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Multifunctional Porous Hydrogen-Bonded Organic Frameworks: Current Status and Future Perspectives
Zu-Jin Lin, Shaheer A. R. Mahammed, Tian-Fu Liu and 1 more
ACS Central Science · 2022 · Review
doi:10.1021/acscentsci.2c01196
Abstract
Hydrogen-bonded organic frameworks (HOFs), self-assembled from organic or metalated organic building blocks (also termed as tectons) by hydrogen bonding, π-π stacking, and other intermolecular interactions, have become an emerging class of multifunctional porous materials. So far, a library of HOFs with high porosity has been synthesized based on versatile tectons and supramolecular synthons. Benefiting from the flexibility and reversibility of H-bonds, HOFs feature high structural flexibility, mild synthetic reaction, excellent solution processability, facile healing, easy regeneration, and good recyclability. However, the flexible and reversible nature of H-bonds makes most HOFs suffer from poor structural designability and low framework stability. In this Outlook, we first describe the development and structural features of HOFs and summarize the design principles of HOFs and strategies to enhance their stability. Second, we highlight the state-of-the-art development of HOFs for diverse applications, including gas storage and separation, heterogeneous catalysis, biological applications, sensing, proton conduction, and other applications. Finally, current challenges and future perspectives are discussed.
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From PubMed Central, U.S. National Library of Medicine, as current on Oct 24, 2026. Paragraph numbers are ours, so an answer can point at one.
Introduction
Porous materials have been widely utilized in modern industry, being indispensable in our daily life. In the last three decades, great progress has been achieved in a special type of porous materials that have order structures and contain organic components, which can be divided into metal–organic frameworks (MOFs, also known as porous coordination polymers), covalent organic frameworks (COFs), and hydrogen-bonded organic frameworks (HOFs). They are usually constructed by predesigned organic building blocks and preconceived topologies. Therefore, these materials have much richer structural diversity, higher structural flexibility, and larger structural tunability than traditional inorganic porous materials like zeolites and porous carbons. Through either one-pot synthesis or postsynthesis, the porosity, surface area, pore size and shape, and even the chemical functionality of the MOFs/COFs/HOFs can be tailored for various applications, such as gas storage and separation, catalysis, drug delivery, sensing, etc.
HOFs are often prepared by self-assembling elegantly predesigned organic or metalated organic building blocks (also termed tectons) via hydrogen bonding, π–π packing, and other intermolecular interactions. The concept of HOFs was coined by Chen et al. in 2011. They reported the first HOF (i.e., HOF-1) with permanent porosity, which was used as a solid absorbent for highly selective adsorptive separation of C2H2 and C2H4 at room temperature. Interestingly, many scientists had started to investigate this type of material even before the introduction of the HOF concept. In 1969, Duchamp and Marsh isolated a 2D honeycomb hydrogen-bonded network that was self-assembled by benzene-1,3,5-tricarboxylic acid (TMA). No voids could be observed in this material because of the catenation in the 2D network. In 1987, Herbstein et al. used long-chain alkanes and primary alcohols as a template to prepare noncatenated hydrogen-bonded networks based on TMA, in which 1D channels are filled with long-chain template molecules. In 1988, Ermer reported a 3D hydrogen-bonded network based on adamantane-1,3,5,7-tetracarboxylic acid (ADTA), which is nonporous due to the 5-fold interpenetration of the dia network. In 1991, Ermer and Wuest independently synthesized 3D hydrogen-bonded networks with small guest molecules filled in their channels., Subsequently, a series of guest-inclusion hydrogen-bonded networks with 1D to 3D architectures was successively reported. Indeed, these early studies largely promote the evolution and progress of constructing porous HOFs. However, the permanent porosity of hydrogen-bonded networks was not established until 2010. The permanent porosity establishment that came with the introduction of the HOF concept played an important role in propelling the HOF development. Since then, emphasis has been put on how to prepare porous HOFs and how to exploit their functionalities. Nowadays, HOFs have become a unique type of porous multifunctional material for various applications.−
Although substantial progress has been achieved, the development of HOFs still largely lags behind those of their MOF and COF counterparts. On one hand, the interactions between adjacent building blocks in HOFs are mainly H-bonds, whose bonding energy (e.g., 10–40 kJ mol–1 for H-bonds) is much smaller than those of coordination bonds (90–350 kJ mol–1) in MOFs and covalent bonds in COFs (300–600 kJ mol–1). As a result, most HOFs suffer from framework instability, which cannot retain their porous frameworks after removing guest solvents from their voids. On the other hand, H-bonds are more flexible, reversible, and less directional as compared to coordination and covalent bonds, making HOFs more challenging to predict and design precisely. A slight change in tectons may significantly alter HOF structures and properties. Additionally, polymorphism resulting from different linkages or distinct degrees of interpenetration/catenation also easily occurs during the self-assembly of HOFs. That is, dramatic structural change may be observed by only a subtle change in self-assembled conditions. For example, the self-assembly of 4,4′,4″-(1,3,5-triazine-2,4,6-triyl)tribenzoic acid (H3TATB) in three different solvents can yield three HOFs termed PFC-11–13, which have the same linkages yet very distinct structures and properties because of the different degrees of catenation.
Just as one coin has two sides, hydrogen bond’s weakness, flexibility, and reversibility endow HOFs with unique features, including mild preparation, easy regeneration and recyclability, good solution processability, feasible self-healing, high biocompatibility, etc. Because of their weakness and reversibility, HOFs can be synthesized in high crystallinity under mild conditions. Besides, HOFs can be easily dissociated into pristine organic building frameworks in some solvents. In turn, the resulting solvents may form HOFs after the removal of volatile solvents by volatilization. Such a reversible process facilitates HOFs for solution processability, regeneration, and recyclability. H-bonding interactions are flexible and reversible, which may help the injured HOFs to recover their structures and thus enable HOFs to serve as seal-healing materials. In addition, compared with their MOF counterpart, most HOFs are metal-free, avoiding the cytotoxicity of metal ions. The above-mentioned advantages make HOFs an ideal platform for constructing multifunctional materials.
So far, some rules for structural design and stability enhancement for HOFs have been proposed. In this context, a growing number of robust HOFs with permanent porosity has been synthesized, and HOFs may also be considered as raw precursors that can be combined with other functional materials to fabricate multifunctional composite materials. Of late, some excellent reviews about the synthesis and applications of HOFs were also reported.− In this Outlook, we would like to summarize the basic principles for the design and construction of robust HOFs. Emphasis was put on the discussion about recent impressive progress in the application of HOFs. Finally, we discuss some major opportunities and challenges for HOF-based multifunctional materials.
Structural Design of HOFs
Although many HOFs are synthesized by serendipity, the design of HOFs is a long-term pursuit of researchers. Reticular chemistry, which utilizes the geometry-guided design of periodic materials by the connection of well-defined building blocks through strong bonds, has been extensively employed to predict and design crystalline materials. To use this strategy, readily accessible building blocks with special geometries are essential, in addition to the other essential requirements called isoreticular chemistry, which enables the modification, replacement, expansion, and contraction of building blocks to customize the structural properties of periodic materials for different properties. Due to the discovery of plenty of well-defined metal-containing clusters (or metal ions) termed secondary building units (SBUs) and the easy accessibly of many robust organic ligands, reticular chemistry has proven to be an extremely effective platform for designing and predicting MOFs. Such a design method also can be directly transplanted to COFs because of the ready accessibility of well-defined building blocks of COFs, significantly spurring COF development.
Reticular chemistry, however, is not widely applicable for the accurate prediction and design of HOFs. Although tectons with well-defined geometries are readily accessible, the connection linkages between tectons in HOFs, are always chaotic and unpredictable. The weak interaction combined with the great flexibility and low directionality of hydrogen bonds jointly contribute to the difficulty in obtaining fixed and robust linkages with a specific diagram during HOF synthesis. The instabilities and fragilities of linkages, as well as the interpenetration and catenation, significantly obstruct the design of HOFs by reticular chemistry.
Fortunately, scientists have explored supramolecular synthons that formed by multiple H-bonding pairs. Some of them have high directionality and exhibit a special spatial geometry, which can serve as relatively stable linkages for HOF design by reticular chemistry. As shown in Figure 1, carboxyl dimer, 2,4-daiminotriazine (DAT) dimer, cyclic pyrazolyl trimer, benzimidazolone chain, amidinium-carboxylate, and guanidinium-sulfonate are the most common supramolecular synthons used for the building of HOFs. Figure 2 shows typical examples for HOF design by reticular chemistry. So far, a library of stable HOFs with permanent porosity was successfully designed and synthesized by the collaborative choice of the above supramolecular synthons and rigid tectons.,,, Some HOFs are so stable that their structures can be well retained even in harsh conditions like extremely acidic or basic aqueous solutions.
Besides organic tectons, it is should be noted that metalated organic building blocks also can be utilized as tectons for the design and synthesis of HOFs (Figure 3). Metal complexes are one of the representative metalated organic building blocks that are most commonly employed for HOF construction. For example, a paddle-wheel metal complex [Cu2(ade)4] (ade = adenine, Figure 3), formed by the coordination of copper ions with adenines, is demonstrated to be a very good tecton to build microporous HOFs. Based on this tecton, several HOFs including SMOF-1/SMOF-2, MPM-1-TiFSIX, HOF-21, HOF-ZJU-101/HOF-ZJU-102, and SMOF-PFSIX-1/SMOF-AsFSIX-1 have been prepared, which exhibited very good performances in gas adsorption and separation. Metal–organic cages also can serve as metalated organic building blocks for the preparation of HOFs. Gong et al. reported that the self-assembly of chiral 4,4′,6,6′-tetrakis(4-benzoic acid)-1,1′-spinol phosphonate (H4L) and M4-calixarene could isolate metal–organic-based octahedral cages (Figure 3), which further connected to each other through H-bonds to form 3D HOFs. Besides, some metal–organic clusters bearing hydrogen donors and acceptors can also be employed as metalated organic building blocks for HOF design and preparation. For instance, Yam et al. successfully isolated a cluster-based HOF LH-Au10S4-Cl [LH = 4,5-bis(diphenylphosphanyl)-2H-1,2,3-triazole] based on a decanuclear gold(I)-sulfido cluster (Figure 3), which is capable of separating benzene/cyclohexane accompanied by luminescence color changes. Through elegantly choosing metalated organic building blocks, HOFs with permanent porosity can be realized, which largely enriches the structures and functionalities of the HOF library.
Recently, the computational approach has also been employed to screen and predict the structure of HOFs. In principle, the probability of obtaining a structure is directly related to its lattice energy. The lower the energy, the higher the probability that a stacking arrangement can be isolated experimentally. For a given tecton, the possible stacking arrangements could be computationally sampled, whose lattice energy could also be computationally calculated. In this regard, the packing arrangements with porous structures could be discovered by the comparison of the lattice energy of simulated structures. Based on this methodology, Cooper, Day, and their coauthors combined the computational crystal structure prediction (CSP) with a high-throughput crystallization screen to discover HOF polymorphs with high porosity and relatively high stability. Taking two widely used molecules benzene-1,3,5-tricarboxylic acid (TMA) and adamantane-1,3,5,7-tetracarboxylic acid (ADTA) as an example, they successfully predicted and isolated a novel porous polymorph of TMA (denoted as δ-TMA) and three new solvent-inclusion polymorphs of ADTA, verifying the feasibility of this methodology. Day et al. further combined CSP and property prediction to build energy–structure–function (ESF) maps, which were applied to predict the possible structures and properties of a candidate tecton. Based on this strategy, three new porous polymorphs of triptycene imidazolone T2 (i.e., T2-β, T2-γ, and T2-δ) and an ultra-low-density form of T2E (i.e., T2E-α) were discovered and experimentally characterized. Especially, T2-γ has a BET surface area of 3425 m2 g–1, which represents the highest surface area for the reported HOFs. Interestingly, the calculated structures and properties (i.e., nitrogen adsorption isotherms) are in good agreement with those of experimental results. Later, they popularized this strategy to a series of rigid molecules that comprise either a triptycene or a spiro-biphenyl core and are separately functionalized with six different hydrogen-bonding moieties. Very recently, CSP was further employed to predict and construct a cage-based and low-density (0.54 g cm–3) mesoporous HOF (i.e., Cage-3-NH2), which has a BET surface area of 1750 m3 g–1 and represents the first non-interpenetrating mesoporous 3D HOF with permanent porosity. ESP maps have been shown as a very promising method for discovering novel HOFs, but the cost of acquiring an ESF map is still too high for routine integration into high-throughput virtual screening workflows. To address this problem, Pyzer-Knapp et al. utilized parallel Bayesian optimization to selectively acquire energy and property data, generating the same levels of insight at a fraction of the computational cost. This approach could be used to improve the navigation of ESP maps and accelerate computational discovery of porous HOFs.
Stability Enhancement
Owing to the fragility of linkages, it is difficult for most HOFs to retain their porosity after the removal of guest solvents. Given that low stability is mainly due to weak hydrogen bonds, increasing the numbers of intermolecular hydrogen bonds would unambiguously enhance framework stability. Therefore, using rigid tectons and robust supramolecular synthons with multiple hydrogen pairs is one of the primary strategies to obtain stable HOFs. Besides, the synergy of H-bonds with other intermolecular or even covalent bonding interactions can also largely strengthen the skeleton of HOFs. Several strategies, such as π–π interaction, framework interpenetration, electrostatic interactions, and covalent bonding interactions, have been proposed and utilized to construct porous HOFs (Figure 4). It should be noted that in most cases more than one strategy was employed to synergistically enhance the stability of HOFs. For instance, the π–π interaction, framework interpenetration, and electrostatic interactions were simultaneously introduced into BioHOF-1, making it very stable in aqueous solutions even in boiling water (Figure 4c). In this part, we will briefly discuss these strategies one by one.
π–π Interactions
Generally, π–π interaction is an attractive interaction between aromatic rings. Therefore, the synergy of H-bonding and π–π stacking interactions is a reliable method to stabilize HOFs. This strategy is particularly applicable when 2D hydrogen-bonded layers are packed together through face to face π–π stacking. In this case, organic tectons are first connected by H-bonds to form 2D hydrogen-bonded layers, which were further packed by π–π stacking interactions to obtain 3D frameworks with 1D open channels along the packing direction. The planar and large π-conjugated tectons with C2-, C3-, C4-, and C6-symmetry are very suitable for constructing stable HOFs due to their facile accessibility to 2D hydrogen-bonded layers.
The 2D square lattice (sql net) is the most common platform used for the construction of stable HOFs.− For example, Liu and Cao et al. isolated a crystalline PFC-1 based on 1,3,6,8-tetrakis(p-benzoic acid)pyrene (H4TBAPy) that comprises a large π-conjugated planar scaffold pyrene and four benzoic acid arms (Figure 4a). In PFC-1, each H4TBAPy is connected by four adjacent ones by carboxyl dimers, forming 2D hydrogen-bonded layers with sql topology. The sql layers were further packed together in an AA packing mode, resulting in a 3D open framework with an extraordinarily high BET surface area of 2122 m2 g–1. Due to the shape-matching, both the pyrene scaffold and four benzoic acid arms are perfectly packed with adjacent pyrene and benzoic, respectively, in an AA mode. Therefore, PFC-1 is highly stable, and its structure is not changed after treatment in concentrated HCl for at least 117 days. Chen et al. successfully expanded this platform to HOF-14 by replacing benzoic acid arms with naphthoic acid arms. HOF-14 has the largest pore aperture (3.1 nm) among the reported HOFs, whose structure can be well retained even after treatment in strong alkaline solutions with a pH of 14. Later, Farha and Li et al. further demonstrated how isoreticular chemistry is applied to this platform for the tunability of HOFs’ structures and properties., Very recently, Liu et al. reported three HOFs, namely, PFC-71–73, which are self-assembled by [5,10,15,20-tetrakis(4-carboxyphenyl)porphyrin] (TCPP) or metallization TCPP (M-TCPP). Interestingly, the metallization materials PFC-72–73 have a higher stability than metal-free PFC-72 because of more effective π–π stacking between sql layers in PFC-72–73 than that in PFC-71.
The hexagonal (hxl) net is another platform commonly used for the π–π stacking strategy. Hisaki et al. employed various C3-symmetric π-conjugated tectons that possess three o-bis(4-carboxyphenyl)benzene moieties in the periphery of the core to synthesize isostructural HOFs with hexagonal networks. In these HOFs, the hexagonal layers are stacked without interpenetration, providing permanent porosity for various applications.− The honeycomb (hcb) net is also a 2D network very suitable for the introduction of π–π stacking interaction. For example, Hashim et al. prepared a series of HOFs with hcb topology based on C3-symmetric organic building blocks and cyclic pyrazolyl trimers, which are highly porous and possess large hexagonal pores.
The strategy is also applicable to 3D networks. For example, Yuan et al. built a 3D ultrastable and easily regenerated HOF-TCBP with dia topology for light hydrocarbon adsorption and separation; Chen and Zhang et al. employed a tetrahedral organic tecton to build a highly stable 3D HOF (HOF-20) with ThSi2 topology for aniline sensing. Li and Chen et al. synthesized a 3D HOF-76 with a pcu network for selective ethane/ethylene separation. The ultrahigh stability of the above-mentioned 3D HOFs is mainly ascribed to the strong face-to-face π–π stacking between adjacent hydrogen-bonded nets.
Framework Interpenetration
Although framework interpenetration will reduce the pore size and pore void of an HOF, it can improve the framework’s stability because of the multiple-interpenetrated framework being thermodynamically favorable compared with its noninterpenetrated counterpart. Therefore, framework interpenetration is also a common strategy to strengthen HOFs. A typical example is demonstrated by Stoddart et al. They successfully controlled the level of interpenetration by tuning crystallization conditions in the self-assembly of a peripherally extended triptycene H6PET {4,4′,4″,4‴,4‴′,4‴″-(9,10-dihydro-9,10-[1,2]benzenoanthracene-2,3,6,7,14,15-hexayl)hexabenzoic acid}. Two acs networks, PETHOF-1 and PETHOF-2, with 2- and 5-fold interpenetration, respectively, were isolated. PETHOF-1 and PETHOF-2 show BET surface areas larger than 1100 m2 g–1 (Figure 4b). Similarly, Liu and coauthors reported that the self-assembly of H3BTB can obtain undulated 2D layers with hcb topology, which finally generates PFC-11–13 with different degrees of polycations. Despite the high degree of catenation, PFC-11 and PFC-12 still have BET surface areas of 751.3 and 653.6 m2 g–1, respectively. Likewise, Chen et al. reported a 10-fold interpenetrated diamond HOF-30 for the selective adsorption of propyne over propylene, which shows a reversible H-bond and H-bond transformation during the solvent adsorption and desorption processes.
Electrostatic Attractions
The introduction of electrostatic attractions between positive and negative ions is also a viable strategy to enhance the stability of HOFs. Typically, the so-called charge-assisted H-bonding interactions, formed through strong acidic and basic components, is a representative example to introduce electrostatic attractions for strength enhancement of linkages (Figure 4c). So far, several supramolecular synthons containing charge-assisted H-bonding interactions, such as amidinium-carboxylate,− guanidium-sulfonate,− ammonium-sulfonate, and amidinium-sulfonate, have been widely explored to synthesize robust functional HOFs.
Covalent Bonding Interactions
The introduction of covalent bonds to connect tectons in HOFs is also used to improve HOFs’ stability. This strategy was well elucidated by Ke et al. They successfully developed a series of hydrogen-bonded cross-linked organic frameworks (HcOFs) by covalent photoinduced cross-linking organic building blocks that have been preorganized into HOFs (Figure 4d)., The resulting HcOFs show a guest-induced elastic expansion and contraction, expanding their voids to adsorb iodine and reversibly recovering their crystalline form after iodine release. Such a unique guest sorption-induced elastic property is also observed in HcOF-6, which originated from the reversible disruption and restoration of the anion clusters upon guest adsorption and desorption.
Gas Storage and Separation
Because the low density of a material favors its high gravimetric storage capacity, the lack of metal ions in HOFs makes them promising adsorbents for gas storage. So far, HOFs have been used to capture various gases including green gas CO2,,,,,− clean energy gases like H2 and CH4,, valuable industrial gaseous feedstocks like light hydrocarbon,− toxic gases like SO2, etc. SOF-1 is an early attempt of applying HOFs for gas storage, which shows a moderate uptake of CO2 (69 cm3 g–1, STP), C2H2 (124 cm3 g–1, STP), and CH4 (124 cm3 g–1, STP) at 1 bar and 195 K. To improve the gas uptake capacity, a very efficient strategy is increasing the specific surface areas. TTBI, also denoted as T2-α by Pulido, with a BET surface area of 2796 m2 g–1, has a significant adsorption of CO2 (81 cm3 g–1 or 15.9 wt %) at 273 K and 1 bar, as well as H2 (10.8 cm3 g–1 or 2.2 wt %) at 77 K and 1 bar. T2-γ, a polymorph of T2-α, whose BET surface area reaches to 3425 m2 g–1, has a saturation CH4 capacity of 47.4 mol kg–1 (437.4 v/v) at 115 K. KUF-1 can adsorb NH3 in a unique type IV fashion at 298 K, which is the first observation in NH3 uptake. Compared with type I sorption behavior found in other materials for NH3 sorption, such a unique sorption behavior of KUF-1 has a very high working capacity and recyclability at room temperature.
Adsorptive separation by porous materials is regarded as one of the most promising separation technologies for its simplicity and energy-saving property. In view of the great importance of light hydrocarbon separation (e.g., C2H4 and C3H6 purification), HOFs have been widely utilized for the separation of light hydrocarbons.,,− When the pore size of HOFs is much larger than light hydrocarbon molecules, the adsorption selectivity usually relies on the preferred binding affinity of host HOFs to guest molecules. For example, HOF-1 with a pore size of ca. 8.2 Å can adsorb 63.2 cm3 g–1 of C2H2 but can only adsorb 8.3 cm3 g–1 of C2H4 at 273 K and 1 bar, resulting in a high Henry separation selectivity of 19.3 for C2H2/C2H4. Another typical example was demonstrated by PFC-1/PFC-2, which are self-assembled by H4TBAPy and have large pore sizes (Figure 5a, 23 Å for PFC-1 and 29 Å for PFC-2). However, PFC-2 shows a better adsorption of C2 hydrocarbon to CH4 than the PFC-1 counterpart due to the presence of unpaired hydrogen bond acceptor C=O groups in the pore surface of PFC-2 (Figure 5b,c). HOF-30a, a 10-fold interpenetrated dia network with a pore size of about 4.2 Å, enables the selective adsorption of C3H4 over C3H6 with IAST selectivities reaching 7.7 and 7.6 for 1/99 (v/v) and 1/999 of C3H4/C3H6 mixtures, respectively, at 298 K. Other HOFs including HOF-TCBP also display selective adsorption of light hydrocarbons based on preferred interactions between host framework and guest molecules.
When the pore size is very small, the sieving effect will largely affect the separation performance of HOFs. In this case, the synergy of the sieving effect and preferential binding affinity could significantly boost the separation performance of HOFs. HOF-21, which exhibits a small pore size of 3.6 Å, can adsorb 1.98 mmol g–1 of C2H2 and 1.27 mmol g–1 of C2H4 at 298 and 1 bar, giving a very high ideal adsorbed solution theory (IAST) C2H2/C2H4 selectivity of 7.1. The outstanding separation performance is mainly ascribed to the sieving effect and the superimposed H-bonding interactions between C2H2 and HOF-21. Functioning with free −COOH moieties and possessing a small pore size of 6.7 Å, HOF-16 shows a larger C3H6/C3H8 uptake difference (by 76%) and higher selectivity (5.4) than the HOF-11 counterpart that was constructed by the same organic tecton but with a larger pore size and without free −COOH decoration. HOF-FJU-1, constructed by tetracyano bicarbazole, is flexible but very stable even under harsh conditions such as exposure to strong acidity, basicity, and highly polar solvents (Figure 6a). HOF-FJU-1 displays an evident gate opening behavior at different temperatures. With a suitable pore size of 3.4–3.8 Å (Figure 6b,c), HOF-FJU-1 could solely take up C2H4 (3.28 Å) while blocking C2H6 (3.81 Å) in a C2H4/C2H6 mixture by the control of operating temperatures and gating pressures (the optimized temperature is 333 K, Figure 6e). Breakthrough experiments show that a high purity of C2H4 (99.1%) could be obtained at 333 K, making it one of the best porous materials ever reported for C2H4/C2H6 separation. HOF-FJU-1 also exhibits highly efficient propylene separation from binary C3H6/C3H8 (50/50) with a propylene purity and productivity of over 99.5% and 30.2 L kg–1 at 333 K (Figure 6c,d,f), which even can selectively separate C3H6 and C2H4 in seven-component CH4/C2H4/C3H6/C3H6/C3H8/CO2/H2 cracking gas mixtures. In addition, HOF-FJU-1 can separate C2H2 from CO2 by virtue of their difference in electrostatic potential distribution. Because of the presence of multiple C–H···π and N···H–C hydrogen-bonded interactions between host HOF-FJU-1 and guest C2H2, HOF-FJU-1 exhibits extra strong affinity to C2H2 (46.73 kJ mol–1) and has the highest IAST selectivity of 6675 for C2H2/CO2 separation among the reported adsorbents.
Inverse separation like C2H6-selective or C3H8-selective adsorption separation is highly desired for C2H6/C2H4 and C3H8/C3H6 separation because it can simplify the separation process and is energy-saving. Notably, the inverse separation is much more easily realized in HOFs than the MOF counterparts due to the extremely low polarity of the pore surface in HOFs that benefits the selective adsorption of gas with a low dipole or quadrupole moment. So far, several C2H6-selective or C3H8-selective HOFs have been successfully developed. For instance, ZJU-HOF-1, which is self-assembled by a hexacarboxylate 2,4,6-trimethylbenzene-1,3,5-triylisophthalate (TMBTI), has 1D triangular channels with a pore size of ca. 7.0 Å and hydrophobic pore surfaces resulting from the decorated methyl groups (Figure 7a). Interestingly, plentiful cagelike pockets with a diameter of 4.6 Å were found around the channels due to the 3-fold interpenetration and rod-packing configuration. Remarkably, these pockets match better with the larger C2H6 molecule (4.4 Å) than C2H4 (4.1 Å), leading to a stronger interaction between host framework and C2H6 than C2H4 (Figure 7b). As a consequence of pore confinement and preferential interactions, ZJU-HOF-1 preferentially adsorbs C2H6 over C2H4, showing a high C2H6 uptake of 88 cm3 g–1 at 0.5 bar and 298 K and a C2H6/C2H4 IAST selectivity of 2.25 for C2H6/C2H4 (1/1) mixtures at 298 K and 1 bar (Figure 7c). The obtained IAST selectivity is notably higher than those of HOF-BTB (1.4) and HOF-76 (2.0). It is worthy to note that ZJU-HOF-1 can efficiently capture C2H6 from C2H6/C2H4 (1/1) mixtures in ambient conditions under 60% RH, providing a record polymer-grade C2H4 productivity of 0.98 mmol g–1 (Figure 7d). Another example is demonstrated by HOF-76. HOF-76 can take up 2.95 mmol g–1 of C2H6 but only can adsorb 1.67 mmol g–1 of C2H4, resulting in a high C2H6/C2H4 IAST selectivity of 2.0 for 10/90 (v/v) C2H6/C2H4 mixtures. Breakthrough experiments show that HOF-76 can directly produce high-purity C2H4 gas from C2H6/C2H4 mixtures with a high productivity of 7.2 L/kg at 298 K and 1.01 bar. Similar behavior was also observed in HIAM-102, where C2H6 and C2H4 separation was achieved even under a highly humid condition due to the suitable pore size and the superhydrophobic pore surfaces.
In addition to light hydrocarbon separation, HOFs have also been employed for adsorptive separation of other industrial gases., A flexible and self-healing HOF membrane termed the UPC-HOF-6 membrane was used for H2/N2 separation. BTBA-1a and PTBA-1a show highly selective separation of CO2/N2 with a record high IAST selectivity >2000 under ambient temperature and pressure. An ultrastable HOF termed TAPM-1 was explored as the stationary phase in the high-solution gas chromatographic separation of benzene and cyclohexane or toluene and methylcyclohexane. HOF-ZJU-103/HOF-ZJU-104, HOF-ZJU-201/HOF-ZJU-202, and HOF-40 exhibit a superior separation performance for Xe/Kr mixtures.
Heterogeneous Catalysis
The ease of regeneration and recyclability by simple recrystallization as well as solution processability of HOFs enables them to serve as ideal heterogeneous catalysts. One of the primary strategies for preparing HOF-based catalysts is to choose tectons with the intrinsic catalytic activity for the construction of HOFs.,− Porphyrins, a class of heterocyclic molecules with four pyrrole subunits and a large π-conjugated system, can coordinate with various metal ions to form metalloporphyrins, which are of extreme importance in many biological functions due to their light-harvesting, electron transfer, oxygen transport, and various catalytic molecular transformations. Remarkably, the rigid and intrinsic catalytic active features of porphyrins permit their ordered arrangement to form HOFs as heterogeneous catalysts. For instance, a library of highly porous porphyrin HOFs termed PFC-71–73 based on TCPP/M-TCPP have been synthesized in 2022. In their structures, TCPP or M-TCPP is connected with four other tectons via carboxy dimers to form 2D hydrogen layers with sql topology, which further pack together by ABAB mode to obtain 3D open frameworks with pore sizes ranging from 14.9 to 18.8 Å (Figure 8). Metalated PFC-72–73 are highly stable and can retain their structures after being immersed in concentrated HCl, boiling water, or heated to 270 °C. By contrast, the metal-free PFC-71 has a lower stability than PFC-72–73, whose surface area is also much lower than those of metalated PFC-72–73 (600, 1646, and 1714 m2 g–1 for PFC-71, PFC-72-Co, and PFC-73-Cu, respectively). The observable stability enhancement of PFC-72–73 is mainly ascribed to the more effective π–π stacking among sql H-bonded layers in PFC-72–73. As anticipated, PFC-72 and PFC-73 can catalyze the photoreduction of CO2 to CO, whose catalytic activity largely depends on the chelated metal species in the porphyrin centers. Later, another stable porphyrin HOF-58 platform that can finely tune the ratio of porphyrin and metalloporphyrin tectons was successfully developed (Figure 9a,b). The change of metalloporphyrin content in HOF-58 not only alters the microenvironment surrounding of the active sites but also varies the charge separation efficiency. As a result, HOF-58–30 with 30% of metalloporphyrin has the highest activity in the photocatalytic reduction of CO2 to HCOOH (29.8 μmol g–1 h–1) (Figure 9c). Metalloporphyrin-based HOF is also explored as an electrocatalyst. Lan and Chen et al. synthesized a microporous HOF termed Cu-TDPP based on Cu-porphyrin tectons for electrochemical CO2 reduction reaction (CO2RR) to produce CH4. In the structure of Cu-TDPP, the tectons were connected to each other by two distinct DAT dimers, forming a 2D H-bonded layer with sql topology. These layers are further connected together and packed into a 3D framework via interlayer π–π interactions. Notably, a Cu-TDPP nanosheet with a thickness of ca. 5.08 nm can be isolated by the exfoliation of bulk Cu-TDPP. Cu-TDPP nanosheets were successfully applied in electrochemical CO2RR, exhibiting a superior FECH4 of 70% with a high current density (−183.0 mA cm–2) at −1.6 V under neutral conditions and maintains FECH4 > 51% over a wide potential range of −1.5 to −1.7 V. The high performance is mainly ascribed to the numerous H-bonding networks in Cu-TDPP, which benefit proton migration and intermediate stabilization.
Chiral phosphoric acids are widely used as Brønsted acid catalysts for enantioselective reactions. It is of significant interest but still a long-term challenge to load chiral phosphoric acid into porous materials to realize heterogeneous catalysis for the promotion of various challenging reactions. In 2019, Gong et al. synthesized two chiral HOFs, 1-Ni and 1-Co, based on chiral phosphoric acid tectons. Strikingly, 1-Ni and 1-Co could efficiently catalyze asymmetric [3 + 2] coupling of indoles with quinone monoamine and Friedel–Crafts alkylations of indole with aryl aldimines with 99.9% ee values, respectively.
However, the lack of catalytic active sites like metal species in most HOFs significantly impedes their applications in catalysis. In this case, employing stable HOFs as porous solid supports to encapsulate active catalytic species is the other effective strategy to construct HOF-based heterogeneous catalysts. For example, HOF-25, built by 2,2′-bipyridine(bpy)-derived tectons, possesses free 2,2′-bipyridine(bpy) in its pores (Figure 10a). The tectons are connected with each other by a hydrogen-bonded guanine-quadruplex (G- quadruplex) to form 2D hydrogen-bonded layers with sql topology. These layers further pack to each other by AA mode, leading to a 3D open framework with a BET surface of 173 m2 g–1. Integrating with the guanine-quadruplex and interlayer π–π interaction, HOF-25 is stable and can retain its structure in aqueous solutions with a pH range of 7–11. After reacting with Re(CO)5Cl, HOF-25-Re that functioned with photocatalytic active Re(bpy)(CO)3Cl moieties is successfully isolated, which can efficiently catalyze CO2 photoreduction to CO with both a high CO production rate of 1448 μmol g–1 and high selectivity of 93% in the presence of [Ru(bpy)3]Cl2 under visible light irradiation (Figure 10b). HOF-25 has also been reacted with Ni(II) to get HOF-25-Ni material, in which 20% of bpy was immobilized with Ni(II). Interestingly, the sql layers in HOF-25-Ni can be exfoliated to afford 2D nanosheets (termed HOF-25-Ni NSs) in a high yield of 56% by solvent-assisted sonication method (Figure 10c). The immobilized Ni(II) significantly promote this exfoliation process, which is mainly ascribed to the diminishing interlayer π–π packing interactions by electrostatic repulsion of positive Ni(II) ions. HOF-25-Ni NSs are ultrathin, whose thinness is 4.4 nm. To avoid self-aggregation and facilitate the recycling, HOF-25-Ni NSs were adhered to graphene oxide (GO) with the assistant of strong π–π interactions and Coulomb force (Figure 10d). Strikingly, with the aid of [Ru(bpy)3]2+ and triisopropanolamine, HOF-25-Ni NSs@GO composite with 10 wt % of NSs can efficiently promote CO2 reduction under visible light illumination, showing a 96.3% CO selectivity with a prominent conversion rate up to 24 323 μmol g–1 h–1. In another example, HOF-19, a cage-based HOF with abundant amino triazine groups, was used to load Pd(II) by postsynthesis. The resultant Pd(II)@HOF-19 composite exhibits excellent catalytic performance for the Suzuki–Miyaura coupling reactions with isolation yields of 96–98%. The encapsulation of Ru clusters into HOF-19 by postsynthesis obtained Pd@HOF-19, which was used to catalyze hydrogenation of N-heterocyclic compounds including quinolines and indoles. In addition, the introduction of Pt NPs into PFC-1 by postsynthesis obtained Pt@nano-HOF, which can serve as an efficient photocatalyst for photocatalytic proton reduction., PFC-45/Cu2O heterostructure films were also used for efficient CO2 photoreduction.
Biomedical Applications
Due to the metal-free nature, most HOFs show low cytotoxicity and high biocompatibility. The reversible H-bonds also enable the gradual degradation of HOFs in a physiological environment. Simultaneously, the porosity of HOFs endows them with the capability to encapsulate diverse guest molecules and controllably release cargos under an external stimulus. In this regard, HOFs are very promising materials for biological applications, such as drug delivery, antibacterial, anticancer, etc.,
PFC-1 is the first HOF serving as a drug carrier, which was self-assembled by H4TBAPy. PFC-1 has a large BET surface area of 2122 m2 g–1 and 1D rhombic channels with a pore size of 18 × 23 Å2, which can efficiently encapsulate doxorubicin (an anticancer drug) with a high uptake of 26.5 wt %. Integrating reactive oxygen species (ROS) generated by the photoactive pyrene skeletons, dox@PFC-1 shows a comparable therapeutic efficacy with the commercial doxorubicin yet considerably lower cytotoxicity because of the synergistic chemo-photodynamic therapy.
PFC-33, which is built by H4TCPP tecton, exhibits 1D rectangular channels with a pore size of ca. 15 × 19 Å2 (Figure 11a). The skeleton of PFC-33 is anionic, and the channels were filled with quaternary ammonium as counterions. Strikingly, due to the presence of porphyrin photosensitizer and quaternary ammonium (a commercial biocide), PFC-33 exhibits synergistic photodynamic and chemical antimicrobial efficiency by virtue of the ROS generation by porphyrin backbone and ion-responsible controlled release of biocide via ion-exchange in various physiological conditions (Figure 11b). PFC-33 was further fabricated into a polyHOF membrane with the help of the interfacial interaction between the free carboxyl groups on the surface of PFC-33 and the polymer matrix. The resultant flexible but stable polyHOF membrane shows noticeable bacterial inhibition toward Escherichia coli.
PFC-55, an HOF constructed by perylenediimide (PDI) tectons, can be persistently maintained in a free radical state and show photothermal and photodynamic capacities under visible light illumination. To conquer the weak adsorption in the near-infrared (NIR) region, a core–shell heterostructure was fabricated by PFC-55 as shell and an upconversion nanoparticle (i.e., β-NaYF4:Yb,Er) as core via a “bottle-around-ship” strategy, which exhibits a noticeable NIR-responsive photothermal and photodynamic synergistic antimicrobial performance. The photodynamic antibacterial performance is also found in HOF-101-R (R = H, CH3, F, NH2), which are used for textile coatings. Interestingly, their antibacterial efficiency could be finely tuned by altering the substituents in tectons.
HOFs are particularly useful for the protection of or to add new functions of a biomacromolecule via macromolecular encapsulation by virtue of the dynamic interactions and the adaptive guest accommodation ability. Liang et al. first employed HOFs to encapsulate proteins with the aim of stability enhancement. BioHOF-1 is self-assembled by simply mixing aqueous solutions of tetraamide and tetracarboxylate tectons at ambient temperature, which has pores with an aperture of ca. 6.4 Å (Figure 12). The mild synthetic conditions and the water-soluble tectons of bioHOFs enable it to encapsulate enzymes in aqueous solutions. Various enzymes including catalase (CAT) and alcohol oxidase (AOx) were successfully encapsulated into bioHOF-1 (the loading amount of ca. 6.5% for CAT) through in situ synthesis, which are protected from elevated temperatures, a proteolytic enzyme (trypsin), and a chaotropic agent (urea), yet retain their catalytic activity. Tang et al. reported a nanoscale HOF termed TA-HOFs with a similar structure as another platform to encapsulate various proteins through a similar self-assembly process. Being encapsulated into the HOF structure, enzymes could retain their original catalytic activities. Moreover, the obtained nanoscale protein@TA-HOFs can efficiently enter into cells, which was exploited for biochemical catalysis in living cells for neuroprotection. Wied et al. adopted N-terminal enzyme fusion with the positively charged module Zbasic2 to improve the enzyme loading amount in bioHOF-1. In this seminal work, the pristine d-amino acid oxidase (DAAO) and Zbasic2 functionalized DAAO (named Z-DAAO) were separately incorporated into bioHOF-1 via the same bottom-up synthetic method. The obtained Z-DAAO@bioHOF-1 shows a 2.5-fold enzyme loading amount (50 wt % of enzyme content) and 6.5-fold specific activity to the DAAO@bioHOF-1 counterpart. Such a strategy was successfully extended to other enzymes, demonstrating the versatility of this strategy in the preparation of biohybrid systems.
Nevertheless, the small pore aperture of the host HOFs and/or relatively low loading amount of proteins still limits the practical application of protein@HOF composites. To tackle these problems, Chen et al. described a versatile protein-directed assembly strategy that enables the encapsulation of proteins into mesoporous HOFs. In this seminal work, various proteins were separately encapsulated into three isostructural mesoporous HOFs to obtain composites termed HBF-1, HBF-2, and HBF-3, respectively (Figure 13). HBF-1–3 have large accessible pores (e.g., 18.6 Å × 24.5 Å for HBF-1) that inherited from their pristine HOFs, facilitating the mass transportation of various biocatalytic substrates. To demonstrate the universality of this strategy, proteins regardless of shapes and surface chemistry including bovine serum albumin (BSA), cytochrome c (Cyt c), horseradish peroxidase (HRP), CAT, myoglobin (MB), pepsin, glucose oxidase (GOx), ovalbumin (OVA), and transferrin (TRF) were successfully encapsulated to construct HBFs with a very high protein content ranging from 24.3% to 67.4%. Notably, the encapsulated enzymes show noticeable stability improvement compared to free enzymes. They even show notable advantages for biocatalysis in comparison to those encapsulated in MOFs in terms of ingredient content, robustness, and catalytic efficiency. Such HOF biomimetic entrapment could also modulate the conformation of enzymes (i.e., Cyt c), permitting non-native bioactivity for the enzyme.
The protein-directed assembly strategy is also applicable for the simultaneous encapsulation of multiple enzymes into HOFs. For example, Li and Tang et al. adopted the same strategy to encapsulate multiple enzymes into PFC-1 to obtain HOF-confined cascade systems for point-of-care biosensing. Huang and Yuan et al. employed this strategy to simultaneously encapsulate CAT and GOx into PFC-1 to get EnHOF-101. After loading the photosensitizer chlorine6 (Ce6), the obtained photo-biocatalytic cascade nanoreactor Ce6@EnHOF-101 exhibits an extraordinary capacity for diabetic would healing through the synergistic PDT.
Besides protein/enzyme encapsulation, neural stem cells (NSCs) have also been successfully encapsulated to an amidinium-carboxylate-based HOF to overcome the low therapeutic efficacy during NSC transplantation. In this pioneering work, the encapsulated NSCs can be controllably released by NIR-II irradiation. Further experiments on an Alzheimer’s disease mouse model showed that the resultant NSC delivery system could enhance NSC viability, promote neurogenesis, and ameliorate cognitive impairment.
Sensing
Most HOFs are composed of aromatic organic tectons with larger π-conjugated systems. Such building units usually have intrinsic photoluminescent properties, enabling HOFs with the potential as photonic materials.,− It is worthy to note that the luminescent behavior of an HOF could be different from that of its pristine organic build blocks due to the highly ordered arrangement. Specially, HOFs’ luminescence could be responsive to the slight structural change caused by external stimulus or guest–host interactions, which could be harnessed for the luminescent sensing of the stimulus or guest molecules.− A representative example is demonstrated by the desolvated CPHATN-1a, which exhibits the reversible acid-induced luminescence change., CPHATN-1 is built from a hexaazatrinaphthylene derivative with carboxyphenyl groups, possessing significant thermal stability up to 633 K. A strong luminescence with a maximum emission at 539 nm is observed for desolvated CPHATN-1, which turns off/on upon the reversible adsorption/desorption of HCl vapor as a result of the protonation/deprotonation of pyradyl N atoms. Another example is HOF-20, which exhibits highly efficient turn-up fluorescent sensing of aniline in aqueous solutions. Self-assembled by H4BCPIA [5-(2,6-bis(4-carboxyphenyl)pyridine-4-yl)isophthalic acid] (Figure 14a), HOF-20 has a BET surface area of 1323 m2 g–1 and is very stable in water media. Once excited at 315 nm, HOF-20 emits a strong and broad emission centered at ca. 370 nm. Interestingly, the fluorescent intensity of HOF-20 significantly increases after exposure to aniline (Figure 14c). Such “turn-on” sensing is mainly ascribed to the rigidification of the tectons caused by the synergy of the H-bonding and π–π stacking interactions between the aniline and host framework (Figure 14b). In another work, HOF-FAFU-1 was exploited as a fluorescent sensor for hypochlorite detection by a “turn-off” mode. HOF-FAFU-1, built by 4,4′-OH-TCBP [i.e., 3,3′5,5′-tetrakis(4-carboxyphenyl)-4,4′-dihydroxy-1,1′-biphenyl], is highly stable in aqueous solutions in a pH value ranging from 1 to 9. HOF-FAFU-1 is very sensitive to hypochlorite, whose fluorescent intensities sharply decrease upon the contact with hypochlorite. Such fluorescent quenching is mainly ascribed to the oxidation of 4,4′-OH-TCBP to its nonfluorescent state.
Tetraphenylethylene (TPE), an aggregation-induced emission (AIE) active molecule, is intensively employed as a backbone to synthesize HOF-based photonic materials with extraordinary luminescence properties.− As a flexible molecule, the conformation of TPE is likely to change upon external stimulus by modulating the phenyl rotations as well as the dihedral angles of the ethylene core and phenyl rings. Based on these considerations, Shi et al. have synthesized 11 kinetic-stable and two thermostable HOFs termed 4CN(solvents) with distinct pore structures by a cyano-functionalized TPE organic tecton (Figure 15a). 4CN(solvents) show a guest-dependent fluorescence due to the different conformations of organic building blocks (Figure 15b). As expected, 4CN is highly sensitive to external stimuli like the exposure to solvent vapors or heating, resulting in the reversible luminescence change (including emission color, lifetime, and brightness) caused by the reversible structural transformations. For instance, 4CN(ET2) will lose ethanol upon heating, associating with the structure rearrangement to 4CN(Non1), and in reverse, the nonporous 4CN(Non1) can also be back to the 4CN(ET2) framework by fuming with dichloromethane/ethanol vapor. Similar behavior is also found in 8PN that was constructed by a nitro-modified TPE organic building blocks. Another typical example is elucidated by a dynamic 2D woven HOF (another TPE-based HOF termed 2D-90,) which is self-assembled by a tetra-substituted TPE derivative baring phenyl-hydroxy groups. In this case, 2D-90 exhibits a dark blue fluorescence with a maximum emission at 459 nm upon 365 nm irradiation, which is red-shifted to 474 and 470 nm after the exposure to MeOH and EtOH, respectively. Such guest solvents/vapor regulated photoluminescence is also observed in other TPE-based or non-TPE-derivative dynamic HOFs.−
Besides luminescent sensing, the photo- and/or electroactive properties of HOFs can also be used in other analytic methods. Photoelectrochemical (PEC) detection, which is highly sensitive and excellently reproducible, is regarded as a ground-breaking analytic technology for trace analysis. The PEC sensor highly depends on the photoactive materials, which not only should harvest photos to generate photoelectrons but also should identify the analytes. Wang et al. successfully fabricated AgNPs@HOFs nanocomposites as photoactive materials for PEC sensing. They developed two methods to encapsulate Ag NPs into HOFs (Figure 16a). In the first method, the organic tecton H4TBAPy was thoroughly mixed with Ag(I) ions to form a uniform solution, which was illuminated by a 10 W LED for the photoreduction of Ag(I) ions to Ag NPs. Then, a large amount of methanol was added to obtain nanoscale AgNPs@HOF-101. Alternatively, AgNPs/HOF-101 was obtained after changing the synthetic sequence. Interestingly, the loading amount of Ag NPs can be tuned by the control of the LED illumination time, which further affects the photoactivity of the composites. The photocurrent of AgNPs@HOF-101 composites (0.85–1.91 μA) is significantly higher than those of common MOFs including ZIF-8, HKUST-1, MOF-808, and NU-1000 as well as metal oxides including Cu2O and ZnO. Notably, the photocurrent is more than 3-fold increased after the Ag NPs encapsulation. AgNPs@HOF-101 was used as photoactive material for PEC sensing (Figure 16b). Strikingly, the portable PEC device based on AgNPs@HOF-101 can selectively recognize 13 different mustard gas simulants on the basis of synergistic size-exclusion and specific recognition. The optimized sensor shows a very low detection limit [15.8 nmol L–1 for 2-chloroethyl ethyl sulfide (CEES)], reusability (30 cycles), and long-term working stability (30 days).
Jiang and Wang et al. have synthesized an ultrastable porphyrin-based HOF termed UPC-H4 for selective NO2 sensing. UPC-H4 is constructed by 5,10,15,20-tetrakis(4-(2,4-diaminotriazinyl)phenyl)porphyrin (H2TDPP). The desolvated material UPC-H4a can act as an n-type semiconductor, whose conductivity highly relies on the concentration of NO2. Interestingly, the value of conductivity decrement is linearly related with the NO2 content. Therefore, UPC-H4a can serve as an effective sensor for NO2 sensing, as demonstrated by a very small LOD (lower than 40 ppb), fast response (17.6 s), and good reproducibility. Remarkably, UPC-H4a exhibits a lower LOD and higher selectivity in the NO2 sensing than H2TDPP tectons, which is mainly ascribed to the large number of accessible amino sites to interact with NO2 in UPC-H4a due to the highly ordered structure.
Proton Conduction
The proton-exchange-membrane fuel cell (PEMFC) is regarded as one of the most promising clean energy resources, in which electrolytes with high proton conductivity and durability are necessary. A primary prerequisite for a material’s proton conduction is the formation of hydrogen-bonded networks that enable the proton movement. In this regard, HOFs naturally become candidates as extraordinary proton conductors due to their inherent hydrogen-bonded networks. Theoretically, the diverseness of tectons and linkages permits the creation of well-defined H-bonded networks in the channels of HOFs for proton movement, which usually composes functional groups from the host framework and guest molecules filled in pores. So far, HOFs have become an excellent platform for proton conductors, as validated by the successful development of a library of HOFs with high proton productivity and high durability.−
An appropriate strategy to achieve high proton conductivity for HOFs is optimizing their pore surface’s hydrophobicity to control the amount of water molecules involved in the proton conduction pathways. In an ingenious work, two HOFs, namely, HOF-GS-10 and HOF-GS-11 composed of aryl disulfonate moieties and guanidinium ions, were reported exhibiting ultrahigh proton conduction values of 0.75 × 10–2 and 1.8 × 10–2 S cm–1 at 95% and 30 °C, respectively. In these two HOFs, the connection of guanidinium cations and the sulfonate moieties by [(G)N–H···O(S)] forms 2D hydrogen-bonded architectures, which further connect to each other by hydrophobic aryl groups that serve as pillars (Figure 17). As a result, 1D channels filled with polar guest molecules can be observed along the crystallographic a-axis. Experimental results show that the conductivity of HOF-GS-10 is slightly lower than that of HOF-GS-11 because of the higher hydrophobicity of the naphthalene pillar in HOF-GS-10 than that of the biphenyl pillar in HOF-GS-11. Similar hydrophobicity-dependent proton conductivity is also observed in the other four HOFs assembled by sulfonate anions and ammonium cations.
Another strategy to realize high proton conductivity is changing the guest molecules to optimize the H-bonding networks for proton movement. For instance, porous UPC-H5 based on a nickel tetraphosphonate porphyrin (NiH8TPPP) was reported, whose production conductivity is regulated by guest molecules in the channels (Figure 18). In the structure of UPC-H5, each NiH4TPPP4– provides four H atoms from four −PO3H moieties and accepts four H atoms from another four −PO3H to form eight O–H···O H-bonds, leading to the formation of 2D H-bonded layers. These layers are further connected to adjacent ones to obtain 3D networks by the H-bonding, electrostatic interactions among layers, Me2NH2+ and lattice water molecules, as well as π–π interactions. The guest DMF and lattice water molecules can be removed to get desolvated UPC-H5a, which further turns to UPC-H5a@NH3·H2O after exposure to 25% aqueous ammonia. Remarkably, UPC-H5, UPC-H5a, and UPC-H5a@NH3·H2O have proton conductivities of 1.85 × 10–3, 3.42 × 10–2, and 1.59 × 10–1 S cm–1 at 80 °C and 99% RH, respectively.
Other Applications
The merits of HOFs also enable them as multifunctional materials for many other applications, such as electrochromism,,, photochromism, environmental applications,,, chiral separation, structural determination, molecular actuator, etc. Only several representative examples recently reported are shown below since some of them were summarized by ours’ and others’ review articles.,
Electrochromism involves the reversible optical properties produced electrochemically. In a typical electrochromic process, the electroactive species often undergo reversible reduction or oxidation. HOFs are a potential type of electrochromic material when using tectons with intrinsic electrochromic activity. A good example is demonstrated by Feng et al. They fabricated a nano-PFC-1 film that exhibits reversible electrochromic properties by a facile and inexpensive electrophoretic deposition (EPD) method (Figure 19). The nanoscale PFC-1 materials was first synthesized by a rapid self-assembly of H4TBAPy tecton in a mixture of DMF/EtOH/H2O, which was used as a raw precursor for electrophoretic deposition (Figure 19a). The negative charge of PFC-1, which derives from internal defects or the deprotonation of carboxylate acid, allows the fabrication of PFC-1 film by the EPD method. As anticipated, nano-PFC-1 film was facilely fabricated by the deposition of nano-PFC-1 on transparent FTO substrates in CH2Cl2 solutions in 2 min. Strikingly, the obtained nano-PFC-1 film shows a reversible color change from yellow to blue-violet during CV scans (Figure 19b). Moreover, the successive color changes from yellow to green and then to blue-violet were achieved after modification of nanoPFC-1 with Fe(II) (Figure 19c). Besides, the nano-PFC-1 film can be recycled and regenerated by simply rinsing with DMF or DMSO.
When the reversible color change is induced by photons, the phenomenon is often called photochromism, which also accompanies redox reactions during the color change process. HOFs are potential photochromic materials. For instance, self-assembling by a redox-active viologen ligand, PFC-25 was explored as radiochromic materials, which are highly sensitive to X-ray irradiation (Figure 20a). The single crystal of PFC-25 shows an obvious color change from light yellow to green in 90 s upon X-ray irradiation (Figure 20b, top). In particular, the energy-dependent color change was also observed for PFC-25 (Figure 20b, bottom). Once irradiated by hard X-ray, PFC-25 shows a color change from yellow to dark green. By contrast, a light green was found when PFC-25 was irradiated by a soft X-ray. Most importantly, PFC-25 can be fabricated into a portable naked-eye sensor for X-ray detection based on the significant color change with ultrahigh sensitivity and good stability (Figure 20c).
In some cases, both the electrochromism and photochromism could simultaneously be found in a redox-active HOF. For instance, ECUT-HOF-30, a redox-active HOF, exhibits both photochromic and electrochromic properties (Figure 21).N,N,-Bis(2-isophthalicacid)naphthalenediimide, an organic tecton decorated with a redox-active unit, was selected to prepare ECUT-HOF-30 (Figure 21a). The obtained ECUT-HOF-30 is microporous and has 1D rectangular channels with a size of ca. 4.0 × 4.1 Å2 (Figure 21b). Due to the redox-active unit, ECUT-HOF-30 exhibits an exquisite color change from yellow to purple under CV scans (Figure 21c). Besides, ECUT-HOF-30 is very sensitive to UV light and exhibits a slight color change from light yellow to dark yellow under the UV illumination (365 nm) for 3 min (Figure 21d). During the electrochromic/photochromic process, ECUT-HOF-30 can retain its pristine structure, and the radical formation mainly contributes to the electrochromism and photochromism.
Uranium extraction from seawater (UES) is still a huge challenge but meaningful, which may effectively alleviate the energy shortage in the future. Due to the ultralow U content (ca. 3.3 ppb), the presence of other competing ions, and high salinity gradient in seawater, the exploration of materials with ultrahigh U affinity and stability is the primary prerequisite to realize UES by a low-cost adsorption process. CSMCRIHOF-1, which is self-assembled by PMAP decorated with pyridine and phenoxy-imine groups, exhibits significant UES capacities (Figure 22).CSMCRIHOF-1 is very stable and can retain its structure even under severe acidity, basicity, and saturated salt solutions. A high density of pockets with a diameter of ca. 3.8 Å are present in CSMCRIHOF-1, in which O and N atoms orderly arrange to serve as multidentate sites to bite U (Figure 22a). The presence of inter- and intramolecular hydrogen bonds enables CSMCRIHOF-1 solution processability. Free-standing thin films of CSMCRIHOF-1 (TFCHs) were facilely prepared by solution processing, whose thickness can be tuned from 40 to 500 nm by the control of CSMCRIHOF-1 concentrations and fabricated time (Figure 22b). Surprisingly, the BET surface area also significantly increased from PMAP tecton of 35.8 m2 g–1 to CSMCRIHOF-1 of 35.8 m2 g–1 to TFCH of 584.3 m2 g–1. Thanks to the coordination interactions between N/O and hard U species, the U adsorption over TFCH is mainly ascribed to the chemical adsorption. TFCH exhibits efficient UES capacities of ca. 11 mg g–1 with 5 days and 17.9 mg g–1 in 30 days from natural seawater (Figure 22c). Remarkably, TFCH can be reused and recycled at least five times with a slight decrease of adsorption efficiency (ca. 11.7%). The above U sorption behaviors make TFCH a new benchmark in UES.
Conclusion and Outlook
In this Outlook, we have reviewed the use of reticular chemistry and computational methodology to predict and design HOFs. Four main strategies for promoting the stability of HOFs, including the introduction of π–π stacking interaction, electrostatic attraction, covalent bonding interaction, and interpenetration/catenation, have been systematically described. We then discussed the latest advances of HOFs in gas adsorption and separation, heterogeneous catalysis, biological application, sensing, proton conduction, and other applications. Despite great achievements, many problems still need to be addressed. Some challenges and perspectives of HOF development are listed below.Although reticular chemistry has been successfully used to predict and design HOFs, the precise preparation of HOFs with targeted networks is still a big and long-standing challenge due to the low bonding energy and weakly directional but highly reversible H-bonds. Judiciously choosing tectons with rigid backbone, proper spatial conformation, and synergistic abundant noncovalent interactions is one of the effective solutions. Interestingly, the combination of machine learning and high-throughput crystalline screening may address this problem to some extent and will undoubtedly accelerate the discovery of new functional HOFs. Meanwhile, it is urgent to develop simple but reliable algorithmic models to reduce computational costs and make it practically viable and universal.There is a great need to discover more porous HOFs that are highly stable to meet requirements of various application scenarios. Although several strategies have been proposed to develop stable HOFs, the number of stable HOFs is still very few in comparison to the large number of stable MOF and COF counterparts. Given that structural stability is critically important to its performance reliability, and is of the primary prerequisites for industrial applications, more effort should be devoted to the discovery of porous HOFs with high stability.Some tectons bearing intrinsic catalytic active sites like porphyrins have been utilized to build HOFs for heterogeneous catalysis. In many cases, the π–π stacking and framework interpenetration/catenation will keep them from approaching catalytic substrates and therefore detract from the catalytic efficiency. Besides, most HOFs only have small pores, which may limit the mass transportation of substrates in the channels. Moreover, the lack of metal components in most HOFs also largely impedes their applications in heterogeneous catalysis. The encapsulation of catalytically active moieties such as enzymes, noble metal atoms/clusters/nanoparticles, polyoxometalates, and other catalytic active species into stable porous HOFs may address the above problems. Emphasis should be put not only on how to encapsulate the active species into HOFs but also on how these porous matrixes affect their catalytic performances, which may also open a new pathway to explore functional materials.The stability of HOFs in biological environments needs to be carefully investigated in in vitro and in vivo assays. The long-term biosafety of HOFs also needs to be evaluated for biomedical applications. So far, the size of most reported HOFs is in a millimeter or micrometer scale. Downsizing a bulky HOF to a nanoscale material is very challenging based on current technology. The facile preparation of nanoscale HOFs by either top-down or bottom-up strategies will largely promote their biological and clinic applications.In consideration of the highly ordered arrangement of tectons, AIE-modified organic building blocks are highly desirable to construct HOF-based photonic materials. In future research, HOFs may show their excellent capability in sensing due to their high structural tunability and precise structure information.
Although reticular chemistry has been successfully used to predict and design HOFs, the precise preparation of HOFs with targeted networks is still a big and long-standing challenge due to the low bonding energy and weakly directional but highly reversible H-bonds. Judiciously choosing tectons with rigid backbone, proper spatial conformation, and synergistic abundant noncovalent interactions is one of the effective solutions. Interestingly, the combination of machine learning and high-throughput crystalline screening may address this problem to some extent and will undoubtedly accelerate the discovery of new functional HOFs. Meanwhile, it is urgent to develop simple but reliable algorithmic models to reduce computational costs and make it practically viable and universal.
There is a great need to discover more porous HOFs that are highly stable to meet requirements of various application scenarios. Although several strategies have been proposed to develop stable HOFs, the number of stable HOFs is still very few in comparison to the large number of stable MOF and COF counterparts. Given that structural stability is critically important to its performance reliability, and is of the primary prerequisites for industrial applications, more effort should be devoted to the discovery of porous HOFs with high stability.
Some tectons bearing intrinsic catalytic active sites like porphyrins have been utilized to build HOFs for heterogeneous catalysis. In many cases, the π–π stacking and framework interpenetration/catenation will keep them from approaching catalytic substrates and therefore detract from the catalytic efficiency. Besides, most HOFs only have small pores, which may limit the mass transportation of substrates in the channels. Moreover, the lack of metal components in most HOFs also largely impedes their applications in heterogeneous catalysis. The encapsulation of catalytically active moieties such as enzymes, noble metal atoms/clusters/nanoparticles, polyoxometalates, and other catalytic active species into stable porous HOFs may address the above problems. Emphasis should be put not only on how to encapsulate the active species into HOFs but also on how these porous matrixes affect their catalytic performances, which may also open a new pathway to explore functional materials.
The stability of HOFs in biological environments needs to be carefully investigated in in vitro and in vivo assays. The long-term biosafety of HOFs also needs to be evaluated for biomedical applications. So far, the size of most reported HOFs is in a millimeter or micrometer scale. Downsizing a bulky HOF to a nanoscale material is very challenging based on current technology. The facile preparation of nanoscale HOFs by either top-down or bottom-up strategies will largely promote their biological and clinic applications.
In consideration of the highly ordered arrangement of tectons, AIE-modified organic building blocks are highly desirable to construct HOF-based photonic materials. In future research, HOFs may show their excellent capability in sensing due to their high structural tunability and precise structure information.
Overall, HOFs provide a powerful platform for an ultra-high-performance material by virtue of their metal-free, highly flexible, solution processable, easily regenerated, and recyclable features. We firmly believe that HOFs will achieve more groundbreaking advancements in the near future.
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