Guest-Controlled Incommensurate Modulation in a Meta-Rigid Metal–Organic Framework Material

Structural transitions of host systems in response to guest binding dominate many chemical processes. We report an unprecedented type of structural flexibility within a meta-rigid material, MFM-520, which exhibits a reversible periodic-to-aperiodic structural transition resulting from a drastic distortion of a [ZnO4N] node controlled by the specific host–guest interactions. The aperiodic crystal structure of MFM-520 has no three-dimensional (3D) lattice periodicity but shows translational symmetry in higher-dimensional (3 + 2)D space. We have directly visualized the aperiodic state which is induced by incommensurate modulation of the periodic framework of MFM-520·H2O upon dehydration to give MFM-520. Filling MFM-520 with CO2 and SO2 reveals that, while CO2 has a minimal structural influence, SO2 can further modulate the structure incommensurately. MFM-520 shows exceptional selectivity for SO2 under flue-gas desulfurization conditions, and the facile release of captured SO2 from MFM-520 enabled the conversion to valuable sulfonamide products. MFM-520 can thus be used as a highly efficient capture and delivery system for SO2.


■ INTRODUCTION
Metal−organic framework (MOF) materials are synthetic porous materials constructed from bridging metal centers and organic ligands. 1 MOFs can be either rigid 2 or flexible 3 depending upon the metal−ligand coordination combination, framework topology, and organic functionality. Rigid MOFs retain a well-defined framework structure and pore interior against external variables (e.g., temperature, pressure, and guest inclusion), making them useful for the separation and purification of substrates. 2,4 In contrast, flexible MOFs can undergo reversible breathing transitions between typically two well-defined periodic crystal structures. One form is often described as narrow-pored and the other form is described as large-pored, and these two forms therefore show different porosities and properties. 5−10 Figure 1 illustrates various structural responses to guest binding within a MOF lattice. Breathing and metastable MOFs show two prevailing types of phase transitions, namely, periodic-to-periodic and periodic-to-amorphous. Beyond that, there is also an intriguing class of mesoporous MOFs, allowing the formation of adsorbate superlattices based upon long-range collective adsorbate−adsorbate interactions. 11 The periodic-toaperiodic transition observed here for MFM-520 represents a new type of framework flexibility in crystalline porous solids. Superspace group theory 12 has been used to describe the commensurate structure of crystalline zeolite SSZ-57 13 in higher-dimensional space, and this has been applied to interpret the incommensurate modulated structures described here.

■ EXPERIMENTAL SECTION
Synthesis of MFM-520. All reagents were used as received from commercial suppliers without purification. The synthesis of H 4 L (4,4′bipyridine-2,6,2′,6′-tetracarboxylic acid) and {[Zn 2 (L)·4H 2 O]} ∞ (MFM-520·H 2 O) was carried out using previously reported methods. 14 In Situ Synchrotron Single-Crystal X-ray Diffraction and Structural Characterization. In situ synchrotron X-ray singlecrystal diffraction data were collected on beamline 11.3.1 of the Advanced Light Source using monochromated radiation [λ = 0.7749(1) Å]. After data collection for as-synthesized sample MFM-520·H 2 O, the same single crystal (0.10 × 0.05 × 0.05 mm 3 ) was placed in a capillary gas handling cell and evacuated in situ under dynamic vacuum and a stream of N 2 at 340 K centered on the capillary for 4 h. The single-crystal diffraction data of dehydrated MFM-520 were collected at 290 K. Upon loading of CO 2 into MFM-520 at 1.0 bar and 290 K, three diffraction data sets were collected at 270 K to examine the possible dynamic behavior of the structural relaxation (i.e., adsorbate−adsorbent equilibrium and change in the modulation vector). The single crystal was then reactivated under vacuum and heating to remove all adsorbed gases. The in situ singlecrystal diffraction data for SO 2 -loaded MFM-520 were collected using the same method as for the CO 2 -loaded sample.
The influence of temperature on the periodic-to-aperiodic phase transition was monitored by collecting in situ single-crystal diffraction data for dehydrated MFM-520 at 180−350 K on a Rigaku Oxford XtaLAB diffractometer using Mo-Kα radiation. No change in the modulation vectors of MFM-520 was observed between 180 and 350 K (Table S2), confirming the negligible impact of temperature on the modulation vector of MFM-520.
To examine the reversibility of the periodic-to-aperiodic phase transition observed in MFM-520, a single crystal of rehydrated MFM-520·H 2 O, formed by the treatment of dehydrated MFM-520 with water, was studied by single-crystal diffraction at 180 K. This experiment confirms the absence of satellite reflections of the rehydrated sample ( Figure S6).
In the (3 + 2)D incommensurately modulated structure, each parameter of modulation can be expanded as a Fourier series using eq 1: (1) where x 4 = q 1 r μ + t, x 5 = q 2 r μ + u, and t and u are initial phases in the range of 0 to 1. The real structural parameters can be expressed as eq 2:

∑ ∑
The average structure parameters p ave μ were determined by direct methods and least-squares refinements, and the modulations were refined globally using free variables. All non-hydrogen atoms were refined anisotropically, and hydrogen atoms were placed using a riding model. Given the complexity of the structure, soft constraints on the bond length/angle to both host and guest were applied in the final stage of refinement. All refinements of the crystal structures were performed on the JANA2006 software platform. 15 Gas Adsorption Isotherms. Gravimetric sorption isotherms for N 2 , CO 2 , SO 2 , CH 4 , CO, and O 2 were recorded at various temperatures on a Hiden Isochema IGA-003 system under high vacuum (10 −10 bar) produced by a turbo pumping system. Temperatures were maintained using a programmed water bath. Ultra-pure research grade gases (99.999%) were purchased from BOC or Air Liquide. In a typical gas adsorption experiment, 50 mg of acetone-exchanged MFM-520 was loaded into the IGA system and activated at 393 K under dynamic high vacuum (10 −10 bar) for 1 day Journal of the American Chemical Society pubs.acs.org/JACS Article to give fully desolvated MFM-520. BET surface areas and porosity data were obtained from N 2 isotherm data at 77 K. Gas Separation by Breakthrough Experiments. In the breakthrough experiments, the flow rate of the entering gas mixture was maintained at 50 mL min −1 , and the gas concentration, C, of SO 2 , CO 2 , and N 2 at the outlet was determined by mass spectrometry and compared with the corresponding inlet concentration C 0 , where C/C 0 = 1 indicates complete breakthrough. Breakthrough separation of SO 2 /CO 2 was conducted using a mixture containing SO 2 (2500 ppm) and 15% CO 2 (v/v) diluted in He through a fixed bed packed with MFM-520 at 298 and 318 K and 1 bar at a flow rate of 50 mL min −1 . Figure 2. Column I: views of in situ synchrotron X-ray diffraction images of the hk0 plane. Column II: views of the corresponding crystal structures of MFM-520 as a function of guest inclusion/removal. 8 × 8 × 2 means the unit cell of the modulated structure is 8 times that of the average structure along the a and b axes and 2 times along the c axis; 7 × 7 × 2 means the unit cell of the modulated structure is 7 times that of the average structure along the a and b axes and 2 times along the c axis. Column III: details of the structure shown in the red box in column II. Column IV: molecular details of host−guest interactions. The MOF framework, zinc, oxygen, carbon, and sulfur are shown in blue, green, red, gray, and yellow, respectively. Bond distances are shown in Å. (a) MFM-520·H 2 O, (b) MFM-520, (c) MFM-520·CO 2 , and (d) MFM-520·SO 2 . A comparison of all in situ synchrotron X-ray diffraction images of the hk0.5 and hk1 planes is shown in Figure S5. The reflection conditions of MFM-520·H 2 O are 00l: l = 2 × integer and h00: h = 2 × integer. According to superspace group theory, 12 there is a supercentered setting with a s = a, b s = b, c s = 2c, Q 1 = α(a s * + b s *), and Q 2 = α(−a s * + b s *), which is equivalent to the basic setting a, b, c, q 1 = α(a* + b*) + 0.5c*, and q 2 = α(−a* + b*) + 0.5c*. Because the tables of (3 + 2)D superspace groups 19 provide only reflection conditions with supercenterd settings, we transformed the basic setting to supercentered settings to determine the reflection conditions. With the supercentered setting, the hk0, hk0.5, and hk1 planes are transformed to HK0, HK1, and HK2, respectively ( Figure S5). The reflection conditions of MFM-520, MFM-520·CO 2 , and MFM-520·SO 2 are HKLMN: L + M + N = 2 × integer, HK0MN: M = 2 × integer, HHLM0: L = 2 × integer, HH̅ L0N: N = 2 × integer, H0LMM̅ : 2H + L + 2M = 4 × integer, and 0KLMM: 2K + L + 2M = 4 × integer, corresponding to (3 + 2)D superspace group 136.2.69.10, adopting the symbol P4 2 /mnm(α, α, 1/2) 00qs(−α, α, 1/2)0sq0 with basic settings.
The final results have been converted to dimensionless plots as shown in Figure 4.
The fixed bed of MFM-520 for the adsorptive removal of low concentrations of SO 2 under wet conditions was first exposed to a flow of 1.5% H 2 O in He until the breakthrough of water. A stream of 0.25% SO 2 (i.e., 2500 ppm) diluted in He was then flowed through the packed bed of MFM-520 (approximately 1 g) at a total flow rate of 50 mL min −1 at 298 K and 1.0 bar. Dimensionless breakthrough plots were calculated with the following parameters: bed diameter, d, (7 mm); bed length, L, (120 mm); bed volume (5.0 mL); sample mass (1.0 g); sample framework density (1.55 g/cm 3 ); and flow rate (50 mL/min). The sample occupied a volume of 0.65 mL (assuming 100% purity and no framework collapse), and thus the fractional porosity of the fixed bed, ε, was calculated to be 0.87. The superficial gas velocity, u, at the entrance of the bed corresponded to 0.22 m/s, and the characteristic contact time between the gas and the sample of MFM-520 corresponded to εL/u = 4.82 s. The dimensionless time, τ, was obtained by dividing the actual time, t, by the contact time between the gas and the MFM-520 sample, εL/u (i.e., τ = tu/εL).
Inelastic Neutron Scattering (INS) Experiments. INS spectra were recorded on the TOSCA spectrometer at the ISIS Facility at the STFC Rutherford Appleton Laboratory. TOSCA is an indirect geometry instrument that provides a wide spectral range (−25 to 4000 cm −1 ) with resolution optimized in the 50−2000 cm −1 range. In this region, TOSCA has a resolution of 1.25% of the energy transfer. The instrument is composed of 130 3 He detectors in forward and backscattering geometries located 17 m downstream from a 300 K Gd poisoned water moderator. A temperature of 10 ± 0.2 K was maintained during data collection by two He closed-cycle refrigerators with 30 mbar He as an exchange gas.
A sample of MFM-520 was activated at 120°C and 1 × 10 −7 mbar for 1 day and then placed into an 11-mm-diameter vanadium sample can, which was loaded into a helium closed-cycle refrigerator (CCR) cryostat and cooled to 10 K for data collection. Defined amounts of CO 2 and SO 2 were introduced by warming the sample to 290 K, and the gas was dosed volumetrically from a calibrated volume. The gasloaded sample was then cooled to 10 K over a period of 2 h to ensure good mobility of adsorbed gases within the crystalline MFM-520. The sample was retained at 10 K for an additional 30 min before data collection to ensure thermal equilibrium.
Density Functional Theory (DFT) Calculations. DFT calculations were performed using CASTEP (version 19.11). 16 The generalized gradient approximation (GGA) as implemented by Perdew−Burke−Ernzerhof (PBE) was used to describe the exchange-correlation interactions. On-the-fly norm-conserving pseudopotentials were employed to account for the effects of core electrons with the default energy cutoff (∼870 eV) for the plane-wave basis. The unit cell configuration determined by XRD was used as the initial structure for the simulations. The atomic coordinates of the guest molecules were first relaxed by molecular dynamics at 300 K for 10 ps to find the optimal binding sites that are not constrained by symmetry (the MOF structure was fixed during this relaxation). The final configurations (including both the MOF and the guest molecules) were further relaxed using the conjugate gradient method to allow minimization of the potential energy and the interatomic forces. The energy tolerance for the electronic structure calculations was 5 × 10 −10 eV, and the energy tolerance for ionic relaxation was 5 × 10 −9 eV. The tolerance for the interatomic forces was 1 meV/Å. After convergence, the dynamic matrix was obtained using the linear response method, from which the phonon frequencies and vibrational modes were calculated. The electronic structure calculations were performed on a 3 × 3 × 1 Monkhorst−Pack mesh, and the dynamic matrix was calculated directly on the same mesh and then interpolated on a 7 × 7 × 3 Monkhorst−Pack mesh. The IR intensities were directly computed with CASTEP. 16 The OClimax software 17 was used to convert the DFT-calculated phonon results to the simulated INS spectra.
Conversion of Captured SO 2 . MFM-520 was activated at 393 K under vacuum overnight. The sample was cooled, and MFM-520 was dosed with SO 2 for 1 h to reach adsorption equilibrium. Morpholin-4amine (128.0 mg, 1.25 mmol) and SO 2 @MFM-520 (357 mg, equivalent to 1.18 mmol of SO 2 ) were suspended in CH 3 CN (3 mL) and stirred for 1 h. 4-Methoxy-aryldiazonium tetrafluoroborate (55.0 mg, 0.25 mmol) in CH 3 CN (1 mL) was added dropwise to the above suspension, and the mixture was stirred at room temperature for 1 h. The mixture was filtered, and the filtrate was evaporated. NMR spectroscopy and preparative thin layer chromatography (TLC) were used to quantify the conversion of 4-methoxy-aryldiazonium tetrafluoroborate and the yield of the sulfonamide. Benzenaldehyde was used as an internal standard.   (6), and 1.959(5) Å, respectively] change with the loss of water and lie in ranges of 2.07−2.12, 2.25−2.58, and 1.79−2.11 Å, respectively, for dehydrated MFM-520. This is accompanied by the modulation of the electron density at the Zn(II) center with the formal oxidation state ranging from 1.70(10) to 1.93(10) in MFM-520 as determined by bond valence sum (BVS) calculations 20 for the different Zn(II) centers (Figure 3a). In contrast, those in MFM-520·H 2 O have the same charge of 1.974 (14).
The resulting structure of dehydrated MFM-520 is aperiodic in 3D space but periodic in (3 + 2)D space, and the two modulated vectors (q 1 and q 2 ) are projections of the additional two dimensions along the three directions of 3D reciprocal space. Importantly, all satellite reflections of dehydrated MFM-520 disappear on rehydration to MFM-520·H 2 O, demonstrating the reversibility of this periodic-to-aperiodic phase . The discrepancies, particularly for the lattice modes at low energy (<200 cm −1 ), are due to the limitation that DFT simulations can be conducted only on average unit cells, which does not take the incommensurate modulation into consideration. (g) Dimensionless breakthrough plots for SO 2 /N 2 mixtures under dry (solid lines) and humid (dashed lines) conditions. Dry conditions: 2500 ppm SO 2 , 99.75% N 2 , total flow rate 50 mL min −1 . Wet conditions: 1.5% H 2 O, 2500 ppm SO 2 , 98.25% N 2 , total flow rate 50 mL min −1 . (h) Dimensionless breakthrough plots for SO 2 /CO 2 mixtures at 298 K (15% CO 2 , 2500 ppm SO 2 , 84.75% He, total flow rate 50 mL min −1 ). (i) Dimensionless breakthrough plots for cyclic SO 2 adsorption under both dry and humid conditions. Dry conditions: 2500 ppm SO 2 , 99.75% He, total flow rate 50 mL min −1 . Wet conditions: 1.5% H 2 O, 2500 ppm SO 2 , 98.25% He, total flow rate 50 mL min −1 . For experiments under humid conditions, the bed was first exposed to a flow of 1.5% H 2 O in He until the breakthrough of water.
Journal of the American Chemical Society pubs.acs.org/JACS Article transition ( Figure S6). No change was observed in the modulation vectors for dehydrated MFM-520 between 180 and 350 K (Table S2). Interestingly, for the periodic-toaperiodic phase transitions in inorganic materials, metal alloys, and organic compounds, which are induced by changes in temperature and electric and magnetic fields, 21−24 the periodicto-aperiodic transition observed in MFM-520 is controlled by host−guest interactions, representing the first example of such a phenomenon for an inorganic−organic hybrid material or porous solid. Dehydrated MFM-520 displays a BET surface area of 313 m 2 g −1 and a pore volume of 0.146 cm 3 g −1 , 14 and singlecomponent adsorption isotherms for SO 2 , CO 2 , CH 4 , CO, O 2 , and N 2 in MFM-520 have been recorded at 273−318 K up to 1.0 bar (Figure 4a, Figures S9−S12). The excess adsorption uptake of SO 2 at 298 K and 1.0 bar is 3.38 mmol g −1 , which is higher than those of CO 2 , CH 4 , CO, O 2 , and N 2 (0.77, 0.71, 0.36, 0.19, and 0.18 mmol g −1 , respectively). More significantly, at low pressure (e.g., 0.01 bar, 298 K), where all other gases show negligible uptakes (0.09 mmol g −1 for CO 2 ; <0.01 mmol g −1 for CH 4 , CO, O 2 , and N 2 ), MFM-520 displays a notably higher isothermal uptake of SO 2 (1.66 mmol g −1 ), accompanied by fast adsorption kinetics typically within minutes ( Figures S13 and S14). The static SO 2 uptake of MFM-520 is comparable to those of the best-behaving sorbents but is lower than the dynamic SO 2 uptake of SIFSIX-2-Cu-i, 25 which possesses very narrow pores (Table  S3). Often, there is a trade-off between high adsorption at low pressure and difficulties in the complete regeneration of narrow-pored MOFs. Facile regeneration of the SO 2 -saturated MFM-520 can be readily achieved solely via a pressure swing, and no loss of SO 2 adsorption capacity or crystallinity of MFM-520 was observed after 75 cycles of SO 2 adsorption− desorption (Figure 4b).
Further analysis of the adsorption thermodynamics of MFM-520 reveals that the isosteric heat of adsorption (Q st ) for CO 2 is 32−48 kJ mol −1 and the entropy of adsorption (ΔS) decreases steadily with increasing surface coverage, consistent with the expected ordering of adsorbed CO 2 molecules in MFM-520. In comparison, Q st for SO 2 adsorption reaches ∼120 kJ mol −1 at low surface coverage and decreases gradually to 60 kJ mol −1 with increasing loading of SO 2 . The calculated value of Q st is consistent with the calorimetric measurements of 43 and 96 kJ mol −1 for CO 2 and SO 2 adsorption, respectively ( Figures S15 and S16). The higher value of Q st for SO 2 uptake is consistent with the expected stronger interaction between the framework and SO 2 compared with CO 2 . However, the ΔS for SO 2 adsorption increases steadily from an initial −260 to −135 J K −1 mol −1 with increasing loading of SO 2 . This observation is opposite to the prevailing understanding of gas adsorption in porous materials, where ordering of the gas molecules results in a decrease in ΔS on gas loading 26−28 and implies increasing disorder of the system on SO 2 loading in MFM-520.
We sought to understand the origin of this intriguing pattern in ΔS and have determined the host−guest structures of CO 2and SO 2 -loaded MFM-520 by in situ synchrotron X-ray singlecrystal diffraction (Table S1). On loading CO 2 into MFM-520 at 270 K and 1.0 bar, adsorbed CO 2 molecules are clearly observed in the pores, corresponding to a crystallographic uptake of 2.18 mmol g −1 , in excellent agreement with the isotherm uptake (2.14 mmol g −1 ). All guest CO 2 molecules in MFM-520·CO 2 were found to be incommensurate (Figure 2c).
Thus, instead of showing a constant distance between adjacent CO 2 molecules, the intermolecular distances range from ca. 6.6 to 7.4 Å ( Figure S3), indicating no apparent interaction between adjacent CO 2 molecules. The distances between CO 2 and phenyl rings (C1···pyridyl ring) and between CO 2 and aromatic −CH groups (O3···H1C2−C2) are longer than 3.0 Å (Figure 2c-IV), suggesting only very weak supramolecular interactions between the host framework and CO 2 . Therefore, MFM-520 experiences no change in structure upon CO 2 adsorption, and both the oxidation state of Zn(II) centers [ranging from 1.73(9) to 2.07 (9)] and the geometry of Upon loading of SO 2 into MFM-520 at 270 K and 1.0 bar, a crystallographic uptake of SO 2 of 3.16 mmol g −1 is observed, in excellent agreement with the isotherm uptake (3.38 mmol g −1 ). Since the occupancy of adsorbed SO 2 molecules is 0.359(13) in the refined structural model of MFM-520·SO 2 , half of the closely contacted SO 2 molecules (ca. 1.7 to 1.9 Å) were removed, and the remaining SO 2 molecules have an intermolecular distance of ca. 3.5 Å ( Figure S4), which is shorter than that in MFM-520·CO 2 , suggesting stronger guest−guest interactions between adsorbed SO 2 molecules.
On the other hand, strong MOF−SO 2 binding is indicated by the short distances between SO 2 and aromatic −CH groups (O3···H1C2−C2: ca. 2.33 to 2.75 Å) and between SO 2 and [ZnO 4 N] polyhedra (S1···O2: ca. 2.78 to 3.34 Å) (Figure 2d-IV, Figures S7 and S8). As a result, the structure of MFM-520 is heavily affected by adsorbed SO 2 molecules. The ranges of bond distances Zn−N1, Zn−O1, and Zn−O2 in MFM-520· SO 2 vary from 1.97 to 2.14, 1.92 to 2.73, and 1.75 to 2.19 Å, respectively, much wider than those observed in MFM-520 and MFM-520·CO 2 . The oxidation state of the Zn(II) centers also shows a greater range between 1.79(9) and 2.29(9) (Figure 3c) compared with that in MFM-520 and MFM-520· CO 2 . In MFM-520·SO 2 , the modulation vectors become 0.1407(6)(a* + b*) + 0.5c* and 0.1407(6)(−a* + b*) + 0.5c*, demonstrating a unique incommensurately ordered dynamic equilibrium for SO 2 adsorption. Interestingly, before reaching this equilibrium state, we also identified a transient structure of MFM-520·SO 2 with a corresponding crystallographic SO 2 uptake of 0.532 mmol g −1 that has intermediate modulation vectors of 0.1331(4)(a* + b*) + 0.5c* and 0.1331(4)(−a* + b*) + 0.5c* (Table S1). The change in the incommensurate modulation of MFM-520 induced by the uptake of SO 2 is a dynamic process as a function of diffusion and the settling of SO 2 molecules within the pores of the MOF. This result rationalizes the unusual increase in ΔS on SO 2 loading and confirms that it emanates from a subtle increase in the structural flexibility of meta-rigid MFM-520 upon SO 2 adsorption.
Overall, the incommensurate modulated structure reported here will stimulate a reassessment of a wider range of host− guest systems with unusual adsorption behavior 29,30 and encourage the search for new structural flexibility in other MOFs and porous solids that otherwise may be regarded as entirely rigid.  (denoted  as I, II, III, IV, and V), which are assigned based upon DFT modeling to the stretching (I) and bending (II) modes of the aromatic C−H groups on the pyridyl ring and the symmetric stretching (III) and asymmetric stretching (IV) modes of C− O and the bending (V) mode of C−H groups, respectively. On dosing CO 2 (0−1 bar), peak I shows a blue shift (Δ = 9 cm −1 ) to 3113 cm −1 , indicating a stiffening of the framework as a result of the binding of CO 2 molecules to −CH groups. No notable changes occur in peaks II−V on CO 2 loading, consistent with the very weak MOF−CO 2 interactions. Upon loading SO 2 , a larger blue shift of 12 cm −1 is observed for peak I, accompanied by near-depletion of this band on increasing SO 2 loading, demonstrating a stronger −CH···OSO supramolecular interaction. Furthermore, distinct red shifts of peaks III and IV (C−O, carboxyl) to 1682 and 1566 cm −1 (Δ = 6 and 5 cm −1 , respectively) and peak V (C−H, pyridyl ring) to 1385 cm −1 (Δ = 5 cm −1 ) are observed, entirely consistent with the presence of structural distortion as observed in crystallographic studies and DFT-calculated IR spectra ( Figure  4e). Difference INS spectra recorded (Figure 4f) between bare and CO 2 -, SO 2 -, and D 2 O-loaded MFM-520 reveal shifts of peaks associated with deformation and twisting modes of the pyridyl rings at low frequencies (200−300 cm −1 ) as well as C− H bending modes at higher frequencies (900−1300 cm −1 ), as confirmed by DFT modeling. SO 2 and D 2 O both display notably stronger interactions with MFM-520 than CO 2 , again consistent with the crystallographic studies.
Unlike conventional once-through FGD (flue gas desulfurization) methods where SO 2 permanently binds to sorbent materials to form solid inorganic waste, the SO 2 captured by MFM-520 remains available to undergo chemical transformation to valuable products. 31,32 A proof-of-concept experiment was thus conducted by coupling 4-methoxylaryldiazonium tetrafluoroborates and hydrazine in a solution containing a suspension of MFM-520·SO 2 to synthesize aryl Naminosulfonamides (Scheme 1). 33 A nearly quantitative conversion of 4-methoxyl-aryldiazonium tetrafluoroborates and an 80% yield of the sulfonamide were achieved. Immobilization and then release of SO 2 using a stable MOF can thus be used to drive organic reactions effectively, removing the high risk of the large-scale use of caustic and toxic SO 2 . In line with the observed structural stability of MFM-520, we have confirmed its reusability for three cycles to produce sulfonamide (Table S6). Thus, MFM-520 represents a stable and efficient platform for the capture, storage, and conversion of SO 2 .

■ CONCLUSIONS
The metal−organic framework material MFM-520 exhibits a reversible periodic-to-aperiodic structural transition. The aperiodic crystal structure of MFM-520 has no threedimensional (3D) lattice periodicity but shows translational symmetry in higher-dimensional (3 + 2)D space. Filling of MFM-520 with CO 2 and SO 2 reveals that while CO 2 has a minimal structural influence, SO 2 can further modulate the structure incommensurately. In addition, MFM-520 shows high selectivity for SO 2 under flue gas desulfurization conditions, and the facile release of captured SO 2 from MFM-520 can be used as an SO 2 delivery system for subsequent reactivity.
■ ASSOCIATED CONTENT * sı Supporting Information