Asia R. Y.
Almuhana
ab,
Sarah L.
Griffin
b and
Neil R.
Champness
*b
aKing Faisal University, P.O. 380, Al-Ahsa 31982, Saudi Arabia
bSchool of Chemistry, The University of Birmingham, Birmingham, UK. E-mail: n.champness@bham.ac.uk
First published on 27th July 2024
The synthesis of charge assisted amidinium⋯phosphonate hydrogen-bonded organic frameworks (HOFs) is reported. Two tectons, with either a biphenyl or naphthalene diimide backbone, were combined with bis-amidinium salts to afford HOF1 and HOF2, respectively. Whereas HOF1 formed rapidly, typically within two days of mixing, HOF2 proved more challenging to synthesise. Interestingly, the presence of sunlight facilitated the rapid formation of HOF2 within a few hours. Although crystals of tectons 1H4 or 2Et4 exhibited densely packed structures, combination of the corresponding phosphonate bases with bis-amidinium cations, through amidinium⋯phosphonate interactions, gave open framework materials. The HOFs formed through this approach exhibited notable stability limitations, including a propensity for phase transformations or structural collapse upon solvent removal.
Charge-assisted hydrogen bonds have been shown to be an effective approach to creating HOFs, notably using the interaction between bis-amidinium cations and carboxylate anions.10–14 In this study we demonstrate how this strategy can be modified to employ a charge-assisted supramolecular synthon adopted between bis-phosphonate anions and bis-amidinium cations. To our knowledge previous reports of the amidinium⋯phosphonate synthon being used for HOF formation are relatively unusual,15,16 particularly in comparison to corresponding amidinium⋯carboxylate systems.10–14 Notably, anti-electrostatic hydrogen bonds have been employed using phosphonate anions, providing an alternative strategy to incorporating phosphonate into self-assembled structures.17,18
In this study two distinct backbones are used for the bis-phosphonate tecton, biphenyl and naphthalene diimide (NDI), which afford distinct structural properties allowing us to draw comparisons between related HOFs. Thus, we demonstrate that when combined with amidinium tectons, these phosphonate anions engage in a diverse range of intermolecular hydrogen bonding interactions, resulting in the formation of extended framework structures.
A biphenyl-4,4′-diphosphonate 1 was selected as the first anionic tecton. 1 has been used previously as a ligand for MOF synthesis, including examples that exhibit increased quantum yields or moisture stability.19–231H4 consists of a rigid centre linked to flexible phosphonate moieties via methylene groups. It has previously been suggested that the more flexible the tecton, the more readily it can adapt to form hydrogen bonds, thus facilitating the growth of co-crystals,24 and by analogy HOFs. The phosphonate groups tend to pack densely, resulting in layered structures without pores; however, it is anticipated that using a secondary tecton to form a HOF could facilitate the construction of porous structures.
Rylene diimides are interesting examples of tectons for HOF formation,14,25 due to their redox and photochemical activity, as well as high thermal and chemical stability.26 Indeed, we have recently reported the synthesis and photoinduced radical formation in a NDI-containing HOF constructed using amidinium⋯carboxylate synthons.14 The rich chemistry of NDIs means they are readily functionalized with a variety of moieties,27 enabling the introduction of a variety of hydrogen-bonding sites, making them ideal tecton candidates for HOF formation.
Single crystals of 1H4 were grown from a water and MeOH mixture, whereas colourless needle-shaped single crystals of 2(Et)4 were grown via slow evaporation of a solution of the compound in CH2Cl2. The crystal structures of these two tectons allows the determination of the conformational arrangement of the molecules in the solid state (Fig. 1). The structure of 1H4 reveals a co-planar arrangement of the biphenyl unit and a transoid configuration of the two phosphonate groups. In the case of 2(Et)4 the two phenyl groups attached to the imide groups adopt an angle of 70.12° with respect to the plane of the NDI, and the phosphonates, once again, adopt a transoid arrangement.
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Fig. 1 Compounds a) 1H4 and b) 2(Et4 accompanied by views of their single crystal structures viewed along the b-axis and c-axis respectively. |
Crystals of HOF1 were grown by layering an aqueous solution of 1,4-phenyl-bis-amidinium dichloride over an aqueous solution of 1H4, containing two drops of 1 M NaOH to deprotonate the acid. The two layers were separated by 1 mL of MeOH in order to slow the crystallization process. Colourless needle crystals were formed which were of suitable quality for analysis by single crystal X-ray diffraction (SCXRD). The crystal structure of HOF1 reveals that the anion was partially deprotonated, releasing two of the four protons, to form 1H22−. Thus, each phosphonate group presents two hydrogen bond acceptors and one donor, enabling the anionic components to interact with each other by hydrogen bonds, as well as interacting with bis-amidinium cations. The anionic and cationic tectons pack in a layered arrangement, with a layer of cations followed by an anion layer (Fig. 2a). This results in a sheet-like structure with pores that encapsulate two water molecules. The biphenyl group is buckled in the 1H22− tectons (14.2° interplanar angle between phenyls) and the phosphonate groups are arranged in a cisoid fashion, in contrast to the free tecton (see above), leading to an extensive network of interactions formed between cations and anions, with each 1H22− tecton interacting with four adjacent bis-amidinium cations (Fig. 3). Each phosphonate group interacts with two bis-amidinium cations, one through two parallel O⋯H–N interactions (d2a2), and the other through a single hydrogen bond (d1a1).
The ability of HOF1 to survive solvent removal was evaluated by powder X-ray diffraction (PXRD) studies revealing that air-dried crystals lose crystallinity. Notably HOF1 showed no evidence of π-based interactions which might be anticipated to provide additional stability to the framework. Therefore, it was decided to explore a tecton with a larger aromatic surface, 3.
Crystals of HOF2 were formed using a layering approach at room temperature (ca. 25–27 °C) in the presence of sunlight. After 5 hours of diffusion, long yellow needle crystals (HOF2) were formed (Fig. 4a). The crystallisation process was sensitive to sunlight and temperature. Indeed, the crystallisation process was found to be highly irreducible and was extremely sensitive to the laboratory environment, simply changing laboratory made attempts at crystal growth unsuccessful. The use of light to grow crystals is a common technique for growing amino acid crystals.22–24 Light may also be used to control monomer self-assembly and facilitate crystallization by modifying the solubility of molecules after irradiation.28–30 Notably this has previously been demonstrated for the crystallisation of an amidinium⋯carboxylate based HOF.31 In the study by White et al., light is believed to control tecton release for self-assembly into the crystalline framework through photoinduced isomerisation. Although photoinduced isomerisation is unlikely to be pertinent to the crystallisation of HOF2, it is likely that the crystallisation process is aided by localised heating from the incident sunlight. However, we cannot rule out that photoexcitation of the NDI may contribute to the crystallisation process.
HOF2 crystallizes with one 35− anion and two and a half bis-amidinium cations in the crystallographic asymmetric unit accompanied by multiple solvent molecules. It is known that imide groups are susceptible to ring-opening in the presence of base,14 and HOF2 exhibits this behaviour with one of the NDI imide rings opening to generate an additional carboxylate moiety (Fig. 4c), leading to charge-balance in the system. The intact phenyl imide moiety maintains an angle of 78.1° between the planes formed by the phenyl and naphthalene imide group, similar to the arrangement seen in the structure of 2(Et)4. In HOF2 the anion is fully deprotonated, unlike in HOF1. The components of the HOF are arranged in a 3D pillared structure, where the bis-amidinium is both involved in the formation of the sheet alongside the NDI-based anions, whilst also serving as a pillar between the layers of the sheet (Fig. 1b). The crystal structure of HOF2 reveals that the phosphonate benzene ring in the closed imide ring sits perpendicularly to the NDI plane (83.7°), inhibiting close aggregation between adjacent molecules.
The anion in HOF2, 35−, is hydrogen-bonded to seven surrounding molecules: six bis-amidinium cations and one 35− anion (Fig. 4c), affording a total of 13 H-bond interactions per anion. The two phosphonate groups are H-bonded to four neighbouring bis-amidinium molecules, forming parallel interactions with each of them (d2a2), with interaction distances (P–O⋯H–N) ranging from 1.86 Å to 2.14 Å and ∠OHN 177.2° to 141.0°. One of the carbonyl groups of the closed ring interacts with a nearby amidinium, creating a weak single (d1a1) interaction (CO⋯H–N, 2.16 Å, and ∠OHN 127.5°).
The stability of HOF2 was examined by thermogravimetric analysis (TGA) and powder X-ray diffraction (PXRD). TGA measurements indicated that the network gradually released guest water molecules, up to ca. 85 °C, accounting for approximately 20% of the total weight of the sample (Fig. 5a). A sharp weight loss, attributed to the decomposition of bis-amidinium cations, is then observed above ∼180 °C. The frameworks phase purity, crystallinity, and stability were evaluated using PXRD. A PXRD experiment was conducted on air-dried crystals without grinding, and the observed diffraction pattern was compared with the calculated pattern derived from the single crystal structure. Grinding of the sample results in significant peak broadening and loss of crystallinity. The stability of the framework after activating the sample under vacuum for two days was also assessed (Fig. 5b). The PXRD pattern obtained for this dried sample showed notable changes suggesting decomposition or a phase transition due to solvent removal.
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Fig. 5 a) Thermogravimetric analysis for HOF2; b) PXRD patterns recorded for HOF2: simulated (top – green), as synthesised (middle – pink), and dried sample (bottom – purple). |
Crystal data for C14H20O8P2 (M = 378.24 g mol−1): monoclinic, space group P21/c (no. 14), a = 14.8893(5) Å, b = 6.2149(2) Å, c = 9.0927(3) Å, α = γ = 90°, β = 93.663(3)°, V = 839. 86(5) Å3, Z = 2, T = 100.00(10) K, μ(Cu Kα) = 2.730 mm−1, Dcalc = 1.496 g cm−3, 7416 reflections measured (5.95° ≤ 2θ ≤ 155.246°), 1792 unique (Rint = 0.0586) which were used in all calculations. The final R1 was 0.04895 (I > 2σ(I)) and wR2 was 0.1484 (all data).
Crystal data for C22H26N4O6P2 (M = 504.41 g mol−1): monoclinic, space group C2/c (no. 15), a = 12.0665(2) Å, b = 13.6291(3) Å, c = 15.2147(2) Å, α = γ = 90°, β = 92.9890(10)°, V = 2498.74(8) Å3, Z = 4, T = 100.02(16) K, μ(Cu Kα) = 2.062 mm−1, Dcalc = 1.341 g cm−3, 11250 reflections measured, 2643 unique (Rint = 0.0494) which were used in all calculations. The final R1 was 0.1162 (I > 2σ(I)) and wR2 was 0.2245 (all data).
Crystal data for C36H36N2O10P2 (M = 359.30 g mol−1): monoclinic, space group P21/n (no. 14), a = 5.51236(3) Å, b = 15.23409(8) Å, c = 19.29148(11) Å, α = γ = 90°, β = 97.9423(6)°, V = 1604.478(15) Å3, Z = 2, T = 100.02(16) K, μ(Cu Kα) = 1.796 mm−1, Dcalc = 1.487 g cm−3, 27458 reflections measured, 3248 unique (Rint = 0.0191) which were used in all calculations. The final R1 was 0.0303 (I > 2σ(I)) and wR2 was 0.0802 (all data).
Crystal data for C28H16N2O11P2·2.5(C8H12N4) (M = 1028.91 g mol−1): triclinic, space group P (no. 2), a = 10.7489(1) Å, b = 11.1092(1) Å, c = 28.1083(2) Å, α = 92.980(1)°, β = 92.563(1)°, γ = 102.701(1)°, V = 3264.47(5) Å3, Z = 2, T = 100.15 K, μ(CuKα) = 1.448 mm−1, Dcalc = 1.413 g cm−3, 117
847 reflections measured, 13
490 unique (Rint = 0.0431) which were used in all calculations. The final R1 was 0.0923 (I > 2σ(I)) and wR2 was 0.2732 (all data).
Footnote |
† Electronic supplementary information (ESI) available: CCDC 2352949–2352952. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d4ce00479e |
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