Ganga
Singh
,
Ruchika
Choudhary
and
Debaprasad
Mandal
*
Department of Chemistry, Indian Institute of Technology Ropar, Rupnagar, Punjab 140001, India. E-mail: dmandal@iitrpr.ac.in
First published on 2nd July 2025
Orbital engineering through the cooperative effect of different transition metals (TMs) is a powerful and versatile approach for modulating the chemistry of polyoxometalates (POMs), either by introducing novel POM structures or by designing POM hybrids for more effective catalytic applications. Here, we present a cooperative mixed-metal strategy for the synthesis of mixed-addenda (Mo/W) sandwich POMs with varying compositions, denoted by the general formula [(TMi)2(TMe)2(H2O)2(XMoxW9−xO34)2]n− (TMe(2+) = Fe/Co/Ni/Zn and TMi(3+) = Mn/Fe, X = Zn/Co/Fe). Using this cooperative mix-metal strategy, overall, we report 24 new POMs, including 8 mixed-addenda, 12 W-based sandwich POMs, and 4 POM-based 1-D coordination frameworks. Structural analyses reveal that Mo-addenda incorporation into the POM framework, alongside W (Mo/W), is strongly influenced by the variation of the transition metal composition at the sandwich core, their oxidation states, and the pH of the reaction media. Electrospray ionization mass spectrometry (ESI-MS) and energy dispersive X-ray (EDAX) analysis confirm the detailed POM compositions, while UV-vis spectroscopy and complementary density functional theory (DFT) analysis provide insights into orbital engineering via distinctive charge transfer processes. Theoretical and electrochemical studies demonstrate that electron transfer modulation occurs through both mixed-addenda incorporation and mixed-metal substitution at the sandwich position. This is further elucidated by enhanced oxygen evolution (OER) activity, where the cooperative mixed-metal and mixed-addenda POMs exhibit significantly improved performance, with an overpotential of 500 mV at 1 mA cm−2, compared to 570 mV in a pH 7.1 buffer. Additionally, this cooperative mixed-metal, mixed-addenda strategy extends to the formation of 1-D polyoxometalate coordination frameworks (POMCFs), where the oxidation state of precursor metals plays a vital role in determining the overall structural attributes.
Recently, we have also demonstrated fine-tuning of the optical and redox properties of P-based mixed addenda sandwich POMs, [(TM)4(H2O)2(PMoxW9−xO34)2]n−, which opens up a wide range of possibilities for the synthesis of these TMSPs with desired properties.18 Conversely, another set of TMSPs with d-block elements as heteroatoms [(TM)4(H2O)2(XW9O34)2]n− (where TM = X = Mn/Fe/Ni/Cu) and [W(TM)3(H2O)2(XW9O34)2]n− (where TM = X = Co/Zn), with W addenda atoms have been reported.19–22 Despite these advantages, a mixed addenda POM with the incorporation of Mo, V, or Nb alongside W in these tetrasubstituted TMSPs remains unexplored, which holds potential for fine-tuning the optical and redox properties. Alternatively, a mixed transition metal approach is widely used for the synthesis of W-only Keggin and Dawson-based tetrasubstituted sandwich, banana, cap, and tetramer TMSPs with improved catalytic activity. For example, [Ni2Co2(H2O)2(PW9O34)2]10− and [Fe2Co2(H2O)2(CoW9O34)2]14− have been reported as highly active OER catalysts.23–27 However, a systematic study of transition metal variations at different positions, such as the heteroatom position and sandwich (internal and external) positions, and the possible role of mixed metals in Mo addenda incorporation into the framework, and its impact on their band gap modulation, is still lacking. Also, the effect of the charge densities of lacunary POMs (overall charge divided by the number of atoms, Table 1) on binding with transition metals remains unexplored in these TMSPs, as observed in Nb-based POMs.28,29
Formula | Charge (−ve) | (non-H) atoms | Charge density (charge/atoms) |
---|---|---|---|
ZnW9O34 or ZnMoxW9−xO34 | 12 | 44 | 0.27 |
CoW9O34 or CoMoxW9−xO34 | 12 | 44 | 0.27 |
FeW9O34 or FeMoxW9−xO34 | 11 | 44 | 0.25 |
PW9O34 or PMoxW9−xO34 | 9 | 44 | 0.20 |
ZnW12O40 | 6 | 53 | 0.11 |
PW12O40 | 3 | 53 | 0.05 |
Thus, we propose TMSPs with mixed addenda to leverage the combined advantages of W and Mo along with various transition metals at the sandwich core and heteroatom position (Scheme 1). In this context, our efforts focus on the systematic approach for the synthesis of mixed metal, mixed-addenda TMSPs featuring late 3d transition metals (Mn, Fe, Co, Ni, Cu, and Zn) with the general formula [(TMe)2(TMi)2(H2O)2(XMoxW9−xO34)2]14− (TMe = X = Zn/Co/Fe, TMi = Mn/Fe). Moreover, the inclusion of mixed addenda in TMSPs alters the electron density of the framework, which can serve as a template for the construction of POM-based 1-D coordination frameworks30–33 (POMCFs). All these POMs are characterized using single crystal X-ray diffraction (SC-XRD), ESI-MS, Fourier transform infrared (FT-IR) and Raman spectroscopy, X-ray photoelectron spectroscopy (XPS), thermogravimetric analysis (TGA), EDAX, powder X-ray diffraction (PXRD) and their role in dioxygen activation34–38 has been emphasized. Furthermore, electronic and optical properties are elucidated through electrochemical, UV-vis spectroscopy and DFT studies.39–42
However, Fe is in a +2 oxidation state at external sandwich positions (TMe) and +3 at the heteroatom and internal sandwich position (TMi) in 1. The characteristic Fe–O bond lengths are between 1.8 and 2.1 Å with X-Oμ4-TMi (X = TMi = Fe) distances found to be 3.87 Å. FeCl2 plays a crucial role in incorporating mixed addenda into these POMs as FeCl3 as a precursor favors precipitation after some time, which could not be analyzed further. FeCl2 over FeCl3 not only facilitates crystallization but also maintains the required solution pH; i.e., FeCl3 drastically decreases the pH to less than 4 from 6.6, whereas the pH decreases to 5.0 in FeCl2. The crystallization of 1-M is slow and takes approximately 15 days with KCl. The use of Fe3+ instead of Fe2+ results in fast precipitation rather than gradual crystallization.
![]() | ||
Fig. 1 (a) Combined polyhedral and ball-stick representation of 2 (left) and 2-M (right) with μ2, μ3, and μ4 oxygen atoms (counter cations and hydrogen atoms are omitted for clarity); ESI-MS envelope of peaks with the assigned formula table for 2-M (full ESI-MS and simulated spectra in Fig. S14, ESI†). (b) Frontier molecular orbitals from the DFT optimized structure with the theoretically calculated band gap and (c) solid-state UV-vis spectra and (d) corresponding optical band-gap derived from the Kubelka–Munk (K–M) function in 2 and 2-M. |
Furthermore, DFT optimization of the auxiliary structure of [Zn4(H2O)2(ZnW9O34)2]16− suggests that the X–Oμ4–TMi distance of 4.03 Å with one of the Zn–O bond length (3.01 Å) elongation results in the distortion of the structure (Fig. S11, ESI†). Moreover, it was observed that the introduction of W(VI) in the sandwich position of these POMs not only enhances the structural stability but also facilitates the substitution of TMs at the external sandwich position within these sandwich POMs.46,51,52 Similarly, other higher oxidation state transition metals at the internal sandwich position also enhance the structural stability in these mixed metal TMSPs. For example, Fe3+ and Ru4+ substituted TMSPs, [Co2Fe2(H2O)2(CoW9O34)2]14− and [Zn2Ru2(H2O)2(ZnW9O34)2]12−, are reported to be highly stable under the strong oxidizing conditions of the OER.25,53 The good structural stability and TM substitution possibilities at the external sandwich position in Zn and Co-based TMSPs motivated us to exploit the potential impact of mixed TMs, particularly with those with a high oxidation state TM at the sandwich position. In this context, different transition metals such as V4+, Cr3+, Mn3+, Fe3+, Y3+, and Zr4+ were tested for sandwich POMs with Zn/Co as the heteroatom, out of which Mn3+ and Fe3+ showed excellent stability when taken as mixed metal precursors along with Zn/Co salts. Other TMs either lead to an insoluble precipitate or form [Zn3W(H2O)2(ZnW9O34)2]12− under our conditions (pH range: 6–8). Four compounds with the general formula [(TMe)2(TMi)2(H2O)2(XW9O34)2]14− (where TMi = Fe3+/Mn3+, X = TMe = Zn/Co) were obtained in situ from a mixture of Zn/Co, Fe/Mn and W salt solution after microwave heating at 80 °C for 45 min at pH 7.8. Except for 3,25 all these POMs are new and the obtained molecular formulas are Na14[(Zne)2(Fei)2(H2O)2(ZnW9O34)2]·23H2O (2); Na14[(Coe)2(Fei)2(H2O)2(CoW9O34)2]·15H2O (3); Na14[(Zne)2(Mni)2(H2O)2(ZnW9O34)2]·24H2O (4); Na14[(Coe)2(Mni)2(H2O)2(CoW9O34)2]·22H2O (5).
SC-XRD indicates that all these TMSPs crystallized in 2 h as monoclinic (P21/n) lattices except for 2, which crystallized in a triclinic (P) lattice (details, Fig. S12–S46†). BVS calculations indicate that all TMi atoms are in +3 and TMe/X is in a +2 oxidation state with the characteristic TMi–O bond length average found to be 2.04 Å. In the case of 4/5, two TMi–O bond lengths are found to be longer (2.30 Å) than the average of the other four TMi–O bond lengths (1.94 Å) due to z-out Jahn Teller distortions in 3d4 {Mn3+} configurations. The X–(Oμ4)–TMi bond distances were found to be 3.86–3.93 Å. These POMs were then characterized using FT-IR (W = Ot at 900–930 cm−1 and W–Oc–W at 835–840 cm−1) and ESI-MS confirms the fragments of H11[2] at m/z 1594 (z = –3), H11[3] at 1585 (z = –3), H11[4] at 1593 (z = –3), and H11[5] at 1584 (z = –3). From the SC-XRD of 2, it was observed that Fe(+3) is present at the internal sandwich position, while Zn is located at the heteroatom position as well as the external sandwich position. This was further confirmed by ESI-MS, which shows only a single peak at m/z 1594 (z = −3) ascribed to the presence of H11[Zn2Fe2(ZnW9O34)2]3−. The FT-IR study of O2-activated 2/3 indicates dioxygen activation with two characteristic peaks at 1149 and 1203/1205 cm−1, which was further confirmed by Raman spectra (peaks at 722 and 1063 cm−1) (Fig. S17a/S27b, ESI†).
This cooperative mixed-metal approach seems useful for the synthesis of mixed-metal sandwich POMs, and we have extended it for the synthesis of mixed addenda with Zn/Co as the heteroatom. Using Fe3+ along with Zn2+/Co2+ as mixed transition metals results in the formation of mixed metal-mixed addenda sandwich POMs with the formula Na14[Zn2Fe2(H2O)2(ZnMoxW9−xO34)2]·23H2O (2-M) and Na14[Co2Fe2(H2O)2(CoMoxW9−xO34)2]·19H2O (3-M). The SC-XRD of 2-M (light yellow-colored) and 3-M (purple-colored) confirms the structures with the space group P21/n (Fig. 2). The distribution of the Mo addenda shows preferential binding with μ2 oxygen connected to substituted transition metals. The higher binding affinity of Mo to μ2 oxygens with lower charge density compared to other oxygens (μ3 and μ4) can be attributed to its lower effective nuclear charge and higher π-acceptor ability compared to W. Shifts in characteristic FT-IR peaks in 2/3 indicate Mo incorporation into the POM framework (Fig. S17a/S27c, ESI†).
In 2-M, Fe competes with Zn at the heteroatom position. BVS indicates Fei in +3, Zne in +2, and Zn at the heteroatom in +2 with 0.5 discrepancies indicating the presence of Fe(+3) along with Zn in 2-M, which was further confirmed by ESI-MS (Tables S10 and S13, ESI†) and 57Fe Mössbauer spectroscopy showing the presence of two types of Fe in the structure (two singlets) (Fig. S17d, ESI†). In ESI-MS, the isotopic single envelope of peaks at m/z 1594 (z = –3) for 2 shifts to isotopic multiple envelopes of peaks ranging from m/z 1340 to 1565 (z = –3) for 2-M due to the incorporation of Mo addenda atoms. Similarly, the isotopic single envelope of peaks at m/z 1585 (z = –3) for 3 shifts to isotopic multiple envelopes of peaks ranging from m/z 1320 to 1550 (z = –3) in 3-M. The most abundant anion in 2-M gave the composition of Mo:
W (2
:
7) with the formula H9[Zn2Fe2(H2O)2(Fe2Mo4W14O34)]3−, while the Mo
:
W ratio varies from 1
:
17 to 8
:
10 for z = –3. EDAX and PXRD further confirm the bulk purity of 2-M (Fig. S16, ESI†). In 3-M, the most abundant anion has a Mo
:
W ratio of 5
:
13 with the formula H9[Co2Fe2(H2O)2(Fe2Mo5W13O34)]3−, while the Mo
:
W ratio varies from 3
:
15 to 7
:
11 for z = –3 (Fig. S25, ESI†).
We have also performed pH-dependent studies, which indicate that the Mo/W ratio increases for the most abundant peak with decreasing pH from 7.5 to 6.0 for 2-M and 3-M. However, a further decrease in pH results in the formation of the Keggin framework, indicating the crucial role of pH in obtaining maximum Mo incorporation into the framework (details, Fig. S15/S26, ESI†). BVS indicates Fei in +3, Coe in +2, and Co at the heteroatom in +2 with 0.5 discrepancies, supporting the presence of Fe(+3) along with Co2+ in 3-M similar to 2-M, which was confirmed by XPS analysis, otherwise difficult to predict from SC-XRD and ESI-MS. The UV-visible spectra show the LMCT, d–d transition and small intensity peaks (at 473/480 nm) due to metal to POM charge transfer (MPCT) in 2/3 and 2-M/3-M. The band gap calculated from the Kubelka–Munk plot was found to be less in the case of 2-M/3-M when compared to 2/3 (e.g., 3.03 eV in 2 to 2.68 eV in 2-M; see Fig. 1c and S25, ESI†). The DFT optimization of mixed addenda TMSPs shows that the LUMO lies at Mo atoms rather than W (Fig. 1a and b, detailed discussion on 2/2-M, ESI†), resulting in the reduction of the band gap, which is also observed from UV-visible spectra.
Using a similar approach, mixed addenda were introduced into Zn/Mn3+ or Co/Mn3+ based sandwich POMs. SC-XRD and ESI-MS confirm the molecular formula Na14[(Zne)2(Mni)2(H2O)2(ZnMoxW9−xO34)2]·22H2O (4-M) and Na14[(Coe)2(Mni)2(H2O)2(CoMoxW9−xO34)2]·19H2O (5-M), with only a little Mo addenda incorporation (the highest Mo:
W ratio obtained: 2
:
16). SC-XRD reveals Mo at only two addenda positions connected with the transition metal at the external sandwich position through μ2 oxygen (Fig. S32/S44, ESI†). Thus, we observed changing the TM at the internal sandwich position, i.e., when we go from 2 to 4 (3–5, Tables 2-A and 3-A), the optical band gap decreases, which was also observed in the DFT study, indicating the significant effect of the change in the transition metal at the internal sandwich position. Also, going from 2-M to 4-M, it was observed that the TM at the internal sandwich position impacts the Mo incorporation into the framework.
POMs (reference code) | Optical band gap from DRS (eV) | Mo![]() ![]() |
|
---|---|---|---|
Abundant Mo![]() ![]() |
Maximum Mo![]() ![]() |
||
A. Effect of changing the transition metal at internal sandwich positions | |||
2 vs. 4 | 3.03 vs. 2.31 | — | — |
3 vs. 5 | 1.98 vs. 1.37 | — | — |
2-M vs. 4-M | 2.68 vs. 1.65 | 4![]() ![]() ![]() ![]() |
7![]() ![]() ![]() ![]() |
3-M vs. 5-M | 1.73 vs. 1.29 | 5![]() ![]() ![]() ![]() |
7![]() ![]() ![]() ![]() |
B. Effect of changing the transition metal at external sandwich positions | |||
2a → 2b → 2c | 1.80 → 2.26 → 2.41 | — | — |
3a → 3 → 3b → 3c | 1.65 → 1.98 → 2.59 → 2.66 | — | — |
C. Effect of change in heteroatoms | |||
2 vs. 3d | 3.03 vs. 2.02 | — | — |
2b vs. 3 | 2.26 vs. 1.98 | — | — |
D. Effect of charge density (sandwich to 1-D framework) | |||
3 vs. 7 | 1.98 vs. 2.07 | — | — |
2-M vs. 6-M | 2.68 vs. 2.43 | 4![]() ![]() ![]() ![]() |
7![]() ![]() ![]() ![]() |
E. Effect of changing the heteroatom along with external sandwich positions (using the same metal) | |||
2 vs. 3 | 3.03 vs. 1.98 | — | — |
4 vs. 5 | 2.31 vs. 1.37 | — | — |
2-M vs. 3-M | 2.68 vs. 1.73 | 4![]() ![]() ![]() ![]() |
7![]() ![]() ![]() ![]() |
4-M vs. 5-M | 1.65 vs. 1.29 | 1![]() ![]() ![]() ![]() |
2![]() ![]() ![]() ![]() |
F. Effect of Mo incorporation into the framework | |||
1 vs. 1-M | 2.24 vs. 1.82 | 3![]() ![]() |
6![]() ![]() |
2 vs. 2-M | 3.03 vs. 2.68 | 4![]() ![]() |
7![]() ![]() |
3 vs. 3-M | 1.98 vs. 1.73 | 5![]() ![]() |
7![]() ![]() |
4 vs. 4-M | 1.84 vs. 1.65 | 1![]() ![]() |
2![]() ![]() |
5 vs. 5-M | 1.37 vs. 1.29 | 1![]() ![]() |
2![]() ![]() |
POMs | Band gap (eV) LMCT (O → W/Mo)/MPCT (SOMO → W/Mo) | Atom/group of atoms contributing to | LUMO position (eV) | |
---|---|---|---|---|
Highest SOMO | LUMO | |||
A. Effect of changing the transition metal at the internal sandwich position | ||||
2 vs. 4 | 4.62/4.09 vs. 4.01/3.78 | Fe3+vs. Oc; Mn3+ | W vs. Mn3+ | −1.51 vs. −2.09 |
B. Effect of the transition metal at the external sandwich position on MPCT | ||||
2a → 2b → 2c → 2d | 3.35 < 3.76 < 3.85 < 4.16 | Mn/Fe3+; Fe3+/Zn; Fe3+; Fe3+ | W only for all | −1.57 → −1.52 → −1.57 → −1.62 |
3a → 3 → 3b → 3c → 3d | 3.26 < 3.64 = 3.64 < 3.76 < 3.98 | Mn/Fe3+; Fe3+/Co; Fe3+/Co; Fe3+/Co; Fe3+/Zn | W only for all | −1.58 → −1.58 → −1.58 → −1.64 → −1.53 |
C. Effect of change in the heteroatom on MPCT | ||||
2 vs. 3d | 4.09 vs. 3.98 | Fe3+; Fe3+/Zn | W only | −1.51 vs. −1.53 |
3 vs. 2b | 3.64 vs. 3.76 | Fe3+/Co; Fe3+/Zn | W only | −1.58 vs. −1.52 |
D. Effect of change in the heteroatom along with the transition metal at the external sandwich position | ||||
2 vs. 3 | 4.62/4.09 vs. 4.70/3.64 | Fe3+ for both | W for both | −1.51 vs. −1.58 |
2-M vs. 3-M | 4.12/3.73 vs. 4.32/3.29 | Fe3+ for both | Mo for both | −1.94 vs. −1.95 |
E. Effect of Mo incorporation: W-only vs. W/Mo TMSPs | ||||
2 vs. 2-M | 4.62/4.09 vs. 4.12/3.73 | Fe3+ for both | W vs. Mo | −1.51 vs. −1.94 |
3 vs. 3-M | 4.70/3.64 vs. 4.32/3.29 | Fe3+ for both | W vs. Mo | −1.58 vs. −1.95 |
4 vs. 4-M | 4.01/3.78 vs. 3.97/3.36 | Oc + Mn3+; Oc + Mn3+ | W vs. Mn | −2.09 vs. −2.07 |
6 vs. 6-M | 4.63/4.12 vs. 4.32/3.83 | Fe3+ for both | W vs. Mo | −2.09 vs. −2.41 |
![]() | ||
Fig. 3 (a) Different views of the 1-D framework of 6-M and (b) 1-D framework of 7 (counter cations and hydrogen atoms are omitted for clarity). |
BVS calculations indicate that all Fe atoms are in +3, Zn in +2 and Mo/W in a +6 oxidation state. Using Fe2+/Zn2+ precursor salts instead of Fe3+/Zn2+ in W-only POM, 2, resulted in rapid precipitation of microcrystalline POMCFs, which are difficult to characterize via SC-XRD. A similar POMCF formation was observed when Co2+/Fe2+ precursor salts were used instead of Co2+/Fe3+ in W-only POM, 3, and when Zn2+/Mn2+ salts replaced Zn2+/Mn3+ in 4. For example, 1-D POMCFs were obtained for [Co2Fe2(H2O)2(CoW9O34)2]14− (7) with Fe2+ as a linker and [ZnWMn2(H2O)2(ZnW9O34)2]12− (8) with Mn2+ as a linker between two POM frameworks (details in Fig. S47–S62, ESI†). BVS calculations indicate Fe3+ occupies the sandwich position, Fe2+ outside the POM framework, Co and Mn in +2, and W in +6 oxidation states. Additionally, the cation exchange of 3 with excess Fe2+ led to the formation of an insoluble crystalline powder with matching PXRD (Fig. S56d, ESI†), indicating POMCF formation.
To explore the influence of high negative charge density on the POM structure resulting from the low oxidation state TM (Fe2+), we conducted the DFT optimization of the auxiliary structures [(TMe)2(TMi)2(H2O)2(ZnW9O34)2]16− (TMe = Zn2+ or Fe2+, TMi = Fe2+). The optimized structures of [Fe4(H2O)2(ZnW9O34)2]16− (TMe = TMi = Fe2+, X = Zn2+) and [Zn2Fe2(H2O)2(ZnW9O34)2]16− (TMe = X = Zn2+, TMi = Fe2+) revealed an elongation of the TMe–H2O bond due to increased charge density (Fig. S60, ESI†). This elongation further increased in the case of mixed addenda POMs (representative structure of 6-M; [Fe4(H2O)2(ZnMo4W5O34)2]16−, Fig. S60c, ESI†). These findings indicate the crucial role of the precursor's oxidation states/charge density of lacunary POMs in influencing the self-assembly towards POMCFs as well as Mo incorporation; e.g., when we go from 2-M to 6-M (Table 2-D), Mo incorporation decreases from 7:
11 to 2
:
16.
![]() | ||
Fig. 4 (a) SC-XRD structure of 2 (left) and representative trimetallic sandwich POMs 2a/2b/2c/2d (right) (counter cations and hydrogen atoms are omitted for clarity). (b) Optical images and ESI-MS with a single envelope of peaks along with the assigned formula table in 2a/2b/2c/2d/2 (full range ESI-MS spectra, zoomed part of the highest intensity peak of 2 (m/z = 1593.43 with z = –3) and its corresponding simulated spectra in Fig S65, ESI†). |
Mixed addenda of these trimetallic sandwich POMs were also synthesized in situ directly from their precursors, e.g., Na14[Ni2Fe23+(H2O)2(ZnMoxW9−xO34)2]·12H2O (2c-M) and Na14[Ni2Fe23+(H2O)2(CoMoxW9−xO34)2]·28H2O (3b-M), which were synthesized from Ni/Fe/TM (TM = Zn/Co) and Mo/W salts. The Mo:
W ratio was observed to be 5
:
13 in the most abundant peak of 3b-M in ESI-MS (Fig. S79 and Table S33, ESI†), which is similar to 3-M, thus indicating that the transition metal at external positions has a negligible effect on mixed addenda in these trimetallic sandwich POMs. The UV-vis spectra exhibit LMCT, MPCT and d–d transitions in the solid state (Fig. S68c, ESI†). This trimetallic sandwich POM approach was also applied to Mn3+ (Zn/Mn3+/TM) for the synthesis of Na14[(Fee)2(Mni)2(H2O)2(ZnW9O34)2]·25H2O (4a) (Fig. S85–S88, ESI†) and its mixed addenda analogue [(Fee)2(Mni)2(H2O)2(ZnMoxW9−xO34)2]14− (4a-M), where only a negligible Mo
:
W ratio (1
:
17) was observed in ESI-MS (Fig. S87, ESI†). From this, we observed that the transition metal at the external sandwich position impacts the optical band gap; however, the effect is comparatively less than that at the internal sandwich position (Tables 2-B and 3-B).
From the synthesis of these mixed-metal based W-only/mixed-addenda TMSPs, it was observed that two factors play a crucial role in the self-assembly: (a) the charge density of the trivacant lacunary part due to the heteroatom and (b) the cooperative effects of transition metals (TMs) at the sandwich position. This cooperative effect is especially prominent in TMSPs with higher charge density lacunary POMs with a transition metal at the heteroatom, which also allows Mo addenda incorporation into these TMSPs. In terms of Mo incorporation into these TMSPs, the cooperative effect of mixed metals like Zn/Fe3+ or Co/Fe3+ was found to be superior.
This is summarized in Fig. 5 as a diagram, and the following few essential points are discussed as the synthetic strategy for these TMSPs: (1) TMs as heteroatoms (Zn and Co) form high charge density trivacant lacunary POMs (e.g., ZnW9O34), while the P-heteroatom forms relatively low charge density trivacant lacunary POMs (e.g., PW9O34) (Table 1). (2) High charge density lacunary POMs with TMs as heteroatoms preferentially bind with TMs of high oxidation states (e.g., W6+, Ru4+, and Fe3+) at internal sandwich positions to form TMSPs. Meanwhile, using a low oxidation state TM with high charge density lacunary POMs results in the formation of 1-D frameworks instead of mixed metal at the sandwich position. For example, Zn as the heteroatom (i.e., ZnW9O34) forms TMSPs with Fe3+ in 3, while it forms a 1-D framework with Fe2+ in 7. (3) The P-heteroatom forms low charge density lacunary POMs preferentially binding with TMs of low oxidation states at both internal and external sandwich positions (e.g., Zn2+, Co2+, etc.).18 (4) In TM-heteroatom based TMSPs, the TM at internal sandwich positions has a pronounced impact on Mo incorporation into the mixed addenda as compared to the external sandwich position and heteroatom position. For example, Fe3+ favors more Mo incorporation into 2 than Mn3+ in 4 at the internal sandwich position.
Following the synthesis of various mixed-metal, mixed-addenda TMSPs and theoretical analysis of these POMs using DFT, it is evident that orbital engineering and electronic bandgap align with the optical bandgap, as summarized in Table 2. The data in Table 2 indicate that modifying a transition metal at sandwich or heteroatom positions within these TMSPs or incorporating Mo addenda significantly impacts bandgap modulation. For example, when moving from right to left across a row of 3d transition metals (Zn to Mn), altering the transition metal at the individual sandwich (whether internal or external) or heteroatom position decreases the band gap (factor 1), a trend also supported by theoretical calculations (Table 3). Furthermore, a significant decrease in the bandgap was observed due to the combined effects of the heteroatom and the external sandwich position while moving from TMSP 2 to 3. Notably, the incorporation of Mo into mixed addenda POMs not only decreases the bandgap (factor 2) but also changes the LUMO position; e.g., the LUMO, which is located at W in TMSP 2, shifts entirely to Mo in 2-M. While both factors reduce the bandgap, the internal sandwich position (Fe to Mn) has a more pronounced impact on lowering the bandgap and providing a lower-lying LUMO compared to Mo incorporation, as supported by theoretical calculations (Table 3). The heteroatom effect is most pronounced with Co as the heteroatom, while the external sandwich position has comparatively less impact on the bandgap.
Following the trend of decreasing band gap, TMSPs with Co as the heteroatom and Mn at the internal sandwich position along with mixed addenda reveal the lowest band gap, which was indeed experimentally observed in 5-M (1.29 eV) among all the reported TMSPs here due to the combined effect of Co, Mn3+, and W/Mo. Similarly, 3-M shows a lower bandgap with Co as the heteroatom but higher than 5-M due to Fe instead of Mn at the sandwich position. Although the optical band gap is slightly lowered (by 0.2 eV) in 4-M compared to 4, DFT shows that the LUMO of 4-M remains entirely on Mn for both 4 and 4-M, thereby minimizing the effect of Mo incorporation (bandgap of −2.09 vs. −2.07 eV from DFT).
These POMs exhibit quasi-reversible redox couples in CV, characterized by their half-wave potentials (E1/2) and peak separations (ΔEp = |Epc − Epa|) (Fig. 6 and Table S38, ESI†). The CV of 2 shows quasi-reversible redox peaks of W, mostly on the negative side, while the 3d transition metal (Fe) at the sandwich position exhibits quasi-reversible peaks on the positive side, corresponding to the stepwise oxidation of the Fe2+/Fe3+ and Fe3+/Fe4+ couples vs. Ag/AgCl/3 M KCl. In the mixed-addenda analogue, peak assignment for Mo and W is challenging due to their similar redox potentials and multiple influencing factors. Mo-related peaks were distinguished by comparing the CV of W-only POMs (2) with that of mixed addenda (2-M). A comparison of CVs of 2 and 2-M (Fig. 6a/b and Table S38, ESI†) revealed that 2-M exhibits quasi-reversible redox peaks on the negative side, similar to 2. However, the redox peaks are broad in 2-M (possibly due to different Mo/W ratios) and appear slightly less negative than those in 2, indicating more facile electron transfer in 2-M due to lower reduction potential.
To further understand orbital modulation and the influence of electron transfer in mixed-addenda as well as mixed-metal POMs, we investigated the electrocatalytic oxygen evolution reaction (OER) activity of 2, 2-M, 3, 3b, and 3-M. Cesium salts of these POMs (Cs[2], Cs[2-M], Cs[3], Cs[3b], and Cs[3-M]) were obtained through ion-exchange metathesis (details in the ESI†), and their OER activity was checked by coating onto a glassy carbon electrode (electrode preparation details in the ESI†). Linear sweep voltammetry (LSV) demonstrated well-defined OER responses for all the POMs, with overpotentials at 1 mA cm−2 of 600, 540, 570, and 530 mV vs. RHE for Cs[2], Cs[2-M], Cs[3], and Cs[3-M], respectively (Fig. 6c/d). These results clearly indicate that mixed-addenda POMs, Cs[2-M], and Cs[3-M], show better OER activity in terms of overpotential than their W-only counterparts, Cs[2] and Cs[3]. Furthermore, Cs[3b] demonstrated much improved OER activity, with an overpotential of 500 mV at 1 mA cm−2, compared to Cs[3] (570 mV) (Fig. 6d). This suggests that OER activity is modulated by a trimetallic mixed-metal W-only POM (Ni/Co/Fe combinations at the sandwich position/hetero) or by a mixed-addenda POM approach. These OER overpotentials are comparable to similar reported POMs with OER activity under neutral conditions.17 Given the vast potential for trimetallic mixed-metal substitutions along with mixed-addenda modifications in these sandwich POMs, they present a promising avenue for future catalytic applications.
Crystallographic data for all compounds has been deposited at the CCDC under [2330238–2330240, 2330242–2330250, 2330252–2330258 and 2330261†].
Footnote |
† Electronic supplementary information (ESI) available: Experimental details and characterization (SC-XRD structure and details, optical images, ESI-MS, TGA, PXRD, EDAX, FT-IR, Raman, and UV-visible spectroscopy with the Kubelka–Munk plot, XPS, ICP-MS, and BVS calculations and cyclic voltammetry), DFT study (HOMO, LUMO, and SOMO representation), and molecular oxygen binding/activation for 1/1-M, 2/2-M, 3/3-M, 4/4-M, 5/5-M, 6/6-M, 7, 8, 2-series (2a/2b/2c/2d/2c-M), 3-series (3a/3b/3c/3d/3b-M), and 4-series (4a/4a-M) and electrochemistry of sandwich POMs (2/2-M). CCDC 2330238, 2330239, 2330240, 2330242, 2330243, 2330244, 2330245, 2330246, 2330247, 2330248, 2330249, 2330250, 2330252, 2330253, 2330254, 2330255, 2330256, 2330257, 2330258, 2330261. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d5qi00961h |
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