Determining the Location of Co2+ in Zeolites by UV-Vis Diffuse Reflection Spectroscopy: A Critical View

UV–Vis spectroscopy as well as in situ FTIR spectroscopy of pyridine and CO adsorption were applied to determine the nature of Co species in microporous, mesoporous, and mixed oxide materials like Co–ZSM-5, Co/Na–ZSM-5, Co/Al–SBA-15, and Co/Al2O3–SiO2. Because all sample types show comparable UV–Vis spectra with a characteristic band triplet, the former described UV–Vis band deconvolution method for determination and quantification of individual cationic sites in the zeolite appears doubtful. This is also confirmed by results of pyridine and CO adsorption revealing that all Co–zeolite samples contain two types of Co2+ species located at exchange positions as well as in oxide-like clusters independent of the Co content, while in Co/Al–SBA-15 and Co/Al2O3–SiO2 only Co2+ species in oxide-like clusters occur. Consequently, the measured UV–Vis spectra represent not exclusively isolated Co2+ species, and the characteristic triplet band is not only related to γ-, β-, and α-type Co2+ sites in the zeolite but also to those dispersed on the surface of different oxide supports. The study demonstrates that for proper characterization of the formed Co species, the use of complementary methods is required.

As Co ions are most stable in the form of Co 2+ , two [AlO 4 ] − sites are needed to stabilize the charge. Thus, only Al-O-(Si-O) 2 -Al units occurring in close proximity in the zeolite rings are able to charge balance divalent cations, while single Al atoms can only balance monovalent ions [15]. Therefore, the concentration and location of incorporated Co species are controlled by the distribution of Al atoms in the zeolite framework. Reversely, the zeolite exchange capacity for Co 2+ can be used to probe the Al distribution in the zeolite framework [16]. Assuming a fully exchanged zeolite, the quantification of the rings containing two Al atoms in the same channel is possible. The preparation conditions to guarantee a complete exchange were described in this reference. Thus, in the group of Wichterlová [17][18][19][20], a procedure was developed enabling the discrimination between those sites using starting zeolite material was constant, the exchange degree is mainly influenced by the applied Co salt concentration. When using Na-ZSM-5 as starting material, the Na ions were not completely exchanged. For comparison, two catalysts were also prepared utilizing materials that have no microporous zeolite structure. On the one hand a mesoporous Al-SBA-15 was used for ion exchange, and on the other hand a mixed oxide SiO 2 /Al 2 O 3 with open pore structure was loaded with Co by incipient wetness impregnation.

UV-Vis DRS Studies
The UV-Vis-DR spectra of the catalysts measured at room temperature after dehydration in Heat 400 • C are depicted in Figure 1. For all samples, similar spectra were obtained showing a characteristic triplet of bands with maxima around 495 nm, 585 nm, and 645 nm as earlier described in literature for Co-ZSM-5 samples [19]. The intensity ratios of these band maxima vary, as can be seen in detail by inspecting the deconvoluted spectra ( Figure S1), but a clear trend in terms of Co concentration and/or used materials is not visible. Interestingly, comparable spectra with a characteristic band triplet were also obtained from the samples 1.79 Co-SiAl and 0.8 Co-AlSBA, which have no zeolite structures. This suggests, in agreement with conclusion made by the Busca group, [11,26] that the assignment of the observed band triplet to three different types of sites (α, β, γ) located in the internal cavities of pentasil-containing zeolites [17][18][19] might not be correct, particularly since such a characteristic band triplet is not restricted to zeolite materials and was also described, e.g., for cobalt-based blue pigments, [28] cobalt spinels, [29,30] cobalt oxide-apatite materials, [31] Co/Al 2 O 3 , [32], and Co-doped ZnO [33].
splitting is observed, which may be due to (i) a low symmetry perturbation, which lifts the degeneracy of the two 4 T1 excited levels and which induces an asymmetrical band splitting; (ii) a dynamic Jahn-Teller effect, which splits the two bands into three symmetrically spaced peaks; (iii) spin-orbit coupling [38,39]. Taking these facts into account, it is not surprising that the spectra of all dehydrated Co 2+ -containing samples, not only those of zeolites, exhibit a band triplet in the visible region between 400-750 nm. The observed different shapes of the band triplets might by related to the specific coordination geometry of Co 2+ influenced by the individual surrounding of the Co 2+ ions in the respective solids. Thus, it can be expected that the splitting pattern in the case of Co-containing zeolites changes depending on the occupied positions (γ-, β-, or α-type sites), e.g., in pentasil-containing zeolites [17][18][19][20]. Therefore, one can consider that the splitting pattern provides information concerning the successive occupation of respective sites with increasing Co content as described by Dědeček et al. [19], e.g., for Co-ZSM-5 samples. Indications for that can also be seen by comparing the spectra of 0.32 Co and 2.44 Co in Figure 1. However, when Co 2+ ions are evenly distributed on γ-, β-, and α-type sites, then each type of Co species gives rise to an own triplet band, consequently leading to three superimposed triplet bands, which contribute to the observed spectrum. Therefore, it is practically impossible to discriminate between Co species at different sites and to quantify the percentage of occupied sites by deconvolution of the observed spectra. Nevertheless, based on spectral deconvolution, Dědeček et al. [19] described different components which were ascribed to three types of Co ions located at specific cationic sites in Co-ZSM-5: A single band at 15,000 cm −1 for α-sites; four bands at 16,000, 17,150, 18,600, 21,200 cm −1 for β-sites; and a doublet at 20,100, 22,000 cm −1 for γ-sites. This might be mathematically correct, but not from the physical point of view. Moreover, as we have shown, the triplet bands can also be properly deconvoluted on the basis of only three components (cf. Figure S1).
It has to be mentioned here that for determining the location of the Co 2+ ions, it was presupposed [15,19] that all Co 2+ ions are isolated due to the exchange of protons (Brønsted sites), which are created by the incorporation of Al in the zeolite matrix. Hence, only the Co/Al ratio was taken into account. We demonstrate in the next paragraph that this supposition cannot be made without inclusion of additional characterization methods. Octahedral and tetrahedral Co 2+ (d 7 ) complexes, particularly in zeolite materials, have been widely studied by optical spectroscopy in the past [34][35][36][37][38][39]. It is known that Co 2+ changes from high-spin octahedral state in hydrated samples to tetrahedral coordination in the respective dehydrated ones, visible by the color change from pink to blue. Tetrahedral Co 2+ (d 7 ) exhibits three symmetry and spin allowed transitions from the ground state : [36,39]. While ν 1 is observed in the infrared region between 2500 and 6000 cm −1 , the ν 2 and ν 3 transitions are observable in the near infrared and visible region. For the ν 2 and ν 3 transitions, a band splitting is observed, which may be due to (i) a low symmetry perturbation, which lifts the degeneracy of the two 4 T 1 excited levels and which induces an asymmetrical band splitting; (ii) a dynamic Jahn-Teller effect, which splits the two bands into three symmetrically spaced peaks; (iii) spin-orbit coupling [38,39]. Taking these facts into account, it is not surprising that the spectra of all dehydrated Co 2+ -containing samples, not only those of zeolites, exhibit a band triplet in the visible region between 400-750 nm.
The observed different shapes of the band triplets might by related to the specific coordination geometry of Co 2+ influenced by the individual surrounding of the Co 2+ ions in the respective solids. Thus, it can be expected that the splitting pattern in the case of Co-containing zeolites changes depending on the occupied positions (γ-, β-, or α-type sites), e.g., in pentasil-containing zeolites [17][18][19][20]. Therefore, one can consider that the splitting pattern provides information concerning the successive occupation of respective sites with increasing Co content as described by Dědeček et al. [19], e.g., for Co-ZSM-5 samples. Indications for that can also be seen by comparing the spectra of 0.32 Co and 2.44 Co in Figure 1. However, when Co 2+ ions are evenly distributed on γ-, β-, and α-type sites, then each type of Co species gives rise to an own triplet band, consequently leading to three superimposed triplet bands, which contribute to the observed spectrum. Therefore, it is practically impossible to discriminate between Co species at different sites and to quantify the percentage of occupied sites by deconvolution of the observed spectra. Nevertheless, based on spectral deconvolution, Dědeček et al. [19] described different components which were ascribed to three types of Co ions located at specific cationic sites in Co-ZSM-5: A single band at 15,000 cm −1 for α-sites; four bands at 16,000, 17,150, 18,600, 21,200 cm −1 for β-sites; and a doublet at 20,100, 22,000 cm −1 for γ-sites. This might be mathematically correct, but not from the physical point of view. Moreover, as we have shown, the triplet bands can also be properly deconvoluted on the basis of only three components (cf. Figure S1). It has to be mentioned here that for determining the location of the Co 2+ ions, it was presupposed [15,19] that all Co 2+ ions are isolated due to the exchange of protons (Brønsted sites), which are created by the incorporation of Al in the zeolite matrix. Hence, only the Co/Al ratio was taken into account. We demonstrate in the next paragraph that this supposition cannot be made without inclusion of additional characterization methods.

FTIR Studies: Pyridine and CO Adsorption
Brønsted and Lewis acidic sites can be well characterized by FTIR spectroscopic investigation of pyridine adsorption [40,41]. The typical bands resulting from pyridine adsorbed on Brønsted acid sites (PyH + ) are observed around 1540 cm −1 , while the bands from pyridine interacting with Lewis acid sites (L-Py) are detected at around 1450 cm −1 and in the region of 1625-1595 cm −1 . From the band positions in the latter region, the strength of Lewis acid sites can be evaluated [41]. The pyridine adsorbate spectra of the studied catalysts measured at 150 • C are depicted in Figure 2. As expected, the Co-free H-ZSM-5 sample shows an intense PyH + band at 1545 cm −1 , the intensity of which decreases with Co loading. Upon comparing the band intensities of the PyH + band, it is obvious that even the highly loaded sample 3.19 Co possesses a quite high number of Brønsted acid sites, although the Co/Al ratio is very close to 0.5. This means that a part of the Co 2+ ions is obviously not located on exchange positions, which points to an exchange process with a more complex stoichiometry as also observed by other authors [10].

FTIR Studies: Pyridine and CO Adsorption
Brønsted and Lewis acidic sites can be well characterized by FTIR spectroscopic investigation of pyridine adsorption [40,41]. The typical bands resulting from pyridine adsorbed on Brønsted acid sites (PyH + ) are observed around 1540 cm −1 , while the bands from pyridine interacting with Lewis acid sites (L-Py) are detected at around 1450 cm −1 and in the region of 1625-1595 cm −1 . From the band positions in the latter region, the strength of Lewis acid sites can be evaluated [41]. The pyridine adsorbate spectra of the studied catalysts measured at 150 °C are depicted in Figure 2. As expected, the Co-free H-ZSM-5 sample shows an intense PyH + band at 1545 cm −1 , the intensity of which decreases with Co loading. Upon comparing the band intensities of the PyH + band, it is obvious that even the highly loaded sample 3.19 Co possesses a quite high number of Brønsted acid sites, although the Co/Al ratio is very close to 0.5. This means that a part of the Co 2+ ions is obviously not located on exchange positions, which points to an exchange process with a more complex stoichiometry as also observed by other authors [10]. By comparing the intensities of the L-Py band of H-ZSM-5 with that of the Co-containing samples, it is seen that additional Lewis acid sites are created with increasing Co content as indicated by the bands at 1450/1610 cm −1 (Co 2+ ) and 1443/1596 cm −1 (Na + ). Furthermore, a splitting of the L-Py band in the region above 1600 cm −1 into two components at 1610 and 1616 cm −1 is observable, revealing two Co 2+ Lewis sites of different strength, possibly located at different sites in the zeolite lattice.
A suitable method for characterizing the nature of Co species is adsorption of CO at low temperatures [12,13,[42][43][44]. Thus, one can distinguish Co 2+ located at exchange positions from Co 2+ being part of oxide-like clusters because the respective νCo 2+ −CO bands appear at different positions, namely at 2204 cm −1 for Co 2+ in exchange positions and at 2194 cm −1 for Co 2+ in oxide-like clusters. The CO adsorbate spectra of the studied samples are compared in Figure 3. Here, the spectra measured at −60 °C are shown because the band stemming from the interaction of CO with OH groups at 2174 cm −1 [45] has negligible intensity at this temperature. This band is intense at the adsorption temperature of −120 °C but vanishes at higher temperatures because the interaction of CO with hydroxyl groups is not as strong as the interaction with Co 2+ ions [14]. It is obvious that all Co-zeolite samples (Figure 3a) contain Co 2+ species at exchange positions (2204 cm −1 ) as well as in oxide-like clusters (2195 cm −1 ) independent from the Co content. This is in accordance with the results of By comparing the intensities of the L-Py band of H-ZSM-5 with that of the Co-containing samples, it is seen that additional Lewis acid sites are created with increasing Co content as indicated by the bands at 1450/1610 cm −1 (Co 2+ ) and 1443/1596 cm −1 (Na + ). Furthermore, a splitting of the L-Py band in the region above 1600 cm −1 into two components at 1610 and 1616 cm −1 is observable, revealing two Co 2+ Lewis sites of different strength, possibly located at different sites in the zeolite lattice.
A suitable method for characterizing the nature of Co species is adsorption of CO at low temperatures [12,13,[42][43][44]. Thus, one can distinguish Co 2+ located at exchange positions from Co 2+ being part of oxide-like clusters because the respective νCo 2+ −CO bands appear at different positions, namely at 2204 cm −1 for Co 2+ in exchange positions and at 2194 cm −1 for Co 2+ in oxide-like clusters. The CO adsorbate spectra of the studied samples are compared in Figure 3. Here, the spectra measured at −60 • C are shown because the band stemming from the interaction of CO with OH groups at 2174 cm −1 [45] has negligible intensity at this temperature. This band is intense at the adsorption Catalysts 2020, 10, 123 6 of 12 temperature of −120 • C but vanishes at higher temperatures because the interaction of CO with hydroxyl groups is not as strong as the interaction with Co 2+ ions [14]. It is obvious that all Co-zeolite samples (Figure 3a) contain Co 2+ species at exchange positions (2204 cm −1 ) as well as in oxide-like clusters (2195 cm −1 ) independent from the Co content. This is in accordance with the results of pyridine adsorption, where two Co 2+ Lewis sites of different strength have been identified. The bands at 2177 and 2112 cm −1 in the 0.35 Co/1.98 Na sample are related to νNa + −CO and νNa + −OC vibrations, respectively [46].  In the CO adsorbate spectra of 1.79 Co-SiAl and 0.8 Co-AlSBA (Figure 3b), only Co 2+ in oxidelike clusters is observed as reflected by the band position. With respect to the UV-Vis spectra, which are similar for both types of samples (cf. Figure 1), the results of CO adsorption lead to the conclusion that the triplet bands observed in the spectra are related to tetrahedral Co 2+ sitting at exchange positions as well as in oxide-like clusters, which can be located inside as well as outside the zeolite channels, depending on the cluster size. The latter conclusion is based on CO adsorption experiments in which o-toluonitrile was preadsorbed on Co-H-MFI [12,13]. In this way, the discrimination between cationic sites inside and outside the channels was possible because the bulky molecule is not able to penetrate the channels of zeolites like ZSM-5 or MOR and therefore block respective sites. Thus, it could be demonstrated for Co-H-MFI that Co 2+ ions are distributed at both the external and internal surfaces. This has to be assumed too for the Co-ZSM-5 catalysts studied in this work.
To be sure that the findings of pyridine and CO adsorption are not influenced by the used preparation methods, being different from that described by Dědeček et al. [19] we have also prepared a sample according to this protocol. As a result, the sample 1.96 Co was obtained (cf. Table  1), the characterization results of which in comparison with those of 2.44 Co are shown in Figure 4. In the CO adsorbate spectra of 1.79 Co-SiAl and 0.8 Co-AlSBA (Figure 3b), only Co 2+ in oxide-like clusters is observed as reflected by the band position. With respect to the UV-Vis spectra, which are similar for both types of samples (cf. Figure 1), the results of CO adsorption lead to the conclusion that the triplet bands observed in the spectra are related to tetrahedral Co 2+ sitting at exchange positions as well as in oxide-like clusters, which can be located inside as well as outside the zeolite channels, depending on the cluster size. The latter conclusion is based on CO adsorption experiments in which o-toluonitrile was preadsorbed on Co-H-MFI [12,13]. In this way, the discrimination between cationic sites inside and outside the channels was possible because the bulky molecule is not able to penetrate the channels of zeolites like ZSM-5 or MOR and therefore block respective sites. Thus, it could be demonstrated for Co-H-MFI that Co 2+ ions are distributed at both the external and internal surfaces. This has to be assumed too for the Co-ZSM-5 catalysts studied in this work.
To be sure that the findings of pyridine and CO adsorption are not influenced by the used preparation methods, being different from that described by Dědeček et al. [19] we have also prepared a sample according to this protocol. As a result, the sample 1.96 Co was obtained (cf. Table 1), the characterization results of which in comparison with those of 2.44 Co are shown in Figure 4.
Thus, it could be demonstrated for Co-H-MFI that Co 2+ ions are distributed at both the external and internal surfaces. This has to be assumed too for the Co-ZSM-5 catalysts studied in this work.
To be sure that the findings of pyridine and CO adsorption are not influenced by the used preparation methods, being different from that described by Dědeček et al. [19] we have also prepared a sample according to this protocol. As a result, the sample 1.96 Co was obtained (cf. Table  1), the characterization results of which in comparison with those of 2.44 Co are shown in Figure 4. It is seen that the UV-Vis-DR as well as the pyridine and CO adsorbate spectra are very similar. While the UV-Vis spectra are nearly identical (Figure 4a), the Brønsted acidity of the 1.96 Co sample is slightly higher compared to that of 2.44 Co (Figure 4b), which might be due to the lower Co content and therefore lower exchange level. This is also true for the intensities of the observed CO adsorbate bands, whereas the intensity ratio of the bands at 2204/2195 cm −1 is nearly the same. In summary, it can be stated that in both catalysts, independent of the applied exchange procedure, Co 2+ species are located both at exchange positions and in oxide-like clusters. Hence, as already mentioned above, the respective UV-Vis spectra reflect not only Co 2+ ions located at α, β, γ sites in the internal cavities of the zeolite but also those in oxide-like clusters inside and/or outside the zeolite channels.
The existence of oxide-like clusters implies the possible presence of Co 3+ besides Co 2+ ions. Considering the fact that the samples were calcined in synthetic air at 500 • C, the presence of Co 3+ has to be taken into account, which was also proven by NO adsorption in a former study [14]. For investigating the possible influence of calcination conditions on the nature of formed Co species, we analyzed sample 1.96 Co sample by respective FTIR experiments with CO and exemplarily the 2.44 Co catalyst by UV-Vis-DRS.
In Figure 5a, the normalized CO adsorbate spectra of 1.96 Co are shown measured at −60 • C after pretreatment of the fresh, non-calcined sample in situ in the FTIR reaction cell by heating in vacuum for 1 h at 500 • C (vac.) and heating in synthetic air at 500 • C for 45 min (air). For comparison, the spectrum of the calcined (calc.) sample is also shown. The spectrum of the latter is similar to that of the vacuum-treated sample exhibiting the typical bands of CO adsorbed on Co 2+ at exchange positions as well as Co 2+ in oxide-like clusters (vide supra). In the spectrum of the air-treated sample, only Co 2+ in oxide-like clusters is detectable. The high intensity of the νOH−CO band around 2172 cm −1 in this sample in relation to the respective ν Co 2+ −CO bands suggests an agglomeration of the Co 2+ species that recreates Brønsted sites, i.e., not exchanged protons. Figure 5b shows the UV-Vis spectra of the sample 2.44 Co measured at room temperature after heating at 400 °C for 60 min followed by heating in 2 vol% O2/He at 400 °C for 45 min. After oxidation a new band around 340 nm appears, which is attributed to a ligand to metal charge transfer transition from framework oxide ions to Co 3+ ions [37,39,47]. In parallel, the intensity of the triplet band of Co 2+ decreases accordingly. This means that a part of Co 2+ species, most probably those occurring in oxidelike clusters, has been oxidized to Co 3+ .   Figure 5b shows the UV-Vis spectra of the sample 2.44 Co measured at room temperature after heating at 400 • C for 60 min followed by heating in 2 vol% O 2 /He at 400 • C for 45 min. After oxidation a new band around 340 nm appears, which is attributed to a ligand to metal charge transfer transition from framework oxide ions to Co 3+ ions [37,39,47]. In parallel, the intensity of the triplet band of Co 2+ decreases accordingly. This means that a part of Co 2+ species, most probably those occurring in oxide-like clusters, has been oxidized to Co 3+ .
These experiments reveal that the calcination/dehydration conditions influence the nature and location of formed Co species, but even treatment in vacuum at high temperature does not inevitably lead to Co 2+ located only at exchange positions. The fact that part of the Co 2+ species can be easily oxidized leads to the conclusion that these Co 2+ ions occur mainly in oxide-like agglomerates located inside and/or outside the zeolite channels. This means in terms of the UV-Vis spectra of such samples that the observed spectra represent not exclusively isolated Co 2+ species but also those located in agglomerated, oxide-like species inside and/or outside the zeolite channels. The same conclusion was drawn from the results of pyridine and CO adsorption as described above.
These findings are in accordance with those from former studies [12,25,26] revealing that the distribution of Co species is by far more complex, as deduced from previous papers in which UV-Vis, EXAFS, and XRD data have been discussed [17][18][19]48]. Insofar, a detailed analysis and quantification of Co positions in the zeolite matrix on the basis of deconvoluted UV-Vis spectra is practically not possible because the spectrum reflects Co species occupying positions inside the zeolite channels as well as positions on internal and external surfaces. This conclusion is also supported by the fact that for Co sites in zeolite cavities as well as for those dispersed on the surface of different oxide supports, similar UV-Vis spectra with the characteristic band triplet are obtained. The characteristic band splitting is due to symmetry perturbation, dynamic Jahn-Teller effect, and spin-orbit coupling [38,39] and is observed in general for Co 2+ ions independently from the surrounding matrix. For determining nature and distribution of Co 2+ species in Co-exchanged zeolites, the use of only UV-Vis-DRS cannot reflect the real situation. For this purpose, the combination of several, complementary methods have to be applied.
From the presented results the following conclusions can be derived. The observed triplet bands in the UV-Vis spectra of Co 2+ -containing samples reflect the sum of spectra of all existing Co 2+ species (isolated and oxide-like) located at different positions inside the zeolite channels as well as on internal and external surfaces. The characteristic band splitting is due to symmetry perturbation, dynamic Jahn-Teller effect, and spin-orbit coupling and is generally observed for Co 2+ ions in zeolite as well as oxide materials. Because comparable UV-Vis spectra with a characteristic band triplet is observed for Co 2+ ions independently from the surrounding matrix, the former described UV-Vis band deconvolution method for determination and quantification of individual cationic sites in zeolites is not applicable.

Materials and Methods
The Co-ZSM-5 catalysts were prepared starting from NH 4 -ZSM-5 (Zeolyst, CBV 2314, SiO 2 /Al 2 O 3 = 23). Co was introduced by wet ion-exchange (IE) using solutions of Co(NO 3 ) 2 -6H 2 O (Sigma-Aldrich, St. Louis, MO, USA) or Co(CH 3 COO) 2 -4H 2 O (Sigma-Aldrich, St. Louis, MO, USA), adapting the method described by Beznis et al. [27]. The used conditions are summarized in Table 1. The zeolite was suspended in the respective Co salt aqueous solution and preheated to 60 • C. The pH was adjusted to 6.9, and the solution was stirred for 24 h. After filtration, the material was washed with 400 mL desalinated water/g solid. After drying over night at 90 • C, the solids were calcined in synthetic air at 500 • C for 6 h. For the preparation of the Na-ZSM-5, a solution of NaNO 3 (Sigma-Aldrich, St. Louis, MO, USA) was used. The exchange procedure and subsequent washing was repeated two times. Finally, the solid was dried at 100 • C for 24 h and calcined in synthetic air at 500 • C for 6 h. For comparison, the respective H-ZSM-5 catalyst was prepared applying the same IE method but using only water. The sample 1.96 Co was prepared by the method described by Dědeček et al. [19] with adjusted pH of 5.5.
The Co-SiAl sample was prepared by incipient wetness impregnation (IWI) of a Siralox sample from Sasol (49.2% SiO 2 , 50.8% Al 2 O 3 ), which was dried overnight at 120 • C. After dropwise adding of a respective volume of a solution of Co(CH 3 COO) 2 ·4H 2 O (Carl Roth, Karlsruhe, Germany) under stirring and further stirring for 2 h, the suspension was dried overnight and calcined at 500 • C for 6 h in synthetic air.
For the preparation of Co-AlSBA, the starting Al-SBA-15 material was prepared according the method described by Wu et al. [49]. The obtained solid was dried for 12 h at 70 • C and then calcined in synthetic air at 650 • C for 16 h. This Al-SBA-15 (Si/Al = 20) was used for the IE procedure described for Co-ZSM-5 above.
The Si/Al ratio of H-ZSM-5 and the contents of Co, Al, Na were determined by ICP-OES analysis. The UV-Vis-DR spectra were recorded in diffuse reflection mode between 200 and 800 nm on a Cary 5000 spectrophotometer (Agilent, Santa Clara, CA, USA) equipped with a diffuse reflection accessory (Praying mantis) and a Harrick reaction cell. After treatment, the samples were heated at 400 • C for 30 min, and the spectra were measured at room temperature.
In situ FTIR measurements were carried out in transmission mode on a Bruker Tensor 27 spectrometer or Nicolet iS10 spectrometer (Thermo Fisher Scientific, Waltham, MA, USA) equipped with custom-made reaction cells with CaF 2 windows for adsorption studies of pyridine and CO, respectively. The sample powders were pressed into self-supporting wafers with a diameter of 20 mm and a weight of 50 mg. For each experiment, the sample was pretreated in synthetic air at 400 • C for 1 h. After cooling down to the respective adsorption temperature and evacuation of the cell a background, spectrum of the sample was recorded. Pyridine was adsorbed at 150 • C temperature until saturation. Then, the reaction cell was evacuated to remove physisorbed pyridine, and an adsorbate spectrum was recorded. For CO adsorption, a 5% CO/He mixture was used, dosed in pulses at −120 • C until saturation. To remove the physisorbed CO, the cell was evacuated, and the CO adsorbate spectrum was recorded. Subsequently, the CO desorption under vacuum was followed by continuously heating the sample and measuring a spectrum every 10 • C. Generally, the spectrum of the catalyst measured after pretreatment at adsorption temperature was subtracted from the respective adsorbate spectra of pyridine and CO.