Synthesis and Characterization of a Crystalline Imine-Based Covalent Organic Framework with Triazine Node and Biphenyl Linker and Its Fluorinated Derivate for CO2/CH4 Separation

A catalyst-free Schiff base reaction was applied to synthesize two imine-linked covalent organic frameworks (COFs). The condensation reaction of 1,3,5-tris-(4-aminophenyl)triazine (TAPT) with 4,4′-biphenyldicarboxaldehyde led to the structure of HHU-COF-1 (HHU = Heinrich-Heine University). The fluorinated analog HHU-COF-2 was obtained with 2,2′,3,3′,5,5′,6,6′-octafluoro-4,4′-biphenyldicarboxaldehyde. Solid-state NMR, infrared spectroscopy, X-ray photoelectron spectroscopy, and elemental analysis confirmed the successful formation of the two network structures. The crystalline materials are characterized by high Brunauer–Emmett–Teller surface areas of 2352 m2/g for HHU-COF-1 and 1356 m2/g for HHU-COF-2. The products of a larger-scale synthesis were applied to prepare mixed-matrix membranes (MMMs) with the polymer Matrimid. CO2/CH4 permeation tests revealed a moderate increase in CO2 permeability at constant selectivity for HHU-COF-1 as a dispersed phase, whereas application of the fluorinated COF led to a CO2/CH4 selectivity increase from 42 for the pure Matrimid membrane to 51 for 8 wt% of HHU-COF-2 and a permeability increase from 6.8 to 13.0 Barrer for the 24 wt% MMM.


Introduction
Covalent organic frameworks (COFs) are porous crystalline materials built entirely by covalent bonds between light elements. Since the first COFs, namely COF-1 and COF-5, were synthesized in 2005 [1], research on COFs has been rapidly developing. The opportunity to change, for example, the linkers or the linkage leads to a broad variety of two-dimensional (2D) or three-dimensional (3D) structures [2]. The associated tunable material characteristics open up the possibility of applications in various areas such as gas storage [3], molecular separation [4][5][6], catalysis [7], sensing [8], energy storage [9], and optoelectronics [10].
COFs synthesized via a condensation reaction of an aldehyde and an amine represent the class of imine-COFs. The dynamic formation process based on Schiff base chemistry results in crystalline and porous materials with high chemical and thermal stability [11]. In 2009, the first imine-COF (COF-300) was synthesized from tetra-(4-anilyl)methane and terephthalaldehyde (TA), resulting in a crystalline 3D COF with diamond topology. COF-300 exhibited permanent porosity with a Brunauer-Emmett-Teller (BET) surface Scheme 1. Schematic formation of HHU-COF-1 and HHU-COF-2 from TAPT and BPDCA or OF-BPDCA, respectively, indicating the idealized hexagonal ring and network in the HHU-COF products (HHU = Heinrich-Heine University). The given triazine-centroid triazine-centroid (tz-tz) distance along the edges and the edge-edge distances were determined from the most intense (100) reflexes in the powder X-ray diffractograms, assuming a hexagonal unit cell for the honeycomb layer (cf. Figure S16). The given tz-tz distance along the edge is half the tz-tz distance across the ring.

Synthesis of HHU-COF-1
A total of 84.1 mg (0.400 mmol) of BPDCA, 94.5 mg (0.267 mmol) of TAPT, and 1 mL of the solvent mixture of 1,4-dioxane and mesitylene (1:1, v/v) were placed in a glass ampoule, followed by an ultra-sonification treatment for 15 min in order to ensure sufficient mixing of the educts. The mixture was degassed by applying three freeze-pump-thaw cycles, and the ampoule was flame sealed under vacuum. After heating at 120 °C for three days, the crude product was washed with THF, followed by Soxhlet extraction for 24 h each in THF and in ethanol to remove unreacted monomers. Drying was performed with supercritical CO2 (yield: 147 mg; 89.5%). Scheme 1. Schematic formation of HHU-COF-1 and HHU-COF-2 from TAPT and BPDCA or OF-BPDCA, respectively, indicating the idealized hexagonal ring and network in the HHU-COF products (HHU = Heinrich-Heine University). The given triazine-centroid triazine-centroid (tz-tz) distance along the edges and the edge-edge distances were determined from the most intense (100) reflexes in the powder X-ray diffractograms, assuming a hexagonal unit cell for the honeycomb layer (cf. Figure S16). The given tz-tz distance along the edge is half the tz-tz distance across the ring.

Synthesis of HHU-COF-1
A total of 84.1 mg (0.400 mmol) of BPDCA, 94.5 mg (0.267 mmol) of TAPT, and 1 mL of the solvent mixture of 1,4-dioxane and mesitylene (1:1, v/v) were placed in a glass ampoule, followed by an ultra-sonification treatment for 15 min in order to ensure sufficient mixing of the educts. The mixture was degassed by applying three freeze-pump-thaw cycles, and the ampoule was flame sealed under vacuum. After heating at 120 • C for three days, the crude product was washed with THF, followed by Soxhlet extraction for 24 h each in THF and in ethanol to remove unreacted monomers. Drying was performed with supercritical CO 2 (yield: 147 mg; 89.5%).

Preparation of HHU-COF-1/Matrimid and HHU-COF-2/Matrimid MMMs
To ensure that all MMMs are prepared from the same batch, the COF materials obtained from the larger-scale syntheses were applied as filler materials in the MMMs. Characterization of these COFs can be found in Section S3, Supplementary Materials. The HHU-COF-1/Matrimid and HHU-COF-2/Matrimid MMMs were prepared by solution casting with filler loadings of 8, 16, and 24 wt% ( Figures S23 and S24). The filler loading was calculated according to Equation (1): The 8 wt% membranes were prepared as follows: 250 mg of Matrimid (stored at 80 • C) were dissolved in 3 mL of DCM. A total of 22 mg (48 mg for 16 wt% and 79 mg for 24 wt%) of COF were dispersed in 4 mL of DCM. Both polymer and COF were stirred for 24 h. The COF dispersion was ultrasonicated using a Microtip 630-0419 (VCX 750 Sonics) three times for 15 min (amplitude of 20%) with 30 min stirring between the ultra-sonification steps. Afterward, 0.29 mL (0.62 mL for 16 wt% and 1.01 mL for 24 wt%) of the Matrimid solution was added to the COF dispersion, followed by stirring for another 24 h. The same ultra-sonification procedure was repeated, and the remaining Matrimid solution was added to the COF dispersion. After stirring for two hours, the final dispersion was casted into a metal ring placed on a flat and even glass surface. To ensure slow evaporation of DCM, an inverted funnel covered with a paper tissue was placed above the MMM until the DCM was evaporated. The membrane was cut out of the metal ring with a scalpel. The membranes were dried at 150 • C in a vacuum oven (20 mbar) overnight.

Instrumentation and Characterization Methods
Supercritical CO 2 drying was conducted with an EM CPD300 (Leica, Wetzlar, Germany). Ethanol was exchanged for CO 2 with 50 cycles for each product. Solid-state NMR experiments were performed with an AVANCE 600 spectrometer (Bruker, Billerica, MA, USA) under a static field of 14 T. The samples were packed into 2.5 mm zirconia rotors with Vespel top and bottom plugs and spun at 35 kHz under the magic angle (MAS) in a double resonant wide-bore probe at room temperature. Typical acquisition parameters for the 13 C MAS NMR spectra were a repetition period (d1) equal to or higher than 12 s; 9 ms contact time (cross-polarization), and 1-2 µs for the 90 • pulses. During a typical acquisition time of about 10 ms, 1 H was decoupled using the spinal64 sequence. Very long experiments with accumulations between 16 and 64 k scans were performed in order to overcome the low sensitivity observed for those samples. For 19 F solid-state NMR experiments, the sample was spun in a 2.5 mm zirconia rotor with Vespel top and bottom plugs at 35 kHz (MAS). The EASY pulse program [37] was applied, in which two 90 • pulses were irradiated with a little delay in between. By subtracting the FID after each of those pulses, the background signal was canceled. Subsequent processing involved Fourier transformation, phase adjustment, and baseline correction (Bernstein polynomials, fourth-order or higher). Attenuated total reflection infrared spectroscopy (ATR-IR, platinum ATR-QL, diamond) spectra were obtained on a Tensor 37 (Bruker). X-ray photoelectron spectroscopy (XPS) measurements were performed on a VersaProbe II (Ulvac-Phi) with a monochromatic Al X-ray source (1486.6 eV). The C1s signal at 284.8 eV was taken as the reference for the binding energy scale. Analysis of the spectra was carried out with the program CasaXPS. C, H, N-analysis was carried out on a Vario MICRO cube from Elementar Analysentechnik. Scanning electron microscopy (SEM) images were recorded with a JSM-6510LV (Jeol) with a LaB 6 cathode (20 keV). The membrane cross-sections were obtained by freeze-fracturing with liquid nitrogen and coated with gold by a JFC 1200 (Jeol) sputter coater for imaging. Energy-dispersive X-ray spectroscopy (EDX) was carried out using an Xflash silicon drift detector (Bruker). Thermogravimetric analysis (TGA) was performed under a nitrogen atmosphere with a TG 209 F3 Tarsus (Netzsch, Selb, Germany) in a range from 25 to 1000 • C with a heating rate of 5 K/min. An Autosorb-6 (Quantachrome, Boynton Beach, FL, USA) was used to perform the nitrogen sorption measurements. Prior to the measurements, all samples were activated by degassing under vacuum at 120 • C for 8 h. The Brunauer-Emmett-Teller (BET) surface area was calculated from the range of 0.05 to 0.3 p/p 0 of the nitrogen adsorption isotherms. CO 2 and CH 4 sorption isotherms were obtained with an Autosorb iQ MP (Quantachrome). The samples were activated in vacuo (5 × 10 -3 mbar) at 120 • C for 8 h. In order to calculate the ideal adsorbed solution theory (IAST) selectivity for the gas pair CO 2 /CH 4, the sorption isotherms of HHU-COF-1 were fitted with the Langmuir isotherm (LAI) model by applying Equation (2): The isotherms of HHU-COF-2 were fitted with the Toth isotherm model (Equation (3)), where q and K refer to the loading in mmol/g and the affinity constant, respectively. The heterogeneity exponent is expressed as t with the unit 1/bar. After isotherm fitting, the final IAST selectivity was calculated by Equation (4), where x i is the absorbed gas amount in mmol/g and y i is the mole fraction.
Powder X-ray diffraction (PXRD) patterns were obtained from a Miniflex 600 (Rigaku, Tokyo, Japan) using Cu Kα1 radiation with λ = 1.5406 Å (40 kV, 15 mA, 600 W) and a flat silicon low background sample holder in the range of 2 • < 2θ < 50 • . For determination of the (skeletal) density, a He-pycnometer AccuPyc 1330 (Micromeritics) was used. The density applied for calculations was obtained by including the total pore volume from N 2 -sorption as shown in Equation (5): The tensile strength of the pure Matrimid membrane and MMMs was measured using a TAXT.plus texture analyzer (Stable Micro Systems). The force (N) was divided by the product of the thickness and width of the membrane to obtain the tensile strength to break the membrane in MPa. CO 2 /CH 4 mixed-gas separation measurements were carried out with an OSMO inspector (Convergence Industry B.V.) connected to an Agilent 490 Micro GC (Agilent Technologies, Santa Clara, CA, USA) with a fused silica column PoraPLOT Q and a thermal conductivity detector. A diagram of the experimental setup is shown in Figure S25. The membranes were placed in the permeation module and fixed with a Viton O-ring with an inner diameter of 3.6 cm (area: 11.3 cm 2 ) inside the permeation module. A CO 2 /CH 4 feed gas volume ratio of 1:1 was applied, and helium was used as the sweep gas. The transmembrane pressure and the temperature were set to 3 bar and 25 • C, respectively. All measurements were carried out every 30 min until the equilibrium state was reached. The permeability P is expressed in the unit Barrer (1 Barrer = 10 -10 cm 3 (STP) cm cm -2 s −1 cmHg −1 ) and was calculated according to Equation (6): x A describes the molar fraction of the gas A, Q He is the volumetric flow rate of the sweep gas helium, d is the thickness of the membrane (measured at 10 different points) and x He is the molar fraction of the sweep gas. A stands for the area of the membrane (cm 2 ), p 2 for the feed pressure (cmHg), x f A for the molar fraction of the gas A in the feed, and p 1 for the permeate pressure (cmHg). The molar fractions (x) on the permeate and the feed side were used to calculate the selectivity of the two gases (A, B), according to Equation (7):

Characterization of HHU-COF-1 and HHU-COF-2
The Schiff base reaction of 1,3,5-tris-(4-aminophenyl)triazine (TAPT) with either 4,4 -biphenyldicarboxaldehyde (BPDCA) or the corresponding octafluoro derivative OF-BPDCA yielded the two COFs HHU-COF-1 and HHU-COF-2 as yellow and orange powder (Scheme 1, Figure S17). A three-day synthesis was carried out in ampoules to allow for a slow, reversible reaction leading to crystalline products. Both COFs were reproducibly synthesized on the scale of 0.13 to 0.8 mmol of TAPT in a 1:1.5 ratio with (OF-)BPDCA under the same reaction conditions (cf. Supplementary Materials). Yields ranging from 84% to 90% could be reached. 13 C CP MAS NMR spectra confirmed the formation of the imine bond at 158 ppm for HHU-COF-1 and 153 ppm for HHU-COF-2 ( Figure 1). These values agree well with the related TRITER-1 (158 ppm) [14] and SCF-FCOF-1 (152 ppm) [15] for their carbon atoms of the imine bond. Both COFs exhibited a peak at 171 ppm, referring to the carbon atoms of the triazine ring again identical to TRITER-1 [14]. The signals in the range from 120 to 150 ppm can be assigned to the carbon atoms in the benzene rings. For HHU-COF-1, the small peak at 191 ppm can be attributed to some unreacted aldehyde [38]. Because of the extensive purification with Soxhlet extraction, we assume that the aldehyde signal did not originate from unreacted monomers and is instead caused by partially incomplete network formation, that is, defect sites. In the 19 F CP MAS NMR spectrum of HHU-COF-2 ( Figure 2), the two peaks expected from solution NMR of OF-BPDCA at −136 and −144 ppm ( Figure S3) can only be seen as one peak at −141 ppm due to the line broadening in solid-state NMR.  FT-IR spectra ( Figure 3) showed weak bands at 1626 and 1193 cm -1 for HHU-COF-1 and at 1624 and 1211 cm -1 for HHU-COF-2, which could be assigned to the imine bond [12]. N-H stretching bands from the amino groups in TAPT, which typically appear between 3500 and 3300 cm -1 , were no longer visible in the spectra of the two COFs, proving the conversion of the amine groups and, therefore, the consumption of the linker molecule TAPT. The C=O stretching band of BPDCA at 1686 cm -1 can still be detected as a small band in the spectrum of HHU-COF-1 (at 1700 cm -1 ), indicating residual aldehyde, as was already seen in the 13 C NMR spectrum ( Figure 1a). The absence of the C=O stretching band of OF-BPDCA at 1708 cm -1 in the respective COF indicates a complete conversion of the aldehyde groups of the educt in HHU-COF-2. The XPS survey spectra in the range of binding energies from 0 to 1100 eV can be seen in Figure S7. In this overview, C1s peaks and N1s peaks are visible for both COFs, as well as additional peaks in the F1s and F2s region. In the high-resolution C1s XPS spectra  FT-IR spectra ( Figure 3) showed weak bands at 1626 and 1193 cm -1 for HHU-COF-1 and at 1624 and 1211 cm -1 for HHU-COF-2, which could be assigned to the imine bond [12]. N-H stretching bands from the amino groups in TAPT, which typically appear between 3500 and 3300 cm -1 , were no longer visible in the spectra of the two COFs, proving the conversion of the amine groups and, therefore, the consumption of the linker molecule TAPT. The C=O stretching band of BPDCA at 1686 cm -1 can still be detected as a small band in the spectrum of HHU-COF-1 (at 1700 cm -1 ), indicating residual aldehyde, as was already seen in the 13 C NMR spectrum ( Figure 1a). The absence of the C=O stretching band of OF-BPDCA at 1708 cm -1 in the respective COF indicates a complete conversion of the aldehyde groups of the educt in HHU-COF-2. The XPS survey spectra in the range of binding energies from 0 to 1100 eV can be seen in Figure S7. In this overview, C1s peaks and N1s peaks are visible for both COFs, as well as additional peaks in the F1s and F2s region. In the high-resolution C1s XPS spectra FT-IR spectra ( Figure 3) showed weak bands at 1626 and 1193 cm −1 for HHU-COF-1 and at 1624 and 1211 cm −1 for HHU-COF-2, which could be assigned to the imine bond [12]. N-H stretching bands from the amino groups in TAPT, which typically appear between 3500 and 3300 cm −1 , were no longer visible in the spectra of the two COFs, proving the conversion of the amine groups and, therefore, the consumption of the linker molecule TAPT. The C=O stretching band of BPDCA at 1686 cm −1 can still be detected as a small band in the spectrum of HHU-COF-1 (at 1700 cm −1 ), indicating residual aldehyde, as was already seen in the 13 C NMR spectrum ( Figure 1a). The absence of the C=O stretching band of OF-BPDCA at 1708 cm −1 in the respective COF indicates a complete conversion of the aldehyde groups of the educt in HHU-COF-2.  FT-IR spectra ( Figure 3) showed weak bands at 1626 and 1193 cm -1 for HHU-COF-1 and at 1624 and 1211 cm -1 for HHU-COF-2, which could be assigned to the imine bond [12]. N-H stretching bands from the amino groups in TAPT, which typically appear between 3500 and 3300 cm -1 , were no longer visible in the spectra of the two COFs, proving the conversion of the amine groups and, therefore, the consumption of the linker molecule TAPT. The C=O stretching band of BPDCA at 1686 cm -1 can still be detected as a small band in the spectrum of HHU-COF-1 (at 1700 cm -1 ), indicating residual aldehyde, as was already seen in the 13 C NMR spectrum ( Figure 1a). The absence of the C=O stretching band of OF-BPDCA at 1708 cm -1 in the respective COF indicates a complete conversion of the aldehyde groups of the educt in HHU-COF-2. The XPS survey spectra in the range of binding energies from 0 to 1100 eV can be seen in Figure S7. In this overview, C1s peaks and N1s peaks are visible for both COFs, as well as additional peaks in the F1s and F2s region. In the high-resolution C1s XPS spectra The XPS survey spectra in the range of binding energies from 0 to 1100 eV can be seen in Figure S7. In this overview, C1s peaks and N1s peaks are visible for both COFs, as well as additional peaks in the F1s and F2s region. In the high-resolution C1s XPS spectra of HHU-COF-1 ( Figure S8), the peaks at 284.8 and 286.2 eV were assigned to the carboncarbon/carbon-hydrogen bonds and the carbon-nitrogen bonds (C=N-C), respectively [39]. Fitting of the N1s region revealed a peak at 398.8 eV corresponding to the imine bond formed by the Schiff base reaction as well as the carbon-nitrogen bonds in the triazine unit [22,40]. For HHU-COF-2, the corresponding peaks in the C1s region ( Figure S9) were located at 284.6 and 286.1 eV. The additional peak at 287.8 eV refers to the C-F bonds. The nitrogen-carbon bonds are evident in the N1s region, with a peak at again 398.8 eV [39]. The F1s peak was detected at 687.7 eV (Figure S10), and by integrating the peak area, a fluorine content of 19.5 at%, which corresponds to 27.3 wt% within C, N, and F, was determined for HHU-COF-2 (Table S1), which matches well with the calculation of 27.4 wt% from the ideal formula. Hydrogen cannot be detected by XPS, so the H wt% has to remain unaccounted for. Its missing share increases the wt% of C, N, and F.
The CHN elemental analysis of HHU-COF-1 and HHU-COF-2 in Table 1 was in suitable accordance with the calculated theoretical values for both COFs. In agreement with the XPS data (F wt% = 27.3 wt%), the residual content of 26.78 wt% in the CHN elemental analysis for HHU-COF-2 can be mainly attributed to the fluorine content. A uniform distribution of fluorine in HHU-COF-2 was shown with element mapping by SEM-EDX ( Figure 4). SEM images exhibited agglomerated spherical particles with an average size between 2 and 5 µm in diameter for both COFs (Figures 4, S11 and S12). of HHU-COF-1 ( Figure S8), the peaks at 284.8 and 286.2 eV were assigned to the carboncarbon/carbon-hydrogen bonds and the carbon-nitrogen bonds (C=N-C), respectively [39]. Fitting of the N1s region revealed a peak at 398.8 eV corresponding to the imine bond formed by the Schiff base reaction as well as the carbon-nitrogen bonds in the triazine unit [22,40]. For HHU-COF-2, the corresponding peaks in the C1s region ( Figure S9) were located at 284.6 and 286.1 eV. The additional peak at 287.8 eV refers to the C-F bonds. The nitrogen-carbon bonds are evident in the N1s region, with a peak at again 398.8 eV [39]. The F1s peak was detected at 687.7 eV ( Figure S10), and by integrating the peak area, a fluorine content of 19.5 at%, which corresponds to 27.3 wt% within C, N, and F, was determined for HHU-COF-2 (Table S1), which matches well with the calculation of 27.4 wt% from the ideal formula. Hydrogen cannot be detected by XPS, so the H wt% has to remain unaccounted for. Its missing share increases the wt% of C, N, and F. The CHN elemental analysis of HHU-COF-1 and HHU-COF-2 in Table 1 was in suitable accordance with the calculated theoretical values for both COFs. In agreement with the XPS data (F wt% = 27.3 wt%), the residual content of 26.78 wt% in the CHN elemental analysis for HHU-COF-2 can be mainly attributed to the fluorine content. A uniform distribution of fluorine in HHU-COF-2 was shown with element mapping by SEM-EDX ( Figure 4). SEM images exhibited agglomerated spherical particles with an average size between 2 and 5 µm in diameter for both COFs (Figures 4, S11 and S12). The thermal stabilities of the two COFs were investigated by TGA measurements under a nitrogen atmosphere (Figure 5a). The decomposition of HHU-COF-1 started at 450 °C with a maximum weight loss of about 40% up to 800 °C and ~55% at 1000 °C. For HHU-COF-2, gradual decomposition started at the lower temperature of ~180 °C and rather steadily continued up to 1000 °C, amounting to a weight loss of 70%. In the related TRITER-1 and SCF-FCOF-1, decomposition started at 480 and 430 °C, respectively ( Figure  S32). The thermal stabilities of the two COFs were investigated by TGA measurements under a nitrogen atmosphere (Figure 5a). The decomposition of HHU-COF-1 started at 450 • C with a maximum weight loss of about 40% up to 800 • C and~55% at 1000 • C. For HHU-COF-2, gradual decomposition started at the lower temperature of~180 • C and rather steadily continued up to 1000 • C, amounting to a weight loss of 70%. In the related TRITER-1 and SCF-FCOF-1, decomposition started at 480 and 430 • C, respectively ( Figure S32).  Figure S15.
N2-sorption ( Figure 6a) showed type IV(a) isotherms for both COFs, which turn into a type II or III isotherm at higher relative pressure. The type IV isotherm with a narrow H1 hysteresis loop reflects the micro-mesoporous nature of the COFs. The type II or III isotherm with an H4 hysteresis reflects the condensation of N2 in the macroporous interparticle voids from the aggregation of the COF particles [41]. HHU-COF-1 and HHU-COF-2 exhibited high BET surface areas of 2352 m 2 /g (p/p0 = 0.18-0.28) and 1356 m 2 /g (p/p0 = 0.15-0.25), respectively. The total pore volumes (at p/p0 = 0.97) of HHU-COF-1 and its fluorinated analog were determined as 0.78 and 0.73 cm 3 /g, respectively. We note that the trend in surface area was reversed for the TA analogs SCF-HCOF-1 (SBET = 318 m 2 /g, no Vpore given) and SCF-FCOF-1 (SBET = 1602-2056 m 2 /g, 5 h to 3 d synthesis time, Vpore = 1.69 cm 3 /g) [15]. However, the data for SCF-HCOF-1 cannot be taken as representative since the product was obtained in only 45% yield (96% for SCF-FCOF-1) and was noted to be of poor crystallinity, possibly due to the low activity of the TA under the solvothermal catalyst-free (SCF) synthesis conditions [15]. Under a 12 h reflux synthesis in DMF, the SCF-HCOF-1-identical TRITER-1 (cf. Scheme S1) showed a BET surface area of 716 m 2 /g [14]. In this respect, it is remarkable that BPDCA and its octafluoro-congener exhibit no differences in reactivity and yield. Concerning the high porosity of the SCF-FCOF-1 products with the triazine ring node, it is peculiar that the SCF-FCOF-2 analog with the benzene node (cf. Scheme S1) has only a BET surface area of 1245 m 2 /g and a pore volume of 0.64 cm 3 /g. We also synthesized the SCF-HCOF-1 (TRITER-1) and SCF-FCOF-1 with the smaller linkers TA and TFTA (Scheme S1, Figure S34). The synthesis and analytical results can be found in Section S5, Supplementary Materials. From our synthesis it was possible to obtain BET surface areas for SCF-HCOF-1 of 977 m 2 /g (Vpore = 0.64 cm 3 /g) and for SCF-  (110) and (200) planes, respectively [15], the peaks for the HHU-COFs were shifted to lower 2θ values due to the larger linker molecule. If one assumes a honeycomb (hcb) lattice with almost eclipsed stacked layers, the three measured peaks and corresponding (100), (110), and (200) planes can be matched to the edge-edge distance of the hexagonal rings (Scheme 1, Figure S16). Notably, a diffraction peak at about 25 • -26 • 2θ for the (001) plane from the interlayer π-π stacking is not seen. N 2 -sorption ( Figure 6a) showed type IV(a) isotherms for both COFs, which turn into a type II or III isotherm at higher relative pressure. The type IV isotherm with a narrow H1 hysteresis loop reflects the micro-mesoporous nature of the COFs. The type II or III isotherm with an H4 hysteresis reflects the condensation of N 2 in the macroporous interparticle voids from the aggregation of the COF particles [41]. HHU-COF-1 and HHU-COF-2 exhibited high BET surface areas of 2352 m 2 /g (p/p 0 = 0.18-0.28) and 1356 m 2 /g (p/p 0 = 0.15-0.25), respectively. The total pore volumes (at p/p 0 = 0.97) of HHU-COF-1 and its fluorinated analog were determined as 0.78 and 0.73 cm 3 /g, respectively. We note that the trend in surface area was reversed for the TA analogs SCF-HCOF-1 (S BET = 318 m 2 /g, no V pore given) and SCF-FCOF-1 (S BET = 1602-2056 m 2 /g, 5 h to 3 d synthesis time, V pore = 1.69 cm 3 /g) [15]. However, the data for SCF-HCOF-1 cannot be taken as representative since the product was obtained in only 45% yield (96% for SCF-FCOF-1) and was noted to be of poor crystallinity, possibly due to the low activity of the TA under the solvothermal catalyst-free (SCF) synthesis conditions [15]. Under a 12 h reflux synthesis in DMF, the SCF-HCOF-1-identical TRITER-1 (cf. Scheme S1) showed a BET surface area of 716 m 2 /g [14]. In this respect, it is remarkable that BPDCA and its octafluoro-congener exhibit no differences in reactivity and yield. Concerning the high porosity of the SCF-FCOF-1 products with the triazine ring node, it is peculiar that the SCF-FCOF-2 analog with the benzene node (cf. Scheme S1) has only a BET surface area of 1245 m 2 /g and a pore volume of 0.64 cm 3 /g. We also synthesized the SCF-HCOF-1 (TRITER-1) and SCF-FCOF-1 with the smaller linkers TA and TFTA (Scheme S1, Figure S34). The synthesis and analytical results can be found in Section S5, Supplementary Materials. From our synthesis it was possible to obtain BET surface areas for SCF-HCOF-1 of 977 m 2 /g (V pore = 0.64 cm 3 /g) and for SCF-FCOF-1 of 2276 m 2 /g (V pore = 1.46 cm 3 /g). Although it was possible to generate SCF-HCOF-1 with a larger surface area, the reversed trend in surface area is still evident for the HHU-COFs with the larger linkers. This was also observed with the larger-scale products (Section S3, Supplementary Materials), where HHU-COF-1 (larger scale) exhibited the larger BET surface area of 2351 m 2 /g (V pore = 0.69 cm 3 /g) compared to HHU-COF-2 (larger scale) with 1346 m 2 /g (V pore = 0.68 cm 3 /g). A similar trend to the HHU-COFs was observed for CTFs, which were ionothermally trimerized from 4,4 -biphenyldicarbonitrile and its octafluoro derivative. The BET surface area of the fluorinated CTF was about 35% lower compared to the non-fluorinated compound [23]. tion S3, Supplementary Materials), where HHU-COF-1 (larger scale) exhibited the larger BET surface area of 2351 m 2 /g (Vpore = 0.69 cm 3 /g) compared to HHU-COF-2 (larger scale) with 1346 m 2 /g (Vpore = 0.68 cm 3 /g). A similar trend to the HHU-COFs was observed for CTFs, which were ionothermally trimerized from 4,4′-biphenyldicarbonitrile and its octafluoro derivative. The BET surface area of the fluorinated CTF was about 35% lower compared to the non-fluorinated compound [23].
Pore size distributions for HHU-COF-1 and HHU-COF-2 were calculated by applying the carbon slit-pore, non-local density functional theory (NLDFT) equilibrium model and revealed maxima at 13, 17, and 25 Å for HHU-COF-1 (Figure 6b). The maxima for HHU-COF-2 were located at 13, 16, and 24 Å. In the region of the larger ~25 Å pores, a lower incremental volume was found for HHU-COF-2, which is consistent with the presence of fluorine atoms. The diameters of the hexagonal rings in the idealized hcb lattice are estimated from Scheme 1 to 37-39 Å by taking into account the aryl ring radii, C-H and C-F bond lengths, and the vdW radii of the surface H and F atoms (1.2 and 1.35 Å, respectively). In addition, CO2 and CH4 sorption studies were performed at a temperature of 273 K ( Figure S13). HHU-COF-2 exhibited a higher CO2 uptake than the non-fluorinated HHU-COF-1, as would be expected for fluorinated materials, which are generally associated with a CO2-philic character [42]. HHU-COF-1 and HHU-COF-2 showed maximum CO2 uptakes of 1.08 and 1.74 mmol/g, respectively, which can be considered moderate compared with other imine-COFs (Table S3). The CH4 adsorption capacities were found to be 0.52 and 0.66 mmol/g for HHU-COF-1 and HHU-COF-2, respectively. The adsorption isotherms at 273 K were further applied to calculate the IAST selectivity for the gas pair CO2/CH4. Therefore, the isotherms of HHU-COF-1 were fitted with the Langmuir (LAI) isotherm model and the isotherms of HHU-COF-2 with the Toth model (Table S4). The CO2/CH4 selectivity ( Figure S14) for a binary (50:50; v:v) mixture of the gases at 1 bar pressure was 2.1 for HHU-COF-1 and 2.6 for HHU-COF-2, respectively.

Characterization of MMMs
In order to investigate the distribution of the dispersed phase in the Matrimid matrices, cross-section SEM images (Figure 7) were acquired. No major defects that could lead to a reduction in selectivity were observed in any of the MMMs. However, with the increasing filler content of HHU-COF-1, more minor defects became visible. This was especially the case for the 24 wt% MMM, where slight sedimentation was observed as well. Pore size distributions for HHU-COF-1 and HHU-COF-2 were calculated by applying the carbon slit-pore, non-local density functional theory (NLDFT) equilibrium model and revealed maxima at 13, 17, and 25 Å for HHU-COF-1 (Figure 6b). The maxima for HHU-COF-2 were located at 13, 16, and 24 Å. In the region of the larger~25 Å pores, a lower incremental volume was found for HHU-COF-2, which is consistent with the presence of fluorine atoms. The diameters of the hexagonal rings in the idealized hcb lattice are estimated from Scheme 1 to 37-39 Å by taking into account the aryl ring radii, C-H and C-F bond lengths, and the vdW radii of the surface H and F atoms (1.2 and 1.35 Å, respectively).
In addition, CO 2 and CH 4 sorption studies were performed at a temperature of 273 K ( Figure S13). HHU-COF-2 exhibited a higher CO 2 uptake than the non-fluorinated HHU-COF-1, as would be expected for fluorinated materials, which are generally associated with a CO 2 -philic character [42]. HHU-COF-1 and HHU-COF-2 showed maximum CO 2 uptakes of 1.08 and 1.74 mmol/g, respectively, which can be considered moderate compared with other imine-COFs (Table S3). The CH 4 adsorption capacities were found to be 0.52 and 0.66 mmol/g for HHU-COF-1 and HHU-COF-2, respectively. The adsorption isotherms at 273 K were further applied to calculate the IAST selectivity for the gas pair CO 2 /CH 4 . Therefore, the isotherms of HHU-COF-1 were fitted with the Langmuir (LAI) isotherm model and the isotherms of HHU-COF-2 with the Toth model (Table S4). The CO 2 /CH 4 selectivity ( Figure S14) for a binary (50:50; v:v) mixture of the gases at 1 bar pressure was 2.1 for HHU-COF-1 and 2.6 for HHU-COF-2, respectively.

Characterization of MMMs
In order to investigate the distribution of the dispersed phase in the Matrimid matrices, cross-section SEM images (Figure 7) were acquired. No major defects that could lead to a reduction in selectivity were observed in any of the MMMs. However, with the increasing filler content of HHU-COF-1, more minor defects became visible. This was especially the case for the 24 wt% MMM, where slight sedimentation was observed as well. For all MMMs with HHU-COF-2 as filler, a uniform distribution of the filler particles and a defect-free appearance could be confirmed. These observations suggest a better dispersion of the fluorinated COF with the Matrimid matrix, which agrees with the gas separation performance.
For all MMMs with HHU-COF-2 as filler, a uniform distribution of the filler particles and a defect-free appearance could be confirmed. These observations suggest a better dispersion of the fluorinated COF with the Matrimid matrix, which agrees with the gas separation performance. In addition, SEM images were taken of the top surface of the MMMs ( Figure S26). As expected, more particles are visible on the surface at higher loadings, so that complete sedimentation of the COF particles can be excluded. The distribution of the filler HHU-COF-2 in the MMMs was investigated by fluorine element mapping using SEM-EDX (Figure S27). Due to the inaccuracy of EDX measurements for elements lighter than fluorine, these results should be considered critically. However, it can be seen that the COF particles are present throughout the whole membrane cross-sections.
The mechanical stability of the MMMs was investigated by determining the tensile strength. The maximum applied force until fracture of the respective MMM is summarized in Table S7. As expected, the pure Matrimid membrane exhibits the highest tensile strength of 91 MPa. For the MMMs with 8 and 16 wt% filler, values between 74 and 79 MPa were obtained. High loading of 24 wt% COF resulted in a reduction in the mechanical stability to below 60 MPa.

Gas Permeability and Selectivity
The membrane performance of the two systems, HHU-COF-1/Matrimid and HHU-COF-2/Matrimid (Table 2; Figure 8), was investigated with respect to CO2/CH4 separation. The pure membranes and the membranes with 8, 16, and 24 wt% filler content were prepared in duplicate. Final permeability P was calculated with the thickness of the membranes given in Table S6. The CO2 permeability of the 8 and 16 wt% HHU-COF-1/Matrimid MMMs increased to 9.1 Barrer compared to the neat polymer membrane with 6.8 Barrer. This was accompanied by a moderate CO2/CH4 selectivity increase from 42 to 46. However, this increase from 6.8 to 9.1 Barrer is not very significant when compared with other porous organic framework MMMs (vide infra). With an increase in the filler content to 24 wt%, the permeability and selectivity decreased again to the approximate value of the neat Matrimid membrane, in line with the sedimentation noted from SEM. The HHU-COF-2-based MMMs showed a continuous enhancement in CO2 permeability upon increasing the filler content from 8 to 24 wt%. The CO2/CH4 selectivity was raised from 42 for neat Matrimid to 51 for the 8 wt% MMM. For the 16 and 24 wt% MMMs, the selectivity was back at the level of the pure polymer. The lower membrane efficiency of the HHU- In addition, SEM images were taken of the top surface of the MMMs ( Figure S26). As expected, more particles are visible on the surface at higher loadings, so that complete sedimentation of the COF particles can be excluded. The distribution of the filler HHU-COF-2 in the MMMs was investigated by fluorine element mapping using SEM-EDX ( Figure S27). Due to the inaccuracy of EDX measurements for elements lighter than fluorine, these results should be considered critically. However, it can be seen that the COF particles are present throughout the whole membrane cross-sections.
The mechanical stability of the MMMs was investigated by determining the tensile strength. The maximum applied force until fracture of the respective MMM is summarized in Table S7. As expected, the pure Matrimid membrane exhibits the highest tensile strength of 91 MPa. For the MMMs with 8 and 16 wt% filler, values between 74 and 79 MPa were obtained. High loading of 24 wt% COF resulted in a reduction in the mechanical stability to below 60 MPa.

Gas Permeability and Selectivity
The membrane performance of the two systems, HHU-COF-1/Matrimid and HHU-COF-2/Matrimid (Table 2; Figure 8), was investigated with respect to CO 2 /CH 4 separation. The pure membranes and the membranes with 8, 16, and 24 wt% filler content were prepared in duplicate. Final permeability P was calculated with the thickness of the membranes given in Table S6. The CO 2 permeability of the 8 and 16 wt% HHU-COF-1/Matrimid MMMs increased to 9.1 Barrer compared to the neat polymer membrane with 6.8 Barrer. This was accompanied by a moderate CO 2 /CH 4 selectivity increase from 42 to 46. However, this increase from 6.8 to 9.1 Barrer is not very significant when compared with other porous organic framework MMMs (vide infra). With an increase in the filler content to 24 wt%, the permeability and selectivity decreased again to the approximate value of the neat Matrimid membrane, in line with the sedimentation noted from SEM. The HHU-COF-2-based MMMs showed a continuous enhancement in CO 2 permeability upon increasing the filler content from 8 to 24 wt%. The CO 2 /CH 4 selectivity was raised from 42 for neat Matrimid to 51 for the 8 wt% MMM. For the 16 and 24 wt% MMMs, the selectivity was back at the level of the pure polymer. The lower membrane efficiency of the HHU-COF-1-based membranes in comparison to HHU-COF-2 as filler material could be related to the blocking of the pores by (inter)penetrating polymer chains as well as the aggregation of the filler particles. A lower filler content of HHU-COF-1 seems to be recommended to achieve the optimum membrane performance for this system. For HHU-COF-2 as a dispersed phase, the known trade-off relationship between (high/low) permeability and (low/high) selectivity is seen as in the Robeson plots [43,44]. It was possible to consistently increase permeability with increasing filler content, which at the same time led to a decrease in selectivity. Overall, the fluorinated material showed better compatibility with the Matrimid matrix and led to a better separation performance for the gas pair CO 2 /CH 4 . Table 2. Gas permeabilities (P) and mixed-gas selectivity factors (α) of the pristine Matrimid membrane and COF/Matrimid MMMs 1 . 13.0 ± 1.0 0.32 ± 0.02 40 ± 1 1 The errors for the permeability (P) and for the selectivity (α) were taken from the range of two to three measurements and include the upper and lower value.

Filler Material
COF-1-based membranes in comparison to HHU-COF-2 as filler material could be related to the blocking of the pores by (inter)penetrating polymer chains as well as the aggregation of the filler particles. A lower filler content of HHU-COF-1 seems to be recommended to achieve the optimum membrane performance for this system. For HHU-COF-2 as a dispersed phase, the known trade-off relationship between (high/low) permeability and (low/high) selectivity is seen as in the Robeson plots [43,44]. It was possible to consistently increase permeability with increasing filler content, which at the same time led to a decrease in selectivity. Overall, the fluorinated material showed better compatibility with the Matrimid matrix and led to a better separation performance for the gas pair CO2/CH4. 13.0 ± 1.0 0.32 ± 0.02 40 ± 1 For a better understanding and classification of the permeation results, the fractional free volume (FFV) was calculated, and a comparison with permeability models was drawn. For the density (1.20 g/cm 3 ) [45] and the FFV (0.167) [46] of Matrimid, the values reported in the literature were applied. The FFV of HHU-COF-1 and HHU-COF-2 was obtained by multiplying pore volume and density (from Equation (5)) and was calculated to be 0.558 and 0.560, respectively. The FFV of a MMM is the sum of the FFV of the polymer multiplied by the volume fraction of the continuous phase and the FFV of the filler material multiplied by the volume fraction of the dispersed phase , as given in Equation (8): The FFV does not contain the interface (void) volume. The logarithm of the CO2 and CH4 permeability versus 1/FFV for 0 to 24 wt% HHU-COF-1 and HHU-COF-2 as dispersed phases in Matrimid MMMs is plotted in Figure 9. Relating the free volume to the CO2 and CH4 permeability, HHU-COF-1 shows only a small increase up to a content of 16 For a better understanding and classification of the permeation results, the fractional free volume (FFV) was calculated, and a comparison with permeability models was drawn. For the density (1.20 g/cm 3 ) [45] and the FFV (0.167) [46] of Matrimid, the values reported in the literature were applied. The FFV of HHU-COF-1 and HHU-COF-2 was obtained by multiplying pore volume and density (from Equation (5)) and was calculated to be 0.558 and 0.560, respectively. The FFV of a MMM is the sum of the FFV of the polymer multiplied by the volume fraction of the continuous phase φ c and the FFV of the filler material multiplied by the volume fraction of the dispersed phase φ d , as given in Equation (8): The FFV does not contain the interface (void) volume. The logarithm of the CO 2 and CH 4 permeability versus 1/FFV for 0 to 24 wt% HHU-COF-1 and HHU-COF-2 as dispersed phases in Matrimid MMMs is plotted in Figure 9. Relating the free volume to the CO 2 and CH 4 permeability, HHU-COF-1 shows only a small increase up to a content of 16 wt%. For HHU-COF-1/Matrimid, the permeability of the 24 wt% MMM corresponds to the neat polymer (within experimental error) ( Table 2). In turn, the actually available FFV of the 24 wt% MMM would only be that of the neat polymer. Thus, the theoretically calculated free volume from the filler is not available for permeation due to its aggregation and blocking or filling of the filler pores by polymer chains, as becomes clear when the FFV is put in relation to the permeability. For HHU-COF-2, lgP increases as 1/FFV decreases (i.e., when the amount of filler is increased) as expected. This is relatively more pronounced at high filler contents since the FFV of the filler material (0.560) is higher than that of the polymer (0.167).
wt%. For HHU-COF-1/Matrimid, the permeability of the 24 wt% MMM corresponds to the neat polymer (within experimental error) ( Table 2). In turn, the actually available FFV of the 24 wt% MMM would only be that of the neat polymer. Thus, the theoretically calculated free volume from the filler is not available for permeation due to its aggregation and blocking or filling of the filler pores by polymer chains, as becomes clear when the FFV is put in relation to the permeability. For HHU-COF-2, lgP increases as 1/FFV decreases (i.e., when the amount of filler is increased) as expected. This is relatively more pronounced at high filler contents since the FFV of the filler material (0.560) is higher than that of the polymer (0.167). To better assess the filler volume-dependent CO2 permeability increase, a comparison with the Maxwell model was carried out [47]. At first, it should be noted that this model describes an ideal particle distribution of the filler in the polymer. It also assumes spherical particles with a volume fraction of the dispersed filler phase up to 0.2. The simplified Maxwell model for the case that the permeability of the dispersed phase, Pd, is much higher than the permeability of the pure continuous (polymer) phase, Pc, is shown in Equation (9), where Peff stands for the permeability of the MMMs: In addition, three further modified models were used, which assume Pd = 8Pc, Pd = 4Pc, and Pd = 2Pc. Models that are applicable to higher [48,49] also show much higher values for Peff /Pc as a function of and are not applicable for a comparison in this case. Figure 10 plots the ratio Peff /Pc of the gas CO2 versus for the filler materials HHU-COF-1 and HHU-COF-2 in the polymer Matrimid in comparison to the Maxwell model and the modified models. The higher volume fractions of HHU-COF-1 over HHU-COF-2 are due to the lower density of the HHU-COF-1 for equivalent mass percentages. For the HHU-COF-1 MMMs, a low filler efficiency is confirmed with respect to CO2 permeability.
Only the 8 wt% MMM shows an increase in permeability, which agrees with the Maxwell model for Pd = 8Pc. The 16 wt% HHU-COF-1 MMM already exceeds the filler volume fraction of 0.2, for which the Maxwell model is applicable. As the filler content of HHU-COF-2 increases, the Peff /Pc ratio increases significantly higher. The 8 wt% MMM agrees with the model prediction for Pd = 2Pc and the 16 wt% MMM with Pd = 8Pc. The 24 wt% MMM represents the most efficient membrane in terms of CO2 permeability. With a Peff /Pc ratio of 1.9, it exceeds the Maxwell model for Pd = 8Pc. To better assess the filler volume-dependent CO 2 permeability increase, a comparison with the Maxwell model was carried out [47]. At first, it should be noted that this model describes an ideal particle distribution of the filler in the polymer. It also assumes spherical particles with a volume fraction of the dispersed filler phase φ d up to 0.2. The simplified Maxwell model for the case that the permeability of the dispersed phase, P d, is much higher than the permeability of the pure continuous (polymer) phase, P c, is shown in Equation (9), where P eff stands for the permeability of the MMMs: In addition, three further modified models were used, which assume P d = 8P c , P d = 4P c, and P d = 2P c. Models that are applicable to higher φ d [48,49] also show much higher values for P eff /P c as a function of φ d and are not applicable for a comparison in this case. Figure 10 plots the ratio P eff /P c of the gas CO 2 versus φ d for the filler materials HHU-COF-1 and HHU-COF-2 in the polymer Matrimid in comparison to the Maxwell model and the modified models. The higher volume fractions of HHU-COF-1 over HHU-COF-2 are due to the lower density of the HHU-COF-1 for equivalent mass percentages. For the HHU-COF-1 MMMs, a low filler efficiency is confirmed with respect to CO 2 permeability. Only the 8 wt% MMM shows an increase in permeability, which agrees with the Maxwell model for P d = 8P c . The 16 wt% HHU-COF-1 MMM already exceeds the filler volume fraction of 0.2, for which the Maxwell model is applicable. As the filler content of HHU-COF-2 increases, the P eff /P c ratio increases significantly higher. The 8 wt% MMM agrees with the model prediction for P d = 2P c and the 16 wt% MMM with P d = 8P c . The 24 wt% MMM represents the most efficient membrane in terms of CO 2 permeability. With a P eff /P c ratio of 1.9, it exceeds the Maxwell model for P d = 8P c .
A comparison with literature values of Matrimid-based MMMs for CO 2 /CH 4 separation shows that the performance of the 8 wt% HHU-COF-1 MMM with a CO 2 permeability of 9.1 Barrer agrees with comparable systems, such as ACOF-1 [31] or CTF-fluorene [50] in Matrimid. The system with 8 wt% of the azine-linked structure ACOF-1 in Matrimid achieved a CO 2 permeability value of 9.6 Barrer, and the corresponding weight percentage of CTF-fluorene in Matrimid increased the CO 2 permeability to 9.2 Barrer. The application of 8 wt% of a biphenyl-based CTF with a larger pore volume resulted in a value of 12.0 Barrer [36]. At this point, it is once again confirmed that increasing the pore size is only beneficial up to a certain level. A comparison with different filler materials in matrices such as 6FDA-DAM [51], Pebax [52], and PIM-1 [32,53] can be found in Table S9. In contrast, the higher filler amounts of HHU-COF-2 showed a much larger increase in CO 2 permeability.
Compared to the pure Matrimid membrane, the CO 2 permeability for the 24 wt% MMM was increased by 91% to 13.0 Barrer. A comparison with literature values of Matrimid-based MMMs for CO2/CH4 separation shows that the performance of the 8 wt% HHU-COF-1 MMM with a CO2 permeability of 9.1 Barrer agrees with comparable systems, such as ACOF-1 [31] or CTF-fluorene [50] in Matrimid. The system with 8 wt% of the azine-linked structure ACOF-1 in Matrimid achieved a CO2 permeability value of 9.6 Barrer, and the corresponding weight percentage of CTF-fluorene in Matrimid increased the CO2 permeability to 9.2 Barrer. The application of 8 wt% of a biphenyl-based CTF with a larger pore volume resulted in a value of 12.0 Barrer [36]. At this point, it is once again confirmed that increasing the pore size is only beneficial up to a certain level. A comparison with different filler materials in matrices such as 6FDA-DAM [51], Pebax [52], and PIM-1 [32,53] can be found in Table S9. In contrast, the higher filler amounts of HHU-COF-2 showed a much larger increase in CO2 permeability. Compared to the pure Matrimid membrane, the CO2 permeability for the 24 wt% MMM was increased by 91% to 13.0 Barrer.
To test the long-term stability of the MMMs, we performed permeability measurements again after one year (Table S8). All 12 MMMs were covered but stored without further protection at an average temperature of 20 °C in ambient air. The 8 and 16 wt% HHU-COF-1/MMMs showed reduced CO2 permeability with values of 8.6 and 8.0 Barrer, respectively. The 24 wt% MMM proved to be stable in terms of CO2 permeability, but the CO2/CH4 selectivity was reduced to 28, so the MMM can be considered defective. The HHU-COF-2 MMMs not only showed the best results in terms of initial membrane performance but also exhibited consistent CO2 permeability after one year of storage. CO2 permeability of 7.1 (8 wt%), 10.5 (16 wt%), and 12.9 Barrer (24 wt%) was measured with CO2/CH4 selectivity between 44 and 45 after this one year.
In summary, from the permeability and FFV values, it is evident that the high theoretical filler FFV does not contribute to a significant increase in permeability. Evidently, the pore openings in HHU-COF-1 and HHU-COF-2 are too large (cf. Scheme 1) so that they allow for (inter)penetration of polymer chains that then drastically decrease this fractional free volume contribution from the filler. The higher increase in permeability for HHU-COF-2 over HHU-COF-1 for the 16 and 24 wt% MMMs indicates that HHU-COF-2 with the fluorinated linker has a higher filler contribution. This is explained by a hindrance of the (inter)penetration of the non-fluorinated polymer chains into the fluorous HHU-COF-2 inner pores, akin to fluorous chemistry with the lower affinity or even separation of perfluorinated compounds from non-fluorinated phases. To test the long-term stability of the MMMs, we performed permeability measurements again after one year (Table S8). All 12 MMMs were covered but stored without further protection at an average temperature of 20 • C in ambient air. The 8 and 16 wt% HHU-COF-1/MMMs showed reduced CO 2 permeability with values of 8.6 and 8.0 Barrer, respectively. The 24 wt% MMM proved to be stable in terms of CO 2 permeability, but the CO 2 /CH 4 selectivity was reduced to 28, so the MMM can be considered defective. The HHU-COF-2 MMMs not only showed the best results in terms of initial membrane performance but also exhibited consistent CO 2 permeability after one year of storage. CO 2 permeability of 7.1 (8 wt%), 10.5 (16 wt%), and 12.9 Barrer (24 wt%) was measured with CO 2 /CH 4 selectivity between 44 and 45 after this one year.
In summary, from the permeability and FFV values, it is evident that the high theoretical filler FFV does not contribute to a significant increase in permeability. Evidently, the pore openings in HHU-COF-1 and HHU-COF-2 are too large (cf. Scheme 1) so that they allow for (inter)penetration of polymer chains that then drastically decrease this fractional free volume contribution from the filler. The higher increase in permeability for HHU-COF-2 over HHU-COF-1 for the 16 and 24 wt% MMMs indicates that HHU-COF-2 with the fluorinated linker has a higher filler contribution. This is explained by a hindrance of the (inter)penetration of the non-fluorinated polymer chains into the fluorous HHU-COF-2 inner pores, akin to fluorous chemistry with the lower affinity or even separation of perfluorinated compounds from non-fluorinated phases.

Conclusions
Two imine-linked COFs were synthesized via a Schiff base reaction applying 1,3,5-tris-(4-aminophenyl)triazine as an amine compound. 4,4 -biphenyldicarboxaldehyde and the corresponding octafluoro derivative were chosen as linkers to form HHU-COF-1 and HHU-COF-2. The successful formation of the materials was confirmed by 13 C and 19 F CP MAS NMR, IR, XPS, and elemental analysis. Both materials are crystalline, and the synthesis with the biphenyl-based linkers led to high BET surface areas of 2352 m 2 /g for HHU-COF-1 and 1356 m 2 /g for HHU-COF-2. Moreover, both syntheses were successfully carried out on a larger scale in order to apply the products as filler materials in Matrimid-based MMMs for CO 2 /CH 4 separation, where the fluorinated COF led to the better membrane performance with a CO 2 permeability increase from 6.8 to 13.0 Barrer for the 24 wt% MMM.

Institutional Review Board Statement: Not applicable.
Informed Consent Statement: Not applicable.

Data Availability Statement:
The data presented in this study are available on request from the corresponding author.