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Stabilisation and functional enhancement of a metal–organic framework purinate-glass composite

Yujun Rong a, Ashleigh M. Chestera, Bethan Turnerb, Georgina P. Robertsonac, Ayano Konoa, Philip A. Chaterc, Lauren N. McHughb, David A. Keend, Thomas D. Bennettae and Celia Castillo-Blas§ *a
aDepartment of Materials Science and Metallurgy, University of Cambridge, Cambridge, CB3 0FS, UK. E-mail: castillo@icmm.csic.es
bDepartment of Chemistry, University of Liverpool, Crown Street, Liverpool L69 7ZD, UK
cDiamond Light Source Ltd, Diamond House, Oxfordshire, OX11 0DE, UK
dISIS Facility, Rutherford Appleton Laboratory, Harwell Campus, Didcot, Oxfordshire OX11 0QX, UK
eSchool of Physical and Chemical Sciences, University of Canterbury, Private Bag 4800, Christchurch 8140, New Zealand

Received 17th March 2025 , Accepted 16th July 2025

First published on 16th July 2025


Abstract

The development of metal–organic framework (MOF) crystal-glass composites (CGCs) has been hindered by the scarcity of MOF glass matrices with low glass transition temperatures (Tgs). Here, we investigate a CGC consisting of a low-Tg MOF glass (agZIF-UC-7) and UiO-66. Powder X-ray diffraction and stability tests in phosphate buffer saline solution showed UiO-66 was stabilised in the glass matrix. Additionally, the composite exhibited enhanced dye uptake and gas adsorption relative to agZIF-UC-7.


Metal–organic frameworks (MOFs) are nanoporous materials formed by the self-assembly of metal ion-based nodes and organic linkers.1 They have exhibited promise in a variety of applications, including gas separation, catalysis and biomedicine.2 The biomedical application of MOFs has gained interest because of their tuneable pore size and chemistry, achieved by combining different nodes and linkers. For example, MOFs can be used to store and release drugs, influence inflammatory wound environments and can be used in implants for improving host-tissue implant interfaces.3 To develop biocompatible MOFs, it is essential to use building blocks such as bioactive metal ions (e.g. Zr4+, Zn2+ or Fe2+) and bioactive organic linkers such as amino acid, peptides, nucleobases and saccharides.

Zeolitic imidazolate frameworks (ZIFs) are a subclass of MOFs consisting of tetrahedrally-coordinated metal ions (Zn2+, Co2+, Mn2+, Fe2+) linked by imidazolate (Im) derivatives. Several ZIFs can form glasses, such as ZIF-624 [Zn(Im)1−x(bIm)x] (Im = imidazolate, bIm = benzimidazolate, 0.1 < x < 0.33).5,6 These hybrid glasses can be defined as amorphous solids that exhibit a heat-induced transition from a brittle to a viscoelastic state over a temperature range given by the glass transition temperature (Tg).

Recently, ZIFs consisting of bioactive cations such as Zn2+ and biocompatible linkers such as purine, a family of nucleobases, have been successfully developed. Examples include ZIF-UC-7, [Zn(Im)x(pur)2−x] (pur = purinate), [Zn(pur, nIm)] (nIm = 4-nitro-2-phenoxymethanesulfonanilide) and [Zn(pur)Br·0.25DMF].7–9 Purine-containing ZIFs have both potential bioactivity and glass-forming ability, which might be promising for the fabrication of bioactive hybrid glasses. ZIF-UC-7 displays excellent glass forming ability thanks to its relatively low Tg and Tm compared to other meltable ZIFs. Despite their functional advantages in biomedical applications,10 MOFs are limited by their chemical instability and poor processability to form bulk products and are typically synthesised as microcrystalline powders.11

To address these manufacture limitations, MOF composites have received increased attention in the last years.12,13 One of the methods for manufacturing bulk MOF-derived materials is dispersing MOF crystals in a polymer matrix to fabricate mixed matrix membranes (MMMs).14 However, MMMs have various limitations, such as the formation of interfacial mesoporous voids and aggregation of MOF components within the matrix.15

Due to their excellent compatibility with crystalline MOFs, MOF glasses have been suggested as an alternative to polymer matrices.16 MOF crystal-glass composites (MOF CGCs), combining both crystalline and glassy MOFs, have shown improved gas adsorption properties relative to the MOF glass,17 where MOF glasses typically have reduced porosity relative to their parent crystals. Here, we investigate a new MOF CGC comprising a bioactive MOF glass matrix (agZIF-UC-7), selected for its low Tg (273 °C) and bioactive linker.7 Selecting a lower Tg glass means a lower working temperature (Tw) can be used because the Tw must exceed the Tg of the glass to facilitate composite formation. The composite was synthesised using a previous methodology (Fig. 1). Specifically, UiO-66, [Zr6O4(OH)4 (BDC)6·xH2O] (UiO = Universitetet i Oslo; BDC = 1,4-benzene dicarboxylic acid), was dispersed into the glass matrix; UiO-66 was selected because of its high surface area (1050 m2 g−1) and thermal stability (stable up to 500 °C).18


image file: d5cc01366f-f1.tif
Fig. 1 (a) UiO-66 structure (Zr-orange tetrahedra, C-grey, O-purple), (b) ZIF-UC-7 structure and precursors (Zn-purple, C-grey, N-blue), (c) Scheme of the MOF-CGC fabrication.

ZIF-UC-7 was synthesised solvothermally (Fig. S1, ESI), with powder X-ray diffraction (PXRD) confirming its crystalline structure (Fig. S2 and Table S1, ESI).7 CHN analysis and solution state 1H NMR (acid digested) support the [Zn(Im)1.75(pur)0.25] formula (Table S2 and Fig. S3, ESI). Thermogravimetric analysis (TGA) of the crystalline ZIF-UC-7 shows a thermal decomposition temperature (Td) of 521 °C (Fig. S4, ESI). Differential scanning calorimetry (DSC) confirmed the melting temperature (Tm) and Tg (Fig. S5, ESI). The first DSC upscan of crystalline ZIF-UC-7 shows a Tm of 336.7 °C and the second DSC scan shows a Tg of 273.1 °C, consistent with the literature.7 agZIF-UC-7, formed by melt-quenching, shows no Bragg peaks in its PXRD (Fig. 2a and Fig. S6, ESI), confirming its amorphous nature. DSC analysis on agZIF-UC-7 shows Tgs of 277 and 278 °C in the first and second upscans respectively (Fig. S5, ESI); TGA shows a Td of ∼507 °C (Fig. S7, ESI). Fourier-transform infrared spectroscopy (FTIR) and 1H NMR (acid-digested) of agZIF-UC-7 and ZIF-UC-7 confirm retention of the chemical features post-melt-quenching (Fig. S8 and S9, ESI). UiO-66 was synthesised based on reported methods; its structure was confirmed by Pawley refinement of the PXRD data (Fig, S10 and Table S3, ESI). TGA shows a Td of ∼350 °C (Fig. S11, ESI), giving a working range for composite formation of 278< Tw <350 °C; a Tw of 300 °C was selected to reduce loss of Bragg peak intensities (Fig. S12, ESI). The working pressure was 0.074 GPa to minimise Bragg peak broadening (Fig. S13, ESI). With these working parameters, equal weight percentages (wt%) of the starting materials were ball-milled to form a physical mixture, defined as (UiO-66)(agZIF-UC-7)(50/50). This mixture was then pelletised and heated to 300 °C, exceeding the Tg of agZIF-UC-7, enabling it to enter its supercooled liquid state and embed the UiO-66 crystallites. After cooling under vacuum, a cohesive, non-powdery [(UiO-66)0.5(agZIF-UC-7)0.5] composite was produced (Fig. S17, ESI).


image file: d5cc01366f-f2.tif
Fig. 2 (a) PXRD of the physical mixture and composite, inset: SEM image of composite and (b) X-ray PDFs, D(r)s, of the composite and starting materials, insets show the Zr6O4(OH)4 cluster and BDC linker of UiO-66 (Zr-yellow, C-black, O-pink) and imidazolate of agZIF-UC-7 (Zn-purple, C-black, N-blue, H-white).

PXRD (Fig. 2a) shows UiO-66 Bragg peaks in both the (UiO-66)(agZIF-UC-7)(50/50) and [(UiO-66)0.5(agZIF-UC-7)0.5] patterns, confirming UiO-66 crystallinity post composite synthesis. Bragg intensity is maintained after pelletisation and increases after heating (Fig. S14, ESI). The lattice parameters extracted from Pawley refinement match the literature values, indicating retention of the UiO-66 structure in the composite (Fig. S15 and Table S4, ESI). In contrast, the UiO-66 controls show no such preservation (Fig. S13, ESI), suggesting that the agZIF-UC-7 matrix stabilised the UiO-66 structure under pressure and heat. FTIR also confirms the presence of agZIF-UC-7 and UiO-66 in both the physical mixture and composite (Fig. S16, ESI). CHN and ICP analysis confirmed the composite and physical mixture compositions. The composite matched the target [(UiO-66)0.50(agZIF-UC-7)0.5] composition (Tables S5–S7, ESI). Similar ICP results for the physical mixture and composite indicate minimal decomposition of the agZIF-UC-7 component during composite formation after the thermal treatment.

The starting materials, physical mixture and composite were analysed by optical microscopy (Fig. S18 and S19, ESI) and SEM (Fig. S20–S30, ESI). SEM images of the (UiO-66)(agZIF-UC-7)(50/50) physical mixture show UiO-66 crystallites on the agZIF-UC-7 surface (Fig. S21, ESI). The pelletised physical mixture shows UiO-66 and agZIF-UC-7 particles (Fig. S22, ESI). Heating to 300 °C (above Tg = 278 °C) forms a composite with flow marks and UiO-66 crystallites embedded in the matrix (Fig. 2 inset; Fig. S23, ESI). The composite surface is not uniform, likely because of the low pelletisation pressure limiting contact between agZIF-UC-7 and UiO-66. EDX (Fig. S24–S26, ESI) shows similar Zr[thin space (1/6-em)]:[thin space (1/6-em)]Zn ratios (∼1.4–1.6) for both the pelletised physical mixture and composite, again suggesting minimal decomposition. Smaller regions (10–30 μm) reveal heterogeneity, with UiO-66 crystallites distinguishable from the agZIF-UC-7 (Fig. S26, ESI) by atomic and wt% ratios. EDX mapping also confirms distinct microdomains (Fig. S27–S30, ESI).

Pair distribution function (PDF) analysis confirms the structural integrity of the phases.19 The structure factor, S(Q),20 of UiO-66 show Bragg peaks (Fig. S31a, ESI) consistent with its crystal structure; Bragg peaks are not present in the S(Q) of agZIF-UC-7 because of its amorphous glass structure (Fig. S31b, ESI). The [(UiO-66)0.5(agZIF-UC-7)0.5] composite retained the UiO-66 Bragg features, indicating its preservation during composite synthesis (Fig. S32a, ESI). S(Q)s of the composite and its physical mixture are largely similar, suggesting no decomposition or recrystallisation of the starting materials after composite fabrication (Fig. S32a, ESI). Fourier transforming the S(Q)s produced the real-space D(r) functions (PDFs).22 The D(r) from the pristine materials matched reported D(r)s (Fig. S33 and S34, ESI),7,21 and the composite and physical mixture D(r)s were nearly identical (Fig. S32b, ESI), with short-range correlations from both starting materials (Fig. 2b) and longer-range peaks (beyond ∼8 Å) arising from UiO-66 (See ESI for assignment of starting materials’ D(r)s). The PDF results show that both phases were maintained after composite formation. Thermal stability was evaluated by TGA (Fig. S35–S37, ESI), which shows Tds of 411 °C and 425 °C for the physical mixture and composite respectively. DSC analysis on the physical mixture and composite show a peak at ∼100 °C in the first DSC upscan, corresponding to water evaporation, also present in the TGA of of UiO-66 (Fig. S38, ESI). The agZIF-UC-7 Tg (∼273 °C) is present in both DSC upscans of the physical mixture and [(UiO-66)0.5(agZIF-UC-7)0.5], indicating structural preservation of the agZIF-UC-7.

The CO2 uptake of ZIF-UC-7 (51.1 cm3 g−1), agZIF-UC-7 (14.8 cm3 g−1) and UiO-66 (95.0 cm3 g−1) matched reported literature values.7 The [(UiO-66)0.5(agZIF-UC-7)0.5] composite, however, exhibits a CO2 uptake of 30.9 cm3 g−1 (Fig. 3a and Table S8, ESI), indicating enhanced gas sorption capacity because of UiO-66 incorporation into the glass matrix. For N2 adsorption, the agZIF-UC-7 glass has slightly higher uptake and BET surface area (55.4 m2 g−1) than its crystalline parent ZIF-UC-7 (41.8 m2 g−1), similar to previous analysis on crystalline ZIF-62 and its glass (Table S9, ESI).22 The composite and UiO-66 have BET surface areas of 214 and 852 m2 g−1 respectively (Fig. 3b), confirming increased surface area when the UiO-66 is added to the glass matrix. Pore widths for ZIF-UC-7 and its glass could not be determined by N2 and CO2 adsorption because of gas size limitations, but the composite exhibits pore widths similar to the UiO-66 (Fig. S33, ESI).


image file: d5cc01366f-f3.tif
Fig. 3 a) CO2 gas sorption isotherms for all the materials at 273 K. (b) N2 gas sorption isotherms for all the materials at 77 K. Open and closed circles represent adsorption and desorption respectively. (c) pH stability tests in PBS over a 4 day period. (d) Methylene blue uptake over time, concentration of the starting solution was 5 ppm. UV-vis maximum was fixed at 664 nm (see Experimental methods).

To evaluate biomedical potential, the pH stability of [(UiO-66)0.5(agZIF-UC-7)0.5], agZIF-UC-7 and UiO-66 in phosphate-buffered saline (PBS) solution was monitored over time (Fig. 3c). PBS, with a physiological pH of 7.4, mimics the concentration of ions in the human body and is widely used in biomedical research.23 The pH increased over time for agZIF-UC-7, likely due to imidazolate linker release, previously shown by ZIF-8, [Zn(mIm)2], where mIm is 2-methylimidazolate. UiO-66 immersion caused a decrease in pH, attributed to phosphate-induced degradation and terephthalate release.24,25 In contrast, [(UiO-66)0.5(agZIF-UC-7)0.5] showed minimal pH changes, maintaining a stable environment, which is crucial for biomedical applications because it can protect drugs from environment-induced degradation and allow for slower release of encapsulated drugs within the composite.26 Moreover, after PBS immersion, the composite maintains its N2 uptake, suggesting its suitability for drug capture in PBS media (Table S8 and Fig. S39, S40, ESI). Optical and SEM images after 24 hours in PBS show that the composite retains its surface morphology, with UiO-66 crystallites visible in the composite (Fig. S41 and S42, ESI). EDX analysis gives a Zr[thin space (1/6-em)]:[thin space (1/6-em)]Zn ratio of 1.3–1.9 (Fig. S43 and S44, ESI), suggesting minimal degradation of either component and microdomains are still visible in the EDX mapping (Fig. S45, ESI). ICP-OES analysis shows a small decrease in the Zr[thin space (1/6-em)]:[thin space (1/6-em)]Zn ratio (1[thin space (1/6-em)]:[thin space (1/6-em)]1.23 to 1[thin space (1/6-em)]:[thin space (1/6-em)]1.07) after PBS immersion, likely from agZIF-UC-7 leaching into the PBS solution (Table S10, ESI).23 This is corroborated by the higher Zr[thin space (1/6-em)]:[thin space (1/6-em)]Zn ratio of 1[thin space (1/6-em)]:[thin space (1/6-em)]1.74 in the PBS supernatant. PXRD analysis on the UiO-66 control after immersion in PBS containing 5 ppm of methylene blue (MB) over 24 hours confirms UiO-66's degradation, given by a lack of Bragg peaks (Fig. S46, ESI). However, in the composite, UiO-66 retained its crystallinity, highlighting the agZIF-UC-7 matrix's ability to effectively stabilise the UiO-66 structure in PBS and prevent its degradation.

To assess drug delivery ability of the composite, MB dye was used as a proxy; UiO-66 efficiently adsorbs MB in neutral/basic solutions.27 Samples were immersed in 5 ppm MB solutions in PBS (Fig. 3d), reaching 92%, 62%, and 81% adsorption for UiO-66, agZIF-UC-7 and the composite respectively after 8 hours. Despite a lower UiO-66 molar ratio, the composite's adsorption is similar to the pristine UiO-66, likely because of its stable pH (the adsorption capacity of UiO-66 increases as pH increases).27 PXRD (Fig. S46, ESI) shows that UiO-66 degrades after 24 hours, while the composite retains Bragg peaks, highlighting UiO-66's improved stability in the glass matrix.

In conclusion, this study reports the synthesis of a novel MOF CGC by dispersing UiO-66 in agZIF-UC-7. FTIR, PDF, and PXRD confirmed the preservation of the starting materials, while DSC scans showed the expected Tg of agZIF-UC-7. The [(UiO-66)0.5(agZIF-UC-7)0.5] composite combines UiO-66's high surface area, gas sorption, and dye uptake with the amorphous flexibility of agZIF-UC-7. Enhanced CO2 uptake and BET surface area reflect the benefits of embedding UiO-66 in the glass matrix. The composite's superior pH stability in PBS, compared to UiO-66, highlights the matrix's protective role. Efficient methylene blue adsorption of the composite, despite its lower UiO-66 content, confirms MOF preservation post immersion. These findings suggest promising applications in gas storage, biomedical devices, drug delivery and environmental remediation, paving the way for future MOF CGC research.

AMC and CCB acknowledge Leverhulme Trust Research (RPG-2020-005). CCB also thanks Comunidad de Madrid (2024-T1/TEC-31450). TDB thanks the Royal Society (URF\R\211013, RGS\R2\212221). We acknowledge to Diamond Light Source (I15-1, CY29957). LNM and BT (Faculty of Science and Engineering) thank the University of Liverpool for funding.

CCB conceptualised the project. AMC, YR and CCB wrote the manuscript with input from all authors. YR and CCB synthesised all materials. YR conducted FTIR, SEM-EDX, PXRD, TGA and DSC analysis under CCB and AMC's supervision. CCB, GPR, PAC, DAK, and AK collected PDF data, processed by AMC. TDB funded the work and contributed with discussions. BT and LNM collected gas sorption data, analysed by CCB. CCB conducted dye uptake experiments and analysis.

Conflicts of interest

There are no conflicts to declare.

Data availability

The data supporting this article have been included as part of the ESI for SEM, ICP and pH stability tests. Data for this article, including DSC, PXRD, PDF, FTIR, TGA, gas sorption isotherms and UV-vis are available at Open Science Framework at DOI https://doi.org/10.17605/OSF.IO/QY8ZT.

References

  1. H. Furukawa, K. E. Cordova, M. O’Keeffe and O. M. Yaghi, Science, 2013, 341, 1230444 CrossRef PubMed.
  2. A. Dhakshinamoorthy, Z. Li and H. Garcia, Chem. Soc. Rev., 2018, 47, 8134–8172 RSC.
  3. J. Yang and Y.-W. Yang, Small, 2020, 16, 1906846 CrossRef CAS PubMed.
  4. T. D. Bennett, Y. Yue, P. Li, A. Qiao, H. Tao, N. G. Greaves, T. Richards, G. I. Lampronti, S. A. T. Redfern, F. Blanc, O. K. Farha, J. T. Hupp, A. K. Cheetham and D. A. Keen, J. Am. Chem. Soc., 2016, 138, 3484–3492 CrossRef CAS PubMed.
  5. L. Frentzel-Beyme, M. Kloß, P. Kolodzeiski, R. Pallach and S. Henke, J. Am. Chem. Soc., 2019, 141, 12362–12371 CrossRef CAS PubMed.
  6. L. León-Alcaide, R. S. Christensen, D. A. Keen, J. L. Jordá, I. Brotons-Alcázar, A. Forment-Aliaga and G. Mínguez Espallargas, J. Am. Chem. Soc., 2023, 145, 11258–11264 CrossRef PubMed.
  7. A. M. Bumstead, C. Castillo-Blas, I. Pakamorė, M. F. Thorne, A. F. Sapnik, A. M. Chester, G. Robertson, D. J. M. Irving, P. A. Chater, D. A. Keen, R. S. Forgan and T. D. Bennett, Chem. Commun., 2023, 59, 732–735 RSC.
  8. J. Kahr, J. P. S. Mowat, A. M. Z. Slawin, R. E. Morris, D. Fairen-Jimenez and P. A. Wright, Chem. Commun., 2012, 48, 6690–6692 RSC.
  9. L. Longley, N. Li, F. Wei and T. D. Bennett, R. Soc. Open Sci., 2017, 4, 171355 CrossRef CAS PubMed.
  10. I. Abánades Lázaro and R. S. Forgan, Coord. Chem. Rev., 2019, 380, 230–259 CrossRef.
  11. J. Ren, H. W. Langmi, B. C. North and M. Mathe, Int. J. Energy Res., 2015, 39, 607–620 CrossRef CAS.
  12. N. Yuan, X. Zhang and L. Wang, Coord. Chem. Rev., 2020, 421, 213442 CrossRef CAS.
  13. S. Yang, L. Peng, S. Bulut and W. L. Queen, Chem. – Eur. J., 2019, 25, 2161–2178 CrossRef CAS PubMed.
  14. Y. Cheng, S. J. Datta, S. Zhou, J. Jia, O. Shekhah and M. Eddaoudi, Chem. Soc. Rev., 2022, 51, 8300–8350 RSC.
  15. Y. Zhang, X. Feng, S. Yuan, J. Zhou and B. Wang, Inorg. Chem. Front., 2016, 3, 896–909 RSC.
  16. T. D. Bennett, Y. Yue, P. Li, A. Qiao, H. Tao, N. G. Greaves, T. Richards, G. I. Lampronti, S. A. T. Redfern, F. Blanc, O. K. Farha, J. T. Hupp, A. K. Cheetham and D. A. Keen, J. Am. Chem. Soc., 2016, 138, 3484–3492 CrossRef CAS PubMed.
  17. C. W. Ashling, D. N. Johnstone, R. N. Widmer, J. Hou, S. M. Collins, A. F. Sapnik, A. M. Bumstead, P. A. Midgley, P. A. Chater, D. A. Keen and T. D. Bennett, J. Am. Chem. Soc., 2019, 141, 15641–15648 CrossRef CAS PubMed.
  18. D. Zou and D. Liu, Mater. Today Chem., 2019, 12, 139–165 CrossRef CAS.
  19. C. Castillo-Blas, J. M. Moreno, I. Romero-Muñiz and A. E. Platero-Prats, Nanoscale, 2020, 12, 15577–15587 RSC.
  20. D. A. Keen, J. Appl. Crystallogr., 2001, 34, 172–177 CrossRef CAS.
  21. J. Hou, C. W. Ashling, S. M. Collins, A. Krajnc, C. Zhou, L. Longley, D. N. Johnstone, P. A. Chater, S. Li, M. V. Coulet, P. L. Llewellyn, F. X. Coudert, D. A. Keen, P. A. Midgley, G. Mali, V. Chen and T. D. Bennett, Nat. Commun., 2019, 10, 2580 CrossRef PubMed.
  22. L. Frentzel-Beyme, P. Kolodzeiski, J.-B. Weiß, A. Schneemann and S. Henke, Nat. Commun., 2022, 13, 7750 CrossRef CAS PubMed.
  23. M. D. J. Velásquez-Hernández, R. Ricco, F. Carraro, F. T. Limpoco, M. Linares-Moreau, E. Leitner, H. Wiltsche, J. Rattenberger, H. Schröttner, P. Frühwirt, E. M. Stadler, G. Gescheidt, H. Amenitsch, C. J. Doonan and P. Falcaro, CrystEngComm, 2019, 21, 4538–4544 RSC.
  24. I. Abánades Lázaro, S. Haddad, S. Sacca, C. Orellana-Tavra, D. Fairen-Jimenez and R. S. Forgan, Chem, 2017, 2, 561–578 Search PubMed.
  25. D. Bůžek, S. Adamec, K. Lang and J. Demel, Inorg. Chem. Front., 2021, 8, 720–734 RSC.
  26. H. Kaur, G. C. Mohanta, V. Gupta, D. Kukkar and S. Tyagi, J. Drug Delivery Sci. Technol., 2017, 41, 106–112 CrossRef CAS.
  27. A. A. Mohammadi, A. Alinejad, B. Kamarehie, S. Javan, A. Ghaderpoury, M. Ahmadpour and M. Ghaderpoori, Int. J. Environ. Sci. Technol., 2017, 14, 1959–1968 CrossRef CAS.

Footnotes

Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5cc01366f
Both authors contributed equally.
§ Present address: Materials Science Institute of Madrid – Spanish National Research Council (ICMM-CSIC), C/Sor Juana Inés de la Cruz 3, Madrid, 28049, Spain.

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