy bandgap between the HOMO and LUMO of 20, shifting the emission to 577 nm (yellow) (Scheme b).
We also studied and characterized our target compounds to evaluate their potential as photosensitizers in photovoltaic applications (Figure S2). These studies were complemented by cyclic voltammetry (CV) measurements of the three dyes in solution using a three-electrode electrochemical cell to depict their energy level alignments (Figure S3). With these data (UV–vis and CV experiments), we calculated the optical bandgap (E g) and molecular energy levels for compounds 19 and 20 to estimate their ability to promote and inject electrons in photovoltaic devices. These values are summarized in Table S1.
To shed light on the charge transfer capabilities between the dyes and the semiconductors such as TiO2, we first performed time-correlated single photon counting (TCSPC) of the dyes in solution (Figure S4 and Table S2), and then we recorded the transient absorption spectra (TAS) to elucidate the charge transfer kinetics of dyes 2, 19, and 20 sensitized on 4 μm TiO2 films (Figure S5).
The regeneration kinetics of the excited states of the dyes 2, 19, and 20 were studied at 920 nm in films with and without electrolyte ([Cu(II/I)(tmby)2][TFSI]2/1) (Figures S6 and S7).
As was expected, in the absence of an electrolyte, recombination of the photoinjected electrons in TiO2 and the oxidized dye is slower. However, the faster regeneration in the presence of the electrolyte can be explained by the energy of the HOMO level, which promotes a higher driving force for the electrolyte regeneration (Figures S8).
In conclusion, we have designed and developed an efficient synthetic route, based on Suzuki coupling and C–H arylation, to introduce the anthranil scaffold as a π-conjugated bridge in the structures of novel molecular photosensitizers. The selective C–H activation was studied using different Pd catalysts, establishing a protocol for the controlled C3 arylation of anthranils substituted with donor or acceptor groups in good yields and preventing side reactions and the ring opening of the anthranilic core. We found that placing donor and acceptor groups at the C3 and C7 positions ultimately changes the electron density within the molecule, altering their energetic levels and the nature of the excited species and resulting in compound 20 being more efficient for electron regeneration on solid-state films. Overall, we report the synthesis of two new anthranil-based photosensitizers with fast excited state lifetimes and properties that make them candidates for the fabrication of cosensitized DSSCs and low-intensity illumination devices.
Supplementary Material
Acknowledgments
This work was supported by the Spanish Government and AGAUR (Ministerio de Ciencia e Innovacion Severo Ochoa Grant MCIN/AEI/10.13039/501100011033 (CEX2019-000925-S), PID2022-139866NB-I00, FOTO-AVAN RED2022-134939-T, and 2021 SGR 01261, respectively). Financial support from the European Union by ERC Advanced grant ERC 101097684-Excited and Horizon 2020 Marie Skłodowska-Curie COFUND (grant agreement No 801474) for C.P. is appreciated. L.M. acknowledges financial support from the MINECO predoctoral fellowship (PREP2022-000271). E.P. also acknowledges ICIQ, CERCA, and ICREA for financial support. The authors thanks Marta Grados Rion for designing the graphical abstract.
The study’s data are available in the published article and its Supporting Information.
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.joc.5c00389.
The authors declare no competing financial interest.
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Supplementary Materials
Data Availability Statement
The study’s data are available in the published article and its Supporting Information.






