Shriya
Saha
a,
Dolores G.
Gil-Gavilán
b,
Matthias J.
Gutmann
c,
Debasish
Manna
d,
Souvik
Roy
*b and
Raja
Mitra
*ae
aSchool of Chemical and Materials Sciences, Indian Institute of Technology Goa, Farmagudi, Goa 403401, India. E-mail: rajamitra@iitgoa.ac.in
bSchool of Natural Sciences, University of Lincoln, Green Lane, Lincoln, Lincolnshire LN6 7DL, UK. E-mail: sroy@lincoln.ac.uk
cRutherford Appleton Laboratory, ISIS Facility, Chilton Didcot, Oxfordshire OX11 0QX, UK
dDepartment of Chemistry, Indian Institute of Science Education and Research Bhopal, Bhopal, MP 462066, India
eCenter of Excellence in Sustainable Energy, Indian Institute of Technology Goa, Farmagudi, Goa-403401, India
First published on 29th April 2026
4-Ferrocenyl-bipyridine ligands (2a–d) and their respective [Re(L)(CO)3Br] (L = 3a–d) complexes were synthesized and investigated for CO2 photoreduction. The single-crystal analysis showed the formation of a by-product, 2d′, and its synthesis by self-aldol condensation explains the low yield observed for ligands. The Re(I) complexes showed CO2 photoreduction with >90% selectivity for CO.
In a non-bonding type of secondary sphere modification, ferrocene is studied for its ability to modulate the electron density and provide the structural stability for catalysis.37 Van Meervelt et al.,38 reported a method for synthesising a ferrocene-appended bpy ligand at the 4-position via palladium-catalysed Sonogashira coupling of 4-bromobipyridine with ethynylferrocene, achieving a yield of 56%. Pt, Cu, and Mn-coordinated complexes of the bpy ligand with ferrocene group at the 5-position were investigated for their photophysical, electrochemical, and catalytic properties.39,40 Ferrocene moiety at the 6-position of bpy has been investigated as an electrochemical marker.41 Although ferrocene-appended κ2-NN and κ3-NNN systems have been studied for their structural and electrochemical properties, their role in CO2 reduction remains limited.37,42,43 In our prior work,36 Re(I) complex with 4′-ferrocene-tpy ligand (fctpy) was found to be unstable under potential and light, prompting modifications by replacing the aromatic amine at the 6-position with another group. Herein, we report a generalised synthetic methodology for the 4-ferrocene-bpy ligand and aim to introduce steric hindrance at the 6,6′ positions to prevent dimerisation of catalytically active Re(0) species. We further investigate the impact of ferrocene substituents at the 4-position on the photoreduction of CO2 (Fig. 1b).
We report an improved synthesis of the ferrocene-substituted unsymmetrical bipyridine ligands by modifying Housecroft's methodology from a one-step procedure to a two-step synthesis (Fig. 2a).44 The yields from the reported method were consistently in the range of 20–30%,44 and no improvement was observed with longer reaction times. We addressed the problem of low yields by purifying and isolating the intermediate chalcones (1a–d) obtained after cross-aldol condensation between an acetylpyridine derivative and ferrocene carboxaldehyde,45 with yields of 60–96%. In the next step, condensation of the chalcone with the pyridinium methyl ketone salt in the presence of ammonium acetate yielded bpy ligands (2a–d) with yields of 25–65% (for characterisation data see Fig. S1). Ligand 2b consistently gave a lower yield (∼25%), and longer reflux (>24 h) led to decomposition of the product. Similarly, an analogue of ligand 2a was synthesised to probe the effect of the 6-substituent by replacing the methyl group at the 6-position with a phenyl group (2e), yielding 34% using the modified synthetic protocol.46,47 Solid-state molecular structure of ligand 2c was determined by single crystal X-ray diffraction48–51 (Fig. 2b), which showed that 2c crystallised in monoclinic space group P21/c. The angle between the ferrocene and bpy rings is ∼60° (Fig. S2), in line with the analogous compound reported by Van Meervelt et al.38 Serendipitously, a hexasubstituted cyclohexyl derivative (2d′, Fig. 2c) was isolated while investigating 2d. To understand its formation, it was synthesised independently, as depicted in Fig. 2d. The by-product (2d′) results from the self-aldol condensation of three acetylpyridine derivatives, which likely contributes to the lower yield of ligand 2d and may explain the low yield in the earlier two-step process.44 The successful synthesis of the ligands was further confirmed by NMR and mass spectrometry (Fig. S2). The UV-vis absorption spectra of ligands (2a–e), recorded in acetonitrile (Fig. S2), showed peaks in three distinct regions: the transitions below 300 nm are assigned to π → π* transition in the bpy ligand; transitions in the range of 300–400 nm might be due to intraligand charge transfer and the transition above 400 nm are assigned to the weak d–d transitions in the ferrocene moiety.52
The tricarbonyl rhenium(I) complexes (3a–e) were synthesised from Re(CO)5Br and the corresponding bpy ligands (2a–e) with yields in the range of 50–78%. A single crystal was obtained for 3e (Fig. 3), where the phenyl ring is perpendicular to the two-pyridine ring coordinated to the Re(I) centre, with a bond length of Re–N as 2.187(2) Å (Table S5), similar to that in Rebpy (2.163(1) Å).53 The bond angle between N1–Re1–N2 is 75°, whereas the rest of the bond angles with Re(I) centre are ∼90°, indicating a distorted octahedra with a facial geometry (Fig. 3). The thermogravimetric profile of 3a–e (Fig. S3) showed a consistent stepwise loss of the bromine atoms and the carbonyl moiety. However, for 3c, the complex decomposed in a single step at 338 °C, indicating that it is stable over a higher temperature range than the other derivatives. Complexes 3a–e were characterised by ATR-IR to probe the characteristic carbonyl stretching vibrations (νstr(C
O)), which serve as an indicator of the electron density on Re and the extent of Re-to-carbonyl back-donation.54 Complexes 3a–d exhibit only marginal shifts in the νstr(C
O) bands compared to Rebpy, suggesting that the methyl substituents at the 6-position of bpy, as well as the ferrocene substituent, exert minimal electronic influence on the back-donating capability of the bpy ligand, and the complexes retain a similar coordination geometry to that of Rebpy. Introduction of phenyl at the 6-position in 3e led to an increase of νstr(C
O) frequencies by ∼20 cm−1, presumably due to steric hindrance from the 6-phenyl group, which distorts coordination geometry and reduces metal-to-carbonyl back-donation.55 The NMR spectra of the rhenium complexes were recorded in DMSO-d6, where a visible change was observed in the 1H NMR spectrum compared to those of the ligands, further confirming complexation (Fig. S3). Three additional peaks in the 1H NMR spectrum of the complex 3d at 7.25, 7.18 & 2.30 ppm related to toluene were observed,56 consistent with the thermogravimetric profile of 3d (Fig. S3). Three distinct 13C resonances corresponding to the carbonyl were observed in the expected range36 of 190–198 ppm for all complexes, downfield of the free 13CO (180 ppm).57 The UV-vis spectra of all metal complexes in acetonitrile showed a ∼20 nm bathochromic shift in the 300–400 nm range compared to the pure ligands, attributed to metal coordination. Additionally, weak d–d transitions in the 400–450 nm range for free ligands shifted ∼50 nm for all metal complexes (Fig. S3).
The redox properties of the ligands were studied under non-catalytic conditions by cyclic voltammetry in acetonitrile under argon, and all potentials are reported relative to the ferrocene couple (Fc+/0) (Fig. S4). All ligands displayed a small reversible peak ∼−1.60 V, assigned to bpy/bpy˙−, and an irreversible peak at ∼−2.10 V, assigned to additional ligand-based reductions.58,59 The ferrocene peaks for the complexes are anodically shifted to more positive potentials by 0.30–0.45 V compared to unmodified ferrocene, which is consistent with the π-acceptor nature of the bpy ring (Fig. S5–S9).60 As shown in Fig. 4a and Fig. S10–S13, CVs of 3a–e showed a reversible peak at ∼−1.75 V under argon, indicating the bpy/bpy˙− reduction. Under CO2-saturated conditions, complexes 3a, 3d, and 3e showed the disappearance of this reversible peak, and a new peak appeared at ∼−1.90 V,61 accompanied by an increase in current, indicating formation of a new product (Fig. 4a, S10 and S13). However, complexes 3b and 3c showed no significant increase in current at around −1.90 V (Fig. S11 and S12). The catalytic parameter icat/ip is determined for all complexes under CO2-standardised conditions, with values ranging from 1.10 to 4.70 (Table S7), suggesting CO2 reduction activity depends on the substituent present on the ligand. Mechanistic investigations were carried out using IR spectroelectrochemistry (IR-SEC), following the methodology reported by Kubiak et al.22 In the potential range of −1.6 to −1.7 V, a broad band was observed at 1840–1895 cm−1, consisting of multiple CO vibrations, and two more prominent bands at 1958–1967 cm−1, and 1987–2005 cm−1 (Fig. 4b and S14). These peaks are consistent with the formation of the singly reduced species, [Re(L)(CO)3(NCMe)].62–65 As the potential is further decreased to −2.1 V, the peaks become broader, suggesting presence of both [Re(L)(CO)3(NCMe)] and the catalytically active double reduced [Re(L)(CO)3]− species in acetonitrile (Fig. S15).22,61–65 However, the possibility of formation of the Re0–Re0 dimer could not be ruled out based on the IR-SEC data for 3a–d, as the dimer characteristic IR bands at 1950 and 1990 cm−1,21,66 are masked by signals from other species. Only for 3e, the formation of the dimer under reducing conditions can be conclusively excluded by the absence of any band in the 1950 cm−1 region. This can be attributed to the steric hindrance of the phenyl substituent on the ligand in 3e, preventing dimerisation.
The photocatalytic activity of the complexes towards CO2 reduction was evaluated in CO2-saturated acetonitrile using [Ru(bpy)3]Cl2 as a photosensitiser, triethanolamine (TEOA) and 1,3-dimethyl-2-phenyl-2,3-dihydro-1H-benzo[d]imidazole (BIH) as electron donors. Gas chromatography of the headspace confirmed the generation of CO and H2 by 3a–e upon visible-light irradiation; results from 1 h of irradiation are shown in Fig. 4c and Table S8. Control experiments demonstrated that all components, including the catalyst, [Ru(bpy)3]Cl2, TEOA, visible light, and CO2, were required for photocatalysis, and a negligible amount of CO was produced in the absence of any component. This confirms that the CO is produced from CO2. The protons released from the decomposition pathway of oxidised TEOA serve as the source for H2.673a and 3c displayed best activity amongst the series with evolution of ∼26 µmol CO after 1 h with >91% selectivity. However, the reference Rebpy complex outperformed 3a–e, yielding 35 µmol of CO at 100% selectivity. A control experiment with only ligand 2e, lacking the Re(CO)3Br unit, showed negligible CO formation (2 µmol), which highlights the essential role of the Re catalytic site. These results indicate that incorporating ferrocene into the optimally substituted bpy framework can facilitate CO2 photoreduction to CO, giving CO yields close to that of the reference Rebpy catalyst. However, this corroborates minimal direct influence of ferrocene substituent on the catalytic property of the complexes, which is in line with the IR data of the complexes.
The photocatalysis results demonstrate the effect of substituents on bpy. 3a, with a methyl substituent, and 3d, with methyl and bromo substituents, displayed the highest CO evolution among the series. In contrast, 3b and 3c, which contain methyl groups at different positions (4′ and 6′, respectively), showed slightly lower CO yields (21 and 19 µmol, respectively) and product selectivity (86% and 85%, respectively). We speculate that this may be due to the electron-donating nature of the methyl groups, as reported previously for Re-complexes with para-substituted bipyridine ligands.25 The positioning of the methyl substituents in 3c can introduce additional steric hindrance, potentially restricting the access of substrates to the Re centre. Increasing the irradiation time to 3 h shows that for all complexes, CO evolution largely plateaued after ∼1 h, including the reference Rebpy catalyst (Fig. S16). For example, 3a showed only a small increase in CO amount from ∼26 µmol after 1 h to ∼28 µmol after 3 h. Interestingly, the CO/H2 ratio remained unchanged over 3 h of irradiation, suggesting that the catalyst decomposition products do not mediate hydrogen evolution. Overall, these findings highlight that the nature and position of substituents on Fc-bpy ligands can critically influence CO2 photoreduction performance through electronic and steric modulation.68
In conclusion, a two-step synthesis method for ferrocene-substituted unsymmetrical bipyridines (2a–d) was developed, enhancing synthetic efficiency over the one-pot approach. The by-product, an unusual hexasubstituted cyclohexane derivative (2d′), accounts for the lower yield of the ligands. Re(I) tricarbonyl complexes (3a–e) showed ligand-controlled photoreduction of CO2 to CO with more than 90% selectivity, which is comparable to the activity of the well-known Rebpy catalyst.
CCDC 2443100 (3e), 2443118 (2c) and 2532926 (2d′) contain the supplementary crystallographic data for this paper.69a–c
| This journal is © The Royal Society of Chemistry 2026 |