 Open Access Article
 Open Access Article
      
        
          
            Lei 
            Wang
          
        
      , 
      
        
          
            Irina 
            Rörich
          
        
      , 
      
        
          
            Charusheela 
            Ramanan
          
        
       , 
      
        
          
            Paul W. M. 
            Blom
          
        
      , 
      
        
          
            Wei 
            Huang
          
        
      , 
      
        
          
            Run 
            Li
          
        
       and 
      
        
          
            Kai A. I. 
            Zhang
, 
      
        
          
            Paul W. M. 
            Blom
          
        
      , 
      
        
          
            Wei 
            Huang
          
        
      , 
      
        
          
            Run 
            Li
          
        
       and 
      
        
          
            Kai A. I. 
            Zhang
          
        
       *
*
      
Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, Germany. E-mail: kai.zhang@mpip-mainz.mpg.de
    
First published on 21st June 2018
Electron-donating sacrificial reagents are highly important for certain photo-redox reactions. However, the use of excessive amounts of sacrificial reagents, mostly amines, often leads to undesired side products and is especially troublesome for product purification. Herein, we take the light-induced electron transfer cascade process of natural photosystems as a role model and assemble organic photocatalysts into cooperative photocatalyst couples. The cooperative photocatalyst couples could undergo intermolecular electron transfer to facilitate the charge separation process and overcome the need for an extra electron donor. Time-resolved photoluminescence spectroscopy was conducted to precisely characterize the photo-excited dynamics within the cooperative photocatalyst couples. As a model photoredox reaction, the carbon–carbon formation reaction between heteroarenes and malonates, which usually requires electron-donating sacrificial reagents such as amines, was conducted to demonstrate the feasibility of the cooperative photocatalyst couples under visible light irradiation. A significant reaction conversion improvement from trace conversion for a single photocatalyst system to over 90% by cooperative photocatalyst couples was achieved.
Natural photosystems offer a promising model to overcome the charge recombination issue, where a series of stepwise electron transfer processes are involved to enhance the photogenerated charge separation and transfer process.12 So far, chemists have designed different photocatalytic systems for enhancing the photocatalytic efficiency. For example, bridged transition metal complexes13–15 have been reported to greatly promote the photogenerated charge separation and transfer.
Organic semiconductor (OS)-containing photocatalysts have emerged as a promising alternative to traditional metal-containing photocatalysts due to their highly tunable electronical properties via flexible structural design. Recent research activities have demonstrated a vast number of structural design methods of small molecular8,10,16–20 or macromolecular21–30 OS systems as efficient photocatalysts for visible light-promoted photoredox reactions. Nevertheless, most developed OS photocatalysts, similar to traditional transition metal complexes,31–38 are single photocatalytic systems. As illustrated in Fig. 1a, the photocatalytic ability of the OS system originates from the photo-generated electron/hole pair, which can function as the reductive and oxidative species. To maintain the efficient electron transfer from the ground to the exited state of the OS, extra sacrificial agents are usually needed due to direct recombination of the electron/hole pair. To overcome the necessary use of electron-donating sacrificial reagents, the single photocatalyst system is not sufficient; a new concept of catalyst design is needed.
Herein, we aim to take the mechanism of the light-induced electron transfer cascade process of natural photosystems as a role model and assemble organic photocatalysts into cooperative photocatalyst couples. As illustrated in Fig. 1b, the two molecular OS photocatalysts within the cooperative couple consisted of different organic photocatalysts possessing different highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) levels. By coupling the OSs, an extra intermolecular electron transfer could occur between the OSs, leading to enhanced photo-generated electron/hole separation under light irradiation and thereby more stable reductive and oxidative species. The intermolecular electron transfer within the OS couple can decay the direct recombination of the electron/hole pair and overcome the mandatory requirement of extra electron donors during the photoredox cycle. As a model reaction, the photocatalytic carbon–carbon formation reaction between electron-rich heteroarenes and malonates, which usually required electron-donating sacrificial reagents,9,39 was chosen to demonstrate the feasibility and photocatalytic activity of the cooperative photocatalyst couple. No extra sacrificial reagents were needed. The light-induced electron transfer between the OSs within the cooperative photocatalyst couple and the substrates could be revealed by mechanistic studies.
|  | ||
| Scheme 1 Structure and HOMO/LUMO levels (vs. SCE) of the OS molecules in both designed photocatalyst couples. | ||
The three OSs possessed different HOMO and LUMO band positions, which could be determined via cyclic voltammetry (Fig. S1†). As shown in Scheme 1, Th-BTz-Th exhibited a significantly high LUMO level at −1.68 V vs. saturated calomel electrode (SCE), followed by TA-BT-TA with −1.20 V vs. SCE and Th-BT-Th with −1.15 V vs. SCE. In comparison, TA-BT-TA exhibited the lowest HOMO level at +1.54 V vs. SCE, followed by Th-BT-Th with +1.12 V vs. SCE and Th-BTz-Th with +0.95 V vs. SCE. In addition, the excited state redox potentials are calculated to be +1.16 V and −1.01 V vs. SCE for Th-BT-Th, +0.62 V and −1.35 V vs. SCE for Th-BTz-Th, and +1.14 V and −0.80 V vs. SCE for TA-BT-TA, respectively. The data are listed in Table S1 in the ESI† using the calculation described in a previous report.40 Given the different energy band positions, we assembled the three OSs in two photocatalyst couples for this study, particularly, Th-BTz-Th/Th-BT-Th for cooperative photocatalyst couple 1 and Th-BTz-Th/TA-BT-TA for couple 2.
Steady-state fluorescence quenching experiments showed that by only exciting Th-BT-Th (at 500 nm) or TA-BT-TA (at 450 nm) in both couples, the fluorescence intensity of couple 2 exhibited a larger decrease in PL intensity than that of couple 1, indicating an enhanced electron transfer within couple 2, which was likely caused by the larger distance between the two HOMO levels (Fig. S2†).
To further study the photo-induced charge transfer within the couples, time-resolved photoluminescence (TRPL) spectroscopy was conducted to characterize the photo-excited dynamics within the OS couples. The PL measurements of the pristine materials and a 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 (mol%) blend were all performed in DMF solution with excitation at 400 nm (Fig. 2c and d). The selected PL decays correspond to the emission maximum for each component OS (Fig. 2c). The fluorescence features of the different component materials overlap with each other. Therefore, the decay associated spectra (DAS) were derived by a global fitting analysis41 of the TRPL data (Fig. S2†). This allows us to characterize the spectral distribution and lifetime of each emitting species, particularly for the measurements of couple 1 and couple 2. In couple 1 (Fig. S2a†), one can see that DAS 1, centered at 460 nm, matches exactly with the fluorescence spectrum of Th-BTz-Th and decays in 0.6 ns, which is quenched with respect to the pristine donor (2.6 ns). DAS 2, which is centered at 590 nm, matches the fluorescence spectrum of Th-BT-Th and decays with the same ∼12 ns lifetime as the pristine Th-BT-Th sample, exhibiting no quenching. This indicates that in couple 1 the excitation energy transfer (EET) from Th-BTz-Th to Th-BT-Th likely dominates the excited state dynamics, as illustrated in Fig. 2e. In couple 2 (Fig. S2b†), the DAS 1, centered at 460 nm, originates again from Th-BTz-Th and decays in 0.97 ns, which is quenched with respect to the pristine Th-BTz-Th (2.6 ns). DAS 2, centered at 530 nm, is assigned to the emission of TA-BT-TA and has a decay time of 10.6 ns. Here, the fluorescence of both Th-BTz-Th and TA-BT-TA is quenched with respect to the pristine materials. This indicates an electron transfer from Th-BTz-Th to TA-BT-TA and an enhanced charge transfer within couple 2 (Fig. 2f).
1 (mol%) blend were all performed in DMF solution with excitation at 400 nm (Fig. 2c and d). The selected PL decays correspond to the emission maximum for each component OS (Fig. 2c). The fluorescence features of the different component materials overlap with each other. Therefore, the decay associated spectra (DAS) were derived by a global fitting analysis41 of the TRPL data (Fig. S2†). This allows us to characterize the spectral distribution and lifetime of each emitting species, particularly for the measurements of couple 1 and couple 2. In couple 1 (Fig. S2a†), one can see that DAS 1, centered at 460 nm, matches exactly with the fluorescence spectrum of Th-BTz-Th and decays in 0.6 ns, which is quenched with respect to the pristine donor (2.6 ns). DAS 2, which is centered at 590 nm, matches the fluorescence spectrum of Th-BT-Th and decays with the same ∼12 ns lifetime as the pristine Th-BT-Th sample, exhibiting no quenching. This indicates that in couple 1 the excitation energy transfer (EET) from Th-BTz-Th to Th-BT-Th likely dominates the excited state dynamics, as illustrated in Fig. 2e. In couple 2 (Fig. S2b†), the DAS 1, centered at 460 nm, originates again from Th-BTz-Th and decays in 0.97 ns, which is quenched with respect to the pristine Th-BTz-Th (2.6 ns). DAS 2, centered at 530 nm, is assigned to the emission of TA-BT-TA and has a decay time of 10.6 ns. Here, the fluorescence of both Th-BTz-Th and TA-BT-TA is quenched with respect to the pristine materials. This indicates an electron transfer from Th-BTz-Th to TA-BT-TA and an enhanced charge transfer within couple 2 (Fig. 2f).
We chose the photocatalytic carbon–carbon formation reaction between electron-rich heteroarenes and malonates as a model reaction.9,10 Previous studies demonstrated the mandatory use of sacrificial reagents, mostly amines, which ought not to only act as electron donors, but also as electron mediators between the radical intermediate and the photo-generated hole of the photocatalyst (Fig. S4†). We first tested the three designed OSs as single photocatalyst systems without using sacrificial reagents. As expected, by using 3-methylbenzofuran and diethyl bromomalonate in the model reaction, no product was obtained using Th-BT-Th and TA-BT-TA as photocatalysts (entries 1 and 2 in Table 1). Interestingly, using Th-BTz-Th as a photocatalyst led to a slight conversion of 9%. This indicates that a minimal electron transfer could still occur between the photocatalyst and the substrate, which corresponds to the highest LUMO level of Th-BTz-Th among the three OSs and thereby the largest overpotential for the reduction of diethyl bromomalonate.
| Entry | Catalyst | Substrate | Product | Convb [%] | Yieldc [%] | 
|---|---|---|---|---|---|
| a Reaction conditions: 1 equiv. (0.38 mmol) heteroarene, 2 equiv. diethyl bromomalonate, 0.1 equiv. photocatalyst (for the coupled system, the ratio between the two OSs was 1 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1) in 2.5 mL DMF, white LED lamp (0.07 Wcm−2), 24 h.
                  b Determined by GC-MS.
                  c Isolated yield.
                  d Blue LED (450 nm, 0.1 Wcm−2).
                  e 48h.
                  f 0.05 equiv. photocatalyst, 24 h.
                  g No catalyst, under light.
                  h No light. | |||||
| 1 | Th-BT-Th |   |   | Trace | — | 
| 2 | TA-BT-TA |   |   | 0 | — | 
| 3 | Th-BTz-Th |   |   | 9 | — | 
| 4 | Couple 1 |   |   | 43 | 39 | 
| 5 | Couple 2 |   |   | 93 | 87 | 
| 6d | Couple 2 |   |   | 98 | 85 | 
| 7e | Couple 2 |   |   | 78 | 75 | 
| 8e | Couple 2 |   |   | 92 | 85 | 
| 9e | Couple 2 |   |   | 85 | 80 | 
| 10f | Th-BTz-Th/TA-BT-TA (2 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1) |   |   | 72 | 60 | 
| 11f | Connected cat. |   |   | 31 | 22 | 
| 12g | — |   |   | 0 | — | 
| 13h | Couple 2 |   |   | 0 | — | 
In contrast, by using both cooperative photocatalyst couples, the product could be obtained in significantly higher conversions, in particular, 43% for couple 1 and 93% for couple 2 (entries 4 and 5). Both the apparent quantum yield (ΦAQY) and catalytic turnover number (TON) for the model reaction (entry 5) using coupling 2 as a photocatalyst were calculated to be 0.04% and 8.7, respectively (ESI†). A kinetic study confirmed the superior catalytic activity of couple 2 compared to couple 1 via a fluorescence quenching experiment by the substrates (Fig. S6†). This is in agreement with the photophysical study (Fig. 2), indicating that the enhanced charge transfer between Th-BTz-Th and TA-BT-TA in couple 2 led to a better catalytic efficiency than that of couple 1 containing Th-BTz-Th and Th-BT-Th. The reason could lie on the larger HOMO energy gap (ΔEHOMO = 0.59 V) between Th-BTz-Th and TA-BT-TA than that (ΔEHOMO = 0.17 V) in couple 1 between Th-BTz-Th and Th-BT-Th.42,43 By using a single wavelength light source (blue LED, 450 nm), where only TA-BT-TA of couple 2 could be excited, the model reaction exhibited a high conversion of 98%. This indicates a hole transfer from TA-BT-TA to Th-BTz-Th, leading to a similar effect of an electron transfer from Th-BTz-Th back to TA-BT-TA, as illustrated in Fig. 2f.
In comparison with the use of Th-BT-Th as a single photocatalyst with the employment of an extra sacrificial electron donor, in particular, triphenylamine from our previous report for the model reaction,44 where the apparent quantum yield was calculated to be 0.96%, the apparent quantum yield of couple 2 was lower due to the longer reaction time. However, the avoidance of the extra sacrificial electron donor using the molecular photocatalyst couples is still advantageous. It can efficiently prevent the post-purification procedures caused by the addition of usually excess amounts of amine donors.
Screening experiments using different substrates confirmed the feasibility of the OS couple as a photocatalyst (entries 7–9). Other control experiments either without the photocatalyst or without light led to no product formation (entries 12 and 13), indicating the mandatory roles of both components.
To gain more mechanistic insight into the interaction between the photocatalyst and substrate, we conducted further fluorescence quenching experiments. It was shown that the fluorescence of the OSs as single photocatalysts could be only minimally quenched by adding diethyl bromomalonate (Fig. S5†). In contrast, the fluorescence of both photocatalyst couples could be gradually quenched by adding diethyl bromomalonate (Fig. S6†), confirming the possible electron transfer between the photocatalyst couple and the substrate.
To precisely study the actual electron transfer process within the catalytic cycle, we then employed ethyl bromoacetate as a substrate, which possessed a reduction potential of −1.43 V vs. SCE (Fig. 3). By using couple 2 as a photocatalyst, it could be determined that only traces of the final product could be obtained (Fig. S11†). This reveals that the photo-generated electron could indeed only transfer from the LUMO of Th-BTz-Th (−1.68 V vs. SCE) to the LUMO of TA-BT-TA (−1.20 V vs. SCE) in the first step, from which the further electron transfer to the higher reduction level of ethyl bromoacetate was not possible. Additionally, a direct electron transfer from Th-BTz-Th to ethyl bromoacetate could not occur either. In comparison, diethyl bromomalonate (Ered. = −1.00 V vs. SCE) could be reduced via electron transfer originating from the LUMO of TA-BT-TA, leading to the formation of the malonate radical, which further reacts with 3-methylbenzofuran to form the final product in the following step of the catalytic cycle. An additional model reaction using Th-BTz-Th as the single photocatalyst system and triphenylamine as the sacrificial reagent led to the formation of the final product, confirming that a direct electron transfer from Th-BTz-Th to ethyl bromoacetate was only possible in the absence of TA-BT-TA (Fig. S12†). It is also worth noting that further scope reactions with other substrates led to high product yields using couple 2 as a photocatalyst, demonstrating the general feasibility of the cooperative photocatalyst design. It is worth noting that a possible radical chain mechanism as introduced by Yoon et al.45 could be clearly ruled out due to our previous study on the influence of the oxidation potential of the photocatalysts on the reaction rate.10
|  | ||
| Fig. 3 Study of the electron transfer pathway using comparative substrates with different reduction potentials. Light source: white LED lamp (0.07 Wcm−2, λ > 420 nm). Interm.: intermediate. | ||
The reason for the lower efficiency using the cooperative photocatalyst couple in comparison with the one catalyzed in the presence of sacrificial reagents might be caused by different factors. The multi-step electron transfer within the photocatalyst couple and further to the substrate might not be efficient due to the low concentration of the catalysts. Another important factor might be the electron transfer steps between the intermediates and the photogenerated hole. For this point, an additional study was conducted as described below.
The photo-induced electron transfer within the cooperative photocatalyst couple usually occurs based on the rather random contact between the two OSs in the liquid reaction medium. To create a non-random contact and thereby a more defined electron transfer process, we then connected Th-BTz-Th and TA-BT-TA via the C6 alkyl chain as a molecular bridge as a control photocatalyst. As displayed in Fig. 4c, a large molecule of Th-BTz-Th@TA-BT-TA containing both OSs in couple 2 was synthesized. Remarkably, the fluorescence intensity of Th-BTz-Th/TA-BT-TA strongly decreased after connection compared to their unconnected form as couple 2 (Fig. S8†). This result suggests a strong interaction between the two OSs inside the large molecule. A study on the impact of Th-BTz-Th/TA-BT-TA in couple 2 on their photocatalytic efficiency showed that the highest reaction rate was achieved with a ratio of 2![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 of Th-BTz-Th/TA-BT-TA (Fig. 4a), which in fact corresponds to the connected molecule of Th-BTz-Th@TA-BT-TA. However, when comparing the catalytic efficiency between the connected catalyst Th-BTz-Th@TA-BT-TA and the unconnected couple 2 with the same ratio between both OSs, only a decreased conversion was observed for the connected catalyst (Fig. 4b). In spite of the better electron transfer occurring within connected system, the reduced catalytic efficiency could be likely caused by the steric hindrance within the large molecule or the competing charge recombination process,46 which limits the contact between the substrate and the individual OSs in the large molecule and efficient electron transfer between the catalyst and substrate. To overcome this limitation, new molecular bridges other than the C6 alkyl chain could be needed.
1 of Th-BTz-Th/TA-BT-TA (Fig. 4a), which in fact corresponds to the connected molecule of Th-BTz-Th@TA-BT-TA. However, when comparing the catalytic efficiency between the connected catalyst Th-BTz-Th@TA-BT-TA and the unconnected couple 2 with the same ratio between both OSs, only a decreased conversion was observed for the connected catalyst (Fig. 4b). In spite of the better electron transfer occurring within connected system, the reduced catalytic efficiency could be likely caused by the steric hindrance within the large molecule or the competing charge recombination process,46 which limits the contact between the substrate and the individual OSs in the large molecule and efficient electron transfer between the catalyst and substrate. To overcome this limitation, new molecular bridges other than the C6 alkyl chain could be needed.
 
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a white solid (1.28 g, 45%). 1H NMR (300 MHz, CDCl3) δ: 7.37 (s, 2H), 4.72 (t, J = 7.4 Hz, 2H), 2.06 (m, 2H), 1.41–1.29 (m, 2H), 0.91 (t, J = 7.4 Hz, 3H). 13C NMR (300 MHz, CDCl3) δ: 143.71, 129.51, 109.97, 57.22, 32.17, 19.82, 13.51.
1 as the eluent gave the final product as a white solid (1.28 g, 45%). 1H NMR (300 MHz, CDCl3) δ: 7.37 (s, 2H), 4.72 (t, J = 7.4 Hz, 2H), 2.06 (m, 2H), 1.41–1.29 (m, 2H), 0.91 (t, J = 7.4 Hz, 3H). 13C NMR (300 MHz, CDCl3) δ: 143.71, 129.51, 109.97, 57.22, 32.17, 19.82, 13.51.
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a light red solid (713 mg, 70%). 1H NMR (300 MHz, CDCl3) δ: 8.03 (dd, J = 3.7, 1.2 Hz, 2H), 7.56 (s, 2H), 7.31 (dd, J = 5.1, 1.2 Hz, 2H), 7.12 (dd, J = 5.1, 3.7 Hz, 2H), 4.76 (t, J = 7.4 Hz, 2H), 2.16–2.07 (m, 2H), 1.44–1.34 (m, 2H), 0.94 (t, J = 7.4 Hz, 3H). 13C NMR (75 MHz, CDCl3) δ: 142.10, 139.97, 128.12, 126.97, 125.55, 123.59, 122.78, 56.61, 32.08, 19.89, 13.57.
1 as the eluent gave the final product as a light red solid (713 mg, 70%). 1H NMR (300 MHz, CDCl3) δ: 8.03 (dd, J = 3.7, 1.2 Hz, 2H), 7.56 (s, 2H), 7.31 (dd, J = 5.1, 1.2 Hz, 2H), 7.12 (dd, J = 5.1, 3.7 Hz, 2H), 4.76 (t, J = 7.4 Hz, 2H), 2.16–2.07 (m, 2H), 1.44–1.34 (m, 2H), 0.94 (t, J = 7.4 Hz, 3H). 13C NMR (75 MHz, CDCl3) δ: 142.10, 139.97, 128.12, 126.97, 125.55, 123.59, 122.78, 56.61, 32.08, 19.89, 13.57.
          
         
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a light yellow solid (2.78 g, 83%). The H-NMR data was consistent with the literature reported.48
1 as the eluent gave the final product as a light yellow solid (2.78 g, 83%). The H-NMR data was consistent with the literature reported.48
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a light brown solid (420 mg, 876%). The H-NMR data was consistent with the literature reported.48
1 as the eluent gave the final product as a light brown solid (420 mg, 876%). The H-NMR data was consistent with the literature reported.48
          
          
             
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a white solid (1.82 g, 41%). 1H NMR (300 MHz, CDCl3) δ: 7.38 (s, 2H), 4.73 (t, J = 7.4 Hz, 2H), 3.33 (t, J = 7.4 Hz, 2H), 2.16–2.06 (m, 2H), 1.84–1.75 (multi, 2H), 1.50–1.39 (multi, 2H), 1.34–1.29 (multi, 2H). 13C NMR (75 MHz, CDCl3) δ: 143.76, 129.64, 110.00, 57.24, 33.58, 32.39, 29.99, 27.54, 25.70.
1 as the eluent gave the final product as a white solid (1.82 g, 41%). 1H NMR (300 MHz, CDCl3) δ: 7.38 (s, 2H), 4.73 (t, J = 7.4 Hz, 2H), 3.33 (t, J = 7.4 Hz, 2H), 2.16–2.06 (m, 2H), 1.84–1.75 (multi, 2H), 1.50–1.39 (multi, 2H), 1.34–1.29 (multi, 2H). 13C NMR (75 MHz, CDCl3) δ: 143.76, 129.64, 110.00, 57.24, 33.58, 32.39, 29.99, 27.54, 25.70.
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a yellow solid (750 mg, 76%). 1H NMR (300 MHz, CDCl3) δ: 8.66 (s, 2H), 8.59 (s, 2H), 7.36 (s, 4H), 4.72 (t, J = 7.4 Hz, 4H), 4.42 (t, J = 7.4 Hz, 4H), 2.16–2.07 (m, 4H), 2.00–1.94 (m, 4H), 1.42–1.39 (m, 8H). 13C NMR (75 MHz, CDCl3) δ: 152.26, 143.74, 143.14, 129.65, 126.15, 123.82, 122.58, 109.98, 57.12, 50.30, 30.11, 29.86, 25.94.
1 as the eluent gave the final product as a yellow solid (750 mg, 76%). 1H NMR (300 MHz, CDCl3) δ: 8.66 (s, 2H), 8.59 (s, 2H), 7.36 (s, 4H), 4.72 (t, J = 7.4 Hz, 4H), 4.42 (t, J = 7.4 Hz, 4H), 2.16–2.07 (m, 4H), 2.00–1.94 (m, 4H), 1.42–1.39 (m, 8H). 13C NMR (75 MHz, CDCl3) δ: 152.26, 143.74, 143.14, 129.65, 126.15, 123.82, 122.58, 109.98, 57.12, 50.30, 30.11, 29.86, 25.94.
          
          
            ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 as the eluent gave the final product as a yellow-red solid (403 mg, 53%). 1H NMR (300 MHz, CDCl3) δ: 8.59 (s, 2H), 8.55 (s, 2H), 7.98 (dd, J = 3.7, 1.2 Hz, 4H), 7.52 (s, 4H), 7.29–7.27 (m, 4H), 7.08 (dd, J = 5.1, 3.7 Hz, 4H), 4.74 (t, J = 7.4 Hz, 4H), 4.39 (t, J = 7.4 Hz, 4H), 2.16–2.12 (m, 4H), 1.98–1.93 (m, 4H), 1.45–1.42 (m, 8H). 13C NMR (75 MHz, CDCl3) δ: 152.21, 143.15, 142.09, 139.84, 128.10, 126.92, 126.04, 125.63, 123.72, 123.55, 122.82, 122.59, 56.52, 50.30, 30.15, 29.70, 26.03, 25.97.
1 as the eluent gave the final product as a yellow-red solid (403 mg, 53%). 1H NMR (300 MHz, CDCl3) δ: 8.59 (s, 2H), 8.55 (s, 2H), 7.98 (dd, J = 3.7, 1.2 Hz, 4H), 7.52 (s, 4H), 7.29–7.27 (m, 4H), 7.08 (dd, J = 5.1, 3.7 Hz, 4H), 4.74 (t, J = 7.4 Hz, 4H), 4.39 (t, J = 7.4 Hz, 4H), 2.16–2.12 (m, 4H), 1.98–1.93 (m, 4H), 1.45–1.42 (m, 8H). 13C NMR (75 MHz, CDCl3) δ: 152.21, 143.15, 142.09, 139.84, 128.10, 126.92, 126.04, 125.63, 123.72, 123.55, 122.82, 122.59, 56.52, 50.30, 30.15, 29.70, 26.03, 25.97.
          
        | Footnote | 
| † Electronic supplementary information (ESI) available: Experiment details and characterization, 1H and 13C NMR spectra, fluorescence quenching experiments and control experiments are described. See DOI: 10.1039/c8cy01072b | 
| This journal is © The Royal Society of Chemistry 2018 |