Tunable Donor–Acceptor Linear Conjugated Polymers Involving Cyanostyrylthiophene Linkages for Visible-Light-Driven Hydrogen Production

In this paper, an atom- and step-economic direct C-H arylation polymerization (DArP) strategy was developed to access cyanostyrylthiophene (CST)-based donor–acceptor (D–A) conjugated polymers (CPs) used for photocatalytic hydrogen production (PHP) from water reduction. The new CST-based CPs CP1–CP5 with varied building blocks were systematically studied by X-ray single-crystal analysis, FTIR, scanning electron microscopy, UV-vis, photoluminescence, transient photocurrent response, cyclic voltammetry measurements, and a PHP test, which showed that the phenyl-cyanostyrylthiophene-based CP3 exhibits a superior hydrogen evolution rate (7.60 mmol h−1 g−1) compared to other conjugated polymers. The structure–property–performance correlation results obtained in this study will provide an important guideline for the rational design of high-performance D–A CPs for PHP applications.


Introduction
Energy consumption is ever increasing with the rapid development of human society. The exploration of clean and renewable energies has become the top priority of governments all over the world. Hydrogen energy is regarded as one of the most promising alternatives to traditional fossil fuels. Solar-driven hydrogen production from water, i.e., photocatalytic hydrogen production (PHP), is a potential way to solve environmental issues and the global energy crisis [1][2][3][4][5][6][7].
In recent years, π-conjugated polymers (CPs), consisting of alternating double and single bonds with C, H, N, O, and S light elements, have emerged as a type of promising soft photocatalyst due to their high stability and their strong absorptance toward visible light [8][9][10][11][12][13][14][15]. In comparison to state-of-the-art polymeric graphitic carbon nitride (g-C 3 N 4 ) with relatively fixed structures [10,16], CPs with alternating electron donors' (Ds') and acceptors' (As') building blocks, i.e., D-A CPs, are expected to be potentially efficient photocatalysts, due to the abundance of D-A interactions, which can finely modulate the opto-electronic properties by varying the D/A ratios or by adjusting π-conjugated structures [14,[17][18][19][20]. The highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO), corresponding to the valence and conduction bands of an inorganic semiconductor, are governed, respectively, by the electron-donating and electron-accepting building blocks, which endows D-A CPs with a wide range of tunabilities regarding light absorption, frontier molecular orbital (FMO) levels, and photocatalytic redox capacity [14,18,21].

Synthesis and Characterization of the CPs
As shown in Figure 1, a series of CST-based polymers, CP1-CP5, were synthesized separately in five pots of Pd-catalyzed C-H direct arylated coupling polymerization [24][25][26] starting from building blocks CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP, which were facilely obtained via Knoevenagel condensation between varied bromo-substituted aromatic aldehydes and 2-(thiophen-2-yl)acetonitrile (Th-ACN). The structures of these CST-based CPs were characterized by Fourier transform infrared (FT-IR) spectra ( Figure 2). All CPs displaying peaks at~1640 cm −1 wavelength were assigned to the stretching vibration of C=C double bonds, revealing the presence of vinylene linkers. The infra-red absorption peaks at about 2232 cm −1 were the skeleton vibration of the -CN groups in all these CPs. 26] starting from building blocks CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP, which were facilely obtained via Knoevenagel condensation between varied bromosubstituted aromatic aldehydes and 2-(thiophen-2-yl)acetonitrile (Th-ACN). The structures of these CST-based CPs were characterized by Fourier transform infrared (FT-IR) spectra ( Figure 2). All CPs displaying peaks at ~1640 cm −1 wavelength were assigned to the stretching vibration of C=C double bonds, revealing the presence of vinylene linkers. The infra-red absorption peaks at about 2232 cm −1 were the skeleton vibration of the -CN groups in all these CPs. To understand the structural correlation between the monomers and the corresponding polymers, the optimal geometries and the dihedral angles of the CSTbased monomers and dimers were predicted by a density-function-theory (DFT) calculation. When considering the coupled unit as a system, the dihedral angles between the donor units of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP and the thiophenyl unit were 1.2°, 1.5°, 30.1°, 52.4°, and 53.6°, respectively ( Figure S1). Due to the steric effect, a large dihedral angle was observed between the two units. The dihedral angles of pyridine and thiophene rings were similar, which was helpful in revealing the effect of the electron-donating ability of the pyridine and thiophene units on the optoelectronic properties and performance. The planarity of CP3 showed little change owing to the equivalent thiophene-thiophene rings involved. The steric hindrance of the naphthalene ring and the methyl group enlarged the dihedral angles of CP4 and CP5, which would be less conducive to the charge transfer.
In the CST-based monomers, the dihedral angles between the donor and acceptor units of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP were 28.0°, 26.0°, 23.9°, 46.4°, and 15.1°, respectively ( Figure S2). This was because vinyl can form a strong conjugation effect with the donor and acceptor units; thus, the dihedral angles between them were greatly changed. In the dimer models of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP, the dihedral angles between the donor unit and the acceptor unit were changed to 29.0°, 28.1°, 20.8°, 43.1°, and 19.9°, respectively ( Figure S3). Therefore, this trend of change can help us predict whether the dihedral angle of polymer molecules is favorable for photocatalytic hydrogen production. For example, the dihedral angle of CP5 increased dramatically, which would be detrimental to the transport of photogenerated carriers.
The above point was also experimentally supported by single-crystal X-ray analysis. To explore the impact of CST substitutes, the single crystals of monomers CST-BT, CST-BP, and CST-BMP were successfully grown and subjected to X-ray crystalline structural analysis ( Figure 3). Among the monomers, CST-BT and CST-BMP were two newly To understand the structural correlation between the monomers and the corresponding polymers, the optimal geometries and the dihedral angles of the CST-based monomers and dimers were predicted by a density-function-theory (DFT) calculation. When considering the coupled unit as a system, the dihedral angles between the donor units of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP and the thiophenyl unit were 1.2 • , 1.5 • , 30.1 • , 52.4 • , and 53.6 • , respectively ( Figure S1). Due to the steric effect, a large dihedral angle was observed between the two units. The dihedral angles of pyridine and thiophene rings were similar, which was helpful in revealing the effect of the electron-donating ability of the pyridine and thiophene units on the opto-electronic properties and performance. The planarity of CP3 showed little change owing to the equivalent thiophene-thiophene rings involved. The steric hindrance of the naphthalene ring and the methyl group enlarged the dihedral angles of CP4 and CP5, which would be less conducive to the charge transfer.
In the CST-based monomers, the dihedral angles between the donor and acceptor units of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP were 28.0 • , 26.0 • , 23.9 • , 46.4 • , and 15.1 • , respectively ( Figure S2). This was because vinyl can form a strong conjugation effect with the donor and acceptor units; thus, the dihedral angles between them were greatly changed. In the dimer models of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP, the dihedral angles between the donor unit and the acceptor unit were changed to 29.0 • , 28.1 • , 20.8 • , 43.1 • , and 19.9 • , respectively ( Figure S3). Therefore, this trend of change can help us predict whether the dihedral angle of polymer molecules is favorable for photocatalytic hydrogen production. For example, the dihedral angle of CP5 increased dramatically, which would be detrimental to the transport of photogenerated carriers.
The above point was also experimentally supported by single-crystal X-ray analysis. To explore the impact of CST substitutes, the single crystals of monomers CST-BT, CST-BP, and CST-BMP were successfully grown and subjected to X-ray crystalline structural analysis ( Figure 3 bonds were formed in CST-BT, CST-BP, and CST-BMP with distances of 2.496 Å, 2.638 Å, and 2.718 Å, respectively. Based on the data, the spatial potential resistance effect had a significant impact on the distance of the CST unit. reported crystals (CCDC2190738 and CCDC2190742, CIF files in SI). The results demonstrated that the molecules of CST-BT, CST-BP, and CST-BMP pertained to the triclinic space group. Z = 4, with cell parameters of a = 6.8270 Å, b = 23.045 Å, c = 7.4519 Å, α = 90°, β = 97.604°, and γ = 90° for CST-BT; Z = 4, with cell parameters of a = 3.9619 Å, b = 24.465 Å, c = 12.6409 Å, α = 90°, β = 96.409°, and γ = 90° for CST-BP. Z = 2, with cell parameters of a = 7.5030 Å, b = 8.5195 Å, c = 11.1655 Å, α = 86.355°, β = 79.693°, and γ = 67.892° for CST-BMP. For the one-dimensional chain structures, the intermolecular hydrogen bonds were formed in CST-BT, CST-BP, and CST-BMP with distances of 2.496 Å, 2.638 Å, and 2.718 Å, respectively. Based on the data, the spatial potential resistance effect had a significant impact on the distance of the CST unit. To gain deeper insight into the morphologies of varied CST-based CPs at micro-and nanoscales, all the CPs were investigated by scanning electron microscopy (SEM). The morphology and structure of photocatalysts in promoting the separation of photogenerated carriers contribute to the improvement of photocatalytic activity. CP1-CP5 each displayed a well-defined dimension and morphology (Figure 4), which showed that the morphologies of CP1-CP5 are different from each other's. The enhanced planarities of starting monomers CST-BPD and CST-BT endowed CP1 and CP2 a tightly packed irregular morphology. Nevertheless, CP4 and CP5 displayed a dendritic-like morphology, which was consistent with the spatial steric resistance of the naphthalene ring and the methyl group. Compared with the other CPs, the SEM morphologies of CP3 had a more regular lamellar compact structure, which was instrumental in charge transport and separation of carriers to the photocatalytic reaction. To gain deeper insight into the morphologies of varied CST-based CPs at micro-and nanoscales, all the CPs were investigated by scanning electron microscopy (SEM). The morphology and structure of photocatalysts in promoting the separation of photogenerated carriers contribute to the improvement of photocatalytic activity. CP1-CP5 each displayed a well-defined dimension and morphology (Figure 4), which showed that the morphologies of CP1-CP5 are different from each other's. The enhanced planarities of starting monomers CST-BPD and CST-BT endowed CP1 and CP2 a tightly packed irregular morphology. Nevertheless, CP4 and CP5 displayed a dendritic-like morphology, which was consistent with the spatial steric resistance of the naphthalene ring and the methyl group. Compared with the other CPs, the SEM morphologies of CP3 had a more regular lamellar compact structure, which was instrumental in charge transport and separation of carriers to the photocatalytic reaction.

Opto-Electronic Properties of the CPs
The opto-electronic properties of CP1-CP5 were systematically studied by UV-vis absorption, photoluminescence (PL), transient photocurrent response (TPR) and cyclic voltammetry (CV) measurements ( Figure 5). The UV-vis diffuse reflectance spectroscopy (DRS) revealed that all of the CPs had extensive absorption in the range of 300-600 nm (Figure 5a), which benefits visible-light harvesting. This suggests that introducing the electron-D/A-capability units into the conjugate backbone can tune the energy level of the CPs and lead to changes in the spectral absorption of the materials alteration. The

Opto-Electronic Properties of the CPs
The opto-electronic properties of CP1-CP5 were systematically studied by UV-vis absorption, photoluminescence (PL), transient photocurrent response (TPR) and cyclic voltammetry (CV) measurements ( Figure 5). The UV-vis diffuse reflectance spectroscopy (DRS) revealed that all of the CPs had extensive absorption in the range of 300-600 nm (Figure 5a), which benefits visible-light harvesting. This suggests that introducing the electron-D/A-capability units into the conjugate backbone can tune the energy level of the CPs and lead to changes in the spectral absorption of the materials alteration. The absorption trend was consistent with the colors of CPs: better absorbance toward longer wavelengths had deeper colors (insets in Figure 5a). The nitrogen atom of the pyridine ring in CP1 had the induction effect of electron absorption and the conjugation effect of electron absorption, which led to the wide absorption range and darker color of CP1 in the state of solid aggregation. CP2 with a range absorption too wide led to a narrow band gap, which resulted in an easier return of electrons from the excited state to the ground state; thus, the recombination of photogenerated electron holes sharply increased, reducing the effect of hydrogen production. The optical bandgaps (E g ) of CP1-CP5 estimated by the plotting curves of (αhν) 2 vs. hν were 1.88, 1.85, 1.98, 2.06, and 1.97 eV, respectively ( Figure S5). Although CP1-CP5 had no solubility in common solvents such as CH 2 Cl 2 , CHCl 3 and toluene, they all could form colloidal dispersions in N-methyl-pyrrolidinone (NMP). The UV-vis spectra of CP1-CP5 colloidal dispersions in NMP exhibited maximum absorption peaks at 420.5, 526.5, 455, 426.5, and 531.5 nm wavelengths, respectively ( Figure S4). Minimizing the exciton-binding energy can increase the yield of charge-carrier generation and improve photocatalytic activity [17]. Typically, the recombination of photogenerated electron-hole pairs can be evaluated by steady-state PL spectroscopy. The PL spectra of CP1-CP5 were collected, as shown in Figure 5b, to facilitate a full comparison of their PL intensities, i.e., photo-to-photo conversions. CP4 and CP5 stimulated by a 365 nm wavelength displayed a strong fluorescence. The weaker the PL intensity, the lower the recombination rate of electron-hole (e − -h + ) pairs [14], which favors to the photogenerated carrier separation. CP1-CP3 had a lower PL intensity, suggesting a decreased ratio of e − -h + recombination (insets in Figure 5b). The above results reveal that the alternating-electron D and A building blocks involved in the polymeric backbones can effectively promote the internal electron transfer and reduce the exciton recombination.
For an excellent photocatalyst, a suitable band gap is needed to ensure a sufficient Minimizing the exciton-binding energy can increase the yield of charge-carrier generation and improve photocatalytic activity [17]. Typically, the recombination of photogenerated electron-hole pairs can be evaluated by steady-state PL spectroscopy. The PL spectra of CP1-CP5 were collected, as shown in Figure 5b, to facilitate a full comparison of their PL intensities, i.e., photo-to-photo conversions. CP4 and CP5 stimulated by a 365 nm wavelength displayed a strong fluorescence. The weaker the PL intensity, the lower the recombination rate of electron-hole (e − -h + ) pairs [14], which favors to the photogenerated carrier separation. CP1-CP3 had a lower PL intensity, suggesting a decreased ratio of e − -h + recombination (insets in Figure 5b). The above results reveal that the alternating-electron D and A building blocks involved in the polymeric backbones can effectively promote the internal electron transfer and reduce the exciton recombination.
For an excellent photocatalyst, a suitable band gap is needed to ensure a sufficient light absorptance to produce e − -h + pairs. In addition, the photogenerated electron and hole separately transfer to the photocatalytic redox reaction before being recombined. Typically, the band gap should be greater than 1.8 eV and less than 2.2 eV to simultaneously ensure the sufficient driven force for PHP and the efficient absorption toward visible light [8]. In order to obtain materials with efficient carrier separation, we hoped to minimize the overlap between the HOMO levels while also achieving the LUMO levels, to realize the spatial separation of electron-hole pairs. Here, the electrochemical property and the FMOs of CP1-CP5 were estimated by CV measurements ( Figure S6). The LUMO levels of CP1-CP5 were calculated, E LUMO = −4.80 − (E red − E Fc/Fc+ ), and the HOMO levels were calculated based on E g and LUMOs: E HOMO = E LUMO − E g . Typically, the more negative the value of LUMO is, the higher the reduction ability will be. The results showed that the LUMO levels of CP1-CP5 had sufficient driving force to reduce water to obtain hydrogen. Compared with CP1, CP2, CP4 and CP5, the FMOs of CP3 weree optimal, as its LUMO orbitals made it easier to obtain electrons and its HOMO orbitals made it easier to lose its electrons.
TPR measurement was employed to investigate the photo-to-current conversion efficiencies of CP1-CP5. As shown in Figure 5d, CP1-CP3 showed the maximum photocurrent, which meant that the electron-hole separation efficiency of the CP1-CP3 composite was effectively improved. Furthermore, the TPR current of CP3 was higher than those of CP1 and CP2, which also reflected its highest photocatalytic activity.

Photocatalytic Hydrogen Production Performances of the CPs
The PHP performances of the polymers ( Figure 6) were evaluated by using water and ascorbic acid as a hydrogen source and an SED, respectively. The HERs of CP1-CP5 were 0.00, 1.89, 7.60, 1.17, and 2.47 mmol h −1 g −1 , respectively. The zero HER of CP1 might be ascribed to its being ascribed to its deepest LUMO levels with the smallest driving force for the proton reduction (Figure 5c). It shows that a stronger electron-donor effect is more conducive to affecting the efficiency of hydrogen production. An HER of 7.60 mmol h −1 g −1 for CP3 was achieved, which was much higher than that of other CPs and outperformed most of the reported linear CPs (Table S1). Because the electrondonating ability of thiophene and thiophene is equivalent, it was hard to form a D-A effect for CP2 that could be corroborated by the LUMO level and the HOMO level ( Figure 5c). As revealed by DFT, the major factor on the PHP performance of CP4 and CP5 was the steric hindrance of the building blocks, which was greatly increased after introducing the naphthyl and methyl groups into CP4 and CP5, respectively. The high steric hindrance decreased the planarity and the effective conjugation lengths of the polymeric chains, which was unfavorable to the intramolecular D-A interaction and the internal spatial charge carrier separation; thus, it was less conducive to the surface photocatalytic redox reaction.
Molecules 2023, 28, x FOR PEER REVIEW 7 of 12 optimal, as its LUMO orbitals made it easier to obtain electrons and its HOMO orbitals made it easier to lose its electrons. TPR measurement was employed to investigate the photo-to-current conversion efficiencies of CP1-CP5. As shown in Figure 5d, CP1-CP3 showed the maximum photocurrent, which meant that the electron-hole separation efficiency of the CP1-CP3 composite was effectively improved. Furthermore, the TPR current of CP3 was higher than those of CP1 and CP2, which also reflected its highest photocatalytic activity.

Photocatalytic Hydrogen Production Performances of the CPs
The PHP performances of the polymers ( Figure 6) were evaluated by using water and ascorbic acid as a hydrogen source and an SED, respectively. The HERs of CP1-CP5 were 0.00, 1.89, 7.60, 1.17, and 2.47 mmol h −1 g −1 , respectively. The zero HER of CP1 might be ascribed to its being ascribed to its deepest LUMO levels with the smallest driving force for the proton reduction (Figure 5c). It shows that a stronger electron-donor effect is more conducive to affecting the efficiency of hydrogen production. An HER of 7.60 mmol h −1 g −1 for CP3 was achieved, which was much higher than that of other CPs and outperformed most of the reported linear CPs (Table S1). Because the electron-donating ability of thiophene and thiophene is equivalent, it was hard to form a D-A effect for CP2 that could be corroborated by the LUMO level and the HOMO level ( Figure 5c). As revealed by DFT, the major factor on the PHP performance of CP4 and CP5 was the steric hindrance of the building blocks, which was greatly increased after introducing the naphthyl and methyl groups into CP4 and CP5, respectively. The high steric hindrance decreased the planarity and the effective conjugation lengths of the polymeric chains, which was unfavorable to the intramolecular D-A interaction and the internal spatial charge carrier separation; thus, it was less conducive to the surface photocatalytic redox reaction.
Catalytic cycling stability is an important index to evaluate the practical application of photocatalysts. Here, the cycling test of the highest-performing CP3 was evaluated and it showed no obvious decreasing trend in the continuous photocatalytic reaction ( Figure  6c). After four times cycles, about 80% (0.116 mmol H2 evolution) of CP3 initial H2 evolution was still retained. This showed that CP3 has an excellent cycling stability toward a sacrificial PHP reaction.

Materials and Methods
All of the starting materials and reagents were purchased from commercial suppliers and used directly without further purification.  Catalytic cycling stability is an important index to evaluate the practical application of photocatalysts. Here, the cycling test of the highest-performing CP3 was evaluated and it showed no obvious decreasing trend in the continuous photocatalytic reaction (Figure 6c). After four times cycles, about 80% (0.116 mmol H 2 evolution) of CP3 initial H 2 evolution was still retained. This showed that CP3 has an excellent cycling stability toward a sacrificial PHP reaction.

Materials and Methods
All of the starting materials and reagents were purchased from commercial suppliers and used directly without further purification.
The NMR spectra were carried out on the Bruker Advance III 400 model 400 MHz NMR spectrometer (Germen). The single crystals structural data of CST-BT, CST-BP, and CST-BMP were collected by the Bruker SMART APEX II CCD instrument diffractometer (Germen) at 293 K with Mo Kα radiation upon graphite mono-chromization (λ = 0.71073). To solve the structures of CST-BT, CST-BP, and CST-BMP, the Siemens SHELXTL version 5 crystallographic software package [27] was used. The full-matrix least-squares techniques were used to refine. FT-IR spectra in the range of 4000-500 cm −1 were performed on an FT-IR spectrometer (Bruker, ALPHA). The morphology of the photocatalysts were observed by the SEM (MLA650F, American). The DRS spectra were studied using the UV-2600 scanning UV-vis spectrophotometer. The HORIBA Instruments FL-1000 fluorescence spectrometer was used to characterize PL spectra. The CV measurement was carried out on the CHI660E (Chenhua, Shanghai) electrochemical workstation, which used the normal three-electrodecell system. In the system, glassy carbon electrode was the working electrode, Ag/AgCl electrode was the reference electrode, and platinum wire was the counter electrode. The tetra-n-butylammonium hexafluorophosphate (TBAPF 6 , 1.5 g) was dissolved by the 5 mL acetonitrile as a supporting electrolyte. The electrochemical workstation (CHI650E/700E, Shanghai) was equipped with a conventional three electrode system, which was used to characterize the TPR. In the electrochemical workstation, the configuration Ag/AgCl (saturated with KCl) was the reference electrode and the platinum plate was the counter electrode. A Gaussian 09 program using M062X-D3 density function with the 6-31+G(d,p) basis set was used for the all theoretical calculations [28][29][30]. By frequency analysis at 298 K, the chemical structure was optimized and characterized.

Synthesis of CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP
Monomers CST-BPD, CST-BT, CST-BP, CST-BN, and CST-BMP were synthesized by the same procedure via Knoevenagel condensation [31][32][33][34]. The chemical structures and properties of all the monomers were characterized by 1 H & 13 C NMR (copies of spectra can be found in the Supplementary Materials).
After cooling to room temperature, the reaction mixture was washed by CH 2 Cl 2 and filtered to remove the solvent. The undissolved crude CPs product on the filter paper was washed successively by CH 2 Cl 2 , methanol, water to remove the unreacted small molecules and the inorganic salt, respectively. Then the product was dried in a vacuum for 24 h at 70 • C and obtained the powder of polymers CP1, CP2, CP3, CP4, and CP5 in yields of 23.3%, 93.4%, 77.1%, 93.6%, and 94.2%, respectively.

PHP Tests
A gas chromatograph (GC9790, FuLi) was linked with the photocatalytic online analysis system (LabSolar-III AG, Beijing Perfect Light) for the typical PHP test; it was equipped with the thermal conductive detector (TCD) and used argon as the carrier gas. A mixed aqueous solution containing 30 mL H 2 O and 5 g AA as the sacrificial agent was prepared for the photocatalysts CP1-CP5 (10 mg) ultrasonic dispersal. The KOH solution was added to adjust the pH to 4.0. The oil pump was used to remove the dissolved air in the mixture and maintai in vacuum. To irradiate the reaction vessel, a 300 W Xe lamp (Beijing Perfect Light, PLS-SXE300) under full-arc light irradiation was used. To fix the reaction temperature at 25 • C, a flow of cooling water was used.

Conclusions
A series of tunable linear donor-acceptor conjugated-polymer photocatalysts with CST linkages were designed and facilely synthesized via an atom-and step-economic direct C-H arylation polymerization with the merits of low-cost starting material and high synthetic yields. The opto-electronic properties of CP1-CP5 and their PHP reaction driven by visible light were systematically studied according to several instructive structureproperty-performance correlations. (1) With the enhancement of electron-donating ability along the linear direction, CST-based conjugated polymers can have better photocatalytic performance in hydrogen evolution; (2) The higher the steric hindrance of the donor substituents, the lower the PHP performance of the CST-based CPs; (3) The introduction of phenyl into the CST-based CPs can not only broaden the light-absorption range, but also further improve the photocatalytic reduction ability, which is conducive to improving PHP performance. As a result, CP3 exhibits the highest HER among the five linear CPbased photocatalysts and outperforms most of the reported linear CPs. Such π-conjugated materials with a definite structure offer a new prototype for further developing highefficiency photocatalysts toward solar to chemical energy conversion.