Open AccessCCS ChemistryCOMMUNICATIONS2 Sep 2022Phosphonium-Based Ionic Thermally Activated Delayed Fluorescence Emitters for High-Performance Partially Solution-Processed Organic Light-Emitting Diodes Xu-Lin Chen, Xiao-Dong Tao, Ya-Shu Wang, Zhuangzhuang Wei, Lingyi Meng, Dong-Hai Zhang, Fu-Lin Lin and Can-Zhong Lu Xu-Lin Chen State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Fujian Science & Technology Innovation Laboratory for Optoelectronic Information of China, Fuzhou, Fujian 350108 Google Scholar More articles by this author , Xiao-Dong Tao State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Google Scholar More articles by this author , Ya-Shu Wang State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Google Scholar More articles by this author , Zhuangzhuang Wei State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Google Scholar More articles by this author , Lingyi Meng State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Google Scholar More articles by this author , Dong-Hai Zhang State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Google Scholar More articles by this author , Fu-Lin Lin State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Google Scholar More articles by this author and Can-Zhong Lu *Corresponding author: E-mail Address: [email protected] State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian 350002 Xiamen Key Laboratory of Rare Earth Photoelectric Functional Materials, Xiamen Institute of Rare Earth Materials, Haixi Institutes, Chinese Academy of Sciences, Xiamen, Fujian 361021 Fujian Science & Technology Innovation Laboratory for Optoelectronic Information of China, Fuzhou, Fujian 350108 Google Scholar More articles by this author https://doi.org/10.31635/ccschem.022.202202145 SectionsSupplemental MaterialAboutAbstractPDF ToolsAdd to favoritesDownload CitationsTrack Citations ShareFacebookTwitterLinked InEmail Ionic thermally activated delayed fluorescence (TADF) emitters are rarely investigated due to their poor photoluminescence and electroluminescence performance. Herein, highly efficient ionic TADF emitters with charged donor–acceptor (D–A+) and D–A+–D architectures are designed, innovatively based on the phosphonium cation electron acceptor. The symmetric D–A+–D compound in doped film exhibits a high photoluminescence quantum yield of 0.91 and a short emission lifetime of 1.43 microseconds. Partially solution-processed organic light-emitting diodes based on these ionic TADF emitters achieve a maximum external quantum efficiency (EQE) of 18.3% and a peak luminance of 14,532 candelas per square meter (cd/m2) and show a small efficiency roll-off of 7.1% (EQE = 17%) at a practical high luminance of 1000 cd/m2. These results demonstrate the high potential of phosphonium cations as promising electron acceptors to construct TADF emitters for high-performance electroluminescence devices. The current study opens up an appealing way for future exploitation of high-efficiency ionic TADF materials. Download figure Download PowerPoint Introduction Thermally activated delayed fluorescence (TADF) molecules have been developed as third-generation organic light-emitting diode (OLED) emitters, owing to their potential to realize an internal quantum efficiency of unity without using noble metals.1,2 While numerous highly efficient TADF-based OLEDs have been reported to date, some key challenges remain to be tackled for practical applications.3 For example, TADF-OLEDs usually suffer from severe efficiency roll-off during high-luminance operations owing to exciton annihilation.4–6 To prevent the formation of high-energy excitons and reduce efficiency roll-off in OLEDs, efficient TADF emitters with short emission lifetimes7–10 and fast reverse intersystem crossing (RISC)11–14 are highly desired. TADF emitters are generally composed of suitable electron-donor (D) and electron-acceptor (A) moieties that can create spatial separation of the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO). Finding the ideal D and A species is the priority in order to exploit TADF molecules. Unlike electron donors that are almost limited to arylamine derivatives,15 a wide variety of electron acceptors based on main-group elements have been utilized to construct TADF emitters,16 including arylboron,17–22N-heterocycle,23–26 cyano,1,27,28 sulfone,29 carbonyl30–35 groups, and so on. To date, the vast majority of TADF materials are constructed based on neutral D and A moieties ( Supporting Information Figure S5). Charged luminescent materials (e.g., cyanines, rhodamines, ionic metal complexes, etc.) have been utilized in versatile photonic applications due to their ionic nature, diverse photophysical properties, and unique solubility. For instance, many ionic organic dyes have been ultilized as chemosensors in living systems because of their excellent photophysical properties, appreciable water solubility, and biocompatibility.36,37 Ionic transition metal complexes have been employed as emitters in light-emitting electrochemical cells.38 Ionic luminescent compounds are often overlooked in OLED applications, owing to their poor photoluminescence/electroluminescence (PL/EL) properties and inability to be processed via vacuum deposition. However, their intrinsic ionic nature and unique solubility may offer possibilities for developing multilayer solution-processed OLEDs. Recently, a few ionic TADF materials39–47 containing anion/cation moieties or D/A ion-pairs have revealed their potential for PL and EL applications. Nevertheless, it remains a formidable challenge to realize high-performance OLEDs based on ionic TADF emitters ( Supporting Information Table S8). Owing to its 3s23p3 valence shell, phosphorus favors valences ranging from 3 to 5 in organophosphorus compounds. The lone-pair electrons can make trivalent phosphorus atoms act as a donor in organophosphorus molecules, but oxidation to pentavalent phosphine oxide or arylation/alkylation to tetravalent phosphonium cations drastically changes its properties to a typical electron acceptor. Compared with phosphine oxide, which has usually been employed as a weak electron-deficient unit to build n-type and ambipolar host materials for OLEDs,48,49 the phosphonium cation is a noticeably stronger electron acceptor,50,51 offering appealing opportunities to yield visible-light emitters with strong intramolecular charge-transfer (ICT) character. For example, Koshevoy and coworkers52,53 recently reported the unique PL behaviors in solvents of a series of D–π–A fluorophores containing phosphonium cation acceptors. Inspired by the intrinsic electron-deficient property of phosphonium cations, we have selected tetraphenylphosphonium cation as acceptor and designed two ionic TADF materials, namely DMAC-TPP[PF6] and 2DMAC-TPP[PF6] (Figure 1a). These emitters exhibit efficient TADF in doped films with high photoluminescence quantum yields (PLQYs) and short emission lifetimes. Partially solution-processed OLEDs based on these emitters achieve high external quantum efficiencies (EQEs) with only minor efficiency roll-off, demonstrating the high potential of phosphonium cation electron acceptors for the construction of high-performance ionic TADF materials. Figure 1 | (a) Chemical structures; (b) frontier orbital distributions (left: DMAC-TPP[PF6]; right: DMAC-TPP[PF6]); (c) crystal structure (DMAC-TPP[PF6]). Download figure Download PowerPoint Results and Discussion The electronic properties of these compounds were investigated by density functional theory (DFT) and time-dependent DFT (TD-DFT) calculations at the M06-2X/6-311G(d,p) level. As shown in Figure 1b, each compound shows spatially separated frontier molecular orbitals, with the HOMO predominantly distributed over the acridinyl unit and the LUMO mainly located on the remainder of the molecule. The TD-DFT calculations predict that the S1 and T1 states are characterized by HOMO–LUMO ICT transitions Supporting Information Figure S1, with S1–T1 energy difference (ΔEST) of 0.07 eV for DMAC-TPP[PF6] and 0.01 eV for 2DMAC-TPP[PF6], respectively. Owing to the symmetrical molecular structure, the excited states of 2DMAC-TPP[PF6] appear in pairs degenerately (S1/S2, T1/T2, T3/T4, etc.). The calculated energy levels of excited states and spin–orbit coupling (SOC) constants are summarized in Supporting Information Table S1. For 2DMAC-TPP[PF6], the total SOC between S1/S2 and T1/T2 states which have dominant CT exciton characters was calculated to be 0.145 cm−1, while the calculated SOC between S1/S2 and higher-lying triplet states, namely T3/T4 and T5/T6, reach up to 3.807 and 4.021 cm−1, respectively. The same situation exists in the case of DMAC-TPP[PF6] with SOCS1–T1, SOCS1–T2, and SOCS1–T3 of 0.270, 1.946, and 1.171 cm−1, respectively. The first-order mixing coefficient between singlet and triplet states is proportional to their spin–orbit interaction and inversely proportional to the energy gap between them.2 Considering the large energy gaps (over 0.5 eV) between the higher-lying triplet states and S1 states, we speculate that the small ΔEST rather than the higher-lying triplet states play a key role in spin-flip conversion between the S1 and T1 states. These tetraarylphosphonium salts were synthesized in high yields via nickel-catalyzed coupling reactions52,54 between triarylphosphines and aryl bromides and the subsequent anion-exchange reactions (see Supporting Information for details). These compounds are quite air stable in the solid state as well as in solution. The powders survive in ambient conditions without decomposition over at least several months. As depicted in Supporting Information Figure S2, DMAC-TPP[PF6] and 2DMAC-TPP[PF6] show excellent thermal stability with high decomposition temperatures (Td, 5% weight loss) of 399 and 394 °C, respectively. Atomic-force microscopy (AFM) images ( Supporting Information Figure S3) reveal that the spin-coated doped films of these materials (30 wt % in PYD2, the same as the OLED-emitting layers) show fairly smooth surfaces with small root-mean-square surface roughness (Rq) values of 0.246 and 0.256 nm for DMAC-TPP[PF6] and 2DMAC-TPP[PF6], respectively. The excellent thermal stability and high-quality film morphologies support EL device fabrication via solution processes. The crystal structure of DMAC-TPP[PF6] (Figure 1c) reveals that the phosphorus atom (sp3-hybridization) adopts tetrahedral geometry with tetrahedral angles of approximately 109°. The cationic moiety exhibits nearly perpendicular D–A linkage with a dihedral angle of 81.4°, which can result in spatially well-separated frontier molecular orbitals and small ΔEST. Moreover, there exist significant intramolecular (Figure 1c) and intermolecular interactions ( Supporting Information Figure S4) in the lattice, which are expected not only to suppress nonradiative deactivation by rigidifying molecular conformation but also to facilitate the formation of high-quality thin films.55,56 The photophysical properties of these emitters were investigated in dichloromethane and 30 wt %-doped polymethyl methacrylate (PMMA) films. Both compounds exhibit similar absorption profiles, composed of two types of absorption bands (Figure 2a). The intense absorptions below 370 nm are assigned to the π–π* transition originating from the donor moieties while the much weaker absorption bands between 370 and 460 nm are attributed to the ICT transitions from the DMAC donor(s) to the tetraphenylphosphonium acceptor. From the onset of absorption spectra ( Supporting Information Figure S5), optical bandgaps (Eg) were calculated to be 2.76 and 2.74 eV for DMAC-TPP[PF6] and 2DMAC-TPP[PF6], respectively. The increased number of donors results in slightly red-shifted absorption bands. These compounds exhibit strong yellow emission (λmax = 563 and 567 nm, respectively) in degassed dichloromethane at room temperature. The broad and structureless PL spectra as well as their solvent-polarity-dependent behaviors ( Supporting Information Figure S14 and Table S4) confirm CT characteristics of the emissive states. The transient PL decay curves of the investigated emitters in dichloromethane before and after Ar bubbling were compared to verify the involvement of triplet states in the light-emitting process (Figure 2b). A conspicuous delayed decay with significantly increased intensity was observed after 15 min of Ar bubbling to remove dissolving oxygen which can quench the triplet excited states of emitters. This behavior clearly confirms the contribution of triplet states to the fluorescence processes. Remarkably, the delayed decay components of DMAC-TPP[PF6] and 2DMAC-TPP[PF6] in degassed dichloromethane were fitted with ultrashort single-exponential lifetimes of 600 and 549 ns ( Supporting Information Figures S9 and S10), respectively. Figure 2 | (a) Absorption and PL spectra measured in dichloromethane (c = 2 × 10−5 M) at room temperature; (b) transient PL decay curves in dichloromethane (c = 2 × 10−5 M) before/after Ar bubbling for 15 min at room temperature; (c) transient PL decay curves of 2DMAC-TPP[PF6] in 30 wt %-doped PMMA film at different temperatures; (d) time-resolved PL spectra in the 30 wt %-doped PMMA films at 77 K. Fluo.: fluorescence; Phos.: phosphorescence. The PL measurements were excited at 335 nm. Download figure Download PowerPoint The 30 wt %-doped PMMA films of DMAC-TPP[PF6] and 2DMAC-TPP[PF6] display bluish-green PL with emission maxima of 511 and 514 nm ( Supporting Information Figure S11 and Table 1) and PLQYs of 0.75 and 0.91, respectively. Compared with those recorded in dilute solution, for example, in dichloromethane, ethanol, and acetonitrile ( Supporting Information Figure S14 and Table S4), the PL spectra in 30 wt %-doped PMMA films significantly blue-shift. This behavior probably originates from two contributions. First, the solvation effect on the CT-excited states is considerably weakened in the doped nonpolar polymer films. Second, in the more rigid environment of the polymer films, intramolecular rotations and excited-state distortions are effectively restricted, thereby decreasing the vertical transition energies from the emissive ICT states (S1) to ground state (S0), resulting in significantly blue-shifted PL spectrum maxima. As shown in Figure 2c and Supporting Information Figure S12, temperature dependence of transient PL decay reveals that the intensity ratio of delayed fluorescence to prompt fluorescence increased when temperature was increased from 77 to 300 K. At ambient temperature (300 K), the observed emission originates from the S1 state, which is significantly populated via thermally-activated upconversion from the energetically lower-lying T1 state, demonstrating the TADF process. From onsets of the time-resolved PL spectra (fluorescence and phosphorescence spectra) taken at 77 K (Figure 2d and Supporting Information Figure S6), S1 and T1 energies and ΔEST are estimated to be 2.88, 2.82, and 0.06 eV for DMAC-TPP[PF6] and 2.86, 2.81, and 0.05 eV for 2DMAC-TPP[PF6], respectively. Such small ΔEST values would facilitate rapid upconversion of excitons from T1 to S1 through RISC process.57 At 300 K, the prompt fluorescence lifetimes (τPF) and delayed fluorescence lifetimes (τDF) were measured to be 16.6 ns and 1.67 μs for DMAC-TPP[PF6], and 18.2 ns and 1.43 μs for 2DMAC-TPP[PF6], respectively (see Supporting Information for detailed decay-curve fitting). The emission lifetimes are as short as those of representative phosphorescence Ir(III) complexes.58,59 Based on the PLQY and lifetime data, rate constants of the key photophysical processes were estimated using a previously reported method derived by Tsuchiya et al.60 (see Supporting Information for details). The radiative decay rate constants ( k r S ) from S1 to S0 are nearly the same and exceed 1.7 × 107 s−1 for both compounds, which are much higher than corresponding nonradiative rate constants ( k nr S ) (5.80 × 106 and 1.69 × 106 s−1 for DMAC-TPP[PF6] and 2DMAC-TPP[PF6], respectively). The ISC process of each compound (kISC = 2.75 × 107 s−1 for DMAC-TPP[PF6] and kISC = 3.51 × 107 s−1 for 2DMAC-TPP[PF6]) is much faster than its competitive processes, namely the radiative and nonradiative transition of the S1 state, implying that the initially generated singlet excitons in these compounds are significantly transformed to triplet excitons. Notably, the rate constants of RISC (kRISC) of DMAC-TPP[PF6] and 2DMAC-TPP[PF6] reach up to 1.55 × 106 and 2.05 × 106 s−1, respectively. Fast radiative transition together with fast RISC of these emitters result in efficient utilization of excitons and short exciton lifetimes.61 Table 1 | Photophysical Data of the Invesigated Compounds in 30 wt %-Doped PMMA Films at 300 K Compound λPLa (nm) ΦPLb ΦPF/ΦDFc τPF/τDFd (ns/μs) ES1/ET1/ΔESTe (eV) k r S / k nr S f (106 s−1) kISC/kRISCg (106 s−1) DMAC-TPP[PF6] 511 0.75 0.29/0.46 16.6/1.67 2.88/2.82/0.06 17.5/5.80 27.5/1.55 2DMAC-TPP[PF6] 514 0.91 0.31/0.60 18.2/1.43 2.86/2.81/0.05 17.0/1.69 35.1/2.05 aThe wavelength at PL maximum (excited at 335 nm). bOverall PLQY. cΦPF and ΦDF are the quantum yields of prompt fluorescence and delayed fluorescence, respectively. dτPF and τDF are the lifetimes of prompt fluorescence and delayed fluorescence, respectively. eEnergy levels of S1 and T1 state were estimated from the onsets of time-resolved PL spectra at 77 K ( Supporting Information Figure S6). f k r S and k nr S represent the radiative and nonradiative rate constants of S1 states, respectively. gkISC and kRISC refer to the rate constants of intersystem crossing (ISC) and reverse ISC, respectively. The film thickness of samples was 100 nm. To evaluate EL properties of these emitters, partially solution-processed OLEDs were fabricated with a device structure of indium tin oxide (ITO)│poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) (30 nm)│poly[(9,9-dioctylfluorenyl-2,7-diyl)-co-(4,4′-(N-(4-sec-butylphenyl) diphenylamine)] (TFB) (10 nm)│PYD2: emitter (7:3, 40 nm)/m4PO (8 nm)│TPBi (45 nm)│LiF (1 nm)│Al (100 nm) (Figure 3a), where PEDOT:PSS, TFB, m4PO,62 TPBi, and LiF, act as the hole-injection, hole-transporting, hole-blocking, electron-transporting, and electron-injection layers, respectively ( Supporting Information Figure S16). PYD263 was selected as a host material due to its high triplet energy (T1 = 2.93 eV), which is conducive to confining triplet excitons of the investigated greenish-blue emitters (T1 = 2.81–2.82 eV), and due to its proper HOMO and LUMO energies (EHOMO/ELUMO = −5.7 eV/−2.3 eV) which fit the corresponding values of the emitters and adjacent layers for effective carrier transporting. The host–guest ratio was optimized ( Supporting Information Table S7 and Figures S17–S18). The results show that 30 wt % doped devices achieved the best device performance with efficient host to guest energy transfer. The HOMO and LUMO levels of DMAC-TPP[PF6] and 2DMAC-TPP[PF6] were estimated from the oxidation potentials and optical bandgaps ( Supporting Information Figures S15 and Tables S6). EL performances are shown in Figure 3b–d and Table 2. Figure 3 | (a) Energy-level diagram of the OLEDs; (b) current density–voltage–luminance characteristics; (c) EL spectra at various voltages; (d) EQE, current efficiency (CE) and power efficiency (PE) versus luminance characteristics. Download figure Download PowerPoint Table 2 | Summary of Device Performances Device (30 wt %-Doped) λELa (nm) Vonb (V) Lmaxc (cd/m2) EQEd (%) CEe (cd/A) PEf (lm/W) CIE1931g (x, y) DMAC-TPP[PF6] 508 5.0 9496 15.3/13.6/9.9 42.7/37.9/27.6 19.2/10.6/6.0 (0.25, 0.47) 2DMAC-TPP[PF6] 512 4.7 14532 18.3/17.0/13.2 53.4/49.5/38.5 26.0/15.2/9.3 (0.27, 0.49) aThe wavelength at EL maximum (recorded at 12 V). bTurn-on voltage at 1 cd/m2. cMaximum luminance. dEQE maximum value, value at 1000 cd/m2 and value at 5000 cd/m2. eCE maximum value, value at 1000 cd/m2, and value at 5000 cd/m2. fPE maximum value, value at 1000 cd/m2, and value at 5000 cd/m2. gCIE coordinates measured at 12 V. The 30 wt %-doped OLEDs employing DMAC-TPP[PF6] and 2DMAC-TPP[PF6] turned on at approximately 4.7 and 5.0 V, and exhibited bluish-green EL with emission maxima of 508 nm [Commission Internatinale de L’Eclairage (CIE) = 0.25, 0.47] and 512 nm (CIE = 0.27, 0.49), respectively. It is particularly worth mentioning that these devices exhibited perfect emission-color stability over a wide range of operating voltages (Figure 3c). The DMAC-TPP[PF6]- and 2DMAC-TPP[PF6]-based devices showed maximum EQEs of 15.3% and 18.3% and peak luminances of 9496 and 14532 cd/m2, respectively. The DMAC-TPP[PF6]-based device exhibits efficiency roll-offs of 11.1% (EQE = 13.6%) and 35.3% (EQE = 9.9%) at luminances of 1000 and 5000 cd/m2, respectively. Notably, the 2DMAC-TPP[PF6]-based device reached the maximum EQE at a luminance of 117 cd/m2 and showed low efficiency roll-offs of 7.1% (EQE = 17.0%) and 27.9% (EQE = 13.2%) at practical high luminances of 1000 and 5000 cd/m2, respectively. These device efficiencies and efficiency roll-offs represent the best device performance of ionic-TADF-emitter-based OLEDs hitherto and are comparable with those state-of-the-art partially solution-processed OLEDs based on neutral TADF emitters ( Supporting Information Table S8). The small efficiency roll-offs obtained at high luminances can mainly be attributed to the short-lived TADF emitters, which can alleviate the exciton annihilation in the emitting layers. Conclusion Tetraphenylphosphonium cation has been used as the electron acceptor to construct highly efficient ionic TADF emitters with D–A+ and D–A+–D architectures. These ionic TADF emitters, namely DMAC-TPP[PF6] and 2DMAC-TPP[PF6], show high PLQYs of 0.75 and 0.91 and short decay fluorescence lifetimes of 1.67 and 1.43 μs in doped films, respectively. High EL performance has been achieved in partially solution-processed OLEDs. 2DMAC-TPP[PF6]-based device realized EQEmax of 18.3% and peak luminance of 14532 cd/m2. More importantly, the EQE values remain high with only tiny efficiency roll-off even at practical high luminances. Our results suggest that cationic acceptors are a promising choice for the design of high-performance TADF materials and that this research opens an avenue for designing new ionic TADF materials. Supporting Information Supporting Information is available and includes general methods, detailed synthetic procedures, computational methodology and results, photophysical properties, analysis of rate constants, thermogravimetric analysis curves, AFM images, cyclic voltammetry, X-ray crystallographic analyses (see the Cambridge Crystallographic Data Centre at www.ccdc.cam.ac.uk, CCDC 2141438), device fabrication and characterization, device performance comparisons, 1H NMR spectra, and mass spectra. Conflict of Interest There is no conflict of interest to report. Funding Information This research was made possible as a result of a generous grant from the Key Research Program of Frontier Science, the Chinese Academy of Sciences (CAS) (grant no. QYZDJ-SSW-SLH033), the National Natural Science Foundation of China (grant no. 52073286), the Natural Science Foundation of Fujian Province (grant no. 2006L2005), the Fujian Science and Technology Innovation Laboratory for Optoelectronic Information of China (grant nos. 2021ZR132 and 2021ZZ115), the Youth Innovation Foundation of Xiamen City (grant nos. 3502Z20206082 and 3502Z20206083), and the Major Research Project of Xiamen (grant no. 3502Z20191015).
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