Metal–organic frameworks (MOFs) that respond to external stimuli such as guest molecules, temperature, or redox conditions are highly desirable. Herein, we coupled redox-switchable properties with breathing behavior induced by guest molecules in a single framework. Guided by topology, two flexible isomeric MOFs, compounds 1 and 2, with a formula of In(Me2NH2)(TTFTB), were constructed via a combination of [In(COO)4]− metal nodes and tetratopic tetrathiafulvalene-based linkers (TTFTB). The two compounds show different breathing behaviors upon the introduction of N2. Single-crystal X-ray diffraction, accompanied by molecular simulations, reveals that the breathing mechanism of 1 involves the bending of metal–ligand bonds and the sliding of interpenetrated frameworks, while 2 undergoes simple distortion of linkers. Reversible oxidation and reduction of TTF moieties changes the linker flexibility, which in turn switches the breathing behavior of 2. The redox-switchable breathing behavior can potentially be applied to the design of stimuli-responsive MOFs.
Metal–organic frameworks (MOFs) are a promising class of highly ordered porous materials with diverse applications in the fields of gas storage and separation, sensing, and catalysis1,2,3,4,5. Over the past few decades, a significant number of MOFs with various structures, porosities, and framework compositions have been extensively explored6. Amongst them, flexible MOFs have garnered particular interest because they combine crystalline order of the underlying coordination framework with cooperative structural transformability7,8,9,10,11,12. Additionally, they are able to respond to various chemical and physical stimuli such as light, pressure, temperature, redox environment, or the introduction of guest molecules13,14,15,16,17,18. A representative example is the breathing effect in which the framework experiences a reversible unit-cell dimensional change resulting from guest adsorption or desorption19. This leads to unique sorption behaviors which have never been observed in other systems20,21,22. On the other hand, the redox activity of MOFs has been explored through the introduction of redox-active metal nodes or organic ligands. These materials have shown promise for applications in microporous conductors, electrocatalysts, energy storage devices, and electrochemical sensors23,24,25,26,27.
The host structures in flexible MOFs can be altered by external stimuli, potentially altering the availability of the cavity to guest molecules. Building off this concept, we intended to couple the breathing behavior induced by guest molecules with redox-switchable properties in a single framework. The resulting materials are expected to show dual-stimuli-responsive behavior. Compared with other porous materials, the crystalline nature of MOFs provides a unique advantage through the study of their behavior via crystallography, therefore maximizing the understanding of the correlation between applied stimuli and ensuing properties28,29,30. To realize redox regulation of MOF porosity, a flexible framework with redox-active triggers is indispensable. The tetrathiafulvalene (TTF) is a sulfur-rich conjugated molecule with two reversible and easily accessible oxidation states (i.e., radical TTF•+ cation and TTF2+ dication) that have been widely studied as a critical electron donor component for conductive25,26,27, optoelectronic, and magnetic23, 24 materials. The oxidation of TTF to TTF•+ or TTF2+ converts the 7π-electron dithiolylidene ring to the aromatic 6π-electron configuration, and consequently results in a rigid, fully conjugated aromatic system. Bearing this in mind, the TTF moiety was incorporated into the linker of a MOF as a redox switch to control the flexibility of the framework. Although numerous flexible MOFs have been reported, redox-controlled flexibility in MOFs has never been studied.
Herein, two flexible isomeric MOFs with TTF moieties, compounds 1 and 2, were constructed using topology analysis as a guide. The two compounds display different breathing behaviors derived from the bending of linkers, the distortion of metal–ligand bonds and the relative sliding of interpenetrated networks. The TTF moieties allow for the reversible oxidation by I2 and reduction via treatment with N,N-dimethylformamide (DMF), which switches the linker flexibility and the breathing behavior of compound 2. As compound 2 is an anionic MOF, the effect of counterions on the breathing behavior is also studied using cation exchange experiments.
Topology-guided design of flexible MOFs
To obtain a flexible MOF with redox-responsive behavior, a topology-guided design was adopted. The tetratopic TTF-based linker, tetrathiafulvalene tetrabenzoate (TTFTB), was adopted as the redox switch, which can be regarded as a 4-connected square planar node (Fig. 1b). Topologically, the 4-connected square planar linker is able to form a variety of binodal networks when combined with different metal nodes. Among the numerous MOFs with square planar linkers in the literature, flexible frameworks have rarely been observed. The reported MOFs with square planar linkers are generally formed by inorganic building units that have high connectivity, mainly resulting in rigid frameworks. In this respect, the [In(COO)4]− seems to be a suitable inorganic building unit for the construction of flexible MOFs as it is a mononuclear metal node with relatively low connectivity. Topologically, it can be simplified into a 4-connected tetrahedral vertex (Fig. 1a), which could be extended by combination with square planar linkers into a pts type framework (Fig. 1c). The pts net is expected to show flexibility by changing bond angles between nodes.
As expected, the reaction between In3+ and TTFTB gave rise to the designed MOF structure. Interestingly, two isomeric MOFs were isolated by tuning the synthetic conditions. The isomeric MOFs displayed the same topology but different arrangements of linkers. Although the TTFTB was topologically simplified into a square, it shows a rectangular geometry in the structure. Taking this into consideration, two structures can be derived from the pts net. If all the linkers are aligned with the same orientation throughout the structure, compound 1 will be generated (Fig. 1d, f). On the other hand, if linkers with perpendicular orientations are arranged alternately within the structure, compound 2 (Fig. 1e, g) will be observed.
Single-crystal X-ray diffraction (SC-XRD) analysis reveals that compound 1 crystallizes in the orthorhombic space group Cccm (Supplementary Tables 1 and 2). The asymmetric unit (Supplementary Fig. 1a) contains half of an In3+ ion, half of a TTFTB ligand, and half of a dimethylammonium cation (Me2NH2+). As shown in Supplementary Fig. 1b, the [In(COO)4]− adopts a distorted tetrahedron coordination geometry with the four carboxylates from TTFTB ligands in chelating bidentate coordination. The central C=C bond of the TTF unit is 1.343(9) Å, which is comparable of the neutral TTF moiety state. As an anionic framework formed by [In(COO)4]− nodes, Me2NH2+ exists in the cavity to balance the charge. Overall, compound 1 is a twofold interpenetrated framework with a porosity of 48.2% determined by the PLATON31 calculations (Supplementary Fig. 2).
Interestingly, a framework isomer, compound 2, was isolated by reducing the reaction temperature. The crystal structure of compound 2 crystallizes in the triclinic space group Pī (Supplementary Tables 4 and 5). The asymmetric unit (Supplementary Fig. 3a) contains two In3+ ions, two TTFTB ligands, and two molecules of Me2NH2+. Two TTFTB with different conformations were observed within the structure (Supplementary Fig. 3b). They are perpendicular to each other and arranged alternately throughout the framework (Supplementary Fig. 4). This arrangement is different from that of the TTFTB in compound 1, which shows the same configuration and orientation throughout the structure. Compound 2 is also a twofold interpenetrated anionic MOF with Me2NH2+ located in the cavity. The PLATON31 calculations show that the total solvent-accessible volume gives a porosity of 46.9%. Both compounds 1 and 2 are formulated as In(Me2NH2)(TTFTB).
Breathing behaviors induced by N2 sorption
Usually, the breathing behaviors of MOFs can be triggered by the adsorption or desorption of guest molecules. Herein, the N2 sorption measurements at 77 K were conducted to assess the porosity and flexibility of compounds 1 and 2. The N2 uptake of compound 1 quickly reaches 100 cm3 g−1 at 0.05 bar before saturating. However, with the increase of pressure, another adsorption stage emerges at 0.18 bar which eventually pushes the N2 uptake to 375 cm3 g−1 (Fig. 2a). Similar to 1, the N2 isotherm of 2 exhibits low initial N2 uptake (70 cm3 g−1), followed by another distinct adsorption step (Fig. 2b). However, in 2, the second adsorption step appears at a lower pressure (0.05 bar). An adsorption vs. desorption hysteresis was observed which is an indication of discontinuous structural transition32. The gas adsorption isotherms of compounds 1 and 2 do not fit in any of six isotherm types classified by International Union of Pure and Applied Chemistry. In fact, the stepped isotherms are an indication of flexible frameworks which possess narrow-pore structures when no guests are present, and transform to an open structure triggered by adsorbed guests. Note that the dynamic behavior of compound 1 is not fully reversible, with a loss of crystallinity and porosity after each adsorption–desorption cycle, as suggested by PXRD and N2 isotherms (Supplementary Figs. 5 and 6). On the other hand, the breathing effect of compound 2 is fully reversible for at least three adsorption–desorption cycles.
The most distinctive advantage of MOFs over other porous materials is their long-range ordered crystalline structure, which can provide a unique insight into the structure–property correlation by means of crystallography29, 33. Therefore, SC-XRD analysis was carried out to provide direct structural evidence of the breathing behavior, and to shed light on the mechanism. The crystals of compounds 1 and 2 were examined under N2 flow at various temperatures, mimicking the N2 sorption process (Supplementary Table 8). The desolvated compound 2 shows a narrow-pore structure with blocked channels. The TTF moieties on the linker do not form a fully conjugated aromatic system and the linker adopts a bent conformation. Linkers bent in different directions are alternately arranged within each framework, resulting in a blocked channel and a narrow-pore structure (Fig. 2e and Supplementary Fig. 7). Reducing the temperature to 80 K saturates the pore with N2 molecules, which triggers the pore opening. In the structure of N2@2, linkers are arranged along the same direction within the framework so that an open-pore structure is observed (Fig. 2f and Supplementary Fig. 7). In a word, the flexible TTFTB within compound 2 partially changes its conformation, which explains the pore-opening upon N2 uptake.
The diffraction quality of crystals for compound 1 after desolvation is not good enough to allow for structural refinement. Thus, we turned to molecular simulations to explain the breathing behavior. The molecular model of desolvated compound 1 was built from the single structure of the synthesized sample by removing solvent molecules and performing geometry optimization. Compared with the as-synthesized structure, the optimized 1-desolvated structure shows a shrinkage in unit-cell volume and a mutual movement of two sets of frameworks (Fig. 2c). The simulated total N2 uptake of this narrow-pore structure is 130 cm3 g−1, which matches well with the experimental results. Molecular dynamics simulation reveals that the structure adapts to the loading of N2 molecules through the bending of metal–ligand bonds and the sliding of interpenetrated frameworks (Fig. 2d). The structural change opens the cavity and increases the pore volume, which explains the experimentally observed stepped adsorption isotherms. The change of unit-cell volume and the relative movement of two sets of frameworks in 1 causes a significant structural change which gradually decomposes the framework after each adsorption–desorption cycle. On the other hand, compound 2 undergoes a relatively mild linker flip, resulting in the observation of fully reversible breathing behavior.
Redox-controlled breathing behaviors
Experimentally obtained single-crystal structure indicates that the breathing behavior of compound 2 is derived from the flexibility of the TTFTB linker (Fig. 3). Therefore, we hypothesize that the breathing behavior of compound 2 can be controlled by tuning the linker flexibility. It is well known that TTF is an electron donor, and each dithiolylidene ring is a 7π-electron system with two electrons from each S atom and one from each sp2-C atom. Therefore, the TTF is not a fully conjugated aromatic system, which is also reflected by the bent conformation in the crystal structure. However, oxidation of TTF converts the S-heterocycles into an aromatic 6π-electron configuration, consequently transforming the central double bond to essentially a single bond. A conjugated aromatic system is formed which rigidifies the TTF moiety (Fig. 4c). In other words, the oxidation of TTF is expected to turn off its flexibility by forming a fully conjugated aromatic system.
Bearing this in mind, we explored the possibility of switching the MOF flexibility by redox chemistry. Solid state electrochemistry was performed on the compounds 1 and 2 to probe its redox behavior. Cyclic voltammetry of compounds 1 and 2 show the expected TTF processes. The two one-electron oxidation waves were observed at E1/2 = 0.16 and 0.43 V vs. Fc/Fc+ for compound 1 and E1/2 = 0.05 and 0.52 V vs. Fc/Fc+ for compound 2, respectively. These can be assigned to the TTF/TTF•+ and TTF•+/TTF2+ redox couples (Supplementary Figs. 9 and 10). I2 was reported as a modest oxidant for conversion of TTF into its radical state TTF•+ while maintaining the crystallinity of MOF to the maximum extent. Compounds 1 and 2 were oxidized by soaking their crystals in a solution of I2 in cyclohexane (0.1 M) at room temperature for 12 h. An obvious color change was observed which is attributed to the incorporation of I2 and the formation of TTF•+ (Supplementary Fig. 11). The diffuse reflectance ultraviolet–visible–near infrared (UV–Vis–NIR) spectrum of 1 (Supplementary Fig. 12) reveals low intensity bands at 4200 and 13,700 cm−1, ruling out the existence of TTF•+ in the as-synthesized samples. Upon oxidation with I2, the aforementioned bands significantly increase in intensity, which is consistent with the oxidation of neutral TTF to TTF•+. This result was corroborated by solid state Vis–NIR spectroelectrochemical measurements (Supplementary Fig. 13), where in situ oxidation of the parent compound over a potential range of 0–2 V led to an intensification of the band at 13,700 cm−1. This oxidation process was shown to be reversible because the band at 13,700 cm−1 decreased in intensity as the potential was returned to 0 V. Solid state UV–Vis–NIR spectroscopy of 2 revealed weak bands which can be assigned to the TTF radical cation; bands found at 4380 and 13,870 cm−1 may be assigned to the [TTF2]•+ mixed-valence state and [TTF2]2+ π-radical dimer, respectively (Supplementary Fig. 12). The presence of the TTF radical cation in the parent framework 2 is likely due to the low oxidation potential of the initial one-electron oxidation of the TTF moiety (confirmed by electrochemistry of the framework). The spectrum of the iodine-doped species, I3−@2, revealed a significant intensification of the previously described features as a result of the chemical oxidation of the framework with I2.
Electron paramagnetic resonance (EPR) studies of the solid compounds at 110 K further confirmed the generation of TTF•+ radical (Supplementary Fig. 14). All EPR spectra (which were recorded under the same conditions) showed an axial set of g values (g x,y = 2.006, g z = 2.013 for I3−@1 and g x,y = 2.005, g z = 2.010 for I3−@2), typical of TTF• + cation radicals, confirming that the TTF moiety in these compounds is the redox-active unit23, 34, 35. A negligible signal in the EPR spectrum of pristine 1 and 2 indicates the presence of the vast majority of the TTF moiety in its neutral form, which is consistent with the very weak band at ~13,500 cm−1 in the UV–Vis–NIR spectra23, 34, 35. The EPR signal increased after I2 doping, confirming the increased concentration of the TTF• + radical cation.
The magnetic susceptibility data of polycrystalline samples of I3−@1 and I3−@2 are displayed in Supplementary Fig. 15 as the χmT vs. T plot in a DC field of 1 kOe. The χmT (0.375 and 0.361 cm3 K mol−1 for I3−@1 and I3−@2 at 300 K, respectively) gradually decreased when the temperature dropped, revealing the existence of antiferromagnetic interactions. The result indicates the magnetic contribution of the radical electrons. The expected χmT value for the isolated S = 1/2 radical electrons (TTF•+) was consistent with the result of the EPR measurement. The room temperature electrical conductivities of 1 and 2 (1.23 × 10−9 and 1.16 × 10−9 S cm−1 for 1 and 2, respectively, Supplementary Fig. 16 and Supplementary Table 7) were significantly improved upon oxidation (5.50 × 10−8 and 1.68 × 10−7 S cm−1 for I3−@1 and I3−@2, respectively, Supplementary Fig. 16 and Supplementary Table 7). However, the lack of suitable conducting channels still results in poor conductivity. The altered conductivity can be attributed to the TTF radical cation of the doped compound compared to their neutral counterparts.
Direct structural evidence of I3−@1 and I3−@2 are provided by X-ray crystallography (Supplementary Tables 3 and 6). Due to their good chemical stability, compounds 1 and 2 maintained single crystalline after the oxidation, thus their structural transformations can be monitored by SC-XRD. The existence of I3− as the product of oxidation reaction is observed in the crystal structure of both 1 and 2, which is relatively rare among I2 doped MOFs (Fig. 3). The oxidized MOFs, namely I3−@1 and I3−@2, are isomers with the same formula of In2(Me2NH2)(TTFTB•+)2(I3−). After I2 oxidation, the space group and cell parameters of compound 1 are very similar (Fig. 4d). However, I3− as the product of oxidation reaction was observed in the channel along with a slight conformational change of linkers (Fig. 3b and Supplementary Fig. 17). The central C···C distance of the TTF units increases from 1.343(9) to 1.387(6) Å, corresponding to the partial conversion of neutral TTF to its radical cationic state TTF•+. The crystal structure of compound 2, however, undergoes dramatic change upon I2 oxidation (Fig. 4e). The crystal system transformed from triclinic to monoclinic along with the space group change from Pī to P2/m. The bent TTFTB ligand in compound 2 became coplanar in I3−@2, along with the changes of bond lengths and angles around the [In(COO)4]− node (Fig. 3d and Supplementary Fig. 18). The conformational change of TTFTB increases the symmetry by creating an inversion center and a twofold axis through the molecule, which in turn changes the space group of the whole structure. The central C···C distance of the TTF units in I3−@2 were measured to be 1.418(13) and 1.416(11) Å, which is significantly longer than the neutral compounds. More importantly, the flexible TTFTB became rigid. Since the breathing effect of 2 is resulted from the conformational change of flexible TTFTB, a rigid linker is expected to result in the loss of breathing behavior (Supplementary Fig. 19).
As expected, the I3−@2 shows a type I isotherm indicating a rigid microporous structure (Fig. 4b). The step at 0.05 bar disappeared upon oxidation, suggesting that the framework flexibility is turned off by oxidation. However, the I3−@1 still shows a stepped isotherm with hysteresis loops, although the total uptake is reduced due to the pore space that is partially occupied by I3− (Fig. 4a). Obviously, the flexibility of compound 1 is not affected by the change within the linkers. This is in line with the breathing mechanism of 1 which involves the bending of metal–ligand bonds and the sliding of two mutually interpenetrated frameworks. The relative movement of two interpenetrated frameworks is independent of the linker flexibility. Note that the oxidation of TTF moieties in compounds 1 and 2 are reversible. I3−@1 and I3−@2 could return to their initial structures by DMF treatment which reduced the TTF•+ and removed the I3− (Supplementary Fig. 20). The restored 1 and 2 displayed the same crystal structure and sorption properties as the pristine samples. These results clearly demonstrates that the dynamic behavior of flexible MOFs is a reversible process that can be switched on and off by redox chemistry. It should be noted that oxidation of 1 and 2 by I2 occurs along with the formation of I3− as counterions. We cannot rule out the possible influence of I3− as guest species on the breathing behavior of MOFs.
Effects of counterions
As an anionic framework, the [Me2NH2]+ counterions could also play an important role on the behavior of the framework. Indeed, the counterions serve as a special guest molecule that interacts with the framework though coulombic interactions, which could lead to dramatic differences in gas adsorption capacity36. However, it is usually difficult to precisely determine the position of the counterions by X-ray crystallography because they are not bound to the framework. This also hinders the estimation of sorption behaviors by molecular simulation as the counterions can move upon temperature changes or gas adsorption/desorption. In fact, the porosities of 2-desolvated and N2@2 were estimated by molecular simulation based on their respective single-crystal structures using N2 as a probe, which indicated similar accessible pore volume. Therefore, 2-desolvated and N2@2 are expected to have the same theoretical N2 uptake, contradicting the experimental results. This is tentatively explained by the steric effect of the counterions, which are large enough to block the small channel of 2-desolvated resulting in an almost non-porous structure. The window size of N2@2, on the other hand, is large enough for both [Me2NH2]+ counterions and N2 molecules resulting in the observation of a porous structure. To systematically investigate the effect of counterions, cationic exchange was conducted on compound 2.
The [Me2NH2]+ can be readily replaced by [Me4N]+, [Et4N]+ and [Bu4N]+ (Supplementary Fig. 22). Based on the 1H-NMR results (Supplementary Figs. 23–26), [Me2NH2]+ was fully replaced by the [Bu4N]+ cation, whereas the exchange by Et4N+ was incomplete. N2 adsorption isotherms further demonstrate that [Bu4N]+@2 has an open structure without any flexible behavior. On the other hand, the [Me4N]+@2 and [Et4N]+@2 are almost non-porous (Fig. 5a). This counter-intuitive result is rationalized by the crystal structures of [Bu4N]+@2 and [Et4N]+@2 (Supplementary Fig. 28 and Supplementary Table 9). Based on the single-crystal structure, the [Bu4N]+@2 always shows an open structure (Fig. 5b), while the channels in [Et4N]+@2 remain closed even in DMF (Fig. 5c). Therefore, [Bu4N]+@2 exhibits a rigid porous structure while [Et4N]+@2 is almost non-porous. Note that the linker in the structure of [Et4N]+@2 is disordered even at low temperature (100 K), owing to the incomplete cation exchange. In fact, the exchange of [Me2NH2]+ by [Et4N]+ closes the external MOF cavities, which formed a non-porous shell and prevents further ion exchange in the core of the framework. The pore-opening effect of Bu4N+ is tentatively attributed to its steric hindrance, which prevents the movement of TTFTB linkers. The cation exchange experiment highlights the important role of [Me2NH2]+ on the N2-induced structural change of compound 2.
In conclusion, we show that the breathing behavior of MOFs can be controlled by redox chemistry in a flexible TTF-based MOF. The structural transformations upon guest adsorption and oxidation are investigated by SC-XRD and corroborated by molecular simulations. The effect of counterions on the breathing behavior are also studied by cation exchange experiments. The redox-controlled dynamic behavior of MOFs is reminiscent of sophisticated biological behavior such as redox regulation of enzymes. We believe that the discovery of redox-switchable breathing MOFs should not only lead to a new generation of unique adsorbents, but also facilitate the applications of flexible MOFs in gas storage and separation, molecular sensing, and switchable catalysis.
Synthesis of compound 1
To the solution of H4TTFTB (0.013 g, 0.034 mmol) in 2 mL DMF, a solution of In(NO3)3·4.5H2O (0.020 g, 0.052 mmol) in 0.5 mL H2O was added, followed by the addition of 0.5 mL ethanol and 0.4 mL CH3COOH. The mixture was heated to 120 °C for 72 h, then allowed to cool down to room temperature at the rate of 5 °C h−1. The red octahedral crystals (0.018 g) of 1, [(TTFTB)In]•(CH3NH2CH3)•0.7(C2H5OH)•(C3H7ON), were obtained by filtration and washed with DMF and CH3COCH3 three times, respectively. Thermogravimetric analysis (TGA) data was shown in Supplementary Fig. 8a. Yield 82.57% (based on H4TTFTB). Calcd for C16.4H19.2InN2O9.7S4 (Mr = 642.61): C, 30.65; H, 3.01; N, 4.36%; S, 19.96%. Found: C, 30.20; H, 2.54; N, 2.63%; S, 19.96%. FT-IR (KBr pellet, cm−1): 3675 w, 2782 w, 2360 w, 2796 w, 1700 w, 1653 m, 1603 s, 1539 s, 1506 m, 1380 vs., 1174 m, 1137 m, 1097 m, 1018 m, 862 m, 825 m, 765 s, 705 m, 668 m, 569 m, 483 m, 419 m.
Synthesis of compound I3 −@1
The iodine doping of I3−@1 was undertaken using a diffusion technique. Crystals of 1 were soaked in a solution of iodine in cyclohexane (0.1 M) at room temperature for 12 h. Note that the color of the crystals became deeper as the doping time was increased (Supplementary Fig. 11). The crystals of I3−@1, [(TTFTB)2In2]•(I3)•(CH3NH2CH3)•4(C6H12), were washed with cyclohexane. The quantities of iodine incorporated were confirmed by TGA (Supplementary Fig. 21) and elemental analysis: one I3− for I3−@1 per unit cell. Anal. Calcd. for C46H56I3In2NO16S8 (Mr = 1745.80): C, 31.65; H, 3.23; N, 0.80; S, 14.69. Found: C, 31.96; H, 1.55; N, 17.23; S, 10.07. Selected IR data (KBr, cm−1): 3675 w, 2989 w, 2546 w, 2360 m, 2342 m, 1705 vs., 1653 s, 1604 s, 1526 m, 1405 vs., 1317 m, 1285 s, 1177 m, 1119 m, 1015 s, 864 m, 763 s, 696 m, 668 w, 551 w, 481 w, 418 w.
Synthesis of compound 2
To the solution of H4TTFTB (0.013 g, 0.034 mmol) in 2 mL DMF, a solution of In(NO3)3·4.5H2O (0.020 g, 0.052 mmol) in 0.5 mL H2O was added, followed by the addition of 0.5 mL ethanol and 0.3 mL CH3COOH. The mixture was heated to 60 °C for 72 h. After that, 0.3 mL CH3COOH was added, and the mixture was heated to 120 °C for 72 h again, then allowed to cool down to room temperature at a rate of 5 °C h−1. The red rod-like crystals (0.008 g) of 2, [(TTFTB)2In2]•(CH3NH2CH3)2•2(C2H5OH)•2(C3H7ON), were obtained by filtration and washed with DMF and CH3COCH3 three times, respectively. TGA data was shown in Supplementary Fig. 8b. Yield 43.79% (based on H4TTFTB). Calcd for C34H42In2N4O20S8 (Mr = 1312.87): C,31.30; H, 3.22; N, 4.27%; S, 19.54%. Found: C, 30.20; H, 2.54; N, 2.63%; S, 4.27%. FT-IR (KBr pellet, cm−1): 3649 w, 3003 w, b, 2546 w, 1705 s, 1603 s, 1540 vs., 1374 vs., 1175 m, 1137 m, 1100 m, 1016 s, 860 m, 831 s, 783 m, 767 s, 704 m, 674 m, 568 w, 483 m, 436 m.
Synthesis of compound I3 −@2
The iodine doping of I3−@2 was undertaken using a diffusion technique. Crystals of 2 were soaked in a solution of iodine in cyclohexane (0.1 M) at room temperature for 12 h. Note that the color of the crystals became deeper as the doping time was increased (Supplementary Fig. 11). The crystals of I3−@2, [(TTFTB)2In2]•(I3)•(CH3NH2CH3)•4(C6H12), were washed with cyclohexane. The quantities of iodine incorporated were confirmed by TGA (Supplementary Fig. 21) and elemental analysis: one I3− for I3−@2 per unit cell. Anal. Calcd. for C46H56I3In2NO16S8 (Mr = 1745.80): C, 31.65; H, 3.23; N, 0.80; S, 14.69. Found: C, 31.96; H, 1.55; N, 17.23; S, 10.07. Selected IR data (KBr, cm−1): 3073 w, 2920 m, 1607 m, 1540 m, 1507 m, 1428 s, b, 1283 m, 1176 m, 1138 m, 1102 m, 1016 s, 902 w, 869 m, 856 s, 823 m, 781 m, 769 s, 703 m, 682 m, 485 w, 464 m, 438 m.
Synthesis of compound [Me4N]+@2, [Et4N]+@2, and [Bu4N]+@2
The cation exchanged guest@2 was obtained by the exchange of [Me2NH2]+ counterions. The crystals of compound 2 were immersed in the 0.01 mol L−1 [Me4N]Cl, [Et4N]Cl, and [Bu4N]Cl DMF solution, respectively. Over 10 days, the solution was changed every 12 h to facilitate the counterion exchange. After the exchange process was complete, the crystals were immersed in fresh DMF for one day to remove the guest cations. TGA data was shown in Supplementary Fig. 27.
Elemental analyses for C, H, N, and S were performed on Perkin-Elmer 240C analyzer. FT-IR data were recorded on Vector27 Bruker Spectrophotometer with KBr pellets in the 4000–400 cm−1 region. TGA data were obtained on an STA 449C thermal analysis system with a heating rate of 10 °C min−1 under N2 atmosphere. The PXRD were collected with a scan speed of 0.1 s deg−1 on a Bruker Advance D8 (40 kV, 40 mA) diffractometer with Cu radiation (λ = 1.54056 Å) at room temperature. Calculated PXRD patterns were generated using Mercury 3.0. Magnetic susceptibility measurements were performed using a Quantum Design SQUID VSM magnetometer on microcrystalline samples for all compounds. EPR spectra were obtained by using a Bruker EMX-10/12 variable-temperature apparatus at 110 K. Gas sorption measurements were conducted using a Micrometritics ASAP 2020 system. See Supplementary Methods for details.
The X-ray crystallographic coordinates for structures reported in this article have been deposited at the Cambridge Crystallographic Data Centre (CCDC), under deposition number CCDC 1560234, 1560199, 1560204, 1560221, 1560235, 1560236, 1560237, and 1560977 for compound 1, I3−@1, 2, I3−@2, 2-close, 2-open, TEA@2, and TBA@2, respectively. These data can be obtained free of charge from the Cambridge Crystallographic Data Centre via www.ccdc.cam.ac.uk/data_request/cif. All relevant data supporting the findings of this study are available from the corresponding authors on request.
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This work was supported by the Major State Basic Research Development Program (No. 2013CB922101), and the National Natural Science Foundation of China (Nos. 91433113 and 21631006). The gas adsorption–desorption studies of this research were supported by the Center for Gas Separations Relevant to Clean Energy Technologies, an Energy Frontier Research Center funded by the US Department of Energy, Office of Science, Office of Basic Energy Sciences under Award Number DE-SC0001015. Structural analyses were supported as part of the Hydrogen and Fuel Cell Program under Award Number DE-EE0007049. Prof. Deanna M. D’Alessandro and Dr. Chanel Leong in School of Chemistry, the University of Sydney are acknowledged for their assistance in diffuse reflectance UV–Vis–NIR spectra, solid state electrochemical, and spectroelectrochemical measurements. This computational work was funded by the Robert A. Welch Foundation through a Welch Endowed Chair to H.C.-Z (A-0030). Texas A&M Supercomputing Facility was acknowledged to provide computing resources. The Distinguished Scientist Fellowship Program (DSFP) at KSU is gratefully acknowledged for supporting this work. The authors also acknowledge the financial supports of US Department of Energy Office of Fossil Energy, National Energy Technology Laboratory (DE-FE0026472). S.Y. also acknowledges the Texas A&M Energy Institute Graduate Fellowship Funded by ConocoPhillips and Dow Chemical Graduate Fellowship.
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