Trifluoromethyl-Substituted Large Band-Gap Polytriphenylamines for Polymer Solar Cells with High Open-Circuit Voltages

Two large band-gap polymers (PTPACF and PTPA2CF) based on polytriphenylamine derivatives with the introduction of electron-withdrawing trifluoromethyl groups were designed and prepared by Suzuki polycondensation reaction. The chemical structures, thermal, optical and electrochemical properties were characterized in detail. From the UV-visible absorption spectra, the PTPACF and PTPA2CF showed the optical band gaps of 2.01 and 2.07 eV, respectively. The cyclic voltammetry (CV) measurement displayed the deep highest occupied molecular orbital (HOMO) energy levels of −5.33 and −5.38 eV for PTPACF and PTPA2CF, respectively. The hole mobilities, determined by field-effect transistor characterization, were 2.5 × 10−3 and 1.1 × 10−3 cm2 V−1 S−1 for PTPACF and PTPA2CF, respectively. The polymer solar cells (PSCs) were tested under the conventional device structure of ITO/PEDOT:PSS/polymer:PC71BM/PFN/Al. All of the PSCs showed the high open circuit voltages (Vocs) with the values approaching 1 V. The PTPACF and PTPA2CF based PSCs gave the power conversion efficiencies (PCEs) of 3.24% and 2.40%, respectively. Hence, it is a reliable methodology to develop high-performance large band-gap polymer donors with high Vocs through the feasible side-chain modification.


Introduction
In the past decades, the photovoltaic cells are one of versatile technologies realizing the clean energy, including the silicon-based inorganic solar cells and carbon-based organic/polymer solar cells [1][2][3]. Among them, bulk-heterojunction polymer solar cells (BHJ PSCs) are becoming an attractive technology both academically and commercially, due to their excellent merits in low cost, flexibility, large-scale fabrication and feasible accessibility of organic chemicals [4][5][6]. Recently, the power conversion efficiencies (PCEs) of BHJ PSCs have been exceeding 14% for the single-junction PSCs [7]. This achievement makes the potential realization in converting the solar power to the electricity for the general marketing application.
Triphenylamine (TPA) is a versatile aromatic moiety which is utilized widely in organic electronics, attributing to its advantages in low cost, feasibly chemical modification, high hole mobility, highly thermal stability and deep highest occupied molecular orbital (HOMO) energy levels [24,25]. The functional molecules prepared from TPA showed high hole transporting ability and high light-emitting properties in organic light-emitting diodes (OLEDs) [26]. Furthermore, the TPA-based conjugated polymers or small molecules can be utilized as electron donors and electron acceptors in PCSs [27,28]. Due to the deep HOMO energy level of TPA unit, the polymers based on TPA also displayed the high open circuit voltages (Vocs) in PSCs [29]. Moreover, the nature of high hole mobility triggers the huge application of TPA-based molecules and polymers as hole transporting layers (HTLs) in organic-halide perovskite solar cells (PVSCs); owing to the introduction of these versatile materials in PVSCs, both of the Vocs and film formability were improved dramatically with the very high photovoltaic performance [30]. Hence, these achievements of TPA-based molecules and polymers in optoelectronic devices will continue the drastic developments of new TPA-based materials via synthetic functionalization. As displayed in Figure 1, the bare TPA unit has the potential modification by anchoring functional groups to improve the optoelectronic properties. For instance, the bare positions of 3-, 4-and 5-are un-functionalized, and they could be modified by introducing the electron-withdrawing or electron-donating groups to tune the energy levels of the targeting polymers. Herein, two large band-gap TPA-based polymers were designed and synthesized. One of them is trifluoromethyl-substituted polymer (PTPACF), and another is bis(trifluoromethyl)-substituted polymer (PTPA2CF). Ascribing to the electron-withdrawing ability of trifluoromethyl group, the HOMO energy levels of PTPACF and PTPA2CF can be tuned to deeper level approaching to about −5.40 eV. Through testing the photovoltaic performance using PTPACF and PTPA2CF as polymer donors and [6,6]-phenyl-C71-butyric acid methyl ester (PC71BM) as the acceptors, the Vocs were Herein, two large band-gap TPA-based polymers were designed and synthesized. One of them is trifluoromethyl-substituted polymer (PTPACF), and another is bis(trifluoromethyl)-substituted polymer (PTPA2CF). Ascribing to the electron-withdrawing ability of trifluoromethyl group, the HOMO energy levels of PTPACF and PTPA2CF can be tuned to deeper level approaching to about −5.40 eV. Through testing the photovoltaic performance using PTPACF and PTPA2CF as polymer donors and [6,6]-phenyl-C71-butyric acid methyl ester (PC 71 BM) as the acceptors, the V oc s were improved to about 1 V. Therefore, this is a reasonable methodology to develop the high-performance polymer donors with high V oc values.

Characterization and Instrumentation
Through utilizing Bruker 300 (or 600) MHz DRX spectrometer (Bruker, Karlsruhe, Germany) with tetramethylsilane (TMS) as the reference, the 1 H nuclear magnetic resonance (NMR) and 13 C NMR spectra were characterized in detail. By using the linear polystyrene (PS) as standards with the tetrahydrofuran (THF) as eluent, the number-averaged molecular weight (M n ) and weight-averaged molecular weight (M w ) of the targeting polymers were tested on a Waters gel permeation chromatography (GPC) system. Cyclic voltammetry (CV) measurement was performed on a CHI600D electrochemical workstation (CH Instruments, Shanghai, China) in a nitrogen-saturated anhydrous acetonitrile solution with a 0.1 mol·L -1 tetrabutylammonium hexafluorophosphates (Bu4NPF6) as electrolyte. In CV test, it is utilized with a standard three electrodes cell, comprising of a platinum (Pt) working electrode, a Pt wire counter electrode, against saturated calomel electrode (SCE) as reference electrode. At the same time, the scan rate was performed at 50 mV·s -1 , and the ferrocene/ferrocenium (Fc/Fc + ) was applied as the internal reference. The results of UV-vis absorption spectra were recorded on a SHIMADZU UV-3600 spectrophotometer (SHIMADZU, Kyoto, Japan). The atomic force microscopy (AFM) under the tapping-mode was carried out on a Veeco Nanoscope V scanning probe microscope, for testing topography and phase images of blending films.

Device Fabrication
All devices were fabricated on indium tin oxide (ITO)-coated glass substrates. A thin-layer (40 nm) of poly (3,4-ethylenedioxythiophene):poly(4-styrenesulfonate) (PEDOT:PSS) (Clevios 4083) was spin-coated onto UV-ozone treated ITO substrates at 4000 rpm for 40 s and then baked at 140 • C for 15 min in air. The solution containing the polymers and PC 71 BM with different weight ratios in o-dichlorobenzene (ODCB) were spin-coated inside a glove-box with nitrogen at 1200 rpm for 40 s to form the active layers (~80 nm). In this study, the conventional device structure was ITO/PEDOT-PSS/active layer/ PFN/Al, where the PFN is poly[(9,9-dioctyl-2,7-fluorene)-alt-(9,9-bis (3 -(N,N-dimethylamino)propyl)-2,7-fluorene)]. The PFN layer with a thickness of about 5 nm was prepared by spin-casting a mixed solution (0.2 mg/ml) in methanol with a trace of acetic acid before the cathode evaporation. Aluminum (80 nm) was utilized as cathode by thermally evaporation under vacuum (~10 −6 torr) with a shadow mask of 0.16 cm 2 . The current-voltage (J-V) curves were measured on a Keithley 2400 multimeter under AM 1.5 G solar illumination at 100 mW cm −2 . The incident photon-to-current conversion efficiency (IPCE) values were recorded by a monochromator under calibrating with a silicon photodiode. Hole mobility data of neat polymer films were measured by field-effect transistors (FETs) method with the device configuration of Al/AlOx:Nd/PMMA/PTPACF or PTPA2CF/Au (W/L = 500 µm/70 µm).

Synthesis
The detailed synthetic routes of polymers are presented in Scheme 1. The polymers PTPACF and PTPA2CF were prepared via the general Suzuki polycondensation in the presence of active Pd(PPh 3 ) 4 as the catalyst. The crude polymers were purified via the Soxhlet extraction by methanol, acetone, hexane and chloroform, respectively. Finally, the chloroform solution containing the polymers was precipitated in methanol to obtain the targeting polymers as the red solids. The PTPACF and PTPA2CF showed high solubility in common organic solvents, such as toluene, tetrahydrofuran, chloroform and chlorobenzene. The molecular weights of PTPACF and PTPA2CF were characterized by the Gel Permeation Chromatography (GPC), using the tetrahydrofuran as the eluent. The measured number-averaged molecular weights (M n s) of PTPACF and PTPA2CF were 9100 and 8400 with the polydispersity index (PDIs) of 1.73 and 1.54, respectively. (See Table 1)

Thermal Stability
In PSCs, the thermal stability of polymers is one of the significant parameters to evaluate the device sustainability and life time, and the highly thermal stability of polymers will permit the high stability of PSCs for longtime application [31][32][33]. In this study, the thermal gravimetric analysis (TGA) was characterized to estimate the thermal stability of PTPACF and PTPA2CF, and the corresponding TGA curves are presented in Figure 2. From the TGA curves, it is found that the degradation temperatures at 5% weight loss of PTPACF and PTPA2CF are 335 and 338 °C, respectively. (See Table 1) These high degradation temperatures indicate that all of the polymers can be stable up to 300 °C.

UV-vis Absorption and Electrochemical Properties
The UV-vis absorption spectra of the polymers in chloroform and in thin film are shown in Figure 3a. The details acquired from UV-vis absorption measurement are summarized in Table 2. From Figure 3a, these two polymers display the classic "double hump" absorption peaks; some are located at short wavelength due to the localized π-π* transition and the others appear at long wavelength resulting from the internal charge transfer (ICT) interaction between the donor and acceptor units [34]. In chloroform solution, PTPACF and PTPA2CF showed the very similar Scheme 1. The synthetic routes for polymers.

Thermal Stability
In PSCs, the thermal stability of polymers is one of the significant parameters to evaluate the device sustainability and life time, and the highly thermal stability of polymers will permit the high stability of PSCs for longtime application [31][32][33]. In this study, the thermal gravimetric analysis (TGA) was characterized to estimate the thermal stability of PTPACF and PTPA2CF, and the corresponding TGA curves are presented in Figure 2. From the TGA curves, it is found that the degradation temperatures at 5% weight loss of PTPACF and PTPA2CF are 335 and 338 • C, respectively. (See Table 1) These high degradation temperatures indicate that all of the polymers can be stable up to 300 • C.

Thermal Stability
In PSCs, the thermal stability of polymers is one of the significant parameters to evaluate the device sustainability and life time, and the highly thermal stability of polymers will permit the high stability of PSCs for longtime application [31][32][33]. In this study, the thermal gravimetric analysis (TGA) was characterized to estimate the thermal stability of PTPACF and PTPA2CF, and the corresponding TGA curves are presented in Figure 2. From the TGA curves, it is found that the degradation temperatures at 5% weight loss of PTPACF and PTPA2CF are 335 and 338 °C, respectively. (See Table 1) These high degradation temperatures indicate that all of the polymers can be stable up to 300 °C.

UV-vis Absorption and Electrochemical Properties
The UV-vis absorption spectra of the polymers in chloroform and in thin film are shown in Figure 3a. The details acquired from UV-vis absorption measurement are summarized in Table 2. From Figure 3a, these two polymers display the classic "double hump" absorption peaks; some are located at short wavelength due to the localized π-π* transition and the others appear at long wavelength resulting from the internal charge transfer (ICT) interaction between the donor and acceptor units [34]. In chloroform solution, PTPACF and PTPA2CF showed the very similar

UV-vis Absorption and Electrochemical Properties
The UV-vis absorption spectra of the polymers in chloroform and in thin film are shown in Figure 3a. The details acquired from UV-vis absorption measurement are summarized in Table 2. From Figure 3a, these two polymers display the classic "double hump" absorption peaks; some are located at short wavelength due to the localized π-π* transition and the others appear at long wavelength resulting from the internal charge transfer (ICT) interaction between the donor and acceptor units [34]. In chloroform solution, PTPACF and PTPA2CF showed the very similar absorption spectra around 363 and 495 nm because of the similarly chemical structures. In solid thin films, both of PTPACF and PTPA2CF give the red-shifted absorption spectra by more than 10 nm, which indicate that they form the π-π stacking between the polymer main chains in the solid state. The onsets of the UV-vis absorption spectra in solid films are 616 and 610 nm, corresponding to the optical band gaps of 2.01 and 2.07 eV for PTPACF and PTPA2CF, respectively [35]. From optical band gaps, it implies that all of these two polymers present the large band gaps. absorption spectra around 363 and 495 nm because of the similarly chemical structures. In solid thin films, both of PTPACF and PTPA2CF give the red-shifted absorption spectra by more than 10 nm, which indicate that they form the π-π stacking between the polymer main chains in the solid state. The onsets of the UV-vis absorption spectra in solid films are 616 and 610 nm, corresponding to the optical band gaps of 2.01 and 2.07 eV for PTPACF and PTPA2CF, respectively [35]. From optical band gaps, it implies that all of these two polymers present the large band gaps.  The HOMO energy levels (EHOMOs) of polymers were demonstrated by cyclic voltammetry (CV) measurement. Electrochemical CV characterization were carried out by the well-known method with the three electrodes of Pt electrode, saturated calomel electrode, and Pt wire utilized as the working electrode, reference electrode, and counter electrode, respectively, and 0.1 mol·L −1 tetrabutylammonium hexafluorophosphate (Bu4NPF6) solution in dry acetonitrile (CH3CN) was used as the electrolyte. The EHOMOs of the polymers were calculated from CV measurements using the oxidation onset potentials relative to ferrocene as an internal standard, and the relative CV curves are shown in Figure 3b. The redox potential of Fc/Fc + internal reference is 0.39 V vs. SCE. The EHOMOs of PTPACF and PTPA2CF, determined by calculating from the empirical formula of EHOMO = −e(Eox + 4.8 − E1/2, (Fc/Fc+)), are −5.33 and −5.38 eV, respectively [36]. As we did not obtain the reductive curves from CV measurements, the lowest unoccupied molecular orbit (LUMO) energy levels (ELUMOs) of polymers were determined by calculating from the formula of ELUMO = Eg, optical + EHOMO, where Eg, optical means the optical band gap. Through the calculation, ELUMOs of PTPACF and PTPA2CF are −3.32 and −3.31 eV, respectively. From CV data, we can see that both of these two polymers show the deep HOMO energy levels, which will potentially realize the high Vocs in these two polymers based PSCs.

Hole Mobility
To evaluate the charge transporting properties of semiconducting polymers, the hole mobility is an important parameter for polymer donors in PSCs. In this study, we acquired the hole mobility data of PTPACF and PTPA2CF by utilizing the field-effect transistors (FETs) method. The detailed FETs properties containing output and transfer characteristics of the PTPACF and PTPA2CF under the device structure of Al/AlOx:Nd/PMMA/PTPACF or PTPA2CF /Au (W/L = 500 μm/70 μm) were displayed in Figure 4, and the hole mobility values were summarized in Table 3. From the FETs characterization, it shows that the hole mobilities are 2.5 ×10 −3 and 1.1 × 10 −3 cm 2 ·V −1 ·S −1 for PTPACF and PTPA2CF, respectively. As a comparison, we can see that the hole mobilities of PTPACF and PTPA2CF coincide with the results based on the TPA-derived polymers published in the literature, The HOMO energy levels (E HOMO s) of polymers were demonstrated by cyclic voltammetry (CV) measurement. Electrochemical CV characterization were carried out by the well-known method with the three electrodes of Pt electrode, saturated calomel electrode, and Pt wire utilized as the working electrode, reference electrode, and counter electrode, respectively, and 0.1 mol·L −1 tetrabutylammonium hexafluorophosphate (Bu 4 NPF 6 ) solution in dry acetonitrile (CH 3 CN) was used as the electrolyte. The E HOMO s of the polymers were calculated from CV measurements using the oxidation onset potentials relative to ferrocene as an internal standard, and the relative CV curves are shown in Figure 3b. The redox potential of Fc/Fc + internal reference is 0.39 V vs. SCE. The E HOMO s of PTPACF and PTPA2CF, determined by calculating from the empirical formula of E HOMO = −e(E ox + 4.8 − E 1/2, (Fc/Fc+) ), are −5.33 and −5.38 eV, respectively [36]. As we did not obtain the reductive curves from CV measurements, the lowest unoccupied molecular orbit (LUMO) energy levels (E LUMO s) of polymers were determined by calculating from the formula of E LUMO = E g, optical + E HOMO , where E g, optical means the optical band gap. Through the calculation, E LUMO s of PTPACF and PTPA2CF are −3.32 and −3.31 eV, respectively. From CV data, we can see that both of these two polymers show the deep HOMO energy levels, which will potentially realize the high V oc s in these two polymers based PSCs.

Hole Mobility
To evaluate the charge transporting properties of semiconducting polymers, the hole mobility is an important parameter for polymer donors in PSCs. In this study, we acquired the hole mobility data of PTPACF and PTPA2CF by utilizing the field-effect transistors (FETs) method. The detailed FETs properties containing output and transfer characteristics of the PTPACF and PTPA2CF under the device structure of Al/AlOx:Nd/PMMA/PTPACF or PTPA2CF /Au (W/L = 500 µm/70 µm) were displayed in Figure 4, and the hole mobility values were summarized in Table 3. From the FETs characterization, it shows that the hole mobilities are 2.5 ×10 −3 and 1.1 × 10 −3 cm 2 ·V −1 ·S −1 for PTPACF and PTPA2CF, respectively. As a comparison, we can see that the hole mobilities of PTPACF and PTPA2CF coincide with the results based on the TPA-derived polymers published in the literature, in which the hole mobilities would be affected efficiently by different modification of substituting groups and co-polymerizing monomers [27,29,37]. Furthermore, the PTPACF gives the twice higher hole mobility than PTPA2CF, which is possibly because PTPACF exists in a better molecular stacking state than PTPA2CF. These high hole mobilities will be potentially beneficial for the charge transport in PSCs and achieving high photovoltaic performance. in which the hole mobilities would be affected efficiently by different modification of substituting groups and co-polymerizing monomers [27,29,37]. Furthermore, the PTPACF gives the twice higher hole mobility than PTPA2CF, which is possibly because PTPACF exists in a better molecular stacking state than PTPA2CF. These high hole mobilities will be potentially beneficial for the charge transport in PSCs and achieving high photovoltaic performance.

Photovoltaic Performance
To study the photovoltaic performance of these two polymers as donors, the PSCs based on PTPACF and PTPA2CF were fabricated under the device structure of ITO/PEDOT:PSS/polymer: PC71BM/PFN/Al, where the PFN is poly[(9,9-dioctyl-2,7-fluorene)-alt-(9,9-bis(30-(N,Ndimethylamino)propyl)-2,7-fluorene)]. The optimized weight ratio of polymer to PC71BM is 1:4. Here, the PSCs were prepared without further post treatment, such as thermal annealing and solvent additives. Moreover, PFN was utilized as a cathode interfacial layer in this device architecture attributing to its versatile functions in protecting active layer when cathode evaporation, and decreasing the work function of cathode and possibly existing the built-in electric fields between the active layer and cathode [38][39][40]. The current density-voltage (J-V) curves and incident photon-tocurrent conversion efficiency (IPCE) curves measured under AM1.5G, 100 mW·cm −2 are shown in Figure 5, and the photovoltaic properties in details are summarized in Table 3. From the photovoltaic

Photovoltaic Performance
To study the photovoltaic performance of these two polymers as donors, the PSCs based on PTPACF and PTPA2CF were fabricated under the device structure of ITO/PEDOT:PSS/polymer: PC 71 BM/PFN/Al, where the PFN is poly[(9,9-dioctyl-2,7-fluorene)alt-(9,9-bis (30- (N,N-dimethylamino)propyl)-2,7-fluorene)]. The optimized weight ratio of polymer to PC 71 BM is 1:4. Here, the PSCs were prepared without further post treatment, such as thermal annealing and solvent additives. Moreover, PFN was utilized as a cathode interfacial layer in this device architecture attributing to its versatile functions in protecting active layer when cathode evaporation, and decreasing the work function of cathode and possibly existing the built-in electric fields between the active layer and cathode [38][39][40]. The current density-voltage (J-V) curves and incident photon-to-current conversion efficiency (IPCE) curves measured under AM1.5G, 100 mW·cm −2 are shown in Figure 5, and the photovoltaic properties in details are summarized in Table 3. From the photovoltaic characterization, it was found that all devices incorporating these two polymers showed short circuit current density (J sc ) at about 6 mA cm −2 , but they gave the quite impressive high V oc values of about 1.0 V resulting from the deep HOMO energy levels of PTPACF and PTPA2CF within the modification by electron-withdrawing trifluoromethyl groups. Both of PTPACF and PTPA2CF shows the higher V oc s than the other published bare TPA-based polymers without any substitution. In these bare TPA-based PSCs, the values of V oc were only located at about 0.9 V [27,29]. The PTPACF-based PSC showed the J sc of 6.42 mA·cm −2 , V oc of 0.98 V, fill factor (FF) of 52.0% and PCE of 3.24%, respectively. On the other hand, the PTPA2CF-based PSC displayed the J sc of 5.81 mA·cm −2 , V oc of 0.99 V, FF of 41.8% and PCE of 2.40%, respectively. From photovoltaic performance, PTPA2CF gives the higher V oc than PTPACF-based PSC, which is possibly because the PTPA2CF has the deeper HOMO energy level than PTPACF. This deeper HOMO energy level may improve the V oc positively in PTPA2CF-based PSC. Furthermore, the high hole mobility of PTPACF also improve the charge carriers transport and helps to explain the high J sc and FF achieved in PTPACF:PC 71 BM-based device. The corresponding IPCE curves in Figure 5b exhibited a broad photoresponse in the range of 300-700 nm for all polymers-based PSCs. Especially for PTPACF:PC 71 BM device, IPCE exceeded 30% from 330 to 580 nm, with a peak of 48% at 470 nm. Therefore, PTPACF based device yielded the highest J sc . The calculated J sc s from the IPCE spectra are in good agreement with the values obtained from J-V measurements.

Atomic Force Microscopy (AFM) Morphologies
To study the interaction of blend films between these two polymers and PC71BM, the Atomic Force Microscope (AFM) images of the blend films are shown in Figure 6. In the topography of Figure  6a,b, the root-mean-square (RMS) roughness of blend films are 0.476, 0.23 nm for PTPACF and PTPA2CF, respectively, which means that PTPACF and PTPA2CF based blend films have quite smoothly topographic morphologies with less obvious density fluctuations. Furthermore, the phase images (Figure 6c,d) display that PTPACF-based blend films give the better nano-scale phase separation, while PTPA2CF-based blend films show worse phase separation and form bigger aggregation that would cause carrier transport limitations and nongeminate recombination seriously, and ultimately decrease the FF values and photovoltaic performance. According to the photovoltaic performance in Table 3, it also depicts that PTPACF exhibits higher FF value than PTPA2CF, ascribing to their better nano-scale phase separation in PTPACF:PC71BM blend film.

Atomic Force Microscopy (AFM) Morphologies
To study the interaction of blend films between these two polymers and PC 71 BM, the Atomic Force Microscope (AFM) images of the blend films are shown in Figure 6. In the topography of Figure 6a,b, the root-mean-square (RMS) roughness of blend films are 0.476, 0.23 nm for PTPACF and PTPA2CF, respectively, which means that PTPACF and PTPA2CF based blend films have quite smoothly topographic morphologies with less obvious density fluctuations. Furthermore, the phase images (Figure 6c,d) display that PTPACF-based blend films give the better nano-scale phase separation, while PTPA2CF-based blend films show worse phase separation and form bigger aggregation that would cause carrier transport limitations and nongeminate recombination seriously, and ultimately decrease the FF values and photovoltaic performance. According to the photovoltaic performance in Table 3, it also depicts that PTPACF exhibits higher FF value than PTPA2CF, ascribing to their better nano-scale phase separation in PTPACF:PC 71 BM blend film.

Conclusions
In summary, two large band-gap polymer donors PTPACF and PTPA2CF with different trifluoromethyl substitution in TPA unit were designed and synthesized. The optical band gaps of PTPACF and PTPA2CF were 2.01 and 2.07 eV, respectively. Ascribing to the introduction of electronwithdrawing trifluoromethyl groups, the PTPACF and PTPA2CF showed deep HOMO energy levels with −5.33 and −5.38 eV, respectively. Through the photovoltaic characterization in BHJ PSCs, these two polymer donors displayed high Vocs approaching to 1 V. These results with high Voc values are very beneficial for the PSCs realizing highly photovoltaic performance. Even though the PCEs of PTPACF and PTPA2CF based PSCs by utilizing PC71BM as electron acceptors are not so high, it may be believed that the higher photovoltaic performance would be achieved in non-fullerene PSCs by using the low band-gap organic acceptors, originating from the versatile merits of PTPACF and PTPA2CF in large band gaps and low HOMO energy levels. Hence, it is a feasibly accessible way to develop high-performance polymer donors via side-chain functionalization in polytriphenylamine derivatives.

Conclusions
In summary, two large band-gap polymer donors PTPACF and PTPA2CF with different trifluoromethyl substitution in TPA unit were designed and synthesized. The optical band gaps of PTPACF and PTPA2CF were 2.01 and 2.07 eV, respectively. Ascribing to the introduction of electron-withdrawing trifluoromethyl groups, the PTPACF and PTPA2CF showed deep HOMO energy levels with −5.33 and −5.38 eV, respectively. Through the photovoltaic characterization in BHJ PSCs, these two polymer donors displayed high V oc s approaching to 1 V. These results with high V oc values are very beneficial for the PSCs realizing highly photovoltaic performance. Even though the PCEs of PTPACF and PTPA2CF based PSCs by utilizing PC 71 BM as electron acceptors are not so high, it may be believed that the higher photovoltaic performance would be achieved in non-fullerene PSCs by using the low band-gap organic acceptors, originating from the versatile merits of PTPACF and PTPA2CF in large band gaps and low HOMO energy levels. Hence, it is a feasibly accessible way to develop high-performance polymer donors via side-chain functionalization in polytriphenylamine derivatives.