1 Introduction

Transition metal hexacyanometallates are coordination complexes with a number of special physiochemical properties such as having the ability to accommodate two different transition metal ions within the same compound [1], and these two metals both have mixed valencies [2, 3], it can act as an electron transfer mediator [4], some show supermagnetism, [5], electrochromism [6], energy storage capability [7], and it is insoluble in water [8]. Even upon oxidation or reduction of the metals, the particles do not dissolve due to the zeolitic-like structure which allows for the movement of ions in and out to maintain neutrality of the compound [9]. Due to these and many other useful properties, transition metal hexacyanometallates have found applications in many different fields. One field that is not fully exploited is the use of metal hexacyanometallates as heterogeneous catalysts. There are reports available on the catalytic polymerization of ethylene oxide [10], manufacturing of polyether polyols [11], copolymerization of carbon dioxide and propylene oxide using metal hexacyanometallates [12]. As for the heterogeneous catalytic transformation of fine chemicals, the oxidation of alcohols have been reported [13, 14]. However, little is known about the effect of the different metals, the oxidation state of the metals or even particle size on the catalytic oxidation of alcohols. Here we report the preparation of metal hexcyanometallate nanoparticles by two different methods namely co-precipitation and reverse micro-emulsion to obtain nanoparticle of different sizes. A spectroscopic characterisation study was conducted to determine the percentage of the II and III oxidation state of both iron and cobalt. The influence of the variations of the spectroscopic data are related to the turn over frequency (TOF) of the heterogeneous catalytic oxidation benzyl alcohol using hydrogen peroxide as an oxidant.

2 Experimental

2.1 Synthesis of Nanoparticles

All solvents and solid reagents namely: potassium hexacyanocobaltate, potassium hexacyanoferrate(III), cobalt(II) chloride hexahydrate, anhydrous iron(III)chloride and dioctyl sulfosuccinate sodium salt (AOT) (purchased from Aldrich) were used as received. Distilled water was used in all procedures.

2.2 Co-precipitation Method

1a–4a were all prepared according to the same synthetic procedure, 1a will be shown as an example.

2.3 Preparation of 1a

Potassium hexacyanocobaltate, K3[CoIII(CN)6] (503 mg, 1.5 mmol) was dissolved in water (15 ml), creating an aqueous solution with a concentration of 0.1 M. To this cobalt-cyano- containing solution was added 15 ml of a 0.1 M aqueous solution of cobalt(II) chloride hexahydrate, CoCl2·6H2O (356 mg, 1.5 mmol). The resulting combined solution turned light pink and was stirred at room temperature for 15 min. Following this the solution was centrifuged at 8500 rpm for 30 min at 15 °C. The supernatant was discarded and the precipitate dried overnight in vacuo at 60 °C. The resulting purple powder was crushed to yield 0.301 g (93.7%) of pure 1a.


ATR FTIR v(C≡N)=2166 (MII–CN–M′III), 2052 (MII–CN–M′II) cm− 1.


XPS: Binding energy = 781.31 eV (CoII 2p3/2); 782.59 eV (CoIII 2p3/2).

2.4 Characterisation Data for 2a

Yield 44.5% green powder


ATR FTIR v(C≡N) = 2174 (MIII–CN–M′III), 2166 (MII–CN–M′III) cm− 1.


XPS: Binding energy = 709.48 eV (FeII 2p3/2); 711.03 eV (FeIII 2p3/2).

2.5 Characterisation Data for 3a

Yield 73.1% black powder


ATR FTIR v(C≡N) = 2160 (MII–CN–M′III), 2108 (MII–CN–M′II) cm− 1.


XPS: Binding energy = 708.20 eV (FeII 2p3/2); 709.86 eV (FeIII 2p3/2); 781.53 eV (CoII 2p3/2); 783.01 eV (CoIII 2p3/2).

2.6 Characterisation Data for 4a

Yield 23.4% pale yellow powder


ATR FTIR v(C≡N) = 2175 (MII–CN–M′III) cm− 1.


XPS: Binding energy = 709.66 eV (FeII 2p3/2); 711.17 eV (FeIII 2p3/2); 781.89 eV (CoII 2p3/2); 782.67 eV (CoIII 2p3/2).

2.7 Reverse Micro-emulsion Method

1b–4b were all prepared according to the same synthetic procedure, 1b will be shown as an example. M(AOT)2 with M=Co and Fe was prepared as described in Ref [15].

2.8 Preparation of 1b

Potassium hexacyanocobaltate, K3[CoIII(CN)6] (664 mg, 2 mmol) was dissolved in a mixture of 2,2,4-trimethylpentane (10 ml) and water (10 ml). To this was added a solution of Na-AOT (450 mg, 1 mmol) dissolved in 2,2,4-trimethylpentane (10 ml), constituting Solution “A”. Solution “B” was prepared by dissolving the previously prepared Co(AOT)2 surfactant (2.289 g, 2.6 mmol) in 2,2,4-trimethylpentane (20 ml) and water (400 ml). Solution “A” was added dropwise to Solution “B” while stirring at room temperature for 15 min. The combined solution was sonicated for 15 min after which it was centrifuged (at 8500 rpm for 30 min at 15 °C). The clear supernatant was discarded and the precipitate washed with methanol to be centrifuged (at 8500 rpm for 30 min at 15 °C) again. The methanol supernatant was discarded and the pink precipitate was allowed to dry overnight in vacuo at 60 °C, yielding 252 mg (58.9%) of pure 1b.


ATR FTIR v(C≡N) = 2075 (MII–CN–M′II) cm− 1.


XPS: Binding energy = 780.91 eV (CoII 2p3/2); 782.59 eV (CoIII 2p3/2).

2.9 Characterisation Data for 2b

Yield 1.7% dark green powder


ATR FTIR v(C≡N) = 2174 (MIII–CN–M′III) cm− 1.


XPS: Binding energy = 710.33 eV (FeII 2p3/2); 712.59 eV (FeIII 2p3/2).

2.10 Charaterisation Data for 3b

Yield 15.3% brown-maroon powder


ATR FTIR v(C≡N) = 2157 (MII–CN–M′III), 2088 (MII–CN–M′II) cm− 1.


XPS: Binding energy = 708.49 eV (FeII 2p3/2); 710.44 eV (FeIII 2p3/2); 781.41 eV (CoII 2p3/2); 782.94 eV (CoIII 2p3/2).

2.11 Charaterisation Data for 4b

Yield 0.2% pale yellow powder


ATR FTIR v(C≡N) = 2175 (MIII–CN–M′III), 2082 (MII–CN–M′II) cm− 1.


XPS: Binding energy = 710.73 eV (FeII 2p3/2); 713.50 eV (FeIII 2p3/2); 781.92 eV (CoII 2p3/2); 782.84 eV (CoIII 2p3/2).

2.12 Characterisation

Infrared spectra of neat samples were recorded with a Thermo Scientific IR spectrometer and NICOLET iS50 ATR attachment, running OMNIC software (Version 9.2.86).

2.13 X-ray Photoelectron Spectroscopy

XPS data was recorded on a PHI 5000 Versaprobe system, with a monochromatic Al Kα X-ray source. Powered samples were mounted on the sample holder by means of carbon tape. Spectra were obtained using the aluminium anode (Al Kα = 1486.6 eV), operating at 50 µm, 12.5 W and 15 kV energy (97 X-ray beam). A low energy neutraliser electron gun was used to minimise charging of the samples. The instrument work function was calibrated to give a binding energy of 284.8 eV for the lowest binding energy peak of the carbon 1s envelope, corresponding to adventitious carbon. Survey scans were recorded at constant pass energy of 187.85 eV, while detailed region scans were recorded at constant pass energy of 29.35 eV for C and O, and 93.90 eV for the metals, with an energy step of 0.1 eV; the analyzer resolution is ≤ 0.5 eV. Charge neutralisation was enhanced by shooting the mounted sample with an Ar gun during data recording. The resolution of the PHI 5000 Versaprobe system is FWHM = 0.53 eV at a pass energy of 23.5 eV and FWHM = 1.44 eV at a pass energy of 93.90 eV. The background pressure was 2 × 10− 8 mbar. Spectra have been charge corrected to the main line of the carbon 1s spectrum, which was set to 284.8 eV. XPS data was analysed utilising Multipak version 8.2c computer software [16], and applying Gaussian/Lorentz fits (the Gaussian/Lorentz ratios were always > 95%). The photoelectron lines were charge corrected against the lowest binding energy of the fitted adventitious C 1s peak at 284.8 eV (the normal position of C–C according to the XPS Handbook [16]).

2.14 Transmission Electron Microscopy

Transmission electron microscopy (TEM) was performed with a Phillips (FEI) CM100 equipped with a Megaview III digital camera and coupled to an Oxford X-Max (80 nm2), energy-dispersive X-ray spectroscope (EDS). The digital images were analysed utilizing Soft Imaging System (analySIS) software. Multiple dispersions were prepared by mixing the powder with methanol and deposited on a 300-mesh nickel grid. Digital images were obtained after preparation.

2.15 Heterogeneous Catalytic Oxidation of Benzyl Alcohol

A mixture of benzyl alcohol (5.2 ml, 50 mmol) and 0.030 g of the catalyst (either 1–4) were heated till reflux while stirring. Hydrogen peroxide (2.3 ml, 96.7 mmol) was added with the evolution of gas (bubbling occurred). Small samples were periodically remove for ATR FTIR analysis to follow the progression of the reaction.

3 Results and discussion

Metal hexacyanometallate nanoparticles which has a general formula of KxMy[M′(CN)6]z·qH2O, with x, y, z and q representing stoichiometric numbers and M=M′=Co (1) or Fe (2), M=Co and M′=Fe (3) and M=Fe and M′=Co (4) were prepared by two different methods. The first method is a simple co-precipitation reaction which involves the mixing of the water soluble starting materials, a metal halide and the potassium hexacyanometallate at room temperature in ambient air. This resulted in the formation of the water-insoluble metal hexacyanometallates (1a4a). The yields obtained from co-precipitation ranged from 23% (4a) to 93% (1a).

The second method forms a surfactant stabilized nanoparticle utilising the anionic surfactant sodium bis(2-ethylhexyl)sulfosusuccinate (Na-AOT). This allowed for the confinement of the synthesis to occur in nanoscale droplets, an additional measure to ensure the formation of nanoparticles. The preparation involves the vigorous mixing of two micro-emulsions, the surfactant metal salt (M(AOT)2 with M=Co or Fe) [15] and the potassium hexacyanometallate surfactant-containing solution. This resulted in a milky but colourful fine suspension, which indicates that the exchange of cations between different droplets (of the two different micro-emulsions) are sufficient to activate nucleation and growth. Yields obtained for the reverse micro emulsion procedure were very low (ranging between 0.2–58.9%).

Infra-red spectroscopy is useful to distinguish between different functional groups within a sample. Stretching frequencies of hydroxyl groups (vOH) can be identified between 3650 and 3100 cm− 1 [17], cyanide groups (vC≡N) between 2300 and 2000 cm− 1 [18, 19], cyanates (v-NCO) at ca. 2250 cm− 1 [20], metal-bound carbon monoxide (vC≡O) between 1900 and 2200 cm− 1 [21, 22], while carbonyls stretching frequencies (vCO) can be found between 1600 and 1800 cm− 1 [23, 24]. Factors such as the electronic influence of the chemical surroundings also affects the wavenumber of the stretching frequency of the functional group [17].

The ATR FTIR spectra of the metal hexacyanometallates and their starting materials are shown in the Figures S1–S5, in the Supplementary Information. From the ATR FTIR spectra of 1–4 revealed the presence of water within the samples, adsorbed on the outside as well as being trapped in the inside of the zeolite-structure of the metal hexacyanometallates. The OH stretching frequency (vOH) of water adsorbed on the outside of the structure is located at ca. 3600–3100 cm− 1, while the δHOH bending vibration of the coordinated water molecules which are trapped inside the structure in the intercalated positions can be detected at ca. 1600 cm− 1 [25]. With the exception if 1b and 4a, two peaks were observed in the characteristic cyanide stretching frequency area. Since it is known that shifts in vibration frequencies is an indicator of different oxidation of the metal to which the CN is bound, the different peaks were assigned to the different possible MII/III–CN–M′II/III chains in correlation to published reports [18, 19], and the data summarised in Table 1.

Table 1 The ATR FTIR measured stretching frequencies detected for 1a4b

To further characterise the metal hexacyanometallate nanoparticles, X-ray Photoelectron Spectroscopy (XPS) was conducted. The binding energy measured of each element corresponds with the atomic potential which provides insight into the oxidation status as well as the chemical and electronic environment of the element [26,27,28,29,30,31].

In the survey scans of all the compounds C, N, O, Fe, Co and K were detected. All the binding energies of the photoelectron spectra were referenced against the lowest binding energy of the C–C simulated adventitious C 1s photoelectron line, which was set at 284.8 eV [16]. The carbon of nanoparticles, M–C≡N–M′ was measured at ca. 288 eV, while the N 1s photoelectron line from the –C ≡ N– group is located at ca. 398 eV (see Figure S6).

Figure 1 shows the detail scan of Fe 2p and Co 2p area, including the simulated peak fittings, of 3a as an example. The XPS data of the metal hexacyanometallates, 1a4b, with respect to the N 1s, Fe 2p3/2 and Co 2p3/2 photoelectron lines are presented in Table 2.

Fig. 1
figure 1

XPS detail scans of the Fe 2p (top) and Co 2p areas of 3a

Table 2 Binding energies (eV) of N 1s photoelectron line, the Fe 2p3/2 photoelectron line of FeII and FeIII, the Co 2p3/2 photoelectron line of CoII and CoIII

Both the Fe 2p1/2 and Fe 2p3/2 photoelectron lines of the iron-containing compounds, 2–4, shows splitting of the photoelectron line into two sharp well-defined peaks (see Fig. 1 top), which is assigned to FeII and FeIII (at the higher binding energy). The Fe 2p3/2 photoelectron lines assigned to FeII have an average binding energy of ca. 709.5 eV (see Table 2), with a spin orbit splitting between the Fe 2p3/2 and Fe 2p1/2 photoelectron lines of ca. 12.9 eV. Whereas the Fe 2p3/2 photoelectron lines assigned to FeIII is located at a binding energy of ca. 711.4 eV (see Table 2), an average of 1.9 eV higher than the FeII. The average atomic ratio (AR) between the amount of FeII and FeIII present is 2.1:1 (see Table 2). The Fe 2p photoelectron lines are slightly asymmetric towards the high energy side, where a small shake-up peak could be fitted at ca. 2.8 eV higher than the main Fe 2p envelope.

The calculated average binding energy for the FeII (709.5 eV) correlates good with published values for the binding energy of the FeII within ferrocene anchored onto an aminoalkyl silane-capped silicon-wafer (709.7 eV) [32]. While the calculated average binding energy for the FeIII (711.4 eV) was found to be slightly higher than reported data for iron(III) tris(β-diketonato) complexes (710.9 eV) [57], but in good agreement with sodium iron(III) oxide (711.5 eV) [33], and iron(III) chloride (711.3 eV) [34].

The detail scans of the cobalt Co 2p photoelectron lines, did not show the CoII and CoIII as separate peaks like the iron. However, a small shoulder is clearly present on the low energy side, while the photoelectron line is asymmetric in shape towards the high energy side. The Co 2p photoelectron lines were fitted with three simulated peaks (see Fig. 1 bottom left). The simulated fit of the Co 2p3/2 photoelectron lines were assigned in order from the low energy side: CoII at a binding energy of ca. 781.7 eV, CoIII at a binding energy of ca. 782.9 eV (see Table 2), and the last simulated peak at ca. 787.2 eV is a shake-up peak. The allocation correlates well with the 781.7 eV reported for CoII in a bimetallic carboxylate complex spin-coated onto a Si-wafer [35], and the 782.4 eV reported for CoIII in CoF3 [34]. The average atomic ratio between the amount of CoII and CoIII present is 2.1:1 (see Table 2).

Using the atomic ratios obtained between the potassium, cobalt and/or iron, as well as the relative % of the oxidation states from the XPS, it is possible to derive the a quantified stoichiometric formula for 1–4 in the form of KxMy[Fe(CN)6]z:

  • 1a: K0.7Co0.4[Co(CN)6]1

  • 1b: K0.9Co0.7[Co(CN)6]1

  • 2a: K1.5Fe0.7[Fe(CN)6]1

  • 2b: K1.1Fe0.75[Fe(CN)6]1

  • 3a: K1.3Co1[Fe(CN)6]1 or K1.3CoII0.8/CoIII0.2[FeII0.66/FeIII0.34(CN)6]1

  • 3b: K0.97Co1.69[Fe(CN)6]1 or K0.97CoII0.87/CoIII0.33[FeII0.33/FeIII0.67(CN)6]1

  • 4a: K1.2Fe0.8[Co(CN)6]1 or K1.2FeII0.5/FeIII0.3[CoII0.75/CoIII0.25(CN)6]1

  • 4b: K1.2Fe1.1[Co(CN)6]1 or K1.2FeII0.78/FeIII0.32[CoII0.40/CoIII0.6(CN)6]1

The Transmission electron microscopy (TEM) images of 1a and b, the cobalt hexacyanocobaltate nanoparticle prepared respectively by co-precipitation and reverse micro-emulsion are shown in Fig. 2 as examples. The mean particle distribution (nm) of 1–4 range between ca. 180 nm (for 3b) and 520 nm (for 3a), and are summarised in Table 3. The size depends on the different metals as well as the preparation method. In general, it was found that the nanoparticles prepared by reverse micro-emulsion are slightly smaller. The shape and size detected by TEM image are similar to the variety of Prussian blue analogues (including iron hexacyanocobaltate (Fe–Co) and manganese-iron hexacyanocobaltate (Mn0.5Fe0.5–Co), which is comparable with 1ab) prepared by a “co-polymer-co-morphology” concept using PVP [36]. This shows that it is possible to obtain similar shape using different methods of preparation.

Fig. 2
figure 2

TEM image of the nanoparticles of (left) cobalt hexacyanocobaltate (1a) prepared by co-precipitation and (right) cobalt hexacyanocobaltate (1b) prepared by reverse micro- emulsion (right)

Table 3 Summary of the TOF (determined from catalysis), the pseudo first order rate constant (kobs as determine from following the kinetic of the catalysis process), mean diameter (from TEM) and oxidation state ratio of the Fe and Co (from XPS) in 1–4

Considering the physical properties such mixed valencies, high surface area, insolubility (making the metals self-supporting) of metal hexacyanometallates, which are all favourable for utilisation as a heterogeneous catalyst, the catalytic activities of 1–4 was tested for the solvent-free oxidation of benzyl alcohol using the environmentally friendly oxidant hydrogen peroxide [14].

The progression of the catalytic reaction was monitored using Attenuated Total Reflection Fourier Transformed Infrared (ATR FTIR) analysis, see Fig. 3. From the ATR FTIR spectra the formation of the oxidation products bearing a carbonyl (C=O) groups could be detected following the appearance of the characteristic FTIR stretching frequency at ca. 1700 cm− 1. This approach could also be used to monitor the consumption of the starting material, the benzyl alcohol, by following the disappearance of the carbon-hydroxy C–O–H stretching frequency at 1006 cm− 1.

Fig. 3
figure 3

Left: ATR FTIR spectra sections showing the appearance and disappearance of stretching frequencies at 1698 and 1006 cm− 1 over time of the solvent-free catalytic oxidation of benzyl alcohol using the environmentally friendly oxidant H2O2 using 4b as the heterogeneous catalyst. Right: Comparative ATR FTIR spectra of the carbonyl stretching frequency area showing from top to bottom benzoic acid, benzaldehyde, the progress of the catalytic reaction and benzyl benzoate

Closer inspection of the carbonyl stretching frequency (vCO) revealed that it consisted of two overlapping peaks at 1698 and 1715 cm− 1, see Fig. 3 Left. The carbonyl stretching frequency at 1698 cm− 1 started as the favourable product but as the reaction progressed the oxidation product with a vCO at 1715 cm− 1 started to appear. This is on contrast to what was observed by Ali et al. who found benzaldehyde as the only oxidation product [14].

Determination of the oxidation products responsible for the carbonyl stretching frequencies observed at 1698 and 1715 cm− 1, were identified by comparison to commercially available benzaldehyde and benzoic acid. From the results obtained of the commercial samples, the vCO at 1698 cm− 1 was assigned to benzaldehyde, however no carbonyl stretching frequency for benzoic acid (which appeared at 1676 cm− 1) could be detected in the FTIR spectra of the oxidation products (see Fig. 3 Right). However, the vCO at 1715 cm− 1 obtained from the oxidation product was detected at the same the carbonyl stretching frequency of commercially available benzyl benzoate, located at 1718 cm− 1 (see Fig. 3 Left).

Since benzyl benzoate is the condensation product formed between benzyl alcohol and benzoic acid, it is implied that benzoic acid must have formed and that the characteristic carbonyl stretching frequency is probably hidden underneath the water peak or that as soon as the benzoic acid is formed it condenses with the benzyl alcohol to form benzyl benzoate. The formation of this series of oxidation products (benzaldehyde, benzoic acid and benzyl benzoate) along with the formation of toluene (not detectable/distinguishable from ATF FTIR) has been reported in literature [37].

From the data collected for the solvent-free catalytic oxidation of benzyl alcohol using hydrogen peroxide as the oxidant over 1–4, the turn over frequencies (TOF) were calculated after 180 min and summarised in Table 3.

The turn over frequencies (TOF) was calculated after 180 min using Eq. 1. The amount of molecules converted was determined using the intensity ratio between the vCO (at 1698 cm−1) for benzaldehyde and vC–OH (at 1006 cm− 1) for benzyl alcohol. From a calibration curve the percentage aldehyde/alcohol (% convertion) present after 180 min could be measured (see Figure S7). Using data of catalyzed by 4b as an example, after 180 min (3 h) the intensity ratio between vCO:vC–OH = 1.8. From the calibration curve it is measured that ca. 78% of the molecules converted. Since the catalytic reaction was started with 50 mmol (3.011 × 1022 molecules) benzyl alcohol and 78% of the molecules converted, the amount of molecules converted is 2.3 × 1022. Considering that ca. 1.1 × 10− 4 mol (30 mg) of catalyst was added to the reaction, the amount of active sites present is ca. 6.6 × 1019. Thus the TOF (for 4b) = [(2.3 × 1022/6.6 × 1019)/3 h] ≈ 119 h− 1 or 1.99 min− 1.

$${\text{TOF}}=\frac{{\left( {\frac{{{\text{amount}}\,{\text{of}}\,{\text{molecules}}\,{\text{converted}}}}{{{\text{amount}}\,{\text{of}}\,{\text{active}}\,{\text{sites}}}}} \right)}}{{{\text{time}}\,{\text{in}}\,{\text{h}}}}$$
(1)

The TOF of 1–4 ranged between 48 h− 1 (for 3a) and 122 h− 1 (for 2b), which is comparable to 123 h− 1 reported in literature [14]. The TOF of the catalyst with the same composition e.g. Fe–CN–Co 3a (48 h− 1) and 3b (128 h− 1) varied significantly. To determine the cause of this variation as well as to determine other factors influencing the TOF, relationships were established between the TOF and mean particle diameter, % occurrence of the different oxidation states of Fe and Co, combined metal electronegativity and the degree of covalence of the metal–ligand bonds (see Figs. 4, 5).

Fig. 4
figure 4

Left: Relationship between the Mean particle diameter (as determined from TEM) and the TOF (as determined from the catalysis) of 1–4. Middle: Relationship between the % occurrence of FeIII (●) and CoII (♦), as determined from XPS, and the TOF (as determined from the catalysis) of 1–4. Right: Relationship between the % occurrence of FeII (●) and CoIII (♦), as determined from XPS, and the TOF (as determined from the catalysis) of 1–4

Fig. 5
figure 5

Left: Relationship between the Total electronegativity and the TOF (as determined from the catalysis) of 1–4. Middle: Relationship between the degree of covalence of the Co (an indication from XPS) and the TOF (as determined from the catalysis) of 1–4. Right: Relationship between the degree of covalence of the Fe (an indication from XPS) and the TOF (as determined from the catalysis) of 1–4

In general, as the mean particle diameter of the nanoparticles decreased, the TOF of the catalytic solvent-free oxidation of benzyl alcohol increased (Fig. 4 Left), which is consistent with many data reported on literature on various catalytic systems [38,39,40,41]. Even though the metal hexacyanometallate systems are not normal supported catalyst, but self-supporting catalyst, the smaller particles exposes more active metal sites to the surface giving rise to the higher TOF.

The metal hexacyanometallates are a combination of different metals (for 3–4) with each metal also having different oxidation states namely II and III, which would influence the TOF differently. The influence of the % occurrence of the II and III oxidation state of both Fe and Co on the TOF is shown in Fig. 4 Middle and Right. Inversely proportional relationships were obtained for the correlation between TOF and % occurrence of FeIII and CoII, while directly proportional relationships were found for the correlation between TOF and % occurrence of FeII and CoIII. This shows that a higher % occurrence of FeII and CoIII increases the TOF, while a higher % occurrence of FeIII and CoII decreases the TOF. The % occurrence of FeII and FeIII does not play as big a role in TOF as Co oxidation state as can be seen from the slope of the graphs.

Seeing as it is well reported that oxidation reaction utilising H2O2 as an oxidant according the Fenton mechanism starts with a FeII source as the catalyst [24, 42, 43], the higher TOF found by the higher % occurrence of FeII thus is expected. A number of results published the use of homogenous CoII/III and FeII/III complexes for oxidation reactions. It has been indicated that the use of a homogenous FeIII complex having the same ligand system than its CoII counterpart is superior in its catalytic activity for the oxidation of alcohols [44], and the use of a CoII Schiff base complex has also been reported to need the addition of a bromide ion as promotor [45, 46]. All confirming that the variation in the % occurrence of Fe has a smaller effect on the oxidation than the % occurrence of Co.

There are numerous reports available on how the electronegativity of molecular fragments influences the physical properties of the compounds. For instance, many linear relationships have been established to indicate the dependence of physical properties such as reaction rates [47], oxidation potentials [48,49,50,51,52], binding energies [53,54,55,56,57] on electronegativity, using the Gordy scale group electronegativity of molecular fragments. Electronegativity also influence TOF and since it is known that electronic environment of metals also influence the catalytic activity [61], an attempt was made to demonstrate how the electronegativity of 1–4 influence the TOF. However, seeing as the Gordy group electronegativity scale (scale used for organic molecular fragments) could not be used, the electronegativity of metal ions as determined by Li et al. [58] was used. A combined metal electronegativity for each compound (1–4) was determined using the following equation:

$$\left[ {\left( {\% {\text{ occurrence of F}}{{\text{e}}^{{\text{II}}}}} \right){\text{ }} \times {\text{ }}\left( {{\text{EN of F}}{{\text{e}}^{{\text{II}}}}} \right)} \right]{\text{ }}+{\text{ }}\left[ {\left( {\% {\text{ occurrence of F}}{{\text{e}}^{{\text{III}}}}} \right) \times \left( {{\text{EN of F}}{{\text{e}}^{{\text{III}}}}} \right)} \right]+\left[ {\left( {\% {\text{ occurrence of C}}{{\text{o}}^{{\text{II}}}}} \right) \times \left( {{\text{EN of C}}{{\text{o}}^{{\text{II}}}}} \right)} \right]+\left[ {\left( {\% {\text{ occurrence of C}}{{\text{o}}^{{\text{III}}}}} \right) \times \left( {{\text{EN of C}}{{\text{o}}^{{\text{III}}}}} \right)} \right]$$

The % occurrence of each oxidation state for each metal was obtained from XPS (Table 2) and the electronegativity (EN) of each metal ion is: EN of FeII = 2.636, EN of FeIII = 3.835, EN of CoII = 2.706 and EN of CoIII = 4.520 [58]. For compounds 1 and 2, having only Co and Fe respectively, the calculated combined metal electronegativity was doubled to compensate for the fact that only two types of metal ions are present within one compound where as 3 and 4 has four types of metal ions are present within one compound (see Table 3). With the exception of 2b, a directly proportional relationship was displayed between the combined metal electronegativity and the TOF. Thus, the more electronegative compounds resulted in higher TOF’s. The normal Fenton mechanism involves the oxidation of the FeII and the reduction in FeIII by hydrogen peroxide, where the net effect is the disproportionation of H2O2 to produce.

two different radicals (HO· and HOO·) and water. It can be deduced that the more electronegative (more electron poor) the compound in totality, the easier it is to disproportionate hydrogen peroxide, causing the higher TOF.

It is known that the shake-up peak (satellite peak) of metal photoelectron lines in XPS represents the charge transfer process and the separation (in eV) between the main and shake-up peak is a measure of the degree of covalence of the metal–ligand bond [59]. The lower the degree of covalence of a metal–ligand bond, the more “ionic” character will be displayed by the bond. An inversely proportional relationship was established between degree of covalence of the metal–ligand bond (for both Fe and Co) and the TOF (see Fig. 5 middle and right).

Though the degree of covalence of the metal–ligand bond is not the same as the metal–ligand bond strength it is a feature of molecular orbital energy [59], which corresponds to bond strength (the higher the molecular orbital energy the higher the bond strength). Considering this, the inversely proportional relationship found for the degree of covalence of the metal–ligand bond and TOF is consistent with reported data. During catalytic oxidation reactions using metal oxides, the M–O bond strength has been reported to be an important factor influencing the catalytic reaction [60, 61]. An inversely proportional relationship exist between M–O bond strength and catalytic activity, which is consistent with our findings. When the M–O bond strength is high the catalytic activity is low, up to a point where the M–O bond strength is so strong that the catalyst could be inactive. While a weak bond strength could lead to total and even over oxidation.

The kinetics of the catalytic oxidation of benzyl alcohol to benzaldehyde was also investigated (further oxidation to the acid and ester was not investigated). Figure 6 (Right) shows the kinetic time trace of the formation of benzaldehyde using using H2O2 as oxidant and 4b (as an example) as the catalyst. The graph in Fig. 6 (Middle) confirms that the behavior of the catalytic reaction is “pseudo” first-order and the slope of this graph corresponds to the observed rate constant (kobs) for the reaction under solvent free conditions at 25 °C. The % conversion as well as the observed rate constant (kobs) for the catalytic oxidation reaction using reaction 1–4 are summarised in Table 3.

Fig. 6
figure 6

Left: Time trace showing the conversion of benzyl alcohol to its oxidation products at 25 °C using H2O2 as oxidant and 4b as the catalyst. Middle: A kinetic plot of data for this process that leads to the observed first order rate constant kobs. Right: Relationship between the TOF and the kobs measure during the catalytic oxidation of benzyl alcohol using 1–4 as the catalysts

Comparison of the TOF with the kobs value (Fig. 6 Right), revealed a directly proposional relationship, the higher TOF the higher the kobs.

4 Conclusion

Based on the spectroscopic characterisation (ATR FTIR and XPS) of the metal hexacaynometallates, 1–4, in combination with the correlation studies on the effect of mean particle diameter, % occurrence of CoII/III and/or FeII/III, total metal electronegativity and the degree of covalence of the Co- and Fe–ligand bond on the catalytic activity, it is clarified that smaller particles with a high % FeII and CoIII content, a high total metal electronegativity and a low degree of covalence produces the best self-supporting metal hexacyanometallate catalyst for the oxidation of benzyl alcohol under solvent-free oxidation using H2O2 as oxidant.