Open Access Article
Subrata Mandal
a,
Novitasari Sinambela
a,
Johannes Biskupekb,
Riccarda Müller
c,
Ute Kaiserb,
Kerstin Leopold
c and
Andrea Pannwitz
*adef
aInstitute of Inorganic Chemistry I, University Ulm, Albert-Einstein-Allee 11, 89081 Ulm, Germany
bCentral Facility of Electron Microscopy, Electron Microscopy Group of Material Science, University of Ulm, Albert-Einstein-Allee 11, Ulm 89081, Germany
cInstitute of Analytical and Bioanalytical Chemistry, University Ulm, 89081 Ulm, Germany
dInstitute for Inorganic and Analytical Chemistry, Friedrich-Schiller-University Jena, Humboldtstr. 8, 07743 Jena, Germany. E-mail: Andrea.pannwitz@uni-jena.de
eCenter for Energy and Environmental Chemistry Jena (CEEC), Friedrich-Schiller-Universität Jena, Philosophenweg 7a, 07743 Jena, Germany
fHelmholtz Institute for Polymers in Energy Applications Jena (HIPOLE Jena), Lessingstraße 12-14, 07743 Jena, Germany
First published on 13th October 2025
The selective oxidation of amines to imines is an essential transformation in many chemical syntheses. Driving such reactions with light and earth abundant catalysts is highly interesting in the context of solar light energy conversion and broadening the reaction scope in organic synthesis. The here reported bimetallic metal–organic framework (MOF), UiO-67 Ru50-Mn10, allows oxidation of benzylamine under ambient conditions via dual electron and energy transfer with oxygen. UiO-67 Ru50-Mn10 integrates [Mn(bpy)2(Cl)2] active sites and light-active [Ru(bpy)3]2+ photosensitizers at the linkers of the UiO-67 scaffold. The spatial organisation of photo and redox-active centres enables efficient charge separation and mass transport. Under 460 nm LED irradiation for 24 h and ambient aerobic conditions, UiO-67 Ru50-Mn10 catalyses the oxidation of benzylamine to N-benzylidene-1-phenylmethanamine with turnover numbers up to 634, which is 1.6 to 1.8 times higher than homogeneous analogues and the Mn-free UiO-67 Ru50. Structural and spectroscopic studies confirm successful incorporation of both metals, while mechanistic analyses reveal dual electron and energy transfer pathways, influenced by the solvent environment. This work highlights the potential of heterometallic MOFs with earth-abundant catalytic sites as efficient platforms for photocatalytic oxidative transformations.
For example, Li and co-workers reported the oxidation reactions of a series of amines to imines with conversion yields of around 41–99% and selectivity of around 45–90% using molecular O2 as an oxidant over the MOF NH2-MIL-125(Ti) under visible light irradiation.8 Bai et al. reported that the MOF LTG-NiRu, constructed from a [Ru(phen)3]2+-derived linker and Ni2+-functionalized nodes, exhibited exceptional catalytic activity in the aerobic photocatalytic oxidative coupling of amine derivatives, achieving nearly 100% conversion of benzylamines within 1 h under visible light.9 Jin and co-workers developed a mixed-linker Zr-MOF incorporating both electron donor and acceptor linkers based on naphthalene diimide and porphyrin, which showed high photocatalytic activity for aerobic oxidative coupling of benzylamine.10 However, in such systems, catalytic activity or charge separation often occurs between the parent linker and the secondary building unit (SBU), which can result in partial framework degradation.11 Although the latter one is stable, it lacks defined active sites and selective reaction pathways.
Incorporation of PS and single-site catalysts into a MOF represents a very interesting field for other photocatalytic reactions, such as the H2 evolution reaction (HER),12,13 CO2 reduction reaction (CO2RR),14–17 and alcohol oxidation,18 however, their application related to benzylamine oxidation is rarely explored.
Nature's Photosystem II (PS II) provides a blueprint for light-driven, redox chemistry through the precise arrangement of a chlorophyll-based photosensitizer (P680) and a Mn4CaO5 cluster that catalyses water oxidation.19 While synthetic molecular models of PSII have largely aimed to replicate water oxidation,20 often using Ru-based photosensitizers linked to manganese centres,21,22 the potential of such systems for alternative oxidative transformations remains underexplored.
In this study, a Ru(bpy)32+-functionalized MOF (UiO-67 Rux) was synthesized and further modified by coordinating Mn2+ sites via post-synthetic modification (PSM) to the bipyridine linkers of the framework, yielding the bimetallic system UiO-67 Rux-Mny. The concept is based on leveraging the structural stability and modularity of the UiO-67 backbone to organize photoactive ruthenium complexes and redox-active manganese centres in proximity, mimicking the compartmentalized environment of natural photosystem II. The resulting hybrid material was explored as a visible-light-responsive catalyst for the oxidative conversion of benzylamine to imine in aerobic conditions, and its activity was benchmarked against related systems, mono-functionalized analogues (UiO-67 Ru and UiO-67 Mn), and homogeneous reference complexes such as Ru(bpy)32+ and Mn(bpy)2Cl2. To validate successful Ru and Mn integration and preserve framework structure, multiple analytical tools were employed, including X-ray diffraction (XRD), infrared (IR) spectroscopy, nuclear magnetic resonance (NMR) spectroscopy, transmission electron microscopy (TEM), and X-ray photoelectron spectroscopy (XPS). To probe charge separation and electron-transfer behaviour, a combination of steady-state and time-resolved spectroscopic techniques, UV-vis absorption, photoluminescence quenching, and time-resolved emission, was employed, along with electrochemical studies.
This work sheds light on the cooperative effects between integrated light-absorbing and catalytic centres in MOF-based systems, offering new directions for the rational design of high-performance photocatalytic platforms for oxidative reactions.
:
y = 5
:
1 and 1
:
1). In these processes, the MOFs UiO-67 Rux-Mny (10
:
10 and 50
:
10) were designed and synthesized by a mixed-ligand synthetic strategy to introduce the Ru-units, and subsequently post-synthetic metalation (PSM) to introduce the Mn-sites. The metallo-ligand linker [Ru(H2bpydc)(bpy)2]Cl2 was prepared according to the previously published method.23 The red coloured MOFs UiO-67 Ru10 and UiO-67 Ru50 (10 and 50% Ru respective to the bpdyc) were synthesized by carefully adjusting the ratio of 2,2′-bipyridine-5,5′-dicarboxylic acid (H2bpydc) and [Ru(H2bpydc)(bpy)2]Cl2 to react with ZrCl4 under solvothermal conditions and in presence of benzoic acid (BA) in N,N-dimethylformamide (DMF) at 120 °C (Fig. 1).24 To generate control samples, white colour UiO-67 was synthesized by using only the H2bpydc. The PSM of UiO-67 Rux and UiO-67 were performed by treating those nanocrystals with feed amounts of 10% (respective to the bpdyc) MnCl2 and 10% additional bipyridine (bpy) solution in ethanol (Fig. 1).
The crystallinity of these UiO-67 MOFs was maintained well in UiO-67-Rux and UiO-67 Rux-Mn10 and UiO-67 Mn10, which was confirmed by PXRD patterns similar to that of the here synthesized reference UiO-67 (Fig. 2a). Moreover, each phase exhibited characteristic reflection planes (111), (200), (220), (311), (222), and (400) at angles 5.7°, 6.6°, 9.3°, 10.9°, 11.4°, and 13.2°, respectively, confirming that they are isostructural to the reported face-centred cubic phase of UiO-67 (bpdc) (bpdc = biphenyl dicarboxylate) with the space group Fm
m.25 This unique topology of UiO-67 (Fig. S5) has a periodic structure with an ideal unit cell formula of Zr6O4(OH)4(BPDC)6, where this cluster adopts an octahedral geometry with six Zr(IV) cations occupying its vertices.26 Successful incorporation of Ru and Mn moieties was supported by diffuse reflectance UV/vis spectroscopy. A broad absorption (∼400–700 nm) in the spectrum of UiO-67 Ru50-Mn10 was consistent with the absorption of UiO-67 Ru50, which can be attributed to the metal-to-ligand charge transfer (MLCT) absorption of [Ru(bpy)3]2+ moiety in the UiO-67 framework (Fig. 2b). An increase in the absorption edge and blue shift of the highest absorption MLCT band compared to spectra of homogenous [Ru(H2bydc)(bpy)2]2+ (Fig. S2) can be attributed to the immobilization effect of the complex in a rigid environment.27 The immobilization of the Mn complex, however, is not distinguishable, but can be supported by studying the diffuse reflectance UV-visible spectroscopy of the control UiO-67 Mn10 counterparts. As shown in Fig. 2b, an additional broad absorption in the range of 360–500 nm in UiO-67 Mn10 is observed compared to that of pristine UiO-67, resulting in a yellow colored solid (Fig. 2b, inset), which can be attributed to the absorption resulting from the Mn-complex.28 Compared to the spectra of its homogeneous molecular model [Mn(bpy)2Cl2] (Fig. S2), a significant red shift in the MOF can be ascribed to the role of the solvent effect on the absorption band, tentatively assigned to an MLCT.28
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| Fig. 2 (a) PXRD patterns of UiO-67 Ru50-Mn10 and their counterparts (UiO-67, UiO-67 Mn10, UiO-67 Ru50) and the simulated XRD pattern of UiO-67 made up of biphenyl dicarboxylate (bpdc) linker obtained from the crystallographic data reported earlier,25 and their (b) UV-vis absorption spectra obtained from the solid-state diffuse reflectance spectroscopy. Inset on the right side of the figures shows the photograph of the prepared samples. (c) Transmission electron microscopic (TEM) images of the UiO-67, UiO-67 Mn10, UiO-67 Ru50, and UiO-67 Ru50-Mn10 (from left to right). The colour code of the MOFs is as follows: black = UiO-67, green = UiO-67 Mn10, orange = UiO-67 Ru50, and brown = UiO-67 Ru50-Mn10. | ||
The TEM images of UiO-67 Ru50 and UiO-67 Ru50-Mn10 (Fig. 1c) reveal that both samples exhibit a well-defined octahedral crystalline morphology, with crystal sizes ranging from approximately 1 to 2 μm. Notably, no significant morphological changes are observed when compared to their UiO-67 and UiO-67 Mn10 counterparts. However, a pronounced difference in crystal size is evident: UiO-67 and UiO-67 Mn10 crystals are considerably smaller, typically ranging from 200 to 500 nm. This variation in crystal size is likely attributed to differences in reaction kinetics between Zr(IV) and the H2bpydc linker vs. the [Ru(H2bpydc)(bpy)2]Cl2 complex. Additionally, factors such as linker acidity, solubility, and geometry, which are altered upon metalation, can significantly affect the nucleation and growth processes during synthesis, ultimately influencing the final crystal size.29 Notably, in both cases, post-synthetic modification (PSM) for Mn incorporation does not result in any observable changes in crystal size or shape, indicating that the overall framework integrity remains unaffected.
High-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) images together with corresponding energy dispersive X-ray (EDX) element mappings of UiO-67 Ru50-Mn10 are shown in Fig. 3 and S6, S7, SI, for UiO-67 Ru50, respectively. The HAADF-STEM and EDX images clearly show the presence of elements Zr, C, N, O, Cl, and Ru, which are distributed throughout the entire structure of each MOF. The signals for Mn were detected in UiO-67 Ru50-Mn10. Unlike C, N, O, and Zr in both the framework, the Ru, Cl in both the framework, and Mn metals in UiO-67 Ru50-Mn10 appear to be more spatially isolated. This observation may be attributed either to the separation of individual metal-complex centers within the linker motif, as enforced by the framework structure, or to the relatively low composition of these elements in the overall material. Notably, the EDX spectra of these MOFs (Fig. S6, S7 and Table S2, SI) confirm the presence of Ru and Cl signals; however, the Mn signal observed in UiO-67 Ru50-Mn10 arises from the overlap of the Mn Kβ line with the Fe Kα line, where Fe originates from stray electrons scattered on the TEM column made of iron. Consequently, the Mn elemental map should largely be regarded as an artifact. The experimentally determined average Zr/Ru ratios for UiO-67 Ru50 and UiO-67 Ru50-Mn10 are ∼1.12–6.35 and ∼11.4, respectively. These values deviate significantly from the expected stoichiometric ratio of Zr/Ru = 2, according to the ideal formulas: UiO-67 Ru50 ([Zr6O4(OH)4(bpydc)3]·3[Ru(bpy)2(bpydc)]Cl2) and UiO-67 Ru50-Mn10 ([Zr6O4(OH)4(bpydc)2.4]·3[Ru(bpy)2(bpydc)]Cl2·0.60[Mn(bpy)(bpydc)Cl2]). This discrepancy suggests that the distribution of Ru within the framework is random and that both MOFs deviate from their idealized formulas, either due to residual solvent molecules from the synthesis or the presence of linker vacancies.
The chemical compositions of UiO-67 and UiO-67-Rux were determined by 1H-NMR measurements in DMSO-d6 by digesting them in DCl/D2O (see SI page 8–9 for detailed calculations). A previous report had suggested that benzoic acid is commonly entrapped within the pore of the MOF and, consequently, cannot be completely removed during the washing process.30 In our case, the 1H-NMR spectrum displayed similar signals corresponding to benzoate, while the presence of a negligible amount of formate (HCOO−) is there, although formate was not used in the initial synthesis, this molecule was produced due to the decomposition of DMF during the solvothermal reaction (Fig. S8).30 These molecules likely participate in the Zr-cluster assemblies similar to some Zr-MOFs, where the modulators were identified in the crystal structures.30,31 As the formate peak is negligible it is ignored for the current analysis. Based on the integration of the signals of BA, including the bpydc, the chemical formula of UiO-67 was estimated to be [Zr6O4(OH)4(bpydc)5.82(BA)0.36] (Table S3). In UiO-67 Ru50 and UiO-67 Ru10, the [Ru(bpy)2(bpydc)]Cl2 moiety can be characterized by 1H NMR, and analysis was possible because it remains intact under these MOF digestion conditions (Fig. S8). Based on the integration of the proton resonances for [Ru(bpy)2(bpydc)]Cl2 in UiO-67 Ru50, and UiO-67 Ru10 the chemical formula was estimated to be [Zr6O4(OH)4(bpydc)4.724(BA)1.13]·0.7[Ru(bpy)2(bpydc)]Cl2, and [Zr6O4(OH)4(bpydc)5.48(BA)0.71]·0.16[Ru(bpy)2(bpydc)]Cl2, respectively, and the degree of Ru modification in UiO-67 Rux MOFs is 13% and 3%, respectively, indicating that complete incorporation of the Ru moiety did not take place. Unfortunately, the quantification of Mn quantification via NMR is not possible, as Mn2+ is paramagnetic, resulting in a broad signal as observed in UiO-67 Ru10-Mn10 (Fig. S8).
X-ray photoelectron spectroscopy (XPS) was used to determine the precise elemental composition, the integrity of the Ru and Mn complexes, and their electronic states within the MOFs (Fig. 4a). All shifts for the samples were corrected by normalizing the C (1s) binding energy to 284.8 eV (Fig. S9a). In all the MOFs, including C 1s, all characteristic peaks for Zr 3d at 180.95–187.05 eV (Fig. 4b), N 1s at 395.90–402.30 eV (Fig. S9b), and O 1s at 528.00–535.50 eV32,33 (Fig. S9c) were observed, corresponding to the primary backbone (linker and SBU), and notably, slight changes are observed in UiO-67-Ru50, and UiO-67 Ru50-Mn10 MOFs for the local environment exerted by the Ru and Mn molecular moieties. For instance, the binding energy of N 1s in UiO-67 is 398.2 eV, which is attributed to N in bpydc2− (Fig. S9b). The electron density of nitrogen at this region was reduced, followed by the formation of coordination interactions between bpydc2− and the Ru2+ and Mn2+ species in UiO-67 Ru50 and UiO-67 Ru50-Mn10, leading to distinct N 1s peaks at 398.6 eV and 399.00 eV, respectively. The change in the peak of N 1s to higher binding energy indicates that the N atom on the bipyridine (bpydc2−) is coordinated with the Ru ion in UiO-67 Ru50 and Ru and Mn ions, which reduces the electron density at the N atom.34,35 Additionally, in contrast to UiO-67, for both UIO-67 Ru50 and UIO-67 Ru50-Mn10, two peaks are apparent in the Ru regions at 285.37 and 281.12 eV, which are assigned to Ru2+ 3d3/2 and 3d5/2, respectively (Fig. S9a) which almost overlaps with the C 1s signal (Fig. 4a). Fig. 4c shows the respective peaks at around 462.12 eV assigned to the Ru 2p3/2 region and, which are in good agreement with the pattern of divalent ruthenium, Ru2+.12 No other valence state peaks, such as Ru3+ or Ru4+, were detected. The Mn 2p spectra (Fig. 4d) observed in UiO-67 Ru50-Mn10 contain two main peaks centred at 640.75 eV (Mn 2p3/2) and 652.5 eV (Mn 2p1/2), while no Mn3+ and Mn4+ species are observed, which are generally observed at higher energies than the Mn2+ species. Additionally, the spectra consist of satellite peaks with considerable intensity at ∼5 eV higher binding energy (645.10 eV) compared to that of the corresponding main Mn 2p3/2 peak. These spectral features reflect that the valence of the central manganese ion in the UiO-67 Ru50-Mn10 is +2 (ref. 36 and 37) and [Mn(bpy)(bpydc)Cl2] remained stable during the PSM process. It should be noted that the Cl 2p peaks in UiO-67 Ru50 and UiO-67 Ru50-Mn10 MOFs at around 195.25–201.62 eV exist (Fig. S9d), representing Cl anion as a counter anion.
Despite the presence of the Ru peak being detected in UiO-67 Ru50-Mn10, Ru was not taken into account for estimating the Ru/Mn ratio due to the overlap with C and a weak signal. Therefore, the Zr/Mn ratio was considered instead, which was found to be 7.73 in UiO-67-Ru50-Mn10. Combined with the Zr
:
Ru ratio of 8.57 obtained from NMR analysis of UiO-67-Ru50 (assuming no leaching occurred during the post-synthetic modification, PSM), these measurements allowed the estimated atomic ratio of Zr
:
Ru
:
Mn to be calculated as 1
:
0.117
:
0.129. Based on this, the proposed chemical formula of UiO-67 Ru50-Mn10 is: [Zr6O4(OH)4(bpydc)3.944(BA)1.13]·0.70[Ru(bpy)2(bpydc)]Cl2·0.78[Mn(bpy)(bpydc)Cl2]. In accordance with the above formulation, the molar Ru/Mn ratio is nearly 0.89. This ratio is expected to be reflected in the high resolution-continuum graphite furnace atomic absorption spectrometry (HR-CS-GFAAS) and total X-ray fluorescence spectrometry (TXRF) measurements of the MOF (see SI for details and Fig. S10). Indeed, the element analysis in Table S5 confirms that the Ru/Mn molar ratio is ∼1.02, providing excellent corroboration of the structural formulation.
:
H2O (4
:
1 v/v) under an air atmosphere. The reaction setup utilized a 3D-printed modular photoreactor equipped with a 460 nm LED light source (800–1250 mW) operating at a current of 0.7 A and a voltage of 4 V.27,30 The reaction progress was initially monitored under radiation for 36 h (Fig. S11), and the imine product N-benzylidene-1-phenylmethanamine formed after 24 h for each set of reactions were quantified using 1H NMR spectroscopy, with 1,3,5-trioxane employed as an internal standard (see SI page 17 for details and Fig. S12), and the yields (%) calculated for the conversion to N-benzylidene-1-phenylmethanamine are listed in Table 2.
| Samples | Calculated formula of the MOF [Zr6O4(OH)4(bpydc)x(BA)y] |
|---|---|
| a The ratio of Ru and Mn in UiO-67 Ru50-Mn10 MOF was calculated from the combination of 1H NMR and XPS data in Tables S3 and S4. | |
| UiO-67 | [Zr6O4(OH)4(bpydc)5.82(BA)0.36] |
| UiO-67 Ru50 | [Zr6O4(OH)4(bpydc)4.724(BA)1.13]·0.70[Ru(bpy)2(bpydc)]Cl2 |
| UiO-67 Ru10 | [Zr6O4(OH)4(bpydc)5.48(BA)0.71]·0.16[Ru(bpy)2(bpydc)]Cl2 |
| UiO-67 Ru50-Mn10 | [Zr6O4(OH)4(bpydc)3.944(BA)1.13]·0.70[Ru(bpy)2(bpydc)]Cl2·0.78[Mn(bpy)(bpydc)Cl2] |
| # | Catalysts | Conditions | Yieldb (%) | Selectivityb (%) | TONc | TOFc (h−1) | Rate (μmol gMOF−1 h−1) |
|---|---|---|---|---|---|---|---|
a Reaction condition: MOF (1 mg), CH3CN : H2O (4 mL, 4 : 1 v/v) or pure CH3CN, benzylamine (80 μL, 0.734 mmol), (λ = 460 nm LED, 24 or 6 h), air (1 atm).b Determined by 1H NMR using 1,3,5-trioxane as the internal standard.c For TON and TOF calculation Ru content was calculated from their respective MOF (1 mg) as per structure formula listed in Table 1. For homogeneous conditions: [Ru] = [Ru(bpy)2(bpydc)]Cl2, [Mn] = [Mn(bpy)2Cl2]·H2O, 0.28 μmole of [Ru] was used. |
|||||||
| 1 | UiO-67 | CH3CN/H2O 6 h | 1.0 | 81 | — | — | 157 |
| 2 | UiO-67 Mn10 | CH3CN/H2O 6 h | 0.2 | 76 | — | — | 28 |
| 3 | UiO-67 Ru50 | CH3CN/H2O 24 h | 27.6 | 75 | 358 | 14.9 | 4218 |
| 4 | UiO-67 Ru50-Mn10 | CH3CN/H2O 24 h | 45.1 | 85 | 634 | 26.4 | 6895 |
| 5 | UiO-67 Ru50-Mn10 | CH3CN/H2O 24 h, dark | — | — | — | — | — |
| 6 | No catalyst | CH3CN/H2O 6 h | — | — | — | — | — |
| 7 | UiO-67 | CH3CN, 24 h | 1.4 | 77 | — | — | 213 |
| 8 | UiO-67 Mn10 | CH3CN, 24 h | 0.7 | 71 | — | — | 101 |
| 9 | UiO-67 Ru50 | CH3CN, 24 h | 11.9 | 93 | 154 | 6.4 | 1822 |
| 10 | UiO-67 Ru50-Mn10 | CH3CN, 24 h | 14.6 | 94 | 205 | 8.5 | 2229 |
| 11 | UiO-67 Ru50-Mn10 | CH3CN/H2O 24 h, Ar | — | — | — | — | — |
| 12 | UiO-67 Ru10 | CH3CN, 24 h | 4.7 | 80 | 240 | 10.0 | 721 |
| 13 | UiO-67 Ru10-Mn10 | CH3CN, 24 h | 3.7 | 79 | 193 | 8.1 | 564 |
| 14 | [Ru] | CH3CN/H2O 24 h | 15.7 | 88 | 206 | 8.6 | — |
| 15 | [Ru] + [Mn] | CH3CN/H2O 24 h | 29.1 | 93 | 382 | 15.9 | — |
| 16 | [Ru] | CH3CN, 24 h | 49.5 | 94 | 648 | 27.8 | — |
| 17 | [Ru] + [Mn] | CH3CN, 24 h | 58.2 | 99 | 763 | 31.0 | — |
The control experiments under dark conditions, in absence of any catalyst or MOF are listed in Table 2 entries 5 and 6 and yielded no detectable oxidation products, confirming the necessity of both light and the MOF catalyst for photocatalytic activity. Among the tested materials, UiO-67-Ru50 and UiO-67 Ru50-Mn10 exhibited significant catalytic activity for the oxidation of benzylamine to the corresponding imine (N-benzylidene-1-phenylmethanamine) with yields of 27.6% (selectivity 75%) and 45.1% (selectivity 85%), respectively. Notably, no significant imine products under the light-irradiation were observed for the other two counterparts, UiO-67 (yield = 1%) and UiO-67 Mn10 (yield = 0.2%), indicating that both light and the Ru moiety are essential components for catalytic activity. In particular and according to the kinetic study, UiO-67 Ru50-Mn10 showed superior fast performance with a rate of 6895 μmol gMOF−1 h−1. This rate is enhanced compared to UiO-67 Ru50 (4218 μmol gMOF−1 h−1) (Fig. 5a). The enhancement observed upon Mn2+ incorporation can be attributed to an improved charge transfer efficiency and the presence of additional catalytic sites facilitated by Mn2+ within the framework.
The influence of the solvent environment was tested via additional experiments in pure acetonitrile (CH3CN). While the overall yield of imine products in photocatalysis with the MOFs was lower in pure CH3CN, the observed trend in photocatalytic performance among the different MOFs matches the trend in the solvent mixture CH3CN
:
H2O (4
:
1 v/v). Specifically, UiO-67 Ru50-Mn10 with a yield of 14.6% (selectivity 94%) and rate of 2229 μmol gMOF−1 h−1 continued to outperform UiO-67 Ru (yield: 11.9%, with selectivity 93% and rate: 1822 μmol gMOF−1 h−1), highlighting the robustness of its superior activity regardless of the solvent conditions (Fig. 5a). Interestingly, compared to the CH3CN/H2O mixture, the oxidation reaction of benzylamine in CH3CN alone proceeded with higher selectivity, irrespective of the MOF photocatalysts. In aqueous media, a photocatalytic system can form hydroxyl radicals, which can oxidise the substrate and product indiscriminately, thereby reducing the selectivity of the reaction.38
Furthermore, the effect of the Ru loading was examined. At low Ru concentrations, only minimal product formation was observed, with UiO-67-Ru10 yielding 4.7% and UiO-67 Ru10-Mn10 yielding 3.7%. No consistent trend was observed at this range (Table 2), further underscoring the pivotal role of the Ru moiety as the primary photosensitizing centre. These findings highlight the necessity of an optimized Ru loading to achieve effective photocatalysis, emphasizing that suboptimal concentrations result in diminished activity, likely due to insufficient active sites for efficient light absorption. Atmospheric conditions were also found to be critical for the reaction. No product formation was observed when the reaction was conducted under an argon atmosphere (Table 2 entry 11), confirming the requirement of molecular oxygen as the terminal oxidant in the photocatalytic cycle.
To assess the role of the MOF-assembly, the homogeneous system was tested, using the molecular analogues [Ru(bpy)2(bpydc)]Cl2 ([Ru]) and [Mn(bpy)2Cl2]·H2O ([Mn]) in respective combinations in CH3CN/H2O (v/v 4
:
1) and pure CH3CN. As shown in Fig. 5b and Table 2, both molecular systems exhibit similar activity trends, with [Ru] alone (TON = 206) < [Ru] + [Mn] (TON = 382). However, their corresponding MOF systems, UiO-67-Ru50 and UiO-67-Ru50-Mn10, display approximately 1.6-fold higher TONs (358 and 634, respectively) under identical conditions, highlighting the enhanced performance imparted by the heterogeneous framework.
Interestingly, under pure CH3CN conditions, the homogeneous systems exhibited a strong increase in TON (643 for [Ru] alone and 763 for [Ru] + [Mn]). A kinetic analysis also revealed that the reaction plateau is reached more quickly in CH3CN than in the CH3CN/H2O mixture (Fig. S13). This trend is opposite to that observed for their MOF counterparts (Table 2 and Fig. 5b) and might be attributed to differences in reaction pathways influenced by the solvent and the 3D-assembly in the MOF vs. the diffusion-controlled process in homogeneous conditions.39,40
It is interesting to note that, similar to the MOF experiments, the combination of [Ru] and [Mn] in homogeneous solution outperforms [Ru] alone under all tested conditions, suggesting a synergistic interaction between the Ru and Mn components that is preserved even outside of the MOF matrix. More details of the proposed reaction pathways, including electron transfer between the Ru-photosensitizer and the Mn-unit, are discussed vide infra.
:
1) solvent mixture for both the homogeneous [Ru] system and the UiO-67 Ru50 catalyst (Fig. 6a and b). In contrast, for UiO-67 Ru50-Mn10 and the homogenous [Ru] + [Mn] systems, although Im1 was identified, the transient intermediate Im2 was either absent (UiO-67 Ru50-Mn10) or detected inconsistently ([Ru] + [Mn]), as indicated by the 1H NMR spectra (Fig. 6b and S14–S17). This observation suggests that the hemiaminal species undergoes more rapid decay in the presence of Mn2+-incorporated catalysts, particularly UiO-67 Ru50-Mn10, than in UiO-67 Ru50 or the homogeneous [Ru] system. The incorporation of Mn2+ likely accelerates the overall reaction rate by promoting a faster conversion of N-benzyl-1-phenylmethanediamine to the final imine product, N-benzylidene-1-phenylmethanamine. This may occur via enhanced electron or proton transfer steps, facilitating more efficient ammonia elimination.
In pure CH3CN, no such intermediates were observed for either the MOF-based or homogeneous systems (Fig. 6c and S18–S21), suggesting that an alternative reaction mechanism predominates under non-aqueous conditions. Specifically, energy transfer from the 3MLCT (triplet metal-to-ligand charge transfer) state to oxygen, forming the reactive oxygen species 1O2 can yield to an alternative reaction pathway, followed by rapid condensation of Im1 and dehydration of Im2, which is likely operative as discussed vide infra.
These findings highlight the critical absence or presence of water in modulating the reaction mechanism, modulating both the efficiency and the turnover frequency of the MOF-based catalysts. To further substantiate our observations, we compared the photocatalytic performance of UiO-67 Ru50-Mn10 with other MOF-based photocatalysts reported previously (Table 3). Since experimental parameters such as initial substrate concentration, catalyst loading, reaction time, and solvent systems vary significantly across studies, we adopted the rate of oxidative coupling (μmol gMOF−1 h−1) in CH3CN as a basis for comparison. Compared to benzene dicarboxylate-based and amine functionalized MOFs: UiO-66, UiO-66 NH2, and m-NH2-MIL-125, n-NH2-MIL-125 (Table 3 entries 1–3, and 6), our UiO-67 Ru50-Mn10 MOF exhibits a rate of 2229 μmol gMOF−1 h−1, which is nearly 16-, 8-, 5-, and 2-fold higher, respectively, under similar solvent conditions. Notably, the rate is quite relatable to the Ru(bpy)3@MIL-125 system (Table 3 entry 5). Furthermore, many of the reference MOFs, such as Ti-PMOF-DMA, Zr-NDI-PCOOH, and UiO-68-BT (Table 3 entries 4, 8, and 9), employ novel linker systems and often involve higher synthetic complexity, which may also contribute to their enhanced activity. It is important to note, however, that other experimental factors, particularly the light source characteristics (power and wavelength), were not normalised across these studies, and such variations may exert a significant influence on catalytic performance. Taking this into account, the activity of UiO-67 Ru50-Mn10 can be considered moderate when compared to those MOFs.
| # | Catalysts | Solvent | Catalyst/benzylamine | Light source, time | Conv. (%) | Selectivity (%) | Yield (%) | Rate (μmol gMOF−1 h−1) |
|---|---|---|---|---|---|---|---|---|
| a The oxidative coupling rate (μmol gMOF−1 h−1) for MOFs is calculated based on their respective catalyst/benzylamine ratio, reaction time and N-benzylidene-1-phenylmethanamine yield reported in the literature. | ||||||||
| 1 | UiO-66 (ref. 41) | CH3CN | 15 mg/0.1 mmol | 300 W Xe lamp (no filter), 10 h | 42.0 | >99 | 42 | 140a |
| 2 | n-NH2-MIL-125 (ref. 42) | CH3CN | 10 mg/0.2 mmol | 300 W Xe lamp (no filter), 9 h | 98.5 | 99 | 97.5 | 1063 |
| 3 | m-NH2-MIL-125 (ref. 42) | CH3CN | 10 mg/0.2 mmol | 300 W Xe lamp (no filter), 12 h | 62.8 | 92.6 | 58.15 | 475 |
| 4 | Ti-PMOF-DMA43 | CH3CN | 5 mg/0.3 mmol | 623 ± 8 nm, 0.5 h | 94.0 | 88 | 82.7 | 49 620a |
| 5 | Ru(bpy)3@MIL-125 (ref. 44) | CH3CN | 5 mg/0.1 mmol | Visible light (>440 nm), 3 h | 75 | >99 | 74.2 | 2473a |
| 6 | UiO-66-NH2 (ref. 45) | CH3CN | 15 mg/0.1 mmol | 300 W Xe lamp (no filter), 10 h | 83.0 | >99 | 82.2 | 274 |
| 7 | LTG-NiRu46 | DMF | 1 mmol%/0.5 mmol | 300 W Xe lamp (420–780 nm), 1 h | >99 | >99 | 99% | — |
| 8 | Zr-NDI-PCOOH47 | CH3CN | 10 mg/0.4 mmol | 300 W Xe lamp (full wavelength), 0.75 h | 90 | 100 | 90 | 24 000a |
| 9 | UiO-68-BT48 | CH3CN | 5 mg/0.3 mmol | 415 nm (3 W × 4), 0.42 h | 96 | 99 | 95 | 67 857a |
| 10 | This work (UiO-67 Ru50-Mn10) | CH3CN/H2O | 1 mg/0.7 mmol | 460 nm (LED 800–1250 mW), 24 h | 53 | 85 | 45.1 | 6895 |
| CH3CN | 15.5 | 94 | 14.6 | 2229 | ||||
:
1), the recovered catalyst yielded only negligible amounts of N-benzylidene-1-phenylmethanamine in the second cycle. Such structural collapse of MOFs in aqueous environments is a commonly encountered issue, which may occur either through chemical decomposition or under light irradiation. The dissolution can arise from competitive coordination of ˙OH radicals or amine substrates with the Zr-SBUs, leading to framework breakdown.38,49
In contrast, UiO-67 Ru50-Mn10 exhibited recyclability in pure CH3CN (Fig. S23). In this case, the solid MOF could be separated from the reaction medium by centrifugation, washed with CH3CN (twice), and reused for further photocatalytic cycles with fresh benzylamine. Although the oxidative coupling of benzylamine in pure CH3CN proceeded with lower efficiency (14.6% yield, 2229 μmol gMOF−1 h−1), corresponding to nearly three times lower activity compared to the CH3CN/H2O system, the catalyst maintained stable performance over multiple cycles without significant loss of photocatalytic activity (Fig. 7).
:
1 v/v) solution by photoluminescence (PL) spectroscopy in the presence and absence of [Mn] counterparts under both air and Ar atmospheres. The 3MLCT emission of the photosensitizer at 640 nm and the characteristic 1O2 emission at 1277 nm were monitored (Fig. 8a and b). The assignment of the 1O2 emission was confirmed by comparison with the PL spectra of a standard [Ru(bpy)3]2+ solution in CD3CN (Fig. 8b). Consistent with the behaviour of [Ru(bpy)3]2+ (Fig. S24), the 3MLCT emission at 640 nm was significantly quenched under air relative to Ar, by ∼50% for [Ru] alone and ∼30% for the [Ru] + [Mn] system (Fig. 8a). Interestingly, 1O2 emission at 1277 nm was detected for [Ru] alone, suggesting energy transfer (EnT) from the 3MLCT state to ground-state 3O2. Nevertheless, an electron transfer (ET) pathway from the 1MLCT state cannot be excluded, since in the [Ru] + [Mn] system the 3MLCT emission was quenched (by ∼30%) without a corresponding increase in 1O2 generation (Fig. 8b). Additionally, [Mn] itself was found to quench PL of [Ru] by ∼50% even under Ar atmosphere, highlighting its critical role in facilitating ET processes within the [Ru] + [Mn] system under both aerobic and anaerobic conditions.
Therefore, only photoluminescence (PL) spectra and time-resolved PL measurements were conducted on the MOFs to evaluate the charge separation efficiency of photo-excited electron–hole pairs (see SI for experimental details), and all measurements concerning the charge transfer between photoexcited Ru-photosensitizer and Mn were performed under an inert Ar atmosphere. As depicted in Fig. 8c, the MOF sample UiO-67-Ru50, containing only the [Ru(bpy)2(bpydc)]Cl2 photosensitizer, exhibited strong phosphorescence emissions centred at 639 nm in CH3CN and 648 nm in H2O upon photoexcitation at 450 nm. In contrast, the phosphorescence intensity of UiO-67-Ru50-Mn10, which incorporates both the PS and [Mn(bpy)(bpydc)Cl2] redox-active unit, was significantly reduced in both of these solvents, and consistent with the observations made for the homogeneous [Ru] + [Mn] models.
Time-resolved PL measurements are shown in Fig. 8d and summarized in Table 4, with detailed fitting parameters provided in Table S7. In CH3CN, the 3MLCT lifetime of the Ru-based photosensitizer decreased from 246 ns in UiO-67 Ru50 to 62 ns in UiO-67 Ru50-Mn10. Similarly, in H2O, the lifetime was reduced from 112 ns to 47 ns, as summarized in Table 4. Both of these results demonstrate that the quenching of PS emission in UiO-67 Ru50-Mn10 arises from accelerated decay of the 3MLCT excited state, driven by efficient, solvent-independent interaction and likely reductive electron transfer between the [RuII]* and [MnII] complexes within the MOF framework. However, various studies suggest that, in the presence of external electron acceptors like methyl viologen or O2, an oxidative quenching pathway from [RuII]* to [RuIII] is followed by electron transfer (ET) from the donor Mn2+ in homogeneous systems.22,52–54
| Compounds | 1MLCT absorption | Optical gap | 3MLCT emission | ||
|---|---|---|---|---|---|
| λmax (nm) | Eg = EHOMO–LUMO (eV) | λ (nm) | τav (ns) | ||
| a Absorption spectra acquired from the diffuse reflectance spectroscopy of the MOF in the solid state.b Optical energy gaps (Eg) of the solids were estimated from the Kubelka Munk functions. | |||||
| [Ru(bpy)2(bpydc)]Cl2 | CH3CN | 460 | 2.45 | 615 | 750 |
| H2O | 450 | — | 670 | 23 | |
| UiO-67 Ru50 | CH3CN | 446a | 2.10b | 639 | 246 |
| H2O | 648 | 112 | |||
| UiO-67 Ru50-Mn10 | CH3CN | 444a | 2.10b | 654 | 62 |
| H2O | 661 | 47 | |||
To evaluate the influence of solvent environment and framework effects, steady-state and time-resolved PL spectroscopy of the [Ru] complex were performed in CH3CN and H2O under Ar atmosphere and compared with the corresponding measurements for the MOFs. The homogeneous [Ru] complex in CH3CN exhibits phosphorescence peaks centred at 615 nm and 670 nm in CH3CN and H2O, respectively, with corresponding excited-state (3MLCT) lifetimes of 750 ns and 23 ns (Fig. S27 and Table 4). Interestingly, both MOF systems in CH3CN exhibited significantly shorter 3MLCT lifetimes relative to the homogeneous Ru-complex, implying the impact of the MOF platform. However, the homogeneous complex showed a much faster decay in H2O, indicating its lower stability of the 3MLCT state in aqueous media compared to the MOF systems. These findings highlight two key points: (i) solvent molecules significantly influence the 3MLCT state lifetimes, and (ii) the MOF framework provides enhanced stability and lifetime control for the photosensitizer in aqueous environments.
Furthermore, cyclic voltammetry (CV) experiments were conducted on the individual complexes in CH3CN under both Ar and air atmospheres to gain further insight into the electron transfer processes. In the CV profile of [Ru(bpy)2(bpydc)]Cl2 (Fig. 9a and S28a), three distinct reduction peaks were observed at −1.60 V, −1.90 V, and −2.13 V vs. Fc/Fc+, corresponding to the successive reductions of the ligand in Ru-based photosensitizer (PS), as summarized vs. NHE in Table S8.52,55 An oxidation peak attributed to the Ru2+/Ru3+ redox couple (HOMO level) was also detected at +0.84 V vs. Fc/Fc+ (Fig. 9b).55 The estimated HOMO and LUMO energy levels are to be +1.53 V, and −0.91 V vs. NHE, respectively (Fig. 9c). For [Mn(bpy)2Cl2]·H2O, a well-defined oxidation peak corresponding to the Mn2+ to Mn3+ transition appeared at +0.41 V vs. Fc/Fc+ (+1.10 V vs. NHE) (Fig. S28b and 9b), which is consistent with previously reported values.52,54,55 Notably, this oxidation potential +1.10 V vs. NHE is slightly less positive than the estimated HOMO level (+1.53 V vs. NHE) of [Ru(bpy)2(bpydc)]Cl2, indicating a thermodynamically favourable pathway for electron transfer from Mn2+ to the oxidized Ru3+ species. Under an O2 atmosphere, an additional reduction peak attributable to the O2/O2˙− couple at −1.17 vs. Fc/Fc+ (−0.48 V vs. NHE)56,57 was observed in the CV of [Ru(bpy)2(bpydc)]Cl2 (Fig. 9a and S28c). The LUMO level of the Ru-complex (−0.91 V vs. NHE) lies higher in energy than the O2/O2˙− redox couple (−0.48 V vs. NHE), providing a driving force for electron transfer from the excited 1MLCT Ru-PS to molecular oxygen (Fig. 9c). These observations suggest that electron transfer from Ru-PS to O2, followed by Mn2+ to the oxidized Ru centre, or vice versa, is both energetically feasible.
As the ET processes from the excited state are expected to be kinetically fast, we conducted nanosecond transient absorption spectroscopy of the [Ru] complex in CH3CN/H2O in the presence and absence of [Mn], and under aerobic and anaerobic conditions. The spectra shown in Fig. 10 and S25 were recorded with a delay of 100 ns after the laser pulse (λ = 450 nm). For the [Ru] complex alone in aqueous environment under Ar, the spectrum showed a ground-state bleach (GSB) at 450 nm and excited-state absorption at around 400 nm, along with two new positive absorption features centred at around 550 nm and around 800 nm, corresponding to reduced [Ru]˙+ and solvated electron (esolv), respectively.58–60 Notably, these species are the common photolyzed intermediates that originate in an aqueous environment and lead to decomposition.58 Interestingly, when the spectra were acquired in the presence of [Mn] under Ar, the absorption band centred at 550 nm increased, accompanied by a decrease in GS bleach. This clearly indicates an increase in the formation of a reduced PS ([Ru]˙+), confirming electron transfer to the PS, i.e., the excited state of [Ru] is reductively quenched. It is further notable that when both systems ([Ru] alone and [Ru] + [Mn]) were purged with air, a decrease in the absorption band in this region was observed. This effect was more pronounced in the [Ru] + [Mn] system, irrespective of the sequence of addition of [Mn] and air. These results suggest that O2 acts as an electron acceptor, reverting the reduced PS to its ground state. This observation not only supports the validity of the initial reductive quenching mechanism but also illustrates the second step of the electron transfer process occurring between light-driven and dark reactions. Collectively, the results indicate that the PS is quenched by [Mn] via a reductive quenching mechanism, with no clear evidence of oxidative quenching.
Additionally, in the stimulated 3MLCT emission (SE) region around 660 nm,61 a significant negative bleaching effect was observed under aerobic conditions, more prominently in the [Ru] + [Mn] system, supporting the partial energy transfer mechanism as well in the photocatalytic systems.
Electrochemical study and ns-transient absorption spectroscopy confirm that electron transfer thermodynamics are evident under homogeneous conditions. These homogeneous studies provide essential reference points for interpreting the corresponding behaviour of the components in the MOF framework. The integration of Ru- and Mn-complexes into a unified UiO-67 framework (UiO-67 Ru50-Mn10) retains this synergistic character, as shown by phosphorescence quenching experiments (Fig. 8c, d and Table 4) by comparing between UiO-67 Ru50 and UiO-67 Ru50-Mn10. However, a comparison between homogeneous vs. MOF systems clearly highlights the contribution of the MOF (Table 4). The spatial proximity of Ru and Mn within the framework facilitates more efficient electron transfer than in homogeneous [Ru] + [Mn] systems, while the rigid architecture of the MOF enhances the stability of the photoactive units compared to homogeneous conditions, particularly in a CH3CN/H2O.
Although the 3MLCT states of Ru-complexes are not energetically suitable for O2˙− formation,39 they can undergo energy transfer with ambient 3O2 to produce 1O2.62 This EnT mechanism is more prominent in CH3CN and homogeneous systems than in MOFs.40
Spectroscopic and photocatalytic results and intermediate identification across solvent environments suggest both electron transfer (ET) and energy transfer (EnT) pathways can operate in UiO-67 Ru50-Mn10 to convert benzylamine and O2 into N-benzylidene-1-phenylmethanamine (Fig. 11). In the ET pathway (Fig. 11 and S14–S21): photoexcitation converts [RuII] to [RuII]* (1MLCT), which is reduced by [MnII] to generate [Ru]˙+ and becomes [MnIII]. O2 accepts an electron to [Ru]˙+ to regenerate [RuII], by becoming O2˙−. [MnIII] (E° = +1.10 V vs. NHE) oxidizes benzylamine (E° = +0.76 V vs. NHE) to benzylamine radical (PhCH2NH2˙+), which reacts with O2˙− to form phenylmethanimine (Im1) and H2O2. In the EnT pathway (Fig. 11, bottom): 3O2 formed via 3MLCT of [RuII]* reacts with benzylamine to yield the same intermediates. Formation of H2O2 through 1O2 and O2˙− is well established and was also confirmed for the UiO-67 Ru50-Mn10 MOF using the TiOSO4 method63,64 (see SI and Fig. S29). Finally, phenylmethanimine, formed via both pathways, undergoes a condensation reaction to generate the hemiaminal intermediate (Im2), which subsequently eliminates NH3 to yield the final product. It is hypothesised that the rapid decay of intermediates in pure CH3CN prevents their detection in both the UiO-67 Ru50-Mn10 MOF and the homogeneous systems. In contrast, in CH3CN/H2O the decay of intermediates is relatively slower, enabling their observation (Fig. 6 and S14–S21).
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| Fig. 11 Oxidative amine coupling reaction mechanisms through the electron transfer (ET) and energy transfer (EnT) pathways. | ||
UiO-67 Ru50-Mn10 exhibits significantly enhanced photocatalytic performance, showing ∼3.1, 1.65, and ∼1.8-fold higher TON than [Ru] alone, [Ru] + [Mn], and UiO-67 Ru50, respectively, in CH3CN/H2O. The superior photocatalytic activity of UiO-67 Ru50-Mn10 over UiO-67 Ru50, homogenous [Ru] alone, and [Ru] + [Mn] systems in CH3CN/H2O reflects a prominent role of the ET pathways and the role of Mn in facilitating ET for the primary one-electron oxidation of benzylamine. This role of manganese as an electron transfer mediator was previously reported.65
While the homogeneous system in CH3CN shows superior activity than MOFs due to a more efficient EnT via 3MLCT, Mn remains critical in both solvent systems for promoting oxidation, thereby enhancing overall reaction kinetics in both [Ru] + [Mn] and UiO-67 Ru50-Mn10 compared to systems without Mn.
:
1) solvent system plays a critical role by improving the polarity of the reaction medium, which collectively facilitates faster and more efficient charge separation and electron transfer. While homogeneous systems benefit more in pure CH3CN due to faster energy transfer (EnT), the MOF-based catalyst performs best in the mixed solvent due to stabilized intermediates and enhanced electron transfer pathways (ET). Spectroscopic and electrochemical studies further confirm enhanced photostability and charge dynamics in the MOF system. The MOF system provides all advantages of MOFs, being a dispersible, highly porous materials that maintains the molecular functions of its building blocks and has the potential for easy recyclability. The cooperative interaction between Ru and Mn centres within the robust MOF framework provides a blueprint for designing efficient, photocatalysts using earth-abundant catalysts for sustainable oxidative chemistry.
:
1 equiv. of MnCl2·4H2O and 2,2′-bipyridine (bpy). The resulting suspension was stirred under an argon atmosphere at reflux temperature for 4 h to facilitate coordination of Mn(II) to the Ru-functionalized MOF framework. Upon completion, the solid product was isolated by centrifugation, thoroughly washed with ethanol to remove any unbound metal species or ligands, and dried under vacuum before use.
:
H2O (4
:
1 v/v) solvent mixture in an 8 mL vial and ultrasonicated for 5 minutes to ensure homogeneous dispersion. Subsequently, 0.734 mmol of benzylamine (80 μL) was added using a micropipette. The reaction mixture was kept in the dark overnight at ambient conditions. After the dark period, the vial was irradiated using a 460 nm LED light source (Azula Photoreactor, λ = 460 nm, 800–1250 mW) operating at 0.7 A and 4 V under continuous stirring.For control experiments, the same procedure was followed by replacing the MOF catalyst with either (1) a combination of 0.28 μmol of [Ru(bpydc)(bpy)2]Cl2 and 0.14 μmol of [Mn(bpy)2Cl2]H2O, or (2) 0.28 μmol of [Ru(bpydc)(bpy)2]Cl2 (0.204 mg) alone in 4 mL of CH3CN with 0.734 mmol of benzylamine (80 μL).
At selected time intervals (initial, 0 h (dark), 1–24 h for kinetics; and 24 h for final yield), 240 μL aliquots were withdrawn and centrifuged at 15
000 rpm for 5 minutes to remove the solid MOF. Then, 200 μL of the supernatant was transferred to a rotavapor vial, and CH3CN was evaporated under reduced pressure at 50 °C, 150 rpm, gradually lowering the pressure from 230 mbar to 72 mbar, followed by full vacuum. The residue was redissolved in 800 μL of CD3CN containing a known quantity of internal standard (1,3,5-trioxane, 3 mg, 0.037 mmol), transferred to an NMR tube, and analysed by 1H NMR (64 scans).
For homogeneous control reactions, the centrifugation step was omitted. After evaporation of the solvent from 200 μL of the reaction mixture, the residue was treated with 800 μL of CD3CN containing the internal standard and analysed directly by 1H NMR.
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