Fangyuan
Kang
a,
Jie
Yang
a and
Qichun
Zhang
*ab
aDepartment of Materials Science and Engineering, City University of Hong Kong, Hong Kong, SAR 999077, P. R. China. E-mail: qiczhang@cityu.edu.hk
bCenter of Super-Diamond and Advanced Films (COSDAF), City University of Hong Kong, Hong Kong, SAR 999077, P. R. China
First published on 4th January 2022
Azaacenes have emerged as a new and important class of organic materials, and their synthesis strategies and applications as organic semiconductors have gained significant progress in recent years. Generally, adopting sterically-shielding substituents such as attaching large silylethynyl groups at selected peripheral positions or extending the π-conjugation with pyrene units is the common method used to stabilize larger azaacenes. However, another way to stabilize and enlarge azaacenes, as well as to tune their optical and electronic properties by inserting nonbenzenoid rings such as four-membered rings into the skeletons, has also been developed but has received much less attention. Therefore, in this review, we summarize the recent progress in their syntheses, properties, and applications in organic electronics. Moreover, we highlight the effect of nonbenzenoid units in the systems. Finally, we discuss the current challenges and perspectives through comparison with conventional azaacenes.
Alternatively, introducing nonbenzenoid rings such as four-membered cyclobutadiene (CBD) into conjugated skeletons has been recently demonstrated as an intriguing method to extend the length of π-conjugation and simultaneously increase the stability accounting for the increase of the degree of Clar aromatic sextets.20 This is very important because a larger but stable π-backbone not only favors the intermolecular π–π stacking in solid states but promises a facilely reversible oxidation to its radical cation, thus resulting in their better performance in organic electronics.18 Moreover, the intrinsic non/anti-aromaticity of nonbenzenoid rings leads to the reduced aromaticity of the whole system, resulting in varied HOMO–LUMO energy levels with a reduced band gap,16,21 enhanced conductance,22 and tailored fluorescence.23 Unfortunately, this category of molecules is presently not as popular as their singly annulated homologues in terms of synthesis strategies and applications. Considering their many desirable behaviors, a timely review on their advances is essential and very important.
Here, this review focuses on the synthesis methods, properties, and applications in devices beyond this group of untypical azaacenes. We firstly introduce azaacenes containing a four-membered ring and systematically compare the influence of the inserted cyclobutadiene ring on the resulting materials, then we provide an introduction of azaacenes bearing a five-membered ring. To access the four-membered-ring fused azaacenes, apart from using the classic condensation reactions and Pd-mediated coupling reactions, new methods approaching novel structures include the intramolecular condensation of privileged precursors24 and Pd-mediated arene-oxanorbornene annulation (CANAL).23 Similarly, the newly developed strategy of ruthenium-catalyzed butadiene-mediated benzannulation allows a quick synthesis of azaacenes bearing a five-membered ring with high yields.25 We also include several interesting azaacenes bridged by macrocycles (≥7-membered ring) and highlight their size-dependent properties. It is worth pointing out that some selected molecules in this review may not be as ordered as those formally well-defined (aza)acenes26–37 due to the diverse scaffolds and irregular shapes of the embedded units. Nevertheless, we aim to understand how the inclusion of these unusual rings in azaacenes can modulate their properties and subsequently affect their performance in devices. In addition, due to the small reorganization energies, attractive ionization potentials, favorable FMO energies,38etc.,39 pyrazine-containing azaacenes, also called pyrazinacenes, are becoming the main representatives and receiving the most extensive research interest. Thereby the untypical structures pertaining to this review are also only complementary to those of quinoxaline-type azaacenes.
In 1962, Blatchly et al. synthesized the first unsubstituted biphenylene-containing azaacene 3a through a reaction between biphenylene-2,3-quinone and o-phenylenediamine in acetic acid.48 The as-prepared yellow needles were only characterized by melting point and elemental analysis at that time. Not until 2015 did the Bunz group follow this work, simultaneously obtaining three new biphenylene-containing azaacenes 3b–d with tri(isopropylsilyl)ethynyl (TIPS-ethynyl) substitutions (Scheme 1a).41 Interestingly, the condensation reaction involving biphenylene-2,3-quinone 1 gave the corresponding oxidized forms directly with high yields (68–84%); this was not observed during the synthesis of their relatives 3′ when using ortho-benzoquinone as one of the precursors, where only the N,N′-dihydro intermediates were obtained under this condition.49 This was attributed to the anti-aromatic property of CBD in the system leading to the much higher energy of hydrogenation (−16.7 vs. −26.7 kcal mol−1 for compounds 3d and 3d′, respectively). However, as shown in Scheme 1b, their further exploration was demonstrated when the condensation reaction was conducted between 1 and phenazinodiamine 4. The yield of product 5 dramatically dropped to only 18%.42 In addition, more challenging species of symmetrically bibenzocyclobutadiene end-capped tetraazapentacenes 9a–b were also synthesized via sequential condensation reactions by the same group (Scheme 1c).42 Surprisingly, the overall yield of the three steps for target 9a was two times higher than that of the congener 9b, substantiating that the steric substitutions at the periphery could significantly influence the stability of synthetic intermediates and the resultant azaacenes. Alternatively, 9a could also be obtained by a stepwise coupling between 1 and the diaminoimine 10 in an acceptable yield (Scheme 1d). Apparent redshifts in ultraviolet-visible (UV/Vis) absorption and emission spectra were observed as the enlarging of acene subunits. The maximal absorption bands for 3b–c were 450 nm, 540 nm, and 650 nm, respectively. On the other hand, compared with the corresponding classic azaacenes 3′/TIPS-TAP, the longest absorption wavelength showed a blue shift by 30–40 nm per added benzocyclobutadiene group. Moreover, the biphenylene substitution almost had no impact on the general electrochemical behavior. NICS-calculations suggested that only those benzene rings near the four-membered rings showed the reduced aromaticity, and the aromaticity of the remaining benzene rings was not influenced by the typical π, zz-values of −23 to −34 ppm as the benzene rings in common larger arenes are (Fig. 2a). In all, the aromaticity of the whole molecule was reduced, but it did not compromise the stability of the resulting skeletons, and all the materials exhibited enhanced stability in solid states. Meanwhile, the reduced aromaticity led to the destabilization of the LUMO, which considerably shifted compared with the corresponding classic counterparts. Quantum chemical calculations demonstrated that the HOMO was situated on the heteroacene motif, while the LUMO was distributed over the whole π-system (Fig. 2b), and the unequal distribution suggested their potential n-type semiconductor behaviors. However, the unfavorable stacking modes in the solid state may thwart them as ideal charge transporting materials. Compounds 3b–d and 9a adopted isolated one-dimensional stacks while compound 5 was arranged in a brick wall motif without any interlocking within layers in their single crystals (Fig. 2c).
Fig. 2 (a) NICS (1)πZZ calculations of compounds 3b-d, 5 and 9a compared to benzene A and biphenylene B. (b) Calculated frontier molecular orbital surfaces and LUMO (upper) and HOMO (bottom) energies (in eV) of 3d, 5 and 9a (from left to right). (c) X-ray crystal structure (left) and crystal packing (right) of 5 and 9a from various angles. Adapted with permission from ref. 41 and 42. Copyright 2015 Wiley-VCH. Copyright 2016 Wiley-VCH. |
In 1972, Hermann Pütter constructed an aza analogue of biphenylene 16avia the intramolecular condensation of squaric 1,3-diamidine 15a,24,44 followed by a smooth oxidation with O2. Interestingly, the central CBD was stabilized by two flanked pyrazine rings. Halogenation is a successful strategy to tailor electronic features and π–π stacking modes, thereby improving the electron transporting ability in n-type organic semiconductors.50 Taking advantage of this, in 2015, Yang et al.51 followed Pütter's approach with a slight modification to synthesize a group of chlorinated analogues 16b–f (Scheme 2a). It is worth noting that the cyclization precursor 15, arising from an amine exchange between (chloro)-o-phenylenediamine 14 and intermediate 13,24 was a complicated mixture. Thereby, the regioisomers 16d and 16e were also mixed. All compounds showed good thermal stability in the air even when heated up to 250 °C. The chlorinated 16b–f showed similar UV-Vis absorption as the unsubstituted parent compound 16a with absorption maxima at 449 to 471 nm in solvents. In addition, their intense UV-Vis absorption and red-shifted behavior relative to quinoxaline (Fig. 3a, using 16a as an example) suggested that two quinoxaline subunits were remarkably conjugated via the central CBD. However, this conclusion seemed to directly contradict the analysis of the bond lengths in single crystals (Fig. 3b). As all compounds showed the same molecular backbone in single crystals, compound 16a was taken as a representative. For the four bonds in the CBD ring, half of them (C5a–C5b and C11a–C11b) are 1.5 Å long, which is even longer than the length of the single bond between two sp2-hybridized carbon atoms in a typical non-conjugated system (1.47–1.48 Å). On the other hand, the length of the remaining two bonds (C5a–C5b and C11a–C11b, 1.44 Å) is larger than that of typical aromatic or alkenyl CC double bonds but almost equal to the single bond between two sp2-hybridized carbon atoms in a conjugated system (1.45–1.46 Å). Moreover, the length of the four C–N bonds (1.29–1.30 Å) around the central CBD is not only shorter than the other C–N bonds in the structure, but also shorter than the typical C–N double in imines (1.35 Å). All these suggest that the conjugation between two quinoxaline subunits was very weak. Nevertheless, this contradiction could be explained by the special role of CBD units in the π-system, which often led to a weak conjugation in ground-state geometry in crystal structures but exhibited excited-state aromaticity in the UV-Vis absorption spectra.20,52 The chlorine substituents did stabilize the HOMO and LUMO energy, and the estimated LUMO levels were lowered from −3.92 to −4.14 eV as the number of chlorine substituents increased from 16a to 16f. Their thin films were vacuum-deposited onto a high-k dielectric of 12-cyclohexyldodecylphosphonic acid (CDPA)-pre-treated aluminium oxide and titanium oxide (AlOy/TiOx) as semiconductors in OFETs, where 16e and 16d/16e exhibited a field-effect mobility of 0.23 ± 0.07 and 0.11 ± 0.05 cm2 V−1 s−1, with the best performance up to 0.42, and 0.20 cm2 V−1 s−1 under vacuum (Fig. 3c, Table 1), respectively. However, 16a-c and 16f were insulated, probably due to the face-on orientation or the morphology of isolated crystallites in the thin films.
Fig. 3 (a) UV-Vis spectra for 0.01 mM solutions of 16a in hexane/CH2Cl2 (99:1, v/v) and quinoxaline in hexane. (b) Crystal structure of 16a with highlighted bond lengths. (c) Drain current (IDS) versus gate voltage (VGS) with a drain voltage (VDS) at 50 V for an OTFT of 16e with an active channel of W = 1 mm and L = 50 mm as measured under vacuum. Reproduced with permission from ref. 51. Copyright 2015, Royal Society of Chemistry. |
Compound | Absmax (nm) | Absedge (nm) | Emmax [nm] | E red1 [V] | HOMO [eV] | LUMO [eV] | Gap [eV] | Behavior | Ref. |
---|---|---|---|---|---|---|---|---|---|
a Optical bandgap estimated by its UV-vis spectrum. b Energy level calculated from cyclic voltammograms. c Energy level calculated from CV data and the optical bandgap. d DFT calculation value. PSCs: perovskite solar cells. PCE: power conversion efficiencies; EQEs: maximum external quantum efficiencies; PHOLEDs: phosphorescent organic light emitting diodes. | |||||||||
16e | — | 475 | — | −1.06 | −4.04 | −6.65 | 2.61 | Mobility in OTFTs: μe = 0.42 cm2 V−1 s−1 | 51 |
19a | 570 | — | — | −0.77 | −4.15c | −4.33b | 2.11a | Mobility in OTFTs: μe = (1.5 ± 0.7) × 10−3 cm2 V−1 s−1 | 43 |
19b | 685 | — | — | −0.68 | −4.16c | −4.22b | 1.7a | Mobility in OTFTs: 0.015 ± 0.004 cm2 V−1 s−1 | 43 |
22c | 513 | — | 527 | −1.15 | −6.29d | −3.50d | — | Mobility in OTFTs: 0.13 ± 0.05 cm2 V−1 s−1 | 20 |
27bc | 643 | 584 | 715 | −1.04 | −5.58 | −3.76 | 1.82 | Ambipolar organic semiconductors: μh = 2.77 × 10−4 cm2 V−1 s−1 | 53 |
μ e = 2.81 × 10−4 cm2 V−1 s−1 | |||||||||
32b | 348, 366 | — | 348, 366 | — | −5.33c | −2.03b | — | EQEs in PHOLEDs: 21.4% | 54 |
36d | 642 | 667 | 651 | −0.83 | −5.99c | −4.15b | 1.84a | PCE in OPVs as acceptors: 1.6% | 55 |
43e | 550 | — | — | −0.88 | −6.23d | −3.98d | 2.25 | Mobility in transistors: μe = 0.037 cm2 V−1 s−1 | 56 |
45c | 422 | 610 | — | — | −5.74c | −3.71b | 2.03 | PCE in inverted PSCs: 10.26% | 57 |
47b | 487 | — | 497 | −1.56 | −5.60d | −2.86d | 2.45a | Max. luminance in OLED: 6 kcd m−2 | 58 |
51c | 397 | — | — | −1.90 | −6.03 | −3.78 | 2.25 | Mobility in OTFTs: μe = 0.005 cm2 V−1 S−1 | 59 |
65b | 475, 504 | — | 533 | −1.91 | — | — | 2.33 | Mobility in OFETs: μh = 0.07 cm2 V−1 S−1 | 60 |
67 | 233, 266, 379 | — | — | −1.22 | −5.34 | −3.20 | 2.43a | ON2/ON1/OFF current ratios in memory device: 106.3/104.3/1 | 61 |
The Pd-catalyzed aryl amination is an efficient method to build up pyrazine units in azaacenes. Considering that higher N-heteroacenes can principally feature more extensive electron delocalization and stronger interaction between π-planes in the solid states, this improves the n-type semiconducting performance in devices. Yang et al. synthesized two large π-conjugated systems through Pd-catalyzed coupling reactions (Scheme 2b).43 They firstly prepared the o-brominated intermediate 17 by modifying the synthetic route of 16, which reacted with phenylenediamine derivatives 2 in the presence of Pd(PPh)3 and 1,1′-bis(diphenylphosphino)ferrocene (dppf) to afford dihydro form 18a, partially with or without final compounds 19, and treating the mixture or dihydro form intermediates with MnO2 yielded the final compounds 19 in overall yields of 26–35% after a routine separation. Despite the extended backbone, they displayed a very similar trend in properties as compounds 16. Furthermore, the thin films of 19b had a field-effect mobility of 0.015 ± 0.004 cm2 V−1 s−1 in air, which was 10 times higher than that of 19a. In contrast, the comparing compound 19a′ was an insulator and the field-effect mobility of 19b′ was only (4.1 ± 2.0) × 10−3 cm2 V−1 s−1 in air. Following a similar approach, in 2018, the same group reported four symmetrical cyclobuta[1,2-b:3,4-b′]diphenazine (CBDPs) 22a–d attaching four silylethynyl substitutions on different positions of the terminal rings to understand the effect of the substitution groups at the periphery and the role of the four-membered bridge in π-conjugation (Scheme 2c).20 As expected, properly adjusting the position of silylethynyl substituting groups provided interesting optical and electronic properties. Only 22c showed strong green fluorescence in CH2Cl2 solvent when excited at 513 nm, and the other materials including two comparison compounds exhibited negligible fluorescence. The varied substitutions gave apparent deviation from the FMOs energy levels, and the estimated LUMO levels based on the first reduction potentials for 22a–d were −3.89 eV, −3.95 eV, −3.57 eV, and −3.62 eV, respectively. The dip-coated films of 22b and 22c consisting of crystalline ribbons and fibers were fabricated as n-type semiconductors into OFETs. Compound 22b showed n-type semiconductor behavior with a field-effect mobility of 0.13 ± 0.05 cm2 V−1 s−1 and the highest value of 0.3 cm2 V−1 s−1 in vacuum, while the reference compounds 22a′ and 22c′ showed very poor performance due to their high LUMO energy level, the weak π-overlap in the solid states, and the limited stability of crystalline fibers.
Another apparent advantage of using CBD as the bridge to extend the azaacenes is the maintainability of the linear shape of the skeleton. To investigate the impact of different fusion patterns on the aromaticity of azaacenes, in 2018, the Xia group developed a class of linear, bent and angular-shaped CBD-containing azaacene regioisomers via their previously reported CANAL method.23 As shown in Scheme 3, two linear CBD-containing azaacenes 25a–b were furnished by CANAL between brominated phenazines and oxanorbornenes (oNBE) in the solvent of 1,4-dioxane at 150 °C, following an aromatization with strong acid. The overall two-step yield was as high as 50%. Moreover, the installation of dixylyl groups in compound 25b ensured its solubility. Also, other bent and angular regioisomers 25c–d and 25e could be easily synthesized under similar conditions by adjusting the number and position of the brominated substitutions on the starting materials. As expected, the shape of the backbone significantly influenced the properties of the resultant materials. Compound 25b showed much better stability than these bent or angular isomers and could persist for more than 10 days of light irradiation under ambient conditions without decomposition. Moreover, the as-obtained regioisomers displayed distinct features in absorption and fluorescence emission (Fig. 4a). The linear isomer 25b exhibited strong absorption with λmax = 503 nm and λonset = 523 nm, while the bent and angular isomers 25d and 25e showed broad absorption with a remarkable bathochromic shift due to the symmetry-forbidden HOMO–LUMO transition. Interestingly, only compound 25b showed bright greenish-blue fluorescence with a quantum yield of 0.58. The estimated LUMO level based on cyclic voltammetry was decreased from −3.36 eV to −3.75 eV going from linear to angular isomers. NICS calculations (Fig. 4b) revealed that the enhanced anti-aromaticity as the backbone changed from linear to bent to angular shape resulting in the stabilized LUMO, the reduced bandgap, and the strongly quenched fluorescence.
Fig. 4 (a) UV-Vis absorption spectra of 25b, 25d, and 25e in CHCl3. The inserted photographs are the dilute solutions of 25b, 25d, and 25e (from left to right) under room light and 365 nm UV irradiation. (b) NICS (1)π,ZZ calculations on 25a and 25c. Reproduced with permission from ref. 26. Copyright 2018, American Chemical Society. |
Fig. 6 (a) Normalized (lowest-energy maximum) absorption spectra of 27aa–27ac, 28aa and 3c′ in n-hexane. (b) CV of 27ba–27bc, 27bb, 28ba, and 28c in CH2Cl2 and 0.1 M Bu4NPF6 on a Pt electrode at a scan rate of 50 mV s−1vs. Ag/AgCl wire. (c and d) Absorption spectra and frontier molecular orbital diagram of 27ba–27bc (upper) and 27bb, 28ba, and 28c (bottom) in CH2Cl2. (e) Packing structures of 31 (black, left; red, right, bottom) and 31′ (right, upper) in single crystals. (a) was reproduced with permission from ref. 70. Copyright 2016, American Chemical Society. (b, c, and d) were reproduced with permission from ref. 53. Copyright 2019, Royal Society of Chemistry. (e) was reproduced with permission from ref. 74. Copyright 2008, American Chemical Society. |
Currently, the precise control of energy levels is still quite challenging. Modifying the sp3-hybridized carbon of a five-membered ring can offer very novel structures with interesting characters. For example, introducing the electron-withdrawing carbonyl group on the protruded carbon atom of diazaindenone can not only enhance the electron accepting ability,66,71,72 but also restore the whole conjugated character of resultant azaacenes. In 2019, the Gao group53 synthesized the indanone-fused azaacenes 27ba–bc and 28ba with different end-capped groups via the one-step condensation reactions between aromatic diamines and trione derivative 26b in AcOH under 100 °C (Scheme 4a). In addition, in order to understand the impact of different fused units, 28c fusing with a thienyl unit was also prepared in a similar manner. All compounds exhibited two reversible reduction waves with a slight increase of the first reduction waves in cyclic voltammetry as the size of the acene unit increased, and the values were also more positive relative to the corresponding non-carbonyl group-decorated species 27aa–ac and 28aa,70,73 demonstrating their better electron accepting abilities (Fig. 6b and c). Significant bathochromic shifts were observed in UV/Vis and emission spectra as the acene backbones were enlarged from 27ba to 27bc (Fig. 6d). On the contrary, remarkable redshifts were observed compared with 27aa–ac, corroborating the role of the attached carbonyl group in tuning the electronic delocalization, which was also in accord with the results of DFT calculations. For comparison, 27bc and 28ba were used to investigate their electron and hole mobilities via a space-charge-limited current (SCLC) method. As a result, 27bc and 28ba displayed balanced hole and electron transport characteristics, and the hole and electron mobilities for 27bc were μh = 2.77 × 10−4 cm2 V−1 s−1 and μe = 2.81 × 10−4 cm2 V−1 s−1, respectively. Yamashita's group74 synthesized a series of indenofluorenediones to investigate their FET performance. In order to further increase the electron affinity, diindenopyrazinedione and its difluoride derivative 31 were also prepared via a five-step protocol using commercially available fluorobenzene as the starting materials (Scheme 4b),74 and the critical pyrazine ring was formed by the self-condensation of 2-nitrosoindan-1-one 29. Compared to the non-aza-substituted equivalent 31′, incorporating nitrogen atoms led to a remarkable decrease in reduction potentials. The first and second reduction potentials for 31 and 31′ were −0.7 vs. −1.02 eV, and −1.32 vs. −1.52 eV, respectively, substantiating the N-doping strategy as an effective way to lower the LUMO levels. Single crystals showed that both compounds were planar, and 31′ adopted a face-to-face π-stacking with an interplanar distance of 3.30 Å. On the other hand, 31 displayed polymorphism with two different colored (red and black) single crystals because of the different degrees of overlapping (Fig. 6e). The black crystalline 31 and its non-fluorine derivative,75 as well as 31′, were fabricated on the hexamethyldisilazane (HMDS) treated SiO2/Si substrates in a bottom contact geometry. As expected, all of them showed n-type FET behaviors despite the relatively low performances. The electron mobility of 31′ was 0.17 cm2 V−1 s−1, which was two orders of magnitude higher than 31 and its non-fluorine derivative. However, when fabricated in top contact geometry, the results were totally overturned. The performance for 31 was dramatically improved with a field-effect mobility of 0.17 cm2 V−1 s−1 and on/off ratio of 107, while the value of 31′ was decreased to 6.6 × 10−2 cm2 V−1 s−1 (on/off ratio: ∼104) due to its rough surface leading to the poor contact between the active layer and the electrodes.
Besides the role in tuning energy levels,71,72,76 another advantage of attaching carbonyl groups in the system is to facilitate the post-functionalization of materials. Liu et al.54 spiraled the carbon by reacting diazafluorenone derivatives with lithiated triphenylamine to yield three novel spirocycles, 10-phenyl-10H-spiro[acridine-9,9′-indeno[1,2-b]pyrazine] (SAIP, 32a), 10-phenyl-10H-spiro[acridine-9,11′-indeno[1,2-b]quinoxaline] (SAIQ, 32b) and 10-phenyl-10H-spiro[acridine-9,13′-benzo[g]indeno[1,2-b]quinoxaline] (SABIQ, 32c) (Scheme 5). This novel design produced very different properties relative to those typical N-heteroacenes. Three spiral materials displayed excellent thermal behaviors with decomposition temperatures as high as ∼400 °C due to the rigid and bulky spiro-structures. Their triplet energies (ETs) were calculated to be 2.71 eV for SAIP, 2.47eV for SAIQ, and 2.38 eV for SABIQ based on the first emission peaks in the well-defined Phos spectra, which were lower than their non-aza-substituting analogues77 because of the electron-withdrawing effect of the pyrazine unit. Three compounds were fabricated as host materials in blue, green and red phosphorescent OLEDs (PHOLEDs) to explore their electroluminescence (EL) properties. Due to the high ETs and good thermal stability, SAIP and SAIQ based green and red devices exhibited better performances with maximum CE/PE/EQE values of 62.5 cd A−1/81.5 lm W−1/17.8% and 63.0 cd A−1/82.3 lm W−1/17.9%, respectively. Moreover, their charge transport properties were also investigated by fabricating them as hole-only and electron-only devices. SAIP and SAIQ displayed the bipolar transport characters with the estimated hole- and electron-mobility of μSAIP,h = 6.2 × 10−5 cm V−1 s−1, μSAIP,e = 1.3 × 10−7 cm V−1 s−1; μSAIQ,h = 5.7 × 10−5 cm V−1 s−1, and μSAIQ,e = 3.2 × 10−7 cm V−1 s−1, respectively. Despite the mediocre performances, these studies opened new horizons for potential applications of azaacenes.
The strong tendency to crystallize hampers the applications of azaacenes in modern bulk-heterojunction organic photovoltaic devices (OPVs). Oligomerization is a useful approach to alleviate aggregation and modulate morphology in bulk or mixtures, thus improving the photovoltaic performance. The Bunz group disclosed a series of azaacene dimers (36a–c, 36e) spiro-bridged through two five-membered rings. As shown in Scheme 6, they first prepared the key building block 33 by NaIO4 oxidation of the corresponding tetraol precursor. Its high reactivity but good stability at ambient conditions facilitated the condensation reactions with different diamines, thereby producing the spiro-connected targets with high yields.55,78 In addition, due to the outstanding performance of thiadiazol derivatives as active elements in organic conductors and solar cells,79–82 the analogues of phenazinothiadiazole dimers (36d, 36f) were prepared and studied similarly. It is worth noting that one dimer (36g) bridged by a nonaromatic six-membered ring was also prepared to investigate the impact of the linker on crystallinity. The dimerization almost had no effect on the UV/Vis absorption in solution compared with the corresponding monomers 36′, and the narrowed and well-resolved UV/Vis spectra in spun-cast thin films suggest that they have fewer intermolecular interactions and less π-stacking and thus formed amorphous films, which was supported by polarizing light microscopy (inserted photographs in Scheme 6). In contrast, the companion monomers were often crystalline. All compounds were investigated as electron acceptors in organic bulk heterojunction (BHJ) solar cells by mixing with the donor polymer (PTB7). The rising features below 500 nm from the external quantum efficiency spectra indicated their contribution to the photocurrent generation as acceptors since only negligible absorption came from the donor PTB7 in this spectral range. Among them, 36d displayed a maximum conversion efficiency of 1.62% without extensive optimization.
Scheme 6 Synthetic routes to azaacene dimers 36a–g (inserted photographs are microscopic images of the spin-coated thin films of 36d, 36f, 36g and 36d′, 36e′). Reproduced with permission from ref. 55 and 78. Copyright 2019, John Wiley and Sons. Copyright 2021, Royal Society of Chemistry. |
Recently, Wang et al.63 reported a conjugated diradical 10,12-diaryldiindeno[1,2-b:2′,1′-e]pyrazine (m-DIP2) by simply altering the carbonyl groups with two stabilizing 9-anthryl groups through a two-step reaction (Scheme 7a). Meanwhile, the control molecule of 10,12-diaryldiindeno [1,2-b:1,2′-e] pyrazine (p-DIP) was also prepared for comparison. Surprisingly, m-DIP2 presented a quite stable triplet ground state and could persist for a long time with a half-life time of 22 days under ambient conditions, which was far more stable than the isomer of indeno-[1,2-a]fluorene,62 and one of the slow decomposition compounds was m-DIP-mono2. UV-Vis-NIR absorption spectra showed that the diradical m-DIP2 had a dramatically broadened near-infrared absorption band (up to 1200 nm) driven by the structurally radical character. However, the comparison compound p-DIP only displayed common absorption characteristics as indenofluorene-related structures. An electron paramagnetic resonance experiment is a useful way to detect the radical ground state nature of molecules. A sharp featureless peak in the continuous-wave electron paramagnetic resonance spectra (cw-EPR) demonstrates the open-shell triplet electronic structure of m-DIP2 (Fig. 7a). According to the calculation, the spin density mainly delocalized within the meta-pyrazine motifs (Fig. 7b), and the calculated singlet–triplet gap (ΔES–T) of m-DIP2 was 1.01 kcal mol−1. In addition, nucleus-independent chemical shift (NICS)-XY scans were performed to explain the differences between their electronic structures. The results suggested that the central pyrazine ring in the closed-shell singlet p-DIP was a 4π electron system with anti-aromaticity, while it was a triplet state with 6π electrons in m-DIP1 (simplified molecule of m-DIP2 for calculation). The outer benzenoid rings exhibited significant aromaticity, suggesting m-DIP1 to be a better representative upon Hückel-aromatic rules. Furthermore, a long spin lattice relaxation time (T1) of 4.3 ms and quantum phase memory time (T3) of 3.0 ms were observed in m-DIP2 solution, indicating its promising applications in organic spintronics. Later on, the Bunz group56 did a similar work and successfully synthesized a group of diindenopyrazines 43a–g through three different routes depending on the substitution groups (Scheme 7b). They found that the solubility, redox potentials, and optical properties could be modulated by the introduction of different functional aryl groups on the 6- and 12-positions. Particularly, the absorption of compounds 43d and 43e was the most blue-shifted compared to other compounds due to the larger degree of twisting of the aryl rings with respect to the diindenopyrazine (Fig. 7c), whereas all the compounds exhibited a red-shift in comparison with indenofluorene 43′ because of the favorable planar geometry and electronic effect of the pyrazine ring. Furthermore, their HOMO and LUMO levels were stabilized by the electron-withdrawing pyrazine unit, and the electron affinity of 43e was surprisingly decreased to −4 eV. As a representative, the drop-cast crystalline thin film of 43e was used in transistors and displayed an average mobility of 0.022 cm2 V−1 s−1 with a top mobility of μmax = 0.037 cm2 V−1 s−1. It is worth noting that this un-optimized result was an order of magnitude higher than that of 43′.63
Fig. 7 (a) EPR spectra of m-DIP2 and p-DIP in the Δms = ±1 region (insert: the EPR signal of m-DIP2 in the Δms =±2 region). (b) Theoretical assessment of m-DIP1 and p-DIP. (c) Single crystal structure for 43c and 43d. (a and b) reproduced with permission from ref. 63. Copyright 2021, John Wiley and Sons. (c) was reproduced with permission from ref. 56. Copyright 2021, John Wiley and Sons. |
Fig. 8 SEM images of nanostructured DQNDN nanofibers. At (a) low resolution and (b) high resolution. (c) Device architecture and the PEC cell. (d) The corresponding current density–potential curve of DQNDN. (e) Absorption spectrum of perovskite and bilayer perovskite/QCAPZ thin films in the range of 350–900 nm. (f) Relative PL intensity of perovskite thin films with and without QCAPZ. (g) Device architecture and corresponding energy level diagram. (h) The device performance of a perovskite solar cell employing QCAPZ as the electron-transport layer. (a–d) were reproduced with permission from ref. 88. Copyright 2016, Royal Society of Chemistry. (e–h) were reproduced with permission from ref. 57. Copyright 2016, John Wiley and Sons. |
Very recently, the Krische group25 synthesized a class of highly soluble N-doped rubicenes through their previously reported strategy of ruthenium-catalyzed butadiene-mediated benzannulation. Initially, chemoselective condensation of the critical tetraketone 52 with various 1,2-diamines enabled mono-condensation products 53a–d in good yields (Scheme 9a). However, an additional step of aromatization with 2,3-dichloro-5,6-dicyano-1,4-benzoquinone (DDQ) was needed when saturated vicinal diamines were employed (53d). After that, the butadiene benzannulation of N-doped diketones 53a–d was conducted to form the initial cycloadducts, which readily underwent p-TsOH-catalyzed dehydrative aromatization to provide N-doped rubicenes 55a–d in moderate to good yields. Alternatively, as illustrated in Scheme 9b, the tetraazarubicene 55e could also be effectively achieved via double condensation between tetraketone 52 and 1,2-diaminocyclohexane with comparable yield. Spectroscopic and theoretical research indicated electronic states of the rubicene core was scarcely impacted by the end-capping substituents, whereas the solid-state structures can be varied from a typical herringbone packing motif to a face-to-face arrangement in response to outer π-systems.
In 2018, the Bunz group reported a family of dibenzosuberone-fused N-heteroacenes with negative curvature.91 They first prepared a highly reactive trione 57 by oxidation of dibenzosuberone with SeO2, which could react with different aromatic diamines or tetraamines to give mono- or bissuberones end-capped targets (58a–g) in moderate to high yields (Scheme 10a). Interestingly, according to the UV-Vis spectra, it is easy to find that each added dibenzosuberone exerts a similar impact on the electronic properties as half of the attached benzene ring. For example, the absorption maxima for symmetrical 58f and 58g are 544 and 731 nm, respectively, which are very close to the values of their corresponding hydrocarbon analogues.92,93 All the as-prepared materials, except 58g, exhibited bright fluorescence both in solution and in solid states (Fig. 10a). In particular, the quantum yield of solid-state 58b was up to 0.23, which was much higher than the corresponding simple azaacene.94 Their single crystals could be easily obtained based on their good solubility and stability in ambient conditions. As expected, all species displayed significant negative curvature in the solid state due to the inherent non-planar character of the seven-membered ring. 58c and 58d adopted a kinked brick wall motif with typical π-stacks (Fig. 10b, 58d as an example), combined with their low band gap behaviors, making them promising materials for OFETs.
Fig. 10 (a) Pictures of 58a–g (from left to right) under ambient light (top) and UV-light (bottom, λmax,ex = 365 nm). (b) Single crystal structures and packing of 58d. (c) Different views of the single crystal structures of Di2. (d) Calculated structure and NICS values of Di2 with ghost atoms along the scanned axis through the saddle-shaped cyclooctatetraene-ring. (e) Schematic of bent-to-planar conformational change. (f) Real-time analysis of polystyrene free volume using the N-FLAP dopant. λF: Fluorescence wavelength. (a and b) were reproduced with permission from ref. 91. Copyright 2020, American Chemical Society. (c and d) were reproduced with permission from ref. 95. Copyright 2018, John Wiley and Sons. (e and f) were reproduced with permission from ref. 96. Copyright 2021, American Chemical Society. |
Moreover, the same group also reported several interesting azaacenes bearing an eight-membered ring.95 The three different-sized cyclooctatetraene derivatives (Di1-3) could be synthesized by smooth coupling between tetrabromide 59 and the corresponding diamino-arenes in the presence of a highly loaded catalyst of PdRuPhos in yields ranging from 21 to 28% after oxidation with MnO2 (Scheme 10b). It was noted that mono-coupled compound Di2b was one of the by-products during the synthesis of Di1. As a representative, Di2 displayed a typical saddle-shaped structure in the solid state (Fig. 10c). The NICS scan of Di2 presented a variation of the aromatic character along the scanned axis through the saddle-shaped cyclooctatetraene-ring (Fig. 10d). Obviously, the positive values in the saddle region corroborated the anti-aromatic property of the cyclooctatetraene unit. Very recently, Saito and coworkers96 developed a dual fluorescent flapping molecular probe (N-FLAP) to monitor the dynamic polymer free volume by single-molecule spectroscopy (Scheme 10c). The introduction of nitrogen atoms into the backbone not only alleviated undesired photoreactions, but also enabled efficient visible excitation, leading to a significant improvement in brightness (22 times) compared to the previously reported flapping anthracene analogue. When it was dispersed in a spin-coated polystyrene thin film to determine the polymer free volume, due to the presence of the bridging cyclooctatetraene ring, a bent-to-planar conformational change could take place in the lowest singlet excited state (S1), and more importantly, it immediately went back to the most stable V-shaped structure in the singlet ground state (S0), resulting in frequent jumps between short- and long-wavelength form in single molecular fluorescence spectra (Fig. 10e). As the dynamic planarization process requires certain free space, which can be driven by the segmental relaxation of surrounded polymers (Fig. 10f), the polymer-free volume was thus roughly determined according to the time intervals of the green fluorescence excitation and emission in a flapping molecular probe.
In all, diverse structures of heterocycles significantly enrich this sub-class of azaacenes. Concomitantly, the special properties of newly introduced heterocycles often induce very different behaviors from the typical azaacenes. Moreover, the properties of the resultant materials are sometimes even dominated by the additional heterocycles, which provides possibilities to get unexpected performances in devices. No doubt, their distinctive properties will continue to captivate new generations of researchers.
As mentioned in this review, many strategies such as chlorine substitution, thiadiazol fusing and dimerization have been attempted in order to improve the performance of the resulting materials in devices. There is no doubt that most of the disclosed device performances are still not satisfactory. Therefore, there is still great potential for investigation of many aspects. Future research efforts should first focus on developing powerful methods to approach the processable and stable molecules with novel skeletons, as well as to improve the performance in organic electronics. Besides, despite the investigation of traditional photoelectric and photophysical property-based devices such as OFETs, solar cells and OLEDs, emphasizing their inherent characters such as structural curvature effect, anti-aromatic and diradical properties and developing related applications may provide more exciting results. Along this direction, we believe that increasing scientific interest will be focused in this direction as a result of the property-based advantages over their classic congeners.
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