Sr(II) and Ba(II) Alkaline Earth Metal–Organic Frameworks (AE-MOFs) for Selective Gas Adsorption, Energy Storage, and Environmental Application

Two new alkaline earth metal–organic frameworks (AE-MOFs) containing Sr(II) (UPJS-15) or Ba(II) (UPJS-16) cations and extended tetrahedral linker (MTA) were synthesized and characterized in detail (UPJS stands for University of Pavol Jozef Safarik). Single-crystal X-ray analysis (SC-XRD) revealed that the materials are isostructural and, in their frameworks, one-dimensional channels are present with the size of ~11 × 10 Å2. The activation process of the compounds was studied by the combination of in situ heating infrared spectroscopy (IR), thermal analysis (TA) and in situ high-energy powder X-ray diffraction (HE-PXRD), which confirmed the stability of compounds after desolvation. The prepared compounds were investigated as adsorbents of different gases (Ar, N2, CO2, and H2). Nitrogen and argon adsorption measurements showed that UPJS-15 has SBET area of 1321 m2 g−1 (Ar) / 1250 m2 g−1 (N2), and UPJS-16 does not adsorb mentioned gases. From the environmental application, the materials were studied as CO2 adsorbents, and both compounds adsorb CO2 with a maximum capacity of 22.4 wt.% @ 0 °C; 14.7 wt.% @ 20 °C and 101 kPa for UPJS-15 and 11.5 wt.% @ 0°C; 8.4 wt.% @ 20 °C and 101 kPa for UPJS-16. According to IAST calculations, UPJS-16 shows high selectivity (50 for CO2/N2 10:90 mixture and 455 for CO2/N2 50:50 mixture) and can be applied as CO2 adsorbent from the atmosphere even at low pressures. The increased affinity of materials for CO2 was also studied by DFT modelling, which revealed that the primary adsorption sites are coordinatively unsaturated sites on metal ions, azo bonds, and phenyl rings within the MTA linker. Regarding energy storage, the materials were studied as hydrogen adsorbents, but the materials showed low H2 adsorption properties: 0.19 wt.% for UPJS-15 and 0.04 wt.% for UPJS-16 @ −196 °C and 101 kPa. The enhanced CO2/H2 selectivity could be used to scavenge carbon dioxide from hydrogen in WGS and DSR reactions. The second method of applying samples in the area of energy storage was the use of UPJS-15 as an additive in a lithium-sulfur battery. Cyclic performance at a cycling rate of 0.2 C showed an initial discharge capacity of 337 mAh g−1, which decreased smoothly to 235 mAh g−1 after 100 charge/discharge cycles.


UPJS-
were purchased from eMolecules, Acros Organics and Sigma-Aldrich companies, and used without further purification. H 4 MTA, as an organic part of MOFs, was synthesized by multi-step organic reactions according to the published literature procedure [70].

Used Chemicals
All the chemicals used in the preparation of methanetetrayltetrakis(benzene-4,1diyl)tetrakis(aza))tetrakis(methan-1-yl-1-yliden)tetrabenzoic acid, H4MTA (see Figure  1), UPJS-15, and UPJS-16 were purchased from eMolecules, Acros Organics and Sigma-Aldrich companies, and used without further purification. H4MTA, as an organic part of MOFs, was synthesized by multi-step organic reactions according to the published literature procedure [70]. Orange needle-shaped crystals of the compounds were prepared by hydrothermal synthesis. A mixture of Sr(NO3)2·4H2O (18.5 mg, 0.088 mmol) or Ba(NO3)2 (22.9 mg, 0.088 mmol) and H4MTA (10 mg, 0.011 mmol) and 6 mL of DMF was sealed into a 23 mL glass vial. After the complete dissolution of the reactants, 2 mL of water was slowly added dropwise to the reaction mixture. The vessels were heated to 80 °C at a heating rate of 10 °C min −1 , held at this temperature for 96 h, and then cooled to ambient temperature. The obtained crystals of materials were filtered, washed several times with DMF, acetone, and dried in the air stream. The yield of assynthesized samples was 11.3 mg for UPJS-15 (AS) and 10.6 mg for UPJS-16 (AS), corresponding to 73% and 69%, respectively, based on H4MTA.  and 6 mL of DMF was sealed into a 23 mL glass vial. After the complete dissolution of the reactants, 2 mL of water was slowly added dropwise to the reaction mixture. The vessels were heated to 80 • C at a heating rate of 10 • C min −1 , held at this temperature for 96 h, and then cooled to ambient temperature. The obtained crystals of materials were filtered, washed several times with DMF, acetone, and dried in the air stream. The yield of as-synthesized samples was 11.3 mg for UPJS-15 (AS) and 10.6 mg for UPJS-16 (AS), corresponding to 73% and 69%, respectively, based on H 4

Solvent Exchange Process and Activation of the Compounds
To prepare the materials for gas adsorption measurements, an ethanol exchange process to replace the solvents located in the pores of materials (DMF, H 2 O) was performed. The compounds were prepared by soaking the as-synthesized material in a 98% ethanol solution for two weeks. Then, the suspension was decanted each 24 h. The ethanolexchanged materials prepared by the above-described procedure were designed as UPJS-15 (EX = EXchanged) and UPJS-16 (EX) in the following text. Before the gas adsorption measurements, the solvent-exchanged samples were outgassed in a vacuum at 120 • C for Nanomaterials 2023, 13, 234 5 of 30 16 h to eliminate solvents from the channel system. The materials were heated gradually at a heating rate of 3 • C min −1 with an isothermal step at 60 • C with a soaking time of half hour. Activated materials were designed as UPJS-15 (AC: ACtivated) and UPJS-16 (AC) in the further text.

Preparation of S-MOF-Based Electrode Material
All chemicals used to prepare electrode slurry and electrolytes were purchased from Timcal or Sigma-Aldrich companies.
Synthesized and activated metal-organic framework UPJS-15 (AC) was applied as a carrier for sulphur in Li-S batteries. UPJS-15 (AC), sulphur, and carbon Super P were milled by wet ball milling in ethanol at 500 rpm for 30 min using a zirconium oxide grinding jar. The electrode tar was synthesized by combining sulphur, UPJS-15 (AC), Super P, and poly (vinylidene) difluoride (PVDF) in N-methyl-2-pyrrolidone (NMP), and the final mass ratio of electrode components was 60:15:15:10. The cathode slurry was overlayed on aluminium foil using carbon modification on the surface by a coating bar and subsequently dried in the oven at 60 • C for one day. Electrode disks with a diameter of 18 mm were compressed with a pressure of 350 kg cm −2 and then dried under a vacuum at 60 • C inside a glove box. The sulphur loading in the cathode material was controlled at around 2.8 mg cm −2 .

Cell Assembly
The Li-S cells were constructed in a glove box filled with high-purity argon (Jacomex) to El-Cell ® by using a Li metal foil as an anode, S/UPJS-15 as a cathode, and a glass fibre-based separator. The electrolyte was in a composition of 0.7 M solution of lithium bis(tri-fluoromethanesulfonyl) imide (LiTFSI) and 0.25 M solution of LiNO 3 in 1,3-dioxolane (DOL) and 1,2-dimethoxyethane (DME) with the volume ratio of 1:2.

Elemental and ICP-MS Analyses
Elemental analysis (EA) was carried out using a CHNOS Elemental Analyzer Vario MICRO from Elementar Analysensysteme GmbH with~5 mg mass.
Inductively coupled plasma-mass spectrometry (ICP-MS) analysis was applied to determine the strontium (II) and barium (II) quantity in the as-synthesized compounds. Prior to the measurement, the materials were mineralized in a warm aqua regia.

Infrared Spectroscopy
The infrared spectra of the materials were performed at room temperature and recorded on an Avatar FTIR 6700 apparatus in the wavenumber range of 4000-400 cm −1 with 64 repetitions for one spectrum and a resolution of 4 cm −1 using the KBr pellets. Samples were assembled in the form of KBr discs with a weight ratio (sample: KBr/1: 100). Before infrared measurements, potassium bromide was heated at 600 • C for 16 h and further cooled in a desiccator. Diffuse reflectance infrared Fourier transform (DRIFT) measurements were carried out using the same device equipped with a DTGS detector in the wavenumber region of 4000-500 cm −1 . Each given spectrum averages 200 measurements, while the resolution is 4 cm −1 . The Praying Mantis in situ heating cell under vacuum was used for the measurements, and as a reference background, the pure KBr was used.

Thermal Analysis
The thermal properties of as-synthesized, solvent-exchanged, and activated materials were investigated by thermogravimetric analysis (TA) using platinum crucibles and a sample weight of~25 mg. TA measurements were carried out on a TGA Q500 apparatus. The materials were heated in a dynamic atmosphere of air with a flow rate of 60 cm 3 min −1 . The samples were measured in the temperature range of 25-800 • C with a heating rate of 10 • C min −1 . In situ heating high-energy powder X-ray diffraction (HE-PXRD) measurements were performed at the P02.1 beamline of the PETRA III storage ring in Deutsches Elektronen Synchrotron (DESY, Hamburg, Germany). The beam size during experiments was set to 0.6 × 0.6 mm 2 , and the radiation wavelength was λ = 0.20727 Å. The samples were added in a glass capillary with a wall thickness of 20 µm and a diameter of 1.2 mm. Diffracted photons from the samples were recorded using a Perkin Elmer PEI1621 2D detector. Sample to detector distance (1526 mm) and detector tilt to beam axis were calibrated and calculated using a diffraction pattern from LaB 6 as standard reference material. The compounds were heated in the temperature range of 30-700 • C with a heating rate of 5 • C min −1 , while the diffraction data were recorded every 50 • C. The 2D diffraction patterns obtained were integrated using the Fit2D program [71].
Powder X-ray diffraction (PXRD) measurements were performed in the reflection geometry using a Rigaku Ultima IV multipurpose diffractometer. To obtain a parallel and pure X-ray beam for PXRD measurements, the initially divergent Cu/Kα radiation (λ = 1.54056 Å) emitted from the X-ray lamp was further guided through a multilayer mirror and a set of slits. PXRD experiments were conducted by 2θ continuous scans from 5 • to 60 • with a measurement speed of 0.5 • min −1 , and a NaI scintillation detector was used for the recording of diffracted photons.

Scanning Electron Microscopy and Energy-Dispersive X-ray Spectroscopy
The morphology of the materials for electrochemical measurements was studied on a TESCAN VEGA3 equipped with an EDAX analyser using energy-dispersive X-ray spectroscopy (EDS) and scanning electron microscopy (SEM).

Single-Crystal X-ray Structure Measurements and Determination
The single-crystal X-ray diffraction (SC-XRD) data set was collected on a Nonius Kappa CCD diffractometer equipped with a Bruker APEX II detector. For UPJS-15 (AS) and UPJS-16 (AS) Cu/Kα (λ = 1.54178 Å) @ −153(2) • C, and data reduction was conducted using the diffractometer software. The phase problem was solved by direct methods and refined with full-matrix least-squares on F 2 using the Shelxl-2018 program suite [72]. All atoms, excluding hydrogen atoms, were refined anisotropically. Aromatic hydrogen atoms were included in an ideal position, with U iso (H) assigned to 1.2U eq of the adjacent carbon atom and the C−H bond fixed to 0.95 Å. Guest molecules located in the cavities of the materials were subtracted by the SQUEEZE procedure in Platon [73]. The structure images were visualized using DIAMOND software [74]. Crystal data for UPJS-15 (AS) and UPJS-16 (AS) are listed in Table S1 in Supplementary Materials and selected bond lengths and angles in Tables S2 and S3 in Supplementary Materials. The crystal structures of UPJS-15 (AS) and UPJS-16 (AS) under the registration numbers 2117419 and 2117420, respectively, were deposited in the Cambridge Crystallographic Data Centre (CCDC) and can be retrieved free of charge from https://www.ccdc.cam.ac.uk/structures (accessed on 4.1.2023). The topological analysis of the frameworks was performed using ToposPro software [75,76].
Nitrogen (99.999% purity) adsorption experiments were measured on an ASAP 2020 Micromeritics apparatus @ −196 • C, and argon (99.999%) adsorption measurements @ −186 • C on a Quantachrome AUTOSORB-1-MP automated gas sorption system. Based on the nitrogen and argon adsorption/desorption measurements, the BET specific surface area (S BET ) of each sample was calculated by adsorption data in a p/p 0 range from 0.03 to 0.15. DFT method was used for the calculation of the pore size diameter (d) and pore volume (V p ). CO 2 adsorption isotherms (99.999% purity) @ 0 • C and 20 • C were carried out using a Quantachrome AUTOSORB-iQ-C with a combined dynamic and volumetric sorption system. The CO 2 isotherms were performed in the range of 0.5-101 kPa of abs. pressure.
The H 2 (99.999% purity) adsorption measurements were performed on the Autosorb iQ-XR static manometric adsorption system developed by Quantachrome Instruments. The hydrogen adsorption isotherms were collected @ −196 • C in the range of 0.5-101 kPa of absolute pressure.

DFT Modelling and Computational Studies
Theoretical studies were based on density functional theory (DFT) computations using Gaussian16, Revision C.01 [77]. All computations utilized the B3LYP functional [78][79][80], the Stuttgart/Dresden ECP [81] for the Sr atoms, and the 6-311+G(3d,p) basis set for all other atoms. The correction for empirical dispersion was included as Grimme's dispersion using the D3 damping function [82].
MTA linker: The geometry of MTA molecule was first fully optimized by imposing the S 4 point group for this anionic species. Since the optimization could only utilize C 2 symmetry as the largest Abelian subgroup of S 4 , the density matrix was symmetrized before each SCF cycle to match the molecular symmetry. The geometry optimization procedure used a Hessian estimated prior the first optimization step and was updated at each step during the course of optimization. The three MTA-CO 2 models were obtained by performing partial optimizations on models, which included the optimized geometry of a frozen MTA linker, while complete optimization was allowed for the auxiliary CO 2 molecules placed into three different starting positions. After obtaining appropriate stationary points on the potential hypersurfaces, the total interaction energies between MTA linker and the CO 2 molecules were obtained from counterpoise computations. These counterpoise computations subdivided models into two fragments-MTA linker and CO 2 ; their interaction energy was then obtained as the difference of the full-system total energy and the sum of the total energies of the two fragments using the full-system basis set for both fragments.
Sr(II) cluster: The geometry optimization of the Sr(II) cluster was initially attempted too, but due to termination effects, the structure motif underwent major alterations upon optimization and got into a significant disagreement with the experimental motif (mostly in the orientation of the organic residues). These undesired geometry changes could not be fully prevented even upon freezing some redundant coordinates (typically involving the positions of the Sr atoms) during the optimization. The geometry of cluster was further used as obtained from the diffraction experiment and by replacing its diazo groups for hydrogen atoms with the C-H interatomic distances fixed at 0.95 Å and attempting no geometry optimization. The interaction energy between Sr(II) cluster and three CO 2 molecules was obtained by conducting a partial optimization for cluster-CO 2 that included the cluster part frozen, while the three CO 2 molecules were fully free to optimize. After reaching an appropriate stationary point, the interaction energy between the cluster and the CO 2 molecules was obtained by a counterpoise computation on the optimized model, where the supersystem was divided into two fragments-he cluster (first fragment) and the three CO 2 molecules (second fragment).

Electrochemical Characterization
The electrochemical measurements were carried out using a VMP3 potentiostat (Biologic). Electrochemical characterization was studied by galvanostatic cycling (GC) and cycling voltammetry (CV). CV was carried out within the potential window from 1.8 to 3.0 V vs Li/Li+ at a scan rate of 0.1 mV s −1 . GC measurement was realized with the potential range of 1.8-2.8 V vs Li/Li+. The capacities obtained from cycling at 0.2 C were related to the weight of sulphur.

Results and Discussion
Tetrahedral tetraazo-tetracarboxylic acid (H 4 MTA) was produced by the multistep organic synthesis based on the described procedure [70]. A solvothermal reaction between H 4 (UPJS-16 (AS)) suitable for SC-XRD analysis and further characterization. These formulae were proposed based on the SC-XRD measurements, elemental and ICP-MS analyses, thermogravimetric analysis (TG), and infrared spectroscopy (IR). Thermal stability and activation condition of the compounds were studied by the combination of in situ heating HE-PXRD, in situ heating DRIFT, and TG. The activated compounds were further investigated as gas sorbents for argon, nitrogen, carbon dioxide and hydrogen, and as an additive in Li-S batteries.

Description of Crystal Structures
A single-crystal structure determination reveals that UPJS-15 (AS) (see Figure 2) and UPJS-16 (AS) are isostructural and crystallize in the tetragonal space group I-42d, containing four formula units, and the cell lengths a = 32.3789(8); 31.6708(9) Å, c = 7.3286(2); 7.7689(2) Å, respectively. Detailed information about the crystal structure refinements is listed in Table S1 in Supplementary Materials. Based on the crystallographic review of the CCDC database, it can be stated that the tetragonal system is preferred for compounds containing tetrahedral carboxylate ligands [83]. The asymmetric unit of the compounds contains one quarter of the MTA linker, one water molecule, and one alkaline earth metal ion. All carboxylic groups of H 4 MTA linker are deprotonated and bonded to the central atoms in chelate-anti mode. One MTA ion coordinates to eight alkaline earth central atoms, as can be seen from Figure 2c. The tetrahedral MTA linker lost its C 3 rotational axes by distorting the angles of its two shoulders from the ideal 109 • 28 to 111.9 • . Additionally, phenyl rings that are connected by an azo bond display a dihedral angle of 5.3 • , which disrupts ligand rigidity. Based on the above facts, the linker symmetry was reduced from tetrahedral (T d ) to D 2d , resulting in the tetragonal space group of the compounds. The M-O bond distances have typical lengths between 2.499(4) and 2.621(4) Å for Sr-O and 2.676(9)-2.842(11) Å for Ba-O. Selected bond distances and angles in the crystal structure of compounds are summarized in Table S2 for UPJS-15 (AS) and Table S3 for UPJS-16 (AS) in Supplementary Materials. One coordinated water molecule completed the coordination sphere of each central atom, which makes a bridge between two alkaline metal ions. According to the described coordination of ligands, the donor set of each central ion is [MO 8 ], and the coordination polyhedron can be expressed as a distorted tetragonal antiprism (see Figure 2a). By bridging the carboxylate and aqua ligands, the central atoms are arranged in 1D linear chains propagating along the c crystallographic axis (see Figure 2b). The distances between M···M within the polymeric chains are 3.805 Å and 4.119 Å for Sr(II) and Ba(II), respectively. The crystal structures of UPJS-15 (AS) and UPJS-16 (AS) can be described as 3D polymeric frameworks, which exhibit [6,8-c] network topology according to ToposPro analysis [75,76]. In the frameworks, a 1D channel system along the c crystallographic axis is present, and the sizes of channel apertures are 11.19 × 10.10 Å 2 for UPJS-15 (AS) and 10.69 × 9.70 Å 2 for UPJS-16 (AS) (see Figure 2d). The total accessible volume in desolvated UPJS-15 (AS) and UPJS-16 (AS), after removal of guest solvents using squeeze procedure, was calculated using the Platon/Void procedure [73] to be 3673.6 Å 3 and 3103.5 Å 3 , representing 47.8% and 39.8%, respectively.

Characterization, Thermal Stability and Activation Study
The thermal stability and activation of the prepared compounds were initially studied by thermal analysis in an air atmosphere in the [30-800 • C] temperature range; the measured TG curves are shown in Figure 3. The desolvation process of as-synthesized compounds UPJS-15 (AS) and UPJS-16 (AS) (see black and red curves in Figure 3 Subsequently, the desolvated compounds are thermally stable up to 360 • C, and, as seen by the plateau on TG curves, further heating of the materials leads to their thermal decomposition. Successful activation of the compounds is evident from the obtained TG curves of UPJS-15 (AC) and UPJS-16 (AC) (see wine and grey curves in Figure 3) because no significant weight loss is observed up to 400 • C.

Characterization, Thermal Stability and Activation Study
The thermal stability and activation of the prepared compounds were initially studied by thermal analysis in an air atmosphere in the [30-800 °C] temperature range; the measured TG curves are shown in Figure 3. The desolvation process of as-synthesized compounds UPJS-15 (AS) and UPJS-16 (AS) (see black and red curves in Figure 3 Figure S1 in Supplementary Materials), the resulting thermal decomposition products are SrCO3 and BaCO3 [84,85]. The experimental residual masses correlate well with calculated values (exp. 20.12 wt.%, clcd. 20.90 wt.% for SrCO3; exp. 26.23 wt.%, clcd. 26.10 wt.% for BaCO3). In ethanol-exchanged samples, the solvent molecules are released at lower temperatures compared to as-synthesized materials. The desolvation of UPJS-15 (EX) and UPJS-16 (EX) (see green and orange curves in Figure 3) occurs in the temperature range of [30-150 °C]. Subsequently, the desolvated compounds are thermally stable up to 360 °C, and, as seen by the plateau on TG curves, further heating of the materials leads to their thermal decomposition. Successful activation of the compounds is evident from the obtained TG curves of UPJS-15 (AC) and UPJS-16 (AC) (see wine and grey curves in Figure 3) because no significant weight loss is observed up to 400 °C. Infrared spectroscopy was applied to confirm the presence of building blocks and solvents (MTA, DMF, and water) in the materials and also to monitor the solvent exchange and activation processes. The IR spectra of compounds are shown in Figure 4, and the assignment of characteristic absorption bands to the bond type vibrations is summarized in Table 1. The isostructurality of the materials is also shown in infrared spectroscopy by the similarity of obtained IR spectra (see Figure 4). The presence of coordinated and crystallization water molecules in as-synthesized UPJS-15 (AS) and UPJS-16 (AS) materials is Infrared spectroscopy was applied to confirm the presence of building blocks and solvents (MTA, DMF, and water) in the materials and also to monitor the solvent exchange and activation processes. The IR spectra of compounds are shown in Figure 4, and the assignment of characteristic absorption bands to the bond type vibrations is summarized in Table 1. The isostructurality of the materials is also shown in infrared spectroscopy by the similarity of obtained IR spectra (see Figure 4). The presence of coordinated and crystallization water molecules in as-synthesized UPJS-15 (AS) and UPJS-16 (AS) materials is evident from the broad absorption band about 3400 cm −1 , which could be attributed to the stretching ν(OH) vibrations. DMF molecules located in the cavities are evidenced by the stretching vibration of aliphatic ν(CH) vibration in the region 3050-3060 cm −1 and the strong and sharp absorption band of carbonyl groups (ν(C=O)) in the range of 1640-1650 cm −1 for both compounds. The unambiguous presence of the mentioned solvents was confirmed by comparing the IR spectra of water and N,N -dimethylformamide with the synthesized compounds (see Figure 4). The MTA linker in the compound s frameworks is evident from the presence of several characteristic absorption bands: aromatic stretching vibrations ν(CH) ar , ν(C=C) ar and carboxylate symmetric and antisymmetric stretching (ν(COO − ) s , ν(COO − ) as ), as well as deformation vibrations (δ(COO -)) (see Figure 4 and Table 1). The successful ethanol exchange process in the IR spectra of UPJS-15 (EX) and UPJS-16 (EX) was confirmed by the absence of the ν(C=O) band, which is characteristic for DMF, and also by the presence of three new aliphatic CH vibrations in the interval 2966-2844 cm −1 . All absorption bands typical for MTA were observed in the samples after the solvent exchange process. Figure 4 also shows the IR spectra of activated compounds (AC), which confirm the successful removal of solvents after the activation process due to the absence of characteristic absorption bands for solvents, ethanol, and water (see Table 1). evident from the broad absorption band about 3400 cm −1 , which could be attributed to the stretching ν(OH) vibrations. DMF molecules located in the cavities are evidenced by the stretching vibration of aliphatic ν(CH) vibration in the region 3050-3060 cm −1 and the strong and sharp absorption band of carbonyl groups (ν(C=O)) in the range of 1640-1650 cm −1 for both compounds. The unambiguous presence of the mentioned solvents was confirmed by comparing the IR spectra of water and N,N′-dimethylformamide with the synthesized compounds (see Figure 4). The MTA linker in the compound´s frameworks is evident from the presence of several characteristic absorption bands: aromatic stretching vibrations ν(CH)ar, ν(C=C)ar and carboxylate symmetric and antisymmetric stretching (ν(COO − )s, ν(COO − )as), as well as deformation vibrations (δ(COO -)) (see Figure 4 and Table  1). The successful ethanol exchange process in the IR spectra of UPJS-15 (EX) and UPJS-16 (EX) was confirmed by the absence of the ν(C=O) band, which is characteristic for DMF, and also by the presence of three new aliphatic CH vibrations in the interval 2966-2844 cm −1 . All absorption bands typical for MTA were observed in the samples after the solvent exchange process. Figure 4 also shows the IR spectra of activated compounds (AC), which confirm the successful removal of solvents after the activation process due to the absence of characteristic absorption bands for solvents, ethanol, and water (see Table 1).    The activation process of ethanol-exchanged samples was also investigated by in situ heating infrared spectroscopy (DRIFT) under a vacuum from ambient temperature up to 350 • C (see Figure 5). A broad band dip around 3400 cm −1 was observed, corresponding to the O-H stretching vibrations (ν(OH)) of crystallization ethanol and coordinated water molecules from the pore system. Moreover, a decreased intensity of the absorption bands under 3000 cm −1 to 2800 cm −1 was observed that corresponds to the stretching vibrations of aliphatic C-H groups (ν(CH) aliph ) of the aliphatic system of ethanol. Otherwise, the other bands in the spectrum were without changes, confirming the thermal stability of porous materials during the degassing process under a vacuum. The results of the described study are important, especially in the process of material desolvation that occurs during the activation of materials during adsorption measurements.
High-energy powder X-ray diffraction (HE-PXRD) measurements at DESY (Hamburg, Germany) were performed to investigate the framework stability/lability of solventexchanged materials during in situ heating. Figure 6 shows comparisons of measured diffraction patterns with calculated patterns of the compounds from the results of singlecrystal X-ray diffraction analysis (SC-XRD) (see insets in Figure 6a,b) and results of in situ heating HE-PXRD measurements in the temperature range of 30-700 • C with 50 • C steps (see Figure 6a,b). As can be seen from the comparison in insets of Figure 6, the measured and calculated diffraction patterns of the materials are in good agreement, representing the phase purity of the bulks and the stability of the compounds during the solvent exchange process. From the results of in situ HE-PXRD measurements (see Figure 6a,b), it can be stated that the materials show a similar, moderate thermal stability, which is in good agreement with the conclusions of TG experiments (see text above). The compounds are stable in the temperature range of 30-350 • C due to the presence of characteristic diffraction peaks for the compounds without the presence of a phase change. According to Kitagawa s MOF classification, materials UPJS-15 and UPJS-16 should be included in the second generation, with stable and robust frameworks without the presence of guest molecules in the channels [86]. Above 350 • C in the temperature range of 400-500 • C, the framework's collapse is associated with the thermal decomposition of the MTA linker, as only an amorphous phase is present, and no clearly defined diffraction peaks are present in the patterns. In the temperature range of 550-700 • C, the formation of new diffraction peaks can be observed, which correspond to the creation of carbonates of the respective metals as the final decomposition products (see Figure S1 in Supplementary Materials). High-energy powder X-ray diffraction (HE-PXRD) measurements at DESY (Ham burg, Germany) were performed to investigate the framework stability/lability of solven exchanged materials during in situ heating. Figure 6 shows comparisons of measured di fraction patterns with calculated patterns of the compounds from the results of singl crystal X-ray diffraction analysis (SC-XRD) (see insets in Figure 6a,b) and results of in sit heating HE-PXRD measurements in the temperature range of 30-700 °C with 50 °C step (see Figure 6a,b). As can be seen from the comparison in insets of Figure 6, the measure and calculated diffraction patterns of the materials are in good agreement, representin the phase purity of the bulks and the stability of the compounds during the solvent ex change process. From the results of in situ HE-PXRD measurements (see Figure 6a,b), can be stated that the materials show a similar, moderate thermal stability, which is i good agreement with the conclusions of TG experiments (see text above). The compound are stable in the temperature range of 30-350 °C due to the presence of characteristic di fraction peaks for the compounds without the presence of a phase change. According t Kitagawa´s MOF classification, materials UPJS-15 and UPJS-16 should be included in th second generation, with stable and robust frameworks without the presence of guest mo ecules in the channels [86]. Above 350 °C in the temperature range of 400-500 °C, th

Gas Adsorption and DFT Modelling/Calculation
To investigate the porosity, storage capacity, and textural properties of prepared materials, argon (@ −186 • C) and nitrogen (@ −196 • C) adsorption/desorption experiments on ethanol-exchanged samples were performed. Subsequently, adsorption measurements of hydrogen (@ −196 • C) and carbon dioxide at two different temperatures (@ 0 • C and @ 20 • C) were realized. The samples were degassed under a vacuum at 120 • C for 16 h to remove solvents from the channel system. All adsorption measurements were carried out on the same batch of the material, and obtained results from gas adsorption experiments are described below. in the patterns. In the temperature range of 550-700 °C, the formation of new diffraction peaks can be observed, which correspond to the creation of carbonates of the respective metals as the final decomposition products (see Figure S1 in Supplementary Materials).

Gas Adsorption and DFT Modelling/Calculation
To investigate the porosity, storage capacity, and textural properties of prepared materials, argon (@ −186 °C) and nitrogen (@ −196 °C) adsorption/desorption experiments on ethanol-exchanged samples were performed. Subsequently, adsorption measurements of hydrogen (@ −196 °C) and carbon dioxide at two different temperatures (@ 0 °C and @ 20 °C) were realized. The samples were degassed under a vacuum at 120 °C for 16 h to remove solvents from the channel system. All adsorption measurements were carried out on the same batch of the material, and obtained results from gas adsorption experiments are described below.
The textural properties, such as SBET area, pore volume, and pore size, were investigated by nitrogen and argon adsorption experiments @ −196 °C and −186 °C, respectively. The textural properties, such as S BET area, pore volume, and pore size, were investigated by nitrogen and argon adsorption experiments @ −196 • C and −186 • C, respectively. Obtained adsorption isotherms are depicted in Figure 7, and calculated textural parameters are summarized in Table 2. The adsorption isotherms for UPJS-15 (AC) (see Figure 7) can be described as type Ia by IUPAC classification [87], which is typical for samples with narrow micropores. BET areas (S BET ) of the activated sample UPJS-15 (AC) were calculated according to the adsorption data in the p/p 0 range from 0.03 to 0.15. The DFT method was used for the calculation of the pore volume (Vp) and pore size (d). Evaluation of data from nitrogen and argon adsorption analysis of UPJS-15 (AC) using the BET equation gave a value of the specific surface area of 1250 m 2 g −1 from the N 2 adsorption isotherm and 1321 m 2 g −1 from the Ar adsorption isotherm. The micropore volume (V p ) and the average pore size diameter (d) of the sample were calculated as 0.83 cm 3 g −1 and 1.76 nm from nitrogen adsorption and 0.85 cm 3 g −1 and 1.82 nm from argon adsorption, respectively.
The increased values of carbon dioxide storage capacities in the described compounds can be explained by the presence of: 1. Coordinatively unsaturated sites (CUS)-one CUS per each central atom in the 1D linear chain within the framework (see description of crystal structure (Section 3.1) above).
2. MTA linker-the presence of an azo group (-N=N-) and phenyl rings. According to previous DFT results performed on system, trans-azobenzene-carbon dioxide showed When comparing the CO 2 capacities of MOF compounds containing ligands with T d symmetry (see Table 2) and UPJS-15 (AC) material, it could be stated that the obtained results exceed many compounds regardless of the linker size used. Furthermore, it should be noted that UPJS-15 (AC) has the highest CO 2 storage capacity of the mentioned compounds under the same experimental conditions (temperature and pressure). A value of 22.4 wt.% @ 0 • C and 101 kPa is comparable to the 2-aminoterephthalate linker containing compound CUI-1 (24.1 wt.% CO 2 ) [104] or SNU-5 (24.1 wt.% CO 2 ) [105] and SNU-21 (24.1 wt.% CO 2 ) [106], which can be included among the top unmodified MOF CO 2 adsorbents. The increased values of carbon dioxide storage capacities in the described compounds can be explained by the presence of: 1. Coordinatively unsaturated sites (CUS)-one CUS per each central atom in the 1D linear chain within the framework (see description of crystal structure (Section 3.1) above).
2. MTA linker-the presence of an azo group (-N=N-) and phenyl rings. According to previous DFT results performed on system, trans-azobenzene-carbon dioxide showed [107] that CO 2 molecules preferentially interact with the lone electron pair of the azo group (17.0 kJ mol −1 , 4 × -N=N-groups per one MTA), and also favourable interactions are with the π-electron system of aromatic rings with maximal stabilization energy of 14.4 kJ mol −1 (12 × phenyl rings per one MTA linker).
3. Pore volume and size effect-3673.6 Å 3 (47.8%) for UPJS-15 (AC) and 3103.5 Å 3 (39.8%) for UPJS-16 (AC) of accessible volume according to SC-XRD (see Section 3.1), which are sufficient to provide attractive ion-dipole, dipole-dipole and van der Waals interactions. DFT calculation is a powerful method used to explain the increased affinity of gas molecules to the porous frameworks in MOF materials, similar to the previous study focused on the adsorption of small gas molecules in Fe-based MOFs [108]. The increased CO 2 storage capacity of UPJS-15 (AC) led us to investigate the active sites and affinities of carbon dioxide using DFT modelling, the results of which are depicted in Figures 10 and 11. The proposed active sites mentioned above were studied first. As can be seen from Figure 10a, phenyl rings and azo bonds are potential sites of possible interaction with CO 2 molecules within the MTA linker, as they show considerable electronegativity. Therefore, they are able to interact with a carbon atom in CO 2 that has a partially positive charge (δ + ). Based on previous studies, it is known that CUSs also serve as active sites for the adsorption of various molecules [32]. Therefore, the electron density isosurface of the Sr(II) cluster was studied, which in addition to possible interactions with phenyl rings, revealed electropositive sites in the cluster that are represented by free orbitals created by the elimination of coordinated water molecules in the material activation process. CUSs are able to interact with carbon dioxide through oxygen atoms that have a partially negative charge (δ − ) within the CO 2 molecule.
[107] that CO2 molecules preferentially interact with the lone electron pair of the azo group (17.0 kJ mol −1 , 4 × -N=N-groups per one MTA), and also favourable interactions are with the π-electron system of aromatic rings with maximal stabilization energy of 14.4 kJ mol −1 (12 × phenyl rings per one MTA linker).
DFT calculation is a powerful method used to explain the increased affinity of gas molecules to the porous frameworks in MOF materials, similar to the previous study focused on the adsorption of small gas molecules in Fe-based MOFs [108]. The increased CO2 storage capacity of UPJS-15 (AC) led us to investigate the active sites and affinities of carbon dioxide using DFT modelling, the results of which are depicted in Figures 10 and  11. The proposed active sites mentioned above were studied first. As can be seen from Figure 10a, phenyl rings and azo bonds are potential sites of possible interaction with CO2 molecules within the MTA linker, as they show considerable electronegativity. Therefore, they are able to interact with a carbon atom in CO2 that has a partially positive charge (δ + ). Based on previous studies, it is known that CUSs also serve as active sites for the adsorption of various molecules [32]. Therefore, the electron density isosurface of the Sr(II) cluster was studied, which in addition to possible interactions with phenyl rings, revealed electropositive sites in the cluster that are represented by free orbitals created by the elimination of coordinated water molecules in the material activation process. CUSs are able to interact with carbon dioxide through oxygen atoms that have a partially negative charge (δ − ) within the CO2 molecule.  Using DFT calculations, the degree of CO 2 interactions with the detected active sites were determined using counterpoint calculations, and obtained results are shown in Figure 11. CO 2 with CUSs within the Sr(II) cluster shows the highest adsorption enthalpy with a value of ∆H = −60.81 kJ mol −1 for each carbon dioxide molecule. The calculated positions of CO 2 molecules in the cluster in different views are shown in Figure 11a. Within the MTA linker (see Figure 11b), several possible active sites were detected, and the calculated enthalpy values can be arranged as follows: the lowest value of ∆H = −7.80 kJ mol −1 (mode A) was identified when the oxygen atom (δ -) of CO 2 interacted with the hydrogen atom of the CH group (δ − ), followed by the interactions of the phenyl ring (δ − , mode B) and the azo bond (δ − , mode C) with a carbon atom of CO 2 (δ − ), whose values are approximately the same, ∆H = 19.32 kJ mol −1 and ∆H = 19.05 kJ mol −1 , respectively.  Figure 11a. Within the MTA linker (see Figure 11b), several possible active sites were detected, and the calculated enthalpy values can be arranged as follows: the lowest value of ΔH = −7.80 kJ mol −1 (mode A) was identified when the oxygen atom (δ -) of CO2 interacted with the hydrogen atom of the CH group (δ − ), followed by the interactions of the phenyl ring (δ − , mode B) and the azo bond (δ − , mode C) with a carbon atom of CO2 (δ − ), whose values are approximately the same, ΔH = 19.32 kJ mol −1 and ΔH = 19.05 kJ mol −1 , respectively.
As experimental results, confirmed by DFT calculations, evidence interesting results regarding CO2 adsorption, we decided to perform ideal adsorbed solution theory (IAST) calculations and comparisons with other porous materials. The selectivity of CO2 over N2 was calculated by IAST in the pressure range of 5-100 kPa. The adsorption selectivities for 50:50 and 10:90 CO2/N2 mixtures were calculated using the pure component isotherm fits, described by: ⁄ Figure 11. Molecular modelling of CO 2 interaction with (a) strontium (II) cluster (representing CUSs) and (b) MTA linker using DFT calculation with corresponding adsorption enthalpies (mode A represents CO 2 ··· π interaction, mode B is CO 2 ··· H-C interaction within phenyl ring and mode C represents CO 2 ··· -N=N-interaction of azo group).
As experimental results, confirmed by DFT calculations, evidence interesting results regarding CO 2 adsorption, we decided to perform ideal adsorbed solution theory (IAST) calculations and comparisons with other porous materials. The selectivity of CO 2 over N 2 was calculated by IAST in the pressure range of 5-100 kPa. The adsorption selectivities for 50:50 and 10:90 CO 2 /N 2 mixtures were calculated using the pure component isotherm fits, described by: where S CO2/N2 is the selectivity of CO 2 in a binary mixture with N 2 , x, and y denoting the equilibrium mole fraction for CO 2 in the adsorbed phase and gas phase, respectively [109,110]. The prediction of adsorption selectivities (S CO2/N2 ) from the experimental carbon dioxide and nitrogen adsorption isotherms were fitted with a triple-site Langmuir equation [111,112]. Calculated selectivities of CO 2 for equimolar and 10:90 CO 2 /N 2 mixtures @ 0 • C on UPJS-15 (AC) and UPJS-16 (AC) are depicted in Figure 9c. Because UPJS-15 (AC) adsorbed large amounts of nitrogen and carbon dioxide, the compound did not show significant selectivity, and the function is almost linear over the entire pressure range. The maximal value S CO2/N2 @ 5 kPa is 0.17 for the CO 2 /N 2 50:50 binary mixture and 0.02 for the CO 2 /N 2 10:90 mixture. For UPJS-16 (AC), significant selectivity at low pressure was observed at 455 for the CO 2 /N 2 equimolar binary mixture and 50 for the CO 2 /N 2 10:90 mixture, which decreases with increasing pressure to 20 and 3 @ 100 kPa, respectively. These results indicate that the material is able to selectively adsorb carbon dioxide at low pressure and low concentration, which is an important prerequisite for its practical use as a selective adsorbent of this greenhouse gas from the atmosphere for environmental application. The selectivity of UPJS-16 (AC) under CO 2 /N 2 50:50 condition exceeds known MOF materials, such as MOF-5, HKUST-1, ZIF-8, or MOF-74 [112,113].
Hydrogen adsorption measurements revealed that compounds adsorbed only limited amounts of hydrogen (see Figure 9d), 21.1 cm 3 g −1 (0.19 wt.%; 0.94 mmol g −1 ) for UPJS-15 (AC) and 4.3 cm 3 g −1 (0.04 wt.%; 0.19 mmol g −1 ) for UPJS-16 (AC) @ −196 • C and 1 bar. It can be stated that among the mentioned MOF materials based on tetrahedral ligands, these are the lowest achieved values (see Table 2). Although the presented materials do not show an excellent hydrogen storage capacity, their high affinity for CO 2 over H 2 predetermines them for removal of carbon dioxide in reactions associated with hydrogen production, such as water-gas shift (WGS) and direct steam reforming (DSR) reactions [122]. Similar behaviour was also observed for compounds of the MOF-76 family [123].

SEM and EDS Analyses
Based on the textural results of UPJS MOFs mentioned above, UPJS-15 was selected as a host for sulphur in Li-S batteries due to its high porosity. UPJS-15 (AC) was investigated by energy-dispersive X-ray spectroscopy analysis (EDS) and scanning electron microscopy For the constructed sulphur cathode, the structural properties on the particle's surface are considered to be critical for its electrochemical performance. Therefore, the surface of S/UPJS-15 composite was analyzed by SEM and EDS. The SEM images of the S/UPJS-15 cathode after pressing are depicted in Figure 13a-c at view fields of 415 μm, 41.5 μm, and 10.4 μm. The electrode surface is uniform only with limited carks or holes and sufficiently porous for electrolyte penetration. The surface mapping of the S/UPJS-15 electrode is shown in Figure 13d, and it can be seen that elements sulphur, carbon, and For the constructed sulphur cathode, the structural properties on the particle's surface are considered to be critical for its electrochemical performance. Therefore, the surface of S/UPJS-15 composite was analyzed by SEM and EDS. The SEM images of the S/UPJS-15 cathode after pressing are depicted in Figure 13a-c at view fields of 415 µm, 41.5 µm, and 10.4 µm. The electrode surface is uniform only with limited carks or holes and sufficiently porous for electrolyte penetration. The surface mapping of the S/UPJS-15 electrode is shown in Figure 13d, and it can be seen that elements sulphur, carbon, and strontium are present and homogenously distributed on the electrode surface and the whole bulk of the material. The EDS spectra and corresponding exact element contents (C, F, S, O, and Sr) in the S/UPJS-15 electrode are summarized in Table 3 and displayed in Figure 14  For the constructed sulphur cathode, the structural properties on the particle's surface are considered to be critical for its electrochemical performance. Therefore, the surface of S/UPJS-15 composite was analyzed by SEM and EDS. The SEM images of the S/UPJS-15 cathode after pressing are depicted in Figure 13a-c at view fields of 415 μm, 41.5 μm, and 10.4 μm. The electrode surface is uniform only with limited carks or holes and sufficiently porous for electrolyte penetration. The surface mapping of the S/UPJS-15 electrode is shown in Figure 13d, and it can be seen that elements sulphur, carbon, and strontium are present and homogenously distributed on the electrode surface and the whole bulk of the material. The EDS spectra and corresponding exact element contents (C, F, S, O, and Sr) in the S/UPJS-15 electrode are summarized in Table 3 and displayed in Figure 14

Electrochemical Properties
The electrochemical performance of the Li-S battery assembled with S/UPJS-15 cathode was systematically investigated in electrochemical test cells. CV curves of the cells at 0.1 mV s −1 within the potential window 1.8-3.0 V are shown in Figure 15a. The typical redox reaction of Li-S batteries was accompanied by two prominent cathodic peaks located at around 2.3 V and 2.0 V. The first cathodic peak could be described as the phase

Electrochemical Properties
The electrochemical performance of the Li-S battery assembled with S/UPJS-15 cathode was systematically investigated in electrochemical test cells. CV curves of the cells at 0.1 mV s −1 within the potential window 1.8-3.0 V are shown in Figure 15a. The typical redox reaction of Li-S batteries was accompanied by two prominent cathodic peaks located at around 2.3 V and 2.0 V. The first cathodic peak could be described as the phase transitions of sulphur to dissolved polysulphides (Li 2 S x , 4 ≤ x ≤ 8) and then to insoluble discharge products Li 2 S 2 /Li 2 S, respectively. The anodic scan is related to the reverse transformation reaction from short-chain polysulphides to long-chain polysulphides, and finally to sulphur. The intensity of CV curves is slightly decreasing with the number of cycles. The charge/discharge curves between the potential range of 1.8 and 2.8 V of the S/UPJS-15 cathode at 0.2 C are presented in Figure 15b. The low-voltage plateau in the first cycle is depressed, though in other cycles both plateaus are visible with correspondence to the CV curves. The cycling performance at a cycling rate of 0.2 C during 100 cycles is depicted in Figure 15c. The initial discharge capacity was 337 mAh g −1 at 0.2 C, and decreased continuously to 235 mAh g −1 after 100 charge/discharge cycles. The capacity retention after 100 cycles was 69.8%, corresponding to a fading rate of 0.3% per cycle. Coulombic efficiency during the cycling procedure at 0.2 C reached a value of around 81.8%. Obtained initial discharge capacity is comparable to Mg-1,4-BDC [124], however, gently lower than HKUST-1 [125], RT-MOF-5 [126], Ce-UiO-66-BPDC [127], or MOF-5 [128]. It could be noted that although these materials show higher initial discharge capacities, the final capacity is significantly decreased during cycling and thus offers lower capacity retentions compared to UPJS-15 (see Table 4).    In summary, it could be concluded that UPJS-15 can be applied in Li-S batteries. By adjusting the electrode material preparation process, it will be possible to improve properties and achieve higher discharge capacities of the battery cell.

Conclusions
In this study, two new alkaline earth metal-organic frameworks (AE-MOFs) containing Sr(II) (UPJS-15)/Ba(II) (UPJS-16) ions and prolonged tetrahedral tetraazo-tetracarboxylic acid (H 4 MTA) were synthesized and investigated in detail in various fields of application. Single-crystal X-ray (SC-XRD) analysis revealed that the materials are isostructural and their crystal structures are constructed by alkaline-earth metal ions sequenced in 1D polymeric chains connected by MTA linkers. In their porous frameworks, 1D channels with sizes of about 11.19 × 10.10 Å 2 for UPJS-15 (AS) and 10.69 × 9.70 Å 2 for UPJS-16 (AS) are located. The porous channels are filled with solvents represented by DMF and H 2 O molecules. Solvents situated in the frameworks were solvent-exchanged for a lower boiling solvent, especially ethanol, for simpler and more effective activation. Synthesized AE-MOFs were studied by the combination of various analytical techniques EDS, SEM, HE-PXRD, PXRD, TG, DRIFT, IR, ICP-MAS, and EA. The compounds' activation processes were investigated by a combination of in situ heating HE-PXRD, TG, and in situ heating DRIFT, which confirmed the stability of the materials' frameworks after the degassing process. The samples were further investigated as adsorbents of different gases (Ar, N 2 , CO 2 , and H 2 ), and the obtained adsorption outcomes were compared with other metal-organic frameworks consisting of tetrahedral linkers. Argon (@ −186 • C) and nitrogen (@ −196 • C) adsorption/desorption measurements demonstrated that the UPJS-15 compound exhibits a S BET area of 1321 m 2 g −1 (Ar)/1250 m 2 g −1 (N 2 ) and UPJS-16 material adsorbs only a limited quantity of mentioned adsorbates. It should be noted that both materials are able to store CO 2 molecules with maximum capacities of 22.4 wt.% (5.08 mmol g −1 ) @ 0 • C; 14.7 wt.% (3.34 mmol g −1 ) @ 20 • C and 101 kPa for UPJS-15 and 11.5 wt.% (2.63 mmol g −1 ) @ 0 • C; 8.4 wt.% (1.89 mmol g −1 ) @ 20 • C and 101 kPa for UPJS-16. Moreover, DFT modelling was used to investigate the active adsorption sites within the alkaline earth central atoms and the MTA molecule (azo-functional group, C-H and π electron system of aromatic rings). The DFT results reveal that the primary adsorption sites are three coordinatively unsaturated sites (CUSs) located on the central atoms (∆H = −60.81 kJ mol −1 ) and azo groups (∆H = −19.05 kJ mol −1 for -N=N-··· CO 2 interaction)/phenyl-rings (∆H = −19.32 kJ mol −1 for π ··· CO 2 interaction and −∆H = −7.80 kJ mol −1 for C-H ··· CO 2 interaction) within the MTA linker. Based on the IAST calculation, UPJS-16 showed considerable selectivity at low pressure with a maximum at 50 for CO 2 /N 2 10:90 mixture and 455 for CO 2 /N 2 50:50 mixture. Calculated results prove that UPJS-16 could store and catch huge quantities of carbon dioxide from the air, even at low pressures. The mentioned measurements, calculations, and findings are especially important in the selective capture of CO 2 and the reduction of its concentration in the air, which is crucial from the point of view of environmental applications for reducing global warming. From the point of view of energy storage, the materials were also studied as hydrogen adsorbents, but the measurements show only limited adsorbed quantities of H 2 by prepared compounds: 0.19 wt.% (0.94 mmol g −1 ) for UPJS-15 and 0.04 wt.% (0.19 mmol g −1 ) for UPJS-16 at @ −196 • C and 1 bar. Although the materials adsorbed small amounts of hydrogen, it is also possible to find a positive in this result, which lies in the high selectivity of the CO 2 and H 2 separation. Because the purification of hydrogen in the mentioned gas mixture is important in many technological processes of hydrogen production, such as WGS and DSR reactions. The second way of using synthesized compounds in the field of energy storage presented in this study was the application of UPJS-15 as a support for sulphur in a Li-S battery. The battery constructed from UPJS-15 material showed an initial discharge capacity of 337 mAh g −1 at a cycling rate of 0.2 C, which decreased continuously slowly to 235 mAh g −1 after 100 charge/discharge cycles with a final capacity retention of~70%. Although the material displayed a slightly lower final discharge capacity than other metal-organic framework materials, it has a higher capacity retention at the end of the cycling processes.